835 research outputs found
Search for Kaluza-Klein Graviton Emission in ppˉ Collisions at s=1.8 TeV using the Missing Energy Signature
- Author
- Acosta D
- Affolder T
- Akimoto H
- Albrow MG
- Ambrose D
- Amidei D
- Anikeev K
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
- Asakawa T
- Ashmanskas W
- Azfar F
- Azzi-Bacchetta P
- Bacchetta N
- Bachacou H
- Badgett W
- Bailey S
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Barone M
- Bauer G
- Bedeschi F
- Behari S
- Belforte S
- Bell WH
- Bellettini G
- Bellinger J
- Benjamin D
- Bensinger J
- Beretvas A
- Berryhill J
- Bhatti A
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
- Bloom K
- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bolla G
- Bolshov A
- Bonushkin Y
- Bortoletto D
- Boudreau J
- Brandl A
- Bromberg C
- Brozovic M
- Brubaker E
- Bruner N
- Budagov J
- Budd HS
- Burkett K
- Busetto G
- Byrum KL
- Cabrera S
- Calafiura P
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cecco SD
- Cerri A
- Cerrito L
- Chan AW
- Chang PS
- Chang PT
- Chapman J
- Chen C
- Chen YC
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
- Chu ML
- Chung JY
- Chung WH
- Chung YS
- Ciobanu CI
- Clark AG
- Coca M
- Connolly A
- Convery M
- Conway J
- Cordelli M
- Cranshaw J
- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
- Dagenhart D
- de Barbaro P
- de Troconiz JF
- de Troconiz JF
- DeJongh F
- Dell'Agnello S
- Dell'Orso M
- Demers S
- Demortier L
- Deninno M
- Denis RS
- Derwent PF
- Devlin T
- Dionisi C
- Dittmann JR
- Dominguez A
- Donati S
- Dorigo T
- Eddy N
- Einsweiler K
- Engels E
- Erbacher R
- Errede D
- Errede S
- Eusebi R
- Fan Q
- Farrington S
- Feild RG
- Fernandez JP
- Ferretti C
- Field RD
- Fiori I
- Flaugher B
- Flores-Castillo LR
- Foster GW
- Franklin M
- Freeman J
- Friedman J
- Fukui Y
- Furic I
- Galeotti S
- Gallas A
- Gallinaro M
- Gao T
- Garcia-Sciveres M
- Garfinkel AF
- Gatti P
- Gay C
- Gerdes DW
- Gerstein E
- Giagu S
- Giannetti P
- Giolo K
- Giordani M
- Giromini P
- Glagolev V
- Glenzinski D
- Gold M
- Goldschmidt N
- Goldstein J
- Gomez G
- Goncharov M
- Gorelov I
- Goshaw AT
- Gotra Y
- Goulianos K
- Green C
- Greene MG
- Gresele A
- Grim G
- Grosso-Pilcher C
- Guenther M
- Guillian G
- Haas RM
- Haber C
- Hahn SR
- Halkiadakis E
- Hall C
- Handa T
- Handler R
- Happacher F
- Hara K
- Hardman AD
- Harris RM
- Hartmann F
- Hatakeyama K
- Hauser J
- Heinrich J
- Heiss A
- Hennecke M
- Herndon M
- Hill C
- Hocker A
- Hoffman KD
- Hollebeek R
- Holloway L
- Hou S
- Huffman BT
- Hughes R
- Huston J
- Huth J
- Ikeda H
- Incandela J
- Introzzi G
- Iori M
- Issever C
- Ivanov A
- Iwai J
- Iwata Y
- Iyutin B
- James E
- Jones M
- Joshi U
- Kambara H
- Kamon T
- Kaneko T
- Kang J
- Karr K
- Kartal S
- Kasha H
- Kato Y
- Keaffaber TA
- Kelley K
- Kelly M
- Kennedy RD
- Kephart R
- Khazins D
- Kikuchi T
- Kilminster B
- Kim BJ
- Kim DH
- Kim HS
- Kim MJ
- Kim SB
- Kim SH
- Kim TH
- Kim YK
- Kirby M
- Kirk M
- Kirsch L
- Klimenko S
- Koehn P
- Kondo K
- Konigsberg J
- Korn A
- Korytov A
- Kostritskiy AV
- Kotcher J
- Kotelnikov K
- Kothari B
- Kotwal AV
- Kovacs E
- Kovacs E
- Kozelov AV
- Kozlovsky EA
- Krane J
- Krishnaswamy MR
- Krivkova P
- Kroll J
- Kroll J
- Kruse M
- Kruse M
- Krutelyov V
- Krutelyov V
- Krzywdzinski S
- Kubantsev M
- Kuhlmann SE
- Kuhlmann SE
- Kuleshov S
- Kulik Y
- Kunori S
- Kupco A
- Kurino K
- Kurino K
- Kuwabara T
- Kuwabara T
- Kuznetsov VE
- Kuznetsova N
- Kuznetsova N
- Laasanen AT
- Laasanen AT
- Lai N
- Lai N
- Lami S
- Lami S
- Lammel S
- Lammel S
- Lamoureux JI
- Lancaster J
- Lancaster J
- Lancaster M
- Lancaster M
- Lander R
- Lander R
- Landsberg G
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- Leonidopoulos C
- Lewis JD
- Lewis JD
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- Lima JGR
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- Linnemann J
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- Litvintsev DO
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- Manankov V
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- McKigney E
- McMahon T
- Melanson HL
- Melnitchouk A
- Menguzzato M
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- Menzione A
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- Merkin M
- Merritt KW
- Mesropian C
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- Miettinen H
- Mihalcea D
- Miller JS
- Miller JS
- Miller R
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- Minato H
- Minato H
- Miscetti S
- Miscetti S
- Mishina M
- Mishina M
- Mitselmakher G
- Mitselmakher G
