98 research outputs found
A human in vitro model system for investigating genome-wide host responses to SARS coronavirus infection
- Author
- A Aggarwal
- B Sar
- Beijing Group of National Research projects for SARS
- C Drosten
- CP Su
- CY Cheung
- E Pace
- E Traggiai
- Edison T Liu
- Ee-Chee Ren
- Eng-Eong Ooi
- EW Drost
- F Buhling
- GF Wu
- GJ Nau
- H Hemmi
- HA Ball
- I Julkunen
- J Cinatl
- Jenny Tan
- Jer-Ming Chia
- JM Nicholls
- JSM Peiris
- K Singh
- K To
- Karuturi R Krishna Murthy
- Kin-Fai Tang
- KV Holmes
- L Gillim-Ross
- L Li
- Lisa FP Ng
- M Miyamoto
- M Zaitsu
- MA Marra
- Martin L Hibberd
- MJ Robertson
- MW Raza
- NS Paul
- PA Rota
- Q Huang
- S Akira
- S Gordon
- Soek-Ying Neo
- TG Ksiazek
- TJ Franks
- U Arndt
- V Hornung
- Vinsensius B Vega
- Y Shi
- YC Liao
- YJ Ruan
- Z Zou
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2004
- Field of study
10.1186/1471-2334-4-34BMC Infectious Diseases4-BIDM
Curation of viral genomes: challenges, applications and the way forward
- Author
- AE Matusan
- AS Kolaskar
- AS Kolaskar
- Ashok S Kolaskar
- AT Brunger
- AZ Randall
- B Capecchi
- B Falgout
- C Brooksbank
- C Desjardins
- C Kuiken
- CM Fauquet
- CM Fraser
- CS Riesenfeld
- D Raoult
- DD Womble
- DP Mindell
- DV Jobes
- E Espagne
- EA Gould
- EJ Lefkowitz
- F Preugschat
- FX Heinz
- FX Heinz
- G Rinck
- G Seibel
- G Sunitha Manjari
- GN Ramachandran
- H Ni
- H Tokita
- HM Krishna Murthy
- HM Murthy
- J Kyte
- J Nitkiewicz
- JB Nousbaum
- JJ Perona
- JM Claverie
- JM Kaper
- JT Roehrig
- K Eilbeck
- K Hiramatsu
- K Liolios
- K Sandres-Saune
- KJ Chappell
- KS Lole
- L Rocheleau
- LR Jan
- M Bessaud
- M Breitbart
- M Lobigs
- M Salemi
- Manali Joshi
- MB Crabtree
- MJ Sippl
- MM Alba
- N Deshpande
- N Hulo
- N Yao
- O Bergh
- R Bartenschlager
- R Brodie
- R Chenna
- R Colina
- RA Laskowski
- RG van der Most
- S Clum
- Sandeep Bansode
- SC Wu
- SF Altschul
- Shriram G Bhosle
- SV Tiroumourougane
- TJ Chambers
- TP Monath
- TT Wu
- U Kulkarni-Kale
- U Kulkarni-Kale
- U Kulkarni-Kale
- U Kulkarni-Kale
- Urmila Kulkarni-Kale
- V Campanacci
- VF Yamshchikov
- W Fiers
- W Kabsch
- Y Bao
- Y Modis
- Y Shivashankar
- Y Yan
- Publication venue
- BioMed Central
- Publication date
- 01/01/2006
- Field of study
BACKGROUND: Whole genome sequence data is a step towards generating the 'parts list' of life to understand the underlying principles of Biocomplexity. Genome sequencing initiatives of human and model organisms are targeted efforts towards understanding principles of evolution with an application envisaged to improve human health. These efforts culminated in the development of dedicated resources. Whereas a large number of viral genomes have been sequenced by groups or individuals with an interest to study antigenic variation amongst strains and species. These independent efforts enabled viruses to attain the status of 'best-represented taxa' with the highest number of genomes. However, due to lack of concerted efforts, viral genomic sequences merely remained as entries in the public repositories until recently. RESULTS: VirGen is a curated resource of viral genomes and their analyses. Since its first release, it has grown both in terms of coverage of viral families and development of new modules for annotation and analysis. The current release (2.0) includes data for twenty-five families with broad host range as against eight in the first release. The taxonomic description of viruses in VirGen is in accordance with the ICTV nomenclature. A well-characterised strain is identified as a 'representative entry' for every viral species. This non-redundant dataset is used for subsequent annotation and analyses using sequenced-based Bioinformatics approaches. VirGen archives precomputed data on genome and proteome comparisons. A new data module that provides structures of viral proteins available in PDB has been incorporated recently. One of the unique features of VirGen is predicted conformational and sequential epitopes of known antigenic proteins using in-house developed algorithms, a step towards reverse vaccinology. CONCLUSION: Structured organization of genomic data facilitates use of data mining tools, which provides opportunities for knowledge discovery. One of the approaches to achieve this goal is to carry out functional annotations using comparative genomics. VirGen, a comprehensive viral genome resource that serves as an annotation and analysis pipeline has been developed for the curation of public domain viral genome data . Various steps in the curation and annotation of the genomic data and applications of the value-added derived data are substantiated with case studies
