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405 results on '"Park, S.-E."'

2. Sulfur-induced magnetism in FeSe$_{1-x}$S$_x$ thin films on LaAlO$_3$ revealed by muon spin rotation/relaxation

Author

Nabeshima, F., Kawai, Y., Shikama, N., Sakishita, Y., Suter, A., Prokscha, T., Park, S. E., Komiya, S., Ichinose, A., Adachi, T., and Maeda, A.

Subjects
Condensed Matter - Superconductivity
Abstract

Muon spin rotation/relaxation measurements were performed to investigate magnetic properties of FeSe$_{1-x}$S$_x$ thin films on LaAlO$_3$. A drastic decrease of the initial asymmetry was observed together with the peak structure in the temperature dependence of the relaxation rate of muon spins almost at the same temperature where kink anomalies were observed in the temperature dependent resistivity. With increasing S content, the anomaly temperature increased and the magnetic fluctuations at the lowest temperature were suppressed. These results show that the S substitution induces magnetism at low temperatures in FeSe$_{1-x}$S$_x$ thin films. Although the behaviors of the magnetic and nematic phases in FeSe films towards chemical pressure by S substitution are similar to those for bulk FeSe towards hydrostatic pressure, the behavior of $T_{\mathrm c}$ is significantly different between these systems. Our results demonstrate that the detailed comparative investigation among physical and chemical pressure effects is essentially important to understand the interplay of the magnetism, the nematicity and the superconductivity in iron chalcogenides., Comment: 19 pages, 5 figures

Published
2021
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3. The contribution of general practice placements to medical education : an analysis of the construction of general practice placement knowledge in published medical education research

Author

Park, S. E., Pelletier, C., and Newman, M.

Subjects
610.71
Abstract

This thesis examines the dominant discourses within research texts about undergraduate general practice placements. This makes visible what is said to be taught and learnt in placements; how research about placements is justified; and how these characterisations produce particular ways of being and knowing for subjects. Analysis examines rules of acceptability and discursive assumptions, exploring the 'thinkable' and 'unthinkable'. This process uses categories of object, subject position, concept and strategy, to build a map of ways in which texts characterise placements; how this produces particular ways of being and relations between students, patients, GPs and researchers; how these link with ways of conceptualising learning; and how overall strategies produce power relations. Two ways of characterizing placements are identified. A 'gaze of discovery' views placements as opportunistic experiential learning with patients, producing possibilities for patients as 'educator' and 'contextualised disease'; GP-teacher as 'facilitator'; and student as 'participatory learner' or 'intruder'. A more dominant 'gaze of deciphering' treats placements as pre-determined curricula compartments using mind-body and knowledge-skills-attitude distinctions to imagine different learning in different spaces. Placements are treated as basic, early or filling gaps in hospital-based curricula. This produces patient as 'subject with x'; student as 'learner of curriculum'; and GPs as 'teacher or clinician' and 'not knowing'. Evaluation is the dominant way of justifying research, positioning placements as innovative (and thereby un-established) and researcher as 'evaluator', distinct from clinician-teacher. Other texts justify research as 'making voices heard', some legitimising co-construction of knowledge with participants, and an integrated position for the researcher-practitioner. Overall, strategies position placements as supplementary and different to hospital teaching. Justifying research as evaluation produces challenges for the legitimacy of the field, in relation to other research. While teaching is treated as exchange of existing knowledge, research is positioned as informing teaching practice, legitimising its value through production of new knowledge.

Published
2017

4. Gamma-Rays Produced in Cosmic-Ray Interactions and the TeV-band Spectrum of RX J1713.7-3946

Author

Huang, C. -Y., Park, S. -E., Pohl, M., and Daniels, C. D.

Subjects
Astrophysics
Abstract

We employ the Monte Carlo particle collision code DPMJET3.04 to determine the multiplicity spectra of various secondary particles (in addition to $\pi^0$'s) with $\gamma$'s as the final decay state, that are produced in cosmic-ray ($p$'s and $\alpha$'s) interactions with the interstellar medium. We derive an easy-to-use $\gamma$-ray production matrix for cosmic rays with energies up to about 10 PeV. This $\gamma$-ray production matrix is applied to the GeV excess in diffuse Galactic $\gamma$-rays observed by EGRET, and we conclude the non-$\pi^0$ decay components are insufficient to explain the GeV excess, although they have contributed a different spectrum from the $\pi^0$-decay component. We also test the hypothesis that the TeV-band $\gamma$-ray emission of the shell-type SNR RX J1713.7-3946 observed with HESS is caused by hadronic cosmic rays which are accelerated by a cosmic-ray modified shock. By the $\chi^2$ statistics, we find a continuously softening spectrum is strongly preferred, in contrast to expectations. A hardening spectrum has about 1% probability to explain the HESS data, but then only if a hard cutoff at 50-100 TeV is imposed on the particle spectrum., Comment: 3 pages; 4 figures; Contribution to the First GLAST Symposium, Standord, 2007

Published
2007
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5. Diffuse Gamma-Rays Produced in Cosmic-Ray Interactions and the TeV-band Spectrum of RX J1713.7-3946

Author

Huang, C. -Y., Pohl, M., Park, S. -E., and Daniels, C. D.

Subjects
Astrophysics
Abstract

We employ the Monte Carlo particle collision code DPMJET3.04 to determine the multiplicity spectra of various secondary particles (in addition to $\pi^0$'s) with $\gamma$'s as the final decay state, that are produced in cosmic-ray ($p$'s and $\alpha$'s) interactions with the interstellar medium. We derive an easy-to-use $\gamma$-ray production matrix for cosmic rays with energies up to about 10 PeV. This $\gamma$-ray production matrix is applied to the GeV excess in diffuse Galactic $\gamma$-rays observed by EGRET, and we conclude the non-$\pi^0$ decay components are insufficient to explain the GeV excess, although they have contributed a different spectrum from the $\pi^0$-decay component. We also test the hypothesis that the TeV-band $\gamma$-ray emission of the shell-type SNR RX J1713.7-3946 observed with HESS is caused by hadronic cosmic rays which are accelerated by a cosmic-ray modified shock. By the $\chi^2$ statistics, we find a continuously softening spectrum is strongly preferred, in contrast to expectations. A hardening spectrum has about 1% probability to explain the HESS data, but then only if a hard cutoff at 50-100 TeV is imposed on the particle spectrum., Comment: 4 pages; 5 figures; Contribution to the 30th ICRC, Merida, Mexico, 2007; References included

Published
2007

6. Gamma-Rays Produced in Cosmic-Ray Interactions and the TeV-band Spectrum of RX J1713-3946

Author

Huang, C. -Y., Park, S. -E., Pohl, M., and Daniels, C. D.

Subjects
Astrophysics
Abstract

In this work we study the individual contribution to diffuse $\gamma$-ray emission from the secondary products in hadronic interactions generated by cosmic rays (CRs), in addition to the contribution of $\pi^0$ decay via the decay mode $\pi^0 \to 2\gamma$. For that purpose we employ the Monte Carlo particle collision code DPMJET3.04 to determine the multiplicity spectra of various secondary particles with $\gamma$'s as the final decay state, that result from inelastic collisions between cosmic-ray protons and Helium nuclei and the interstellar medium with standard composition. We thus derive an easy-to-use $\gamma$-ray production matrix for cosmic ray up to about 10 PeV, that can be used to interpret the $\gamma$-ray spectra of diffuse galactic emission and supernova remnants (SNR). We apply the $\gamma$-ray production matrix to the GeV excess in diffuse galactic $\gamma$-rays that was seen with EGRET. Although the non-$\pi^0$ contributions to the total emission have a different spectrum than the $\pi^0$-decay component, they are insufficient to explain the GeV excess. We also test the hypothesis that the TeV-band $\gamma$-ray emission of the shell-type SNR RX J1713-3946, that was observed with HESS, is caused by shock-accelerated hadronic cosmic rays. This scenario implies a very high efficacy of particle acceleration, so the particle spectrum is expected to continuously harden toward high energies on account of cosmic-ray modification of the shock. Using the $\chi^2$ statistic we find that a continuously softening spectrum is strongly preferred, in contrast to expectations. A hardening spectrum has about 1% probability to explain the HESS data, but then only if a hard cut-off at 50-100 TeV is imposed on the particle spectrum., Comment: minor revision; Astropart. Phys. in press

Published
2006
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7. Electric-field induced phase transitions in rhombohedral PZN-xPT

Author

Noheda, B., Zhong, Z., Cox, D. E., Shirane, G., Park, S-E., and Rehring, P.

