205 research outputs found
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
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonelli S
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arms KE
- Armstrong SR
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barashkou A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bee C
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Belhorma B
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellina F
- Bellomo G
- Bellomo M
- Belloni A
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benedict BH
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernardet K
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertin A
- Bertinelli F
- Bertolucci F
- Besana MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianco M
- Biebel O
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Bingul A
- Bini C
- Biscarat C
- Bischof R
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Boaretto C
- Bobbink GJ
- Bobrovnikov VB
- Bocci A
- Bock R
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bona M
- Boonekamp M
- Boorman G
- Booth CN
- Booth JRA
- Booth P
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borroni S
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Boulahouache C
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Braccini S
- Bracinik J
- Braem A
- Brambilla E
- Branchini P
- Branco MDO
- Brandenburg GW
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Brett ND
- Bright-Thomas PG
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brubaker E
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Buescher V
- Bueso XP
- Bugge L
- Buira-Clark D
- Buis EJ
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butin F
- Butler B
- Butler JM
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- Zhemchugov A
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
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- Zhemchugov A
- Zheng S
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- Zitoun R
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- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
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- Amram N
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- Arabidze G
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- Castillo IS
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- Demirkoz B
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- Enari Y
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- Escalier M
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- Esch H
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- Escobar C
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- Espinal Curull X
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- Esposito B
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- Etienne F
- Etienne F
- Etienvre AI
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- Etzion E
- Etzion E
- Evans H
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- Fabbri L
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- Facini G
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- Farrell S
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- Farrington SM
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- Farthouat P
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- Fassi F
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- Fassnacht P
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- Fassouliotis D
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- Favareto A
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- Federic P
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- Fedin OL
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- Fedorko W
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- Fehling-Kaschek M
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- Feigl S
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- Feligioni L
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- Feng C
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- Feng EJ
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- Fenyuk AB
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- Fernando W
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- Ferrando BMS
- Ferrando J
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- Ferrara V
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- Ferrari A
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- Fiedler F
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- Filipcic A
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- Filipuzzi M
- Filipuzzi M
- Filthaut F
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- Fincke-Keeler M
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- Fitzgerald EA
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- Fleck I
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- Fleischmann S
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- Fletcher G
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- Floderus A
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- Florez Bustos AC
- Flowerdew MJ
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- Formica A
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- Forti A
- Forti A
- Fortin D
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- Francavilla P
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- Franklin M
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- Franz S
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- French ST
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- Gadatsch S
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- Gadomski S
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- Gagnon P
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- Gallo V
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- Gallop BJ
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- Garcia BRM
- Garcia C
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- Gardner RW
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- Garelli N
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- Garonne V
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- Garrido MDMC
- Gatti C
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- Gaudio G
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- Gaur B
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- Gauzzi P
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- Gavrilenko IL
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- Gay C
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- Gaycken G
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- Gazis EN
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- Ge P
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- Gecse Z
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- Gee CNP
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- Geerts DAA
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- Geich-Gimbel C
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- Gellerstedt K
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- Gemme C
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- Genest MH
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- Gentile S
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- George M
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- Gerbaudo D
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- Gershon A
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- Ghazlane H
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- Ghodbane N
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- Giacobbe B
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- Giannetti P
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- Giokaris N
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- Giordani MP
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- Giordano R
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- Giugni D
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- Giuliani C
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- Gorini E
- Gorini E
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- Gornicki E
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- Goshaw AT
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- Gostkin MI
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
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- Yoshihara K
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- Youssef S
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- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- Zeniš T
- Zerwas D
- Zevi Della Porta G
- Zhang D
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- Zhang L
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- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivković L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MS
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Gonzalez BA
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Bella LA
- Apolle R
- Arabidze G
- Aracena I
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
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- Zeitnitz C
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- Zerwas D
- della Porta GZ
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
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- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fb−1 of s=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan β < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
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- Abdallah J
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- Yilmaz M
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- Zaidan R
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- Zajacova Z
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- Zanzi D
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- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Z′ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fb−1 in the e + e − channel and 5.0 fb−1 in the μ + μ −channel. A Z ′ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal Z′ Models
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adam ER
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- Adragna P
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- Aesky S
- Agar-Savedra JA
- Agustoni M
- Ahlen SP
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- Ahsan M
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- Akesson TPA
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- Akimov AV
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- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
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- Allbrooke BMM
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- Zobernig G
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- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Convergence among Non-Sister Dendritic Branches: An Activity-Controlled Mean to Strengthen Network Connectivity
- Author
- A Mason
- A Ostling
- A Polsky
- A Roxin
- A van Ooyen
- A van Ooyen
- AI Gulyás
- B Lin
- BL Chen
- CF Olson
- D Baranes
- D Baranes
- Danny Baranes
- DB Chklovskii
- Eshel Ben-Jacob
- ET Kavalali
- G Liu
- GA Chauvet
- H Hasegawa
- J van Pelt
- JC López-García
- JG Jefferys
- JH Kong
- JL Krichmar
- Joshua Cove
- JQ Zheng
- JZ Parrish
- L Lovmar
- LF Lago-Fernandes
- LS Furtado
- M Kohrmann
- M Maletic-Savatic
- M Migliore
- Maytal Foox
- N Kalisman
- N Masuda
- O Shefi
- P Rousseeuw
- P Vetter
- Pablo Blinder
- PB Sargent
- Q Wen
- R Condit
- R Criado
- S Dudoit
- S Konur
- SD Washington
- SE Grebenyuk
- TS Skoglund
- V Latora
- V Latora
- V Sytnyk
- ZA Bortolotto
- ZF Mainen
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2008
- Field of study
The manner by which axons distribute synaptic connections along dendrites remains a fundamental unresolved issue in neuronal development and physiology. We found in vitro and in vivo indications that dendrites determine the density, location and strength of their synaptic inputs by controlling the distance of their branches from those of their neighbors. Such control occurs through collective branch convergence, a behavior promoted by AMPA and NMDA glutamate receptor activity. At hubs of convergence sites, the incidence of axo-dendritic contacts as well as clustering levels, pre- and post-synaptic protein content and secretion capacity of synaptic connections are higher than found elsewhere. This coupling between synaptic distribution and the pattern of dendritic overlapping results in ‘Economical Small World Network’, a network configuration that enables single axons to innervate multiple and remote dendrites using short wiring lengths. Thus, activity-mediated regulation of the proximity among dendritic branches serves to pattern and strengthen neuronal connectivity
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