28 results on '"Pucella G."'
Search Results
2. CVD diamond photodetectors for FTU plasma diagnostics
- Author
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Cesaroni, S., Angelone, M., Apruzzese, G., Bombarda, F., Gabellieri, L., Marinelli, M., Milani, E., Palomba, S., Pucella, G., Romano, A., Verona, C., Verona-Rinati, G., Centioli, C., Grosso, A., Piergotti, V., Rocchi, G., Sibio, A., and Tilia, B.
- Published
- 2021
- Full Text
- View/download PDF
3. Density fluctuations induced by MARFE on FTU
- Author
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Zeng, L., Tudisco, O., Gao, W., Zhang, S., Gao, X., Pucella, G., and Apruzzese, G.
- Published
- 2013
- Full Text
- View/download PDF
4. First results about on-ground calibration of the silicon tracker for the AGILE satellite
- Author
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Cattaneo, P.W., Argan, A., Boffelli, F., Bulgarelli, A., Buonomo, B., Chen, A.W., D’Ammando, F., Froysland, T., Fuschino, F., Galli, M., Gianotti, F., Giuliani, A., Longo, F., Marisaldi, M., Mazzitelli, G., Pellizzoni, A., Prest, M., Pucella, G., Quintieri, L., Rappoldi, A., Tavani, M., Trifoglio, M., Trois, A., Valente, P., Vallazza, E., Vercellone, S., Zambra, A., Barbiellini, G., Caraveo, P., Cocco, V., Costa, E., De Paris, G., Del Monte, E., Di Cocco, G., Donnarumma, I., Evangelista, Y., Feroci, M., Ferrari, A., Fiorini, M., Labanti, C., Lapshov, I., Lazzarotto, F., Lipari, P., Mastropietro, M., Mereghetti, S., Morelli, E., Moretti, E., Morselli, A., Pacciani, L., Perotti, F., Piano, G., Picozza, P., Pilia, M., Porrovecchio, G., Rapisarda, M., Rubini, A., Sabatini, S., Soffitta, P., Striani, E., Vittorini, V., Zanello, D., Colafrancesco, S., Giommi, P., Pittori, C., Santolamazza, P., Verrecchia, F., and Salotti, L.
- Published
- 2011
- Full Text
- View/download PDF
5. Preliminary results on TeV sources search with AGILE
- Author
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Rappoldi, A., Longo, F., Argan, A., Barbiellini, G., Boffelli, F., Bulgarelli, A., Caraveo, P., Cattaneo, P.W., Chen, A.W., Cocco, V., Colafrancesco, S., Costa, E., D’ Ammando, F., De Paris, G., Del Monte, E., Di Cocco, G., Donnarumma, I., Evangelista, Y., Ferrari, A., Feroci, M., Fiorini, M., Froysland, T., Fuschino, F., Galli, M., Gianotti, F., Giommi, P., Giuliani, A., Labanti, C., Lapshov, I., Lazzarotto, F., Lipari, P., Marisaldi, M., Mastropietro, M., Mereghetti, S., Morelli, E., Moretti, E., Morselli, A., Pacciani, L., Pellizzoni, A., Perotti, F., Piano, G., Picozza, P., Pilia, M., Pittori, C., Porrovecchio, G., Prest, M., Pucella, G., Rapisarda, M., Rubini, A., Sabatini, S., Salotti, L., Santolamazza, P., Soffitta, P., Striani, E., Tavani, M., Trifoglio, M., Trois, A., Vallazza, E., Verrecchia, F., Vercellone, S., Vittorini, V., Zambra, A., and Zanello, D.
- Published
- 2011
- Full Text
- View/download PDF
6. The flaring blazars of the first 1.5 years of the AGILE mission
- Author
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Pacciani, L., Bulgarelli, A., Chen, A.W., D’Ammando, F., Donnarumma, I., Giuliani, A., Longo, F., Pucella, G., Tavani, M., Vercellone, S., Vittorini, V., Argan, A., Barbiellini, G., Boffelli, F., Caraveo, P., Cattaneo, P.W., Cocco, V., Costa, E., De Paris, G., Del Monte, E., Di Cocco, G., Evangelista, Y., Ferrari, A., Feroci, M., Fiorini, M., Froysland, T., Fuschino, F., Galli, M., Gianotti, F., Labanti, C., Lapshov, I., Lazzarotto, F., Lipari, P., Marisaldi, M., Mastropietro, M., Mereghetti, S., Morelli, E., Moretti, E., Morselli, A., Pellizzoni, A., Perotti, F., Piano, G., Picozza, P., Pilia, M., Porrovecchio, G., Prest, M., Rapisarda, M., Rappoldi, A., Rubini, A., Sabatini, S., Soffitta, P., Trifoglio, M., Trois, A., Vallazza, E., Zambra, A., Zanello, D., Antonelli, L.A., Colafrancesco, S., Giommi, P., Pittori, C., Verrecchia, F., Santolamazza, P., and Salotti, L.
- Published
- 2011
- Full Text
- View/download PDF
7. Galactic sources science with AGILE: The case of the Carina Region
- Author
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Sabatini, S., Tavani, M., Pian, E., Bulgarelli, A., Caraveo, P., Viotti, R., Corcoran, M.F., Giuliani, A., Pittori, C., Verrecchia, F., Vercellone, S., Mereghetti, S., Argan, A., Barbiellini, G., Boffelli, F., Cattaneo, P.W., Chen, A.W., Cocco, V., D’Ammando, F., Costa, E., Paris, G. De, Monte, E. Del, Cocco, G. Di, Donnarumma, I., Evangelista, Y., Ferrari, A., Feroci, M., Fiorini, M., Froysland, T., Fuschino, F., Galli, M., Gianotti, F., Labanti, C., Lapshov, I., Lazzarotto, F., Lipari, P., Longo, F., Marisaldi, M., Mastropietro, M., Morelli, E., Moretti, E., Morselli, A., Pacciani, L., Pellizzoni, A., Perotti, F., Piano, G., Picozza, P., Pilia, M., Porrovecchio, G., Pucella, G., Prest, M., Rapisarda, M., Rappoldi, A., Rubini, A., Soffitta, P., Trifoglio, M., Trois, A., Vallazza, E., Vittorini, V., Zambra, A., Zanello, D., Santolamazza, P., Giommi, P., Colafrancesco, S., Antonelli, L.A., and Salotti, L.
- Published
- 2011
- Full Text
- View/download PDF
8. The observation of gamma ray bursts and terrestrial gamma-ray flashes with AGILE
- Author
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Del Monte, E., Barbiellini, G., Fuschino, F., Giuliani, A., Longo, F., Marisaldi, M., Mereghetti, S., Moretti, E., Trifoglio, M., Vianello, G., Costa, E., Donnarumma, I., Evangelista, Y., Feroci, M., Gallil, M., Lapshov, I., Lazzarotto, F., Lipari, P., Pacciani, L., Rapisarda, M., Soffitta, P., Tavani, M., Vercellone, S., Cutini, S., Boffelli, F., Bulgarelli, A., Caraveo, P., Cattaneo, P.W., Chen, A., Di Cocco, G., Gianotti, F., Labanti, C., Morselli, A., Pellizzoni, A., Perotti, F., Piano, G., Picozza, P., Pilia, M., Prest, M., Pucella, G., Rappoldi, A., Sabatini, S., Striani, E., Trois, A., Vallazza, E., Vittorini, V., Antonelli, L.A., Pittori, C., Preger, B., Santolamazza, P., Verrecchia, F., Giommi, P., and Salotti, L.
