243 research outputs found
Outcome of coronary plaque burden: a 10-year follow-up of aggressive medical management
- Author
- A Menotti
- AS Agatston
- Chu-Pak Lau
- D Laurier
- DJ Brenner
- DK Tso
- DV Anand
- E Lau
- GA Diamond
- H-W Hense
- IU Haq
- J Liu
- JA Hoff
- JA Rumberger
- JE Maher
- John A Rumberger
- K Sutton-Tyrrell
- KS Woo
- KS Woo
- LC Chen
- M Hosoi
- Matthew J Budoff
- MJ Budoff
- ND Wong
- NK Kalia
- P Raggi
- RA Kronmal
- S Achenbach
- S Mao
- SP Raya
- SS Mao
- Stefan Mohlenkamp
- Stephan Achenbach
- T F Thomsen
- Third Report of the National Cholesterol Education Program (NCEP) Expert Panel on Detection Evaluation, and Treatment of High Blood Cholesterol in Adults (Adult Treatment Panel III)
- TL Mitchell
- TQ Callister
- TQ Callister
- Victor K Goh
- WE Boden
- WG Goodman
- WR Janowitz
- Publication venue
- BioMed Central
- Publication date
- 01/03/2010
- Field of study
<p>Abstract</p> <p>Background</p> <p>The effect of aggressive medical therapy on quantitative coronary plaque burden is not generally known, especially in ethnic Chinese.</p> <p>Aims</p> <p>We reasoned that Cardiac CT could conveniently quantify early coronary atherosclerosis in our patient population, and hypothesized that serial observation could differentiate the efficacy of aggressive medical therapy regarding progression and regression of the atherosclerotic process, as well as evaluating the additional impact of life-style modification and the relative effects of the application of statin therapy.</p> <p>Methods</p> <p>We employed a standardized Cardiac CT protocol to serially scan 113 westernized Hong Kong Chinese individuals (64 men and 49 women) with Chest Pain and positive coronary risk factors. In all cases included for this serial investigation, subsequent evaluation showed no significantly-obstructive coronary disease by functional studies and angiography. After stringent risk factor modification, including aggressive statin therapy to achieve LDL-cholesterol lowering conforming to N.C.E.P. ATP III guidelines, serial CT scans were performed 1-12 years apart for changes in coronary artery calcification (CAC), using the Agatston Score (AS) for quantification.</p> <p>Results</p> <p>At baseline, the mean AS was 1413.6 for males (mean age 54.4 years) and 2293.3 for females (mean age 62.4 years). The average increase of AS in the entire study population was 24% per year, contrasting with 16.4% per year on strict risk factor modification plus statin therapy, as opposed to 33.2% per year for historical control patients (p < 0.001). Additionally, 20.4% of the 113 patients demonstrated decreasing calcium scores. Medical therapy also yielded a remarkably low adverse event rate during the follow-up period --- 2 deaths, 2 strokes and only 1 case requiring PCI.</p> <p>Conclusions</p> <p>This study revealed that aggressive medical therapy can positively influence coronary plaque aiding in serial regression of calcium scores.</p
Coronary artery calcium screening: current status and recommendations from the European Society of Cardiac Radiology and North American Society for Cardiovascular Imaging
- Author
- A Becker
- A Becker
- A Bellasi
- A Gopal
- A Jemal
- A Knez
- A Knez
- A Schmermund
- A Taylor
- AB Newman
- AB Sevrukov
- AE Cassidy
- AE Stillman
- AE Stillman
- AJ Einstein
- AJ Einstein
- AJ Taylor
- AL Daniell
- Allen J. Taylor
- AP Guerin
- Arthur E. Stillman
- AY Wang
- B Lu
- CA Geluk
- CH McCollough
- CH Mielke
- CR Becker
- Cynthia H. McCollough
- D Georgiou
- D Russo
- DA Laudon
- DE Bild
- DH Lamont
- DS Berman
- DV Anand
- E Khaleeli
- G Assmann
- GA Block
- GA Block
- GK Sirineni
- GM Chertow
- GM Chertow
- GR Thompson
- GT Kondos
- HC Yoon
- HH Oei
- I Graham
- J Braun
- J Hausleiter
- J Horiguchi
- J Horiguchi
- J Horiguchi
- J Hsia
- J Oh
- J Shemesh
- JA Hoff
- JC Olson
- JE Hokanson
- JE Manson
- JJ Carr
- JK Snell-Bergeon
- JM Groen
- K Nasir
- K Sutton-Tyrrell
- KE Fleischmann
- L Wexler
- Leslee J. Shaw
- Lewis Wexler
- LH Kuller
- LJ Shaw
- LJ Shaw
- M Bursztyn
- M Kawakubo
- M Matsuoka
- M Sigrist
- Matthijs Oudkerk
- MJ Budoff
- MJ Budoff
- MJ Budoff
- MJ Budoff
- MJ Budoff
- MJ Budoff
- MJ Budoff
- MJ Greuter
- MJ LaMonte
- MJ Pletcher
- ML Rasouli
- MR Patel
- ND Wong
- ND Wong
- NK Kalia
- P Greenland
- P Greenland
- P Raggi
- P Raggi
- P Raggi
- P Raggi
- P Raggi
- P Raggi
- P Raggi
- P Raggi
- P Raggi
- P Raggi
- P Therasse
- Paolo Raggi
