165 research outputs found
Effective-energy budget in multiparticle production in nuclear collisions
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Non-perturbative computation of double inclusive gluon production in the Glasma
- Author
- A Adare
- A Adare
- A Dumitru
- A Dumitru
- A Kovner
- A Kovner
- A Krasnitz
- A Krasnitz
- A Krasnitz
- A Krasnitz
- A Krasnitz
- A Krasnitz
- A Krasnitz
- A Majumder
- AH Mueller
- AH Mueller
- AM Stasto
- B Alver
- BI Abelev
- BI Abelev
- C-Y Wong
- CB Chiu
- D Kharzeev
- DE Kharzeev
- E Ferreiro
- E Iancu
- E Iancu
- E Iancu
- E Iancu
- EV Shuryak
- F Gelis
- F Gelis
- F Gelis
- F Gelis
- F Gelis
- F Gelis
- F Gelis
- F Gelis
- F Wang
- H Fujii
- H Kowalski
- H Weigert
- H Weigert
- I Balitsky
- I Balitsky
- I Balitsky
- I Balitsky
- J Adams
- J Adams
- J Bartels
- J Jalilian-Marian
- J Jalilian-Marian
- J Jalilian-Marian
- J Jalilian-Marian
- J Jalilian-Marian
- JF Gunion
- JL Nagle
- JP Blaizot
- JP Blaizot
- K Dusling
- K Fukushima
- KJ Golec-Biernat
- KJ Golec-Biernat
- L Molnar
- LD McLerran
- LD McLerran
- LD McLerran
- M Daugherity
- M Gyulassy
- N Armesto
- PK Netrakanti
- R. Venugopalan
- S Gavin
- S. Srednyak
- SA Voloshin
- T Lappi
- T Lappi
- T Lappi
- T Lappi
- T Lappi
- T Lappi
- T. Lappi
- YV Kovchegov
- YV Kovchegov
- YV Kovchegov
- YV Kovchegov
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 02/03/2010
- Field of study
The near-side ridge observed in A+A collisions at RHIC has been described as
arising from the radial flow of Glasma flux tubes formed at very early times in
the collisions. We investigate the viability of this scenario by performing a
non-perturbative numerical computation of double inclusive gluon production in
the Glasma. Our results support the conjecture that the range of transverse
color screening of correlations determining the size of the flux tubes is a
semi-hard scale, albeit with non-trivial structure. We discuss our results in
the context of ridge correlations in the RHIC heavy ion experiments.Comment: 25 pages, 11 figures, uses JHEP3.cls V2: small clarifications,
published in JHE
Azimuthal anisotropy and correlations at large transverse momenta in p+p and Au+Au collisions at sNN= 200 GeV
- Author
- Adams J
- Aggarwal MM
- Ahammed Z
- Amonett J
- Anderson BD
- Arkhipkin D
- Averichev GS
- Badyal SK
- Bai Y
- Balewski J
- Barannikova O
- Barnby LS
- Baudot J
- Bekele S
- Belaga VV
- Bellwied R
- Berger J
- Bezverkhny BI
- Bharadwaj S
- Bhasin A
- Bhati AK
- Bhatia VS
- Bichsel H
- Billmeier A
- Bland LC
- Blyth CO
- Bonner BE
- Botje M
- Boucham A
- Brandin AV
- Bravar A
- Bystersky M
- Cadman RV
- Cai XZ
- Caines H
- Carroll J
- Castillo J
- Cebra D
- Chajecki Z
- Chaloupka P
- Chattopdhyay S
- Chen HF
- Chen Y
- Cheng J
- Cherney M
- Chikanian A
- Christie W
- Coffin JP
- Cormier TM
- Cramer JG
- Crawford HJ
- Das D
- Das S
- de Moura MM
- de Toledo AS
- Derevschikov AA
- Didenko L
- Dietel T
- Dogra SM
- Dong WJ
- Dong X
- Draper JE
- Du F
- Dubey AK
- Dunin VB
- Dunlop JC
- Eckardt V
- Edwards WR
- Efimov LG
- Emelianov V
- Engelage J
- Eppley G
- Erazmus B
- Estienne M
- Fachini P
- Faivre J
- Fatemi R
- Fedorisin J
- Filimonov K
- Filip P
- Finch E
- Fine V
- Fisyak Y
- Foley KJ
- Fomenko K
- Fu J
- Gagliardi CA
- Gans J
- Ganti MS
- Gaudichet L
- Geurts F
- Ghazikhanian V
- Ghosh P
- Gonzalez JE
- Grachov O
- Grebenyuk O
- Grosnick D
- Guertin SM
- Guo Y
- Gupta A
- Gutierrez TD
- Hallman TJ
- Hamed A
- Hardtke D
- Harris JW
- Heinz M
- Henry TW
- Hepplemann S
- Hippolyte B
- Hirsch A
- Hjort E
- Hoffmann GW
- Huang HZ
- Huang SL
- Hughes EW
- Humanic TJ
- Igo G
- Ishihara A
- Jacobs P
- Jacobs WW
- Janik M
- Jiang H
- Jones PG
- Judd EG
- Kabana S
- Kang K
- Kaplan M
- Keane D
- Khodyrev VY
- Kiryluk J
- Kisiel A
- Kislov EM
- Klay J
- Klein SR
- Klyachko A
- Koetke DD
- Kollegger T
- Kopytine M
- Kotchenda L
- Kramer M
- Kravtsov P
- Kravtsov VI
- Krueger K
- Kuhn C
- Kulikov AI
- Kumar A
- Kunz CL
- Kutuev RK
- Kuznetsov AA
- Lamont MAC
- Landgraf JM
- Lange S
- Laue F
- Lauret J
- Lebedev A
