139 research outputs found
Major colonic complications of hepatic transplantation
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1979
- Field of study
The counseling african americans to control hypertension (caatch) trial: baseline demographic, clinical, psychosocial, and behavioral characteristics
- Author
- A Schoenthaler
- AI Qureshi
- Andrea Cassells
- AV Chobanian
- Chamanara Kalida
- CL Ogden
- CL Roumie
- D Hedeker
- D Hedeker
- D Perloff
- DE Morisky
- DG Altman
- EH Wagner
- FM Sacks
- G Ogedegbe
- G Ogedegbe
- Gbenga Ogedegbe
- HA Taylor Jr
- HB Bosworth
- HB Bosworth
- HB Bosworth
- JA Cutler
- JE Ware
- JG Ford
- Jonathan N Tobin
- K Kroenke
- KM Gans
- L Corsino
- L Osterberg
- LE Boulware
- LE Fields
- LJ Appel
- LJ Appel
- LJ Appel
- LP Svetkey
- LP Svetkey
- LS Hicks
- M Johns
- MA Albert
- MA McDowell
- Marleny Diaz-Gloster
- MW Johns
- ND Wong
- P Muntner
- Q Gu
- RG Victor
- RJ Dolor
- RS Paffenbarger
- SB Wyatt
- Senaida Fernandez
- T Giles
- T Young
- T Young
- TC Davis
- VK Kapur
- W Gerin
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>Effectiveness of combined physician and patient-level interventions for blood pressure (BP) control in low-income, hypertensive African Americans with multiple co-morbid conditions remains largely untested in community-based primary care practices. Demographic, clinical, psychosocial, and behavioral characteristics of participants in the Counseling African American to Control Hypertension (CAATCH) Trial are described. CAATCH evaluates the effectiveness of a multi-level, multi-component, evidence-based intervention compared with usual care (UC) in improving BP control among poorly controlled hypertensive African Americans who receive primary care in Community Health Centers (CHCs).</p> <p>Methods</p> <p>Participants included 1,039 hypertensive African Americans receiving care in 30 CHCs in the New York Metropolitan area. Baseline data on participant demographic, clinical (<it>e.g</it>., BP, anti-hypertensive medications), psychosocial (<it>e.g</it>., depression, medication adherence, self-efficacy), and behavioral (<it>e.g</it>., exercise, diet) characteristics were gathered through direct observation, chart review, and interview.</p> <p>Results</p> <p>The sample was primarily female (71.6%), middle-aged (mean age = 56.9 ± 12.1 years), high school educated (62.4%), low-income (72.4% reporting less than $20,000/year income), and received Medicaid (35.9%) or Medicare (12.6%). Mean systolic and diastolic BP were 150.7 ± 16.7 mm Hg and 91.0 ± 10.6 mm Hg, respectively. Participants were prescribed an average of 2.5 ± 1.9 antihypertensive medications; 54.8% were on a diuretic; 33.8% were on a beta blocker; 41.9% were on calcium channel blockers; 64.8% were on angiotensin converting enzyme (ACE) inhibitors/angiotensin receptor blockers (ARBs). One-quarter (25.6%) of the sample had resistant hypertension; one-half (55.7%) reported medication non-adherence. Most (79.7%) reported one or more co-morbid medical conditions. The majority of the patients had a Charlson Co-morbidity score ≥ 2. Diabetes mellitus was common (35.8%), and moderate/severe depression was present in 16% of participants. Participants were sedentary (835.3 ± 1,644.2 Kcal burned per week), obese (59.7%), and had poor global physical health, poor eating habits, high health literacy, and good overall mental health.</p> <p>Conclusions</p> <p>A majority of patients in the CAATCH trial exhibited adverse lifestyle behaviors, and had significant medical and psychosocial barriers to adequate BP control. Trial outcomes will shed light on the effectiveness of evidence-based interventions for BP control when implemented in real-world medical settings that serve high numbers of low-income hypertensive African-Americans with multiple co-morbidity and significant barriers to behavior change.</p