- Peter M. A. van Ooijen
- PM Ooijen van
- PW Wilson
- R Detrano
- R Erbel
- R Haberl
- R Mehrotra
- R Rubinshtein
- R Vliegenthart
- RA Kronmal
- RA O’Rourke
- RC Detrano
- RC Hendel
- RD Abbott
- RD Santos
- RJ Gibbons
- RJ Glynn
- RL Morin
- RM Conroy
- Rozemarijn Vliegenthart
- S Achenbach
- S Leschka
- S Mao
- S Schurgin
- S Ulzheimer
- Sandra S. Halliburton
- SC Smith Jr
- SM Grundy
- SM Harman
- Stefan Möhlenkamp
- T Jain
- TC Andrews
- TC Villines
- TM Doherty
- TQ Callister
- TS Church
- U Hoffmann
- VV McLaughlin
- VY Cheng
- W Qu
- WB Kannel
- WG Goodman
- Willi A. Kalender
- William Stanford
- Y Arad
- Y Arad
- Publication venue
- Springer Netherlands
- Publication date
- 01/01/2008
- Field of study
Current guidelines and literature on screening for coronary artery calcium for cardiac risk assessment are reviewed for both general and special populations. It is shown that for both general and special populations a zero score excludes most clinically relevant coronary artery disease. The importance of standardization of coronary artery calcium measurements by multi-detector CT is discussed
Worldwide trends in body-mass index, underweight, overweight, and obesity from 1975 to 2016: a pooled analysis of 2416 population-based measurement studies in 128·9 million children, adolescents, and adults.
- Author
- Abarca-Gomez L
- Abdeen ZA
- Abu-Rmeileh NM
- Acosta-Cazares B
- Acuin C
- Adams RJ
- Aekplakorn W
- Afsana K
- Aguilar-Salinas CA
- Agyemng C
- Ahmadvand A
- Ahrens W
- Ajlouni K
- Akhtaeva N
- Al Nsour M
- Al-Hazzaa HM
- Al-Othman AR
- Al-Raddadi R
- AlBuhairan F
- AlDhukai S
- Ali MM
- Ali O
- Alkerwi A
- Alvarez-Pedrerol M
- Aly E
- Amarapurkar DN
- Amouyel P
- Amuzu A
- Andersen LB
- Anderssen SA
- Andrade DS
- Angquist LH
- Anjana RM
- Anselmo Olinto MT
- Aounallah-Skhiri H
- Araujo J
- Arianse I
- Aris T
- Arlappa N
- Arveiler D
- Aryal KK
- Aspelund T
- Assah FK
- Assuncao MCF
- Aung MS
- Avdicova M
- Azevedo A
- Azizi F
- Babu BV
- Bahijri S
- Baker JL
- Balakrishna N
- Bamoshmoosh M
- Banach M
- Bandosz P
- Banegas JR
- Bao KLN
- Bao TQ
- Barbagallo CM
- Barcelo A
- Barkat A
- Barros AJD
- Barros MVG
- Bata I
- Batieha AM
- Batista RL
- Batyrbek A
- Baur LA
- Beaglehole R
- Bebakar WMW
- Ben Romdhane H
- Benedics J
- Benet M
- Bennet JE
- Bennet JE
- Bentham J
- Bernabe A
- Bernotiene G
- Bettiol H
- Bhagyalaxmi A
- Bharadwaj S
- Bhargava SK
- Bhatti Z
- Bhutta ZA
- Bhutta ZA
- Bi H
- Bi Y
- Biehl A
- Bikbov M
- Bilano V
- Bista B
- Bixby H
- Bjelica DJ
- Bjerregaard P
- Bjertnes E
- Bjness MB
- Bjorkelund C
- Blokstra A
- Bo S
- Bobak M
- Boddy LM
- Boehm BO
- Boeing H
- Boggia JG
- Boissonnet CP
- Boker LK
- Bonaccio M
- Bongard V
- Bovet P
- Braeckevelt L
- Braeckman L
- Bragt MCE
- Brajkovich I
- Branca F
- Braunerova RT
- Breckenkamp J
- Breda J
- Brenner H
- Brewster LM
- Brian GR
- Brinduse L
- Bruno G
- Bueno-de-Mesquita HB
- Bugge A
- Buoncristiano M
- Burazeri G
- Burns C
- Cabrera de Leon A
- Cacciottolo J
- Cadena LH
- Cai H
- Cama T
- Cameron C
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- Can G
- Candido APCC
- Capanzana M
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- Casas JP
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- Chan AW
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- Chen C-J
- Chen F
- Chen H
- Chen S
- Chen Z
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- Chetrit A
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- Chiolero A
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- Chirita-Emandi A
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- Chirlaque M-D
- Cho B
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- Christensen K
- Christofaro DG
- Chudek J
- Cifkova R
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- Claessens F
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- Concin H
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- Cottel D
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- Damasceno A
- Damsgaard CT
- Danae G
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- Dauchet L
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- de Oliveira PD
- De Ridder K
- De Smedt D
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- Deepa M
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- Delisle H
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- Dorosty AR
- dos Santos RN
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- Yamborisut U
