61 research outputs found
A Brief Review of Higher Dietary Protein Diets in Weight Loss: A Focus on Athletes
- Author
- AA Mero
- AK Gosby
- AR Josse
- D Fouque
- DR Moore
- E Brandle
- EA Martens
- EC Haakonssen
- EM Weinheimer
- ER Helms
- I Garthe
- Institute of Medicine
- J Bohe
- J Maestu
- JD Bosse
- JL Areta
- JL Walberg
- JR Poortmans
- JW Krieger
- KR Westerterp
- L Havemann
- LM Burke
- LM Burke
- MS Westerterp-Plantenga
- NR Rodriguez
- OC Witard
- PJ Atherton
- PT Res
- S Mettler
- SJ Simpson
- SM Pasiakos
- SM Phillips
- SM Phillips
- Stuart M. Phillips
- T Stellingwerff
- TA Churchward-Venne
- TB Chaston
- TL Halton
- TN Frimel
- TP Wycherley
- WF Martin
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Post-Exercise Protein Trial: Interactions between Diet and Exercise (PEPTIDE): study protocol for randomized controlled trial
- Author
- Abdullah F Alghannam
- AF Alghannam
- AJ Vickers
- AM Rivera-Brown
- C Compher
- C Taylor
- D Thompson
- DB Dill
- DK Levenhagen
- DM Di Donato
- DR Moore
- DR Moore
- DS Rowlands
- DW West
- Dylan Thompson
- E Borsheim
- G Sun
- GA Borg
- H Taylor
- HW Goforth Jr
- I Mujika
- J Bergstrom
- J Betts
- J Bohe
- JA Betts
- JA Betts
- JA Hawley
- James A Betts
- James Bilzon
- JE Tang
- JM Berardi
- JM Berardi
- JO Holloszy
- JR Zierath
- JS Thomson
- JT Cramer
- JV Passonneau
- K Okazaki
- K Tsintzas
- KF Schulz
- KF Schulz
- KM Hill
- Kostas Tsintzas
- KR Howarth
- L Breen
- L Breen
- L Ferguson-Stegall
- L Ferguson-Stegall
- L Leick
- LJ James
- LJC van Loon
- M Beelen
- M Powney
- MP Harber
- NA Burd
- NA Jeacocke
- O Neubauer
- OC Witard
- PT Res
- RJ Little
- S Bird
- SB Wilkinson
- SJ Solomon
- SL Miller
- SM Pasiakos
- SM Shirreffs
- TA Churchward-Venne
- VG Coffey
- WR Lunn
- Y Liu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 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
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benitez JF
- Benussi L
- Beretvas A
- Bergauer T
- Berger P
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- Beri SB
- Bernardes CA
- Bernet C
- Berry D
- Berryhill J
- Bertacchi V
- Besancon M
- Beschi A
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- 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
- Boimska B
- Boletti A
- Bologna S
- Bols ES
- Bonacorsi D
- Bonanomi M
- Bonchev M
- Bonomally S
- Boos E
- Boran F
- Borchsh V
- Borg J
- Borgonovi L
- Bornheim A
- Borras K
- Bortignon P
- Bose T
- Bossini E
- Botta C
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- Bouhali O
- Bourgatte G
- Bourilkov D
- Bouza VR
- Bozzo M
- Bragagnolo A
- Braghieri A
- Braibant-Giacomelli S
- Brainerd C
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- Breedon R
- Breeze S
- Brew C
- Brigljevic V
- Brinkerhoff A
- Brivio F
- Brom J-M
- Brondolin E
- Brooke JJ
- Brown RM
- Brunner D
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- 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
- Cadamuro L
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- Cakir A
- Calandri A
- Calderon A
- Cali IA
- Call K
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- Calzaferri S
- Camen C
- Caminada L
- Campagnari C
- Campanini R
- Campbell A
- Campderros JD
- Camporesi T
- Candelise V
- Canelli MF
- Canepa A
- Cankocak K
- Capiluppi P
- Cappati A
- Caputo C
- Caraway B
- Cardini A
- Cardwell B
- Carle A
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- Cartiglia N
- Carvalho W
- Casarsa M
- Caspart R
- Cassese A
- Castaldi R
- Castilla-Valdez H
- Castro A
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Ceballos GG
- Ceccarelli R
- Cepaitis V
- Cepeda M
- Cerati GB
- Cerci DS
- Cerci S
- Cerminara G
- Cerrada M
- Cerri O
- Cetorelli F
- Chabert EC
- Chagas EBBD
- Chahal GS
- Chang P
- Chang P
- Chanon N
- Chao Y
- Chapon E
- Charaf O
- Charlot C
- Chatterjee RM
- Chatterjee S
- Chauhan S
- Chauhan S
- Chawla R
- Checchia P
- Chekhovsky V
- Chen C
- Chen GM
- Chen HS
- Chen KF
- Chen M
- Chen PH
- Chen X
- Chen Y
- Chen Y
- Chen Z
- Chenarani S
- Cheng T
- Cheng Y
- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhibra SS
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- Chistov R
- Chlebana F
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- Choi Y
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- Choudhary BC
- Choudhury S
- Chowdhury SR
- Chu J
- Chudasama R
- Chwalek T
- Ciangottini D
- Cifuentes JAB
- Ciocci MA
- Cipriani M
- Ciriolo V
- Cirkovic P
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clement E
- Clerbaux B
- CMS Collaboration
- Cockerill DJA
- Coelho E
- Colaleo A
- Cole JE
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- Collard C
- Colling D
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- Connor P
- Contardo D
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- Cornelis T
- Cortezon EP
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- Cossutti F
- Costa M
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- Coubez X
- Couderc F
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- Covarelli R
- Cox B
- Cox PT
- Cranshaw DJ
- Creanza D
- Cremonesi M
- Cristella L
- Croce DD
- Cruz SS
- Csanad M
- Csorgo T
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cummings G
- Cussans D
- Cutts D
- Czellar S
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Da Rold A
- Da Silva De Araujo FT
- Da Silveira GG
- Dabrowski A
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- Dalchenko M
- Dallavalle GM
- Damarseckin S
- Damgov J
- Damiani DD
- Danilov M
- Danilov V
- Daponte V
- Darwish MR
- Das P
- Das S
- Dasgupta A
- Dash D
- Daskalakis G
- Dasu S
- Datta A
- Dauncey P
- David A
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- De Barbaro P
- De Boer W
- De Bruyn I
- De Cassagnac RG
- De Castro Manzano P
- De Clercq J
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- De Fatis TT
- De Filippis N
- De Guio F
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- De Jesus Damiao D
- De Klundert MV
- De La Barca Sanchez MC
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Leo K
- De Monchenault GH
- De Oliveira ACA
- De Palma M
- De Roeck A
- De Souza SF
- De Trocóniz JF
- De Wit A
- De Wolf EA
- Deelen N
- Defranchis MM
- Deile M
- Dejardin M
- Delaere C
- Delannoy AG
- Delcourt M
- Delgado A
- Delgado MAS
- Dell'Orso R
