579 research outputs found
The Ï(1S,2S), Ï(1S,2S), ΄(1S,2S) and Ïtâ(1S,2S) mesons in a double pole QCD Sum Rule
- Author
- A Martinez Torres
- AP Bakulev
- Bern-Graz-Regensburg Collaboration: T. Burch
- CMS Collaboration: P. Kokkas
- CP-PACS Collaboration: T. Yamazaki
- D Arndt
- D Becirevic
- D Becirevic
- D Ebert
- D Guadagnoli
- D Harnett
- DB Leinweber
- DELPHI Collaboration: J. Abdallah
- ETM Collaboration: K. Jansen
- F-K Guo
- FS Navarra
- JJ Dudek
- JJ Dudek
- JP Singh
- K Ohtani
- LS Kisslinger
- M. S. Maior de Sousa
- MA Shifman
- MA Shifman
- ME Bracco
- N Fabiano
- N Mathur
- O Lakhina
- P Gubler
- P Gubler
- Particle Data Group: J. Beringer
- R. Rodrigues da Silva
- RG Edwards
- RM Albuquerque
- S Godfrey
- S-x Qin
- UKQCD Collaboration: C. McNeile
- VA Novikov
- VA Novikov
- VI Zakharov
- Y Kiyo
- YP Goncharov
- ZG Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 30/09/2016
- Field of study
We use the method of double pole QCD sum rule which is basically a fit with
two exponentials of the correlation function, where we can extract the masses
and decay constants of mesons as a function of the Borel mass. We apply this
method to study the mesons: Ï(1S,2S), Ï(1S,2S), ΄(1S,2S) and
Ïtâ(1S,2S). We also present predictions for the toponiuns masses
Ïtâ(1S,2S) of m(1S)=357 GeV and m(2S)=374 GeV.Comment: 14 pages, 11 figures in Braz J Phys (2016
Radiation from a D-dimensional collision of shock waves: proof of first order formula and angular factorisation at all orders
- Author
- ATLAS collaboration
- ATLAS collaboration
- C Herdeiro
- Carlos Herdeiro
- CMS collaboration
- CMS collaboration
- FG Friedlander
- FlĂĄvio S. Coelho
- FS Coelho
- FS Coelho
- FS Coelho
- FS Coelho
- H Yoshino
- H Yoshino
- I Antoniadis
- JL Albacete
- JL Feng
- K Tanabe
- K Tanabe
- KA Khan
- L Anchordoqui
- L Randall
- L Randall
- L Rezzolla
- L Smarr
- L Ălvarez-GaumĂ©
- Marco O. P. Sampaio
- MOP Sampaio
- N Arkani-Hamed
- PC Aichelburg
- PC Argyres
- PD DâEath
- PD DâEath
- PD DâEath
- PD DâEath
- R Emparan
- S Dimopoulos
- SB Giddings
- U Sperhake
- V Cardoso
- WE East
- Y Nutku
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Dark matter with two inert doublets plus one Higgs doublet
- Author
- A Abramowski
- A Djouadi
- A Djouadi
- A Goudelis
- ATLAS collaboration
- ATLAS collaboration
- B Grzadkowski
- C Arina
- CMS collaboration
- CMS collaboration
- CMS collaboration
- CP Burgess
- D Sokolowska
- Dorota Sokolowska
- DS Akerib
- DS Akerib
- E Aprile
- E Dolle
- E Lundstrom
- E Ma
- EM Dolle
- FS Queiroz
- G Bertone
- G BĂ©langer
- G BĂ©langer
- G BĂ©langer
- G Jungman
- G Servant
- H-C Cheng
- HE Haber
- HP Nilles
- IP Ivanov
- IP Ivanov
- IP Ivanov
- J McDonald
- K Kannike
- L Bergstrom
- L Lopez Honorez
- L Lopez Honorez
- L Lopez Honorez
- M Ackermann
- M Ackermann
- M Cirelli
- M Krawczyk
- MHG Tytgat
- NG Deshpande
- Q-H Cao
- R Barbieri
- Stefano Moretti
- Stephen F. King
- V Keus
- V Keus
- Venus Keus
- X Chu
- Y Mambrini
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Measurement of the running of the QED coupling in small-angle Bhabha scattering at LEP
- Author
- Abbiendi G
- Ainsley C
- Akesson PF
- Alexander G
- Anagnostou G
- Anderson KJ
- Asai S