Subjects
Condensed Matter - Materials Science
Abstract

High-energy x-ray diffraction experiments peformed on rhombohedral (1-x)Pb(Zn1/3Nb2/3)O3-xPbTiO3(PZN-xPT) crystals with x= 4.5 and 8% show that an electric field applied along the [001] direction induces the tetragonal phase, as proposed by Park and Shrout. Our experiments reveal that in 4.5PT such phase change occurs via a third phase with monoclinic symmetry, MA, which is observed at intermediate field values. This is in agreement with first-principles calculations by Fu and Cohen predicting the rotation of the polarization between the rhombohedral and tetragonal phases in this material. A different polarization path between the rhombohedral and tetragonal phases, through a second monoclinic phase, MC, has been previously reported in 8PT. The microscopic characterization of these crystals allows us to explain the ultra-high macroscopic strain observed in PZN-x%PT under an electric field. Moreover, some unusual scattering profiles displayed by exceptionally good crystals, are experimental evidence of the high anharmonicities and near-degeneracy of the different phases in these extremely deformable materials., Comment: REVTeX4, 8 two-column pages, 8 figures embedded

Published
2002
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8. Dynamical effects of the nanometer-sized polarized domains in Pb(Zn1/3Nb2/3)O3

Author

Gehring, P. M., Park, S. -E., and Shirane, G.

Subjects
Condensed Matter - Materials Science
Abstract

Recent neutron scattering measurements performed on the relaxor ferroelectric Pb[(Zn1/3Nb2/3)0.92Ti0.08]O3 (PZN-8%PT) in its cubic phase at 500 K, have revealed an anomalous ridge of inelastic scattering centered ~0.2 A-1 from the zone center (Gehring et al., Phys. Rev. Lett. 84, 5216 (2000)). This ridge of scattering resembles a waterfall when plotted as a phonon dispersion diagram, and extends vertically from the transverse acoustic (TA) branch near 4 meV to the transverse optic (TO) branch near 9 meV. No zone center optic mode was found. We report new results from an extensive neutron scattering study of pure PZN that exhibits the same waterfall feature. We are able to model the dynamics of the waterfall using a simple coupled-mode model that assumes a strongly q-dependent optic mode linewidth Gamma1(q) that increases sharply near 0.2 A-1 as one approaches the zone center. This model was motivated by the results of Burns and Dacol in 1983, who observed the formation of a randomly-oriented local polarization in PZN at temperatures far above its ferroelectric phase transition temperature. The dramatic increase in Gamma1 is believed to occur when the wavelength of the optic mode becomes comparable to the size of the small polarized micro-regions (PMR) associated with this randomly-oriented local polarization, with the consequence that longer wavelength optic modes cannot propagate and become overdamped. Below Tc=410 K, the intensity of the waterfall diminishes. At lowest temperatures ~30 K the waterfall is absent, and we observe the recovery of a zone center transverse optic mode near 10.5 meV., Comment: 8 pages, 9 figures (one color). Submitted to Physical Review B

Published
2000
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9. Polarization rotation via a monoclinic phase in the piezoelectric 92%PbZn1/3Nb2/3O3-8%PbTiO3

Author

Noheda, B., Cox, D. E., Shirane, G., Park, S-E., Cross, L. E., and Zhong, Z.

Subjects
Condensed Matter - Materials Science
Abstract

The origin of ultrahigh piezoelectricity in the relaxor ferroelectric PbZn1/3Nb2/3O3-PbTiO3 was studied with an electric field applied along the [001] direction. The zero-field rhombohedral R phase starts to follow the direct polarization path to tetragonal symmetry via an intermediate monoclinic M phase, but then jumps irreversibly to an alternate path involving a different type of monoclinic distortion. Details of the structure and domain configuration of this novel phase are described. This result suggests that there is a nearby R-M phase boundary as found in the Pb(Ti,Zr)O3 system., Comment: REVTeX file. 4 pages. New version after referees' comments

Published
2000
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10. The monoclinic phase in PZT: new light on morphotropic phase boundaries

Author

Noheda, B., Gonzalo, J. A., Guo, R., Park, S. -E., Cross, L. E., Cox, D. E., and Shirane, G.

Subjects
Condensed Matter - Materials Science
Abstract

A summary of the work recently carried out on the morphotropic phase boundary (MPB) of PZT is presented. By means of x-ray powder diffraction on ceramic samples of excellent quality, the MPB has been successfully characterized by changing temperature in a series of closely spaced compositions. As a result, an unexpected monoclinic phase has been found to exist in between the well-known tetragonal and rhombohedral PZT phases. A detailed structural analysis, together with the investigation of the field effect in this region of compositions, have led to an important advance in understanding the mechanisms responsible for the physical properties of PZT as well as other piezoelectric materials with similar morphotropic phase boundaries., Comment: 5 pages REVTeX file, 6 figures embedded. Presented at the Workshop on "Fundamental Physics of Ferroelectrics" held in Aspen, February 00. To appear in the proceedings

Published
2000
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11. Soft Phonon Anomalies in the Relaxor Ferroelectric Pb(Zn_1/3Nb_2/3)_0.92Ti_0.08O_3

Author

Gehring, P. M., Park, S. E., and Shirane, G.

Subjects
Condensed Matter - Materials Science
Abstract

Neutron inelastic scattering measurements of the polar TO phonon mode dispersion in the cubic relaxor Pb(Zn_1/3Nb_2/3)_0.92Ti_0.08O_3 at 500K reveal anomalous behavior in which the optic branch appears to drop precipitously into the acoustic branch at a finite value of the momentum transfer q=0.2 inverse Angstroms, measured from the zone center. We speculate this behavior is the result of nanometer-sized polar regions in the crystal., Comment: 4 pages, 4 figures

Published
2000
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12. Origin of the high piezoelectric response in PbZr(1-x)TixO3

Author

Guo, R., Cross, L. E., Park, S-E., Noheda, B., Cox, D. E., and Shirane, G.

Subjects
Condensed Matter - Materials Science
Abstract

High resolution x-ray powder diffraction measurements on poled PbZr(1-x)TixO3 (PZT) ceramic samples close to the rhombohedral-tetragonal phase boundary (the so-called morphotropic phase boundary, MPB) have shown that for both rhombohedral and tetragonal compositions, the piezoelectric elongation of the unit cell does not occur along the polar directions but along those directions associated with the monoclinic distortion. This work provides the first direct evidence for the origin of the very high piezoelectricity in PZT., Comment: 4 pages, 4 EPS figures embedded. More specific title and abstract. To appear in Phys. Rev. Lett

Published
1999
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13. A tetragonal-to-monoclinic phase transition in a ferroelectric perovskite: the structure of PbZr(0.52)Ti(0.48)O3

Author

Noheda, B., Gonzalo, J. A., Cross, L. E., Guo, R., Park, S-E., Cox, D. E., and Shirane, G.

