855 research outputs found
[Plasma 2020 Decadal] Disentangling the Spatiotemporal Structure of Turbulence Using Multi-Spacecraft Data
- Author
- Publication venue
- 'Center for Open Science'
- Publication date
- 13/03/2019
- Field of study
This white paper submitted for 2020 Decadal Assessment of Plasma Science concerns the importance of multi-spacecraft missions to address fundamental questions concerning plasma turbulence. Plasma turbulence is ubiquitous in the universe, and it is responsible for the transport of mass, momentum, and energy in such diverse systems as the solar corona and wind, accretion discs, planet formation, and laboratory fusion devices. Turbulence is an inherently multi-scale and multi-process phenomenon, coupling the largest scales of a system to sub-electron scales via a cascade of energy, while simultaneously generating reconnecting current layers, shocks, and a myriad of instabilities and waves. The solar wind is humankind's best resource for studying the naturally occurring turbulent plasmas that permeate the universe. Since launching our first major scientific spacecraft mission, Explorer 1, in 1958, we have made significant progress characterizing solar wind turbulence. Yet, due to the severe limitations imposed by single point measurements, we are unable to characterize sufficiently the spatial and temporal properties of the solar wind, leaving many fundamental questions about plasma turbulence unanswered. Therefore, the time has now come wherein making significant additional progress to determine the dynamical nature of solar wind turbulence requires multi-spacecraft missions spanning a wide range of scales simultaneously. A dedicated multi-spacecraft mission concurrently covering a wide range of scales in the solar wind would not only allow us to directly determine the spatial and temporal structure of plasma turbulence, but it would also mitigate the limitations that current multi-spacecraft missions face, such as non-ideal orbits for observing solar wind turbulence. Some of the fundamentally important questions that can only be addressed by in situ multipoint measurements are discussed
Search for a New Heavy Gauge Boson Wprime with Electron + missing ET Event Signature in ppbar collisions at sqrt(s)=1.96 TeV
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
- Adam N
- Adams MR
- Adams T
- Agostino L
- Akgun B
- Akgun U
- Alagoz E
- Albayrak EA
- Albrow M
- Alexander J
- Almenar CC
- Alver B
- Alverson G
- Amerio S
- Amidei D
- Anastassov A
- Anastassov A
- Anderson J
- Anghel IM
- Annovi A
- Antonelli L
- Antos J
- Apanasevich L
- Apollinari G
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Askew A
- Atac M
- Auerbach B
- Aurisano A
- Avery P
- Azfar F
- Baarmand MM
- Baden A
- Badgett W
- Bai Y
- Bakken JA
- Bandurin D
- Banerjee S
- Barbaro-Galtieri A
- Barberis E
- Baringer P
- Barnes VE
- Barnes VE
- Barnett BA
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bazterra VE
- Bean A
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Bendavid J
- Benelli G
- Benjamin D
- Beretvas A
- Beretvas A
- Berry D
- Berry E
- Berryhill J
- Betchart B
- Betts RR
- Bhat PC
- Bhatti A
- Bilki B
- Binkley M
- Biselli A
- Bisello D
- Bizjak I
- Bland KR
- Blekman F
- Bloch I
- Bloom K
- Blumenfeld B
- Blumenfeld B
- Bocci A
- Bochenek J
- Bodek A
- Bodek A
- Boeriu O
- Bolla G
- Bolton T
- Bonato A
- Borcherding F
- Borrello L
- Bortoletto D
- Bortoletto D
- Bose S
- Boudreau J
- Boulahouache C
- Bourilkov D
- Boutemeur M
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
- Bromberg C
- Brucken E
- Bucciantonio M
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Burkett K
- Busetto G
- Bussey P
- Busza W
- Butler JN
- Butt J
- Butz E
- Buzatu A
- Bylsma B
- Calamba A
- Calancha C
- Cali IA
- Callner J
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Cankocak K
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carroll R
- Carron S
- Casal B
- Casarsa M
- Castro A
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- Ciobanu CI
- Ciocci MA
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- Yun JC
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- Zablocki J
- Zakaria M
- Zanetti A
- Zanetti A
- Zanetti M
- Zang SL
- Zatserklyaniy A
- Zeng Y
- Zeng Y
- Zennamo J
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- Zhukova V
- Ziegler J
- Zucchelli Slli Sira D
- Zucchelli SYun JC
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2010
- Field of study
We present a search for a new heavy charged vector boson W′ decaying
to an electron-neutrino pair in ppˉ collisions at a center-of-mass
energy of 1.96\unit{TeV}. The data were collected with the CDF II detector
and correspond to an integrated luminosity of 5.3\unit{fb}^{-1}. No
significant excess above the standard model expectation is observed and we set
upper limits on σ⋅B(W′→eν). Assuming standard
model couplings to fermions and the neutrino from the W′ boson decay to
