99 research outputs found
Clinicopathological and prognostic significance of EGFR, VEGF, and HER2 expression in cholangiocarcinoma
- Author
- A Altimari
- A Nakeeb
- A Sandler
- A Viloria Petit
- AE Sirica
- AM Gonzalez Angulo
- BA Gusterson
- BL Strom
- BR Zetter
- C Hassan
- D Tang
- D Yoshikawa
- DE Neal
- F Leone
- G Des Guetz
- GY Gwak
- H Han
- H Hurwitz
- H Ojima
- J Tabernero
- JH Yoon
- K Endo
- K Nakazawa
- K Shirabe
- LH Sobin
- M Iwasaki
- M Ohtsuka
- M Yamamoto
- MA Olayioye
- MF Sprinzl
- ML DeOliveira
- N Hiraoka
- N Shiojiri
- N Weidner
- NW Wilkinson
- PA Philip
- RA Mohammed
- RI Nicholson
- S Hirohashi
- S Kasai
- SA Khan
- SI Aishima
- SR Hamilton
- T Kosuge
- T Shibata
- TA Sohn
- TW Huang
- Y Hida
- Y Ito
- Y Morimoto
- Y Ukita
- Y Yarden
- YH Shaib
- Publication venue
- Nature Publishing Group
- Publication date
- 01/01/2008
- Field of study
Epidermal growth factor receptor (EGFR), vascular endothelial growth factor (VEGF), and human epidermal growth factor receptor 2 (HER2) have been considered as potential therapeutic targets in cholangiocarcinoma, but no studies have yet clarified the clinicopathological or prognostic significance of these molecules. Immunohistochemical expression of these molecules was assessed retrospectively in 236 cases of cholangiocarcinoma, as well as associations between the expression of these molecules and clinicopathological factors or clinical outcome. The proportions of positive cases for EGFR, VEGF, and HER2 overexpression were 27.4, 53.8, and 0.9% in intrahepatic cholangiocarcinoma (IHCC), and 19.2, 59.2, and 8.5% in extrahepatic cholangiocarcinoma (EHCC), respectively. Clinicopathologically, EGFR overexpression was associated with macroscopic type (P=0.0120), lymph node metastasis (P=0.0006), tumour stage (P=0.0424), lymphatic vessel invasion (P=0.0371), and perineural invasion (P=0.0459) in EHCC, and VEGF overexpression with intrahepatic metastasis (P=0.0224) in IHCC. Multivariate analysis showed that EGFR expression was a significant prognostic factor (hazard ratio (HR), 2.67; 95% confidence interval (CI), 1.52–4.69; P=0.0006) and also a risk factor for tumour recurrence (HR, 1.89; 95% CI, 1.05–3.39, P=0.0335) in IHCC. These results suggest that EGFR expression is associated with tumour progression and VEGF expression may be involved in haematogenic metastasis in cholangiocarcinoma
Hepatitis reactivation in patients with rheumatic diseases after immunosuppressive therapy—a report of long-term follow-up of serial cases and literature review
- Author
- A Pyrpasopoulou
- A Tamori
- C Charpin
- C Rodriguez-Escalera
- CH Yang
- D Kishida
- D Vassilopoulos
- D Wendling
- D Wendling
- Dandan Xuan
- DU Cansu
- E Doubrawa
- E Ghrenassia
- EASL clinical practice guidelines
- G Germanidis
- G Raimondo
- GY Gwak
- H Robinson
- Hejian Zou
- HH Ryu
- I Nordgaard-Lassen
- J Cheng
- J Tan
- JH Bae
- Jiali Wang
- JL Lan
- JM Wu
- K Nakanishi
- K Watanabe
- Linyun Shao
- M Andres
- MB Carroll
- MG Anelli
- O Durmus
- P Ostuni
- PP Kaur
- R Caporali
- RP Perrillo
- S Ito
- S Mori
- SA Zanati
- SJ Chung
- T Matsumoto
- Wenhong Zhang
- WM Lee
- X Li
- X Verhelst
- Y Oshima
- Y Urata
- Yiqi Yu
- YT Cho
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Expert consensus document:Cholangiocarcinoma: current knowledge and future perspectives consensus statement from the European Network for the Study of Cholangiocarcinoma (ENS-CCA)
- Author
- A Claperon
- A Claperon
- A Evrard
- A Franchitto
- A Fritscher-Ravens
- A Fritscher-Ravens
- A Fujimoto
- A Gentilini
- A Gigliozzi
- A Jimeno
- A Kreso
- A Lamarca
- A Laquiere
- A Lautem
- A Lederer
- A Mancino
- A Menakongka
- A Nakeeb
- A Rullier
- A Saborowski
- A Sica
- A Techasen
- A Thelen
- A Thelen
- A Wannhoff
- AE Sirica
- AE Sirica
- AE Sirica
- AG Singal
- AM De Rose