Subjects
Condensed Matter - Materials Science
Abstract

The perovskite-like ferroelectric system PbZr(1-x)Ti(x)O3 (PZT) has a nearly vertical morphotropic phase boundary (MPB) around x=0.45-0.50. Recent synchrotron x-ray powder diffraction measurements by Noheda et al. [Appl. Phys. Lett. 74, 2059 (1999)] have revealed a new monoclinic phase between the previously-established tetragonal and rhombohedral regions. In the present work we describe a Rietveld analysis of the detailed structure of the tetragonal and monoclinic PZT phases on a sample with x= 0.48 for which the lattice parameters are respectively: at= 4.044 A, ct= 4.138 A, at 325 K, and am= 5.721 A, bm= 5.708 A, cm= 4.138 A, beta= 90.496 deg., at 20K. In the tetragonal phase the shifts of the atoms along the polar [001] direction are similar to those in PbTiO3 but the refinement indicates that there are, in addition, local disordered shifts of the Pb atoms of ~0.2 A perpendicular to the polar axis.. The monoclinic structure can be viewed as a condensation along one of the <110> directions of the local displacements present in the tetragonal phase. It equally well corresponds to a freezing-out of the local displacements along one of the <100> directions recently reported by Corker et al.[J. Phys. Condens. Matter 10, 6251 (1998)] for rhombohedral PZT. The monoclinic structure therefore provides a microscopic picture of the MPB region in which one of the "locally" monoclinic phases in the "average" rhombohedral or tetragonal structures freezes out, and thus represents a bridge between these two phases., Comment: REVTeX, 7 figures. Modifications after referee's suggestion: new figure (figure 5), comments in 2nd para. (Sect.III) and in 2nd & 3rd para. (Sect. IV-a), in the abstract: "...of ~0.2 A perpendicular to the polar axis."

Published
1999
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14. A monoclinic ferroelectric phase in the Pb(Zr1-xTix)O3 solid solution

Author

Noheda, B., Cox, D. E., Shirane, G., Gonzalo, J. A., Cross, L. E., and Park, S-E.

Subjects
Condensed Matter - Materials Science
Abstract

A previously unreported ferroelectric phase has been revealed on a highly homogeneous sample of Pb(Zr0.52Ti0.48)O3 by high-resolution synchrotron x-ray powder diffraction measurements. At ambient temperature the sample has tetragonal symmetry (at= 4.037 A, ct= 4.138 A), and transforms below ~250 K into a phase which, unexpectedly, has monoclinic symmetry (am= 5.717 A, bm= 5.703 A, cm= 4.143 A, beta= 90.53 deg., at 20K). The intensity data strongly indicate that the polar axis lies in the monoclinic ac plane close to the pseudo-cubic [111] direction, which would be an example of the species m3m(12)A2Fm predicted on symmetry grounds by Shuvalov., Comment: 6 pages HTML file including 4 figures. Replaced to add Journal ref. Figures format changed. No change in the content

Published
1999
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34. X-ray diffraction and phenomenological studies of the engineered monoclinic crystal domains in single crystal relaxor ferroelectrics

Author

Durbin, M. K., Hicks, J. C., Park, S. E., and Shrout, T. R.

Subjects
Titanates -- Electric properties, Lead compounds -- Electric properties, Ferroelectric crystals -- Electric properties, Physics
Abstract

X-ray diffraction data is presented by demonstrating after high field poling, solid solutions of lead zinc niobate with 8% lead titanate (PZN-PT) consisting of mixture of a dominant monoclinic phase and a remnant tetragonal phase. Diffraction shows a slight distorted version of the rhombohedral zero field solution resulting from the domain walls that consist of a tetragonal phase.

Published
2000

42. Contributions of biodiversity to the sustainable intensification of food production:The State of the World’s Biodiversity for Food and Agriculture

Author

Dawson, I.K., Attwood, S. J., Park, S. E., Jamnadass, R., Powell, W., Sunderland, T., Kindt, R., McMullin, S., Hoebe, P.N., Baddeley, J., Staver, C., Vadez, V., Carsan, S., Roshetko, J. M., Amri, A., Karamura, E., Karamura, D., Breugel, P. van, Hossain, E, Phillips, M., Kumar, A., Lillesø, Jens-Peter Barnekow, Benzie, J., Sebastian, G.E., Ekesa, B., Ocimati, W., and Graudal, Lars

Published
2019

43. Probing the chiral magnetic wave in pPb and PbPb collisions at root S-NN=5.02 TeV using charge-dependent azimuthal anisotropies

