655 research outputs found
Skull base repair following endonasal pituitary and skull base tumour resection: a systematic review.
- Author
- Publication venue
- Pituitary
- Publication date
- 01/01/2021
- Field of study
PURPOSE: Postoperative cerebrospinal fluid rhinorrhoea (CSFR) remains a frequent complication of endonasal approaches to pituitary and skull base tumours. Watertight skull base reconstruction is important in preventing CSFR. We sought to systematically review the current literature of available skull base repair techniques. METHODS: Pubmed and Embase databases were searched for studies (2000-2020) that (a) reported on the endonasal resection of pituitary and skull base tumours, (b) focussed on skull base repair techniques and/or postoperative CSFR risk factors, and (c) included CSFR data. Roles, advantages and disadvantages of each repair method were detailed. Random-effects meta-analyses were performed where possible. RESULTS: 193 studies were included. Repair methods were categorised based on function and anatomical level. There was absolute heterogeneity in repair methods used, with no independent studies sharing the same repair protocol. Techniques most commonly used for low CSFR risk cases were fat grafts, fascia lata grafts and synthetic grafts. For cases with higher CSFR risk, multilayer regimes were utilized with vascularized flaps, gasket sealing and lumbar drains. Lumbar drain use for high CSFR risk cases was supported by a randomised study (Oxford CEBM: Grade B recommendation), but otherwise there was limited high-level evidence. Pooled CSFR incidence by approach was 3.7% (CI 3-4.5%) for transsphenoidal, 9% (CI 7.2-11.3%) for expanded endonasal, and 5.3% (CI 3.4-7%) for studies describing both. Further meaningful meta-analyses of repair methods were not performed due to significant repair protocol heterogeneity. CONCLUSIONS: Modern reconstructive protocols are heterogeneous and there is limited evidence to suggest the optimal repair technique after pituitary and skull base tumour resection. Further studies are needed to guide practice
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Wissing C
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- Wood JS
- Worm SD
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- Xiao H
- Xie S
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- Yang F
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- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
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- Xiao H
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- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
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- Alcaraz Maestre J
- Alda Junior WL
- Alexander J
- Aliev T
- Alimena J
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- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunovic Z
- Apanasevich L
- Appelt E
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- Arcidiacono R
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- Bauerdick LAT
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- Bazterra VE
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- Behr J
- Behrenhoff W
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- Bell AJ
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- Beuselinck R
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
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- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
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- Zarubin A
- Zatserklyaniy A
- Zeinali M
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- Zeuner WD
- Zeyrek M
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- Zheng Y
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- Zhukov V
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- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
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- Choudhary BC
- Choudhury S
- Christiansen T
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- Chuang SH
- Chwalek T
- Ciesielski R
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- Cittolin S
- Ciulli V
- Civinini C
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- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Coarasa Perez JA
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Abbiendi G
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- Yilmaz Y
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- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Dabrowski A
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- de Cassagnac RG
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- Yilmaz Y
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of
2.76 TeV per nucleon pair was studied using data collected with the CMS
detector at the LHC. Fragmentation functions are constructed using
charged-particle tracks with transverse momenta pt > 4 GeV for dijet events
with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events