- Lednicky R
- Lehocka S
- LeVine MJ
- Li C
- Li Q
- Li Y
- Lindenbaum SJ
- Lisa MA
- Liu F
- Liu L
- Liu QJ
- Liu Z
- Ljubicic T
- Llope WJ
- Long H
- Longacre RS
- Lopez-Noriega M
- Love WA
- Lu Y
- Ludlam T
- Lynn D
- Ma GL
- Ma JG
- Ma YG
- Magestro D
- Mahajan S
- Mahapatra DP
- Majka R
- Mangotra LK
- Manweiler R
- Margetis S
- Markert C
- Martin L
- Marx JN
- Matis HS
- Matulenko YA
- Mazumdar MRD
- McClain CJ
- McShane TS
- Meissner F
- Melnick Y
- Meschanin A
- Miller ML
- Milosevich Z
- Minaev NG
- Mironov C
- Mischke A
- Mishra DK
- Mitchell J
- Mohanty B
- Molnar L
- Moore CF
- Morozov DA
- Munhoz MG
- Nandi BK
- Nayak SK
- Nayak TK
- Nelson JM
- Netrakanti PK
- Nikitin VA
- Nogach LV
- Nurushev SB
- Odyniec G
- Ogawa A
- Okorokov V
- Oldenburg M
- Olson D
- Pal SK
- Panebratsev Y
- Panitkin SY
- Pavlinov AI
- Pawlak T
- Peitzmann T
- Perevoztchikov V
- Perkins C
- Peryt W
- Petrov VA
- Phatak SC
- Picha R
- Planinic M
- Pluta J
- Porile N
- Porter J
- Poskanzer AM
- Potekhin M
- Potrebenikova E
- Potukuchi BVKS
- Prindle D
- Pruneau C
- Putschke J
- Rai G
- Rakness G
- Raniwala R
- Raniwala S
- Ravel O
- Ray RL
- Razin SV
- Reichhold D
- Reid JG
- Renault G
- Retiere F
- Ridiger A
- Ritter HG
- Roberts JB
- Rogachevskiy OV
- Romero JL
- Rose A
- Roy C
- Ruan L
- Sahoo R
- Sakrejda I
- Salur S
- Sanchez MCD
- Sandweiss J
- Savin I
- Sazhin PS
- Schambach J
- Scharenberg RP
- Schmitz N
- Schroeder LS
- Schweda K
- Seger J
- Seyboth P
- Shahaliev E
- Shao M
- Shao W
- Sharma M
- Shen WQ
- Shestermanov KE
- Shimanskiy SS
- Sichtermann E
- Simon F
- Singaraju RN
- Skoro G
- Smirnov N
- Snellings R
- Sood G
- Sorensen P
- Sowinski J
- Speltz J
- Spinka HM
- Srivastava B
- Stadnik A
- Stanislaus TDS
- STAR Collaboration .
- Stock R
- Stolpovsky A
- Strikhanov M
- Stringfellow B
- Suaide AAP
- Sugarbaker E
- Suire C
- Sumbera M
- Surrow B
- Symons TJM
- Szarwas P
- Tai A
- Takahashi J
- Tang AH
- Tarnowsky T
- Thein D
- Thomas JH
- Timoshenko S
- Tokarev M
- Trentalange S
- Tribble RE
- Tsai OD
- Ulery J
- Ullrich T
- Underwood DG
- Urkinbaev A
- Van Buren G
- van Leeuwen M
- Vander Molen AM
- Varma R
- Vasilevski IM
- Vasiliev AN
- Vernet R
- Vigdor SE
- Viyogi YP
- Vokal S
- Voloshin SA
- Vznuzdaev M
- Waggoner WT
- Wang F
- Wang G
- Wang G
- Wang XL
- Wang Y
- Wang Y
- Wang ZM
- Ward H
- Watson JW
- Webb JC
- Wells R
- Westfall GD
- Wetzler A
- Whitten C
- Wieman H
- Wissink SW
- Witt R
- Wood J
- Wu J
- Xu N
- Xu Z
- Xu ZZ
- Yamamoto E
- Yepes P
- Yurevich VI
- Zanevsky YV
- Zhang H
- Zhang WM
- Zhang ZP
- Zolnierczuk PA
- Zoulkarneev R
- Zoulkarneeva Y
- Zubarev AN
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2004
- Field of study
Results on high transverse momentum charged particle emission with respect to
the reaction plane are presented for Au+Au collisions at sNN=
200 GeV. Two- and four-particle correlations results are presented as well as a
comparison of azimuthal correlations in Au+Au collisions to those in p+p at
the same energy. Elliptic anisotropy, v2, is found to reach its maximum at
pt∼3 GeV/c, then decrease slowly and remain significant up to
pt≈7 -- 10 GeV/c. Stronger suppression is found in the back-to-back
high-pt particle correlations for particles emitted out-of-plane compared to
those emitted in-plane. The centrality dependence of v2 at intermediate
pt is compared to simple models based on jet quenching.Comment: 4 figures. Published version as PRL 93, 252301 (2004
Azimuthal anisotropy in Au+Au collisions at sqrtsNN = 200 GeV
- Author
- Adams J.
- Aggarwal MM
- Ahammed Z.
- Amonett J.
- Anderson BD
- Arkhipkin D.
- Averichev GS
- Badyal SK
- Bai Y.
- Balewski J.
- Barannikova O.
- Bari DD
- Barnby LS
- Baudot J.
- Bekele S.
- Belaga VV
- Bellwied R.
- Berger J.
- Bezverkhny BI
- Bharadwaj S.
- Bhasin A.
- Bhati AK
- Bhatia VS
- Bichsel H.
- Bielcik J.
- Bielcikova J.
- Billmeier A.
- Bland LC
- Blyth CO
- Bonner BE
- Botje M.
- Boucham A.
- Braem A.
- Brandin AV
- Bravar A.
- Bystersky M.
- Cadman RV
- Cai XZ
- Caines H.
- Castillo J.
- Cataldo GD
- Catu O.
