374 research outputs found
Changes in arginase isoforms in a murine model of neonatal brain hypoxia-ischemia.
- Author
- A Alizadeh
- A Di Ieva
- A Quirié
- AB Petrone
- AG Estévez
- D Cai
- D Jonathan
- E Shosha
- GD Adamek
- H Li
- H Yu
- H Yu
- J Krystofova
- JM Crain
- K Deng
- L Konarska
- LK Paul
- M Ahn
- M Martinez-Biarge
- MA Grillo
- MC Nguyen
- MJ LaFemina
- N Gulyaaeva
- N Hellström Erkenstam
- N Villalba
- O Bendel
- P Liu
- P Liu
- P Liu
- RR Handley
- S Choi
- S Fumagalli
- S Hamzei Taj
- S Lee
- S Morris
- TR Hammond
- Y Huang
- Publication venue
- eScholarship, University of California
- Publication date
- 01/03/2021
- Field of study
BackgroundArginases (ARG isoforms, ARG-1/ARG-2) are key regulatory enzymes of inflammation and tissue repair; however, their role after neonatal brain hypoxia (H) and hypoxia-ischemia (HI) remains unknown.MethodsC57BL/6 mice subjected to the Vannucci procedure on postnatal day (P9) were sacrificed at different timepoints. The degree of brain damage was assessed histologically. ARG spatiotemporal localization was determined via immunohistochemistry. ARG expression was measured by Western blot and activity spectrophotometrically.ResultsARG isoform expression increased during neurodevelopment (P9-P17) in the cortex and hippocampus. This was suppressed with H and HI only in the hippocampus. In the cortex, both isoforms increased with H alone and only ARG-2 increased with HI at 3 days. ARG activity during neurodevelopment remained unchanged, but increased at 1 day with H and not HI. ARG-1 localized with microglia at the injury site as early as 4 h after injury, while ARG-2 localized with neurons.ConclusionsARG isoform expression increases with age from P9 to P17, but is suppressed by injury specifically in the hippocampus and not in the cortex. Both levels and activity of ARG isoforms increase with H, while ARG-1 immunolabelling is upregulated in the HI cortex. Evidently, ARG isoforms in the brain differ in spatiotemporal localization, expression, and activity during neurodevelopment and after injury.ImpactArginase isoforms change during neurodevelopment and after neonatal brain HI. This is the first study investigating the key enzymes of inflammation and tissue repair called arginases following murine neonatal brain HI. The highly region- and cell-specific expression suggests the possibility of specific functions of arginases. ARG-1 in microglia at the injury site may regulate neuroinflammation, while ARG-2 in neurons of developmental structures may impact neurodevelopment. While further studies are needed to describe the exact role of ARGs after neonatal brain HI, our study adds valuable data on anatomical localization and expression of ARGs in brain during development and after stroke
Spatial Distribution of Calcium-Gated Chloride Channels in Olfactory Cilia
- Author
- AM Berezhkovskii
- AS Shah
- BP Menco
- BPhM Menco
- BPhM Menco
- BPM Menco
- D Badamdorj
- DA French
- DM Bers
- Donald A. French
- Dorjsuren Badamdorj
- GD Adamek
- H Takeuchi
- H Takeuchi
- Hiroaki Matsunami
- HP Larsson
- J Lee
- J Reisert
- J Reisert
- J Reisert
- JA Green
- JJB Jack
- K Fujiu
- K Schwarzenbacher
- L Quarmby
- LB Hartzell
- MK Higgins
- MS Lidow
- NF Berbari
- O Matsuzaki
- P Kalinay
- P Satir
- RA Bloodgood
- RJ Flannery
- S Antolin
- S Frings
- S Frings
- S Pifferi
- SJ Kleene
- SJ Kleene
- SJ Kleene
- SJ Kleene
- SJ Kleene
- SJ Kleene
- Steven J. Kleene
- TA Lohret
- TS Reese
- TV Getchell
- W Rall
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
Background: In vertebrate olfactory receptor neurons, sensory cilia transduce odor stimuli into changes in neuronal membrane potential. The voltage changes are primarily caused by the sequential openings of two types of channel: a cyclic-nucleotide-gated (CNG) cationic channel and a calcium-gated chloride channel. In frog, the cilia are 25 to 200 mm in length, so the spatial distributions of the channels may be an important determinant of odor sensitivity. Principal Findings: To determine the spatial distribution of the chloride channels, we recorded from single cilia as calcium was allowed to diffuse down the length of the cilium and activate the channels. A computational model of this experiment allowed an estimate of the spatial distribution of the chloride channels. On average, the channels were concentrated in a narrow band centered at a distance of 29 % of the ciliary length, measured from the base of the cilium. This matches the location of the CNG channels determined previously. This non-uniform distribution of transduction proteins is consistent with similar findings in other cilia. Conclusions: On average, the two types of olfactory transduction channel are concentrated in the same region of the cilium
