52 results on '"Ruggero Vaglio"'
Search Results
2. A Novel Low-Cost Uroflowmetry for Patient Telemonitoring
- Author
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Savio Domenico Pandolfo, Federica Crauso, Achille Aveta, Simone Cilio, Biagio Barone, Luigi Napolitano, Antonio Scarpato, Benito Fabio Mirto, Francesco Serino, Francesco Del Giudice, Benjamin I. Chung, Fabio Crocerossa, Erika Di Zazzo, Francesco Trama, Ruggero Vaglio, Zhenjie Wu, Paolo Verze, Ciro Imbimbo, Felice Crocetto, Pandolfo, Savio Domenico, Crauso, Federica, Aveta, Achille, Cilio, Simone, Barone, Biagio, Napolitano, Luigi, Scarpato, Antonio, Mirto, Benito Fabio, Serino, Francesco, Del Giudice, Francesco, Chung, Benjamin I, Crocerossa, Fabio, Di Zazzo, Erika, Trama, Francesco, Vaglio, Ruggero, Wu, Zhenjie, Verze, Paolo, Imbimbo, Ciro, and Crocetto, Felice
- Subjects
software ,Health, Toxicology and Mutagenesis ,BPH ,Public Health, Environmental and Occupational Health ,uroflow ,urodynamic ,home uroflowmetry ,urodynamics - Abstract
Uroflowmetry (UF) is a crucial guideline-recommended tool for men with benign prostatic obstruction (BPO). Moreover, UF is a helpful decision-making tool for the management of patients with lower urinary tract symptoms (LUTS) and benign prostatic hyperplasia (BPH). In the last few years, telemedicine and telehealth have increased exponentially as cost-effective treatment options for both patients and physicians. Telemedicine and telehealth have been well positioned during the COVID-19 pandemic to prevent healthcare system overload and to ensure adequate management of patients through screening, diagnosis, and follow-up at home. In the present manuscript, the main characteristics and performance of a novel and low-cost device for home-based UF have been analyzed. The simple weight-transducer method has been applied to perform UF. An inexpensive load cell connected to a 24 bit analogic digital converter (ADC) sends data to a cloud server via SIM card or home Wi-Fi. Data are processed and shown in graphics with both volume and flow rate as a function of time, allowing for measurement of average flow rate, maximum flow rate, voided volume, and voiding time. A numerical algorithm allows for filtering of the dynamic effect due to the urine gravity acceleration and for removing the funnel to simplify the home measurement procedure. Through an online platform, the physician can see and compare each UF data. The device’s reliability has been validated in a first laboratory setting and showed excellent performance. This approach based on domiciliary tests and an online platform can revolutionize the urologic clinic landscape by offering a constant patient cost-effective follow-up, eliminating the time wasted waiting in the office setting.
- Published
- 2023
- Full Text
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3. High-Temperature Superconductor Coatings for Beam Impedance Reduction in Particle Colliders: Nonlinear Effects
- Author
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Ruggero Vaglio and Sergio Calatroni
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Physics ,Particle accelerator ,Condensed Matter Physics ,Accelerators and Storage Rings ,01 natural sciences ,Electronic, Optical and Magnetic Materials ,Vortex ,Magnetic field ,law.invention ,Computational physics ,law ,Condensed Matter::Superconductivity ,Electric field ,Magnet ,0103 physical sciences ,Physics::Accelerator Physics ,Boundary value problem ,Electrical and Electronic Engineering ,010306 general physics ,Electrical impedance ,Beam (structure) - Abstract
Coating of surfaces facing particle beams with high-temperature superconductors (HTS) for reducing the beam coupling impedance is being considered for the next generation of hadron colliders, such as the FCC-hh at CERN, where HTS would be exposed to the high-frequency wakefields generated by the particle bunches and to the strong field of the steering magnets. In this frame, we present a simple model for the calculation of the microwave response of HTS exposed to a strong external magnetic field, which takes into account the nonlinearity of the pinning potential of the vortex lattice. The equation of motion of the vortex lattice is solved in first-order approximation, and we calculate the amplitude of the third-harmonic components in the electric field produced by vortex oscillation. We deduce the time-dependent surface impedance, which could serve as a boundary condition in the simulation codes for the calculation of beam-stability phenomena in particle accelerators. Finally, time-integration of the surface impedance allows exploring the dependence of the surface impedance on surface currents, useful for analyzing the experimental results obtained using simple resonators in terms of our model.
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- 2021
4. High-Frequency Electromagnetic Properties
- Author
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Adrian Porch, Enrico Silva, and Ruggero Vaglio
- Published
- 2022
5. HE-LHC: The High-Energy Large Hadron Collider Future Circular Collider Conceptual Design Report Volume 4
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Pushpalatha C Bhat, B. Seeber, C. Pagliarone, Marco Statera, Victor P. Goncalves, Daria Astapovych, W. Bartmann, S. Iwamoto, M. Mentink, Alessandro Tricoli, E. R. Bielert, Laurent Chevalier, Patrick Koppenburg, Marco Calviani, C. Montag, P. Spiller, Jan Uythoven, P. Di Nezza, G. Guillermo Canton, B. Sailer, Markus Elsing, Sara Khatibi, Luca Vecchi, Luigi Palumbo, J. P. Penttinen, T. Podzorny, Maneesh Kumar, J. M. Rifflet, C. Kotnig, Jean Zinn-Justin, Christopher B. Verhaaren, A. Chernoded, Alessandro Bertarelli, L. M. Tkachenko, C. Koeberl, P. J. Mallon, M. Takeuchi, W. Venturini Delsolaro, G. Lamanna, S. Weinzierl, J. Gao, W. Kaabi, David D'Enterria, D. Barna, Paolo Castelnovo, Rajat Gupta, Oliver Boine-Frankenheim, Adarsh Pyarelal, Andreas Salzburger, Tessa Charles, M.E. Biagini, O. Panella, M. Stuart, A. Kollegger, V. Garcia Diaz, Olcay Bolukbasi, Maurizio Pierini, H. Aksakal, Tord Riemann, Abhishek M. Iyer, V. Shiltsev, D. Buttazzo, J. Blümlein, Prateek Agrawal, L. Sestini, Martin Bauer, Felicitas Pauss, S. Fiorendi, F. Bossu, Marco Nardecchia, C. Leonidopoulos, Wojciech Kotlarski, A. Saba, I. Bautista-Guzmán, W. Hillert, Giorgio Ambrosio, T. Lehtinen, Michael Andrew Parker, Silvia Taroni, Gian F. Giudice, Ph. Lebrun, Johann A. Briffa, T. Risselada, Giuseppe Lerner, A. Lechner, L. S. Miralles, M. Kuze, J. M. Valet, P. S. B. Dev, S. Holleis, Ph. Schwemling, M. Biglietti, S. Banerjee, Thomas Schörner-Sadenius, A. Sanz Ull, V. Tikhomirov, S. Savelyeva, Jiayin Gu, D. Zhou, Federico Ravotti, S. A. Bogacz, Daniele Mirarchi, R. Tomás García, Yann Coadou, F. Yu, Y. Cai, T. Lari, F. Holdener, D. Shwartz, C. Bhat, Ramesh Gupta, Markus Klute, E. Palmieri, P. Collier, Branislav Sitar, Yves Sirois, Livio Fanò, S. Rojas-Torres, E. Locci, Ruben Garcia Alia, I. Božović Jelisavić, R. Chehab, J. A. Aguilar-Saavedra, M. Pasquali, A. Di Cicco, Bernhard Auchmann, Klaus Heinemann, Alessia Tricomi, D. Lucchesi, B. Haerer, M. Morrone, Paolo Giacomelli, Sonia Carra, A. Senol, Ivan Koop, Luca Silvestrini, Anna Stakia, Heather Gray, E. Skordis, A. D. Kovalenko, Paul Langacker, R. Li, Bernardo Bordini, R. Rata, Arjan Verweij, Shehu S. AbdusSalam, Andrey Karyukhin, U. van Rienen, Gianluigi Arduini, Bernhard Holzer, S. A. Nikitin, S. S. Kozub, Satoshi Mishima, B. Di Micco, S. Izquierdo Bermudez, N. Pukhaeva, Nigel Watson, F. Prino, Jean-Michel Sallese, Sotirios Vlachos, Alessandro Vicini, A. Valassi, Daniel Treille, F. Dordei, A. M. Fernandez Navarro, B. Dziewit, Marcello Abbrescia, J. M. Hauptman, I. Chaikovska, Paolo Giubellino, Michael J. Baker, V.V. Kashikhin, Friedrich Lackner, Filippo Sala, A. Langner, D. Pulikowski, H. Eriksson, Matteo Turri, Andrea Wulzer, M. Aiba, Lisa Borgonovi, I. Morozov, V. Haurylavets, J. F. Croteau, S. Boselli, L. A. Gonzalez Gomez, Claudia Tambasco, F. Mahmoudi, Sébastien Descotes-Genon, A. Luciani, Pavel Piminov, M. Varasteh, T. Herzig, Sandra Aumon, Cristina Bernini, Joseph Bramante, Roberta Arnaldi, G. Zick, Daniel Schulte, R. Santoro, Anna Kulesza, I. Turk Cakir, M. Nonis, Silvia Posada Arias, Livia Soffi, T. Wojtoń, E. Cennini, Florian Bauer, B. Rousset, J.-L. Grenard, C. Neubüser, Frederic Derue, Loukas Gouskos, Rainer Wallny, G. Calderini, M. Merk, M. Mühlegger, Roberto Cimino, M. Ramsey-Musolf, P. Rebello Teles, Mario Galanti, Mikhail Shaposhnikov, A. Andreazza, Maria Vittoria Garzelli, Masaya Ishino, José W. F. Valle, Colin Bernet, G. Velev, Cristina Botta, E. Fischer, J. Malclés, Giuseppe Montenero, Tripurari Srivastava, E. Renner, Shahnam Gorgi Zadeh, D. Cantore-Cavalli, Paul Laycock, J. Komppula, Simon C. Hopkins, Helmut Burkhardt, Eric Lancon, I. Aichinger, Andre Sznajder, F. Bordry, Massimo Giovannozzi, Aidan Robson, Anna Giunta, A. Carvalho, S. Farinon, Daniel Wollmann, M. Fouaidy, Martti Raidal, R. Gerard, Giovanni Volpini, U. Niedermayer, A. Alekou, Alexander J.G. Lunt, Vincenzo Cavasinni, Andrzej Siodmok, U. Kaya, Matthias Schott, Marumi Kado, S. A. Arsenyev, José Zurita, John Osborne, Patrick Meade, Gianmarco Bovone, G. Li, Klaus Schlenga, Antti Stenvall, D. Duellmann, Werner Riegler, I. Garzia, Yasuyuki Okumura, G. Pikurs, F. Maltoni, Massimo Sorbi, M. Arzeo, B. Strauss, Y. W. Baek, Mauro Chiesa, K. Ilyina-Brunner, Javier L. Albacete, R. Farinelli, C. Pes, Nicolas Morange, S. M. Zernov, U. Wagner, Emmanuelle Perez, G. G. Da Silveira, J. Neundorf, Néstor Armesto, T. Hahn, Roman N. Lee, Roderik Bruce, B. Y. Sharkov, T. du Pree, G. Cibinetto, Evelin Meoni, R. Rinaldesi, James A. Ellison, Radim Slovak, Silvia Franchino, Mikko Laine, T. Pugnat, S. P. Das, Yuji Enari, Emanuela Barzi, Cihan Bayindir, R. Boels, Jana Faltova, M. Moreno Llácer, Scott A. Yost, Michael Spannowsky, Florian Burkart, Marcin Chrzaszcz, K. Suzuki, Luca Trentadue, S. Masciocchi, Gilad Perez, Steve Peggs, K. Sugita, Eleonora Belli, Carmine Senatore, K. Y. Oyulmaz, Aldo Deandrea, Irakli Minashvili, Desmond P. Barber, M. I. Martínez-Hernández, A. Apyan, S. Petracca, Mikael Chala, Urs Achim Wiedemann, T. Sian, Olivier Deschamps, R. Monge, G. Avrillaud, Jan Kieseler, Hubert Spiesberger, J. Maitre, G. D. Shirkov, M. Hofer, Emanuela Sirtori, Sinan Kuday, Kirill Skovpen, Sara Casalbuoni, Johann Usovitsch, N. Chen, G. Tejeda-Muñoz, F. Bellini, E. Chyhyrynets, Michael Stöger-Pollach, M. Vogel, J. G. Mendes Saraiva, A. Rivetti, M. Podeur, Luc Poggioli, V. A. Gromov, R. Sirvinskaite, S. B. Leith, Giancarlo D'Ambrosio, Tony Price, Philippe Mermod, Rabindra N. Mohapatra, T. Mitshuhashi, Koji Terashi, Leonel Ferreira, L. Vale Silva, N. Muchnoi, J. L. Stanyard, Thomas Marriott-Dodington, A. Andriatis, Oleg Solovyanov, A. Daljevec, A. Butterworth, S. Myers, D. Chanal, Tatiana Pieloni, M. Rodríguez-Cahuantzi, G. Nardini, D. Boscherini, Kazuhito Ohmi, James Molson, S. Kowalski, Christoph Haberstroh, Martin Aleksa, K. Kershaw, M. Mulder, Leonid Rivkin, G. Vorotnikov, Luigi Salvatore Esposito, J. Kalinowski, Michele Cascella, Francesco Giffoni, Alessandro Polini, Georges Azuelos, M. Prioli, Wolfgang Altmannshofer, S. K. Patra, H. J. He, J. J. Aguilera-Verdugo, Hannu Paukkunen, P. Chomaz, Shoji Asai, Nicolas Magnin, Gavin P. Salam, R. Wang, F. Avino, Alexander Romanenko, A. Rossi, Steve Muanza, Richard Ruiz, Dmitry Teytelman, S. Klöppel, S. Atieh, M. Mohammadi Najafabadi, L. Apolinario, Andrea Tesi, M. Maggiora, A. Falkowski, Janusz Gluza, M. Sauvain, Hamzeh Khanpour, S. Chance, Ansgar Denner, Ma. Greco, Andreas Papaefstathiou, Manuela Boscolo, Joydeep Chakrabortty, E. Franco, R. R. Bosley, G. Peón, Fred Olness, Simone Alioli, Andrea Gaddi, M. K. Sullivan, M. Segreti, M. Panareo, Florian Goertz, Z. G. Zhao, H. Chanal, O. Martin, P. Azzurri, Agnieszka Chmielinska, M. Kordiaczyńska, O. Brunner, J. Von Ahnen, Jose Santiago, K. Foraz, Y. Alexahin, Marcello Mannelli, Christian Schwanenberger, S. Ganjour, Simone Marzani, T. M. Taylor, S. Di Vita, J. Womersley, I. Karpov, Valentina Morretta, Saverio D'Auria, Patrick Draper, B. Hacışahinoğlu, E. Gorini, Andrew J. Long, S. La Mendola, G. Zevi Dell Porta, I. Abdyukhanov, M. Cobal, Luca Marzola, E. Rochepault, A. Kusina, German Rodrigo, R. Schmidt, Jan Steggemann, E. Premat, P. Slavich, F. Gianotti, P. Jarry, Ram Krishna Dewanjee, L. Felsberger, T. Martinez, A. Niemi, Jürgen Reuter, P. A. Bruckman de Renstrom, Ryu Sawada, J. T. Childers, Gelsomina Catalano, P. Barjhoux, O. R. Blanco-García, Pilar Hernández, H. Correia-Rodrigues, V. Ippolito, S. De Curtis, Juan Rojo, Ayberk Yilmaz, S. Baird, Morteza Khatiri Yanehsari, Enrico Scomparin, Daniel Appelö, J. Kozaczuk, Matthew Jones, B. Caiffi, C. Del Bo, Susanna Guiducci, Giuliano Panico, M. Knecht, J. Coupard, M. Ciuchini, H. Kritscher, Claire Gwenlan, P. Costa Pinto, Thibaut Lefèvre, N. Bellegarde, Christian Scheuerlein, P. Ferreira da Silva, M. Verducci, X. Ruan, H. Pikhartova, Juan M. O'Callaghan, Kazuro Furukawa, D. Saez de Jauregui, Maria Rescigno, Stephan Eisenhardt, Andrea Dainese, Z. Drásal, G. H. Corral, J. M. Camalich, John Ellis, E. Gabrielli, L. Rumyantsev, A. Caliskan, K. Brunner, K. Tang, P. Sopicki, J. Fan, Marcin Kucharczyk, S. Gorgi Zadeh, Carlos A. Salgado, Simone Bologna, Y. Muttoni, A. Chancé, Patrick Jenny, Mark Boland, G. Yang, G. Wilkinson, Roger J. Hernández-Pinto, M. Novák, Gennady Stupakov, E. Jensen, Lance D. Cooley, Torbjörn Sjöstrand, S. Su, Matthew Luzum, J. Casas, Per Osland, T. Robens, Oscar A. Sampayo, Evgeny Levichev, P. N. Ratoff, G. Rolandi, M. A. Valdivia Garcia, Anthony Keith Morley, L. van Riesen-Haupt, A. Sublet, M. A. Mazzoni, J.L. Gutierrez, A. Abramov, Abbas Kenan Ciftci, A. Provino, L. Delle Rose, John Fox, Barry M. Dillon, V. Smirnov, G. N. Taylor, Anke-Susanne Müller, C. Pira, Fulvio Piccinini, A. Faus-Golfe, Pietro Antonioli, S. Sanfilippo, Julien Cogan, A. Ribon, Andrew Hutton, Frank Zimmermann, Lev Dudko, Erez Etzion, J. Polinski, G. Bencivenni, M. Gil Costa, L. K. Gladilin, Yannis Papaphilippou, Michael