7 research outputs found
Combination of searches for WW, WZ, and ZZ resonances in pp collisions at root s=8 TeV with the ATLAS detector
- Author
- Aad G
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
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- Akerstedt H
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- Alberghi GL
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- Alconada Verzini MJ
- Aleksa M
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- ATLAS Collaboration .
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- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 10/04/2016
- Field of study
The ATLAS experiment at the CERN Large Hadron Collider has performed searches for new, heavy bosons decaying to WW, WZ and ZZ final states in multiple decay channels using 20.3 fb-1 of pp collision data at s=8 TeV. In the current study, the results of these searches are combined to provide a more stringent test of models predicting heavy resonances with couplings to vector bosons. Direct searches for a charged diboson resonance decaying to WZ in the ℓνℓ'ℓ' (ℓ=μ, e), ℓℓqq-, ℓνqq- and fully hadronic final states are combined and upper limits on the rate of production times branching ratio to the WZ bosons are compared with predictions of an extended gauge model with a heavy W' boson. In addition, direct searches for a neutral diboson resonance decaying to WW and ZZ in the ℓℓqq-, ℓνqq-, and fully hadronic final states are combined and upper limits on the rate of production times branching ratio to the WW and ZZ bosons are compared with predictions for a heavy, spin-2 graviton in an extended Randall-Sundrum model where the Standard Model fields are allowed to propagate in the bulk of the extra dimension
Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
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- Acharya BS
- Adachi S
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- Aguilar-Saavedra JA
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- Alberghi GL
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- Perepelitsa DV
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- Pernegger H
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- Worm SD
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- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiza H Duran
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
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- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
The rejection of forward jets originating from
additional proton–proton interactions (pile-up) is crucial for
a variety of physics analyses at the LHC, including Standard
Model measurements and searches for physics beyond
the Standard Model. The identification of such jets is challenging
due to the lack of track and vertex information in
the pseudorapidity range |η| > 2.5. This paper presents a
novel strategy for forward pile-up jet tagging that exploits
jet shapes and topological jet correlations in pile-up interactions.
Measurements of the per-jet tagging efficiency are
presented using a data set of 3.2 fb−1 of proton–proton collisions
at a centre-of-mass energy of 13 TeV collected with the
ATLAS detector. The fraction of pile-up jets rejected in the
range 2.5 < |η| < 4.5 is estimated in simulated events with
an average of 22 interactions per bunch-crossing. It increases
with jet transverse momentum and, for jets with transverse
momentum between 20 and 50 GeV, it ranges between 49%
and 67% with an efficiency of 85% for selecting hard-scatter
jets. A case study is performed in Higgs boson production
via the vector-boson fusion process, showing that these techniques
mitigate the background growth due to additional
proton–proton interactions, thus enhancing the reach for such
signatures
Recommended from our members
A neural network clustering algorithm for the ATLAS silicon pixel 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
- Adamczyka 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
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- 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
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Araquea JP
- Arce ATH
- Arguin JF
- Argyropoulos S
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Bella LA
- Coutinho YA
- Gonzalez BA
- Khalek SA
- Verzini MJA
- Åkesson TPA
- Publication venue
- eScholarship, University of California
- Publication date
- 01/09/2014
- Field of study
