Quantum Physics

Lýsing:
Quantum physics allows us to understand the nature of the physical phenomena which govern the behavior of solids, semi-conductors, lasers, atoms, nuclei, subnuclear particles and light. In Quantum Physics, Le Bellac provides a thoroughly modern approach to this fundamental theory. Throughout the book, Le Bellac teaches the fundamentals of quantum physics using an original approach which relies primarily on an algebraic treatment and on the systematic use of symmetry principles.
In addition to the standard topics such as one-dimensional potentials, angular momentum and scattering theory, the reader is introduced to more recent developments at an early stage. These include a detailed account of entangled states and their applications, the optical Bloch equations, the theory of laser cooling and of magneto-optical traps, vacuum Rabi oscillations and an introduction to open quantum systems.
Annað
- Höfundur: Michel Le Bellac
- Útgáfa:1
- Útgáfudagur: 01-12-2011
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- Format:Page Fidelity
- ISBN 13: 9780511345562
- Print ISBN: 9781107602762
- ISBN 10: 0511345569
Efnisyfirlit
- Half-title
- Title
- Copyright
- Contents
- Foreword
- Preface
- Acknowledgments
- Addendum for the English edition
- Units and physical constants
- 1 Introduction
- 1.1 The structure of matter
- 1.1.1 Length scales from cosmology to elementary particles
- 1.1.2 States of matter
- 1.1.3 Elementary constituents
- 1.1.4 The fundamental interactions
- 1.2 Classical and quantum physics
- 1.3 A bit of history
- 1.3.1 Black-body radiation
- 1.3.2 The photoelectric effect
- 1.4 Waves and particles: interference
- 1.4.1 The de Broglie hypothesis
- 1.4.2 Diffraction and interference of cold neutrons
- 1.4.3 Interpretation of the experiments
- 1.4.4 Heisenberg inequalities I
- 1.5 Energy levels
- 1.5.1 Energy levels in classical mechanics and classical models of the atom
- 1.5.2 The Bohr atom
- 1.5.3 Orders of magnitude in atomic physics
- 1.6 Exercises
- 1.6.1 Orders of magnitude
- 1.6.2 The black body
- 1.6.3 Heisenberg inequalities
- 1.6.4 Neutron diffraction by a crystal
- 1.6.5 Hydrogen-like atoms
- 1.6.6 The Mach–Zehnder interferometer
- 1.6.7 Neutron interferometry and gravity
- 1.6.8 Coherent and incoherent neutron scattering by a crystal
- 1.7 Further reading
- 1.1 The structure of matter
- 2 The mathematics of quantum mechanics I: finite dimension
- 2.1 Hilbert spaces of finite dimension
- 2.2 Linear operators on H
- 2.2.1 Linear, Hermitian, unitary operators
- 2.2.2 Projection operators and Dirac notation
- 2.3 Spectral decomposition of Hermitian operators
- 2.3.1 Diagonalization of a Hermitian operator
- 2.3.2 Diagonalization of a 2×2 Hermitian matrix
- 2.3.3 Complete sets of compatible operators
- 2.3.4 Unitary operators and Hermitian operators
- 2.3.5 Operator-valued functions
- 2.4 Exercises
- 2.4.1 The scalar product and the norm
- 2.4.2 Commutators and traces
- 2.4.3 The determinant and the trace
- 2.4.4 A projector in R3
- 2.4.5 The projection theorem
- 2.4.6 Properties of projectors
- 2.4.7 The Gaussian integral
- 2.4.8 Commutators and a degenerate eigenvalue
- 2.4.9 Normal matrices
- 2.4.10 Positive matrices
- 2.4.11 Operator identities
- 2.4.12 A beam splitter
- 2.5 Further reading
- 3 Polarization: photons and spin-1/2 particles
- 3.1 The polarization of light and photon polarization