- Miyazaki Y
- Moggi N
- Moggi N
- Mokhov N
- Mondal NK
- Montgomery HE
- Moore E
- Moore E
- Moore R
- Moore R
- Moore RW
- Morita Y
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- Moulik T
- Moulik T
- Mukherjee A
- Mukherjee A
- Mulhearn M
- Mulhearn M
- Muller T
- Muller T
- Munar A
- Munar A
- Murat P
- Murat P
- Murgia S
- Murgia S
- Musy M
- Mutaf YD
- Nachtman J
- Nachtman J
- Nagaslaev V
- Nagy E
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- Nakada H
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- Napora R
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- Narasimham VS
- Naumann NA
- Neal HA
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- Negret JP
- Nelson C
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- Neubauer MS
- Neubauer MS
- Neuberger D
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- Newman-Holmes C
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- Pappas SP
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- Rescigno M
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- Reucroft S
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- Riegler W
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- Rimondi F
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- Riveline M
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- Rubinov P
- Ruchti R
- Ruiz A
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- Safonov A
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- Sajot G
- Sakumoto WK
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- Schamberger RD
- Schellman H
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- Schmitt M
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- Schwartzman A
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- Shapiro MD
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- Shepard PF
- Shibayama T
- Shibayama T
- Shimojima M
- Shimojima M
- Shivpuri RK
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- Shpakov D
- Shupe M
- Sidoti A
- Sidoti A
- Sidwell RA
- Siegrist J
- Siegrist J
- Signorelli G
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- Singh P
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- Slattery P
- Slaughter AJ
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- Speer T
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- Spezziga M
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- Spiegel L
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- Spinella F
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- Spiropulu M
- St Denis R
- Stanton NR
- Steele J
- Stefanini A
- Stefanini A
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- Stoker D
- Stolin V
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- Strang MA
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- Stutte L
- Sukhanov A
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- Sumorok K
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- Takashima R
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- Tamburello P
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- Tannenbaum B
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- Tecchio M
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- Teng PK
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- Terashi K
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- Wenzel H
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- Wolinski S
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- Yun JC
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- Zanello L
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- Zaw I
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- Zhou J
- Zsenei A
- Zucchelli Spatra AK
- Zucchelli Sychev D
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2004
- Field of study
We report on a search for direct Kaluza-Klein graviton production in a data
sample of 84 pb−1 of \ppb collisions at s = 1.8 TeV, recorded
by the Collider Detector at Fermilab. We investigate the final state of large
missing transverse energy and one or two high energy jets. We compare the data
with the predictions from a 3+1+n-dimensional Kaluza-Klein scenario in which
gravity becomes strong at the TeV scale. At 95% confidence level (C.L.) for
n=2, 4, and 6 we exclude an effective Planck scale below 1.0, 0.77, and 0.71
TeV, respectively.Comment: Submitted to PRL, 7 pages 4 figures/Revision includes 5 figure
Measurement of the average time-integrated mixing probability of b-flavored hadrons produced at the Tevatron
- Author
- Acosta D
- Affolder T
- Akimoto H
