Institution
Tata Institute of Fundamental Research
Education•Mumbai, Maharashtra, India•
About: Tata Institute of Fundamental Research is a education organization based out in Mumbai, Maharashtra, India. It is known for research contribution in the topics: Magnetization & Large Hadron Collider. The organization has 7786 authors who have published 21742 publications receiving 622368 citations. The organization is also known as: TIFR.
Topics: Magnetization, Large Hadron Collider, Galaxy, Higgs boson, Lepton
Papers published on a yearly basis
Papers
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TL;DR: In this article, the authors acknowledge the enduring support for the construction and operation of the LHC and the CMS detector provided by the following funding agencies: BMWFW and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MOST, and NSFC (China); COLCIEN-CIAS (Colombia); DAE and DST (India); IPM (Iran);
156 citations
TL;DR: In this article, the authors studied Z 2 -orbifolds of 11-dimensional M-theory on tori of various dimensions and showed that the resulting six-dimensional theory is equivalent to the type IIB string compactified on K3.
156 citations
S. Chatrchyan1, Vardan Khachatryan1, Albert M. Sirunyan1, Armen Tumasyan1 +3893 more•Institutions (138)
TL;DR: In this article, a doubly-charged Higgs boson search was performed using events with three or more isolated charged leptons of any flavor, giving sensitivity to the decays of pair-produced triplet components.
Abstract: A search for a doubly-charged Higgs boson in pp collisions at root s = 7 TeV is presented. The data correspond to an integrated luminosity of 4.9 fb(-1), collected by the CMS experiment at the LHC. The search is performed using events with three or more isolated charged leptons of any flavor, giving sensitivity to the decays of pair-produced triplet components Phi(++)Phi(--), and Phi(++)Phi(-) from associated production. No excess is observed compared to the background prediction, and upper limits at the 95 % confidence level are set on the Phi(++) production cross section, under specific assumptions on its branching fractions. Lower bounds on the Phi(++) mass are reported, providing significantly more stringent constraints than previously published limits.
156 citations
University of Tokyo1, Budker Institute of Nuclear Physics2, École Polytechnique Fédérale de Lausanne3, Tata Institute of Fundamental Research4, University of Sydney5, University of Melbourne6, Panjab University, Chandigarh7, Polish Academy of Sciences8, University of Maribor9, National Taiwan University10, National Central University11, Hanyang University12, Sungkyunkwan University13, Virginia Tech14, University of Cincinnati15, University of Ljubljana16, Korea University17, Nagoya University18, Osaka University19, Tohoku Gakuin University20, Kyungpook National University21, Saga University22, Tokyo Institute of Technology23, Yonsei University24, Chiba University25, Niigata University26, Graduate University for Advanced Studies27, University of Giessen28, Seoul National University29, Austrian Academy of Sciences30, Osaka City University31, Tokyo University of Agriculture and Technology32, Nara Women's University33, Toho University34, Kanagawa University35, University of Illinois at Urbana–Champaign36, University of Nova Gorica37, Tokyo Metropolitan University38, National United University39, University of Science and Technology of China40
TL;DR: In this article, the processes e+e-→J/ψD(*)D*D* were studied and a new charmonium-like state X(4160) was observed.
Abstract: We report a study of the processes e+e-→J/ψD(*)D(*). In J/ψD*D* we observe a significant enhancement in the D*D* invariant mass spectrum, which we interpret as a new charmoniumlike state and denote X(4160). The X(4160) parameters are M=(4156-20+25±15)MeV/c2 and Γ=(139-61+111±21)MeV. We also report a new measurement of the X(3940) mass and width: M=(3942-6+7±6) MeV/c2 and Γ=(37-15+26±8)MeV. The analysis is based on a 693fb-1 data sample recorded near the Υ(4S) resonance by the Belle detector at the KEKB asymmetric-energy collider. © 2008 The American Physical Society.
156 citations
12 Oct 2012
TL;DR: In this paper, the authors compared the fragmentation functions in pp and PbPb collisions at a centre-of-mass energy of 2.76 TeV per nucleon pair using data collected with the CMS detector at the LHC.
Abstract: Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of 2.76 TeV per nucleon pair was studied using data collected with the CMS detector at the LHC. Fragmentation functions are constructed using charged-particle tracks with transverse momenta pt > 4 GeV for dijet events with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events are compared to those in pp data as a function of collision centrality, as well as dijet-pt imbalance. Special emphasis is placed on the most central PbPb events including dijets with unbalanced momentum, indicative of energy loss of the hard scattered parent partons. The fragmentation patterns for both the leading and subleading jets in PbPb collisions agree with those seen in pp data at 2.76 TeV. The results provide evidence that, despite the large parton energy loss observed in PbPb collisions, the high-pt component of the fragmentation function evaluated with respect to the reconstructed jet momentum is not strongly modified in comparison to jet fragmentation in vacuum.
156 citations
Authors
Showing all 7857 results
| Name | H-index | Papers | Citations |
|---|---|---|---|
| Pulickel M. Ajayan | 176 | 1223 | 136241 |
| Suvadeep Bose | 154 | 960 | 129071 |
| Subir Sarkar | 149 | 1542 | 144614 |
| Sw. Banerjee | 146 | 1906 | 124364 |
| Dipanwita Dutta | 143 | 1651 | 103866 |
| Ajit Kumar Mohanty | 141 | 1124 | 93062 |
| Tariq Aziz | 138 | 1646 | 96586 |
| Andrew Mehta | 137 | 1444 | 101810 |
| Suchandra Dutta | 134 | 1265 | 87709 |
| Kajari Mazumdar | 134 | 1295 | 94253 |
| Bobby Samir Acharya | 133 | 1121 | 100545 |
| Gobinda Majumder | 133 | 1523 | 87732 |
| Eric Conte | 132 | 1206 | 84593 |
| Prashant Shukla | 131 | 1341 | 85287 |
| Alessandro Montanari | 131 | 1387 | 93071 |