USH822H - Method of amplitude modulating a laser beam - Google Patents

Method of amplitude modulating a laser beam Download PDF

Info

Publication number
USH822H
USH822H US07/344,723 US34472389A USH822H US H822 H USH822 H US H822H US 34472389 A US34472389 A US 34472389A US H822 H USH822 H US H822H
Authority
US
United States
Prior art keywords
aotf
laser
laser beam
voltage
amplitude
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Abandoned
Application number
US07/344,723
Inventor
John E. Nettleton
Dallas N. Barr
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
United States Department of the Army
Original Assignee
United States Department of the Army
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by United States Department of the Army filed Critical United States Department of the Army
Priority to US07/344,723 priority Critical patent/USH822H/en
Assigned to UNITED STATES OF AMERICA, THE, AS REPRESENTED BY THE SECRETARY OF THE ARMY reassignment UNITED STATES OF AMERICA, THE, AS REPRESENTED BY THE SECRETARY OF THE ARMY ASSIGNMENT OF ASSIGNORS INTEREST. Assignors: BARR, DALLAS N., NETTLETON, JOHN E.
Application granted granted Critical
Publication of USH822H publication Critical patent/USH822H/en
Abandoned legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/11Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on acousto-optical elements, e.g. using variable diffraction by sound or like mechanical waves

Definitions

  • This invention is in the field of amplitude modulators for laser beams.
  • the known modulators run the gamut from variable density filters to acousto-optic (AO) and electro-optic (EO) devices.
  • AO and EO devices are preferred, although both are very lossy (20%-60%).
  • they each generate two output beams, such that even the beam power remaining after the internal losses is split in half.
  • the present invention overcomes these disadvantages by the new of an old device to effect laser beam amplitude modulation.
  • This old device is a colinear acousto-optic tunable filter.
  • This invention is a method of amplitude modulating a laser beam by the new use of an old device, specifically, an acoustic-optic tunable filter (AOTF).
  • This AOTF consists of an anisotropic crystalline material such as thallium arsenic selenide (TI 3 AsSe 3 , or TAS for short) with a reflective interface and a piezo-electric transducer (PZT) affixed to one end of the TAS.
  • PZT piezo-electric transducer
  • FIG. 1 is a schematic showing of one optical layout on which the invention may be practiced.
  • FIG. 2 is another schematic showing of an optical layout on which the invention may be practiced.
  • AOTF acoustic-optical tunable filter
  • This AOTF includes a crystal of thallium arsenic selenide (TAS), an internal reflector, and a piezo-electric transducer (PZT) for operating the device.
  • This PZT designated with reference numeral 16 in the drawing is fed an A.C. signal or voltage from a modulating frequency generator 17.
  • the externally located (with respect to laser cavity) AOTF acts as an amplitude modulator whenever 17 feeds an A.C. voltage to PZT 17.
  • the output of 17 will be chosen.
  • 17 will provide a highly-stable frequency in order that the phase the modulation envelope of the reflected beam power from a distant object may be compared with the phase of the output of 17. If the beam is used for communication, 17 vary in frequency as required.
  • FIG. 2 shows laser 20 with highly reflective mirrors 21 and 22 output mirror 23.
  • Output beam 24 passes through half-wave plate 26, is reflected by mirror 27 and passes through Bragg-angle reflector 28.
  • Output beam 25 reflects from 28 and combined beam 29 enters AOTF 30.
  • the 26-27-28 arrangement produces two orthogonal linear polarizations in beam 29. This insures proper AOTF AM operation.
  • the AOTF 30 modulates input beam 29 under the action of PZT 31 fed by generator 32, to produce output beam 33.
  • the method of the invention is the new use of a well-known acoustic-optic tunable filter. Rather than use the filter for its normally intended purpose, it is used to amplitude modulate a laser beam. It is especially useful for high-powered lasers such as the CO 2 type.
  • the method thus includes the steps of directing the laser beam into the AOTF, and applying an A.C. voltage to the PCT of the AOTF.

Landscapes

  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)
  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)

Abstract

An acousto-optic tunable filter (AOTF), instead of being used for its intended use of frequency or wavelength tuning a laser from within its resonant cavity, is used outside the laser cavity to amplitude modulate the output beam of the laser. This is accomplished by directing the laser output beam into the AOTF and applying an A.C. voltage to a piezo-electric transducer which is a part of the AOTF.

