77 research outputs found
Search for Higgs Boson Pair Production in the Four b Quark Final State in Proton-Proton Collisions at root s=13 TeV
- Author
- Aarrestad T
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WW
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Adam W
- Adamidis K
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- Adloff C
- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J
- Aguilar-Benitez M
- Ahmad A
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- Ahmad WH
- Ahmed A
- Ahuja S
- Aime` C
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- Yumiceva F
- Yusli M
- Yzquierdo AP
- Zabi A
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- Zahid S
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- Zalewski P
- Zanetti M
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- Zarucki M
- Zecchinelli A
- Zeinali M
- Zeuner W
- Zghiche A
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- Zhizhin I
- Zhokin A
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- Zoi I
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- Zorbilmez C
- Zotto P
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- Zuo X
- Zuolo D
- Zygala L
- Álvarez CR
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2022
- Field of study
Search for invisible decays of the Higgs boson produced via vector boson fusion in proton-proton collisions at root s=13 TeV
- Author
- Aarrestad T
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim A
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Acosta HE
- Adam W
- Adamidis K
- Adams E
- Adams M
- Adams T
- Addesa F
- Adloff C
- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aimè C
- Akchurin N
- Akgun B
- Akpinar A
- Albergo S
- Albert A
- Albrecht S
- Albrow M
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Almond J
- Alonso AG
- Alpana A
- Alvarez JR
- Alverson G
- Alves BFS
- Alves G
- Aly R
- Alyari M
- Amapane N
- Amaral SSD
- Amarilo KM
- Ambrozas M
- Amendola C
- Amin N
- Amram O
- Amsler C
- An S
- An Y
- Anagnostou G
- Anampa KH
- Andrea J
- Andreassi G
- Andreev V
- Andreev Y
- Andrejkovic J
- Andrews M
- Androsov K
- Anguiano J
- Antchev G
- Antequera JB
- Anthony D
- Antunovic Z
- Anuar AB
- Apollinari G
- Apparu D
- Appelt E
- Apresyan A
- Apyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton M
- Argiro S
- Arneodo M
- Aruta C
- Asavapibhop B
- Asawatangtrakuldee C
- Asenov P
- Asghar M
- Asilar E
- Askew A
- Asmuss P
- Atakisi I
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awais A
- Awan M
- Ayala E
- Ayala G
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand M
- Babaev A
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Bakshi A
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banos LE
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barnes V
- Barney D
- Baron O
- Barrera CB
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- Yoon I
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- Yu I
- Yu Pr
- Yu S
- Yuan L
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- Yuldashev B
- Yumiceva F
- Yzquierdo AP
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli A
- Zeinali M
- Zeuner W
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu R
- Ziemons T
- Zipper N
- Zoi I
- Zolkapli Z
- Zorbakir I
- Zorbilmez C
- Zotto P
- Zotz A
- Zou D
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez CR
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2022
- Field of study
Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at root s=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aime' C
- Akchurin N
- Akgun B
- Akpinar A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allen B
- Almond J
- Alonso AG
- Alvarez JDR
- Alverson G
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amaral SMSD
- Amendola C
- Amin N
- Amram O
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Angioni GLP
- Antchev G
- Antunovic Z
- Anuar AAB
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Apyan A
- Araujo M
- Arbelaez NV
- Arbol PMRD
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Aruta C
- Asavapibhop B
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Asmuss P
- Atakisi IO
- Atanasov I
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awan MIM
- Ayala E
- Ayala G
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Banos LIE
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barnes VE
- Barney D
- Baron O
- Barrera CB
- Barrera CO
- Bartek R
- Bartosik N
- Bartók M
- Bastos D
- Battilana C
- Baty A
- Bauerdick LAT
- Baur S
- Baxter S
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Becerra DAS
- Bechtel J
- Bedoya CF
- Beghin D
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Bellora A
- Belyaev A
- Belyaev A
- Benaglia A
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- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benitez JF
- Benussi L
- Beretvas A
- Bergauer T
- Berger P
- Berger T
- Beri SB
- Bernardes CA
- Bernet C
- Berry D
- Berryhill J
- Bertacchi V
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- Beschi A
- Bhal E
- Bhardwaj A
- Bharti M
- Bhat MA
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- Bhattacharya S
- Bhattacharya S
- Bheesette S
- Bhowmik D
- Bhowmik S
- Bhyun JH
- Bi R
- Bialkowska H
- Bianchini L
- Bianco M
- Bianco S
- Biasini M
- Bihan A-CL
- Biino C
- Bilei GM
- Bilin B
- Bindhu VKMN
- Bisello D
- Black K
- Blekman F
- Blinov V
- Bloch D
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Boccali T
- Bocci A
- Bodek A
