175 research outputs found
Measurement of jet production in deep inelastic scattering and NNLO determination of the strong coupling at ZEUS
- Author
- Abt I
- Aggarwal R
- Aushev V
- Behnke O
- Bertolin A
- Bloch I
- Brock I
- Brook NH
- Brugnera R
- Bruni A
- Bussey PJ
- Caldwell A
- Catterall CD
- Chwastowski J
- Ciborowski J
- Ciesielski R
- Cooper-Sarkar AM
- Corradi M
- Dementiev RK
- Dusini S
- Ferrando J
- Foster B
- Gallo E
- Gangadharan D
- Garfagnini A
- Geiser A
- Grzelak G
- Gwenlan C
- Hochman D
- Jomhari NZ
- Kadenko I
- Karshon U
- Kaur P
- Klanner R
- Klein U
- Korzhavina IA
- Kovalchuk N
- Kuze M
- Levchenko BB
- Levy A
- Lohrmann E
- Longhin A
- Lorkowski F
- Lunghi E
- Löhr B
- Makarenko I
- Malka J
- Masciocchi S
- Nagano K
- Nam JD
- Onishchuk Y
- Paul E
- Pidhurskyi I
- Polini A
- PrzybycieĆ M
- Quintero A
- Ruspa M
- Schneekloth U
- Schörner-Sadenius T
- Selyuzhenkov I
- Shchedrolosiev M
- Shcheglova LM
- Sherrill N
- Skillicorn IO
- Solano A
- Stanco L
- Stefaniuk N
- Surrow B
- SĆomiĆski W
- Tokushuku K
- Turkot O
- Tymieniecka T
- Verbytskyi A
- Wan Abdullah WAT
- Wichmann K
- Wing M
- Yamada S
- Yamazaki Y
- Zenaiev O
- ƻarnecki AF
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/11/2023
- Field of study
A new measurement of inclusive-jet cross sections in the Breit frame in neutral current deep inelastic scattering using the ZEUS detector at the HERA collider is presented. The data were taken in the years 2004â2007 at a centre-of-mass energy of 318GeV and correspond to an integrated luminosity of 347pb-1 . The jets were reconstructed using the kt -algorithm in the Breit reference frame. They have been measured as a function of the squared momentum transfer, Q2 , and the transverse momentum of the jets in the Breit frame, pâ„ , Breit . The measured jet cross sections are compared to previous measurements and to perturbative QCD predictions. The measurement has been used in a next-to-next-to-leading-order QCD analysis to perform a simultaneous determination of parton distribution functions of the proton and the strong coupling, resulting in a value of αs(MZ2)=0.1142±0.0017(experimental/fit)-0.0007+0.0006(model/parameterisation)-0.0004+0.0006(scale) , whose accuracy is improved compared to similar measurements. In addition, the running of the strong coupling is demonstrated using data obtained at different scales
Search for effective Lorentz and CPT violation using ZEUS data
- Author
- Abt I
- Aggarwal R
- Aushev V
- Behnke O
- Bertolin A
- Bloch I
- Brock I
- Brook NH
- Brugnera R
- Bruni A
- Bussey PJ
- Caldwell A
- Catterall CD
- Chwastowski J
- Ciborowski J
- Ciesielski R
- Cooper-Sarkar AM
- Corradi M
- Dementiev RK
- Dusini S
- Ferrando J
- Foster B
- Gallo E
- Gangadharan D
- Garfagnini A
- Geiser A
- Grzelak G
- Gwenlan C
- Hochman D
- Jomhari NZ
- Kadenko I
- Karshon U
- Kaur P
- Klanner R
- Korzhavina IA
- Kovalchuk N
- Kuze M
- Levchenko BB
- Levy A
- Longhin A
- Lorkowski F
- Lunghi E
- Löhr B
- Makarenko I
- Malka J
- Masciocchi S
- Nagano K
- Nam JD
- Onishchuk Y
- Paul E
- Pidhurskyi I
- Polini A
- PrzybycieĆ M
- Quintero A
- Ruspa M
- Schneekloth U
- Schörner-Sadenius T
- Selyuzhenkov I
- Shchedrolosiev M
- Shcheglova LM
- Sherrill N
- Skillicorn IO
- Solano A
- Stanco L
- Stefaniuk N
- Surrow B
- SĆomiĆski W
- Tokushuku K
- Turkot O
- Tymieniecka T
- Verbytskyi A
- Wan Abdullah WAT
- Wichmann K
- Wing M
- Yamada S
- Yamazaki Y
- Zarnecki AF
- Zenaiev O
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/05/2023
- Field of study
