In strong-field laser physics, ponderomotive energy is the cycle-averaged quiver energy of a free electron in an electromagnetic field.[1]
The ponderomotive energy is given by
Up={e2E2\over4m
2} | |
\omega | |
0 |
where
e
E
\omega0
m
I
I=c\epsilon0E2/2
2 | |
U | |
p={e |
I\over2c\epsilon0m
2}={2e | |
\omega | |
0 |
2\overc\epsilon0m} ⋅ {I\over
2} | |
4\omega | |
0 |
where
\epsilon0
For typical orders of magnitudes involved in laser physics, this becomes:
Up(eV)=9.33 ⋅ I(1014 W/cm2) ⋅ λ2(\mum2)
where the laser wavelength is
λ=2\pic/\omega0
c
In atomic units,
e=m=1
\epsilon0=1/4\pi
\alphac=1
\alpha ≈ 1/137
Up=
E2 | ||||||
|
.
The formula for the ponderomotive energy can be easily derived. A free particle of charge
q
E\cos(\omegat)
F=qE\cos(\omegat)
The acceleration of the particle is
am={F\overm}={qE\overm}\cos(\omegat)
Because the electron executes harmonic motion, the particle's position is
x={-a\over\omega2}=-
qE | |
m\omega2 |
\cos(\omegat)=-
q | \sqrt{ | |
m\omega2 |
2I0 | |
c\epsilon0 |
For a particle experiencing harmonic motion, the time-averaged energy is
U=
|
In laser physics, this is called the ponderomotive energy
Up