參考文獻 |
[1] Observation of a new boson at a mass of 125 gev with the cms experiment at the lhc. Physics Letters B, 716(1):30 – 61, 2012.
[2] Observation of a new boson at a mass of 125 gev with the cms experiment at the lhc. Physics Letters B, 716(1):30 – 61, 2012.
[3] Observation of a new particle in the search for the standard model higgs boson with the atlas detector at the lhc. Physics Letters B, 716(1):1 – 29, 2012.
[4] Observation of a new particle in the search for the standard model higgs boson with the atlas detector at the lhc. Physics Letters B, 716(1):1 – 29, 2012.
[5] Higgs boson decays to γγ and zγ in models with higgs extensions. Phys. Rev. D, 87:033003, Feb 2013.
[6] CMS Luminosity Measurements for the 2016 Data Taking Period. 3 2017.
[7] Particle-flow reconstruction and global event description with the CMS detector. Particle-flow reconstruction and global event description with the CMS detector. JINST, 12(CMS-PRF-14-001. CMS-PRF-14-001-004. 10):P10003. 82 p, Jun 2017. Replaced with the published ver- sion. Added the journal reference and DOI. All the figures and ta- bles can be found at http://cms-results.web.cern.ch/cms-results/public- results/publications/PRF-14-001 (CMS Public Pages).
√s =13 TeV. [9] Observation of higgs boson decay to bottom quarks. Phys. Rev. Lett.,
[8] CMS luminosity measurement for the 2017 data-taking period at 6 2018.
121:121801, Sep 2018.
[10] Observation of hdecays and vh production with the atlas detector. Physics
Letters B, 786:59 – 86, 2018.
[11] Observation of the higgs boson decay to a pair of τ leptons with the cms
detector. Physics Letters B, 779:283 – 316, 2018.
[12] CMS luminosity measurement for the 2018 data-taking period at s 13 TeV. 5 2019.
[13] Georges Aad et al. Observation of an new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC. Phys. Lett. B, 716:1– 29, 2012.
[14] Georges Aad et al. Search for Higgs boson decays to a photon and a Z boson
in pp collisions at 732:8–27, 2014.
s=7 and 8 TeV with the ATLAS detector. Phys. Lett. B,
cross sections in pp collisions at 10:132, 2011.
√
[15] Claude Amsler, V Chiochia, S. Visscher, and Ryszard Romaniuk. Calibration of the cms drift tube chambers and measurement of the drift velocity with cosmic rays. Journal of Instrumentation, 5:t03016, 03 2010.
[16] L. Bergström and G. Hulth. Induced higgs couplings to neutral bosons in e+e collisions. Nuclear Physics B, 259(1):137 – 155, 1985.
[17] R.N. Cahn, M.S. Chanowitz, and N. Fleishon. Higgs particle production by h → zγ. Physics Letters B, 82(1):113 – 116, 1979.
[18] Marcela Carena, Ian Low,and Carlos E.M.Wagner. Implications of a Modified Higgs to Diphoton Decay Width. JHEP, 08:060, 2012.
[19] Serguei Chatrchyan et al. Measurement of the inclusive W and Z production
s = 7 TeV with the CMS experiment. JHEP,
[20] Serguei Chatrchyan et al. Observation of a new boson at a mass of 125 GeV
with the CMS experiment at the LHC. Phys. Lett. B, 716:30–61, 2012.
[21] Chian-Shu Chen, Chao-Qiang Geng, Da Huang, and Lu-Hsing Tsai. New
scalar contributions to h → zγ. Phys. Rev. D, 87:075019, Apr 2013.
[22] Mingshui Chen and et al. Higgs measurements in the h to zz to 4l channel
using kinematic fitting technique. CMS Analysis Note, 15/286, 2015.
[23] Yi Chen, Adam Falkowski, Ian Low, and Roberto Vega-Morales. New Observ-
ables for CP Violation in Higgs Decays. Phys. Rev. D, 90(11):113006, 2014.
