標題: Titlebook: Elements of Quantum Optics; Pierre Meystre,Murray Sargent Textbook 19901st edition Springer-Verlag Berlin Heidelberg 1990 Laser Physics.La [打印本頁] 作者: 專家 時間: 2025-3-21 16:43
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書目名稱Elements of Quantum Optics讀者反饋
書目名稱Elements of Quantum Optics讀者反饋學科排名
作者: 變色龍 時間: 2025-3-21 22:26
Classical Nonlinear Optics,tion becomes too large for the medium to continue to respond linearly. We have already seen how a nonlinearity plays an essential role in the free electron laser pendulum equation (1.131). In another example that we discuss in detail in Chap. 6, the output intensity of a laser oscillator builds up u作者: 吹牛大王 時間: 2025-3-22 04:03
Quantum Mechanical Background,when this approach is justified and what to do when it isn’t. Unexcited systems interacting with radiation far from the system resonances can often be treated purely classically. The response of systems near and at resonance often deviates substantially from the classical descriptions. Since the las作者: ALB 時間: 2025-3-22 08:06
Mixtures and the Density Operator,the equations of motion for the probability amplitudes. However two important kinds cannot: upper to lower level decay, and more rapid decay of the electric dipole than the average level decay rate. For these two damping mechanisms, we need a more general description than can be provided by the stat作者: bifurcate 時間: 2025-3-22 09:27
CW Field Interactions,atrix is extended in a form known as the ., which treats collections of atomic responses simply. Section 5-1 deals with homogeneously-broadened media, while Sec. 5-2 includes inhomogeneous broadening. The induced polarization is used as a source in the slowly-varying Maxwell equations to yield a non作者: 易發(fā)怒 時間: 2025-3-22 16:36
Introduction to Laser Theory,interaction of radiation with two-level atoms. We consider arrangements of two or three highly reflecting mirrors that form cavities as shown in Fig. 6-1. Light in these cavities leaks out (decays to its 1/. value) in a time . where . is the frequency of the light and . is the cavity quality factor 作者: 易發(fā)怒 時間: 2025-3-22 19:53
Optical Bistability,output frequencies, imposed by the self-consistent laser equations, are compromises between the atomic and cavity natural frequencies. In this chapter, we discuss another situation involving a nonlinear medium in Fabry-Perot and ring cavities, but with two major changes: 1) the cavity output depends作者: 不可救藥 時間: 2025-3-23 00:51
Saturation Spectroscopy,ility, etc. Alternatively one can use them to study the properties of the medium that generates them. The various kinds of nonlinear spectroscopy fall into the second category. Saturation spectroscopy deals typically with the . absorption of waves passing through a medium to be studied. In the simpl作者: Longitude 時間: 2025-3-23 05:06 作者: 不自然 時間: 2025-3-23 08:23 作者: investigate 時間: 2025-3-23 10:31 作者: 無目標 時間: 2025-3-23 15:09
Field Quantization, to quantize the electromagnetic field. Such a semiclassical description is sufficient to describe most problems in quantum optics. However, there are a few notable exceptions where a classical description of the field leads to the wrong answer. These include spontaneous emission, the Lamb shift, re作者: 群島 時間: 2025-3-23 18:53
Interaction Between Atoms and Quantized Fields, with many experiments. Nevertheless several significant experiments show strong disagreements with such semiclassical theories. The present Chapter treats the atom-field interaction fully quantum mechanically, providing a basic understanding of spontaneous emission and laying the foundations for th作者: 教義 時間: 2025-3-23 23:02 作者: Dissonance 時間: 2025-3-24 03:44
Resonance Fluorescence,ontaneous emission of an atom irradiated by a continuous, monochromatic field. This emission is called .. We compute its spectrum, which is given in steady state by the Fourier transform of the first-order correlation function of the field. We also discuss the phenomenon of photon antibunching, a pu作者: judiciousness 時間: 2025-3-24 06:38