Spira, Maria Paola Lombardo, M. Fiascaris, Darius A. Faroughy, S. O. Kara, Peter Braun-Munzinger, A. Wohlfahrt, A. A. Krasnov, S.A. Gourlay, W. Da Silva, Jacqueline Keintzel, Radja Boughezal, Renat Sadykov, L. R. Sulak, Valentin V. Khoze, T. Tydecks, S. Puławski, Daniel de Florian, Pedro Schwaller, A. Akay, Nicola Serra, Sukanta Dutta, Christophe Royon, Alessandro Ricci, A. Kuendig, C. G. Honorato, K. Kołodziej, L. Deniau, Michael Kramer, J. Ferradas Troitino, A. Arbey, A. M. Staśto, Marcel Demarteau, Ralph Aßmann, O. Grimm, D. Forkel-Wirth, Owain Rhodri Jones, A. M. Kolano, G. Chiarello, William Trischuk, Andrea Dell'Acqua, Elisabetta Gallo, H. Song, Frank Petriello, N. Ibarrola, C. Colldelram, A. I. Ryazanov, A. Meier, Phillip Allport, J. de Blas, S. Chattopadhyay, Massimo Florio, X. Jiang, Bertrand Baudouy, T. Otto, Tevong You, Christoph Englert, Roberto Pittau, G. M. Bilei, Matthew McCullough, N. S. Ramírez-Uribe, J. Charles, Amalia Ballarino, Federico Antinori, A. V. Kotwal, P. Le Guen, Berndt Müller, Chiara Roda, Xavier Buffat, D. K. Hong, Matthias Liepe, G. Gorine, V. A. Okorokov, D. Bozzini, N. Simand, Giuseppe Francesco Tartarelli, C. Marquet, R. Contino, A. M. Teixeira, R. Trant, Roberto Losito, M. Quispe, Valery I. Telnov, Helga Timko, D. Lissauer, Giulio Aielli, Giorgio Chiarelli, M. J. Baldwin, A. Winter, X. Sarasola, E. E. Boos, Aleandro Nisati, Cedric Garion, Monica D'Onofrio, S. M. Gascon-Shotkin, Daniele Barducci, G. Rosaz, Nathaniel Craig, L. D’Aloia Schwartzentruber, A. Falou, A. Henriques, Tobias Hurth, Michael Eisterer, Andreas Grau, Austin Ball, D. Delikaris, P. A. McIntosh, E. Graverini, Kadri Ozdemir, F. Valchkova, Marco Zanetti, Guenakh Mitselmakher, S. Albergo, Peter Levai, Caterina Vernieri, F. Stivanello, Michael Barnes, Henri Bachacou, Daniel Fournier, L. T. Wang, D. Boutin, S. Moretti, B. Riemann, Michael Murray, Aleksandr Azatov, C. T. A. Cook, Valentina Maria Cairo, J. B. De Vivie De Regie, H. Schmickler, M. Schenk, Georgios Voutsinas, André Schöning, S. G. Bondarenko, Giorgio Bellomo, Andrei Seryi, Jane Nachtman, Clement Helsens, E. De Lucia, Jakob Salfeld-Nebgen, Lorenzo Pezzotti, Z. Townsend, B. Dalena, Mogens Dam, Yasar Onel, Yi-Ming Zhong, B. Curé, A. A. Kolomiets, A. M. Valente-Feliciano, Laurette Ponce, David Olivier Jamin, P. Krkotic, Alexandre Louzguiti, Marina Putti, Holger Podlech, Petr Volkov, M. Angelucci, F. Duval, I. Hiekkanen, W. M. Yao, Giancarlo Ferrera, C. Lorin, Y. Dydyshka, Kurt R. Peters, Gergely Gabor Barnafoldi, V. Vysotsky, V. Arı, E. Pilicer, M. Chamizo-Llatas, G. Kuhlmann, Hans Quack, R. Valizadeh, Tiina Salmi, Thomas Kramer, Adam Jeff, A. Abada, J. M. Duval, J. Abelleira Fernandez, A. Leveratto, E. Tal Hod, X. Wu, Laurent Serin, Sarah Aull, Samuele Mariotto, A. Poiron, Sabine Riemann, P. Selva, V. I. Pantsyrny, Gianluca Valentino, K. Kahle, S. Aune, K. Potamianos, Eros Cazzato, M. Giovannetti, Petr Mandrik, S. Sidorov, F. Collamati, Simone Gilardoni, S. Bertolucci, Alexander V. Zlobin, Mehmet Sahin, Marco Delmastro, G. Aydın, A. Doblhammer, Alan S. Cornell, S. J. De Jong, M. Caccia, M. Lueckhof, P. Sollander, Mauro Taborelli, J. Shelton, Frank Gerigk, Robert Rimmer, Ayres Freitas, Pierluigi Bruzzone, Brajesh K. Singh, K. Keppel, N. Alipour Tehrani, C. Prasse, Louis Rinolfi, Emma Slade, W. Flieger, Alexey Dudarev, H. J. Yang, T. Köttig, L. Mether, C. Weiland, Andrea Malagoli, Sunghoon Jung, F. Conventi, I. Tropin, G. H. A. Viehhauser, Tomas Davidek, Y. O. Günaydin, Daniel Andreas Britzger, F. Toral, James John Brooke, R. Steerenberg, G. Morello, Mauro Migliorati, Alexej Grudiev, C. Tetrel, Wolfgang Höfle, J. V. Minervini, L. García Tabarés, V. Yermolchik, Claude Guyot, D. Guadagnoli, Giorgio Vallone, N. De Filippis, Oleksii Beznosov, P. Charitos, N. Schwerg, Ahmed Hammad, P. Manil, F. Niccoli, Lydia Iconomidou-Fayard, R. Aleksan, K. Hahn, P. Meridiani, Peter Skands, Tobias Golling, Lucio Rossi, G. Gobbi, Michael Hance, A. J. Barr, V. Del Duca, V. Guzey, M. Pont, Michele Selvaggi, Oliver Brüning, J. Barreiro Guimarães da Costa, A. Drago, Y. Zhang, Giovanni Punzi, Viktor Matveev, Anadi Canepa, Clemens Lange, B. L. Militsyn, Martijn Mulders, Max Klein, V. D’Auria, M. Mylona, Valeria Braccini, S. DasBakshi, David Calvet, Sophia Borowka, David Marzocca, S. Jadach, A. A. Pankov, Christophe Ochando, A. A. Tudora, I. Masina, Jure Zupan, A. Preinerstorfer, Benjamin Fuks, H. K. Soltveit, G. Rolando, E.E. Perepelkin, T. G. Rizzo, Saleh Sultansoy, Federico Roncarolo, K. Elsener, R. Q. Pan, P. Zhuang, David Attié, Jac Perez, K. Kravalis, F. Anulli, V. Ruhlmann-Kleider, S. Malvezzi, Steffen A. Bass, E. La Francesca, Heinz Pernegger, K. Grzanka, M. T. Tiirakari, Alberto Ventura, Alessandro Cerri, Marco Peruzzi, Eric Montesinos, O. Etisken, F. Grancagnolo, S. Kartal, H. Humer, Oliver Fischer, M. Primavera, Marco Toliman Lucchini, P. Vedrine, Felix Kling, M. Altınlı, Sergio Calatroni, C. Han, Olivier Leroy, R. T. D’Agnolo, N. Klinkenberg, A. Audurier, Tatsushi Nakamoto, Ali Bozbey, Bernd A. Kniehl, Carl J. Debono, I. P. J. Shipsey, Gregorio Bernardi, Paolo Nason, William James Fawcett, J. M. Jiménez, D. Denisov, M. Serluca, David Curtin, Arif Akhundov, M. García Pérez, Iacopo Vivarelli, Emanuele Bacchiocchi, Markus Zerlauth, Julia Hrdinka, F. Butin, F. Müller, D. Tikhonov, Jorg Wenninger, A. Kilic, Fabrizio Ferro, J. Tanaka, S. A. Antipov, Miroslav Atanasov, S. Kuttimalai, A. Y. Starikov, F. R. Blánquez, S. V. Furuseth, G. Gaudio, L. Malgeri, J. Curti, B. Turbiarz, S. Li, A. Romanov, Costas G. Papadopoulos, Brennan Goddard, Frank Krauss, Lidija Zivkovic, Toms Torims, Michaela Lackner, D. A. Lyubimtsev, G. Borghello, J. F. Grosse-Oetringhaus, A. Bogomyagkov, H. Duran Yildiz, N. Foppiani, Arthur Schaffer, J. Zhou, D. Liberati, Vincenzo Guidi, Naeem A. Tahir, M. Besançon, Daniel Schoerling, Joe Incandela, Giacomo Polesello, O. Cakir, I. Ruehl, Ruggero Vaglio, Z. Zhang, Bruno Spataro, Davide Tommasini, F. Millet, H. D. Yoo, Carlo V. Fiorio, S. Deghaye, C. Bozzi, A. Shivaji, G. Corcella, I. Bellafont, Valentina Mariani, D. E. Martins, Michael Syphers, C. Hati, Peter Marquard, Nicola Bacchetta, Matthew Crouch, David Woog, Oliver Kortner, A. Milanese, Ricardo Gonçalo, Guido Montagna, Mikhail Zobov, F. Bedeschi, Eugene Bulyak, M. Aburaia, R. Tenchini, G. Marchiori, H. Rafique, G. Calderola, M. Antonello, Andrea Thamm, S. Glukhov, F. Hug, Robert Ruprecht, Veysi Erkcan Ozcan, K. Lee, Angelo Infantino, V. Makarenko, Z. Nergiz, Sergei Chekanov, Benjamin C. Allanach, C. Dachauer, H. Zhang, C. Biscari, A. J. Lankford, Scott Thomas, P. Kostka, Thomas Gehrmann, O. Azzolini, M. Ploskon, S. F. Ge, K. Oide, Andrea Bastianin, Daniela Bortoletto, Ingo Schienbein, J. L. Biarrotte, M. van Leeuwen, D. Stöckinger, Harald Ita, J. Katharina Behr, A. Cholakian, T. Kwon, L. Medina, Evgeny Starchenko, G. Mancinelli, L. Zanotto, F. Menez, L. Bellagamba, J. P. Burnet, Mogens H. Jensen, J. P. Tock, V. Raginel, J. Cervantes, L. V. Kalinovskaya, S. Vallecorsa, Peter Williams, I. Leon-Monzon, Christophe Grojean, Marco Andreini, J. Perez Morales, A. O. Acar, A.S. Lobko, Tian Yu, Joachim Mnich, V. Völkl, Ievgen Dubovyk, Tatsuya Masubuchi, P. Sphicas, F. Cerutti, P. Francavilla, A. Apollonio, Sylvie Braibant-Giacomelli, D. Denegri, Elie Aslanides, M. Zahnd, J. M. Bernhardt, Maxim Perfilov, G. Felici, E. Cantergiani, M. Daibo, F. Costanza, Christopher Rogan, M. Khatiri Yanehsari, R. Kriske, Vladimir G. Baryshevsky, Curtis R. Young, T. Baumgartner, Rafael de la Torre, Yuri Nosochkov, T. P. Watson, L. Pontecorvo, D. W. Kim, Patrick Janot, Benjamin Todd, Giulia Sylva, Maciej Chorowski, Stephane Monteil, J. Proudfoot, Dmitry Shatilov, Tord Ekelof, L. Bottura, M. Ortino, Paolo Chiggiato, L. Scibile, Stefano Giagu, G. Ferrara, M. Testa, A. M. Krainer, P. A. Keinz, E. Leogrande, Johann Collot, J. Barranco García, Vera Chetvertkova, G. 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Zurita, J, Işık Üniversitesi, Mühendislik Fakültesi, İnşaat Mühendisliği Bölümü, Işık University, Faculty of Engineering, Department of Civil Engineering, Bayındır, Cihan, Universitat Politècnica de Catalunya. Departament de Teoria del Senyal i Comunicacions, Universitat Politècnica de Catalunya. RF&MW - Grup de Recerca de sistemes, dispositius i materials de RF i microones, Abada A., Abbrescia M., AbdusSalam S.S., Abdyukhanov I., Abelleira Fernandez J., Abramov A., Aburaia M., Acar A.O., Adzic P.R., Agrawal P., Aguilar-Saavedra J.A., Aguilera-Verdugo J.J., Aiba M., Aichinger I., Aielli G., Akay A., Akhundov A., Aksakal H., Albacete J.L., Albergo S., Alekou A., Aleksa M., Aleksan R., Alemany Fernandez R.M., Alexahin Y., Alia R.G., Alioli S., Alipour Tehrani N., Allanach B.C., Allport P.P., Altinli M., Altmannshofer W., Ambrosio G., Amorim D., Amstutz O., Anderlini L., Andreazza A., Andreini M., Andriatis A., Andris C., Andronic A., Angelucci M., Antinori F., Antipov S.A., Antonelli M., Antonello M., Antonioli P., Antusch S., Anulli F., Apolinario L., Apollinari G., Apollonio A., Appelo D., Appleby R.B., Apyan A., Arbey A., Arbuzov A., Arduini G., Ari V., Arias S., Armesto N., Arnaldi R., Arsenyev S.A., Arzeo M., Asai S., Aslanides E., Assmann R.W., Astapovych D., Atanasov M., Atieh S., Attie D., Auchmann B., Audurier A., Aull S., Aumon S., Aune S., Avino F., Avrillaud G., Aydin G., Azatov A., Azuelos G., Azzi P., Azzolini O., Azzurri P., Bacchetta N., Bacchiocchi E., Bachacou H., Baek Y.W., Baglin V., Bai Y., Baird S., Baker M.J., Baldwin M.J., Ball A.H., Ballarino A., Banerjee S., Barber D.P., Barducci D., Barjhoux P., Barna D., Barnafoldi G.G., Barnes M.J., Barr A., Barranco Garcia J., Barreiro Guimaraes da Costa J., Bartmann W., Baryshevsky V., Barzi E., Bass S.A., Bastianin A., Baudouy B., Bauer F., Bauer M., Baumgartner T., Bautista-Guzman I., Bayindir C., Beaudette F., Bedeschi F., Beguin M., Bellafont I., Bellagamba L., Bellegarde N., Belli E., Bellingeri E., Bellini F., Bellomo G., Belomestnykh S., Bencivenni G., Benedikt M., Bernardi G., Bernardi J., Bernet C., Bernhardt J.M., Bernini C., Berriaud C., Bertarelli A., Bertolucci S., Besana M.I., Besancon M., Beznosov O., Bhat P., Bhat C., Biagini M.E., Biarrotte J.-L., Bibet Chevalier A., Bielert E.R., Biglietti M., Bilei G.M., Bilki B., Biscari C., Bishara F., Blanco-Garcia O.R., Blanquez F.R., Blekman F., Blondel A., Blumlein J., Boccali T., Boels R., Bogacz S.A., Bogomyagkov A., Boine-Frankenheim O., Boland M.J., Bologna S., Bolukbasi O., Bomben M., Bondarenko S., Bonvini M., Boos E., Bordini B., Bordry F., Borghello G., Borgonovi L., Borowka S., Bortoletto D., Boscherini D., Boscolo M., Boselli S., Bosley R.R., Bossu F., Botta C., Bottura L., Boughezal R., Boutin D., Bovone G., Bozovic Jelisavic I., Bozbey A., Bozzi C., Bozzini D., Braccini V., Braibant-Giacomelli S., Bramante J., Braun-Munzinger P., Briffa J.A., Britzger D., Brodsky S.J., Brooke J.J., Bruce R., Bruckman De Renstrom P., Bruna E., Bruning O., Brunner O., Brunner K., Bruzzone P., Buffat X., Bulyak E., Burkart F., Burkhardt H., Burnet J.-P., Butin F., Buttazzo D., Butterworth A., Caccia M., Cai Y., Caiffi B., Cairo V., Cakir O., Calaga R., Calatroni S., Calderini G., Calderola G., Caliskan A., Calvet D., Calviani M., Camalich J.M., Camarri P., Campanelli M., Camporesi T., Canbay A.C., Canepa A., Cantergiani E., Cantore-Cavalli D., Capeans M., Cardarelli R., Cardella U., Cardini A., Carloni Calame C.M., Carra F., Carra S., Carvalho A., Casalbuoni S., Casas J., Cascella M., Castelnovo P., Castorina G., Catalano G., Cavasinni V., Cazzato E., Cennini E., Cerri A., Cerutti F., Cervantes J., Chaikovska I., Chakrabortty J., Chala M., Chamizo-Llatas M., Chanal H., Chanal D., Chance S., Chance A., Charitos P., Charles J., Charles T.K., Chattopadhyay S., Chehab R., Chekanov S.V., Chen N., Chernoded A., Chetvertkova V., Chevalier L., Chiarelli G., Chiarello G., Chiesa M., Chiggiato P., Childers J.T., Chmielinska A., Cholakian A., Chomaz P., Chorowski M., Chou W., Chrzaszcz M., Chyhyrynets E., Cibinetto G., Ciftci A.K., Ciftci R., Cimino R., Ciuchini M., Clark P.J., Coadou Y., Cobal M., Coccaro A., Cogan J., Cogneras E., Collamati F., Colldelram C., Collier P., Collot J., Contino R., Conventi F., Cook C.T.A., Cooley L., Corcella G., Cornell A.S., Corral G.H., Correia-Rodrigues H., Costanza F., Costa Pinto P., Couderc F., Coupard J., Craig N., Crespo Garrido I., Crivellin A., Croteau J.F., Crouch M., Cruz Alaniz E., Cure B., Curti J., Curtin D., Czech M., Dachauer C., D'Agnolo R.T., Daibo M., Dainese A., Dalena B., Daljevec A., Dallapiazza W., D'Aloia Schwartzentruber L., Dam M., D'Ambrosio G., Das S.P., DasBakshi S., da Silva W., da Silveira G.G., D'Auria V., D'Auria S., David A., Davidek T., Deandrea A., de Blas J., Debono C.J., De Curtis S., De Filippis N., de Florian D., Deghaye S., de Jong S.J., Del Bo C., Del Duca V., Delikaris D., Deliot F., Dell'Acqua A., Delle Rose L., Delmastro M., De Lucia E., Demarteau M., Denegri D., Deniau L., Denisov D., Denizli H., Denner A., d'Enterria D., de Rijk G., De Roeck A., Derue F., Deschamps O., Descotes-Genon S., Dev P.S.B., de Vivie de Regie J.B., Dewanjee R.K., Di Ciaccio A., Di Cicco A., Dillon B.M., Di Micco B., Di Nezza P., Di Vita S., Doblhammer A., Dominjon A., D'Onofrio M., Dordei F., Drago A., Draper P., Drasal Z., Drewes M., Duarte L., Dubovyk I., Duda P., Dudarev A., Dudko L., Duellmann D., Dunser M., du Pree T., Durante M., Duran Yildiz H., Dutta S., Duval F., Duval J.M., Dydyshka Y., Dziewit B., Eisenhardt S., Eisterer M., Ekelof T., El Khechen D., Ellis S.A., Ellis J., Ellison J.A., Elsener K., Elsing M., Enari Y., Englert C., Eriksson H., Eskola K.J., Esposito L.S., Etisken O., Etzion E., Fabbricatore P., Falkowski A., Falou A., Faltova J., Fan J., Fano L., Farilla A., Farinelli R., Farinon S., Faroughy D.A., Fartoukh S.D., Faus-Golfe A., Fawcett W.J., Felici G., Felsberger L., Ferdeghini C., Fernandez Navarro A.M., Fernandez-Tellez A., Ferradas Troitino J., Ferrara G., Ferrari R., Ferreira L., Ferreira da Silva P., Ferrera G., Ferro F., Fiascaris M., Fiorendi S., Fiorio C., Fischer O., Fischer E., Flieger W., Florio M., Fonnesu D., Fontanesi E., Foppiani N., Foraz K., Forkel-Wirth D., Forte S., Fouaidy M., Fournier D., Fowler T., Fox J., Francavilla P., Franceschini R., Franchino S., Franco E., Freitas A., Fuks B., Furukawa K., Furuseth S.V., Gabrielli E., Gaddi A., Galanti M., Gallo E., Ganjour S., Gao J., Garcia Diaz V., Garcia Perez M., Garcia Tabares L., Garion C., Garzelli M.V., Garzia I., Gascon-Shotkin S.M., Gaudio G., Gay P., Ge S.