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Comparison of Small Baseline Interferometric SAR Processors for Estimating Ground Deformation

Author: Agram PS
Gong W
Hinz S
Hooper A
Meyer FJ
Thiele A
Publication venue: 'MDPI AG'
Publication date: 15/04/2016
Field of study

The small Baseline Synthetic Aperture Radar (SAR) Interferometry (SBI) technique has been widely and successfully applied in various ground deformation monitoring applications. Over the last decade, a variety of SBI algorithms have been developed based on the same fundamental concepts. Recently developed SBI toolboxes provide an open environment for researchers to apply different SBI methods for various purposes. However, there has been no thorough discussion that compares the particular characteristics of different SBI methods and their corresponding performance in ground deformation reconstruction. Thus, two SBI toolboxes that implement a total of four SBI algorithms were selected for comparison. This study discusses and summarizes the main differences, pros and cons of these four SBI implementations, which could help users to choose a suitable SBI method for their specific application. The study focuses on exploring the suitability of each SBI module under various data set conditions, including small/large number of interferograms, the presence or absence of larger time gaps, urban/vegetation ground coverage, and temporally regular/irregular ground displacement with multiple spatial scales. Within this paper we discuss the corresponding theoretical background of each SBI method. We present a performance analysis of these SBI modules based on two real data sets characterized by different environmental and surface deformation conditions. The study shows that all four SBI processors are capable of generating similar ground deformation results when the data set has sufficient temporal sampling and a stable ground backscatter mechanism like urban area. Strengths and limitations of different SBI processors were analyzed based on data set configuration and environmental conditions and are summarized in this paper to guide future users of SBI techniques

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Measurement of the top-quark mass in tt¯ events with dilepton final states in pp collisions at √s = 7 TeV

Author: Abbaneo D.
Abbiendi G.
Abbrescia M.
Abdullin S.
Abdulsalam A.
Acosta D.
Acosta J. G.
Acosta M. Vazquez
Adair A.
Adam N.
Adam W.
Adams M. R.
Adams T.
Adiguzel A.
Adler V.
Adzic P.
Agram J. L.
Aguilar Benitez M.
Aguilo E.
Ahmad M.
Ahmad W. Haj
Ahuja S.
Akchurin N.
Akgun B.
Akgun U.
Akin I. V.
Alagoz E.
Albajar C.
Albayrak E. A.
Albergo S.
Albrow M.
Alcaraz Maestre J.
AldaJunior W. L.
Alexander J.
Aliev T.
Alimena J.
Almeida N.
Alverson G.
Alves A.
Alves G. A.
Amapane N.
Amsler C.
Anagnostou G.
Anastassov A.
Anderson J.
Anderson M.
Andrea J.
Andreev V.
Andreev V.
Andreev Y.u.
Andrews W.
Anghel I. M.
Anh TV
Anjos T. S.
Ansari M. H.
Antonelli L.
Antunes J. Rodrigues
Antunovic Z.
Apanasevich L.
Appelt E.
Apresyan A.
Apyan A.
Arce P.
Arcidiacono R.
Arenton M. W.
Arfaei H.
Argiro S.
Arneodo M.
Arora S.
Asawatangtrakuldee C.
Asghar M. I.
Askew A.
Assran Y.
Ata M.
Attikis A.
Auffray E.
Autermann C.
Auzinger G.
Avdeeva E.
Avery P.
Avetisyan A.
Avila C.
Azarkin M.
Azhgirey I.
Aziz T.
Azzi P.
Azzolini V.
Azzurri P.
Baarmand M. M.
Babb J.
Bacchetta N.
Bachtis M.
Baden A.
Baeni L.
Baffioni S.
Bagliesi G.
Bai Y.
Baillon P.
Bainbridge R.
Bakhshiansohi H.
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Barbagli G.
Barberis E.
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MESSINEO ALBERTO MARIA
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Publication venue: 'Springer Science and Business Media LLC'
Publication date: 01/01/2012
Field of study

