120 research outputs found
Randomized clinical trial of surgery versus conservative therapy for carpal tunnel syndrome [ISRCTN84286481]
- Author
- A Cheadle
- A Osman
- AA Gerritsen
- AA Gerritsen
- AA Gerritsen
- AG Filler
- AR Bonebrake
- D Campion
- D Rempel
- D Sen
- DF Reinert
- DF Salerno
- DS Cho
- DW Levine
- ES Michael
- GR Ebenbichler
- GS Phalen
- H Flor
- H Garland
- H Ozdogan
- HL Lew
- HM Finestone
- I Atroshi
- J Bruske
- J Ellis
- JA Turner
- JB Saunders
- JC MacDermid
- JC Stevens
- JG Jarvik
- JG Jarvik
- JG Jarvik
- JM Ellis
- JM Ellis
- JM Ellis
- JM Ellis
- JN Katz
- JN Katz
- JN Katz
- JN Katz
- JN Katz
- JN Katz
- JW Dammers
- KA Glowacki
- L Bessette
- L Bessette
- LM Rozmaryn
- LR Derogatis
- LR Derogatis
- LR Derogatis
- LR Robinson
- M Feuerstein
- M Harrast
- M Stransky
- MA Vargas Busquets
- MH Chang
- MH Chang
- MJ Concannon
- MJ Sullivan
- MS Garfinkel
- N Kanaan
- P Girlanda
- PA Nathan
- PT Davis
- PT Davis
- R Celiker
- RG Marx
- RJ Verdugo
- RJ Volk
- RM Szabo
- RT Katz
- S Herskovitz
- SM Wong
- W Sequeira
- WE Pryse-Phillips
- Publication venue
- BioMed Central
- Publication date
- 01/01/2005
- Field of study
BACKGROUND: Conservative treatment remains the standard of care for treating mild to moderate carpal tunnel syndrome despite a small number of well-controlled studies and limited objective evidence to support current treatment options. There is an increasing interest in the usefulness of wrist magnetic resonance imaging could play in predicting who will benefit for various treatments. METHOD AND DESIGN: Two hundred patients with mild to moderate symptoms will be recruited over 3 1/2 years from neurological surgery, primary care, electrodiagnostic clinics. We will exclude patients with clinical or electrodiagnostic evidence of denervation or thenar muscle atrophy. We will randomly assign patients to either a well-defined conservative care protocol or surgery. The conservative care treatment will include visits with a hand therapist, exercises, a self-care booklet, work modification/ activity restriction, B6 therapy, ultrasound and possible steroid injections. The surgical care would be left up to the surgeon (endoscopic vs. open) with usual and customary follow-up. All patients will receive a wrist MRI at baseline. Patients will be contacted at 3, 6, 9 and 12 months after randomization to complete the Carpal Tunnel Syndrome Assessment Questionnaire (CTSAQ). In addition, we will compare disability (activity and work days lost) and general well being as measured by the SF-36 version II. We will control for demographics and use psychological measures (SCL-90 somatization and depression scales) as well as EDS and MRI predictors of outcomes. DISCUSSION: We have designed a randomized controlled trial which will assess the effectiveness of surgery for patients with mild to moderate carpal tunnel syndrome. An important secondary goal is to study the ability of MRI to predict patient outcomes
Changes in Scoliosis Patient and Parental Assessment of Mental Health in the Course of Cheneau Brace Treatment Based on the Strengths and Difficulties Questionnaire
- Author
- A Apter
- A Rinella
- A Thompson
- AE Oestreich
- AG Aulisa
- BV Reamy
- D Boyd
- D Hearst
- Ewa Misterska
- F Viviani
- FM Smith
- H Brosnan
- H Matsumoto
- J Mazur
- J Peltonen
- J Roberts
- J Zhang
- JE Lonstein
- JO Sanders
- Joanna Latuszewska
- JW Roach
- Katarzyna Adamczyk
- KD Koch
- KH Bridwell
- LP D'Andrea
- M Takemitsu
- M Tones
- Maciej Glowacki
- MB Dobbs
- MJ Donnelly
- MP McCabe
- N Rumsey
- N Rumsey
- NH Miller
- P Trobisch
- PL Smith
- R Buchanan
- R Goodman
- R Goodman
- SF White
- WE MacLean Jr
- WJ Kane
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
International Consensus Statement on Rhinology and Allergy: Rhinosinusitis
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- Aanaes K
- Abadie WM
- Abi Najm S
- Abigail P
- Abrahams JJ
- Abrass LJ
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- Abuzeid WM
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- Achar P
- Ackerhans M
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- Agache I
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- Ahn CN
- Ahn HJ
- Ahn JC
- Ahn SH
- Ahovuo‐Saloranta A
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- Akbari E
- Akdis CA
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- Akiyama K
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- Al Komser MK
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- Alandejani T
- Alanin MC
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- Kern RC
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- Keswani A
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- Kim JH
- Kim JH
- Kim JS
- Kim JY
- Kim J‐Y
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- Kong IG
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- Koskinen A
- Koteswara CM
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- Koutsourelakis I
- Kouzaki H
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- Orlandi RR
- Ostovar A
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- Ozturan A