Phenomenon of declining blood pressure in elderly - high systolic levels are undervalued with Korotkoff method
- Author
- A Araghi
- A Ungar
- Arkadiusz Siennicki-Lantz
- B Fagher
- B Riegel
- C Qiu
- C Qiu
- C Qiu
- D Perloff
- DE Strandness Jr
- E Umana
- F Forette
- FH Messerli
- I Skoog
- J Belmin
- J Verghese
- K Hirata
- K Svardsudd
- LJ Launer
- M Kähönen-Väre
- MC Morris
- NS Beckett
- P Gosse
- PE Nielsen
- S Landahl
- SE Nilsson
- SG Blank
- SM Hakala
- SM Hakala
- Sölve Elmståhl
- TE Strandberg
- TG Pickering
- WJ Burke
- WW Holland
- Z Guo
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>Systolic blood pressure (SBP) decline has been reported in octogenarians. The aim was to study if it could be observed while measuring SBP with two methods: Korotkoff (K-BP) and Strain-Gauge-Finger-Pletysmography (SG-BP), and which of them were more reliable in expressing vascular burden.</p> <p>Methods</p> <p>A cohort of 703 men from a population of Malmö, Sweden, were included in "Men born in 1914-study" and followed-up at ages: 68 and 81 years. 176 survivors were examined with K-BP and SG-BP at both ages, and 104 of them with Ambulatory Blood Pressure at age 81/82. Ankle Brachial Index (ABI) was measured on both occasions, and Carotid Ultrasound at age 81.</p> <p>Results</p> <p>From age 68 to 81, mean K-BP decreased in the cohort with mean 8.3 mmHg, while SG-BP increased with 13.4 mmHg. K-BP decreased in 55% and SG-BP in 31% of the subjects. At age 81, K-BP was lower than SG-BP in 72% of subjects, and correlated to high K-BP at age 68 (r = --.22; p < .05). SG-BP at age 81 was correlated with mean ambulatory 24-h SBP (r = .480; p < .0001), daytime SBP (r = .416; p < .0001), nighttime SBP (r = .395; p < .0001), and daytime and nighttime Pulse Pressure (r = .452; p < .0001 and r = .386; p < .0001). KB-BP correlated moderately only with nighttime SBP (r = .198; p = .044), and daytime and nightime pulse pressure (r = .225; p = .021 and r = .264; p = .007). Increasing SG-BP from age 68 to 81, but not K-BP, correlated with: 24-h, daytime and nighttime SBP, and mean daytime and nighttime Pulse Pressure. Increasing SG-BP was also predicted by high B-glucose and low ABI at age 68, and correlated with carotid stenosis and low ABI age 81, and the grade of ABI decrease over 13 years.</p> <p>Conclusion</p> <p>In contrast to K-BP, values of SG-BP in octogenarians strongly correlated with Ambulatory Blood Pressure. The SG-BP decline in the last decade was rare, and increasing SG-BP better than K-BP reflected advanced atherosclerosis. It should be aware, that K-BP underdetected 46% of subjects with SG-BP equal/higher than 140 mmHg at age 81, which may lead to biased associations with risk factors due to differential misclassification by age.</p
A Semi-Physiologically Based Pharmacokinetic Model Describing the Altered Metabolism of Midazolam Due to Inflammation in Mice
- Author
- A Cleton
- A Gandhi
- AE Aitken
- B Davies
- C Kirman
- CP Granvil
- D Coutant
- E Elovaara
- E Morgan
- F Chowdhury
- G Robertson
- GK Woo
- HE Cubitt
- I Matsumoto
- J De Vries
- J Kuze
- J Kuze
- J Lu
- J Wang
- J Yang
- J-I Lee
- K Higai
- K Machavaram
- K Samuelsson
- KC Patki
- KE Thummel
- Kenneth Ruterbories
- KM Piafsky
- LJ Dickmann
- M Czerwiński
- M Martignoni
- M. Laird Forrest
- MD Perloff
- MD Reed
- N Kajikawa
- N Palmqvist
- Ninad Varkhede
- Nita Patel
- P Charles
- P Heizmann
- PK Smith
- R Bockermann
- R Kato
- RF Frye
- RP Brown
- S Kamath
- TV Masyuk
- W Zhang
- William Chang
- X Zhang
- Y Xu
- ZE Barter
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/10/2019
- Field of study
This is the author's accepted manuscript.Purpose
To investigate influence of inflammation on metabolism and pharmacokinetics (PK) of midazolam (MDZ) and construct a semi-physiologically based pharmacokinetic (PBPK) model to predict PK in mice with inflammatory disease.
