2,045 research outputs found
Production of the top-pions at the THERA collider based Îłp collisions
- Author
- Publication venue
- 'Elsevier BV'
- Publication date
- 14/09/2003
- Field of study
In the framework of the topcolor-assisted technicolor (TC2) models, we study
the production of the top-pions Ït0â, Ït±â via the
processes epâÎłcâÏt0âc and epâÎłcâÏt±âb
mediated by the anomalous top coupling tcÎł. We find that the production
cross section of the process epâÎłcâÏt0âc is very small. With
reasonable values of the parameters in TC2 models, the production cross section
of the process epâÎłcâÏt±âb can reach 1.2pb. The charged
top-pions Ït±â might be directly observed via this process at the
THERA collider based Îłp collisions.Comment: 10 pages, 3 figure
P-wave excited baryons from pion- and photo-induced hyperon production
- Author
- A. Anisovich
- A. Bock
- A. de la Puente
- A. Lleres
- A. Lleres
- A. Sibirtsev
- A. Sibirtsev
- A. Sibirtsev
- A. Usov
- A. Usov
- A. V. Anisovich
- A. V. Sarantsev
- A.a. Belyaev
- A.A. Belyaev
- A.A. Belyaev
- A.S. Bratashevsky
- A.S. Bratashevsky
- A.V. Anisovich
- A.V. Anisovich
- A.V. Anisovich
- A.V. Anisovich
- A.V. Sarantsev
- A.V. Sarantsev
- A.Y. Korchin
- B. Borasoy
- B. Bouquet
- B. Julia-Diaz
- B. Julia-Diaz
- B. Julia-Diaz
- B. Krusche
- C. Amsler
- C. Betourne
- C. Weinheimer
- CB-ELSA Collaboration (V. Crede)
- CLAS Collaboration (M. Williams)
- D. Drechsel
- D.H. Saxon
- D.J. Candlin
- D.J. Candlin
- D.M. Manley
- E. Gutz
- E. Klempt
- E. Klempt
- F. Huang
- F.K. Guo
- F.V. Adamian
- G. Barbiellini
- G. Blanpied
- G. Blanpied
- G. Höhler
- G. Knies
- G. Penner
- G. Penner
- G.Y. Chen
- G.Y. Chen
- H. Dutz
- H. Forkel
- H. Genzel
- H. Haberzettl
- H. Herr
- H. van Pee
- H.R. Crouch
- H.W. Dannhausen
- I. Arai
- I. Horn
- I. Horn
- I.G. Alekseev
- I.G. Alekseev
- I.G. Alekseev
- I.G. Alekseev
- I.G. Aznauryan
- J. Ahrens
- J. Ahrens
- J. Ahrens
- J. Ahrens
- J. Ahrens
- J. Ajaka
- J. Ajaka
- J. Alspector
- J. Bocquet
- J. Durand
- J. He
- J.C. David
- J.C. Hart
- J.W.C. McNabb
- K. Buechler
- K. Egawa
- K. Ekstrand
- K. Fujii
- K. Nakayama
- K.H. Althoff
- K.H. Althoff
- K.H. Althoff
- K.H. Althoff
- K.H. Althoff
- K.H. Glander
- K.S. Agababian
- K.W. Bell
- L. Tiator
- M. Batinic
- M. Doring
- M. Doring
- M. Doring
- M. Dugger
- M. Dugger
- M. Fuchs
- M. Fukushima
- M. Fukushima
- M.E. McCracken
- M.M. Asaturian
- N. Kaiser
- N. Sparks
- N. Suzuki
- N.C. Debenham
- O. Bartalini
- O. Bartalini
- O. Bartholomy
- O. Bartholomy
- O. Krehl
- O. Scholten
- P. Feller
- P. Feller
- P. Vancraeyveld
- P.J. Bussey
- P.J. Bussey
- P.J. Bussey
- P.J. Bussey
- P.S.L. Booth
- R. Arndt
- R. Beck
- R. Beck
- R. Bradford
- R. Bradford
- R. Castelijns
- R. Lawall
- R. Shyam
- R. Shyam
- R. Workman
- R.A. Arndt
- R.A. Arndt
- R.A. Arndt
- R.A. Arndt
- R.A. Arndt
- R.A. Williams
- R.C. Smith
- R.D. Baker
- R.E. Taylor
- R.G.T. Zegers
- R.L. Workman
- R.M. Brown
- R.O. Avakyan
- S. Arai
- S. Ceci
- S. Ceci
- S. Ceci
- S. Janssen
- S. Kato
- S. Prakhov
- S. Prakhov
- S.D. Ecklund
- S.J. Brodsky
- S.N. Yang
- S.S. Kamalov
- S.S. Kamalov
- T. Corthals
- T. Corthals
- T. Feuster
- T. Feuster
- T. Feuster
- T. Fujii
- T. Fujii
- T. Mart
- T.M. Knasel
- T.P. Vrana
- T.S.H. Lee
- U. Thoma
- U. Thoma
- V. A. Nikonov
- V. Crede
- V. Shklyar
- V. Shklyar
- V. Shklyar
- V. Shklyar
- V.A. Getman
- V.A. Getman
- V.A. Nikonov
- V.B. Ganenko
- V.G. Gorbenko
- V.G. Gorbenko
- V.G. Gorbenko
- V.G. Gorbenko
- W. Deinet
- W.B. Richards
- W.T. Chiang
- Y. Assafiri
- Y.I. Azimov