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- Park D‐Y
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- Park SM
- Parma V
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- Pasaje CF
- Pasaje CF
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- Passali D
- Passali D
- Passali D
- Passàli D
- Passàli D
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- Patel NA
- Patel NN
- Patel VS
- Patel ZM
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- Patou J
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- Payne SC
- Payne SJ
- Pearlman AN
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- Peng Y
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- Penttila M
- Perez‐Novo CA
- Peric A
- Peric A
- Perica A
- Perić A
- Perkasa MF
- Perloff JR
- Persson EK
- Peters AT
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- Pfaar O
- Pfaar O
- Pfaar O
- Pham V
- Phillips KM
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- Philpott C
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- Pimenta F
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- Pinto Bezerra Soter AC
- Pinto JM
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- Poachanukoon O
- Poetker DM
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- Ponikau JU
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- Porter PC
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- Prajapati DP
- Prickett KK
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- Principi N
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- Pumhirun P
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- Quintanilla‐Dieck L
- Quinti I
- Qvarnberg Y
- Rabago D
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- Rachelefsky GS
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- Ragab A
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- Ramakrishnan V
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- Ramanathan M
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- Reh DD
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- Ricciardolo FLM
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- Rosenfeld RM
- Rostkowska‐Nadolska B
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- Rostkowska‐Nadolska BLM
- Rotenberg BW
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- Rowan NR
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- Roxbury CR
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- Scangas GA
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- Scheinberg PA
- Schenkel E
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- Scheuller MC
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- Schmidt F
- Schneider S
- Schreiber CP
- Schubert MS
- Schwartz HJ
- Schwartz JS
- Schwarzbach HL
- Schwitzguébel AJ‐P
- Scott JR
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- Sedaghat AR
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- Sedaghat AR
- Seiberling K
- Seiberling KA
- Seiberling KA
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- Sejima T
- Sella GCP
- Sener M
- Senior BA
- Senior BA
- Senturk M
- Seppanen M
- Seresirikachorn K
- Servat JJ
- Seshadri S
- Sethi DS
- Sethi N
- Sethi RKV
- Sethi S
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- Settipane RA
- Setzen G
- Seybt MW
- Seys SF
- Shaari J
- Shah GB
- Shah SA
- Shaikh N
- Shaikh N
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- Shaikh N
- Shak S
- Shamji MH
- Shanbhag S
- Shapiro AJ
- Shapiro GG
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- Sharif‐Askari FS
- Sharma P
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- Sharp HJ
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- Shin HW KD
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- Shinkwin CA
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- Siedek V
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- Siegel GJ
- Sieskiewicz A
- Sikand A
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- Silveira MLC
- Silverman RA
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- Singhal D
- Singla G
- Sintobin I
- Sirikci A
- Sitarek P
- Siu J
- Sivaci R
- Sjogren PP
- Slavin RG
- Sleigh MA
- Sleigh MA
- Small CB
- Smith A
- Smith KA
- Smith KA
- Smith KA
- Smith KA
- Smith KA
- Smith KA
- Smith SS
- Smith SS
- Smith T
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snow DG
- Snyderman CH
- Sohn HG
- Sohn JH
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
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- Soler ZM
- Song W
- Sonnet MH
- Soteres DF
- Soudry E
- Southwood JE
- Sowerby LJ
- Soyka MB
- Spencer LA
- Speth MM
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- Sreenath SB
- Srisomboon Y
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- Steelant B
- Steele TO
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- Steinke JW
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- Stelter K
- Stelter K
- Stentzel S
- Stern‐Shavit S
- Stevens PR
- Stevens WW
- Stevens WW
- Stevens WW
- Stevens WW
- Stevens WW
- Stevens WW
- Stevenson DD
- Stevenson DD
- Stewart RA
- Stjarne P
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- Stjarne P
- Stjarne P.
