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In physics, specifically in quantum mechanics, a coherent state is the specific quantum state of the quantum harmonic oscillator, often described as a state which has dynamics most closely resembling the oscillatory behavior of a classical harmonic oscillator. It was the first example of quantum dynamics when Erwin Schrödinger derived it in 1926, while searching for solutions of the Schrödinger equation that satisfy the correspondence principle.〔E. Schrödinger, Der stetige Übergang von der Mikro- zur Makromechanik, ''Naturwissenschaften'' 14 (1926) 664-666.〕 The quantum harmonic oscillator and hence, the coherent states, arise in the quantum theory of a wide range of physical systems.〔J.R. Klauder and B. Skagerstam, ''Coherent States'', World Scientific, Singapore, 1985.〕 For instance, a coherent state describes the oscillating motion of a particle confined in a quadratic potential well (for an early reference, see e.g. Schiff's textbook〔L.I. Schiff, ''Quantum Mechanics'', McGraw Hill, New York, 1955.〕). These states, expressed as ''eigenvectors of the lowering operator'' and forming an ''overcomplete'' family, were introduced in the early papers of John R. Klauder, e.g. .〔J. R. Klauder, The action option and a Feynman quantization of spinor fields in terms of ordinary c-numbers, ''Ann. Physics'' 11 (1960) 123–168.〕 In the quantum theory of light (quantum electrodynamics) and other bosonic quantum field theories, coherent states were introduced by the work of Roy J. Glauber in 1963. The coherent state describes a state in a system for which the ground-state wavepacket is displaced from the origin of the system. This state can be related to classical solutions by a particle oscillating with an amplitude equivalent to the displacement. However, the concept of coherent states has been considerably generalized, to the extent that it has become a major topic in mathematical physics and in applied mathematics, with applications ranging from quantization to signal processing and image processing (see Coherent states in mathematical physics). For this reason, the coherent states associated to the quantum harmonic oscillator are sometimes referred to as ''canonical coherent states'' (CCS), ''standard coherent states'', ''Gaussian'' states, or oscillator states. == Coherent states in quantum optics == In quantum optics the coherent state refers to a state of the quantized electromagnetic field, etc.〔〔W-M. Zhang, D. H. Feng, and R. Gilmore, Coherent states: Theory and some applications, ''Rev. Mod. Phys.'' 62 (1990) 867-927.〕〔J-P. Gazeau, ''Coherent States in Quantum Physics'', Wiley-VCH, Berlin, 2009.〕 that describes a maximal kind of coherence and a classical kind of behavior. Erwin Schrödinger derived it as a "minimum uncertainty" Gaussian wavepacket in 1926, searching for solutions of the Schrödinger equation that satisfy the correspondence principle.〔 It is a minimum uncertainty state, with the single free parameter chosen to make the relative dispersion (standard deviation in natural dimensionless units) equal for position and momentum, each being equally small at high energy. Further, in contrast to the energy eigenstates of the system, the time evolution of a coherent state is concentrated along the classical trajectories. The quantum linear harmonic oscillator, and hence coherent states, arise in the quantum theory of a wide range of physical systems. They occur in the quantum theory of light (quantum electrodynamics) and other bosonic quantum field theories. While minimum uncertainty Gaussian wave-packets had been well-known, they did not attract full attention until Roy J. Glauber, in 1963, provided a complete quantum-theoretic description of coherence in the electromagnetic field.〔R.J. Glauber, Coherent and incoherent states of radiation field,''Phys. Rev.'' 131 (1963) 2766-2788.〕 In this respect, the concurrent contribution of E.C.G. Sudarshan should not be omitted,〔E.C.G. Sudarshan, Equivalence of semiclassical and quantum mechanical descriptions of statistical light beams, ''Phys. Rev. Lett.'' 10 (1963) 277-279.〕 (there is, however, a note in Glauber's paper that reads: "Uses of these states as generating functions for the -quantum states have, however, been made by J. Schwinger 〔J. Schwinger, Theory of quantized fields. III, ''Phys. Rev.'' 91 (1953) 728-740〕). Glauber was prompted to do this to provide a description of the Hanbury-Brown & Twiss experiment which generated very wide baseline (hundreds or thousands of miles) interference patterns that could be used to determine stellar diameters. This opened the door to a much more comprehensive understanding of coherence. (For more, see Quantum mechanical description.) In classical optics, light is thought of as electromagnetic waves radiating from a source. Often, coherent laser light is thought of as light that is emitted by many such sources that are in phase. Actually, the picture of one photon being in-phase with another is not valid in quantum theory. Laser radiation is produced in a resonant cavity where the resonant frequency of the cavity is the same as the frequency associated with the atomic electron transitions providing energy flow into the field. As energy in the resonant mode builds up, the probability for stimulated emission, in that mode only, increases. That is a positive feedback loop in which the amplitude in the resonant mode increases exponentially until some non-linear effects limit it. As a counter-example, a light bulb radiates light into a continuum of modes, and there is nothing that selects any one mode over the other. The emission process is highly random in space and time (see thermal light). In a laser, however, light is emitted into a resonant mode, and that mode is highly coherent. Thus, laser light is idealized as a coherent state. (Classically we describe such a state by an electric field oscillating as a stable wave. See Fig.1) The energy eigenstates of the linear harmonic oscillator (e.g., masses on springs, lattice vibrations in a solid, vibrational motions of nuclei in molecules, or oscillations in the electromagnetic field) are fixed-number quantum states. The Fock state (e.g. a single photon) is the most particle-like state; it has a fixed number of particles, and phase is indeterminate. A coherent state distributes its quantum-mechanical uncertainty equally between the canonically conjugate coordinates, position and momentum, and the relative uncertainty in phase (heuristically ) and amplitude are roughly equal—and small at high amplitude. 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「coherent states」の詳細全文を読む スポンサード リンク
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