-F., Gehrmann T., Genest M.H., Gerard R., Gerigk F., Gerwig H., Giacomelli P., Giagu S., Gianfelice-Wendt E., Gianotti F., Giffoni F., Gilardoni S.S., Gil Costa M., Giovannetti M., Giovannozzi M., Giubellino P., Giudice G.F., Giunta A., Gladilin L.K., Glukhov S., Gluza J., Gobbi G., Goddard B., Goertz F., Golling T., Goncalves V.P., Goncalo R., Gonzalez Gomez L.A., Gorgi Zadeh S., Gorine G., Gorini E., Gourlay S.A., Gouskos L., Grancagnolo F., Grassellino A., Grau A., Graverini E., Gray H.M., Greco M., Grenard J.-L., Grimm O., Grojean C., Gromov V.A., Grosse-Oetringhaus J.F., Grudiev A., Grzanka K., Gu J., Guadagnoli D., Guidi V., Guiducci S., Guillermo Canton G., Gunaydin Y.O., Gupta R., Gupta R.S., Gutierrez J., Gutleber J., Guyot C., Guzey V., Gwenlan C., Haberstroh C., Hacisahinoglu B., Haerer B., Hahn K., Hahn T., Hammad A., Han C., Hance M., Hannah A., Harris P.C., Hati C., Haug S., Hauptman J., Haurylavets V., He H.-J., Hegglin A., Hegner B., Heinemann K., Heinemeyer S., Helsens C., Henriques A., Hernandez P., Hernandez-Pinto R.J., Hernandez-Sanchez J., Herzig T., Hiekkanen I., Hillert W., Hoehn T., Hofer M., Hofle W., Holdener F., Holleis S., Holzer B., Hong D.K., Honorato C.G., Hopkins S.C., Hrdinka J., Hug F., Humann B., Humer H., Hurth T., Hutton A., Iacobucci G., Ibarrola N., Iconomidou-Fayard L., Ilyina-Brunner K., Incandela J., Infantino A., Ippolito V., Ishino M., Islam R., Ita H., Ivanovs A., Iwamoto S., Iyer A., Izquierdo Bermudez S., Jadach S., Jamin D.O., Janot P., Jarry P., Jeff A., Jenny P., Jensen E., Jensen M., Jiang X., Jimenez J.M., Jones M.A., Jones O.R., Jowett J.M., Jung S., Kaabi W., Kado M., Kahle K., Kalinovskaya L., Kalinowski J., Kamenik J.F., Kannike K., Kara S.O., Karadeniz H., Karaventzas V., Karpov I., Kartal S., Karyukhin A., Kashikhin V., Katharina Behr J., Kaya U., Keintzel J., Keinz P.A., Keppel K., Kersevan R., Kershaw K., Khanpour H., Khatibi S., Khatiri Yanehsari M., Khoze V.V., Kieseler J., Kilic A., Kilpinen A., Kim Y.-K., Kim D.W., Klein U., Klein M., Kling F., Klinkenberg N., Kloppel S., Klute M., Klyukhin V.I., Knecht M., Kniehl B., Kocak F., Koeberl C., Kolano A.M., Kollegger A., Kolodziej K., Kolomiets A.A., Komppula J., Koop I., Koppenburg P., Koratzinos M., Kordiaczynska M., Korjik M., Kortner O., Kostka P., Kotlarski W., Kotnig C., Kottig T., Kotwal A.V., Kovalenko A.D., Kowalski S., Kozaczuk J., Kozlov G.A., Kozub S.S., Krainer A.M., Kramer T., Kramer M., Krammer M., Krasnov A.A., Krauss F., Kravalis K., Kretzschmar L., Kriske R.M., Kritscher H., Krkotic P., Kroha H., Kucharczyk M., Kuday S., Kuendig A., Kuhlmann G., Kulesza A., Kumar M., Kusina A., Kuttimalai S., Kuze M., Kwon T., Lackner F., Lackner M., La Francesca E., Laine M., Lamanna G., La Mendola S., Lancon E., Landsberg G., Langacker P., Lange C., Langner A., Lankford A.J., Lansberg J.P., Lari T., Laycock P.J., Lebrun P., Lechner A., Lee K., Lee S., Lee R., Lefevre T., Le Guen P., Lehtinen T., Leith S.B., Lenzi P., Leogrande E., Leonidopoulos C., Leon-Monzon I., Lerner G., Leroy O., Lesiak T., Levai P., Leveratto A., Levichev E., Li G., Li S., Li R., Liberati D., Liepe M., Lissauer D.A., Liu Z., Lobko A., Locci E., Logothetis Agaliotis E., Lombardo M.P., Long A.J., Lorin C., Losito R., Louzguiti A., Low I., Lucchesi D., Lucchini M.T., Luciani A., Lueckhof M., Lunt A.J.G., Luzum M., Lyubimtsev D.A., Maggiora M., Magnin N., Mahmoud M.A., Mahmoudi F., Maitre J., Makarenko V., Malagoli A., Malcles J., Malgeri L., Mallon P.J., Maltoni F., Malvezzi S., Malyshev O.B., Mancinelli G., Mandrik P., Manfrinetti P., Mangano M., Manil P., Mannelli M., Marchiori G., Marhauser F., Mariani V., Marinozzi V., Mariotto S., Marquard P., Marquet C., Marriott-Dodington T., Martin R., Martin O., Martin Camalich J., Martinez T., Martinez Bruzual H., Martinez-Hernandez M.I., Martins D.E., Marzani S., Marzocca D., Marzola L., Masciocchi S., Masina I., Massimiliano A., Massironi A., Masubuchi T., Matveev V.A., Mazzoni M.A., McCullough M., McIntosh P.A., Meade P., Medina L., Meier A., Meignan J., Mele B., Mendes Saraiva J.G., Menez F., Mentink M., Meoni E., Meridiani P., Merk M., Mermod P., Mertens V., Mether L., Metral E., Migliorati M., Milanese A., Milardi C., Milhano G., Militsyn B.L., Millet F., Minashvili I., Minervini J.V., Miralles L.S., Mirarchi D., Mishima S., Missiaen D.P., Mitselmakher G., Mitshuhashi T., Mnich J., Mohammadi Najafabadi M., Mohapatra R.N., Mokhov N., Molson J.G., Monge R., Montag C., Montagna G., Monteil S., Montenero G., Montesinos E., Moortgat F., Morange N., Morello G., Moreno Llacer M., Moretti M., Moretti S., Morley A.K., Moros A., Morozov I., Morretta V., Morrone M., Mostacci A., Muanza S., Muchnoi N., Muhlegger M., Mulder M., Mulders M., Muller B., Muller F., Muller A.-S., Munilla J., Murray M.J., Muttoni Y., Myers S., Mylona M., Nachtman J., Nakamoto T., Nardecchia M., Nardini G., Nason P., Nergiz Z., Nesterenko A.V., Netto J.A., Nettstrater A., Neubuser C., Neundorf J., Niccoli F., Nicrosini O., Nie Y., Niedermayer U., Niedziela J., Niemi A., Nikitin S.A., Nisati A., No J.M., Nonis M., Nosochkov Y., Novak M., Novokhatski A., O'Callaghan J.M., Ochando C., Ogur S., Ohmi K., Oide K., Okorokov V.A., Okumura Y., Oleari C., Olness F.I., Onel Y., Ortino M., Osborne J., Osland P., Otto T., Oyulmaz K.Y., Ozansoy A., Ozcan V., Ozdemir K., Pagliarone C.E., Pais da Silva H.F., Palmieri E., Palumbo L., Pampaloni A., Pan R.-Q., Panareo M., Panella O., Panico G., Panizzo G., Pankov A.A., Pantsyrny V., Papadopoulos C.G., Papaefstathiou A., Papaphilippou Y., Parker M.A., Parma V., Pasquali M., Patra S.K., Patterson R., Paukkunen H., Pauss F., Peggs S., Penttinen J.-P., Peon G., Perepelkin E.E., Perez E., Perez J.C., Perez G., Perez F., Perez Codina E., Perez Morales J., Perfilov M., Pernegger H., Peruzzi M., Pes C., Peters K., Petracca S., Petriello F., Pezzotti L., Pfeiffer S., Piccinini F., Pieloni T., Pierini M., Pikhartova H., Pikurs G., Pilicer E., Piminov P., Pira C., Pittau R., Placzek W., Plagge M., Plehn T., Pleier M.-A., Ploskon M., Podeur M., Podlech H., Podzorny T., Poggioli L., Poiron A., Polesello G., Poli Lener M., Polini A., Polinski J., Polozov S.M., Ponce L., Pont M., Pontecorvo L., Portaluri T., Potamianos K., Prasse C., Prausa M., Preinerstorfer A., Premat E., Price T., Primavera M., Prino F., Prioli M., Proudfoot J., Provino A., Pugnat T., Pukhaeva N., Pulawski S., Pulikowski D., Punzi G., Putti M., Pyarelal A., Quack H., Quispe M., Racioppi A., Rafique H., Raginel V., Raidal M., Ramirez-Uribe N.S., Ramsey-Musolf M.J., Rata R., Ratoff P., Ravotti F., Rebello Teles P., Reboud M., Redaelli S., Renner E., Renteria-Olivo A.E., Rescigno M., Reuter J., Ribon A., Ricci A.M., Riegler W., Riemann S., Riemann B., Riemann T., Rifflet J.M., Rimmer R.A., Rinaldesi R., Rinolfi L., Rios Rubiras O., Risselada T., Rivetti A., Rivkin L., Rizzo T., Robens T., Robert F., Robson A.J., Rochepault E., Roda C., Rodrigo G., Rodriguez-Cahuantzi M., Rogan C., Roig M., Rojas-Torres S., Rojo J., Rolandi G., Rolando G., Roloff P., Romanenko A., Romanov A., Roncarolo F., Rosado Sanchez A., Rosaz G., Rossi L., Rossi A., Rossmanith R., Rousset B., Royon C., Ruan X., Ruehl I., Ruhlmann-Kleider V., Ruiz R., Rumyantsev L., Ruprecht R., Ryazanov A.I., Saba A., Sadykov R., Saez de Jauregui D., Sahin M., Sailer B., Saito M., Sala F., Salam G.P., Salfeld-Nebgen J., Salgado C.A., Salini S., Sallese J.M., Salmi T., Salzburger A., Sampayo O.A., Sanfilippo S., Santiago J., Santopinto E., Santoro R., Sanz Ull A., Sarasola X., Sarpun I.H., Sauvain M., Savelyeva S., Sawada R., Sborlini G.F.R., Schaffer A., Schaumann M., Schenk M., Scheuerlein C., Schienbein I., Schlenga K., Schmickler H., Schmidt R., Schoerling D., Schoning A., Schorner-Sadenius T., Schott M., Schulte D., Schwaller P., Schwanenberger C., Schwemling P., Schwerg N., Scibile L., Sciuto A., Scomparin E., Sebastiani C., Seeber B., Segreti M., Selva P., Selvaggi M., Senatore C., Senol A., Serin L., Serluca M., Serra N., Seryi A., Sestini L., Sfyrla A., Shaposhnikov M., Shaposhnikova E., Sharkov B.Y., Shatilov D., Shelton J., Shiltsev V., Shipsey I.P., Shirkov G.D., Shivaji A., Shwartz D., Sian T., Sidorov S., Siemko A., Silvestrini L., Simand N., Simon F., Singh B.K., Siodmok A., Sirois Y., Sirtori E., Sirvinskaite R., Sitar B., Sjostrand T., Skands P., Skordis E., Skovpen K., Skrzypek M., Slade E., Slavich P., Slovak R., Smaluk V., Smirnov V., Snoeys W., Soffi L., Sollander P., Solovyanov O., Soltveit H.K., Song H., Sopicki P., Sorbi M., Spallino L., Spannowsky M., Spataro B., Sphicas P., Spiesberger H., Spiller P., Spira M., Srivastava T., Stachel J., Stakia A., Stanyard J.L., Starchenko E., Starikov A.Y., Stasto A.M., Statera M., Steerenberg R., Steggemann J., Stenvall A., Stivanello F., Stockinger D., Stoel L.S., Stoger-Pollach M., Strauss B., Stuart M., Stupakov G., Su S., Sublet A., Sugita K., Sulak L., Sullivan M.K., Sultansoy S., Sumida T., Suzuki K., Sylva G., Syphers M.J., Sznajder A., Taborelli M., Tahir N.A., Takeuchi M., Tal Hod E., Tambasco C., Tanaka J., Tang K., Tapan I., Taroni S., Tartarelli G.F., Tassielli G., Tavian L., Taylor T.M., Taylor G.N., Teixeira A.M., Tejeda-Munoz G., Telnov V.I., Tenchini R., ten Kate H.H.J., Terashi K., Tesi A., Testa M., Tetrel C., Teytelman D., Thaler J., Thamm A., Thomas S., Tiirakari M.T., Tikhomirov V., Tikhonov D., Timko H., Tisserand V., Tkachenko L.M., Tkaczuk J., Tock J.P., Todd B., Todesco E., Tomas Garcia R., Tommasini D., Tonelli G., Toral F., Torims T., Torre R., Townsend Z., Trant R., Treille D., Trentadue L., Tricoli A., Tricomi A., Trischuk W., Tropin I.S., Tuchming B., Tudora A.A., Turbiarz B., Turk Cakir I., Turri M., Tydecks T., Usovitsch J., Uythoven J., Vaglio R., Valassi A., Valchkova F., Valdivia Garcia M.A., Valente P., Valente R.U., Valente-Feliciano A.-M., Valentino G., Vale Silva L., Valet J.M., Valizadeh R., Valle J.W.F., Vallecorsa S., Vallone G., van Leeuwen M., van Rienen U.H., van Riesen-Haupt L., Varasteh M., Vecchi L., Vedrine P., Velev G., Veness R., Ventura A., Venturini Delsolaro W., Verducci M., Verhaaren C.B., Vernieri C., Verweij A.P., Verwilligen O., Viazlo O., Vicini A., Viehhauser G., Vignaroli N., Vignolo M., Vitrano A., Vivarelli I., Vlachos S., Vogel M., Vogt D.M., Volkl V., Volkov P., Volpini G., von Ahnen J., Vorotnikov G., Voutsinas G.G., Vysotsky V., Wagner U., Wallny R., Wang L.-T., Wang R., Wang K., Ward B.F.L., Watson T.P., Watson N.K., Ws Z., Weiland C., Weinzierl S., Welsch C.P., Wenninger J., Widorski M., Wiedemann U.A., Wienands H.-U., Wilkinson G., Williams P.H., Winter A., Wohlfahrt A., Wojton T., Wollmann D., Womersley J., Woog D., Wu X., Wulzer A., Yanehsari M.K., Yang G., Yang H.J., Yao W.-M., Yazgan E., Yermolchik V., Yilmaz A., Yoo H.-D., Yost S.A., You T., Young C., Yu T.-T., Yu F., Zaborowska A., Zadeh S.G., Zahnd M., Zanetti M., Zanotto L., Zawiejski L., Zeiler P., Zerlauth M., Zernov S.M., Zevi Dell Porta G., Zhang Z., Zhang Y., Zhang C., Zhang H., Zhao Z., Zhong Y.-M., Zhou J., Zhou D., Zhuang P., Zick G., Zimmermann F., Zinn-Justin J., Zivkovic L., Zlobin A.V., Zobov M., Zupan J., Zurita J., BAİBÜ, Fen Edebiyat Fakültesi, Fizik Bölümü, Denizli, Haluk, TOBB ETU, Faculty of Engineering, Department of Electrical & Electronics Engineering, TOBB ETU, Faculty of Engineering, Department of Material Science & Nanotechnology Engineering, TOBB ETÜ, Mühendislik Fakültesi, Elektrik ve Elektronik Mühendisliği Bölümü, TOBB ETÜ, Mühendislik Fakültesi, Malzeme Bilimi ve Nanoteknoloji Mühendisliği Bölümü, Bozbey, Ali, Sultansoy, Saleh, Özdemir, Kadri, Giresun Üniversitesi, UCL - SST/IRMP - Institut de recherche en mathématique et physique, and Ege Üniversitesi
- Subjects
Beam losses ,IMPACT ,Physics::Instrumentation and Detectors ,Physics beyond the Standard Model ,EVENT BUILDER ,hadron collider ,General Physics and Astronomy ,Mathematics and natural science: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP] ,01 natural sciences ,7. Clean energy ,law.invention ,Subatomär fysik ,chemistry.chemical_compound ,Conceptual design ,Colliding beam accelerators ,law ,HE-LHC ,Subatomic Physics ,General Materials Science ,Hadron colliders ,Física::Física de partícules::Hadrons [Àrees temàtiques de la UPC] ,Large Hadron Collider ,Acceleradors de partícules ,Physics ,Settore FIS/01 - Fisica Sperimentale ,Beams (radiation) ,Settore FIS/02 - Fisica Teorica, Modelli e Metodi Matematici ,Upgrade ,Impact ,collimators ,partikkelfysikk ,Future Circular Collider ,High-Energy ,Systems engineering ,HE-LHC: The High-Energy Large Hadron Collider ,Col·lisionadors d'hadrons ,Applied physics ,Collimators ,Socio-culturale ,Fizik ,Hadrons ,Accelerator Physics and Instrumentation ,HE-LHC physics ,Condensed Matter::Materials Science ,0103 physical sciences ,Physics::Atomic and Molecular Clusters ,beam losses ,ddc:530 ,High Energy Physics ,partikkelakselerator ,Physical and Theoretical Chemistry ,Niobium-tin ,010306 general physics ,Collider ,Particle Physics ,Beams (radiation) | Collimators | Beam losses ,Energies::Energia nuclear [Àrees temàtiques de la UPC] ,Large Hadron Collider HE-LHC ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,Colliders (Nuclear physics) ,Acceleratorfysik och instrumentering ,Event builder ,Accelerators and Storage Rings ,Particle accelerators ,chemistry ,Experimental High Energy Physics ,Physics::Accelerator Physics ,High Energy Physics::Experiment ,Future Colliders - Abstract
