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標(biāo)題: Titlebook: Coherence and Quantum Optics IV; Proceedings of the F Leonard Mandel,Emil Wolf Conference proceedings 1978 Springer Science+Business Media [打印本頁]

作者: infection    時(shí)間: 2025-3-21 18:07
書目名稱Coherence and Quantum Optics IV影響因子(影響力)




書目名稱Coherence and Quantum Optics IV影響因子(影響力)學(xué)科排名




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書目名稱Coherence and Quantum Optics IV網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Coherence and Quantum Optics IV被引頻次




書目名稱Coherence and Quantum Optics IV被引頻次學(xué)科排名




書目名稱Coherence and Quantum Optics IV年度引用




書目名稱Coherence and Quantum Optics IV年度引用學(xué)科排名




書目名稱Coherence and Quantum Optics IV讀者反饋




書目名稱Coherence and Quantum Optics IV讀者反饋學(xué)科排名





作者: magenta    時(shí)間: 2025-3-21 20:31

作者: Cardiac-Output    時(shí)間: 2025-3-22 04:01

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作者: Culmination    時(shí)間: 2025-3-22 14:29

作者: Culmination    時(shí)間: 2025-3-22 18:50

作者: carotid-bruit    時(shí)間: 2025-3-23 00:33
Resonance Fluorescence under Finite Bandwidth Excitationexperiments, the need arises for a more realistic description of the excitation field in the theory. We have generalized our earlier quantum field treatment of the problem of resonance fluorescence from a two-level atom, [1, 2] to take account of the finite bandwidth of the exciting laser field. In
作者: 吸引人的花招    時(shí)間: 2025-3-23 02:57

作者: 不容置疑    時(shí)間: 2025-3-23 06:50
Two-Level Atoms in an Intense Monochromatic Field: A Review of Recent Experimental Investigationstable tunable lasers and atomic beams. A number of researchers have measured the spectrum of the emission, and more recently, the absorption of the strongly driven atoms for both on-resonance and off-resonance excitation. In addition, the energy levels of the atoms have been carefully probed to exam
作者: 小蟲    時(shí)間: 2025-3-23 13:06
Quantum Mechanical Resonant Light Scatteringics [2]. The accuracy of the method, which relied upon an assumption of statistical factorization of atomic and emission field variables, was subsequently confirmed by theoretical analyses carried out both in the Schr?dinger picture, where solutions for the complete correlated atom-field state vecto
作者: escalate    時(shí)間: 2025-3-23 16:40
Resonance Fluorescence in 3-Level Systemsther has two lower levels each coupled to a single upper level. The atomic steady state populations and the spectrum of the scattered light are determined as a function of the various atomic and laser parameters. It is assumed that the only damping is due to spontaneous emission.
作者: 連鎖,連串    時(shí)間: 2025-3-23 19:17
Thermodynamics of a Non-Equilibrium Quantum System — Resonance Fluorescenceed little comment is that it provides a most interesting example of nonequilibrium thermodynamics in a quantum system. Conceptually the situation is simple. The two-level atom is subject to two interactions (a) a coherent interaction with a driving field, (b) an incoherent interaction with a thermal
作者: 聯(lián)邦    時(shí)間: 2025-3-23 23:56
The Theory of the Optical Autler-Tonnes Effect in Sodium Including Degeneracy and DetuningAutler-Townes theory (1955) each of the levels will be split into a doublet, the magnitude of the splitting being proportional to the square root of the intensity of the laser field. If one of the levels is connected to a third level by a second weak laser beam, the doublet structure can be probed b
作者: 專心    時(shí)間: 2025-3-24 05:16

作者: capsule    時(shí)間: 2025-3-24 08:52
Robert C. Dalang,Francesco Russo,Marco DozziNa sum-frequency generation can be described as phase matched emission from oscillating atomic quadrupole moments driven at frequency ω. = ω. + ω. by two applied fields, as shown schematically in Fig. 1. The quadrupole moment density is given by:
作者: Offensive    時(shí)間: 2025-3-24 13:17
https://doi.org/10.1007/978-1-4684-9169-2s that have been performed so far by the various groups, a comparison of the experimental results with theoretical predictions, as well as a discussion of the experimental problems in performing such measurements.
作者: encyclopedia    時(shí)間: 2025-3-24 18:16
Second-Order Sum- and Difference-Frequency Generation via Quadrupole Transitions in Atomic VaporsNa sum-frequency generation can be described as phase matched emission from oscillating atomic quadrupole moments driven at frequency ω. = ω. + ω. by two applied fields, as shown schematically in Fig. 1. The quadrupole moment density is given by:
作者: 通知    時(shí)間: 2025-3-24 21:25