Author

Sirunyan, A. M., Tumasyan, A., Adam, W., Ambrogi, F., Asilar, E., Bergauer, T., Stetter, J., Brondolin, E., Dragicevic, M., Ero, J., Flechl, M., Friedl, M., Fruhwirth, R., Ghete, V. M., Grossmann, J., Hrubec, J., Jeitler, M., Konig, A., Krammer, N., Kratschmer, I., Liko, D., Madlener, T., Mikulec, I., Pree, E., Rabady, D., Rad, N., Rohringer, H., Schieck, J., Schofbeck, R., Spanring, M., Spitzbart, D., Waltenberger, W., Wittmann, J., Wulz, C. -E., Zarucki, M., Chekhovsky, V., Mossolov, V., Gonzalez, J. Suarez, De Wolf, E. A., Di Croce, D., Janssen, X., Lauwers, J., Van Haevermaet, H., Van Mechelen, P., Van Remortel, N., Abu Zeid, S., Blekman, F., D'Hondt, J., De Bruyn, I., De Clercq, J., Deroover, K., Flouris, G., Lontkovskyi, D., Lowette, S., Moortgat, S., Moreels, L., Python, Q., Skovpen, K., Tavernier, S., Van Doninck, W., Van Mulders, P., Van Parijs, I., Brun, H., Clerbaux, B., De Lentdecker, G., Delannoy, H., Fasanella, G., Favart, L., Goldouzian, R., Grebenyuk, A., Karapostoli, G., Lenzi, T., Luetic, J., Maerschalk, T., Marinov, A., R, le-conde, A., Seva, T., V, er Velde, C., Vanlaer, P., Vannerom, D., Yonamine, R., Zenoni, F., Zhang, F., Cimmino, A., Cornelis, T., Dobur, D., Fagot, A., Gul, M., Khvastunov, I., Poyraz, D., Roskas, C., Salva, S., Tytgat, M., Verbeke, W., Zaganidis, N., Bakhshiansohi, H., Bondu, O., Brochet, S., Bruno, G., Caputo, C., Caudron, A., De Visscher, S., Delaere, C., Delcourt, M., Francois, B., Giammanco, A., Jafari, A., Komm, M., Krintiras, G., Lemaitre, V., Magitteri, A., Mertens, A., Musich, M., Piotrzkowski, K., Quertenmont, L., Marono, M. Vidal, Wertz, S., Beliy, N., Alda Junior, W. L., Alves, F. L., Alves, G. A., Brito, L., Correa Martins Junior, M., Hensel, C., Moraes, A., Pol, M. E., Rebello Teles, P., Belchior Batista Das Chagas, E., Carvalho, W., Chinellato, J., Custodio, A., Da Costa, E. M., Da Silveira, G. G., De Jesus Damiao, D., De Souza, S. Fonseca, Huertas Guativa, L. M., Malbouisson, H., Melo De Almeida, M., Mora Herrera, C., Mundim, L., Nogima, H., Santoro, A., Sznajder, A., Manganote, E. J. Tonelli, Torres Da Silva De Araujo, F., Vilela Pereira, A., Ahuja, S., Bernardes, C. A., Fern, ez Perez Tomei, T. R., Gregores, E. M., Mercadante, P. G., Novaes, S. F., Padula, S, Ra, S., Abad, D. Romero, Ruiz Vargas, J. C., Aleks, Rov, A., Hadjiiska, R., Iaydjiev, P., Misheva, M., Rodozov, M., Shopova, M., Stoykova, S., Sultanov, G., Dimitrov, A., Glushkov, I., Litov, L., Pavlov, B., Petkov, P., Fang, W., Gao, X., Ahmad, M., Bian, J. G., Chen, G. M., Chen, H. S., Chen, M., Chen, Y., Jiang, C. H., Leggat, D., Liao, H., Liu, Z., Romeo, F., Shaheen, S. M., Spiezia, A., Tao, J., Wang, C., Wang, Z., Yazgan, E., Zhang, H., Zhang, S., Zhao, J., Ban, Y., Chen, G., Li, Q., Liu, S., Mao, Y., Qian, S. J., Wang, D., Xu, Z., Avila, C., Cabrera, A., Sierra, L. F. Chaparro, Florez, C., Gonzalez, Hern, C. F., Ez, Ruiz Alvarez, J. D., Courbon, B., Godinovic, N., Lelas, D., Puljak, I., Ribeiro Cipriano, P. M., Sculac, T., Antunovic, Z., Kovac, M., Brigljevic, V., Ferencek, D., Kadija, K., Mesic, B., Starodumov, A., Susa, T., Ather, M. W., Attikis, A., Mavromanolakis, G., Mousa, J., Nicolaou, C., Ptochos, F., Razis, P. A., Rykaczewski, H., Finger, M., Finger, J, R., Carrera Jarrin, E., Assran, Y., Mahmoud, M. A., Mahrous, A., Dewanjee, R. K., Kadastik, M., Perrini, L., Raidal, M., Tiko, A., Veelken, C., Eerola, P., Pekkanen, J., Voutilainen, M., Harkonen, J., Jarvinen, T., Karimaki, V., Kinnunen, R., Lampen, T., Lassila-Perini, K., Lehti, S., Linden, T., Luukka, P., Tuominen, E., Tuominiemi, J., Tuovinen, E., Talvitie, J., Tuuva, T., Besancon, M., Couderc, F., Dejardin, M., Denegri, D., Faure, J. L., Ferri, F., Ganjour, S., Ghosh, S., Givernaud, A., Gras, P., Hamel de Monchenault, G., Jarry, P., Kucher, I., Locci, E., Machet, M., Malcles, J., Negro, G., Er, J., Rosowsky, A., Sahin, M. O., Titov, M., Abdulsalam, A., Antropov, I., Baffioni, S., Beaudette, F., Busson, P., Cadamuro, L., Charlot, C., Granier de Cassagnac, R., Jo, M., Lisniak, S., Lobanov, A., Martin Blanco, J., Nguyen, M., Och, O, C., Ortona, G., Paganini, P., Pigard, P., Regnard, S., Salerno, R., Sauvan, J. B., Sirois, Y., Stahl Leiton, A. G., Strebler, T., Yilmaz, Y., Zabi, A., Zghiche, A., Agram, J. -L., Andrea, J., Bloch, D., Brom, J. -M., Buttignol, M., Chabert, E. C., Chanon, N., Collard, C., Conte, E., Coubez, X., Fontaine, J. -C., Gele, D., Goerlach, U., Jansova, M., Le Bihan, A. -C., Tonon, N., Van Hove, P., Gadrat, S., Beauceron, S., Bernet, C., Boudoul, G., Chierici, R., Contardo, D., Depasse, P., El Mamouni, H., Fay, J., Finco, L., Gascon, S., Gouzevitch, M., Grenier, G., Ille, B., Lagarde, F., Laktineh, I. B., Lethuillier, M., Mirabito, L., Pequegnot, A. L., Perries, S., Popov, A., Sordini, V., er Donckt, M., Viret, S., Toriashvili, T., Bagaturia, I., Autermann, C., Beranek, S., Feld, L., Kiesel, M. K., Klein, K., Lipinski, M., Preuten, M., Schomakers, C., Schulz, J., Verlage, T., Zhukov, V., Albert, A., Dietz-Laursonn, E., Duchardt, D., Endres, M., Erdmann, M., Erdweg, S., Esch, T., Fischer, R., Guth, A., Hamer, M., Hebbeker, T., Heidemann, C., Hoepfner, K., Knutzen, S., Merschmeyer, M., Meyer, A., Millet, P., Mukherjee, S., Olschewski, M., Padeken, K., Pook, T., Radziej, M., Reithler, H., Rieger, M., Scheuch, F., Teyssier, D., Thuer, S., Flugge, G., Kargoll, B., Kress, T., Kunsken, A., Lingemann, J., Muller, T., Nehrkorn, A., Nowack, A., Pistone, C., Pooth, O., Stahl, A., Martin, M. Aldaya, Arndt, T., Asawatangtrakuldee, C., Beernaert, K., Behnke, O., Behrens, U., Bermudez Martinez, A., Bin Anuar, A. A., Borras, K., Botta, V., Campbell, A., Connor, P., Contreras-Campana, C., Costanza, F., Pardos, C. Diez, Eckerlin, G., Eckstein, D., Eichhorn, T., Eren, E., Gallo, E., Garay Garcia, J., Geiser, A., Gizhko, A., Grados, Luy, J. 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Subjects
Science & Technology, Physics, Nuclear, EVENT, Physics::Instrumentation and Detectors, Physics, PARITY VIOLATION, Physical Sciences, Centre for High Energy Physics, SIDE ANGULAR-CORRELATIONS, LONG-RANGE, nucl-ex, Nuclear Experiment
Abstract

