Trends in Quantum Optics∗ a Personal Perspective

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Trends in Quantum Optics∗ a Personal Perspective GENERAL ARTICLE Trends in Quantum Optics∗ A Personal Perspective Subhashish Banerjee and Arun M Jayannavar Here, we review some of the recent developments in quantum optics. After a brief introduction to the historical develop- ment of the subject, we discuss some of the modern aspects of quantum optics including atom field interactions, quantum state engineering, metamaterials and plasmonics, optomechan- ical systems, PT (parity-time) symmetry in quantum optics, as well as, quasi-probability distributions and quantum state tomography. Further, the recent developments in topological Subhashish Banerjee is a photonics is briefly discussed. The potent role of the subject physicist at the Indian in the development of our understanding of quantum physics Institute of Technology Jodhpur. His major interest is and modern technologies is highlighted. in the field of open quantum systems and also works in the fields of quantum field theory, 1. Introduction quantum optics, and quantum information. Light is intimately connected to the existence of all forms of life. The systematic study of light is known as ‘optics’ and could be traced historically to [1]. The notion of light as an electromag- netic field was made clear by Maxwell, resulting in his cele- brated work on what is now known as Maxwell equations. He showed that electromagnetic fields in vacuum propagate at the Arun M Jayannavar is a senior scientist at Institute of speed of light. The next step in the history of this subject were Physics, Bhubaneswar. He is the questions raised by the Michelson–Morley experiment and interested in general the Rayleigh–Jeans catastrophe associated with black-body radi- condensed matter physics and ation. The former lead to the development of the special theory emergent phenomena. of relativity and the later to Planck’s resolution, which provided the first seeds for the field of quantum mechanics. The notion of Keywords photon, essentially considering it as a particle, was first realized Quantum optics, metamaterials, plasmonics, optomechanical sys- ff in Einstein’s work on the photoelectric e ect. tems, parity-time symmetry. A large number of phenomena, related to optics, could be ex- ∗Vol.25, No.11, DOI: https://doi.org/10.1007/s12045-020-1075-y RESONANCE | November 2020 1559 GENERAL ARTICLE plained by invoking the concept of photons involving a classical electromagnetic field along with vacuum fluctuations. It was soon realized, in the wake of experimental developments that to under- stand the full potential of the photon, one needs to treat it quan- tum mechanically. This lead to the development of the quantum theory of radiation, which in turn, was the precursor to quantum optics [2]. The photon provides an example of a simple quantum state labelled by, say, its horizontal and vertical polarizations as: |ψi = c1 |Hi + c2 |Vi . Here, |ψi, pronounced as ket psi, denotes the state of the sys- tem and is a vector and is an example of a superposition state. Also, c1 and c2 are in general, complex numbers such that the 2 2 sum of squares of their modulus |c1| + |c2| = 1. The states |Hi 2 2 and |Vi can exist simultaneously with probabilities |c1| and |c2| , respectively. This is the surprising content of quantum mechan- In quantum mechanics, ics that makes it stand apart from classical physics. This feature we deal with operators can be used as a resource for achieving things not possible in the characterizing the classical realms. Further, it should be noted that in quantum me- observables. For example, energy is chanics, we deal with operators characterizing the observables. represented by the For example, energy is represented by the operator Hˆ called the operator Hˆ called the Hamiltonian of the system. Experiments typically involve mak- Hamiltonian of the ing measurements of the operator on the state vector and what is system. Experiments typically involve making obtained as a result of the measurement is the eigenvalue of the measurements of the operator. A simple example of measurement would be a projec- operator on the state tion operator that acts on the state of the system to be measured vector and what is and take it to the final state. A basic tenet of quantum mechanics obtained as a result of the measurement is the is that the results of the process of measurement are probabilistic eigenvalue of the in nature, and is known as the Born rule. operator. Quantum measurements are described, in general, by a collec- tion {Mm} of measurement operators, acting on the state space of the system being measured. The index m refers to the mea- surement outcomes that may occur in the experiment. If the state of the quantum system is |ψii immediately before the measure- † ment, then the probability that result m occurs is hψi|Mm Mm|ψii. 1560 RESONANCE | November 2020 GENERAL ARTICLE † Here, hψi|Mm is the Hermitian conjugate of the vector Mm|ψii. The measurement leaves the