Acousto-optical laser isolator

Claim 2

An acousto-optical isolator for isolating, from a laser beam having a predetermined frequency and propagating forwardly along a predefined path, any unwanted, backwardly propagating laser beam having a like frequency, the isolator comprising: first frequency shift means, disposed to receive a laser beam propagating along the predefined path, for shifting the frequency of the received beam by a first amount; second frequency shift means, disposed forwardly of the first frequency shift means to receive a laser beam propagating along the path, for shifting the frequency of the received beam by a second amount, the second amount being the converse of the first, whereby the frequency of a forwardly propagating beam is shifted by the first amount as the the beam propagates through the first shift means and then is shifted back to the predetermined frequency as the beam propagates through the second shift means, and the frequency of any unwanted, backwardly propagating beam is shifted by the second amount as the beam propagates through the second shift means and then is shifted back to the predetermined frequency as the beam propagates through the first shift means; and attenuation means, disposed between the first and second shift means to receive any laser beam propagating either forwardly or backwardly therebetween, to attenuate any laser beam having a frequency equal to the predetermined frequency shifted by the second amount, whereby any unwanted, backwardly propagating beam is attenuated and is thereby isolated.

Claim 3

An isolator according to claim 1 wherein the attenuation means attenuates any laser beam having a frequency equal to the predetermined frequency.

Claim 4

An isolator according to claim 1 wherein the attenuation means comprises a gas.

Claim 5

An isolator according to claim 1 wherein the attenuation means comprises a Fabry-Perot resonator.

Claim 6

An isolator according to claim 1 wherein one of the frequency shift means comprises a Bragg cell and signal means to provide an energizing signal to the Bragg cell.

Claim 7

An isolator according to claim 5 wherein the Bragg cell comprises tellurium dioxide.

Claim 8

An isolator according to claim 1 wherein the first frequency shift means comprises a reversible frequency shift means and the second shift means comprises a reversible frequency shift means, said isolator further comprising control means to reverse the operation of both frequency shift means such that the first shift means shifts the frequency of a beam propagating therethrough by the second amount and the second shift means shifts the frequency of a beam propagating therethrough by the first amount, the attenuation means being operative when operation of both shift means has been reversed to attenuate a forwardly propagating beam rather than a backwardly propagating beam.

Claim 9

An isolator according to claim 7 wherein one of the frequency shift means comprises a dual-transducer Bragg cell and signal means operative to provide an energizing signal to the Bragg cell, and the control means comprises means to apply the energizing signal selectively to either of the transducers.

Claim 10

An isolator according to claim 1 and further comprising means to deactivate the first and second frequency shift means.

Claim 11

An acousto-optical isolator for isolating, from a laser beam having a predetermined frequency and propagating forwardly along a predefined path, any unwanted, backwardly propagating laser beam having a like frequency, the isolator comprising: frequency shift means, disposed to receive a laser beam propagating along a first portion of the path for shifting the frequency thereof by a first amount, and disposed to receive a laser beam propagating along a second portion of the predefined path for shifting the frequency thereof by a second amount, the second amount being the converse of the first; reflecting means, operative to reflect a forwardly propagating laser beam from a first portion of the path onto a second portion thereof and to reflect a backwardly propagating laser beam from the second portion of the path onto the first portion thereof, whereby the frequency of a forwardly propagating beam is shifted by the first amount as the beam propagates through the shift means along the first portion of the path and then is shifted back to the predetermined frequency as the beam propagates through the shift means along the second portion of the path after having been reflected from the first portion onto the second portion by the reflecting means, and the frequency of any unwanted, backwardly propagating beam is shifted by the second amount as the beam propagates through the shift means along the second portion of the path and then is shifted back to the predetermined frequency as the beam propagates through the shift means along the first portion of the path after having been reflected from the second portion onto the first portion by the reflecting means; and attenuation mean, disposed to receive any beam that is being reflected from either portion of the path onto the other and to attenuate any beam having a frequency equal to the predetermined frequency shifted by the second amount whereby any unwanted, backwardly propagating beam is attenuated and is thereby isolated from the desired beam.