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
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
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- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
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- Al Khoury K
- Alberghi GL
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- Aleksa M
- Aleksandrov IN
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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 VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
- Author
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Zhemchugov A
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- Zimmermann S
- Zinonos Z
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- Zobernig G
- Zoccoli A
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- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
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- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
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- Alves FLL
- Alviggi MG
- Ambler A
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- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
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- Buschmann E
- Bussey PJ
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- Buttinger W
- Buzatu A
- Buzykaev AR
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- Calafiura P
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- Chiu I
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- Zhao P
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
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- Zimmermann S
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- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
Search for excited electrons singly produced in proton–proton collisions at \sqrt{s} = 13 TeV with the ALAS experiment at the LHC
- Author
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- Zhemchugov A
- Zheng Z
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- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
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- Zwalinski L
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2019
- Field of study
A search for excited electrons produced in pp collisions at s√ = 13 TeV via a contact interaction qq¯→ee∗ is presented. The search uses 36.1 fb −1 of data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron into an electron and a pair of quarks ( eqq¯ ) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a W boson ( νW ) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying W boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the pp→ee∗→eeqq¯ and pp→ee∗→eνW production cross sections as a function of the excited electron mass me∗ at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter Λ of the model as a function of me∗ . For me∗<0.5 TeV , the lower bound for Λ is 11 TeV . In the special case of me∗=Λ , the values of me∗<4.8 TeV are excluded. The presented limits on Λ are more stringent than those obtained in previous searches
Search for heavy neutral Higgs bosons produced in association with b-quarks and decaying into b-quarks at root s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Acharya BS
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- Alberghi GL
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- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 13/08/2020
- Field of study
A search for heavy neutral Higgs bosons produced in association with one or two
b
-quarks and decaying to
b
-quark pairs is presented using
27.8
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider during 2015 and 2016. No evidence of a signal is found. Upper limits on the heavy neutral Higgs boson production cross section times its branching ratio to
b
¯
b
