Method and apparatus for optimizing coupled laser resonator performance

Claim 1

An apparatus for use with first and second laser resonators each having a gain medium in a cavity and a displaceable mirror for selecting a resonator cavity length, said resonators providing output beams at an electromagnetic frequency having a beam power with a relative value of phase and coherence, said apparatus comprising; a means for adjusting the cavity length of said resonators so that the electromagnetic frequency of said resonator beams are equal to a value ν-ν 0 ; a means for sampling each resonator beam with a means for providing signals indicative of the power of said resonator beams; a means for electromagnetically coupling said beams, thereby ensuring that the frequencies of the laser resonator output beams are locked at a frequency ν=ν 0 ; a spectrophone means for sampling each beam for providing signals indicative of the electromagnetic frequency of said beams independent of the coherence and phase thereof, said spectrophone means having an operating range of frequencies with a maximum spectrophone means signal amplitude at an electromagnetic frequency ν 0 ; a controller for receiving said resonator beam power signals and said spectrophone means signals and, for each resonator, said controller for normalizing said spectrophone means signals with respect to said resonator beam power signals, thereby ensuring said spectrophone means signals are a function of only said resonator beam frequency; generating, for each resonator, from said spectrophone means signals mirror control signals for positioning said mirror at a cavity length such that said spectrophone means signal value is equal to the value thereof at said frequency ν=ν 0 .

Claim 2

An apparatus for use with first and second laser resonators each having a gain medium in a cavity and a displaceable mirror for selecting a resonator cavity length, said resonators providing output beams at an electromagnetic frequency having a beam power with a relative value of phase and coherence, said apparatus comprising; a means for adjusting the cavity length of said resonators so that the electromagnetic frequency of said resonator beams are equal to a value ν-ν 0 ; a means for sampling each resonator beam with a means for providing signals indicative of the power of said resonator beams; a means for electromagnetically coupling said beams, thereby ensuring that the frequencies of the laser resonator output beams are locked at a frequency ν=ν 0 ; a spectrophone means for sampling each beam for providing signals indicative of the electromagnetic frequency of said beams independent of the coherence and phase thereof, said spectrophone means having an operating range of frequencies with a maximum spectrophone means signal amplitude at an electromagnetic frequency ν 0 ; a controller for receiving said resonator beam power signals and said spectrophone means signals and, for each resonator, said controller for normalizing said spectrophone means signals with respect to said resonator beam power signals, thereby ensuring said spectrophone means signals are a function of only said resonator beam frequency; generating, for each resonator, from said spectrophone means signals mirror control signals for positioning said mirror at a cavity length such that said spectrophone means signal value is equal to the value thereof at said frequency ν=ν 0 .

Claim 3

A method for use with first and second laser resonators each having a gain medium in a cavity and a displaceable mirror for selecting a resonator cavity length, said resonators generating beams at an electromagnetic frequency having a beam power with a relative value of phase and coherence, said method comprising the steps of: adjusting the cavity length of said resonators so that the electromagnetic frequency of said resonator beams are equal to a value ν=ν 0 ; sampling each resonator beam with a means for providing signals indicative of the power of said resonator beams; electromagnetically coupling said beams, thereby ensuring that the frequencies of the laser resonator output beams are locked at a frequency ν=ν 0 ; sampling each resonator beam with a spectrophone means for providing signals indicative of the electromagnetic frequency of said resonator beams independent of the coherence and phase thereof, said spectrophone means having an operating range of frequencies with a maximum spectrophone means signal value at said electromagnetic frequency ν=ν 0 ; receiving said resonator beam power signals and said resonator beam frequency signals at a controller and, normalizing said spectrophone means signals with respect to said resonator beam power signals, thereby ensuring said spectrophone means signals are a function of only said resonator beam frequency; generating, for each resonator, from said spectrophone means signals, mirror control signals for positioning said mirror at a cavity length such that said spectrophone means signal value is equal to the value thereof at said frequency ν=ν 0 .

Claim 4

A method for use with first and second laser resonators each having a gain medium in a cavity and a displaceable mirror for selecting a resonator cavity length, said resonators generating beams at an electromagnetic frequency having a beam power with a relative value of phase and coherence, said method comprising the steps of: adjusting the cavity length of said resonators so that the electromagnetic frequency of said resonator beams are equal to a value ν=ν 0 ; sampling each resonator beam with a means for providing signals indicative of the power of said resonator beams; electromagnetically coupling said beams, thereby ensuring that the frequencies of the laser resonator output beams are locked at a frequency ν=ν 0 ; sampling each resonator beam with a spectrophone means for providing signals indicative of the electromagnetic frequency of said resonator beams independent of the coherence and phase thereof, said spectrophone means having an operating range of frequencies with a maximum spectrophone means signal value at said electromagnetic frequency ν=ν 0 ; receiving said resonator beam power signals and said resonator beam frequency signals at a controller and, normalizing said spectrophone means signals with respect to said resonator beam power signals, thereby ensuring said spectrophone means signals are a function of only said resonator beam frequency; generating, for each resonator, from said spectrophone means signals, mirror control signals for positioning said mirror at a cavity length such that said spectrophone means signal value is equal to the value thereof at said frequency ν=ν 0 .