Authors: A. AbadaM. AbbresciaS. S. AbdusSalamI. AbdyukhanovJ. Abelleira FernandezA. AbramovM. AburaiaA. O. AcarP. R. AdzicP. AgrawalJ. A. Aguilar-SaavedraJ. J. Aguilera-VerdugoM. AibaI. AichingerG. AielliA. AkayA. AkhundovH. AksakalJ. L. AlbaceteS. AlbergoA. AlekouM. AleksaR. AleksanR. M. Alemany FernandezY. AlexahinR. G. AlíaS. AlioliN. Alipour TehraniB. C. AllanachP. P. AllportM. AltınlıW. AltmannshoferG. AmbrosioD. AmorimO. AmstutzL. AnderliniA. AndreazzaM. AndreiniA. AndriatisC. AndrisA. AndronicM. AngelucciF. AntinoriS. A. AntipovM. AntonelliM. AntonelloP. AntonioliS. AntuschF. AnulliL. ApolinárioG. ApollinariA. ApollonioD. AppelöR. B. ApplebyA. ApyanA. ApyanA. ArbeyA. ArbuzovG. ArduiniV. ArıS. AriasN. ArmestoR. ArnaldiS. A. ArsenyevM. ArzeoS. AsaiE. AslanidesR. W. AßmannD. AstapovychM. AtanasovS. AtiehD. AttiéB. AuchmannA. AudurierS. AullS. AumonS. AuneF. AvinoG. AvrillaudG. AydınA. AzatovG. AzuelosP. AzziO. AzzoliniP. AzzurriN. BacchettaE. BacchiocchiH. BachacouY. W. BaekV. BaglinY. BaiS. BairdM. J. BakerM. J. BaldwinA. H. BallA. BallarinoS. BanerjeeD. P. BarberD. BarducciP. BarjhouxD. BarnaG. G. BarnaföldiM. J. BarnesA. BarrJ. Barranco GarcíaJ. Barreiro Guimarães da CostaW. BartmannV. BaryshevskyE. BarziS. A. BassA. BastianinB. BaudouyF. BauerM. BauerT. BaumgartnerI. Bautista-GuzmánC. BayındırF. BeaudetteF. BedeschiM. BéguinI. BellafontL. BellagambaN. BellegardeE. BelliE. BellingeriF. BelliniG. BellomoS. BelomestnykhG. BencivenniM. BenediktG. BernardiJ. BernardiC. BernetJ. M. BernhardtC. BerniniC. BerriaudA. BertarelliS. BertolucciM. I. BesanaM. BesançonO. BeznosovP. BhatC. BhatM. E. BiaginiJ. -L. BiarrotteA. Bibet ChevalierE. R. BielertM. BigliettiG. M. BileiB. BilkiC. BiscariF. BisharaO. R. Blanco-GarcíaF. R. BlánquezF. BlekmanA. BlondelJ. BlümleinT. BoccaliR. BoelsS. A. BogaczA. BogomyagkovO. Boine-FrankenheimM. J. BolandS. BolognaO. BolukbasiM. BombenS. BondarenkoM. BonviniE. BoosB. BordiniF. BordryG. BorghelloL. BorgonoviS. BorowkaD. BortolettoD. 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DelmastroE. De LuciaM. DemarteauD. DenegriL. DeniauD. DenisovH. DenizliA. DennerD. d’EnterriaG. de RijkA. De RoeckF. DerueO. DeschampsS. Descotes-GenonP. S. B. DevJ. B. de Vivie de RégieR. K. DewanjeeA. Di CiaccioA. Di CiccoB. M. DillonB. Di MiccoP. Di NezzaS. Di VitaA. DoblhammerA. DominjonM. D’OnofrioF. DordeiA. DragoP. DraperZ. DrasalM. DrewesL. DuarteI. DubovykP. DudaA. DudarevL. DudkoD. DuellmannM. DünserT. du PreeM. DuranteH. Duran YildizS. DuttaF. DuvalJ. M. DuvalY. DydyshkaB. DziewitS. EisenhardtM. EistererT. EkelofD. El KhechenS. A. EllisJ. EllisJ. A. EllisonK. ElsenerM. ElsingY. EnariC. EnglertH. ErikssonK. J. EskolaL. S. EspositoO. EtiskenE. EtzionP. FabbricatoreA. FalkowskiA. FalouJ. FaltovaJ. FanL. FanòA. FarillaR. FarinelliS. FarinonD. A. FaroughyS. D. FartoukhA. Faus-GolfeW. J. FawcettG. FeliciL. FelsbergerC. FerdeghiniA. M. Fernandez NavarroA. Fernández-TéllezJ. Ferradas TroitinoG. FerraraR. FerrariL. FerreiraP. Ferreira da SilvaG. FerreraF. FerroM. FiascarisS. FiorendiC. FiorioO. FischerE. FischerW. FliegerM. FlorioD. FonnesuE. FontanesiN. FoppianiK. ForazD. Forkel-WirthS. ForteM. FouaidyD. FournierT. FowlerJ. FoxP. FrancavillaR. FranceschiniS. FranchinoE. FrancoA. FreitasB. FuksK. FurukawaS. V. FurusethE. GabrielliA. GaddiM. GalantiE. GalloS. GanjourJ. GaoJ. GaoV. Garcia DiazM. García PérezL. García TabarésC. GarionM. V. GarzelliI. GarziaS. M. Gascon-ShotkinG. GaudioP. GayS. -F. GeT. GehrmannM. H. GenestR. GerardF. GerigkH. GerwigP. GiacomelliS. GiaguE. Gianfelice-WendtF. GianottiF. GiffoniS. S. GilardoniM. Gil CostaM. GiovannettiM. GiovannozziP. GiubellinoG. F. GiudiceA. GiuntaL. K. GladilinS. GlukhovJ. GluzaG. GobbiB. GoddardF. GoertzT. GollingV. P. GoncalvesR. GonçaloL. A. Gonzalez GomezS. Gorgi ZadehG. GorineE. GoriniS. A. GourlayL. GouskosF. GrancagnoloA. GrassellinoA. GrauE. GraveriniH. M. GrayMa. GrecoMi. GrecoJ. -L. GrenardO. GrimmC. GrojeanV. A. GromovJ. F. Grosse-OetringhausA. GrudievK. GrzankaJ. GuD. GuadagnoliV. GuidiS. GuiducciG. Guillermo CantonY. O. GünaydinR. GuptaR. S. GuptaJ. GutierrezJ. GutleberC. GuyotV. GuzeyC. GwenlanC. HaberstrohB. HacışahinoğluB. HaererK. HahnT. HahnA. HammadC. HanM. HanceA. HannahP. C. HarrisC. HatiS. HaugJ. HauptmanV. HaurylavetsH. -J. HeA. HegglinB. HegnerK. HeinemannS. HeinemeyerC. HelsensA. HenriquesA. HenriquesP. HernandezR. J. Hernández-PintoJ. Hernandez-SanchezT. HerzigI. HiekkanenW. HillertT. HoehnM. HoferW. HöfleF. HoldenerS. HolleisB. HolzerD. K. HongC. G. HonoratoS. C. HopkinsJ. HrdinkaF. HugB. HumannH. HumerT. HurthA. HuttonG. IacobucciN. IbarrolaL. Iconomidou-FayardK. Ilyina-BrunnerJ. IncandelaA. InfantinoV. IppolitoM. IshinoR. IslamH. ItaA. IvanovsS. IwamotoA. IyerS. Izquierdo BermudezS. JadachD. O. JaminP. JanotP. JarryA. JeffP. JennyE. JensenM. JensenX. JiangJ. M. JiménezM. A. JonesO. R. JonesJ. M. JowettS. JungW. KaabiM. KadoK. KahleL. KalinovskayaJ. KalinowskiJ. F. KamenikK. KannikeS. O. KaraH. KaradenizV. KaraventzasI. KarpovS. KartalA. KaryukhinV. KashikhinJ. Katharina BehrU. KayaJ. KeintzelP. A. KeinzK. KeppelR. KersevanK. KershawH. KhanpourS. KhatibiM. Khatiri YanehsariV. V. KhozeJ. KieselerA. KilicA. KilpinenY. -K. KimD. W. KimU. KleinM. KleinF. KlingN. KlinkenbergS. KlöppelM. KluteV. I. KlyukhinM. KnechtB. KniehlF. KocakC. KoeberlA. M. KolanoA. KolleggerK. KołodziejA. A. KolomietsJ. KomppulaI. KoopP. KoppenburgM. KoratzinosM. KordiaczyńskaM. KorjikO. KortnerP. KostkaW. KotlarskiC. KotnigT. KöttigA. V. KotwalA. D. KovalenkoS. KowalskiJ. KozaczukG. A. KozlovS. S. KozubA. M. KrainerT. KramerM. KrämerM. KrammerA. A. KrasnovF. KraussK. KravalisL. KretzschmarR. M. KriskeH. KritscherP. KrkoticH. KrohaM. KucharczykS. KudayA. KuendigG. KuhlmannA. KuleszaM. KumarM. KumarA. KusinaS. KuttimalaiM. KuzeT. KwonF. LacknerM. LacknerE. La FrancescaM. LaineG. LamannaS. La MendolaE. LançonG. LandsbergP. LangackerC. LangeA. LangnerA. J. LankfordJ. P. LansbergT. LariP. J. LaycockP. LebrunA. LechnerK. LeeS. LeeR. LeeT. LefevreP. Le GuenT. LehtinenS. B. LeithP. LenziE. LeograndeC. LeonidopoulosI. Leon-MonzonG. LernerO. LeroyT. LesiakP. LévaiA. LeverattoE. LevichevG. LiS. LiR. LiD. LiberatiM. LiepeD. A. LissauerZ. LiuA. LobkoE. LocciE. Logothetis AgaliotisM. P. LombardoA. J. LongC. LorinR. LositoA. LouzguitiI. LowD. LucchesiM. T. LucchiniA. LucianiM. LueckhofA. J. G. LuntM. LuzumD. A. LyubimtsevM. MaggioraN. MagninM. A. MahmoudF. MahmoudiJ. MaitreV. MakarenkoA. MalagoliJ. MalclésL. MalgeriP. J. MallonF. MaltoniS. MalvezziO. B. MalyshevG. MancinelliP. MandrikP. ManfrinettiM. ManganoP. ManilM. MannelliG. MarchioriF. MarhauserV. MarianiV. MarinozziS. MariottoP. MarquardC. MarquetT. Marriott-DodingtonR. MartinO. MartinJ. Martin CamalichT. MartinezH. Martinez BruzualM. I. Martínez-HernándezD. E. MartinsS. MarzaniD. MarzoccaL. MarzolaS. MasciocchiI. MasinaA. MassimilianoA. MassironiT. MasubuchiV. A. MatveevM. A. MazzoniM. McCulloughP. A. McIntoshP. MeadeL. MedinaA. MeierJ. MeignanB. MeleJ. G. Mendes SaraivaF. MenezM. MentinkE. MeoniP. MeridianiM. MerkP. MermodV. MertensL. MetherE. MétralM. MiglioratiA. MilaneseC. MilardiG. MilhanoB. L. MilitsynF. MilletI. MinashviliJ. V. MinerviniL. S. MirallesD. MirarchiS. MishimaD. P. MissiaenG. MitselmakherT. MitshuhashiJ. MnichM. Mohammadi NajafabadiR. N. MohapatraN. MokhovJ. G. MolsonR. MongeC. MontagG. MontagnaS. MonteilG. MonteneroE. MontesinosF. MoortgatN. MorangeG. MorelloM. Moreno LlácerM. MorettiS. MorettiA. K. MorleyA. MorosI. MorozovV. MorrettaM. MorroneA. MostacciS. MuanzaN. MuchnoiM. MühleggerM. MulderM. MuldersB. MüllerF. MüllerA. -S. MüllerJ. MunillaM. J. MurrayY. MuttoniS. MyersM. MylonaJ. NachtmanT. NakamotoM. NardecchiaG. NardiniP. NasonZ. NergizA. V. NesterenkoJ. A. NettoA. NettsträterC. NeubüserJ. NeundorfF. NiccoliO. NicrosiniY. NieU. NiedermayerJ. NiedzielaA. NiemiS. A. NikitinA. NisatiJ. M. NoM. NonisY. NosochkovM. NovákA. NovokhatskiJ. M. O’CallaghanC. OchandoS. OgurK. OhmiK. OideV. A. OkorokovY. OkumuraC. OleariF. I. OlnessY. OnelM. OrtinoJ. OsborneP. OslandT. OttoK. Y. OyulmazA. OzansoyV. ÖzcanK. ÖzdemirC. E. PagliaroneH. F. Pais da SilvaE. PalmieriL. PalumboA. PampaloniR. -Q. PanM. PanareoO. PanellaG. PanicoG. PanizzoA. A. PankovV. PantsyrnyC. G. PapadopoulosA. PapaefstathiouY. PapaphilippouM. A. ParkerV. ParmaM. PasqualiS. K. PatraR. PattersonH. PaukkunenF. PaussS. PeggsJ. -P. PenttinenG. PeónE. E. PerepelkinE. PerezJ. C. PerezG. PerezF. PérezE. Perez CodinaJ. Perez MoralesM. PerfilovH. PerneggerM. PeruzziC. PesK. PetersS. PetraccaF. PetrielloL. PezzottiS. PfeifferF. PiccininiT. PieloniM. PieriniH. PikhartovaG. PikursE. PilicerP. PiminovC. PiraR. PittauW. PłaczekM. PlaggeT. PlehnM. -A. PleierM. PłoskońM. PodeurH. PodlechT. PodzornyL. PoggioliA. PoironG. PoleselloM. Poli LenerA. PoliniJ. PolinskiS. M. PolozovL. PonceM. PontL. PontecorvoT. PortaluriK. PotamianosC. PrasseM. PrausaA. PreinerstorferE. PrematT. PriceM. PrimaveraF. PrinoM. PrioliJ. ProudfootA. ProvinoT. PugnatN. PukhaevaS. PuławskiD. PulikowskiG. PunziM. PuttiA. PyarelalH. QuackM. QuispeA. RacioppiH. RafiqueV. RaginelM. RaidalN. S. Ramírez-UribeM. J. Ramsey-MusolfR. RataP. RatoffF. RavottiP. Rebello TelesM. ReboudS. RedaelliE. RennerA. E. Rentería-OlivoM. RescignoJ. ReuterA. RibonA. M. RicciW. RieglerS. RiemannB. RiemannT. RiemannJ. M. RiffletR. A. RimmerR. RinaldesiL. RinolfiO. Rios RubirasT. RisseladaA. RivettiL. RivkinT. RizzoT. RobensF. RobertA. J. RobsonE. RochepaultC. RodaG. RodrigoM. Rodríguez-CahuantziC. RoganM. RoigS. Rojas-TorresJ. RojoG. RolandiG. RolandoP. RoloffA. RomanenkoA. RomanovF. RoncaroloA. Rosado SanchezG. RosazL. RossiA. RossiR. RossmanithB. RoussetC. RoyonX. RuanI. RuehlV. Ruhlmann-KleiderR. RuizL. RumyantsevR. RuprechtA. I. RyazanovA. SabaR. SadykovD. Saez de JaureguiM. SahinB. SailerM. SaitoF. SalaG. P. SalamJ. Salfeld-NebgenC. A. SalgadoS. SaliniJ. M. SalleseT. SalmiA. SalzburgerO. A. SampayoS. SanfilippoJ. SantiagoE. SantopintoR. SantoroA. Sanz UllX. SarasolaI. H. SarpünM. SauvainS. SavelyevaR. SawadaG. F. R. SborliniA. SchafferM. SchaumannM. SchenkC. ScheuerleinI. SchienbeinK. SchlengaH. SchmicklerR. SchmidtD. SchoerlingA. SchoningT. Schörner-SadeniusM. SchottD. SchulteP. SchwallerC. SchwanenbergerP. SchwemlingN. SchwergL. ScibileA. SciutoE. ScomparinC. SebastianiB. SeeberM. SegretiP. SelvaM. SelvaggiC. SenatoreA. SenolL. SerinM. SerlucaN. SerraA. SeryiL. SestiniA. SfyrlaM. ShaposhnikovE. ShaposhnikovaB. Y. SharkovD. ShatilovJ. SheltonV. ShiltsevI. P. ShipseyG. D. ShirkovA. ShivajiD. ShwartzT. SianS. SidorovA. SiemkoL. SilvestriniN. SimandF. SimonB. K. SinghA. SiódmokY. SiroisE. SirtoriR. SirvinskaiteB. SitarT. SjöstrandP. SkandsE. SkordisK. SkovpenM. SkrzypekE. SladeP. SlavichR. SlovakV. SmalukV. SmirnovW. SnoeysL. SoffiP. SollanderO. SolovyanovH. K. SoltveitH. SongP. SopickiM. SorbiL. SpallinoM. SpannowskyB. SpataroP. SphicasH. SpiesbergerP. SpillerM. SpiraT. SrivastavaJ. StachelA. StakiaJ. L. StanyardE. StarchenkoA. Y. StarikovA. M. StaśtoM. StateraR. SteerenbergJ. SteggemannA. StenvallF. StivanelloD. StöckingerL. S. StoelM. Stöger-PollachB. StraussM. StuartG. StupakovS. SuA. SubletK. SugitaL. SulakM. K. SullivanS. SultansoyT. SumidaK. SuzukiG. SylvaM. J. SyphersA. SznajderM. TaborelliN. A. TahirM. TakeuchiE. Tal HodC. TambascoJ. TanakaK. TangI. TapanS. TaroniG. F. TartarelliG. TassielliL. TavianT. M. TaylorG. N. TaylorA. M. TeixeiraG. Tejeda-MuñozV. I. TelnovR. TenchiniH. H. J. ten KateK. TerashiA. TesiM. TestaC. TetrelD. TeytelmanJ. ThalerA. ThammS. ThomasM. T. TiirakariV. TikhomirovD. TikhonovH. TimkoV. TisserandL. M. TkachenkoJ. TkaczukJ. P. TockB. ToddE. TodescoR. Tomás GarciaD. TommasiniG. TonelliF. ToralT. TorimsR. TorreZ. TownsendR. TrantD. TreilleL. TrentadueA. TricoliA. TricomiW. TrischukI. S. TropinB. TuchmingA. A. TudoraB. TurbiarzI. Turk CakirM. TurriT. TydecksJ. UsovitschJ. UythovenR. VaglioA. ValassiF. ValchkovaM. A. Valdivia GarciaP. ValenteR. U. ValenteA. -M. Valente-FelicianoG. ValentinoL. Vale SilvaJ. M. ValetR. ValizadehJ. W. F. ValleS. VallecorsaG. ValloneM. van LeeuwenU. H. van RienenL. van Riesen-HauptM. VarastehL. VecchiP. VedrineG. VelevR. VenessA. VenturaW. Venturini DelsolaroM. VerducciC. B. VerhaarenC. VernieriA. P. VerweijO. VerwilligenO. ViazloA. ViciniG. ViehhauserN. VignaroliM. VignoloA. VitranoI. VivarelliS. VlachosM. VogelD. M. VogtV. VölklP. VolkovG. VolpiniJ. von AhnenG. VorotnikovG. G. VoutsinasV. VysotskyU. WagnerR. WallnyL. -T. WangR. WangK. WangB. F. L. WardT. P. WatsonN. K. WatsonZ. WsC. WeilandS. WeinzierlC. P. WelschJ. WenningerM. WidorskiU. A. WiedemannH. -U. WienandsG. WilkinsonP. H. WilliamsA. WinterA. WohlfahrtT. WojtońD. WollmannJ. WomersleyD. WoogX. WuA. WulzerM. K. YanehsariG. YangH. J. YangW. -M. YaoE. YazganV. YermolchikA. YilmazA. YilmazH. -D. YooS. A. YostT. YouC. YoungT. -T. YuF. YuA. ZaborowskaS. G. ZadehM. ZahndM. ZanettiL. ZanottoL. ZawiejskiP. ZeilerM. ZerlauthS. M. ZernovG. Zevi Dell PortaZ. ZhangY. ZhangC. ZhangH. ZhangZ. ZhaoY. -M. ZhongJ. ZhouD. ZhouP. ZhuangG. ZickF. ZimmermannEmail authorJ. Zinn-JustinL. ZivkovicA. V. ZlobinM. ZobovJ. ZupanJ. Zuritathe FCC Collaboration, In response to the 2013 Update of the European Strategy for Particle Physics (EPPSU), the Future Circular Collider (FCC) study was launched as a world-wide international collaboration hosted by CERN. The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. This document constitutes the fourth volume of the FCC Conceptual Design Report, devoted to the High-Energy Large Hadron Collider HE-LHC. It summarizes the HE-LHC physics discovery opportunities, presents the HE-LHC accelerator design, performance reach, and operation plan, discusses the underlying technologies, the civil engineering and technical infrastructure, and also sketches a possible implementation. Combining ingredients from the Large Hadron Collider (LHC), the high-luminosity LHC upgrade and adding novel technologies and approaches, the HE-LHC design aims at a hadron collider with about twice the centre-of-mass collision energy that the LHC can reach. Its performance aims at exploring physics beyond the Standard Model, signi cantly extending the LHC's direct and indirect sensitivity to new physics and discoveries.
