90 research outputs found
Single-Event Effect Testing of the Linear Technology LTC6103HMS8#PBF Current Sense Amplifier
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The LTC6103HMS8#PBF (henceforth abbreviated as LTC6103) current sense amplifier from Linear Technology was tested for both destructive and non-destructive single-event effects (SEE) using the heavy-ion cyclotron accelerator beam at Lawrence Berkeley National Laboratory (LBNL) Berkeley Accelerator Effects (BASE) facility. During testing, the input voltages and output currents were monitored to detect single event latch-up (SEL) and single-event transients (SETs)
Compendium of Current Total Ionizing Dose and Displacement Damage Results from NASA GSFC and NEPP
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- Field of study
Total ionizing dose and displacement damage testing was performed to characterize and determine the suitability of candidate electronics for NASA space utilization. Devices tested include opto-electronics, digital, analog, linear bipolar devices, and hybrid devices
Compendium of Current Total Ionizing Dose and Displacement Damage Results from NASA Goddard Space Flight Center and NASA Electronic Parts and Packaging Program
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Total ionizing dose and displacement damage testing was performed to characterize and determine the suitability of candidate electronics for NASA space utilization. Devices tested include optoelectronics, digital, analog, linear bipolar devices, and hybrid devices. Displacement Damage, Optoelectronics, Proton Damage, Single Event Effects, and Total Ionizing Dose
Compendium of Current Total Ionizing Dose and Displacement Damage Results from NASA Goddard Space Flight Center and Selected NASA Electronic Parts and Packaging Program
- Author
- Publication venue
- Publication date
- Field of study
Total ionizing dose and displacement damage testing was performed to characterize and determine the suitability of candidate electronics for NASA space utilization. Devices tested include optoelectronics, digital, analog, linear bipolar devices, and hybrid devices
Anatomy of the sign-problem in heavy-dense QCD
- Author
- Adam E Romero
- Aranda C Padilla
- Arjanovic MM
- Armadans R Caminal
- Astigarraga ME Pozo
- Barajas CA Chavez
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr JK
- Belanger-Champagne C
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Beringer J
- Berlendis S
- Berlingen J Montejo
- Bernard NR
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertram IA
- Bertsche C
- Bertsche D
- Besjes GJ
- Bessner M
- Besson N
- Betancourt C
- Bethke S
- Bevan AJ
- Bhimji W
- Bianchi RM
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- Biebel O
- Biedermann D
- Bielski R
- Biesuz NV
- Biglietti M
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- Bocchetta SS
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- Yildirim E
- Yildiz H Duran
- Yorita K
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- Yoshihara K
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- Youssef S
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- Yuen SPY
- Yusuff I
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- Zaidan R
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- Zalieckas J
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- Zeitnitz C
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- Zemla A
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- Zeng Q
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- Zenis T
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- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
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- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
QCD at finite densities of heavy quarks is investigated
using the density-of-states method. The phase factor
expectation value of the quark determinant is calculated to
unprecedented precision as a function of the chemical potential.
Results are validated using those from a reweighting
approach where the latter can produce a significant signalto-noise
ratio. We confirm the particle–hole symmetry at low