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- Boletti A
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- Bols ES
- Bonacorsi D
- Bonanomi M
- Bonchev M
- Bonomally S
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- Bornheim A
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- Bortignon P
- Bose T
- Bossini E
- Botta C
- Botta V
- Boudoul G
- Bouhali O
- Bourgatte G
- Bourilkov D
- Bouza VR
- Bozzo M
- Bragagnolo A
- Braghieri A
- Braibant-Giacomelli S
- Brainerd C
- Brandt S
- Branson JG
- Breedon R
- Breeze S
- Brew C
- Brigljevic V
- Brinkerhoff A
- Brivio F
- Brom J-M
- Brondolin E
- Brooke JJ
- Brown RM
- Brunner D
- Bruno G
- Brzhechko D
- Brücken E
- Bucci R
- Buccilli A
- Buchanan J
- Buchmuller O
- Bueghly J
- Bundock A
- Bunichev V
- Bunin P
- Bunkowski K
- Buontempo S
- Burgo RD
- Burkett K
- Burkle B
- Burt K
- Bury F
- Busson P
- Busza W
- Butalla S
- Butler JN
- Butler PH
- Butz E
- Bylinkin A
- Bylsma B
- Byszuk A
- Caballero IG
- Cabrera A
- Cabrillo IJ
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- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe
A Deep Neural Network for Simultaneous Estimation of b Jet Energy and Resolution
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- Publication venue
- Publication date
- 01/01/2020
- Field of study
We describe a method to obtain point and dispersion estimates for the energies of jets arising from b quarks produced in proton-proton collisions at an energy of s = 13 TeV at the CERN LHC. The algorithm is trained on a large sample of simulated b jets and validated on data recorded by the CMS detector in 2017 corresponding to an integrated luminosity of 41 fb - 1 . A multivariate regression algorithm based on a deep feed-forward neural network employs jet composition and shape information, and the properties of reconstructed secondary vertices associated with the jet. The results of the algorithm are used to improve the sensitivity of analyses that make use of b jets in the final state, such as the observation of Higgs boson decay to b b ¯
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- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
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- Özçelik Ö
- Publication venue
- Springer Science and Business Media LLC
- Publication date
- 07/07/2022
- Field of study
A Correction to this paper has been published (18 October 2023) : https://doi.org/10.1038/s41586-023-06164-8.Data availability:
Tabulated results are provided in the HEPData record for this analysis. Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS data preservation, re-use and open acess policy.Code availability:
The CMS core software is publicly available on GitHub (https://github.com/cms-sw/cmssw).In July 2012, the ATLAS and CMS collaborations at the CERN Large Hadron Collider announced the observation of a Higgs boson at a mass of around 125 gigaelectronvolts. Ten years later, and with the data corresponding to the production of a 30-times larger number of Higgs bosons, we have learnt much more about the properties of the Higgs boson. The CMS experiment has observed the Higgs boson in numerous fermionic and bosonic decay channels, established its spin–parity quantum numbers, determined its mass and measured its production cross-sections in various modes. Here the CMS Collaboration reports the most up-to-date combination of results on the properties of the Higgs boson, including the most stringent limit on the cross-section for the production of a pair of Higgs bosons, on the basis of data from proton–proton collisions at a centre-of-mass energy of 13 teraelectronvolts. Within the uncertainties, all these observations are compatible with the predictions of the standard model of elementary particle physics. Much evidence points to the fact that the standard model is a low-energy approximation of a more comprehensive theory. Several of the standard model issues originate in the sector of Higgs boson physics. An order of magnitude larger number of Higgs bosons, expected to be examined over the next 15 years, will help deepen our understanding of this crucial sector.BMBWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, FAPERGS, and FAPESP (Brazil); MES and BNSF (Bulgaria); CERN; CAS, MoST, and NSFC (China); MINCIENCIAS (Colombia); MSES and CSF (Croatia); RIF (Cyprus); SENESCYT (Ecuador); MoER, ERC PUT and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRI (Greece); NKFIH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); MSIP and NRF (Republic of Korea); MES (Latvia); LAS (Lithuania); MOE and UM (Malaysia); BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MOS (Montenegro); MBIE (New Zealand); PAEC (Pakistan); MES and NSC (Poland); FCT (Portugal); MESTD (Serbia); MCIN/AEI and PCTI (Spain); MOSTR (Sri Lanka); Swiss Funding Agencies (Switzerland); MST (Taipei); MHESI and NSTDA (Thailand); TUBITAK and TENMAK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA). Individuals have received support from the Marie-Curie programme and the European Research Council and Horizon 2020 Grant, contract Nos. 675440, 724704, 752730, 758316, 765710, 824093, 884104, and COST Action CA16108 (European Union); the Leventis Foundation; the Alfred P. Sloan Foundation; the Alexander von Humboldt Foundation; the Belgian Federal Science Policy Office; the Fonds pour la Formation à la Recherche dans l’Industrie et dans l’Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the F.R.S.