Lorentz and CPT symmetry in the quark sector of the Standard Model are studied in the context of an effective field theory using ZEUS e±p data. Symmetry-violating effects can lead to time-dependent oscillations of otherwise time-independent observables, including scattering cross sections. An analysis using five years of inclusive neutral-current deep inelastic scattering events corresponding to an integrated HERA luminosity of 372 pb-1 at s=318 GeV has been performed. No evidence for oscillations in sidereal time has been observed within statistical and systematic uncertainties. Constraints, most for the first time, are placed on 42 coefficients parametrizing dominant CPT-even dimension-four and CPT-odd dimension-five spin-independent modifications to the propagation and interaction of light quarks
Impact of jet-production data on the next-to-next-to-leading-order determination of HERAPDF2.0 parton distributions
- Author
- Abdullah WAT Wan
- Abt I
- Aggarwal R
- Andreev V
- Arratia M
- Aushev V
- Baghdasaryan A
- Baty A
- Begzsuren K
- Behnke O
- Belousov A
- Bertolin A
- Bloch I
- Boudry V
- Brandt G
- Brock I
- Brook NH
- Brugnera R
- Bruni A
- Buniatyan A
- Bussey PJ
- Bystritskaya L
- Caldwell A
- Campbell AJ
- Cantun Avila KB
- Catterall CD
- Cerny K
- Chekelian V
- Chen Z
- Chwastowski J
- Ciborowski J
- Ciesielski R
- Contreras JG
- Cooper-Sarkar AM
- Corradi M
- Currie J
- Cvach J
- Dainton JB
- Daum K
- Dementiev RK
- Deshpande A
- Diaconu C
- Dusini S
- Eckerlin G
- Egli S
- Elsen E
- Favart L
- Fedotov A
- Feltesse J
- Ferrando J
- Fleischer M
- Fomenko A
- Foster B
- Gal C
- Gallo E
- Gangadharan D
- Garfagnini A
- Gayler J
- Gehrmann T
- Gehrmann-De Ridder A
- Geiser A
- Gladilin LK
- Glover EWN
- Goerlich L
- Gogitidze N
- Golubkov Yu A
- Gouzevitch M
- Grab C
- Greenshaw T
- Grindhammer G
- Grzelak G
- Gwenlan C
- Haidt D
- Henderson RCW
- Hladky J
- Hochman D
- Hoffmann D
- Horisberger R
- Hreus T
- Huber F
- Huss A
- Jacobs PM
- Jacquet M
- Janssen T
- Jomhari NZ
- Jung AW
- Jung H
- Kadenko I
- Kapichine M
- Karshon U
- Katzy J
- Kaur P
- Kiesling C
- Klanner R
- Klein M
- Klein U
- Kleinwort C
- Klest HT
- Kogler R
- Korzhavina IA
- Kostka P
- Kovalchuk N
- Kretzschmar J
- Kruecker D
- Kruger K
- Kuze M
- Landon MPJ
- Lange W
- Laycock P
- Lee SH
- Levchenko BB
- Levonian S
- Levy A
- Li W
- Lin J
- Lipka K
- List B
- List J
- Lobodzinski B
- Loehr B
- Lohrmann E
- Long OR
- Longhin A
- Lorkowski F
- Lukina O Yu
- Makarenko I
- Malinovski E
- Malka J
- Martyn H-U
- Masciocchi S
- Maxfield SJ
- Mehta A
- Mendez L Cunqueiro
- Meyer AB
- Meyer J
- Mikocki S
- Mikuni VM
- Mondal MM
- Morgan T
- Morozov A
- Muller K
- Nachman B
- Nagano K
- Nam JD
- Naumann Th
- Newman PR
- Niebuhr C
- Niehues J
- Nowak G
- Olsson JE
- Onishchuk Yu
- Ozerov D
- Park S
- Pascaud C
- Patel GD
- Paul E
- Perez E
- Petrukhin A
- Picuric I
- Pidhurskyi I
- Pires J
- Pitzl D
- Polifka R
- Polini A
- Preins S
- Przybycien M
- Quintero A
- Rabbertz K
- Radescu V
- Raicevic N
- Ravdandorj T
- Reimer P
- Rizvi E
- Robmann P
- Roosen R
- Rostovtsev A
- Rotaru M
- Ruspa M
- Sankey DPC
- Sauter M
- Sauvan E
- Schmitt S
- Schmookler BA
- Schneekloth U
- Schoeffel L
- Schoening A
- Schoerner-Sadenius T
- Sefkow F
- Selyuzhenkov I
- Shchedrolosiev M
- Shcheglova LM
- Shushkevich S
- Skillicorn IO
- Slominski W
- Solano A
- Soloviev Y
- Sopicki P
- South D
- Spaskov V
- Specka A
- Stanco L
- Steder M
- Stefaniuk N
- Stella B
- Straumann U
- Sun C
- Surrow B
- Sutton MR
- Sykora T
- Thompson PD
- Tokushuku K
- Traynor D
- Tseepeldorj B
- Tu Z
- Turkot O
- Tymieniecka T
- Valkarova A
- Vallee C
- Van Mechelen P
- Verbytskyi A
- Wegener D
- Wichmann K
- Wing M
- Wunsch E
- Yamada S
- Yamazaki Y
- Zacek J
- Zarnecki AF
- Zenaiev O
- Zhang J
- Zhang Z
- Zlebcik R
- Zohrabyan H
- Zomer F
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 21/03/2022
- Field of study
