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Journal of Physics B Atomic Molecular and Optical Physics

Jaynes–Cummings theory out of the box

Elizabeth Groves, B. D. Clader, Joseph H. Eberly

Published Nov 7, 2013• 8 citations
Publisher

Abstract

We report new results in neoclassical quantum optics by applying the central theme of the Jaynes–Cummings paper of 1963. This theme, which Jaynes and Cummings emphasized in several ways, is the key role that must be assigned to radiative back reaction in quantum radiation dynamics. Its consequences are well known in subjects related to cavity quantum electrodynamics, and its influence on optical pulse evolution theory is equally strong. Here we provide a new solitonic extension of the radiation reaction theme to short-pulse broad-bandwidth propagation theory. We report a single formula encapsulating a three-pulse scenario in which the stable imprint of signal-pulse coherence, placed in an atomic medium at a predictable location by an initial pulse pair, is subsequently transferred by a third pulse to a different location. This is analysed by reference to our new analytic solution of the nonlinearly coupled density matrix equations that incorporate the radiation reaction fields obtained from the Maxwell equations for the pulses in the atomic medium.

DOI
10.1088/0953-4075/46/22/224005

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The Jaynes-Cummings paper treats the problem of one-atom interacting with one cavity mode with two alternative theories: quantum electrodynamics and semiclassical theory, and compares the predictions. The semiclassical theory was later extended to treat a single atom in free space interacting with a classical field including radiation reaction. The resulting theory was called Neoclassical theory, and is described by nonlinear optical Bloch equations. These nonlinear equations have shown up in a number of physical systems and were the subject of the famous Jaynes-Franken bet that was a prominent feature of the early Rochester Coherence and Quantum Optics Conferences. We will touch on all of these topics in a historical review.

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Some aspects of cavity quantum electrodynamics

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We have in this thesis looked at two very different problems related to quantum optics. In Part I we have studied the Jaynes-Cummings model with cavity damping and a thermal background. To give an introduction to the field we started Chapter 2 by repeating how one in general derives the master equations for a system coupled to a reservoir. We then repeat the Jaynes-Cummings model and show extensions of the Jaynes-Cummings model where cavity-damping and a thermal background are taken into account. We proceed, in Chapter 3, by finding an analytical solution to the Jaynes-Cummings model with cavity damping in a thermal background when there is no detuning in the system, i.e. we have resonance between the energy of the photons in the cavity and the energy difference in the excited and ground state of the atom. We derive analytical expressions for P+(t), the probability of finding the atom in an excited state after some transition time t given that the atom was prepared in an excited state, and P++(t), the probability of finding the atom in an excited state after some transition time t when a previous atom was measured to be in the excited state. Both atoms where initially prepared in the excited state. We also, in Section 3.7 make use of the Poisson summation formula to rewrite the analytical solution P+(t) in terms of a Fourier series, from which we can predict the location of the revivals in the system. In Section 3.8 we derive stationary results, i.e. when the transition time t→∞, for the probabilities P+(t) and P++(t) and the mean number of photons ‹ n(t) › in the cavity. From our analytical results one is, for instance, led to believe that the probability P+(t) approaches 0 as the transitiontime increases, when it in reality approaches the value nb/(1 + 2nb). The results of our study of the extended Jaynes-Cummings model is presented in the article “Macroscopic Interference Effects in Resonant Cavities” and is published in Physica Scripta [5]. The article is reprinted as Article 1 at the end of this thesis. In Chapter 4 we present the result of a numerical solution of the Jaynes-Cummings model with cavity damping in a thermal background. Here we consider both the resonant case and also the case where detuning is present in the system. When we compare our numerical simulation with our analytical solutions we find that the correlation between the two are close to 1, at least when experimental values of Walther et al. [22] and Brune et al. [15, 16] are used. We also present some figures that show how the revival times and probabilities previously discussed is affected by detuning. In Section 4.2 we find an analytical formula for the revival time where detuning is embedded. In Chapter 4 we also, shortly, discuss how the detuning changes the effective number of photons in the cavity and what criteria should be present in order to separate the revival times.In Part II we study some aspects of quantum mechanical phase. We start, in Section 5.1, by repeating the definition and some results of the Susskind-Glogower phase operator. We then turn our attention to the Pegg-Barnett phase operator [26, 27, 28] in Section 5.4. We describe how to evaluate expectation-values and variances of the Pegg-Barnett phase. In Section 5.5 we establish an upper and lower bound on the phase based on the Pegg-Barnett phase description.In Section 5.9 we repeat some details of a new formalism of the phase which we have conveniently called the NFM-formalism after its inventors Noh, Foug`eres and Mandel [29, 30, 31]. We then describe how to find expectation-values using the Pegg-Barnett phase operator definition applied to the NFM-experiment described in Section 5.9. Our work on the quantum mechanical phase operator is presented in the paper “On the Quantum Phase Operator for Coherent States” and is published in Physica Scripta [6]. This paper is reprinted as Article II at the end of this thesis.