- Published
- 2011
- Full Text
- View/download PDF
9. Analysis of deposited layers with deuterium and impurity elements on samples from the divertor of JET with ITER-like wall
- Author
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Strom, P., Petersson, P., Rubel, M., Fortuna-Zalesna, E., Widdowson, A., Sergienko, G., Litaudon, X., Abduallev, S., Abhangi, M., Abreu, P., Afzal, M., Aggarwal, K. M., Ahlgren, T., Ahn, J. H., Aho-Mantila, L., Aiba, N., Airila, M., Albanese, R., Aldred, V., Alegre, D., Alessi, E., Aleynikov, P., Alfier, A., Alkseev, A., Allinson, M., Alper, B., Alves, E., Ambrosino, G., Ambrosino, R., Amicucci, L., Amosov, V., Sunden, E. Andersson, Angelone, M., Anghel, M., Angioni, C., Appel, L., Appelbee, C., Arena, P., Ariola, M., Arnichand, H., Arshad, S., Ash, A., Ashikawa, N., Aslanyan, V., Asunta, O., Auriemma, F., Austin, Y., Avotina, L., Axton, M. D., Ayres, C., Bacharis, M., Baciero, A., Baiao, D., Bailey, S., Baker, A., Balboa, I., Balden, M., Balshaw, N., Bament, R., Banks, J. W., Baranov, Y. F., Barnard, M. A., Barnes, D., Barnes, M., Barnsley, R., Wiechec, A. Baron, Orte, L. Barrera, Baruzzo, M., Basiuk, V., Bassan, M., Bastow, R., Batista, A., Batistoni, P., Baughan, R., Bauvir, B., Baylor, L., Bazylev, B., Beal, J., Beaumont, P. S., Beckers, M., Beckett, B., Becoulet, A., Bekris, N., Beldishevski, M., Bell, K., Belli, F., Bellinger, M., Belonohy, E., Ben Ayed, N., Benterman, N. A., Bergsaker, H., Bernardo, J., Bernert, M., Berry, M., Bertalot, L., Besliu, C., Beurskens, M., Bieg, B., Bielecki, J., Biewer, T., Bigi, M., Bilkova, P., Binda, F., Bisoffi, A., Bizarro, J. P. S., Bjorkas, C., Blackburn, J., Blackman, K., Blackman, T. R., Blanchard, P., Blatchford, P., Bobkov, V., Boboc, A., Bodnar, G., Bogar, O., Bolshakova, I., Bolzonella, T., Bonanomi, N., Bonelli, F., Boom, J., Booth, J., Borba, D., Borodin, D., Borodkina, I., Botrugno, A., Bottereau, C., Boulting, P., Bourdelle, C., Bowden, M., Bower, C., Bowman, C., Boyce, T., Boyd, C., Boyer, H. J., Bradshaw, J. M. A., Braic, V., Bravanec, R., Breizman, B., Bremond, S., Brennan, P. D., Breton, S., Brett, A., Brezinsek, S., Bright, M. D. J., Brix, M., Broeckx, W., Brombin, M., Broslawski, A., Brown, D. P. D., Brown, M., Bruno, E., Bucalossi, J., Buch, J., Buchanan, J., Buckley, A., Budny, R., Bufferand, H., Bulman, M., Bulmer, N., Bunting, P., Buratti, P., Burckhart, A., Buscarino, A., Busse, A., Butler, N. K., Bykov, I., Byrne, J., Cahyna, P., Calabro, G., Calvo, I., Camenen, Y., Camp, P., Campling, D. C., Cane, J., Cannas, B., Capel, A. J., Card, P. J., Cardinali, A., Carman, P., Carr, M., Carralero, D., Carraro, L., Carvalho, B. B., Carvalho, I., Carvalho, P., Casson, F. J., Castaldo, C., Catarino, N., Caumont, J., Causa, F., Cavazzana, R., Cave-Ayland, K., Cavinato, M., Cecconello, M., Ceccuzzi, S., Cecil, E., Cenedese, A., Cesario, R., Challis, C. D., Chandler, M., Chandra, D., Chang, C. S., Chankin, A., Chapman, I. T., Chapman, S. C., Chernyshova, M., Chitarin, G., Ciraolo, G., Ciric, D., Citrin, J., Clairet, F., Clark, E., Clark, M., Clarkson, R., Clatworthy, D., Clements, C., Cleverly, M., Coad, J. P., Coates, P. A., Cobalt, A., Coccorese, V., Cocilovo, V., Coda, S., Coelho, R., Coenen, J. W., Coffey, I., Colas, L., Collins, S., Conka, D., Conroy, S., Conway, N., Coombs, D., Cooper, D., Cooper, S. R., Corradino, C., Corre, Y., Corrigan, G., Cortes, S., Coster, D., Couchman, A. S., Cox, M. P., Craciunescu, T., Cramp, S., Craven, R., Crisanti, F., Croci, G., Croft, D., Crombe, K., Crowe, R., Cruz, N., Cseh, G., Cufar, A., Cullen, A., Curuia, M., Czarnecka, A., Dabirikhah, H., Dalgliesh, P., Dalley, S., Dankowski, J., Darrow, D., Davies, O., Davis, W., Day, C., Day, I. E., De Bock, M., de Castro, A., de la Cal, E., de la Luna, E., De Masi, G., de Pablos, J. L., De Temmerman, G., De Tommasi, G., de Vries, P., Deakin, K., Deane, J., Agostini, F. Degli, Dejarnac, R., Delabie, E., den Harder, N., Dendy, R. O., Denis, J., Denner, P., Devaux, S., Devynck, P., Di Maio, F., Di Siena, A., Di Troia, C., Dinca, P., D'Inca, R., Ding, B., Dittmar, T., Doerk, H., Doerner, R. P., Donne, T., Dorling, S. E., Dormido-Canto, S., Doswon, S., Douai, D., Doyle, P. T., Drenik, A., Drewelow, P., Drews, P., Duckworth, Ph., Dumont, R., Dumortier, P., Dunai, D., Dunne, M., Duran, I., Durodie, F., Dutta, P., Duval, B. P., Dux, R., Dylst, K., Dzysiuk, N., Edappala, P. V., Edmond, J., Edwards, A. M., Edwards, J., Eich, Th., Ekedahl, A., El-Jorf, R., Elsmore, C. G., Enachescu, M., Ericsson, G., Eriksson, F., Eriksson, J., Eriksson, L. G., Esposito, B., Esquembri, S., Esser, H. G., Esteve, D., Evans, B., Evans, G. E., Evison, G., Ewart, G. D., Fagan, D., Faitsch, M., Falie, D., Fanni, A., Fasoli, A., Faustin, J. M., Fawlk, N., Fazendeiro, L., Fedorczak, N., Felton, R. C., Fenton, K., Fernades, A., Fernandes, H., Ferreira, J., Fessey, J. A., Fevrier, O., Ficker, O., Field, A., Fietz, S., Figueiredo, A., Figueiredo, J., Fil, A., Finburg, P., Firdaouss, M., Fischer, U., Fittill, L., Fitzgerald, M., Flammini, D., Flanagan, J., Fleming, C., Flinders, K., Fonnesu, N., Fontdecaba, J. M., Formisano, A., Forsythe, L., Fortuna, L., Fortune, M., Foster, S., Franke, T., Franklin, T., Frasca, M., Frassinetti, L., Freisinger, M., Fresa, R., Frigione, D., Fuchs, V., Fuller, D., Futatani, S., Fyvie, J., Gal, K., Galassi, D., Galazka, K., Galdon-Quiroga, J., Gallagher, J., Gallart, D., Galvao, R., Gao, X., Gao, Y., Garcia, J., Garcia-Carrasco