Optical wavelength converter device and optical wavelength converter module

Abstract: Fiber Cherenkov type optical wavelength converter device includes a cladding having an exit end for emitting a wavelength-converted wave. The exit end of the cladding is either of a conical shape, or supports a grating composed of concentric patterns which convert the conical wavefront of the wavelength-converted wave into a plane or spherical wavefront. Alternatively, the optical wavelength converter module comprises a fiber Cherenkov type optical converter device and an optical device, such as a lens or grating device, which convert the conical wavefront of the wavelength-converted wave into a plane or spherical wavefront.

Description: The present invention relates to an optical wavelength converter device, in accordance with the generic clauses of claims 1, 2, 18 and 19, which converts a fundamental wave into a second harmonic, having a wavelength which is 1/2 of that of the fundamental wave; to a fiber-type optical wavelength converter device which converts a fundamental wave into a third harmonic; to a fiber-type optical wavelength converter device which converts fundamental waves having two different wavelengths into a wave having a frequency equal to the sum of or the difference between the fundamental waves; and to an optical wavelength converter module which employs such an optical wavelength converter device. More particularly, it relates to an optical wavelength converter device and an optical wavelength converter module, both of which can convert the conical wavefront of a wavelength-converted wave into a plane or spherical wavefront. Such an optical wavelength converter is already described in Patent Abstracts of Japan, vol. 12, no. 220 (p-720) [3067] 23rd June 1988; JP-A-63 15 235 which discloses an optical wavelength converter device for obtaining a second higher harmonic beam having a small diameter by forming the end part of the second higher harmonic side of the clad in a tapered shape, such that the diameter of its beam emitting end face is extremely small. From document EP-A-0 342 523 an arrangement for generating light at a second harmonic of an input light is already known. In order to produce parallel light rays, a collimator lens is applied to collimate the second harmonic beam. Various attempts have heretofore been made to convert the wavelength of a laser beam into a second harmonic, i.e., shortening the wavelength of a laser beam, using nonlinear optical material. One well known example of such an optical wavelength converter device for effecting such laser wavelength conversion is the bulk crystal type converter device as disclosed in Introduction to Optical Electronics, pages 200 - 204, written by A. Yariv and translated by Kunio Tada and Takeshi Kamiya (published by Maruzen K.K.). This optical wavelength converter device relies upon the birefringence of a crystal in order to meet phase matching conditions. Therefore, material which does not exhibit birefringence, or exhibits only small birefringence, even if it has high nonlinearity cannot be employed. To solve the above problem, a fiber type optical wavelength converter device is proposed. The optical wavelength converter device of this type is in the form of an optical fiber comprising a core made of nonlinear optical material and surrounded by a cladding. One example of such an optical fiber is shown in the vol. 3, No. 2, pages 28 - 32, bulletin of the microoptics research group of a gathering of the Applied Physics Society. Recently, many efforts are directed to the study of the fiber type optical wavelength converter device since it can easily gain phase matching between a guided mode in which a fundamental is guided through the core and a radiated mode in which a second harmonic is radiated into the cladding (the so-called Cherenkov radiation). The wavelength-converted wave produced by any of the above optical wavelength converter devices is emitted from the output end of the cladding and has various applications. In many of the applications, the wavelength-converted wave is converged into a small spot. For example, the wavelength-converted wave is focused into a very small spot for higher recording density when a wavelength-converted wave is used optically to record information signals. However, it is recognized that the wavelength-converted wave emitted from the fiber Cherenkov type optical wavelength converter device cannot converge into a small spot even if the emitted wave is passed through a general spherical lens. It is an object of the present invention to provide an optical wavelength converter device, capable of converging a wavelength-converted wave into a small spot, and an optical wavelength converter module, which employs such an optical wavelength converter device. This object is met by the characterizing features of claims 1,2,18 and 19. The principles of the present invention are based on the finding that a wavelength-converted wave (which is emitted at a certain phase matching angle and in phase with a fundamental wave) radiated into the cladding of a fiber Cherenkov type optical wavelength converter device has a conical wavefront. According to the present invention, an optical wavelength converter device comprises a fiber Cherenkov type optical wavelength converter device which includes a cladding having an exit end for emitting a wavelength-converted wave, the exit end of the cladding being conical so that if converts the conical wavefront of the wavelength-converted wave into a plane wavefront. As will be described later on, the slanted surface of the conical exit end of the cladding must have a certain angle selected on the phase matching angle in order to convert the conical wavefront into a plane wavefront. Japanese Unexamined Patent Publication No. 63(1988)-15235 discloses a fiber type optical wavelength converter device which has a cladding that is progressively tapered toward its exit end. However, the wavelength-converted wave is not emitted from the tapered portion of the cladding, but from a small inner cladding end perpendicular to the axis of the fiber. Since the angle of the tapered surface of the cladding is not selected on the phase matching angle, the disclosed fiber type