SINGLE MIRROR INTEGRAL RAMAN LASER

Abstract: A Raman laser (10) using a pump laser (22) as a source of radiation at a first wavelength and a Raman cell (30) for converting the first wavelength radiation to a second wavelength. The pump laser (20) provides polarized radiation at a predetermined first wavelength which is focused by a focusing means (40) into a Raman medium (32) which converts radiation at the first wavelength to a predetermined second wavelength by Raman scattering processes. A reflection means (50) which is aligned normal to the first wavelength radiation is disposed between the pump laser (20) and focusing means (40). The reflection means is substantially 100% reflective of radiation at the second wavelength and substantially non-reflective of radiation at the first wavelength. A polarizing means (70) and quarter-wave plate (60) are disposed along the optical path between the Raman medium (32) and the pump laser (20) for allowing propagation of the first wavelength to the Raman medium (32) but preventing SBS radiation from entering the pump laser (20) from the Raman medium. Alternatively, the pump laser includes an output reflection means (126) that is substantially (100% reflective of radiation at the second wavelength and partially reflective of radiation at the first wavelength. This embodiment achieves automatic alignment of the pump laser and the Raman medium (32) and does not use additional reflection means, polarization means, or a quarter-wave plate.

Description: SINGLE MIRROR INTEGRAL RAMAN LASER BACKGROUND OF THE INVENTION This invention relates to lasers and more particularly to Raman lasers or Raman cells driven by laser sources. The invention further relates to Nd:ϊAG driven Raman lasers. Advanced ranging or tracking devices use reflected light from a laser source in order to ascertain target and range data for many applications. It is obviously desirable to operate such devices at wavelengths which are considered "eye-safe" in order to reduce risk to personnel encountering the direct or reflected beams of laser light. The term "eye-safe" is applied to radiation that does not, in general, cause tissue damage to the human eye. It is known that for wavelengths between 400 and 1400 nanometers, radiation tends to cause retinal damage; while for wavelengths longer than 1400 nanometers, the radiation is absorbed within or near the surface of the cornea and much higher levels of radiation can be tolerated before reaching the level that can cause corneal damage. Research in the area of laser safety has led to the development of specific standards for "eye-safe" lasers. The "Regulations for the Administration and Enforcement of the Radiation Control for Health and Safety Act of 1968", published by the U.S. Department of Health, generally supports the wavelength of 1.54μm as the standard for "eye-safe." The standards for lasers operating at this wavelength allow several orders of magnitude greater output energy and power than for non "eye-safe" lasers. Raman lasers utilizing a Raman scattering medium can be used to convert laser radiation of one wavelength to a longer wavelength. This allows lasers operating at non "eye-safe" wavelengths to produce radiation within the "eye-safe" wavelength region. For example, by using methane with a frequency shift of 2916 cm' 1 , a Nd:YAG laser operating at a wavelength of 1.06μm can have its output converted to the "eye-safe" 1.54μm wavelength. The 1.06μm laser radiation is coupled into a resonator containing the methane Raman medium and produces scattered radiation at the 1.54μm wavelength. Raman shifted lasers such as those described in U.S. Patent Numbers 4,103,179, issued to W. Schniedt, and 3,668,420 issued to J. T. Vanderslice use a Raman cell resonator to convert l.Oδμra wavelength radiation from a pump laser to 1.54μm. The Raman resonator of each of these patents has a pressurized gas medium disposed along an optical path between two mirrors. One mirror, the input mirror, is substantially totally transmissive at 1.06μm and substantially totally reflective at 1.54μm. This allows 1.06μm radiation to enter the cell but does not allow 1.54μm radiation back into the pumping laser. The second mirror, the output mirror, is partially reflective at 1.54μm and substantially totally reflective at 1.06μm. This configuration allows the output of 1.54μm radiation from the Raman resonator but traps the 1.06μm pumping radiation. However, this Raman resonator technique is not without its limitations. The Raman scattering process is intensity dependent. Therefore, any decrease in pump radiation intensity lessens the conversion efficiency of radiation to the new wavelength. Improper alignment, spacing or curvature of the mirrors in the Raman cell resonator causes the radiation to diverge from central axis or degrade the focus within the Raman cell. This in turn lowers the intensity and thus decreases conversion. The Raman