, A., Garcia-Munoz, M., Gardarein, J. -L., Garzotti, L., Gaudio, P., Gauthier, E., Gear, D. F., Gee, S. J., Geiger, B., Gelfusa, M., Gerasimov, S., Gervasini, G., Gethins, M., Ghani, Z., Ghate, M., Gherendi, M., Giacalone, J. C., Giacomelli, L., Gibson, C. S., Giegerich, T., Gil, C., Gil, L., Gilligan, S., Gin, D., Giovannozzi, E., Girardo, J. B., Giroud, C., Giruzzi, G., Gloeggler, S., Godwin, J., Goff, J., Gohil, P., Goloborod'ko, V., Gomes, R., Goncalves, B., Goniche, M., Goodliffe, M., Goodyear, A., Gorini, G., Gosk, M., Goulding, R., Goussarov, A., Gowland, R., Graham, B., Graham, M. E., Graves, J. P., Grazier, N., Grazier, P., Green, N. R., Greuner, H., Grierson, B., Griph, F. S., Grisolia, C., Grist, D., Groth, M., Grove, R., Grundy, C. N., Grzonka, J., Guard, D., Guerard, C., Guillemaut, C., Guirlet, R., Gurl, C., Utoh, H. H., Hackett, L. J., Hacquin, S., Hagar, A., Hager, R., Hakola, A., Halitovs, M., Hall, S. J., Cook, S. P. Hallworth, Hamlyn-Harris, C., Hammond, K., Harrington, C., Harrison, J., Harting, D., Hasenbeck, F., Hatano, Y., Hatch, D. R., Haupt, T. D. V., Hawes, J., Hawkes, N. C., Hawkins, J., Hawkins, P., Haydon, P. W., Hayter, N., Hazel, S., Heesterman, P. J. L., Heinola, K., Hellesen, C., Hellsten, T., Helou, W., Hemming, O. N., Hender, T. C., Henderson, M., Henderson, S. S., Henriques, R., Hepple, D., Hermon, G., Hertout, P., Hidalgo, C., Highcock, E. G., Hill, M., Hillairet, J., Hillesheim, J., Hillis, D., Hizanidis, K., Hjalmarsson, A., Hobirk, J., Hodille, E., Hogben, C. H. A., Hogeweij, G. M. D., Hollingsworth, A., Hollis, S., Homfray, D. A., Horacek, J., Hornung, G., Horton, A. R., Horton, L. D., Horvath, L., Hotchin, S. P., Hough, M. R., Howarth, P. J., Hubbard, A., Huber, A., Huber, V., Huddleston, T. M., Hughes, M., Huijsmans, G. T. A., Hunter, C. L., Huynh, P., Hynes, A. M., Iglesias, D., Imazawa, N., Imbeaux, F., Imrisek, M., Incelli, M., Innocente, P., Irishkin, M., Ivanova-Stanik, I., Jachmich, S., Jacobsen, A. S., Jacquet, P., Jansons, J., Jardin, A., Jarvinen, A., Jaulmes, F., Jednorog, S., Jenkins, I., Jeong, C., Jepu, I., Joffrin, E., Johnson, R., Johnson, T., Johnston, Jane, Joita, L., Jones, G., Jones, T. T. C., Hoshino, K. K., Kallenbach, A., Kamiya, K., Kaniewski, J., Kantor, A., Kappatou, A., Karhunen, J., Karkinsky, D., Karnowska, I., Kaufman, M., Kaveney, G., Kazakov, Y., Kazantzidis, V., Keeling, D. L., Keenan, T., Keep, J., Kempenaars, M., Kennedy, C., Kenny, D., Kent, J., Kent, O. N., Khilkevich, E., Kim, H. T., Kim, H. S., Kinch, A., King, C., King, D., King, R. F., Kinna, D. J., Kiptily, V., Kirk, A., Kirov, K., Kirschner, A., Kizane, G., Klepper, C., Klix, A., Knight, P., Knipe, S. J., Knott, S., Kobuchi, T., Koechl, F., Kocsis, G., Kodeli, I., Kogan, L., Kogut, D., Koivuranta, S., Kominis, Y., Koepen, M., Kos, B., Koskela, T., Koslowski, H. R., Koubiti, M., Kovari, M., Kowalska-Strzeciwilk, E., Krasilnikov, A., Krasilnikov, V., Krawczyk, N., Kresina, M., Krieger, K., Krivska, A., Kruezi, U., Ksiazek, I., Kukushkin, A., Kundu, A., Kurki-Suonio, T., Kwak, S., Kwiatkowski, R., Kwon, O. J., Laguardia, L., Lahtinen, A., Laing, A., Lam, N., Lambertz, H. T., Lane, C., Lang, P. T., Lanthaler, S., Lapins, J., Lasa, A., Last, J. R., Laszynska, E., Lawless, R., Lawson, A., Lawson, K. D., Lazaros, A., Lazzaro, E., Leddy, J., Lee, S., Lefebvre, X., Leggate, H. J., Lehmann, J., Lehnen, M., Leichtle, D., Leichuer, P., Leipold, F., Lengar, I., Lennholm, M., Lerche, E., Lescinskis, A., lesnoj, S., Letellier, E., Leyland, M., Leysen, W., Li, L., Liang, Y., Likonen, J., Linke, J., Linsmeier, Ch., Lipschultz, B., Liu, G., Liu, Y., Lo Schiavo, V. P., Loarer, T., Loarte, A., Lobel, R. C., Lomanowski, B., Lomas, P. J., Lonnroth, J., Lopez, J. M., Lopez-Razola, J., Lorenzini, R., Losada, U., Lovell, J. J., Loving, A. B., Lowry, C., Luce, T., Lucock, R. M. A., Lukin, A., Luna, C., Lungaroni, M., Lungu, C. P., Lungu, M., Lunniss, A., Lupelli, I., Lyssoivan, A., Macdonald, N., Macheta, P., Maczewa, K., Magesh, B., Maget, P., Maggi, C., Maier, H., Mailloux, J., Makkonen, T., Makwana, R., Malaquias, A., Malizia, A., Manas, P., Manning, A., Manso, M. E., Mantica, P., Mantsinen, M., Manzanares, A., Maquet, Ph., Marandet, Y., Marcenko, N., Marchetto, C., Marchuk, O., Marinelli, M., Marinucci, M., Markovic, T., Marocco, D., Marot, L., Marren, C. A., Marshal, R., Martin, A., Martin, Y., de Aguilera, A. Martin, Martinez, F. J., Martin-Solis, J. R., Martynova, Y., Maruyama, S., Masiello, A., Maslov, M., Matejcik, S., Mattei, M., Matthews, G. F., Maviglia, F., Mayer, M., Mayoral, M. L., May-Smith, T., Mazon, D., Mazzotta, C., McAdams, R., McCarthy, P. J., McClements, K. G., McCormack, O., McCullen, P. A., McDonald, D., McIntosh, S., McKean, R., McKehon, J., Meadows, R. C., Meakins, A., Medina, F., Medland, M., Medley, S., Meigh, S., Meigs, A. G., Meisl, G., Meitner, S., Meneses, L., Menmuir, S., Mergia, K., Merrigan, I. R., Mertens, Ph., Meshchaninov, S., Messiaen, A., Meyer, H., Mianowski, S., Michling, R., Middleton-Gear, D., Miettunen, J., Militello, F., Militello-Asp, E., Miloshevsky, G., Mink, F., Minucci, S., Miyoshi, Y., Mlynar, J., Molina, D., Monakhov, I., Moneti, M., Mooney, R., Moradi, S., Mordijck, S., Moreira, L., Moreno, R., Moro, F., Morris, A. W., Morris, J., Moser, L., Mosher, S., Moulton, D., Murari, A., Muraro, A., Murphy, S., Asakura, N. N., Na, Y. S., Nabais, F., Naish, R., Nakano, T., Nardon, E., Naulin, V., Nave, M. F. F., Nedzelski, I., Nemtsev, G., Nespoli, F., Neto, A., Neu, R., Neverov, V. S., Newman, M., Nicholls, K. J., Nicolas, T., Nielsen, A. H., Nielsen, P., Nilsson, E., Nishijima, D., Noble, C., Nocente, M., Nodwell, D., Nordlund, K., Nordman, H., Nouailletas, R., Nunes, I., Oberkofler, M., Odupitan, T., Ogawa, M. T., O'Gorman, T., Okabayashi, M., Olney, R., Omolayo, O., O'Mullane, M., Ongena, J., Orsitto, F., Orszagh, J., Oswuigwe, B. I., Otin, R., Owen, A., Paccagnella, R., Pace, N., Pacella, D., Packer, L. W., Page, A., Pajuste, E., Palazzo, S., Pamela, S., Panja, S., Papp, P., Paprok, R., Parail, V., Park, M., Diaz, F. Parra, Parsons, M., Pasqualotto, R., Patel, A., Pathak, S., Paton, D., Patten, H., Pau, A., Pawelec, E., Soldan, C. Paz, Peackoc, A., Pearson, I. J., Pehkonen, S. -P., Peluso, E., Penot, C., Pereira, A., Pereira, R., Puglia, P. P. Pereira, von Thun, C. Perez, Peruzzo, S., Peschanyi, S., Peterka, M., Petravich, G., Petre, A., Petrella, N., Petrzilka, V., Peysson, Y., Pfefferle, D., Philipps, V., Pillon, M., Pintsuk, G., Piovesan, P., Pires dos Reis, A., Piron, L., Pironti, A., Pisano, F., Pitts, R., Pizzo, F., Plyusnin, V., Pomaro, N., Pompilian, O. G., Pool, P. J., Popovichev, S., Porfiri, M. T., Porosnicu, C., Porton, M., Possnert, G., Potzel, S., Powell, T., Pozzi, J., Prajapati, V., Prakash, R., Prestopino, G., Price, D., Price, M., Price, R., Prior, P., Proudfoot, R., Pucella, G., Puglia, P., Puiatti, M. E., Pulley, D., Purahoo, K., Puetterich, Th., Rachlew, E., Rack, M., Ragona, R., Rainford, M. S. J., Rakha, A., Ramogida, G., Ranjan, S., Rapson, C. J., Rasmussen, J. J., Rathod, K., Ratta, G., Ratynskaia, S., Ravera, G., Rayner, C., Rebai, M., Reece, D., Reed, A., Refy, D., Regan, B., Regana, J., Reich, M., Reid, N., Reimold, F., Reinhart, M., Reinke, M., Reiser, D., Rendell, D., Reux, C., Reyes Cortes, S. D. A., Reynolds, S., Riccardo, V., Richardson, N., Riddle, K., Rigamonti, D., Rimini, F. G., Risner, J., Riva, M., Roach, C., Robins, R. J., Robinson, S. A., Robinson, T., Robson, D. 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Rachlew, E, Rack, M, Ragona, R, Rainford, M, Rakha, A, Ramogida, G, Ranjan, S, Rapson, C, Rasmussen, J, Rathod, K, Ratta, G, Ratynskaia, S, Ravera, G, Rayner, C, Rebai, M, Reece, D, Reed, A, Refy, D, Regan, B, Regana, J, Reich, M, Reid, N, Reimold, F, Reinhart, M, Reinke, M, Reiser, D, Rendell, D, Reux, C, Reyes Cortes, S, Reynolds, S, Riccardo, V, Richardson, N, Riddle, K, Rigamonti, D, Rimini, F, Risner, J, Riva, M, Roach, C, Robins, R, Robinson, S, Robinson, T, Robson, D, Roccella, R, Rodionov, R, Rodrigues, P, Rodriguez, J, Rohde, V, Romanelli, F, Romanelli, M, Romanelli, S, Romazanov, J, Rowe, S, Rubinacci, G, Rubino, G, Ruchko, L, Ruiz, M, Ruset, C, Rzadkiewicz, J, Saarelma, S, Sabot, R, Safi, E, Sagar, P, Saibene, G, Saint-Laurent, F, Salewski, M, Salmi, A, Salmon, R, Salzedas, F, Samaddar, D, Samm, U, Sandiford, D, Santa, P, Santala, M, Santos, B, Santucci, A, Sartori, F, Sartori, R, Sauter, O, Scannell, R, Schlummer, T, Schmid, K, Schmidt, V, Schmuck, S, Schneider, M, Schoepf, K, Schworer, D, Scott, S, Sertoli, M, Shabbir, A, Sharapov, S, Shaw, A, Shaw, R, Sheikh, H, Shepherd, A, Shevelev, A, Shumack, A, Sias, G, Sibbald, M, Sieglin, B, Silburn, S, Silva, A, Silva, C, Simmons, P, Simpson, J, Simpson-Hutchinson, J, Sinha, A, Sipila, S, Sips, A, Siren, P, Sirinelli, A, Sjostrand, H, Skiba, M, Skilton, R, Slabkowska, K, Slade, B, Smith, N, Smith, P, Smith, R, Smith, T, Smithies, M, Snoj, L, Soare, S, Solano, E, Somers, A, Sommariva, C, Sonato, P, Sopplesa, A, Sousa, J, Sozzi, C, Spagnolo, S, Spelzini, T, Spineanu, F, Stables, G, Stamatelatos, I, Stamp, M, Staniec, P, Stankunas, G, Stan-Sion, C, Stead, M, Stefanikova, E, Stepanov, I, Stephen, A, Stephen, M, Stevens, A, Steven, B, Strachan, J, Strand, P, Strauss, H, Stubbs, G, Studholme, W, Subba, F, Summers, H, Svensson, J, Swiderski, L, Szabolics, T, Szawlowski, M, Szepesi, G, Suzuki, T, Tal, B, Tala, T, Talbot, A, Talebzadeh, S, Taliercio, C, Tamain, P, Tame, C, Tang, W, Tardocchi, M, Taroni, L, Taylor, D, Taylor, K, Tegnered, D, Telesca, G, Teplova, N, Terranova, D, Testa, D, Tholerus, E, Thomas, J, Thomas, P, Thompson, A, A, Thompson, V, Thorne, L, Thornton, A, Thrysoe, A, Tigwell, P, Tipton, N, Tiseanu, I, Tojo, H, Tokitani, M, Tolias, P, Tomes, M, Tonner, P, Towndrow, M, Trimble, P, Tripsky, M, Tsalas, M, Tsavalas, P, Tskhakaya Jun, D, Turner, I, Turner, M, Turnyanskiy, M, Tvalashvili, G, Tyrrell, S, Uccello, A, Ul-Abidin, Z, Uljanovs, J, Ulyatt, D, Urano, H, Uytdenhouwen, I, Vadgama, A, Valcarcel, D, Valentinuzzi, M, Valisa, M, Vallejos Olivares, P, Valovic, M, Van De Mortel, M, Van Eester, D, Van Renterghem, W, van Rooij, G, Varje, J, Varoutis, S, Vartanian, S, Vasava, K, Vasilopoulou, T, Vega, J, Verdoolaege, G, Verhoeven, R, Verona, C, Verona Rinati, G, Veshchev, E, Vianello, N, Vicente, J, Viezzer, E, Villari, S, Villone, F, Vincenzi, P, Vinyar, I, Viola, B, Vitins, A, Vizvary, Z, Vlad, M, Voitsekhovitch, I, Vondracek, P, Vora, N, Vu, T, Pires de Sa, W, Wakeling, B, Waldon, C, Walkden, N, Walker, M, Walker, R, Walsh, M, Wang, E, Wang, N, Warder, S, Warren, R, Waterhouse, J, Watkins, N, Watts, C, Wauters, T, Weckmann, A, Weiland, J, Weisen, H, Weiszflog, M, Wellstood, C, West, A, Wheatley, M, Whetham, S, Whitehead, A, Whitehead, B, Wiesen, S, Wilkinson, J, Williams, J, Williams, M, Wilson, A, Wilson, D, Wilson, H, Wilson, J, Wischmeier, M, Withenshaw, G, Withycombe, A, Witts, D, Wood, D, Wood, R, Woodley, C, Wray, S, Wright, J, Wu, J, Wukitch, S, Wynn, A, Xu, T, Yadikin, D, Yanling, W, Yao, L, Yavorskij, V, Yoo, M, Young, C, Young, D, Young, I, Young, R, Zacks, J, Zagorski, R, Zaitsev, F, Zanino, R, Zarins, A, Zastrow, K, Zerbini, M, Zhang, W, Zhou, Y, Zilli, E, Zoita, V, Zoletnik, S, and Zychor, I