optical wavelength converter device is different from the optical wavelength converter device according to the present invention. Another optical wavelength converter device according to the present invention comprises a fiber Cherenkov type optical wavelength converter device which includes a cladding with an exit end for emitting a wavelength-converted wave. The exit end has a grating composed of equally spaced concentric patterns which convert the conical wavefront of the wavelength-converted wave into a plane wavefront. Also, according to the present invention, there is an optical wavelength converter module comprising an optical wavelength converter device, of the type described above, and an optical device disposed in a position to receive a wavelength-converted wave emitted from the exit end of the cladding of the optical wavelength converter device, which converts the conical wavefront of the received wavelength-converted wave into a plane wavefront. The optical device may for example be a lens either having a conical entrance surface and/or a conical exit surface, a graded-index lens which is functionally equivalent to the above lens, or a grating having equally spaced concentric patterns. The optical device may be spaced from, or held intimately against, the exit end of the cladding. If the conical wavefront of the wavelength-converted wave is converted into a plane wavefront by the optical lens, the conical exit end of the cladding, or the grating of equally spaced concentric patterns on the exit end of the cladding, then the wavelength-converted wave can converge into a small spot when passed through an ordinary spherical lens. According to the present invention, still another optical wavelength converter device comprises a fiber Cherenkov type optical wavelength converter device which includes a cladding having an exit end for emitting a wavelength-converted wave, and the exit end of the cladding having an aspherical lens surface for converting the conical wavefront of the wavelength-converted wave into a spherical wavefront. Yet another optical wavelength converter device according to the present invention comprises also a fiber Cherenkov type optical wavelength converter device including a cladding which has an exit end for emitting a wavelength-converted wave, the exit end having a grating composed of concentric patterns for converting the conical wavefront of the wavelength-converted wave into a spherical wavefront. The present invention further provides an optical wavelength converter module comprising an optical wavelength converter device of the type described above and an optical device disposed in a position to receive the wavelength-converted wave emitted from the exit end of the cladding of the optical wavelength converter; this converts the conical wavefront of the received wavelength-converted wave into a spherical wavefront. The optical device may for example be a lens having entrance and exit surfaces thereof, being conical and spherical or a grating having concentric patterns which functions equivalently to the above lens. The optical device may be spaced from, or held intimately against, the exit end of the cladding. If the conical wavefront of the wavelength-converted wave is converted into a convergent spherical wavefront by the optical lens, the aspherical lens surface of the exit end of the cladding, or the grating of concentric patterns on the exit end of the cladding, then the wavelength-converted wave can be converged into a small spot. Even if the conical wavefront of the wavelength-converted wave has been converted into a divergent spherical wavefront, the wavelength-converted wave can be converged into a small spot by passing it through an ordinary spherical lens. The above object and other objects, as well as the features and advantages of the present invention will become more apparent in the following description taken in conjunction with the accompanying figures in which the preferred embodiments of the present invention are shown. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a schematic perspective view of an optical wavelength converter device according to the first embodiment of the present invention, Figure 2 is a side elevational view showing the manner in which the optical wavelength converter shown in Figure 1 is used, Figure 3 is a schematic view showing a process of manufacturing the optical wavelength converter device shown in Figure 1, Figure 4 is an enlarged fragmentary sectional side elevational view of the optical wavelength converter device shown in Figure 1, Figure 5 is a sectional side elevational view and Figure 6 is a front elevational view of an optical wavelength converter device according to the second embodiment of the present invention, Figures 7, 8, 9, 10, 11, 12, 13 and 14 are sectional side elevational views of optical wavelength converter modules according to the respective third, fourth, fifth, sixth, seventh eighth, ninth and tenth embodiments of the present invention, Figure 15 is a schematic perspective view of an optical wavelength converter device according to the eleventh embodiment of the present invention, Figure 16 is a side elevational view showing the manner in which the optical wavelength converter shown in Figure 15 is used, Figure 17 is an enlarged fragmentary sectional side elevational view of the optical wavelength converter device shown in Figure 15, Figure 18 is a sectional side elevational view and Figure 19 is a front elevational view of an optical wavelength converter device according to the twelfth embodiment of the present invention, Figures 20, 21 and 22 are sectional side elevational views of optical wavelength converter modules according to the thirteenth, fourteenth, and fifteenth embodiments, respectively, of the present invention, Figure 23 is a fragmentary sectional side elevational view illustrating the configuration of a grating of concentric patterns in the optical wavelength converter module shown in Figure 22, Figure 24 shows the manner in which the optical wavelength converter module is produced, and Figure 25 is a sectional side elevational view of an optical wavelength converter module in accordance with the sixteenth embodiment of the present invention. DESCRIPTION