- Stokken J
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- Stolovitzky JP
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- Strauss G
- Stringer SP
- Stryjewska‐Makuch G
- Su MC
- Subramanian HN
- Succar EF
- Sugimoto I
- Sugino T
- Suh JD
- Sullivan PW
- Sultan B
- Sunadome H
- Sundaresan AS
- Sunkaraneni VS
- Suzuki S
- Svider PF
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- Swanson PB
- Sweis AM
- Swierczynska‐Krepa M
- Sykes DA
- Sylvester DC
- Szaleniec J
- Szczeklik A
- Szczygielski K
- Tabaee A
- Tabaee A
- Tabaee A
- Tabrizi R
- Taccariello M
- Tahamiler R
- Tahkokallio O
- Tait S
- Tajudeen BA
- Takabayashi T
- Takabayashi T
- Takabayashi T
- Takahashi T
- Takeda K
- Takeuchi K
- Talat R
- Tam J
- Tamashiro E
- Tamashiro E
- Tammemagi CM
- Tan BK
- Tan BK
- Tan BK
- Tan BK
- Tan BK
- Tan BK
- Tan KS
- Tan KS
- Tan NC
- Tan NC
- Tan NC
- Tanaka S
- Tang C
- Tanner SB
- Tarrant BJ
- Tas M
- Taschieri S
- Taulu R
- Taulu R
- Tay TR
- Taylor MJ
- Telmesani LM
- Tesche S
- Teufelberger AR
- Tewfik MA
- Thacker NM
- Thamboo A
- Thamboo A
- Thamboo A
- Tharakan A
- Theodoraki MN
- Thilsing T
- Thomas AJ
- Thomas JK
- Thomas M
- Thomas WW
- Thulasidas P
- Tieu DD
- Tipirneni KE
- Tipirneni KE
- Tipirneni KE
- Tirelli G
- Tirelli G
- Tirumandas M
- Tizzano M
- Tizzano M
- Todman MS
- Tomassen P
- Tomassen P
- Tomassen P
- Tomassen P
- Toppila‐Salmi S
- Tos M
- Tosca MA
- Tosca MA
- Toskala E
- Tosun F
- Tournas A
- Tran Khai Hoan N
- Tripathi A
- Trompette A
- Tscopp KP
- Tsetsos N
- Turan A
- Turan A
- Turfe Z
- Turner JH
- Turner JH
- Turner JH
- Turner JH
- Turner JH
- Tyler MA
- Tyler MA
- Tyler MA
- Tyler MA
- Tzelnick S
- Ualiyeva S
- Ueda D
- Ulualp SO
- Ulualp SO
- Unlu HH
- Unsal AA
- Ural A
- Uri N
- Uri N
- Vaezi MF
- Vaidyanathan S
- Vaiman M
- Vaira LA
- Vaira LA
- Valdes CJ
- Valentine R
- Valentine R
- Valentine R
- Valera FCP
- Van Bruaene N
- Van Crombruggen K
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- Van Der Veen J
- Van der Veken P
- Van Doremalen N
- Van Gerven L
- Van Zele T
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- Van Zele T
- Van Zele T
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- Varvyanskaya A
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- Vaughan C
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- Vceva A
- Velasquez N
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- Venekamp RP
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- Veskitkul J
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- Videler WJ
- Villari CR
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- Zielinska‐Blizniewska H
- Zou L
- Zuckerman JD
- Zurlo JJ
- Zuskin E
- Čulig J
- Publication venue
- 'Wiley'
- Publication date
- 01/01/2021
- Field of study
Background: The 5 years since the publication of the first International Consensus Statement on Allergy and Rhinology: Rhinosinusitis (ICAR‐RS) has witnessed foundational progress in our understanding and treatment of rhinologic disease. These advances are reflected within the more than 40 new topics covered within the ICAR‐RS‐2021 as well as updates to the original 140 topics. This executive summary consolidates the evidence‐based findings of the document. Methods: ICAR‐RS presents over 180 topics in the forms of evidence‐based reviews with recommendations (EBRRs), evidence‐based reviews, and literature reviews. The highest grade structured recommendations of the EBRR sections are summarized in this executive summary. Results: ICAR‐RS‐2021 covers 22 topics regarding the medical management of RS, which are grade A/B and are presented in the executive summary. Additionally, 4 topics regarding the surgical management of RS are grade A/B and are presented in the executive summary. Finally, a comprehensive evidence‐based management algorithm is provided. Conclusion: This ICAR‐RS‐2021 executive summary provides a compilation of the evidence‐based recommendations for medical and surgical treatment of the most common forms of RS
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- Xiao M
- Xie S
- Xie W
- Yagil A
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- Yan F
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- Yanes E
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- Yang UK
- Yang Y
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yi K
- Yi R
- Yigitbasi E
- Yockey H
- Yohay R
- Yoo HD
- Yoo J
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu I
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yusuff I
- Zabi A
- Zabolotny W
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zaza A
- Zecchinelli AG
- Zehetner P
- Zeinali M
- Zejdl P
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Y