A novel technique to identify and split clusters created by multiple charged particles in the ATLAS pixel detector using a set of artificial neural networks is presented. Such merged clusters are a common feature of tracks originating from highly energetic objects, such as jets. Neural networks are trained using Monte Carlo samples produced with a detailed detector simulation. This technique replaces the former clustering approach based on a connected component analysis and charge interpolation. The performance of the neural network splitting technique is quantified using data from proton-proton collisions at the LHC collected by the ATLAS detector in 2011 and from Monte Carlo simulations. This technique reduces the number of clusters shared between tracks in highly energetic jets by up to a factor of three. It also provides more precise position and error estimates of the clusters in both the transverse and longitudinal impact parameter resolution
Combination of searches for WW, WZ, and ZZ resonances in pp collisions at root s=8 TeV with the ATLAS detector
- Author
- Aad G
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Aranda CP
- Araquea JP
- Arayab ST
- Arce ATH
- Arduh FA
- Arguin JF
- Argyropoulos S
- Arik M
- Aring kesson TP
- Aring sman B
- Armadans RC
- Armbruster AJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
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- Kourkoumelis C
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- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2016
- Field of study
The ATLAS experiment at the CERN Large Hadron Collider has performed searches for new, heavy bosons decaying to WW, WZ and ZZ final states in multiple decay channels using 20.3 fb(-1) of pp collision data at root s = 8 TeV. In the current study, the results of these searches are combined to provide a more stringent test of models predicting heavy resonances with couplings to vector bosons. Direct searches for a charged diboson resonance decaying to WZ in the l nu l'l' (l = mu, e), llq (q) over bar, l nu q (q) over bar and fully hadronic final states are combined and upper limits on the rate of production times branching ratio to the WZ bosons are compared with predictions of an extended gauge model with a heavy W' boson. In addition, direct searches for a neutral diboson resonance decaying to WW and ZZ in the llq (q) over bar, l nu q (q) over bar, and fully hadronic final states are combined and upper limits on the rate of production times branching ratio to the WW and ZZ bosons are compared with predictions for a heavy, spin-2 graviton in an extended Randall-Sundrum model where the Standard Model fields are allowed to propagate in the bulk of the extra dimension. (C) 2016 CERN for the benefit of the ATLAS Collaboration. Published by Elsevier B.V
Performance of the ATLAS track reconstruction algorithms in dense environments in LHC Run 2
- Author
- Aaboudd M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
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- Vazquez JGP
- Verzini MJA
- Villara DIN
- Walls FMG
- Yildiz HD
- Publication venue
- Publication date
- 01/01/2017
- Field of study
With the increase in energy of the Large Hadron Collider to a centre-of-mass energy of 13 TeV for Run 2, events with dense environments, such as in the cores of highenergy jets, became a focus for new physics searches as well as measurements of the Standard Model. These environments are characterized by charged-particle separations of the order of the tracking detectors sensor granularity. Basic track quantities are compared between 3.2 fb(-1) of data collected by the ATLAS experiment and simulation of protonproton collisions producing high-transverse-momentum jets at a centre-of-mass energy of 13 TeV. The impact of chargedparticle separations and multiplicities on the track reconstruction performance is discussed. The track reconstruction efficiency in the cores of jets with transverse momenta between 200 and 1600 GeV is quantified using a novel, datadriven, method. The method uses the energy loss, dE/ dx, to identify pixel clusters originating from two charged particles. Of the charged particles creating these clusters, themeasured fraction that fail to be reconstructed is 0.061 +/- 0.006 (stat.) +/- 0.014 (syst.) and 0.093 +/- 0.017 (stat.) +/- 0.021 (syst.) for jet transverse momenta of 200-400GeV and 1400-1600GeV, respectively
Measurement of the relative width difference of the B0-Bˉ0 system with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Aba BSA
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaitia Y
- Adamczyka L
- Adams DL
- Adelman J
- Adomeitioi S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alstaty M
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorirn A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
