Fiber type wavelength converter

Abstract: A fiber type optical wavelength converter (3) comprising an optical fiber, has a core (10) made of nonlinear optical crystal and a clad (20) surrounding the core. The optical fiber has an effective refractive index N ω satisfying the following inequality |(n G 2ω )² - (N ω )²| < 0.093(λ/a)² wherein n G 2ω represents a refractive index of the core to the second harmonic wave corresponding to a dielectric tensor effectively utilized in the conversion, λ represents the wavelength of the fundamental wave and a represents the radius of the core in the cross-section. The optical wavelength converter converts the fundamental wave λ into the second harmonic wave λ/2 at a high efficiency.

Description: The present invention relates to an optical wavelength converter, in particularly to a fiber type wavelength converter using Cerenkov radiation phase matching. Wavelength converters have been actively developed, which use nonlinear optical crystal to constitute an optical waveguide passage to guide an optical wave to a minute area, and effectively generate a second harmonic wave. These wavelength converters are generally classified into two types depending on the method for satisfying phase matching. The first type matches the phase velocity of a nonlinear polarization wave excited by incident light of a fundamental wave with that of the second harmonic wave, and executes the phase matching between both the guide modes of the fundamental wave and of the second harmonic wave. The other type executes so-called Cerenkov radiation phase matching, i.e., the phase matching between the guide mode of the fundamental wave and the radiation mode of the second harmonic wave. An optical wavelength converter is known, which is constituted in the shape of an optical fiber comprising a core made of nonlinear optical crystal and a clad surrounding the core. This optical wavelength converter employs the Cerenkov radiation phase matching. This optical wavelength converter is also known as an optical fiber type second harmonic wave generator (hereinafter referred to as "SHG"). Fig. 1 is a conceptual diagram of an SHG 3, which comprises a columnar core 10 and a cylindrical clad layer 20 concentrically surrounding the core 10. When the fundamental wave propagates through the core 10 from the left to the right in the diagram, a second harmonic wave is generated. In other words, the nonlinear polarization wave propagates at the same phase velocity and generates the second harmonic waves with a predetermined angle to the clad layer. The second harmonic waves are reflected within the inside surface of the clad layer 20 and propagate from the left to the right in the diagram. The phase matching between the guide mode of the fundamental wave and the radiation mode of the second harmonic wave is executed in the clad layer and the core. The second harmonic wave and reflected wave at the boundary between the clad layer 20 are emitted from the end of the fiber in a corn shape as shown in Fig. 1. The equiphase wave surface of the wavefront of the thus emitted second harmonic wave is conical with the center axis of the fiber as its axis. According to the Cerenkov radiation system, it is possible to generate the second harmonic wave whose optical phase is almost automatically matched. The SHG is therefore applied as a short-wave light generator. As shown in Fig. 3, the short-wave light generator comprises a semiconductor laser 1, a coupling lens 2, an SHG 3 of which core is constituted by nonlinear optical crystal, and an axicon lens 4. The coupling lens 2 collects and guides the light emitted from the semiconductor laser 1 onto the end face of the SHG 3. The axicon lens 4 shapes the wavefront of the second harmonic wave, which is emitted after conversion by the optical wavelength converter, to form the second harmonic wave in the form of parallel light. In this way, the short-wave light generator module is constituted by the above SHG. However, the optical nonlinear material of this type which has an efficiently large nonlinear polarization constant has not yet been found. In addition, it is difficult to a material for the claddings, which surround the core, having a refractive index suitable for the core. Consequently, the wavelength converting efficiency (the output power of an emitted second harmonic wave / the output power of the semiconductor laser) is about 0.1% at maximum. GB-A-2235986 describes a prior art fibre-type wavelength converter. The preamble to claim 1 is based on that document. It is therefore an object of the present invention to provide a fiber type SHG which makes a sufficient use of the performance of a non-linear optical material for the core and has a high converting efficiency. To achieve