Zebrafish Whole-Adult-Organism Chemogenomics for Large-Scale Predictive and Discovery Chemical Biology
- Author
- A Dobs
- A Luch
- AJ Hill
- AR Cossins
- B Ganter
- BP Gomez
- C Kakiuchi
- C Konradi
- C Parng
- C Xu
- D Ron
- DW Nebert
- DY Wang
- E Sonneveld
- Edison T. Liu
- F Boess
- F Girardot
- FB Pichler
- H Ostlund
- H Wang
- Haixia Li
- I Kola
- J Matthews
- JA Caruso
- JF Pritchard
- JH Pedra
- JM Rotchell
- K Dooley
- K Reichert
- KW Fried
- L Fang
- L Yang
- LI Zon
- M Bredel
- M Yang
- MB Eisen
- N Custodia
- PE Bayliss
- R. Krishna Murthy Karuturi
- RJ Lewis
- S Aittomäki
- S Nilsson
- S Safe
- S Safe
- SH Lam
- SH Lam
- Siew Hong Lam
- Sinnakarupan Mathavan
- Stuart K. Kim
- TV Beischlag
- VG Tusher
- Vinsensius B. Vega
- W Zhang
- Y Ma
- Yan Tong
- Yilian Wu
- Z Dvorak
- Z Kostova
- Zhiyuan Gong
- Publication venue
- Public Library of Science
- Publication date
- 01/07/2008
- Field of study
The ability to perform large-scale, expression-based chemogenomics on whole adult organisms, as in invertebrate models (worm and fly), is highly desirable for a vertebrate model but its feasibility and potential has not been demonstrated. We performed expression-based chemogenomics on the whole adult organism of a vertebrate model, the zebrafish, and demonstrated its potential for large-scale predictive and discovery chemical biology. Focusing on two classes of compounds with wide implications to human health, polycyclic (halogenated) aromatic hydrocarbons [P(H)AHs] and estrogenic compounds (ECs), we generated robust prediction models that can discriminate compounds of the same class from those of different classes in two large independent experiments. The robust expression signatures led to the identification of biomarkers for potent aryl hydrocarbon receptor (AHR) and estrogen receptor (ER) agonists, respectively, and were validated in multiple targeted tissues. Knowledge-based data mining of human homologs of zebrafish genes revealed highly conserved chemical-induced biological responses/effects, health risks, and novel biological insights associated with AHR and ER that could be inferred to humans. Thus, our study presents an effective, high-throughput strategy of capturing molecular snapshots of chemical-induced biological states of a whole adult vertebrate that provides information on biomarkers of effects, deregulated signaling pathways, and possible affected biological functions, perturbed physiological systems, and increased health risks. These findings place zebrafish in a strategic position to bridge the wide gap between cell-based and rodent models in chemogenomics research and applications, especially in preclinical drug discovery and toxicology
The one dimensional Kondo lattice model at partial band filling
- Author
- Abdalla E
- Aeppli G
- Anderson PW
- Anderson PW
- Anderson PW
- Anderson PW
- Anderson PW
- Anderson PW
- Anderson PW
- Andrei N
- Andrei N
- Apostol M
- Aristov DN
- Ashcroft NW
- Assad FF
- Bares PA
- Batista CD
- Batista CD
- Batlogg B
- Baxter RJ
- Baym G
- Belavin AA
- Bethe HA
- Biedenharn LC
- Blatt JM
- Bowen G
- Bray J
- Brazovskii S
- Brézin E
- Capponi A
- Caprara S
- Caron LG
- Chan R
- Chan R
- Chan R
- Chan R
- Chan R
- Chao KA
- Chen Y
- Coleman P
- Coleman S
- Coll CF
- Coqblin B
- Dagotto E
- Dagotto E
- Daul S
- Daul S
- Doniach S
- Dwight HB
- Emery VJ
- Emery VJ
- Emery VJ
- Fetter AL
- Feynman RP
- Finkel'stein AM
- Fisher DS
- Fisher DS
- Fisk Z
- Fradkin E
- Fradkin E
- Fröhlich H
- Fujimoto S
- Fulde P
- Fye RM
- Fye RM
- Garcia DJ
- Glazek SD
- Goodenough JB
- Gradshteyn IS
- Griffiths RB
- Gross EKU
- Guerrero M
- Gulácsi M
- Gulácsi M
- Gulácsi M
- Gulácsi M
- Gulácsi Zs.