20 pages plus author list + cover page (38 pages total), 5 figures, 2 tables, submitted to Journal of High Energy Physics, All figures including auxiliary figures are available at http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/BPHY-2015-01/ - See paper for full list of authorsInternational audienceThis paper presents the measurement of the relative width difference ΔΓd/Γd of the B0-Bˉ0 system using the data collected by the ATLAS experiment at the LHC in pp collisions at s=7 TeV and s=8 TeV and corresponding to an integrated luminosity of 25.2 fb−1. The value of ΔΓd/Γd is obtained by comparing the decay-time distributions of B0→J/ψKS and B0→J/ψK∗0(892) decays. The result is \Delta \Gamma_d / \Gamma_d = (-0.1 \pm 1.1~\mbox{(stat.)} \pm 0.9~\mbox{(syst.)}) \times 10^{-2}. Currently, this is the most precise single measurement of ΔΓd/Γd. It agrees with the Standard Model prediction and the measurements by other experiments
Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector (vol 77, 580, 2017)
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
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- Alberghi GL
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- Rauscher F
- Rave S
- Ravinovich I
- Rawling JH
- Raymond M
- Read AL
- Readioff NP
- Realea M
- Rebuzzia DM
- Redelbach A
- Redlinger G
- Reece R
- Reed RG
- Reeves K
- Rehnisch L
- Reichert J
- Reiss A
- Rembser C
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- Resconia S
- Resseguie ED
- Rettie S
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- Rezanova OL
- Reznicek P
- Rezvani R
- Richter R
- Richter S
- Richter-Was E
- Ricken O
- Ridel M
- Rieck P
- Riegel CJ
- Rieger J
- Rifki O
- Rijssenbeek M
- Rimoldi M
- Rimoldia A
- Rinaldia L
- Ripellino G
- Risti B
- Ritsch E
- Riu I
- Rizatdinova F
- Rizvi E
- Rizzi C
- Roberts RT
- Robertson SH
- Robichaud-Veronneau A
- Robinson D
- Robinson JEM
- Robson A
- Rocco E
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- Rodina Y
- Rodriguez DR
- Rodriguez LP
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- Rogan CS
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- Rossi E
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- Rosten JHN
- Rosten R
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- Rozanov A
- Rozas AJ
- Rozen Y
- Ruan X
- Rubbo F
- Ruhr F
- Ruiz-Martinez A
- Rurikova Z
- Rusakovich NA
- Russell HL
- Rutherfoord JP
- Ruthmann N
- Ryabov YF
- Rybar M
- Rybkin G
- Ryu S
- Ryzhov A
- Rzehorz GF
- Saadi DS
- Saavedra AF
- Sabato G
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- Sadrozinski HF-W
- Sadykov R
- Saez SMR
- Saha P
- Sahinsoy M
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- Saito M
- Saito T
- Sakamoto H
- Sakurai Y
- Salamanna G
- Salek D
- Salihagic D
- Salnikov A
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- Salvatore D
- Salvatore F
- Salvucci A
- Salzburger A
- Sammel D
- Sampsonidis D
- Sampsonidou D
- Sanchez CAS
- Sanchez FJM
- Sanchez J
- Sandaker H
- Sandbach RL
- Sander CO
- Sandhoff M
- Sandoval C
- Sankey DPC
- Sannino M
- Sansoni A
- Santoni C
- Santonico R
- Santos H
- Santurio EV
- Sapronov A
- Saraiva JG
- Sarrazin B
- Sasaki O
- Sato K
- Sauvan E
- Savage G
- Savard P
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- Saxon J
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- Sbrizzi A
- Scanlon T
- Scannicchio DA
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- Scarfone V
- Schaarschmidt J
- Schacht P
- Schachtner BM
- Schaefer D
- Schaefer L
- Schaefer R
- Schaeffer J
- Schaepe S
- Schaetzel S
- Schafer U
- Schaffer AC
- Schaile D
- Schamberger RD
- Scharf V
- Schegelsky VA
- Scheirich D
- Schernau M
- Schiavi C
- Schier S
- Schildgen LK
- Schillo C
- Schioppa M
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schmitz S
- Schnoor U
- Schoeffel L
- Schoening A
- Schoenrock BD
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schroeder TV
- Schuh N
- Schulte A
- Schultens MJ
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schweiger H
- Schwemling P
- Schwienhorst R
- Schwindling J
- Sciandra A
- Sciolla G
- Scuri F
- Scutti F
- Seabra LFO
- Searcy J
- Seema P
- Seidel SC
- Seiden A
- Seixas JM
- Sekhniaidze G
- Sekhon K
- Sekula SJ
- Semprini-Cesari N
- Senkin S
- Serfon C
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- Serkin L
- Sessa M
- Seuster R
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shaikh NW
- Shan LY
- Shang R
- Shank JT
- Shapiro M
- Shatalov PB
- Shaw K
- Shaw SM
- Shcherbakova A
- Shehu CY
- Shen Y
- Sherafati N
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet MJ
- Shojaii S
- Shope DR
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