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Neoclassicism challenges QED

Some physicists are questioning the necessity of quantum electrodynamics in quantum optics and perhaps elsewhere. A lively discussion on possible alternatives developed during the Third Rochester Conference on Coherence and Quantum Optics at the end of June. The most widely discussed alternative was the neoclassical theory of Edwin Jaynes and his collaborators (Washington University in St. Louis). This theory regards the Maxwell equations as describing the radiation field while the Schrödinger equation is applied to the atoms. The charge and current sources of the Maxwell field are taken to be given by the corresponding probability densities of wave mechanics. Jaynes contends that these nonlinear equations describe physical phenomena better than has been appreciated in earlier times.

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Self-Consistent Radiation Reaction in Quantum Optics – Jaynes' Influence and a New Example in Cavity QED

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. It is pointed out that the self-consistent treatment of radiation reaction is a common feature of many Ph.D. theses of E. T. Jaynes' students and “grandstudents” in the 30-year period 1962 - 1992. In this way they are all descended from Microwave Laboratory Report 502, written by Jaynes at Stanford in 1958. A number of examples are described briefly, and a new example that extends the framework laid down in M. L. 502 is presented. Microwave Laboratory Report 502 In 1958 E. T. Jaynes wrote a paper entitled Some Aspects of Maser Theory that was issued as Microwave Laboratory Report No. 502 at Stanford University. The cover of the report is shown in Fig. 1. In the Abstract of M. L. 502 Jaynes identified the work as an examination of the relation between quantum electrodynamics and the semiclassical theory of radiation. M. L. 502 was intended to serve as a preliminary step in a study of the ultimate limitations on noise figure and frequency stability in molecular-beam masers. The Abstract says, among other things, that “the semiclassical theory, as extended here, is a far more reliable means of calculating radiation processes than usually supposed.” In the present author's view, M. L. 502 reported the first examination of dynamical questions that are now associated with the field of cavity quantum electrodynamics.

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Coherence and Quantum Optics V: Proceedings of the Fifth Rochester Conference on Coherence and Quantum Optics held at the University of Rochester, June 13–15, 1983

Joseph H. Eberly, L. Mandeļ, E. Wolf

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•Jan 9, 2014•0 citations

Weinberg’s nonlinear wave mechanics

K. Wódkiewicz, Marlan O. Scully

From Weinberg's nonlinear wave equation we derive the nonlinear generalization of the optical Bloch equations with radiative damping. We compare these equations with Fermi's nonlinear radiation-reaction theory and with Jaynes's neoclassical theory. The nonlinear constant \ensuremath{\epsilon}, which is small if compared to the binding energy per nucleon, can be comparable to the radiative lifetime of an excited state of an ion stored in an ion trap. We show that in such a case the nonlinear modification of the optical Bloch equations can lead to large-scale effects in coherent transients, in atomic quantum jumps, and in resonance fluorescence and can modify the emission line shape.