The HERAPDF2.0 ensemble of parton distribution functions (PDFs) was introduced in 2015. The final stage is presented, a next-to-next-to-leading-order (NNLO) analysis of the HERA data on inclusive deep inelastic ep scattering together with jet data as published by the H1 and ZEUS collaborations. A perturbative QCD fit, simultaneously of αs(M2Z) and the PDFs, was performed with the result αs(M2Z)=0.1156±0.0011 (exp) +0.0001â0.0002 (model +parameterisation) ±0.0029 (scale). The PDF sets of HERAPDF2.0Jets NNLO were determined with separate fits using two fixed values of αs(M2Z), αs(M2Z)=0.1155 and 0.118, since the latter value was already chosen for the published HERAPDF2.0 NNLO analysis based on HERA inclusive DIS data only. The different sets of PDFs are presented, evaluated and compared. The consistency of the PDFs determined with and without the jet data demonstrates the consistency of HERA inclusive and jet-production cross-section data. The inclusion of the jet data reduced the uncertainty on the gluon PDF. Predictions based on the PDFs of HERAPDF2.0Jets NNLO give an excellent description of the jet-production data used as input
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmed A
- Ahuja S
- Aime C
- Akchurin N
- Akgun B
- Akpinar A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- AldĂĄ JĂșnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allen B
- Almond J
- Alvarez Gonzalez B
- Alverson G
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amendola C
- Amin N
- Amram O
- Amsler C
- Anagnostou G
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Antchev G
- Antunovic Z
- Apanasevich L
- Apollinari G
- 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
- Aspell P
- Atakisi IO
- Atanassov I
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awais A
- Awan MIM
- Ayala E
- Ayala G
- Aydogmus Sen F
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Baginyan A
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Bakirci MN
- Baldenegro Barrera C
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barnes VE
- Barney D
- Baron O
- Barrio Luna M
- Bartek R
- Bartosik N
- BartĂłk M
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baxter S
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Becerril Gonzalez H
- Bechtel J
- Bedoya CF
- Beghin D
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Belchior Batista Das Chagas E
- 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
- Berardi V
- Berenguer Antequera J
- Beretvas A
- Bergauer T
- Berger P
- Berger T
- Beri SB
- BermĂșdez MartĂnez A
- Bernardes CA
- Bernet C
- Berretti M
- Berry D
- Berryhill J
- Bertacchi V
- Besancon M
- Beschi A
- Bhal E
- Bhardwaj A
- Bharti M
- Bhat MA
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- Bhattacharya S
- Bhattacharya S
- Bheesette S
- Bhowmik D
- Bhowmik S
- Bhyun JH
- Bi R
- Bialkowska H
- Bianchini L
- Bianco M
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bin Anuar AA
- 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
- Boletti A
- Bologna S
- Bols ES
- Bonacorsi D
- Bonanomi M
- Bonham B
- Bonomally S
- Boos E
- Boran F
- Borchsh V
- Borg J
- Borgonovi L
- Bornheim A
- Borras K
- Bortignon P
- Bose T
- Bossini E
- Botta C
- Botta V
- Bottigli U
- Boudoul G
- Bouhali O
- Bourgatte G
- Bourilkov D
- Bozzo M
- Bragagnolo A
- Braghieri A
- Braibant-Giacomelli S
- Brainerd C
- Brandao Malbouisson H
- Brandt S
- Branson JG
- Breedon R
- Breeze S
- Brew C
- Brigljevic V
- Brinkerhoff A
- Brivio F
- Brochero Cifuentes JA
- Brom J-M
- Brondolin E
- Brooke JJ
- Brown RM
- Brunner D
- Bruno G
- Brzhechko D
- BrĂŒcken E
- Bucci R
- Buccilli A
- Buchanan J
- Buchmuller O
- Buchot Perraguin A
- Bueghly J
- Bundock A
- Bunkowski K
- Buontempo S
- Burkett K
- Burkhardt H
- Burkle B
- Burt K
- Bury F
- Busson P
- Busza W
- Butalla S
- Butler JN
- Butler PH