Open Access: This article is distributed under the terms of the Creative Commons Attribution License.-- Chatrchyan, S. et al.The top-quark mass is measured in proton-proton collisions at s√=7 TeV using a data sample corresponding to an integrated luminosity of 5.0 fb−1 collected by the CMS experiment at the LHC. The measurement is performed in the dilepton decay channel tt¯→(ℓ+νℓb)(ℓ−ν¯¯ℓb¯), where ℓ=e,μ. Candidate top-quark decays are selected by requiring two leptons, at least two jets, and imbalance in transverse momentum. The mass is reconstructed with an analytical matrix weighting technique using distributions derived from simulated samples. Using a maximum-likelihood fit, the top-quark mass is determined to be 172.5±0.4 (stat.)±1.5 (syst.) GeV.Acknowledge support from BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); MoER, SF0690030s09 and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France);BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); MSI (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MON, RosAtom, RAS and RFBR (Russia); MSTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); ThEP, IPST and NECTEC (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA). Individuals have received support from the Marie-Curie program and the European Research Council (European Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander von Humboldt Foundation; the Austrian Science Fund (FWF); 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 (IWTBelgium); the Ministry of Education, Youth and Sports (MEYS) of Czech Republic; the Council of Science and Industrial Research, India; the Compagnia di San Paolo (Torino); and the HOMING PLUS program of Foundation for Polish Science, cofinanced from European Union, Regional Development Fund.Peer Reviewe

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Publication date: 01/01/2022
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Bestintzanos I
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Cabrera A
Cabrillo IJ
Cacchio V
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Cheng C
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Chernyavskaya N
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Cheung HWK
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Christoforou K
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Ciangottini D
Cifuentes JAB
Ciocci MA
Cipriani M
Citron M
Cittolin S
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Civinini C
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Clare R
Clement E
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Cockerill DJA
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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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Abu Zeid S
Acharya H
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Alcerro Alcerro LF
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Aldá Júnior WL
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Alves Gallo Pereira M
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Publication venue: Springer Science and Business Media LLC
Publication date: 27/07/2023
Field of study

A search for long-lived particles decaying in the outer regions of the CMS silicon tracker or in the calorimeters is presented. The search is based on a data sample of proton-proton collisions at √s = 13 TeV recorded with the CMS detector at the LHC in 2016–2018, corresponding to an integrated luminosity of 138 fb−1. A novel technique, using nearly trackless and out-of-time jet information combined in a deep neural network discriminator, is employed to identify decays of long-lived particles. The results are interpreted in a simplified model of chargino-neutralino production, where the neutralino is the next-to-lightest supersymmetric particle, is long-lived, and decays to a gravitino and either a Higgs or Z boson. This search is most sensitive to neutralino proper decay lengths of approximately 0.5 m, for which masses up to 1.18 TeV are excluded at 95% confidence level. The current search is the best result to date in the mass range from the kinematic limit imposed by the Higgs boson mass up to 1.8 TeV.SCOAP

Brunel University Research Archive

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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