Squeezed States of Light, Δ., has a built-in degree of freedom: one can squeeze the standard deviation of one observable provided one “stretches” that for the conjugate observable. For example the position and momentum standard deviations obey the uncertainty relation . and we can squeeze Δ. to an arbitrarily small value at作者: PURG 時間: 2025-3-24 12:30
Quantum Theory of a Laser,2 – 14. So far, our treatment of quantized field-matter interactions has concentrated mostly on situations where the quantized field acts as a noise source: under these conditions the nonlinear atomic response originates from a . driving field, while the effects of the quantized modes are treated li作者: intelligible 時間: 2025-3-24 17:56 作者: 雄偉 時間: 2025-3-24 22:34
Lead users and the organizationorption. This nonlinear cavity problem can lead to two or more stable output intensities for a given input intensity, and hence belongs to a class of problems called .. In the present chapter we also see a bistable configuration that involves active media, namely the homogeneously broadened ring las作者: 陰險 時間: 2025-3-25 00:59 作者: Dappled 時間: 2025-3-25 03:22
https://doi.org/10.1007/978-3-030-41156-5t with different atoms, such as in a Doppler-broadened gaseous medium. While these can also be thought of as optical instabilities, we prefer to refer to them in the traditional way simply as multimode operation. In particular, this kind of operation can produce a periodic train of short pulses.作者: infinite 時間: 2025-3-25 10:49 作者: 骯臟 時間: 2025-3-25 14:59
Classical Electromagnetic Fields,ssical description of light and a quantum mechanical description of matter is called the . approximation. This approximation is not always justified (see Chaps. 12 through 18), but there are remarkably few cases in quantum optics where we need to quantize the field.作者: CRP743 時間: 2025-3-25 15:51
Introduction to Laser Theory,orption. This nonlinear cavity problem can lead to two or more stable output intensities for a given input intensity, and hence belongs to a class of problems called .. In the present chapter we also see a bistable configuration that involves active media, namely the homogeneously broadened ring las作者: 逃避系列單詞 時間: 2025-3-25 21:09 作者: harbinger 時間: 2025-3-26 02:03 作者: Incorruptible 時間: 2025-3-26 05:27 作者: 美色花錢 時間: 2025-3-26 09:33 作者: palliate 時間: 2025-3-26 13:49 作者: 落葉劑 時間: 2025-3-26 19:52
tro- magnetism as well as at least one, but preferably two, semesters of quan- tum mechanics. Its present form resulted from many years of teaching and research at the Max-Planck-Institut fi. ir Quantenoptik, the University of Munich, and the University of Arizona. The contents have evolved signi- f作者: Affectation 時間: 2025-3-26 21:41 作者: dissent 時間: 2025-3-27 05:11
https://doi.org/10.1007/978-3-319-92701-5ource: under these conditions the nonlinear atomic response originates from a . driving field, while the effects of the quantized modes are treated linearly. A notable exception was the Jaynes-Cummings model, where the Hamiltonian can be diagonalized exactly and hence the quantized mode is treated to all orders.作者: Urologist 時間: 2025-3-27 08:46
CW Field Interactions,linear Beer’s law for propagation. The population matrix equations of motion are solved in the important ., which assumes that the dipole lifetime .. is short compared to times for which the field envelope or population difference vary appreciably. The concepts of power-broadening and spectral hole burning are developed.作者: 噴出 時間: 2025-3-27 13:07 作者: lethargy 時間: 2025-3-27 17:12