Made available in DSpace on 2020-12-11T05:11:56Z (GMT). No. of bitstreams: 0 Previous issue date: 2019-12-18 BMWFW (Austria) FWF (Austria) FNRS (Belgium) FWO (Belgium) Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES) Fundação de Amparo à Pesquisa do Estado do Rio de Janeiro (FAPERJ) Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) MES (Bulgaria) CERN CAS (China) MoST (China) NSFC (China) COLCIENCIAS (Colombia) MSES (Croatia) CSF (Croatia) RPF (Cyprus) SENESCYT (Ecuador) MoER (Estonia) ERC IUT (Estonia) ERDF (Estonia) Academy of Finland (Finland) MEC (Finland) HIP (Finland) CEA (France) CNRS/IN2P3 (France) BMBF (Germany) DFG (Germany) HGF (Germany) GSRT (Greece) OTKA (Hungary) NIH (Hungary) DAE (India) DST (India) IPM (Iran) SFI (Ireland) INFN (Italy) MSIP (Republic of Korea) NRF (Republic of Korea) LAS (Lithuania) MOE (Malaysia) UM (Malaysia) BUAP (Mexico) CINVES-TAV (Mexico) CONACYT (Mexico) LNS (Mexico) SEP(Mexico) UASLP-FAI (Mexico) MBIE (New Zealand) PAEC (Pakistan) MSHE (Poland) NSC (Poland) FCT (Portugal) JINR (Dubna) MON (Russia) RosAtom (Russia) RAS (Russia) RFBR (Russia) RAEP (Russia) MESTD (Serbia) SEIDI (Spain) CPAN (Spain) PCTI (Spain) FEDER (Spain) MST (Taipei) ThEPCenter (Thailand) IPST (Thailand) STAR (Thailand) NSTDA (Thailand) TUBITAK (Turkey) TAEK (Turkey) NASU (Ukraine) SFFR (Ukraine) STFC (United Kingdom) DOE (USA) NSF (USA) Marie Curie program European Research Council Horizon 2020 Grant Leventis Foundation the A. P. Sloan Foundation Alexander von Humboldt Foundation Belgian Federal Science Policy Office Fonds pour la Formation a la Recherche dans l'Industrie et dans l'Agriculture (FRIABelgium) Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium) Ministry of Education, Youth and Sports (MEYS) of the Czech Republic Council of Science and Industrial Research, India HOMING PLUS program of the Foundation for Polish Science European Union, Regional Development Fund Mobility Plus program of the Ministry of Science and Higher Education National Science Center (Poland) the National Priorities Research Program by Qatar National Research Fund Programa Clarin-COFUND del Principado de Asturias Thalis program Aristeia program EU-ESF Greek NSRF Rachadapisek Sompot Fund for Postdoctoral Fellowship, Chulalongkorn University Chulalongkorn Academic into Its 2nd Century Project Advancement Project (Thailand) Welch Foundation Weston Havens Foundation (USA) Charge-dependent anisotropy Fourier coefficients (v(n)) of particle azimuthal distributions are measured in pPb and PbPb collisions at root S-NN = 5.02 TeV with the CMS detector at the LHC. The normalized difference in the second-order anisotropy coefficients (v(2)) between positively and negatively charged particles is found to depend linearly on the observed event charge asymmetry with comparable slopes for both pPb and PbPb collisions over a wide range of charged particle multiplicity. In PbPb, the third-order anisotropy coefficient v(3) shows a similar linear dependence with the same slope as seen for v(2). The observed similarities between the v(2) slopes for pPb and PbPb, as well as the similar slopes for v(2) and v(3) in PbPb, are compatible with expectations based on local charge conservation in the decay of clusters or resonances, and constitute a challenge to the hypothesis that, at LHC energies, the observed charge asymmetry dependence of v(2) in heavy ion collisions arises from a chiral magnetic wave. Yerevan Phys Inst, Yerevan, Armenia Inst Hochenergiephys, Vienna, Austria Inst Nucl Problems, Minsk, BELARUS Univ Antwerp, Antwerp, Belgium Vrije Univ Brussel, Brussels, Belgium Univ Libre Bruxelles, Brussels, Belgium Univ Ghent, Ghent, Belgium Univ Catholoque Louvain, Louvain La Neuve, Belgium Univ Mons, Mons, Belgium Ctr Brasileiro Pesquisas Fis, Rio De Janeiro, Brazil Univ Estado Rio de Janeiro, Rio De Janeiro, Brazil Univ Estadual Paulista, Sao Paulo, Brazil Univ Fed ABC, Sao Paulo, Brazil Bulgaria Acad Sci, Inst Nucl Res & Nucl Energy, Bulgaria, Romania Univ Sofia, Sofia, Bulgaria Beihang Univ, Beijing, Peoples R China Inst High Energy Phys, Beijing, Peoples R China Peking Univ, State Key Lab Nucl Phys & Technol, Beijing, Peoples R China Univ Los Andes, Bogota, Colombia Univ Split, Fac Elect Engn Mech Engn & Naval Architecture, Split, Croatia Univ Split, Fac Sci, Split, Croatia Inst Rudjer Boskov, Zagreb, Croatia Univ Cyprus, Nicosia, Cyprus Charles Univ Prague, Prague, Czech Republic Univ San Francisco Quito, Quito, Ecuador Acad Sci Res & Technol Arab Republ Egypt, Egyptian Network High Energy Phys, Cairo, Egypt NICPB, Tallinn, Estonia Univ Helsinki, Dept Phys, Helsinki, Finland Helsinki Inst Phys, Helsinki, Finland Lappeenranta Univ Technol, Lappeenranta, Finland Univ Paris Saclay, IRFU, CEA, Gif Sur Yvette, France Univ Paris Saclay, CNRS IN2P3, Ecole Polytech, Lab Leprince Ringuet, Palaiseau, France Univ Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France CNRS IN2P3, Villeurbanne, France Univ Claude Bernard Lyon 1, Univ Lyon, CNRS IN2P3, Inst Phys Nucl Lyon, Villeurbanne, France Georgian Tech Univ, Tbilisi, Georgia Tbilisi State Univ, Tbilisi, Georgia Rhein Westfal TH Aachen, Phys Inst 1, Aachen, Germany Rhein Westfal TH Aachen, Phys Inst A 3, Aachen, Germany Rhein Westfal TH Aachen, Phys Inst B 3, Aachen, Germany Deutsch Elekt Synchrotron, Hamburg, Germany Univ Hamburg, Hamburg, Germany Inst Expt Kernphys, Karlsruhe, Germany INPP, NCSR Demokritos, Aghia Paraskevi, Greece Univ Athens, Athens, Greece Natl Tech Univ Athens, Athens, Greece Univ Ioannina, Ioannina, Greece Eotvos Lorand Univ, MTA ELTE Lendulet CMS Particle, Budapest, Hungary Eotvos Lorand Univ, Nucl Phys Grp, Budapest, Hungary Wigner Res Ctr Phys, Budapest, Hungary Inst Nucl Res ATOMKI, Debrecen, Hungary Univ Debrecen, Inst Phys, Debrecen, Hungary Indian Inst Sci IISc, Bangalore, Karnataka, India Natl Inst Sci Educ & Res, Bhubaneswar, India Panjab Univ, Chandigarh, India Univ Delhi, Delhi, India Saha Inst Nucl Phys, HBNI, Kolkata, India Indian Inst Technol Madras, Madras, Tamil Nadu, India Bhabha Atom Res Ctr, Mumbai, Maharashtra, India Tata Inst Fundamental Res A, Mumbai, Maharashtra, India Tata Inst Fundamental Res B, Mumbai, Maharashtra, India IISER, Pune, Maharashtra, India Inst Res Fundamental Sci IPM, Tehran, Iran Univ Coll Dublin, Dublin, Ireland INFN Sez Bari, Bari, Italy Univ Bari, Bari, Italy Politecn Bari, Bari, Italy INFN Sez Bologna, Bologna, Italy Univ Bologna, Bologna, Italy INFN Sez Catania, Catania, Italy Univ Catania, Catania, Italy INFN Sez Firenze, Florence, Italy Univ Firenze, Florence, Italy INFN Lab Nazl Frascati, Frascati, Italy INFN Sez Genova, Genoa, Italy Univ Genoa, Genoa, Italy INFN Sez Milano Bicocca, Milan, Italy Univ Milano Bicocca, Milan, Italy INFN Sez Napoli, Naples, Italy Univ Napoli Federico II, Naples, Italy Univ Basilicata, Potenza, Italy Univ G Marconi, Rome, Italy INFN Sez Padova, Padua, Italy Univ Padua, Padua, Italy Univ Trento, Trento, Italy INFN Sez Pavia, Pavia, Italy Univ Pavia, Pavia, Italy INFN Sez Perugia, Perugia, Italy Univ Perugia, Perugia, Italy INFN Sez Pisa, Pisa, Italy Univ Pisa, Pisa, Italy Scuola Normale Super Pisa, Pisa, Italy INFN Sez Roma, Rome, Italy Sapienza Univ Roma, Rome, Italy INFN Sez Torino, Turin, Italy Univ Torino, Turin, Italy Univ Piemonte Orientale, Turin, Italy INFN Sez Trieste, Trieste, Italy Univ Trieste, Trieste, Italy Kyungpook Natl Univ, Daegu, South Korea 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Spain Utah Valley Univ, Orem, UT USA Beykent Univ, Istanbul, Turkey Bingol Univ, Bingol, Turkey Sinop Univ, Sinop, Turkey Mimar Sinan Univ, Istanbul, Turkey Texas A&M Univ, Doha, Qatar Univ Estadual Paulista, Sao Paulo, Brazil Horizon 2020 Grant: 675440 National Science Center (Poland): Harmonia 2014/14/M/ST2/00428 National Science Center (Poland): Opus 2014/13/B/ST2/02543 National Science Center (Poland): 2014/15/B/ST2/03998 National Science Center (Poland): 2015/19/B/ST2/02861 National Science Center (Poland): Sonata-bis 2012/07/E/ST2/01406 Welch Foundation: C-1845

Published
2019

44. Probing the chiral magnetic wave in pPb and PbPb collisions at root S-NN=5.02 TeV using charge-dependent azimuthal anisotropies