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 28/10/2010
- Field of study
We report evidence for N(1710)P11â, N(1875)P11â, N(1900)P13â,
Î(1600)P33â, Î(1910)P31â, and Î(1920)P33â, and find
indications that N(1900)P13â might have a companion state at 1970\,MeV. The
controversial Î(1750)P31â is not seen. The evidence is derived from a
study of data on pion- and photo-induced hyperon production, but other data are
included as well. Most of the resonances reported here were found in the
Karlsruhe-Helsinki (KH84) and the Carnegie-Mellon (CM) analyses but were
challenged recently by the Data Analysis Center at GWU. Our analysis is
constrained by the energy independent ÏN scattering amplitudes from either
KH84 or GWU. The two ÏN amplitudes from KH84 or GWU, respectively, lead to
slightly different ÏN branching ratios of contributing resonances but the
debated resonances are required in both series of fits.Comment: 22 pages, 28 figures. Some additional sets of data are adde
Analysis of recent eta photoproduction data
- Author
- A. Sibirtsev
- A. Sibirtsev
- A. Sibirtsev
- A. Sibirtsev
- A. Sibirtsev
- A. Sibirtsev
- A. Sibirtsev
- A.C. Irving
- A.V. Sarantsev
- B.H. Kellett
- F. Henyey
- F. Huang
- H. Primakoff
- I. Jaegle
- J. Dewire
- J. Haidenbauer
- J. He
- J.N.J. White
- J.N.J. White
- J.R. Bergervoet
- M. Batinic
- M. Dugger
- M. Guidal
- M. Rahnama
- M. Vanderhaeghen
- M. Williams
- P. BydzovskĂœ
- P.J. Bussey
- P.J. Bussey
- Particle Data Group (C. Amsler)
- R. Koch
- R. Timmermans
- R.A. Adelseck
- R.A. Arndt
- R.A. Arndt
- R.E. Cutkosky
- R.L. Anderson
- S. Ceci
- S. Krewald
- T.P. Vrana
- U. -G. MeiĂner
- V. Crede
- V. Crede
- W. Braunschweig
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2010
- Field of study
Recent data on eta-meson photoproduction off a proton target in the energy
range 2 < sqrt{s} < 3 GeV are analyzed with regard to their overall
consistency. Results from the ELSA and CLAS measurements are compared with
predictions of a Regge model whose reaction amplitude was fixed via a global
fit to pre-2000 measurements of differential cross sections and polarization
observables for gamma p -> eta p at higher energies. We find that all recent
experimental results on differential cross sections for eta-meson
photoproduction are in good agreement with each other, except for the CLAS data
from 2009. However, the latter can be made consistent with the other data at
the expense of introducing an energy-dependent renormalization factor. We point
out that there indications in the data for a possible excitation of baryon
resonances with masses around 2.1 and 2.4 GeV.Comment: 13 pages, 13 figures; small modifications in the text, some figures
are improved, accepted for publication by Eur. Phys. J.
Neutral top-pion and tÎł(z) production at the HERA and THERA colliders
- Author
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2004
- Field of study
In the context of top-color assisted technicolor (TC2) models, we calculate
the contributions of the neutral top-pion Ït0â to tÎł and tz
production via the processes epâÎłcâtÎł and epâÎłcâtz at the HERA and THERA colliders. Our results show that the cross
sections ÏtÎłâ(s) and Ïtzâ(s) are very small at the
HERA collider with sâ=320GeV. However, in most of the parameter
space, ÏtÎłâ(s) or Ïtzâ(s) is in the range of about
0.1pbâŒ1pb at the THERA collider with sâ=1000GeV.Comment: 10 pages, typos corrected, version accepted for publication in Phys.
Lett.
The NEWMEDS rodent touchscreen test battery for cognition relevant to schizophrenia.
