Plasma Spectroscopy: The Influence of Microwave and Laser Fields

Plasma Spectroscopy: The Influence of Microwave and Laser Fields
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等离子体光谱:微波和激光场的影响

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发表时间:
1995
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通讯作者:
E. Oks
E. Oks
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作者:
E. Oks

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1. 介绍。- 2。量子系统准能态计算的解析方法。- 2.1量子系统与非平稳场的相互作用。- 2.2简并量子系统量子点的微扰理论。- 2.2.1作为平稳问题的质量问题的计算。- 2.2.2微扰理论。- 2.3高频或强非平稳场。- 2.3.1作为平稳问题的质量问题的计算。- 2.3.2微扰理论。- 2.3.3概括。- 3。一维准单色电场(QEF)对库仑发射体的作用。- 3.1单模QEF中类氢谱线的分裂。- 3.1.1分析性调查。- 3.1.2数值计算。半宽度和强度的振荡行为。- 3.1.3多普勒展宽。QEFs下汤姆逊散射的形式类比。- 3.2多模QEF中类氢谱线的分裂。- 3.2.1接近无穷且等于2的模态数的分析研究。- 3.2.2数值计算。- 3.3类氢谱线的影响展宽。- 3.3.1因质素评估而扩大影响的修订。- 3.3.2修正qef因冲击扩大引起的线分裂。- 3.4类氢发射器与共振激光场和低频QEF相互作用的频率积分辐射特性。- 3.4.1共振多量子相互作用。- 3.4.2非简并情况。- 3.4.3退化情况。- 3.4.4结果的应用。- 4。多维动态电场对库仑发射体的作用。- 4.1平面极化QEF中类氢谱线的分裂。- 4.1.1圆偏振场的分析结果。- 4.1.2椭圆偏振场中的多量子动态共振。- 4.1.3高频限制下的椭圆极化场。- 4.1.4椭圆偏振场参数的测量。- 4.1.5二维多模QEFs的分析研究。- 4.2 QEF和准静态EF对类氢谱线的共同作用。- 4.2.1动态共振。- 4.2.2多量子动态共振和远离共振的类氢谱线。- 4.2.3 L?共振失谐谱线。4.2.4共振效应导致氢光谱线下降。- 4.2.5 stark内光谱。诊断建议。- 4.3具有准静态电磁场的高频或强量子电磁场中的类氢谱线。- 4.3.1准能态的计算。- 4.3.2 L?L ?和H ?行配置文件。- 4.3.3静电磁场作用的进一步概括。- 5所示。一维QEF对非库仑发射体的作用。- 5.1由量子电磁场非共振作用引起的偶极子禁止谱线卫星(三能级方案)。- 5.1.1狄拉克摄动理论。测量QEF参数的Baranger-Mozer方法。- 5.1.2卫星绝热理论和QEF参数测量的准局部方法。- 5.1.3卫星极化。- 5.1.4极强量子电磁场中卫星分布的强不对称性。- 5.1.5单重态和三重态混合对类氦离子卫星的修饰。5.1.6随机QEF中的卫星。- 5.2共振量子电磁场中偶极子禁止谱线的卫星。三级计划。- 5.2.1两级子系统中的多量子共振。- 5.2.2在多量子共振中自发跃迁到第三能级的频谱。- 5.3更复杂(四能级)系统中偶极禁止谱线的卫星。- 5.3.1三电平子系统在高频或强场中的量子质量。- 5.3.2类氢离子在高频或强场中2P1/2、2S1/2、2P3/2态的辐射跃迁。- 5.4与强相干辐射相互作用的等离子体中的电子振荡位移。- 5.4.1直线轨迹近似中的计算。- 5.4.2计算包括曲线轨迹。- 5.4.3讨论。- 5.5 QEFs对双原子极性分子的作用。- 5.5.1振动-旋转光谱中的卫星。- 5.5.2低温等离子体中弱量子电磁场的超灵敏激光诱导荧光测量。- 5.6与共振激光场和低频QEF相互作用的非柱发射器的频率积分辐射特性。- 6所示。多维动态电场下的非库仑发射体(椭圆极化QEFs准静态QEF + QEF)。- 6.1由椭圆极化QEF引起的偶极禁止谱线的卫星。- 6.1.1三电平方案,非谐振QEF。- 6.1.2三电平方案,谐振QEF。—6.1.3四级方案。- 6.2 QEF和质内准静态EF对非库仑发射体的联合作用。- 6.2.1准静态EF对偶极子禁线卫星的强烈影响。- 6.2.2 stark内光谱。- 6.2.3准静态电磁场和高频量子电磁场对类氢离子的联合作用。精细结构和兰姆位移。低频等离子体湍流振幅角分布的局部测量。- 6.3椭圆极化QEF中双原子极性分子谱线的移动。- 7所示。理论在实验等离子体诊断中的应用。—7.1备注。- 7.2个QEFs ?- 7.2.1磁场湮灭下的QEFs。- 7.2.2快速压缩下的QEFs箍缩等离子体。7.3 QEFs在Z-Pinch。- 7.4高密度等离子体引起的斯塔克内光谱的新特征。-托卡马克有7.5个qf。- 7.5.1 T-10托卡马克边缘等离子体的强电场- 7.5.2托卡马克电子束的新型光谱诊断。- 7.6与强微波场相互作用的等离子体QEFs。- 7.6.1利用氢或氘管线的技术。- 7.6.2利用非库仑发射线的准局部测量技术。- 7.6.3局部激光荧光诊断技术。——附录。双色EF中氢原子的广义量子阱。束缚电子对Langmuir振荡频率和阻尼的影响。——引用。