be light, we exclude a W′ boson with mass less than
1.12\unit{TeV/}c^2 at the 95\unit{%} confidence level.Comment: 7 pages, 2 figures Submitted to PR
Measurement of the Forward-Backward Asymmetry in the B -> K(*) mu+ mu- Decay and First Observation of the Bs -> phi mu+ mu- Decay
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
- Adam N
- Adams MR
- Adams T
- Agostino L
- Akgun B
- Akgun U
- Alagoz E
- Albayrak EA
- Albrow M
- Alexander J
- Almenar CC
- Alver B
- Alverson G
- Amerio S
- Amidei D
- Anastassov A
- Anastassov A
- Anderson J
- Anghel IM
- Annovi A
- Antonelli L
- Antos J
- Apanasevich L
- Apollinari G
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Askew A
- Atac M
- Auerbach B
- Aurisano A
- Avery P
- Azfar F
- Baarmand MM
- Baden A
- Badgett W
- Bai Y
- Bakken JA
- Bandurin D
- Banerjee S
- Barbaro-Galtieri A
- Barberis E
- Baringer P
- Barnes VE
- Barnes VE
- Barnett BA
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bazterra VE
- Bean A
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Bendavid J
- Benelli G
- Benjamin D
- Beretvas A
- Beretvas A
- Berry D
- Berry E
- Berryhill J
- Betchart B
- Betts RR
- Bhat PC
- Bhatti A
- Bhatti A
- Bilki B
- Binkley M
- Biselli A
- Bisello D
- Bizjak I
- Bland KR
- Blekman F
- Bloch I
- Blocker C
- Bloom K
- Blumenfeld B
- Blumenfeld B
- Bocci A
- Bochenek J
- Bodek A
- Bodek A
- Boeriu O
- Bolla G
- Bolton T
- Bonato A
- Borcherding F
- Borrello L
- Bortoletto D
- Bortoletto D
- Bose S
- Boudreau J
- Boulahouache C
- Bourilkov D
- Boutemeur M
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
- Bromberg C
- Brucken E
- Bucciantonio M
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Burkett K
- Busetto G
- Bussey P
- Busza W
- Butler JN
- Butt J
- Butz E
- Buzatu A
- Bylsma B
- Cabrera S
- Calamba A
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- Yi K
- Yi K
- Yilmaz Y
- Yoh J
- Yoo HD
- Yoon AS
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- Yumiceva F
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- Zanetti A
- Zanetti M
- Zang SL
- Zatserklyaniy A
- Zeng Y
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- Zhukova V
- Ziegler J
- Zielinski M
- Zucchelli SZucchelli Sira D
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We reconstruct the rare decays B+→K+μ+μ−, B0→K∗(892)0μ+μ−, and Bs0→ϕ(1020)μ+μ− in a data sample
corresponding to 4.4fb−1 collected in ppˉ collisions at
s=1.96TeV by the CDF II detector at the Fermilab Tevatron
Collider. Using 121±16 B+→K+μ+μ− and 101±12 B0→K∗0μ+μ− decays we report the branching ratios. In addition, we report
the measurement of the differential branching ratio and the muon
forward-backward asymmetry in the B+ and B0 decay modes, and the K∗0
longitudinal polarization in the B0 decay mode with respect to the squared
dimuon mass. These are consistent with the theoretical prediction from the
standard model, and most recent determinations from other experiments and of
comparable accuracy. We also report the first observation of the Bs0→ϕμ+μ−decayandmeasureitsbranchingratio{\mathcal{B}}(B^0_s \to
\phi\mu^+\mu^-) = [1.44 \pm 0.33 \pm 0.46] \times 10^{-6}using27 \pm 6signalevents.ThisiscurrentlythemostrareB^0_s$ decay observed.Comment: 7 pages, 2 figures, 3 tables. Submitted to Phys. Rev. Let
Measurements of the properties of Lambda_c(2595), Lambda_c(2625), Sigma_c(2455), and Sigma_c(2520) baryons
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
- Adam N
- Adams MR
- Adams T
- Agostino L
- Akgun B
- Akgun U
- Alagoz E
- Albayrak EA
- Albrow M
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- Anderson J
- Anghel IM
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- Apollinari G
- Apollinari G
- Appel JA
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- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
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- Atac M
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- Aurisano A
- Avery P
- Azfar F
- Baarmand MM
- Baden A
- Badgett W
- Bai Y
- Bakken JA
- Bandurin D
- Banerjee S
- Barbaro-Galtieri A
- Barberis E
- Baringer P
- Barnes VE
- Barnes VE
- Barnett BA
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- Bauer G
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- Baumgartel D
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- Chakaberia I
- Chan M
- Chasco M
- Chatterjee A
- Chen J
- Chen M
- Chen YC
- Chertok M
- Chetluru V
- Cheung HWK
- Chiarelli G
- Chlachidze G
- Chlebana F
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- Cho K
- Chokheli D
- Chou JP
- Chung WH
- Chung YS
- Chung YS
- Cihangir S
- Ciobanu CI
- Ciocci MA
- Cirino G
- Claes DR
- Clarida W
- Clark A
- Clarke C
- Cole P
- Compostella G
- Convery ME
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- Culbertson R
- Cumalat JP
- Cuplov V
- Cushman P
- d'Ascenzo N
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Dahmes B
- Das S
- Datta M
- de Barbaro P
- de Barbaro P
- De Benedetti A