Author: Aarrestad TK
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Duric S
Durkin LS
Dutta I
Dutta S
Dutta S
Dutta V
Dziwok C
Dünser M
D’Alessandro R
D’Alfonso M
D’Amante V
d’Enterria D
D’Hondt J
Eble F
Ebrahimi A
Eckerlin G
Ecklund KM
Eckstein D
Eerola P
Ehataht K
Eich M
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Eliseev D
Elkafrawy T
Ellis KV
Elmer P
Elmetenawee W
Elvira VD
Emediato L
Eno SC
Epshteyn V
Erbacher R
Erdmann M
Erdmann W
Erice C
Errico F
Escobar JV
Eskut E
Espinosa TAG
Estrada CU
Etesami SM
Eusebi R
Evangelou I
Evans A
Evdokimov O
Everaerts P
Eysermans J
Fabbri F
Fabozzi F
Faccioli P
Fackeldey P
Faham HE
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
Feindt F
Feld L
Feng Y
Ferbel T
Ferencek D
Ferguson T
Fernandez M
Fernández AÁ
Fernández JRG
Ferrero DDR
Ferri F
Ferro F
Field RD
Figueiredo DM
Filatov O
Filho MBF
Finco L
Finger M
Finger M
Fiore L
Fiorendi S
Fiorina D
Fischer B
Flacher H
Flix J
Florent A
Florez C
Florio AD
Flowers Z
Flügge G
Focardi E
Folgueras S
Fontanesi E
Ford WT
Forthomme L
Foudas C
Fouz MC
Fraga J
Francis B
Frankenthal A
Franzoni G
Freed S
Freeman J
Freer C
Fröhlich A
Funk W
Gadallah MMA
Gadkari D
Galanti M
Galli M
Gallinaro M
Gallo E
Galloni C
Gandrajula RP
Gandrakota A
Ganjour S
Gao X
Garbers C
Garcia F
Garcia JMV
Garcia-Bellido A
García CL
Gardner P
Garutti E
Gary JW
Gascon S
Gastler D
Gavrilov G
Gavrilov V
Gecse Z
Gedia K
Geiser A
Gennai S
Gerber CE
Gerosa R
Gershtein Y
Geurts FJM
Ghezzi A
Ghosh S
Ghosh S
Giacomelli P
Giammanco A
Giani S
Gianneios P
Giannini L
Giassi A
Giffels M
Gigi D
Gilbert A
Giljanovic D
Gill K
Gilmore J
Giommi L
Giraldi A
Glege F
Glessgen F
Gleyzer SV
Glowacki M
Gninenko S
Godinovic N
Goerlach U
Goh J
Goldouzian R
Goldstein J
Golf F
Golovtcov V
Golubev N
Golutvin I
Gomber B
Gomez G
Gomez JP
Gomez-Ceballos G
Goncharov M
Gonzalez BA
Gonzalez HB
Gorbunov I
Gordon M
Gosewisch JO
Gottmann A
Goulianos K
Gouskos L
Gouzevitch M
Govoni P
Govorkova E
Grab C
Grandi C
Gras P
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Greau G
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Greenberg B
Greene S
Gregores EM
Grenier G
Grimault C
Grippo M
Gritsan AV
Grohsjean A
Grosso G
Grunewald M
Grynyov B
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Grünendahl S
Guchait M
Guerrero D
Guglielmi V
Guiang J
Guiducci L
Guisao JM
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Gupta R
Gurrola A
Gutay L
Guthoff M
Gutiérrez GR
Gutsche O
Guzzi L
Gómez LU
Górski M
Gülmez E
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Habibullah R
Hacisahinoglu B
Haddad Y
Hadjiiska R
Hadley M
Hadley NJ
Hagopian V
Hahn KA
Hajdu C
Hajheidari M
Hakala J
Hakimi A
Halkiadakis E
Hall AR
Hall G
Haller J
Hamilton D
Han S
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Hanson G
Haranko M
Harder K
Harikrishnan B
Harilal A
Harper S
Harris P
Harris RM
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Hassani A
Hassanshahi MH
Hatakeyama K
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Heath HF
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Heikkilä JK
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Heintz U
Heller R
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Hernandez AC
Hernandez AMV
Hernandez JM
Herndon M
Hernández AS
Herrera CAM
Herrera CM
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Herwig TC
Higginbotham S
Hildreth M
Hill C
Hiltbrand J
Hindrichs O
Hinzmann A
Hirosky R
Hirschauer J
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Hoepfner K
Hofman DJ
Hogan JM
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Hoh SY
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Hollar J
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Holmes T
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Hoorani HR
Horisberger R
Horvath D
Horyn L
Horzela M
Hos I
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Hove PV
Howard A
Hu M
Hu Z
Huang T
Huh C
Husemann U
Hussain PS
Huwiler M
Iaselli G
Iashvili I
Iaydjiev P
Ibarguen HAS
Iemmi F
Ignatenko M
Iles G
Ille B
Incandela J
Ince M
Ingram Q
Innocente V
Iorio AOM
Iqbal MA
Isidori T
Isik C
Isildak B
Ivanchenko V
Ivanov A
Ivanov T
Ivanov Y
Ivone F
J. WI
Jabeen S
Jabusch HR
Jafari A
Jaffel K
Jain S
Jain S
James T
Jang W
Janot P
Janssen T
Jaramillo J
Jaroslawski D
Jarrin EC
Jarry P
Javaid T
Jayananda MK
Jayatilaka B
Jeitler M
Jensen F
Jeon S
Jessop C
Jiang CH
Jin W
Jindariani S
Jofrehei A
Johns W
Johnson M
Jomhari NZ
Jones M
Joo C
Josa MI
Joshi BM
Joshi U
Joyce M
Jung AW
Juodagalvis A
Júnior WLA
Kaadze K
Kachanov V
Kadastik M
Kaech B
Kaestli HC
Kailasapathy B
Kalbhor P
Kalinowski A
Kalogeropoulos A
Kamalieddin R
Kamon T
Kamtsikis C
Kang DY
Kang Y
Kansal B
Kansal R
Kanuganti AR
Kapoor A
Kapsiak C
Kar C
Kara O
Karacheban O
Karaman G
Karancsi J
Karapinar G
Karapostoli G
Karasavvas D
Karathanasis G
Karchin PE
Kardapoltsev L
Karjavine V
Karmakar S
Karneyeu A
Kasem A
Kasemann M
Kasieczka G
Kaspar J
Katsoulis P
Kaur A
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Kaur H
Kaur M
Kaveh H
Kaya M
Kaya O
Kaynak B
Kazana M
Keicher P
Kello T
Kellogg RG
Khakzad M
Khan A
Khan WA
Kharchilava A
Khazaie E
Khukhunaishvili A
Khurana R
Kiani B
Kieseler J
Kilminster B
Kilpatrick M