Claim 12

An acousto-optical isolator for isolating, from a laser beam having a predetermined frequency and propagating forwardly along a predefined path, any unwanted, backwardly propagating laser beam having a like frequency, the isolator comprising: frequency shift means, disposed to receive a laser beam propagating along a first portion of the path for shifting the frequency thereof by a first amount, and disposed to receive a laser beam propagating along a second portion of the predefined path for shifting the frequency thereof by a second amount, the second amount being the converse of the first; reflecting means, operative to reflect a forwardly propagating laser beam from a first portion of the path onto a second portion thereof and to reflect a backwardly propagating laser beam from the second portion of the path onto the first portion thereof, whereby the frequency of a forwardly propagating beam is shifted by the first amount as the beam propagates through the shift means along the first portion of the path and then is shifted back to the predetermined frequency as the beam propagates through the shift means along the second portion of the path after having been reflected from the first portion onto the second portion by the reflecting means, and the frequency of any unwanted, backwardly propagating beam is shifted by the second amount as the beam propagates through the shift means along the second portion of the path and then is shifted back to the predetermined frequency as the beam propagates through the shift means along the first portion of the path after having been reflected from the second portion onto the first portion by the reflecting means; and attenuation mean, disposed to receive any beam that is being reflected from either portion of the path onto the other and to attenuate any beam having a frequency equal to the predetermined frequency shifted by the second amount whereby any unwanted, backwardly propagating beam is attenuated and is thereby isolated from the desired beam.

Claim 13

An isolator according to claim 10 wherein the attenuation means attenuates any laser beam having a frequency equal to the predetermined frequency.

Claim 14

An isolator according to claim 10 wherein the attenuation means comprises a gas.

Claim 15

An isolator according to claim 10 wherein the attenuation means comprises a Fabry-Perot resonator.

Claim 16

An isolator according to claim 10 wherein the frequency shift means comprises a Bragg cell and signal means to provide an energizing signal to the Bragg cell.

Claim 17

An isolator according to claim 14 wherein the Bragg cell comprises tellurium dioxide.

Claim 18

An isolator according to claim 10 wherein the frequency shift means comprises a reversible frequency shift means, and further comprising control means to reverse the operation of the frequency shift means such that the shift means shifts the frequency of a beam propagating therethrough along the first portion of the path by the second amount and the frequency of a beam propagating therethrough along the second portion of the path by the first amount, the attenuation means being operative when the operation of the shift means has been reversed to attenuate a forwardly propagating beam rather than a backwardly propagating beam.

Claim 19

An isolator according to claim 16 wherein: the frequency shift means comprises a dual-transducer Bragg cell and signal means to provide an energizing signal to the Bragg cell, and the control means comprises means to apply the energizing signal selectively to either of the transducers.

Claim 20

An isolator according to claim 10 and further comprising means to deactivate the frequency shift means.

Claim 21

An isolator according to claim 10 wherein the attenuation means is disposed between the reflecting means and the shift means across both portions of the path.

Claim 22

An isolating ring laser oscillator comprising: amplifier means, having an input for receiving a forwardly propagating laser beam of predetermined frequency, for amplifying the received laser beam; a plurality of reflector means, disposed to receive the amplified laser beam from the amplifier means and to reflect the beam around the amplifier and back into the input for further amplification; and an acousto-optical isolator for isolating from the forwardly propagating amplified laser beam any unwanted, backwardly propagating beam of like frequency, the isolator comprising: first frequency shift means, disposed to receive the amplified laser beam and to shift the frequency thereof by a first amount; second frequency shift means, disposed forwardly of the first shift means to receive the amplified laser beam from the first shift means and to shift the frequency thereof by a second amount, the second amount being the converse of the first amount, whereby the frequency of the amplified laser beam is shifted back to the predetermined frequency by the second shift means, and whereby the frequency of any backwardly propagating beam is shifted by the second amount as it propagates through the second shift means and then is shifted back to the predetermined frequency as it propagates through the first shift means; and attenuation means, disposed between the first and second shift means to receive any beam propagating therebetween and to attenuate any beam having a frequency equal to the predetermined frequency shifted by the second amount whereby any backwardly propagating beam is attenuated and is thereby isolated from the amplified laser beam.