- Cebra D.
- Chajecki Z.
- Chaloupka P.
- Chattopadhyay S.
- Chen HF
- Chen Y.
- Cheng J.
- Cherney M.
- Chikanian A.
- Christie W.
- Coffin JP
- Cormier TM
- Cramer JG
- Crawford HJ
- Das D.
- Das S.
- Davenport M.
- de Moura MM
- de Toledo AS
- Derevschikov AA
- Didenko L.
- Dietel T.
- Dogra SM
- Dong WJ
- Dong X.
- Draper JE
- Du F.
- Dubey AK
- Dunin VB
- Dunlop JC
- Eckardt V.
- Edwards WR
- Efimov LG
- Emelianov V.
- Engelage J.
- Eppley G.
- Erazmus B.
- Estienne M.
- Fachini P.
- Faivre J.
- Fatemi R.
- Fedorisin J.
- Filimonov K.
- Filip P.
- Finch E.
- Fine V.
- Fisyak Y.
- Fomenko K.
- Fu J.
- Gagliardi Carl A.
- Gaillard L.
- Gans J.
- Ganti MS
- Gaudichet L.
- Ghazikhanian V.
- Ghosh P.
- Gonzalez JE
- Grachov O.
- Grebenyuk O.
- Grosnick D.
- Guertin SM
- Guerts F.
- Guo Y.
- Gupta A.
- Gutierrez TD
- Hallman TJ
- Hamed A.
- Hardtke D.
- Harris JW
- Heinz M.
- Henry TW
- Hepplemann S.
- Hippolyte B.
- Hirsch A.
- Hjort E.
- Hoffmann GW
- Huang HZ
- Huang SL
- Hughes EW
- Humanic TJ
- Igo G.
- Ishihara A.
- Jacobs P.
- Jacobs WW
- Janik M.
- Jiang H.
- Jones PG
- Judd EG
- Kabana S.
- Kang K.
- Kaplan M.
- Keane D.
- Khodyrev VY
- Kiryluk J.
- Kisiel A.
- Kislov EM
- Klay J.
- Klein SR
- Koetke DD
- Kollegger T.
- Kopytine M.
- Kotchenda L.
- Kramer M.
- Kravtsov P.
- Kravtsov VI
- Krueger K.
- Kuhn C.
- Kulikov AI
- Kumar A.
- Kutuev RK
- Kuznetsov AA
- Lamont MAC
- Landgraf JM
- Langacre RS
- Lange S.
- Laue F.
- Lauret J.
- Lebedev A.
- Lednicky R.
- Lehocka S.
- LeVine MJ
- Li C.
- Li Q.
- Li Y.
- Lin G.
- Lindenbaum SJ
- Lisa MA
- Liu F.
- Liu L.
- Liu QJ
- Liu Z.
- Ljubicic T.
- Llope WJ
- Long H.
- Lopez-Noriega M.
- Love WA
- Lu Y.
- Ludlam T.
- Lynn D.
- Ma GL
- Ma JG
- Ma YG
- Magestro D.
- Mahajan S.
- Mahapatra DP
- Majka R.
- Mangotra LK
- Manweiler R.
- Margetis S.
- Markert C.
- Martin L.
- Martinengo P.
- Marx JN
- Matis HS
- Matulenko YA
- Mazumdar MRD
- McClain CJ
- McShane TS
- Meissner F.
- Melnick Y.
- Meschanin A.
- Miller ML
- Minaev NG
- Mironov C.
- Mischke A.
- Mishra DK
- Mitchell J.
- Mohanty B.
- Molen AMV
- Molnar L.
- Moore CF
- Morozov DA
- Munhoz MG
- Nandi BK
- Nappi E.
- Nayak SK
- Nayak TK
- Nelson JM
- Netrakanti PK
- Nikitin VA
- Nogach LV
- Nurushev SB
- Odyniec G.
- Ogawa A.
- Okorokov V.
- Oldenburg M.
- Olson D.
- Paic G.
- Pal SK
- Panebratsev Y.
- Panitkin SY
- Pavlinov AI
- Pawlak T.
- Peitzmann T.
- Perevoztchikov V.
- Perkins C.
- Peryt W.
- Petrov VA
- Phatak SC
- Picha R.
- Planinic M.
- Pluta J.
- Porile N.
- Porter J.
- Posa E.
- Poskanzer AM
- Potekhin M.
- Potrebenikova E.
- Potukuchi BVKS
- Prindle D.
- Pruneau C.
- Puiz F.
- Putschke J.
- Rakness G.
- Raniwala R.
- Raniwala S.
- Ravel O.
- Ray RL
- Razin SV
- Reichhold D.
- Reid JG
- Renault G.
- Retiere F.
- Ridiger A.
- Ritter HG
- Roberts JB
- Rogachevskiy OV
- Romero JL
- Rose A.
- Roy C.
- Ruan L.
- Sahoo R.
- Sakrejda I.
- Salur S.
- Sanchez MCD
- Sandweiss J.
- Sarsour M.
- Savin I.
- Sazhin PS
- Schambach J.
- Scharenberg RP
- Schmitz N.
- Schweda K.
- Schyns E.
- Seger J.
- Seyboth P.
- Shahaliev E.
- Shao M.
- Shao W.
- Sharma M.
- Shen WQ
- Shestermanov KE
- Shimanskiy SS
- Sichtermann E.
- Simon F.
- Singaraju RN
- Skoro G.
- Smirnov N.
- Snellings R.
- Sood G.
- Sorensen P.
- Sowinski J.
- Speltz J.
- Spinka H. M.
- Srivastava B.
- Stadnik A.
- Stanislaus TDS
- Star Collaboration
- STAR-RICH Collaboration.
- Stock R.
- Stolpovsky A.
- Strikhanov M.
- Stringfellow B.
- Suaide AAP
- Sugarbaker E.