- Albrow MG
- Ambrose D
- Amidei D
- Anikeev K
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
- Asakawa T
- Ashmanskas W
- Azfar F
- Azzi-Bacchetta P
- Bacchetta N
- Bachacou H
- Badgett W
- Bailey S
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Barone M
- Bauer G
- Bedeschi F
- Behari S
- Belforte S
- Bell WH
- Bellettini G
- Bellinger J
- Benjamin D
- Bensinger J
- Beretvas A
- Berryhill J
- Bhatti A
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
- Bloom K
- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bolla G
- Bolshov A
- Bonushkin Y
- Bortoletto D
- Boudreau J
- Brandl A
- Bromberg C
- Brozovic M
- Brubaker E
- Bruner N
- Budagov J
- Budd HS
- Burkett K
- Busetto G
- Byrum KL
- Cabrera S
- Calafiura P
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cerri A
- Cerrito L
- Chan AW
- Chang PS
- Chang PT
- Chapman J
- Chen C
- Chen YC
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
- Chu ML
- Chung JY
- Chung WH
- Chung YS
- Ciobanu CI
- Clark AG
- Coca M
- Connolly A
- Convery M
- Conway J
- Cordelli M
- Cranshaw J
- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
- Dagenhart D
- de Barbaro P
- De Cecco S
- De Pedis D
- de Troconiz JF
- de Troconiz JF
- DeJongh F
- Dell'Agnello S
- Dell'Orso M
- Demers S
- Demortier L
- Deninno M
- Derwent PF
- Devlin T
- Dionisi C
- Dittmann JR
- Dominguez A
- Donati S
- Dorigo T
- Eddy N
- Einsweiler K
- Engels E
- Erbacher R
- Errede D
- Errede S
- Eusebi R
- Fan Q
- Farrington S
- Feild RG
- Fernandez JP
- Ferretti C
- Field RD
- Fiori I
- Flaugher B
- Flores-Castillo LR
- Foster GW
- Franklin M
- Freeman J
- Friedman J
- Fukui Y
- Furic I
- Galeotti S
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 08/09/2003
- Field of study
We have measured the number of like-sign (LS) and opposite-sign (OS) lepton
pairs arising from double semileptonic decays of b and bˉ-hadrons,
pair-produced at the Fermilab Tevatron collider. The data samples were
collected with the Collider Detector at Fermilab (CDF) during the 1992-1995
collider run by triggering on the existence of μμ and eμ candidates
in an event. The observed ratio of LS to OS dileptons leads to a measurement of
the average time-integrated mixing probability of all produced b-flavored
hadrons which decay weakly, χˉ=0.152±0.007 (stat.) ±0.011
(syst.), that is significantly larger than the world average χˉ=0.118±0.005.Comment: 47 pages, 10 figures, 15 tables Submitted to Phys. Rev.
Measurement of CP-violation asymmetries in D0 to Ks pi+ pi-
- Author
- Aaltonen T
- Ahmed S
- Alam MS
- Albert J
- Amerio S
- Amidei D
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- Antos J
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- Appel JA
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- Aurisano A
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- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of time-integrated CP-violation asymmetries in the
resonant substructure of the three-body decay D0 to Ks pi+ pi- using CDF II
data corresponding to 6.0 invfb of integrated luminosity from Tevatron ppbar
collisions at sqrt(s) = 1.96 TeV. The charm mesons used in this analysis come
from D*+(2010) to D0 pi+ and D*-(2010) to D0bar pi-, where the production
flavor of the charm meson is determined by the charge of the accompanying pion.
We apply a Dalitz-amplitude analysis for the description of the dynamic decay
structure and use two complementary approaches, namely a full Dalitz-plot fit
employing the isobar model for the contributing resonances and a
model-independent bin-by-bin comparison of the D0 and D0bar Dalitz plots. We
find no CP-violation effects and measure an asymmetry of ACP = (-0.05 +- 0.57
(stat) +- 0.54 (syst))% for the overall integrated CP-violation asymmetry,
consistent with the standard model prediction.Comment: 15 page
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- Blumenfeld
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- Yi
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- Yu
- Yu
- Yu
- Yun
- Z.
- Zanetti
- Zeng
- Zhou
- Zucchelli
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of the bottom-strange meson mixing phase \beta_s
using the time evolution of B0_s -> J/\psi (->\mu+\mu-) \phi (-> K+ K-) decays
in which the quark-flavor content of the bottom-strange meson is identified at
production. This measurement uses the full data set of proton-antiproton
collisions at sqrt(s)= 1.96 TeV collected by the Collider Detector experiment
at the Fermilab Tevatron, corresponding to 9.6 fb-1 of integrated luminosity.