are set, ranging from 4.0 to 0.6 pb at 95% confidence level over a Higgs boson mass range of 450 to 1400 GeV. Results are interpreted within the two-Higgs-doublet model and the minimal supersymmetric Standard Model
Erratum: Measurement of angular and momentum distributions of charged particles within and around jets in Pb + Pb and pp collisions at √sNN = 5.02 TeV with the ATLAS detector [Phys. Rev. C 100 , 064901 (2019)]
- Author
- Aad G
- Abbott B
- Abbott Dc
- Abed Abud A
- Abeling K
- Abhayasinghe Dk
- Abidi Sh
- Abouzeid Os
- Abraham Nl
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya Bs
- Achkar B
- Adachi S
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder Aa
- Afik Y
- Agapopoulou C
- Agaras Mn
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra Ja
- Ahmadov F
- Ahmed Ws
- Ai X
- Aielli G
- Akatsuka S
- Akesson Tpa
- Akilli E
- Akimov Av
- Al Khoury K
- Alberghi Gl
- Albert J
- Alconada Verzini Mj
- Alderweireldt S
- Aleksa M
- Aleksandrov In
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire Sp
- Allaire C
- Allbrooke Bmm
- Allen Bw
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- Alshehri Aa
- Alvarez Estevez M
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- Alviggi Mg
- Amaral Coutinho Y
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- Amidei D
- Amor Dos Santos Sp
- Amoroso S
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- An F
- Anastopoulos C
- Andari N
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- Angerami A
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- Burr Jtp
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- Buscher V
- Buschmann E
- Bussey Pj
- Butler Jm
- Buttar Cm
- Butterworth Jm
- Butti P
- Buttinger W
- Buxo Vazquez Cj
- Buzatu A
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- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo Vmm
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- Calafiura P
- Calandri A
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- Calvente Lopez S
- Calvet D
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- Camarda S
- Camarero Munoz D
- Camarri P
- Cameron D
- Caminal Armadans R
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cano Bret M
- Cantero J
- Cao T
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- Capeans Garrido Mdm
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson Bt
- Carminati L
- Carney Rmd
- Caron S
- Carquin E
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- Carter Jws
- Casado Mp
- Casha Af
- Casper Dw
- Castelijn R
- Castillo Gimenez V
- Castillo Fl
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- Catinaccio A
- Catmore Jr
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerny K
- Cerqueira As
- Cerri A
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- Cerutti F
- Cervelli A
- Cetin Sa
- Chadi Z
- Chakraborty D
- Chan Sk
- Chan Ws
- Chan Wy
- Chapman Jd
- Chargeishvili B
- Charlton Dg
- Charman Tp
- Chau Cc
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- Chekanov S
- Chekulaev Sv
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- Chen B
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- Chen J
- Chen J
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- Cheng Hc
- Cheng Hj
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalerias Tja
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm As
- Chitan A
- Chiu I
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- Chouridou S
- Chow Ys
- Chu Mc
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- Cieri D
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- Cinca D
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- Cioara Ia
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- Coniavitis E
- Connell Sh
- Connelly Ia
- Constantinescu S
- Conventi F
- Cooper-Sarkar Am
- Cormier F
- Cormier Kjr
- Corpe Ld
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- Costa Mj
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- Costanzo D
- Cowan G
- Cowley Jw
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- Cranmer K
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- Crescioli F
- Cristinziani M
- Croft V
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- Cueto A
- Cuhadar Donszelmann T
- Cukierman Ar
- Cunningham Wr
- Czekierda S
- Czodrowski P
- D'Amen G
- D'Amico V
- D'Auria S