Physical Review A•Nov 1, 1990•59 citations
We report new results in neoclassical quantum optics by applying the central theme of the Jaynes–Cummings paper of 1963. This theme, which Jaynes and Cummings emphasized in several ways, is the key role that must be assigned to radiative back reaction in quantum radiation dynamics. Its consequences are well known in subjects related to cavity quantum electrodynamics, and its influence on optical pulse evolution theory is equally strong. Here we provide a new solitonic extension of the radiation reaction theme to short-pulse broad-bandwidth propagation theory. We report a single formula encapsulating a three-pulse scenario in which the stable imprint of signal-pulse coherence, placed in an atomic medium at a predictable location by an initial pulse pair, is subsequently transferred by a third pulse to a different location. This is analysed by reference to our new analytic solution of the nonlinearly coupled density matrix equations that incorporate the radiation reaction fields obtained from the Maxwell equations for the pulses in the atomic medium.
The Jaynes-Cummings paper treats the problem of one-atom interacting with one cavity mode with two alternative theories: quantum electrodynamics and semiclassical theory, and compares the predictions. The semiclassical theory was later extended to treat a single atom in free space interacting with a classical field including radiation reaction. The resulting theory was called Neoclassical theory, and is described by nonlinear optical Bloch equations. These nonlinear equations have shown up in a number of physical systems and were the subject of the famous Jaynes-Franken bet that was a prominent feature of the early Rochester Coherence and Quantum Optics Conferences. We will touch on all of these topics in a historical review.
We have in this thesis looked at two very different problems related to quantum optics. In Part I we have studied the Jaynes-Cummings model with cavity damping and a thermal background. To give an introduction to the field we started Chapter 2 by repeating how one in general derives the master equations for a system coupled to a reservoir. We then repeat the Jaynes-Cummings model and show extensions of the Jaynes-Cummings model where cavity-damping and a thermal background are taken into account. We proceed, in Chapter 3, by finding an analytical solution to the Jaynes-Cummings model with cavity damping in a thermal background when there is no detuning in the system, i.e. we have resonance between the energy of the photons in the cavity and the energy difference in the excited and ground state of the atom. We derive analytical expressions for P+(t), the probability of finding the atom in an excited state after some transition time t given that the atom was prepared in an excited state, and P++(t), the probability of finding the atom in an excited state after some transition time t when a previous atom was measured to be in the excited state. Both atoms where initially prepared in the excited state. We also, in Section 3.7 make use of the Poisson summation formula to rewrite the analytical solution P+(t) in terms of a Fourier series, from which we can predict the location of the revivals in the system. In Section 3.8 we derive stationary results, i.e. when the transition time t→∞, for the probabilities P+(t) and P++(t) and the mean number of photons ‹ n(t) › in the cavity. From our analytical results one is, for instance, led to believe that the probability P+(t) approaches 0 as the transitiontime increases, when it in reality approaches the value nb/(1 + 2nb). The results of our study of the extended Jaynes-Cummings model is presented in the article “Macroscopic Interference Effects in Resonant Cavities” and is published in Physica Scripta [5]. The article is reprinted as Article 1 at the end of this thesis. In Chapter 4 we present the result of a numerical solution of the Jaynes-Cummings model with cavity damping in a thermal background. Here we consider both the resonant case and also the case where detuning is present in the system. When we compare our numerical simulation with our analytical solutions we find that the correlation between the two are close to 1, at least when experimental values of Walther et al. [22] and Brune et al. [15, 16] are used. We also present some figures that show how the revival times and probabilities previously discussed is affected by detuning. In Section 4.2 we find an analytical formula for the revival time where detuning is embedded. In Chapter 4 we also, shortly, discuss how the detuning changes the effective number of photons in the cavity and what criteria should be present in order to separate the revival times.In Part II we study