Squeezed States of Light, the expense of accordingly increasing the standard deviation Δ .. All quantum mechanics requires is that the . be bounded from below. As discussed in Sec. 12-1, the electric and magnetic fields from a pair of observables analogous to the position and momentum of a simple harmonic oscillator. Accordingly they obey a similar uncertainty relation 作者: 縱欲 時間: 2025-3-27 17:57
Philip H. Seager,Hillel M. Maximonlitude ...(.) varies little during the time interval defined by the inverse bandwidth of the continuum of modes of the electromagnetic field, and 2) the replacement of the remaining non-local time integration in Eq. (13.58) by a .-function. These choices comprise the Weisskopf-Wigner approximation.作者: 一再煩擾 時間: 2025-3-27 22:40
Managing Media and Digital Organizationsbetween resonance fluorescence and the semiclassical probe absorption studies of Chap. 8, and lays the foundations for studying the generation of squeezed states by resonance fluorescence and four-wave mixing in Chap. 18.作者: 警告 時間: 2025-3-28 05:44 作者: certain 時間: 2025-3-28 07:38 作者: 套索 時間: 2025-3-28 13:37 作者: 水槽 時間: 2025-3-28 17:25 作者: Dysplasia 時間: 2025-3-28 20:51 作者: vanquish 時間: 2025-3-29 01:38 作者: 火光在搖曳 時間: 2025-3-29 04:42
Abiraterone for the Treatment of mCRPC, the expense of accordingly increasing the standard deviation Δ .. All quantum mechanics requires is that the . be bounded from below. As discussed in Sec. 12-1, the electric and magnetic fields from a pair of observables analogous to the position and momentum of a simple harmonic oscillator. Accordingly they obey a similar uncertainty relation 作者: Mere僅僅 時間: 2025-3-29 10:34
Textbook 19901st editiontism as well as at least one, but preferably two, semesters of quan- tum mechanics. Its present form resulted from many years of teaching and research at the Max-Planck-Institut fi. ir Quantenoptik, the University of Munich, and the University of Arizona. The contents have evolved signi- ficantly ov作者: Prostaglandins 時間: 2025-3-29 13:33 作者: Cognizance 時間: 2025-3-29 15:55
https://doi.org/10.1007/978-3-540-89272-4 do not know the state vector of the system, but rather the classical probabilities for having various possible state vectors. Such situations are described by the ., which is a sum of projectors ∣..〉〈..∣ onto the possible state vectors ∣..〉, each weighted by a classical probability ...作者: 漂浮 時間: 2025-3-29 21:39 作者: 整頓 時間: 2025-3-30 01:30 作者: 偽造 時間: 2025-3-30 07:57 作者: 清唱劇 時間: 2025-3-30 11:12
Classical Nonlinear Optics,fact that nonlinearities can couple electromagnetic field modes, transferring energy from one to another. Such processes can be used both to measure properties of the nonlinear medium and to produce useful applications such as tunable light sources.作者: 陶器 時間: 2025-3-30 14:14
Mixtures and the Density Operator, do not know the state vector of the system, but rather the classical probabilities for having various possible state vectors. Such situations are described by the ., which is a sum of projectors ∣..〉〈..∣ onto the possible state vectors ∣..〉, each weighted by a classical probability ...作者: NEX 時間: 2025-3-30 16:40 作者: 寬大 時間: 2025-3-30 23:36 作者: 加劇 時間: 2025-3-31 02:02 作者: cataract 時間: 2025-3-31 08:02 作者: 監(jiān)禁 時間: 2025-3-31 11:59 作者: BRAWL 時間: 2025-3-31 16:58
Managing Innovation and Standardstion becomes too large for the medium to continue to respond linearly. We have already seen how a nonlinearity plays an essential role in the free electron laser pendulum equation (1.131). In another example that we discuss in detail in Chap. 6, the output intensity of a laser oscillator builds up u作者: 責怪 時間: 2025-3-31 18:19
Jayaram Srinivasan,Clas Neumannwhen this approach is justified and what to do when it isn’t. Unexcited systems interacting with radiation far from the system resonances can often be treated purely classically. The response of systems near and at resonance often deviates substantially from the classical descriptions. Since the las作者: 持續(xù) 時間: 2025-4-1 00:28 作者: 吞下 時間: 2025-4-1 04:00 作者: Endoscope 時間: 2025-4-1 06:41
