Determination of αS using OPAL hadronic event shapes at $\sqrt{s} = 91\mbox{--}209~\mathrm{GeV}$ and resummed NNLO calculations
暂无分享,去创建一个
C. Hajdu | S. Marcellini | B. W. Kennedy | G. G. Hanson | J. Letts | A. Skuja | A. Harel | P. Gagnon | R. Seuster | D. Lellouch | P. Renkel | E. A. Wolf | O. Pooth | M. Schröder | S. Söldner-Rembold | H. Voss | D. R. Ward | T. G. Shears | S. Tarem | C. Pahl | J. Schieck | P. Vannerem | G. Anagnostou | K. Rabbertz | K. W. Bell | F. Fiedler | P. Jovanovic | W. Menges | J. R. Carter | G. Duckeck | G. Wolf | A. Frey | N. Wermes | E. Etzion | G. Mikenberg | I. Nakamura | J. C. Hill | I. P. Duerdoth | G. Herten | P. Giacomelli | T. Kobayashi | P. J. Bell | G. Benelli | M. Tasevsky | D. G. Charlton | H. A. Neal | C. P. Ward | E. Duchovni | K. Nagai | C. Ciocca | L. Zivkovic | P. Ferrari | C. Rembser | G. Alexander | K. Kawagoe | S. Kluth | T. Kuhl | A. Quadt | P. Scharff-Hansen | M. Cuffiani | G. W. Wilson | J. M. Roney | H. Landsman | S. Campana | M. Dallavalle | A. M. Rossi | A. Michelini | M. J. Oreglia | E. Torrence | A. Csilling | W. Mohr | T. R. Wyatt | P. Mättig | K. J. Anderson | S. Asai | T. Barillari | P. Bechtle | S. Bethke | O. Biebel | A. Bellerive | K. Desch | F. Fabbri | I. Fleck | J. Kanzaki | P. Krieger | T. Mashimo | H. Nanjo | A. Oh | Y. Rozen | P. Sherwood | T. Wengler | M. Hauschild | M. Giunta | T. Junk | T. Shears | M. Kupper | P. Gagnon | D. Karlen | G. Alexander | K. Anderson | S. Asai | D. Axen | E. Barberio | T. Barillari | P. Bechtle | P. Bell | G. Bella | S. Bethke | O. Biebel | H. Burckhart | J. Carter | D. Charlton | C. Ciocca | K. Desch | J. Dubbert | E. Duchovni | G. Duckeck | I. Duerdoth | E. Etzion | P. Ferrari | F. Fiedler | I. Fleck | C. Geich-Gimbel | E. Gross | R. Hawkings | G. Herten | J. Kanzaki | K. Kawagoe | T. Kawamoto | R. Keeler | S. Kluth | M. Kobel | A. Krasznahorkay | P. Krieger | T. Kuhl | D. Lellouch | L. Levinson | S. Lloyd | F. Loebinger | A. Ludwig | J. Ludwig | P. Mättig | T. Mashimo | R. McPherson | F. Merritt | G. Mikenberg | W. Mohr | K. Nagai | H. Neal | A. Oh | M. Oreglia | C. Pahl | G. Pásztor | J. Pater | J. Pilcher | J. Pinfold | M. Przybycien | A. Quadt | C. Rembser | Y. Rozen | J. Schieck | M. Schumacher | R. Seuster | P. Sherwood | R. Sobie | F. Spanò | R. Ströhmer | D. Strom | S. Tarem | M. Tasevsky | R. Teuscher | M. Thomson | E. Torrence | I. Trigger | I. Ueda | O. Boeriu | J. Vossebeld | P. Watkins | A. Watson | T. Wengler | N. Wermes | J. Wilson | L. Živković | T. Mori | S. Braibant | A. Bellerive | A. Carter | C. Hawkes | J. Hill | P. Wells | T. Wyatt | E. Wolf | D. Lanske | O. Pooth | M. Schröder | K. Rabbertz | C. Hajdu | D. Horvath | Z. Trocsanyi | B. Ujvári | G. Abbiendi | P. Capiluppi | M. Cuffiani | S. Marcellini | A. Roeck | F. Meijers | K. Bell | R. Brown | B. Kennedy | G. Hanson | J. Letts | G. Benelli | M. Boutemeur | R. Kellogg | A. Skuja | A. Harel | A. Rossi | Paolo Giacomelli | P. Renkel | S. Söldner-Rembold | M. Verzocchi | G. Wilson | D. Miller | B. Shen | A. Frey | I. Nakamura | S. Mihara | T. Behnke | S. Komamiya | D. Ward | T. Saeki | I. Bailey | S. Yamashita | R. Batley | C. Ainsley | J. Roney | A. Stahl | H. Mes | A. Gupta | R. Barlow | T. Kobayashi | W. Mader | R. Ströhmer | P. Scharff-Hansen | D. Zer-Zion | F. Fabbri | P. Bock | R. Carnegie | S. Dado | B. Dienes | G. Giacomelli | J. Goldberg | J. Grunhaus | M. Gruwe | R. Heuer | P. Igo-Kemenes | K. Ishii | H. Jérémie | P. Jovanović | J. Krogh | A. Michelini | S. O'neale | S. Orito | D. Plane | K. Runge | K. Sachs | A. Schaile | O. Schaile | A. Smith | E. Tsur | M. F. Turner-Watson | H. Voss | C. Ward | N. Watson | J. Lu | H. Nanjo | T. Schörner-Sadenius | H. Landsman | P. Vannerem | G. Lafferty | R. Vértesi | G. Wolf | T. Krämer | The Opal Collaboration | P. F. Åkesson | Á. Csilling | M. Dallavalle | M. Ford | M. Hamann | J. Lillich | W. Menges | N. Meyer | A. Mutter | D. Toya | C. Vollmer | G. Bella | R. Teuscher | D. Strom | R. M. Brown | R. G. Kellogg | T. Mori | J. R. Pater | D. Lanske | J. W. Gary | G. D. Lafferty | D. J. Miller | M. Schumacher | K. Runge | C. M. Hawkes | T. Kawamoto | R. K. Keeler | S. L. Lloyd | F. K. Loebinger | R. A. McPherson | F. S. Merritt | J. E. Pilcher | I. Ueda | P. M. Watkins | A. T. Watson | P. S. Wells | J. A. Wilson | M. Przybycień | T. Schörner-Sadenius | M. Giunta | M. Boutemeur | O. Schaile | E. Barberio | M. A. Thomson | D. Axen | S. Orito | H. J. Burckhart | R. J. Barlow | J. Grunhaus | F. Meijers | G. Abbiendi | P. Capiluppi | A. Roeck | E. Gross | J. Ludwig | M. Verzocchi | M. Hauschild | M. Kobel | R. Sobie | R. Ströhmer | D. Karlen | G. Pásztor | N. K. Watson | R. Vértesi | A. J. Martin | C. Ainsley | T. Behnke | P. Bock | O. Boeriu | S. Braibant | R. K. Carnegie | A. A. Carter | C. Y. Chang | B. Dienes | J. Dubbert | M. Ford | G. Giacomelli | J. Goldberg | M. Gruwé | R. Hawkings | R. D. Heuer | P. Igo-Kemenes | K. Ishii | H. Jeremie | T. R. Junk | M. Kupper | J. Lillich | J. Lu | W. Mader | H. Mes | S. Mihara | J. Pinfold | D. E. Plane | K. Sachs | T. Saeki | A. D. Schaile | B. C. Shen | A. M. Smith | E. Tsur | S. Yamashita | D. Zer-Zion | R. J. Batley | A. Gupta | M. Hamann | T. Krämer | A. Mutter | F. Spano | D. Toya | C. F. Vollmer | S. W. O’Neale | L. Levinson | S. Komamiya | I. Bailey | J. Vossebeld | E. Sarkisyan | A. Stahl | S. Dado | C. Geich-Gimbel | D. Horváth | A. Jr. Krasznahorkay | J. Krogh | A. Ludwig | J. McKenna | N. Meyer | E. K. G. Sarkisyan | I. Trigger | Z. Trócsányi | B. Ujvári | The OPAL Collaboration | A. Martin | J. Mckenna | J. Gary | S. Campana | G. Anagnostou | C. Y. Chang | B. Ujvari | A. Gupta | J. Gary | Takashi Mori | P. Åkesson | O. Pooth | G. Anagnostou | D. Ward | M. Schröder | G. Wilson | G. Wilson | G. Wolf | S. O'Neale | J. Hill | A. Carter | J. Ludwig | K. Desch | T. Junk | J. Schieck | M. Schröder | D. Strom | A. Harel | T. Shears | W. Mader | F. Merritt | N. Watson | A. Rossi | M. Kupper | A. Rossi | C. Ward
[1] C. Kurz,et al. Electroweak corrections to hadronic event shapes and jet production in e+e− annihilation , 2010, 1003.0986.