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- Dandoy Jr
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- Debenedetti C
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- Delabat Diaz Y
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- Denisov Sp
- Denysiuk D
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- Du D
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- Dutta B
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- Dyckes Gi
- Dyndal M
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- Ecker Km
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- Ferrer A
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- Gaudio G
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- Helling Cm
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- Henderson Rcw
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- Henriques Correia Am
- Herbert Gh
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- Herget V
- Hernandez Jimenez Y
- Herr H
- Herrmann Mg
- Herrmann T
- Herten G
- Hertenberger R
- Hervas L
- Herwig Tc
- Hesketh Gg
- Hessey Np
- Higashida A
- Higashino S
- Higon-Rodriguez E
- Hildebrand K
- Hill E
- Hill Jc
- Hill Kk
- Hiller Kh
- Hillier Sj
- Hils M
- Hinchliffe I
- Hinterkeuser F
- Hirose M
- Hirose S
- Hirschbuehl D
- Hiti B
- Hladik O
- Hlaluku Dr
- Hoad X
- Hobbs J
- Hod N
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- Hoecker A
- Hoenig F
- Hohn D
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- Holmes Tr
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- Hong Tm
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- Honle A
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- Semprini-Cesari N
- Sen S
- Senkin S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shahinian Jd
- Shaikh Nw
- Shaked Renous D
- Shan Ly
- Shang R
- Shank Jt
- Shapiro M
- Sharma A
- Sharma As
- Shatalov Pb
- Shaw K
- Shaw Sm
- Shcherbakova A
- Shehade M
- Shen Y
- Sherafati N
- Sherman Ad
- Sherwood P
- Shi L
- Shimizu S
- Shimmin Co
- Shimogama Y
- Shimojima M
- Shipsey Ipj
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet Mj
- Shojaii J
- Shope Dr
- Shrestha S
- Shrif Em
- Shulga E
- Sicho P
- Sickles Am
- Sidebo Pe
- Sideras Haddad E
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva Oliveira Mv
- Silva Mj
- Silverstein Sb
- Simion S
- Simioni E
- Simoniello R
- Simsek S
- Sinervo P
- Sinetckii V
- Sinev Nb
- Sioli M
- Siral I
- Sivoklokov Sy
- Sjolin J
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart Bh
- Smiesko J
- Smirnov N
- Smirnov Sy
- Smirnov Y
- Smirnova Ln
- Smirnova O
- Smith Jw
- Smizanska M
- Smolek K
- Smykiewicz A
- Snesarev Aa
- Snoek Hl
- Snyder Im
- Snyder S
- Sobie R
- Soffer A
- Sogaard A
- Sohns F
- Solans Sanchez Ca
- Soldatov Ey
- Soldevila U
- Solodkov Aa
- Soloshenko A
- Solovyanov Ov
- Solovyev V
- Sommer P
- Son H
- Song W
- Song Wy
- Sopczak A
- Sopkova F
- Sotiropoulou Cl
- Sottocornola S
- Soualah R
- Soukharev Am
- South D
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spieker Tm
- Spighi R
- Spigo G
- Spina M
- Spiteri Dp
- Spousta M
- Stabile A
- Stamas Bl
- Stamen R
- Stamenkovic M
- Stanecka E
- Stanislaus B
- Stanitzki Mm
- Stankaityte M
- Stapf B
- Starchenko Ea
- Stark Gh
- Stark J
- Stark Sh
- Staroba P
- Starovoitov P
- Starz S
- Staszewski R
- Stavropoulos G
- Stegler M
- Steinberg P
- Steinhebel Al
- Stelzer B
- Stelzer Hj
- Stelzer-Chilton O
- Stenzel H
- Stevenson Tj
- Stewart Ga
- Stockton Mc
- Stoicea G
- Stolarski M
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Strohmer R
- Strom Dm
- Stroynowski R
- Strubig A
- Stucci Sa
- Stugu B
- Stupak J
- Styles Na
- Su D
- Suchek S
- Sulin Vv
- Sullivan Mj
- Sultan Dms
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suruliz K
- Suster Cje
- Sutton Mr
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift Sp
- Swirski T
- Sydorenko A
- Sykora I
- Sykora M
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Takai H
- Takashima R
- Takeda K
- Takeshita T
- Takeva Ep
- Takubo Y
- Talby M
- Talyshev Aa
- Tamir Nm
- Tanaka J
- Tanaka M
- Tanaka R
- Tapia Araya S
- Tapprogge S
- Tarek Abouelfadl Mohamed A
- Tarem S
- Tariq K
- Tarna G
- Tartarelli Gf
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
- Taylor Aj
- Taylor Gn
- Taylor W
- Tee As
- Teixeira De Lima R