Methods
Glucose-6-phosphate isomerase (GPI)-mediated inflammation was used as a preclinical model of arthritis in DBA/1 mice. CYP3A substrate MDZ was selected to study changes in metabolism and PK during the inflammation. The semi-PBPK model was constructed using mouse physiological parameters, liver microsome metabolism, and healthy animal PK data. In addition, serum cytokine, and liver-CYP (cytochrome P450 enzymes) mRNA levels were examined.
Results
The in vitro metabolite formation rate was suppressed in liver microsomes prepared from the GPI-treated mice as compared to the healthy mice. Further, clearance of MDZ was reduced during inflammation as compared to the healthy group. Finally, the semi-PBPK model was used to predict PK of MDZ after GPI-mediated inflammation. IL-6 and TNF-α levels were elevated and liver-cyp3a11 mRNA was reduced after GPI treatment.
Conclusion
The semi-PBPK model successfully predicted PK parameters of MDZ in the disease state. The model may be applied to predict PK of other drugs under disease conditions using healthy animal PK and liver microsomal data as inputs
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton 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 G
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- 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
- Aleksandrov A
- Alexakhin V
- Alexander J
- Alhusseini M
- Ali MAB Md
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JD Ruiz
- 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
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arndt T
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asghar MI
- Asilar E
- Askew A
- Assran Y
- Atakisi IO
- Atay S
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avila C
- Ayala E
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Bagliesi G
- Bahinipati S
- Baidali S
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Ball AH
- Ball F
- Ban Y
- Band R
- Banerjee S
- Banerjee S
- Bani L
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barker A
- Barnes VE
- Barney D
- Baron O
- Barone L
- Barrera C Oropeza
- Barria P
- Barrio Luna M
- Bartek R
- Barth C
- Bartok M
- Bartosik N
- Baselga M
- Baskakov A
- Bat A
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baur S
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Becerra DA Sanz
- Beck L
- Beernaert K
- Beghin D
- Behera PK
- Behnke O
- Behrens U
- Bein S
- Beirao Da Cruz E Silva C
- Belchior Batista Das Chagas E
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benussi L
- Benvenuti AC
- Beretvas A
- Bergauer T
- Berger P
- Beri SB
- Bernardes CA
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- Berry D
- Berryhill J
- Bertsche D
- Besancon M
- Beschi A
- Betts RR
- Bhandari R
- Bhardwaj A
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- Bhat MA
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
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- Bhawandeep U
- Bheesette S
- Bhopatkar V
- Bhowmik D
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- Bialkowska H
- Bian JG
- Bianchini L
- Bianco M
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- Biasini M
- Biino C
- Bilei GM
- Bilin B
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- Bin Anuar AA
- Bitioukov S
- Blanco J Martin
- Blekman F
- Blinov V
- Blobel V
- Bloch D
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- Bloom K
- Bluj M
- Blumenfeld B
- Boccali T
- Bocci A
- Bodek A
- Boimska B
- Boletti A
- Bolla G
- Bonacorsi D
- Bondu O
- Boos E
- Boran F
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- Borg J
- Borgonovi L
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bose T
- Botta C
- Botta V
- Boudoul G
- Bouhali O
- Bourilkov D
- Bouvier E
- Bowen J
- Bradmiller-Feld J
- Bragagnolo A
- Braghieri A
- Braibant-Giacomelli S
- Brainerd C
- Brandstetter J
- Brandt S
- Branson JG
- Bravo C
- Breedon R
- Breeze S
- Brew C
- Brianza L
- Brigljevic V
- Brinkerhoff A
- Brivio F
- Brochero Cifuentes JA
- Brochet S
- Brodski M
- Brom J-M
- Brondolin E
- Brooke JJ
- Brown RM
- Brun H
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- Brzhechko D
- Bucci R
- Buccilli A
- Buchanan J
- Buchmuller O
- Bundock A
- Bunin P
- Bunkowski K
- Buontempo S
- Burkett K
- Burns D
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- Burt K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butz E
- Bylinkin A
- Bylsma B
- Byszuk A
- Cabrera A
- Cabrillo IJ
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- Cakir A
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- Calderon A
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- Caminada L
- Campagnari C
- Campanini R
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- Camporesi T
- Candelise V
- Canelli MF
- Canepa A
- Cankocak K
- Capiluppi P
- Caputo C
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- Carlsmith D
- Carnes A
- Carrillo Montoya CA
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- Carvalho W
- Carver M
- Casarsa M
- Casasso S
- Caspart R
- Castaldi R
- Castilla-Valdez H
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- Cavallari F