- Gutzwiller MC
- Ha YK
- Haldane FDM
- Harris AB
- Haug A
- Heidenreich R
- Hewson AC
- Hirsch JE
- Hirsch JE
- Hirsch JE
- Hirsch JE
- Holstein T
- Holstein T
- Honner G
- Honner G
- Honner G
- Honner G
- Honner G
- Honner G
- Horsch P
- Huang K
- Hubbard J
- Hubbard J
- Itoyama H
- Itzykson C
- Jauch JM
- Jin S
- Jonker GH
- Jullien R
- Juozapavicius A
- Juozapavicius A
- Jurecka C
- Kasuya T
- Kehrein SK
- Kittel C
- Kohn W
- Koller W
- Kolley E
- Kondo J
- Korepin VE
- Krishna-Murthy HR
- Kubo K
- Lacroix C
- Lacroix C
- Landau LD
- Langer W
- Lavagna M
- Le Hur K
- Le Hur K
- Lebedev NN
- Lee PA
- Lieb E
- Lieb EH
- Linden von der W
- Luther A
- Luther A
- Luther A
- Luttinger JM
- Mahan GD
- Mahan GD
- Makhankov VG
- Mandelstam S
- Mattis DC
- Mattis DC
- Matveenko S
- McCulloch IP
- McCulloch IP
- McCulloch IP
- McCulloch IP
- McCulloch IP
- McCulloch IP
- McCulloch IP
- Miklós Gulácsi *
- Millis AJ
- Moukouri S
- Moukouri S
- Nagaoka Y
- Negele JW
- Newns DM
- Nishino T
- Noack RM
- Novais E
- Novais E
- Nozières P
- Nozières P
- Ogata M
- Ogawa MY
- Ogawa T
- Oshikawa M
- Overhauser AW
- Peschel I
- Pfeuty P
- Pfeuty P
- Prugovečki E
- Pépin C
- Roth L
- Ruderman MA
- Sakamoto H
- Satija II
- Satija II
- Satija II
- Schick M
- Schlottmann P
- Schlottmann P
- Schotte KD
- Schrieffer JR
- Schulz HJ
- Schulz HJ
- Schönhammer K
- Searle CW
- Shankar R
- Shen S-Q
- Shi ZP
- Shibata N
- Shibata N
- Shibata N
- Shibata N
- Sierra G
- Sigrist M
- Sigrist M
- Sigrist M
- Sikkema A
- Sokoloff JB
- Stewart GR
- Stone M
- Strong SP
- Su WP
- Su WP
- Sutherland B
- Suzuki T
- Sólyom J
- SØrensen ES
- Tokura Y
- Tomonaga S
- Toulouse G
- Troyer M
- Tsunetsugu H
- Tsunetsugu H
- Tsunetsugu H
- Tsunetsugu H
- Tsvelick AM
- Tsvelik AM
- Van Santen JH
- Van Vleck JH
- Varma CM
- Varma CM
- Varma CM
- Varma CM
- Visscher PB
- Voit J
- von Delft J
- Wagner W
- Wang Z
- Wang Z
- White SR
- White SR
- White SR
- White SR
- White SR
- Wiegmann PB
- Wiegmann PB
- Wilson KG
- Witten E
- Xavier JC
- Xavier JC
- Yafet Y
- Yamanaka M
- Yanagisawa T
- Yanagisawa T
- Yosida K
- Yosida K
- Yosida K
- Yu CC
- Yunoki S
- Yuval G
- Zaanen J
- Zachar O
- Zang J
- Zener C
- Zhang GM
- Zheng W
- Zhou L-J
- Östlund S
- Publication venue
- 'Informa UK Limited'
- Publication date
- 02/02/2005
- Field of study
The Kondo lattice model introduced in 1977 describes a lattice of localized
magnetic moments interacting with a sea of conduction electrons. It is one of
the most important canonical models in the study of a class of rare earth
compounds, called heavy fermion systems, and as such has been studied
intensively by a wide variety of techniques for more than a quarter of a
century. This review focuses on the one dimensional case at partial band
filling, in which the number of conduction electrons is less than the number of
localized moments. The theoretical understanding, based on the bosonized
solution, of the conventional Kondo lattice model is presented in great detail.