this object, there is provided a fiber type optical wavelength converter comprising an optical fiber including a core made of a nonlinear optical crystal and a clad surrounding the core, in which a fundamental wave having a wavelength λ entering and propagating in the direction of the center axis of the core is converted into a second harmonic wave having a half wavelength λ/2, wherein said core and said clad are made of a nonlinear optical material and an optical glass satisfying the following inequality respectively: (n G 2ω ) 2 - (N ω ) 2 < 0.093(λ/a) 2 where n G 2ω represents a refractive index of said core to the second harmonic wave corresponding to a dielectric tensor effectively utilized in the conversion, N ω represents an effective refractive index of the optical fiber, λ represents the wavelength of the fundamental wave and a represents the radius of said core in the cross-section in such a manner that the core radius satisfies inequality 1; and characterized in that: the output power P 2ω of said second harmonic wave is defined by the following equation 11 P 2ω = 4π 2 ω 3 µ 0 ε 0 2 d 2 C 2 LG(2β)F(2β) where ω denotes the angular frequency of the fundamental wave; µ 0 denotes the permeability of vacuum; ε 0 denotes the dielectric constant of vacuum; d denotes a constant of a nonlinear polarization tensor effectively utilized in the wavelength conversion; C denotes a constant number based on the fundamental wave; G(2β) denotes a factor influencing an interface reflection that the second harmonic wave undergoes at the boundary between the core and clad due to a refractive index difference therebetween which corresponds to a Fresnel coefficient of transmittance and is defined by the following equation 10 ϒ = (4ω 2 µ 0 ε G 2ω -κ 2 ) 1/2 η = (4ω 2 µ 0 ε S 2ω -κ 2 ) 1/2 where ε G 2ω denotes a dielectric constant of the core with respect to the second harmonic wave; ε S 2ω denotes a dielectric constant of the clad with respect to the second harmonic wave; N 0 and N 1 denote the zeroth and the first Neumann functions respectively; J 1 and J 0 denote the first and the zeroth Bessel functions of the first kind respectively; and H 1 and H 0 denote the first and the zeroth deformation Hankel functions respectively; F(2β) denotes a factor influencing a so-called overlap integral between the distribution of a nonlinear polarization and an electric field; β denotes a propagation constant of the fundamental wave propagating in the fiber; and L denotes the length of core crystal; and in that said wavelength λ is a selected wavelength of the fundamental wave corresponding to a value of the factor G(2β) within the full width at half maximum of one peak of a curve of said factor G(2β) including a plurality of peaks in a contour map prepared on the basis of the following equations 19 and 20 ζ 2 | K=2β = (2k) 2 ((n G 2ω ) 2 -(N ω ) 2 ) η 2 | K=2β = (2k) 2 ((n S 2ω ) 2 -(N ω ) 2 ) in which the abscissa indicates an increasing ratio of the refractive index of the core with respect to the second harmonic wave from the effective refractive index of the optical fiber (n G 2ω ) 2 - (N ω ) 2 , and the ordinate indicates an increasing ratio of the refractive index of the clad with respect to the second harmonic wave from the effective refractive index of the optical fiber (n S 2ω ) 2 - (N ω ) 2 , the curves being plotted along the equivalent values of G(2β) in the plane containing the two coordinate axes, such that the direction indicating the high value of G(2β) corresponds to a vertical direction to such a plane. In a preferred embodiment, the effective refractive index of the fiber is the root of the following characteristic equation 4: UJ 1 (U)/J 0 (U) = WK 1 (W)/K 0 (W) U = k 0 a[(n G ω ) 2 -(N ω ) 2 ] 1/2 W = k 0 a[(N ω ) 2 -(n S ) 2 ] 1/2 where J 1 and J 0 denote the first and the zeroth Bessel functions of the first kind respectively; K 1 and K 0 denote the first and the zeroth deformation Hankel functions respectively; n G ω represents the refractive index of the core with respect to the fundamental wave; n S ω represents the refractive index of the clad with respect to the fundamental wave; and k 0 denotes the propagation constant 2π/λ in vacuum. Said constant number based on the fundamental wave C may be approximated by the following formula 3: C ≅ 2(µ 0 /ε 0 ) 1/2 W 2 P ω π a 2 N ω ( U 2 + W 2 ) where a denotes the core radius; N ω denotes an effective refractive index in an LP 0l mode for propagating a fundamental wave with the propagation constant β in the fiber; and P ω denotes the power of the fundamental wave. According to the selection of core materials, the wavelength of the fundamental wave, the radius of the core and clad materials satisfying the above inequality 1, the fiber type optical wavelength converter