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Exact solution of the Hu-Paz-Zhang master equation
Quantum Physics · Submitted 13 Jan 2003
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim As a consequence, worthwhile results for the equation can only be obtained in the high temperature limit, where zero-point oscillations are neglected.
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The abstract, sentence by sentence
The Hu-Paz-Zhang equation is a master equation for an oscillator coupled to a linear passive bath. It is exact within the assumption that the oscillator and bath are initially uncoupled . Here an exact general solution is obtained in the form of an expression for the Wigner function at time t in terms of the initial Wigner function. The result is applied to the motion of a Gaussian wave packet and to that of a pair of such wave packets. A serious divergence arising from the assumption of an initially uncoupled state is found to be due to the zero-point oscillations of the bath and not removed in a cutoff model. As a consequence, worthwhile results for the equation can only be obtained in the high temperature limit, where zero-point oscillations are neglected. In that limit closed form expressions for wave packet spreading and attenuation of coherence are obtained. These results agree within a numerical factor with those appearing in the literature, which apply for the case of a particle at zero temperature that is suddenly coupled to a bath at high temperature. On the other hand very different results are obtained for the physically consistent case in which the initial particle temperature is arranged to coincide with that of the bath.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The Hu-Paz-Zhang equation is a master equation for an oscillator coupled to a linear passive bath. | background 1.00 | 0.07 | 0.03 | asserted 1.00 |
| s1 | It is exact within the assumption that the oscillator and bath are initially uncoupled . | background 0.55 | 0.12 | 0.06 | asserted 1.00 |
| s2 | Here an exact general solution is obtained in the form of an expression for the Wigner function at time t in terms of the initial Wigner function. | contribution 0.78 | 0.95 | 0.38 | asserted 1.00 |
| s3 | The result is applied to the motion of a Gaussian wave packet and to that of a pair of such wave packets. | contribution 0.81 | 0.90 | 0.07 | asserted 1.00 |
| s4 | A serious divergence arising from the assumption of an initially uncoupled state is found to be due to the zero-point oscillations of the bath and not removed in a cutoff model. | result 0.80 | 0.89 | 0.25 | asserted 1.00 |
| s5 | As a consequence, worthwhile results for the equation can only be obtained in the high temperature limit, where zero-point oscillations are neglected. | limitation 0.71 | 0.81 | 0.60 | asserted 0.96 |
| s6 | In that limit closed form expressions for wave packet spreading and attenuation of coherence are obtained. | result 0.98 | 0.91 | 0.16 | asserted 1.00 |
| s7 | These results agree within a numerical factor with those appearing in the literature, which apply for the case of a particle at zero temperature that is suddenly coupled to a bath at high temperature. | result 0.82 | 0.54 | 0.10 | asserted 0.96 |
| s8 | On the other hand very different results are obtained for the physically consistent case in which the initial particle temperature is arranged to coincide with that of the bath. | result 0.97 | 0.89 | 0.19 | asserted 1.00 |
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Original abstract
The Hu-Paz-Zhang equation is a master equation for an oscillator coupled to a linear passive bath. It is exact within the assumption that the oscillator and bath are initially uncoupled . Here an exact general solution is obtained in the form of an expression for the Wigner function at time t in terms of the initial Wigner function. The result is applied to the motion of a Gaussian wave packet and to that of a pair of such wave packets. A serious divergence arising from the assumption of an initially uncoupled state is found to be due to the zero-point oscillations of the bath and not removed in a cutoff model. As a consequence, worthwhile results for the equation can only be obtained in the high temperature limit, where zero-point oscillations are neglected. In that limit closed form expressions for wave packet spreading and attenuation of coherence are obtained. These results agree within a numerical factor with those appearing in the literature, which apply for the case of a particle at zero temperature that is suddenly coupled to a bath at high temperature. On the other hand very different results are obtained for the physically consistent case in which the initial particle temperature is arranged to coincide with that of the bath.
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