* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download PHY982 12th week Electromagnetic field and coupling with photons
Abraham–Minkowski controversy wikipedia , lookup
Electrostatics wikipedia , lookup
Magnetohydrodynamics wikipedia , lookup
Electromagnetic compatibility wikipedia , lookup
Photoelectric effect wikipedia , lookup
Magnetic monopole wikipedia , lookup
Electromagnetism wikipedia , lookup
Multiferroics wikipedia , lookup
Faraday paradox wikipedia , lookup
Lorentz force wikipedia , lookup
Maxwell's equations wikipedia , lookup
Electromagnetic radiation wikipedia , lookup
Gauge fixing wikipedia , lookup
Upconverting nanoparticles wikipedia , lookup
Quantum electrodynamics wikipedia , lookup
Computational electromagnetics wikipedia , lookup
Electron scattering wikipedia , lookup
Mathematical descriptions of the electromagnetic field wikipedia , lookup
PHY982 12th week Electromagnetic field and coupling with photons 1 Maxwell’s equations o magnetic H and electric E fields are related Charge current and charge density o radiative capture reactions: coupling of photons and the nucleus one radiative photon at a time 1 Maxwell’s equations o vector potential and scalar potential o gauge invariance o transverse gauge (Coulomb gauge) Maxwell’s equations o vector potential and scalar potential o gauge invariance o transverse gauge (Coulomb gauge) – one photon approximation (density and scalar field at time independent) 2 Coupling photons and particles Connecting the classical EM description with quantum particle dynamics o free field source flux o particle current to photon production (capture) Coupling photons and particles o photon current to particle flux minimal gauge coupling o photo-disintegration equation o initial state is bound state and we need equation coupling the incoming photon field to the particle in the continuum 3 Photon flux and normalization o photon outgoing wave o The Poynting vector provide energy flux o outgoing photon flux is energy flux per photon energy o normalized photon wave Coupled photon-particle equations o photo-production o photo-disintegration o generalization of wavefunction to incorporate photon channel 4 Partial wave decomposition for photons o expanding photon into vector spherical harmonics o radial coupled channel equations o from asymptotics obtain T-matrix or S-matrix and construct observables. Capture cross sections o starting from incoming particle channel o T-matrix equivalent integral expression o no potential in photon wave! o All analysis ignored gauge invariance… µ=-1,0,+1 5 Photon gauge invariant plane wave o incoming photon along z axis: Photon gauge invariant plane wave o incoming photon along z axis: o splitting into magnetic and electric parts 6 EM field normalization and other properties oThe vector field is normalized like a plane wave oThey are related by: Selection rules 7 Final state photons oFor photon in exit channel – generalize k in z-axis for any direction o vector T-matrix can be written in this general form too: Longitudinal part of the field o does not satisfy the transverse gauge o differs only previous by coefficients o long wavelength approximation (neglect L=J+1) 8 Electric transitions – standard form o long wavelength approximation oSiegert’s theorem: uses continuity equation to transform current into charge density Integration by parts Continuity eq+ Schrodinger eq Electric transitions – standard form o long wavelength approximation o Siegert theorem gives a matrix element proportional to multipole operator o putting it back in the T matrix 9 Extensions and limitation of framework o T-matrix o Ψ(R) – separation of two bodies whereas Z(r) – distance from center of mass non-local equation! Extensions and limitations - coupled channel framework can describe A+B -> (AB)* to many channels - only two bodies = photon+AB - decay process AB -> A’+B’ needs separate formulation (Hauser-Feshbach) Capture cross sections and B(EL) o electric multipole operator appearing in Coulomb inelastic scattering o transition strength function from scattering to bound o photons in long wavelength approximation o capture cross section 10 Photo-absorption cross section oUsing detailed balance this can be obtained from capture o work out specific form for E1 – homework 6 o work out specific properties for protons – homework 8 o work out long wave approximation for magnetic field - homework 9 examples E1 only 11 examples 12