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ToF-ERDA ,Nuclear and High Energy Physics ,Materials science ,Tokamak ,oxidation ,02 engineering and technology ,release ,01 natural sciences ,Plasma-wall interactions ,010305 fluids & plasmas ,law.invention ,[SPI.MECA.MEFL]Engineering Sciences [physics]/Mechanics [physics.med-ph]/Fluids mechanics [physics.class-ph] ,Plasma-wall interaction ,law ,Impurity ,0103 physical sciences ,General Materials Science ,Fusion ,NRA ,SEM ,Composite material ,Quartz ,Jet (fluid) ,Divertor ,[SPI.FLUID]Engineering Sciences [physics]/Reactive fluid environment ,Settore FIS/01 - Fisica Sperimentale ,021001 nanoscience & nanotechnology ,Elastic recoil detection ,Nuclear Energy and Engineering ,Deuterium ,0210 nano-technology ,section - Abstract
Inconel-600 blocks and stainless steel covers for quartz microbalance crystals from remote corners in the JET-ILW divertor were studied with time-of-flight elastic recoil detection analysis and nuclear reaction analysis to obtain information about the areal densities and depth profiles of elements present in deposited material layers. Surface morphology and the composition of dust particles were examined with scanning electron microscopy and energy-dispersive X-ray spectroscopy. The analysed components were present in JET during three ITER-like wall campaigns between 2010 and 2017. Deposited layers had a stratified structure, primarily made up of beryllium, carbon and oxygen with varying atomic fractions of deuterium, up to more than 20%. The range of carbon transport from the ribs of the divertor carrier was limited to a few centimeters, and carbon/deuterium co-deposition was indicated on the Inconel blocks. High atomic fractions of deuterium were also found in almost carbon-free layers on the quartz microbalance covers. Layer thicknesses up to more than 1 mu m were indicated, but typical values were on the order of a few hundred nm. Chromium, iron and nickel fractions were less than or around 1% at layer surfaces while increasing close to the layer-substrate interface. The tungsten fraction depended on the proximity of the plasma strike point to the divertor corners. Particles of tungsten, molybdenum and copper with sizes less than or around 1 mu m were found. Nitrogen, argon and neon were present after plasma edge cooling and disruption mitigation. Oxygen-18 was found on component surfaces after injection, indicating in-vessel oxidation. Compensation of elastic recoil detection data for detection efficiency and ion-induced release of deuterium during the measurement gave quantitative agreement with nuclear reaction analysis, which strengthens the validity of the results. Crown Copyright (C) 2018 Published by Elsevier B.V. All rights reserved.
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- 2019
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10. The AGILE silicon tracker: Pre-launch and in-flight configuration
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Bulgarelli, A., Argan, A., Barbiellini, G., Basset, M., Chen, A., Di Cocco, G., Foggetta, L., Gianotti, F., Giuliani, A., Longo, F., Mereghetti, S., Monzani, F., Nicolini, L., Pavesi, R., Pellizzoni, A., Pontoni, C., Prest, M., Pucella, G., Tavani, M., Trifoglio, M., Trois, A., Vallazza, E., and Vercellone, S.
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- 2010
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11. The AGILE space mission
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Tavani, M., Barbiellini, G., Argan, A., Bulgarelli, A., Caraveo, P., Chen, A., Cocco, V., Costa, E., De Paris, G., Del Monte, E., Di Cocco, G., Donnarumma, I., Feroci, M., Fiorini, M., Froysland, T., Fuschino, F., Galli, M., Gianotti, F., Giuliani, A., Evangelista, Y., Labanti, C., Lapshov, I., Lazzarotto, F., Lipari, P., Longo, F., Marisaldi, M., Mastropietro, M., Mauri, F., Mereghetti, S., Morelli, E., Morselli, A., Pacciani, L., Pellizzoni, A., Perotti, F., Picozza, P., Pontoni, C., Porrovecchio, G., Prest, M., Pucella, G., Rapisarda, M., Rossi, E., Rubini, A., Soffitta, P., Trifoglio, M., Trois, A., Vallazza, E., Vercellone, S., Zambra, A., Zanello, D., Giommi, P., Antonelli, A., and Pittori, C.
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- 2008
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12. Single crystal diamond detectors grown by chemical vapor deposition
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Tuvè, C., Angelone, M., Bellini, V., Balducci, A., Donato, M.G., Faggio, G., Marinelli, M., Messina, G., Milani, E., Morgada, M.E., Pillon, M., Potenza, R., Pucella, G., Russo, G., Santangelo, S., Scoccia, M., Sutera, C., Tucciarone, A., and Verona-Rinati, G.
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- 2007
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13. Diamond-based photoconductors for deep UV detection
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Balducci, A., Bruzzi, M., De Sio, A., Donato, M.G., Faggio, G., Marinelli, M., Messina, G., Milani, E., Morgada, M.E., Pace, E., Pucella, G., Santangelo, S., Scoccia, M., Scuderi, S., Tucciarone, A., and Verona-Rinati, G.