- Teixeira-Dias P
- Ten Kate H
- Teoh Jj
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher Rj
- Thais Sj
- Theveneaux-Pelzer T
- Thiele F
- Thomas Dw
- Thomas Jo
- Thomas Jp
- Thompson As
- Thompson Pd
- Thomsen La
- Thomson E
- Thorpe Ej
- Ticse Torres Re
- Tikhomirov Vo
- Tikhonov Ya
- Timoshenko S
- Tipton P
- Tisserant S
- Todome K
- Todorova-Nova S
- Todt S
- Tojo J
- Tokar S
- Tokushuku K
- Tolley E
- Tomiwa Kg
- Tomoto M
- Tompkins L
- Tong B
- Tornambe P
- Torrence E
- Torres H
- Torro Pastor E
- Tosciri C
- Toth J
- Tovey Dr
- Traeet A
- Treado Cj
- Trefzger T
- Tresoldi F
- Tricoli A
- Trigger Im
- Trincaz-Duvoid S
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trovatelli M
- Trovato F
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tseng JC-
- Tsiareshka Pv
- Tsirigotis A
- Tsiskaridze V
- Tskhadadze Eg
- Tsopoulou M
- Tsukerman Ii
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure Tt
- Tuna An
- Turchikhin S
- Turgeman D
- Turk Cakir I
- Turner Rj
- Turra Rt
- Tuts Pm
- Tzamarias S
- Tzovara E
- Ucchielli G
- Uchida K
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro Fc
- Unno Y
- Uno K
- Urban J
- Urquijo P
- Usai G
- Uysal Z
- Vacavant L
- Vacek V
- Vachon B
- Vadla Koh
- Vaidya A
- Valderanis C
- Valdes Santurio E
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance Ra
- Vallier A
- Valls Ferrer Ja
- Van Daalen Tr
- Van Gemmeren P
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandewall Er
- Vaniachine A
- Vannicola D
- Vari R
- Varnes Ew
- Varni C
- Varol T
- Varouchas D
- Varvell Ke
- Vasile Me
- Vasquez Ga
- Vasquez Jg
- Vazeille F
- Vazquez Furelos D
- Vazquez Schroeder T
- Veatch J
- Vecchio V
- Veen Mj
- Veloce Lm
- Veloso F
- Veneziano S
- Ventura A
- Venturi N
- Verbytskyi A
- Vercesi V
- Verducci M
- Vergel Infante Cm
- Vergis C
- Verkerke W
- Vermeulen At
- Vermeulen Jc
- Vetterli Mc
- Viaux Maira N
- Vicente Barreto Pinto M
- Vickey Boeriu Oe
- Vickey T
- Viehhauser Gha
- Vigani L
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter Mg
- Virdee Gs
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
- Von Buddenbrock Se
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld Jh
- Vozak M
- Vranjes Milosavljevic M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Walbrecht Vm
- Walder J
- Walker R
- Walker Sd
- Walkowiak W
- Wallangen V
- Wang Am
- Wang C
- Wang C
- Wang F
- Wang H
- Wang H
- Wang J
- Wang J
- Wang J
- Wang P
- Wang Q
- Wang R
- Wang R
- Wang R-
- Wang Sm
- Wang W
- Wang Wt
- Wang Wx
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward Cp
- Wardrope Dr
- Warrack N
- Washbrook A
- Watson At
- Watson Mf
- Watts G
- Waugh Bm
- Webb Af
- Webb S
- Weber C
- Weber Ms
- Weber Sa
- Weber Sm
- Weidberg Ar
- Weingarten J
- Weirich M
- Weiser C
- Wells Ps
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner Md
- Wessels M
- Weston Td
- Whalen K
- Whallon Nl
- Wharton Am
- White A
- White As
- White Mj
- Whiteson D
- Whitmore Bw
- Wiedenmann W
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs Lam
- Wilk F
- Wilkens Hg
- Wilkins Lj
- Williams Hh
- Williams S
- Willis C
- Willocq S
- Wilson Ja
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston Oj
- Winter Bt
- Wittgen M
- Wobisch M
- Wolf A
- Wolf Tmh
- Wolff R
- Wolker Rw
- Wollrath J
- Wolter Mw
- Wolters H
- Wong Vws
- Woods Nl
- Worm Sd
- Wosiek Bk
- Wozniak Kw
- Wraight K
- Wu Sl
- Wu X
- Wu Y
- Wyatt Tr
- Wynne Bm
- Xella S
- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yajima K
- Yallup Dp
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang Hj
- Yang Ht
- Yang S
- Yang X
- Yang Y
- Yao W-
- Yap Yc
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yexley Mr
- Yigitbasi E
- Yorita K
- Yoshihara K
- Young C
- Young Cjs
- Yu J
- Yuan R
- Yue X
- Yuen Spy
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev Am
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas Dr
- Zeissner Sv
- Zeitnitz C
- Zemaityte G
- Zeng Jc
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang Df
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou Ms
- Zhou N
- Zhou Y
- Zhu C
- Zhu Cg
- Zhu H
- Zhu Hl
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine Ni
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas Tg
- Zou R
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2020
- Field of study
- …