Search for s channel single top quark production in pp collisions at s=7 and 8 TeV
Journal of High Energy Physics Springer Nature 2016:9 (2016) 27
Authors:
The CMS collaboration, V Khachatryan, AM Sirunyan, A Tumasyan, W Adam, E Asilar, T Bergauer, J Brandstetter, E Brondolin, M Dragicevic, J Erö, M Flechl, M Friedl, R Frühwirth, VM Ghete, C Hartl, N Hörmann, J Hrubec, M Jeitler, V Knünz, A König, M Krammer, I Krätschmer, D Liko, T Matsushita, I Mikulec, D Rabady, N Rad, B Rahbaran, H Rohringer, J Schieck, R Schöfbeck, J Strauss, W Treberer-Treberspurg, W Waltenberger, C-E Wulz, V Mossolov, N Shumeiko, J Suarez Gonzalez, S Alderweireldt, T Cornelis, EA De Wolf, X Janssen, A Knutsson, J Lauwers, S Luyckx, M Van De Klundert, H Van Haevermaet, P Van Mechelen, N Van Remortel, A Van Spilbeeck, S Abu Zeid, F Blekman, J D’Hondt, N Daci, I De Bruyn, K Deroover, N Heracleous, J Keaveney, S Lowette, L Moreels, A Olbrechts, Q Python, D Strom, S Tavernier, W Van Doninck, P Van Mulders, GP Van Onsem, I Van Parijs, P Barria, H Brun, C Caillol, B Clerbaux, G De Lentdecker, W Fang, G Fasanella, L Favart, R Goldouzian, A Grebenyuk, G Karapostoli, T Lenzi, A Léonard, T Maerschalk, A Marinov, L Perniè, A Randle-conde, T Seva, C Vander Velde, P Vanlaer, R Yonamine, F Zenoni, F Zhang, K Beernaert, L Benucci, A Cimmino, S Crucy, D Dobur, A Fagot, G Garcia, M Gul, J Mccartin, AA Ocampo Rios, D Poyraz, D Ryckbosch, S Salva, M Sigamani, M Tytgat, W Van Driessche, E Yazgan, N Zaganidis, S Basegmez, C Beluffi, O Bondu, S Brochet, G Bruno, A Caudron, L Ceard, C Delaere, D Favart, L Forthomme, A Giammanco, A Jafari, P Jez, M Komm, V Lemaitre, A Mertens, M Musich, C Nuttens, L Perrini, K Piotrzkowski, A Popov, L Quertenmont, M Selvaggi, M Vidal Marono, N Beliy, GH Hammad, WL Aldá Júnior, FL Alves, GA Alves, L Brito, M Correa Martins Junior, M Hamer, C Hensel, A Moraes, ME Pol, P Rebello Teles, E Belchior Batista Das Chagas, W Carvalho, J Chinellato, A Custódio, EM Da Costa, D De Jesus Damiao, C De Oliveira Martins, S Fonseca De Souza, LM Huertas Guativa, H Malbouisson, D Matos Figueiredo, C Mora Herrera, L Mundim, H Nogima, WL Prado Da Silva, A Santoro, A Sznajder, EJ Tonelli Manganote, A Vilela Pereira, S Ahuja, CA Bernardes, A De Souza Santos, S Dogra, TR Fernandez Perez Tomei, EM Gregores, PG Mercadante, CS Moon, SF Novaes, Sandra S Padula, D Romero Abad, JC Ruiz Vargas, A Aleksandrov, R Hadjiiska, P Iaydjiev, M Rodozov, S Stoykova, G Sultanov, M Vutova, A Dimitrov, I Glushkov, L Litov, B Pavlov, P Petkov, M Ahmad, JG Bian, GM Chen, HS Chen, M Chen, T Cheng, R Du, CH Jiang, D Leggat, R Plestina, F Romeo, SM Shaheen, A Spiezia, J Tao, C Wang, Z Wang, H Zhang, C Asawatangtrakuldee, Y Ban, Q Li, S Liu, Y Mao, SJ Qian, D Wang, Z Xu, C Avila, A Cabrera, LF Chaparro Sierra, C Florez, JP Gomez, B Gomez Moreno, JC Sanabria, N Godinovic, D Lelas, I Puljak, PM Ribeiro Cipriano, Z Antunovic, M Kovac, V Brigljevic, K Kadija, J Luetic, S Micanovic, L Sudic, A Attikis, G Mavromanolakis, J Mousa, C Nicolaou, F Ptochos, PA Razis, H Rykaczewski, M Bodlak, M Finger, M Finger, E El-khateeb, T Elkafrawy, A Mohamed, E Salama, B Calpas, M 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TeV with the ATLAS detector
Journal of High Energy Physics Springer Nature 2016:9 (2016) 173
Authors:
The ATLAS collaboration, M Aaboud, G Aad, B Abbott, J Abdallah, O Abdinov, B Abeloos, R Aben, OS AbouZeid, NL Abraham, H Abramowicz, H Abreu, R Abreu, Y Abulaiti, BS Acharya, L Adamczyk, DL Adams, J Adelman, S Adomeit, T Adye, AA Affolder, T Agatonovic-Jovin, J Agricola, JA Aguilar-Saavedra, SP Ahlen, F Ahmadov, G Aielli, H Akerstedt, TPA Åkesson, AV Akimov, GL Alberghi, J Albert, S Albrand, MJ Alconada Verzini, M Aleksa, IN Aleksandrov, C Alexa, G Alexander, T Alexopoulos, M Alhroob, B Ali, M Aliev, G Alimonti, J Alison, SP Alkire, BMM Allbrooke, BW Allen, PP Allport, A Aloisio, A Alonso, F Alonso, C Alpigiani, M Alstaty, B Alvarez Gonzalez, D Álvarez Piqueras, MG Alviggi, BT Amadio, K Amako, Y Amaral Coutinho, C Amelung, D Amidei, SP Amor Dos Santos, A Amorim, S Amoroso, G Amundsen, C Anastopoulos, LS Ancu, N Andari, T Andeen, CF Anders, G Anders, JK Anders, KJ Anderson, A Andreazza, V Andrei, S Angelidakis, I Angelozzi, P Anger, A Angerami, F Anghinolfi, AV Anisenkov, N Anjos, A 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Wozniak, M