Kim B
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Kim GN
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Kim M
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Kim TJ
Kim V
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Kiminsu U
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Kinnunen R
Kioseoglou PGK
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Kirpichnikov D
Kirsanov M
Kirschenmann H
Klanner R
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Kleinwort C
Klijnsma T
Klima B
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Klyukhin V
Knolle J
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Kozyrev A
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Kratochwil N
Kravchenko I
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Kress T
Krikler B
Krintiras G
Krishna A
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Krolikowski J
Krupa J
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Krücker D
Kubota Y
Kukral O
Kumar A
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Kumar S
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Kumari P
Kuo CM
Kutzner V
Kuznetsova E
Kveton A
Kwan S
Kwok KHM
Kwon H
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Kyberd P
Kyriacou S
Kyriakis A
Köseyan OK
La Cruz IH-D
Labe F
Laflotte I
Laha A
Lai Y
Laktineh IB
Lam T
Lambrecht L
Lamichhane K
Lammel S
Lampén T
Lanaro A
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Lanev A
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Lara CEP
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Lawrence J
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Legger F
Lehti S
Leiton AGS
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Lemaitre V
Lemos DS
Lenzi P
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Leontsinis S
Lesauvage A
Lethuillier M
Letts J
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Liechti SP
Ligabue F
Liko D
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Linden JVD
Lindsey C
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Lipton R
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Litomin A
Litov L
Liu C
Liu G
Liu M
Liu T
Liu Y
Liu Z-A
Liyanage K
Lizzo M
Lo KH
Lobanov A
Loeliger A
Lohezic V
Lohmann W
Lomidze I
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Longo E
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Lopez OG
Lopez SG
Lopez-Fernandez R
Lotti M
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Lourenço C
Loveless R
Lowette S
Lu C
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Luna MB
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Lyon A-M
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Macchiolo A
MacDonald E
Madhu AM
Madigan G
Madrazo CF
Madrid C
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Maggi G
Maggi M
Magherini M
Maghrbi Y
Magnan A-M
Mahdavikhorrami M
Mahieu CL
Mahmoud MA
Maier B
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Maity M
Major P
Majumder D
Majumder G
Makarenko I
Makarenko V
Maksimovic P
Mal P
Malakhov A
Malara A
Malawski M
Malberti M
Malbouisson HB
Malcles J
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Malik S
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Mallampalli A
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Mamouni HE
Manca E
Mandal K
Mandorli G
Manganelli N
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Manousakis-Katsikakis A
Mans J
Manteca PJF
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Mantilla C
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Manzoni RA
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Marcellini S
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Marco ED
Margjeka I
Margoni M
Mariani V
Mariano J
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Marini AC
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Marzocchi B
Maríñez LGG
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Maselli S
Masetti G
Mason D
Massironi A
Masterson P
Mastrapasqua V
Mastrolorenzo L
Matchev K
Matorras F
Matthies C
Mattia AD
Matveev V
May S
Mazumdar K
Mcalister I
McBride P
McCauley T
Mcgrady C
McLean C
McMaster B
Mecca A
Mechelen PV
Meena M
Mehta A
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Meiring P
Melo A
Melzer-Pellmann I-A
Menasce D
Meneguzzo AT
Menendez JF
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Mikulec I
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Mohanty GB
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Monroy J
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Montoya CAC
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Morabit KE
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Mulargia R
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Mussgiller A
Muthumuni S
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Nasr-Storey SSE
Navarria FL
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Neogi O
Nessi-Tedaldi F
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Nicolaou C
Niedziela J
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Nielsen C
Nigamova A
Nikitenko A
Niknejad T
Nissan Y
Noehte L
Nogima H
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Noonan D
Norberg S
Norjoharuddeen NB