-FNRS and FWO (Belgium) under the “Excellence of Science – EOS” – be.h project n. 30820817; the Beijing Municipal Science & Technology Commission, No. Z191100007219010; the Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Stavros Niarchos Foundation (Greece); the Deutsche Forschungsgemeinschaft (DFG), under Germany’s Excellence Strategy – EXC 2121 “Quantum Universe” – 390833306, and under project number 400140256 - GRK2497; the Hungarian Academy of Sciences, the New National Excellence Program - ÚNKP, the NKFIH research grants K 124845, K 124850, K 128713, K 128786, K 129058, K 131991, K 133046, K 138136, K 143460, K 143477, 2020-2.2.1-ED-2021-00181, and TKP2021-NKTA-64 (Hungary); the Council of Science and Industrial Research, India; the Latvian Council of Science; the Ministry of Education and Science, project no. 2022/WK/14, and the National Science Center, contracts Opus 2021/41/B/ST2/01369 and 2021/43/B/ST2/01552 (Poland); the Fundação para a Ciência e a Tecnologia, grant CEECIND/01334/2018 (Portugal); the National Priorities Research Program by Qatar National Research Fund; MCIN/AEI/10.13039/501100011033, ERDF “a way of making Europe”, and the Programa Estatal de Fomento de la Investigación Científica y Técnica de Excelencia María de Maeztu, grant MDM-2017-0765 and Programa Severo Ochoa del Principado de Asturias (Spain); the Chulalongkorn Academic into Its 2nd Century Project Advancement Project, and the National Science, Research and Innovation Fund via the Program Management Unit for Human Resources & Institutional Development, Research and Innovation, grant B05F650021 (Thailand); the Kavli Foundation; the Nvidia Corporation; the SuperMicro Corporation; the Welch Foundation, contract C-1845; and the Weston Havens Foundation (USA)
Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production
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- Yumiceva F
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- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
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- Zecchinelli AG
- Zeinali M
- Zeuner WD
- Zghiche A
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- Zorbilmez C
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- Zuolo D
- Zygala L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Since the discovery of the Higgs boson in 2012, detailed studies of its properties have been ongoing. Besides its mass, its width—related to its lifetime—is an important parameter. One way to determine this quantity is to measure its off-shell production, where the Higgs boson mass is far away from its nominal value, and relating it to its on-shell production, where the mass is close to the nominal value. Here we report evidence for such off-shell contributions to the production cross-section of two Z bosons with data from the CMS experiment at the CERN Large Hadron Collider. We constrain the total rate of the off-shell Higgs boson contribution beyond the Z boson pair production threshold, relative to its standard model expectation, to the interval [0.0061, 2.0] at the 95% confidence level. The scenario with no off-shell contribution is excluded at a p-value of 0.0003 (3.6 standard deviations). We measure the width of the Higgs boson as ΓH=3.2+2.4−1.7MeV, in agreement with the standard model expectation of 4.1 MeV. In addition, we set constraints on anomalous Higgs boson couplings to W and Z boson pairs
Recommended from our members
Precision measurement of the W boson decay branching fractions in proton-proton collisions at √s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullah WATW
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- Yumiceva F
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- Yzquierdo AP-C
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- Zahid S
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- Zalewski P
- Zanetti M
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- Zecchinelli AG
- Zeinali M
- Zeuner WD
- Zghiche A
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- Zorbilmez C
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- Zuolo D
- Zygala L
- Álvarez CR
- Özçelik Ö
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 26/04/2022
- Field of study
The leptonic and inclusive hadronic decay branching fractions of the W boson are measured using
proton-proton collision data collected at ffiffi s p ¼ 13 TeV by the CMS experiment at the CERN LHC,
corresponding to an integrated luminosity of 35.9 fb−1. Events characterized by the production of one or
two W bosons are selected and categorized based on the multiplicity and flavor of reconstructed leptons, the
number of jets, and the number of jets identified as originating from the hadronization of b quarks. A
binned maximum likelihood estimate of the W boson branching fractions is performed simultaneously in
each event category. The measured branching fractions of the W boson decaying into electron, muon, and
tau lepton final states are ð10.83 0.10Þ%, ð10.94 0.08Þ%, and ð10.77 0.21Þ%, respectively,
consistent with lepton flavor universality for the weak interaction. The average leptonic and inclusive
hadronic decay branching fractions are estimated to be ð10.89 0.08Þ% and ð67.32 0.23Þ%, respec tively. Based on the hadronic branching fraction, three standard model quantities are subsequently derived: the sum of squared elements in the first two rows of the Cabibbo–Kobayashi–Maskawa (CKM) matrix
P ij jVijj 2 ¼ 1.984 0.021, the CKM element jVcsj ¼ 0.967 0.011, and the strong coupling constant at