Wu, M Wu, SL Wu, X Wu, Y Wu, TR Wyatt, BM Wynne, S Xella, Z Xi, D Xu, L Xu, B Yabsley, S Yacoob, D Yamaguchi, Y Yamaguchi, A Yamamoto, S Yamamoto, T Yamanaka, K Yamauchi, Y Yamazaki, Z Yan, H Yang, H Yang, Y Yang, Z Yang, W-M Yao, YC Yap, Y Yasu, E Yatsenko, KH Yau Wong, J Ye, S Ye, I Yeletskikh, AL Yen, E Yildirim, K Yorita, R Yoshida, K Yoshihara, C Young, CJS Young, S Youssef, DR Yu, J Yu, JM Yu, J Yu, L Yuan, SPY Yuen, I Yusuff, B Zabinski, R Zaidan, AM Zaitsev, N Zakharchuk, J Zalieckas, A Zaman, S Zambito, L Zanello, D Zanzi, C Zeitnitz, M Zeman, A Zemla, JC Zeng, Q Zeng, K Zengel, O Zenin, T Ženiš, D Zerwas, D Zhang, F Zhang, G Zhang, H Zhang, J Zhang, L Zhang, R Zhang, R Zhang, X Zhang, Z Zhang, X Zhao, Y Zhao, Z Zhao, A Zhemchugov, J Zhong, B Zhou, C Zhou, L Zhou, L Zhou, M Zhou, N Zhou, CG Zhu, H Zhu, J Zhu, Y Zhu, X Zhuang, K Zhukov, A Zibell, D Zieminska, NI Zimine, C Zimmermann, S Zimmermann, Z Zinonos, M Zinser, M Ziolkowski, L Živković, G Zobernig, A Zoccoli, M zur Nedden, L ZwalinskiBaryonic acoustic oscillations from 21cm intensity mapping: the Square Kilometre Array case
(2016)
Authors:
Francisco Villaescusa-Navarro, David Alonso, Matteo VielSearch for high-mass new phenomena in the dilepton final state using proton–proton collisions at √s = 13 TeV with the ATLAS detector
Physics Letters B Elsevier 761 (2016) 372-392
Authors:
G Amundsen, C Anastopoulos, LS Ancu, N Andari, T Andeen, CF Anders, G Anders, P Anger, A Angerami, N Anjos, A Annovi, M Antonelli, F Anulli, L Aperio Bella, JP Araque, J-F Arguin, AJ Armbruster, O Arnaez, H Arnold, A Artamonov, K Assamagan, R Astalos, M Atkinson, NB Atlay, K AugstenAbstract:
© 2016 The Author A search is conducted for both resonant and non-resonant high-mass new phenomena in dielectron and dimuon final states. The search uses 3.2fb−1 of proton–proton collision data, collected at √s=13TeV by the ATLAS experiment at the LHC in 2015. The dilepton invariant mass is used as the discriminating variable. No significant deviation from the Standard Model prediction is observed; therefore limits are set on the signal model parameters of interest at 95% credibility level. Upper limits are set on the cross-section times branching ratio for resonances decaying to dileptons, and the limits are converted into lower limits on the resonance mass, ranging between 2.74 TeV and 3.36 TeV, depending on the model. Lower limits on the ℓℓqq contact interaction scale are set between 16.7 TeV and 25.2 TeV, also depending on the model.Evidence for magnetic field compression in shocks within the jet of V404 Cyg
Monthly Notices of the Royal Astronomical Society Oxford University Press 463:2 (2016) 1822-1830
Authors:
T Shahbaz, DM Russell, S Covino, Kunal Mooley, Robert Fender, C RumseyAbstract:
We present optical and near-IR linear polarimetry of V404 Cyg during its 2015 outburst and in quiescence. We obtained time-resolved r΄-band polarimetry when the source was in outburst, near-IR polarimetry when the source was near quiescence and multiple waveband optical polarimetry later in quiescence. The optical-to-near-IR linear polarization spectrum can be described by interstellar dust and an intrinsic variable component. The intrinsic optical polarization, detected during the rise of one of the brightest flares of the outburst, is variable, peaking at 4.5 per cent and decaying to 3.5 per cent. We present several arguments that favour a synchrotron jet origin to this variable polarization, with the optical emission originating close to the jet base. The polarization flare occurs during the initial rise of a major radio flare event that peaks later, and is consistent with a classically evolving synchrotron flare from an ejection event. We conclude that the optical polarization flare represents a jet launching event, the birth of a major ejection. For this event, we measure a rather stable polarization position angle of −9° E of N, implying that the magnetic field near the base of the jet is approximately perpendicular to the jet axis. This may be due to the compression of magnetic field lines in shocks in the accelerated plasma, resulting in a partially ordered transverse field that have now been seen during the 2015 outburst. We also find that this ejection occurred at a similar stage in the repetitive cycles of flares.