Author

Sirunyan, A. M. Tumasyan, A. Adam, W. Ambrogi, F. and Asilar, E. Bergauer, T. Brandstetter, J. Brondolin, E. and Dragicevic, M. Ero, J. Flechl, M. Friedl, M. Fruhwirth, R. Ghete, V. M. Grossmann, J. Hrubec, J. Jeitler, M. and Konig, A. Krammer, N. Kratschmer, I. Liko, D. Madlener, T. Mikulec, I. Pree, E. Rabady, D. Rad, N. and Rohringer, H. Schieck, J. Schofbeck, R. Spanring, M. and Spitzbart, D. Waltenberger, W. Wittmann, J. Wulz, C. -E. and Zarucki, M. Chekhovsky, V. Mossolov, V. Gonzalez, J. Suarez and De Wolf, E. A. Di Croce, D. Janssen, X. Lauwers, J. and Van Haevermaet, H. Van Mechelen, P. Van Remortel, N. Abu Zeid, S. Blekman, F. D'Hondt, J. De Bruyn, I. De Clercq, J. Deroover, K. Flouris, G. Lontkovskyi, D. Lowette, S. and Moortgat, S. Moreels, L. Python, Q. Skovpen, K. and Tavernier, S. Van Doninck, W. Van Mulders, P. Van Parijs, I. and Brun, H. Clerbaux, B. De Lentdecker, G. Delannoy, H. and Fasanella, G. Favart, L. Goldouzian, R. Grebenyuk, A. and Karapostoli, G. Lenzi, T. Luetic, J. Maerschalk, T. and Marinov, A. Randle-conde, A. Seva, T. Vander Velde, C. and Vanlaer, P. Vannerom, D. Yonamine, R. Zenoni, F. Zhang, F. Cimmino, A. Cornelis, T. Dobur, D. Fagot, A. Gul, M. Khvastunov, I. Poyraz, D. Roskas, C. Salva, S. and Tytgat, M. Verbeke, W. Zaganidis, N. Bakhshiansohi, H. and Bondu, O. Brochet, S. Bruno, G. Caputo, C. Caudron, A. and De Visscher, S. Delaere, C. Delcourt, M. Francois, B. and Giammanco, A. Jafari, A. Komm, M. Krintiras, G. and Lemaitre, V. Magitteri, A. Mertens, A. Musich, M. and Piotrzkowski, K. Quertenmont, L. Marono, M. Vidal Wertz, S. and Beliy, N. Alda Junior, W. L. Alves, F. L. Alves, G. A. and Brito, L. Correa Martins Junior, M. Hensel, C. Moraes, A. Pol, M. E. Rebello Teles, P. Belchior Batista Das Chagas, E. Carvalho, W. Chinellato, J. Custodio, A. Da Costa, E. M. Da Silveira, G. G. De Jesus Damiao, D. De Souza, S. Fonseca Huertas Guativa, L. M. Malbouisson, H. Melo De Almeida, M. Mora Herrera, C. Mundim, L. Nogima, H. and Santoro, A. Sznajder, A. Manganote, E. J. Tonelli Torres Da Silva De Araujo, F. Vilela Pereira, A. Ahuja, S. Bernardes, C. A. Fernandez Perez Tomei, T. R. Gregores, E. M. and Mercadante, P. G. Novaes, S. F. Padula, Sandra S. Abad, D. Romero Ruiz Vargas, J. C. Aleksandrov, A. Hadjiiska, R. and Iaydjiev, P. Misheva, M. Rodozov, M. Shopova, M. and Stoykova, S. Sultanov, G. Dimitrov, A. Glushkov, I. and Litov, L. Pavlov, B. Petkov, P. Fang, W. Gao, X. and Ahmad, M. Bian, J. G. Chen, G. M. Chen, H. S. Chen, M. and Chen, Y. Jiang, C. H. Leggat, D. Liao, H. Liu, Z. and Romeo, F. Shaheen, S. M. Spiezia, A. Tao, J. Wang, C. Wang, Z. Yazgan, E. Zhang, H. Zhang, S. Zhao, J. and Ban, Y. Chen, G. Li, Q. Liu, S. Mao, Y. Qian, S. J. Wang, D. Xu, Z. Avila, C. Cabrera, A. Sierra, L. F. Chaparro Florez, C. Gonzalez Hernandez, C. F. Ruiz Alvarez, J. D. Courbon, B. Godinovic, N. Lelas, D. and Puljak, I. Ribeiro Cipriano, P. M. Sculac, T. Antunovic, Z. and Kovac, M. Brigljevic, V. Ferencek, D. Kadija, K. and Mesic, B. Starodumov, A. Susa, T. Ather, M. W. Attikis, A. Mavromanolakis, G. Mousa, J. Nicolaou, C. Ptochos, F. and Razis, P. A. Rykaczewski, H. Finger, M. Finger, Jr., M. and Carrera Jarrin, E. Assran, Y. Mahmoud, M. A. Mahrous, A. and Dewanjee, R. K. Kadastik, M. Perrini, L. Raidal, M. and Tiko, A. Veelken, C. Eerola, P. Pekkanen, J. and Voutilainen, M. Harkonen, J. Jarvinen, T. Karimaki, V. and Kinnunen, R. Lampen, T. Lassila-Perini, K. Lehti, S. and Linden, T. Luukka, P. Tuominen, E. Tuominiemi, J. and Tuovinen, E. Talvitie, J. Tuuva, T. Besancon, M. and Couderc, F. Dejardin, M. Denegri, D. Faure, J. L. Ferri, F. Ganjour, S. Ghosh, S. Givernaud, A. Gras, P. and Hamel de Monchenault, G. Jarry, P. Kucher, I. Locci, E. and Machet, M. Malcles, J. Negro, G. Rander, J. Rosowsky, A. and Sahin, M. O. Titov, M. Abdulsalam, A. Antropov, I. and Baffioni, S. Beaudette, F. Busson, P. Cadamuro, L. and Charlot, C. Granier de Cassagnac, R. Jo, M. Lisniak, S. and Lobanov, A. Martin Blanco, J. Nguyen, M. Ochando, C. and Ortona, G. Paganini, P. Pigard, P. Regnard, S. Salerno, R. Sauvan, J. B. Sirois, Y. Stahl Leiton, A. G. and Strebler, T. Yilmaz, Y. Zabi, A. Zghiche, A. Agram, J. -L. Andrea, J. Bloch, D. Brom, J. -M. Buttignol, M. and Chabert, E. C. Chanon, N. Collard, C. Conte, E. Coubez, X. Fontaine, J. -C. Gele, D. Goerlach, U. Jansova, M. and Le Bihan, A. -C. Tonon, N. Van Hove, P. Gadrat, S. and Beauceron, S. Bernet, C. Boudoul, G. Chierici, R. and Contardo, D. Depasse, P. El Mamouni, H. Fay, J. Finco, L. Gascon, S. Gouzevitch, M. Grenier, G. Ille, B. and Lagarde, F. Laktineh, I. B. Lethuillier, M. Mirabito, L. and Pequegnot, A. L. Perries, S. Popov, A. Sordini, V. and Vander Donckt, M. Viret, S. Toriashvili, T. Bagaturia, I. and Autermann, C. Beranek, S. Feld, L. Kiesel, M. K. and Klein, K. Lipinski, M. Preuten, M. Schomakers, C. and Schulz, J. Verlage, T. Zhukov, V. Albert, A. and Dietz-Laursonn, E. Duchardt, D. Endres, M. Erdmann, M. and Erdweg, S. Esch, T. Fischer, R. Guth, A. Hamer, M. and Hebbeker, T. Heidemann, C. Hoepfner, K. Knutzen, S. and Merschmeyer, M. Meyer, A. Millet, P. Mukherjee, S. and Olschewski, M. Padeken, K. Pook, T. Radziej, M. and Reithler, H. Rieger, M. Scheuch, F. Teyssier, D. Thuer, S. Flugge, G. Kargoll, B. Kress, T. Kunsken, A. and Lingemann, J. Muller, T. Nehrkorn, A. Nowack, A. and Pistone, C. Pooth, O. Stahl, A. Martin, M. Aldaya Arndt, T. Asawatangtrakuldee, C. Beernaert, K. Behnke, O. and Behrens, U. Bermudez Martinez, A. Bin Anuar, A. A. Borras, K. Botta, V. Campbell, A. Connor, P. Contreras-Campana, C. Costanza, F. Pardos, C. Diez Eckerlin, G. Eckstein, D. Eichhorn, T. Eren, E. Gallo, E. Garay Garcia, J. and Geiser, A. Gizhko, A. Grados Luyando, J. M. Grohsjean, A. and Gunnellini, P. Guthoff, M. Harb, A. Hauk, J. Hempel, M. Jung, H. Kalogeropoulos, A. Kasemann, M. Keaveney, J. and Kleinwort, C. Korol, I. Krucker, D. Lange, W. Lelek, A. Lenz, T. Leonard, J. Lipka, K. Lohmann, W. and Mankel, R. Melzer-Pellmann, I. -A. Meyer, A. B. Mittag, G. and Mnich, J. Mussgiller, A. Ntomari, E. Pitzl, D. and Raspereza, A. Roland, B. Savitskyi, M. Saxena, P. and Shevchenko, R. Spannagel, S. Stefaniuk, N. Van Onsem, G. P. and Walsh, R. Wen, Y. Wichmann, K. Wissing, C. Zenaiev, O. Bein, S. Blobel, V. Vignali, M. Centis Dreyer, T. and Garutti, E. Gonzalez, D. Haller, J. Hinzmann, A. and Hoffmann, M. Karavdina, A. Klanner, R. Kogler, R. and Kovalchuk, N. Kurz, S. Lapsien, T. Marchesini, I. and Marconi, D. Meyer, M. Niedziela, M. Nowatschin, D. and Pantaleo, F. Peiffer, T. Perieanu, A. Scharf, C. and Schleper, P. Schmidt, A. Schumann, S. Schwandt, J. and Sonneveld, J. Stadie, H. Steinbruck, G. Stober, F. M. and Stover, M. Tholen, H. Troendle, D. Usai, E. Vanelderen, L. Vanhoefer, A. Vormwald, B. Akbiyik, M. Barth, C. and Baur, S. Butz, E. Caspart, R. Chwalek, T. Colombo, F. and De Boer, W. Dierlamm, A. Freund, B. Friese, R. and