OF THE PREFERRED EMBODIMENTS Identical parts are denoted by identical reference numerals throughout the figures. Figures 1 and 2 show an optical wavelength converter device 10 according to the first embodiment of the present invention. The optical wavelength converter device 10 comprises an optical fiber including a core 11, which is made of a nonlinear optical material and filled into the hollow space defined centrally in the cladding 12. The nonlinear optical material of the core 11 is preferably an organic nonlinear optical material having a high wavelength conversion efficiency. In this embodiment, the core 11 is made of 3,5-dimethyl-1-(4-nitrophenyl)pyrazole (hereinafter referred to as "PRA"). The process of manufacturing the optical wavelength converter device 10 will be described below with reference to Figure 3. It is assumed that the core 11 is made of PRA and the cladding 12 is made of SFS3 glass. A hollow glass fiber 12′ which will serve as the cladding 12 is provided, the hollow glass fiber 12′ having an outside diameter of about 3mm and the hollow space therein having a diameter of about 2µm, for example. As shown in Figure 3, PRA is kept as a molten solution 11′ in a furnace, and one end of the glass fiber 12′ is immersed in the molten solution 11′. The molten solution 11′ of PRA then enters the hollow space in the glass fiber 12′ due to capillarity. The molten solution 11′ is kept at a temperature slightly higher than the melting point of PRA (102°C) in order to prevent the PRA from being decomposed. Thereafter, the glass fiber 12′ is quickly cooled, causing the PRA in the hollow space to be polycrystallized. Then, the glass fiber 12′ is gradually pulled from the furnace, which is kept at a temperature higher than the melting point of PRA (e.g. 102.5°C), into the outer space, which is kept at a temperature lower than that melting point, thereby causing the molten PRA to be monocrystallized continuously at the point where it is withdrawn from the furnace. The core 11 thus prepared is of highly long monocrystalline form with a uniform crystal orientation. The optical wavelength converter device 10 is thereby made sufficiently long. After the core 11 is filled in the glass fiber 12′, the opposite ends of the glass fiber 12′ are cut off at suitable points. One end 10a (Figure 2) of the glass fiber, which is to serve as an entrance for receiving the light beam, is cut perpendicularly to the axis of the glass fiber. The other cladding end 12a of the glass fiber is finished to a conical shape by a known grinding process. In this manner, the optical wavelength converter device 10, shown in Figures 1 and 2, is produced. The configuration of the cladding end 12a will be described later on. The optical wavelength converter device 10 is used as shown in Figure 2. A semiconductor laser 16, capable of emitting a laser beam 15 (having a wavelength of 870nm, for example), is employed as the fundamental wave generating means. The laser beam (fundamental wave) 15 emitted as a divergent beam from the semiconductor laser 16 is converted by a collimator lens 25 to a parallel beam whose cross section is then shaped into a circular shape by beam shaper prisms 26, 27. The laser beam 15 is then converged by an objective lens 28 and applied to the entrance end 10a (the end of the core 11) of the optical wavelength converter device 10. The laser beam 15 now enters the core 11. The laser beam or fundamental wave 15 is then converted by the PRA of the core 11 into a second harmonic 15′ whose wavelength is 1/2 of the wavelength of the fundamental wave 15. The second harmonic 15′ is radiated into the cladding 12 and travels through the device 10 toward the opposite exit end thereof. Phase matching is achieved between a guided mode, in which the fundamental wave 15 is guided through the core 11, and a radiated mode, in which the second harmonic 15′ is radiated into the cladding 12 (Cherenkov radiation). The second harmonic 15′ is emitted out of the device 10 from the end 12a of the cladding 12. The fundamental wave 15, which has been guided through the core 11, is emitted from the end 11a of the core 11. A light beam 15″, containing the second harmonic 15′, and the fundamental wave 15 then goes through a filter 18 which passes only the second harmonic 15′. Therefore, only the second harmonic 15′ is extracted by the filter 18. The second harmonic 15′ then passes through a condenser lens 19 in the form of a general spherical lens by which it is converged into a small beam spot P. Figure 2 does not show any device which utilizes the second harmonic 15′. However, such a device usually utilizes the focused spot of the second harmonic 15′. Operation of the conically shaped end 12a of the cladding 12 will hereinafter be described in detail. In this embodiment, as shown in Figure 4, the cladding 12 is thick enough for the second harmonic 15′ radiated into the cladding 12 at a phase matching angle  to be emitted out of the device 10 directly from the cladding end 12a without being totally reflected by the outer surface of the cladding 12. To achieve this, the diameter D of the cladding 12 should be selected to meet the condition: D > 2L·tan + d where d is the diameter of the core 11 and L is the length of the outer peripheral surface of the cladding 12. With such dimensional limitations, the wavefront of the second harmonic 15′ traveling through the cladding 12 is oriented as indicated by the arrows W in Figure 4 in one plane including the core axis. Therefore, the wavefront is of a conical shape as a whole. It is now assumed that the refractive index of the cladding 12 is indicated by n C , the refractive index of a medium (usually air) around the device 10 by n A , the angle of incidence of the second harmonic 15′ to the cladding end 12a by α, and the angle at which the cladding end 12a is inclined to a plane normal to the core axis by δ. Then, if the following equation is satisfied: n C sinα = n A sinδ the wavefront of the second harmonic 15′ emitted out of the cladding 12 will become a plane wavefront. By putting α = δ -  into the above equation and solving the equation for δ, we get: δ = tan -1 ( n C sin n C cos - n A ) since the angle δ at which the cladding end 12a is cut is selected to be of the value