- Yan W
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- Yiallouros PK
- Yngve A
- Yoshihara A
- You QS
- Younger-Coleman NO
- Yusof SM
- Yusoff F
- Yusoff MFM
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- Zaccagni L
- Zafiropulos V
- Zainuddin AA
- Zambon S
- Zampelas A
- Zamrazilova H
- Zdrojewski T
- Zeng Y
- Zhao D
- Zhao W
- Zheng W
- Zheng Y
- Zholdin B
- Zhou B
- Zhou M
- Zhu A
- Zhu D
- Zhussupov B
- Zimmermann E
- Publication venue
- Lancet
- Publication date
- 01/01/2017
- Field of study
BACKGROUND: Underweight, overweight, and obesity in childhood and adolescence are associated with adverse health consequences throughout the life-course. Our aim was to estimate worldwide trends in mean body-mass index (BMI) and a comprehensive set of BMI categories that cover underweight to obesity in children and adolescents, and to compare trends with those of adults. METHODS: We pooled 2416 population-based studies with measurements of height and weight on 128·9 million participants aged 5 years and older, including 31·5 million aged 5-19 years. We used a Bayesian hierarchical model to estimate trends from 1975 to 2016 in 200 countries for mean BMI and for prevalence of BMI in the following categories for children and adolescents aged 5-19 years: more than 2 SD below the median of the WHO growth reference for children and adolescents (referred to as moderate and severe underweight hereafter), 2 SD to more than 1 SD below the median (mild underweight), 1 SD below the median to 1 SD above the median (healthy weight), more than 1 SD to 2 SD above the median (overweight but not obese), and more than 2 SD above the median (obesity). FINDINGS: Regional change in age-standardised mean BMI in girls from 1975 to 2016 ranged from virtually no change (-0·01 kg/m2 per decade; 95% credible interval -0·42 to 0·39, posterior probability [PP] of the observed decrease being a true decrease=0·5098) in eastern Europe to an increase of 1·00 kg/m2 per decade (0·69-1·35, PP>0·9999) in central Latin America and an increase of 0·95 kg/m2 per decade (0·64-1·25, PP>0·9999) in Polynesia and Micronesia. The range for boys was from a non-significant increase of 0·09 kg/m2 per decade (-0·33 to 0·49, PP=0·6926) in eastern Europe to an increase of 0·77 kg/m2 per decade (0·50-1·06, PP>0·9999) in Polynesia and Micronesia. Trends in mean BMI have recently flattened in northwestern Europe and the high-income English-speaking and Asia-Pacific regions for both sexes, southwestern Europe for boys, and central and Andean Latin America for girls. By contrast, the rise in BMI has accelerated in east and south Asia for both sexes, and southeast Asia for boys. Global age-standardised prevalence of obesity increased from 0·7% (0·4-1·2) in 1975 to 5·6% (4·8-6·5) in 2016 in girls, and from 0·9% (0·5-1·3) in 1975 to 7·8% (6·7-9·1) in 2016 in boys; the prevalence of moderate and severe underweight decreased from 9·2% (6·0-12·9) in 1975 to 8·4% (6·8-10·1) in 2016 in girls and from 14·8% (10·4-19·5) in 1975 to 12·4% (10·3-14·5) in 2016 in boys. Prevalence of moderate and severe underweight was highest in India, at 22·7% (16·7-29·6) among girls and 30·7% (23·5-38·0) among boys. Prevalence of obesity was more than 30% in girls in Nauru, the Cook Islands, and Palau; and boys in the Cook Islands, Nauru, Palau, Niue, and American Samoa in 2016. Prevalence of obesity was about 20% or more in several countries in Polynesia and Micronesia, the Middle East and north Africa, the Caribbean, and the USA. In 2016, 75 (44-117) million girls and 117 (70-178) million boys worldwide were moderately or severely underweight. In the same year, 50 (24-89) million girls and 74 (39-125) million boys worldwide were obese. INTERPRETATION: The rising trends in children's and adolescents' BMI have plateaued in many high-income countries, albeit at high levels, but have accelerated in parts of Asia, with trends no longer correlated with those of adults. FUNDING: Wellcome Trust, AstraZeneca Young Health Programme
Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
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- Adzic P
- Afanasiev S
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- Aleksandrov A