- 3.1.1 The polarization of an electromagnetic wave
- 3.1.2 The photon polarization
- 3.1.3 Quantum cryptography
- 3.2 Spin 1/2
- 3.2.1 Angular momentum and magnetic moment in classical physics
- 3.2.2 The Stern–Gerlach experiment and Stern–Gerlach filters
- 3.2.3 Spin states of arbitrary orientation
- 3.2.4 Rotation of spin 1/2
- 3.2.5 Dynamics and time evolution
- 3.3 Exercises
- 3.3.1 Decomposition and recombination of polarizations
- 3.3.2 Elliptical polarization
- 3.3.3 Rotation operator for the photon spin
- 3.3.4 Other solutions of (3.45)
- 3.3.5 Decomposition of a 2×2 matrix
- 3.3.6 Exponentials of Pauli matrices and rotation operators
- 3.3.7 The tensor Epsilonijk
- 3.3.8 A 2 rotation of spin 1/2
- 3.3.9 Neutron scattering by a crystal: spin-1/2 nuclei
- 3.4 Further reading
- 3.1 The polarization of light and photon polarization
- 4 Postulates of quantum physics
- 4.1 State vectors and physical properties
- 4.1.1 The superposition principle
- 4.1.2 Physical properties and measurement
- 4.1.3 Heisenberg inequalities II
- 4.2 Time evolution
- 4.2.1 The evolution equation
- 4.2.2 The evolution operator
- 4.2.3 Stationary states
- 4.2.4 The temporal Heisenberg inequality
- 4.2.5 The Schrödinger and Heisenberg pictures
- 4.3 Approximations and modeling
- 4.4 Exercises
- 4.4.1 Dispersion and eigenvectors
- 4.4.2 The variational method
- 4.4.3 The Feynman–Hellmann theorem
- 4.4.4 Time evolution of a two-level system
- 4.4.5 Unstable states
- 4.4.6 The solar neutrino puzzle
- 4.4.7 The Schrödinger and Heisenberg pictures
- 4.4.8 The system of neutral K mesons
- 4.5 Further reading
- 4.1 State vectors and physical properties
- 5 Systems with a finite number of levels
- 5.1 Elementary quantum chemistry
- 5.1.1 The ethylene molecule
- 5.1.2 The benzene molecule
- 5.2 Nuclear magnetic resonance (NMR)
- 5.2.1 A spin 1/2 in a periodic magnetic field
- 5.2.2 Rabi oscillations
- 5.2.3 Principles of NMR and MRI
- 5.3 The ammonia molecule
- 5.3.1 The ammonia molecule as a two-level system
- 5.3.2 The molecule in an electric field: the ammonia maser
- 5.3.3 Off-resonance transitions
- 5.4 The two-level atom
- 5.5 Exercises
- 5.5.1 An orthonormal basis of eigenvectors
- 5.5.2 The electric dipole moment of formaldehyde
- 5.5.3 Butadiene
- 5.5.4 Eigenvectors of the Hamiltonian (5.47)
- 5.5.5 The hydrogen molecular ion H+2
- 5.5.6 The rotating-wave approximation in NMR
- 5.6 Further reading
- 5.1 Elementary quantum chemistry
- 6 Entangled states
- 6.1 The tensor product of two vector spaces
- 6.1.1 Definition and properties of the tensor product
- Postulate V
- 6.1.2 A system of two spins 1/2
- 6.1.1 Definition and properties of the tensor product
- 6.2 The state operator (or density operator)
- 6.2.1 Definition and properties
- 6.2.2 The state operator for a two-level system
- 6.2.3 The reduced state operator
- 6.2.4 Time dependence of the state operator
- 6.2.5 General form of the postulates
- 6.3 Examples
- 6.3.1 The EPR argument
- 6.3.2 Bell inequalities
- 6.3.3 Interference and entangled states
- 6.3.4 Three-particle entangled states (GHZ states)
- 6.4 Applications
- 6.4.1 Measurement and decoherence
- 6.4.2 Quantum information
- 6.5 Exercises
- 6.5.1 Independence of the tensor product from the choice of basis
- 6.5.2 The tensor product of two 2×2 matrices
- 6.5.3 Properties of state operators
- 6.5.4 Fine structure and the Zeeman effect in positronium
