Abstract
We give the normalized leading asymptotic Q2 dependence of the pion form factor in quantum chromodynamics: Fπ(Q2)→Q2→±a-2fπ2bQ2n|Q2|, where fπ is the pion decay constant and b=(11-23Nf)16π2. Up to non-leading-logarithmic corrections, this is equivalent to Fπ(Q2)→Q2→±a 8παs(Q2)fπ2(-Q2). These results are obtained by solving the light-cone pion Bethe-Salpeter equation in quantum chromodynamics to leading-logarithmic accuracy.
Original language | English (US) |
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Pages (from-to) | 246-249 |
Number of pages | 4 |
Journal | Physical Review Letters |
Volume | 43 |
Issue number | 4 |
DOIs | |
State | Published - 1979 |
ASJC Scopus subject areas
- General Physics and Astronomy