- Axen D
- Bailey I
- Barberio E
- Barillari T
- Barlow RJ
- Batley RJ
- Bechtle P
- Behnke T
- Bell KW
- Bell PJ
- Bella G
- Bellerive A
- Benelli G
- Bethke S
- Biebel O
- Bock P
- Boeriu O
- Boutemeur M
- Braibant S
- Brown RM
- Burckhart HJ
- Campana S
- Capiluppi P
- Carnegie RK
- Carter AA
- Carter JR
- Chang CY
- Charlton DG
- Ciocca C
- Csilling A
- Cuffiani M
- Dado S
- Dallavalle GM
- De Roeck A
- De Wolf EA
- Desch K
- Dienes B
- Dubbert J
- Duchovni E
- Duckeck G
- Duerdoth IP
- Etzion E
- Fabbri F
- Ferrari P
- Fiedler F
- Fleck I
- Ford M
- Frey A
- Gagnon P
- Gary JW
- Geich-Gimbel C
- Giacomelli G
- Giacomelli P
- Giacomelli R
- Giunta M
- Goldberg J
- Gross E
- Grunhaus J
- Gruwe M
- Gunther PO
- Gupta A
- Hajdu C
- Hamann M
- Hanson GG
- Harel A
- Hauschild M
- Hawkes CM
- Hawkings R
- Hemingway RJ
- Herten G
- Heuer RD
- Hill JC
- Horvath D
- Igo-Kemenes P
- Ishii K
- Jeremie H
- Jovanovic P
- Junk TR
- Kanzaki J
- Karlen D
- Kawagoe K
- Kawamoto T
- Keeler RK
- Kellogg RG
- Kennedy BW
- Kluth S
- Kobayashi T
- Kobel M
- Komamiya S
- Kramer T
- Krieger P
- Kuhl T
- Kupper M
- Lafferty GD
- Landsman H
- Lanske D
- Lellouch D
- Letts J
- Levinson L
- Lillich J
- Lloyd SL
- Loebinger FK
- Lu J
- Ludwig A
- Ludwig J
- Mader W
- Marcellini S
- Martin AJ
- Mashimo T
- Mattig P
- McKenna J
- McPherson RA
- Meijers F
- Menges W
- Merritt FS
- Mes H
- Meyer N
- Michelini A
- Mihara S
- Mikenberg G
- Miller DJ
- Mohr W
- Mori T
- Mutter A
- Nagai K
- Nakamura I
- Nanjo H
- Neal HA
- Nisius R
- O'Neale SW
- Oh A
- OPAL Collaboration
- Oreglia MJ
- Orito S
- Pahl C
- Pasztor G
- Pater JR
- Pilcher JE
- Pinfold J
- Plane DE
- Pooth O
- Przybycien M
- Quadt A
- Rabbertz K
- Rembser C
- Renkel P
- Roney JM
- Rossi AM
- Rozen Y
- Runge K
- Sachs K
- Saeki T
- Sarkisyan EKG
- Schaile AD
- Schaile O
- Scharff-Hansen P
- Schieck J
- Schorner-Sadenius T
- Schroder M
- Schumacher M
- Seuster R
- Shears TG
- Shen BC
- Sherwood P
- Skuja A
- Smith AM
- Sobie R
- Soldner-Rembold S
- Spano F
- Stahl A
- Strohmer R
- Strom D
- Tarem S
- Tasevsky M
- Teuscher R
- Thomson MA
- Torrence E
- Toya D
- Tran P
- Trigger I
- Trocsanyi Z
- Tsur E
- Turner-Watson MF
- Ueda I
- Ujvari B
- Vannerem P
- Vertesi R
- Verzocchi M
- Vollmer CF
- von Krogh J
- Voss H
- Vossebeld J
- Ward CP
- Ward DR
- Watkins PM
- Watson AT
- Watson NK
- Wells PS
- Wengler T
- Wermes N
- Wilson GW
- Wilson JA
- Wolf G
- Wyatt TR
- Yamashita S
- Zer-Zion D
- Zivkovic L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 21/02/2005
- Field of study
Using the OPAL detector at LEP, the running of the effective QED coupling
alpha(t) is measured for space-like momentum transfer from the angular
distribution of small-angle Bhabha scattering. In an almost ideal QED
framework, with very favourable experimental conditions, we obtain:
Delta alpha(-6.07GeV^2) - Delta alpha(-1.81GeV^2) = (440 pm 58 pm 43 pm 30) X
10^-5, where the first error is statistical, the second is the experimental
systematic and the third is the theoretical uncertainty. This agrees with
current evaluations of alpha(t).The null hypothesis that alpha remains constant
within the above interval of -t is excluded with a significance above 5sigma.