- Cavallo FR
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- Ceballos G Gomez
- Cecchi C
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- Cepeda M
- Cerati GB
- Cerci S
- Cerminara G
- Cerrada M
- Chabert EC
- Chang P
- Chang YH
- Chanon N
- Chao Y
- Chaparro Sierra LF
- Chapon E
- Charaf O
- Charlot C
- Chatterjee K
- Chatterjee RM
- Chatterjee S
- Chauhan S
- Chauhan S
- Chaves J
- Chawla R
- Chazin Quero B
- Checchia P
- Chekhovsky V
- Chen G
- Chen GM
- Chen HS
- Chen KF
- Chen M
- Chen PH
- Chen X
- Chen Y
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- Chen Z
- Chenarani S
- Cheng KY
- Cheng T
- Cheng Y
- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhibra SS
- Chierici R
- Chinellato J
- Chistov R
- Chlebana F
- Cho S
- Choi S
- Choi Y
- Chou JP
- Choudhary BC
- Choudhury S
- Chowdhury S Roy
- Chu J
- Chudasama R
- Chwalek T
- Ciangottini D
- Cieri D
- Ciocca C
- Ciocci MA
- Cipriani M
- Ciriolo V
- Cirkovic P
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cockerill DJA
- Cocoros A
- Codispoti G
- Coelho E
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collaboration CMS
- Collard C
- Colling D
- Colombo F
- Cometti S
- Connor P
- Contardo D
- Conte E
- Contreras-Campana C
- Conway J
- Conway R
- Cooper SI
- Cooperstein S
- Cornelis T
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- Correia Silva G
- Cossutti F
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- Coubez X
- Couderc F
- Coughlan JA
- Courbon B
- Cousins R
- Covarelli R
- Cox B
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- Creanza D
- Cremonesi M
- Cristella L
- Csanad M
- Cucciati G
- Cuevas J
- Cuffiani M
- Cumalat JP
- Curry D
- Cussans D
- Cutts D
- Czellar S
- D'Alessandro R
- D'Alfonso M
- d'Enterria D
- D'Hondt J
- Da Costa EM
- Da Silveira GG
- Dabrowski A
- Daci N
- Dalchenko M
- Dallavalle GM
- Damarseckin S
- Damgov J
- Damiani D Dominguez
- Danilov M
- Danilov V
- Daponte V
- Das P
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- Dasgupta A
- Daskalakis G
- Dasu S
- Datta A
- Dauncey P
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- Davies G
- Davignon O
- de Barbaro P
- De Boer W
- De Bruyn I
- de Cassagnac R Granier
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- De Cosa A
- de Fatis T Tabarelli
- De Filippis N
- De Guio F
- De Jesus Damiao D
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Lima R Teixeira
- De Mattia M
- de Monchenault G Hamel
- De Oliveira Martins C
- De Oliveira A Carvalho Antunes
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- de Troconiz JF
- De Wit A
- De Wolf EA
- Deelen N
- Defranchis MM
- Deiters K
- Dejardin M
- Del Burgo R
- Del Re D
- Del Valle A Escalante
- Delaere C
- Delannoy AG
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- Delgado A
- Dell'Orso R
- Della Negra M
- Della Porta G Zevi
- Della Ricca G
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- Demina R
- Demiragli Z
- Demiroglu ZS
- Denegri D
- Depasse P
- Derdzinski M
- Dermenev A
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- Dev N
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- Dewanjee RK
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- Dhingra N
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- Di Guida S
- Di Maria R
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- Diemoz M
- Dierlamm A
- Dildick S
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- Dittmann J
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- Dragicevic M
- Dremin I
- Dreyer T
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- Dubinin M
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- Dudenas V
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- Duh YT
- Dulemba JL
- Dumanoglu I
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- Duran-Osuna MC
- Durgut S
- Duric S
- Durkin LS
- Dutt S
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- Dutta V
- Eckerlin G
- Ecklund KM
- Eerola P
- Ehataht K
- Eichhorn T
- El Mamouni H
- El Morabit K
- Elayavalli R Kunnawalkam
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- Elliott-Peisert A
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- Elumakhov D
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- Elwood A
- Eminizer N
- Endres M
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
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- Errico F
- Ershov A
- Esch T
- Espinosa TA Gomez
- Estrada C Uribe
- Etesami SM
- Eusebi R
- Evangelou I
- Evans A
- Evdokimov O
- Everaerts P
- Eysermans J
- Fabbri F
- Fabbri F
- Fabozzi F
- Faccioli P
- Fagot A
- Fallavollita F
- Fallon C
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- Fanfani A
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- Fangmeier C
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- Fasanella D
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- Faure JL
- Favart L
- Fay J
- Fedi G
- Fehling D
- Felcini M
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- Ferencek D
- Ferguson T
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- Fernandez Manteca PJ
- Fernandez Menendez J
- Fernandez Perez Tomei TR
