Full table of contents
- Prologue
- Let the journey begin
- Overview of the content
- Multiple paths through the book
- Resources, units, and conventions
- Introduction to special relativity
- Light and time
- Inertial frames and the Lorentz transformations
- Consequences of the Lorentz transformations
- Relativity of simultaneity
- Length contraction and time dilation
- Non-relativistic limit
- Transformation of velocities and accelerations
- Relativistic aberration and Doppler shift
- The inertia of energy
- Mass, momentum, and energy
- Steps towards general relativity
- Emission from accelerated charges
- Introduction
- Why do accelerated charges radiate?
- Radiation emitted by relativistic charges
- Angular distribution of the emitted radiation
- Radiation emitted by charges in circular motion
- Radiation emitted by charges in linear motion
- Radiation emitted by charges in bending magnets
- Introduction
- Moving charge in a constant magnetic field
- Energy loss and time structure of synchrotron light
- Spectrum of light emitted by a dipole magnet: qualitative discussion
- Spectrum of light emitted by a dipole magnet: quantitative discussion
- Power radiated into each harmonic
- Characteristic harmonic and critical harmonic
- Large-order approximation of the spectrum
- Maximum-emission harmonic
- Angular spectral density and asymptotic expansion of the spectrum
- Number of emitted photons per revolution
- Polarisation of synchrotron light
- Final remarks
- Insertion devices
- Introduction
- Equations of motion in a wiggler
- Electron trajectory in a periodic magnetic field
- Deflection angle and deflection parameter
- Critical energy
- Electron trajectory revisited
- Spectrum of the emission from an insertion device
- Qualitative description
- Simplified model for an insertion device
- Qualitative model for the transition from an undulator to a wiggler
- Planar undulators: the undulator equation
- The undulator equation from relativistic aberration and Doppler shift
- The undulator equation obtained via an interference condition
- Pulse duration, line width, and divergence of an undulator beam
- Relativistic effects in the undulator spectrum
- Basic considerations
- Higher-order harmonics
- Polarisation of the light from insertion devices
- Generating linear polarisation by combining elliptically polarised waves with opposite helicity
- Polarisation of insertion-device emission
- Source comparison and final remarks
- Quantum effects in synchrotron radiation
- Introduction
- Breakdown of electron-trajectory concept
- Compton scatter
- Inverse Compton scatter
- Basic formalism
- Analogy between inverse Compton scattering and undulator radiation
- A hypothetical case study
- Breakdown of classical synchrotron emission model: Schwinger magnetic field
- Shrinking a storage ring
- Electron recoil
- Storage-ring radius and the Compton wavelength
- Shining too weakly
- Shining too strongly
- Radiative damping
- Critical energy density
- Schwinger magnetic field: discussion
- Quantum effects in relativistic charged-particle orbits
- Introduction
- Relativistic quantum mechanics of circular charged-particle trajectories
- Plane waves and wave-functions
- Correspondence rules
- Klein–Gordon equation
- Klein–Gordon model for a relativistic charged particle in a uniform magnetic field
- Radiative polarisation and spin light
- Sokolov–Ternov relaxation time: rough estimate
- The Golden Rule
- Sokolov–Ternov relaxation via the Golden Rule
- Spin light
- Discussion
- Comparison of characteristic timescales
- Some characteristic timescales associated with synchrotron light
- Comparison of characteristic timescales associated with synchrotron light
- The free-electron laser
- Light–matter interaction: absorption and emission
- Planck’s law
- Absorption, spontaneous emission, and stimulated emission by atomic electrons
- Phenomenological model of a low-gain laser
- Low-gain regime for free-electron laser
- Microscopic interactions in an FEL
- Why do FELs need an undulator?