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- Demina R
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- Demiroglu ZS
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- Dermenev A
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- Dewanjee RK
- Dezoort G
- Dharmaratna WGD
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- Diamantopoulou M
- Diaz D
- Didukh L
- Diemoz M
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- Dildick S
- Dilsiz K
- Dimitrov A
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- Dinardo ME
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- Dittmann J
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- Dobur D
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- Domenico MRD
- Dominguez A
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- Donegà M
- Donertas IS
- Doninck WV
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- Dubinin M
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- Dugad S
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- Dulemba JL
- Dumanoglu I
- Dupont N
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- Fernández JRG
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- 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
Observation of triple J/ψ meson production in proton-proton collisions
- Author
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- Zahid S
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- Zalewski P
- Zanetti M
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- Zygala L
- Álvarez CR
- 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-
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Search for low-mass dilepton resonances in Higgs boson decays to four-lepton final states in proton–proton collisions at √s=13TeV
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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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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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- Yuldashev BS
- 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
- Zeinali M
- Zeuner WD
- Zghiche A
- Zhang F
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- Zhizhin I
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- Zhu RY
- Ziemons T
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
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- Zou R
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- Zumerle G
- Zuo X
- 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 light Higgs bosons from supersymmetric cascade decays in pp collisions at √s=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Acosta HAE
- 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 A
- Alvarez JDR
- Alverson G
- Alves GA
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- Zorbilmez C
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- Zuolo D
- Zygala L
- 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
Search for long-lived particles decaying to leptons with large impact parameter in proton-proton collisions at root s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- 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
- Aime‘ 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
- Angioni GLP
- 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
- Asilar E
- Askew A
- Asmuss P
- Assran Y
- Atakisi IO
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- Auzinger G
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- Ayala G
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- Azhgirey I
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- Azzurri P
- Baarmand MM
- Babaev A
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- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Bagliesi G
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- Yumiceva F
- Yusli MN
- Yzquierdo AP-C
- Zabi A
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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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- Zhizhin I
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- Zorbilmez C
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- Zuolo D
- Zygala L
- Álvarez CR
- Özçelik Ö
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/11/2021
- Field of study
Copyright © CERN for the benefit of the CMS collaboration 2022. A search for new long-lived particles decaying to leptons using proton–proton collision data produced by the CERN LHC at s√=13TeV is presented. Events are selected with two leptons (an electron and a muon, two electrons, or two muons) that both have transverse impact parameter values between 0.01 and 10cm and are not required to form a common vertex. Data used for the analysis were collected with the CMS detector in 2016, 2017, and 2018, and correspond to an integrated luminosity of 118 (113)fb−1 in the ee channel (eμ and μμ channels). The search is designed to be sensitive to a wide range of models with displaced eμ, ee, and μμ final states. The results constrain several well-motivated models involving new long-lived particles that decay to displaced leptons. For some areas of the available phase space, these are the most stringent constraints to date.SCOAP3
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
- 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
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- Araujo M
- Arbelaez NV
- 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
- Attikis A
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- Yi K
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- Yumiceva F
- Yusli MN
- Yzquierdo AP-C
- Zabi A
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- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zenaiev O
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
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- Zhizhin I
- Zhokin A
- Zhu DH
- Zhu RY
- Ziemons T
- Zientek M
- Zlebcik R
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
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- 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
Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullin S
- Abercrombie D
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- 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
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