- Zhizhin I
- Zhokin A
- Zhou C
- Zhu RY
- Ziemons T
- Zilizi G
- Zimermmane Castro Santos A
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- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
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- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- Elsevier
- Publication date
- 02/02/2024
- Field of study
Data availability:
Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in “CMS data preservation, re-use and open access policy” available online at: https://cms-docdb.cern.ch/cgi-bin/PublicDocDB/RetrieveFile?docid=6032&filename=CMSDataPolicyV1.2.pdf&version=2 .A preprint of this article is available online at arXiv:2311.03261v2 [hep-ex] https://arxiv.org/abs/2311.03261v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/TOP-22-010 (CMS Public Pages)A search is presented for new Higgs bosons in proton-proton (pp) collision events in which a same-sign top quark pair is produced in association with a jet, via the pp → tH/A → tt¯c and pp → tH/A → tt¯u processes. Here, H and A represent the extra scalar and pseudoscalar boson, respectively, of the second Higgs doublet in the generalized two-Higgs-doublet model (g2HDM). The search is based on pp collision data collected at a center-of-mass energy of 13 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 138 fb−1. Final states with a same-sign lepton pair in association with jets and missing transverse momentum are considered. New Higgs bosons in the 200-1000 GeV mass range and new Yukawa couplings between 0.1 and 1.0 are targeted in the search, for scenarios in which either H or A appear alone, or in which they coexist and interfere. No significant excess above the standard model prediction is observed. Exclusion limits are derived in the context of the g2HDM.SCOAP3
Recommended from our members
Measurement of energy correlators inside jets and determination of the strong coupling αS(mZ)
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- Aarup Petersen H
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- Yuldashev BS
- Yusuff I
- Zabi A
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- Zacharopoulou A
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- Zalewski P
- Zanetti M
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- Zeuner WD
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- Zilizi G
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- Zoi I
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- Zorbilmez C
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- American Physical Society (APS)
- Publication date
- 14/08/2024
- Field of study
A preprint version of this article is available at arXiv:2402.13864v2 [hep-ex], https://arxiv.org/abs/2402.13864 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/SMP-22-015 (CMS Public Pages). Report number: CMS-SMP-22-015, CERN-EP-2024-010 .Energy correlators that describe energy-weighted distances between two or three particles in a hadronic jet are measured using an event sample of √ = 13 TeV proton-proton collisions collected by the CMS experiment and corresponding to an integrated luminosity of 36.3 fb^−1. The measured distributions are consistent with the trends in the simulation that reveal two key features of the strong interaction: confinement and asymptotic freedom. By comparing the ratio of the measured three- and two-particle energy correlator distributions with theoretical calculations that resum collinear emissions at approximate next-to-next-to-leading-logarithmic accuracy matched to a next-to-leading-order calculation, the strong coupling is determined at the boson mass: () = 0.1229+0.0040 −0.0050, the most precise () value obtained using jet substructure observables.SCOAP3
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- Author
- Aarrestad TK
- Aarup Petersen H
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- Zhou C
- Zhu RY
- Ziemons T
- Zilizi G
- Zimermmane Castro Santos A
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 19/03/2024
- Field of study