- Suire C.
- Sumbera M.
- Surrow B.
- Symons TJM
- Szarwas P.
- Tai A.
- Takahashi J.
- Tang AH
- Tarnowsky T.
- Thein D.
- Thomas JH
- Timoshenko S.
- Tokarev M.
- Trainor TA
- Trentalange S.
- Tribble Robert E.
- Tsai OD
- Ulery J.
- Ullrich T.
- Underwood DG
- Urkinbaev A.
- van Buren G.
- van Leeuwen M.
- Varma R.
- Vasilevski IM
- Vasiliev AN
- Vernet R.
- Vigdor SE
- Viyogi YP
- Vokal S.
- Voloshin SA
- Vznuzdaev M.
- Waggoner WT
- Wang F.
- Wang G.
- Wang G.
- Wang XL
- Wang Y.
- Wang Y.
- Wang ZM
- Ward H.
- Watson JW
- Webb JC
- Wells R.
- Westfall GD
- Wetzler A.
- Whitten C.
- Wieman H.
- Wissink SW
- Witt R.
- Wood J.
- Wu J.
- Xu N.
- Xu Z.
- Xu ZZ
- Yamamoto E.
- Yepes P.
- Yurevich VI
- Zanevsky YV
- Zhang H.
- Zhang WM
- Zhang ZP
- Zoulkarneev R.
- Zoulkarneeva Y.
- Zubarev AN
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2005
- Field of study
The results from the STAR Collaboration on directed flow (v_1), elliptic flow
(v_2), and the fourth harmonic (v_4) in the anisotropic azimuthal distribution
of particles from Au+Au collisions at sqrtsNN = 200 GeV are summarized and
compared with results from other experiments and theoretical models. Results
for identified particles are presented and fit with a Blast Wave model.
Different anisotropic flow analysis methods are compared and nonflow effects
are extracted from the data. For v_2, scaling with the number of constituent
quarks and parton coalescence is discussed. For v_4, scaling with v_2^2 and
quark coalescence is discussed.Comment: 26 pages. As accepted by Phys. Rev. C. Text rearranged, figures
modified, but data the same. However, in Fig. 35 the hydro calculations are
corrected in this version. The data tables are available at
http://www.star.bnl.gov/central/publications/ by searching for "flow" and
then this pape
Azimuthal Charged-Particle Correlations and Possible Local Strong Parity Violation
- Author
- ABELEV BI
- AGGARWAL MM
- AHAMMED Z
- ALAKHVERDYANTS AV
- ANDERSON BD
- ARKHIPKIN D
- AVERICHEV GS
- BALEWSKI J
- BARANNIKOVA O
- BARNBY LS
- BAUMGART S
- BEAVIS DR
- BELLWIED R
- BENEDOSSO F
- BETANCOURT MJ
- BETTS RR
- BHASIN A
- BHATI AK
- BICHSEL H
- BIELCIK J
- BIELCIKOVA J
- BIRITZ B
- BLAND LC
- BNZAROV I
- BONNER BE
- BOUCHET J
- BRAIDOT E
- BRANDIN AV
- BRIDGEMAN A
- BRUNA E
- BUELTMANN S
- BURTON TP
- CAI XZ
- CAINES H
- CATU O
- CEBRA D
- CENDEJAS R
- CERVANTES MC
- CHAJECKI Z
- CHALOUPKA P
- CHATTOPADHYAY S
- CHEN HF
- CHEN JH
- CHEN JY
- CHENG J
- CHERNEY M
- CHIKANIAN A
- CHOI KE
- CHRISTIE W
- CHUNG P
- CLARKE RF
- CODRINGTON MJM
- CORLISS R
- CORMIER TM
- COSENTINO MR
- CRAMER JG
- CRAWFORD HJ
- DAS D
- DASH S
- DAUGHERITY M
- DE SILVA LC
- DE SOUZA RD
- DE TOLEDO A
- DEDOVICH TG
- DEPHILLIPS M
- DEREVSCHIKOV AA
- DIDENKO L
- DJAWOTHO P
- DOGRA SM
- DONG X
- DRACHENBERG JL
- DRAPER JE
- DUNLOP JC
- DZHORDZHADZE V
- EFIMOV LG
- ELHALHULI E
- ELNIMR M
- ENGELAGE J
- EPPLEY G
- ERAZMUS B
- ESTIENNE M
- EUN L
- FACHINI P
- FATEMI R
- FEDORISIN J
- FENG A
- FILIP P
- FINCH E
- FINE V
- FISYAK Y
- GAGLIARDI CA
- GANGADHARAN DR
- GANTI MS
- GARCIA-SOLIS EJ
- GEROMITSOS A
- GEURTS F
- GHAZIKHANIAN V
- GHOSH P
- GORBUNOV YN
- GORDON A
- GREBENYUK O
- GROSNICK D
- GRUBE B
- GUERTIN SM
- GUIMARAES KSFF
- GUPTA A
- GUPTA N
- GURYN W
- HAAG B
- HALLMAN TJ
- HAMED A
- HARRIS JW
- HEINZ M
- HEPPELMANN S
- HIRSCH A
- HJORT E
- HOFFMAN AM
- HOFFMANN GW
- HOFMAN DJ
- HOLLIS RS
- HUANG HZ
- HUMANIC TJ
- HUO L
- IGO G
- IORDANOVA A
- JACOBS P
- JACOBS WW
- JAKL P
- JENA C
- JIN F
- JONES CL
- JONES PG
- JOSEPH J
- JUDD EG
- KABANA S
- KAJIMOTO K
- KANG K
- KAPITAN J
- KAUDER K
- KEANE D
- KECHECHYAN A
- KETTLER D
- KHODYREV VY