the W boson mass scale, αSðm2 WÞ ¼ 0.095 0.033
Observation of triple J/ψ meson production in proton-proton collisions
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullah WATW
- Abdullin S
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- Choudhury S
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- Özçelik Ö
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 19/01/2023
- Field of study
Data availability:
Tabulated results are provided in the HEPData record for this analysis71. Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in CMS data preservation, re-use and open access policy.Code availability:
The CMS core software is publically available at https://github.com/cms-sw/cmssw.Copyright . Protons consist of three valence quarks, two up-quarks and one down-quark, held together by gluons and a sea of quark-antiquark pairs. Collectively, quarks and gluons are referred to as partons. In a proton-proton collision, typically only one parton of each proton undergoes a hard scattering – referred to as single-parton scattering – leaving the remainder of each proton only slightly disturbed. Here, we report the study of double- and triple-parton scatterings through the simultaneous production of three J/ψ mesons, which consist of a charm quark-antiquark pair, in proton-proton collisions recorded with the CMS experiment at the Large Hadron Collider. We observed this process – reconstructed through the decays of J/ψ mesons into pairs of oppositely charged muons – with a statistical significance above five standard deviations. We measured the inclusive fiducial cross-section to be 272+141−104(stat)±17(syst)fb, and compared it to theoretical expectations for triple-J/ψ meson production in single-, double- and triple-parton scattering scenarios. Assuming factorization of multiple hard-scattering probabilities in terms of single-parton scattering cross-sections, double- and triple-parton scattering are the dominant contributions for the measured process.SCOAP3.Change history:
27 February 2023A Correction to this paper has been published: https://doi.org/10.1038/s41567-023-01992-
Recommended from our members
Search for light Higgs bosons from supersymmetric cascade decays in pp collisions at √s=13TeV
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- Álvarez CR
- Özçelik Ö
- Publication venue
- Springer Science and Business Media LLC
- Publication date
- 06/07/2023
- Field of study
A search is reported for pairs of light Higgs
bosons (H1) produced in supersymmetric cascade decays in
f
inal states with small missing transverse momentum. A data
set of LHC pp collisions collected with the CMS detector
at √s = 13TeV and corresponding to an integrated lumi
nosity of 138fb−1 is used. The search targets events where
both H1 bosons decay into b¯b pairs that are reconstructed
as large-radius jets using substructure techniques. No evi
dence is found for an excess of events beyond the back
ground expectations of the standard model (SM). Results
from the search are interpreted in the next-to-minimal super
symmetric extension of the SM, where a “singlino” of small
mass leads to squark and gluino cascade decays that can pre
dominantly end in a highly Lorentz-boosted singlet-like H1
andasinglino-likeneutralinoofsmalltransversemomentum.
Upperlimitsaresetontheproductofthesquarkorgluinopair
production cross section and the square of the b¯b branching
fraction of the H1 in a benchmark model containing almost
mass-degenerategluinosandlight-flavoursquarks.Underthe
assumption of an SM-like H1 → b¯b branching fraction, H1
bosonswithmassesintherange40–120GeVarisingfromthe
decays of squarks or gluinos with a mass of 1200–2500GeV
are excluded at 95% confidence level.SCOA
Performance of the CMS muon trigger system in proton-proton collisions at root s=13 TeV
- Author
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- Abbaneo D
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- Zenaiev O
- Zeuner WD
- Zghiche A
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2021
- Field of study
The muon trigger system of the CMS experiment uses a combination of hardware and software to identify events containing a muon. During Run 2 (covering 2015–2018) the LHC achieved instantaneous luminosities as high as 2 × 1034 while delivering proton-proton collisions at √(s) = 13. The challenge for the trigger system of the CMS experiment is to reduce the registered event rate from about 40MHz to about 1kHz. Significant improvements important for the success of the CMS physics program have been made to the muon trigger system via improved muon reconstruction and identification algorithms since the end of Run 1 and throughout the Run 2 data-taking period. The new algorithms maintain the acceptance of the muon triggers at the same or even lower rate throughout the data-taking period despite the increasing number of additional proton-proton interactions in each LHC bunch crossing. In this paper, the algorithms used in 2015 and 2016 and their improvements throughout 2017 and 2018 are described. Measurements of the CMS muon trigger performance for this data-taking period are presented, including efficiencies, transverse momentum resolution, trigger rates, and the purity of the selected muon sample. This paper focuses on the single- and double-muon triggers with the lowest sustainable transverse momentum thresholds used by CMS. The efficiency is measured in a transverse momentum range from 8 to several hundred
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