are compared to those in pp data as a function of collision centrality, as well
as dijet-pt imbalance. Special emphasis is placed on the most central PbPb
events including dijets with unbalanced momentum, indicative of energy loss of
the hard scattered parent partons. The fragmentation patterns for both the
leading and subleading jets in PbPb collisions agree with those seen in pp data
at 2.76 TeV. The results provide evidence that, despite the large parton energy
loss observed in PbPb collisions, the partition of the remaining momentum
within the jet cone into high-pt particles is not strongly modified in
comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
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The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Role of Novelty Seeking Personality Traits as Mediator of the Association between COMT and Onset Age of Drug Use in Chinese Heroin Dependent Patients
- Author
- A Heck
- AJ Saxon
- AM Lindenberg
- B Schmid
- BT Conner
- C Guindalin
- CH Ko
- CR Cloninger
- CR Cloninger
- CR Cloninger
- CR Cloninger
- D Hien
- DH Han
- DJ Vandenbergh
- Dongxiang Wang
- ED Gunnarsdottir
- G Parker
- G Suzuki
- Haifeng Jiang
- Hanhui Chen
- HW Gordon
- J Chen
- J Silberg
- JB Becker
- JC Anthony
- JC Barrett
- JH Lai
- Jiang Du
- JL Castroman
- Ke Xu
- Kim D. Janda
- KS Kendler
- L Hosak
- LA Ray
- LP Cao
- M Laucht
- M Laucht
- M Whitty
- Min Zhao
- MJ Thomas
- ML Freedman
- MS Najafabadi
- P Basiaux
- PC Griesler
- PE Shrout
- PW Kalivas
- R Hashimoto
- R Horowitz
- R Tikkanen
- RE Tarter
- S Barnow
- S Dawe
- S Purcell
- SA Gruber
- Shunying Yu
- SJ Tsai
- SY Hill
- TA Wills
- Ting Li
- VE Golimbet
- XX Chen
- YC Chuan
- Yingmei Fu
- Z Ronai
- Publication venue
- Public Library of Science
- Publication date
- 17/08/2011
- Field of study
Personality traits such as novelty seeking (NS) are associated with substance dependence but the mechanism underlying this association remains uncertain. Previous studies have focused on the role of the dopamine pathway.Examine the relationships between allelic variants of the catechol-O-methyltransferase (COMT) gene, NS personality traits, and age of onset of drug use in heroin-dependent subjects in China.The 478 heroin dependent subjects from four drug rehabilitation centers in Shanghai who were genotyped for eight tagging single nucleotide polymorphisms (SNP) on the COMT gene completed the NS subscale from the Temperament and Character Inventory. Multivariate analyses were used to assess the potential mediating role of NS personality traits in the association between COMT gene variants and the age of onset of heroin use.In the univariate analysis the COMT rs737866 gene variants were independently associated with both NS and age of onset of drug use: those with the TT genotype had higher NS subscale scores and an earlier onset age of heroin use than individuals with CT or CC genotypes. In the multivariate analysis the inclusion of the NS subscore variable weakened the relationship between the COMT rs737866 TT genotype and an earlier age of onset of drug use. Our findings that COMT is associated with both NS personality traits and with the age of onset of heroin use helps to clarify the complex relationship between genetic and psychological factors in the development of substance abuse
Precise determination of the mass of the Higgs boson and tests of compatibility of its couplings with the standard model predictions using proton collisions at 7 and 8 TeV
- Author
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- Saxena P
- Scarborough T
- Schael S
- Schettler H
- Schizzi A
- Schleper P
- Schlieckau E
- Schmidt A
- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoerner-Sadenius T
- Schröder M
- Schulte JF
- Schwick C
- Schäfer C
- Schöfbeck R
- Scodellaro L
- Seez C
- Seidel M
- Seif El Nasr-Storey S
- Seitz C
- Seixas J
- Sekaric J
- Sekmen S
- Selvaggi G
- Selvaggi M
- Semenov S
- Sen S
- Senkin S
- Serban AT
- Seva T
- Sexton-Kennedy E
- Sgandurra L
- Sguazzoni G
- Shalhout S
- Sharan M
- Sharma A
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- Sharma V
- Sharp P
- Shchutska L
- Sheffield D
- Sheldon P
- Shepherd-Themistocleous CH
- Shi X
- Shipsey I
- Shmatov S
- Shoaib M
- Shrinivas A
- Shukla P
- Shumeiko N
- Siegrist P
- Sigamani M
- Sikler F
- Silkworth C
- Silva P
- Silvers D
- Silvestris L
- Simon M
- Simon S
- Simonetto F
- Simonis HJ
- Singh G
- Singh JB
- Singovsky A
- Sinthuprasith T
- Sirois Y
- Siroli GP
- Sirunyan AM
- Skatchkov N
- Skhirtladze N
- Skinnari L
- Skovpen K
- Skuja A
- Smirnov I
- Smirnov V
- Smith G
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- Smith VJ
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- Snow GR
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- Sola V
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- Sonnenschein L
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- Sorokin P
- Spagnolo P
- Spalding WJ
- Spanier S
- Spannagel S
- Speer T
- Sperka D
- Sphicas P
- Spiegel L
- Spiezia A