Similarly, our results are inconsistent at the level of 3sigma with the
hypothesis that only leptonic loops contribute to the running. This is
currently the most significant direct measurment where the running alpha(t) is
probed differentially within the measured t range.Comment: 43 pages, 12 figures, Submitted to Euro. Phys. J.
A Measurement of Rb using a Double Tagging Method
- Author
- Abbiendi G
- Ackerstaff K
- Alexander G
- Allison J
- Altekamp N
- Anderson KJ
- Anderson S
- Arcelli S
- Asai S
- Ashby SF
- Axen D
- Azuelos G
- Ball AH
- Barberio E
- Barlow RJ
- Bartoldus R
- Batley JR
- Baumann S
- Bechtluft J
- Behnke T
- Bell KW
- Bella G
- Bellerive A
- Bentvelsen S
- Bethke S
- Betts S
- Biebel O
- Biguzzi A
- Bird SD
- Blobel V
- Bloodworth IJ
- Bobinski M
- Bock P
- Bohme J
- Bonacorsi D
- Boutemeur M
- Braibant S
- Bright-Thomas P
- Brigliadori L
- Brown RM
- Burckhart HJ
- Burgard C
- Burgin R
- Capiluppi P
- Carnegie RK
- Carter AA
- Carter JR
- Chang CY
- Charlton DG
- Chrisman D
- Ciocca C
- Clarke PEL
- Clay E
- Cohen I
- Conboy JE
- Cooke OC
- Couyoumtzelis C
- Coxe RL
- Cuffiani M
- Dado S
- Dallavalle GM
- Davis R
- De Jong S
- de Roeck A
- del Pozo LA
- Desch K
- Dienes B
- Dixit MS
- Dubbert J
- Duchovni E
- Duckeck G
- Duerdoth IP
- Eatough D
- Estabrooks PG
- Etzion E
- Evans HG
- Fabbri F
- Fanti M
- Faust AA
- Fiedler F
- Fierro M
- Fleck I
- Folman R
- Furtjes A
- Futyan DI
- Gagnon P
- Gary JW
- Gascon J
- Gascon-Shotkin SM
- Gaycken G
- Geich-Gimbel C
- Giacomelli G
- Giacomelli P
- Gibson V
- Gibson WR
- Gingrich DM
- Glenzinski D
- Goldberg J
- Gorn W
- Grandi C
- Gross E
- Grunhaus J
- Gruwe M
- Hanson GG
- Hansroul M
- Hapke M
- Harder K
- Hargrove CK
- Hartmann C
- Hauschild M
- Hawkes CM
- Hawkings R
- Hemingway RJ
- Herndon M
- Herten G
- Heuer RD
- Hildreth MD
- Hill JC
- Hillier SJ
- Hobson PR
- Hocker A
- Homer RJ
- Honma AK
- Horvath D
- Hossain KR
- Howard R
- Huntemeyer P
- Igo-Kemenes P
- Imrie DC
- Ishii K
- Jacob FR
- Jawahery A
- Jeremie H
- Jimack M
- Jones CR
- Jovanovic P
- Junk TR
- Karlen D
- Kartvelishvili V
- Kawagoe K
- Kawamoto T
- Kayal PI
- Keeler RK
- Kellogg RG
- Kennedy BW
- Klier A
- Kluth S
- Kobayashi T
- Kobel M
- Koetke DS
- Kokott TP
- Kolrep M
- Komamiya S
- Kowalewski RV
- Kress T
- Krieger P
- Kuhl T
- Kyberd P
- Lafferty GD
- Lanske D
- Lauber J
- Lautenschlager SR
- Lawson I
- Layter JG
- Lazic D
- Lee AM
- Lellouch D
- Letts J
- Levinson L
- Liebisch R
- List B
- Littlewood C
- Liu D
- Lloyd AW
- Lloyd SL
- Loebinger FK
- Long GD
- Losty MJ
- Ludwig J
- Macchiolo A
- Macpherson A
- Mader W
- Mannelli M
- Marcellini S
- Markopoulos C
- Martin AJ
- Martin JP
- Martinez G
- Mashimo T
- Mattig P
- McDonald WJ
- McKenna J
- Mckigney EA
- McMahon TJ
- McPherson RA
- Meijers F
- Menke S
- Merritt FS
- Mes H
- Meyer J
- Michelini A
- Mihara S
- Mikenberg G
- Miller DJ
- Mir R
- Mohr W
- Montanari A
- Mori T
- Nagai K
- Nakamura I
- Neal HA
- Nellen B
- Nisius R
- O'Neale SW
- Oakham FG
- Odorici F
- Ogren HO
- OPAL Collaboration
- Oreglia MJ
- Orito S