- Sickles AM
- Sidebo PE
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- Silverstein SB
- Simak V
- Simic L
- Simion S
- Simioni E
- Simmons B
- Simon M
- Sinervo P
- Sinev NB
- Sioli M
- Siragusa G
- Siral I
- Sivoklokov SY
- Sjolin J
- Skinner MB
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith JW
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snyder IM
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Soh DA
- Sokhrannyi G
- Sola JDB
- Solar M
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Sopczak A
- Sosa D
- Sotiropoulou CL
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spettel F
- Spieker TM
- Spighi R
- Spigo G
- Spiller LA
- Spousta M
- St Denis RD
- Stabile A
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- Stamm S
- Stanecka E
- Stanek RW
- Stanescu C
- Stanitzki MM
- Stapf BS
- Stapnes S
- Starchenko EA
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- Stark SH
- Staroba P
- Starovoitov P
- Staszewski R
- Steinberg P
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stewart GA
- Stockton MC
- Stoebe M
- Stoicea G
- Stolte P
- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Strohmer R
- Strom DM
- Stroynowski R
- Strubig A
- Strz S
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Suchek S
- Sugaya Y
- Suk M
- Sulin VV
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suruliz K
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Taiblum N
- Takai H
- Takashima R
- Takasugi EH
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tanaka J
- Tanaka M
- Tanaka R
- Tanaka S
- Tanioka R
- Tannenwald BB
- Tapprogge S
- Tarem S
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tayalati Y
- Taylor AC
- Taylor GN
- Taylor PTE
- Taylor W
- Tehrani FS
- Teixeira-Dias P
- Temple D
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Theenhausen HMZ
- Theveneaux-Pelzer T
- Thomas JP
- Thomas-Wilsker J
- Thompson AS
- Thompson PD
- Thomsen LA
- Thomson E
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
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- Toro RC
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- Toth J
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- Trefzger T
- Tresoldi F
- Tricoli A
- Triggera IM
- Trincaz-Duvoid S
- Tripiana MF
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- Truong L
- Trzebinski M
- Trzupek A
- Tsang KW
- Tseng JC-L
- Tsiareshka PV
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsui KM
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turgeman D
- Turra R
- Tuts PM
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Unverdorben C
- Urban J
- Urban SC
- Urquijo P
- Urrejola P
- Usai G
- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Vaidya A
- Valderanis C
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallier A
- Van den Wollenberg W
- van der Graaf H
- van Gemmeren P
- Van Nieuwkoop J
- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vardanyan G
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vasquez GA
- Vasquez JG
- Vazeille F
- Vazquez JGP
- Veatch J
- Veeraraghavan V
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Verzini MJA
- Vetterli MC
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Villa M
- Villar DIN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vlasak M
- Vogel M
- Vokac P
- Volpi G
- von der Schmitt H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
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- Walkowiak W
- Wallangen V
- Walls FMG
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- Wanotayaroj C
- Warburton A
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- Wardrope DR
- Washbrook A
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- Watson AT
- Watson MF
- Watts G
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- Waugh BM
- Webb AF
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- Weber MS
- Weber SA
- Weber SW
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weirich M
- Weiser C
- Weits H
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Werner P
- Wessels M
- Whalen K
- Whallon NL
- Wharton AM
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- White R
- Whiteson D
- Whitmore BW
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- 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 TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong KHY
- Wong VWS
- Worm SD
- Wosiek BK
- Wotschack J
- Wozniak KW
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu L
- Xu T
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamatani M
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiza HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
SCOAP