Giffels, M. Gilbert, A. Haitz, D. Hartmann, F. Heindl, S. M. Husemann, U. Kassel, F. Kudella, S. Mildner, H. and Mozer, M. U. Muller, Th. Plagge, M. Quast, G. and Rabbertz, K. Schroder, M. Shvetsov, I. Sieber, G. and Simonis, H. J. Ulrich, R. Wayand, S. Weber, M. Weiler, T. Williamson, S. Wohrmann, C. Wolf, R. Anagnostou, G. and Daskalakis, G. Geralis, T. Giakoumopoulou, V. A. and Kyriakis, A. Loukas, D. Topsis-Giotis, I. Karathanasis, G. and Kesisoglou, S. Panagiotou, A. Saoulidou, N. Kousouris, K. Evangelou, I. Foudas, C. Kokkas, P. Mallios, S. and Manthos, N. Papadopoulos, I. Paradas, E. Strologas, J. and Triantis, F. A. Csanad, M. Filipovic, N. Pasztor, G. and Veres, G. I. Bencze, G. Hajdu, C. Horvath, D. Hunyadi, A. Sikler, F. Veszpremi, V. Zsigmond, A. J. Beni, N. and Czellar, S. Karancsi, J. Makovec, A. Molnar, J. and Szillasi, Z. Bartok, M. Raics, P. Trocsanyi, Z. L. and Ujvari, B. Choudhury, S. Komaragiri, J. R. Bahinipati, S. and Bhowmik, S. Mal, P. Mandal, K. Nayak, A. Sahoo, D. K. Sahoo, N. Swain, S. K. Bansal, S. Beri, S. B. and Bhatnagar, V. Chawla, R. Dhingra, N. Kalsi, A. K. Kaur, A. Kaur, M. Kumar, R. Kumari, P. Mehta, A. Singh, J. B. Walia, G. Bhardwaj, A. Chauhan, S. Choudhary, B. C. and Garg, R. B. Keshri, S. Kumar, A. Kumar, Ashok and Malhotra, S. Naimuddin, M. Ranjan, K. Shah, Aashaq and Sharma, R. Bhardwaj, R. Bhattacharya, R. Bhattacharya, S. and Bhawandeep, U. Dey, S. Dutt, S. Dutta, S. Ghosh, S. and Majumdar, N. Modak, A. Mondal, K. Mukhopadhyay, S. and Nandan, S. Purohit, A. Roy, A. Roy, D. Chowdhury, S. Roy and Sarkar, S. Sharan, M. Thakur, S. Behera, P. K. and Chudasama, R. Dutta, D. Jha, V. Kumar, V. Mohanty, A. K. and Netrakanti, P. K. Pant, L. M. Shukla, P. Topkar, A. and Aziz, T. Dugad, S. Mahakud, B. Mitra, S. Mohanty, G. B. and Sur, N. Sutar, B. Banerjee, S. Bhattacharya, S. and Chatterjee, S. Das, P. Guchait, M. Jain, Sa. Kumar, S. and Maity, M. Majumder, G. Mazumdar, K. Sarkar, T. and Wickramage, N. Chauhan, S. Dube, S. Hegde, V. Kapoor, A. and Kothekar, K. Pandey, S. Rane, A. Sharma, S. and Chenarani, S. Tadavani, E. Eskandari Etesami, S. M. Khakzad, M. Najafabadi, M. Mohammadi Naseri, M. Mehdiabadi, S. Paktinat Hosseinabadi, F. Rezaei Safarzadeh, B. Zeinali, M. and Felcini, M. Grunewald, M. Abbrescia, M. Calabria, C. and Colaleo, A. Creanza, D. Cristella, L. De Filippis, N. De Palma, M. Errico, F. Fiore, L. Iaselli, G. Lezki, S. and Maggi, G. Maggi, M. Miniello, G. My, S. Nuzzo, S. and Pompili, A. Pugliese, G. Radogna, R. Ranieri, A. and Selvaggi, G. Sharma, A. Silvestris, L. Venditti, R. and Verwilligen, P. Abbiendi, G. Battilana, C. Bonacorsi, D. and Braibant-Giacomelli, S. Campanini, R. Capiluppi, P. Castro, A. Cavallo, F. R. Chhibra, S. S. Codispoti, G. Cuffiani, M. Dallavalle, G. M. Fabbri, F. Fanfani, A. Fasanella, D. Giacomelli, P. Grandi, C. Guiducci, L. Marcellini, S. and Masetti, G. Montanari, A. Navarria, F. L. Perrotta, A. and Rossi, A. M. Rovelli, T. Siroli, G. P. Tosi, N. and Albergo, S. 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C. Abercrombie, D. Allen, B. and Azzolini, V. Barbieri, R. Baty, A. Bi, R. Brandt, S. and Busza, W. Cali, I. A. D'Alfonso, M. Demiragli, Z. and Ceballos, G. Gomez Goncharov, M. Hsu, D. Iiyama, Y. and Innocenti, G. M. Klute, M. Kovalskyi, D. Lai, Y. S. Lee, Y. -J. Levin, A. Luckey, P. D. Maier, B. Marini, A. C. and Mcginn, C. Mironov, C. Narayanan, S. Niu, X. Paus, C. Roland, C. Roland, G. Salfeld-Nebgen, J. Stephans, G. S. F. Tatar, K. Velicanu, D. Wang, J. Wang, T. W. and Wyslouch, B. Benvenuti, A. C. Chatterjee, R. M. Evans, A. and Hansen, P. Kalafut, S. Kubota, Y. Lesko, Z. Mans, J. and Nourbakhsh, S. Ruckstuhl, N. Rusack, R. Turkewitz, J. and Acosta, J. G. Oliveros, S. Avdeeva, E. Bloom, K. and Claes, D. R. Fangmeier, C. Suarez, R. Gonzalez Kamalieddin, R. Kravchenko, I. Monroy, J. Siado, J. E. Snow, G. R. and Stieger, B. Alyari, M. Dolen, J. Godshalk, A. and Harrington, C. Iashvili, I. Nguyen, D. Parker, A. and Rappoccio, S. Roozbahani, B. Alverson, G. Barberis, E. and Hortiangtham, A. Massironi, A. Morse, D. M. Nash, D. and Orimoto, T. De Lima, R. Teixeira Trocino, D. Wood, D. and Bhattacharya, S. Charaf, O. Hahn, K. A. Mucia, N. Odell, N. Pollack, B. Schmitt, M. H. Sung, K. Trovato, M. and Velasco, M. Dev, N. Hildreth, M. Anampa, K. Hurtado and Jessop, C. Karmgard, D. J. Kellams, N. Lannon, K. and Loukas, N. Marinelli, N. Meng, F. Mueller, C. Musienko, Y. Planer, M. Reinsvold, A. Ruchti, R. Smith, G. and Taroni, S. Wayne, M. Wolf, M. Woodard, A. Alimena, J. and Antonelli, L. Bylsma, B. Durkin, L. S. Flowers, S. and Francis, B. Hart, A. Hill, C. Ji, W. Liu, B. Luo, W. and Puigh, D. Winer, B. L. Wulsin, H. W. Cooperstein, S. and Driga, O. Elmer, P. Hardenbrook, J. Hebda, P. and Higginbotham, S. Lange, D. Luo, J. Marlow, D. Mei, K. and Ojalvo, I. Olsen, J. Palmer, C. Piroue, P. and Stickland, D. Tully, C. Malik, S. Norberg, S. Barker, A. and Barnes, V. E. Das, S. Folgueras, S. Gutay, L. Jha, M. K. Jones, M. Jung, A. W. Khatiwada, A. Miller, D. H. and Neumeister, N. Peng, C. C. Schulte, J. F. Sun, J. and Wang, F. Xie, W. Cheng, T. Parashar, N. Stupak, J. and Adair, A. Akgun, B. Chen, Z. Ecklund, K. M. Geurts, F. J. M. Guilbaud, M. Li, W. Michlin, B. Northup, M. and Padley, B. P. Park, S. E. Roberts, J. Rorie, J. Tu, Z. and Zabel, J. Bodek, A. De Barbaro, P. Demina, R. Duh, Y. T. Ferbel, T. Galanti, M. Garcia-Bellido, A. Han, J. and Hindrichs, O. Khukhunaishvili, A. Lo, K. H. Tan, P. and Verzetti, M. Ciesielski, R. Goulianos, K. Mesropian, C. and Agapitos, A. Chou, J. P. Gershtein, Y. Espinosa, T. A. Gomez and Halkiadakis, E. Heindl, M. Hughes, E. Kaplan, S. and Elayavalli, R. Kunnawalkam Kyriacou, S. Lath, A. Montalvo, R. Nash, K. Osherson, M. Saka, H. Salur, S. and Schnetzer, S. Sheffield, D. Somalwar, S. Stone, R. and Thomas, S. Thomassen, P. Walker, M. Delannoy, A. G. and Foerster, M. Heideman, J. Riley, G. Rose, K. Spanier, S. and Thapa, K. Bouhali, O. Hernandez, A. Castaneda Celik, A. and Dalchenko, M. De Mattia, M. Delgado, A. Dildick, S. and Eusebi, R. Gilmore, J. Huang, T. Kamon, T. Mueller, R. and Pakhotin, Y. Patel, R. Perloff, A. Pernie, L. and Rathjens, D. Safonov, A. Tatarinov, A. Ulmer, K. A. and Akchurin, N. Damgov, J. De Guio, F. Dudero, P. R. and Faulkner, J. Gurpinar, E. Kunori, S. Lamichhane, K. Lee, S. W. Libeiro, T. Peltola, T. Undleeb, S. Volobouev, I. and Wang, Z. Greene, S. Gurrola, A. Janjam, R. Johns, W. and Maguire, C. Melo, A. Ni, H. Sheldon, P. Tuo, S. and Velkovska, J. Xu, Q. Arenton, M. W. Barria, P. Cox, B. and Hirosky, R. Joyce, M. Ledovskoy, A. Li, H. Neu, C. and Sinthuprasith, T. Wang, Y. Wolfe, E. Xia, F. Harr, R. Karchin, P. E. Sturdy, J. Zaleski, S. Brodski, M. and Buchanan, J. Caillol, C. Dasu, S. Dodd, L. Duric, S. and Gomber, B. Grothe, M. Herndon, M. Herve, A. Hussain, U. and Klabbers, P. Lanaro, A. Levine, A. Long, K. and Loveless, R. Pierro, G. A. Polese, G. Ruggles, T. Savin, A. Smith, N. Smith, W. H. Taylor, D. Woods, N. CMS Collaboration