- Palinkas J
- Pasztor G
- Pater JR
- Patrick GN
- Patt J
- Perez-Ochoa R
- Petzold S
- Pfeifenschneider P
- Pilcher JE
- Pinfold J
- Plane DE
- Poffenberger P
- Polok J
- Przybycien M
- Rembser C
- Rick H
- Robertson S
- Robins SA
- Rodning N
- Roney JM
- Roscoe K
- Rossi AM
- Rozen Y
- Runge K
- Runolfsson O
- Rust DR
- Sachs K
- Saeki T
- Sahr O
- Sang WM
- Sarkisyan EKG
- Sbarra C
- Schaile AD
- Schaile O
- Scharf F
- Scharff-Hansen P
- Schieck J
- Schmitt B
- Schmitt S
- Schoning A
- Schroder M
- Schumacher M
- Schwick C
- Scott WG
- Seuster R
- Shears TG
- Shen BC
- Shepherd-Themistocleous CH
- Sherwood P
- Siroli GP
- Sittler A
- Skuja A
- Smith AM
- Snow GA
- Sobie R
- Soldner-Rembold S
- Sproston M
- Stahl A
- Stephens K
- Steuerer J
- Stoll K
- Strohmer R
- Strom D
- Surrow B
- Talbot SD
- Tanaka S
- Taras P
- Tarem S
- Teuscher R
- Thiergen M
- Thomson MA
- Torrence E
- Towers S
- Trigger I
- Trocsanyi Z
- Tsur E
- Turcot AS
- Turner-Watson MF
- Van Kooten R
- Vannerem P
- Verzocchi M
- von Krogh J
- von Torne E
- Voss H
- Wackerle F
- Wagner A
- Ward CP
- Ward DR
- Watkins PM
- Watson AT
- Watson NK
- Wells PS
- Wermes N
- White JS
- Wilson GW
- Wilson JA
- Wyatt TR
- Yamashita S
- Yekutieli G
- Zacek V
- Zer-Zion D
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/08/1998
- Field of study
The fraction of Z to bbbar events in hadronic Z decays has been measured by
the OPAL experiment using the data collected at LEP between 1992 and 1995. The
Z to bbbar decays were tagged using displaced secondary vertices, and high
momentum electrons and muons. Systematic uncertainties were reduced by
measuring the b-tagging efficiency using a double tagging technique. Efficiency
correlations between opposite hemispheres of an event are small, and are well
understood through comparisons between real and simulated data samples. A value
of Rb = 0.2178 +- 0.0011 +- 0.0013 was obtained, where the first error is
statistical and the second systematic. The uncertainty on Rc, the fraction of Z
to ccbar events in hadronic Z decays, is not included in the errors. The
dependence on Rc is Delta(Rb)/Rb = -0.056*Delta(Rc)/Rc where Delta(Rc) is the
deviation of Rc from the value 0.172 predicted by the Standard Model. The
result for Rb agrees with the value of 0.2155 +- 0.0003 predicted by the
Standard Model.Comment: 42 pages, LaTeX, 14 eps figures included, submitted to European
Physical Journal
Measurement of the B+ and B-0 lifetimes and search for CP(T) violation using reconstructed secondary vertices
- Author
- Abbiendi G
- Ackerstaff K
- Alexander G
- Allison J
- Altekamp N
- Anderson KJ
- Anderson S
- Arcelli S
- Asai S
- Ashby SF
- Axen D
- Azuelos G
- Ball AH
- Barberio E
- Barlow RJ
- Bartoldus R
- Batley JR
- Baumann S
- Bechtluft J
- Behnke T
- Bell KW
- Bella G
- Bellerive A
- Bentvelsen S
- Bethke S
- Betts S
- Biebel O
- Biguzzi A
- Bird SD
- Blobel V
- Bloodworth IJ
- Bock P
- Bohme J
- Bonacorsi D
- Boutemeur M
- Braibant S
- Bright-Thomas P
- Brigliadori L
- Brown RM
- Burckhart HJ
- Capiluppi P
- Carnegie RK
- Carter AA