Novaes SF
Novak A
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Nowack A
Nowotny F
Nuzzo S
Nürnberg A
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Obraztsov S
Ocalan K
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Okawa H
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Onsem GPV
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Orimoto T
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Ortona G
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Osterberg K
Otarid Y
Ott J
Overton D
Ovtin I
Ozdemir K
Ozkorucuklu S
Paasch A
Pacher L
Padley BP
Padula SS
Paganis E
Paganoni M
Pak SI
Palichik V
Palit P
Palla F
Palmer C
Palomo LV
Panagiotou A
Pandey S
Pandolfi F
Pantaleo F
Panwar L
Paoletti S
Paolucci P
Papadimitriou V
Papadopoulos I
Papageorgakis C
Papakrivopoulos I
Papavergou I
Paramatti R
Paramesvaran S
Parashar N
Paredes S
Parida G
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Park SK
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Parolia S
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Patterson JR
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Paus C
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Pedraza I
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Pelayo JP
Pellecchia A
Pellett D
Pelliccioni M
Peltola T
Pena C
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Pereira AV
Pereira MAG
Perelygin V
Perera N
Perez CM
Perez CU
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Peris AD
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Pernia DL
Perovic V
Perraguin AB
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Perrotta A
Peruzzi M
Pervan N
Pesaresi M
Petersen HA
Petkov P
Petrilli A
Petrillo KFD
Petrov A
Petrow H
Petrucciani G
Petrushanko S
Petyt D
Pfeiffer A
Piccinelli A
Piccolo D
Pieri M
Pierini M
Pigazzini S
Pikurs G
Pinna D
Pinolini BS
Piparo D
Piperov S
Pisano M
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Pitters FM
Polatoz A
Polikarpov S
Pompili A
Pooth O
Popov V
Popova E
Portales L
Postiau N
Potenza R
Poudyal N
Pozdnyakov A
Pradhan R
Presilla M
Prieels C
Primavera F
Prosper H
Psallidas A
Ptochos F
Pugliese G
Pujahari PR
Puljak I
Purohit A
Pásztor G
Pétré L
Qian SJ
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Quach D
Quadfasel T
Quaranta C
Quast G
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Quijada JAM
Quinnan M
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Radburn-Smith BC
Radchenko O
Radogna R
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Rappoccio S
Raspereza A
Rastogi A
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Raymond DM
Razis PA
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Reed I
Regnard S
Regnery B
Reichert J
Reichmann M
Reid ID
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Reimers A
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Reitenspiess T
Reithler H
Rendón C
Revering M
Ricardo RES
Ricca GD
Riccardi C
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Rieger O
Rinkevicius A
Ristic B
Ristori L
Riti F
Rivero CM
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Robutti E
Rodozov M
Rodriguez KJP
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Rodríguez AS
Rodríguez SC
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Roguljic M
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Romeo F
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Rudrabhatla S
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Ryu MS
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Sahin MÖ
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Salfeld-Nebgen J
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Santanastasio F
Santocchia A
Santoro A
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Saradhy R
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Sauvan JB
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Savoy-Navarro A
Savrin V
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Schnepf M
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Schwanenberger C
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Schöfbeck R
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Senger M
Seo H
Setti F
Sexton-Kennedy E
Sfar HR
Sguazzoni G
Shafiei N
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Shang V
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Shchedrolosiev M
Shchelina K
Sheldon P
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Shepherd-Themistocleous CH
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Shopova M
Shtipliyski A
Shukla R
Shulha S
Shumka E
Shvetsov I
Si W
Siado JE
Siddireddy P
Siikonen H
Sikdar AK
Sikler F
Silva GC
Silva P
Silvestris L
Simkina P
Simone FM
Simonetto F
Simonis HJ
Simpson F
Simsek AE
Simsek C
Singh JB
Singla A
Sirois Y
Siroli GP
Siviero F
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Skovpen K
Skovpen Y
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Smirnov V
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Smith VJ
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Snow GR
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Zygala L
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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