Subjects
Physics::Instrumentation and Detectors, Nuclear Experiment
Abstract

Charge-dependent anisotropy Fourier coefficients (v(n)) of particle azimuthal distributions are measured in pPb and PbPb collisions at root S-NN = 5.02 TeV with the CMS detector at the LHC. The normalized difference in the second-order anisotropy coefficients (v(2)) between positively and negatively charged particles is found to depend linearly on the observed event charge asymmetry with comparable slopes for both pPb and PbPb collisions over a wide range of charged particle multiplicity. In PbPb, the third-order anisotropy coefficient v(3) shows a similar linear dependence with the same slope as seen for v(2). The observed similarities between the v(2) slopes for pPb and PbPb, as well as the similar slopes for v(2) and v(3) in PbPb, are compatible with expectations based on local charge conservation in the decay of clusters or resonances, and constitute a challenge to the hypothesis that, at LHC energies, the observed charge asymmetry dependence of v(2) in heavy ion collisions arises from a chiral magnetic wave.

Published
2019

45. Contributions of biodiversity to the sustainable intensification of food production:Thematic study for The State of the World’s Biodiversity for Food and Agriculture

Author

Dawson, I.K., Attwood, S. J., Park, S. E., Jamnadass, R., Powell, W., Sunderland, T., Kindt, R., McMullin, S., Hoebe, P.N., Baddeley, J., Staver, C., Vadez, V., Carsan, S., Roshetko, J. M., Amri, A., Karamura, E., Karamura, D., Breugel, P. van, Hossain, E, Phillips, M., Kumar, A., Lillesø, Jens-Peter Barnekow, Benzie, J., Sebastian, G.E., Ekesa, B., Ocimati, W., and Graudal, Lars

Published
2019

49. Evaluation of Tanzania local ceramic raw materials for high voltage porcelain insulators production

Author

Ngayakamo, B. and Park, S. E.

Subjects
isolador de porcelana, vermiculite, porcelain insulator, vermiculita, physical-mechanical properties, dielectric strength, propriedades físico-mecânicas, rigidez dielétrica
Abstract

This study evaluated the potential of locally sourced-ceramic raw materials in Tanzania, Pugu kaolin, Same clay, vermiculite and feldspar, for production of high voltage porcelain insulators. The chemical, mineral phases and microstructural characterization of raw materials and porcelain samples were carried out using the X-ray fluorescence, X-ray diffraction, and scanning electron microscopy techniques, respectively. The mineral phases of the fired porcelain sample identified were mullite and quartz. The porcelain bodies were fabricated using the dry pressing method by varying the composition of the selected ceramic raw materials. The physical-mechanical properties and dielectric strength were measured for each porcelain sample. The sample with the composition of 20% Pugu kaolin, 20% Same clay, 20% vermiculite and 40% feldspar was found to have the dielectric strength of 50.8 kV.mm-1, bending strength of 20 MPa and water absorption of 0.46%, which satisfies the main requisite properties for high voltage porcelain insulators. Resumo Este estudo avaliou o potencial de matérias-primas cerâmicas de origem local na Tanzânia, caulim Pugu, argila Same, vermiculita e feldspato, para a produção de isoladores de porcelana de alta tensão. As caracterizações química, de fases minerais e microestrutural das matérias-primas e amostras de porcelana foram realizadas utilizando as técnicas de fluorescência de raios X, difração de raios X e microscopia eletrônica de varredura, respectivamente. As fases minerais da amostra de porcelana queimada identificadas foram mulita e quartzo. Os corpos de porcelana foram fabricados utilizando o método de prensagem a seco, variando a composição das matérias-primas cerâmicas selecionadas. As propriedades físico-mecânicas e a rigidez dielétrica foram medidas para cada amostra de porcelana. A amostra com composição de 20% de caulim Pugu, 20% de argila Same, 20% de vermiculita e 40% de feldspato apresentou rigidez dielétrica de 50,8 kV.mm-1, resistência à flexão de 20 MPa e absorção de água de 0,46%, que satisfazem as principais propriedades necessárias para isoladores de porcelana de alta tensão.

Published
2018

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