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- 2020
6. Future Circular Collider beam screen: progress on Tl-1223 HTS coating
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Johannes Bernardi, Emilio Bellingeri, A. Moros, C. Bernini, B Henrist, A. Saba, A. Leveratto, Sigrid Holleis, Carlo Ferdeghini, S Fernandez-Peña, Ruggero Vaglio, Mario Putti, Sergio Calatroni, M Himmerlich, and Michael Eisterer
- Subjects
Materials science ,High-temperature superconductivity ,engineering.material ,01 natural sciences ,7. Clean energy ,Future Circular Collider ,law.invention ,high temperature superconductors ,thallium ,Coating ,law ,0103 physical sciences ,Materials Chemistry ,Electrical and Electronic Engineering ,010306 general physics ,Thesaurus (information retrieval) ,010308 nuclear & particles physics ,Metals and Alloys ,Condensed Matter Physics ,Engineering physics ,Accelerators and Storage Rings ,Tl-1223 ,Ceramics and Composites ,engineering ,Physics::Accelerator Physics ,Beam (structure) - Abstract
Thallium-1223, a superconductor with high critical temperature (T c ∼ 120 K) and high irreversibility line is a promising alternative to copper layers as a low surface impedance material in particle accelerator components. In the existing design of the Future Circular Collider (FCC-hh), for reasons of cryogenic efficiency and vacuum stability, the beam screen that shields the dipoles from synchrotron radiation has to stay at best in the temperature range between 40 and 60 K, in which copper surface resistance might be too high to prevent beam instabilities due to wakefields. This paper reports the progress on the realization of thallium-1223 based high temperature superconducting (HTS) coatings realized by electrochemical deposition. The study of the Tl-1223 phase has been carried out on precursor-pellets and films. Transport characterization revealing a very high irreversibility line and also high local critical currents obtained from Scanning Hall Probe Microscopy (SHPM) measurements will be shown. A first analysis of compatibility in vacuum has been carried out and the generation of secondary electrons (SEY) has been investigated as well. The encouraging results, although not conclusive, will state that thallium-based phase could be suitable for the proposed application.
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- 2020
7. Surface Resistance of Superconductors in the Presence of a DC Magnetic Field: Frequency and Field Intensity Limits
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Ruggero Vaglio, Sergio Calatroni, Calatroni, Sergio, and Vaglio, Ruggero
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particle accelerator ,Niobium ,chemistry.chemical_element ,Condensed Matter Physic ,02 engineering and technology ,01 natural sciences ,Future Circular Collider ,law.invention ,law ,Condensed Matter::Superconductivity ,0103 physical sciences ,Electrical and Electronic Engineering ,010306 general physics ,Sheet resistance ,Superconductivity ,Physics ,Condensed matter physics ,Electronic, Optical and Magnetic Material ,Particle accelerator ,High-temperature superconductor (HTS) ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,Magnetic flux ,surface impedance ,Electronic, Optical and Magnetic Materials ,Magnetic field ,chemistry ,Physics::Accelerator Physics ,0210 nano-technology ,Beam (structure) - Abstract
We revisit the classical rigid-fluxon model which describes the effect of an applied magnetic flux on the RF surface resistance of a superconductor and discuss explicit formulations for a few limit cases. As an application, we discuss the role of magnetic flux on the enhanced surface resistance of RF accelerating cavities based on niobium, depending on its material properties. We also assess the conditions for the use of high-temperature superconductors for carrying the beam image RF currents in future high-energy circular hadron colliders such as the future circular collider being studied at CERN.
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- 2017
8. Simple model for the rf field amplitude dependence of the trapped flux sensitivity in superconducting rf cavities
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Ruggero Vaglio and S. Calatroni
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Accelerator Physics (physics.acc-ph) ,Nuclear and High Energy Physics ,cond-mat.supr-con ,Physics and Astronomy (miscellaneous) ,FOS: Physical sciences ,Flux ,01 natural sciences ,Superconductivity (cond-mat.supr-con) ,0103 physical sciences ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,Sensitivity (control systems) ,010306 general physics ,physics.acc-ph ,Superconductivity ,Physics ,Condensed matter physics ,010308 nuclear & particles physics ,Condensed Matter - Superconductivity ,Order (ring theory) ,Surfaces and Interfaces ,Dissipation ,Accelerators and Storage Rings ,Magnetic flux ,Amplitude ,lcsh:QC770-798 ,Physics - Accelerator Physics ,Pinning force - Abstract
The improvement of the performance of superconducting rf cavities has recently motivated a considerable research effort in order to elucidate the effect of trapped magnetic flux on the surface resistance ${R}_{s}$. In this paper, we show that, by introducing a nonlinear pinning force in the Gittleman-Rosenblum equations for the rf power dissipation due to a trapped magnetic flux in a superconductor, we can empirically describe the linear dependence on the rf field amplitude ${B}_{rf0}$ of the additional surface resistance ${R}_{fl}$. We also show that the proportionality between the rf-field-dependent and -independent terms ${R}_{fl}^{1}$ and ${R}_{fl}^{0}$ and the frequency dependence of ${R}_{fl}^{1}$ follow naturally from this approach.
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- 2019
9. Perylene-diimide molecules with cyano functionalization for electron-transporting transistors
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Ruggero Vaglio, Federico Chianese, F. Chiarella, Antonio Cassinese, Mario Barra, Barra, Mario, Chiarella, Fabio, Chianese, Federico, Vaglio, Ruggero, and Cassinese, Antonio
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Materials science ,Fabrication ,Computer Networks and Communications ,lcsh:TK7800-8360 ,Nanotechnology ,Thin film characterization ,02 engineering and technology ,010402 general chemistry ,Thin film deposition ,01 natural sciences ,chemistry.chemical_compound ,Diimide ,Molecule ,Thin film ,Electrical and Electronic Engineering ,Contact resistance ,lcsh:Electronics ,electron-transporting devices ,021001 nanoscience & nanotechnology ,Evaporation (deposition) ,0104 chemical sciences ,Computer Networks and Communication ,chemistry ,Control and Systems Engineering ,Hardware and Architecture ,Signal Processing ,Surface modification ,0210 nano-technology ,Perylene ,Electron-transporting device - Abstract
Core-cyanated perylene diimide (PDI_CY) derivatives are molecular compounds exhibiting an uncommon combination of appealing properties, including remarkable oxidative stability, high electron affinities, and excellent self-assembling properties. Such features made these compounds the subject of study for several research groups aimed at developing electron-transporting (n-type) devices with superior charge transport performances. After about fifteen years since the first report, field-effect transistors based on PDI_CY thin films are still intensely investigated by the scientific community for the attainment of n-type devices that are able to balance the performances of the best p-type ones. In this review, we summarize the main results achieved by our group in the fabrication and characterization of transistors based on PDI8-CN2 and PDIF-CN2 molecules, undoubtedly the most renowned compounds of the PDI_CY family. Our attention was mainly focused on the electrical properties, both at the micro and nanoscale, of PDI8-CN2 and PDIF-CN2 films deposited using different evaporation techniques. Specific topics, such as the contact resistance phenomenon, the bias stress effect, and the operation in liquid environment, have been also analyzed.
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- 2019
10. Advances in the study of HTS superconductors for the beam impedance mitigation in CERN-FCC: the thermal runaway problem
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Sergio Calatroni, Ruggero Vaglio, Vaglio, R., and Calatroni, S.
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010302 applied physics ,Superconductivity ,Materials science ,Large Hadron Collider ,Thermal runaway ,Thermal resistance ,General Physics and Astronomy ,Superconducting magnet ,01 natural sciences ,Future Circular Collider ,law.invention ,Computational physics ,law ,0103 physical sciences ,Physics::Accelerator Physics ,General Materials Science ,Physical and Theoretical Chemistry ,010306 general physics ,Collider ,Beam (structure) - Abstract
In CERN Future Circular Collider (FCC-hh), a possible next-generation high-energy hadron–hadron collider, the center-of-mass collision energy will be of 100 TeV, with opposite proton beams of 50 TeV steered in a 100-km circumference tunnel by 16 T superconducting magnets. The synchrotron radiation, emitted by the beams, is absorbed by a beam-facing screen held at 50 K. The surface impedance of this screen has a strong impact on the beam stability, and copper at 50 K allows only tight beam stability margin. This has motivated investigating the possibility of high-temperature superconductors (HTSs) coatings on the beam screen internal surface, as a possible solution. In this communication, we will briefly review the general theory of the surface resistance of HTS in high field, low frequency regimes and will present specific calculations for REBCO commercial tapes that represent one of the possible envisaged solutions. The possible “thermal runaway” problems arising using REBCO tapes are then discussed. In particular, the upper limit for the transverse thermal resistance that guarantees thermal stability is quantitatively determined as a function of the REBCO superconducting properties at FCC operating conditions.
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- 2019
11. Thallium-based high-temperature superconductors for beam impedance mitigation in the Future Circular Collider
- Author
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Carlo Ferdeghini, Mario Putti, T. Baumgartner, Michael Eisterer, Ruggero Vaglio, Emilio Bellingeri, Sergio Calatroni, Calatroni, S., Bellingeri, E., Ferdeghini, C., Putti, M., Vaglio, R., Baumgartner, T., and Eisterer, M.
- Subjects
Materials Chemistry2506 Metals and Alloys ,High-temperature superconductivity ,Synchrotron radiation ,Ceramics and Composite ,02 engineering and technology ,Superconducting magnet ,Condensed Matter Physic ,01 natural sciences ,Future Circular Collider ,law.invention ,Nuclear physics ,law ,Beam screen ,0103 physical sciences ,HTS coating ,Materials Chemistry ,FCC ,Thallium ,Electrical and Electronic Engineering ,010306 general physics ,Collider ,Electrical impedance ,Physics ,Large Hadron Collider ,Metals and Alloys ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,Engineering physics ,Accelerators and Storage Rings ,Tl-1223 ,Ceramics and Composites ,2506 ,Physics::Accelerator Physics ,0210 nano-technology ,Beam (structure) - Abstract
CERN has recently started a design study for a possible next-generation high-energy hadron–hadron collider (Future Circular Collider—FCC-hh). The FCC-hh study calls for an unprecedented center-of-mass collision energy of 100 TeV, achievable by colliding counter-rotating proton beams with an energy of 50 TeV steered in a 100 km circumference tunnel by superconducting magnets which produce a dipole field of 16 T. The beams emit synchrotron radiation at high power levels, which, to optimize cryogenic efficiency, is absorbed by a beam-facing screen, coated with copper, and held at 50 K in the current design. The surface impedance of this screen has a strong impact on beam stability, and copper at 50 K allows for a limited beam stability margin only. This motivates the exploration of whether high-temperature superconductors (HTS), the only known materials possibly having a surface impedance lower than copper under the required operating conditions, would represent a viable alternative. This paper summarizes the FCC-hh requirements and focuses on identifying the best possible HTS material for this purpose. It reviews in particular the properties of Tl-based HTS, and discusses the consequent motivation for developing a deposition process for such compounds, which should be scalable to the size of the FCC components.
- Published
- 2017
12. The Aladin2 experiment: status and perspectives
- Author
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Giuseppe Bimonte, Evgeni Il'ichev, Luigi Rosa, Giampiero Esposito, Ruggero Vaglio, Francesco Tafuri, Ornella Scaldaferri, Enrico Calloni, D. Born, Uve Hubner, Bimonte, GIUSEPPE ROBERTO, Born, D., Calloni, Enrico, Esposito, G., Ill’Ichev, E., Rosa, Luigi, Scaldaferri, O., Tafuri, Francesco, Vaglio, Ruggero, Hubner, U., Giuseppe, Bimonte, Detlef, Born, Enrico, Calloni, Giampiero, Esposito, Evgeni, I'Lichev, Luigi, Rosa, Ornella, Scaldaferri, and RUGGERO VAGLIO AND UWE, Hubner
- Subjects
rigid cavity ,Superconductivity ,Physics ,Quantum Physics ,Phase transition ,FOS: Physical sciences ,General Physics and Astronomy ,Statistical and Nonlinear Physics ,Signal ,Term (time) ,Casimir effect ,Quantum electrodynamics ,Casimir energy ,Sensitivity (control systems) ,Quantum Physics (quant-ph) ,Critical field ,Mathematical Physics ,Quantum fluctuation - Abstract
Aladin2 is an experiment devoted to the first measurement of variations of Casimir energy in a rigid cavity. The main scientific motivation relies on the possibility of the first demonstration of a phase transition influenced by vacuum fluctuations. The guiding principle of the measurement, based on the behaviour of the critical field for an in-cavity superconducting film, will be only briefly recalled. In this paper, after an introduction to the long term motivations, the experimental apparatus and the results of the first measurement of sensitivity will be presented in detail, particularly in comparison with the expected signal. Last, the most important steps towards the final measurement will be discussed., Comment: Talk given by Calloni at QFEXT05 Conference in Barcelona: Quantum Field Theory Under the Influence of External Conditions
- Published
- 2006
13. Performance analysis of superconducting rf cavities for the CERN rare isotope accelerator
- Author
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G. Rosaz, A. Sublet, Sergio Calatroni, Ruggero Vaglio, W. Venturini Delsolaro, Vincenzo Palmieri, Akira Miyazaki, Calatroni, S., Miyazaki, A., Rosaz, G., Sublet, A., Venturini Delsolaro, W., Vaglio, R., and Palmieri, V.