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- Field RD
- Fienga F
- Filipovic N
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- Finger M
- Fiore L
- Fiorendi S
- Fiori F
- Fischer R
- Flacher H
- Flechl M
- Flix J
- Florent A
- Flores C
- Florez C
- Flouris G
- Flowers S
- Fluegge G
- Focardi E
- Folgueras S
- Fonseca De Souza S
- Fontaine J-C
- Ford WT
- Foudas C
- Fouz MC
- Francis B
- Francois B
- Franzoni G
- Freed S
- Freeman J
- Freer C
- Freund B
- Frueboes T
- Fruehwirth R
- Fulcher J
- Funk G
- Funk W
- Gadrat S
- Galanti M
- Galati G
- Galinhas B
- Gallinaro M
- Gallo E
- Galloni C
- Gandrajula RP
- Ganjour S
- Gao X
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- Garcia-Bellido A
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- Gary JW
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- Gasparini F
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- Gastler D
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- Gavrilov V
- Gecse Z
- Geiser A
- Gele D
- Gelli S
- Gelmi A
- Gennai S
- Geralis T
- Gerber CE
- Gerosa R
- Gershtein Y
- Geurts FJM
- Ghete VM
- Ghezzi A
- Ghosh S
- Ghosh S
- Giacomelli P
- Giammanco A
- Gianneios P
- Giannini L
- Giassi A
- Giffels M
- Gigi D
- Gilbert A
- Gilbert D
- Gill K
- Gilmore J
- Girgis S
- Givernaud A
- Glege F
- Gleyzer SV
- Gninenko S
- Go Y
- Godinovic N
- Godizov A
- Godshalk A
- Goerlach U
- Goh J
- Gokbulut G
- Gola M
- Goldouzian R
- Goldstein J
- Golf F
- Golovtsov V
- Golubev N
- Golunov A
- Golutvin I
- Gomber B
- Gomez G
- Goncharov M
- Gonzalez Caballero I
- Gonzalez Fernandez JR
- Gonzalez Hernandez CF
- Gonzalez Lopez O
- Gonzalez D
- Gonzalez ID Sandoval
- Gonzalez J Suarez
- Gorbounov N
- Gorski M
- Gottschalk E
- Gouskos L
- Gouzevitch M
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- 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 dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at 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
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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 strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
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- Aarrestad TK
- Aarup Petersen H
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- Yumiceva F
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- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeinali M
- Zenaiev O
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
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- 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
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
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- Abbrescia M
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- Wichmann K
- Wickramage N
- Wiederkehr SA
- Wightman A
- Wilkinson R
- Williams T
- Wimpenny S
- Winer BL
- Winterbottom D
- Wisecarver A
- Wissing C
- Wittich P
- Wittmann J
- Wittmer B
- Woehrmann C
- Wolf M
- Wolf R
- Wolfe E
- Womersley WJ
- Wong K
- Wood D
- Wood J
- Woodard A
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- Wright D
- Wright J
- Wu Z
- Wulz C-E
- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
- Xiao R
- Xie S
- Xie W
- Xu Q
- Yagil A
- Yalvac M
- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
- You C
- Yu D
- 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
- Zhang J
- 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
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
- Acosta D
- Acosta JG
- Adam W
- Adams MR
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- Civinini C
- Claes DR
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- Kovac M
- Kovalchuk N
- Kovalskyi D
- Kraetschmer I
- Krammer M
- Krammer N
- Krasnikov N
- Kravchenko I
- Kreczko L
- Kreis B
- Kress T
- Krintiras G
- Krofcheck D
- Krohn M
- Krolikowski J
- Kropivnitskaya A
- Kruecker D
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- Kubota Y
- Kucher I
- Kudella S
- Kukral O
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- Kumar A
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- Kuo CM
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- Kutzner V
- Kuznetsova E
- Kwan S
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- Kyberd P
- Kyriacou S
- Kyriakis A
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- Lacroix F
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- Lagarde F
- Laird E
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- Lampen T
- Lanaro A
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- Landsberg G
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- Meneguzzo AT
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- Mikulec I
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- Murillo Quijada JA
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- Neutelings I
- Newbold DM
- Newman HB
- Ngadiuba J
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- Niedziela M
- Niemeyer CEN
- Nikitenko A
- Niu X
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- Novaes SF
- Nowack A
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- Obertino MM
