190 research outputs found
Hospitalisation with Infection, Asthma and Allergy in Kawasaki Disease Patients and Their Families: Genealogical Analysis Using Linked Population Data
- Author
- A Elixhauser
- A Harnden
- A Read
- AH Rowley
- AL Baker
- Angeline M. Loh
- CD Holman
- CL Brosius
- D Burgner
- D Burgner
- David P. Burgner
- DL Worthley
- EJ Glasson
- ES Selamet Tierney
- FJ Stanley
- FJ Tsai
- HC Kuo
- IR Mackay
- J Kimura
- JA Royle
- JC Burns
- JJ Kim
- JM Anaya
- JW Newburger
- K Ding
- Kim W. Carter
- KS Carville
- LM Maier
- Lyle J. Palmer
- Marie-Pierre Dubé
- MH Biezeveld
- MH Biezeveld
- MP Glode
- N Chahal
- Nicole M. Warrington
- NM Nielsen
- PC Sham
- R Ihaka
- R Uehara
- RC Gualano
- RC Holman
- Rebecca J. Webster
- RR Dietert
- S Matsuoka
- S Sato
- SM Benseler
- Sophie Zaloumis
- T Matsubara
- Taco W. Kuijpers
- TW Kuijpers
- V Gee
- WK Liew
- Y Fujita
- Y Onouchi
- Y Shikishima
- YF Cheung
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Background: Kawasaki disease results from an abnormal immunological response to one or more infectious triggers. We hypothesised that heritable differences in immune responses in Kawasaki disease-affected children and their families would result in different epidemiological patterns of other immune-related conditions. We investigated whether hospitalisation for infection and asthma/allergy were different in Kawasaki disease-affected children and their relatives. Methods/Major Findings: We used Western Australian population-linked health data from live births (1970-2006) to compare patterns of hospital admissions in Kawasaki disease cases, age- and sex-matched controls, and their relatives. There were 295 Kawasaki disease cases and 598 age- and sex-matched controls, with 1,636 and 3,780 relatives, respectively. Compared to controls, cases were more likely to have been admitted at least once with an infection (cases, 150 admissions (50.8%) vs controls, 210 admissions (35.1%); odds ratio (OR) = 1.9, 95% confidence interval (CI) 1.4-2.6, P = 7.2×10-6), and with asthma/allergy (cases, 49 admissions (16.6%) vs controls, 42 admissions (7.0%); OR = 2.6, 95% CI 1.7-4.2, P = 1.3×10-5). Cases also had more admissions per person with infection (cases, median 2 admissions, 95% CI 1-5, vs controls, median 1 admission, 95% CI 1-4, P = 1.09×10-5). The risk of admission with infection was higher in the first degree relatives of Kawasaki disease cases compared to those of controls, but the differences were not significant. Conclusion: Differences in the immune phenotype of children who develop Kawasaki disease may influence the severity of other immune-related conditions, with some similar patterns observed in relatives. These data suggest the influence of shared heritable factors in these families
Comparative Genomics and Transcriptomics of Propionibacterium acnes
- Author
- A Holmberg
- A Liavonchanka
- A Maghnouj
- A McDowell
- AL Cogen
- Andrea Thürmer
- Antje Wollherr
- B Soderquist
- C Dessinioti
- C Holland
- DH Shin
- E Fernandez
- E Jakab
- Elzbieta Brzuszkiewicz
- EM Gribbon
- GA Churchill
- Gerhard Gottschalk
- GM Graham
- H Brüggemann
- H Falentin
- Hans B. Lomholt
- Hans-Joachim Mollenkopf
- HB Lomholt
- HE Wilcox
- HG Wood
- HK Chahal
- Holger Brüggemann
- I Nagy
- I Nagy
- J Kim
- January Weiner
- JE Miskin
- Jennifer Hüpeden
- K Engelhardt
- KE Nelson
- KS Makarova
- L Fassi Fehri
- LCW Brown
- M Gamper
- M Mujacic
- M Tech
- Malcolm James Horsburgh
- MD Farrar
- MD Farrar
- MG Jorgensen
- MG Langille
- MJ Lodes
- Mogens Kilian
- P Gruening
- R Overbeek
- R Staden
- R Wernersson
- Rolf Daniel
- S Jugeau
- S Valanne
- SA Jones
- T Tanabe
- Thomas F. Meyer
- TJ Carver
- U Jappe
- V Datta
- Y Hu
- Y Yu
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
