alpha(s) from the non-perturbatively renormalised lattice three-gluon vertex

被引:90
作者
Alles, B
Henty, DS
Panagopoulos, H
Parrinello, C
Pittori, C
Richards, DG
机构
[1] UNIV PISA, DIPARTIMENTO FIS, I-56126 PISA, ITALY
[2] UNIV EDINBURGH, DEPT PHYS & ASTRON, EDINBURGH EH9 3JZ, MIDLOTHIAN, SCOTLAND
[3] UNIV CYPRUS, DEPT NAT SCI, CY-1678 NICOSIA, CYPRUS
[4] UNIV LIVERPOOL, DEPT MATH SCI, LIVERPOOL L69 3BX, MERSEYSIDE, ENGLAND
[5] UNIV PARIS 11, PHYS THEOR & HAUTES ENERGIES LAB, F-91405 ORSAY, FRANCE
[6] FERMILAB NATL ACCELERATOR LAB, BATAVIA, IL 60510 USA
关键词
D O I
10.1016/S0550-3213(97)00483-5
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
We compute the running QCD coupling on the lattice by evaluating two-point and three-point off-shell gluon Green's functions in a fixed gauge and imposing non-perturbative renormalisation conditions on them. Our exploratory study is performed in the quenched approximation at beta = 6.0 on 16(4) and 24(4) lattices. We show that, for momenta in the range 1.8-2.3 GeV, our coupling runs according to the two-loop asymptotic formula, allowing a precise determination of the corresponding Lambda parameter, The role of lattice artifacts and finite-volume effects is carefully analysed and these appear to be under control in the momentum range of interest. Our renormalisation procedure corresponds to a momentum subtraction scheme in continuum field theory, and therefore lattice perturbation theory is not needed in order to match our results to the <(MS)over bar> scheme, thus eliminating a major source of uncertainty in the determination of alpha(<(MS)over bar>). Our method can be applied directly to the unquenched case. (C) 1997 Elsevier Science B.V.
引用
收藏
页码:325 / 342
页数:18
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