RADIATION COUPLING ARRANGEMENTS

Abstract: An optical apparatus including a laser producing in use an output laser beam and an optical guide for guiding radiation of the output laser beam when incident thereon and characterised by means for depleting of free charge carriers a region in a path to be traversed by the output laser beam between the laser and the guide.

Description: Radiation coupling arrangements The present invention relates to radiation coupling arrangements. In particular, it relates to a method and an apparatus for coupling laser radiation into an optical guide. There are many practical applications in which high power laser beams are required to be transmitted via optical guides. For example, lasers used in surgical applications are employed together with optical fibre cables. There are a number of technical difficulties associated with the coupling of high power, pulsed laser radiation with optical fibre cables. One such difficulty arises when the laser beam is focused into the fibre. Since many fibres have core diameters less than 1 mm, very large peak power densities of laser radiation may be produced on the end face of the fibres. This can result in significant damage to the fibres and, therefore, a rapid deterioration in the optical transmission characteristics of the fibres. To date, a number of techniques have been developed to facilitate the coupling into optical fibres of radiation outputs of high power pulsed lasers. One such technique involves the use of tapered fibres. This type of fibre is manufactured in such a way that one end has a considerably larger diameter than the other end (eg 1 cm and 1 mm respectively) . When a laser beam is focused onto the larger diameter end, power densities on the face of the fibre are considerably reduced. However, these tapered fibres are very expensive and are not ideally suited to certain applications (eg laser surgery) as the fibres are expensive and the cost of replacing the fibres after each use is likely to be prohibitive. In a typical laser-to-fibre guide coupling arrangement the output laser beam is normally focused by a lens onto the fibre(ε). The focal point of the lens is set to be soi.e distance in front of the fibre in order that a diverging beam enters the fibre. If the focal point of the lens is situated within the fibre, very high laser power densities will be produced at the focus within the fibre material resulting in a high probability of fibre •damage. In the known coupling arrangement described, a problem arises at very high laser powers in the following way. There is a limiting laser power density above which the air through which the laser beam travels becomes ionised and produces a plasma ("laser-induced plasma") . Typical power densities required to produce a plasma in air are of the order 10^-° watts per cm 2 . Power densities of this order a readily obtainable when the output beams of certain pulsed lasers such as Nd.YAG (Q-switched) are focused using conventional optical lenses. Once a plasma is produced, plasma shielding prevents further laser radiation from entering the fibre. It is the purpose of the present invention to provide an arrangement for coupling the output of a laser, especially a high power pulsed laser beam, into an optical guide in which the problem of producing a laser-induced plasma is eliminated or at least reduced in effect. According to the present invention in a first aspect there is provided an optical apparatus including a laser producing in use an output laser beam and an optical guide for guiding radiation of the output laser beam when incident thereon and characterised by means for depleting of free charge carriers a region in a path to be traversed by the output laser beam between the laser and the guide. According to the present invention in a second aspect there is provided a method of coupling laser radiation from a laser to an optical guide using the apparatus of the first aspect which includes directing the output laser beam produced by the laser onto the guide whilst maintaining, in a region in the path traversed by the output laser beam, a depletion of free charge carriers. The said means for depleting may comprise means for producing in the said region an electric field. The said means for depleting may comprise an electrode to which an electrical potential may be applied from a high voltage source. The applied potential may exceed lkV, and desirably exceeds 5kV. The applied potential may be negative (with respect to earth) to facilitate depletion of free electrons existing in the atmospheric gas in the said region by repulsion in a direction away from the electrode. Charge carriers, specifically free electrons, will normally exist in the air through which the output laser beam has to pass. Electrons may be present due, for example, to cosmic ray interactions or dust particles. These electrons may be accelerated to high energies by a laser beam via a process known as inverse Bremsstrahlung. They may then interact with the gas atoms and molecules of the air and create an avalanche of electrons. The avalanche electrons are also accelerated by the laser radiation and eventually a plasma can be formed. This process takes place over a timescale of the order of nano¬ seconds. However, if the air in the path of the laser beam is depleted of free-electrons in accordance with the present invention, then the probability of plasma formation for a given laser power density is considerably reduced. This allows laser radiation to be coupled into the optical guide with reduced risk of cut-off. The region between the laser and the guide is conveniently in an evacuable chamber in which the air pressure may be reduced in order to lower the number of potential sites at which free charge carriers may exist. The electrode preferably provides a sharp point which facilitates the production of a localised high intensity electric field. The electrode conveniently comprises a portion providing a pin electrode. The said point is desirably located close to the path traversed by the laser beam. The output laser beam may be focused by one or more lenses in order to reduce the cross-sectional area of the beam to better match that of the guide. The focal point of the lens or combination of lenses may be in front of the guide (ie between the lens and the guide) . The said region depleted of free carriers may include the focal point. For example, the said electrode point may be located adjacent to the focal point preferably with the point of the electrode aimed substantially at the focal point. The optical guide may comprise a known optical guide, eg one or more optical fibres, eg a bundle of fibres, eg made of a suitable high quality glass. The laser may be any known laser which produces an output beam capable of producing a laser induced plasma in normal atmospheric conditions. The laser may for instance, be a solid state laser, a dye laser, or gas laser which may provide a continuous or pulsed output. The output may be in the visible electromagnetic region but it could be non-visible, eg infra-red radiation, depending upon the application to which the radiation is to be put. Where the laser provides a pulsed output it may for instance be a Q-switched laser. Where the laser is a solid state laser it may for example be a ruby laser or a garnet laser, eg Nd-YAG. Where the laser is gas laser it may be a C0 2 laser, an He-Ne laser or an excimer laser. The apparatus according to the present invention may be employed in a variety of known applications employing guided optical radiation, eg surgical inspection, surface decontamination and encapsulation techniques (as in Applicants' PCT WO 93/13531), surface stripping as in Applicants' GB 9322845, surface profile measurement as in Applicants' GB 9323054.8, remote temperature sensing as Applicants' EP 93308966.6. Embodiments of the present invention will now be described by way of example with reference to the accompanying drawings, in which: Figure 1 is a diagrammatic side view of a laser beam production, coupling and guiding arrangement embodying the present invention. As shown in Figure 1, a Nd-YAG Q-switched laser 1 provides an output pulsed laser beam 3 of average peak power -10 10 watts per cm 2 . The beam 3 is directed toward a fibre-optic bundle guide 7 having an end 7a. The beam 3 is focused by a lens 5 to a focal point F in front of the end 7a of the guide 7, the cross-sectional area of the beam 3 incident on the end 7a being less than that of the beam emerging from the laser 1. A high voltage source 9 is connected to an electrode 11 having a projection comprising a pin 13. The end of the pin 13 remote from the source 9 is adjacent to the focal point F. The region extending from the laser to the guide 7 through the focus F is in a chamber (not shown) at reduced pressure. In use, the source 9 provides a high negative voltage of about 6kV. The electrode 11 and the pin 13 are thus maintained at a negative potential of about -6kV. The strong electric field produced in the region of the focal point F by the pin 13 causes acceleration of free electrons away from the focal point F thereby depleting that region of free electrons. When the laser 1 is energised, the probability of plasma formation in the region of the focal point F is thereby reduced and the beam 3 is allowed to reach the end 7a of the guide 7 without cut-off. The guide 7 is flexible and guides the laser radiation from the beam 3 to an object (not shown) to which it is applied in a known way eg for one of the purposes mentioned above.