We report confidence regions in the two-dimensional space of \beta_s and the
B0_s decay-width difference \Delta\Gamma_s, and measure \beta_s in [-\pi/2,
-1.51] U [-0.06, 0.30] U [1.26, \pi/2] at the 68% confidence level, in
agreement with the standard model expectation. Assuming the standard model
value of \beta_s, we also determine \Delta\Gamma_s = 0.068 +- 0.026 (stat) +-
0.009 (syst) ps-1 and the mean B0_s lifetime, \tau_s = 1.528 +- 0.019 (stat) +-
0.009 (syst) ps, which are consistent and competitive with determinations by
other experiments.Comment: 8 pages, 2 figures, Phys. Rev. Lett 109, 171802 (2012
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
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- Youssef S
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- Yusuff I
- Zabinski B
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- Zanzi D
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- Zenin O
- Zenis T
- Zerwas D
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- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhou N
- Zhu CG
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- 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
- Almond J
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- Alviggi MG
- Amako K
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- Amelung C
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- Amram N
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- Anastopoulos C
- Ancu LS
- Andari N
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- Anders CF
- Anders G
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- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
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- Anh TV
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- Youssef S
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- Yusuff I
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- Zaidan R
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- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
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- Zenin O
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- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Measurement of the polar-angle distribution of leptons from W boson decay as a function of the W transverse momentum in proton-antiproton collisions at sqrt{s}=1.8 TeV
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- Spinella F
- Spiropulu M
- Stefanini A
- Stelzer J
- Strologas J
- Stuart D
- Su D
- Sukhanov A
- Sullivan MK
- Sumorok K
- Suzuki T
- Takashima R
- Takikawa K
- Tan P
- Tanaka M
- Tecchio M
- Tehrani FS
- Teng PK
- Terashi K
- Tesarek RJ
- Tether S
- Thom J
- Thompson AS
- Thomson E
- Tipton P
- Tkaczyk S
- Toback D
- Tollefson K
- Tonelli D
- Tonnesmann M
- Toyoda H
- Trischuk W
- Tseng J
- Tsybychev D
- Turini N
- Ukegawa F
- Unel MK
- Unverhau T
- Va'vra J
- Vaiciulis T
- Varganov A
- Varnes EW
- Vasseur G
- Vataga E
- Vejcik S
- Velev G
- Veramendi G
- Vidal R
- Vila I
- Vilar R
- Vitale L
- Voena C
- Volobouev I
- von der Mey M
- von Wimmersperg-Toeller JH
- von Wimmersperg-Toeller JH
- von Wimmersperg-Toeller JH
- Vuagnin G
- Wagner G
- Wagner RG
- Wagner RL
- Wagner SR
- Wagner W
- Wagoner DE
- Waldi R
- Walsh J
- Wan Z
- Wang C
- Wang MJ
- Wang SM
- Wappler FR
- Ward B
- Waschke S
- Waters D
- Watts T
- Weaver M
- Weber M
- Weidemann AW
- Weinstein AJR
- Wester WC
- Whitehouse B
- Wicklund AB
- Wicklund E
- Williams HH
- Wilson P
- Winer BL
- Wisniewski WJ
- Wolbers S
- Wolter M
- Worm S
- Wright DH
- Wu J
- Wu J
- Wu J
- Wu SL
- Wu SL
- Wu SL
- Wu X
- Wurthwein F
- Xella SM
- Yang UK
- Yao W
- Ye S
- Yeche C
- Yeh GP
- Yi K
- Yoh J
- Yoshida T
- Young CC
- Yu I
- Yu S
- Yu Z
- Yu Z
- Yu Z
- Yumiceva FX
- Yun JC
- Zanello L
- Zanetti A
- Zetti F
- Zito M
- Zucchelli SRama M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 24/11/2003
- Field of study
We present a measurement of the coefficient alpha_2 of the leptonic
polar-angle distribution from W boson decays, as a function of the W transverse
momentum. The measurement uses an 80+/-4 pb^{-1} sample of proton-antiproton
collisions at sqrt{s}=1.8 TeV collected by the CDF detector and includes data
from both the W->e+nu and W->mu+nu decay channels. We fit the W boson
transverse mass distribution to a set of templates from a Monte Carlo event
generator and detector simulation in several ranges of the W transverse
momentum. The measurement agrees with the Standard Model expectation, whereby
the ratio of longitudinally to transversely polarized W bosons, in the
Collins-Soper W rest frame, increases with the W transverse momentum at a rate
of approximately 15% per 10 GeV/c.Comment: 47 pages, 16 figures, submitted to Physical Review
A study of the associated production of photons and b-quark jets in p-pbar collisions at sqrt{s} = 1.96 TeV
- Author
- Aaltonen T
- Adelman J
- Almenar CC
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Attal A