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- 2006
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14. Temperature evolution of the surface region of CVD diamond: an electron spectroscopy study
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Filippi, M., Calliari, L., Pucella, G., and Verona-Rinati, G.
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- 2004
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15. Peaked density profiles in neon and lithium doped discharges on FTU.
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Mazzotta, C., Apicella, M.L., Botrugno, A., Gabellieri, L., Marinucci, M., Mazzitelli, G., Pucella, G., Sozzi, C., and Tudisco, O.
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NEON , *LITHIUM , *GLOW discharges , *TOKAMAKS , *FUSION reactor limiters , *PLASMA gases , *LIQUID metals - Abstract
Peaked density profiles are observed in FTU discharges when the recycling condition of the chamber is influenced by the action of the liquid lithium limiter (LLL) [1] . Turbulence analysis of lithium doped FTU plasmas [2,3] has shown that the presence of the light impurity modifies the phase between fluctuating fields responsible for transport and consequently leads to an inward deuterium pinch and outward impurity flux. Analogous peaked discharges were produced by Ne-gas puffing in different L mode plasma scenarios that have been recently obtained on FTU with following plasma parameters: I = 360 kA, B = 5–6.5 T, n e0 = 0.2–1 × 10 20 m −3 , T e0 = 1–4 keV, as well as in similar experiments on other machines [4] . In fact the Ne seeded plasmas show an increase of the peaking factor around 30% [5] . UV spectroscopy measurements confirm that the electron-density peaking arises from a convective flow and cannot be attributed to the contribution of the injected Ne alone. The Ne doped discharges analysis together with lithium conditioned ones is useful to extend the interpretative framework of the particle transport. In this work a comparison of the diffusion coefficient and of the pinch velocity of the two cases is conducted. By using a two-colors scanning interferometer providing very high spatial and time resolution, it is indeed possible to estimate the D and U coefficients of a simple model for the particle flux [6] . [ABSTRACT FROM AUTHOR]
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- 2014
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16. A first approach to runaway electron control in FTU.
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Boncagni, L., Carnevale, D., Cianfarani, C., Esposito, B., Granucci, G., Maddaluno, G., Marocco, D., Martin-Solis, J.R., Pucella, G., Sozzi, C., Varano, G., Vitale, V., and Zaccarian, L.
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PLASMA confinement , *TOKAMAKS , *ELECTRON beams , *ELECTRIC currents , *NUCLEAR physics experiments - Abstract
Abstract: The Plasma Control System (PCS) of the Frascati Tokamak Upgrade (FTU) is not equipped with any runaway electron (RE) beam control or suppression tool. In this paper we propose an upgraded PCS including an architecture for the control of disruption-generated REs that, making use of filtering techniques to estimate the onsets of the current quench (CQ) and of the RE beam current plateau, provides a controlled plasma current shut-down and a simultaneous RE position control. The control strategy is based on a nonlinear technique, called Input Allocation, that allows to re-configure the current in the poloidal field (PF) coils and improve the PCS responsiveness needed for RE position control. Preliminary results on the implementation of the Input Allocation and an experimental proposal to test the control scheme architecture are discussed. [Copyright &y& Elsevier]
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- 2013
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17. Characterization of a tagged beam line at the Beam Test Facility
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Cattaneo, P.W., Argan, A., Boffelli, F., Bulgarelli, A., Buonomo, B., Chen, A.W., D'Ammando, F., Foggetta, L., Froysland, T., Fuschino, F., Galli, M., Gianotti, F., Giuliani, A., Longo, F., Marisaldi, M., Mazzitelli, G., Pellizzoni, A., Prest, M., Pucella, G., and Quintieri, L.
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TESTING laboratories , *PARTICLE beams , *NUCLEAR physics instruments , *ARTIFICIAL satellites , *GAMMA rays , *IMAGE converters , *PARTICLE tracks (Nuclear physics) , *SIMULATION methods & models , *DIPOLE moments - Abstract
Abstract: At the core of the AGILE scientific instrument, designed to operate on a satellite, there is the Gamma Ray Imaging Detector (GRID) consisting of a Silicon Tracker (ST), a Cesium Iodide Mini-Calorimeter and an Anti-Coincidence system of plastic scintillator bars. The ST needs an on-ground calibration with a beam to validate the simulation used to calculate the energy response function and the effective area versus the energy and the direction of the rays. A tagged beam line was designed at the Beam Test Facility (BTF) of the INFN Laboratori Nazionali of Frascati (LNF), based on an electron beam generating through bremsstrahlung in a position-sensitive target. The energy is deduced by difference with the post-bremsstrahlung electron energy . The electron energy is measured by a spectrometer consisting of a dipole magnet and an array of position sensitive silicon strip detectors, the Photon Tagging System (PTS). The use of the combined BTF-PTS system as tagged photon beam requires understanding the efficiency of tagging, the probability of fake tagging, the energy resolution and the relation of the PTS hit position versus the energy. This paper describes this study comparing data taken during the AGILE calibration occurred in 2005 with simulation. [Copyright &y& Elsevier]
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- 2012
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18. Gamma-ray blazars: The view from AGILE
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D’Ammando, F., Bulgarelli, A., Chen, A.W., Donnarumma, I., Giuliani, A., Longo, F., Pacciani, L., Pucella, G., Striani, E., Tavani, M., Vercellone, S., Vittorini, V., Covino, S., Krimm, H.A., Raiteri, C.M., Romano, P., and Villata, M.
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GAMMA rays , *BL Lacertae objects , *DETECTORS , *WAVELENGTHS , *REFLECTION electron microscopy , *ACTIVE galactic nuclei , *QUASARS , *ASTRONOMICAL observatories - Abstract
Abstract: During the first 3years of operation the Gamma-Ray Imaging Detector onboard the AGILE satellite detected several blazars in a high γ-ray activity: 3C 279, 3C 454.3, PKS 1510-089, S5 0716+714, 3C 273, W Comae, Mrk 421, PKS 0537-441 and 4C +21.35. Thanks to the rapid dissemination of our alerts, we were able to obtain multiwavelength data from other observatories such as Spitzer, Swift, RXTE, Suzaku, INTEGRAL, MAGIC, VERITAS, and ARGO as well as radio-to-optical coverage by means of the GASP Project of the WEBT and the REM Telescope. This large multifrequency coverage gave us the opportunity to study the variability correlations between the emission at different frequencies and to obtain simultaneous Spectral Energy Distributions of these sources from radio to γ-ray energy bands, investigating the different mechanisms responsible for their emission and uncovering in some cases a more complex behavior with respect to the standard models. We present a review of the most interesting AGILE results on these γ-ray blazars and their multifrequency data. [Copyright &y& Elsevier]
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- 2011
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19. Pulse height defect in pCVD and scCVD diamond based detectors
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Tuve', C., Potenza, R., Chiorboli, M., Grimaldi, M.G., La Rosa, F., Raimondo, F., Marinelli, M., Milani, E., Tucciarone, A., Verona Rinati, G., Donato, M., Faggio, G., Messina, G., Santangelo, S., and Pucella, G.