- Andreas Geier
- Antonio Benedetti
- B Abu-Wasel
- B Blechacz
- B Fan
- B Goeppert
- B Juntermanns
- BL Wang
- C Benckert
- C Chuaysri
- C Gandou
- C Greenhill
- C Hahnvajanawong
- C Han
- C Levy
- C Raggi
- C Subimerb
- C Subimerb
- CB Rosen
- CD Fingas
- CD Fingas
- CH Sukowati
- Chiara Raggi
- CJ Wehrkamp
- CK Ong
- CL Leggett
- CN Yeh
- CR Ferrone
- D Alvaro
- D Alvaro
- D Alvaro
- D Alvaro
- D Alvaro
- D Hanahan
- D Liu
- D Lu
- D Sachdev
- D Sia
- D Sia
- D Tang
- D Yamada
- D Yoshikawa
- Diego F. Calvisi
- DM Harnois
- Domenico Alvaro
- DR Borger
- DS Uppal
- E Bjornsson
- E Herraez
- E Lozano
- E Lozano
- EG Huntzicker
- Eugenio Gaudio
- F Meng
- F Meng
- F Sabbatino
- G Alpini
- G Carpino
- G Carpino
- G Fava
- G Fava
- G Fava
- G Frampton
- G Morris-Stiff
- G Nuzzo
- Guido Carpino
- Guro E. Lind
- GY Gwak
- H Asakawa
- H Bismuth
- H Francis
- H Francis
- H Francis
- H Haga
- H Hasita
- H Isomoto
- H Isomoto
- H Momoi
- H Nakamura
- H Nathan
- H Okabe
- H Okabe
- H Sasaki
- H Wehbe
- H Yoon
- H Zhang
- HB Zhou
- HR Shin
- HS Ryu
- I Borbath
- I Leake
- IG Hwang
- J Bridgewater
- J Dai
- J Fevery
- J Harder
- J Hunter
- J Park
- J Rimola
- J Romagnuolo
- J Sato
- J Valle
- J Zhang
- JA Magee
- JA Roth
- Javier Vaquero
- JB Andersen
- JC Mansour
- JC Mertens
- JE Visvader
- Jesper B. Andersen
- Jesus M. Banales
- JF Mosnier
- JH Lee
- JH Yoon
- JH Yoon
- JH Yoon
- JK Heimbach
- Joachim C. Mertens
- Jose J. G. Marin
- JP Cai
- JP Lu
- JR Bledsoe
- JS Jang
- JS Ross
- JW Valle
- JY Liau
- K Andresen
- K Araki
- K Burak
- K Habara
- K Han
- K Isse
- K Leelawat
- K Nakazawa
- K Nishihara
- K Obama
- K Rycaj
- K Shirabe
- K Soreide
- K Wlcek
- KD Lindor
- Kirsten M. Boberg
- KM Boberg
- L Boulter
- L Cao
- L Fabris
- L Huang
- L Li
- L Maroni
- L Sulpice
- L Sulpice
- L Yao
- Laura Fouassier
- LK Sampson
- LM Boehm
- Luca Maroni
- M Cadamuro
- M Coufal
- M El Khatib
- M Iavarone
- M Jaiswal
- M Jaiswal
- M Kobayashi
- M Komuta
- M Komuta
- M Marzioni
- M Marzioni
- M Marzioni
- M Miyamoto
- M Nagino
- M Simbolo
- M Taniai
- Marco Marzioni
- Maria J. Perugorria
- ME Ortner
- MF Byrne
- Michael Trauner
- MJ Borad
- MJ Grainge
- MJ Gu
- MJ Liberato
- ML Deoliveira
- ML O'Connor
- MR Junttila
- MT Dill
- N Haraguchi
- N Ishimura
- N Kanno
- N Namwat
- N Razumilava
- N Tepsiri
- NJ Chiang
- NW Werneburg
- O Farges
- O Govaere
- O Govaere
- O Hyder
- P Angulo
- P Kornprat
- P Martinez-Becerra
- P Onori
- P Pawar
- P Wang
- Pietro Invernizzi
- Q Gao
- Q Zhou
- R Chapman
- R Kemmerling
- R Liu
- RC Martin
- RK Kelley
- RM Franke
- Rocio I. R. Macias
- RR Plentz
- S Aishima
- S Darwish Murad
- S Darwish Murad
- S DeMorrow
- S DeMorrow
- S Friman
- S Kobayashi
- S Lemoinne
- S Ohira
- S Rau
- S Rizvi
- S Rizvi
- S Rizvi
- S Sekiya
- S Tanaka
- S Turcan
- S Udali
- S Vander Borght
- S Yamasaki
- S Zou
- SA Gradilone
- SA Khan
- SA Khan
- SB Edge
- SC Song
- SI Grivennikov
- SJ Kim
- SK Lau
- SK Saha
- SM Ibrahim
- SM Weber
- Stuart J. Forbes
- SV Ambudkar
- SY Park
- T Andre
- T Ebata
- T Limpaiboon
- T Nakajima
- T Okusaka
- T Panichakul
- T Patel
- T Patel
- T Rosch
- T Rosch
- T Terada
- T Wu
- T Yamashita
- TF Fernandez
- TM Welzel
- Trine Folseraas
- TY Lee
- U Navaneethan
- U Navaneethan
- U Navaneethan
- U Srimunta
- V Cardinale
- V Cardinale
- V Cardinale
- V Cardinale
- V Cardinale
- V Cardinale
- Vincenzo Cardinale
- VM Zaydfudim
- W Chan-On
- W Dolak
- W Loilome
- WC Palmer
- WL Campbell
- WR Jarnagin
- WR Wu
- WT Chen
- X Ge
- X Jiang
- Y Arai
- Y Han
- Y Jiao
- Y Kim
- Y Lu
- Y Nakanuma
- Y Nakanuma
- Y Nakanuma
- Y Nakanuma
- Y Sato
- Y Sato
- Y Sato
- Y Takayama
- YM Wu
