A continuous sequence of infinitesimal unitary transformations is used to d
iagonalize the quantum sine-Gordon model for beta (2) is an element of (2 p
i, infinity). This approach can be understood as an extension of perturbati
ve scaling theory since it links weak- to strong-coupling behavior in a sys
tematic expansion: a small expansion parameter is identified and this param
eter remains small throughout the entire flow unlike the diverging running
coupling constant of perturbative scaling. Our approximation consists in ne
glecting higher orders in this small parameter. We find very accurate resul
ts for the single-particle/hole spectrum in the strong-coupling phase and c
an describe the full crossover from weak to strong-coupling. The integrable
structure of the sine-Gordon model is not used in our approach. Our new me
thod should be of interest for the investigation of nonintegrable perturbat
ions and for other strong-coupling problems. (C) 2001 Elsevier Science B.V.
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