- 6.5.5 Spin waves and magnons
- 6.5.6 Spin echo and level splitting in NMR
- 6.5.7 Calculation of E(a, b)
- 6.5.8 Bell inequalities involving photons
- 6.5.9 Two-photon interference
- 6.5.10 Interference of emission times
- 6.5.11 The Deutsch algorithm
- 6.6 Further reading
- 6.1 The tensor product of two vector spaces
- 7 Mathematics of quantum mechanics II: infinite dimension
- 7.1 Hilbert spaces
- 7.1.1 Definitions
- 7.1.2 Realizations of separable spaces of infinite dimension
- 7.2 Linear operators on H
- 7.2.1 The domain and norm of an operator
- 7.2.2 Hermitian conjugation
- 7.3 Spectral decomposition
- 7.3.1 Hermitian operators
- 7.3.2 Unitary operators
- 7.4 Exercises
- 7.4.1 Spaces of infinite dimension
- 7.4.2 Spectrum of a Hermitian operator
- 7.4.3 Canonical commutation relations
- 7.4.4 Dilatation operators and the conformal transformation
- 7.5 Further reading
- 7.1 Hilbert spaces
- 8 Symmetries in quantum physics
- 8.1 Transformation of a state in a symmetry operation
- 8.1.1 Invariance of probabilities in a symmetry operation
- 8.1.2 The Wigner theorem
- 8.2 Infinitesimal generators
- 8.2.1 Definitions
- 8.2.2 Conservation laws
- 8.2.3 Commutation relations of infinitesimal generators
- 8.3 Canonical commutation relations
- 8.3.1 Dimension d = 1
- 8.3.2 Explicit realization and von Neumann’s theorem
- 8.3.3 The parity operator
- 8.4 Galilean invariance
- 8.4.1 The Hamiltonian in dimension d = 1
- 8.4.2 The Hamiltonian in dimension d = 3
- 8.5 Exercises
- 8.5.1 Rotations
- 8.5.2 Rotations and SU(2)
- 8.5.3 Commutation relations between momentum and angular momentum
- 8.5.4 The Lie algebra of a continuous group
- 8.5.5 The Thomas–Reiche–Kuhn sum rule
- 8.5.6 The center of mass and the reduced mass
- 8.5.7 The Galilean transformation
- 8.6 Further reading
- 8.1 Transformation of a state in a symmetry operation
- 9 Wave mechanics
- 9.1 Diagonalization of X and P and wave functions
- 9.1.1 Diagonalization of X
- 9.1.2 Realization in…
- 9.1.3 Realization in…
- 9.1.4 Evolution of a free wave packet
- 9.2 The Schrödinger equation
- 9.2.1 The Hamiltonian of the Schrödinger equation
- 9.2.2 The probability density and the probability current density
- 9.3 Solution of the time-independent Schrödinger equation
- 9.3.1 Generalities
- 9.3.2 Reflection and transmission by a potential step
- The potential step: total reflection
- The potential step: reflection and transmission
- 9.3.3 The bound states of the square well
- 9.4 Potential scattering
- 9.4.1 The transmission matrix
- 9.4.2 The tunnel effect
- 9.4.3 The S matrix
- 9.5 The periodic potential
- 9.5.1 The Bloch theorem
- 9.5.2 Energy bands
- 9.6 Wave mechanics in dimension d = 3
- 9.6.1 Generalities
- 9.6.2 The phase space and level density
- 9.6.3 The Fermi Golden Rule
- 9.7 Exercises
- 9.7.1 The Heisenberg inequalities
- 9.7.2 Wave-packet spreading
- 9.7.3 A Gaussian wave packet
- 9.7.4 Heuristic estimates using the Heisenberg inequality
- 9.7.5 The Lennard–Jones potential for helium
- 9.7.6 Reflection delay
- 9.7.7 A delta-function potential
- 9.7.8 Transmission by a well
- 9.7.9 Energy levels of an infinite cubic well in dimension d = 3
- 9.7.10 The probability current in three dimensions
- 9.7.11 The level density
- 9.7.12 The Fermi Golden Rule
- 9.7.13 Study of the Stern–Gerlach experiment
- 9.7.14 The von Neumann model of measurement
- 9.7.15 The Galilean transformation