- Z Zhang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Cholangiocarcinoma (CCA) is a heterogeneous group of malignancies with features of biliary tract differentiation. CCA is the second most common primary liver tumour and the incidence is increasing worldwide. CCA has high mortality owing to its aggressiveness, late diagnosis and refractory nature. In May 2015, the "European Network for the Study of Cholangiocarcinoma" (ENS-CCA: www.enscca.org or www.cholangiocarcinoma.eu) was created to promote and boost international research collaboration on the study of CCA at basic, translational and clinical level. In this Consensus Statement, we aim to provide valuable information on classifications, pathological features, risk factors, cells of origin, genetic and epigenetic modifications and current therapies available for this cancer. Moreover, future directions on basic and clinical investigations and plans for the ENS-CCA are highlighted
Recommended from our members
Evidence for tWZ production in proton-proton collisions at √s=13 TeV in multilepton final states
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbott S
- Abbrescia M
- Abdullin S
- Abreu A
- Abu Zeid S
- Acharya H
- Acharya S
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams MR
- Adams T
- Addesa FM
- Adloff C
- Adzic P
- Aebi D
- Afanasiev S
- Agapitos A
- Agarwal G
- Agram J-L
- Aguilar-Benitez M
- Agyel D
- Ahmad A
- Ahmad M
- Ahmed A
- Aimè C
- Ajmal S
- Akchurin N
- Akgun B
- Akpinar A
- Al Kadhim A
- Albert A
- Albrecht A
- Albrecht S
- Albrow M
- Alcaraz Maestre J
- Alcerro Alcerro LF
- Aldaya Martin M
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allmond B
- Ally D
- Almond J
- Alpana A
- Alsufyani B
- Alvarez Gonzalez B
- Alves Gallo Pereira M
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Ambrozas M
- Ameen MM
- Amendola C
- Amoroso S
- Amram O
- Amsler C
- An S
- An Y
- Anagnostou G
- Andrea J
- Andreev V
- Andreev Y
- Andrejkovic JW
- Andrews MB
- Androsov K
- Anguiano J
- Antchev G
- Anthony D
- Antonello M
- Apollinari G
- Apparu D
- Appelt E
- Apresyan A
- Araujo M
- Aravind A
- Arcaro D
- Arcidiacono R
- Ardino R
- Argiro S
- Arneodo M
- Aruta C
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Assiouras P
- Atakisi IO
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awais A
- Awan MIM
- Ayala E
- Ayala G
- Aydilek O
- Azarkin M
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Babbar J
- Bacchetta N
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Bagliesi G
- Bahinipati S
- Bainbridge R
- Bak G
- Bakas G
- Bakhshiansohi H
- Bakshi AS
- Bala A
- Baldenegro Barrera C
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Bansal S
- Baradia S
- Barbagli G
- Barberis E
- Barbosa Trujillo DA
- Bardelli G
- Bargassa P
- Baringer P
- Barman S
- Barnes VE
- Barney D
- Baron O
- Barria P
- Barroso Ferreira Filho M
- Bartek R
- Bartosik N
- Bartók M
- Barzdukas A
- Basnet A
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Bautista I
- Baxter S
- Bayatmakou M
- Bean A
- Beauceron S
- Beaudette F
- Becerril Gonzalez H
- Bedoya CF
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Beirão Da Cruz E Silva C
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Bellora A
- Belvedere A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Benitez JF
- Bennett C
- Benussi L
- Bergauer T
- Beri SB
- Bermúdez Martínez A
- Bernardes CA
- Berry D
- Berryhill J
- Besancon M
- Bestintzanos I
- Bethani A
- Bevilacqua T
- Beyrouthy T
- Bhardwaj A
- Bharthuar S
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- Bhattacharya S
- Bhattacharya S
- Bhowmik D
- Bhowmik S
- Bhyun JH
- Bialkowska H
- Bianchini L
- Bianco M
- Bianco S
- Biino C
- Bilei GM
- Bilin B
- Bin Anuar AA
- Bin Norjoharuddeen N
- Bisello D
- Black K
- Blanco Fernández S
- Blancon B
- Blekman F
- Blend D
- Blinov V
- Bloch D
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Boccali T
- Bocci A
- Bodek A
- Boimska B
- Boldrini G
- Boletti A
- Bols ES
- Bonacorsi D
- Bonanomi M