defined above, the second harmonic 15′ emitted out of the optical wavelength converter device 10 has a plane wavefront. Consequently, it is possible to converge the second harmonic 15′ into a small beam spot P by passing the second harmonic 15′ through the condenser lens 19. An optical wavelength converter device according to the embodiment of the present invention will be described below with reference to Figures 5 and 6. The optical wavelength converter device, denoted at 20, has a cladding end 12a for emitting a second harmonic 15′, the cladding end 12a having a surface extending perpendicularly to the core axis. A grating 21 composed of equally spaced concentric patterns is disposed on the surface of the cladding end 12a. The grating 21 may be formed by the photolithographic process. According to this embodiment, the diameter D of the cladding 12 is thick, ranging from 1mm to 3mm, for example, so that condition (1) given above can be satisfied. Then, the grating 21 can be formed on the cladding end 12a relatively easily. The grating 21 has a pitch Λ (a radial increment) by which the concentric patterns thereof are radially spaced and is selected as follows: Λ = λ n C sin By having the second harmonic 15′ pass through the grating 21, the conical wavefront of the second harmonic 15′ can be converted into a plane wavefront. Thus, the second harmonic 15′ can be focused into a small beam spot P by the condenser lens 19. Figure 7 shows an optical wavelength converter module 30 according to the third embodiment of the present invention. The optical wavelength converter module 30 comprises a fiber Cherenkov type optical wavelength converter device 31, which is similar to the device 20 shown in Figure 5, and a lens 32, which is disposed in confronting relation to the end (exit end) 12a of the cladding 12 of the optical wavelength converter device 31. The lens 32 has a plane surface 32a facing the optical wavelength converter device 31 and a conical surface 32b remote from the device 31. If it is assumed that the refractive index of the cladding 12 is indicated by n C , the refractive index of a medium (usually air) around the device 31 by n A , and the refractive index of the material of the lens 32 by n L , then the following equations are met: n C sin = n A sin 1 n A sin 1 = n L sin 2 n L sin 3 = n A sin 4  3 = ρ -  2 where ρ is the angle at which the lens surface 32b iS inclined. If the second harmonic 15′ that has passed through the lens 32 is a parallel beam, then the angle ρ is ρ = ₄. From the above three equations, we get: n C sin = n L sin(ρ -  3 ) n L sin 3 = n A sinρ Consequently, by selecting the angle ρ of inclination of the conical lens surface 32b so as to meet the above two equations, the second harmonic 15′ that has passed through the lens 32 has a plane wavefront. According to the third embodiment, therefore, the second harmonic 15′ can be converged into a small beam spot in the same manner as the first and second embodiments. An optical wavelength converter module 40 according to the fourth embodiment shown in Figure 8 also comprises an optical wavelength converter device 31 and a lens 42. The lens 42 has a conical surface 42a facing the optical wavelength converter device 31 and a plane surface 42b remote from the device 31. According to the fourth embodiment, the following equations are satisfied: n C sin = n A sin 1 n A sin 2 = n L sin 3  2 = 1 + ρ where ρ is the angle at which the lens surface 42a is inclined. If the second harmonic 15′ that has passed through the lens 32 is a parallel beam, then the angle ρ is ρ = ₃. From the above three equations, we get: n C sin = n L sin 1 n L sin( + ρ) = n L sinρ By selecting the angle ρ of inclination of the conical lens surface 42a so as to meet the above two equations, the second harmonic 15′ that has passed through the lens 42 has a plane wavefront. An optical wavelength converter module according to the fifth embodiment of the present invention will be described with reference to Figure 9. The optical wavelength converter module, denoted at 50, also comprises an optical wavelength converter device 31 and a lens 52. The lens 52 has a flat surface 52a which faces the optical wavelength converter device 31, and a conical surface 52b, which is remote from the device 31. The flat surface 52a is held intimately against the cladding end 12a of the optical wavelength converter device 31. According to the fifth embodiment, the following equations are satisfied: n C sin = n L sin 1 n L sin 2 = n A sin 3  2 = ρ -  1 where ρ is the angle at which the lens surface 52b is inclined. If the second harmonic 15′ that has passed through the lens 52 is a parallel beam, then the angle ρ is ρ = ₃. From the above three equations, we get: n C sin = n L sin 1 n L sin(ρ -  1 ) = n A sinρ By selecting the angle ρ of inclination of the conical lens surface 52b so as to meet the above two equations, the second harmonic 15′ that has passed through the lens 52 has a plane wavefront. In the third, fourth and fifth embodiments, the lenses 32, 42, 52 have one plane surface and one conical surface. According to the sixth embodiment shown in Figure 10, an optical wavelength converter module 60 includes a lens 62 having two opposite conical surfaces 62a, 62b for converting the conical wavefront of the second harmonic 15′ into a plane wavefront. An optical wavelength converter module 70 according to the seventh embodiment illustrated in Figure 11 has a lens 72 having a concave conical surface 72a and an opposite convex conical surface 72b, the convex conical surface 72b being inclined at a greater angle than the concave conical surface 72a. An optical wavelength converter module 80 according to the eighth embodiment of the present invention will hereinafter be described with reference to Figure 12. The optical wavelength converter device 80 comprises a fiber Cherenkov type optical wavelength converter device 31, and a grating device 81, which is disposed in confronting relation to the exit end 12a of the cladding of the device 31. The grating device 81 comprises a grating 21 composed of equally spaced concentric patterns, which is identical to the grating according to the second embodiment shown in Figures 5 and 6, and the grating 21 being disposed on one