temperatures, find a strong sign problem at intermediate values
of the chemical potential, and an inverse Silver Blaze
feature for chemical potentials close to the onset value: here,
the phase-quenched theory underestimates the density of the
full theory
Identification of boosted, hadronically decaying W bosons and comparisons with ATLAS data taken at √s = 8 TeV
- Author
- A Hook
- A. A. Affolder
- A. A. E. Bannoura
- A. A. Elliot
- A. A. Grillo
- A. A. Komar
- A. A. Korol
- A. A. Maier
- A. A. Minaenko
- A. A. Nepomuceno
- A. A. Snesarev
- A. A. Solodkov
- A. A. Talyshev
- A. Aloisio
- A. Alonso
- A. Altheimer
- A. Amorim
- A. Andreazza
- A. Angerami
- A. Annovi
- A. Antonov
- A. Artamonov
- A. Ashkenazi
- A. B. Fenyuk
- A. Baroncelli
- A. Basalaev
- A. Bassalat
- A. Basye
- A. Beddall
- A. Bellerive
- A. Bingul
- A. Bocci
- A. Borisov
- A. Boveia
- A. Brandt
- A. Bruni
- A. Buzatu
- A. C. Daniells
- A. C. König
- A. C. Martyniuk
- A. C. Schaffer
- A. Calandri
- A. Campoverde
- A. Canepa
- A. Castelli
- A. Catinaccio
- A. Cattai
- A. Cerri
- A. Cervelli
- A. Chafaq
- A. Chegwidden
- A. Cheplakov
- A. Chitan
- A. Ciocio
- A. Clark
- A. Coccaro
- A. Corso-Radu
- A. Cortes-Gonzalez
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- A. D. Pilkington
- A. Dafinca
- A. Dattagupta
- A. De Benedetti
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- A. De Santo
- A. Dell’Acqua
- A. Demilly
- A. Dewhurst
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- A. Di Simone
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- W. Davey
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- W. Ehrenfeld
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- W. H. Bell
- W. H. Hopkins
- W. Iwanski
- W. J. Dearnaley
- W. J. Johnson
- W. J. Murray
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- W. K. Brooks
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- W. S. Lockman
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- W. Vandelli
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- W. Wagner
- W. Walkowiak
- W. Wiedenmann
- W.-M. Yao
- X. Chen
- X. Hu
- X. Ju
- X. Lei
- X. Li
- X. Lou
- X. Ruan
- X. Sun
- X. Wang
- X. Wu
- X. Zhang
- X. Zhao
- X. Zhuang
- Y Cui
- Y. A. Kurochkin
- Y. Abulaiti
- Y. Amaral Coutinho
- Y. Arai
- Y. B. Pan
- Y. Bai
- Y. Benhammou
- Y. C. Yap
- Y. Chen
- Y. Cheng
- Y. Coadou
- Y. Davygora
- Y. Enari
- Y. F. Ryabov
- Y. Fang
- Y. Gao
- Y. Guo
- Y. Hasegawa
- Y. Heng
- Y. Hernández Jiménez
- Y. Horii
- Y. Huang
- Y. Ikegami
- Y. Ilchenko
- Y. J. Schnellbach
- Y. Jiang
- Y. K. Kim
- Y. Kataoka
- Y. Komori
- Y. Kulchitsky
- Y. Li
- Y. Liu
- Y. Makida
- Y. Minami
- Y. Ming
- Y. Nagai
- Y. Nagasaka
- Y. Nakahama
- Y. Ninomiya
- Y. Okumura
- Y. Oren
- Y. Qin
- Y. Rozen
- Y. S. Gao
- Y. Sakurai
- Y. Sasaki
- Y. Silver
- Y. Smirnov
- Y. Sugaya
- Y. Takubo
- Y. Tayalati
- Y. Unno
- Y. Wu
- Y. Yamaguchi
- Y. Yamazaki
- Y. Yang
- Y. Yasu
- Y. Zhao
- Y. Zhu
- Yu. A. Tikhonov
- Z. Barnovska
- Z. D. Greenwood
- Z. Dolezal
- Z. Gecse
- Z. H. Citron
- Z. Hajduk
- Z. Hubacek
- Z. Idrissi
- Z. J. Grout
- Z. Kohout
- Z. Liang
- Z. M. Karpova
- Z. Marshall
- Z. Rurikova
- Z. Vykydal
- Z. Yan
- Z. Zhang
- Z. Zhao
- Z. Zinonos
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
This paper reports a detailed study of techniques for identifying boosted, hadronically decaying W bosons using 20.3 fb −¹ of proton–proton collision data collected by the ATLAS detector at the LHC at a centre-of-mass energy √s = 8 TeV. A range of techniques for optimising the signal jet mass resolution are combined with various jet substructure variables. The results of these studies in Monte Carlo simulations show that a simple pairwise combination of groomed jet mass and one substructure variable can provide a 50 % efficiency for identifying W bosons with transverse momenta larger than 200 GeV while maintaining multijet background efficiencies of 2–4 % for jets with the same transverse momentum. These signal and background efficiencies are confirmed in data for a selection of tagging techniques
Search for Higgs and Z Boson Decays to J/ψγ and ϒ(nS)γ with the ATLAS Detector.