The anaerobic Gram-positive bacterium Propionibacterium acnes is a human skin commensal that is occasionally associated with inflammatory diseases. Recent work has indicated that evolutionary distinct lineages of P. acnes play etiologic roles in disease while others are associated with maintenance of skin homeostasis. To shed light on the molecular basis for differential strain properties, we carried out genomic and transcriptomic analysis of distinct P. acnes strains. We sequenced the genome of the P. acnes strain 266, a type I-1a strain. Comparative genome analysis of strain 266 and four other P. acnes strains revealed that overall genome plasticity is relatively low; however, a number of island-like genomic regions, encoding a variety of putative virulence-associated and fitness traits differ between phylotypes, as judged from PCR analysis of a collection of P. acnes strains. Comparative transcriptome analysis of strains KPA171202 (type I-2) and 266 during exponential growth revealed inter-strain differences in gene expression of transport systems and metabolic pathways. In addition, transcript levels of genes encoding possible virulence factors such as dermatan-sulphate adhesin, polyunsaturated fatty acid isomerase, iron acquisition protein HtaA and lipase GehA were upregulated in strain 266. We investigated differential gene expression during exponential and stationary growth phases. Genes encoding components of the energy-conserving respiratory chain as well as secreted and virulence-associated factors were transcribed during the exponential phase, while the stationary growth phase was characterized by upregulation of genes involved in stress responses and amino acid metabolism. Our data highlight the genomic basis for strain diversity and identify, for the first time, the actively transcribed part of the genome, underlining the important role growth status plays in the inflammation-inducing activity of P. acnes. We argue that the disease-causing potential of different P. acnes strains is not only determined by the phylotype-specific genome content but also by variable gene expression
Volumetric and MGMT parameters in glioblastoma patients: Survival analysis
- Author
- A Kowalczuk
- A Pirzkall
- A Pirzkall
- Anastasia G Eleftheraki
- Athanasios Chatzisotiriou
- B Kaur
- BJ Pirotte
- C Nieder
- C Nieder
- CR Johnson
- D Capper
- D Shweiki
- D Xue
- DC Weber
- Despina Misailidou
- Despina Televantou
- DR Macdonald
- DT Blumenthal
- E Andreopoulou
- E Burghardt
- ER Laws
- F Earnest
- F Thiele
- FW Crawford
- G Iliadis
- GA Plataniotis
- GE Keles
- GE Keles
- George Fountzilas
- Georgios Iliadis
- GG Grabenbauer
- H Colman
- HD Segall
- J Felsberg
- J Oh
- J Welsh
- JR Flynn
- JW Jeuken
- KH Plate
- KJ Livak
- KS Tralins
- L Souhami
- M Ammirati
- M Brell
- M Chahal
- M Esteller
- M Lacroix
- M Weller
- MA Hammoud
- MC Chamberlain
- MD Piroth
- MD Piroth
- MG D' Angelo
- NJ Laperriere
- Panagiotis Selviaridis
- PC Burger
- PJ Kelly
- R Cardinale
- R Kurek
- R Martinez
- R Stupp
- R Stupp
- R Stupp
- S Kikuchi
- S Saraswathy
- SJ Hentschel
- SM Raza
- Sofia Lambaki
- T Gorlia
- V Panet-Raymond
- V Rudat
- Vassiliki Kotoula
- X Li
- Y Cao
- YY Wang
- Publication venue
- BioMed Central
- Publication date
- 01/01/2012
- Field of study
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmed A
- Ahuja S
- Aime C
- Akchurin N
- Akgun B
- Akpinar A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allen B
- Almond J
- Alvarez Gonzalez B
- Alverson G
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amendola C
- Amin N
- Amram O
- Amsler C
- Anagnostou G
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Antchev G
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Apyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Aruta C
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- Aspell P
- Atakisi IO
- Atanassov I
- Ather MW
- Attikis A
- Auffray E
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- Auzinger G
- Avati V
- Avery P
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- Ayala E
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- Azhgirey I
- Aziz T
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- Bacchetta N
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- 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
Evidence for Top Quark Production in Nucleus-Nucleus Collisions
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- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2019
- Field of study
Peer reviewe
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
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- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe
Observation of a New Excited Beauty Strange Baryon Decaying to Ξb- π+π-
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- Aarrestad TK
- Aarup Petersen H
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- Yohay R