[24] CMS Collaboration. Cms an-2019/149 – common tools for analyses of higgs
boson decay in the diphoton final state.
[25] CMS Collaboration. Search for a higgs boson decaying into a z boson and a √s = 7 and 8 tev. Phys. Lett. B, 726:587−−609, 2013.
[26] CMSCollaboration. Higgs to 4 leptons with 13 tev with full 2016 dataset.CMS
photon in pp collisions at
Analysis Note, CMS-AN2016-442, 2016.
[27] CMS Collaboration. Search for the decay of a higgs boson in the γ channel in proton-proton collisions at √s= 13 tev. JHEP, 11:152, 2018.
[28] ATLAS Collaboration. Evidence for the higgs-boson yukawa coupling to tau leptons with the atlas detector. 01 2015.
[29] Atlas Collaboration. Searches for the zγ decay mode of the higgs boson and √
s = 13 tev with the atlas detector. Journal of High Energy Physics, 2017(10):112, Oct 2017.
for new high-mass resonances in pp collisions at
[30] CMS Collaboration. Performance of electron reconstruction and selection with the cms detector in proton-proton collisions at sqrt(s) = 8 tev. JINST, 2015.
[31] The CMS collaboration. Measurements of properties of the higgs boson decaying into the four-lepton final state in pp collisions at sqrts=13 tev. J. High Energ. Phys, 2017.
[32] Emlyn Corrin. Development of digital readout electronics for the cms tracker. 04 2003.
[33] P.D.Dauncey, M.Kenzie, N.Wardle, and G.J.Davies. Handling uncertainties in background shapes: the discrete profiling method. Journal of Instrumentation, 10(04):P04015–P04015, apr 2015.
[34] Sally Dawson and Pier Paolo Giardino. Higgs decays to ZZ and Zγ in the standard model effective field theory: An NLO analysis. Phys. Rev. D, 97(9):093003, 2018.
[35] D. de Florian et al. Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector. 2/2017, 10 2016.
[36] A. Dedes, K. Suxho, and L. Trifyllis. The decay h → Zγ in the Standard-Model Effective Field Theory. JHEP, 06:115, 2019.
[37] John Ellis. Higgs Physics. (KCL-PH-TH-2013-49. KCL-PH-TH-2013-49. LCTS- 2013-36. CERN-PH-TH-2013-315):117–168. 52 p, Dec 2013. 52 pages, 45 figures, Lectures presented at the ESHEP 2013 School of High-Energy Physics, to appear as part of the proceedings in a CERN Yellow Report.
[38] F. Englert and R. Brout. Broken symmetry and the mass of gauge vector mesons. Phys. Rev. Lett., 13:321–323, Aug 1964.
[39] K. Ackersta et al. Search for anomalous production of dilepton events with missing transverse momentum in e+eicollisions at sqrts= 161 gev and 172 gev. Eur. Phys. J. C, 1998.
[40] James S. Gainer, Wai-Yee Keung, Ian Low, and Pedro Schwaller. Looking for a light higgs boson in the overlooked channel. JHEP, 2011.
[41] James S.Gainer, KunalKumar, Ian Low,and RobertoVega-Morales.Improving the sensitivity of higgs boson searches in the golden channel. JHEP, 2011.
[42] Rebeca Gonzalez Suarez. Recent CMS results and Higgs physics. Mod. Phys. Lett. A, 32(arXiv:1707.05054. 29):1730026. 15 p, Jul 2017. Updated version of the Wine Cheese: Joint Experimental-Theoretical Physics Seminar ’Recent CMS results in top and Higgs physics’ given at Fermilab, 20 November 2015. To appear in Mod. Phys. Lett. A.
[43] LHC Higgs Cross Section Working Group, S. Dittmaier, C. Mariotti, G. Pas- sarino, and R. Tanaka (Eds.). Handbook of LHC Higgs Cross Sections: 1. Inclusive Observables. CERN-2011-002, CERN, Geneva, 2011.