- Butz E
- Bylinkin A
- Bylsma B
- Cabrera A
- Cabrillo IJ
- Cadamuro L
- Cafagna FS
- Caillol C
- Cakir A
- Calandri A
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Call K
- Calligaris L
- Calzaferri S
- Camen C
- Caminada L
- Campagnari C
- Campanini R
- Campbell A
- Camporesi T
- Candelise V
- Canelli MF
- Canepa A
- Cankocak K
- Capeans Garrido M
- Capiluppi P
- Cappati A
- Caputo C
- Caraway B
- Cardini A
- Cardwell B
- Carle A
- Carlin R
- Carrera Jarrin E
- Carrillo Montoya CA
- Carrillo Moreno S
- Cartiglia N
- Carvalho Antunes De Oliveira A
- Carvalho W
- Casarsa M
- Caspart R
- Cassese A
- Castaldi R
- Castaneda Hernandez A
- Castilla-Valdez H
- Castro A
- Catanesi MG
- 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
- Chang P
- Chanon N
- Chao Y
- Chapon E
- Charaf O
- Charlot C
- Chatterjee RM
- Chatterjee S
- Chaudhary G
- Chauhan S
- Chauhan S
- Chawla R
- Chazin Quero B
- Checchia P
- Chekhovsky V
- Chen C
- Chen GM
- Chen HS
- Chen KF
- Chen M
- Chen PH
- Chen X
- Chen Y
- Chen Y
- Chen Z
- Chenarani S
- Cheng T
- Cheng Y
- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhibra SS
- Chiarito B
- Chinellato J
- Chistov R
- Chlebana F
- Cho S
- Choi J
- Choi S
- Choi Y
- Chou JP
- Choudhary BC
- Choudhury S
- Chu J
- Chudasama R
- Chwalek T
- Ciangottini D
- Ciocca C
- Ciocci MA
- Cipriani M
- Ciriolo V
- Cirkovic P
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clement E
- Clerbaux B
- CMS Collaboration<sup>â </sup>
- Cockerill DJA
- Coelho E
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Cometti S
- Connor P
- Consuegra RodrĂguez S
- Contardo D
- Conway J
- Conway R
- Cooper SI
- Cooperstein S
- Corcodilos L
- Cornelis T
- Cosby C
- Cossutti F
- Costa M
- Costa S
- Coubez X
- Couderc F
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Cranshaw DJ
- Creanza D
- Cremonesi M
- Cristella L
- CsanĂĄd M
- CsörgĆ T
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cummings G
- Cussans D
- Cutts D
- Czellar S
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Da Rold A
- Da Silveira GG
- Dabrowski A
- Daci N
- Dalchenko M
- Dallavalle GM
- Damarseckin S
- Damgov J
- Danilov M
- Danilov V
- Daponte V
- Darwish MR
- Das P
- Das S
- Dasgupta A
- Dash D
- Daskalakis G
- Dasu S
- Datta A
- Dauncey P
- David A
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- Davies G
- Davignon O
- De Barbaro P
- De Boer W
- De Bruyn I
- De Castro Manzano P
- De Clercq J
- De Cosa A
- De Filippis N
- De Guio F
- De Iorio A
- De Jesus Damiao D
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Leo K
- De Leonardis F
- De Palma M
- De Roeck A
- De TrocĂłniz JF
- De Wit A
- De Wolf EA
- Deelen N
- Defranchis MM
- Deile M
- Dejardin M
- Del Burgo R
- Del Re D
- Delaere C
- Delannoy AG
- Delcourt M
- Delgado Peris A
- Delgado A
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demina R
- Demiragli Z
- Demiroglu ZS
- Denegri D
- Depasse P
- Dermenev A
- Dev N
- Dewanjee RK
- Dezoort G
- Dharmaratna WGD
- Dhingra N
- Di Croce D
- Di Domenico MR
- Di Florio A
- Di Marco E
- Di Maria R
- Di Mattia A
- Di Pilato A
- Diab B
- Diamantopoulou M
- Diaz D
- Didukh L
- Diemoz M
- Dierlamm A
- Dildick S
- Dilsiz K
- Dimitrov A
- Dimova T
- Dinardo ME
- Dini P
- Diotalevi T
- Dissertori G
- Dittmann J
- Dittmar M
- Dittmer S
- Dobson M
- Dobur D
- Dogra S
- Dolek F
- Dolen J
- Dominguez A
- DomĂnguez Damiani D
- Donato S
- DonegĂ M
- Donertas IS
- Dordevic M
- Dorfer C
- Dorigo T
- Dorney B
- Doroba K
- Dorsett A
- Doubek M
- Dozen C
- Dragicevic M
- Dremin I
- Dreyer T
- Droll A
- Druzhkin D
- Duarte Campderros J
- Duarte J
- Dube S
- Dubinin M
- Dudko L
- Dugad S
- Duh YT
- Dulemba JL
- Dumanoglu I
- Dupont N
- Durgut S
- Duric S
- Durkin LS
- Dutta D
- Dutta I
- Dutta S
- Dutta V