- Aurisano A
- Azfar F
- Badgett W
- Barbaro Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauer G
- Beauchemin PH
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Bhatti A
- Binkley M
- Bisello D
- Bizjak I
- Blair RE
- Blocker C
- Blumenfeld B
- Bocci A
- Bodek A
- Boisvert V
- Bortoletto D
- Boudreau J
- Boveia A
- Brau B
- Bridgeman A
- Brigliadori L
- Bromberg C
- Brubaker E
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Byrum KL
- Cabrera S
- Calancha C
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli Sforza M
- Cerri A
- Cerrito L
- Chang SH
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Chung K
- Chung WH
- Chung YS
- Chwalek T
- Ciobanu CI
- Ciocci MA
- Clark A
- Clark D
- Compostella G
- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cox CA
- Cox DJ
- Crescioli F
- Cuevas J
- Culbertson R
- Cully JC
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Datta M
- Davies T
- de Barbaro P
- De Cecco S
- De Lorenzo G
- Deisher A
- DELL'ORSO MAURO
- Deluca C
- Demortier L
- Deng J
- Deninno M
- Denis RS
- Di Canto A
- di Giovanni GP
- Di Ruzza B
- Dittmann JR
- DONATI SIMONE
- Dong P
- Dorigo T
- Dube S
- Ebina K
- Elagin A
- Erbacher R
- Errede D
- Errede S
- Ershaidat N
- Eusebi R
- Fang HC
- Farrington S
- Fedorko WT
- Feild RG
- Feindt M
- Fernandez JP
- Fernandez PM
- Ferrazza C
- Field R
- Flanagan G
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Furic I
- Gallinaro M
- Galyardt J
- Garberson F
- Garcia JE
- Garfinkel AF
- Garosi P
- Gerberich H
- Gerdes D
- Gessler A
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Gimmell JL
- Ginsburg CM
- Giokaris N
- Giordani M
- Giromini P
- Giunta M
- Giurgiu G
- Glagolev V
- Glenzinski D
- Gold M
- Goldschmidt N
- Golossanov A
- Gomez Ceballos G
- Gomez G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Gresele A
- Grinstein S
- Griso SP
- Grosso Pilcher C
- Group RC
- Grundler U
- Gunay Unalan Z
- Haber C
- Hahn SR
- Halkiadakis E
- Han BY
- Han JY
- Happacher F
- Hara K
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- Harr RF
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- Hatakeyama K
- Hays C
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- Heinrich J
- Herndon M
- Heuser J
- Hewamanage S
- Hidas D
- Hill CS
- Hirschbuehl D
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- Hou S
- Houlden M
- Hsu SC
- Hughes RE
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- Husemann U
- Hussein M
- Huston J
- Incandela J
- Introzzi G
- Iori M
- Ivanov A
- James E
- Jang D
- Jayatilaka B
- Jeon EJ
- Jha MK
- Jindariani S
- Johnson W
- Jones M
- Joo KK
- Jun SY
- Jung JE
- Junk TR
- Kamon T
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- Karchin PE
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- Kilminster B
- Kim DH
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- Kim YK
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- Kondo K
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- Konigsberg J
- Korytov A
- Kotwal AV
- Kreps M
- Kroll J
- Krop D
- Krumnack N
- Kruse M
- Krutelyov V
- Kuhr T
- Kulkarni NP
- Kurata M
- Kwang S
- Laasanen AT
- Lami S
- Lammel S
- Lancaster M
- Lander RL
- Lannon K
- Lath A
- Latino G
- Lazzizzera I
- LeCompte T
- Lee E
- Lee HS
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- Lee SW
- Leone S
- Lewis JD
- Lin CJ
- Linacre J
- Lindgren M
- Lipeles E
- Lister A
- Litvintsev DO
- Liu C
- Liu T
- Lockyer NS
- Loginov A
- Lovas L
- Lucchesi D
- Lueck J
- Lujan P
- Lukens P
- Lungu G
- Lys J
- Lysak R
- MacQueen D
- Madrak R
- Maeshima K
- Makhoul K
- Maksimovic P
- Malde S
- Malik S
- Manca G
- Manousakis Katsikakis A
- Margaroli F
- Marino C
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- Martin A
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- Mathis M
- Mattson ME
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- McFarland KS
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- Mitra A
- Mitselmakher G
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- Moed S
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- Mondragon MN
- Moon CS
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- Morello MJ
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- Mukherjee A
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- Potamianos K
- Poukhov O
- Prokoshin F
- Pronko A
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- Pueschel E
- PUNZI GIOVANNI
- Pursley J
- Rademacker J
- Rahaman A
- Ramakrishnan V
- Ranjan N
- Redondo I
- Renton P
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- Rescigno M
- Richter S
- Rimondi F
- Ristori L
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- Roser R
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- Saarikko H
- Safonov A
- Sakumoto WK
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- Scuri F
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- Trovato M
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- Volobouev I.