- Author
- A Aleman
- A Bari
- A Giersch
- A Giersch
- A Izquierdo
- A Laurent
- A Markou
- A Prouteau
- A Prouteau
- A Yılmaz
- A. C. Mar
- AA Harrison
- AC Mar
- AC Mar
- AC Mar
- AC Roberts
- AD Huberman
- AE Horner
- AE Simon
- AF Mirsky
- AM Owen
- AM Owen
- B Cornblatt
- B Gamallo-Lana
- B Kolisnyk
- B Kolisnyk
- B Lee
- B Milner
- BA Cornblatt
- BJ Sahakian
- BJ Sahakian
- C Graybeal
- C Lustig
- C Pantelis
- C Pantelis
- C Romberg
- C Romberg
- C. J. Heath
- CA Oomen
- CA Winstanley
- CD Clelland
- CM Niell
- CS Carter
- D Piskulic
- D Zoccolan
- DC Turner
- DE Gard
- DE Gard
- DF Emerich
- DJ Calderone
- DM Barch
- DM Barch
- DM Barch
- E Hoyle
- E Joyce
- E Stip
- EA Holthausen
- EC Dowd
- EM Joyce
- EM Weiss
- G Aubin
- G Donohoe
- G Kumar
- G Schoenbaum
- GB Bissonette
- GW Wohlberg
- H Eichenbaum
- H Eichenbaum
- H Grunebaum
- H Moore
- HE Rosvold
- HF Clarke
- HF Clarke
- HF Clarke
- J Kim
- J McGaughy
- J Nithianantharajah
- J OâDoherty
- J Rutschmann
- J See
- J. Alsiö
- JA Parkinson
- JA Parkinson
- JA Siegel
- JA Weiler
- JC Badcock
- JC Crabbe
- JC Talpos
- JC Talpos
- JC Talpos
- JD Jentsch
- JE Belforte
- JF Keeler
- JH Barnett
- JH Barnett
- JJ Downes
- JK Leutgeb
- JL Brigman
- JL Silverman
- JM Birrell
- JM Gold
- JM Gold
- JN Crawley
- JS Simons
- JW Dalley
- JW Young
- JW Young
- K McAlonan
- KA Burke
- KA Feigenson
- KA McAllister
- KC Ward
- KH Nuechterlein
- KH Nuechterlein
- KH Nuechterlein
- KR Griffiths
- L DePoy
- L Erlenmeyer-Kimling
- L Scoriels
- L. M. Saksida
- M Hvoslef-Eide
- M Lei
- M Levaux
- M OâNeill
- M. Hvoslef-Eide
- MB Knable
- MF Green
- MF Green
- MF Green
- MP Coba
- MS Ritsner
- N Estapé
- NF Forbes
- P Bekinschtein
- P Franke
- PA Dudchenko
- PD Butler
- PE Dickson
- PE Gilbert
- PJ Harrison
- R Elliott
- R Ito
- R OâCarroll
- R Parasuraman
- RF Asarnow
- RL Barlow
- RL McLamb
- RS Keefe
- S Chouinard
- S Ghods-Sharifi
- S Park
- S. R. O. Nilsson
- SB Hutton
- SE Winder-Rhodes
- SJ Bartko
- SJ Bartko
- SJ Luck
- SJ Wood
- SM Groman
- SM McTighe
- SM Silverstein
- SP Baron
- SR Marder
- T Bahri
- T Das
- T Nakashiba
- T. J. Bussey
- T. W. Robbins
- TA Stalnaker
- TJ Bussey
- TJ Bussey
- TJ Bussey
- TJ Bussey
- TJ Bussey
- TJ Bussey
- TJ Bussey
- TJ Walsh
- TR Insel
- TW Robbins
- TW Robbins
- U Muller
- V Boulougouris
- V Boulougouris
- V Voon
- VC Leeson
- XM Gao
- Y Chudasama
- Y Chudasama
- Y Chudasama
- Y Worbe
- Z Kasanova
- Publication venue
- Psychopharmacology (Berl)
- Publication date
- 24/07/2015
- Field of study
RATIONALE: The NEWMEDS initiative (Novel Methods leading to New Medications in Depression and Schizophrenia, http://www.newmeds-europe.com ) is a large industrial-academic collaborative project aimed at developing new methods for drug discovery for schizophrenia. As part of this project, Work package 2 (WP02) has developed and validated a comprehensive battery of novel touchscreen tasks for rats and mice for assessing cognitive domains relevant to schizophrenia. OBJECTIVES: This article provides a review of the touchscreen battery of tasks for rats and mice for assessing cognitive domains relevant to schizophrenia and highlights validation data presented in several primary articles in this issue and elsewhere. METHODS: The battery consists of the five-choice serial reaction time task and a novel rodent continuous performance task for measuring attention, a three-stimulus visual reversal and the serial visual reversal task for measuring cognitive flexibility, novel non-matching to sample-based tasks for measuring spatial working memory and paired-associates learning for measuring long-term memory. RESULTS: The rodent (i.e. both rats and mice) touchscreen operant chamber and battery has high translational value across species due to its emphasis on construct as