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- Yu PR
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- Yuan S
- Yumiceva F
- Yusli MN
- 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
- Zhang H
- Zhang J
- Zhang S
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- Zhao J
- Zhizhin I
- Zhokin A
- Zhu DH
- Zhu RY
- Ziemons T
- Zientek M
- Zlebcik R
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
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- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- American Physical Society
- Publication date
- 01/01/2021
- Field of study
The Ξb-π+π- invariant mass spectrum is investigated with an event sample of proton-proton collisions at s=13 TeV, collected by the CMS experiment at the LHC in 2016-2018 and corresponding to an integrated luminosity of 140 fb-1. The ground state Ξb- is reconstructed via its decays to J/ψΞ- and J/ψΛK-. A narrow resonance, labeled Ξb(6100)-, is observed at a Ξb-π+π- invariant mass of 6100.3±0.2(stat)±0.1(syst)±0.6(Ξb-) MeV, where the last uncertainty reflects the precision of the Ξb- baryon mass. The upper limit on the Ξb(6100)- natural width is determined to be 1.9 MeV at 95% confidence level. The low Ξb(6100)- signal yield observed in data does not allow a measurement of the quantum numbers of the new state. However, following analogies with the established excited Ξc baryon states, the new Ξb(6100)- resonance and its decay sequence are consistent with the orbitally excited Ξb- baryon, with spin and parity quantum numbers JP=3/2-
A Deep Neural Network for Simultaneous Estimation of b Jet Energy and Resolution
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- Zhang S
- Zhang W
- 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
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2020
- Field of study
We describe a method to obtain point and dispersion estimates for the energies of jets arising from b quarks produced in proton-proton collisions at an energy of s = 13 TeV at the CERN LHC. The algorithm is trained on a large sample of simulated b jets and validated on data recorded by the CMS detector in 2017 corresponding to an integrated luminosity of 41 fb - 1 . A multivariate regression algorithm based on a deep feed-forward neural network employs jet composition and shape information, and the properties of reconstructed secondary vertices associated with the jet. The results of the algorithm are used to improve the sensitivity of analyses that make use of b jets in the final state, such as the observation of Higgs boson decay to b b ¯
Observation of the B-s(0) -> X(3872)phi Decay
- Author
- Aarrestad TK
- Aarup Petersen H
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- Abdullin S
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- Vorobiev I
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- Zorbilmez C
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- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2020
- Field of study
Using a data sample of proton-proton collisions at root s = 13 TeV, corresponding to an integrated luminosity of 140 fb(-1) collected by the CMS experiment in 2016-2018, the B-s(0) -> X(3872)phi decay is observed. Decays into J/psi pi(+)pi(-) and K+K- are used to reconstruct, respectively, the X(3872) and phi. The ratio of the product of branching fractions B[B-s(0) -> X(3872)phi]B[X(3872) -> J/psi pi(+)pi(-)] to the product B[B-s(0) ->psi(2S)phi]B[psi(2S) -> J/psi pi(+)pi(-)] is measured to be [2.21 +/- 0.29(stat) +/- 0.17(syst)]%. The ratio B[B-s(0) -> X(3872)phi]/B[B-0 -> X(3872)K-0] is found to be consistent with one, while the ratio B[B-s(0) -> X(3872)phi]/B[B+-> X(3872)K+] is two times smaller. This suggests a difference in the production dynamics of the X(3872) in B-0 and B(0)s meson decays compared to B+. The reported observation may shed new light on the nature of the X(3872) particle.Peer reviewe
Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of τ Leptons in pp collisions at sqrt[s]=13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullin S
- Abercrombie D
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- Lawrence J
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- Le Bihan A-C
- Lechner L
- Lecoq P
- Ledovskoy A
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- Neutelings I
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- Potenza R