- De Cecco S
- De Lorenzo G
- Dell'Orso M
- Deluca C
- Demarteau M
- Demina R
- Demortier L
- Deng J
- Deninno M
- Devoto F
- Di Canto A
- Di Giovanni GP
- Di Ruzza B
- Diamond B
- Dinardo ME
- Dittmann JR
- Dobur D
- Dominguez A
- Donati S
- Dong P
- Dorigo M
- Dorigo T
- Dorney B
- Dragoiu C
- Drell BR
- Drozdetskiy A
- Dudero PR
- Durkin LS
- Duru F
- Dutta V
- Eads M
- Eartly DP
- Ebina K
- Ecklund KM
- Edelmaier CJ
- Eggert N
- Elagin A
- Elmer P
- Elvira VD
- Eno SC
- Eppig A
- Erbacher R
- Errede D
- Errede S
- Ershaidat N
- Eshaq Y
- Eskew C
- Eusebi R
- Everaerts P
- Everett A
- Fang HC
- Farrington S
- Fehling D
- Feindt M
- Ferencek D
- Ferguson T
- Fernandez JP
- Fernandez PM
- Ferrazza C
- Field R
- Field RD
- Fields LJ
- Fisher M
- Fisk I
- Flacher H
- Flanagan G
- Ford WT
- Forrest R
- Frank MJ
- Franklin M
- Franzoni G
- Freeman J
- Freeman JC
- Fu Y
- Funakoshi Y
- Furic I
- Furic IK
- Gallinaro M
- Galyardt J
- Gao Y
- Garcia JE
- Garcia-Bellido A
- Garcia-Solis EJ
- Garfinkel AF
- Garfinkel AF
- Garosi P
- Gartner J
- Gaultney V
- Gecse Z
- Gerbaudo D
- Gerber CE
- Gerberich H
- Gerchtein E
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- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We report measurements of the resonance properties of Lambda_c(2595)+ and
Lambda_c(2625)+ baryons in their decays to Lambda_c+ pi+ pi- as well as
Sigma_c(2455)++,0 and Sigma_c(2520)++,0 baryons in their decays to Lambda_c+
pi+/- final states. These measurements are performed using data corresponding
to 5.2/fb of integrated luminosity from ppbar collisions at sqrt(s) = 1.96 TeV,
collected with the CDF II detector at the Fermilab Tevatron. Exploiting the
largest available charmed baryon sample, we measure masses and decay widths
with uncertainties comparable to the world averages for Sigma_c states, and
significantly smaller uncertainties than the world averages for excited
Lambda_c+ states.Comment: added one reference and one table, changed order of figures, 17
pages, 15 figure
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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- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
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- Youssef S
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- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhang H
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- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- 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
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
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- Zhemchugov A
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- Zobernig G
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- 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
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- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
- Yan Z
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- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Smit GVY
- Ye J
- Ye S
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- 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
- Ziolkowski M
- Zitoun R
- 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
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- 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 R
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- 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
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- 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
- Anh TV
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Atkinson M
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Avramidou R
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Balek P
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
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- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch V
- Basye A
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
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- Yilmaz M
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- Yoshihara K
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- Zaidan R
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- Zhemchugov A
- Zhong J
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- 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 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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- Zu Theenhausen HM
- Zwalinski L
- 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
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
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- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- 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
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- 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
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