作者: OREX    時(shí)間: 2025-3-25 00:18
Photon Statistics, Instabilities and Phase Transitions in Dye Lasersnderstand better the fundamentally different behavior possible in dye lasers, to develop further the differences between the second order and first order laser phase transitions analogies and to examine the role of fluctuations in phase transitions.
作者: Morbid    時(shí)間: 2025-3-25 04:15
Thermodynamics of a Non-Equilibrium Quantum System — Resonance Fluorescence reservoir (spontaneous emission into the radiation field). If the driving field were absent the atom would merely relax into equilibrium with the reservoir and the usual Wigner Weisskopf theory for a damped atom would apply. The effect of the driving field is to maintain the atom away from equilibrium in a new nonequilibrium steady state.
作者: Obloquy    時(shí)間: 2025-3-25 10:28

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作者: 積習(xí)已深    時(shí)間: 2025-3-25 21:20
E. ?inlar,K. L. Chung,J. Glover other optical transient effects which closely parallel the transients of pulsed NMR. Time-dependent interactions involving population and dipole dephasing can be examined in a selective manner and without the influence of Doppler broadening in the case of a gas, or crystalline strain broadening in the case of a solid.
作者: coagulate    時(shí)間: 2025-3-26 00:54

作者: 前奏曲    時(shí)間: 2025-3-26 08:04
The Laser — Trailblazer of Synergeticsaces. The laser-active atoms of the material are pumped energetically from the outside and emit laser light through one of the mirrors. The two mirrors form a Perot-Fabry-interferometer which allows only for those modes, whose wavelengths obey the relation (fig. 2) . (n is an integer and L is the distance between the mirrors).
作者: 山頂可休息    時(shí)間: 2025-3-26 10:50

作者: 征服    時(shí)間: 2025-3-26 16:41
Robert C. Dalang,Marco Dozzi,Francesco Russonderstand better the fundamentally different behavior possible in dye lasers, to develop further the differences between the second order and first order laser phase transitions analogies and to examine the role of fluctuations in phase transitions.
作者: 蘑菇    時(shí)間: 2025-3-26 18:27

作者: 惰性女人    時(shí)間: 2025-3-27 00:16

作者: 公豬    時(shí)間: 2025-3-27 02:39
Martin Hairer,Jonathan C. Mattinglynel junction undergoing dynamical transients first from a quantum optical and then from the common phenomenological point of view. We find that the present results differ from those obtained in the usual phenomenological fashion.
作者: GRUEL    時(shí)間: 2025-3-27 05:30

作者: bleach    時(shí)間: 2025-3-27 11:17

作者: 山崩    時(shí)間: 2025-3-27 15:52
Resonance Fluorescence under Finite Bandwidth Excitationnt under monochromatic excitation, and appear not to have been encountered in previous treatments of the problem. [4, 5] In particular, we show that the spectral density should become asymmetric under offresonance, non-monochromatic excitation.
作者: ATOPY    時(shí)間: 2025-3-27 18:13

作者: 消滅    時(shí)間: 2025-3-28 01:32
Capacity Theory and Weak Duality,troud, and Hercher’s important experiment [12] have with the more recent and precise measurements of Ezekiel and coworkers [13] and Walther and coworkers [14] amply confirmed the predictions of what is now the generally accepted theory [1].
作者: 膽汁    時(shí)間: 2025-3-28 05:17

作者: painkillers    時(shí)間: 2025-3-28 09:00
https://doi.org/10.1007/978-3-0348-7943-9tion at the combination frequency ω. = ω. + ω. ? ω. is created. The intensity generated at ω. reveals resonant interference terms of the material system at ω. + ω., ω. ? ω. and ω. ? ω., respectively. Such interference terms permit the relative nonlinearities of various two-photon absorption and Raman resonant excitations to be calibrated.
作者: defuse    時(shí)間: 2025-3-28 11:38

作者: incontinence    時(shí)間: 2025-3-28 16:20
A Diffusion First Passage Problem,el crossing experiments performed under those conditions has been given. Furthermore experiments in which the frequency distribution of the resonance radiation was analysed using a Fabry-Perot interferometer have been discussed as well as correlation experiments now under way.
作者: 鞭打    時(shí)間: 2025-3-28 22:33