resonator formed by mirrors also needs to be precisely aligned with the pump laser and associated optics to insure optimum radiation transfer into the Raman resonator and maintain maximum pump intensity along the focused optical path. In addition, other scattering processes such as Stimulated Brilluoin Scattering (SBS) can greatly decrease the wavelength conversion efficiency. The SBS radiation returns through the Raman medium and the input mirror to the pump laser. Large enough amounts of radiation returning to the pump laser causes opera- tional problems or damage. SBS normally occurs to some extent within the Raman medium but is greatly enhanced for misaligned optics. The SBS and Raman scattering processes are in direct competition within the medium. The threshold for onset of SRS must be below the SBS threshold so that SRS occurs first, and energy is depleted from the medium by transfer into radiation at the desired Raman wavelength. However, misaligned optics increase the SRS threshold by detuning the Raman resonator and by causing non-overlapping paths for the incident pump radiation and Raman scattered radiation. The SBS is reflected back into the pump laser and can damage the pump laser or severely impact on its performances. What is needed is a method and apparatus to ensure good alignment of the driver laser and Raman cell and simplification of the overall Raman laser. SUMMARY Accordingly, the present invention provides a Raman laser apparatus having the advantage of automatic alignment between the pump laser and Raman medium. Additionally, the invention provides improved efficiency and simplified optics. These and other advantages are realized in a Raman laser using a pump laser for producing a predeter¬ mined wavelength of polarized radiation and a Raman medium for wavelength conversion. The pump laser uses an output reflection means partially reflective of the polarized radiation as an output interface. An enclosure with input and output windows con- ' taining a Raman medium is positioned along the optical path of the pump laser output radiation. A focusing means is positioned adjacent to the Raman medium for focusing radiation from the pump laser into the Raman medium. A second reflection means is positioned on the pump laser side of the focusing means and is substantially totally reflective of 1.54μm radiation but substantially non-reflective of 1.06μm radiation. A polarizer and quarter-wave plate are positioned between the second reflection means and the output reflection means to prevent return of SBS radiation from the Raman medium into the pump laser. In a second embodiment, the output reflection means of the pump laser is partially reflective of 1.06μm radiation and substantially totally reflective of 1.54μm radiation. In addition, a collimating means can be positioned adjacent to the output window of the Raman medium enclosure for collimating 1.54μm radiation produced in the Raman laser. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a schematic view of a Raman laser according to the invention. Figure 2 is a schematic view of another embodiment of a Raman laser of the invention. DETAILED DESCRIPTION OF THE INVENTION We have constructed a new Raman laser without the use of a conventional resonator around the Raman medium. With pump laser radiation input at one end of a Raman medium, Raman shifted output is obtained at the other end without reflectors on both ends of the optical path through the Raman medium. Referring now to Figure 1, Raman laser 10 employs a pump laser 20 as a source of substantially monchromatic polarized radiation. Pump laser 20 comprises many elements (not shown) known in the art and uses one of several known lasing media. For purposes of clarity, the preferred embodiment is described using a Nd:YAG laser operating at 1.064μm (1064nm), although it will become apparent to one skilled in the art that other laser materials and wavelengths can be used. The Nd:YAG medium 22 of pump laser 20, is typically positioned between two reflection means (one shown as 24) forming an optical resonator. In this arrangement, the output occurs through one reflection means 24, which is partially reflective of radiation at 1.06μm. Reflection means 24 can be an optical quality plate with a reflective coating, a polished mirror or other means known in the art. The preferred embodiment for reflection means is an optical quality glass plate having a partially reflective coating on one side. Generally, laser output reflectors are constructed with an anti-reflection coating on the outer surface and the reflective coating on the other. However, the coating location can be reversed. The only requirement is that a sufficient amount of radiation be confined within laser 20 to support the laser oscillation. Typically, the reflective coating on reflection means 24 is approximately 30% reflective of 1.06μm radiation for a Nd:YAG laser. To achieve the high