Speaker
Prof.
Hiroshi Suzuki
Description
An interesting possibility that the ambiguity in perturbation theory caused by the IR renormalon is cancelled by the instability associated with a semi-classical object called bion has been suggested in the context of the resurgence program of asymptotically-free quantum field theories. To reinforce this picture on the IR renormalon, the understanding of the IR renormalon in a compactified space such as seems to be a basic premise. In this talk, I report our recent analysis on the IR renormalon in the gluon condensate in the QCD(adj.) on with the twisted boundary conditions. In the large limit within the so-called large approximation, we find that the vacuum polarization of the W-boson, which acquires the twisted momentum from the boundary conditions, gives rise to the renormalon ambiguity that is identical to that in the system in the un-compactified space, . This situation is completely different from that in the 2D model on (the analyses on the latter will be presented by Dr. Takaura and Mr. Morikawa).