some aspects of quantum mechanical phase. We start, in Section 5.1, by repeating the definition and some results of the Susskind-Glogower phase operator. We then turn our attention to the Pegg-Barnett phase operator [26, 27, 28] in Section 5.4. We describe how to evaluate expectation-values and variances of the Pegg-Barnett phase. In Section 5.5 we establish an upper and lower bound on the phase based on the Pegg-Barnett phase description.In Section 5.9 we repeat some details of a new formalism of the phase which we have conveniently called the NFM-formalism after its inventors Noh, Foug`eres and Mandel [29, 30, 31]. We then describe how to find expectation-values using the Pegg-Barnett phase operator definition applied to the NFM-experiment described in Section 5.9. Our work on the quantum mechanical phase operator is presented in the paper “On the Quantum Phase Operator for Coherent States” and is published in Physica Scripta [6]. This paper is reprinted as Article II at the end of this thesis.
Some physicists are questioning the necessity of quantum electrodynamics in quantum optics and perhaps elsewhere. A lively discussion on possible alternatives developed during the Third Rochester Conference on Coherence and Quantum Optics at the end of June. The most widely discussed alternative was the neoclassical theory of Edwin Jaynes and his collaborators (Washington University in St. Louis). This theory regards the Maxwell equations as describing the radiation field while the Schrödinger equation is applied to the atoms. The charge and current sources of the Maxwell field are taken to be given by the corresponding probability densities of wave mechanics. Jaynes contends that these nonlinear equations describe physical phenomena better than has been appreciated in earlier times.
. It is pointed out that the self-consistent treatment of radiation reaction is a common feature of many Ph.D. theses of E. T. Jaynes' students and “grandstudents” in the 30-year period 1962 - 1992. In this way they are all descended from Microwave Laboratory Report 502, written by Jaynes at Stanford in 1958. A number of examples are described briefly, and a new example that extends the framework laid down in M. L. 502 is presented. Microwave Laboratory Report 502 In 1958 E. T. Jaynes wrote a paper entitled Some Aspects of Maser Theory that was issued as Microwave Laboratory Report No. 502 at Stanford University. The cover of the report is shown in Fig. 1. In the Abstract of M. L. 502 Jaynes identified the work as an examination of the relation between quantum electrodynamics and the semiclassical theory of radiation. M. L. 502 was intended to serve as a preliminary step in a study of the ultimate limitations on noise figure and frequency stability in molecular-beam masers. The Abstract says, among other things, that “the semiclassical theory, as extended here, is a far more reliable means of calculating radiation processes than usually supposed.” In the present author's view, M. L. 502 reported the first examination of dynamical questions that are now associated with the field of cavity quantum electrodynamics.
W1 Resonant Pulse Propagation I.- W1-1 Some Nonlinear Properties of Pulse Propagation.- W1-2 Self-Induced Transparency in the Broadline and Narrowline Limits and Applications.- W1-3 Observation of Zero-Degree Pulse Propagation in a Resonant Medium.- W1-4 Higher Conservation Laws and Coherent Pulse Propagation.- W2 Quantum Electrodynamics and Alternative Theories I.- W2-1 Survey of the Present Status of Neoclassical Radiation Theory.- W2-2 A Test of Jaynes' Neoclassical Theory: Incoherent Resonance Fluorescence from a Coherently Excited State.- W2-3 Experimental Limitations to the Validity of Semiclassical Radiation Theories.- W2-4 Time Delay Statistics of Photoelectric Emissions: An Experimental Test of Classical Radiation Theory.- W3 Coherence Effects in Spontaneous Emission I.- W3-1 Non-Linear Radiation Reaction.- W3-2 Master Equations in the Theory of Incoherent and Coherent Spontaneous Emission.- W3-3 Influence of Resonant Frequency Shifts on Superradiant Damping.- W3-4 Spontaneous Emission Rate in the Presence of a Mirror.- W4 Coherence I.- W4-1 Atomic Coherent States in Quantum Optics.- W4-2 Coherent States in Modern Physics.- W4-3 Debye Representation and Multipole Expansion of the Quantized Free Electromagnetic Field.- W4-4 Volume of Coherence.- T1 Quantum Electrodynamics and Alternative Theories II.- T1-1 A Quantum Treatment of Spontaneous Emission without Photons.- T1-2 Finite Quantum and Classical Electrodynamics.- T1-3 The Use of Classical Solutions in Quantum Optics.- T1-4 Raman Effect in Semiclassical Theory.- T2 Light Scattering I.- T2-1 Theory of Resonant Light Scattering Processes in Solids.