1. Introduction.- 2. Analytical Methods for the Calculation of Quasienergy States (QS) of Quantum Systems.- 2.1 Interaction of Quantum Systems with a Nonstationary Field.- 2.2 Perturbation Theory for QSs of Degenerate Quantum Systems.- 2.2.1 Calculation of the QSs as a Stationary Problem.- 2.2.2 Perturbation Theory.- 2.3 High-Frequency or Very Intense Nonstationary Fields.- 2.3.1 Calculation of the QSs as a Stationary Problem.- 2.3.2 Perturbation Theory.- 2.3.3 Generalizations.- 3. Action of One-Dimensional Quasimonochromatic Electric Fields (QEF) on Coulomb Emitters.- 3.1 Splitting of Hydrogen-like Spectral Lines in a Single-Mode QEF.- 3.1.1 Analytical Investigation.- 3.1.2 Numerical Calculations. Oscillatory Behavior of Halfwidths and Intensities.- 3.1.3 Doppler Broadening. Formal Analogy with Thomson Scattering in the Presence of QEFs.- 3.2 Splitting of Hydrogen-like Spectral Lines in a Multimode QEF.- 3.2.1 Analytical Investigation for the Number of Modes Approaching Infinity, and Equal to 2.- 3.2.2 Numerical Calculations.- 3.3 Impact Broadening of Hydrogen-like Spectral Lines.- 3.3.1 Modifications of Impact Broadening Due to QEF.- 3.3.2 Modification of QEF-induced Line Splitting Due to Impact Broadening.- 3.4 Frequency-integrated Radiative Characteristics of Hydrogen-like Emitters Interacting with a Resonant Laser Field and a Low-Frequency QEF.- 3.4.1 Resonant Multiquantum Interaction.- 3.4.2 Non-Degenerate Case.- 3.4.3 Degenerate Case.- 3.4.4 Applications of the Results.- 4. Action of Multidimensional Dynamic Electric Fields on Coulomb Emitters.- 4.1 Splitting of Hydrogen-like Spectral Lines in a Plane Polarized QEF.- 4.1.1 Analytical Results for a Circularly Polarized Field.- 4.1.2 Multiquantum Dynamic Resonance in an Elliptically Polarized Field.- 4.1.3 Elliptically Polarized Fields in the High-Frequency Limit.- 4.1.4 Measurements of Elliptically Polarized Field Parameters.- 4.1.5 Analytical Investigation of Two-Dimensional Multimode QEFs.- 4.2 Joint Action of QEF and Quasistatic EF on Hydrogen-like Spectral Lines.- 4.2.1 Dynamic Resonance.- 4.2.2 Hydrogen-like Lines at a Multiquantum Dynamic Resonance and Away from the Resonance.- 4.2.3 The L? Spectral Line with Detuning from Resonance.- 4.2.4 Dips in Hydrogen Spectral Lines Resulting from the Resonance Effects.- 4.2.5 Intra-Stark Spectroscopy. Diagnostic Recommendations.- 4.3 Hydrogen-like Spectral Lines in a High-Frequency or Strong QEF with a Quasistatic EF.- 4.3.1 Calculation of Quasienergy States.- 4.3.2 Calculations of the L?, L? and H? Line Profiles.- 4.3.3 Further Generalizations for the Action of a Static Magnetic Field.- 5. Action of a One-Dimensional QEF on Non-Coulomb Emitters.- 5.1 Satellites of Dipole-Forbidden Spectral Lines Caused by a Nonresonant Action of QEFs (Three-Level Scheme).- 5.1.1 Dirac Perturbation Theory. Baranger-Mozer Method for Measurements of QEF Parameters.- 5.1.2 Adiabatic Theory of Satellites and Quasilocal Method for Measurements of QEF Parameters.- 5.1.3 Polarization of Satellites.- 5.1.4 Strong Asymmetry of Satellite Distribution in Very Intense QEFs.- 5.1.5 Modification of Helium-like Ion Satellites Caused by Mixing of Singlet and Triplet Terms.- 5.1.6 Satellites in a Stochastic QEF.