Description

The invention described herein may be manufactured, used, and licensed by the U.S. Government for governmental purposes without the payment of any royalties thereon.
BACKGROUND OF INVENTION
This invention is in the field of amplitude modulators for laser beams. The known modulators run the gamut from variable density filters to acousto-optic (AO) and electro-optic (EO) devices. At present, insofar as response time and efficiency are concerned, AO and EO devices are preferred, although both are very lossy (20%-60%). Moreover, they each generate two output beams, such that even the beam power remaining after the internal losses is split in half. The present invention overcomes these disadvantages by the new of an old device to effect laser beam amplitude modulation. This old device is a colinear acousto-optic tunable filter.
SUMMARY OF THE INVENTION
This invention is a method of amplitude modulating a laser beam by the new use of an old device, specifically, an acoustic-optic tunable filter (AOTF). This AOTF consists of an anisotropic crystalline material such as thallium arsenic selenide (TI3 AsSe3, or TAS for short) with a reflective interface and a piezo-electric transducer (PZT) affixed to one end of the TAS. A laser beam directed into the AOTF is amplitude modulated by an A.C. signal applied to the PZT.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a schematic showing of one optical layout on which the invention may be practiced.
FIG. 2 is another schematic showing of an optical layout on which the invention may be practiced.
DESCRIPTION OF PREFERRED EMBODIMENT
The method of the invention may be best understood if this description is taken in conjunction with the drawings. Referring now to FIG. 1, we see laser 10 with highly-reflective mirror 11 and output mirror 12, and with output beam 13 passing through quarter-wave plate 14 into acoustic-optical tunable filter (AOTF) 15. The quarter-wave plate imparts circular polarization to the linearly polarized beam 13. This is desirable because of the manner in which the AOTF operates. The AOTF is a known device disclosed in a SPIE paper entitled "Rapid Tuning Mechanism for CO2 Lasers" by L. J. Denes, et al., at the SPIE O-E LASE '88 meeting in Los Angeles, CA in January 1988. This AOTF includes a crystal of thallium arsenic selenide (TAS), an internal reflector, and a piezo-electric transducer (PZT) for operating the device. This PZT, designated with reference numeral 16 in the drawing is fed an A.C. signal or voltage from a modulating frequency generator 17. Instead of acting as a tunable filter which it usually does, the externally located (with respect to laser cavity) AOTF acts as an amplitude modulator whenever 17 feeds an A.C. voltage to PZT 17. Depending upon the use to which the modulated laser beam is put, the output of 17 will be chosen. For example, if the beam is used for CW ranging, 17 will provide a highly-stable frequency in order that the phase the modulation envelope of the reflected beam power from a distant object may be compared with the phase of the output of 17. If the beam is used for communication, 17 vary in frequency as required.
FIG. 2 shows laser 20 with highly reflective mirrors 21 and 22 output mirror 23. Output beam 24 passes through half-wave plate 26, is reflected by mirror 27 and passes through Bragg-angle reflector 28. Output beam 25 reflects from 28 and combined beam 29 enters AOTF 30. The 26-27-28 arrangement produces two orthogonal linear polarizations in beam 29. This insures proper AOTF AM operation. The AOTF 30 modulates input beam 29 under the action of PZT 31 fed by generator 32, to produce output beam 33.
The method of the invention is the new use of a well-known acoustic-optic tunable filter. Rather than use the filter for its normally intended purpose, it is used to amplitude modulate a laser beam. It is especially useful for high-powered lasers such as the CO2 type. The method thus includes the steps of directing the laser beam into the AOTF, and applying an A.C. voltage to the PCT of the AOTF.

