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In this section things should be explained by analogy and with pictures and, if necessary, some formulas. | In this section things should be explained by analogy and with pictures and, if necessary, some formulas. | ||
</note> | </note> | ||
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+ | For a nice discussion, see section 11.4 in Rajaramans "Solitons and Instantons" and page 6 in https://arxiv.org/pdf/hep-th/0207046.pdf | ||
+ | <tabbox Researcher> | ||
<note tip> | <note tip> | ||
The motto in this section is: //the higher the level of abstraction, the better//. | The motto in this section is: //the higher the level of abstraction, the better//. | ||
</note> | </note> | ||
- | --> Common Question 1# | + | --> Why isn't the Borel transformation applicable in QCD?# |
- | + | See section 20.7 in Weinberg's QFT book Vol. 2. | |
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- | --> Common Question 2# | + | " In quantum chromodynamics it is the renormalons that obstruct the use of the Borel transformation to sum the perturbation series [...] [T]here are instanton solutions in non Abelian gauge theories like quantum chromodynamics, but these also yield relatively harmless singularities of $B(z)$ on the negative real axis. the real problem in quantum chromodynamics is with a different class of singularities, known as renormalons. " |
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+ | (Renormalons are due to the running of the gauge couplings and originate in diagrams that yield contributions that grow like $n!$. According to Weinberg, they are "associated with terms in the operator product expansion".) | ||
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<-- | <-- | ||
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<tabbox Examples> | <tabbox Examples> |