- Subjects
010302 applied physics ,Superconductivity ,Nuclear and High Energy Physics ,Materials science ,Large Hadron Collider ,Physics and Astronomy (miscellaneous) ,Thermal resistance ,Niobium ,chemistry.chemical_element ,Surfaces and Interfaces ,01 natural sciences ,Accelerators and Storage Rings ,Nuclear physics ,chemistry ,Sputtering ,Cryomodule ,0103 physical sciences ,lcsh:QC770-798 ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,010306 general physics ,Beam (structure) ,Sheet resistance ,Nuclear and High Energy Physic - Abstract
The first cryomodule of the new HIE-ISOLDE rare isotope accelerator has recently been commissioned with beam at CERN, with the second cryomodule ready for installation. Each cryomodule contains five superconducting low-beta quarter wave cavities, produced with the technology of sputtering a thin niobium film onto the copper substrate ($\mathrm{Nb}/\mathrm{Cu}$). This technology has several benefits compared to the bulk niobium solution, but also drawbacks among which the most relevant is the increase of surface resistance with accelerating field. Recent work has established the possible connection of this phenomenon to local defects in the $\mathrm{Nb}/\mathrm{Cu}$ interface, which may lead to increased thermal impedance and thus local thermal runaway. We have analyzed the performance of the HIE-ISOLDE cavities series production, as well as of a few prototypes', in terms of this model, and found a strong correlation between the rf properties and one of the model characteristic quantities, namely the total surface having increased interface thermal impedance.
- Published
- 2016
14. Corrections to 'Surface Resistance of Superconductors in the Presence of a DC Magnetic Field: Frequency and Field Intensity Limits' [Aug 17 Art. no. 3500506]
- Author
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Sergio Calatroni and Ruggero Vaglio
- Subjects
Superconductivity ,Physics ,Field intensity ,Condensed matter physics ,010502 geochemistry & geophysics ,Condensed Matter Physics ,01 natural sciences ,Electronic, Optical and Magnetic Materials ,Magnetic field ,0103 physical sciences ,Electrical and Electronic Engineering ,010306 general physics ,Sheet resistance ,0105 earth and related environmental sciences - Published
- 2017
15. Thermal contact resistance at the Nb/Cu interface as a limiting factor for sputtered thin film RF superconducting cavities
- Author
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Ruggero Vaglio, Vincenzo Palmieri, Palmieri, V., and Vaglio, Ruggero
- Subjects
Superconductivity ,Thermal contact conductance ,Materials science ,Condensed matter physics ,010308 nuclear & particles physics ,Metals and Alloys ,Niobium ,Thermal contact ,chemistry.chemical_element ,Substrate (electronics) ,Condensed Matter Physics ,01 natural sciences ,Copper ,chemistry ,0103 physical sciences ,Materials Chemistry ,Ceramics and Composites ,Interfacial thermal resistance ,Electrical and Electronic Engineering ,Thin film ,010306 general physics - Abstract
The 'Q-slope' problem has so far strongly limited the application of niobium thin film sputtered copper cavities in high field accelerators. In the present paper, based on experimental evidence, we consider the hypothesis that the Q-slope is related to enhanced thermal boundary resistance R Nb/Cu at the Nb/Cu interface, due to poor thermal contact between film and substrate. We have developed a simple model that directly connects the Q versus E acc curves to the distribution function f(R Nb/Cu) of R Nb/Cu values at the Nb/Cu interface over the cavity surface. Starting from different Q versus E acc experimental curves from different sources, using typical 'inverse problem' methods, we deduce the corresponding distribution functions generating those curves. The results show, for all the examined cases, very similar functional dependences of f(R Nb/Cu) and prove that, to describe the experimental Q versus E acc curves, it is sufficient to assume that only a small fraction of the film over the cavity surface is in poor thermal contact with the substrate. The whole body of information and data reported seems to indicate that the main origin of the Q-slope in thin film cavities is related to bad adhesion at the Nb/Cu interface. Strategies to solve the Q-slope problem improving the film adhesion are finally delineated.
- Published
- 2015
16. A simple interpretation of the growth of scientific/ technological research impact leading to hype-type evolution curves
- Author
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M. Campani, Ruggero Vaglio, and Vaglio, Ruggero
- Subjects
FOS: Computer and information sciences ,Sociology of scientific knowledge ,Physics - Physics and Society ,Research impact ,Scope (project management) ,Computer science ,Interpretation (philosophy) ,FOS: Physical sciences ,General Social Sciences ,Computer Science - Digital Libraries ,Physics and Society (physics.soc-ph) ,Library and Information Sciences ,Type (model theory) ,Bibliometrics ,Growth curve (statistics) ,Field (geography) ,Computer Science Applications ,Epistemology ,Hype curves ,Digital Libraries (cs.DL) ,Mathematical economics ,Simple (philosophy) - Abstract
The empirical and theoretical justification of Gartner hype curves is a very relevant open question in the field of Technological Life Cycle analysis. The scope of the present paper is to introduce a simple model describing the growth of scientific/technological research impact, in the specific case where science is the main source of a new idea driving a technological development, leading to hype-type evolution curves. The main idea of the model is that, in a first stage, the growth of the scientific interest of a new specific field (as can be measured by publication numbers) basically follows the classical logistic growth curve. At a second stage, starting at a later trigger time, the technological development based on that scientific idea (as can be measured by patent deposits) can be described as the integral (in a mathematical sense) of the first curve, since technology is based on the overall accumulated scientific knowledge. The model is tested through a bibliometric analysis of the publication and patent deposit rate for Organic Light Emitting Diodes (OLED) scientific research and technology, as well as for other emerging technologies., 8 pages, 2 figures
- Published
- 2015
17. Growth and characterization of hybrid (CnH2n+1NH3)2CuCl4 self-assembled films
- Author
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Carmela Aruta, Mario Barra, T. Besagni, Antonio Cassinese, F. Licci, F. Chiarella, P. Ferro, Andrea Zappettini, Ruggero Vaglio, Chiarella, F, Zappettini, A, Ferro, P, Besagni, T, Licci, F, Cassinese, Antonio, Barra, M, Vaglio, Ruggero, and Aruta, C.
- Subjects
Diffraction ,Morphology (linguistics) ,Chemistry ,Analytical chemistry ,General Chemistry ,Substrate (electronics) ,Surface finish ,Condensed Matter Physics ,Characterization (materials science) ,Electrical resistivity and conductivity ,Organic chemistry ,General Materials Science ,Copper chloride ,Absorption (electromagnetic radiation) - Abstract
Films of self-assembled (CnH2n+1NH3)2CuCl4 (1 ≤ n ≤ 4) hybrid structures were prepared and characterized with respect to the structure, the optical absorption and the transport properties. The films were deposited in-situ, by the Single Source Thermal Ablation (SSTA) procedure on glassy, crystalline and polymeric substrates. The film structure and the morphology, thickness and roughness were almost independent on the substrate. X-ray diffraction analysis showed that the films are well crystallized and c-axis oriented. Optical absorption measurements in the 9000-52000 cm–1 interval confirmed the good quality of the films. They also proved that the absorption phenomena are mainly related to the inorganic CuCl64– clusters and to their geometrical configuration. Due to the high optical quality of the films novel absorption features were revealed. The electrical transport measurements indicated that the films are insulating at 300 K, with resistivity values ranging between 103 and 104 Ωcm. (© 2005 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)
- Published
- 2005
18. HIGH QUALITY FULLY IN-SITU <font>MgB</font>2 THIN FILMS OBTAINED BY DC MAGNETRON SPUTTERING
- Author
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F. Chiarella, Luigi Maritato, M. G. Maglione, Matteo Salvato, Ruggero Vaglio, Serghej L. Prischepa, R. Di Capua, Maglione, M. G., Chiarella, F., DI CAPUA, Roberto, Vaglio, Ruggero, Salvato, M., Maritato, L., and Prischepa, S. L.
- Subjects
Residual resistivity ,Materials science ,Electrical resistivity and conductivity ,Sputtering ,Cavity magnetron ,Analytical chemistry ,Surface roughness ,Sapphire ,Magnesium diboride, thin films, magnetron sputtering, resistivity measurements ,Statistical and Nonlinear Physics ,Thin film ,Sputter deposition ,Condensed Matter Physics - Abstract
MgB 2 thin films were grown in-situ at INFM- University of Naples by a magnetron sputtering technique in a UHV system (10-7 Pa) equipped with 3 focused 2′′ magnetron sources (a stoichiometric MgB 2 and metallic Mg and B targets by Superconducting Components Inc.). The substrates (sapphire or MgO) were placed "on axis" at 7 cm from the target surface on the surface of a molybdenum heater that could be operated up to 1000°C under vacuum. Best results were obtained codepositing MgB 2 and Mg at equal sputtering power (500W) for 10 min on cold substrates, resulting in a Mg rich Mg-B precursor film. The films were then annealed inhyphen;situ at 830°C for 10 min in a In sealed Nb box in presence of saturated Mg vapor. The process is highly reproducible and can be easily scaled to produce large area films. The resulting films were about 1μm thick, with 100nm surface roughness as measured by AFM Resistive transition showed a maximum T c of 35 K and a transition width lower than 0.5 K. The residual resistivity ratio was 1.6 for the best sample. Resistivity measurements in external magnetic field up to 8 T have been performed both in parallel and perpendicular configuration. The upper critical magnetic field vs. temperature behavior has been determined from the experimental data and the superconducting anisotropy has been calculated for samples with different T c .
- Published
- 2003
19. [Untitled]
- Author
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E. Di Gennaro, Ruggero Vaglio, F. Chiarella, Antonello Andreone, and G. Lamura
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Superconductivity ,Materials science ,Physics and Astronomy (miscellaneous) ,Condensed matter physics ,Band gap ,Dielectric resonator ,Condensed Matter Physics ,Electronic, Optical and Magnetic Materials ,Condensed Matter::Materials Science ,Amplitude ,Sputtering ,Condensed Matter::Superconductivity ,Granularity ,Single crystal ,Microwave - Abstract
The electrodynamic response at 20 GHz of c-axis oriented MgB2 superconducting thin films is reported. Mg-rich Mg-B precursor samples were grown on MgO and Al2O3 single crystal substrates by a d.c. planar magnetron sputtering technique, and subsequently annealed in situ at 800°C for 10 min in a In-sealed Nb box in the presence of saturated Mg vapor. The films were characterized by a variety of structural and electronic techniques including XRD, EDS, STM-AFM analyses, and transport measurements. The dependence of the surface impedance from temperature and radiofrequency (r.f.) field amplitude was measured via a dielectric resonator technique. Temperature data clearly confirm the s-wave nature of the newly discovered superconductor, even if the value of the energy gap is smaller than BCS prediction. An effective two-band model can be applied to quantitatively explain the experimental results. In spite of previous reports claiming the absence of weak link behavior in MgB2, the power dependence show that granularity governs the performance of these films in the microwave region.
- Published
- 2003
20. Superconducting dual-mode dual-stage cross-slotted filters
- Author
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Mario Barra, Matteo Cirillo, Gaetano Panariello, Ruggero Vaglio, Roberto Russo, Antonio Cassinese, M., Barra, Cassinese, Antonio, M., Cirillo, G., Panariello, R., Russo, and Vaglio, Ruggero
- Subjects
Superconductivity ,Engineering ,business.industry ,C band ,Electrical engineering ,Dual mode ,Condensed Matter Physics ,Chebyshev filter ,Atomic and Molecular Physics, and Optics ,Electronic, Optical and Magnetic Materials ,Electrical and Electronic Engineering ,business ,Realization (systems) ,Microwave ,Dual stage - Abstract
This Letter reports on the design and realization of HTS dual-mode cross-slotted filters presenting a more compact size if compared with the traditional dual-mode patch filters. Dual-stage filters operating in C band and presenting Chebyshev or quasi-elliptical responses have been realized and tested by using YBa2Cu3O7-x (YBCO) films. © 2002 Wiley Periodicals, Inc. Microwave Opt Technol Lett 33: 389–392, 2002>; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.10331
- Published
- 2002
21. Transport properties of ZrN superconducting films
- Author
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Ruggero Vaglio, Maria Iavarone, M. Grimsditch, Antonio Cassinese, S. Uran, Cassinese, A., Iavarone, M., Vaglio, Ruggero, Grimsditch, M., and Uran, S.
- Subjects
Superconductivity ,Materials science ,Condensed matter physics ,Phonon ,Scattering ,Zirconium nitride ,Nitride ,Condensed Matter::Materials Science ,chemistry.chemical_compound ,symbols.namesake ,chemistry ,Electrical resistivity and conductivity ,Condensed Matter::Superconductivity ,symbols ,Saturation (magnetic) ,Raman scattering - Abstract
Superconductivity in nitrides presents intriguing aspects related to the role of optical phonons. In the present paper we report on high-quality superconducting zirconium nitride film preparation and characterization (including Raman scattering) as well as on both dc and microwave frequency transport properties. The high-temperature dc resistivity shows no evidence of saturation effects, possibly due to the low electron-phonon coupling. Surface impedance data can be well fitted by the standard BCS expressions. The data provide further evidence of the ''conventional'' nature of superconductivity in these compounds.
- Published
- 2000
22. Transport properties of refractory and ceramic superconducting materials
- Author
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F. Fontana, Ruggero Vaglio, and Maria Iavarone
- Subjects
Superconductivity ,Materials science ,Mechanical Engineering ,Transition temperature ,Metallurgy ,Mineralogy ,Yba2cu3o7 δ ,Mechanics of Materials ,Electrical resistivity and conductivity ,visual_art ,visual_art.visual_art_medium ,General Materials Science ,Critical current ,Ceramic ,Thin film ,Refractory (planetary science) - Published
- 1996
23. Observation and explanation of critical current anomalous peaks in transport measurements of YBCO coated conductors
- Author
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Antonio Cassinese, S. Zannella, L. Gianni, and Ruggero Vaglio
- Subjects
Superconductivity ,Materials science ,Condensed matter physics ,Condensed Matter::Superconductivity ,Materials Chemistry ,Metals and Alloys ,Ceramics and Composites ,Critical current ,Electrical and Electronic Engineering ,Current (fluid) ,Condensed Matter Physics ,Electrical conductor ,Voltage - Abstract
Anomalous voltage peaks have been observed below the critical current in dc transport measurements of superconducting YBCO coated conductors for specific contact arrangements. Using a simple concentrated constant-equivalent circuit, it is predicted that current redistributions due to non-homogeneities in the sample may explain the observed effect.
- Published
- 2004
24. Magnetic penetration depth measurements on high-temperature superconducting thin films and their implications
- Author
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F. Miletto Granozio, Ruggero Vaglio, Antonio Cassinese, C. Cantoni, A. Di Chiara, Antonello Andreone, and Marco Salluzzo
- Subjects
Superconducting coherence length ,Superconductivity ,Materials science ,Condensed matter physics ,Meissner effect ,Condensed Matter::Superconductivity ,London penetration depth ,General Physics and Astronomy ,Cuprate ,BCS theory ,Atmospheric temperature range ,Penetration depth - Abstract
Accurate measurements of the magnetic penetration depth λ of n-doped (Nd1.85Ce0.15CuO4−δ) and p-doped (YBa2Cu3O7−δ) high-temperature superconductors using a microscopic resonator are reported. The temperature dependence λ(T) in Nd1.85Ce0.15CuO4−δ films shows that the electrodynamics of this cuprate is well described in the framework of the BCS theory, with a single-valued finite-gap ratio 2Δ0/K B T c≈3.1 throughout the entire temperature range below T c. In contrast, measurements of λ(T) in YBa2Cu3O7−δ cannot be fitted to a BCS temperature dependence derived from a single energy gap. In the low-temperature region, a quadratic behaviour of the penetration depth is observed, instead of the usual exponential law. These peculiar features are discussed in the light of recent theoretical models predicting a different symmetry state for the high-T c superconductors.
- Published
- 1994
25. Scanning tunnelling spectroscopy study of paramagnetic superconducting β'-ET(4)[(H(3)O)Fe(C(2)O(4))(3)]·C(6)H(5)Br crystals
- Author
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Carlos Giménez-Saiz, Marco Affronte, Marco Salluzzo, Alessandro Gambardella, Eugenio Coronado, Carlos J. Gómez-García, Ruggero Vaglio, R. Di Capua, A., Gambardella, M., Salluzzo, DI CAPUA, Roberto, M., Affronte, C., Giménez Saiz, C. J., Gòmez Garcìa, E., Coronado, and Vaglio, Ruggero
- Subjects
Superconducting coherence length ,Superconductivity ,Materials science ,Condensed matter physics ,Transition temperature ,Organic superconductors, order parameter, scanning tunneling spectroscopy ,Analytical chemistry ,BCS theory ,Condensed Matter Physics ,Paramagnetism ,Electrical resistivity and conductivity ,Condensed Matter::Superconductivity ,Density of states ,General Materials Science ,Phase diagram - Abstract
Scanning tunnelling spectroscopy (STS) and microscopy (STM) were performed on the paramagnetic molecular superconductor β''-ET(4)[(H(3)O)Fe(C(2)O(4))(3)]·C(6)H(5)Br. Under ambient pressure, this compound is located near the boundary separating superconducting and insulating phases of the phase diagram. In spite of a strongly reduced critical temperature T(c) (T(c) = 4.0 K at the onset, zero resistance at T(c) = 0.5 K), the low temperature STS spectra taken in the superconducting regions show strong similarities with the higher T(c) ET κ-derivatives series. We exploited different models for the density of states (DOS), with conventional and unconventional order parameters to take into account the role played by possible magnetic and non-magnetic disorder in the superconducting order parameter. The values of the superconducting order parameter obtained by the fitting procedure are close to the ones obtained on more metallic and higher T(c) organic crystals and far above the BCS values, suggesting an intrinsic role of disorder in the superconductivity of organic superconductors and a further confirmation of the non-conventional superconductivity in such compounds.