- Dziwok C
- DĂŒnser M
- Ebrahimi A
- Eckerlin G
- Ecklund KM
- Eckstein D
- Eerola P
- Eggert K
- Ehataht K
- Eich M
- Eichhorn T
- El Mamouni H
- El Morabit K
- Elgammal S
- Eliseev D
- Elkafrawy T
- Elliott-Peisert A
- Ellis KV
- Ellithi Kamel A
- Elmer P
- Elmetenawee W
- Elvira VD
- Eminizer M
- Emriskova N
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Eremin V
- Erice C
- Erodotou E
- Errico F
- Ershov A
- Erö J
- Escalante Del Valle A
- Eskut E
- Estevez Banos LI
- Etesami SM
- Eusebi R
- Evangelou I
- Evans A
- Evdokimov O
- Everaerts P
- Eysermans J
- Fabbri F
- Fabozzi F
- Faccioli P
- Fackeldey P
- Fallavollita F
- Fallon C
- Falmagne G
- Faltermann N
- Fanfani A
- Fang W
- Fangmeier C
- FanĂČ L
- Fasanella D
- Faure JL
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- Ăsterberg K
- Ăzçelik Ă
- Ć irokĂœ J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for dark matter in the form of strongly interacting massive particles (SIMPs) using the CMS detector at the LHC is presented. The SIMPs would be produced in pairs that manifest themselves as pairs of jets without tracks. The energy fraction of jets carried by charged particles is used as a key discriminator to suppress efficiently the large multijet background, and the remaining background is estimated directly from data. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 16.1 fb - 1 , collected with the CMS detector in 2016. No significant excess of events is observed above the expected background. For the simplified dark matter model under consideration, SIMPs with masses up to 100 GeV are excluded and further sensitivity is explored towards higher masses
Evidence for Top Quark Production in Nucleus-Nucleus Collisions
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- Ălvarez FernĂĄndez A
- Ăzçelik Ă
- Publication venue
- Publication date
- 01/01/2019
- Field of study
Peer reviewe
Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at root s=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
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- Ăzçelik Ă
- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe
Observation of a New Excited Beauty Strange Baryon Decaying to Îb- Ï+Ï-
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- Zahid S
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- Zorbilmez C
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- Ălvarez FernĂĄndez A
- Ăzçelik Ă
- Publication venue
- American Physical Society
- Publication date
- 01/01/2021
- Field of study
The Îb-Ï+Ï- invariant mass spectrum is investigated with an event sample of proton-proton collisions at s=13 TeV, collected by the CMS experiment at the LHC in 2016-2018 and corresponding to an integrated luminosity of 140 fb-1. The ground state Îb- is reconstructed via its decays to J/ÏÎ- and J/ÏÎK-. A narrow resonance, labeled Îb(6100)-, is observed at a Îb-Ï+Ï- invariant mass of 6100.3±0.2(stat)±0.1(syst)±0.6(Îb-) MeV, where the last uncertainty reflects the precision of the Îb- baryon mass. The upper limit on the Îb(6100)- natural width is determined to be 1.9 MeV at 95% confidence level. The low Îb(6100)- signal yield observed in data does not allow a measurement of the quantum numbers of the new state. However, following analogies with the established excited Îc baryon states, the new Îb(6100)- resonance and its decay sequence are consistent with the orbitally excited Îb- baryon, with spin and parity quantum numbers JP=3/2-
A Deep Neural Network for Simultaneous Estimation of b Jet Energy and Resolution
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- Simone FM
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- Ăzçelik Ă
- Publication venue
- Publication date
- 01/01/2020
- Field of study