- Spiga D
- Spiridonov A
- Spiropulu M
- Squillacioti P
- Squires M
- Srimanobhas N
- St John J
- Stadie H
- Stahl A
- Staiano A
- Starodumov A
- Steggemann J
- Steinbrück G
- Stenson K
- Stephans GS
- Stickland D
- Stieger B
- Stiliaris E
- Stober FM
- Stolin V
- Stolp D
- Stone R
- Stoye M
- Stoykova S
- Stoynev S
- Strauss J
- Stringer R
- Strobbe N
- Strologas J
- Strom D
- Stuart D
- Stupak J
- Sturdy J
- Suarez Gonzalez J
- Suarez I
- Sudhakar K
- Sudic L
- Sulak L
- Sulimov V
- Sultanov G
- Sumorok K
- Sumowidagdo S
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- Sunar Cerci D
- Sung K
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- Suwonjandee N
- Svintradze I
- Svyatkovskiy A
- Swain SK
- Swanson J
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- Symonds P
- Szillasi Z
- Szleper M
- Sznajder A
- Tabarelli de Fatis T
- Tadel M
- Takahashi M
- Takahashi Y
- Takasugi E
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- Talvitie J
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- Tatarinov A
- Tavernier S
- Taylor D
- Taylor L
- Teles PR
- Tenchini R
- Teo WD
- Teodorescu L
- Teyssier D
- Thea A
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- Thom J
- Thomas L
- Thomas S
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- Thyssen F
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- Tiko A
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- Tonelli Manganote EJ
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- Topsis-Giotis I
- Torassa E
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- Traczyk P
- Tran NV
- Travaglini R
- Treberer-Treberspurg W
- Treille D
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Tropiano A
- Troshin S
- Tsai JF
- Tsamalaidze Z
- Tsirou A
- Tu Y
- Tucker J
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Tuovinen E
- Turkewitz J
- Turner M
- Turner P
- Tuuva T
- Tuve C
- Tytgat M
- Tyurin N
- Tzeng YM
- Tziaferi E
- Ujvari B
- Ulmer KA
- Ulrich R
- Umer T
- Uplegger L
- Usai E
- Uvarov L
- Uzunian A
- Vaandering EW
- Valls N
- Valuev V
- Van De Klundert M
- Van Doninck W
- Van Haevermaet H
- Van Hove P
- Van Mechelen P
- Van Mulders P
- Van Onsem GP
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- Van Spilbeeck A
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- Vander Velde C
- Vanelderen L
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- Vanlaer P
- Vardarlı FI
- Varela J
- Varelas N
- Vargas Trevino AD
- Vartak A
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- Vazquez Valencia F
- Veelken C
- Veeraraghavan V
- Velasco M
- Velicanu D
- Velkovska J
- Venditti R
- Venturi A
- Verdier P
- Verdini PG
- Veres GI
- Vergili M
- Vernieri C
- Verwilligen P
- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vidal Marono M
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Vilela Pereira A
- Villella I
- Vinogradov A
- Virdee T
- Viret S
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- Vishnevskiy D
- Vitulo P
- Vizan Garcia JM
- Vlasov E
- Vlimant R
- Vogel H
- Volkov A
- Volobouev I
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
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- Vuosalo C
- Vutova M
- Wagner SR
- Wagner-Kuhr J
- Walker M
- Wallny R
- Walsh R
- Waltenberger W
- Wan Abdullah WA
- Wang D
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- Wang RJ
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- Wardle N
- Wayand S
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- Weber HA
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- Weiler T
- Weinberg M
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- Werner JS
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- Wetzel J
- Whitbeck A
- Whitmore J
- Wickramage N
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- Wilkinson R
- Williams T
- Wimpenny S
- Winer BL
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
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- Wolf R
- Wolfe E
- Wolfe H
- Wollny H
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Woodard A
- Woods N
- Worm SD
- Wright D
- Wu Z
- Wulsin HW
- Wulz CE
- Wyslouch B
- Wöhri HK
- Würthwein F
- Xiao H
- Xiao M
- Xie S
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- Yagil A
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- Yi K
- Yilmaz Y
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- Zabi A
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- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zeinali M
- Zenoni F
- Zenz SC
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- Zevi Della Porta G
- Zeyrek M
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- Zhang J
- Zhang L
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- Zhu RY
- Zhukov V
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- Zorbilmez C
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- Zsigmond AJ
- Zucchetta A
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- Publication venue
- Publication date
- 01/01/2014
- Field of study
Peer reviewe
- …