system in the state: Mm |ψii |ψii → |ψ f i = . (1) † hψi|MmMm|ψii q The measurement operators satisfy the completeness condition † m Mm Mm = ½, expressing the fact that probabilities sum up to one. For those operators M where M† = M and M2 = M , P m m m m m this reduces to the projection operators mentioned above. Quantum optics provide tools to study the foundations of quan- Quantum optics provide tum mechanics with precision and is the cause of several devel- tools to study the opments in quantum information and quantum technology. An foundations of quantum mechanics with important development in quantum optics came with the formu- precision and is the lation of coherent states [3, 4], which basically ask the question cause of several of what are the states of the field that most nearly describes a developments in classical electromagnetic field. This was originally introduced by quantum information and quantum technology. Schrödinger [5]. Classically, electromagnetic field has a well- defined amplitude and phase, a picture that changes in the quan- tum mechanical scenario. A field in a coherent state is a minimum- uncertainty state with equal uncertainties in the two variables, in this context, often termed as the two quadrature components. For example, this could relate to the standard deviation of two sets of operators, such as position and momentum. This was followed by the development of squeezed states, where fluctuations in one quadrature component are reduced below that of the correspond- ing coherent state. In the quest for characterizing the nonclassical behavior of pho- tons, anti-bunching and sub-Poissonian statistics were investigated. The coherent field is represented by Poissonian photon statistics, in which the photons tend to distribute themselves uniformly, i.e., the variance of the photon distribution is equal to its mean. In con- trast to this, in sub-Poissonian statistics, the variance is less than the mean and was, first experimentally demonstrated in [6]. The deviation from Poissonian statistics is quantified by the Mandel QM parameter, discussed below in the context of quantum cor- RESONANCE | November 2020 1561 GENERAL ARTICLE relations. A closely related albeit distinct phenomenon is that of photon antibunching. Photon bunching is the tendency of photons to distribute themselves in bunches, such that when light falls on a photodetector, more photon pairs are detected close together in time than further apart. In contrast to this, in antibunching, the probability of photon pairs detection further apart is greater than that for pairs close together. Both the phenomena of sub- Poissonian statistics and photon antibunching are purely quantum in nature. A major technological development due to quantum optics has been the development of LASER (Light Amplification by Stim- ulated Emission of Radiation), where coherent states play an es- Quantum entanglement, sential role. Quantum entanglement, which is the quintessence of which is the the quantum world, has been experimentally demonstrated with quintessence of the photons and has proved to be a potential resource in quantum quantum world, has been experimentally computation and communication. Spontaneous Parametric Down demonstrated with Conversion (SPDC) is a frequently used process in quantum op- photons and has proved tics, which is very useful for generating squeezed states, single to be a potential resource and entangled photons. in quantum computation and communication. Having sketched the roots of quantum optics, we will, in the re- maining part of this article, try to provide a flavor for some of the modern developments in the field. In this context, the fol- lowing topics will be discussed: (a) atom-field interactions, (b) quantum state engineering, (c) metamaterials and plasmonics, (d) optomechanical systems, (e) PT (Parity-Time) symmetry in quan- tum optics, (f) quasi-probability distributions and quantum state tomography, and (g) topological photonics. 2. Atom-Field Interactions A canonical model of quantum optics is the Rabi model, which deals with the response of an atom to an applied field in resonance with the atom’s natural frequency. Rabi considered the problem of a spin-half magnetic dipole undergoing precessions in a mag- netic field. He obtained the probability of a spin-half atom flip- ping from |0i = (1 0)T or |1i = (0 1)T to the states |1i or |0i, 1562 RESONANCE | November 2020 GENERAL ARTICLE respectively, by an applied radio-frequency magnetic field. Here, T stands for the transpose of the row matrix. In the context of quantum optics, Rabi oscillations would imply oscillations of the atom, considered as a two-level system, between the upper and lower levels under the influence of the electromagnetic field. The Rabi model led to the development of the well-known Jaynes– Cumming model, which is a generalization of the semi-classical Rabi model in the sense that it invokes the interaction of the atom and the single mode of the electromagnetic field in a cavity.
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