well as face validity. In addition, it offers cognitive profiling of models of diseases with cognitive symptoms (not limited to schizophrenia) through a battery approach, whereby multiple cognitive constructs can be measured using the same apparatus, enabling comparisons of performance across tasks. CONCLUSION: This battery of tests constitutes an extensive tool package for both model characterisation and pre-clinical drug discovery.This work was supported by the Innovative Medicine Initiative Joint Undertaking under grant agreement no. 115008 of which resources are composed of EFPIA in-kind contribution and financial contribution from the European Unionâs Seventh Framework Programme (FP7/2007-2013). The authors thank Charlotte Oomen for valuable comments on the manuscript.This is the author accepted manuscript. The final version is available from Springer via http://dx.doi.org/10.1007/s00213-015-4007-
Angular and Current-Target Correlations in Deep Inelastic Scattering at HERA
- Author
- Abbiendi G
- Abe T
- Abramowicz H
- Acosta D
- Adamczyk L
- Adamus M
- Ahn Sh
- Amelung C
- An Sh
- Anselmo F
- Antonioli P
- Arneodo M
- Bacon Tc
- Badgett Wf
- Bailey Dc
- Bailey Ds
- Bamberger A
- Barbagli G
- Bari G
- Barreiro F
- Barret O
- Bashindzhagyan Gl
- Bashkirov V
- Basile M
- Bauerdick Lat
- Bednarek B
- Behrens U
- Bellagamba L
- Bertolin A
- Bhadra S
- Bienlein Jk
- Blaikley He
- Bohnet I
- Bokel C
- Boogert S
- Bornheim A
- Borzemski P
- Boscherini D
- Botje M
- Breitweg J
- Brock I
- Brook Nh
- Brugnera Riccardo
- Brummer N
- Bruni A
- Bruni G
- Burgard C
- Burow Bd
- Bussey Pj
- Butterworth Jm
- Bylsma B
- CA ZEUS Collaboration
- Caldwell A
- Capua M
- Carlin Roberto
- Cartiglia N
- Cashmore Rj
- Castellini G
- Catterall Cd
- Chapin D
- Chekanov S
- Chwastowski J
- Ciborowski J
- Cifarelli L
- Cindolo F
- Cirio R
- Cloth P
- Coboken K
- Coldewey C
- Cole Je
- Contin A
- COOPER SARKAR Am
- Coppola N
- Cormack C
- Corradi M
- Corriveau F
- Costa M
- Cottingham Wn
- Crittenden J
- Cross R
- D'Agostini G
- Dagan S
- DAL CORSO F
- Dardo M
- DE PASQUALE S
- DE WOLF E
- Deffner R
- DEL PESO J
- Deppe O
- Derrick M
- Deshpande A
- Desler K
- Devenish Rce
- Dhawan S
- Dolgoshein Ba
- Dondana S
- Dosselli U
- Doyle At
- Drews G
- Dulinski Z
- Durkin Ls
- Dusini S
- Eckert M
- Edmonds Jk
- Eisenberg Y
- Eisenhardt S
- Engelen J
- Epperson D
- Ermolov Pf
- Eskreys A
- Fagerstroem Cp
- Fernandez Jp
- Ferrero Mi
- Figiel J
- Filges D
- Foster B
- Foudas C
- FOX MURPHY A
- Fricke U
- Frisken Wr
- Fusayasu T
- Gadaj T
- Galea R
- Gallo E
- Garcia G
- Garcia Yz
- Garfagnini Alberto
- Gendner N
- Gialas I
- Gilmore J
- Ginsburg Cm
- Giusti P
- Gladilin Lk
- Glasman C
- Goebel F
- Golubkov Ya
- Gottlicher P
- Grabosch Hj
- Graciani R
- GROSSE KNETTER J
- Grzelak G
- Haas T
- Hain W
- HALL WILTON R
- Hamatsu R
- Hanna Ds
- Harnew N
- Hart Jc
- Hartmann H
- Hartmann J
- Hartner Gf
- Hasell D
- Hayes Me
- Heapby Ea
- Heath Gp
- Heath Hf
- Hebbel K
- Heinloth K
- Heinz L
- Hernandez Jm
- Heusch C
- Hilger E
- Hirose T
- Hochman D
- Holm U
- Homma K
- Hong Sj
- Howell G
- Hughes Vw
- Iacobucci G
- Iannotti L
- Iga Y
- Inuzuka M
- Ishii T
- Jakob Hp
- Jelen K
- Jeoung Hy
- Jing Z
- Johnson Kf
- Jones Tw
- Kananov S
- Kappes A
- Karshon U
- Kasemann M
- Katz Uf
- Kcira D
- Kerger R
- Khakzad M
- Khein La
- Kim Cl
- Kim Jy
- Kisielewska D
- Kitamura S
- Klanner R
- Klimek K
- Koch W
- Koffeman E
- Kooijman P
- Koop T
- Korotkova Na
- Korzhavina Ia
- Kotanski A
- Kotz U
- Kowal Am
- Kowalski H
- Kowalski T
- Krakauer D
- Kreisel A
- Kuze M
- Kuzmin Va
- Labarga L
- Lamberti L
- Lane Jb
- Laurenti G
- Lee Jh
- Lee Sb
- Lee Sw
- Levi G
- Levman Gm
- Levy A
- Lim H
- Lim It
- Limentani S
- Lindemann L
- Ling Ty
- Liu W
- Lohr B
- Lohrmann E
- Long Kr
- Lukina Oy