This review divides naturally into two parts, the first relating to the
description of the formalism, and the second to its application. After an
all-inclusive description of the bosonization technique, the bosonized form of
the Kondo lattice hamiltonian is constructed in detail. Next the
double-exchange ordering, Kondo singlet formation, the RKKY interaction and
spin polaron formation are described comprehensively. An in-depth analysis of
the phase diagram follows, with special emphasis on the destruction of the
ferromagnetic phase by spin-flip disorder scattering, and of recent numerical
results. The results are shown to hold for both antiferromagnetic and
ferromagnetic Kondo lattice. The general exposition is pedagogic in tone.Comment: Review, 258 pages, 19 figure
Inferring single-trial neural population dynamics using sequential auto-encoders
- Author
- A Afshar
- B Rosin
- BM Yu
- C Pandarinath
- C Pandarinath
- CD Harvey
- Chethan Pandarinath
- D Kobak
- D Sussillo
- D Sussillo
- Daniel J. O’Shea
- David Sussillo
- E Salinas
- Eric M. Trautmann
- F Carnevale
- FR Willett
- Jaimie M. Henderson
- Jasmine Collins
- JC Kao
- JM Fan
- Jonathan C. Kao
- JP Donoghue
- Krishna V. Shenoy
- KV Shenoy
- L Paninski
- L. F. Abbott
- Leigh R. Hochberg
- Lvander Maaten
- M Aghagolzadeh
- Mark M. Churchland
- Matthew T. Kaufman
- MB Ahrens
- MT Kaufman
- NV Klinger
- P Fries
- P Gao
- Patrick T. Sadtler
- R Yuste
- Rafal Jozefowicz
- RS Williamson
- S Kato
- Sergey D. Stavisky
- Simon Little
- Stephen I. Ryu
- V Gilja
- V Gilja
- V Mante
- VN Murthy
- Y Ezzyat
- Y Zhao
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 17/09/2018
- Field of study
Neuroscience is experiencing a revolution in which simultaneous recording of thousands of neurons is revealing population dynamics that are not apparent from single-neuron responses. This structure is typically extracted from data averaged across many trials, but deeper understanding requires studying phenomena detected in single trials, which is challenging due to incomplete sampling of the neural population, trial-to-trial variability, and fluctuations in action potential timing. We introduce latent factor analysis via dynamical systems, a deep learning method to infer latent dynamics from single-trial neural spiking data. When applied to a variety of macaque and human motor cortical datasets, latent factor analysis via dynamical systems accurately predicts observed behavioral variables, extracts precise firing rate estimates of neural dynamics on single trials, infers perturbations to those dynamics that correlate with behavioral choices, and combines data from non-overlapping recording sessions spanning months to improve inference of underlying dynamics
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Measurements of the Higgs boson production cross section and couplings in the W boson pair decay channel in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams MR
- Adams T
- Addesa FM
- Adloff C
- Adzic P
- Afanasiev S
- Agapitos A
- Agarwal G
- Agram J-L
- Aguilar-Benitez M
- Agyel D
- Ahmad A
- Ahmad M
- Ahmed A
- Aimè C
- Akchurin N
- Akgun B
- Akpinar A
- Al-Mashad MA
- 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
- Almond J
- Alpana A
- Alvarez Gonzalez B
- Alverson G
- Alves Gallo Pereira M
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Ambrozas M
- Amendola C
- Amin N
- 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
- Antunovic Z
- Apollinari G
- Apparu D
- Appelt E
- Apresyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Argiro S
- Arneodo M
- Aruta C
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Asmuss P
- 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
- Bagaturia I
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Bakshi AS
- 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
- Bargassa P
- Baringer P
- Barman S
- Barnes VE
- Barney D
- Baron O
- Barria P
- Barroso Ferreira Filho M
- Barroso AV
- Bartek R
- Bartosik N
- Bartók M
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baxter S
- Bayatmakou M
- Bean A
- Beauceron S
- Beaudette F
- Becerril Gonzalez H
- Bechtel J
- Bedoya CF
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Bellora A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benitez JF
- Benussi L
- Bergauer T
- Berger P
- Beri SB
- Bermúdez Martínez A
- Bernardes CA
