90 research outputs found
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
Transcriptomic Analyses of Sexual Dimorphism of the Zebrafish Liver and the Effect of Sex Hormones
- Author
- A Hallare
- A Knoll-Gellida
- A Mode
- AB Rogers
- AB Rogers
- AK Roy
- AT Nguyen
- AT Nguyen
- B Desvergne
- B Gao
- B Ruggeri
- BD Robison
- C Handschin
- C Wang
- C Wen
- C Wolfrum
- C Zhao
- CA Wiwi
- CH Pham
- CM Small
- CM Troxel
- CY Ung
- CY Ung
- DJ Waxman
- DL Howarth
- EM Santos
- EM Sternberg
- FW Goetz
- H Dell
- H Gao
- H Wang
- Hongyan Xu
- Huaien Luo
- IV Deaciuc
- J Correale
- J van Riggelen
- JL Hoffmann
- JL Wang-Buhler
- KJ Groh
- L Levi
- L Yafang
- LK Davis
- LN Moens
- M Gao
- M Stoffel
- MD Robinson
- MD Robinson
- MD Robinson
- ME Baker
- P Kling
- R Sreenivasan
- R. Krishna Murthy Karuturi
- S Curado
- S Curado
- S Hashimoto
- S Zeng
- S Zhao
- SE Hook
- SH Lam
- SH Lam
- SH Lam
- SH Lam
- Siew Hong Lam
- TF Holth
- U Kausch
- W Cheng
- W Huang da
- W Zhang
- Weiling Zheng
- X Liu
- X Taboada
- X Tan
- X Yang
- Y Li
- Y Shang
- Y Shang
- Y Tong
- Y Weng
- Z Li
- Zhanjiang Liu
- Zhiyuan Gong
- ZJ Li
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 17/01/2013
- Field of study
10.1371/journal.pone.0053562PLoS ONE81
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
- GulĂĄcsi M
- GulĂĄcsi M
- GulĂĄcsi M
- GulĂĄcsi M
- GulĂĄcsi 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
- MiklĂłs GulĂĄcsi *
- Millis AJ
- Moukouri S
- Moukouri S
- Nagaoka Y
- Negele JW
- Newns DM
- Nishino T
- Noack RM
- Novais E
- Novais E
- NoziĂšres P
- NoziĂšres P
- Ogata M
- Ogawa MY
- Ogawa T
- Oshikawa M
- Overhauser AW
- Peschel I
- Pfeuty P
- Pfeuty P
- PrugoveÄki E
- PĂ©pin 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
- SĂłlyom J
- SĂrensen 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
- Ăstlund 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
A portrait of the Higgs boson by the CMS experiment ten years after the discovery
- Author
- Aarrestad TK
- 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
- AdĂĄn DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Agyel D
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- AimĂš C
- Akchurin N
- Akgun B
- Akpinar A
- Albert A
- Albrecht A
- Albrecht S
- Albrow M
- Alcerro LFA
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allmond B
- Almond J
- Alonso AG
- Alpana A
- Alvarez JDR
- Alverson G
- Alves Gallo Pereira M
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amarilo KM
- Ambrozas M
- Amendola C
- Amin N
- Amram O
- Amsler C
- An S
- An Y
- Anagnostou G
- Anampa KH
- Andrea J
- Andreev V
- Andreev Y
- Andrejkovic JW
- Andrews MB
- Androsov K
- Anguiano J
- Antchev G
- Antequera JB
- 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
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Bakshi AS
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Banos LIE
- Bansal S
- Baradia S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barman S
- Barnes VE
- Barney D
- Baron O
- Barrera CB
- Barrera CO
- Barria P
- Barrio Luna M
- Barroso Ferreira Filho M
- Barroso AV
- Bartek R
- Bartosik N
- BartĂłk M
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baxter S
- Bayatmakou M
- Bean A
- Beauceron S
- Beaudette F
- 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
- Bemden MV
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benitez JF
- Benussi L
- Bergauer T
- Berger P
- Beri SB
- 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
- Bi R
- Bialkowska H
- Bianchini L
- Bianco M
- Bianco S
- Biino C
- Bilei GM
- Bilin B
- Bin Anuar AA
- Bin Norjoharuddeen N
- Bisello D
- Black K
- 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
- Bonham B
- Bonilla J
- Bonomally S
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- Bornheim A
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- Chaudhary G
- Chauhan S
- Chauhan S
- Chawla R
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- Chekhovsky V
- Chen C
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- Chen HS
- Chen KF
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- Chen PS
- Chen X
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- Cherepanov V
- Chernyavskaya N
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- Cheung HWK
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- Da Silva De Araujo FT
- Da Silveira GG
- Dabrowski A
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- Dallavalle GM
- Damanakis K
- Damgov J
- Dancu JS
- Darej D
- Darwish MR
- Das A
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- de Barbaro P
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- de Cassagnac RG
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- de TrocĂłniz JF
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- Deile M
- Dejardin M
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- Delannoy AG
- Delcourt M
- Delgado Peris A
- Delgado A
- Della Negra M
- Della Ricca G
- DellâOrso R
- Demaria N
- Demina R
- Demiragli Z
- Demiroglu ZS
- Denegri D
- Dengra CP
- Depasse P
- Dermenev A
- Dewanjee RK
- Dezoort G
- Dharmaratna WGD
- Dhingra N
- Di Croce D
- Di Domenico MR
- Di Florio A
- Di Marco E
- Di Mattia A
- Di Petrillo KF
- Diab B
- Diamantopoulou M
- Diaz D
- Dickinson J
- Didukh L
- Diekmann S
- Diemoz M
- Dierlamm A
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- Dimitrov A
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- Dinardo ME
- Dini P
- Diotalevi T
- Dissertori G
- Dittmann J
- Dittmar M
- Dittmer S
- Do Amaral SMS
- Dobson M
- Dobur D