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CHEMICAL vapor deposition , *NUCLEAR reactors , *VAPOR-plating , *NUCLEAR propulsion - Abstract
Abstract: Polycrystalline (pCVD) and single crystal (scCVD) diamond films grown from Chemical Vapour Deposition (CVD), if sufficiently pure at Raman analysis, are very good materials for beam or flux monitors inside accelerators or nuclear reactors. This is because they are very hard to damage in high radiation fields and very resistant to high temperatures. Films of pCVD diamond are, however, not so good as spectroscopy detectors due to inhomogeneities induced by their growth in grains with the consequent presence of grain boundaries which worsen their energy resolution. The latter can be significantly improved by growing scCVD diamond films onto HPHT synthetic diamond substrates. We have shown that it is possible to measure the density of defects inside diamond specimens using as probes suitable penetrating nuclear radiations. With the preliminary results reported here we''ll show that, bombarding CVD diamond films grown at Roma “Tor Vergata” with energetic protons and 4He, 6Li and 12C ions produced in the accelerators of Catania laboratories, the pulse height defects are higher than those in silicon detectors and likewise well described by a power law in the deposited energy. Furthermore, we''ll show that pulse heights for the same particles seem to depend on the duration of the measurement, thus exhibiting a sort of depolarization of the insulator when exposed to the electric voltage which makes it a particle detector. [Copyright &y& Elsevier]
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- 2006
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20. Radiological X-ray dosimetry with single crystal CVD diamond detectors
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Balducci, A., Garino, Y., Giudice, A. Lo, Manfredotti, C., Marinelli, Marco, Pucella, G., and Verona-Rinati, G.
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DRUG dosage , *SCISSION (Chemistry) , *NUCLEAR counters , *REACTION time - Abstract
Abstract: Pulsed X-ray measurements have been carried out by using new single crystal epitaxial CVD diamond samples about 100 μm thick grown by microwave CVD in Roma Tor Vergata Laboratories on a 300 μm thick, low cost, HPHT diamond substrate. Both sandwich arranged and surface interdigitated contacts were used for the detectors in order to compare their performances. A standard X-ray radiological apparatus was used with maximum X-ray energies from 50 to 120 keV. Delivered doses were in the range between 0 and 50 mGy, with pulse duration times between 0.01 and 0.5 s were obtained either by using different time-integrated mAs products or, at a fixed value of mAs, by using different values of the bias voltage of X-ray generator. The linearity of the dose signal Q given by the integrated current with respect to dose recorded by ionization chamber Δ was checked by evaluating dose linearity index, i.e. the exponent in the equation Q = AD Δ. The values of Δ were very close to 1 (between 1.02 and 1.07) in the case of a fixed mAs product, while it was around 0.8 at fixed voltage in the range 50–120 kV. The response time of the detector as deduced from the tail of the pulse was between 15 and 20 ms. The reproducibility was very good among different series of measurements, with no memory or priming effect. These results suggest a strong and actually real possibility for diamond detectors to be used as solid state ionization chambers in radiology and for diagnostic purposes. [Copyright &y& Elsevier]
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- 2006
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21. Growth and characterization of single crystal CVD diamond film based nuclear detectors
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Balducci, A., Marinelli, Marco, Milani, E., Morgada, M.E., Pucella, G., Scoccia, M., Tucciarone, A., Verona-Rinati, G., Angelone, M., Pillon, M., Potenza, R., and Tuvè, C.
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CRYSTAL whiskers , *EPITAXY , *CHEMICAL vapor deposition , *DIAMOND thin films - Abstract
Abstract: The deposition conditions and the detection properties of a homoepitaxial diamond film, grown by microwave Chemical Vapor Deposition (CVD) on a HPHT single crystal substrate are reported. The charge collection spectrum, measured under irradiation with a triple 239Pu 241Am 244Cm source emitting 5.16, 5.48 and 5.80 MeV α-particles respectively, shows three clearly resolved peaks with an energy resolution of about 1.1%. Both the charge collection efficiency and the energy resolution reach saturation values when the applied voltage exceeds 60 V, suggesting 100% collection efficiency. The detector was also tested with 14.8 and 14.1 MeV neutrons. The obtained collection spectra show a well separated 12C(n,α0)9Be reaction peak with an energy spread of 0.5 MeV for 14.8 MeV neutrons and 0.3 MeV for 14.1 MeV neutrons, which are fully compatible with the energy spread of the incident neutrons. [Copyright &y& Elsevier]
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- 2006
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22. High performance CVD-diamond-based thermocouple for gas sensing
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Balducci, A., D’Amico, A., Di Natale, C., Marinelli, M., Milani, E., Morgada, M.E., Pucella, G., Rodriguez, G., Tucciarone, A., and Verona-Rinati, G.
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CHEMICAL vapor deposition , *NONMETALS , *PALLADIUM , *ABSORPTION - Abstract
Abstract: A new thermochemical sensor was developed exploiting the unique properties of CVD-diamond. The thermal transduction step was based on the electric signal produced by a semiconductor–metal thermocouple. A thin film of boron doped polycrystalline diamond was grown by plasma enhanced CVD technique with CH3OH+B2O3 vapour addition. The high melting point, the chemical inertness and the extreme hardness make diamond an interesting candidate for sensing applications in harsh environments. The active thermocouple was completed evaporating a 120nm palladium film on the diamond film. The sensor was then tested for different temperature drops and showed good stability and repeatability in addition to high values of the thermoelectric power (S >350μV/°C). The catalytic properties of thin palladium films allow the thermocouple to be used for gas detection. In particular, hydrogen could be detected due to the palladium Fermi level modification, induced by the absorption process. To this purpose, the diamond–palladium sensor was exposed to different hydrogen concentrations, varying from 0.5 to 2%. The signal due to hydrogen absorption increases linearly with the gas concentration and is superimposed to the one produced by temperature changes. [Copyright &y& Elsevier]
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- 2005
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23. Recent IBIC measurements on epitaxial CVD diamond
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Balducci, A., Jaksic, M., Lo Giudice, A., Manfredotti, C., Marinelli, Marco, Medunic, S., Pucella, G., and Verona-Rinati, G.
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ION bombardment , *ELECTRIC equipment , *DIAMONDS , *NATIVE element minerals - Abstract
Abstract: Frontal IBIC (Ion Beam Induced Current) mesurements have been carried out on new single crystal epitaxial CVD diamond. The sample consists of about 100 μm synthetic diamond grown by microwave CVD on a 300 μm thick, low cost, HPHT diamond substrate (see Balducci et al. – this conference). Both proton and alpha microbeams of energies 3 and 4.5 MeV have been used, with a beam diameter spot of about 1.5–3 μm. Scanned areas varied from 450 μm×450 μm down to 150 μm × 150 μm and the homogeneity of charge collection efficiency (cce) was suitably monitored. At voltage bias of 80–100 V, the average cce was in the range 42–50%. Depending on the scanned surface area and on the beam type, energy resolutions FWHM from 1.3% to 4.1% FWHM have been obtained, even at counting rates as high as 700 cps. [Copyright &y& Elsevier]
- Published
- 2005
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24. Extreme UV single crystal diamond photodetectors by chemical vapor deposition
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Balducci, A., De Sio, A., Marinelli, Marco, Milani, E., Morgada, M.E., Pace, E., Prestopino, G., Pucella, G., Scoccia, M., Tucciarone, A., and Verona-Rinati, G.
