Abstract:It is shown that response properties of a quantum harmonic oscillator are in essence those of a classical oscillator, and that, paradoxical as it may be, these classical properties underlie all quantum dynamical properties of the system. The results are extended to non-interacting bosonic fields, both neutral and charged.
“…An attempt to apply methods of real-time QFT to quantum optics was made by Vinogradov and Stenholm [32]. Generalisation of the conventional time-normal operator ordering [12][13][14] beyond the resonance approximation, making it applicable in relativity, was introduced in [2] for bosons and [3] for fermions.…”
Section: Response Representation)mentioning
confidence: 99%
“…Here our goal is the opposite: we wish to apply wisdom acquired in quantum optics to QFT. The result of this paper in a nutshell is that, firstly, the nonequilibrium real-time QFT is nothing but the nonlinear quantum response problem formulated in phase-space terms, and, secondly, that the most natural physical picture emerges if using the phase-space mapping based on the so-called time-normal operator ordering [2,[12][13][14]. Moreover, in relativistic quantum electrodynamics (QED), mappings based on other orderings (e.g., the Keldysh rotation [11,15]) lead to inconsistencies, due to one's well-known inability to impose the Lorentz condition on the operator of the electromagnetic potential.…”
Section: Introductionmentioning
confidence: 99%
“…In papers [1][2][3], we introduced response transformation of quantum kinematics. In paper [4], response transformation was extended to the key technical tool of quantum field theory (QFT), Wick's theorem [5][6][7][8].…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, in relativistic quantum electrodynamics (QED), mappings based on other orderings (e.g., the Keldysh rotation [11,15]) lead to inconsistencies, due to one's well-known inability to impose the Lorentz condition on the operator of the electromagnetic potential. Imposing this condition on quantum states of the electromagnetic field [16,17] is not sufficient to cancel unphysical contributions to its fluctuations, except in the time-normally-ordered representation (termed in [1][2][3] …”
Section: Introductionmentioning
confidence: 99%
“…Papers [1][2][3] were intended predominantly for the quantum-optical community; our goal was in particular to "market" QFT methods to quantum opticians. Here our goal is the opposite: we wish to apply wisdom acquired in quantum optics to QFT.…”
The connection between real-time quantum field theory (RTQFT) [see, e.g., A. Kamenev and A. Levchenko, Advances in Physics 58 (2009) 197] and phase-space techniques [E. Wolf and L. Mandel, Optical Coherence and Quantum Optics (Cambridge, 1995)] is investigated. The Keldysh rotation that forms the basis of RTQFT is shown to be a phase-space mapping of the quantum system based on the symmetric (Weyl) ordering. Following this observation, we define generalised Keldysh rotations based on the class of operator orderings introduced by Cahill and Glauber [Phys. Rev. 177 (1969) Furthermore, we argue that response transformation is especially suited for RTQFT formulation of spatial, in particular, relativistic, problems, because it extends cancellation of zero-point fluctuations, characteristic of the normal ordering, to interacting fields. As an example, we consider quantised electromagnetic field in the Dirac sea. In the time-normally-ordered representation, dynamics of the field looks essentially classical (fields radiated by currents), without any contribution from zero-point fluctuations. For comparison, we calculate zero-point fluctuations of the interacting electromagnetic field under orderings other than time-normal. The resulting expression is physically inconsistent: it does not obey the Lorentz condition, nor Maxwell's equations.
“…An attempt to apply methods of real-time QFT to quantum optics was made by Vinogradov and Stenholm [32]. Generalisation of the conventional time-normal operator ordering [12][13][14] beyond the resonance approximation, making it applicable in relativity, was introduced in [2] for bosons and [3] for fermions.…”
Section: Response Representation)mentioning
confidence: 99%
“…Here our goal is the opposite: we wish to apply wisdom acquired in quantum optics to QFT. The result of this paper in a nutshell is that, firstly, the nonequilibrium real-time QFT is nothing but the nonlinear quantum response problem formulated in phase-space terms, and, secondly, that the most natural physical picture emerges if using the phase-space mapping based on the so-called time-normal operator ordering [2,[12][13][14]. Moreover, in relativistic quantum electrodynamics (QED), mappings based on other orderings (e.g., the Keldysh rotation [11,15]) lead to inconsistencies, due to one's well-known inability to impose the Lorentz condition on the operator of the electromagnetic potential.…”
Section: Introductionmentioning
confidence: 99%
“…In papers [1][2][3], we introduced response transformation of quantum kinematics. In paper [4], response transformation was extended to the key technical tool of quantum field theory (QFT), Wick's theorem [5][6][7][8].…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, in relativistic quantum electrodynamics (QED), mappings based on other orderings (e.g., the Keldysh rotation [11,15]) lead to inconsistencies, due to one's well-known inability to impose the Lorentz condition on the operator of the electromagnetic potential. Imposing this condition on quantum states of the electromagnetic field [16,17] is not sufficient to cancel unphysical contributions to its fluctuations, except in the time-normally-ordered representation (termed in [1][2][3] …”
Section: Introductionmentioning
confidence: 99%
“…Papers [1][2][3] were intended predominantly for the quantum-optical community; our goal was in particular to "market" QFT methods to quantum opticians. Here our goal is the opposite: we wish to apply wisdom acquired in quantum optics to QFT.…”
The connection between real-time quantum field theory (RTQFT) [see, e.g., A. Kamenev and A. Levchenko, Advances in Physics 58 (2009) 197] and phase-space techniques [E. Wolf and L. Mandel, Optical Coherence and Quantum Optics (Cambridge, 1995)] is investigated. The Keldysh rotation that forms the basis of RTQFT is shown to be a phase-space mapping of the quantum system based on the symmetric (Weyl) ordering. Following this observation, we define generalised Keldysh rotations based on the class of operator orderings introduced by Cahill and Glauber [Phys. Rev. 177 (1969) Furthermore, we argue that response transformation is especially suited for RTQFT formulation of spatial, in particular, relativistic, problems, because it extends cancellation of zero-point fluctuations, characteristic of the normal ordering, to interacting fields. As an example, we consider quantised electromagnetic field in the Dirac sea. In the time-normally-ordered representation, dynamics of the field looks essentially classical (fields radiated by currents), without any contribution from zero-point fluctuations. For comparison, we calculate zero-point fluctuations of the interacting electromagnetic field under orderings other than time-normal. The resulting expression is physically inconsistent: it does not obey the Lorentz condition, nor Maxwell's equations.
We analyse nonperturbatively signal transmission patterns in Green's functions of interacting quantum fields. Quantum field theory is re-formulated in terms of the nonlinear quantum-statistical response of the field. This formulation applies equally to interacting relativistic fields and nonrelativistic models. Of crucial importance is that all causality properties to be expected of a response formulation indeed hold. Being by construction equivalent to Schwinger's closed-time-loop formalism, this formulation is also shown to be related naturally to both Kubo's linear response and Glauber's macroscopic photodetection theories, being a unification of the two with generalisation to the nonlinear quantum-statistical response problem. In this paper we introduce response formulation of bosons; response reformulation of fermions will be subject of a separate paper.
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