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==Equation ==
==Equation ==
The ponderomotive energy is given by
The ponderomotive energy is given by
:<math>U_p = {e^2 E_a^2 \over 4m \omega_0^2}</math>,
:<math>U_p = {e^2 E^2 \over 4m \omega_0^2}</math>,


where <math>e</math> is the [[electron charge]], <math>E_a</math> is the linearly [[Polarization (waves)|polarised]] electric field amplitude, <math>\omega_0</math> is the laser [[carrier frequency]] and <math>m</math> is the [[electron mass]].
where <math>e</math> is the [[electron charge]], <math>E</math> is the linearly [[Polarization (waves)|polarised]] electric field amplitude, <math>\omega_0</math> is the laser [[carrier frequency]] and <math>m</math> is the [[electron mass]].


In terms of the laser [[Intensity (physics)|intensity]] <math>I</math>, using <math>I=c\epsilon_0 E_a^2/2</math>, it reads less simply:
In terms of the laser [[Intensity (physics)|intensity]] <math>I</math>, using <math>I=c\epsilon_0 E^2/2</math>, it reads less simply:
:<math>U_p={e^2 I \over 2 c \epsilon_0 m \omega_0^2}={2e^2 \over c \epsilon_0 m} \cdot {I \over 4\omega_0^2}</math>,
:<math>U_p={e^2 I \over 2 c \epsilon_0 m \omega_0^2}={2e^2 \over c \epsilon_0 m} \cdot {I \over 4\omega_0^2}</math>,


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


:<math> U_p (\mathrm{eV}) = 9.33 \cdot I(10^{14} \mathrm{W/cm}^2) \cdot \lambda(\mathrm{\mu m})^2 </math>,<ref>https://www.phys.ksu.edu/personal/cdlin/class/class11a-amo2/atomic_units.pdf {{Bare URL PDF|date=March 2022}}</ref>
:<math> U_p (\mathrm{eV}) = 9.33 \cdot I(10^{14}\ \mathrm{W/cm}^2) \cdot \lambda^2(\mathrm{\mu m}^2) </math>,<ref>https://www.phys.ksu.edu/personal/cdlin/class/class11a-amo2/atomic_units.pdf {{Bare URL PDF|date=March 2022}}</ref>


where the laser wavelength is <math>\lambda= c/2\pi\omega_0</math>, and <math>c</math> is the speed of light. The units are electronvols (eV), watts (W), centimeters (cm) and micrometers (μm).
where the laser wavelength is <math>\lambda= 2\pi c/\omega_0</math>, and <math>c</math> is the speed of light. The units are electronvolts (eV), watts (W), centimeters (cm) and micrometers (μm).


===Atomic units===
===Atomic units===
In [[atomic units]], <math>e=m=1</math>, <math>\epsilon_0=1/4\pi</math>, <math>\alpha c=1</math> where <math>\alpha \approx 1/137</math>. If one uses the [[Atomic units|atomic unit of electric field]],<ref>CODATA Value: [http://physics.nist.gov/cgi-bin/cuu/Value?auefld atomic unit of electric field]</ref> then the ponderomotive energy is just
In [[atomic units]], <math>e=m=1</math>, <math>\epsilon_0=1/4\pi</math>, <math>\alpha c=1</math> where <math>\alpha \approx 1/137</math>. If one uses the [[Atomic units|atomic unit of electric field]],<ref>CODATA Value: [http://physics.nist.gov/cgi-bin/cuu/Value?auefld atomic unit of electric field]</ref> then the ponderomotive energy is just
:<math>U_p = \frac{E_a^2}{4\omega_0^2}.</math>
:<math>U_p = \frac{E^2}{4\omega_0^2}.</math>


==Derivation==
==Derivation==

Latest revision as of 21:30, 20 July 2024

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

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References and notes

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