- Obraztsov S
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- Ogul H
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- Oh SB
- Oh YD
- Ojalvo I
- Okhotnikov V
- Olaiya E
- Oliveros S
- Olivito D
- Olkar TM
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- Olsson MLV
- Olszewski M
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- Oreshkin V
- Orfanelli S
- Organtini G
- Orimoto T
- Oropeza Barrera C
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- Paganis E
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- Palencia Cortezon E
- Palichik V
- Palla F
- Palladino V
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- Pandolfi F
- Paneva MI
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- Paoletti S
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- Papadopoulos I
- Papakrivopoulos I
- Papavergou I
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- Pardos CD
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- Perloff A
- Pernie L
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- Perrin G
- Perrotta A
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- Perry T
- Peruzzi M
- Pesaresi M
- Petkov P
- Petrilli A
- Petrov V
- Petrucciani G
- Petyt D
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- Piroue P
- Pistone C
- Pitters FM
- Pitzl D
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- Planer M
- Pol ME
- Pompili A
- Pook T
- Pooth O
- Popov A
- Popov V
- Postiau N
- Potenza R
- Poudyal N
- Poyraz D
- Pozdnyakov A
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- Prado Da Silva WL
- Preiato F
- Presilla M
- Preuten M
- Prieels C
- Primavera F
- Priyanka P
- Prokofyev O
- Prosper H
- Psallidas A
- Ptochos F
- Puerta Pelayo J
- Pugliese G
- Puljak I
- Purohit A
- Pyskir A
- Python Q
- Qian SJ
- Qiu H
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- Rabady D
- Rabbertz K
- Racz A
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- Radburn-Smith BC
- Radogna R
- Radziej M
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- Rahatlou S
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- Raics P
- Raidal M
- Rakness G
- Ramirez-Garcia M
- Ramirez-Sanchez G
- Rander J
- Rane A
- Ranieri A
- Ranjan K
- Ranken E
- Rankin D
- Rappoccio S
- Raspereza A
- Rastogi A
- Rathjens D
- Ratti SP
- Rauch MP
- Rauco G
- Ravera F
- Raymond DM
- Razis PA
- Re V
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- Rebello Teles P
- Redjimi R
- Redondo I
- Regnard S
- Reichmann M
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- Reimers A
- Reinsvold A
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- Reissel C
- Reithler H
- Rembser J
- Ressegotti M
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- Rodozov M
- Rodrigo T
- Rodriguez Bouza V
- Rogan C
- Roguljic M
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- Rohe T
- Rohlf J
- Rohringer H
- Roland C
- Roland G
- Rolandi G
- Romeo F
- Romero A
- Romero L
- Ronchese P
- Roozbahani B
- Rorie J
- Rose A
- Rosenzweig D
- Roskas C
- Roskes J
- Rosowsky A
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- Rossi AM
- Rossin R
- Rout PK
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- Ruggles T
- Ruini D
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Ruspa M
- Russo L
- Ryd A
- Rykaczewski H
- Ryutin R
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- Safronov G
- Saggio A
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- Salama E
- Salazar Ibarguen HA
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- Saltzberg D
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- Salvatico R
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- Sanchez Rosas LJ
- Sanchez MCDLB
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- Sandeep K
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- Santocchia A
- Santoro A
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- Sauvan JB
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- Schmitt MH
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- Schoefbeck R
- Schomakers C
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- Schroeder M
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- Schulz J
- Schumann S
- Schwandt J
- Schwanenberger C
- Schweiger K
- Schwick C
- Sciacca C
- Scodellaro L
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- Seez C
- Segura Delgado MA
- Seidel M
- Seitz C
- Seixas J
- Sekmen S
- Selvaggi G
- Selvaggi M
- Sen S
- Seo SH
- Sert H
- Sevilla MF
- Sexton-Kennedy E
- Sguazzoni G
- Shabanov A
- Shah A
- Shah MA
- Shaheen SM
- Shalhout S
- Sharan M
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- Sharma A
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- Sharma V
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- Shchutska L
- Sheffield D
- Sheldon P
- Shepherd-Themistocleous CH
- Shevchenko R
- Shi K
- Shi M
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- Shmatov S
- Shoaib M
- Shopova M
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- Shvetsov I
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- Siado JE
- Siddireddy P