surface of a transparent member 82 which is remote from the optical wavelength converter device 31. The wavefront of the second harmonic 15′ emitted from the cladding end 12a can be converted into a plane wavefront by passing through the grating device 81. While the grating device 81 is spaced from the optical wavelength converter device 31 in the eighth embodiment, the grating device 81 may be held in intimate contact with the cladding end 12a of the device 31 in an optical wavelength converter module 90 according to the ninth embodiment illustrated in Figure 13. An optical wavelength converter module 100 according to the tenth embodiment of the present invention will hereinafter be described with reference to Figure 14. The optical wavelength converter device 100 comprises a fiber Cherenkov type optical wavelength converter device 31, and a graded-index lens 101, which is disposed in confronting relation to the exit end 12a of the cladding 12 of the device 31. The medium around the optical wavelength converter device 31 is air whose refractive index is n A = 1.0, and satisfies the following equation: n C sin = sin10° The wavefront of the second harmonic 15′ can be converted into a plane wavefront if the graded-index lens 101 has a length of 8.66mm and a refractive index distribution n(r) = 1.5 - 0.02r; this means that the refractive index of the lens material is lowered 0.02 per 1mm in a radially inward direction and the refractive index at the center of the lens is 1.5. The graded-index lens 101 may be positioned in close contact with the cladding end 12a. Figures 15, 16 and 17 illustrate an optical wavelength converter device 110 according to the eleventh embodiment of the present invention. The optical wavelength converter device 110 is fabricated in the same manner as the optical wavelength converter device 10 according to the first embodiment shown in Figures 1 through 4. The end of the optical wavelength converter device 110, which will serve as an entrance end 110a for receiving light beams, is cut perpendicularly to the axis of the glass fiber. The other end 112a of cladding 112 is finished to an aspherical lens surface by a known grinding process. In this manner, the optical wavelength converter device 110 shown in Figures 15 and 16 is produced. The configuration of the cladding end 112a will be described later. The optical wavelength converter device 110 is used as shown in Figure 16 as the optical wavelength converter device 10 is used according to the first embodiment. The second harmonic 15′ is emitted out of the device 110 from the cladding end 112a. The fundamental wave 15 which has been guided through the core 111 is emitted from the end 111a of the core 111. A light beam 15″, containing the second harmonic 15′, and the fundamental wave 15 then goes through a filter 18 which passes only the second harmonic 15′. Thereby, only the second harmonic 15′ is extracted by the filter 18. The second harmonic 15′ is converged into a small spot P by the cladding end 112a having an aspherical lens surface. The configuration of the cladding end 112a of the cladding 112 will hereinafter be described in detail. As shown in Figure 17, the cladding 112 is thick enough for the second harmonic 15′ radiated into the cladding 112 at a phase matching angle  to be directly emitted out of the device 110 from the cladding end 112a without being totally reflected by the outer surface of the cladding 112. To achieve this, the cladding 112 is dimensioned to satisfy condition (1) above. With such dimensional limitations, the wavefront of the second harmonic 15′ traveling through the cladding 112 is oriented as indicated by the arrows W in Figure 17, in one plane which includes the core axis. Therefore, as a whole the wavefront is of a conical shape. If the cladding end 112a is shaped as an aspherical lens surface, which is a combination of the conical surface J indicated by the broken line and a spherical surface K indicated by the dot-and-dash line, then the second harmonic 15′ emitted out of the cladding 112 has a convergent spherical wavefront. The configuration of the cladding end 112a will be represented in the y-z coordinate system shown in Figure 17. Since the optical wavelength converter device 110 is an optical system, which is symmetric with respect to its axis, it is sufficient to consider the cladding end 112a in the y-z coordinate system or the y-z plane. (Spherical or other aberrations are not taken into account in this or the following embodiments.) The configuration of the conical surface J is expressed by: z 1 = a|y| and the configuration of the spherical surface K is expressed by: z 2 = r - r 2 - y 2 Therefore, the configuration of the cladding end 112a is represented by: z(y) = z 1 + z 2 = a|y| + r - r 2 - y 2 where a = n C sin n C cos - n A n C : the refractive index of the cladding, : the phase matching angle, and n A : the refractive index of the medium around the device (it is 1 if the medium is air) By defining the configuration of the cladding end 112a according to the equation (2) above, the wavefront of the emitted second harmonic 15' becomes a convergent spherical wavefront, so that the second harmonic 15' can be focused into a small beam spot P. According to the twelfth embodiment of the present invention shown in Figures 18 and 19, an optical wavelength converter device 120 which includes a cladding 112 having an end 112a for emitting the second harmonic 15', the cladding end 112a having a plane surface extending perpendicularly to the core axis, and a grating 121 of concentric patterns disposed on the surface of the cladding end 112a. The grating 121 may be formed by the photolithographic process. The diameter D of the cladding 112 is thick, ranging from lmm to 3mm, for example, so that condition (1) given above can be satisfied. Therefore, the grating 121 can be formed on the cladding end 112a relatively easily. The radius rm of the mth circular pattern or line of the grating 121 will be described below. It is assumed, as shown in Figure 18, that the position along the optical axis is represented by z, the position along the radial direction of the grating 121 by r, the refractive index of the cladding 112, the phase matching angle of the second harmonic l5' by , and the focal length by f. Since the optical wavelength converter device 120 is symmetric with respect to the axis thereof, only one sectional plane across the device 120 will be considered. The phase Φ of the grating 121 is given by: Φ = Φ OUT - Φ IN = 2πm + constant where Φ IN is the phase of an incident wave having a conical wavefront, Φ OUT is the phase of an emitted wave having a spherical wavefront, and m is an integer. Since Φ IN = (rn c sin + zn c cos)2π/λ Φ OUT = { - r 2 + z - f }2π/λ and also z = 0 on the grating surface, we get: Φ = (- r 2 + f 2 - rn C sin)2π/λ = 2πm + constant. If r = 0 when m = 0 as a standard condition, then constant = -f·2π/λ Consequently, the solution rm produced by solving the following quadratic equation: (1 - n C 2 sin 2 )r 2 - 2n C sin(mλ - f)r + (2f - mλ)mλ = 0 for the integer m is the radius of the mth circular pattern of the grating 112a. The grating 121 may be used to converge the second harmonic 15' onto the reflecting surface of an optical disc, for example. In such an application, the radii of the circular patterns of the grating 121 should be determined also in view of the refraction of the second harmonic 15' within the optical disc. By having the second harmonic 15' pass through the grating 121, the conical wavefront of the second harmonic 15' can be converted into a convergent spherical wavefront. Thus, the second harmonic 15' can be converged into a small beam spot P. Figure 20 shows an optical wavelength converter module 130 according to the thirteenth embodiment of the present invention. The optical wavelength converter module 130 comprises a fiber Cherenkov type optical wavelength converter device 131, identical to the previously described optical wavelength converter device, and a lens 132 disposed in confronting relation to the exit 112a of a cladding 112 of the optical wavelength converter device 131. The lens 132 has an aspherical surface 132a, facing the optical wavelength converter device 131, and a plane surface 132b, remote from the device 131. By defining the lens surface 132 according to the following equation: z(y) = z 1 + z 2 = a|y| + r - r 2 - y 2 where a = tanδ = n C sin 0 n L - cos 0 ₀: the angle at which the second harmonic 15' is emitted from the optical wavelength converter device 131, δ: the angle at which the conical surface j is in inclined, and n L : the refractive index of the material of the lens 131, the second harmonic 15' that has passed through the lens 132 has a convergent spherical wavefront. Therefore, by defining the configuration of the lens surface 132a according to the equations (3) and (4) above, the wavefront of the second harmonic 15' that has passed through the lens 132 becomes a convergent spherical wavefront. Therefore, the second harmonic 15' can be focused into a small beam spot P, as with the eleventh and twelfth embodiments. It is possible to design a lens having fewer aberrations by defining its aspherical configuration with coefficients of higher order than those of the above lens configuration. If a lens having one plane surface is used as in this embodiment, the plane lens surface may be positioned closely against the cladding end 112a. An optical wavelength converter module 140 according to the fourteenth embodiment shown in Figure 21 comprises an optical wavelength converter device 131 and a lens 142. The lens 142 has a conical surface 142a, which faces the optical wavelength converter device 131, and an opposite spherical surface 142b. When the second harmonic 15′ emitted from the optical wavelength converter device 131 passes through the conical lens surface 142a of the lens 142, the conical wavefront of the second harmonic 15′ is converted into a plane wavefront. When the second harmonic 15′ then passes through the spherical lens surface 142b, the plane wavefront thereof is converted into a convergent spherical wavefront, so that the second harmonic 15′ can be converged into a small beam spot P. A combination of a lens having a conical surface identical to the lens surface 142a above and an opposite plane surface, and another lens having at least one spherical surface may be employed in place of the lens 142; and it can achieve the same function as the lens 142. An optical wavelength converter module 150 according to the fifteenth embodiment of the present invention will hereinafter be described with reference to Figure 22. The optical wavelength converter device 150 comprises a fiber Cherenkov type optical wavelength converter device 131, and a grating device 151 disposed in confronting relation to the exit end 112a of the cladding 112 of the device 31. The grating device 151 comprises a grating 153, composed of concentric patterns, which is disposed on one surface of a transparent member 152, which is remote from the optical wavelength converter device 131. The wavefront of the second harmonic 15', emitted from the cladding end 112a, can be converted into a convergent spherical wavefront by passing through the grating device 151. The configuration of the grating 153 will hereinafter be described in detail. It is assumed, as shown in Figure 23, that the position along the optical axis is represented by z, the position along the radial direction of the grating 153 by r, the angle at which the second harmonic 15' is emitted from the cladding 112 by °, and the focal length by f. The phase Φ of the grating 153 is given by: Φ = Φ OUT - Φ IN = 2πm + constant where Φ IN is the phase of an incident wave having a conical wavefront, Φ OUT is the phase of an emitted wave having a spherical wavefront, and m is an integer. Since Φ IN = (rsin 0 + zcos 0 )2π/λ Φ OUT = {- r 2 + z - f }2π/λ and also z = 0 on the grating surface, we get Φ = (- r 2 + f 2 - rsin 0 )2π/λ = 2πm + constant. If r = 0 when m = 0 as a standard condition, then constant = -f·2π/λ Consequently, the solution rm produced by solving the following quadratic equation: (cos 2  0 )r 2 + 2sin 0 (f - mλ)r + (2f - mλ)mλ = 0 for the integer m is the radius of the mth circular pattern of the grating 153. The grating 153 can be fabricated by an electron beam lithographic process or a laser beam direct-writing process, or can be fabricated as a hologram using the system shown in Figure 24. The system of Figure 24 includes a lens 161, which