- Bernet C
- Berry D
- Berryhill J
- Bertacchi V
- Besancon M
- Bestintzanos I
- Bethani A
- Beyrouthy T
- Bhal E
- 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
- Biasotto M
- Biino C
- Bilei GM
- Bilin B
- Bin Anuar AA
- Bin Norjoharuddeen N
- Bisello D
- Black K
- Blancon B
- Blekman F
- 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
- Bonomally S
- Boos E
- Boran F
- Borg J
- Borgonovi L
- Bornheim A
- Borras K
- Borshch V
- Bortignon P
- Bose T
- Bossini E
- Botta C
- Botta V
- Boudoul G
- Bouhali O
- Bourgatte G
- Bourilkov D
- Bozzo M
- Bragagnolo A
- Braghieri A
- Brainerd C
- Brandao Malbouisson H
- Branson JG
- Breedon R
- Breeze S
- Brew C
- Bright-Thonney S
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Brivio F
- Brochero Cifuentes JA
- Brom J-M
- Brommer S
- Brondolin E
- Brooke JJ
- Brown CE
- Brown RM
- Brunner D
- Bruno G
- Bruschini D
- Bryant P
- Bryson M
- Brzhechko D
- Brücken E
- Bubanja I
- Bucci R
- Buccilli A
- Buchmuller O
- Buchot Perraguin A
- Budkouski D
- Bueghly J
- Bundock A
- Bunichev V
- Bunkowski K
- Buontempo S
- Burgo RD
- Burkart M
- Burkett K
- Burkle B
- Bury F
- Busson P
- Busza W
- Butalla S
- Butler JN
- Butz E
- Bychkova O
- Bylsma B
- Bärtschi P
- Cabrera A
- Cabrillo IJ
- Cacchio V
- Cadamuro L
- 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
- Carle A
- Carlin R
- Carnahan T
- Carnevali F
- Carrigan M
- Carrillo Montoya CA
- Cartiglia N
- Carvalho Antunes De Oliveira A
- Carvalho W
- Casarsa M
- Caspart R
- Cassese A
- Castaldi R
- Castaneda Hernandez A
- Castells S
- Castilla-Valdez H
- Castro A
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Ceccarelli R
- Cepaitis V
- Cepeda M
- Cerati GB
- Cerci S
- Cerminara G
- Cerrada M
- Cerri O
- Cetorelli F
- Chabert EC
- Chahal GS
- Chang P
- Chanon N
- Chao Y
- Charlot C
- Chatagnon P
- Chatterjee RM
- Chatterjee S
- Chatzistavrou T
- Chaudhary G
- Chauhan S
- Chawla R
- Checchia P
- Chekhovsky V
- Chen C
- Chen GM
- Chen HS
- Chen KF
- Chen M
- Chen PS
- Chen X
- Chen Y
- Chen Y
- Chen Z
- Chenarani S
- Cheng C
- Cheng H
- Cheng T
- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhibra SS
- Chiarito B
- Chinellato J
- Chistov R
- Chitroda BK
- Chlebana F
- Choi J
- Choi J
- Choi M
- Choi S
- Chou JP
- Choudhary BC
- Choudhury S
- Christoforou K
- Chudasama R
- Chwalek T
- Ciangottini D
- Ciocci MA
- Cipriani M
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clement E
- Clerbaux B
- Cockerill DJA
- Coelho E
- Colaleo A
- Coldham K
- Cole JE
- Colino N
- Collard C
- Colling D
- Collura G
- Colombina F
- Connor P
- Consuegra Rodríguez S
- Contardo D
- Conway J
- Cooke C
- Cooper SI
- Cooperstein S
- Corcodilos L
- Cormier K
- Correia Silva G
- Cosby C
- Cossutti F
- Costa M
- Costa S
- Coubez X
- Couderc F
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Cranshaw DJ
- Creanza D
- Cremaldi LM
- Cremonesi M
- Cristella L
- Croce DD
- Crossman B
- Csanád M
- Csorgo T
- Cuevas J
- Cuevas PM
- Cuffiani M
- Cumalat JP
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- Zotto P
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- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 09/10/2022
- Field of study
A preprint version of the article is available at arXiv:2206.09466v2 [hep-ex], https://arxiv.org/abs/2206.09466v2 . 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-20-013 (CMS Public Pages). Report number: CMS-HIG-20-013, CERN-EP-2022-120.Production cross sections of the standard model Higgs boson decaying to a pair of W bosons are measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analysis targets Higgs bosons produced via gluon fusion, vector boson fusion, and in association with a W or Z boson. Candidate events are required to have at least two charged leptons and moderate missing transverse momentum, targeting events with at least one leptonically decaying W boson originating from the Higgs boson. Results are presented in the form of inclusive and differential cross sections in the simplified template cross section framework, as well as couplings of the Higgs boson to vector bosons and fermions. The data set collected by the CMS detector during 2016-2018 is used, corresponding to an integrated luminosity of 138 fb^−1. The signal strength modifier μ, defined as the ratio of the observed production rate in a given decay channel to the standard model expectation, is measured to be μ = 0.95 +0.10−0.09. All results are found to be compatible with the standard model within the uncertainties.SCOAP3
