56 research outputs found
Effects of luteectomy in early pregnancy on the maintenance of gestation and plasma progesterone concentrations in the viviparous temperate lizard Barisia imbricata imbricata
- Author
- A Cree
- AR Bourne
- B Fergusson
- BM Sekharappa
- C Dauphin-Villemant
- C Dauphin-Villemant
- DL Painter
- DM Olson
- DR Highfill
- DR Highfill
- EO Moll
- F Xavier
- FM Guarino
- GL Luna
- Guadalupe Ortiz-López
- HS Cuellar
- HW Ambrose
- IP Callard
- IP Callard
- JJ Roth
- JL Guillette Jr
- JL Guillette Jr
- JP Defaure
- JP Lien
- JRG Challis
- Juana Alba Luis-Díaz
- Leticia Moreno-Fierros
- LJ Guillette Jr
- LJ Guillette Jr
- LJ Guillette Jr
- LJ Guillette Jr
- M Arslan
- M Martínez-Torres
- M Martínez-Torres
- M Martínez-Torres
- M Martínez-Torres
- M Panigel
- M Villagrán-Santa Cruz
- Mario Cárdenas-León
- Marta E Hernández-Caballero
- Martín Martínez-Torres
- N Atkins
- N Badir
- PB Medawar
- R Shine
- RE Jones
- RV Cyrus
- SK Saidapur
- SK Varma
- V Lance
- Z Yaron
- Z Yaron
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
<p>Abstract</p> <p>Background</p> <p>Several studies have shown that the corpus luteum is the principal source of progesterone during the gravidity period in reptiles; however, its participation in the maintenance of gestation in the viviparous squamata is in dispute. The effects of ovariectomy or luteectomy vary according to the species and the time at which the procedure is performed. In this paper, we describe the effects of luteectomy during early pregnancy on the maintenance of gestation and progesterone concentrations in the temperate Mexican viviparous lizard <it>Barisia imbricata imbricata.</it></p> <p>Methods</p> <p>Twenty-four lizards were subjected to three different treatments: luteectomy, sham luteectomy or non-surgical treatment, and blood samples were obtained before and after surgical treatment at different stages of gestation to determine the effects of luteectomy on the maintenance of gestation and progesterone concentrations.</p> <p>Results</p> <p>Spontaneous abortion was not observed in any of the females. However, luteectomy provoked abnormal parturition and a significant reduction in the number of young born alive. Parturition was normal in untreated females as well as those submitted to sham luteectomy. The surgical treatment also caused a significant reduction in progesterone concentrations in luteectomised females during early and middle gestation. However, no significant differences in hormone concentrations were observed among the three groups during late gestation or immediately post-parturition.</p> <p>Conclusions</p> <p>Our observations indicate that the presence of the corpus luteum is not necesary for the maintenance of gestation, but that it does participate in parturition control. Moreover, the corpus luteum of the viviparous lizard <it>B. i. imbricata</it> produces progesterone, at least during the first half of pregnancy, and that an extra-ovarian source of progesterone must maintain gestation in the absence of luteal tissue.</p
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
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- Albergo S
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- Albrow M
- Aleksandrov A
- Alexander J
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- Alonso AG
- Alvarez JDR
- Alverson G
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- Alyari M
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- Amendola C
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- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez CR
- 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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- Özçelik Ö
- 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 ¯
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
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams MR
- Adams T
- Addesa FM
- 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
- 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 K
- Alvarez JDR
- Alverson G
- Alves GA
- Aly R
- Alyari M
- Amapane N
- 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 JW
- Andrews MB
- Androsov K
- Anguiano J
- Antchev G
- Antequera JB
- Anthony D
- Antunovic Z
- Anuar AAB
- Apollinari G
- Apparu D
- Appelt E
- Apresyan A
- Apyan A
- Araujo M
- Arbol PMRD
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Aruta C
- Asavapibhop B
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
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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
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
- Abdullin S
- Abercrombie D
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- Addesa FM
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- Yzquierdo AP-C
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- Zahid S
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- Zalewski P
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- Zecchinelli AG
- Zeinali M
- Zeuner WD
- Zghiche A
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- Zorbakir IS
- 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
Recommended from our members
Search for low-mass dilepton resonances in Higgs boson decays to four-lepton final states in proton–proton collisions at √s=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- 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
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aimè 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
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- Amram O
- Amsler C
- Anagnostou G
- Anampa KH
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
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- Angioni GLP
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- Arbol PMRD
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- Arenton MW
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- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
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- Atakisi IO
- Atanasov I
- Ather MW
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- Barbagli G
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- Özçelik Ö
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/04/2022
- Field of study