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- Razis PA
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- Regnery B
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- Reichmann M
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- Reimers A
- Reinsvold Hall A
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- Reitenspiess T
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- Rejeb Sfar H
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- Ribeiro Lopes B
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- Rinkevicius A
- Ristic B
- Ristori L
- Rizzi A
- Robmann P
- Robutti E
- Rodozov M
- Rodrigo T
- Rodríguez Bouza V
- Roemer J
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- Ruiz Alvarez JD
- Ruiz-Jimeno A
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- Ryu MS
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- Rádl AJ
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- Safonov A
- Saggio A
- Sagir S
- Saha G
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- Sahasransu AR
- Sahin MÖ
- Sahu B
- Saibel A
- Saka H
- Sakulin H
- Salazar González CA
- Salazar Ibarguen HA
- Salerno R
- Salfeld-Nebgen J
- Saltzberg D
- Salur S
- Salvatico R
- Salvini P
- Salyer K
- Samalan A
- Sanchez Cruz S
- Sanchez A
- Sanchez-Hernandez A
- Sandeep K
- Sanders S
- Santanastasio F
- Santocchia A
- Santoro A
- Sanz Becerra DA
- Saoulidou N
- Saradhy R
- Sarica U
- Sarkar S
- Sarkar T
- Sarkar U
- Sathia Narayanan BV
- Saunders M
- Sauvan JB
- Savard C
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- Savoiu D
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- Savrin V
- Sawant S
- Scarfi S
- Scham M
- Scheurer V
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- Schmitt MH
- Schmitz E
- Schnepf M
- Schnetzer S
- Schroeder N
- Schröder M
- Schuh T
- Schuler SC
- Schulte JF
- Schulz J
- Schwandt J
- Schwanenberger C
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- Schütze P
- Sciacca C
- Scodellaro L
- Scott E
- Scribano A
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- Sehrawat A
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- Seidita R
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- Seith D
- Seitova D
- Seixas J
- Sekmen S
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- Selvaggi M
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- Seo H
- Sert H
- Setti F
- Sexton-Kennedy E
- Sguazzoni G
- Shafiei N
- Shah A
- Shah MA
- Shalaev V
- Shang V
- Sharan M
- Sharma A
- Sharma A
- Sharma A
- Sharma R
- Sharma S
- Sharma V
- Sharma V
- Shchablo K
- Shchedrolosiev M
- Shchelina K
- Sheldon P
- Shepherd-Themistocleous CH
- Sheplock J
- Shi K
- Shi W
- Shi Z
- Shmatov S
- Shoaib M
- Shopova M
- Shtipliyski A
- Shukla P
- Shulha S
- Shvetsov I
- Si W
- Siado JE
- Siddireddy P
- Siikonen H
- Sikdar AK
- Sikler F
- Silva Do Amaral SM
- Silva P
- Silvestris L
- Simone FM
- Simonetto F
- Simonis HJ
- Simpson F
- Simsek AE
- Singh B
- Singh JB
- Sirois Y
- Siroli GP
- Siviero F
- Skinnari L
- Skovpen K
- Skovpen Y
- Skuja A
- Slabospitskii S
- Smirnov I
- Smirnov V
- Smith C
- Smith N
- Smith VJ
- Smith WH
- Snoeys W
- Snow GR
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- Sobol A
- Soffi L
- Soha A
- Sola V
- Solano A
- Soldi D
- Somalwar S
- Song D
- Sonnadara DUJ
- Sonneveld J
- Sordini V
- Sorrentino G
- Sosa Ricardo RE
- Sosnov D
- Soto Rodríguez A
- Spagnolo P
- Spalding WJ
- Spanier S
- Sperka D
- Sphicas P
- Spiegel L
- Spiga D
- Spiropulu M
- Spitzbart D
- Srimanobhas N
- Stadie H
- Stafford D
- Stahl Leiton AG
- Stahl A
- Staiano A
- Stakia A
- Stampf V
- Starling E
- Starodumov A
- Steen A
- Steggemann J
- Steinbrück G
- Stenson K
- Stepennov A
- Stephans GSF
- Stickland D
- Stojanovic M
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- Strait J
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- Strologas J
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- Sulimov V
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- Sutantawibul C
- Swain SK
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- Sznajder A
- Sánchez Navas S
- Tabarelli de Fatis T
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- Takahashi Y
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- Tamulaitis G
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- Tavernier S
- Tavolaro VR