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- Wakisaka T
- Wakisaka T.
- Wallny R
- Wallny R.
- Wang S. M.
- Wang SM
- Warburton A
- Warburton A.
- Waters D
- Waters D.
- Weinberger M
- Weinberger M.
- Weinelt J
- Weinelt J.
- Wester W. C. III
- Wester WC
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- Whitehouse B.
- Whiteson D
- Whiteson D.
- Wicklund A. B.
- Wicklund AB
- Wicklund E
- Wicklund E.
- Wilbur S
- Wilbur S.
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- Williams G.
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- Wilson P.
- Winer B. L.
- Winer BL
- Wittich P
- Wittich P.
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- Wolbers S.
- Wolfe C
- Wolfe C.
- Wolfe H
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- Wright T.
- Wu X
- Wu X.
- Wuerthwein F.
- Wurthwein F
- Xie S.
- Yagil A
- Yagil A.
- Yamamoto K
- Yamamoto K.
- Yamaoka J
- Yamaoka J.
- Yang U. K.
- Yang UK
- Yang Y. C.
- Yang YC
- Yao W. M.
- Yao WM
- Yeh G. P.
- Yeh GP
- Yi K
- Yoh J
- Yoh J.
- Yorita K
- Yorita K.
- Yoshida T
- Yoshida T.
- Yu G. B.
- Yu GB
- Yu I
- Yu I.
- Yu S. S.
- Yu SS
- Yun J. C.
- Yun JC
- Zanello L.
- Zanetti A
- Zanetti A.
- Zeng Y
- Zhang X
- Zhang X.
- Zheng Y
- Zheng Y.
- Zucchelli S.
- Zucchelli S. S.
- Publication venue
- Publication date
- 17/12/2009
- Field of study
submitted to PRLThe cross section for photon production in association with at least one jet containing a b-quark hadron has been measured in proton antiproton collisions at s=1.96 TeV. The analysis uses a data sample corresponding to an integrated luminosity of 340 pb−1 collected with the CDF II detector. Both the differential cross section as a function of photon transverse energy ETγ, dσ(pp→γ+≥1b-jet)/dETγ and the total cross section σ(pp→γ+≥1b-jet; ETγ>20 GeV) are measured. Comparisons to a next-to-leading order prediction of the process are presented.The cross section for photon production in association with at least one jet containing a b quark has been measured in proton antiproton collisions at √s=1.96 TeV. The data sample used corresponds to an integrated luminosity of 340 pb-1 collected with the CDF II detector. Both the differential cross section as a function of photon transverse energy ETγ and the total cross section are measured and compared to a next-to-leading order prediction for the process.Peer reviewe
Constraints on models of the Higgs boson with exotic spin and parity using decays to bottom-antibottom quarks in the full CDF data set
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- A. aa
- A. aa
- A. aa
- A. ab
- A. aqar
- A. ay
- A. az
- A. bc
- A. bc
- A. bdbebf
- A. bi
- A. bn
- A. c
- A. F. ax
- A. fg
- A. M. bd
- A. p
- A. T. ax
- Aaltonen
- Amerio
- Amidei
- Anastassov A. p
- Annovi A. r
- Antos
- Apollinari G. p
- Appel J. A. p
- Arisawa
- Artikov A. n
- Asaadi
- Ashmanskas W. p
- Auerbach B. b
- Aurisano
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- Badgett W. p
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- Barbaro Galtieri
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- Barnett B. A. x
- Barria
- Bartos
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- Bedeschi
- Behari S. p
- Bellettini
- Bellinger
- Benjamin D. o
- Beretvas A. p
- Bhatti
- Bland K. R. e
- Blumenfeld B. x
- Bocci A. o
- Bodek
- Bortoletto
- Boudreau
- Boveia A. l
- Brigliadori
- Bromberg
- Brucken
- Budagov J. n
- Budd
- Burkett K. p
- Busetto
- Bussey P. t
- Butti
- Buzatu A. t
- C. ae
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- C. aqat
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- C. bj
- C. bl
- C. l
- Calamba A. k
- Camarda S. d
- Campanelli
- Canelli F. l
- Carls B. w
- Carlsmith
- Carosi
- Carrillo S. q
- Casal B. j
- Casarsa
- Castro
- Catastini P. u
- CAUZ Diego
- Cavaliere V. w
- Cerri