- Published
- 2011
26. In-situ Investigation of the Early Stage of TiO2 epitaxy on (001) SrTiO3
- Author
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Zoran Ristić, N. Lampis, Marco Salluzzo, Milan Radovic, F. Miletto Granozio, Ruggero Vaglio, R. Di Capua, M., Radovic, M., Salluzzo, Z., Ristic, DI CAPUA, Roberto, N., Lampi, Vaglio, Ruggero, and F., Miletto Granozio
- Subjects
Ceramics ,Materials science ,Photoemission spectroscopy ,Analytical chemistry ,General Physics and Astronomy ,FOS: Physical sciences ,02 engineering and technology ,Substrate (electronics) ,Epitaxy ,01 natural sciences ,Crystals ,Pulsed laser deposition ,Diffusion ,Scanning probe microscopy ,Doped Srtio3 ,Phase (matter) ,0103 physical sciences ,Physical and Theoretical Chemistry ,010306 general physics ,Films ,Condensed Matter - Materials Science ,Laalo3 ,Low-energy electron diffraction ,Materials Science (cond-mat.mtrl-sci) ,TiO2, epitaxial growth, pulsed laser deposition, photoemission spectroscopy, scanning probe microscopy ,021001 nanoscience & nanotechnology ,Surfaces ,Electron diffraction ,Gas ,Molecular-Beam Epitaxy ,0210 nano-technology ,Substrate - Abstract
We report on a systematic study of the growth of epitaxial TiO2 films deposited by pulsed laser deposition on Ti-terminated (001) SrTiO3 single crystals. By using in-situ reflection high energy electron diffraction, low energy electron diffraction, x-ray photoemission spectroscopy and scanning probe microscopy, we show that the stabilization of the anatase (001) phase is preceded by the growth of a pseudomorphic Sr-Ti-O intermediate layer, with a thickness between 2 and 4 nm. The data demonstrate that the formation of this phase is related to the activation of long range Sr migration from the substrate to the film. The role of interface Gibbs energy minimization, as a driving force for Sr diffusion, is discussed. Our results enrich the phase diagram of the Sr-Ti-O system under epitaxial strain opening the roudeficient SrTiO phase., Comment: 8 pages, 7 figures
- Published
- 2011
- Full Text
- View/download PDF
27. Anisotropic transport properties in tilted c-axis MgB2 thin films
- Author
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M. Putti, Regina Ciancio, Yi Cui, Maria Iavarone, Pasquale Orgiani, R. Di Capua, V. Ferrando, Ruggero Vaglio, Qi Li, Ke Chen, Xiaoxing Xi, Luigi Maritato, Orgiani, P., Chen, Ke, Cui, Yi, Li, Qi, Ferrando, V., Putti, M., Iavarone, M., DI CAPUA, Roberto, Ciancio, R., Vaglio, Ruggero, Maritato, L., Xi, X. X., Orgiani, Pasquale, Ke, Chen, Cui, Y. i., Q. i., Li, V., Ferrando, M., Putti, M., Iavarone, R., Ciancio, L., Maritato, and X. X., Xi
- Subjects
Materials science ,02 engineering and technology ,Chemical vapor deposition ,Substrate (electronics) ,01 natural sciences ,Condensed Matter::Materials Science ,chemistry.chemical_compound ,Optics ,Planar ,Electrical resistivity and conductivity ,Condensed Matter::Superconductivity ,0103 physical sciences ,Materials Chemistry ,Magnesium diboride ,Magnesium diboride, anisotropic transport, two gap superconductivity ,Electrical and Electronic Engineering ,Thin film ,DEPOSITION ,010306 general physics ,Anisotropy ,Superconductivity ,Condensed matter physics ,business.industry ,superconductivity ,Metals and Alloys ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,chemistry ,Ceramics and Composites ,0210 nano-technology ,business - Abstract
We report on superconducting magnesium diboride MgB(2) thin films grown on both YSZ and MgO substrates, with two different orientations, namely [110] and [211]. MgB(2) off-axis growth mode (namely, with the c-axis tilted with respect to the film surface's normal) is achievable on these substrates. Depending on the type and orientation of the substrate, tilting angle can be varied. As a consequence of tilted growth, anisotropic transport properties are observed. In very thin films, resistance measurements provide an estimate of the resistivity anisotropic ratio rho(c)/rho(ab), where rho(c) is the resistivity along the c axis and rho(ab) is the in-plane resistivity. All these findings clearly demonstrate that tilted MgB(2) films offer new exciting possibilities to both investigate intrinsic fundamental properties of MgB(2) and to explore possible applications in planar superconducting devices
- Published
- 2010
28. Combined experimental and theoretical investigation of optical, structural, and electronic properties ofCH3NH3SnX3thin films(X=Cl,Br)
- Author
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Giovanni Cantele, F. Chiarella, Ivo Borriello, Antonio Cassinese, Domenico Ninno, Andrea Zappettini, Ruggero Vaglio, and Francesca Licci
- Subjects
Crystallography ,Valence (chemistry) ,Materials science ,Condensed matter physics ,Vacuum deposition ,Band gap ,Ab initio quantum chemistry methods ,Lattice (order) ,Density of states ,Density functional theory ,Thin film ,Condensed Matter Physics ,Electronic, Optical and Magnetic Materials - Abstract
Well-oriented thin films of methyl-ammonium trihalogenostannates $\mathrm{C}{\mathrm{H}}_{3}\mathrm{N}{\mathrm{H}}_{3}\mathrm{Sn}{X}_{3}$ compounds $(X=\mathrm{Cl},\mathrm{Br})$ are grown by the single source thermal ablation technique. Optical absorption and structural analysis of $\mathrm{C}{\mathrm{H}}_{3}\mathrm{N}{\mathrm{H}}_{3}\mathrm{Sn}{X}_{3}$ thin films are combined with ab initio calculations in order to clarify their electronic properties and the role of the organic cation. The structural calculations reproduce well the measured lattice parameters, and optical measurements reveal a direct gap absorption onset for both compounds, in agreement with the calculated band structures. It turns out from projected density of states analysis that the valence and conduction bands take negligible contribution from the methylammonium. It is inferred that the band gap mainly depends on the ionicity and size of the inorganic cage $\mathrm{Sn}{X}_{3}$.
- Published
- 2008
29. Scanning tunneling spectroscopy on neutron irradiated MgB2 thin films
- Author
-
Valeria Ferrando, Marina Putti, Ruggero Vaglio, Xiaoxing Xi, Roberto Di Capua, Carlo Ferdeghini, Hans U. Aebersold, Marco Salluzzo, DI CAPUA, Roberto, Salluzzo, Marco, Vaglio, Ruggero, Ferdeghini, Carlo, Ferrando, Valeria, Putti, Marina, Xi, Xiaoxing, and Aebersold, Hans U.
- Subjects
inorganic chemicals ,Materials science ,Band gap ,MgB2, effect of disorder, STM, tunneling measurements ,MgB2 ,Scanning tunneling spectroscopy ,Physics::Medical Physics ,Analytical chemistry ,STM ,Energy Engineering and Power Technology ,tunneling measurements ,law.invention ,effect of disorder ,Nuclear magnetic resonance ,law ,Condensed Matter::Superconductivity ,Neutron ,Irradiation ,Electrical and Electronic Engineering ,Thin film ,Hybrid physical-chemical vapor deposition ,technology, industry, and agriculture ,Condensed Matter Physics ,Electronic, Optical and Magnetic Materials ,Physical vapor deposition ,Scanning tunneling microscope - Abstract
Neutron irradiation was performed on MgB2 thin films grown by hybrid physical chemical vapor deposition. Samples irradiated with different neutron fluences, having different critical temperatures, were studied by scanning tunneling spectroscopy in order to investigate the effect of the introduced disorder on the superconducting and spectroscopic properties. A monotonic increase of the pi gap with increasing disorder was found. (c) 2007 Elsevier B.V. All rights reserved.
- Published
- 2007
30. The Aladin2 experiment: sensitivity study
- Author
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Evgeni Il'ichev, Giampiero Esposito, Giuseppe Bimonte, D. Born, F. Tafuri, Uve Hubner, Luigi Rosa, Ruggero Vaglio, Enrico Calloni, Ornella Scaldaferri, Calloni, Enrico, Bimonte, GIUSEPPE ROBERTO, Vaglio, Ruggero, Rosa, Luigi, Esposito, Giampiero, G., Bimonte, D., Born, E., Calloni, G., Esposito, U., HU BNER, E., Ilichev, L., Rosa, O., Scaldaferria, Tafuri, Francesco, and R., Vaglio
- Subjects
Physics ,Nuclear and High Energy Physics ,Casimir pressure ,Phase transition ,Quantum Physics ,FOS: Physical sciences ,Mechanics ,Rigid body ,Casimir effect ,Classical mechanics ,Vacuum energy ,Casimir energy ,Sensitivity (control systems) ,Quantum Physics (quant-ph) ,Instrumentation ,Quantum fluctuation ,rigid body ,Cosmological constant problem - Abstract
Aladin2 is an experiment devoted to the first measurement of variations of Casimir energy in a rigid body. The main short-term scientific motivation relies on the possibility of the first demonstration of a phase transition influenced by vacuum fluctuations while, in the long term and in the mainframe of the cosmological constant problem, it can be regarded as the first step towards a measurement of the weight of vacuum energy. In this paper, after a presentation of the guiding principle of the measurement, the experimental apparatus and sensitivity studies on final cavities will be presented., 4 pages, Latex macros, 10th Conference on Frontier Detectors for Frontier Physics, Isola D'Elba, 21-27 May 2006
- Published
- 2006
31. High-field superconductivity in alloyedMgB2thin films
- Author
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Qi Li, Alexej Pogrebnyakov, J. E. Giencke, Marina Putti, C. B. Eom, Rakesh Kumar Singh, B. J. Wilkens, Y. Cui, Valeria Braccini, J. M. Rowell, Y. F. Hu, J. M. Redwing, Carlo Ferdeghini, V. Ferrando, E. Haanappel, Chiara Tarantini, Daniele Marré, Nathan Newman, R. Gandikota, Ruggero Vaglio, B. T. Liu, B. H. Moeckly, M. C. Jewell, X. X. Xi, Alex Gurevich, David C. Larbalestier, and Jeonghwan Kim
- Subjects
Superconductivity ,Physics ,Condensed matter physics ,02 engineering and technology ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,01 natural sciences ,Electronic, Optical and Magnetic Materials ,Carbon doping ,Paramagnetism ,0103 physical sciences ,High field ,Thin film ,010306 general physics ,0210 nano-technology ,Critical field - Abstract
We investigated the effect of alloying on the upper critical field ${H}_{c2}$ for 12 $\mathrm{Mg}{\mathrm{B}}_{2}$ films, in which disorder was introduced by growth, carbon doping or He-ion irradiation, finding a significant ${H}_{c2}$ enhancement in C-alloyed films, and an anomalous upward curvature of ${H}_{c2}(T)$. Record high values of $H_{c2}{}^{\ensuremath{\perp}}(4.2)\ensuremath{\approx}35\phantom{\rule{0.3em}{0ex}}\mathrm{T}$ and $H_{c2}{}^{\ensuremath{\Vert}}(4.2)\ensuremath{\approx}51\phantom{\rule{0.3em}{0ex}}\mathrm{T}$ were observed perpendicular and parallel to the $ab$ plane, respectively. The temperature dependence of ${H}_{c2}(T)$ is described well by a theory of dirty two-gap superconductivity. Extrapolation of the experimental data to $T=0$ suggests that $H_{c2}{}^{\ensuremath{\Vert}}(0)$ may approach the paramagnetic limit of $\ensuremath{\sim}70\phantom{\rule{0.3em}{0ex}}\mathrm{T}$.
- Published
- 2005
32. The 6th European Conference on Applied Superconductivity (EUCAS 2003)
- Author
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Ruggero Vaglio and Gordon Donaldson
- Subjects
Political science ,Materials Chemistry ,Metals and Alloys ,Ceramics and Composites ,Library science ,Electrical and Electronic Engineering ,Condensed Matter Physics ,Engineering physics - Abstract
This special issue of Superconductor Science and Technology contains papers presented at the 6th European Conference on Applied Superconductivity (EUCAS), which was held in Sorrento, Italy, 14--18 September 2003. This important biennial event followed previous successful meetings held in Gottingen, Germany; Edinburgh, Scotland; Eindhoven, the Netherlands; Sitges (Barcelona), Spain; and Copenhagen, Denmark. Following tradition, this EUCAS conference focused on the role of superconductivity in bridging various aspects of research with a variety of concrete advanced applications. EUCAS 2003 attracted about 1000 participants from all around the world with large participation from non-European countries. This conference benefited the worldwide superconductivity community tremendously as scientists operating internationally were able to share their knowledge and experience with one another. We are grateful to all those who submitted papers to the Conference Proceedings, which will be published in an Institute of Physics Conference Series, and also to those who contributed to this special issue. Unfortunately we could not consider every one of the large number of papers submitted to this issue and we express our regret to those whose work could not be included.
- Published
- 2004
33. Critical currents ofMgB2thin films depositedin situby sputtering
- Author
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Matteo Salvato, M. G. Maglione, M. L. Della Rocca, Luigi Maritato, Ruggero Vaglio, Serghej L. Prischepa, and R. Di Capua
- Subjects
Superconductivity ,Core (optical fiber) ,Materials science ,Condensed matter physics ,Field (physics) ,Sputtering ,Condensed Matter::Superconductivity ,Transition temperature ,Thin film ,Magnetic field ,Vortex - Abstract
We have measured the temperature and magnetic field dependencies of the critical current density J c (H,T) in MgB 2 thin films, in situ deposited by sputtering. Three-dimensional point like normal core pinning was evidenced by measurements of the magnetic dependence of the pinning forces independently from the superconducting and structural quality of the investigated films. The analysis of the experimental data in terms of the collective pinning model has pointed out the presence of a crossover magnetic field from a single vortex to a small vortex bundle pinning regime. A ΔT c pinning mechanism, i.e., a pinning associated with spatial fluctuations of the transition temperature, has been evidenced by the temperature dependence of this crossover field, in agreement with previous observations performed on MgB 2 bulk materials.
- Published
- 2003
34. Microwave intermodulation distortion of MgB2 thin films
- Author
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John Gallop, Lesley F. Cohen, F. Chiarella, Ruggero Vaglio, A. Andreone, E. Di Gennaro, Ling Hao, G. Lamura, and A. Purnell
- Subjects
Materials science ,Physics and Astronomy (miscellaneous) ,Condensed matter physics ,Condensed Matter - Superconductivity ,FOS: Physical sciences ,Dielectric ,Superconductivity (cond-mat.supr-con) ,Resonator ,Sputtering ,Grain boundary ,Thin film ,Microwave ,Sheet resistance ,Intermodulation - Abstract
The two tone intermodulation arising in MgB2 thin films deposited in-situ by planar magnetron sputtering on sapphire substrates is studied. Samples are characterised using an open-ended dielectric puck resonator operating at 8.8 GHz. The experimental results show that the third order products increase with the two-tone input power with a slope ranging between 1.5 and 2.3. The behaviour can be understood introducing a mechanism of vortex penetration in grain boundaries as the most plausible source of non linearities in these films. This assumption is confirmed by the analysis of the field dependence of the surface resistance, that show a linear behaviour at all temperatures under test., Comment: 13 pages, 3 figures; to be published in Appl. Phys. Lett
- Published
- 2003
- Full Text
- View/download PDF
35. STM tunneling spectroscopic studies ofYNdxBa2−xCu3O7−δthin films
- Author
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R. Di Capua, Maria Iavarone, Goran Karapetrov, Ruggero Vaglio, M.G. Maglione, W. K. Kwok, Marco Salluzzo, and G. W. Crabtree
- Subjects
Superconductivity ,Crystallography ,Materials science ,Impurity ,law ,Condensed Matter::Superconductivity ,Quasiparticle ,Density of states ,Fermi energy ,Scanning tunneling microscope ,Spectroscopy ,Quantum tunnelling ,law.invention - Abstract
We performed tunneling spectroscopy on high quality superconducting ${\mathrm{YNd}}_{x}{\mathrm{Ba}}_{2\ensuremath{-}x}{\mathrm{Cu}}_{3}{\mathrm{O}}_{7\ensuremath{-}\ensuremath{\delta}}$ thin films using a low-temperature scanning tunneling microscope. Superconducting regions show very well-defined gap structures. Disorder introduced by Nd substitution at the Ba site dramatically affects locally the quasiparticle density of states. The measurements show that the impurities induce surface resonant states at energies very close to the Fermi energy, typical of a d-wave superconductor.
- Published
- 2002
36. Study of the microwave electrodynamic response of MgB2 thin films
- Author
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Claudia Cantoni, Marco Salluzzo, Ruggero Vaglio, A. Andreone, E. Di Gennaro, M.G. Maglione, Mariappan Parans Paranthaman, Antonio Cassinese, G. Lamura, Andreone, Antonello, Cassinese, Antonio, C., Cantoni, DI GENNARO, Emiliano, G., Lamura, M. G., Maglione, M., Paranthaman, M., Salluzzo, Vaglio, Ruggero, Cassinese, A., Cantoni, C., DI GENNARO, E., Lamura, G., Maglione, M. G., Paranthaman, M., and Salluzzo, M.