- T2-2 A Generalized Extinction Theorem and Its Role in Scattering Theory.- T2-3 Mode Analysis and Mode Coupling of Electromagnetic Fields in Spatially Dispersive Media.- T2-4 Amplitude Stabilization of Pulses from a Q-Switched Ruby Laser by Means of Interaction with a Non-Linear Medium.- T3 Correlation and Fluctuation Measurements.- T3-1 Two-Photon Time Distributions in Mixed Light Beams.- T3-2 Photocounting Inversion in Presence of Dead Time Effects.- T3-3 Image Reconstruction from the Modulus of the Correlation Function: A Practical Approach to the Phase Problem of Coherence Theory.- T3-4 Photon-Correlation Spectroscopy.- T3-5 Multi-Time Intervals Distributions of Photoelectrons from Stationary Pseudo-Thermal Light with Gaussian Spectrum.- T4 Light Scattering II.- T4-1 Adventures in Green's Land: Light Scattering in Anisotropic Media.- T4-2 Intensity Fluctuation Techniques in Light Scattering.- T4-3 Coherence Properties of Light through a Liquid Crystal.- T4-4 C. Non-Critical Rayleigh Scattering from Pure Liquids.- T5 Coherence Effects in Spontaneous Emission II.- T5-1 Cooperative Effects in Spontaneous Emission.- T5-2 Amplified Spontaneous Emission.- T5-3 Non-Gaussian Statistics of Superradiant Radiation from Saturated Xenon 3.5?m Laser Amplifier.- T5-4 On the Theory of Radiating Electrons.- T6 Coherent Light Interactions.- T6-1 Atomic and Molecular Spectroscopy by Saturation with Coherent Light.- T6-2 Response Functions for Strongly Driven Systems.- T6-3 Mechanism of Interaction of Picosecond Light Pulses with Matter Yielding Self-Trapping.- T6-4 Resonance Fluorescence Lineshapes with Intense Applied Fields.- T6-5 Electron Beams as Carriers of Optical Coherence.- T7 Lasers.- T7-1 Detuned Single Mode Laser and Detailed Balance.- T7-2 Tunable Raman Lasers.- T7-3 Dye Lasers: Recent Advances in Tunable Systems.- F1 Quantum Electrodynamics and Alternative Theories III.- F1-1 A Theory of Light without Photons: Implications from Fermis to Light Years.- F1-2 Blackbody Heat Capacity and Action-at-a-Distance Electrodynamics.- F1-3 The Implications of Radiative Equilibrium in Jaynes' Extension of Semiclassical Radiation Theory.- F1-4 A Quantum Electrodynamic Investigation of the Jaynes-Crisp-Stroud Approach to Spontaneous Emission.- F1-5 Critical Comments on Radiation Theory.- F2 Resonant Pulse Propagation II.- F2-1 Cooperative Phenomena in Resonant Propagation.- F2-2 Theory of Sub-Cooperation-Limit Optical Pulses in Resonant Absorbers.- F2-3 Multiple Pulse Chirping in Self-Induced Transparency.- F2-4 Coupled Superradiance Master Equations: Application to Fluctuations in Coherent Pulse Propagation in Resonant Media.- F3 Coherence II.- F3-1 The Laser-Phase Transition Analogy - Recent Developments.- F3-2 Multiple-Time-Scale Analysis of Coherent Radiation.- F3-3 Orthogonal Operators and Phase Space Distributions in Quantum Optics.- F4 Coherence Effects in Spontaneous Emission III.- F4-1 Radiation by Many Excited Atoms between Mirrors.- F4-2 Transient Coherent Emission.- F4-3 Superradiance from a System of 3-Level Particles.- F4-4 A Quantum Electrodynamic View of Superradiance as a Competition between Stimulated and Spontaneous Atomic Decay.- F5 Post Deadline Session.- F5-1 Third- and Higher-Order Intensity Correlations in Laser Light.- F5-2 Correlation Function of a Laser Beam near Threshold.- F5-3 Localization of Photons.- F5-4 Adiabatic Following and the Self-Defocusing of Light in Rubidium Vapor.- F5-5 Experimental Evidence of an X-Ray Laser.- F5-6 Quantum Theory of Photodetection and Coherence Properties of Electrons.- F5-7 Statistics of Light Scattered by Non-Gaussian Fluctuations.- F6 Quantum Noise.- F6-1 Unified Thermodynamics of Dissipative Structures and Coherence in Nonlinear Optics.- F6-2 The Approach to Thermal Equilibrium in Systems of Coupled Quantum Oscillators Initially in a Generalized Gaussian State.- F6-3 Comparison between Incoherent and Chaotic Sources: Contribution to the Study of the Origin of Bunching Effect.- F6-4 Self-Pulsing in Laser Amplification of Broadband Noise.- Author Index.
From Weinberg's nonlinear wave equation we derive the nonlinear generalization of the optical Bloch equations with radiative damping. We compare these equations with Fermi's nonlinear radiation-reaction theory and with Jaynes's neoclassical theory. The nonlinear constant \ensuremath{\epsilon}, which is small if compared to the binding energy per nucleon, can be comparable to the radiative lifetime of an excited state of an ion stored in an ion trap. We show that in such a case the nonlinear modification of the optical Bloch equations can lead to large-scale effects in coherent transients, in atomic quantum jumps, and in resonance fluorescence and can modify the emission line shape.