- KIKOLA DP
- KIRYLUK J
- KISIEL A
- KLEIN SR
- KNOSPE AG
- KOCOLOSKI A
- KOETKE DD
- KONZER J
- KOPYTINE M
- KORALT I
- KORSCH W
- KOTCHENDA L
- KOUCHPIL V
- KRAVTSOV P
- KRAVTSOV VI
- KRUEGER K
- KRUS M
- KUMAR L
- KURNADI P
- LAMONT MAC
- LANDGRAF JM
- LAPOINTE S
- LAURET J
- LEBEDEV A
- LEDNICKY R
- LEE CH
- LEE JH
- LEIGHT W
- LEVINE MJ
- LI C
- LI N
- LI Y
- LIN G
- LINDENBAUM SJ
- LISA MA
- LIU F
- LIU H
- LIU J
- LIU L
- LJUBICIC T
- LLOPE WJ
- LONGACRE RS
- LOVE WA
- LU Y
- LUDLAM T
- MA GL
- MA YG
- MAHAPATRA DP
- MAJKA R
- MALL OI
- MANGOTRA LK
- MANWEILER R
- MARGETIS S
- MARKERT C
- MASUI H
- MATIS HS
- MATULENKO YA
- MAZUMDAR MRD
- MCDONALD D
- MCSHANE TS
- MESCHANIN A
- MILNER R
- MINAEV NG
- MIODUSZEWSKI S
- MISCHKE A
- MOHANTY B
- MOROZOV DA
- MUNHOZ MG
- NANDI BK
- NATTRASS C
- NAYAK TK
- NELSON JM
- NETRAKANTI PK
- NG MJ
- NOGACH LV
- NURUSHEV SB
- ODYNIEC G
- OGAWA A
- OKADA H
- OKOROKOV V
- OLSON D
- PACHR M
- PAGE BS
- PAL SK
- PANDIT Y
- PANEBRATSEV Y
- PAWLAK T
- PEITZMANN T
- PEREVOZTCHIKOV V
- PERKINS C
- PERYT W
- PHATAK SC
- PILE P
- PLANINIC M
- PLOSKON MA
- PLUTA J
- PLYKU D
- POLJAK N
- POSKANZER AM
- POTUKUCHI BVKS
- PRINDLE D
- PRUNEAU C
- PRUTHI NK
- PUJAHARI PR
- PUTSCHKE J
- RANIWALA R
- RANIWALA S
- RAY RL
- REDWINE R
- REED R
- RIDIGER A
- RITTER HG
- ROBERTS JB
- ROGACHEVSKIY OV
- ROMERO JL
- ROSE A
- ROY C
- RUAN L
- RUSSCHER MJ
- SAHOO R
- SAKAI S
- SAKREJDA I
- SAKUMA T
- SALUR S
- SANCHEZ MCD
- SANDWEISS J
- SCHAMBACH J
- SCHARENBERG RP
- SCHMITZ N
- SEELE J
- SEGER J
- SELYUZHENKOV I
- SEMERTZIDIS Y
- SEYBOTH P
- SHAHALIEV E
- SHAO M
- SHARMA M
- SHI SS
- SHI XH
- SICHTERMANN EP
- SIMON F
- SINGARAJU RN
- SKOBY MJ
- SMIRNOV N
- SORENSEN P
- SOWINSKI J
- SPINKA HM
- SRIVASTAVA B
- STANISLAUS TDS
- STASZAK D
- STRIKHANOV M
- STRINGFELLOW B
- SUAIDE AAP
- SUAREZ MC
- SUBBA NL
- SUMBERA M
- SUN XM
- SUN Y
- SUN Z
- SURROW B
- SYMONS TJM
- TAKAHASHI J
- TANG AH
- TANG Z
- TARINI LH
- TARNOWSKY T
- THEIN D
- THOMAS JH
- TIAN J
- TIMMINS AR
- TIMOSHENKO S
- TLUSTY D
- TOKAREV M
- TRAM VN
- TRENTALANGE S
- TRIBBLE RE
- TSAI OD
- ULERY J
- ULLRICH T
- UNDERWOOD DG
- VAN BUREN G
- VAN NIEUWENHUIZEN G
- VANFOSSEN JA
- VARMA R
- VASCONCELOS GMS
- VASILIEV AN
- VIDEBAEK F
- VIYOGI YP
- VOKAL S
- VOLOSHIN SA
- WADA M
- WALKER M
- WANG F
- WANG G
- WANG H
- WANG JS
- WANG Q
- WANG X
- WANG XL
- WANG Y
- WEBB G
- WEBB JC
- WESTFALL GD
- WHITTEN C
- WIEMAN H
- WISSINK SW
- WITT R
- WU Y
- XIE W
- XU N
- XU QH
- XU Y
- XU Z
- YANG Y
- YEPES P
- YIP K
- YOO IK
- YUE Q
- ZAWISZA M
- ZBROSZCZYK H
- ZHAN W
- ZHANG S
- ZHANG WM
- ZHANG XP
- ZHANG Y
- ZHANG ZP
- ZHAO Y
- ZHONG C
- ZHOU J
- ZHU X
- ZOULKARNEEV R
- ZOULKARNEEVA Y
- ZUO JX
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2009
- Field of study
Parity-odd domains, corresponding to nontrivial topological solutions of the QCD vacuum, might be created during relativistic heavy-ion collisions. These domains are predicted to lead to charge separation of quarks along the system’s orbital momentum axis. We investigate a three-particle azimuthal correlator which is a P even observable, but directly sensitive to the charge separation effect. We report measurements of charged hadrons near center-of-mass rapidity with this observable in Au+Au and Cu+Cu collisions at √sNN=200 GeV using the STAR detector. A signal consistent with several expectations from the theory is detected. We discuss possible contributions from other effects that are not related to parity violation
CASTLEGUARD : anonymised data streams with guaranteed differential privacy
- Author
- Adams J.
- Aggarwal MM
- Ahammed Z.
- Amonett J.
- Anderson BD
- Arkhipkin D.
