CONTROLLING RADIATION BEAM DIAMETERS

Abstract: The invention relates to a method and an apparatus for reducing the diameter tolerance of a laser beam. A lens (3) is positioned so that one of the focal planes of the lens (3) is in the region of a limit (5) of the Rayleigh range of the beam (19). The lens (3) forms a second beam waist at a position (6), where a modulator (10) is placed. The beam (21) then passes through beam expansion apparatus (11,12,13) before being collimated by a lens (14). The collimated beam (25) is then focussed to a third beam waist at the recording drum (17), via a lens (18) and mirror (15).

Description: This invention relates generally to the field of image processing and controlling the diameters of laser beams. Conventional lasers produce beams with a diameter tolerance which is typically ±15%. In the field of digital image reproduction such as described in our European patent application 0095936, a laser beam is controlled in response to digital image information to impinge on a record medium. One of the problems with the wide tolerance in the beam diameter is that with the pixel densities now common in the imaging field, any significant variation in the diameter of the beam will result in some blurring of the resulting image. Another problem with conventional laser beams is that the diameter of the laser beam varies around its cross-section. This results in a beam having an elliptical form which is particularly undesirable when the beam is to be modulated using an acousto-optic modulator. Unless the modulator is particularly accurate, and thus expensive, it will cause the degree of eccentricity to increase. Beam modulators, such as acousto-optic modulators, can also introduce eccentricity into a previously circular beam. All the problems outlined above would be reduced if the tolerance in the beam diameter could be reduced. Normally, this would require the careful adjustment of a number of lenses to set an appropriate magnification. This is time consuming and requires a complex setting arrangement. DE-A-3001653 is concerned with special problems which arise when modulating multiple beams. In accordance with the present invention, apparatus for generating a beam of coherent radiation comprising only the fundamental transverse mode comprises a radiation beam generator of the kind that generates a beam having a beam waist (W₁); a lens positioned such that the focal plane of the lens is positioned in the region of a limit of the Rayleigh range from the beam waist (W₁), such that a second beam waist (W₂) is formed; and a beam modulator situated at the position of the second waist (W₂). The invention makes use of the property of beams of coherent radiation comprising, preferably only, the fundamental transverse mode (ie. TEM₀₀) that the beam diverges from a position at which the beam has a minimum diameter (hereinafter referred to as a "waist"). By positioning a converging lens downstream of the waist, a second waist will be generated with dimensions having a much smaller tolerance than those of the first waist. The general relationship between the radius (W₁) of the first waist, the radius (W₂) of the second waist, the focal length (f) of the lens and the distance (Z) from the lens to the first waist is as follows: It can be shown by solving this equation that the change in the radius of the second waist W₂ with respect to the first waist W₁ is a minimum when ie. the focal plane of the lens is at either end of the Rayleigh range. The Rayleigh range of a radiation beam is defined as the distance from the waist at which the beam diameter has increased by a factor of √2. This in fact corresponds to a distance of: The invention avoids any need for complex lens adjustment and it is not even necessary to know the value of the first waist diameter. As mentioned above, since W₂ has turning points when the distance Z is suitably chosen, the value of W₂ will be substantially invariant relative to variations in the size of the diameter of the first waist. In fact, for a tolerance of ±15% in the diameter of the first waist, it is possible to achieve a tolerance of about ±2% in the diameter of the second waist. The beam may comprise a beam of optical radiation and may be accompanied by other, diffracted beams including transverse oscillation modes. In many cases, the first waist is positioned within the radiation generator such as a laser cavity. In some examples, however, the first waist will be positioned outside the radiation generator. A more detailed discussion of the property of beams which form waists can be found in "Elements of Modern Optical Design" by D.C. O'Shea, published in 1985 by John Wiley & Sons Inc, pages 230-241. The lens may be a converging or diverging lens. The apparatus is particularly suitable in our Crosfield Datrax Imaging system in which a modulator, such as an acousto-optic modulator is positioned at the second waist. This will reduce the extent to which the modulator can increase any ellipticity in the beam. Since the variation in beam diameter at the second waist is very small, and substantially invariant, any eccentricity at the first waist will have been substantially removed from the beam at the second waist. The invention can also be used to reduce the eccentricity introduced in an otherwise circular beam by modulators such as acousto-optic modulators. In that situation, the modulator will cause the value W₁ to vary between two extremes around the cross-section of the beam. This problem can be minimised by utilising the beam at the second waist (eg. by causing the beam at the second waist to impinge on a record medium) at which variations in W₂ around the cross-section will have been minimised. Two examples of a method and apparatus according to the invention will now be described with reference to the accompanying drawings, in which:- Figure 1 is a schematic view