Ponderomotive energy

Summary

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

Equation edit

The ponderomotive energy is given by

 ,

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

In terms of the laser intensity  , using  , it reads less simply:

 ,

where   is the vacuum permittivity.

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

 ,[2]

where the laser wavelength is  , and   is the speed of light. The units are electronvolts (eV), watts (W), centimeters (cm) and micrometers (μm).

Atomic units edit

In atomic units,  ,  ,   where  . If one uses the atomic unit of electric field,[3] then the ponderomotive energy is just

 

Derivation edit

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

 .

The acceleration of the particle is

 .

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

 .

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

 .

In laser physics, this is called the ponderomotive energy  .

See also edit

References and notes edit

  1. ^ Highly Excited Atoms. By J. P. Connerade. p. 339
  2. ^ https://www.phys.ksu.edu/personal/cdlin/class/class11a-amo2/atomic_units.pdf [bare URL PDF]
  3. ^ CODATA Value: atomic unit of electric field