- 5.2 Satellites of Dipole-Forbidden Spectral Lines in Resonant QEFs. Three-Level Scheme.- 5.2.1 Multiquantum Resonance in a Two-Level Subsystem.- 5.2.2 Spectrum of Spontaneous Transitions to a Third Level in a Multiquantum Resonance.- 5.3 Satellites of Dipole-Forbidden Spectral Lines in More Complicated (Four-Level) Systems.- 5.3.1 QSs of a Three-Level Subsystem in a High-Frequency or Intense Field.- 5.3.2 Radiative Transitions from the States 2P1/2, 2S1/2, 2P3/2 of a Hydrogen-like Ion in a High-Frequency or Intense Field.- 5.4 Electron Oscillatory Shift in Plasmas Interacting with a Powerful Coherent Radiation.- 5.4.1 Calculation in the Rectilinear Trajectories Approximation.- 5.4.2 Calculations Including Curved Trajectories.- 5.4.3 Discussion.- 5.5 Action of QEFs on Diatomic Polar Molecules.- 5.5.1 Satellites in Vibrational-Rotational Spectra.- 5.5.2 Ultra-sensitive Laser Induced Fluorescence Measurements of Weak QEFs in Low-Temperature Plasmas.- 5.6 Frequency-Integrated Radiative Characteristics of Non-Coloumb Emitters Interacting with a Resonant Laser Field and Low-Frequency QEF.- 6. Non-Coulomb Emitters Under Multidimensional Dynamic EFs (Elliptically Polarized QEFs Quasistatic EF plus QEF).- 6.1 Satellites of Dipole-Forbidden Spectral Lines Caused by an Elliptically Polarized QEF.- 6.1.1 Three-Level Scheme, Nonresonant QEF.- 6.1.2 Three-Level Scheme, Resonant QEF.- 6.1.3 Four-Level Scheme.- 6.2 Joint Action of QEF and Intraplasmic Quasistatic EF on Non-Coulomb Emitters.- 6.2.1 Strong Influence of a Quasistatic EF on Satellites of Dipole-Forbidden Lines.- 6.2.2 Intra-Stark Spectroscopy.- 6.2.3 Joint Action of a Quasistatic EF and a High-Frequency QEF on a Hydrogen-like Ion. Fine Structure and Lamb Shift. Local Measurements of Amplitude Angular Distributions of Low-Frequency Plasma Turbulence.- 6.3 Shift of Spectral Lines of Diatomic Polar Molecules in an Elliptically Polarized QEF.- 7. Applications of the Theory to Experimental Plasma Diagnostics.- 7.1 Preliminary Remarks.- 7.2 QEFs in ?-Pinches.- 7.2.1 QEFs Under a Magnetic Field Annihilation.- 7.2.2 QEFs Under a Rapid Compression of a ?-Pinch Plasma.- 7.3 QEFs in a Z-Pinch.- 7.4 New Features of Intra-Stark Spectroscopy Caused by a High Density of Plasmas.- 7.5 QEFs in Tokamaks.- 7.5.1 Intense EFs in the Edge Plasma of the T-10 Tokamak.- 7.5.2 Novel Spectroscopic Diagnostics of EFs in Tokamaks.- 7.6 QEFs in Plasmas Interacting with a Strong Microwave Field.- 7.6.1 Technique Utilizing Hydrogen or Deuterium Lines.- 7.6.2 Quasilocal Measurements Technique Utilizing Lines of Non-Coulomb Emitters.- 7.6.3 Techniques of Local Laser Fluorescence Diagnostics.- Appendices.- D Generalized QSs of a Hydrogen Atom in a Bichromatic EF.- E Influence of Bound Electrons on the Frequency and Damping of Langmuir Oscillations.- References.