Brunel University Research Archive

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Observation of electroweak W+W− pair production in association with two jets in proton-proton collisions at √s = 13 TeV

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Zou D
Zou R
Zucchetta A
Zumerle G
Zuo X
Zuolo D
Zygala L
Álvarez Fernández A
Özçelik Ö
Publication venue: 'Elsevier BV'
Publication date: 10/06/2023
Field of study

Copyright © 2022 The Author(s). An observation is reported of the electroweak production of a W+W− pair in association with two jets, with both W bosons decaying leptonically. The data sample corresponds to an integrated luminosity of 138 fb−1 of proton-proton collisions at √s = 13 TeV, collected by the CMS detector at the CERN LHC.Events are selected by requiring exactly two opposite-sign leptons (electrons or muons) and two jets with large pseudorapidity separation and high dijet invariant mass. Events are categorized based on the flavor of the final-state leptons. A signal is observed with a significance of 5.6 standard deviations (5.2 expected) with respect to the background-only hypothesis. The measured fiducial cross section is 10.2 ± 2.0 fb and this value is consistent with the standard model prediction of 9.1 ± 0.6 fb.SCOAP3

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Yumiceva F
Yzquierdo AP-C
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Zahid S
Zaleski S
Zalewski P
Zanetti M
Zarubin A
Zarucki M
Zecchinelli AG
Zeinali M
Zeuner WD
Zghiche A
Zhang F
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Zhao J
Zhizhin I
Zhokin A
Zhu RY
Ziemons T
Zipper N
Zoi I
Zolkapli Z
Zorbakir IS
Zorbilmez C
Zotto P
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Zumerle G
Zuo X
Zuolo D
Zygala L
Álvarez CR
Özçelik Ö
Publication venue: Springer Science and Business Media LLC
Publication date: 06/07/2023
Field of study

A search is reported for pairs of light Higgs bosons (H1) produced in supersymmetric cascade decays in f inal states with small missing transverse momentum. A data set of LHC pp collisions collected with the CMS detector at √s = 13TeV and corresponding to an integrated lumi nosity of 138fb−1 is used. The search targets events where both H1 bosons decay into b¯b pairs that are reconstructed as large-radius jets using substructure techniques. No evi dence is found for an excess of events beyond the back ground expectations of the standard model (SM). Results from the search are interpreted in the next-to-minimal super symmetric extension of the SM, where a “singlino” of small mass leads to squark and gluino cascade decays that can pre dominantly end in a highly Lorentz-boosted singlet-like H1 andasinglino-likeneutralinoofsmalltransversemomentum. Upperlimitsaresetontheproductofthesquarkorgluinopair production cross section and the square of the b¯b branching fraction of the H1 in a benchmark model containing almost mass-degenerategluinosandlight-flavoursquarks.Underthe assumption of an SM-like H1 → b¯b branching fraction, H1 bosonswithmassesintherange40–120GeVarisingfromthe decays of squarks or gluinos with a mass of 1200–2500GeV are excluded at 95% confidence level.SCOA