- Bonilla J
- Boos E
- Boran F
- Borgonovi L
- Bornheim A
- Borras K
- Borshch V
- Bortignon P
- Bose T
- Bossini E
- Botta C
- Botta V
- Bouchamaoui H
- Boudoul G
- Bouhali O
- Bourilkov D
- Bower N
- Boyaryntsev A
- Bozzo M
- Bragagnolo A
- Braghieri A
- Brainerd C
- Brandao Malbouisson H
- Branson JG
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- Brennan L
- Brew C
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- Brigljevic V
- Brinkerhoff A
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- Brochero Cifuentes JA
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- Brücken E
- Bubanja I
- Bucci R
- Buchmuller O
- Buchot Perraguin A
- Budkouski D
- Bueghly J
- Bundock A
- Bunichev V
- Bunkowski K
- Buontempo S
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- Bury F
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- Busza W
- Butalla S
- Butler JN
- Butler PH
- Butz E
- Bylsma B
- Bärtschi P
- Cabrera A
- Cabrillo IJ
- Cacchio V
- Cadamuro L
- Cagnotta A
- Caillol C
- Cakir A
- Calandri A
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Calzaferri S
- Camaiani B
- Caminada L
- Campagnari C
- Campana M
- Campanini R
- Campbell A
- Camporesi T
- Candelise V
- Canelli MF
- Canepa A
- Cankocak K
- Capiluppi P
- Cappati A
- Caputo C
- Caraway B
- Cardini A
- Cardwell B
- Carlin R
- Carnahan T
- Carnevali F
- Carrera Jarrin E
- Carrigan M
- Carrillo Montoya CA
- Cartiglia N
- Carvalho W
- Casarsa M
- Cassese A
- Castaldi R
- Castaneda Hernandez A
- Castells S
- Castilla-Valdez H
- Castro A
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- Cavallo FR
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- Cavanaugh R
- Cazzaniga C
- Ceard L
- Ceccarelli R
- Cepeda M
- Cerati GB
- Cerci S
- Cerminara G
- Cerrada M
- Cerri O
- Cetorelli F
- Chabert EC
- Chahal GS
- Chandra S
- Chang P
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- Chao Y
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- Chatagnon P
- Chatterjee RM
- Chatterjee S
- Chatterjee S
- Chatzistavrou T
- Chaudhary G
- Chauhan S
- Chawla R
- Checchia P
- Chekhovsky V
- Chen GM
- Chen HS
- Chen KF
- Chen M
- Chen PS
- Chen X
- Chen Y
- Chen YM
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- Chen ZG
- Chenarani S
- Cheng C
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- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhetri A
- Chiarito B
- Chinellato J
- Chistov R
- Chitroda BK
- Chlebana F
- Choi J
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- Chou JP
- Choudhary BC
- Christoforou K
- Chudasama R
- Chwalek T
- Ciangottini D
- Ciocci MA
- Cipriani M
- Citron M
- Cittolin S
- Ciulli V
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- Cranshaw DJ
- Creanza D
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- D'Anzi B
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- De Leo K
- De Moor A
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- de Trocóniz JF
- De Wit A
- Defranchis MM
- Deile M
- Dejardin M
- Del Burgo R
- Del Re D
- Delaere C
- Delannoy AG
- Delcourt M
- Delgado Peris A
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demina R
- Demiragli Z
- Demiroglu ZS
- Denegri D
- Depasse P
- Dermenev A
- Dewanjee RK
- Dezoort G
- Dharmaratna WGD
- Dhingra N
- Di Florio A
- Di Marco E
- Di Mattia A
- Diaz D
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- Diekmann S
- Diemoz M
- Dierlamm A
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- Dimitrov A
- Dimova T
- Dinardo ME
- Dini P
- Diotalevi T
- Dissertori G
- Dittmann J
- Dittmar M
- Dittmer S
- Dobson M
- Dobur D
- Dodonova A
- Dogra S
- Dolek F
- Dolen J
- Dominguez A
- Donato S
- Donegà M
- Donertas IS
- Dordevic M
- Dorigo T
- Doroba K
- Dorsett A
- Dozen C
- Dragicevic M
- Dreimanis K
- Droll A
- Druzhkin D
- Duarte Campderros J
- Duarte J