- Averichev GS
- Bai Y.
- Balewski J.
- Barannikova O.
- Barnby LS
- Baudot J.
- Bekele S.
- Belaga VV
- Bellwied R.
- Berger J.
- Bezverkhny BI
- Bharadwaj S.
- Bhatia VS
- Bichsel H.
- Billmeier A.
- Bland LC
- Blyth CO
- Bonner BE
- Botje M.
- Boucham A.
- Brandin A.
- Bravar A.
- Bystersky M.
- Cadman RV
- Cai XZ
- Caines H.
- Carroll J.
- Castillo J.
- Cebra D.
- Chajecki Z.
- Chaloupka P.
- Chattopdhyay S.
- Chen HF
- Chen Y.
- Cheng J.
- Cherney M.
- Chikanian A.
- Christie W.
- Coffin JP
- Cormier TM
- Cramer JG
- Crawford HJ
- Das D.
- Das S.
- De Moura MM
- de Toledo AS
- Derevschikov AA
- Didenko L.
- Dietel T.
- Dong WJ
- Dong X.
- Draper JE
- Du F.
- Dubey AK
- Dunin VB
- Dunlop JC
- Eckardt V.
- Edwards WR
- Efimov LG
- Emelianov V.
- Engelage J.
- Eppley G.
- Erazmus B.
- Estienne M.
- Fachini P.
- Faivre J.
- Fatemi R.
- Fedorisin J.
- Filimonov K.
- Filip P.
- Finch E.
- Fine V.
- Fisyak Y.
- Foley KJ
- Fomenko K.
- Fu J.
- Gagliardi Carl A.
- Gans J.
- Ganti MS
- Gaudichet L.
- Geurts F.
- Ghazikhanian V.
- Ghosh P.
- Gonzalez JE
- Grachov O.
- Grebenyuk O.
- Grosnick D.
- Guertin SM
- Guo Y.
- Gupta A.
- Gutierrez TD
- Hallman TJ
- Hamed A.
- Hardtke D.
- Harris JW
- Heinz M.
- Henry TW
- Hepplemann S.
- Hiort E.
- Hippolyte B.
- Hirsch A.
- Hoffmann GW
- Huang HZ
- Huang SL
- Hughes EW
- Humanic TJ
- Igo G.
- Ishihara A.
- Jacobs P.
- Jacobs WW
- Janik M.
- Jiang H.
- Jones PG
- Judd EG
- Kabana S.
- Kang K.
- Kaplan M.
- Keane D.
- Khodyrev VY
- Kiryluk J.
- Kisiel A.
- Kislov EM
- Klay J.
- Klein SR
- Klyachko A.
- Koetke DD
- Kollegger T.
- Kopytine M.
- Kotchenda L.
- Kramer M.
- Kravtsov P.
- Kravtsov VI
- Krueger K.
- Kuhn C.
- Kulikov AI
- Kumar A.
- Kunz CL
- Kutuev RK
- Kuznetsov AA
- Lamont MAC
- Landgraf JM
- Lane F.
- Lange S.
- Lauret J.
- Lebedev A.
- Lednicky R.
- Lehocka S.
- LeVine MJ
- Li C.
- Li Q.
- Li Y.
- Lindenbaum SJ
- Lisa MA
- Liu F.
- Liu L.
- Liu QJ
- Liu Z.
- Ljubicic T.
- Llope WJ
- Long H.
- Longacre RS
- Lopez-Noriega M.
- Love WA
- Lu Y.
- Ludlam T.
- Lynn D.
- Ma GL
- Ma JG
- Ma YG
- Magestro D.
- Mahajan S.
- Mahapatra DP
- Majka R.
- Mangotra LK
- Manweiler R.
- Margetis S.
- Markert C.
- Martin L.
- Marx JN
- Matis HS
- Matulenko YA
- Mazumdar MRD
- McClain CJ
- McShane TS
- Meissner F.
- Melnick Y.
- Meschanin A.
- Miller ML
- Milosevich Z.
- Minaev NG
- Mironov C.
- Mischke A.
- Mishra D.
- Mitchell J.
- Mohanty B.
- Molnar L.
- Moore CF
- Mora-Corral MJ
- Morozov DA
- Morozov V.
- Munhoz MG
- Nandi BK
- Nayak TK
- Nelson JM
- Netrakanti PK
- Nikitin VA
- Nogach LV
- Norman B.
- Nurushev SB
- Odyniec G.
- Ogawa A.
- Okorokov V.
- Oldenburg M.
- Olson D.
- Pal SK
- Panebratsev Y.
- Panitkin SY
- Pavlinov AI
- Pawlak T.
- Peitzmann T.
- Perevoztchikov V.
- Perkins C.
- Peryt W.
- Petrov VA
- Phatak SC
- Picha R.
- Planinic M.
- Pluta J.
- Porile N.
- Porter J.
- Poskanzer AM
- Potekhin M.
- Potrebenikova E.
- Potukuchi BVKS
- Prindle D.
- Pruneau C.
- Putschke J.
- Rai G.
- Rakness G.
- Raniwala R.
- Raniwala S.
- Ravel O.
- Ray RL
- Razin SV
- Reichhold D.
- Reid JG
- Renault G.
- Retiere F.
- Ridiger A.
- Ritter HG
- Roberts JB
- Rogachevskiy OV
- Romero JL
- Rose A.
- Roy C.
- Ruan L.
- Sakrejda I.
- Salur S.
- Sanchez MCD
- Sandweiss J.
- Savin I.
- Sazhin PS
- Schambach J.
- Scharenberg RP
- Schmitz N.
- Schroeder LS
- Schweda K.
- Seger J.
- Seyboth P.
- Shahaliev E.
- Shao M.
- Shao W.
- Sharma M.
- Shen WQ
- Shestermanov KE
- Shimanskiy SS
- Simon F.
- Singaraju RN
- Skoro G.