Claim 23

An isolating ring laser oscillator comprising: amplifier means, having an input for receiving a forwardly propagating laser beam of predetermined frequency, for amplifying the received laser beam; a plurality of reflector means, disposed to receive the amplified laser beam from the amplifier means and to reflect the beam around the amplifier and back into the input for further amplification; and an acousto-optical isolator for isolating from the forwardly propagating amplified laser beam any unwanted, backwardly propagating beam of like frequency, the isolator comprising: first frequency shift means, disposed to receive the amplified laser beam and to shift the frequency thereof by a first amount; second frequency shift means, disposed forwardly of the first shift means to receive the amplified laser beam from the first shift means and to shift the frequency thereof by a second amount, the second amount being the converse of the first amount, whereby the frequency of the amplified laser beam is shifted back to the predetermined frequency by the second shift means, and whereby the frequency of any backwardly propagating beam is shifted by the second amount as it propagates through the second shift means and then is shifted back to the predetermined frequency as it propagates through the first shift means; and attenuation means, disposed between the first and second shift means to receive any beam propagating therebetween and to attenuate any beam having a frequency equal to the predetermined frequency shifted by the second amount whereby any backwardly propagating beam is attenuated and is thereby isolated from the amplified laser beam.

Claim 24

A ring laser oscillator according to claim 20 wherein the attenuation means comprises a gas.

Claim 25

A ring laser oscillator according to claim 20 wherein the attenuation means comprises a Fabry-Perot resonator.

Claim 26

A ring laser oscillator according to claim 20 wherein one of the frequency shift means comprises a Bragg cell and signal means to provide an energizing signal to the Bragg cell.

Claim 27

A ring laser oscillator according to claim 23 wherein the Bragg cell comprises tellurium dioxide.

Claim 28

A frequency-stabilized isolating ring laser oscillator comprising: amplifier means, having an input for receiving a forwardly propagating laser beam of predetermined frequency to amplify the received beam; a plurality of reflector means, disposed to receive the amplified laser beam from the amplifier means and to reflect the beam along a predefined primary path around the amplifier and back into the input for further amplification; an acousto-optical isolator for deriving from the forwardly propagating amplified laser beam a frequency error signal, and for isolating from the beam any unwanted, backwardly propagating beam of like frequency, the isolator comprising: beam splitting means, disposed to receive the amplified laser beam and to deflect a portion thereof onto a secondary path; first frequency shift means, disposed across the primary and secondary paths, for shifting the frequency of a laser beam propagating along the primary path by a first amount and to shift the frequency of a laser beam propagating along the secondary path by a second amount, the second amount being the converse of the first amount; second frequency shift means, disposed forwardly of the first shift means along the primary path to receive the amplified laser beam and to shift the frequency thereof by said second amount, whereby the frequency of the beam is shifted by the first amount as the beam propagates along the primary path through the first shift means and then is shifted back to the predetermined frequency as the beam propagates through the second shift means and the frequency of any unwanted, backwardly propagating beam is shifted by the second amount as the beam propagates through the second shift means and then is shifted back to the predetermined frequency as the beam propagates through the first shift means; attenuation means, disposed between the shift means to receive any beam propagating therebetween and to attenuate any beam having a frequency equal to the predetermined frequency shifted by the second amount, whereby any backwardly propagating beam is attenuated and is thereby isolated and whereby a beam propagating along the secondary path is also attenuated; and detector means, disposed across the secondary path between the attenuation means and the second frequency shift means to receive the attenuated secondary beam and responsive thereto to provide a frequency error signal; and means responsive to the frequency error signal to correct the frequency of the oscillator.

Claim 29

A frequency-stabilized isolating ring laser oscillator comprising: amplifier means, having an input for receiving a forwardly propagating laser beam of predetermined frequency to amplify the received beam; a plurality of reflector means, disposed to receive the amplified laser beam from the amplifier means and to reflect the beam along a predefined primary path around the amplifier and back into the input for further amplification; an acousto-optical isolator for deriving from the forwardly propagating amplified laser beam a frequency error signal, and for isolating from the beam any unwanted, backwardly propagating beam of like frequency, the isolator comprising: beam splitting means, disposed to receive the amplified laser beam and to deflect a portion thereof onto a secondary path; first frequency shift means, disposed across the primary and secondary paths, for shifting the frequency of a laser beam propagating along the primary path by a first amount and to shift the frequency of a laser beam propagating along the secondary path by a second amount, the second amount being the converse of the first amount; second frequency shift means, disposed forwardly of the first shift means along the primary path to receive the amplified laser beam and to shift the frequency thereof by said second amount, whereby the frequency of the beam is shifted by the first amount as the beam propagates along the primary path through the first shift means and then is shifted back to the predetermined frequency as the beam propagates through the second shift means and the frequency of any unwanted, backwardly propagating beam is shifted by the second amount as the beam propagates through the second shift means and then is shifted back to the predetermined frequency as the beam propagates through the first shift means; attenuation means, disposed between the shift means to receive any beam propagating therebetween and to attenuate any beam having a frequency equal to the predetermined frequency shifted by the second amount, whereby any backwardly propagating beam is attenuated and is thereby isolated and whereby a beam propagating along the secondary path is also attenuated; and detector means, disposed across the secondary path between the attenuation means and the second frequency shift means to receive the attenuated secondary beam and responsive thereto to provide a frequency error signal; and means responsive to the frequency error signal to correct the frequency of the oscillator.