has a concave conical surface for converting the plane wave 160 into the divergent wave 160′, which has a conical wavefront similar to the second harmonic 15′; semireflecting mirrors 162, 163; fully reflecting mirrors 164, 165; and a spherical lens 166, for converting the plane wave 160 into the convergent wave 160″, which has a spherical wavefront. The grating 153 is formed by applying the divergent wave 160′ and the convergent wave 160″ coaxially to a photosensitive layer 160 on the transparent member 152. Figure 25 illustrates an optical wavelength converter module 170 according to the sixteenth embodiment of the present invention. The optical wavelength converter module 170 comprises an optical wavelength converter device 131 and a grating device 171, which has a grating 173 composed of concentric patterns. The grating 173 is formed on a surface of the transparent member 172 and converts the conical wavefront of the second harmonic 15′ into a divergent spherical wavefront. The second harmonic 15′, with its wavefront thus converted, is then converted into a parallel beam of an increased beam width by the collimator lens 174 which comprises a spherical lens. The parallel-beam second harmonic 15′ is then focused into a small beam spot P by the condenser lens 175 which is in the form of a spherical lens. While the grating devices 151, 171 in the fifteenth and sixteenth embodiments are spaced from the respective optical wavelength converter devices 131, they may be held intimately against the cladding ends 112a of the devices 131. The grating devices 151, 171 may be oriented such that the surfaces thereof, which support the gratings 153, 173, face the optical wavelength converter devices 131. Each of the optical wavelength converter devices described above is designed to convert a fundamental wave into a second harmonic. However, the present invention is also applicable to an optical wavelength converter device which converts a fundamental wave into a third harmonic, or to an optical wavelength converter device which converts two fundamental waves into a wave having a frequency which is the sum of or difference between the frequencies of the fundamental waves. In the present invention, since the wavefront of a wavelength-converted wave emitted from a fiber type optical wavelength converter device can be converted into a plane wavefront, the wavelength-converted wave can be focused into a small spot by passing through an ordinary spherical lens, as described above. Furthermore, inasmuch as the wavefront of a wavelength-converted wave emitted from a fiber type optical wavelength converter device can be converted into a spherical wavefront, the wavelength-converted wave can be focused into a small spot by being passed through a collimator lens and a condenser lens, each in the form of an ordinary spherical lens. According to the present invention, therefore, wavelength-converted waves can be utilized in optical recording apparatus in which a light beam is to be focused into a small beam spot. The technology of wavelength conversion thus finds a wider range of applications than previous. Although certain preferred embodiments have been shown and described, it should be understood that many changes and modifications may be made therein without departing from the scope of the appended claims.

Claims: An optical wavelength converter device (10) comprising an optical fiber including: (i) a cladding (12) having a first refractive index; (ii) a core (11) of a nonlinear optical material disposed in said cladding and having a second refractive index higher than said first refractive index, whereby said optical fiber converts the wavelength of a fundamental wave (15) introduced into said core and radiates a wavelength-converted wave (15') with a conical wavefront into said cladding; and (iii) said cladding (12) having an exit end (12a) for emitting the wavelength-converted wave (15'), said exit end having a conical shape characterized in that the optical fiber is thick enough so that the wavelength-converted wave (15') radiated into said cladding (12) at a phase matching angle  can be emitted out of the device (10) without being totally reflected by the outer surface thereof, and the slanted surface of the conical exit end of the cladding has an angle δ selected on the phase matching angle  in order to convert the conical wavefront into a plane wavefront. An optical wavelength converter module (30,40,50,60,70,80,90,100), comprising: i) an optical wavelength converter device including an optical fiber comprising: a) a cladding (12) having a first refractive index; b) a core (11) of a nonlinear optical material disposed in said cladding and having a second refractive index higher than said first refractive index, whereby said optical fiber converts the wavelength of a fundamental wave (15) introduced into said core and radiates a wavelength-converted wave (15') with a conical wavefront into said cladding; and c) said cladding having an exit end for emitting the wavelength-converted wave (15') characterized by (ii) an optical device (32,42,52,62,72,82,81,101) disposed in a position to receive the wavelength-converted wave emitted from said exit end of the cladding of said optical wavelength converter device that is adapted to convert the conical wavefront of the received wavelength-converted wave into a plane wavefront and said optical fibre being thick enough so that the wavelength converted wave (15') radiated into the cladding (12) at a phase matching angle  can be emitted out of the device (10) without being totally reflected by the outer surface thereof. An optical wavelength converter module (20), according to claim 2 characterized in that said optical device is a grating (21) disposed on said exit end and composed of a structure of equally spaced concentric elements. An optical wavelength converter module according to claim 2, wherein said optical device (32,42,52,62,72) is a conical prism, the light entrance and/or exit surface of which is conical. An optical wavelength converter module according to claim 4, wherein said conical prism (42) has a conical entrance surface facing said exit end of said cladding. An optical wavelength converter module according to claim 4, wherein said