[2] G. Dissertori,et al. Precise determination of the strong coupling constant at NNLO in QCD from the three-jet rate in electron-positron annihilation at LEP. , 2009, Physical review letters.
[3] C. Pahl,et al. Determination of the strong coupling αS from hadronic event shapes with $\mathcal{O}(\ensuremath {\alpha _{\mathrm {S}}}^{3})$ and resummed QCD predictions using JADE data , 2009 .
[4] S. Bethke. EPJ manuscript No. (will be inserted by the editor) The 2009 World Average of αs , 2022 .
[5] G. Dissertori,et al. Determination of the strong coupling constant using matched NNLO+NLLA predictions for hadronic event shapes in e+e− annihilations , 2009, 0906.3436.
[6] H. Stenzel,et al. Matching of Resummed NLLA with Fixed NNLO for Event Shapes , 2008, 0810.3599.
[7] S. Weinzierl. Next-to-next-to-leading order corrections to three-jet observables in electron-positron annihilation. , 2008, Physical review letters.
[8] H. Stenzel,et al. Matching NLLA+NNLO for event shape distributions , 2008 .
[9] G. Dissertori,et al. First determination of the strong coupling constant using NNLO predictions for hadronic event shapes in e + e − , 2009 .
[10] T. Gehrmann,et al. NNLO corrections to event shapes in e+e− annihilation , 2007, 0711.4711.
[11] S. Kluth. Tests of quantum chromo dynamics at e+e− colliders , 2006, Reports on progress in physics. Physical Society.
[12] M. Hauschild,et al. Determination of alpha(s) using jet rates at LEP with the OPAL detector , 2006 .
[13] M. Hauschild,et al. Measurement of the Strong Coupling α S from Four-Jet Observables in e + e − Annihilation , 2005 .
[14] The Opal Collaboration. Determination of αS using jet rates at LEP with the OPAL detector , 2005, hep-ex/0507047.
[15] E. al.,et al. Measurement of event shape distributions and moments in e + e $^-\rightarrow \mathrm{hadrons}$ at 91-209 GeV and a determination of $\ensuremath{\alpha_{\mathrm{s}}}$ , 2005, hep-ex/0503051.
[16] J. Abdallah,et al. The measurement of Alpha s from event shapes with the DELPHI detector at the highest LEP energies , 2004 .
[17] C. Rosemann,et al. Studies of hadronic event structure in E+ E- annihilation from 30-Gev to 209-Gev with the L3 detector , 2004 .
[18] V. Lemaître,et al. Studies of QCD at e(+)e(-) centre-of-mass energies between 91 and 209 GeV , 2004 .
[19] R.W. Jones. A combination by the LEP QCD Working Group of αs values derived from event shape variables at LEP , 2004 .
[20] L3 Collaboration. Studies of Hadronic Event Structure in e+e- Annihilation from 30 GeV to 209 GeV with the L3 Detector , 2004, hep-ex/0406049.
[21] Delphi collaboration. The measurement of $\alpha_s$ from event shapes with the DELPHI detector at the highest LEP energies , 2004, hep-ex/0406011.
[22] M. Ford. Studies of event shape observables with the OPAL detector at LEP , 2004, hep-ex/0405054.
[23] Richard J. K. Taylor,et al. Tests of models of color reconnection and a search for glueballs using gluon jets with a rapidity gap , 2004 .
[24] H. Stenzel,et al. Theoretical uncertainties on alpha_s from event-shape variables in e+e? annihilations. , 2003, hep-ph/0312016.
[25] Richard J. K. Taylor,et al. A study of charm and anti-charm production in beauty decays with the OPAL detector at LEP , 2003 .
[26] The Opal Collaboration,et al. Search for the Standard Model Higgs boson with the OPAL detector at LEP , 2002, hep-ex/0209078.