- Subjects
Superconductivity ,Condensed Matter - Materials Science ,Materials science ,Condensed matter physics ,business.industry ,Condensed Matter - Superconductivity ,Niobium ,Materials Science (cond-mat.mtrl-sci) ,FOS: Physical sciences ,Energy Engineering and Power Technology ,chemistry.chemical_element ,Sputter deposition ,Condensed Matter Physics ,Electronic, Optical and Magnetic Materials ,Superconductivity (cond-mat.supr-con) ,chemistry ,Optoelectronics ,Grain boundary ,Electrical and Electronic Engineering ,Thin film ,business ,Boron ,Microwave ,Stoichiometry - Abstract
We present a study on the power dependence of the microwave surface impedance in thin films of the novel superconductor MgB2. 500 nm thick samples exhibiting critical temperatures ranging between 26 and 38 K are synthesized by an ex-situ post-anneal of e-beam evaporated boron in the presence of an Mg vapor at 900 C. Preliminary results on films grown in situ by a high rate magnetron sputtering technique from stoichiometric MgB2 and Mg targets are also reported. Microwave measurements have been carried out employing a dielectrically loaded niobium superconducting cavity operating at 19.8 GHz and 4 K. The study shows that the electrodynamic response of MgB2 films is presently dominated by extrinsic sources of dissipation, appearing already at low microwave power, likely to be ascribed to the presence of grain boundaries and normal inclusions in the samples., 10 pages, 3 figures, proceedings of the conference EUCAS 2001, submitted to Physica C
- Published
- 2002
37. High quality MgB2 thin films in-situ grown by dc magnetron sputtering
- Author
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R. Di Capua, Ruggero Vaglio, M. G. Maglione, Vaglio, Ruggero, M. G., Maglione, R., DI CAPUA, Maglione, M. G., and DI CAPUA, Roberto
- Subjects
Superconductivity ,Materials science ,Condensed matter physics ,Annealing (metallurgy) ,Condensed Matter - Superconductivity ,Metals and Alloys ,Analytical chemistry ,FOS: Physical sciences ,Sputter deposition ,Condensed Matter Physics ,Superconductivity (cond-mat.supr-con) ,chemistry.chemical_compound ,Residual resistivity ,chemistry ,Magnesium diboride, in situ growth, dc magnetron sputtering, critical field ,Materials Chemistry ,Ceramics and Composites ,Magnesium diboride ,Sapphire ,Electrical and Electronic Engineering ,Thin film ,Critical field - Abstract
Thin films of the recently discovered magnesium diboride (MgB2) intermetalic superconducting compound have been grown using a magnetron sputtering deposition technique followed by in-situ annealing at 830 C. High quality films were obtained on both sapphire and MgO substrates. The best films showed maximum Tc = 35 K (onset), a transition width of 0.5 K, a residual resistivity ratio up to 1.6, a low temperature critical current density Jc > 1 MA/cm2 and anisotropic critical field with gamma = 2.5 close to the values obtained for single crystals. The preparation technique can be easily scaled to produce large area in-situ films., 7 pages, 4 figures
- Published
- 2002
38. Evidence for thermal boundary resistance effects on superconducting radiofrequency cavity performances
- Author
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Vincenzo Palmieri, Ruggero Vaglio, Sergey Stark, and Antonio Alessandro Rossi
- Subjects
Superconductivity ,Materials science ,Condensed matter physics ,Liquid helium ,Thermal resistance ,Metals and Alloys ,Lambda point ,chemistry.chemical_element ,Condensed Matter Physics ,law.invention ,chemistry ,law ,Materials Chemistry ,Ceramics and Composites ,Interfacial thermal resistance ,Electrical and Electronic Engineering ,Lambda point refrigerator ,Superfluid helium-4 ,Helium - Abstract
The majority of the literature on superconducting cavities for particle accelerators concentrates on the interaction of a radiofrequency (RF) electromagnetic field with a superconductor cooled in liquid helium, generally either at a fixed temperature of 4.2 K or 1.8 K, basing the analysis of experimental results on the assumption that the superconductor is at the same temperature as the infinite reservoir of liquid helium. Only a limited number of papers have extended their analysis to the more complex overall system composed of an RF field, a superconductor and liquid helium. Only a few papers have analyzed, for example, the problem of the Kapitza resistance, i.e. the thermal boundary resistance between the superconductor and the superfluid helium. Among them, the general conclusion is that the Kapitza resistance, one of the most controversial and less understood topics in physics, is generally negligible, or not relevant for the performance enhancement of cavities. In our work presented here, studying the performance of 6 GHz niobium (Nb) test cavities, we have discovered and studied a new effect consisting of an abrupt change in the surface resistance versus temperature at the superfluid helium lambda transition T?. This abrupt change (or ?jump?) clearly appears when the RF measurement of a cavity is performed at constant power rather than at a constant field. We have correlated this jump to a change in the thermal exchange regime across the lambda transition, and, through a simple thermal model and further reasonable assumptions, we have calculated the thermal boundary resistance between niobium and liquid helium in the temperature range between 4.2 K and 1.8 K. We find that the absolute values of the thermal resistance both above and below the lambda point are fully compatible with the data reported in the literature for heat transfer to pool boiling helium I (HeI) above T? and for the Kapitza interface resistance (below T?) between a polished metal surface and superfluid HeII. Finally, based on the well-documented evidence that the surface status of metal to liquid helium influences the heat exchange towards the fluid, and specifically the Kapitza resistance below T?, we have tested an anodization process external to the cavity, comparing the performances of the cavity before and after external anodization. The tests were done without breaking the vacuum inside the cavity or modifying the inner superconducting layer in any way, and were repeated on different samples. The results show that when the cavity is externally anodized, both the Q-factor and the maximum accelerating field increase. Again, when the oxide layer is removed, the Q-factor shifts towards a lower level and the maximum accelerating field is also reduced.
- Published
- 2014
39. Memorial to Professor Antonio Barone
- Author
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Ruggero Vaglio, Francesco Tafuri, and Giampiero Pepe
- Subjects
Physics ,Josephson effect ,Battle ,Advisory committee ,media_common.quotation_subject ,Metals and Alloys ,Macroscopic quantum phenomena ,Art history ,Condensed Matter Physics ,Left behind ,Long period ,Materials Chemistry ,Ceramics and Composites ,Electrical and Electronic Engineering ,High energy resolution ,Archetype ,media_common - Abstract
Antonio Barone prematurely passed away on 4 December 2011 at the age of 72, after a one-year battle with cancer. He left behind his wife Sveva and his two sons, Alberto and Livio. Antonio was Professor Emeritus at the University of Napoli Federico II, where he had been teaching for about 40 years. The initial research activity of Antonio was in the field of nuclear physics. In this context, almost 45 years ago, the Ge 'Lithium drift' semiconductor detectors represented a novelty, due to the high energy resolution enabled by those devices. Superconductors stimulated new approaches to radiation detection and this motivated Antonio's interest towards superconductivity. Following the birth of the Laboratorio di Cibernetica of the CNR in 1967 he was given the opportunity to work on a joint USA–Italy project (University of Wisconsin, Madison and CNR Naples) in the field of superconductivity on the peculiar subject of the superconductive 'Neuristors'. His research activity on Josephson junctions opened up a wide variety of very stimulating subjects in which he was deeply involved, ranging from the soliton propagation in 'long' Josephson structures to fluctuations phenomena, from light-sensitive junctions and proximity effect to the development of innovative superconducting devices. The strong interaction of Antonio with the Landau Institute for Theoretical Physics of the Academy of Sciences in Moscow, characterizes a long period of his research activity with a precious merging of theoretical and experimental aspects. This body of work converged into the famous monograph on the 'Physics and Applications of the Josephson Effect', written in collaboration with Gianfranco Paterno in 1982. This rapidly became the reference text for the Josephson effect, as documented by thousands of citations and the fact that it was translated into Russian, Japanese and Chinese. In 1983 Antonio was awarded the highest academic title of 'Doctor of the Physical-Mathematical Sciences' by the Academy of Sciences in Moscow, and later the coveted Kapitza Prize. The discovery of high-Tc superconductors (HTS) offered new problems and perspectives. Antonio and his group significantly contributed by reporting original results on the 'archetype' high-Tc Josephson junctions. His studies on unconventional superconductivity, first developed for 'p-wave' superconductors, had great impact and were very influential on the d-wave experiments on HTS compounds, and later on the physics of HTS Josephson junctions. Macroscopic quantum phenomena and particle detectors are the keywords and the logical paths to recall several relevant contributions from Antonio scattered over more than 40 years of activity. Topics of his interest ranged from the fundamentals of macroscopic quantum tunnelling to barrier penetration in non stationary fields, to finally a project encompassing a wider vision of macroscopic quantum phenomena in unconventional systems. He has filled very important positions of scientific management in Italy and participated in many international committees. He chaired (with R Vaglio) the very successful EUCAS 2003 conference in Sorrento, Italy. He has significantly contributed to the popularization of superconductivity as a professor, as a researcher and as a manager. All scientists that had the privilege to deal with him remember Antonio as a real gentleman of science and life, a man of vision and perspective. The local Organizing Committee and the International Advisory Committee of EUCAS 2013 have dedicated the Session 'Junctions and Squids' to the memory of Professor Antonio Barone1. 1A longer version of this memorial has also been published on the Istituto SPIN-CNR website (www.spin.cnr.it/index.php/barone).
- Published
- 2014
40. RF Superconducting Cavities for Accelerators
- Author
-
Ruggero Vaglio
- Subjects
Superconductivity ,Free electron model ,Fabrication ,Materials science ,business.industry ,Niobium ,Physics::Optics ,chemistry.chemical_element ,Particle accelerator ,Electron ,Laser ,law.invention ,chemistry ,law ,Condensed Matter::Superconductivity ,Physics::Accelerator Physics ,Optoelectronics ,Thin film ,business - Abstract
In this chapter the state of the art of rf superconducting cavities for particle accelerators is presented and discussed. The main concepts of rf cavity design and the main physical parameters are first introduced. Fabrication techniques and diagnostic measurements are then described for both bulk and thin film niobium coated cavities. The application of superconducting cavities to Electron Linear Colliders, Proton Linacs and Ion Accelerators as well as Free Electron Lasers is also briefly outlined. A large set of measurements on thin film niobium cavities is then analyzed in order to get insight in the origin of residual and nonlinear losses. Finally the possible role and preliminary results on alternative, high Tc compounds, are discussed m detail.
- Published
- 2001
41. Thickness effect on the structure and superconductivity of Nd1.2Ba1.8Cu3O7+x epitaxial films
- Author
-
G. M. De Luca, Matteo Tropeano, Marco Salluzzo, Ruggero Vaglio, Marina Putti, U. Scotti di Uccio, Daniele Marré, Salluzzo, M., De Luca, G. M., Marre’, D., Putti, M., Tropeano, M., SCOTTI DI UCCIO, Umberto, Vaglio, Ruggero, de Luca, G. M., and Marre, D.
- Subjects
Superconductivity ,STRAIN ,Materials science ,Condensed matter physics ,business.industry ,Thin films ,Energy Engineering and Power Technology ,Bragg's law ,Sputter deposition ,Condensed Matter Physics ,Electronic, Optical and Magnetic Materials ,Optics ,Sputtering ,High critical temperature superconductors ,Phase (matter) ,Strain effect ,CRITICAL-TEMPERATURE ,Orthorhombic crystal system ,Electrical and Electronic Engineering ,Thin film ,business ,Crystal twinning - Abstract
We have studied the effect of thickness on the structure and superconductivity of Nd1.2Ba1.8Cu3O7+x (NdBCO) epitaxial films deposited on SrTiO3 (100) substrates. High quality NdBCO films were deposited by high oxygen pressure sputtering. The samples have been carefully characterized by transport measurements and X-ray diffraction using conventional and synchrotron radiation sources. Two structural transformations are observed. The first one is a crossover from the orthorhombic and twinned structure, typical of thick samples, to a pseudotetragonal phase at thickness lower than 60 unit cells. The pseudotetragonal phase exhibits peculiar X-ray diffuse scattering around the Bragg reflections, associated to nanostructured twinned domains. The second one appears at thickness lower than 20 unit cells and is assigned to a pseudotetragonal-tetragonal transition. The transport properties are not modified at the first crossover, while a substantial decrease of T-c and of the number of holes is observed at the pseudotetragonal-tetragonal transformation. Our results suggest that the structural rearrangement and the transport properties are explained by the ordering of Cu(I)O chains. (c) 2007 Elsevier B.V. All rights reserved.
- Published
- 2007
42. TRANSPORT AND TUNNELING MEASUREMENTS IN SUPERCONDUCTING YNI2B2C
- Author
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Pietro Manfrinetti, F. Fontana, Antonello Andreone, Maria Iavarone, Ruggero Vaglio, Fabio Canepa, A. Palenzona, Andreone, Antonello, F., Fontana, M., Iavarone, Vaglio, Ruggero, F., Canepa, P., Manfrinetti, and A., Palenzona
- Subjects
Superconducting coherence length ,Superconductivity ,Materials science ,Condensed matter physics ,Energy Engineering and Power Technology ,Flory–Huggins solution theory ,Condensed Matter Physics ,Plasma oscillation ,Electronic, Optical and Magnetic Materials ,symbols.namesake ,Tunnel effect ,Electrical resistivity and conductivity ,Condensed Matter::Superconductivity ,symbols ,Electrical and Electronic Engineering ,Debye model ,Quantum tunnelling - Abstract
New transport (resistivity versus temperature) and tunneling (low-temperature STM) measurements are reported on YNi 2 B 2 C samples prepared by inductive melting from the pure elements. Estimations of Debye temperature, electron-photon interaction parameter λ, plasma frequency and superconducting energy gap are given. Normal-state and superconducting data fit in a consistent picture of BCS superconductivity with λ ≤ 1.
- Published
- 1995
43. Superconductivity and Magnetism
- Author
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Attanasio, Carmine, Maritato, Luigi, and Ruggero, Vaglio
- Published
- 1991
44. Radiation damaged MgB2:a comparison with A15 superconductors
- Author
-
Ruggero Vaglio, Marina Putti, and J. M. Rowell
- Subjects
Superconductivity ,Physics ,History ,Condensed matter physics ,Electrical resistivity and conductivity ,Density of states ,Radiation damage ,High radiation ,Radiation ,Constant (mathematics) ,Critical field ,Computer Science Applications ,Education - Abstract
In the present paper we discuss in detail experiments of radiation damage and their effects on MgB2 properties (Tc, resistivity, critical field, gap), making constant reference to similar experiments performed in the seventies and eighties on A15 superconductors (Nb3Sn, V3Si). We will show that the overall behaviour of MgB2 and A15s is surprisingly similar, pointing out that similar mechanisms (smearing of density of states) plays a role at high radiation doses, whereas, at low radiation, two-band effects mainly determine the MgB2 behaviuor.
- Published
- 2008
45. The 6th European Conference on Applied Superconductivity (EUCAS 2003)
- Author
-
Donaldson, Ruggero Vaglio and Gordon, primary
- Published
- 2004
- Full Text
- View/download PDF
46. Observation of Enhancement of the Superconducting Order Parameter in the Coexistent Antiferromagnetic State of SmRh4B4
- Author
-
Kenneth E. Gray, John Zasadzinski, Ruggero Vaglio, and B. D. Terris
- Subjects
Physics ,Superconductivity ,Josephson effect ,Paramagnetism ,Tunnel effect ,Condensed matter physics ,Magnetism ,Condensed Matter::Superconductivity ,General Physics and Astronomy ,Antiferromagnetism ,Condensed Matter::Strongly Correlated Electrons ,Néel temperature ,Quantum tunnelling - Abstract
The first measurements of Josephson tunneling into both the paramagnetic and antiferromagnetic phases of SmRh/sub 4/B/sub 4/ are reported. The results show that the superconducting order parameter of SmRh/sub 4/B/sub 4/ is enhanced by the antiferromagnetic order occurring below the Neel temperature of about 0.87 K. On the basis of this observation, the applicability of various proposed theories of coexistent superconductivity and antiferromagnetism can be determined for SmRh/sub 4/B/sub 4/.
- Published
- 1984
47. Zero‐field ‘‘Fiske’’ steps in small Josephson junctions
- Author
-
M. Russo, Carlo Camerlingo, and Ruggero Vaglio
- Subjects
Pi Josephson junction ,Physics ,Josephson effect ,Tunnel effect ,Condensed matter physics ,Mathematical model ,Zero field ,Condensed Matter::Superconductivity ,General Physics and Astronomy ,Resonance ,Josephson energy ,Condensed Matter::Mesoscopic Systems and Quantum Hall Effect ,Excitation - Abstract
The theory of Fiske steps in Josephson tunnel junctions is extended to include the presence of structural fluctuations in the barrier. The possibility of excitation of zero‐field steps in this case, is discussed. Experimental evidence for the occurrence of zero‐field resonances, due to both regular and randomly distributed nonuniformities in ‘‘small’’ Josephson junctions, is reported.
- Published
- 1982
48. [Ruggero Vaglio, 1887-1951]
- Author
-
RUGGERO, VAGLIO
- Subjects
History ,Pediatrics - Published
- 1951
49. Multi-stage dual-mode cross-slotted superconducting filters for telecommunication application
- Author
-
Antonio Cassinese, Ruggero Vaglio, Mario Barra, Gaetano Panariello, Cassinese, Antonio, M., Barra, G., Panariello, and Vaglio, Ruggero
- Subjects
Superconductivity ,High-temperature superconductivity ,Materials science ,business.industry ,Telecommunication application ,Dual mode ,Chebyshev filter ,law.invention ,Substrate (building) ,law ,Filter (video) ,Electronic engineering ,Optoelectronics ,business ,Realization (systems) - Abstract
Dual mode high temperature superconducting (HTS) filters represent an interesting device class for telecommunication application since they combine a high power handling capability with a miniaturized size. Here we report on the design and realization of dual mode cross slotted filters presenting a more compact size if compared with the traditional dual mode patch filters. Single stage filters operating in C-band with 1% fractional bandwidth have been designed and tested at prototype level by using double sided YBa/sub 2/Cu/sub 3/O/sub 7-x/ (YBCO) and Tl/sub 2/Ba/sub 2/CaCu/sub 2/O/sub 8/ (Tl-2212) superconducting films grown on LaAlO/sub 3/ substrates. The YBCO filter presents insertion losses IL=1 dB and a power handling higher than 10 dBm at T=77 K while the Tl-2212 allows operation at higher temperatures with comparable performances. Dual stage (four poles) and four stage (eight poles) filters with 1% fractional bandwidth operating in C-band and presenting a Chebyshev or a quasi elliptical response have been analyzed. Finally, a four stage filter fitting well on a 1"/spl times/1" substrate was designed.
50. Low noise cryogenic system for the measurement of the Casimir energy in rigid cavities.
- Author
-
Giuseppe Bimonte, Detlef Born, Enrico Calloni, Giampiero Esposito, Uwe Huebner, Evgeni Il, Luigi Rosa, Francesco Tafuri, and Ruggero Vaglio
- Subjects
CASIMIR effect ,LOW temperature engineering ,PHYSICAL measurements ,TRANSITION metal ions ,PHOTONS ,SUPERCONDUCTIVITY ,ALUMINUM films - Abstract
We report on preliminary results on the measurement of variations of the Casimir energy in rigid cavities through its influence on the superconducting transition of in-cavity aluminium (Al) thin films. After a description of the experimental apparatus, we report on a measurement in the presence of thermal photons, discussing its implications for the zero-point photons case. Finally, we show preliminary results for the zero-point case. [ABSTRACT FROM AUTHOR]
- Published
- 2008
- Full Text
- View/download PDF
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