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- Silva P
- Silvestris L
- Simonetto F
- Simonis HJ
- Singh A
- Singh B
- Singh G
- Singh JB
- Sinthuprasith T
- Sirois Y
- Siroli GP
- Sirunyan AM
- Skatchkov N
- Skinnari L
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- Skovpen Y
- Skuja A
- Slabospitskii S
- Smirnov I
- Smirnov V
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- Smith WH
- Snow GR
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- Sola V
- Solano A
- Soldi D
- Somalwar S
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- Spalding WJ
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- Spiegel L
- Spiezia A
- Spiga D
- Spiridonov A
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- Starodumov A
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- Stephans GSF
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- Suarez I
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- Sulimov V
- Sultanov G
- Summers S
- Sumorok K
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- Suranyi O
- Susa T
- Suwonjandee N
- Swain SK
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- Syarif R
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- Taroni S
- Tatar K
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- Tavernier S
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- Taylor D
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- Taylor L
- Tekten S
- Tenchini R
- Teodorescu L
- Terkulov A
- Teroerde M
- Teyssier D
- Thakur S
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- Thueer S
- Tiko A
- Tiras E
- Tishelman-charny A
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- Titterton A
- Tiwari PC
- Tkaczyk S
- Tlisov D
- Tok UG
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- Tomalin IR
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- Tonelli Manganote EJ
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- Tonjes MB
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- Triossi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troshin S
- Trovato M
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- Tsipolitis G
- Tsirou A
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- Turkcapar S
- Turkot O
- Tuuva T
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- Tytgat M
- Tyurin N
- Uchida K
- Ujvari B
- Ulmer KA
- Ulrich R
- Undleeb S
- Uplegger L
- Uribe Estrada C
- Usai E
- Uvarov L
- Uzunian A
- Vaandering EW
- Vagnerini A
- Vai I
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- Valuev V
- Vami TA
- Van de Klundert M
- Van Doninck W
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- Van Hove P
- Van Mechelen P
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- Van Onsem GP
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- Vanlaer P
- Vannerom D
- Varela J
- Varelas N
- Vartak A
- Vavilov S
- Vazquez Valencia F
- Vazzoler F
- Veckalns V
- Veelken C
- Velasco M
- Velde CV
- Velicanu D
- Velkovska J
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- Venditti R
- Venturi A
- Verbeke W
- Verdini PG
- Veres GI
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- Vermassen B
- Vernieri C
- Verweij M
- Verwilligen P
- Verzetti M
- Verzocchi M
- Veszpremi V
- Vesztergombi G
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Vilela Pereira A
- Viliani L
- Virdee T
- Virdi AK
- Viret S
- Vischia P
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- Vlasov E
- Vlimant JR
- Voevodina E
- Volkov A
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- Volobouev I
- Vormwald B
- Vorobiev I
- Vorobyev A
- Voutilainen M
- Voytishin N
- Wadud MA
- Wagner SR
- Walczak M
- Walia G
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- Walsh R
- Waltenberger W
- Wamorkar T
- Wang B
- Wang D
- Wang F
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- Wang Q
- Wang Q
- Wang S
- Wang S
- Wang TW
- Wang X
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- Wang Z
- Waqas M
- Wardle N
- Wayand S
- Wayne M
- Weber HA
- Weber M
- Wei H
- Weiler T
- Weinberg M
- Wen Y
- West C
- Wetzel J
- Whitbeck A
- Wichmann K
- Wickramage N
- Wiederkehr SA
- Wightman A
- Wilkinson R
- Williams T
- Wimpenny S
- Winer BL
- Winterbottom D
- Wisecarver A
- Wissing C
- Wittich P
- Wittmann J
- Wittmer B
- Woehrmann C
- Wolf M
- Wolf R
- Wolfe E
- Womersley WJ
- Wong K
- Wood D
- Wood J
- Woodard A
- Woods N
- Wright D
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- Wu Z
- Wulz C-E
- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
- Xiao R
- Xie S
- Xie W
- Xu Q
- Yagil A
- Yalvac M
- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
- Yu D
- 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
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- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- 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
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
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- Acosta JG
- Acosta M Vazquez
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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
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