- Carter JR
- Chang CY
- Charlton DG
- Chrisman D
- Ciocca C
- Clarke PEL
- Clay E
- Cohen I
- Conboy JE
- Cooke OC
- Couyoumtzelis C
- Coxe RL
- Cuffiani M
- Dado S
- Dallavalle GM
- Davis R
- De Jong S
- de Roeck A
- Dervan P
- Desch K
- Dienes B
- Dixit MS
- Dubbert J
- Duchovni E
- Duckeck G
- Duerdoth IP
- Eatough D
- Estabrooks PG
- Etzion E
- Fabbri F
- Fanti M
- Faust AA
- Fiedler F
- Fierro M
- Fleck I
- Folman R
- Furtjes A
- Futyan DI
- Gagnon P
- Gary JW
- Gascon J
- Gascon-Shotkin SM
- Gaycken G
- Geich-Gimbel C
- Giacomelli G
- Giacomelli P
- Gibson V
- Gibson WR
- Gingrich DM
- Glenzinski D
- Goldberg J
- Gorn W
- Graham K
- Grandi C
- Gross E
- Grunhaus J
- Gruwe M
- Hanson GG
- Hansroul M
- Hapke M
- Harder K
- Harel A
- Hargrove CK
- Hartmann C
- Hauschild M
- Hawkes CM
- Hawkings R
- Hemingway RJ
- Herndon M
- Herten G
- Heuer RD
- Hildreth MD
- Hill JC
- Hobson PR
- Hoch M
- Hocker A
- Hoffman K
- Homer RJ
- Honma AK
- Horvath D
- Hossain KR
- Howard R
- Huntemeyer P
- Igo-Kemenes P
- Imrie DC
- Ishii K
- Jacob FR
- Jawahery A
- Jeremie H
- Jimack M
- Jones CR
- Jovanovic P
- Junk TR
- Karlen D
- Kartvelishvili V
- Kawagoe K
- Kawamoto T
- Kayal PI
- Keeler RK
- Kellogg RG
- Kennedy BW
- Kim DH
- Klier A
- Kluth S
- Kobayashi T
- Kobel M
- Koetke DS
- Kokott TP
- Kolrep M
- Komamiya S
- Kowalewski RV
- Kress T
- Krieger P
- Kuhl T
- Kyberd P
- Lafferty GD
- Landsman H
- Lanske D
- Lauber J
- Lautenschlager SR
- Lawson I
- Layter JG
- Lazic D
- Lee AM
- Lellouch D
- Letts J
- Levinson L
- Liebisch R
- List B
- Littlewood C
- Liu D
- Lloyd AW
- Lloyd SL
- Loebinger FK
- Long GD
- Losty MJ
- Ludwig J
- Macchiolo A
- Macpherson A
- Mader W
- Mannelli M
- Marcellini S
- Markopoulos C
- Martin AJ
- Martin JP
- Martinez G
- Mashimo T
- Mattig P
- McDonald WJ
- McKenna J
- Mckigney EA
- McMahon TJ
- McPherson RA
- Meijers F
- Menke S
- Merritt FS
- Mes H
- Meyer J
- Michelini A
- Mihara S
- Mikenberg G
- Miller DJ
- Mir R
- Mohr W
- Montanari A
- Mori T
- Nagai K
- Nakamura I
- Neal HA
- Nellen B
- Nisius R
- O'Neale SW
- Oakham FG
- Odorici F
- Ogren HO
- OPAL Collaboration
- Oreglia MJ
- Orito S
- Palinkas J
- Pasztor G
- Pater JR
- Patrick GN
- Patt J
- Perez-Ochoa R
- Petzold S
- Pfeifenschneider P
- Pilcher JE
- Pinfold J
- Plane DE
- Poffenberger P
- Polok J
- Przybycien M
- Rembser C
- Rick H
- Robertson S
- Robins SA
- Rodning N
- Roney JM
- Roscoe K
- Rossi AM
- Rozen Y
- Runge K
- Runolfsson O
- Rust DR
- Sachs K
- Saeki T
- Sahr O
- Sang WM
- Sarkisyan EKG
- Sbarra C
- Schaile AD
- Schaile O
- Scharf F
- Scharff-Hansen P
- Schieck J
- Schmitt B
- Schmitt S
- Schoning A
- Schroder M
- Schumacher M
- Schwick C
- Scott WG
- Seuster R
- Shears TG
- Shen BC
- Shepherd-Themistocleous CH
- Sherwood P
- Siroli GP
- Sittler A
- Skuja A
- Smith AM
- Snow GA
- Sobie R
- Soldner-Rembold S
- Spagnolo S
- Sproston M
- Stahl A
- Stephens K
- Steuerer J
- Stoll K
- Strohmer R
- Strom D
- Surrow B
- Talbot SD
- Tanaka S
- Taras P
- Tarem S
- Teuscher R
- Thiergen M
- Thomas J
- Thomson MA
- Torrence E
- Towers S
- Trigger I