- Ma Kj
- Maccarrone G
- Macdonald N
- Magill S
- Mallik U
- Margotti A
- Marini G
- Markun P
- Martin Jf
- Martinez M
- Maselli S
- Massam T
- Mastroberardino A
- Matsushita T
- Mattingly Mck
- Mattingly S
- Mccance Gj
- Mccubbin Na
- Mcfall Jd
- Mellado B
- Menary S
- MEYER LARSEN A
- Meyer A
- Milewski J
- Milite M
- Miller Db
- Monaco V
- Monig K
- Monteiro T
- Morandin M
- Moritz M
- Murray Wn
- Musgrave B
- Nagano K
- Nam Sw
- Nania R
- Nigro A
- Nishimura T
- Notz D
- Nowak Rj
- Noyes Va
- Nylander P
- Ochs A
- Oh By
- Okrasinski Jr
- Olkiewicz K
- Orr Rs
- Pac My
- Padhi S
- Palmonari F
- Park Ih
- Park Sk
- Parsons Ja
- Paul E
- Pavel N
- Pawlak Jm
- Pawlak R
- Pelfer P
- Pellegrino A
- Pelucchi F
- Peroni C
- Pesci A
- Petrucci Mc
- Pfeiffer M
- Piccioni D
- Piotrzkoswski K
- Poelz G
- Polenz S
- Polini A
- Posocco M
- Prinias A
- Proskuryakov As
- Przybycien M
- Przybycien Mb
- Puga J
- Quadt A
- Raach H
- Raso M
- Rautenberg J
- Redondo I
- Reeder Dd
- Repond J
- Ritz S
- Riveline M
- Rohde M
- Romeo Gc
- RULIKOWSKA ZAREBSKA E
- Ruske O
- Ruspa M
- Sabetfakhri A
- Sacchi R
- Sadrozinski Hfw
- Salehi H
- Sampson S
- Sartorelli G
- Saull Prb
- Savin Aa
- Saxon Dh
- Schechter A
- Schioppa M
- Schlenstedt S
- Schmidke Wb
- Schneekloth U
- Schnurbusch H
- Schwarzer O
- Sciulli F
- Scott J
- Sedgbeer Jk
- Seiden A
- Selonke F
- Shah Tp
- Shcheglova Lm
- Sideris D
- Sievers M
- Simmons D
- Sinclair Le
- Skillicorn Io
- Smalska B
- Smith Wh
- Solano A
- Solomin An
- Son D
- ST LAURENT M
- Staiano A
- Stairs Dg
- Stanco L
- Stanek R
- Stifutkin A
- Stonjek S
- Straub Pb
- Strickland E
- Stroili Roberto
- Susinno G
- Suszycki L
- Sutton Mr
- Suzuki I
- Tandler J
- Tapper Ad
- Tapper Rj
- Tassi E
- Terron J
- Tiecke W
- Tokushuku K
- Toothacker Ws
- Tsurugai T
- Tuning N
- Tymieniecka T
- Umemori K
- Vaiciulis A
- VAN SIGHEM A
- Velthuis Jj
- Verkerke W
- Viani Ald
- Voci C
- Vossebeld J
- Votano L
- Walczak R
- Walker R
- Wang Sm
- Waters Ds
- Waugh R
- Weber A
- Whitmore Jj
- Wichmann R
- Wick K
- Wieber H
- Wiggers L
- Wildschek T
- Williams Dc
- Wing M
- Wodarczyk M
- Wolf G
- Wolfle S
- Wollmer U
- Wroblewski Ak
- Yamada S
- Yamashita T
- Yamauchi K
- Yamazaki Y
- Yoshida R
- Youngman C
- Zajac J
- Zakrzewski Ja
- Zarnecki Af
- Zawiejski L
- Zetsche F
- Zeuner W
- Zhu Q
- Zichichi A
- Zotkin Sa
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1999
- Field of study
Correlations between charged particles in deep inelastic ep scattering have
been studied in the Breit frame with the ZEUS detector at HERA using an
integrated luminosity of 6.4 pb-1. Short-range correlations are analysed in
terms of the angular separation between current-region particles within a cone
centred around the virtual photon axis. Long-range correlations between the
current and target regions have also been measured. The data support
predictions for the scaling behaviour of the angular correlations at high Q2
and for anti-correlations between the current and target regions over a large
range in Q2 and in the Bjorken scaling variable x. Analytic QCD calculations
and Monte Carlo models correctly describe the trends of the data at high Q2,
but show quantitative discrepancies. The data show differences between the
correlations in deep inelastic scattering and e+e- annihilation.Comment: 26 pages including 10 figures (submitted to Eur. J. Phys. C
Plastisol Foaming Process. Decomposition of the Foaming Agent, Polymer Behavior in the Corresponding Temperature Range and Resulting Foam Properties
- Author
- Abbiendi G
- Abe T
- Abramowicz H
- Acosta D
- Adamczyk L
- Adamus M
- Amelung C
- Anselmo F
- Antonioli P
- Arneodo M
- Ayad R
- Bacon TC
- Badgett WF
- Bailey DC
- Bailey DS
- Bamberger A
- Barbagli G
- Bari G
- Barreiro F
- Bashindzhagyan GL
- Bashkirov V