- Low-gain FEL: the FEL pendulum equation
- Approximate solution to the pendulum equation: the gain function
- Gain and undulator bandwidth: Madey’s theorem
- One-dimensional high-gain FEL theory
- Revisiting the FEL pendulum equation
- The laser field
- Space-charge effects
- An equation for the current density
- Numerical solution of coupled system of high-gain FEL equations
- Introduction to phase-space dynamics
- The concept of phase space
- Dynamical evolution and Hamilton’s equations
- Beam emittance
- Phase-space filamentation and chaotic dynamics in FELs
- Phase-space filamentation
- Laminar mixing in the low-gain FEL model
- Turbulent chaotic evolution
- Synchrotron light in the cosmos
- Introduction
- Motion of charged particles in magnetic fields, revisited
- Radiated power and emitted spectrum
- Synchrotron emission from an ensemble of particles
- Effect of electron velocity distribution on synchrotron-emission spectrum
- Effect of electron energy distribution on synchrotron-emission spectrum
- Self-absorption of synchrotron light
- Distortion of initial electron spectra by synchrotron emission
- Synchrotron cooling
- Diffusion–loss equation
- Fermi model for acceleration of cosmic rays
- Second-order Fermi acceleration
- First-order Fermi acceleration
- The emergence of power-law spectra
- Minimum energy and equipartition
- Curvature radiation
- Synchrotron radiation in planetary magnetic fields
- Geomagnetic emission in cosmic-ray air showers
- Synchrotron radiation from Jupiter’s magnetosphere
- Synchrotron radiation in galactic magnetic fields
- Synchrotron emission from the Galaxy
- Synchrotron emission from supernova remnants
- Cosmic sources of synchrotron radiation
- Synchrotron emission from active galactic nuclei
- Synchrotron emission from accreting black holes
- Non-photon analogues of synchrotron radiation
- Introduction
- The four known fundamental forces
- Particle-exchange model for the forces of nature
- Some generic aspects of the Standard Model
- Photons as carriers of the electromagnetic force
- W and Z bosons as carriers of the weak force
- Gluons as carriers of the strong force
- Gravitons as carriers of the gravitational force
- Generalised forms of synchrotron radiation
- First generalisation: synchrotron radiation is not exclusive to synchrotron accelerators
- Second generalisation: the accelerating force is not necessarily electromagnetic
- Third generalisation: the particle radiation mechanism is not necessarily electromagnetic
- Caveat emptor
- Weak-force analogues of synchrotron radiation
- Neutrino synchrotron radiation
- Further weak-force synchrotron-radiation analogues
- How synchrotron photons can influence neutrino emission
- Strong-force analogues of synchrotron radiation
- Strong-force analogue of a bending magnet
- Gluon and photon synchrotron radiation induced by QCD vacuum domains
- QCD analogue of Sokolov–Ternov effect
- Hadron jets
- QCD dead cone
- Jet quenching in the quark–gluon plasma
- Gravitational-wave analogues of synchrotron radiation
- Calculation of synchrotron radiation from first principles
- Maxwell equations, electromagnetic potentials, and gauge invariance
- Maxwell equations
- Electromagnetic potentials and gauge invariance
- Scalar and vector potential for an electron in circular motion
- Doppler effect, revisited
- Model for a charge in circular motion
- Vector-potential harmonics
- Green functions for scalar and vector potentials
- Electric-field and magnetic-field harmonics
- Spectrum of synchrotron radiation by electrons in circular motion
- Far-field approximation
- Far-field expressions for harmonics of electromagnetic potentials and fields
- Poynting vector and electromagnetic energy density
- Far-field expressions for radiated Poynting vector and energy density: general case
- Power radiated by a charge in circular motion
- Large-order approximation for the spectral density
- Spatial and temporal structure
- Quantum optics of synchrotron light
- What is a photon?
- First answer to ‘What is a photon?’
- Second answer to ‘What is a photon?’
- Photons via the Poynting vector
- Poisson photon statistics, part one
- An illustrative numerical model
- Poisson photon statistics, part two
- Some omissions
- Interlude
- Third answer to ‘What is a photon?’
- Single-mode and multi-mode photon states
- Localisation
- Single-photon and multi-photon states
- Entanglement
- Photon detection and the intensity operator
- Coherent states of the photon field
- Coherent states: properties and definition
- Coherent states: number-state expansion
- Coherent states: Poisson statistics
- Photon radiation from prescribed classical currents
- Coherent-state displacement operator
- Coherent states from prescribed currents, part one
- Interlude: Schrödinger, Heisenberg, and interaction pictures
- Coherent states from prescribed currents, part two
- Looping back, from photons to classical electrodynamics
- Quantum optics using synchrotron light
- On the plausibility of quantum optics using synchrotron light
- Interlude
- Photon beam splitters
- Parametric down-conversion
- Synchrotron-light pseudo-temperature and the Unruh effect
- Some omissions
- Hierarchy of physical models for light
- Epilogue
- Introduction
- Synchrotron radiation as a connecting thread
- Recurring themes
- Omissions
- Valediction
- Bessel-function sums and trigonometric integrals
- Two infinite Bessel-function sums
- Bessel’s differential equation
- Normal form of Bessel’s equation
- Differential equation for [J_n(x)]^2
- Zeroth Bessel sum
- First Bessel sum
- Second Bessel sum
- Two trigonometric definite integrals
- Trigonometric integral \mathcal{I}_1
- Trigonometric integral \mathcal{I}_2
- Planck’s radiation law and radiometric quantities
- Rayleigh–Jeans law
- Planck’s law
- Radiometric quantities and different formulations of Planck’s law
- Schott’s pioneering contributions to synchrotron light
- Contributions to the physics of synchrotron light
- Upheavals of physical theory in the early 1900s
- The enduring success of Schott’s failure
- Influence of modern computing devices
- Padé approximant for maximum-emission harmonic
- Padé approximant and Taylor series
- Taylor expansion of g(\tau)
- Relation between Taylor and Padé coefficients of g(\tau)
- Final remarks