We describe a method to obtain point and dispersion estimates for the energies of jets arising from b quarks produced in proton-proton collisions at an energy of s = 13 TeV at the CERN LHC. The algorithm is trained on a large sample of simulated b jets and validated on data recorded by the CMS detector in 2017 corresponding to an integrated luminosity of 41 fb - 1 . A multivariate regression algorithm based on a deep feed-forward neural network employs jet composition and shape information, and the properties of reconstructed secondary vertices associated with the jet. The results of the algorithm are used to improve the sensitivity of analyses that make use of b jets in the final state, such as the observation of Higgs boson decay to b b ÂŻ
Observation of the B-s(0) -> X(3872)phi Decay
- Author
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- Aarup Petersen H
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- Publication venue
- Publication date
- 01/01/2020
- Field of study
Using a data sample of proton-proton collisions at root s = 13 TeV, corresponding to an integrated luminosity of 140 fb(-1) collected by the CMS experiment in 2016-2018, the B-s(0) -> X(3872)phi decay is observed. Decays into J/psi pi(+)pi(-) and K+K- are used to reconstruct, respectively, the X(3872) and phi. The ratio of the product of branching fractions B[B-s(0) -> X(3872)phi]B[X(3872) -> J/psi pi(+)pi(-)] to the product B[B-s(0) ->psi(2S)phi]B[psi(2S) -> J/psi pi(+)pi(-)] is measured to be [2.21 +/- 0.29(stat) +/- 0.17(syst)]%. The ratio B[B-s(0) -> X(3872)phi]/B[B-0 -> X(3872)K-0] is found to be consistent with one, while the ratio B[B-s(0) -> X(3872)phi]/B[B+-> X(3872)K+] is two times smaller. This suggests a difference in the production dynamics of the X(3872) in B-0 and B(0)s meson decays compared to B+. The reported observation may shed new light on the nature of the X(3872) particle.Peer reviewe
Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of Ï Leptons in pp collisions at sqrt[s]=13ââTeV
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- Xiang Y
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- Yao Y
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- Yi K
- Yigitbasi E
- Yohay R
- Yoo HD
- Yoo J
- Yoon I
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- Yu D
- Yu GB
- Yu I
- Yu PR
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- Yuan L
- Yuan S
- Yuldashev BS
- Yumiceva F
- Yusli MN
- Zabi A
- Zacharopoulou A
- 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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- Zhizhin I
- Zhokin A
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- Zorbilmez C
- Zotto P
- Zotz A
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- Zuo X
- Zuolo D
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- Ălvarez FernĂĄndez A
- Ăzçelik Ă
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
Measurements of the inclusive and differential fiducial cross sections of the Higgs boson are presented, using the Ï lepton decay channel. The differential cross sections are measured as functions of the Higgs boson transverse momentum, jet multiplicity, and transverse momentum of the leading jet in the event, if any. The analysis is performed using proton-proton collision data collected with the CMS detector at the LHC at a center-of-mass energy of 13ââTeV and corresponding to an integrated luminosity of 138ââfb^{-1}. These are the first differential measurements of the Higgs boson cross section in the final state of two Ï leptons. In final states with a large jet multiplicity or with a Lorentz-boosted Higgs boson, these measurements constitute a significant improvement over measurements performed in other final states
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