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IRRADIATION , *CHEMICAL vapor deposition , *PHOTOCONDUCTIVITY , *ELECTRIC conductivity - Abstract
Abstract: The detection properties of a UV photodetector realized on a 150 μm thick CVD single crystal diamond film, grown at Roma “Tor Vergata” University on a low cost HPHT diamond substrate, are reported. The device was tested in the 210–2400 nm spectral range using pulsed laser irradiation and in the 20–250 nm range in continuous mode by both a deuterium lamp and a helium DC gas source irradiation. The detector shows more than five orders of magnitude of visible/UV rejection ratio, a very sharp signal drop of about 104 being observed in correspondence of the diamond energy gap. In the extreme UV range, the He II 25.6 and 30.4 nm as well as the He I 58.4 nm emission lines are clearly detected. The diamond time response is demonstrated to be considerably lower than 5 ns and 0.2 s in pulse and continuous mode, respectively. The extremely good signal to noise ratio, stability and reproducibility of the device response obtained, indicate that no persistent photoconductivity nor undesirable pumping effects are present, which represented so far the main problems preventing the use of diamond based detectors for UV applications. [Copyright &y& Elsevier]
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- 2005
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25. Separate measurement of electron and hole mean drift distance in CVD diamond
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Marinelli, Marco, Milani, E., Morgada, M.E., Pucella, G., Rodriguez, G., Tucciarone, A., Verona-Rinati, G., Angelone, M., and Pillon, M.
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DIAMOND thin films , *CHEMICAL vapor deposition , *DETECTORS , *IRRADIATION - Abstract
A method to measure independently the electron and hole mean drift distance (CCD) in CVD diamond is presented. Very high quality CVD diamond films were grown, and used as particle detectors. Their efficiency is measured as a function of the particle penetration depth under 5.5 MeV 241Am α-particles irradiation. The data are then fitted with a theoretical formula for the carrier mean drift distances derived from a properly modified Hecht model. Simultaneous fit of spectra collected for both positive and negative detector bias gives a separate evaluation of the mean drift distances of each carrier type. The α-particle penetration depth is controlled either using air as an absorbing layer or varying the particle incidence angle in the 0–80° range. The latter setup is demonstrated to provide higher accuracy. The results show that in our sample the electron and hole CCD are comparable in the as grown state. However, in the pumped state (i.e. after the detector is pre-irradiated with β-particles) the hole contribution is much greater than the electron one, showing that the pumping process is much more effective on hole traps than on electron traps. [Copyright &y& Elsevier]
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- 2004
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26. Raman and photoluminescence analysis of CVD diamond films: influence of Si-related luminescence centre on the film detection properties
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Donato, M.G., Faggio, G., Messina, G., Santangelo, S., Marinelli, Marco, Milani, E., Pucella, G., and Verona-Rinati, G.
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DIAMOND thin films , *CHEMICAL vapor deposition , *PHOTOLUMINESCENCE , *DETECTORS - Abstract
The performance of detectors based on CVD diamond films strongly depends on the material quality, which, in turn, is extremely sensitive to even slight variations of the deposition conditions. In this work, a careful Raman and photoluminescence (PL) study has been carried out on diamond films grown on Si substrates by microwave plasma CVD under nominally identical deposition conditions, but exhibiting, quite surprisingly, different detection sensitivity. Micro-PL measurements performed on the growth surface and on the cross-section of the samples have shown higher incorporation of Si impurities in films having lower detection performance. Optical microscopy on the nucleation side of such films has evidenced a lower nucleation density, leading to diamond grains of greater size, but also to higher incorporation of Si atoms. Thus, a greater grain size does not necessarily guarantee a higher film quality, if the nucleation density is low. On the basis of these results, the nucleation density is identified as the ‘hidden’ variable in the growth process of our CVD diamond films, determining, ultimately, their detection sensitivity. [Copyright &y& Elsevier]
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- 2004
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27. Analysis of traps in high quality CVD diamond films through the temperature dependence of carrier dynamics
- Author
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Marinelli, Marco, Milani, E., Paoletti, A., Pucella, G., Tucciarone, A., Verona Rinati, G., Angelone, M., and Pillon, M.
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DIAMONDS , *THIN films , *ELECTRONS , *ION traps - Abstract
The analysis of the time behavior of pulses generated by CVD diamond films irradiated with α-particles has been recently shown to be a general and powerful tool to investigate trap properties in diamond films (M. Marinelli et al., Phys. Rev. B 64 (2001) 195205). We use here this technique to measure the activation energy of traps in CVD diamond films, through the analysis of the temperature dependence of the dynamics of carriers generated by α-particle irradiation. The samples used in this study are high quality films deposited in a microwave tubular reactor and show very narrow diamond Raman peaks (FWHM approximately 2.4 cm−1) and extremely low photoluminescence background. The time evolution of the response of α-particle detectors built from these films exhibit both a fast and a slow component. Quantitative analysis leads to the conclusion that only deep traps limit the electron mean free path before trapping, while for holes both deep and shallow centers must be taken into account, the latter becoming the limiting factor in the pumped state. The changes in the pulse shapes are analyzed when the film temperature T is varied from −40 to 20 °C. A systematic speed-up of the response is found with increasing temperature, confirming that the slow component is due to thermally activated detrapping from the relative shallow defects. The detrapping time constant τD is connected to the activation energy ED of the defects through the formula 1/τD=s exp(−ED/kT), where s is the attempt frequency. Plotting ln(τD) vs. 1/T allows to determine the activation energy of the shallow defects, which is found to be 0.35 eV. [Copyright &y& Elsevier]
- Published
- 2003
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28. Carrier dynamics in CVD diamond: electron and hole contributions
- Author
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Tuvè, Cristina, Bellini, V., Potenza, R., Randieri, C., Sutera, C., Pucella, G., Marinelli, M., Milani, E., Paoletti, A., Tucciarone, A., and Verona-Rinati, G.
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DIAMONDS , *CHEMICAL vapor deposition - Abstract
The transport properties in synthetic diamond are studied using high quality diamond films grown by microwave plasma enhanced chemical vapor deposition (CVD). In particular, electron and hole contributions to the diamond carrier dynamics are successfully separated and defect distribution inside specimens is obtained. This is achieved through a systematic investigation of the signals obtained from properly biased diamonds irradiated with differently penetrating nuclear particles. To this purpose 12C ions produced by the 15 MV Tandem accelerator of the Southern National Laboratories of INFN in Catania (Italy) are used as a probe. The ion beam energy is varied in the 22–91 MeV range (penetration depth from 10.5 μm to the thickness of the used samples, deposited energies from 22 to 62 MeV and mean energy densities from 0.8 to 2.1 MeV/μm, respectively). The sample responses are studied as a function of the 12C energy and penetration depth, both in the positive and negative bias polarization. The experimental results clearly show that, when the detector is previously driven in the so-called pumped state by 90Sr β-particle irradiation, a different behavior of signals is observed in the positive and negative polarization states. The data are analysed in the framework of a properly modified Hecht model were the different behavior of carriers and influence of the variation in the ionization density along the path of the incident particles are considered. As a novelty the inhomogeneous distribution of defects is taken into account. By fitting the experimental curves with the model, a quantitative estimate of the defects distribution and of the correlated mean drift distance for electron and holes can be obtained. A good agreement is observed, thus allowing a better understanding of the diamond growth. [Copyright &y& Elsevier]
- Published
- 2003
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