- Basile M
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- Westphal D
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- Zarnecki AF
- Zawiejski L
- Zetsche F
- Zeuner W
- Zhang H
- Zhu Q
- Zichichi A
- Zotkin SA
- Publication venue
- WILEY
- Publication date
- 01/01/1998
- Field of study
The decomposition of azodicarbonamide, used as foaming agent in PVC - plasticizer (1/1) plastisols was studied by DSC. Nineteen different plasticizers, all belonging to the ester family, two being polymeric (polyadipates), were compared. The temperature of maximum decomposition rate (in anisothermal regime at 5 K min-1 scanning rate), ranges between 434 and 452 K. The heat of decomposition ranges between 8.7 and 12.5 J g -1. Some trends of variation of these parameters appear significant and are discussed in terms of solvent (matrix) and viscosity effects on the decomposition reactions. The shear modulus at 1 Hz frequency was determined at the temperature of maximum rate of foaming agent decomposition, and differs significantly from a sample to another. The foam density was determined at ambient temperature and the volume fraction of bubbles was used as criterion to judge the efficiency of the foaming process. The results reveal the existence of an optimal shear modulus of the order of 2 kPa that corresponds roughly to plasticizer molar masses of the order of 450 ± 50 g mol-1. Heavier plasticizers, especially polymeric ones are too difficult to deform. Lighter plasticizers such as diethyl phthalate (DEP) deform too easily and presumably facilitate bubble collapse
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
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- Yilmaz M
- Yoosootiniya R
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- Zhemchugov A
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- Zitoun R
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- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anderson KJ
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- Zenin O
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- Zerwas D
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- Zhang D
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- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
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- Zhu CG
- Zhu H
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zilka B
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Jet size dependence of single jet suppression in lead-lead collisions at sqrt(s(NN)) = 2.76 TeV with the ATLAS detector at the LHC
- Author
- A. Ahmad
- A. Aloisio
- A. Alonso
- A. Amorim
- A. Andreazza
- A. Angerami
- A. Anisenkov
- A. Annovi
- A. Antonaki
- A. Antonov
- A. Artamonov
- A. Astbury
- A. Bangert
- A. Barbaro Galtieri
- A. Baroncelli
- A. Battaglia
- A. Beddall
- A. Belloni
- A. Bertin
- A. Bingul
- A. Blondel
- A. Bocci
- A. Bogdanchikov
- A. Bogouch
- A. Borisov
- A. Boveia
- A. Brandt
- A. Bruni
- A. Canepa
- A. Catinaccio
- A. Cattai
- A. Cerri
- A. Chafaq
- A. Cheplakov
- A. Chilingarov
- A. Chitan
- A. Christov
- A. Ciocio
- A. Clark
- A. Coccaro
- A. Cortes-Gonzalez
- A. Dafinca
- A. De Salvo
- A. De Santo
- A. DellÊŒAcqua
- A. Dewhurst
- A. Di Ciaccio
- A. Di Girolamo
- A. Di Mattia
- A. Di Simone
- A. Do Valle Wemans
- A. Doria
- A. Dos Anjos
- A. Dotti
- A. Dudarev
- A. DÊŒOrazio
- A. Engl
- A. Eppig
- A. Ereditato
- A. Farbin
- A. Farilla
- A. Favareto
- A. Ferrari
- A. Ferrer
- A. Ferretto Parodi
- A. FilipÄiÄ
- A. Firan
- A. Floderus
- A. Formica
- A. Forti
- A. Gaponenko
- A. Gemmell
- A. Gershon
- A. Gibson
- A. Glazov
- A. Gomes
- A. GoriĆĄek
- A. Guida
- A. Haas
- A. Hamilton
- A. Harvey
- A. Henrichs
- A. Hoecker
- A. Hoummada
- A. Huettmann
- A. Irles Quiles
- A. Jantsch
- A. Jeremie