- Taylor D
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- Tcherniaev E
- Teague D
- Tedeschi T
- Teklishyn M
- Tekten S
- Templ S
- Tenchini R
- Teodorescu L
- Terkulov A
- Teroerde M
- Terrill W
- Teryaev O
- Tews A
- Teyssier D
- Thakur S
- Thayil SA
- Theofilatos K
- Thiel M
- Thieman J
- Thom J
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- Thomas-Wilsker J
- Tiras E
- Tishelman-Charny A
- Titov M
- Tiwari PC
- Tkaczyk S
- Tok UG
- Toldaiev O
- Tomalin IR
- Tomei TRFP
- Toms M
- Tonelli G
- Tonjes MB
- Tonon N
- Toriashvili T
- Torims T
- Tornago M
- Toropin A
- Torres Da Silva De Araujo F
- Torterotot L
- Tosi M
- Tosi S
- Touquet G
- Townsend A
- Tramontano R
- Tran NV
- Tran TT
- Trapote A
- Treille D
- Trembath-Reichert S
- Trevisani N
- Tricomi A
- Trocino D
- Trocsanyi ZL
- Tropea P
- Troshin S
- Tsamalaidze Z
- Tsatsos A
- Tsipolitis G
- Tsirou A
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Turini N
- Turkcapar S
- Tuuva T
- Tuve C
- Tytgat M
- Tyurin N
- Tziaferi E
- Uchida K
- Ujvari B
- Ulmer KA
- Ulrich R
- Uniyal R
- Uplegger L
- Urda Gómez L
- Uribe Estrada C
- Usai E
- Uvarov L
- Uzunian A
- Vaandering EW
- Vagnerini A
- Vai I
- Valencia Palomo L
- Valsecchi D
- Valuev V
- Van De Klundert M
- Van Der Linden J
- Van Doninck W
- Van Hove P
- Van Mechelen P
- Van Mulders P
- Van Onsem GP
- Van Putte S
- Van Remortel N
- Vanden Bemden M
- Vander Donckt M
- Vander Velde C
- Vanlaer P
- Varela J
- Varelas N
- Vargas Hernandez AM
- Vartak A
- Vats D
- Vazquez Valencia F
- Vazzoler F
- Veckalns V
- Veelken C
- Velasco M
- Velkovska J
- Vellidis K
- Venditti R
- Venturi A
- Verdini PG
- Veres GI
- Vermassen B
- Verwilligen P
- Veszpremi V
- Vetens W
- Viazlo O
- Vico Villalba C
- Vigilante L
- Viinikainen J
- Vila I
- Vilela Pereira A
- Viliani L
- Virdee T
- Virdi AK
- Viret S
- Vischia P
- Vit M
- Vitulo P
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vojinovic M
- Volkov A
- Volkov S
- Volobouev I
- Von Cube RF
- Vorobyev A
- Vourliotis E
- Voutilainen M
- Voytishin N
- Vámi TÁ
- Wadud MA
- Wagner SR
- Walkingshaw Pass K
- Wallny R
- Walsh R
- Waltenberger W
- Walter D
- Wamorkar T
- Wan Abdullah WAT
- Wanczyk J
- Wang B
- Wang C
- Wang D
- Wang F
- Wang H
- Wang J
- Wang J
- Wang J
- Wang L
- Wang Q
- Wang Q
- Wang S
- Wang X
- Wang Y
- Wang Z
- Wang Z
- Waqas M
- Wardle N
- Warner Z
- Wassmer M
- Watson IJ
- Wayne M
- Webb SN
- Weber HA
- Weber M
- Wei K
- Wen Y
- Wertz S
- West C
- Wezenbeek L
- Whitbeck A
- White R
- White S
- Wichmann K
- Wickramage N
- Wickramarathna DDC
- Wiedenbeck S
- Wieland S
- Wiens L
- Wightman A
- Williams A
- Williams J
- Williams T
- Willmott C
- Wilson G
- Wilson J
- Wimpenny S
- Winer BL
- Winterbottom D
- Wisecarver A
- Wissing C
- Wittich P
- Wolf R
- Wolfe E
- Wong K
- Wong WY
- Wood D
- Wozniak KA
- Wozniewski S
- Wright D
- Wu HY
- Wu Z
- Wuchterl S
- Wulz C-E
- Wunsch S
- Wyslouch B
- Würthwein F
- Xiang Y
- Xiao J
- Xiao M
- Xiao R
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yan F
- Yan X
- Yang S
- Yang S
- Yang UK
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yetkin EA
- Yi K
- Yigitbasi E
- Yohay R
- Yoo HD
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu GB
- Yu I
- Yu PR
- Yu SS
- Yuan L
- Yuan S
- 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
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu DH
- Zhu RY
- Ziemons T
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou D
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
Measurements of the inclusive and differential fiducial cross sections of the Higgs boson are presented, using the τ lepton decay channel. The differential cross sections are measured as functions of the Higgs boson transverse momentum, jet multiplicity, and transverse momentum of the leading jet in the event, if any. The analysis is performed using proton-proton collision data collected with the CMS detector at the LHC at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 138 fb^{-1}. These are the first differential measurements of the Higgs boson cross section in the final state of two τ leptons. In final states with a large jet multiplicity or with a Lorentz-boosted Higgs boson, these measurements constitute a significant improvement over measurements performed in other final states
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