Brunel University Research Archive

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Search for a massive scalar resonance decaying to a light scalar and a Higgs boson in the four b quarks final state with boosted topology

Author: Aarrestad TK
Aarup Petersen H
Abbaneo D
Abbiendi G
Abbrescia M
Abdalla H
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
Aggleton R
Agram J-L
Aguilar-Benitez M
Ahmad A
Ahmad M
Ahmed A
Ahuja S
Aimè C
Akchurin N
Akgun B
Akpinar A
Albergo S
Albert A
Albrecht S
Albrow M
Alcaraz Maestre J
Aldaya Martin M
Aldá Júnior WL
Aleksandrov A
Alexander J
Alhusseini M
Alimena J
Alison J
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
Andreassi G
Andreev V
Andreev Y
Andrejkovic JW
Andrews MB
Androsov K
Anguiano J
Antchev G
Anthony D
Antunovic Z
Apollinari G
Apparu D
Appelt E
Apresyan A
Apyan A
Araujo M
Arcaro D
Arcidiacono R
Arenton MW
Argiro S
Arneodo M
Aruta C
Asavapibhop B
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
Azarkin M
Aziz T
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Azzurri P
Baarmand MM
Babaev A
Babbar J
Bacchetta N
Bachiller I
Bachtis M
Backhaus M
Baden A
Baechler J
Bagliesi G
Bahinipati S
Baillon P
Bainbridge R
Bakas G
Bakhshiansohi H
Bakshi AS
Baldenegro Barrera C
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Barnes VE
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Baron O
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Barrio Luna M
Barroso Ferreira Filho M
Bartek R
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Battilana C
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Bauerdick LAT
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Benitez JF
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Berenguer Antequera J
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Bermúdez Martínez A
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Bestintzanos I
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Brigljevic V
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Yohay R
Yoo HD
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Yumiceva F
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Zhizhin I
Zhokin A
Zhu RY
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Zimermmane Castro Santos A
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Zorbilmez C
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Zygala L
Álvarez Fernández A
Özçelik Ö
Publication venue: 'Elsevier BV'
Publication date: 27/08/2022
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”.Copyright © 2022 The Author(s). We search for new massive scalar particles X and Y through the resonant process X → YH → bb¯bb¯,, where H is the standard model Higgs boson. Data from CERN LHC proton-proton collisions are used, collected at a centre-of-mass energy of 13 TeV in 2016–2018 and corresponding to an integrated luminosity of 138 fb−1. The search is performed in mass ranges of 0.9–4 TeV for X and 60–600 GeV for Y, where both Y and H are reconstructed as Lorentz-boosted single large-area jets. The results are interpreted in the context of the next-to-minimal supersymmetric standard model and also in an extension of the standard model with two additional singlet scalar fields. The 95% confidence level upper limits for the production cross section vary between 0.1 and 150 fb depending on the X and Y masses, and represent a significant improvement over results from previous searches.SCOAP3

