TOPAZO 4.0 - A new version of a computer program for evaluation of deconvoluted and realistic observables atr LEP 1 and LEP 2

被引:71
作者
Montagna, G
Nicrosini, O
Piccinini, F
Passerino, G
机构
[1] Univ Pavia, Dipartimento Fis Nucl & Teor, I-27100 Pavia, Italy
[2] Ist Nazl Fis Nucl, Sez Pavia, I-27100 Pavia, Italy
[3] Univ Turin, Dipartimento Fis Teor, I-10125 Turin, Italy
[4] Ist Nazl Fis Nucl, Sez Torino, I-10125 Turin, Italy
关键词
e(+)e(-) annihilation; Bhabha scattering; LEP; Zresonance; electroweak; extrapolated and realistic experimental setup; QCD corrections; QED corrections; pure weak corrections; radiative corrections; minimal standard model; deconvoluted and realistic observables;
D O I
10.1016/S0010-4655(98)00080-0
中图分类号
TP39 [计算机的应用];
学科分类号
081203 ; 0835 ;
摘要
The program TOPAZO was developed for computing a variety of physical observables which are related to the e(+)e(-) annihilation into fermion pairs and to the large angle Bhabha scattering around the Z resonance. Among them the Z parameters or pseudo-observables, the deconvoluted cross sections and those dressed with QED radiation, and finally the forward-backward asymmetries; The calculations are performed both for a completely inclusive experimental setup and for a realistic one, i.e. a setup with cuts on the acollinearity angle, on the energy of the outgoing fermions or on their invariant mass and angular acceptance. The new version, 4.0, includes several innovative features; First of all, the most important new capabilities since previous versions are electroweak, QCD and QED correction factors that are relevant at the Z resonance in the light of the present experimental accuracy. Among them, the effect of the next-to-leading O(alpha(2)m(2),) corrections, the radiative corrections to the hadronic decay of the Z, providing complete corrections of O(alpha alpha(s)) to Gamma (Z --> q (q) over bar) with q = u, d, s, c, and b, and leading O(alpha(3)) QED corrections. Secondly, the program has been upgraded to cover two-fermion final states at LEP 2 energies, where some of the assumptions made for earlier versions are no longer valid. In particular, to this aim all the electroweak radiative corrections relevant far from the Z peak have been added for s-channel processes, e.g, purely weak boxes, next-to-leading O(alpha(2)) and leading O(alpha(3)) QED corrections. (C) 1999 Published by Elsevier Science B.V.
引用
收藏
页码:278 / 289
页数:12
相关论文
共 14 条
[1]  
[Anonymous], 1995, REPORTS WORKING GROU, DOI DOI 10.5170/CERN-1995-003
[2]  
[Anonymous], Z PHYS LEP 1
[3]  
[Anonymous], REPORTS WORKING GROU
[4]  
BOHM M, 1989, Z PHYSICS LEP 1, V1, P203
[5]  
BOUDJEMA F, 1996, PHYSICS LEP2, V2, P229
[6]   QED STRUCTURE FUNCTIONS - A SYSTEMATIC-APPROACH [J].
CACCIARI, M ;
DEANDREA, A ;
MONTAGNA, G ;
NICROSINI, O .
EUROPHYSICS LETTERS, 1992, 17 (02) :123-128
[7]   Nonfactorizable QCD and electroweak corrections to the hadronic Z boson decay rate [J].
Czarnecki, A ;
Kuhn, JH .
PHYSICAL REVIEW LETTERS, 1996, 77 (19) :3955-3958
[8]   Precise calculation of M(W), sin(2)(theta)over-cap(W)(M(Z)), and sin(2)theta(eff)(lept) [J].
Degrassi, G ;
Gambino, P ;
Sirlin, A .
PHYSICS LETTERS B, 1997, 394 (1-2) :188-194
[9]   RELATIONS BETWEEN THE ON-SHELL AND MS FRAMEWORKS AND THE MW-MZ INTERDEPENDENCE [J].
DEGRASSI, G ;
FANCHIOTTI, S ;
SIRLIN, A .
NUCLEAR PHYSICS B, 1991, 351 (1-2) :49-69
[10]   Two-loop heavy top effects on the m(z)-m(w) interdependence [J].
Degrassi, G ;
Gambino, P ;
Vicini, A .
PHYSICS LETTERS B, 1996, 383 (02) :219-226