- Smirnov N.
- Snellings R.
- Sood G.
- Sorensen P.
- Sowinski J.
- Speltz J.
- Spinka H. M.
- Srivastava B.
- Stadnik A.
- Stanislaus TDS
- Stock R.
- Stolpovsky A.
- Strikhanov M.
- Stringfellow B.
- Suaide AAP
- Sugarbaker E.
- Suire C.
- Sumbera M.
- Surrow B.
- Symons TJM
- Szarwas P.
- Tai A.
- Takahashi J.
- Tang AH
- Tarnowsky T.
- Thein D.
- Thomas JH
- Timoshenko S.
- Tokarev M.
- Trainor TA
- Trentalange S.
- Tribble Robert E.
- Tsai O.
- Ulery J.
- Ullrich T.
- Underwood DG
- Urkinbaev A.
- Van Buren G.
- van Leeuwen M.
- Vander Molen AM
- Varma R.
- Vasilevski IM
- Vasiliev AN
- Vernet R.
- Vigdor SE
- Viyogi VP
- Vokal S.
- Voloshin SA
- Vznuzdaev M.
- Waggoner B.
- Wang F.
- Wang G.
- Wang G.
- Wang XL
- Wang Y.
- Wang Y.
- Wang ZM
- Ward H.
- Watson JW
- Webb JC
- Wells R.
- Westfall GD
- Wetzler A.
- Whitten C.
- Wieman H.
- Wissink SW
- Witt R.
- Wood J.
- Wu J.
- Xu N.
- Xu Z.
- Xu ZZ
- Yamamoto E.
- Yepes P.
- Yurevich VI
- Zanevsky YV
- Zhang H.
- Zhang WM
- Zhang ZP
- Zolnierezuk PA
- Zoulkarneev R.
- Zoulkarneeva Y.
- Zubarev AN.
- Publication venue
- 'Institute of Electrical and Electronics Engineers (IEEE)'
- Publication date
- 01/01/2004
- Field of study
Data streams are commonly used by data controllers to outsource the processing of real-time data to third-party data processors. Data protection legislation and best practice in data management support the view that data controllers are responsible for providing a guarantee of privacy for user data contained within published data streams. Continuously Anonymising STreaming data via adaptive cLustEring (CASTLE) is an established method for anonymising data streams with a guarantee of k-anonymity. However, k-anonymity has been shown to be a weak privacy guarantee that has vulnerabilities in practical applications. In this paper we propose Continuously Anonymising STreaming data via adaptive cLustEring with GUAR-anteed Differential privacy (CASTLEGUARD), a data stream anonymisation algorithm that provides a reliable guarantee of k-anonymity, l-diversity and differential privacy to data subjects. We analyse CASTLEGUARD to show that, through safe k-anonymisation and β-sampling, the proposed approach satisfies differentially private k-anonymity. Further, we demonstrate the efficacy of the approach in the context of machine learning, presenting experimental analysis to demonstrate that it can be used to protect the individual privacy of users whilst maintaining the utility of a data stream
Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at root s=8 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adair A
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adzic P
- Agapitos A
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Al-bataineh A
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Alderweireldt S
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alimena J
- Almond J
- Alunni Solestizi L
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Amsler C
- Anagnostou G
- Anderson D
- Anderson I
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Anelli C
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asilar E
- Asin I
- Askew A
- Ata M
- Attikis A
- Aubin A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Awad A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Baber M
- Bacchetta N
- Bachmair F
- Bachtis M
- Baden A
- Baffioni S
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Ball AH
- Ball F
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Barbagli G
- Barberis E
- Barbieri R
- Bargassa P
- Baringer P
- Barker A
- Barnes VE
- Barney D
- Baron O
- Barone L
- Barria P
- Bartek R
- Barth C
- Bartosik N
- Bartók M
- Baskakov A
- Battilana C
- Baty A
- Bauerdick LAT
- Baumgartel D
- Baus C
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Beck L
- Beernaert K
- Behera PK
- Behnamian H
- Behnke O
- Behrens U
- Bein S
- Beirão Da Cruz E Silva C
- Belchior Batista Das Chagas E
- Belforte S
- Beliy N
- Belknap DA
- Bell KW
- Bellan R
- Belloni A
- Beluffi C
- Belyaev A
- Belyaev A
- Benato L
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Beni N
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Besancon M
- Betchart B
- Betts RR
- Bhandari R
- Bhardwaj A
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- Bhattacharya S
- Bhawandeep U
- Bhopatkar V
- Bhowmik S
- Bi R
- Bialkowska H
- Bian JG
- Bianchini L
- Bianco S
- Bierwagen K
- Biino C
- Bilei GM
- Bilin B
- Bilki B
- Bilmis S
- Bin Anuar AA
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Boccali T
- Bocci A
- Bodek A
- Boimska B
- Boletti A
- Bolla G
- Bonacorsi D
- Bonato A
- Bondu O
- Boos E
- Bornheim A
- Borras K
- Bortignon P
- Borzou A
- Bose S
- Bose T
- Botta C
- Boudoul G
- Bouhali O
- Bourilkov D
- Bouvier E
- Bradmiller-Feld J
- Braghieri A
- Braibant-Giacomelli S
- Brandstetter J
- Brandt S
- Branson JG
- Breedon R
- Breto G
- Brew C
- Brianza L
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Brinson J
- Brito L
- Brivio F
- Brochero Cifuentes JA
- Brochet S
- Brodski M
- Brom J-M
- Brondolin E
- Brooke JJ
- Brown RM
- Brun H
- Bruner C
- Bruno G
- Buchmuller O
- Bucinskaite I
- Bundock A
- Bunin P
- Bunkowski K
- Bunn J
- Buontempo S
- Burkett K
- Burns D
