GB2119109A - Optical scanning system - Google Patents

Optical scanning system Download PDF

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Publication number
GB2119109A
GB2119109A GB08211743A GB8211743A GB2119109A GB 2119109 A GB2119109 A GB 2119109A GB 08211743 A GB08211743 A GB 08211743A GB 8211743 A GB8211743 A GB 8211743A GB 2119109 A GB2119109 A GB 2119109A
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GB
United Kingdom
Prior art keywords
light
diffracted
source
optic
interaction region
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.)
Granted
Application number
GB08211743A
Other versions
GB2119109B (en
Inventor
John Stuart Heeks
Stephen Wright
John David Jackson
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.)
STC PLC
Original Assignee
Standard Telephone and Cables PLC
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 Standard Telephone and Cables PLC filed Critical Standard Telephone and Cables PLC
Priority to GB08211743A priority Critical patent/GB2119109B/en
Publication of GB2119109A publication Critical patent/GB2119109A/en
Application granted granted Critical
Publication of GB2119109B publication Critical patent/GB2119109B/en
Expired legal-status Critical Current

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Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/125Optical beam sources therefor, e.g. laser control circuitry specially adapted for optical storage devices; Modulators, e.g. means for controlling the size or intensity of optical spots or optical traces
    • G11B7/128Modulators
    • 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
    • G02F1/29Devices 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 position or the direction of light beams, i.e. deflection
    • G02F1/33Acousto-optical deflection devices

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  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Nonlinear Science (AREA)
  • General Physics & Mathematics (AREA)
  • Optical Recording Or Reproduction (AREA)

Abstract

An optical scanning system comprises an acousto-optic diffraction device 4 with a surface acoustic wave transducer 5 energised 6 with pulses of r.f. causing narrow regions of acoustic wave energy 7 to traverse a planer light beam 3 causing localised diffraction and focussing of the light 11 which scans medium 9. Regions 7 effect frequency and polarisation shift of the light and so a polarising or optical frequency discriminating element may be used to block the undiffracted light. The system may be used in a recording or playback device. <IMAGE>

Description

SPECIFICATION Optical scanning system This invention relates to an optical scanning system having no moving parts, such as may be used in a recording arrangement or an image forming arrangement.
Known prior art optical scanning systems use, for instance, mirrors or prisms which are oscillated or rotated to cause a modulated and focussed beam of light to scan a medium. Such systems often involve precision moving parts and complex beam forming optics. Mechanical scanning systems have inherent speed limiting characteristics and reliability problems.
A system having no mechanical moving parts can provide a fast and high resolution scanner with a reduction in the complexity of its beam forming optics.
According to the present invention there is provided an optical scanning system comprising a light source, means for focussing light from the source into a substantially parallel planar beam, an acoustic-optic device having adjacent one surface a planar acousto-optic interaction region traversed by said planar beam, means for launching into the acousticoptic interaction region a surface acoustic wave pulse propagating in a direction orthogonal to the direction of the light beam whereby the wave pulse causes the interaction region material to effect diffraction and focussing of light traversing the region, and means for discriminating the diffracted and focussed beam of light emerging from the acousto-optic interaction region.
An embodiment of the invention will now be described with reference to the accompanying drawing which illustrates an optical scanning system in diagrammatic form only.
A light source 1, typically a semiconductor laser, has its output focussed by beam forming optics 2 into a collimated planar beam 3. An acoustic-optic device 4 is placed in the path of the beam 3. The device comprises a planar electro-optic and piezoelectric substrate 5, e.g. lithium niobate, into the surface region of which a planar optical waveguide interaction structure is formed by means of thermal indiffusion of metal (e.g. titanium or by ion implantation). Formed on the substrate surface is a surface acoustic wave (SAW) transducer 6, e.g. an interdigitated metal electrode pattern. Energisation of the transducerwith an r.f. signal of a suitable frequency causes a surface acoustic wave 7 to propagate across the interaction region. The far end of the SAW path is provided with an acoustic absorbtion pad 8.If the transducer 6 is driven with a short pulse of r.f.
energy, e.g. a so-calied "chirp" pulse, then the SAW energy is propagated as a short pattern 7. Therefore the effective interaction between the acoustic energy and the beam of light is confined to a narrow region which moves across the collimated beam of light.
The acosto-optic device is configured as a Bragg cell deflector in which the travelling acoustic wave pattern acts as a travelling optical grating simulaneously to diffract and focus a narrow portion of the collimated beam and to scan the focussed portion 11 across a recording medium 9. The acoustic-optic device employs birefringent diffraction to change the optical polarisation of the scanning portion of the beam whilst the rest of the beam remains undiffracted. An optical polarisation filter 10 placed between the device 4 and the medium 9 effectively blocks the undiffracted light whilst the narrow scanning portion, the polarisation of which has been changed, can pass through the filter to reach the medium.
As an alternative to the polarisation filter it is possible to use an optical frequency discrimination element since besides changing the polarisation the diffraction grating also effects a frequency shift on the diffracted light. Hence, if the source 1 is monochromatic a simple frequency filter will effectively discriminate between the diffracted and the undiffracted light.
In a recording arrangement the scanning system is used to scan a signal-modulated beam of light across the recording medium 9.
In addition to using the scanning system to record it can also be used to read pre-recorded media. If the recording is in the form of a mask, e.g. a photographic plate with binary encoded information on it, the narrow diffracted portion can be scanned along a line of binary bits, with a photodetection means (not shown) behind the mask. Alternatively, for a reading system, the polarising or frequency discriminating filter 10 can be placed behind the record medium 9, between the medium and the photodetector means.