- A. Juste Rozas
- A. Kaczmarska
- A. Kapliy
- A. Kastanas
- A. Khanov
- A. Khodinov
- A. Khomich
- A. Khoroshilov
- A. Klier
- A. Klimentov
- A. Knue
- A. Korn
- A. Korol
- A. Kotwal
- A. Koutsman
- A. Krasznahorkay
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- A. Kugel
- A. Kupco
- A. La Rosa
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- A. Limosani
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- A. Lister
- A. Lleres
- A. Loginov
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- A. Lucotte
- A. Ludwig
- A. Macchiolo
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- A. Meade
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- A. Mengarelli
- A. Messina
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- A. Moraes
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- A. Napier
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- A. Nelson
- A. Neusiedl
- A. Nikiforov
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- A. Onofre
- A. Ouraou
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- S.E. Allwood-Spiers
- S.F. Brazzale
- S.H. Kim
- S.H. Oh
- S.H. Robertson
- S.I. Buda
- S.J. Haywood
- S.J. Head
- S.J. Hillier
- S.J. Maxfield
- S.J. McMahon
- S.J. Sekula
- S.J. Wheeler-Ellis
- S.J. Wollstadt
- S.L. Cheung
- S.L. Lloyd
- S.L. Wu
- S.M. Consonni
- S.M. Farrington
- S.M. Gibson
- S.M. Piec
- S.M. Wang
- S.O. Holmgren
- S.P. Ahlen
- S.P. Baranov
- S.P. Bieniek
- S.P. Denisov
- S.P. Mc Kee
- S.R. Whitehead
- S.S. Bocchetta
- S.S.A. Livermore
- S.T. French
- S.V. Chekulaev
- S.V. Mouraviev
- S.V. Peleganchuk
- S.W. OÊŒNeale
- S.W. Snow
- S.Yu. Sivoklokov
- S.Yu. Smirnov
- Sjostrand
- Sw. Banerjee
- T. Adye
- T. Akdogan
- T. Alexopoulos
- T. Andeen
- T. Bain
- T. Barber
- T. Barillari
- T. Barklow
- T. Beau
- T. Berry
- T. Blazek
- T. Bold
- T. Brooks
- T. Buanes
- T. Buran
- T. Burgess
- T. Carli
- T. Colombo
- T. Cornelissen
- T. Costin
- T. Cuhadar Donszelmann
- T. Dai
- T. Davidek
- T. Del Prete
- T. Delemontex
- T. Djobava
- T. Doherty
- T. Dohmae
- T. Eifert
- T. Ekelof
- T. Farooque
- T. Flick
- T. Fonseca Martin
- T. Frank
- T. Gadfort
- T. Golling
- T. Greenshaw
- T. Göpfert
- T. Harenberg
- T. Haruyama
- T. Hayakawa
- T. Hayashi
- T. HenĂ
- T. Holy
- T. HrynÊŒova
- T. Ince
- T. Jakoubek
- T. Jovin
- T. Kanno
- T. Kawamoto
- T. Kishimoto
- T. Kittelmann
- T. Klioutchnikova
- T. Kluge
- T. Kobayashi
- T. Koffas
- T. Kohriki
- T. Koi
- T. Kondo
- T. Kono
- T. Kruker
- T. Kubota
- T. Kuhl
- T. Lagouri
- T. Lari
- T. LeCompte
- T. Lenz
- T. Loddenkoetter
- T. Lohse
- T. Maeno
- T. Mashimo
- T. Masubuchi
- T. Matsushita
- T. Mclaughlan
- T. Meguro
- T. Moa
- T. Mueller
- T. Nakamura
- T. Nattermann
- T. Naumann
- T. Nobe
- T. Nunnemann
- T. Ohshima
- T. Okuyama
- T. Pauly
- T. Perez Cavalcanti
- T. Poghosyan
- T. Rador
- T. Sandoval
- T. Sarangi
- T. Schwindt
- T. Shin
- T. Slavicek
- T. Spreitzer
- T. Sumida
- T. Sykora
- T. Takeshita
- T. Theveneaux-Pelzer
- T. Tic
- T. Todorov
- T. Trefzger
- T. Varol
- T. Vazquez Schroeder
- T. Vickey
- T. Vu Anh
- T. Wang
- T. Wenaus
- T. Wengler
- T. Yamamura
- T. Yamanaka
- T. Yamazaki
- T. Zhao
- T. ĆœeniĆĄ
- T.A. Dietzsch
- T.A. Martin
- T.A. MĂŒller
- T.B. Huffman
- T.B. Sjursen
- T.C. Meyer
- T.C. Petersen
- T.C. Rave
- T.G. McCarthy
- T.J. Jones
- T.J. Khoo
- T.J. Neep
- T.K. Nelson
- T.K.O. Doan
- T.M. Hong
- T.M. Liss
- T.N. Addy
- T.P.A. Ă kesson
- T.T. Voss
- T.Z. Kowalski
- Th.D. Papadopoulou
- U. Bitenc
- U. Blumenschein
- U. Bratzler
- U. De Sanctis
- U. Gul
- U. Husemann
- U. Klein
- U. Kruchonak
- U. Landgraf
- U. Mallik
- U. Parzefall
- U. Schnoor
- U. SchÀfer
- U. Soldevila
- U.K. Yang
- V. Andrei
- V. Arnal
- V. Bansal
- V. Bartsch
- V. Boisvert
- V. Boldea
- V. Bortolotto
- V. BĂŒscher
- V. Canale
- V. Castillo Gimenez