Claim 30

An oscillator according to claim 25 wherein the attenuation means comprises a gas.

Claim 31

An oscillator according to claim 25 wherein the attenuation means comprises a Fabry-Perot resonator.

Claim 32

An oscillator according to claim 25 wherein one of the frequency shift means comprises a Bragg cell and signal means to provide an energizing signal to the Bragg cell.

Claim 33

An oscillator according to claim 25 wherein the Bragg cell comprises tellurium dioxide.

Claim 34

A ring laser according to claim 25 wherein the means to correct the frequency comprises a piezolelectrically tunable mirror.

Claim 35

A noise-isolating laser radar comprising: transmitter means to provide a pulsed laser beam having a predetermined frequency; means to direct the pulsed laser beam toward a target whereby a portion of the beam is reflected back from the target along a reflection path; a switching isolator to isolate the reflected beam from any unwanted noise energy having a like frequency and propagating along the reflection path, the isolator comprising: first frequency shift means, disposed to receive optical energy propagating along the reflection path, responsive to a control signal to shift the frequency of the received energy selectively by a first amount or a second amount, the second amount being the converse of the first; second frequency shift means, disposed forwardly of the first shift means to receive optical energy propagating along the reflection path, responsive to said control signal to shift the frequency of the received energy back to the predetermined frequency; and attenuation means, disposed between the shift means to receive any optical energy propagating therebetween and to attenuate any such energy having a frequency equal to the predetermined frequency shifted by the second amount whereby such energy is attenuated and is thereby isolated; control signal means, responsive to the transmitter means to generate the control signal, the control signal selective the first amount in the first shift means and the second amount in the second shift means when the reflected laser beam is present and reversing said selections when the reflected laser beam is not present; and detector means, to provide a signal indicative of said reflected laser beam.

Claim 36

A noise-isolating laser radar comprising: transmitter means to provide a pulsed laser beam having a predetermined frequency; means to direct the pulsed laser beam toward a target whereby a portion of the beam is reflected back from the target along a reflection path; a switching isolator to isolate the reflected beam from any unwanted noise energy having a like frequency and propagating along the reflection path, the isolator comprising: first frequency shift means, disposed to receive optical energy propagating along the reflection path, responsive to a control signal to shift the frequency of the received energy selectively by a first amount or a second amount, the second amount being the converse of the first; second frequency shift means, disposed forwardly of the first shift means to receive optical energy propagating along the reflection path, responsive to said control signal to shift the frequency of the received energy back to the predetermined frequency; and attenuation means, disposed between the shift means to receive any optical energy propagating therebetween and to attenuate any such energy having a frequency equal to the predetermined frequency shifted by the second amount whereby such energy is attenuated and is thereby isolated; control signal means, responsive to the transmitter means to generate the control signal, the control signal selective the first amount in the first shift means and the second amount in the second shift means when the reflected laser beam is present and reversing said selections when the reflected laser beam is not present; and detector means, to provide a signal indicative of said reflected laser beam.

Claim 37

A laser radar according to claim 31 wherein the control signal means also provides a signal for deactivation following selected ones of the laser pulses, and further comprising means responsive to the signal for deactivation, for deactivating both frequency shift means during reception of said selected ones of the laser pulses.

Claim 38

An isolator according to claim 31 wherein the attenuation means comprises a gas.

Claim 39

An isolator according to claim 31 wherein the attenuation means comprises a Fabry-Perot resonator.

Claim 40

An isolator according to claim 31 wherein: one of the frequency shift means comprises a dual-transducer Bragg cell and signal means to provide an energizing signal to the Bragg cell, and the control means comprises means to apply the energizing signal selectively to either of the transducers.

Claim 41

An isolator according to claim 31 wherein the Bragg cell comprises tellurium dioxide.