intensity required of pump laser 20, an optical Q-switch is included in the optical resonator. The Q-switch (not shown) can be a saturable or bleachable dye cell, or other means known in the art, which is optically bleached to achieve transparency at predetermined energy densities or optical intensities. Therefore, energy builds up in the pump laser resonator until the Q-switch becomes optically transparent at which time the resonator Q greatly increases and a high peak power pulse is produced. In the preferred embodiment, the 1.06μm radiation exiting pump laser 20 through output reflection means 24 is directed to a Raman cell 30 for conversion to 1.54urn. Raman cell 30 employs a Raman medium 32 such as, but not limited to, pressurized methane confined within an enclosure 34 having input and output windows 36 and 38, respectively. The efficiency for the conversion of 1.06μm radiation to 1.54μm by scattering processes within enclosure 34, is dependent on the intensity of the incident radiation Ij., (from pump laser 20) the gain of the Raman medium, g, and the length, L, of the interaction zone in Raman medium 32. These factors are generally related by the expression: where I(- is the transmitted/converted intensity and I 0 is a very low level intensity output due to thermal conversion in the medium. Raman lasers, such as those of Schmidt and Vanderslice, use mirrors adjacent to the input and output windows, to create multi-pass resonators within the Raman medium in enclosure 34. This is done to increase It by increasing factors on the right side of Equation (1). Radiation is concentrated along a narrow beam path by concave mirrors to increase li and given a multi-pass path within the Raman medium to increase L. However, an efficient Raman laser can be constructed without the use of such a resonator for Raman medium 32. For a two- or threefold increase in the intensity of the incident optical radiation, I , no reflective surface is needed adjacent to output window 36 of Raman cell 30. However, high efficiency is difficult to obtain because of competing nonlinear effects. In the preferred embodiment, the factors on the right side of Equation (1) are increased by using a lens and a single reflector. A lens 40 is positioned adjacent the input window 36 of enclosure 34. Alternatively, lens 40 replaces window 36 itself. This lens focuses radiation from pump laser 20 into enclosure 34 and increases the intensity of the incident radiation at its focal point. Near the focal point of lens 40, along the direction of propagation, for some threshold of input energy the radiation intensity is sufficiently high to support Raman scattering and efficiently produce wavelength conversion. However, below this threshold input beam energy, radiation deposited in this region of enclosure 34 is not efficiently converted to the new wavelength. The input energy threshold can be reduced with a longer interaction length to increase the gain. Therefore, a reflection means 50 is provided to create such a longer interaction zone. Reflection means 50 is positioned adjacent lens 40 on the pump laser side of enclosure 34. Reflection means 50 can be, but is not limited to, an optical flat quality glass plate having a coating reflective at 1.54μm. The reflective coating, not shown, on reflection means 50 can reside on either side as in the case of reflection means 24. The only limitation is that reflection means 50 is preferred to be substantially totally reflective of radiation at the converted wavelength of 1.54μm and substantially non-reflective of 1.06μm radiation. There generally exists some thermal noise and spontaneous Raman scattering in Raman medium 32 which give rise to the I 0 term of Equation (1). The thermal noise results from some degree of conversion of local molecular vibrational energy into the wavelength of interest (1.54μm). Such natural radiation exists throughout Raman medium 32. Some thermal noise and/or spontaneous scattered radiation propagates from a region on the output side of enclosure 34 toward lens 40 through the high gain interaction zone in the lens 40 focal region. Here the existing radiation encounters pump laser radiation resulting in stimulated converted radiation at 1.54μm coherently reinforcing the existing radiation and forming a 1.54μm beam propagating toward input window 34 and lens 40. The 1.54μm radiation propagates through lens 40 where it encounters reflection means 50 which reflects the radiation back through lens 40 and enclosure 34. On the return pass through enclosure 34 the radiation stimulates the conversion of more incident pump laser radiation to the 1.54μm wavelength. The converted radiation then propagates as an in-phase 1.54μm laser beam out of enclosure 34 through output window 38. The power required for the wavelength conversion of radiation from pump laser 20 depends on the nature of the Raman medium and pump laser but for purposes of this embodiment, the