- V. Cavasinni
- V. Chavda
- V. Chernyatin
- V. Cindro
- V. Consorti
- V. Dao
- V. Ferrara
- V. Gallo
- V. Garonne
- V. Giakoumopoulou
- V. Giangiobbe
- V. Grassi
- V. Gratchev
- V. Hedberg
- V. Ippolito
- V. Izzo
- V. Jain
- V. Juranek
- V. Kartvelishvili
- V. Kaushik
- V. Khovanskiy
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- V. Nikolaenko
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- V.I. Vassilakopoulos
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- V.O. Tikhomirov
- V.P. Lombardo
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- V.V. Kostyukhin
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- V.V. Zmouchko
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- W. Bhimji
- W. Blum
- W. Buttinger
- W. Cleland
- W. Dabrowski
- W. Davey
- W. Ehrenfeld
- W. Fedorko
- W. Fernando
- W. Iwanski
- W. Ji
- W. Kozanecki
- W. Lampl
- W. Lavrijsen
- W. Liebig
- W. Lukas
- W. Mohr
- W. Park
- W. Taylor
- W. Trischuk
- W. Vandelli
- W. Verkerke
- W. Wagner
- W. Walkowiak
- W. Wiedenmann
- W. Willis
- W.B. Quayle
- W.C. Wong
- W.F. Mader
- W.G. Scott
- W.H. Bell
- W.J. Dearnaley
- W.J. Mills
- W.J. Murray
- W.K. Brooks
- W.S. Lockman
- W.T. Meyer
- Wang
- Wang
- X. Chen
- X. Espinal Curull
- X. Ju
- X. Lei
- X. Li
- X. Lou
- X. Portell Bueso
- X. Prudent
- X. Ruan
- X. Sun
- X. Wu
- X. Zhang
- X. Zhuang
- X.S. Anduaga
- Y. Arai
- Y. Azuma
- Y. Bai
- Y. Benhammou
- Y. Chen
- Y. Coadou
- Y. Davygora
- Y. Doi
- Y. Fang
- Y. Hasegawa
- Y. Hernåndez Jiménez
- Y. Ikegami
- Y. Jiang
- Y. Kataoka
- Y. Komori
- Y. Kulchitsky
- Y. Liu
- Y. Makida
- Y. Ming
- Y. Munwes
- Y. Nagasaka
- Y. Nakahama
- Y. Ninomiya
- Y. Okumura
- Y. Oren
- Y. Pylypchenko
- Y. Rozen
- Y. Silver
- Y. Smirnov
- Y. Sugaya
- Y. Suzuki
- Y. Suzuki
- Y. Takahashi
- Y. Takubo
- Y. Tayalati
- Y. Unno
- Y. Wu
- Y. Yamazaki
- Y. Yang
- Y. Yao
- Y. Yasu
- Y. Zhou
- Y. Zhu
- Y.A. Kurochkin
- Y.A. Tikhonov
- Y.B. Pan
- Y.F. Ryabov
- Y.S. Gao
- Y.V. Grishkevich
- Z. Czyczula
- Z. Dolezal
- Z. Gecse
- Z. Hajduk
- Z. Hubacek
- Z. Kohout
- Z. Liang
- Z. Marshall
- Z. Meng
- Z. Rurikova
- Z. Weng
- Z. Yan
- Z. Yang
- Z. Zajacova
- Z. Zhan
- Z. Zhang
- Z. Zhao
- Z. Zinonos
- Z.D. Greenwood
- Z.L. Ren
- Z.V. Krumshteyn
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/12/2012
- Field of study
Measurements of inclusive jet suppression in heavy ion collisions at the LHC
provide direct sensitivity to the physics of jet quenching. In a sample of
lead-lead collisions at sqrt(s) = 2.76 TeV corresponding to an integrated
luminosity of approximately 7 inverse microbarns, ATLAS has measured jets with
a calorimeter over the pseudorapidity interval |eta| < 2.1 and over the
transverse momentum range 38 < pT < 210 GeV. Jets were reconstructed using the
anti-kt algorithm with values for the distance parameter that determines the
nominal jet radius of R = 0.2, 0.3, 0.4 and 0.5. The centrality dependence of
the jet yield is characterized by the jet "central-to-peripheral ratio," Rcp.
Jet production is found to be suppressed by approximately a factor of two in
the 10% most central collisions relative to peripheral collisions. Rcp varies
smoothly with centrality as characterized by the number of participating
nucleons. The observed suppression is only weakly dependent on jet radius and
transverse momentum. These results provide the first direct measurement of
inclusive jet suppression in heavy ion collisions and complement previous
measurements of dijet transverse energy imbalance at the LHC.Comment: 15 pages plus author list (30 pages total), 8 figures, 2 tables,
submitted to Physics Letters B. All figures including auxiliary figures are
available at
http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HION-2011-02
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