作者: Meager    時(shí)間: 2025-3-28 23:58
https://doi.org/10.1007/978-3-0348-7943-9tion at the combination frequency ω. = ω. + ω. ? ω. is created. The intensity generated at ω. reveals resonant interference terms of the material system at ω. + ω., ω. ? ω. and ω. ? ω., respectively. Such interference terms permit the relative nonlinearities of various two-photon absorption and Rama
作者: hedonic    時(shí)間: 2025-3-29 03:27

作者: conscribe    時(shí)間: 2025-3-29 11:03
Martin Hairer,Jonathan C. Mattinglytion for these investigations has been the close analogy between two-level quantum optical systems and Josephson devices [3]. In particular, the angular momentum formulation of an n-atom system according to Dicke [4] has a close analogy to the corresponding problem of n-Cooper pairs interacting with
作者: 野蠻    時(shí)間: 2025-3-29 11:50

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作者: Radiculopathy    時(shí)間: 2025-3-30 02:11
Topics in Energy and Potential Theory,the total system atom + impinging photons interacting together (dressed-atom). One shows how such an approach gives a simple quantitative understanding of the behaviour of an atom irradiated by an intense resonant laser beam.
作者: 搬運(yùn)工    時(shí)間: 2025-3-30 05:35
An Inequality for Boundary Value Problems,experiments, the need arises for a more realistic description of the excitation field in the theory. We have generalized our earlier quantum field treatment of the problem of resonance fluorescence from a two-level atom, [1, 2] to take account of the finite bandwidth of the exciting laser field. In
作者: AVERT    時(shí)間: 2025-3-30 10:10
A Diffusion First Passage Problem,el crossing experiments performed under those conditions has been given. Furthermore experiments in which the frequency distribution of the resonance radiation was analysed using a Fabry-Perot interferometer have been discussed as well as correlation experiments now under way.
作者: FLORA    時(shí)間: 2025-3-30 13:30

作者: 歌曲    時(shí)間: 2025-3-30 19:29

作者: 牛的細(xì)微差別    時(shí)間: 2025-3-31 00:04
Large Deviations in Ergodic Theory,ther has two lower levels each coupled to a single upper level. The atomic steady state populations and the spectrum of the scattered light are determined as a function of the various atomic and laser parameters. It is assumed that the only damping is due to spontaneous emission.
作者: Compass    時(shí)間: 2025-3-31 02:44

作者: 節(jié)約    時(shí)間: 2025-3-31 08:15
Strict Past Conditioning at Arbitrary Times,Autler-Townes theory (1955) each of the levels will be split into a doublet, the magnitude of the splitting being proportional to the square root of the intensity of the laser field. If one of the levels is connected to a third level by a second weak laser beam, the doublet structure can be probed b
作者: 胎兒    時(shí)間: 2025-3-31 10:29
E. ?inlar,K. L. Chung,J. Gloveres, and solids. Systems which are prepared by laser light may exhibit photon echoes, free induction decay (FID), coherent Raman beats and a variety of other optical transient effects which closely parallel the transients of pulsed NMR. Time-dependent interactions involving population and dipole deph
作者: 脫水    時(shí)間: 2025-3-31 14:02
https://doi.org/10.1007/978-3-7643-8458-6Various types of coherent effects present when atoms interact with intense resonant field are considered. Relaxation and collisions are disregarded. Three- and four-level systems are investigated. As an example, the fine structure in third harmonic generation is calculated.
作者: Texture    時(shí)間: 2025-3-31 19:47

作者: 使糾纏    時(shí)間: 2025-4-1 00:13
Levy Systems and Path Decompositions,Many physical systems can be described by a potential V=V(x.,x.,...,x.). The local properties of the system are then characterized by the local properties of the potential.
作者: Radiation    時(shí)間: 2025-4-1 02:34
A Decomposition of Excessive Measures,The molecular vibration of N. is coherently excited by a single high power picosecond laser pulse via stimulated Raman scattering. With a second picosecond probe pulse the dephasing time is obtained from the intensity of the stimulated anti-Stokes Raman scattering as a function of the time delay between both laser pulses.
作者: discord    時(shí)間: 2025-4-1 09:58

作者: reject    時(shí)間: 2025-4-1 14:04
Higher Order Coherent Raman ScatteringThere has recently been much interest in the third order nonlinear light mixing, especially the process of coherent anti-Stokes (Stokes) Raman scattering — the CARS (CSRS) effect[1–4].
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作者: 刪減    時(shí)間: 2025-4-1 19:37





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