A preprint version of the article is available at arXiv:2312.07484v3 [hep-ex], https://arxiv.org/abs/2312.07484 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/EXO-21-013 (CMS Public Pages)A search for long-lived heavy neutral leptons (HNLs) is presented, which considers the hadronic final state and coupling scenarios involving all three lepton generations in the 2-20 GeV HNL mass range for the first time. Events comprising two leptons (electrons or muons) and jets are analyzed in a data sample of proton-proton collisions, recorded with the CMS experiment at the CERN LHC at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb−1. A novel jet tagger, based on a deep neural network, has been developed to identify jets from an HNL decay using various features of the jet and its constituent particles. The network output can be used as a powerful discriminating tool to probe a broad range of HNL lifetimes and masses. Contributions from background processes are determined from data. No excess of events in data over the expected background is observed. Upper limits on the HNL production cross section are derived as functions of the HNL mass and the three coupling strengths VℓN to each lepton generation ℓ and presented as exclusion limits in the coupling-mass plane, as lower limits on the HNL lifetime, and on the HNL mass. In this search, the most stringent limit on the coupling strength is obtained for pure muon coupling scenarios; values of |VμN|2 > 5 (4) × 10−7 are excluded for Dirac (Majorana) HNLs with a mass of 10 GeV at a confidence level of 95% that correspond to proper decay lengths of 17 (10) mm.SCOAP3
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- Zilizi G
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez CR
- Publication venue
- Springer Nature
- Publication date
- 04/09/2024
- Field of study
A preprint version of the article is available at: arXiv:2402.15366v2 [physics.ins-det], https://arxiv.org/abs/2402.15366 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/MLG-23-001 (CMS Public Pages). Report numbers: CMS-MLG-23-001, CERN-EP-2023-303.Data Availability: No datasets were generated or analyzed during the current study.Computing demands for large scientific experiments, such as the CMS experiment at the CERN LHC, will increase dramatically in the next decades. To complement the future performance increases of software running on central processing units (CPUs), explorations of coprocessor usage in data processing hold great potential and interest. Coprocessors are a class of computer processors that supplement CPUs, often improving the execution of certain functions due to architectural design choices. We explore the approach of Services for Optimized Network Inference on Coprocessors (SONIC) and study the deployment of this as-a-service approach in large-scale data processing. In the studies, we take a data processing workflow of the CMS experiment and run the main workflow on CPUs, while offloading several machine learning (ML) inference tasks onto either remote or local coprocessors, specifically graphics processing units (GPUs). With experiments performed at Google Cloud, the Purdue Tier-2 computing center, and combinations of the two, we demonstrate the acceleration of these ML algorithms individually on coprocessors and the corresponding throughput improvement for the entire workflow. This approach can be easily generalized to different types of coprocessors and deployed on local CPUs without decreasing the throughput performance. We emphasize that the SONIC approach enables high coprocessor usage and enables the portability to run workflows on different types of coprocessors.SCOAP3. Open access funding provided by CERN (European Organization for Nuclear Research
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Search for new heavy resonances decaying to WW, WZ, ZZ, WH, or ZH boson pairs in the all-jets final state in proton-proton collisions at s = 13 TeV
- Author
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- Aarup Petersen H
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- Yockey H
- Yohay R
- Yoo HD
- Yoo J
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu I
- Yu PR
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yumiceva F
- Yusuff I
- Zabi A
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Y
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu RY
- Ziemons T
- Zimermmane Castro Santos A
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- Elsevier
- Publication date
- 26/02/2023
- Field of study
A preprint version of this article is available at arXiv:2210.00043v2 [hep-ex], https://arxiv.org/abs/2210.00043v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables, including additional supplementary figures, can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/B2G-20-009 (CMS Public Pages). Report number: CMS-B2G-20-009, CERN-EP-2022-152.Data availability: see: https://cms-results.web.cern.ch/cms-results/public-results/publications/B2G-20-009 .A search for new heavy resonances decaying to WW, WZ, ZZ, WH, or ZH boson pairs in the all-jets final state is presented. The analysis is based on proton-proton collision data recorded by the CMS detector in 2016-2018 at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of 138 fb^{-1}. The search is sensitive to resonances with masses between 1.3 and 6 TeV, decaying to bosons that are highly