easily converts the fundamental wave into the second harmonic wave of half wavelength at a high efficiency. A preferred embodiment of the present invention will now be described by way of example only and with reference to the accompanying drawings, in which: Fig. 1 is an enlarged perspective view of a fiber type optical wavelength converter; Fig. 2 is a graph showing a power property curve in the fiber type optical wavelength converter according to the present invention; Fig. 3 is a schematic diagram of a short-wave light generator using an SHG; Fig. 4 is graph showing the G(2β) property curve depending on the wavelength of the fundamental wave in an SHG; and Fig. 5 is a graph showing the conversion efficiency with respect to the wavelength of the fundamental wave. The structure of an SHG according to the present invention is approximately the same as the one illustrated in Fig. 1. The SHG is an optical fiber comprising a columnar core made of nonlinear optical crystal, and a cylindrical clad layer made of optical glass enclosing the core concentrically. The SHG has a characteristic that the optical fiber has an effective refractive index N ω satisfying the following inequality (n G 2ω ) 2 - (N ω ) 2 < 0.093(λ/a) 2 wherein n G 2ω represents a refractive index of the core to the second harmonic wave corresponding to an SHG tensor effectively utilized in the conversion, λ represents a wavelength of the fundamental wave and a represents a radius of the core in the cross-section. The effective refractive index N ω is determined by both the indexes of the core and clad and the core radius as described hereinafter. The SHG tensor is a tensor quantity of a second nonlinear optical constant d ijk expressed as a three degree determinant, for example, a 3 x 6 determinant d il : By using this determinant d il , the relationship between a nonlinear polarization in the core P NL and an electric field E ω of the fundamental wave can be expressed as follows: wherein ε 0 denotes the dielectric constant of vacuum. Therefore, both the polarization state of the fundamental wave and the orientation of the core crystal determine both the tensor components in the SHG tensor to be utilized and the polarization state of the second harmonic wave generated by the fiber type wavelength converter. Thus, n G 2ω represents a refractive index of the core with respect to the second harmonic wave in such a polarization state. The inventors have analyzed an electromagnetic field in the SHG while considering the presence of the boundary between the clad and the core with the clad diameter set finite as per the actual SHG. From the analysis, the inventors have found that for an SHG having a fiber radius and a core crystal length (SHG length) such that the second harmonic wave generated once by the core no longer comes back to the core, namely, it is fully reflected at most once by the boundary between the clad layer and air, and for another SHG having an infinite fiber radius and an endless SHG length, the outputs of both these SHGs are substantially equal to each other. In other words, inventors have found out that the output power of the SHG can be approximated by using the SHG length such that the second harmonic wave is fully reflected only once by the boundary between the clad and air, without repeating. Therefore, the output power of the second harmonic wave generated by the SHG comprising a core and an infinite clad layer was analyzed by the following process. Given that a fundamental wave with the propagation constant β in LP 01 mode is propagated in an SHG, a nonlinear polarization P NL to be excited is defined by the following equation: P NL = ε 0 dCJ 0 2 (Ur)exp(-i2βz) where Z denotes a waveguide direction of the SHG; ε 0 denotes the dielectric constant of vacuum; d denotes a constant of the nonlinear polarization tensor effectively utilized in the wavelength conversion; and C denotes a constant number based on the fundamental wave. By using the guided power of the fundamental wave, the constant number C based on the fundamental wave may be approximated by the following formula 3: C ≅ 2(µ 0 /ε 0 ) 1/2 W 2 P ω π a 2 N ω ( U 2 + W 2 ) U = a(ω 2 µ 0 ε g ω -β 2 ) 1/2 W = a(β 2 -ω 2 µ 0 ε S ω ) 1/2 where ω denotes an angular frequency of the fundamental wave; a denotes a core radius of the SHG; N ω denotes an effective refractive index in LP 01 mode for the fundamental wave propagating with the propagation constant β in the fiber of the SHG; µ 0 denotes the permeability of vacuum; ε g ω denotes a dielectric constant of the core with respect to the fundamental wave; and ε S ω denotes a dielectric constant of the clad with respect to the fundamental wave. The effective refractive index of the SHG fiber comprising the core and clad layer N ω is