of one example of the apparatus; Figure 2 is a schematic view of a second example of the apparatus; Figure 3 illustrates part of a third example; and, Figure 4 illustrates how the invention may be used in conjunction with laser scanning apparatus. In Figure 1 a laser 1 generates a coherent beam of optical radiation comprising only the fundamental transverse mode TEM₀₀. The beam 2 is guided to a converging lens 3. As is illustrated diagrammatically in the drawing, the beam 2 diverges from one end 4 of the laser 1 at which it has a minimum radius W₁. In other words, the beam has a waist at this position. At a position labelled 5 the radius of the beam has increased to W₁√2. This position is at the limit of the Rayleigh range of the beam and the length of the Rayleigh range is given by the formula πW₁²/λ . The converging lens 3 is positioned at a distance f from the position 5 equal to its focal length. The converging lens 3 causes the beam to converge downstream of the lens to a minimum radius W₂ defining a second waist 6. The beam thereafter diverges. The variation of W₂ with W₁ is given in equation 1 above. Consider an example in which the system is designed with f = 100 mm and for W₁ to be equal to W₂. In that case W₁ equals 0.155 mm and πW₁²/λ = 70.7 mm and therefore Z₁ equals 170.7 mm. Now consider variations in W₁. These cause corresponding variations in W₂ but to a much smaller extent as set out in the table below. W₁ W₂ Z₂ .124 .148 200.3 .139 .153 185.4 .155 .155 170.7 .170 .153 157.4 .186 .150 146.0 As can be seen, for a variation in W₁ of ±20%, W₂ only varies by ±2.4%. In the table, all magnitudes are in millimetres. It will be seen that the invention also enables the problem of eccentricity to be reduced. Although the value of W₁ may vary around the cross-section of the beam, the corresponding variation in W₂ will be much less and thus the actual values of W₂ around the cross-section will be very similar. In Figure 2 the converging lens 3 has been positioned so that the distance Z₁ from the beam waist W₁ to the lens is equal to the focal length f of the lens minus the Rayleigh range πW 2 / 1/λ. In other words, the focal plane of the lens 3 has been placed at the Rayleigh range limit opposite to that of Figure 1 corresponding to a distance -πW 2 / 1/λ from the beam waist W₁. This is at position 35. Thus Z₁ = f - πW 2 / 1/λ. The performance of the apparatus in this example is identical to the performance of the apparatus in the first example described above. The examples shown in Figures 1 and 2 made use of a converging lens 3. The invention is equally applicable for use with a diverging lens and an example of such an arrangement is shown in Figure 3 although the laser source has been omitted in this drawing. In this example, rays of light from the source impinge on a diverging lens 7 from the left, as seen in the drawing, and, in the absence of the lens 7, would form a waist 8 having a radius W₁. The lens 7 causes the rays to diverge from an apparent, virtual beam waist 9 having a radius W₂ which is substantially invariant as in the Figure 1 example. In a typical example, where f is -100 mm, the Rayleigh range is 100 mm, and W₁ is 0.184 mm, this will mean that Z₁ is 200 mm, W₂ is 0.13 mm, and Z₂ is -150 mm. The invention can be used in conjunction with laser scanning apparatus, as illustrated in Figure 4. The lens 3 is placed at a distance, equal to its focal length, from the Rayleigh range limit 5 of the laser beam 19 emitted from the laser 1. The lens 3 produces a converging beam 20 and at the waist 6 of the beam 20, the acousto-optic modulator 10 is placed. Since the variation in beam diameter at the second waist is very small, and substantially invariant with respect to the first waist, any eccentricity at the first waist will have been substantially removed from the beam at the second waist. The beam 21 exiting from the acousto-optic modulator 10 is then reflected by a plane mirror 11 and passes through a diverging lens 12 which causes beam 23 to diverge, therefore expanding it. The beam 23 is then reflected by a plane mirror 13 and is collimated by a converging lens 14. The collimated laser beam 25 then passes through another converging lens 18 which focusses the beam 27 to a third beam waist at the recording drum 17 at a point 28, after being reflected by a mirror 15 in the centre of the recording drum 17. The mirror 15 is rotated by a shaft 29 attached to a motor 16. This causes the beam 27 to rotate, thereby exposing a section of the recording drum 17. By mounting the mirror 15 and the lens 18 on a lead screw (not shown), they can be made to move axially along the drum 17, thereby exposing the entire surface area of the drum 17. A record medium is positioned on the outer surface of the drum 17 which is transparent. An example of suitable laser scanning apparatus is described in EP-A-0095936.

Claims: Apparatus for generating a modulated beam (2) of coherent radiation comprising only the fundamental transverse mode the apparatus comprising a radiation beam generator (1) of the kind that generates a beam having a beam waist (W₁); a lens (3) positioned such that the focal plane of the lens is positioned in the region of a limit of the Rayleigh range (5) from the beam waist (W₁), such that a second beam waist (W₂) is formed; and a beam modulator (10) situated at the position (6) of the second waist (W₂). Apparatus according to claim 1, wherein the modulator is an acousto-optic modulator (10). An image recording system including apparatus according to claim 1 and a record medium support (17) positioned such that a record medium is situated at a position (28) at which the radiation beam forms a third beam waist.

Inventors: AUGHTON, JOHN EDWARD, GRAY, JAMES HUIE
Applicants: CROSFIELD ELECTRONICS LIMITED
Application year: 1987
Main classification: G02B27
IPC codes: G02B6, B23K26, G02B27, G02F1, G05D25