Lorentz-boosted such that each of the bosons forms a single large-radius jet. Machine learning techniques are employed to identify such jets. No significant excess over the estimated standard model background is observed. A maximum local significance of 3.6 standard deviations, corresponding to a global significance of 2.3 standard deviations, is observed at masses of 2.1 and 2.9 TeV. In a heavy vector triplet model, spin-1 Z' and W' resonances with masses below 4.8 TeV are excluded at the 95% confidence level (CL). These limits are the most stringent to date. In a bulk graviton model, spin-2 gravitons and spin-0 radions with masses below 1.4 and 2.7 TeV, respectively, are excluded at 95% CL. Production of heavy resonances through vector boson fusion is constrained with upper cross section limits at 95% CL as low as 0.1 fb.SCOAP3
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Evidence for tWZ production in proton-proton collisions at √s=13 TeV in multilepton final states
- Author
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- Yalvac M
- Yan F
- Yan X
- Yang H
- Yang S
- Yang TJ
- Yang UK
- Yang Y
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yi K
- Yi R
- Yigitbasi E
- Yockey H
- Yohay R
- Yoo HD
- Yoo J
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu I
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yusuff I
- Zabi A
- Zabolotny W
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zaza A
- Zecchinelli AG
- Zehetner P
- Zeinali M
- Zejdl P
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Y
- Zhizhin I
- Zhokin A
- Zhou C
- Zhu RY
- Ziemons T
- Zilizi G
- Zimermmane Castro Santos A
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- Elsevier BV
- Publication date
- 21/06/2024
- Field of study
Data availability - https://www.sciencedirect.com/science/article/pii/S0370269324003733?via%3Dihub#dav0001 [Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS data preservation, re-use and open access policy (https://cms-docdb.cern.ch/cgi-bin/PublicDocDB/RetrieveFile?docid=6032&filename=CMSDataPolicyV1.2.pdf&version=2)]The first evidence for the standard model production of a top quark in association with a W boson and a Z boson is reported. The measurement is performed in multilepton final states, where the Z boson is reconstructed via its decays to electron or muon pairs. At least one W boson, associated or from top quark decay, decays leptonically, too. The analysed data were recorded by the CMS experiment at the CERN LHC in 2016–2018 in proton-proton collisions at √s=13 TeV, and correspond to an integrated luminosity of 138 fb−1. The measured cross section is 354±54(stat)±95(syst) fb, and corresponds to a statistical significance of 3.4 standard deviations.SCOAP
Recommended from our members
Search for Higgs boson decays to a Z boson and a photon in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
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- 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 Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu RY
- Ziemons T
- Zipper N
- 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
- Springer Nature on behalf of SISSA
- Publication date
- 01/08/2022
- Field of study
A preprint version of the article is available at arXiv:2204.12945v2 [hep-ex], https://arxiv.org/abs/2204.12945v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-19-014 (CMS Public Pages). Report number: CMS-HIG-19-014, CERN-EP-2022-019.Results are presented from a search for the Higgs boson decay H → Zγ, where Z → ℓ+ℓ− with ℓ = e or μ. The search is performed using a sample of proton-proton (pp) collision data at a center-of-mass energy of 13 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 138 fb^{−1}. Events are assigned to mutually exclusive categories, which exploit differences in both event topology and kinematics of distinct Higgs production mechanisms to enhance signal sensitivity. The signal strength μ, defined as the product of the cross section and the branching fraction [σ(pp → H)B(H → Zγ)] relative to the standard model prediction, is extracted from a simultaneous fit to the ℓ+ℓ−γ invariant mass distributions in all categories and is found to be μ = 2.4 ± 0.9 for a Higgs boson mass of 125.38 GeV. The statistical significance of the observed excess of events is 2.7 standard deviations. This measurement corresponds to σ(pp → H)B(H → Zγ) = 0.21 ± 0.08 pb. The observed (expected) upper limit at 95% confidence level on μ is 4.1 (1.8). The ratio of branching fractions B(H → Zγ)/B(H → γγ) is measured to be 1.5 +0.7−0.6, which agrees with the standard model prediction of 0.69 ± 0.04 at the 1.5 standard deviation level.SCOAP3
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