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Title: QCD perturbative expansion for {ital e}{sup +}{ital e}{sup {minus}}{r_arrow}hadrons

Journal Article · · Physical Review, D
 [1];  [2]
  1. Institute of Theoretical Science, University of Oregon, Eugene, Oregon 97403 (United States)
  2. Department of Physics and Astronomy, University of Alabama, Tuscaloosa, Alabama 35487 (United States)

We study the perturbative QCD series for the hadronic width of the {ital Z} boson. We sum a class of large {open_quote}{open_quote}{pi}{sup 2} terms{close_quote}{close_quote} and reorganize the series so as to minimize {open_quote}{open_quote}renormalon{close_quote}{close_quote} effects. We also consider the renormalization scheme-scale ambiguity of the perturbative results. We find that, with three nontrivial known terms in the perturbative expansion, the treatment of the {pi}{sup 2} terms is quite important, while renormalon effects are less important. The measured hadronic width of the {ital Z} is often used to determine the value of {alpha}{sub {ital s}}({ital M}{sup 2}{sub {ital Z}}). A standard method is to use the perturbative expansion for the width truncated at order {alpha}{sup 3}{sub {ital s}} in the {bar M}{bar S} scheme with scale {mu}={ital M}{sub {ital Z}}. We estimate that the determined value of {alpha}{sub {ital s}}({ital M}{sup 2}{sub {ital Z}}) should be increased by 0.6{percent} compared to the value extracted with this standard method. After this adjustment for {pi}{sup 2} and renormalon effects, we estimate that the uncertainty in {alpha}{sub {ital s}}({ital M}{sup 2}{sub {ital Z}}) arising from QCD theory is about 0.4{percent}. This is, of course, much less than the experimental uncertainty of about 5{percent}. {copyright} {ital 1996 The American Physical Society.}

DOE Contract Number:
FG05-84ER40141; FG06-85ER40224
OSTI ID:
389037
Journal Information:
Physical Review, D, Vol. 54, Issue 7; Other Information: PBD: Oct 1996
Country of Publication:
United States
Language:
English