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- Özçelik Ö
- Publication venue
- Springer Science and Business Media LLC
- Publication date
- 07/07/2022
- Field of study
A Correction to this paper has been published (18 October 2023) : https://doi.org/10.1038/s41586-023-06164-8.Data availability:
Tabulated results are provided in the HEPData record for this analysis. 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 acess policy.Code availability:
The CMS core software is publicly available on GitHub (https://github.com/cms-sw/cmssw).In July 2012, the ATLAS and CMS collaborations at the CERN Large Hadron Collider announced the observation of a Higgs boson at a mass of around 125 gigaelectronvolts. Ten years later, and with the data corresponding to the production of a 30-times larger number of Higgs bosons, we have learnt much more about the properties of the Higgs boson. The CMS experiment has observed the Higgs boson in numerous fermionic and bosonic decay channels, established its spin–parity quantum numbers, determined its mass and measured its production cross-sections in various modes. Here the CMS Collaboration reports the most up-to-date combination of results on the properties of the Higgs boson, including the most stringent limit on the cross-section for the production of a pair of Higgs bosons, on the basis of data from proton–proton collisions at a centre-of-mass energy of 13 teraelectronvolts. Within the uncertainties, all these observations are compatible with the predictions of the standard model of elementary particle physics. Much evidence points to the fact that the standard model is a low-energy approximation of a more comprehensive theory. Several of the standard model issues originate in the sector of Higgs boson physics. An order of magnitude larger number of Higgs bosons, expected to be examined over the next 15 years, will help deepen our understanding of this crucial sector.BMBWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, FAPERGS, and FAPESP (Brazil); MES and BNSF (Bulgaria); CERN; CAS, MoST, and NSFC (China); MINCIENCIAS (Colombia); MSES and CSF (Croatia); RIF (Cyprus); SENESCYT (Ecuador); MoER, ERC PUT and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRI (Greece); NKFIH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); MSIP and NRF (Republic of Korea); MES (Latvia); LAS (Lithuania); MOE and UM (Malaysia); BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MOS (Montenegro); MBIE (New Zealand); PAEC (Pakistan); MES and NSC (Poland); FCT (Portugal); MESTD (Serbia); MCIN/AEI and PCTI (Spain); MOSTR (Sri Lanka); Swiss Funding Agencies (Switzerland); MST (Taipei); MHESI and NSTDA (Thailand); TUBITAK and TENMAK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA). Individuals have received support from the Marie-Curie programme and the European Research Council and Horizon 2020 Grant, contract Nos. 675440, 724704, 752730, 758316, 765710, 824093, 884104, and COST Action CA16108 (European Union); the Leventis Foundation; the Alfred P. Sloan Foundation; the Alexander von Humboldt Foundation; the Belgian Federal Science Policy Office; the Fonds pour la Formation à la Recherche dans l’Industrie et dans l’Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the F.R.S.-FNRS and FWO (Belgium) under the “Excellence of Science – EOS” – be.h project n. 30820817; the Beijing Municipal Science & Technology Commission, No. Z191100007219010; the Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Stavros Niarchos Foundation (Greece); the Deutsche Forschungsgemeinschaft (DFG), under Germany’s Excellence Strategy – EXC 2121 “Quantum Universe” – 390833306, and under project number 400140256 - GRK2497; the Hungarian Academy of Sciences, the New National Excellence Program - ÚNKP, the NKFIH research grants K 124845, K 124850, K 128713, K 128786, K 129058, K 131991, K 133046, K 138136, K 143460, K 143477, 2020-2.2.1-ED-2021-00181, and TKP2021-NKTA-64 (Hungary); the Council of Science and Industrial Research, India; the Latvian Council of Science; the Ministry of Education and Science, project no. 2022/WK/14, and the National Science Center, contracts Opus 2021/41/B/ST2/01369 and 2021/43/B/ST2/01552 (Poland); the Fundação para a Ciência e a Tecnologia, grant CEECIND/01334/2018 (Portugal); the National Priorities Research Program by Qatar National Research Fund; MCIN/AEI/10.13039/501100011033, ERDF “a way of making Europe”, and the Programa Estatal de Fomento de la Investigación Científica y Técnica de Excelencia María de Maeztu, grant MDM-2017-0765 and Programa Severo Ochoa del Principado de Asturias (Spain); the Chulalongkorn Academic into Its 2nd Century Project Advancement Project, and the National Science, Research and Innovation Fund via the Program Management Unit for Human Resources & Institutional Development, Research and Innovation, grant B05F650021 (Thailand); the Kavli Foundation; the Nvidia Corporation; the SuperMicro Corporation; the Welch Foundation, contract C-1845; and the Weston Havens Foundation (USA)
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Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at s = 13 TeV
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- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- Springer Nature
- Publication date
- 25/03/2023
- Field of study
A preprint version of the article is available at arXiv:2208.06485v2 [hep-ex], https://arxiv.org/abs/2208.06485v2 . 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/TOP-21-011 (CMS Public Pages). Report number: CMS-TOP-21-011, CERN-EP-2022-168The production of a top quark-antiquark pair in association with a W boson (tt¯W) is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb^{−1}. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive tt¯W production cross section in the full phase space is measured to be 868 ± 40 (stat) ± 51 (syst) fb. The tt¯W+ and tt¯W− cross sections are also measured as 553 ± 30 (stat) ± 30 (syst) and 343 ± 26 (stat) ± 25 (syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 ± 0.15 (stat) +0.07−0.05 (syst). The measured cross sections are larger than but consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.SCOAP3
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Measurement of the differential tt¯ production cross section as a function of the jet mass and extraction of the top quark mass in hadronic decays of boosted top quarks
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- Yumiceva F
- Yusuff I
- Yzquierdo AP-C
- Zabi A
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- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
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- Zecchinelli AG
- Zeid SA
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- Zghiche A
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- Zorbakir IS
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- Zuo X
- Zuolo D
- Zygala L
- Álvarez CR
- Publication venue
- Springer Nature
- Publication date
- 03/07/2023
- Field of study
Data Availability:
This manuscript has no associated data or the data will not be deposited. [Authors’ comment: Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in https://cms-docdb.cern.ch/cgibin/PublicDocDB/RetrieveFile?docid=6032 &filename=CMSDataPolicyV1.2.pdf &version=2.]A measurement of the jet mass distribution in hadronic decays of Lorentz-boosted top quarks is presented. The measurement is performed in the lepton + jets channel of top quark pair production (tt¯
) events, where the lepton is an electron or muon. The products of the hadronic top quark decay are reconstructed using a single large-radius jet with transverse momentum greater than 400GeV
. The data were collected with the CMS detector at the LHC in proton-proton collisions and correspond to an integrated luminosity of 138fb−1
. The differential tt¯
production cross section as a function of the jet mass is unfolded to the particle level and is used to extract the top quark mass. The jet mass scale is calibrated using the hadronic W boson decay within the large-radius jet. The uncertainties in the modelling of the final state radiation are reduced by studying angular correlations in the jet substructure. These developments lead to a significant increase in precision, and a top quark mass of 173.06±0.84GeV.SCOAP
Recommended from our members
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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- 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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