- Dube S
- Dubinin M
- Dudko L
- Dugad S
- Dulemba JL
- Dumanoglu I
- Durkin LS
- Dutta I
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- Ebrahimi A
- Eckerlin G
- Ecklund KM
- Eckstein D
- Ehataht K
- Eich M
- Eich N
- El Faham H
- El Mamouni H
- El Morabit K
- Elgammal S
- Eliseev D
- Elkafrawy T
- Ellis KV
- Ellithi Kamel A
- Elmer P
- Elmetenawee W
- Elvira VD
- Emediato L
- Encinas Acosta HA
- Engelke F
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erice C
- Errico F
- Escalante Del Valle A
- Escobar Franco R
- Eskut E
- Estevez Banos LI
- Etesami SM
- Eusebi R
- Evangelou I
- Evdokimov O
- Everaerts P
- Eysermans J
- Fabbri F
- Fabozzi F
- Faccioli P
- Fackeldey P
- Falke S
- Fallavollita F
- Fallon C
- Falmagne G
- Faltermann N
- Fan J
- Fan X
- Fanfani A
- Fangmeier C
- Fanò L
- Farkas K
- Fasanella D
- Faure JL
- Favart L
- Fay J
- Fayer S
- Fedi G
- Feld L
- Feng Y
- Ferencek D
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- Yuldashev BS
- Yusuff I
- Zabi A
- Zabolotny W
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
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- Zehetner P
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- Zghiche A
- Zhang F
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- Ziemons T
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- Zimermmane Castro Santos A
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- Zisopoulos I
- Zoi I
- Zolkapli Z
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- Zorbilmez C
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- 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 new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at √s = 13 TeV
- Author
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- Aarup Petersen H
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- Yuldashev BS
- Yusuff I
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- Zhizhin I
- Zhokin A
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- Ziemons T
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- 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 the Higgs boson production via vector boson fusion and its decay into bottom quarks in proton-proton collisions at s = 13 TeV
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- Aarup Petersen H
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- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 30/01/2024
- Field of study
A preprint version of the article is available at arXiv:2308.01253v2 [hep-ex], https://arxiv.org/abs/2308.01253v2 . 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-22-009 (CMS Public Pages). Report number: CMS-HIG-22-009, CERN-EP-2023-110.A measurement of the Higgs boson (H) production via vector boson fusion (VBF) and its decay into a bottom quark-antiquark pair (bb¯) is presented using proton-proton collision data recorded by the CMS experiment at s√ = 13 TeV and corresponding to an integrated luminosity of 90.8 fb−1. Treating the gluon-gluon fusion process as a background and constraining its rate to the value expected in the standard model (SM) within uncertainties, the signal strength of the VBF process, defined as the ratio of the observed signal rate to that predicted by the SM, is measured to be μqqHHbb¯ = 1.01 +0.55−0.46. The VBF signal is observed with a significance of 2.4 standard deviations relative to the background prediction, while the expected significance is 2.7 standard deviations. Considering inclusive Higgs boson production and decay into bottom quarks, the signal strength is measured to be μincl.Hbb¯ = 0.99 +0.48−0.41, corresponding to an observed (expected) significance of 2.6 (2.9) standard deviations.SCOAP3, STFC; Marie-Curie program and the European Research Council and Horizon 2020 Gran
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- Aarrestad TK