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search for dark matter produced in association with top quarks in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. The data set used corresponds to an integrated luminosity of 35.9 fb(-1) recorded with the CMS detector at the LHC. Whereas previous searches for neutral scalar or pseudoscalar mediators considered dark matter production in association with a top quark pair only, this analysis also includes production modes with a single top quark. The results are derived from the combination of multiple selection categories that are defined to target either the single top quark or the top quark pair signature. No significant deviations with respect to the standard model predictions are observed. The results are interpreted in the context of a simplified model in which a scalar or pseudoscalar mediator particle couples to a top quark and subsequently decays into dark matter particles. Scalar and pseudoscalar mediator particles with masses below 290 and 300 GeV, respectively, are excluded at 95% confidence level, assuming a dark matter particle mass of 1 GeV and mediator couplings to fermions and dark matter particles equal to unity.Peer reviewe
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
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- Zhaozhong S
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- Zhu DH
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- Zhukov V
- Zientek M
- Zito G
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- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuolo D
- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
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- Aarup Petersen H
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- Yi K
- Yohay R
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- Yuldashev BS
- Yumiceva F
- Yusli MN
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeinali M
- Zenaiev O
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang W
- Zhang Y
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zich J
- Zielinski K
- Ziemons T
- Zientek M
- Zlebcik R
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Österberg K
- Özçelik Ö
- Široký J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for dark matter in the form of strongly interacting massive particles (SIMPs) using the CMS detector at the LHC is presented. The SIMPs would be produced in pairs that manifest themselves as pairs of jets without tracks. The energy fraction of jets carried by charged particles is used as a key discriminator to suppress efficiently the large multijet background, and the remaining background is estimated directly from data. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 16.1 fb - 1 , collected with the CMS detector in 2016. No significant excess of events is observed above the expected background. For the simplified dark matter model under consideration, SIMPs with masses up to 100 GeV are excluded and further sensitivity is explored towards higher masses
Search for the production of W^{\pm} W^{\pm} W^{\mp} events at \sqrt{s} = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
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- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Y
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- 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
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/07/2019
- Field of study
A search for the production of events containing three W bosons predicted by the standard model is reported. The search is based on a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the CMS experiment at the CERN LHC and corresponding to a total integrated luminosity of 35.9 fb^{-1}. The search is performed in final states with three leptons (electrons or muons), or with two same-charge leptons plus two jets. The observed (expected) significance of the signal for W^{\pm} W^{\pm} W^{\mp} production is 0.60 (1.78) standard deviations, and the ratio of the measured signal yield to that expected from the standard model is 0.34_{-0.34}^{+0.62}. Limits are placed on three anomalous quartic gauge couplings and on the production of massive axionlike particles
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullah WATW
- Abdullin S
- Abdulsalam A
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- Abu Zeid S
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- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
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- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