pump laser produces energy in the range of a few megawatts. The above embodiment can still suffer from the previously described misalignment complications. Therefore, a polarizer 70 and quarter wave pTate 60 combination, as known in the art, are used to prevent SBS radiation from re-entering pump laser 20. Polarizer 70 transmits the already polarized radiation from pump laser 20. Quarter-wave plate 60 is oriented to divide polarized radiation from pump laser 20 into two equal components and shift this phase by 90° to produce circularly polarization. SBS radiation reflected back through quarter-wave plate 60 undergoes a second 90° phase shift to become the orthogonal polarization to that of pump laser 20 and is reflected out of the optical path by polarizer 70. Therefore, the combination of polarizer 70 and quarter- wave plate 60, as known in the art, allows polarized pump laser radiation to propagate to Raman cell 30 but prevents SBS from re-entering pump laser 20. This process establishes isolation of the pump laser from SBS radiation previously described. To further decrease alignment and SBS problems, an alternate embodiment of the invention is presented. Referring now to Figure 3, Raman laser 100 uses a pump laser 120 and a Raman cell 130 arranged in the same manner as pump laser 20 and cell 30 of the previous embodiment. Laser medium 22, Raman medium 32, enclosure 34, windows 36 and 38, and lens 40 have the same functions as the corresponding parts in the previously described embodiment. However, output reflection means 24 is replaced by output reflection means 124, and reflection means 50, polarizer 70 and quarter-wave plate 60 are not used. Reflection means 124 has a reflective coating on one surface which is partially reflective of pump laser radiation, in this case, 1.06μm wavelength, and substantially 100% reflective of the wavelength radiation produced in Raman cell 30, here 1.54μm. The reflective coating on reflection means 124 can reside on either side of means 124. The result of this arrangement is that the function of reflecting converted radiation from enclosure 34 back through enclosure 34 is performed by the output reflector for pump laser 20. Therefore, whatever the alignment of Raman cell 130 relative to pump laser 120, radiation transferred through lens 40 into enclosure 34 and converted to the new Raman wavelength, as previously described, returns through lens 40 along substantially the same path. The converted wavelength radiation is then reflected by reflection means 124 back into enclosure 34 where it enhances conversion as previously described. Because the radiation will always cover a closely identical path, automatic alignment of the optics is achieved and the Raman process is very efficient and dominates over SBS. Therefore, very little SBS radiation exists or is reflected toward pump laser 20, eliminating the problem of damage to the pump laser. SUBSTITUTESHEET Example I A Nd:YAG pump laser 20 producing a 50 millijoule output beam of Q-switched 1.06μm radiation was used to drive a Raman cell 30 containing pressurized methane gas and having a reflection means 50 adjacent to a lens 40 as per the embodiment of FIG. 1. The energy output of the Raman laser was 14 millijoules of 1.54μm radiation. Example II The second embodiment, described above, was also tested with reflection means 50 removed and a reflective, optically flat, surface used as part of the output of pump laser 20. This configuration produced 21 milli- joules of 1.54μm radiation from the 50 millijoule beam of l.Oδμm radiation. Therefore, the second embodi- . ment of the invention represents a 50 percent increase in efficiency over the first embodiment, and in addition has the advantage of the automatic alignment described above. Practicing the method and apparatus of the invention provides a Raman laser with improved efficiency and automatic alignment of the pump laser and Raman cell. There is decreased complexity for the optics and a compact unitary structure arises. For purposes of clarity and in keeping with the primary intended application to which the invention is directed, the preferred embodiments have been described using a gaseous Raman medium such as methane. However, the Raman medium employed can be one of several gases, liquids or solids that are known to produce SRS radiation at desired wavelengths. Examples of other Raman media include carbon monoxide, hydrogen, deuterium, ammonia and a variety of glasses. The specific media employed is determined by the desired output wavelength, the laser source wavelength, allowable complexity, and power requirements. The method and apparatus of the present invention provides an improved Raman laser for a variety of Raman media. The foregoing description of preferred embodiments has been presented for purposes of illustration and description. It is not intended to be exhaustive nor to limit the invention to the precise form disclosed, and many modifications and variations are possible in light of the above teaching. The embodiments were chosen and described to best explain the principles of the invention and its practical application to thereby enable others skilled in the art to best utilize the invention in various embodiments and with various modifications as are suited to the particular use contemplated. It is intended that the scope of the invention be defined by the claims and their equivalents,