[44] G.S.Guralnik, C.R.Hagen, and T.W.B.Kibble. Global conservation law sand massless particles. Phys. Rev. Lett., 13:585–587, Nov 1964.
[45] J Hauser, D Acosta, E Boyd, B Bylsma, Rick Cousins, Alexey Drozdetskiy, S Durkin, J Gilmore, Jiji Gu, S Haapanen, A Korytov, Shulin Lee, T Ling, A Madorsky, Misha Matveev, M Mey, Brian Mohr, J Mumford, Paul Padley, and Yuke Zheng. Experience with trigger electronics for the csc system of cms. 01 2004.
[46] Peter W. Higgs. Broken symmetries and the masses of gauge bosons. Phys. Rev. Lett., 13:508–509, Oct 1964.
[47] Peter W. Higgs. Broken symmetries, massless particles and gauge fields. Phys. Lett., 12:132–133, 1964.
[48] Jennifer Jentzsch. Pixel detector modules performance for ATLAS IBL and future pixel detectors. PhD thesis, Tech. U., Dortmund (main), 3 2015.
[49] Thomas Junk. Confidence level computation for combining searches with small statistics. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 434(2):435 – 443, 1999.
[50] Vardan Khachatryan et al. The CMS trigger system. JINST, 12(01):P01020, 2017.
[51] Alexander Yu. Korchin and Vladimir A. Kovalchuk. Polarization effects in the Higgs boson decay to γZ and test of CP and CPT symmetries. Phys. Rev. D, 88(3):036009, 2013.
[52] A. Koutoulaki. The itk strip tracker for the phase-ii upgrade of the atlas detector of the hl-lhc. Journal of Instrumentation, 12:C04022–C04022, 04 2017.
[53] Ian Low, Joseph Lykken, and Gabe Shaughnessy. Singlet scalars as higgs boson imposters at the large hadron collider. Phys. Rev. D, 84:035027, Aug 2011.
[54] Badder Marzocchi. Simulation of the cms electromagnetic calorimeter re- sponse at the energy and intensity frontier. Journal of Physics: Conference Series, 1162:012007, 01 2019.
[55] Esma Mobs. The CERN accelerator complex - August 2018. Complexe des accélérateurs du CERN - Août 2018. Aug 2018. General Photo.
[56] Jorge Molina, CMS Warsaw, Krzysztof Pozniak, Ryszard Romaniuk, and Wo- jciech Zabolotny. Performance of cms hadron calorimeter timing. Journal of Instrumentation, 5:T03013, 03 2010.
[57] A L Read. Presentation of search results: the CLs technique. Journal of Physics G: Nuclear and Particle Physics, 28(10):2693–2704, sep 2002.
[58] Tai Sakuma. Cutaway diagrams of CMS detector. May 2019.
[59] A.M.Sirunyan etal. Performance of the CMS muon detector and muon reconstruction s =13 TeV. JINST, 13(06):P06015,
[60] Yi Sun, Hao-Ran Chang, and Dao-Neng Gao. Higgs decays to gamma l+ l- in
struction with proton-proton collisions at 2018.
the standard model. JHEP, 05:061, 2013.
[61] M. Vesterinen and T.R. Wyatt. A novel technique for studying the z boson transverse momentum distribution at hadron colliders. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 602(2):432 – 437, 2009.
[62] Lorenzo Viliani. CMS Tracker Performance and Readiness for LHC Run II. Technical Report CMS-CR-2015-102, CERN, Geneva, Jun 2015.
[63] W. Erdmann. Offline primary vertex reconstruction with deterministic annealing clustering. CMS Internal note, 2011/014, 2011.
[64] C. S. Wu, E. Ambler, R. W. Hayward, D. D. Hoppes, and R. P. Hudson. Experimental test of parity conservation in beta decay. Phys. Rev., 105:1413–1415, Feb 1957. |