Data Availability: This manuscript has no associated data or the data will not be deposited. [Authors’ comment: For CMS 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” (https://cms-docdb.cern.ch/cgi-bin/PublicDocDB/RetrieveFile?docid=6032&filename=CMSDataPolicyV1.2.pdf&version=2).]Copyright © CERN for the benefit of the CMS collaboration 2022. A search for low-mass dilepton resonances in Higgs boson decays is conducted in the four-lepton final state. The decay is assumed to proceed via a pair of beyond the standard model particles, or one such particle and a Z boson. The search uses proton–proton collision data collected with the CMS detector at the CERN LHC, corresponding to an integrated luminosity of 137fb−1, at a center-of-mass energy s√=13TeV. No significant deviation from the standard model expectation is observed. Upper limits at 95% confidence level are set on model-independent Higgs boson decay branching fractions. Additionally, limits on dark photon and axion-like particle production, based on two specific models, are reported.SCOAP3
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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)
Search for dark matter produced in association with a leptonically decaying Z boson in proton–proton collisions at s√=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
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- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
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- Ahmad WH
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- Asawatangtrakuldee C
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- Asghar MI
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- Atakisi IO
- Atanasov I
- Ather MW
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- Yao Y
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- Yazgan E
- Yetkin EA
- Yi K
- Yohay R
- Yoo HD
- Yoo J
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- Yuan S
- Yumiceva F
- Yusli MN
- Yzquierdo AP-C
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zenaiev O
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang W
- Zhang Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu DH
- Zhu RY
- Ziemons T
- Zientek M
- Zlebcik R
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez CR
- Özçelik Ö
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 07/12/2020
- Field of study
A search for dark matter particles is performed using events with a Z boson candidate and large missing transverse momentum. The analysis is based on proton–proton collision data at a center-of-mass energy of 13TeV, collected by the CMS experiment at the LHC in 2016–2018, corresponding to an integrated luminosity of 137fb−1. The search uses the decay channels Z→ee and Z→μμ. No significant excess of events is observed over the background expected from the standard model. Limits are set on dark matter particle production in the context of simplified models with vector, axial-vector, scalar, and pseudoscalar mediators, as well as on a two-Higgs-doublet model with an additional pseudoscalar mediator. In addition, limits are provided for spin-dependent and spin-independent scattering cross sections and are compared to those from direct-detection experiments. The results are also interpreted in the context of models of invisible Higgs boson decays, unparticles, and large extra dimensions.SCOAP
Measurements of pp → ZZ production cross sections and constraints on anomalous triple gauge couplings at √ = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- 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
- Ambrogi F
- Amendola C
- Amin N
- Amram O
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
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- Angioni GLP
- Antchev G
- Antunovic Z
- Anuar AAB
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- Apollinari G
- Appelt E
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- Arbelaez NV
- Arbol PMRD
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- Arenton MW
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- Asawatangtrakuldee C
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- Asghar MI
- Asilar E
- Askew A
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- Atakisi IO
- Atanasov I
- Ather MW
- Attikis A
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- Banos LIE
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- Barbagli G
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- Baringer P
- Barnes VE
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- Barrera CB
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- Bedoya CF
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- Belyaev A
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- Bendavid J
- Benecke A
- Benelli G
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- Yusli MN
- Yzquierdo AP-C
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- Zalewski P
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- Zeuner WD
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- Zhizhin I
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- Zorbilmez C
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- Özçelik Ö
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 29/12/2020
- Field of study
© 2021 The CMS Collaboration. The production of Z boson pairs in proton–proton (pp) collisions, pp → (Z/∗)(Z/∗) → 2ℓ2ℓ′, where ℓ,ℓ′ = e or μ, is studied at a center-of-mass energy of 13 TeV with the CMS detector at the CERN LHC. The data sample corresponds to an integrated luminosity of 137fb−1, collected during 2016–2018. The ZZ production cross section, tot(pp → ZZ) = 17.4 ± 0.3 (stat) ± 0.5 (syst) ± 0.4 (Theo) ± 0.3 (lumi) pb, measured for events with two pairs of opposite-sign, same-flavor leptons produced in the mass region 60 < ℓ+ℓ− < 120 GeV is consistent with standard model predictions. Differential cross sections are also measured and agree with theoretical predictions. The invariant mass distribution of the four-lepton system is used to set limits on anomalous ZZZ and ZZ couplings.SCOAP
Performance of the CMS muon trigger system in proton-proton collisions at root s=13 TeV
- Author
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- Abbaneo D
- Abbiendi G
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- Zeuner WD
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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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