Classical Mechanics and Fields in Physics
1.RADIATION
J. Planelles
2.Matter and Field
J. Planelles
Newton’s Law
Lagrange
equation
Conservative systems
Classical Mechanics: an overview
No magnetic monopoles
Time-independent field
Velocity-dependent potentials
Define:
Velocity-dependent potentials: cont.
Velocity-dependent potentials: cont.
kinematic
momentum:
canonical
momentum:
Hamiltonian:
Conservative systems: V(x,y,z) & L = T - V
kinematic
momentum:
canonical
momentum:
Hamiltonian:
Gauge
We may select
:
;
Coulomb Gauge
:
Hamiltonian (coulomb gauge)
;
Magnetic field: summary
No magnetic
monopoles:
vector
potential
No conservative field:
velocity-dependent
potential:
Lagrangian:
kinematic momentum
Canonical
momentum:
Hamiltonian:
Coulomb gauge:
Hamiltonian operator:
3. Electron-photon interaction
(selection rules and resonanace)
J. Planelles
Hamiltonian of a charge in an electromagnetic field
Set of charges {qi
}:
Time-dependent perturbation theory
Time-dependent perturbation theory (cont.)
Transition probability:
Taylor expansion:
Time-dependent perturbation theory (cont.)
Time-dependent perturbation theory (cont.)
resonance:
resonance:
selection rule:
Time-dependent perturbation theory (cont.)
First
(and larger) perturbation
term
:
(with
q = - e
,
m
of electron)
Integral involved:
Single photon transition
Spontaneous emission
Time-dependent perturbation theory (cont.)
After some algebra
:
Time-dependent perturbation theory (cont.)
Second
(smaller)
perturbation
term
:
(
q = - e
,
m
of electron)
terms : two-photon transitions
two-photon transitions: weak (
use LASER). e.g. Raman
Explore the concepts of radiation, matter, fields, Hamiltonian, and more in classical mechanics with a focus on velocity-dependent potentials and conservative systems. Dive into the detailed discussions on gauge theory, Coulomb gauge, magnetic fields, and Hamiltonian operators within the framework of physics.
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Presentation Transcript
1.RADIATION J. Planelles
2.Matter and Field J. Planelles
Classical Mechanics: an overview Newton s Law Conservative systems Lagrange equation
Velocity-dependent potentials Time-independent field No magnetic monopoles
Velocity-dependent potentials: cont. kinematic momentum: canonical momentum: Hamiltonian:
Conservative systems: V(x,y,z) & L = T - V canonical momentum: kinematic momentum: Hamiltonian:
Gauge ; We may select : Coulomb Gauge :
Magnetic field: summary No magnetic monopoles: vector potential velocity-dependent potential: No conservative field: Lagrangian: kinematic momentum Canonical momentum: Hamiltonian: Coulomb gauge: Hamiltonian operator:
3. Electron-photon interaction (selection rules and resonanace) J. Planelles
Hamiltonian of a charge in an electromagnetic field Set of charges {qi}:
Time-dependent perturbation theory (cont.) Transition probability: Taylor expansion:
Time-dependent perturbation theory (cont.) resonance: resonance: selection rule:
Time-dependent perturbation theory (cont.) First (and larger) perturbation term: (with q = - e, m of electron) Integral involved: Single photon transition Spontaneous emission
Time-dependent perturbation theory (cont.) After some algebra:
Time-dependent perturbation theory (cont.) Second (smaller) perturbation term: (q = - e, m of electron) terms : two-photon transitions two-photon transitions: weak ( use LASER). e.g. Raman