- Trocsanyi Z
- Tsur E
- Turcot AS
- Turner-Watson MF
- Ueda I
- Van Kooten R
- Vannerem P
- Verzocchi M
- von Krogh J
- von Torne E
- Voss H
- Wackerle F
- Wagner A
- Ward CP
- Ward DR
- Watkins PM
- Watson AT
- Watson NK
- Wells PS
- Wermes N
- White JS
- Wilson GW
- Wilson JA
- Wyatt TR
- Yamashita S
- Yekutieli G
- Zacek V
- Zer-Zion D
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/02/2000
- Field of study
The lifetimes of the B+ and B-0 mesons, and their ratio, have been measured in the OPAL experiment using 2.4 million hadronic Z(0) decays recorded at LEP. Z(0) --> b (b) over bar decays were tagged using displaced secondary vertices and high momentum electrons and muons. The lifetimes were then measured using well-reconstructed charged and neutral secondary vertices selected in this tagged data sample. The results aretau(B+) = 1.643 +/- 0.037 +/- 0.025 pstau(Bo) = 1.523 +/- 0.057 +/- 0.053 pstau(B+)/tau(Bo) = 1.079 +/- 0.064 +/- 0.041,where in each case the first error is statistical and the second systematic.A larger data sample of 3.1 million hadronic Z(o) decays has been used to search for CP and CPT violating effects by comparison of inclusive b and (b) over bar hadron decays, No evidence fur such effects is seen. The CP violation parameter Re(epsilon(B)) is measured to be Re(epsilon(B)) = 0.001 +/- 0.014 +/- 0.003and the fractional difference between b and (b) over bar hadron lifetimes is measured to(Delta tau/tau)(b) = tau(b hadron) - tau((b) over bar hadron)/tau(average) = -0.001 +/- 0.012 +/- 0.008
Measurement of D-s(+) and D-s(*+) production in B meson decays and from continuum e(+)e(-) annihilation at âs=10.6 GeV
- Author
- Abe K
- Abrams GS
- Adam I
- Adye T
- Albert J
- Aleksan R
- Allison J
- Alsmiller JRG
- Andress JC
- Angelini C
- Anjomshoaa A
- Anthony PL
- Anulli F
- Arisaka K
- Aspinwall ML
- Aston D
- Aubert B
- Azzopardi DE
- BABAR Collaboration
- Back JJ
- Bagnasco S
- Baird K
- Baldini-Ferroli R
- Band HR
- Barillari T
- Barlow NR
- Barlow RJ
- Bartoldus R
- Batignani G
- Bauer JM
- Benayoun M
- Berger N
- Beringer J
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- Yushkov AN
- Zacek V
- Zallo A
- Zhang J
- Zhu RY
- Zhu YS
- Zito M
- Publication venue
- American Physical Society
- Publication date
- 01/01/2002
- Field of study
This is the pre-print version of the Article. The official published version can be accessed from the links below. Copyright @ 2002 APSNew measurements of Ds+ and Ds*+ meson production rates from B decays and from qqÌ
continuum events near the ΄(4S) resonance are presented. Using 20.8 fb-1 of data on the ΄(4S) resonance and 2.6 fb-1 off-resonance, we find the inclusive branching fractions B(BâDs+X)=(10.93±0.19±0.58±2.73)% and B(BâDs*+X)=(7.9±0.8±0.7±2.0)%, where the first error is statistical, the second is systematic, and the third is due to the Ds+âÏÏ+ branching fraction uncertainty. The production cross sections Ï(e+e-âDs+X)ĂB(Ds+âÏÏ+)=7.55±0.20±0.34pb and Ï(e+e-âDs*±X)ĂB(Ds+âÏÏ+)=5.8±0.7±0.5pb are measured at center-of-mass energies about 40 MeV below