Brunel University Research Archive

Observation of triple J/ψ meson production in proton-proton collisions

Author: Aarrestad TK
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Abbiendi G
Abbrescia M
Abdelalim AA
Abdullah WATW
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Andrejkovic JW
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Bauerdick LAT
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Cumalat JP
Cummings G
Cussans D
Cutts D
Czellar S
Da Costa EM
Da Silveira GG
Dabrowski A
Dalchenko M
Dallavalle GM
Damanakis K
Damarseckin S
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Danilov M
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Darej D
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de Barbaro P
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de Monchenault GH
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De Souza SF
de Trocóniz JF
De Wolf EA
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Deile M
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González CAS
Gorbunov I
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Gosewisch JO
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Gutiérrez GR
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Jarrin EC
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Júnior WLA
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Khakzad M
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Krolikowski J
Kropivnitskaya A
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Kuznetsova E
Kveton A
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Köseyan OK
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Laha A
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Titov M
Tiwari PC
Tkaczyk S
Tobar ÁN
Tok UG
Toldaiev O
Tomalin IR
Tomei TRFP
Toms M
Tonelli G
Tonjes MB
Tonon N
Topaksu AK
Toriashvili T
Tornago M
Toropin A
Torterotot L
Tosi M
Tosi S
Touquet G
Townsend A
Tramontano R
Tran NV
Tran TT
Trapote A
Treille D
Trembath-Reichert S
Trevisani N
Tricomi A
Trocino D
Trocsanyi ZL
Tropea P
Troshin S
Tsamalaidze Z
Tsatsos A
Tsipolitis G
Tsirou A
Tully C
Tumasyan A
Tuo S
Tuominen E
Tuominiemi J
Turini N
Turkcapar S
Tuuva T
Tuve C
Tytgat M
Tyurin N
Tziaferi E
Uchida K
Ujvari B
Ulmer KA
Ulrich R
Uniyal R
Uplegger L
Usai E
Uvarov L
Uzunian A
Vaandering EW
Vagnerini A
Vai I
Valencia FV
Valsecchi D
Valuev V
Van De Klundert M
Van Der Linden J
Van Doninck W
Van Hove P
Van Mechelen P
Van Onsem GP
Van Putte S
Vanlaer P
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Velde CV
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Venturi A
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Verma RK
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Vila I
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Villalba CV
Virdee T
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Vischia P
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Vlimant JR
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Volkov A
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Von Cube RF
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Webb SN
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Whitbeck A
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Wichmann K
Wickramage N
Wickramarathna DDC
Wiedenbeck S
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Winterbottom D
Wisecarver A
Wissing C
Wit AD
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Wu HY
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Xiang Y
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Yarar H
Yates BR
Yazgan E
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Yetkin EA
Yi K
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Yohay R
Yoo HD
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Yuldashev BS
Yumiceva F
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Yzquierdo AP-C
Zabi A
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Zecchinelli AG
Zeid SA
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Zeuner WD
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Zhang H
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Zhang W
Zhang Y
Zhang Y
Zhang Y
Zhang Z
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Zhizhin I
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Özçelik Ö
Publication venue: 'Springer Science and Business Media LLC'
Publication date: 19/01/2023
Field of study

Data availability: Tabulated results are provided in the HEPData record for this analysis71. 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.Code availability: The CMS core software is publically available at https://github.com/cms-sw/cmssw.Copyright . Protons consist of three valence quarks, two up-quarks and one down-quark, held together by gluons and a sea of quark-antiquark pairs. Collectively, quarks and gluons are referred to as partons. In a proton-proton collision, typically only one parton of each proton undergoes a hard scattering – referred to as single-parton scattering – leaving the remainder of each proton only slightly disturbed. Here, we report the study of double- and triple-parton scatterings through the simultaneous production of three J/ψ mesons, which consist of a charm quark-antiquark pair, in proton-proton collisions recorded with the CMS experiment at the Large Hadron Collider. We observed this process – reconstructed through the decays of J/ψ mesons into pairs of oppositely charged muons – with a statistical significance above five standard deviations. We measured the inclusive fiducial cross-section to be 272+141−104(stat)±17(syst)fb, and compared it to theoretical expectations for triple-J/ψ meson production in single-, double- and triple-parton scattering scenarios. Assuming factorization of multiple hard-scattering probabilities in terms of single-parton scattering cross-sections, double- and triple-parton scattering are the dominant contributions for the measured process.SCOAP3.Change history: 27 February 2023A Correction to this paper has been published: https://doi.org/10.1038/s41567-023-01992-

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Brunel University Research Archive