Ponderomotive energy

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In strong-field laser physics, ponderomotive energy is the cycle-averaged quiver energy of a free electron in an electromagnetic field.[1]

Equation

The ponderomotive energy is given by

Up=e2E24mω02,

where e is the electron charge, E is the linearly polarised electric field amplitude, ω0 is the laser carrier frequency and m is the electron mass.

In terms of the laser intensity I, using I=cϵ0E2/2, it reads less simply:

Up=e2I2cϵ0mω02=2e2cϵ0mI4ω02,

where ϵ0 is the vacuum permittivity.

For typical orders of magnitudes involved in laser physics, this becomes:

Up(eV)=9.33I(1014 W/cm2)λ2(μm2),[2]

where the laser wavelength is λ=2πc/ω0, and c is the speed of light. The units are electronvolts (eV), watts (W), centimeters (cm) and micrometers (μm).

Atomic units

In atomic units, e=m=1, ϵ0=1/4π, αc=1 where α1/137. If one uses the atomic unit of electric field,[3] then the ponderomotive energy is just

Up=E24ω02.

Derivation

The formula for the ponderomotive energy can be easily derived. A free particle of charge q interacts with an electric field Ecos(ωt). The force on the charged particle is

F=qEcos(ωt).

The acceleration of the particle is

am=Fm=qEmcos(ωt).

Because the electron executes harmonic motion, the particle's position is

x=aω2=qEmω2cos(ωt)=qmω22I0cϵ0cos(ωt).

For a particle experiencing harmonic motion, the time-averaged energy is

U=12mω2x2=q2E24mω2.

In laser physics, this is called the ponderomotive energy Up.

See also

References and notes

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