Claims: CLAIMS 1. An optical apparatus including a laser producing in use an output laser beam and an optical guide for guiding radiation of the output laser beam when incident thereon and characterised by means for depleting of free charge carriers a region in a path to be traversed by the output laser beam between the laser and the guide. 2. An apparatus as in Claim 1 and wherein the means for depleting including means for producing an electric field in the said region. 3. An apparatus as in Claim 2 and wherein the means for producing an electric field includes an electrode and a high voltage source for applying an electrical potential to the electrode. 4. An apparatus as in Claim 3 and wherein the electrical potential applicable by the voltage source exceeds lkV. 5. An apparatus as in Claim 3 or Claim 4 and wherein the electrical potential applicable by the voltage source is negative with respect to earth. 6. An apparatus as in any one of Claims 3, 4 or 5 and wherein the electrode provides a sharp point. 7. An apparatus as in any one of the preceding Claims and including one or more lenses to focus the output beam of the laser. 8. An apparatus as in Claim 7 insofar as dependent upon Claim 6 and wherein the point of the electrode is arranged to be adjacent to and aimed at the focal point of the lens or lenses. 9. Apparatus as in any one of the preceding Claims and wherein the optical guide comprises one or more optical fibres. 10. Apparatus as in any one of the preceding Claims and wherein the laser comprises a solid state laser, a dye laser or a gas laser. 11. Apparatus as in Claim 10 and wherein the laser is such as to produce either a continuous or pulsed output. 12. Apparatus as in Claim 1 and substantially as hereinbefore described with reference to the accompanying drawings. 13. A method of coupling laser radiation from a laser to an optical guide using the apparatus claimed in any one of the preceding Claims which includes directing the output laser beam produced by the laser onto the guide whilst maintaining, in a region in the path traversed by the output laser beam, a depletion of free charge carriers. 14. A method as in Claim 13 wherein the region between the laser and the guide is contained in a chamber at reduced atmospheric pressure.

Inventors: PERKS RICHARD MARC, WHITEHOUSE ANDREW IAN, WILLIAMS ALED WYN, PERKS, RICHARD, MARC, WHITEHOUSE, ANDREW, IAN, WILLIAMS, ALED, WYN
Applicants: BRITISH NUCLEAR FUELS PLC, PERKS RICHARD MARC, WHITEHOUSE ANDREW IAN, WILLIAMS ALED WYN, PERKS, RICHARD, MARC, WHITEHOUSE, ANDREW, IAN, WILLIAMS, ALED, WYN
Application year: 1995
Main classification: G02B6
IPC codes: A61B18, G02B6, H01S3