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- Chen Y. C. a
- Chertok M. h
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- Chlachidze G. p
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- Clark A. s
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- Convery M. E. p
- Conway J. h
- Corbo M. p
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- Cox C. A. h
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- Cruz
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- Datta M. p
- De Barbaro
- Demortier
- Deninno M. f
- Devoto
- Di Canto
- Di Ruzza
- Dittmann J. R. e
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- Dorigo
- Driutti
- E. ap
- E. ap
- E. ap
- E. J. zbqbrbsbtbubv
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- Ebina
- Edgar
- Elagin
- Erbacher R. h
- Errede S. w
- Esham B. w
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- F. aq
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- F. ba
- F. bh
- F. vbp
- Farrington
- Fernández Ramos
- Field R. q
- Flanagan G. p
- Forrest R. h
- Franklin M. u
- Freeman J. C. p
- Frisch H. l
- Funakoshi
- G. ab
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- Galloni
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- Gerberich H. w
- Gerchtein E. p
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- Ginsburg C. M. p
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- Goncharov
- González López
- Gorelov
- Goshaw A. T. o
- Goulianos
- Gramellini E. f
- Grosso Pilcher
- Group
- Guimaraes Da Costa
- H. aj
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- H. S. ay
- H. S. zbqbrbsbtbubv
- H. S. zbqbrbsbtbubv
- Hahn S. R. p
- Han
- Happacher F. r
- Hara
- Hare
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- Harrington Taber
- Hatakeyama K. e
- Hays
- Heinrich
- Herndon
- Hocker A. p
- Hong
- Hopkins W. p
- Hou S. a
- Hughes
- Husemann
- Hussein
- Huston
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- Ivanov A. h
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- J. Y. ay
- James E. p
- Jang D. k
- Jayatilaka B. p
- Jeon
- Jindariani S. p
- Jones
- Joo
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- Kamon
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- Konigsberg J. q
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- Kreps M. y
- Kroll
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- Laasanen
- Lammel S. p
- Lancaster
- Lannon
- Latino
- Lee
- Lee
- Leo S. w
- Leone
- Lewis J. D. p
- Limosani A. o
- Lipeles
- Lister A. s
- Liu
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- Liu T. p
- Lockwitz
- Loginov
- Lucà A. r
- Lucchesi
- Lueck J. y
- Lujan
- Lukens P. p
- Lungu
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- M. ab
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- M. ac
- M. ae
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- M. ai
- M. ai
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- M. anao
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- M. aqar
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- M. ax
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- M. babb
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- M. bdbg
- M. bh
- M. bh
- M. bi
- M. bm
- M. E. bl
- M. fg
- M. J. aqat
- Madrak R. p
- Maestro
- Malik
- Manca
- Manousakis Katsikakis
- Marchese L. f
- Margaroli
- Marino
- Matera K. w
- Mattson
- Mazzacane A. p
- Mazzanti P. f
- McNulty
- Mehta
- Mehtala
- Mesropian
- Miao T. p
- Mietlicki
- Mitra A. a
- Miyake
- Moed S. p
- Moggi N. f
- Moon C. S. p
- Moore R. p
- Morello
- Mukherjee A. p
- Muller T. y
- Murat P. p
- Mussini
- N. bk
- Nachtman J. p
- Nagai
- Naganoma
- Nakano
- Napier
- Nett
- Neu
- Nigmanov
- Nodulman L. b
- Noh
- Norniella O. w
- O. ad
- Oakes
- Oh
- Oh S. H. o
- Oksuzian
- Okusawa
- Orava
- Ortolan L. d
- P. aa