Claims (1)

We claim:
1. A method of amplitude modulating a laser beam, including the steps of:
directing said laser beam into a colinear acousto-optic tunable filter including an anisotropic medium with a piezo-electric transducer affixed thereto; and
applying an A.C. voltage to said transducer, whereby said laser is amplitude modulated to produce a modulation envelope in accordance with said A.C. voltage.
US07/344,723 1989-04-28 1989-04-28 Method of amplitude modulating a laser beam Abandoned USH822H (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US07/344,723 USH822H (en) 1989-04-28 1989-04-28 Method of amplitude modulating a laser beam

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US07/344,723 USH822H (en) 1989-04-28 1989-04-28 Method of amplitude modulating a laser beam

Publications (1)

Publication Number Publication Date
USH822H true USH822H (en) 1990-09-04

Family

ID=23351735

Family Applications (1)

Application Number Title Priority Date Filing Date
US07/344,723 Abandoned USH822H (en) 1989-04-28 1989-04-28 Method of amplitude modulating a laser beam

Country Status (1)

Country Link
US (1) USH822H (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5200964A (en) * 1991-03-12 1993-04-06 General Instrument Corporation Broad linewidth lasers for optical fiber communication systems

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3958863A (en) 1975-01-10 1976-05-25 Westinghouse Electric Corporation Tl3 TaS4 and Tl3 TaSe4 crystals and acousto-optical devices
US4217036A (en) 1978-04-17 1980-08-12 Itek Corporation Acoustic-optic coherent modulator and detection system
US4448494A (en) 1981-06-17 1984-05-15 Hazeltine Corporation Acousto-optical signal detector
US4460250A (en) 1981-06-17 1984-07-17 Hazeltine Corporation Acousto-optical channelized processor
US4793676A (en) 1985-08-21 1988-12-27 The Board Of Trustees Of The Leland Stanford Junior University Optical fiber acousto-optic amplitude modulator

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3958863A (en) 1975-01-10 1976-05-25 Westinghouse Electric Corporation Tl3 TaS4 and Tl3 TaSe4 crystals and acousto-optical devices
US4217036A (en) 1978-04-17 1980-08-12 Itek Corporation Acoustic-optic coherent modulator and detection system
US4448494A (en) 1981-06-17 1984-05-15 Hazeltine Corporation Acousto-optical signal detector
US4460250A (en) 1981-06-17 1984-07-17 Hazeltine Corporation Acousto-optical channelized processor
US4793676A (en) 1985-08-21 1988-12-27 The Board Of Trustees Of The Leland Stanford Junior University Optical fiber acousto-optic amplitude modulator

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5200964A (en) * 1991-03-12 1993-04-06 General Instrument Corporation Broad linewidth lasers for optical fiber communication systems

Similar Documents

Publication Publication Date Title
US6031852A (en) Rapid acoustooptic tuner and phase-shifter
US4841528A (en) Frequency doubled, cavity dumped feedback laser
EP1037338B1 (en) Tunable high powered laser
US5230005A (en) Electronic tuning of a broadband laser
US4441186A (en) Electronically switchable multiwavelength laser system
GB1363143A (en) Polarization independent light modulation means using birefringent crystals
JPH0511678B2 (en)
US4788514A (en) Optical modulation arrangement
US5034627A (en) Power laser generator with control of the direction of emission of the output beam
US5721748A (en) Intracavity doubled solid state Raman laser system
US4028636A (en) Acousto-optical deflector tuned organic dye laser
EP0805532B1 (en) Optical parametric oscillator
US5394412A (en) Power laser with deflection
US4110788A (en) Multiple wavelength acoustooptic deflection
US4484333A (en) Coupled waveguide freespace laser
US5754572A (en) Mirrorless, distributed-feedback, ultraviolet, tunable, narrow-linewidth, solid state laser
US4105953A (en) Chirped acousto-optic Q switch
USH822H (en) Method of amplitude modulating a laser beam
GB1356421A (en) Optical resonator apparatus
EP1312224A1 (en) Fibre optic projection device
US3996525A (en) Acousto-optically tuned laser
WO2019145322A1 (en) Device and method for generating laser pulses by kerr lens based mode locking with a loss-modulation device as a kerr medium
US4393517A (en) Pulse code modulation of laser pulse tail
US3902137A (en) Electro-optic diffraction grating tuned laser
EP0556016B1 (en) Wavelength variable laser device

Legal Events

Date Code Title Description
AS Assignment

Owner name: UNITED STATES OF AMERICA, THE, AS REPRESENTED BY T

Free format text: ASSIGNMENT OF ASSIGNORS INTEREST.;ASSIGNORS:NETTLETON, JOHN E.;BARR, DALLAS N.;REEL/FRAME:005253/0982;SIGNING DATES FROM 19890427 TO 19890428

STCF Information on status: patent grant

Free format text: PATENTED CASE