Physics – Condensed Matter – Statistical Mechanics
Scientific paper
2004-10-06
Phys. Rev. Lett. 94, 070604 (2005)
Physics
Condensed Matter
Statistical Mechanics
4 pages, 3 figs; (v2) discussion extended; (v3) marginal changes, final version as published; (v4) added erratum pointing out
Scientific paper
10.1103/PhysRevLett.94.070604
The effective theories for many quantum phase transitions can be mapped onto those of classical transitions. Here we show that such a mapping fails for the sub-ohmic spin-boson model which describes a two-level system coupled to a bosonic bath with power-law spectral density, J(omega) ~ omega^s. Using an epsilon expansion we prove that this model has a quantum transition controlled by an interacting fixed point at small s, and support this by numerical calculations. In contrast, the corresponding classical long-range Ising model is known to have an upper-critical dimension at s = 1/2, with mean-field transition behavior controlled by a non-interacting fixed point for 0 < s < 1/2. The failure of the quantum-classical mapping is argued to arise from the long-ranged interaction in imaginary time in the quantum model.
Bulla Ralf
Tong Ning-Hua
Vojta Matthias
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