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- P. vbp
- Pagliarone
- Palencia E. j
- Palni
- Papadimitriou V. p
- Parker
- PAULETTA Giovanni
- Paulini M. k
- Paus
- Phillips T. J. o
- Piacentino G. p
- Pianori
- Pilot J. h
- Pitts K. w
- Plager C. i
- Pondrom
- Poprocki S. p
- Potamianos
- Pranko
- Prokoshin F. n
- Ptohos F. r
- Punzi
- Q. ax
- R. ab
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- R. E. aj
- R. F. bl
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- R. t
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- Redondo Fernández
- Renton
- Rescigno
- Rimondi F. f
- Ristori
- Robson A. t
- Rodriguez
- Rolli
- Ronzani
- Roser R. p
- Rosner J. L. l
- Ruffini
- Ruiz A. j
- Russ J. k
- Rusu V. p
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- S. mbo
- S. Y. zbqbrbsbtbubv
- S. zbqbrbsbtbubv
- S.t. Denis
- Sakumoto
- Sakurai
- SANTI Lorenzo Gianni
- Sato
- Saveliev V. p
- Savoy Navarro
- Schlabach P. p
- Schmidt E. E. p
- Schwarz
- Scodellaro L. j
- Scuri
- Seidel
- Seiya
- Semenov A. n
- Sforza
- Shalhout S. Z. h
- Shears
- Shepard
- Shimojima
- Shochet M. l
- Shreyber Tecker
- Simonenko A. n
- Sliwa
- Smith J. R. h
- Snider F. D. p
- Song
- Sorin V. d
- Stancari M. p
- Stentz D. p
- Strologas
- Sudo
- Sukhanov A. p
- Suslov I. n
- T. ab
- T. af
- T. af
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- T. zbcbqbrbsbtbubv
- T. zbqbrbsbtbubv
- Takemasa
- Takeuchi
- Tang J. l
- Tecchio
- Teng P. K. a
- Thom J. p
- Thomson
- Thukral
- Toback
- Tokar
- Tollefson
- Tomura
- Tonelli D. p
- Torre S. r
- Torretta D. p
- Totaro
- Trovato
- U. bn
- U. K. zbqbrbsbtbubv
- Ukegawa
- Uozumi
- V. bc
- V. E. ax
- Vázquez F. q
- Velev G. p
- Vellidis C. p
- Vernieri
- Vidal
- Vilar R. j
- Vizán J. j
- Vogel
- Volpi G. r
- W. bm
- W. K. ay
- W. M. aa
- Wagner
- Wallny R. p
- Wang S. M. a
- Waters
- Wester W. C. p
- Whiteson
- Wicklund A. B. b
- Wilbur S. h
- Williams
- Wilson
- Wilson P. p
- Winer
- Wittich P. p
- Wolbers S. p
- Wolfe
- Wright
- Wu X. s
- Wu Z. e
- Y. al
- Y. al
- Y. bh
- Y. bh
- Y. bh
- Y. bk
- Y. bk
- Y. C. zbqbrbsbtbubv
- Y. D. zbqbrbsbtbubv
- Y. J. zbqbrbsbtbubv
- Yamamoto
- Yamato
- Yang
- Yang
- Yang T. p
- Yao
- Yeh G. P. p
- Yi K. p
- Yoh J. p
- Yorita
- Yoshida
- Yu
- Yu G. B. o
- Z. bc
- Zanetti
- Zeng Y. o
- Zhou C. o
- Zucchelli S. fg
- Publication venue
- Publication date
- 01/01/2015
- Field of study
A search for particles with the same mass and couplings as those of the standard model Higgs boson but different spin and parity quantum numbers is presented. We test two specific alternative Higgs boson hypotheses: a pseudoscalar Higgs boson with spin-parity JP=0- and a gravitonlike Higgs boson with JP=2+, assuming for both a mass of 125GeV/c2. We search for these exotic states produced in association with a vector boson and decaying into a bottom-antibottom quark pair. The vector boson is reconstructed through its decay into an electron or muon pair, or an electron or muon and a neutrino, or it is inferred from an imbalance in total transverse momentum. We use expected kinematic differences between events containing exotic Higgs bosons and those containing standard model Higgs bosons. The data were collected by the CDF experiment at the Tevatron proton-antiproton collider, operating at a center-of-mass energy of s=1.96TeV, and correspond to an integrated luminosity of 9.45fb-1. We exclude deviations from the predictions of the standard model with a Higgs boson of mass 125GeV/c2 at the level of 5 standard deviations, assuming signal strengths for exotic boson production equal to the prediction for the standard model Higgs boson, and set upper limits of approximately 30% relative to the standard model rate on the possible rate of production of each exotic state
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