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In [[nonlinear optics]], '''B-Integral''' is a measure of the [[nonlinear]] phase shift of light. It calculates the exponential growth of the least stable [[spatial frequency]] in a [[laser beam]], and is the numerical equivalent of the nonlinear phase shift along the laser system's optical axis.  
 
In a multipass laser system as a cumulative measure of the nonlinear interaction,<ref>{{Cite web|url=http://www.rp-photonics.com/b_integral.html|title=B Integral|publisher=Encyclopedia of Laser Physics and Technology}}</ref> this [[integral]] is given by:
 
: <math>B=\frac{2\pi}{\lambda}\int \! n_2I(z)\,dz \,</math>
 
where <math>I(z)</math> is the optical intensity along the beam axis, <math>z</math> the position in beam direction, and <math>n_2</math> the nonlinear index quantifying the Kerr nonlinearity. As <math>n_2I(z)</math> is the nonlinear change in the refractive index, one easily recognizes the B integral to be the total on-axis nonlinear phase shift accumulated in a passage through the device.
The B integral is frequently used in the context of ultrafast amplifiers, e.g. for optical components such as the Pockels cell of a regenerative amplifier.
 
==See also==
[[Kerr effect]]
 
==References==
{{reflist}}
 
[[Category:Laser science]]
[[Category:Photonics]]
 
 
{{optics-stub}}

Revision as of 20:47, 12 January 2014

In nonlinear optics, B-Integral is a measure of the nonlinear phase shift of light. It calculates the exponential growth of the least stable spatial frequency in a laser beam, and is the numerical equivalent of the nonlinear phase shift along the laser system's optical axis.

In a multipass laser system as a cumulative measure of the nonlinear interaction,[1] this integral is given by:

B=2πλn2I(z)dz

where I(z) is the optical intensity along the beam axis, z the position in beam direction, and n2 the nonlinear index quantifying the Kerr nonlinearity. As n2I(z) is the nonlinear change in the refractive index, one easily recognizes the B integral to be the total on-axis nonlinear phase shift accumulated in a passage through the device. The B integral is frequently used in the context of ultrafast amplifiers, e.g. for optical components such as the Pockels cell of a regenerative amplifier.

See also

Kerr effect

References

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Template:Optics-stub