- Aarup Petersen H
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- 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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- Author
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- Aarup Petersen H
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- Zuolo D
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- 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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Search for dark matter particles in W+W− events with transverse momentum imbalance in proton-proton collisions at √s = 13 TeV
- Author
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- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 02/03/2024
- Field of study
A preprint version of the article is available at arXiv:2310.12229v2 [hep-ex], https://arxiv.org/abs/2310.12229v2 . 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-21-012 (CMS Public Pages).A search for dark matter particles is performed using events with a pair of W bosons and large missing transverse momentum. Candidate events are selected by requiring one or two leptons (ℓ = electrons or muons). The analysis is based on proton-proton collision data collected at a center-of-mass energy of 13 TeV by the CMS experiment at the LHC and corresponding to an integrated luminosity of 138 fb−1. No significant excess over the expected standard model background is observed in the ℓνqq and 2ℓ2ν final states of the W+W− boson pair. Limits are set on dark matter production in the context of a simplified dark Higgs model, with a dark Higgs boson mass above the W+W− mass threshold. The dark matter phase space is probed in the mass range 100–300 GeV, extending the scope of previous searches. Current exclusion limits are improved in the range of dark Higgs masses from 160 to 250 GeV, for a dark matter mass of 200 GeV.SCOAP3
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Search for direct production of GeV-scale resonances decaying to a pair of muons in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
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- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 30/11/2023
- Field of study
A preprint version of the article is available at arXiv:2309.16003v2 [hep-ex], https://arxiv.org/abs/2309.16003v2 . 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/EXO-21-005 (CMS Public Pages). Report number: CMS-EXO-21-005, CERN-EP-2023-165.A search for direct production of low-mass dimuon resonances is performed using s√ = 13 TeV proton-proton collision data collected by the CMS experiment during the 2017-2018 operation of the CERN LHC with an integrated luminosity of 96.6 fb−1. The search exploits a dedicated high-rate trigger stream that records events with two muons with transverse momenta as low as 3 GeV but does not include the full event information. The search is performed by looking for narrow peaks in the dimuon mass spectrum in the ranges of 1.1-2.6 GeV and 4.2-7.9 GeV. No significant excess of events above the expectation from the standard model background is observed. Model-independent limits on production rates of dimuon resonances within the experimental fiducial acceptance are set. Competitive or world's best limits are set at 90% confidence level for a minimal dark photon model and for a scenario with two Higgs doublets and an extra complex scalar singlet (2HDM+S). Values of the squared kinetic mixing coefficient ε2 in the dark photon model above 10−6 are excluded over most of the mass range of the search. In the 2HDM+S, values of the mixing angle sin(θH) above 0.08 are excluded over most of the mass range of the search with a fixed ratio of the Higgs doublets vacuum expectation tanβ = 0.5.SCOAP3
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