Nature Near London (Classic Reprint)

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Nature Near London

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Nature Near London

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Nature Near London, by: Richard Jefferies, Introduction By: Thomas Coke Watkins: John Richard Jefferies (6 November 1848 - 14 August 1887) Was

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Nature Near London

Książki

Sklep: KrainaKsiazek.pl

Nature Near London

Książki

Sklep: KrainaKsiazek.pl

Nature Near London

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Sklep: KrainaKsiazek.pl

Molecular Quantum Electrodynamics Dover Publications Inc.

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PrefaceChapter 1 Introduction1.1 The Nature of Electrodynamics1.2 Maxwell's Equations for the Macroscopic Field1.3 The Microscopic Field Equations1.4 The Electromagnetic Potentials1.5 Lorentz and Coulomb Gauges1.6 Quantum Mechanics of a System of Charges1.7 "Classical Electrodynamics, Quantum Electrodynamics and Semiclassical Electrodynamics"Chapter 2 The Electromagnetic Field in Free Space2.1 The Classical Electromagnetic Field in a Region Free of Sources2.2 "Electromagnetic Waves in a "Box"2.3 "Linear, Elliptical and Circular Polarization"2.4 Lagrangian and Hamiltonian for the Free Field2.5 The Electromagnetic Field as a Sum of Mode Oscillators2.6 Quantization of the Harmonic Oscillator2.7 A System of Oscillators2.8 Quantization of the Free Field2.9 Summations Over Wave Vectors and Polarizations2.10 Uncertainty Relations. Fluctuations of the Vacuum Fields2.11 Coherent States2.12 Coherent States as States of Minimum Uncertainty2.13 Thermal and Chaotic StatesChapter 3 Particles and Fields3.1 Transverse and Longitudinal d-dyadics3.2 Molecules and Fields: Lagrangian Formulation3.3 Molecules and Fields: Hamiltonian Formulation3.4 Instantaneous and Retarded Interactions3.5 Quantization of the Coupled System3.6 The Electric Dipole Approximation3.7 A Higher ApproximationChapter 4 One-Photon Absorption and Emission4.1 Introduction4.2 Time Development in a Two-State Model4.3 Time Evolution and Time-Dependent Perturbations4.4 An Application: the Steady Perturbation4.5 Time-Dependent Perturbations Treated by Dirac's Method4.6 A Discrete State Coupled to a Continuum. The Fermi Golden Rule4.7 One-Photon Absorption4.8 The Einstein B-coefficient4.9 Relaxation of the Number State Assumption4.10 The Sum Rule for Oscillator Strengths4.11 Spontaneous Emission and the Einstein A-coefficient4.12 Stimulated (Induced) Emission4.13 Magnetic Dipole and Electric Quadrupole Transitions 4.13A Magnetic dipole allowed transitions 4.13B Electric quadrupole allowed transitions 4.13C Interference effects4.14 Equivalence of Matrix Elements in Minimal Coupling and Multipolar Formalisms4.15 Calculation of the 2p ? 1s Transition in Hydrogen with the Complete Vector Potential4.16 Calculation of the Photoionization Rate of Hydrogen with the Complete Vector PotentialChapter 5 Two-Photon Absorption Emission5.1 Introduction5.2 Two-Photon Absorption From a Single Beam5.3 Two-Photon Absorption From Two Beams5.4 Selection Rules for Two-Photon Absorption and Emission5.5 Doppler-Free Spectroscopy5.6 Two-Photon Emission5.7 Two-Photon Stimulated Emission5.8 Equivalence of Two-Photo Matrix ElementsChapter 6 Rayleigh and Raman Scattering6.1 Two-Photo Scattering. The Kramers-Heisenberg Dispersion Formula6.2 Rayleigh Scattering6.3 Rayleigh Scattering by Randomly Oriented Molecules6.4 Raman Scattering6.5 Raman Intensities6.6 Stimulated and Inverse Raman ScatteringChapter 7 Interactions Between Molecules7.1 Introduction7.2 The Resonance Interaction in Electric Dipole Approximation7.3 Resonance Interaction in the Minimal Coupling Method7.4 The Dispersion Energy7.5 The Wave-zone Limit: Casimir-Polder Potential7.6 The Near-zone Limit: London Potential7.7 Dispersion Energy. The Complete Potential7.8 Interaction Between Permanent Dipoles7.9 Chiral Discrimination. The Resonance Interaction Between Chiral Systems7.10 Chiral Discrimination. Discriminatory Dispersion Interactions in the Wave-zone7.11 Discriminatory Dispersion Interactions in the Near-zone7.12 Intermolecular Interactions in a Radiation Field7.13 Radiation-induced Chiral DiscriminationChapter 8 Optical Activity8.1 Introduction8.2 Circular Dichroism8.3 Inclusion of Electric Quadrupole Interactions8.4 A Two-State Model for Optical Rotation8.5 Calculation of the Matrix Element for Optical Rotation8.6 Differential Rayleigh and Raman Scattering of Circularly Polarized Light8.7 Quadrupole Contributions to Differential Scattering8.8 Magnetic Circular Dichroism8.9 The Two-Group Model for Circular Dichroism8.10 The Two-Group Model for Optical Rotation8.11 Induced Circular DichroismChapter 9 Non-Linear Optical Processes9.1 Harmonic Generation9.2 Static Field-Induced Second Harmonic Generation9.3 Hyper-Raman Scattering9.4 Selection Rules for Hyper-Raman Scattering9.5 Laser-Induced Circular Dichroism9.6 "The Field "Dressing" Approach to Laser-Induced Circular Dichroism"9.7 Laser-Induced Optical Rotation9.8 Laser-Induced Resonance Fluorescence9.9 The Optical Kerr Effect9.10 Coherent anti-Stokes Raman Scattering (CARS)Chapter 10 Transformations and Multipolar Electrodynamics10.1 Introduction10.2 The Electric Polarization Field10.3 The Magnetization Field10.4 Partitioning of the Current Density10.5 The Multipolar Lagrangian10.6 Atomic Field Equations10.7 The Multipolar Hamiltonian10.8 Cancellation of the Intermolecular Interactions in the Multipolar Hamiltonian10.9 Canonical Transformations10.10 The Multipolar Hamiltonian by the Canonical Transformation Method10.11 Equivalence of Matrix Elements10.12 Canonical Transformation and Perturbation Theory10.13 The Röntgen CurrentChapter 11 Self-Interactions11.1 Introduction11.2 Static Self-Energy11.3 The Transverse Self-Energy of the Free Electron11.4 Mass Renormalization by Canonical Transformation11.5 Mass Renormalization in the Multipolar Formalism11.6 The Lamb Shift11.7 Lamb Shift Calculated by Canonical Transformation11.8 Lamb Shift via the Multipolar HamiltonianAppendix 1 Proofs of Three Identities for Non-commuting OperatorsAppendix 2 Rotational Averaging of TensorsAppendix 3 Principal Equations Expressed in Gaussian UnitsIndex

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Consolations of Philosophy Penguin

Nauki humanistyczne

Alain de Botton, best-selling author of How Proust can Change Your Life, has set six of the finest minds in the history of philosophy to work on the problems of everyday life. Here then are Socrates, Epicurus, Seneca, Montaigne, Schopenhauer and Nietzsche on some of the things that bother us all; lack of money, the pain of love, inadequacy, anxiety, the fear of failure and the pressure to conform.

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