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- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Elsevier BV'
- Publication date
- 10/09/2019
- Field of study
The production cross sections of B_{s}^{0} mesons and charge conjugates are measured in proton-proton (pp) and PbPb collisions via the exclusive decay channel B_{s}^{0}→J/ψϕ→μ^{+}μ^{−}K^{+}K^{−} at a center-of-mass energy of 5.02 TeV per nucleon pair and within the rapidity range |y|<2.4 using the CMS detector at the LHC. The pp measurement is performed as a function of transverse momentum (p_{T}) of the B_{s}^{0} mesons in the range of 7 to 50 GeV/c and is compared to the predictions of perturbative QCD calculations. The B_{s}^{0} production yield in PbPb collisions is measured in two p_{T} intervals, 7 to 15 and 15 to 50 GeV/c, and compared to the yield in pp collisions in the same kinematic region. The nuclear modification factor (R_{AA}) is found to be 1.5±0.6(stat)±0.5(syst) for 7–15 GeV/c, and 0.87±0.30(stat)±0.17(syst) for 15–50 GeV/c, respectively. Within current uncertainties, the B_{s}^{0} results are consistent with models of strangeness enhancement, and suppression by parton energy loss, as observed for the B+ mesons
Search for Higgs boson pair production in the gamma gamma b(b)over-bar final state in pp collisions at root s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Acosta M Vazquez
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggarwal A
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Aleksandrov A
- Alexander J
- Ali MAB Md
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa K Hurtado
- Anderson D
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Angioni GL Pinna
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Arcaro D
- Arcidiacono R
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search is presented for the production of a pair of Higgs bosons, where one decays into two photons and the other one into a bottom quark-antiquark pair. The analysis is performed using proton-proton collision data at root s = 13 TeV recorded in 2016 by the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1) . The results are in agreement with standard model (SM) predictions. In a search for resonant production, upper limits are set on the cross section for new spin-0 or spin-2 particles. For the SM-like nonresonant production hypothesis, the data exclude a product of cross section and branching fraction larger than 2.0 fb at 95% confidence level (CL), corresponding to about 24 times the SM prediction. Values of the effective Higgs boson self-coupling K X are constrained to be within the range -11 < K-lambda < 17 at 95% CL, assuming all other Higgs boson couplings are at their SM value. The constraints on K-lambda, are the most restrictive to date. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
Measurement of the tt¯ production cross section, the top quark mass, and the strong coupling constant using dilepton events in pp collisions at √s = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Acharya H
- Ackert A
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- Acosta JG
- Adam W
- Adams MR
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- Aggleton R
- Agram J-L
- Ahmad A
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- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 29/04/2019
- Field of study
A measurement of the top quark–antiquark pair production cross section σtt¯ in proton–proton collisions at a centre-of-mass energy of 13TeV is presented. The data correspond to an integrated luminosity of 35.9fb−1, recorded by the CMS experiment at the CERN LHC in 2016. Dilepton events (e ± μ ∓, μ+μ−, e+e−) are selected and the cross section is measured from a likelihood fit. For a top quark mass parameter in the simulation of mMCt=172.5GeV the fit yields a measured cross section σtt¯=803±2(stat)±25(syst)±20(lumi)pb, in agreement with the expectation from the standard model calculation at next-to-next-to-leading order. A simultaneous fit of the cross section and the top quark mass parameter in the POWHEG simulation is performed. The measured value of mMCt=172.33±0.14(stat)+0.66−0.72(syst)GeV is in good agreement with previous measurements. The resulting cross section is used, together with the theoretical prediction, to determine the top quark mass and to extract a value of the strong coupling constant with different sets of parton distribution functions
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