- Burns D
- Burt K
- Burton D
- Busson P
- Busza W
- Butler JN
- Butler PH
- Buttignol M
- Butz E
- Bylsma B
- Byszuk A
- Bäni L
- Cabrera A
- Cabrillo IJ
- Cadamuro L
- Caillol C
- Cakir A
- Calabria C
- Calamba A
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Call K
- Calligaris L
- Calpas B
- Calvelli V
- Calvert B
- Calvo E
- Caminada L
- Campagnari C
- Campanini R
- Campbell A
- Camporesi T
- Candelise V
- Canelli MF
- Cankocak K
- Capiluppi P
- Caputo C
- Carlin R
- Carlson B
- Carnes A
- Carrera Jarrin E
- Carrillo Montoya CA
- Carrillo Moreno S
- Cartiglia N
- Carvalho Antunes De Oliveira A
- Carvalho W
- Carver M
- Casal B
- Casarsa M
- Casasso S
- Casimiro Linares E
- Castaldi R
- Castaneda Hernandez A
- Castello R
- Castilla-Valdez H
- Castiñeiras De Saa JR
- Castle J
- Castro A
- Caudron A
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Celik A
- Centis Vignali M
- Cepeda M
- Cerati GB
- Cerminara G
- Cerrada M
- Chabert EC
- Chamizo Llatas M
- Chang P
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Chaparro Sierra LF
- Chapon E
- Charaf O
- Charlot C
- Chasco M
- Chatterjee A
- Chatterjee K
- Chatterjee RM
- Chauhan S
- Chauhan S
- Chaves J
- Chawla R
- Checchia P
- Chen GM
- Chen HS
- Chen KF
- Chen KH
- Chen M
- Chen PH
- Chen Y
- Chen Y
- Chen Z
- Chenarani S
- Cheng T
- Cherepanov V
- Chertok M
- Cheung HWK
- Chhibra SS
- Chierici R
- Chinellato J
- Chiochia V
- Chiorboli M
- Chistov R
- Chlebana F
- Cho S
- Choi M
- Choi S
- Choi Y
- Chou JP
- Choudhary BC
- Choudhury S
- Chtchipounov L
- Chu J
- Chudasama R
- Chwalek T
- Ciangottini D
- Cieri D
- Cihangir S
- Cimmino A
- Ciocci MA
- Cipriani M
- Cirkovic P
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clarke C
- Clement E
- Clerbaux B
- Cockerill DJA
- Cocoros A
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Colombo F
- Connor P
- Contardo D
- Conte E
- Contreras-Campana C
- Contreras-Campana E
- Conway J
- Conway R
- Cooper SI
- Cornelis T
- Corpe L
- Correa Martins Junior M
- Cossutti F
- Costa M
- Costa S
- Costanza F
- Coubez X
- Couderc F
- Coughlan JA
- Courbon B
- Cousins R
- Covarelli R
- Cowden C
- Cox B
- Cox PT
- Creanza D
- Cremonesi M
- Cristella L
- Cuevas J
- Cuffiani M
- Cumalat JP
- Curras E
- Curry D
- Cussans D
- Custódio A
- Cutts D
- Czellar S
- Da Costa EM
- Da Silveira GG
- Dabrowski A
- Daci N
- Dahmes B
- Dalchenko M
- Dallavalle GM
- Dall’Osso M
- Damarseckin S
- Damgov J
- Danilov M
- Daponte V
- Das S
- Daskalakis G
- Dasu S
- Dauncey P
- David A
- Davies G
- Davignon O
- de Barbaro P
- De Boer W
- De Bruyn I
- De Castro Manzano P
- De Cosa A
- De Filippis N
- De Gruttola M
- De Guio F
- De Jesus Damiao D
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Mattia M
- De Nardo G
- De Oliveira Martins C
- De Palma M
- De Roeck A
- de Trocóniz JF
- De Visscher S
- De Wit A
- De Wolf EA
- Degano A
- Deiters K
- Dejardin M
- Del Re D
- Delaere C
- Delannoy AG
- Delannoy H
- Delcourt M
- Delgado Peris A
- Delgado A
- Della Negra M
- Della Ricca G
- Dell’Orso R
- Demaria N
- Demina R
- Demiragli Z
- Demiroglu ZS
- Denegri D
- Depasse P
- Derdzinski M
- Dermenev A
- Deroover K
- Dev N
- Devetak D
- Dewanjee RK
- Dey S
- Di Francesco A
- Di Guida S
- Di Marco E
- Di Matteo L
- Di Mattia A
- Diamond B
- Diemoz M
- Dierlamm A
- Dietz C
- Dietz-Laursonn E
- Diez Pardos C
- Dildick S
- Dilsiz K
- Dimitrov A
- Dinardo ME
- Dishaw A
- Dissertori G
- Dittmann J
- Dittmar M
- Dittmer S
- Doan TH
- Dobson M
- Dobur D
- Dodd L
- Dogra S
- Dolen J
- Dolinska G
- Dominguez A
- Donato S
- Donegà M
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
Peer reviewe
Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
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- Ahmed I
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search for dark matter produced in association with top quarks in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. The data set used corresponds to an integrated luminosity of 35.9 fb(-1) recorded with the CMS detector at the LHC. Whereas previous searches for neutral scalar or pseudoscalar mediators considered dark matter production in association with a top quark pair only, this analysis also includes production modes with a single top quark. The results are derived from the combination of multiple selection categories that are defined to target either the single top quark or the top quark pair signature. No significant deviations with respect to the standard model predictions are observed. The results are interpreted in the context of a simplified model in which a scalar or pseudoscalar mediator particle couples to a top quark and subsequently decays into dark matter particles. Scalar and pseudoscalar mediator particles with masses below 290 and 300 GeV, respectively, are excluded at 95% confidence level, assuming a dark matter particle mass of 1 GeV and mediator couplings to fermions and dark matter particles equal to unity.Peer reviewe
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta G
- Adam W
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
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- 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
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