conical prism (32,52) has a conical exit surface facing away from said exit end of said cladding. An optical wavelength converter module according to claim 6, wherein said conical prism (52) has a plane entrance surface held against said exit end of said cladding. An optical wavelength converter module according to claim 5 or 6, wherein said conical prism (42,32) is spaced from said exit end of said cladding. An optical wavelength converter module according to claim 4, wherein said conical prism (62) has a conical entrance surface facing said exit end of said cladding and a conical exit surface facing away from said exit end of said cladding. An optical wavelength converter module according to claim 9, wherein said conical prism (62) is spaced from said exit end of said cladding. An optical wavelength converter module according to claim 4, wherein said conical prism (72) has a concave conical entrance surface facing said exit end of said cladding and a convex conical exit surface facing away from said exit end of said cladding. An optical wavelength converter module according to claim 11, wherein said conical prism (72) is spaced from said exit end of said cladding. An optical wavelength converter module according to claim 2, wherein said optical device comprises a graded-index lens (100). An optical wavelength converter module according to claim 2, wherein said optical device comprises a grating device (81) having a grating composed of a structure of equally spaced concentric elements. An optical wavelength converter module according to claim 14, wherein said grating device (31) includes a transparent member supporting said grating on one surface thereof which faces away from said exit end of said cladding. An optical wavelength converter module according to claim 15, wherein said grating device (81) is spaced from said exit end of said cladding. An optical wavelength converter module according to claim 15, wherein said grating device (81) is held against said exit end of said cladding. An optical wavelength converter device (110) comprising an optical fiber including: (i) a cladding (12) having a first refractive index; (ii) a core (11) of a nonlinear optical material disposed in said cladding (12) and having a second refractive index higher than said first refractive index, whereby said optical fiber converts the wavelength of a fundamental wave introduced into said core and radiates a wavelength-converted wave (15') with a conical wavefront into said cladding; and characterized in that (iii) said cladding has an exit end for emitting the wavelength-converted wave, said exit end having an aspherical lens (112a) surface adapted to convert the conical wavefront of said wavelength-converted wave into a spherical wavefront, and said optical fiber is thick enough so that the wavelength converted wave (15') radiated into the cladding (12) at a phase matching angle  can be emitted out of the device (10) without being totally reflected by the outer surface thereof. An optical wavelength converter module (130,140,150,170), comprising: i) an optical wavelength converter device including an optical fiber comprising: a) a cladding (12) having a first refractive index; b) a core (11) of a nonlinear optical material disposed in said cladding and having a second refractive index higher than said first refractive index, whereby said optical fiber converts the wavelength of a fundamental wave (15') with a conical wavefront introduced into said core and radiates a wavelength-converted wave into said cladding; and c) said cladding having an exit (12a) end for emitting the wavelength-converted wave; characterized by (ii) an optical device (132,142,151,173,174,175) disposed in a position to receive the wavelength-converted wave emitted from said exit end of the cladding of said optical wavelength converter device adapted to convert the conical wavefront of the received wavelength-converted wave into a spherical wavefront, and said optical fiber being thick enough so that the wavelength converted wave (15') radiated into the cladding (12) at a phase matching angle  can be emitted out of the device (10) without being totally reflected by the outer surface thereof. An optical wavelength converter module (120), according to claim 19, characterized in that said optical device is a grating (121) disposed on said exit end and composed of concentric patterns. An optical wavelength converter module according to claim 19, wherein said optical device (132) comprises a lens having an aspherical entrance surface (132a) facing said exit end of said cladding and a plane exit surface facing away from said exit end (132b) of said cladding. An optical wavelength converter module according to claim 19, wherein said optical device comprises a lens having a conical entrance surface (142a) facing said exit end of said cladding and a spherical exit (142b) surface facing away from said exit end of said cladding. An optical wavelength converter module according to claim 21 or 22, wherein said lens is spaced from said exit end of said cladding. An optical wavelength converter module according to claim 20, wherein said optical device comprises a grating device (151) having a grating composed of a structure of concentric elements. An optical wavelength converter module according to claim 24, wherein said grating device (151) includes a transparent member supporting said grating on one surface thereof which faces away from said exit end of said cladding. An optical wavelength converter module according to claim 25, wherein said grating device (151) is spaced from said exit end of cladding. An optical wavelength converter module according to claim 25, wherein said grating device (151) comprises a hologram. An optical wavelength converter module according to claim 24, wherein said optical device further includes a collimator lens positioned on one side of said grating device (151) remote from said exit end of said cladding, and a condenser lens positioned on one side of said collimatcr lens remote from said grating device.

Inventors: GOTO CHIAKI, GOTO, CHIAKI, GOTO, CHIAKI FUJI PHOTO FILM CO., LTD.
Applicants: FUJI PHOTO FILM CO LTD, FUJI PHOTO FILM CO., LTD.
Application year: 1989
Main classification: G02F1
IPC codes: G02B6, G02F1