- Dodonova A
- Dogra S
- Dolek F
- Dolen J
- Dominguez A
- Donato S
- DonegĂ M
- Donertas IS
- Dordevic M
- Dorigo T
- Doroba K
- Dorsett A
- Dozen C
- Dragicevic M
- Dreimanis K
- Dremin I
- Droll A
- Duarte J
- Dube S
- Dubinin M
- Dudko L
- Dugad S
- Dulemba JL
- Dumanoglu I
- Dupont N
- Duric S
- Durkin LS
- Dutta I
- Dutta S
- Dutta V
- Dziwok C
- DĂŒnser M
- DâAlessandro R
- DâAlfonso M
- DâAmante V
- dâEnterria D
- DâHondt J
- Eble F
- Ebrahimi A
- Eckerlin G
- Ecklund KM
- Eckstein D
- Eerola P
- Ehataht K
- Eich M
- Eich N
- El Faham H
- El Mamouni H
- El Morabit K
- El Nasr-Storey SS
- Eliseev D
- Elkafrawy T
- Elliott-Peisert A
- Ellis KV
- Elmer P
- Elmetenawee W
- Elvira VD
- Emediato L
- Encinas Acosta HA
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erice C
- Errico F
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- Ăzçelik Ă
- 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 125âgigaelectronvolts. 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 spinâparity 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 protonâproton collisions at a centre-of-mass energy of 13âteraelectronvolts. 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 Ă la Recherche dans lâIndustrie et dans lâAgriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the F.R.S.-FNRS and FWO (Belgium) under the âExcellence of Science â EOSâ â 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 Germanyâs Excellence Strategy â EXC 2121 âQuantum Universeâ â 390833306, and under project number 400140256 - GRK2497; the Hungarian Academy of Sciences, the New National Excellence Program - ĂNKP, 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 CiĂȘncia e a Tecnologia, grant CEECIND/01334/2018 (Portugal); the National Priorities Research Program by Qatar National Research Fund; MCIN/AEI/10.13039/501100011033, ERDF âa way of making Europeâ, and the Programa Estatal de Fomento de la InvestigaciĂłn CientĂfica y TĂ©cnica de Excelencia MarĂa 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)
Measurement of the differential ttÂŻ 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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- Zoi I
- Zolkapli Z
- Zorbakir IS
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- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Ălvarez 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. [Authorsâ 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 (ttÂŻ
) 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 138fbâ1
. The differential ttÂŻ
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
Portable Acceleration of CMS Computing Workflows with Coprocessors as a Service
- Author
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- 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
Evidence for tWZ production in proton-proton collisions at âs=13 TeV in multilepton final states
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- Yohay R
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- Yuldashev BS
- Yusuff I
- Zabi A
- Zabolotny W
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
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- Zecchinelli AG
- Zehetner P
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- Zeuner WD
- Zghiche A
- Zhang F
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- Zilizi G
- Zimermmane Castro Santos A
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- Zisopoulos I
- Zoi I
- Zolkapli Z
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- Zorbilmez C
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- Zucchetta A
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- 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 2016â2018 in proton-proton collisions at âs=13 TeV, and correspond to an integrated luminosity of 138 fbâ1. The measured cross section is 354±54(stat)±95(syst) fb, and corresponds to a statistical significance of 3.4 standard deviations.SCOAP
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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- Yusuff I
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- Zeuner WD
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- 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 â = 13ââTeV proton-proton collisions collected by the CMS experiment and corresponding to an integrated luminosity of 36.3ââfb^â1. 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: âĄ() = 0.122âą9+0.0040 â0.0050, the most precise âĄ() value obtained using jet substructure observables.SCOAP3
Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at âs = 13 TeV
- Author
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- Zuolo D
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- 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 âCMS data preservation, re-use and open access policyâ 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 â tH/A â ttÂŻc and pp â tH/A â ttÂŻu 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 fbâ1. 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
Search for long-lived heavy neutral leptons with lepton flavour conserving or violating decays to a jet and a charged lepton
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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 fbâ1. 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 VâN to each lepton generation â 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 |VÎŒN|2 > 5 (4) Ă 10â7 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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