Claims: CLAIMS What is Claimed is; 1. A Raman laser comprising: a pump laser for providing a source of polarized radiation at a predetermined first wavelength; a Raman medium disposed along the optical path of said first wavelength radiation from said pump laser for converting radiation at said first wave¬ length to a predetermined second wavelength by Raman scattering processes; focusing means disposed between said pump laser and said Raman medium and positioned adjacent said Raman medium for focusing said first wavelength radiation into said Raman medium; reflection means disposed between said pump laser and said focusing means and positioned adjacent said focusing means, being substantially 100% reflective of radiation at said second wavelength and substantially non-reflective of said first wavelength radiation; and a polarizing means and quarter-wave plate combination disposed along the optical path of said first wavelength radiation between said pump laser and said reflective means for allowing polarized first wavelength radiation to propagate to said Raman medium but preventing Stimulated Brilluoin Scattered radiation from said Raman medium from propagating to said pump laser. 2. A Raman laser as recited in Claim 1 wherein said pump laser is an optically pumped Nd:YAG laser. 3. A Raman laser as recited in Claim 1 wherein said first wavelength radiation is 1.06μm wavelength radiation. 4. A Raman laser as recited in Claim 1 wherein said second wavelength radiation is 1.54μm wavelength radiation. 5. A Raman laser as recited in Claim 1 further comprising an enclosure surrounding said Raman medium, said enclosure having input and output windows for the passage of radiation. 6. A Raman iaser as recited in Claim 5 wherein said Raman medium comprises a pressurized gas selected from the group consisting of hydrogen, deuterium or methane. 7. A Raman laser as recited in Claim 5 wherein said Raman medium comprises pressurized methane. 8. A Raman laser as recited in Claim 5 further comprising collimation means positioned adjacent said output window of said enclosure for forming a collimated laser beam of radiation at said second wavelength. 9. A Raman laser as recited in Claim 1 wherein said focusing means is a convex lens. 10. A Raman laser as recited in Claim 1 wherein said reflection means is a dielectric coated optically flat glass plate. 11. A Raman laser comprising: a pump laser for producing radiation at a predetermined first wavelength comprising a lasing medium disposed in a resonant optical cavity having an output reflection means that is substantially 100% reflective of radiation at a predetermined second wavelength and partially reflective of radiation at said first wavelength; a Raman medium disposed along the optical path of said first wavelength from said pump laser for converting radiation at said first wavelength to a predetermined second wavelength by Raman scattering processes; and focusing means disposed between said pump laser and said Raman medium for focusing said first wavelength radiation into said Raman medium positioned adjacent said Raman medium. 12. A Raman laser as recited in Claim 11 wherein said lasing medium comprises an optically pumped Nd:YAG medium. 13. A Raman laser as recited in Claim 11 wherein said first wavelength is 1.06μm. 14. A Raman laser as recited in Claim 11 wherein said second wavelength is 1.54μm. 15. A Raman laser as recited in Claim 11 further comprising an enclosure surrounding said Raman medium, said enclosure having input and output windows for the passage of radiation. 16. A Raman laser as recited in Claim 15 wherein said Raman medium comprises a pressurized gas selected from the group consisting of deuterium, hydrogen or methane. 17. A Raman laser as recited in Claim 15 wherein said Raman medium comprises pressurized methane. 18. A Raman laser as recited in Claim 11 wherein said output reflective means is a dielectric coated optically flat glass plate. 19. A Raman laser as recited in Claim 11 wherein said focusing means is a convex lens. _> 20. A Raman laser as recited in Claim 11 further comprising collimating means positioned adjacent said Raman medium for forming a collimated laser beam from radiation at said second wavelength.

Inventors: BRUESSELBACH HANS W, DEWHIRST DONALD R, BRUESSELBACH, HANS, W., DEWHIRST, DONALD, R.
Applicants: HUGHES AIRCRAFT CO, HUGHES AIRCRAFT COMPANY
Application year: 1985
Main classification: H01S3
IPC codes: H01S3