[27] Richard J. K. Taylor,et al. Search for the Standard Model Higgs boson with the OPAL detector at LEP , 2003 .
[28] S. Moretti,et al. HERWIG 6: an event generator for hadron emission reactions with interfering gluons (including supersymmetric processes) , 2001 .
[29] Otmar Biebel,et al. Experimental tests of the strong interaction and its energy dependence in electron–positron annihilation , 2001 .
[30] The Opal Collaboration,et al. QCD studies with ${\rm e^+e^-}$ annihilation data at 172-189 GeV , 2000, hep-ex/0002012.
[31] Z. Was,et al. The precision Monte Carlo event generator KK for two-fermion final states in e+e− collisions☆ , 1999, hep-ph/9912214.
[32] Z. Was,et al. Monte Carlo program KoralW 1.42 for all four-fermion final states in e+e− collisions* , 1999, hep-ph/9906277.
[33] Kraków,et al. Coherent exclusive exponentiation CEEX: the case of the resonant e + e - collision 1 Work supported , 1999, hep-ph/9905453.
[34] T. J. Fraser,et al. Thin scintillating tiles with high light yield for the OPAL endcaps , 1998 .
[35] T. Junk,et al. The extended OPAL silicon strip microvertex detector , 1998 .
[36] Richard J. K. Taylor,et al. QCD studies with e(+)e(-) annihilation data at 172-189 GeV , 1997 .
[37] J. Fujimoto,et al. grc4f v1.1: a four-fermion event generator for e+e− collisions , 1996, hep-ph/9603394.
[38] L. Mir,et al. The ALEPH Collaboration , 1996 .
[39] Dixit,et al. A comparison of b and uds quark jets to gluon jets , 1995 .
[40] T. Sjöstrand. High-energy-physics event generation with PYTHIA 5.7 and JETSET 7.4 , 1994 .
[41] G. E. Richards,et al. A determination ofαs( $$M_{Z^0 } $$ ) at LEP using resummed QCD calculations , 1993 .
[42] J. Vermaseren,et al. The three-loop QCD β-function and anomalous dimensions , 1993, hep-ph/9302208.
[43] B. Webber,et al. Jet broadening measures in e + e - annihilation , 1992 .
[44] L. Lönnblad. Ariadne version 4 — A program for simulation of QDC cascades implementing the colour dipole model , 1992 .
[45] G. M. Dallavalle,et al. The detector simulation program for the OPAL experiment at LEP , 1992 .
[46] N. C. Wood,et al. A global determination of $$\alpha _s (M_{Z^0 } )$$ at LEP , 1992 .
[47] L. Stanco,et al. HERWIG 5.1 - a Monte Carlo event generator for simulating hadron emission reactions with interfering gluons , 1992 .
[48] P. Gavillet. DELPHI Collaboration , 1992 .
[49] B. Webber,et al. New clustering algorithm for multijet cross sections in e+e− annihilation , 1991 .
[50] Gibson,et al. The OPAL Detector at LEP , 1990 .
[51] R. Lathe. Phd by thesis , 1988, Nature.
[52] A. E. Terrano,et al. The perturbative calculation of jet structure in e + e - annihilation , 1981 .
[53] L. Clavelli,et al. Consequences of 2nd order QCD for jet structure in e+e− annihilation , 1981 .
[54] A. Vladimirov,et al. The gell-mann-low function of QCD in the three-loop approximation , 1980 .
[55] F. Low,et al. Tensor analysis of hadronic jets in quantum chromodynamics , 1979 .
[56] G. Parisi. Superinclusive cross sections , 1978 .
[57] E. Farhi. Quantum Chromodynamics Test for Jets , 1977 .
[58] M. Gell-Mann,et al. Advantages of the color octet gluon picture , 1973 .
[59] F. Wilczek,et al. Asymptotically free gauge theories. I , 1973 .
[60] H. Politzer,et al. Reliable Perturbative Results for Strong Interactions , 1973 .
[61] F. Wilczek,et al. Ultraviolet Behavior of Non-Abelian Gauge Theories , 1973 .
[62] R. Sosnowski,et al. The principal axis of jets — an attempt to analyse high-energy collisions as two-body processes , 1964 .
[63] G. D. Liveing,et al. The University of Cambridge , 1897, British medical journal.