Multiple-prism dispersion theory

The generalized mathematical description of multiple-prism dispersion, as a function of the angle of incidence, prism geometry, prism refractive index, and number of prisms, was introduced as a design tool for multiple-prism grating laser oscillators by Duarte and Piper,[4][5] and is given by

${\displaystyle (\partial \phi _{2,m}/\partial \lambda )=H_{2,m}(\partial n_{m}/\partial \lambda )+(k_{1,m}k_{2,m})^{-1}{\bigg (}H_{1,m}(\partial n_{m}/\partial \lambda )\pm \ (\partial \phi _{2,(m-1)}/\partial \lambda ){\bigg )}}$

which can also be written as

${\displaystyle \nabla _{\lambda }\phi _{2,m}=H_{2,m}\nabla _{\lambda }n_{m}+(k_{1,m}k_{2,m})^{-1}{\bigg (}H_{1,m}\nabla _{\lambda }n_{m}\pm \nabla _{\lambda }\phi _{2,(m-1)}{\bigg )}}$

using

${\displaystyle \nabla _{\lambda }=\partial /\partial \lambda }$

Also,

${\displaystyle k_{1,m}=\cos \psi _{1,m}/\cos \phi _{1,m}}$

${\displaystyle k_{2,m}=\cos \phi _{2,m}/\cos \psi _{2,m}}$

${\displaystyle H_{1,m}=(\tan \phi _{1,m})/n_{m}}$

${\displaystyle H_{2,m}=(\tan \phi _{2,m})/n_{m}}$

Here, ${\displaystyle \phi _{1,m}}$ is the angle of incidence, at the mth prism, and ${\displaystyle \psi _{1,m}}$ its corresponding angle of refraction. Similarly, ${\displaystyle \phi _{2,m}}$ is the exit angle and ${\displaystyle \psi _{2,m}}$ its corresponding angle of refraction. The two main equations give the first order dispersion for an array of m prisms at the exit surface of the mth prism. The plus sign in the second term in parentheses refers to a positive dispersive configuration while the minus sign refers to a compensating configuration.[4][5] The k factors are the corresponding beam expansions, and the H factors are additional geometrical quantities. It can also be seen that the dispersion of the mth prism depends on the dispersion of the previous prism (m - 1).

These equations can also be used to quantify the angular dispersion in prism arrays, as described in Isaac Newton's book Opticks, and as deployed in dispersive instrumentation such as multiple-prism spectrometers. A comprehensive review on practical multiple-prism beam expanders and multiple-prism angular dispersion theory, including explicit and ready to apply equations (engineering style), is given by Duarte.[7]

More recently, the generalized multiple-prism dispersion theory has been extended to include positive and negative refraction.[8] Also, higher order phase derivatives have been derived using a Newtonian iterative approach.[9] This extension of the theory enables the evaluation of the Nth higher derivative via an elegant mathematical framework. Applications include further refinements in the design of prism pulse compressors and nonlinear optics.

Single-prism dispersion

For a single generalized prism (m = 1), the generalized multiple-prism dispersion equation simplifies to[3][10]

${\displaystyle (\partial \phi _{2,1}/\partial \lambda )=(sin\psi _{2,1}/cos\phi _{2,1})(\partial n_{1}/\partial \lambda )+(cos\psi _{2,1}/cos\phi _{2,1})tan\psi _{1,1}(\partial n_{1}/\partial \lambda )}$

If the single prism is a right-angled prism with the beam exiting normal to the output face, that is ${\displaystyle \phi _{2,m}}$ equal to zero, this equation reduces to[7]

${\displaystyle (\partial \phi _{2,1}/\partial \lambda )=tan\psi _{1,1}(\partial n_{1}/\partial \lambda )}$

A two-prism pulse compressor as deployed in some femtosecond laser configurations.

This multiple-prism arrangement is used with a diffraction grating to provide tuning in a dye laser.

The first application of this theory was to evaluate the laser linewidth in multiple-prism grating laser oscillators.[4] The total intracavity angular dispersion plays an important role in the linewidth narrowing of pulsed tunable lasers through the equation[4][7]

${\displaystyle \Delta \lambda \approx \Delta \theta \left({\partial \Theta \over \partial \lambda }\right)^{-1}}$

where ${\displaystyle \Delta \theta }$ is the beam divergence and the overall intracavity angular dispersion is the quantity in parentheses (elevated to –1). Although originally classical in origin, in 1992 it was shown that this laser cavity linewidth equation can also be derived from interferometric quantum principles.[11]

For the special case of zero dispersion from the multiple-prism beam expander, the single-pass laser linewidth is given by[7][10]

${\displaystyle \Delta \lambda \approx \Delta \theta \left(M{\partial \theta \over \partial \lambda }\right)^{-1}}$

where M is the beam magnification provided by the beam expander that multiplies the angular dispersion provided by the diffraction grating. In practice, M can be as high as 100-200.[7][10]

When the dispersion of the multiple-prism expander is not equal to zero, then the single-pass linewidth is given by[4][7]

${\displaystyle \Delta \lambda \approx \Delta \theta \left(M{\partial \theta \over \partial \lambda }+{\partial \phi _{2,m} \over \partial \lambda }\right)^{-1}}$

where the first differential refers to the angular dispersion from the grating and the second differential refers to the overall dispersion from the multiple-prism beam expander (given in the section above).[7][10]

In 1987 the multiple-prism angular dispersion theory was extended to provide explicit second order equations directly applicable to the design of prismatic pulse compressors.[12] The generalized multiple-prism dispersion theory is applicable to:

• Amici prisms[13][14]
• laser microscopy,[15][16]
• narrow-linewidth tunable laser design,[17]
• prismatic beam expanders[4][5]
• prism compressors for femtosecond pulse lasers.[18][19][20]

• Beam expander
• Laser linewidth
• Multiple-prism grating laser oscillator

• Prism and Multiple-Prism Pulse Compression: Tutorial