- 9.8 Further reading
- 9.1 Diagonalization of X and P and wave functions
- 10 Angular momentum
- 10.1 Diagonalization of J2 and Jz
- 10.2 Rotation matrices
- 10.3 Orbital angular momentum
- 10.3.1 The orbital angular momentum operator
- 10.3.2 Properties of the spherical harmonics
- 1. Basis on the unit sphere
- 2. Relation to the Legendre polynomials
- 3. Transformation under rotation
- 4. Parity of the spherical harmonics
- 10.4 Particle in a central potential
- 10.4.1 The radial wave equation
- 10.4.2 The hydrogen atom
- 10.5 Angular distributions in decays
- 10.5.1 Rotations by pi, parity, and reflection with respect to a plane
- 10.5.2 Dipole transitions
- 10.5.3 Two-body decays: the general case
- 10.6 Addition of two angular momenta
- 10.6.1 Addition of two spins 1/2
- 10.6.2 The general case: addition of two angular momenta J1 and J2
- 10.6.3 Composition of rotation matrices
- 10.6.4 The Wigner–Eckart theorem (scalar and vector operators)
- 10.7 Exercises
- 10.7.1 Properties of J
- 10.7.2 Rotation of angular momentum
- 10.7.3 Rotations (theta, phi)
- 10.7.4 The angular momenta…
- 10.7.5 Orbital angular momentum
- 10.7.6 Relation between the rotation matrices and the spherical harmonics
- 10.7.7 Independence of the energy from m
- 10.7.8 The spherical well
- 10.7.9 The hydrogen atom for…
- 10.7.10 Matrix elements of a potential
- 10.7.11 The radial equation in dimension d = 2
- 10.7.12 Symmetry property of the matrices d(j)
- 10.7.13 Light scattering
- 10.7.14 Measurement of the Lambda0 magnetic moment
- 10.7.15 Production and decay of the rho+ meson
- 10.7.16 Interaction of two dipoles
- 10.7.17 Sigma0 decay
- 10.7.18 Irreducible tensor operators
- 10.8 Further reading
- 11.1 The simple harmonic oscillator
- 11.1.1 Creation and annihilation operators
- 11.1.2 Diagonalization of the Hamiltonian
- 11.1.3 Wave functions of the harmonic oscillator
- 11.2 Coherent states
- 11.3 Introduction to quantized fields
- 11.3.1 Sound waves and phonons
- 11.3.2 Quantization of a scalar field in one dimension
- 11.3.3 Quantization of the electromagnetic field
- 11.3.4 Quantum fluctuations of the electromagnetic field
- 11.4 Motion in a magnetic field
- 11.4.1 Local gauge invariance
- 11.4.2 A uniform magnetic field: Landau levels
- 11.5 Exercises
- 11.5.1 Matrix elements of Q and P
- 11.5.2 Mathematical properties
- 11.5.3 Coherent states
- 11.5.4 Coupling to a classical force
- 11.5.5 Squeezed states
- 11.5.6 Zero-point energy of the Debye model
- 11.5.7 The scalar and vector potentials in Coulomb gauge
- 11.5.8 Commutation relations and Hamiltonian of the electromagnetic field
- 11.5.9 Quantization in a cavity
- 11.5.10 Current conservation in the presence of a magnetic field
- 11.5.11 Non-Abelian gauge transformations
- 11.5.12 The Casimir effect
- 11.5.13 Quantum computing with trapped ions
- 11.6 Further reading
- 12.1 The cross section and scattering amplitude
- 12.1.1 The differential and total cross sections
- 12.1.2 The scattering amplitude
- 12.2 Partial waves and phase shifts
- 12.2.1 The partial-wave expansion
- 12.2.2 Low-energy scattering
- 12.2.3 The effective potential
- 12.2.4 Low-energy neutron–proton scattering
- 12.3 Inelastic scattering
- 12.3.1 The optical theorem
- 12.3.2 The optical potential
- 12.4 Formal aspects
- 12.4.1 The integral equation of scattering
- 12.4.2 Scattering of a wave packet
- 12.5 Exercises
- 12.5.1 The Gamow peak