the ΄(4S) mass. The branching fractions ÎŁB(BâDs(*)+D(*))=(5.07±0.14±0.30±1.27)% and ÎŁB(BâDs*+D(*))=(4.1±0.2±0.4±1.0)% are determined from the Ds(*)+ momentum spectra. The mass difference m(Ds+)-m(D+)=98.4±0.1±0.3MeV/c2 is also measured.This work was supported by DOE and NSF (USA), NSERC (Canada), IHEP (China), CEA and CNRS-IN2P3 (France), BMBF (Germany), INFN (Italy), NFR (Norway), MIST (Russia), and PPARC (United Kingdom). Individuals have received support from the Swiss NSF, A. P. Sloan Foundation, Research Corporation, and Alexander von Humboldt Foundation
Search for rare quark-annihilation decays, B --> Ds(*) Phi
- Author
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- Abrams GS
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- Zeng Q
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- Zhu YS
- Ziegler V
- Zito M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 12/12/2005
- Field of study
We report on searches for B- --> Ds- Phi and B- --> Ds*- Phi. In the context
of the Standard Model, these decays are expected to be highly suppressed since
they proceed through annihilation of the b and u-bar quarks in the B- meson.
Our results are based on 234 million Upsilon(4S) --> B Bbar decays collected
with the BABAR detector at SLAC. We find no evidence for these decays, and we
set Bayesian 90% confidence level upper limits on the branching fractions BF(B-
--> Ds- Phi) Ds*- Phi)<1.2x10^(-5). These results
are consistent with Standard Model expectations.Comment: 8 pages, 3 postscript figues, submitted to Phys. Rev. D (Rapid
Communications
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
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- Abolins M
- Abramowicz H
- Abreu H
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- 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
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- Werner M
- Werner P
- Werth M
- Wessels M
- Whalen K
- Wheeler-Ellis SJ
- Whitaker SP
- White A
- White MJ
- White S
- Whitehead SR
- Whiteson D
- Whittington D
- Wicek F
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik LAM
- Wildauer A
- Wildt MA
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- Wilkens HG
- Will JZ
- Williams E
- Williams HH
- Willis W
- Willocq S
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- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wolter MW
- Wolters H
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wraight K
- Wright C
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wunstorf R
- Wynne BM
- Xaplanteris L
- Xella S
- Xie S
- Xie Y
- Xu C
- Xu D
- Xu G
- Yabsley B
- Yagci KD
- Yamada M
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang S
- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao W-M
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zdrazil M
- Zeitnitz C
- Zeller M
- Zema PF
- Zemla A
- Zendler C
- Zenin AV
- Zenin O
- Zenis T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- 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
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