371 research outputs found
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
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- Argyropoulos S
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- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
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- Yang UK
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- Yanush S
- Yao L
- Yao W-M
- Yasu Y
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- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
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- Yusuff I
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- Zaidan R
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- Zanello L
- Zanzi D
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- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
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- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
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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
A construção de um ambiente virtual de aprendizagem para educação a distância: uma estratégia educativa em serviço
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Achievable tolerances in robotic feature machining operations using a low-cost hexapod
- Author
- A Olabi
- A Olabi
- A Panda
- AK Kamrani
- B Li
- B Olofsson
- C Doukas
- C Dumas
- C Gong
- C Lehmann
- D Kanaan
- D Karimi
- E Abele
- G Bianchi
- H Chanal
- H Moradi
- H Wu
- H Wu
- H-TT Zhang
- HZH Zhang
- I Zaghbani
- J Chen
- J-HH Jung
- J. D. Barnfather
- JD Barnfather
- JD Barnfather
- JFCP Antunes Simões
- JP Davim
- JP Davim
- K Cheng
- K Young
- KM Li
- LT Tunc
- LT Tunc
- M Agheli
- M Kovářík
- M. J. Goodfellow
- MA Stephens
- MA Stephens
- N Grossi
- NM Razali
- O Sörnmo
- P Pessi
- P Turek
- R Weill
- RM Sakia
- S Zargarbashi
- S Zargarbashi
- SI Matsuoka
- SZ Hosseinifard
- T. Abram
- V Gagnol
- Y Li
- Z Pan
- Z Wang
- ZM Bi
- ZM Bi
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Portable robotic machine tools potentially allow feature machining processes to be brought to large parts in various industries, creating an opportunity for capital expenditure and operating cost reduction. However, robots lack the machining capability of conventional equipment, which ultimately results in dimensional errors in parts. This work showcases a low-cost hexapod-based robotic machine tool and presents experimental research conducted to investigate how the widely researched robotic machining challenges, e.g. structural dynamics and kinematics, translate to achievable tolerance ranges in real-world production to highlight currently feasible applications and provide a context for considering technology improvements. Machining trials assess the total dimensional errors in the final part over multiple geometries. A key finding is error variation which is in the sub-millimetre range, although, in some cases, upper tolerance limits < 100 μm are achieved. Practical challenges are also noted. Most significantly, it is demonstrated that dimensional machining error is mainly systematic in nature and therefore that the total error can be dramatically reduced with in situ measurement and compensation. Potential is therefore found to achieve a flexible, high-performance robotic machining capability despite complex and diverse underlying scientific challenges. Overall, the work presented highlights achievable tolerances in low-cost robotic machining and opportunities for improvement, also providing a practical benchmark useful for process selection
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouzeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlas Collaboration
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
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- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV with the ATLAS Detector
- Author
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- Yildiz H Duran
- Yorita K
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- Yuen SPY
- Yusuff I
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- Zalieckas J
- Zambito S
- Zanzi D
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- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
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- Zerwas D
- Zgubic M
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- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
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- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Operation and performance of the ATLAS Tile Calorimeter in Run 1
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouelfadl 
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez 
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor 
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Argos FC
- Arguin J-
- Argyropoulos S
- Armadans R
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME
- Atkin RJ
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Álvarez Piqueras D
- Åkesson TPA
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahilo JJL
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
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- Baker OK
- Bakker PJ
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M
- Barkeloo J
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- Barreiro F
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- Barton AE
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- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batlamous S
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
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- Bierwagen K
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- Billoud TRV
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- Biswal JP
- Bittrich C
- Bjergaard DM
- Black JE
- Black KM
- Blair RE
- Blazek T
- Bloch I
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- Blumenschein U
- Blunier D
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
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- Cakir I
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- Calvet D
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- Fiolhais MCN
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- Fleck I
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- Lopez 
- Lopez JA
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- Lyubushkin V
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- Ma LL
- Ma Y
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- Machado 
- Maček B
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- Martyniuk AC
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- Naryshkin I
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- Zur 
- Zwalinski L
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The Tile Calorimeter is the hadron calorimeter covering the central region of the ATLAS experiment at the Large Hadron Collider. Approximately 10,000 photomultipliers collect light from scintillating tiles acting as the active material sandwiched between slabs of steel absorber. This paper gives an overview of the calorimeter’s performance during the years 2008–2012 using cosmic-ray muon events and proton–proton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fb−1. The signal reconstruction methods, calibration systems as well as the detector operation status are presented. The energy and time calibration methods performed excellently, resulting in good stability of the calorimeter response under varying conditions during the LHC Run 1. Finally, the Tile Calorimeter response to isolated muons and hadrons as well as to jets from proton–proton collisions is presented. The results demonstrate excellent performance in accord with specifications mentioned in the Technical Design Report
Performance of missing transverse momentum reconstruction with the ATLAS detector using proton–proton collisions at √s = 13 TeV
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- Zhemchugov A
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in proton–proton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying τ -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fb−1
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at root s = 8 TeV with the ATLAS detector (vol 75, 299, 2015)
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- Aad G
- Abbott B
- Abdallah J
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- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- 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 EmissT>150 GeV and EmissT>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 presented
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at root s = 8 TeV with the ATLAS detector (vol 75, 299, 2015)
- Author
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- Abbott B
- Abdallah J
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- Subramaniam R
- Succurro A
- Sugaya Y
- Suhr C
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki Y
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- Swedish S
- Swiatlowski M
- Sykora I
- Sykora T
- Ta D
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- Taenzer J
- Taffard A
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- Talyshev AA
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- Tan KG
- Tanaka J
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- Tanasijczuk AJ
- Tannenwald BB
- Tannoury N
- Tapprogge S
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- Tarrade F
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
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- Teischinger FA
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- Temming KK
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
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- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
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- Thompson EN
- Thompson PD
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- Thomsen LA
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- Tibbetts MJ
- Tikhomirov VO
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- Toro RC
- Torregrosa EF
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- Torres RET
- Torro Pastor E
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- Tran HL
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- Trigger IM
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- Tripiana MF
- Trischuk W
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- Troncon C
- Trottier-McDonald M
- Trovatelli M
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- Trzebinski M
- Trzupek A
- Tsarouchas C
- Tseng JC-L
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tudorache A
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- Tuna AN
- Tupputi SA
- Turchikhin S
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- Tyndel M
- Ueda I
- Ueno R
- Ughetto M
- Ugland M
- Uhlenbrock M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
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- Urban J
- Urquijo P
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- Valladolid Gallego E
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- Veneziano S
- Ventura A
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- Vichou I
- Vickey T
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- Viel S
- Vigne R
- Villa M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Virzi J
- Vivarelli I
- Vlachos S
- Vladoiu D
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- Winklmeier F
- Winter BT
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- Wittkowski J
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- Wosiek BK
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- Yamaguchi Y
- Yamamoto A
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- Yamanaka T
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- Yamazaki Y
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- Yanush S
- Yao L
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
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- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
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- Young CJS
- Youssef S
- Yu DR
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- Yu JM
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- Yurkewicz A
- 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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- Zhemchugov A
- Zhong J
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- Zibell A
- Zieminska D
- Zimine NI
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- Zimmermann R
- 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
- 01/01/2015
- Field of study
- …