1,159 research outputs found
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
Search for the standard model Higgs boson at LEP
- Author
- Abbaneo D
- Abbaneo D
- Abbiendi G
- Abbiendi G
- Abdallah J
- Abreu P
- Achard P
- Adam W
- Adriani O
- Adzic P
- Affholderbach K
- Aguilar-Benitez M
- Ainsley C
- Akesson PF
- Albrecht T
- Alcaraz J
- Alderweireld T
- Alemanni G
- Alemany-Fernandez R
- Alexander G
- Allaby J
- Allison J
- Allmendinger T
- Allport PP
- Aloisio A
- Alviggi MG
- Amaldi U
- Amapane N
- Amaral P
- Amato S
- Anagnostou G
- Anashkin E
- Anderhub H
- Anderson KJ
- Andreazza A
- Andreev VP
- Andringa S
- Anjos N
- Anselmo F
- Antilogus P
- Antonelli A
- Antonelli M
- Apel WD
- Arcelli S
- Arefiev A
- Armstrong SR
- Arnoud Y
- Asai S
- Ask S
- Asman B
- Augustin JE
- Augustinus A
- Awunor O
- Axen D
- Azemoon T
- Aziz T
- Azuelos G
- Azzurri P
- Baarmand M
- Badaud F
- Bagliesi G
- Bagnaia P
- Bailey I
- Baillon P
- Bajo A
- Baksay G
- Baksay L
- Baldew SV
- Ballestrero A
- Bambade P
- Banerjee S
- Banerjee S
- Barate R
- Barate R
- Barberio E
- Barbier R
- Barczyk A
- Bardin D
- Barillere R
- Barker G
- Barklow T
- Barlow RJ
- Baroncelli A
- Bartalini P
- Basile M
- Batalova N
- Batley RJ
- Battaglia M
- Battiston R
- Baubillier M
- Bay A
- Becattini F
- Bechtle P
- Becker U
- Becks KH
- Begalli M
- Behner F
- Behnke T
- Behrmann A
- Bell KW
- Bell PJ
- Bella G
- Bellerive A
- Bellucci L
- Ben-Haim E
- Bencivenni G
- Benekos N
- Benelli G
- Benvenuti A
- Berat C
- Berbeco R
- Berdugo J
- Berges P
- Berggren M
- Berkelman K
- Berntzon L
- Bertrand D
- Bertucci B
- Besancon M
- Besson N
- Betev BL
- Bethke S
- Beuselinck R
- Biasini M
- Biebell O
- Biglietti M
- Biland A
- Binnie DM
- Blair GA
- Blaising JJ
- Bloch D
- Bloch-Devaux B
- Blom M
- Blondel A
- Bloodworth IJ
- Bluj M
- Blumenschein U
- Blyth SC
- Bobbink GJ
- Boccali T
- Bock P
- Boeriun O
- Bohm A
- Bohrer A
- Boix G
- Boldizsar L
- Bologna G
- Bonacorsi D
- Bonesini M
- Bonissent A
- Boonekamp M
- Booth CN
- Booth PSL
- Borean C
- Borgia B
- Borisov G
- Bossi F
- Botner O
- Boucrot J
- Bouhova-Thacker E
- Boumediene D
- Bouquet B
- Bourilkov D
- Bourquin M
- Boutemeur M
- Bowcock TJV
- Bowdery CK
- Boyko I
- Braccini S
- Bracko M
- Braibant S
- Brandt S
- Branson JG
- Bravo S
- Brenner R
- Brient JC
- Brigliadori L
- Brochu F
- Brodet E
- Brown RM
- Bruckman P
- Bruneliere R
- Brunet JM
- Buchmuller O
- Buesser K
- Bugge L
- Buijs A
- Burckhart HJ
- Burger JD
- Burger WJ
- Buschmann P
- Cai XD
- Callot O
- Calvi M
- Cameron W
- Campana R
- Campana S
- Camporesi T
- Canale V
- Capell M
- Capon G
- Carena F
- Carlino G
- Carnegie RK
- Caron B
- Carr J
- Cartacci A
- Carter AA
- Carter JR
- Cartwright S
- Casado MP
- Casaus J
- Castro N
- Cattaneo A
- Cavallari F
- Cavallo F
- Cavallo N
- Cavanaugh R
- Cecchi C
- Cerrada M
- Cerutti F
- Chamizo M
- Chang CY
- Chang YH
- Chapkin M
- Charlton DG
- Charpentier P
- Checchia P
- Chemarin M
- Chen A
- Chen G
- Chen GM
- Chen HF
- Chen HS
- Chiarella V
- Chiefari G
- Chierici R
- Chiliapnikov P
- Chmeissani M
- Chudoba J
- Chung SU
- Cieslik K
- Cifarelli L
- Cindolo F
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- Ueda I
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- Vicinanza D
- Videau H
- Videau I
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- Vogel H
- Vogt H
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- von Wimmersperg-Toeller JH
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- Vorobyov AA
- Voss H
- Vossebeld J
- Vrba V
- Waananen A
- Wachsmuth H
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- Wahlen H
- Waller D
- Wallraff W
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- Wang ZM
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- Ward DR
- Ward JJ
- Washbrook AJ
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- Watkins PM
- Watson AT
- Watson NK
- Weber M
- Weiser C
- Well PS
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- Wermes N
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- Wetterling D
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- Wiedenmann W
- Wienemann P
- Wilkens H
- Wilkinson G
- Wilson GW
- Wilson JA
- Winter M
- Witek M
- Wolf G
- Wolf G
- Wu J
- Wu SL
- Wu SX
- Wu X
- Wunsch M
- Wyatt TR
- Wynhoff S
- Xia L
- Xie Y
- Xu R
- Xu ZZ
- Xue S
- Yamamoto J
- Yamashita S
- Yang BZ
- Yang CG
- Yang HJ
- Yang M
- Yeh SC
- Yuan C
- Yushchenko O
- Zachariadou K
- Zalewska A
- Zalewski P
- Zalite A
- Zalite Y
- Zavrtanik D
- Zeitnitz C
- Zer-Zion D
- Zhang J
- Zhang L
- Zhang ZP
- Zhao J
- Zhao W
- Zhu GY
- Zhu RY
- Zhuang HL
- Zhuravlov V
- Zichichi A
- Ziegler T
- Zilizi G
- Zimin NI
- Zimmermann B
- Zintchenko A
- Zito G
- Zivkovic L
- Zobernig G
- Zoller M
- Zupan M
- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 17/07/2003
- Field of study
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
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- 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
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- 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
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
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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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- 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
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
- Author
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- Zemla A
- Zenin O
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- Zhemchugov A
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- Zhuravlov V
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- Zimin NI
- Zimmermann R
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- ZivkoviÄ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or Ï lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, Ï, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan ÎČ in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
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- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
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- Al Khoury K
- Alberghi GL
- Albert J
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- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi A
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- Alimonti G
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- Allbrooke BMM
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- Allport PP
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- Alviggi MG
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- Ambler A
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- Amidei D
- Amor Dos Santos SP
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- Angerami A
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- Arling J-H
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- Astigarraga MEP
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- 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 fbâ1 of â 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 Emiss T > 150 GeV and Emiss T > 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 presente
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- Yamaguchi H
- Yamamoto A
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- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Smit GVY
- Ye J
- Ye S
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
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- Yu J
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- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
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- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou Y
- Zhu CG
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- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fbâ1 of sâ=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan ÎČ < 40
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