- Author
- (ATLAS Collaboration)
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- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdinov O
- Aben R
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- Abolins M
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- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zurzolo G
- Zwalinski L
- Åkesson TPA
- Åsman B
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
A search for the decays of the Higgs and Z bosons to J/ψγ and ϒ(nS)γ (n=1,2,3) is performed with pp collision data samples corresponding to integrated luminosities of up to 20.3 fb^{-1} collected at sqrt[s]=8 TeV with the ATLAS detector at the CERN Large Hadron Collider. No significant excess of events is observed above expected backgrounds and 95% C.L. upper limits are placed on the branching fractions. In the J/ψγ final state the limits are 1.5×10^{-3} and 2.6×10^{-6} for the Higgs and Z boson decays, respectively, while in the ϒ(1S,2S,3S)γ final states the limits are (1.3,1.9,1.3)×10^{-3} and (3.4,6.5,5.4)×10^{-6}, respectively.We acknowledge the support of ANPCyT,
Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI,
Canada; CERN; CONICYT, Chile; CAS, MOST and
NSFC, China; COLCIENCIAS, Colombia; MSMT CR,MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/ IRFU, France; GNSF, Georgia; BMBF, DFG, HGF,
MPG and AvH Foundation, Germany; GSRT and
NSRF, Greece; ISF, MINERVA, GIF, I-CORE and
Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS,
Japan; CNRST, Morocco; FOM and NWO, Netherlands;BRF and RCN, Norway; MNiSW and NCN, Poland;GRICES and FCT, Portugal; MNE/IFA, Romania; MES of Russia and ROSATOM, Russian Federation; JINR;MSTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain;SRC and Wallenberg Foundation, Sweden; SER, SNSF and Cantons of Bern and Geneva, Switzerland; NSC,Taiwan; TAEK, Turkey; STFC, the Royal Society and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America
Search for resonances in diphoton events at √s = 13 TeV with the ATLAS detector
- Author
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- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou M
- Zhou N
- Zhu Cg
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine Ni
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Searches for new resonances decaying into two photons in the ATLAS experiment at the CERN Large Hadron Collider are described. The analysis is based on proton-proton collision data corresponding to an integrated luminosity of 3.2 fb−1 at s√=13 TeV recorded in 2015. Two searches are performed, one targeted at a spin-2 particle of mass larger than 500 GeV, using Randall-Sundrum graviton states as a benchmark model, and one optimized for a spin-0 particle of mass larger than 200 GeV. Varying both the mass and the decay width, the most significant deviation from the background-only hypothesis is observed at a diphoton invariant mass around 750 GeV with local significances of 3.8 and 3.9 standard deviations in the searches optimized for a spin-2 and spin-0 particle, respectively. The global significances are estimated to be 2.1 standard deviations for both analyses. The consistency between the data collected at 13 TeV and 8 TeV is also evaluated. Limits on the production cross section times branching ratio to two photons for the two resonance types are reported
Performance of the ATLAS muon trigger in pp collisions at [Formula: see text] TeV
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- Publication venue
- Publication date
- 01/03/2015
- Field of study
The performance of the ATLAS muon trigger system is evaluated with proton-proton collision data collected in 2012 at the Large Hadron Collider at a centre-of-mass energy of 8 TeV. It is primarily evaluated using events containing a pair of muons from the decay of [Formula: see text] bosons. The efficiency of the single-muon trigger is measured for muons with transverse momentum [Formula: see text] GeV, with a statistical uncertainty of less than 0.01 % and a systematic uncertainty of 0.6 %. The [Formula: see text] range for efficiency determination is extended by using muons from decays of [Formula: see text] mesons, [Formula: see text] bosons, and top quarks. The muon trigger shows highly uniform and stable performance. The performance is compared to the prediction of a detailed simulation
Performance of algorithms that reconstruct missing transverse momentum in √s= 8 TeV proton-proton collisions in the ATLAS detector
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
The reconstruction and calibration algorithms used to calculate missing transverse momentum (EmissT ) with the ATLAS detector exploit energy deposits in the calorimeter and tracks reconstructed in the inner detector as well as the muon spectrometer. Various strategies are used to suppress effects arising from additional proton–proton interactions, called pileup, concurrent with the hard-scatter processes. Tracking information is used to distinguish contributions from the pileup interactions using their vertex separation along the beam axis. The performance of the EmissT reconstruction algorithms, especially with respect to the amount of pileup, is evaluated using data collected in proton–proton collisions at a centre-of-mass energy of 8 TeV during 2012, and results are shown for a data sample corresponding to an integrated luminosity of 20.3fb−1. The simulation and modelling of EmissT in events containing a Z boson decaying to two charged leptons (electrons or muons) or a W boson decaying to a charged lepton and a neutrino are compared to data. The acceptance for different event topologies, with and without high transverse momentum neutrinos, is shown for a range of threshold criteria for EmissT , and estimates of the systematic uncertainties in the EmissT measurements are presented.ATLAS Collaboration, for complete list of authors see dx.doi.org/10.1140/epjc/s10052-017-4780-2Funding: We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently.We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF and DNSRC, Denmark; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, HGF, and MPG, Germany; GSRT, Greece; RGC, Hong Kong SAR, China; ISF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; RCN, Norway; MNiSW and NCN, Poland; FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russian Federation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons of Bern and Geneva, Switzerland; MOST, Taiwan; TAEK, Turkey; STFC, UK; DOE and NSF, United States of America. In addition, individual groups and members have received support from BCKDF, the Canada Council, CANARIE, CRC, Compute Canada, FQRNT, and the Ontario Innovation Trust, Canada; EPLANET, ERC, FP7, Horizon 2020 and Marie Skłodowska-Curie Actions, European Union; Investissements d’Avenir Labex and Idex, ANR, Région Auvergne and Fondation Partager le Savoir, France; DFG and AvH Foundation, Germany; Herakleitos, Thales and Aristeia programmes co-financed by EU-ESF and the Greek NSRF; BSF, GIF and Minerva, Israel; BRF, Norway; Generalitat de Catalunya, Generalitat Valenciana, Spain; the Royal Society and Leverhulme Trust, United Kingdom. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN, the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA), the Tier-2 facilities worldwide and large non-WLCG resource providers. Major contributors of computing resources are listed in Ref. [58].</p
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