Claims (10)

1. An optical scanning system comprising a light source, means for focussing light from the source into a substantially parallel planar beam, an acoustic-optic device having adjacent one surface a planar acousto-optic interaction region traversed by said planar beam, means for launching into the acousticoptic interaction region a surface acoustic wave pulse propagation in a direction orthogonal to the direction of the light beam whereby the wave pulse causes the interaction region material to effect diffraction and focussing of light traversing the region, and means for discriminating the diffracted and focussed beam of light emerging from the acousto-optic interaction region.
2. A system according to claim 1, including means for modulating the light source with an information signal.
3. A system according to claim 1 or 2, wherein the diffracted light is focussed on a recording medium.
4. A system according to claim 1, wherein the diffracted light is focussed on a pre-recorded medium.
5. A system according to any preceding claim, wherein the discrimination means comprises a polarising filter arranged to block undiffracted light.
6. A system according to any one of claims 1 to 4, wherein the discrimination means comprises a fre quencyfilter arranged to block light at the optical frequency of the source.
7. A system according to claim 5 or 6, wherein the filter is placed between the diffraction means and the recording or pre-recorded medium.
8. A system according to any preceding claim, wherein the light source is a laser.
9. An optical scanning system substantially as described with reference to the accompanying drawing.
10. A method of scanning a beam of light across a surface including the steps of focussing light from a source into a substantially parallel planar beam, directing said planar beam into an acousto-optic diffraction means, energising said diffraction means with a burst of r.f. energy, whereby a narrow acoustic-optic interaction region is caused to traverse the optical beam to diffract the light in the beam and focus the diffracted light and filtering said diffracted and focussed light to discriminate it from the undiffracted light.
GB08211743A 1982-04-22 1982-04-22 Optical scanning system Expired GB2119109B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
GB08211743A GB2119109B (en) 1982-04-22 1982-04-22 Optical scanning system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
GB08211743A GB2119109B (en) 1982-04-22 1982-04-22 Optical scanning system

Publications (2)

Publication Number Publication Date
GB2119109A true GB2119109A (en) 1983-11-09
GB2119109B GB2119109B (en) 1985-08-07

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
GB08211743A Expired GB2119109B (en) 1982-04-22 1982-04-22 Optical scanning system

Country Status (1)

Country Link
GB (1) GB2119109B (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2167202A (en) * 1984-11-16 1986-05-21 Stc Plc Data storage systems
US4887310A (en) * 1986-08-01 1989-12-12 Thomson Csf Identification system using a laser retro-reflecting and modulating set
US5278816A (en) * 1989-09-22 1994-01-11 Russell James T Recording/reproducing system using wavelength/depth selective optical storage medium
WO2008032061A3 (en) * 2006-09-12 2008-10-30 Ucl Business Plc Imaging apparatus and methods
US9069227B2 (en) 2011-04-20 2015-06-30 Ucl Business Plc Methods and apparatus to control acousto-optic deflectors
US9341919B2 (en) 2010-04-21 2016-05-17 Ucl Business Plc Methods and apparatus for controling drive frequencies of acousto-optic deflectors

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB1564911A (en) * 1975-09-10 1980-04-16 Itek Corp Noncollinear tunable acoustic-optic filter

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB1564911A (en) * 1975-09-10 1980-04-16 Itek Corp Noncollinear tunable acoustic-optic filter

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2167202A (en) * 1984-11-16 1986-05-21 Stc Plc Data storage systems
US4887310A (en) * 1986-08-01 1989-12-12 Thomson Csf Identification system using a laser retro-reflecting and modulating set
US5278816A (en) * 1989-09-22 1994-01-11 Russell James T Recording/reproducing system using wavelength/depth selective optical storage medium
WO2008032061A3 (en) * 2006-09-12 2008-10-30 Ucl Business Plc Imaging apparatus and methods
US8294977B2 (en) 2006-09-12 2012-10-23 Ucl Business Plc Imaging apparatus and methods
JP2013152471A (en) * 2006-09-12 2013-08-08 Ucl Business Plc Beam deflection device and method
EP2634622A1 (en) * 2006-09-12 2013-09-04 UCL Business PLC Imaging apparatus and methods
US8687268B2 (en) 2006-09-12 2014-04-01 Ucl Business Plc Imaging apparatus and methods
US9104087B2 (en) 2006-09-12 2015-08-11 Ucl Business Plc Imaging apparatus and methods
US9341919B2 (en) 2010-04-21 2016-05-17 Ucl Business Plc Methods and apparatus for controling drive frequencies of acousto-optic deflectors
US9069227B2 (en) 2011-04-20 2015-06-30 Ucl Business Plc Methods and apparatus to control acousto-optic deflectors

Also Published As

Publication number Publication date
GB2119109B (en) 1985-08-07

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PCNP Patent ceased through non-payment of renewal fee