- 12.5.2 Low-energy neutron scattering by a hydrogen molecule
- 12.5.3 Analytic properties of the neutron–proton scattering amplitude
- 12.5.4 The Born approximation
- 12.5.5 Neutron optics
- 12.5.6 The cross section for neutrino absorption
- 12.6 Further reading
- 13.1 Bosons and fermions
- 13.1.1 Symmetry or antisymmetry of the state vector
- 13.1.2 Spin and statistics
- 13.2 The scattering of identical particles
- 13.3 Collective states
- 13.4 Exercises
- 13.4.1 The Tonos- particle and color
- 13.4.2 Parity of the pi meson
- 13.4.3 Spin-1/2 fermions in an infinite well
- 13.4.4 Positronium decay
- 13.4.5 Quantum statistics and beam splitters
- 13.5 Further reading
- 14.1 Approximation methods
- 14.1.1 Generalities
- 14.1.2 Nondegenerate perturbation theory
- 14.1.3 Degenerate perturbation theory
- 14.1.4 The variational method
- 14.2 One-electron atoms
- 14.2.1 Energy levels in the absence of spin
- 14.2.2 The fine structure
- 14.2.3 The Zeeman effect
- 14.2.4 The hyperfine structure
- 14.3 Atomic interactions with an electromagnetic field
- 14.3.1 The semiclassical theory
- 14.3.2 The dipole approximation
- 14.3.3 The photoelectric effect
- 14.3.4 The quantized electromagnetic field: spontaneous emission
- 14.4 Laser cooling and trapping of atoms
- 14.4.1 The optical Bloch equations
- 14.4.2 Dissipative forces and reactive forces
- 14.4.3 Doppler cooling
- 14.4.4 A magneto-optical trap
- 14.5 The two-electron atom
- 14.5.1 The ground state of the helium atom
- 14.5.2 The excited states of the helium atom
- 14.6 Exercises
- 14.6.1 Second-order perturbation theory and van der Waals forces
- 14.6.2 Order-alpha2 corrections to the energy levels
- 14.6.3 Muonic atoms
- 14.6.4 Rydberg atoms
- 14.6.5 The diamagnetic term
- 14.6.6 Vacuum Rabi oscillations
- 14.6.7 Reactive forces
- 14.6.8 Radiative capture of neutrons by hydrogen
- 14.7 Further reading
- 15.1 Generalized measurements
- 15.1.1 Schmidt’s decomposition
- 15.1.2 Positive operator-valued measures
- 15.1.3 Example: a POVM with spins 1/2
- 15.2 Superoperators
- 15.2.1 Kraus decomposition
- 15.2.2 The depolarizing channel
- 15.2.3 The phase-damping channel
- 15.2.4 The amplitude-damping channel
- 15.3 Master equations: the Lindblad form
- 15.3.1 The Markovian approximation
- 15.3.2 The Lindblad equation
- 15.3.3 Example: the damped harmonic oscillator
- 15.4 Coupling to a thermal bath of oscillators
- 15.4.1 Exact evolution equations
- 15.4.2 The Markovian approximation
- 15.4.3 Relaxation of a two-level system
- 15.4.4 Quantum Brownian motion
- 15.4.5 Decoherence and Schrödinger’s cats
- 15.5 Exercises
- 15.5.1 POVM as projective measurement in a direct sum
- 15.5.2 Using a POVM to distinguish between states
- 15.5.3 A POVM on two arbitrary qubit states
- 15.5.4 Transposition is not completely positive
- 15.5.5 Phase and amplitude damping
- 15.5.6 Details of the proof of the master equation
- 15.5.7 Superposition of coherent states
- 15.5.8 Dissipation in a two-level system
- 15.5.9 Simple models of relaxation
- 15.5.10 Another choice for the spectral function J(omega)
- 15.5.11 The Fokker–Planck–Kramers equation for a Brownian particle
- 15.6 Further reading
- A.1 Proof of the theorem
- A.2 Time reversal
- B.1 An elementary model of measurement
- B.2 Ramsey fringes
- B.3 Interaction with a field inside the cavity
- B.4 Decoherence
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