the root of the following characteristic equation 4: UJ 1 (U)/J 0 (U) = WK 1 (W)/K 0 (W) U = k 0 a[(n G ω ) 2 -(N ω ) 2 ] 1/2 = a(ω 2 µ 0 ε g ω -β 2 ) 1/2 W = k 0 a[(N ω ) 2 -(n S ω ) 2 ] 1/2 = a(β 2 -ω 2 µ 0 ε S ω ) 1/2 where J 1 and J 0 denote the first and the zeroth Bessel functions of the first kind respectively; K 1 and K 0 denote the first and the zeroth deformation Hankel functions respectively; n G ω represents a refractive index of the core with respect to the fundamental wave; n S ω represents a refractive index of the clad with respect to the fundamental wave; and k 0 denotes the propagation constant 2π/λ in vacuum. By using Green's function G D (r,r') in consideration of the boundaries, an electric field of an second harmonic wave E 2ω (r) of the core is expressed as follows: where L denotes a length of the core crystal. Using the Green's function G(r,r') over the whole space and an arbitrary function A(κ), G D (r,r') will be given as follows: G D (r,r') = G(r,r') + A(κ)J 0 (rζ)J 0 (r'ζ) G(r,r') will be expressed as follows: where H 0 ω and J 0 are the zeroth Hankel function of the first kind and the zeroth Bessel function respectively, and ζ 2 = 4ω 2 µ 0 ε g ω - κ 2 . The power of the second harmonic wave P 2ω is obtained by the following equation 8: where G(2β) denotes a factor influencing the interface reflection that the second harmonic wave reflects at the boundary between the core and clad due to a refractive index difference therebetween, which corresponds to a Fresnel coefficient of transmittance; and F(2β) denotes a factor influencing a so-called overlap integral between both distributions of a nonlinear polarization and an electric field. The factor G(2β) can be defined with the boundary conditions. The factors G(2β) and F(2β) are expressed by the following equations 9 and 10: γ = (4ω 2 µ 0 ε G 2ω -κ 2 ) 1/2 η = (4ω 2 µ 0 ε S 2ω -κ 2 ) 1/2 where ε G 2ω denotes a dielectric constant of the core with respect to the second harmonic wave; ε S 2ω denotes a dielectric constant of the clad with respect to the second harmonic wave; N 0 and N 1 denote the zeroth and the first Neumann functions respectively; J 1 and J 0 denote the first and the zeroth Bessel functions of the first kind respectively; and H 1 and H 0 denote the first and the zeroth deformation Hankel functions respectively. Since the term sin 2 [(2β-κ)L/2]/ (2β-κ) 2 in equation 8 may be approximated by Dirac delta function πLδ(2β-κ)/2, the output power of the second harmonic wave P 2ω is obtained as the following equation (11). P 2ω = 4π 2 ω 3 µ 0 ε 0 2 d 2 C 2 LG(2β)F(2β) As can be seen from this equation 11, the output power of the second harmonic wave P 2ω is influenced by these factors G(2β) and F(2β). Since the power of the second harmonic wave is greatly influenced by the factor F(2β) in equation 11, the value of F(2β) should be considered in order to obtain conditions for a high conversion efficiency. Namely, it is understood that the power of the second harmonic wave increases as the value of the following integral, a so-called overlap integral, increases. Since the term J 0 (Ur) 2 in the overlap integral indicates a function that an electric field of the waveguided fundamental wave is distributed in the core, it hardly changes with respect to r . Therefore, given that J 0 (Ur) 2 = 1 , then the overlap integral is calculated as follows: F(2β) = (a 4 /4)[2J 1 (aγ)/(aγ)] 2 The formation of this integral value with respect to aγ indicates a pattern similar to a diffraction image generated from a circular aperture irradiated by light having the maximum fringe at γ = 1. This integral value has a first lobe with the maximum area within aγ < 3.833 which is greater than that of the other lobe areas. γ 2 is expressed by γ 2 = (4π/λ) 2 [(n G 2ω ) 2 -(N ω ) 2 ] In other words, by considering an angle of Cerenkov radiation direction, the power of the second harmonic wave P 2ω will be expressed by the following approximation equation 14: where  represents an angle of Cerenkov radiation, k G represents a normalization frequency expressed by the following equation: k G = 4πn G 2ω /λ, n G 2ω represents a refractive index of the core to the second harmonic wave and λ represents a wavelength of fundamental wave. On the basis of the above approximation equation 14, the power of the second harmonic wave P 2ω will be expressed by such a graph as shown in Fig. 2. It will be understood that the second harmonic wave radiates from the SHG as diffraction light components in the Cerenkov radiation direction within the diffracted light having the amplitude distribution J 0 (Ur) 2 . The power distribution of the second harmonic wave appears as the Airy pattern. In other words, equation 14 implies that the wavelength converter irradiates only light diffracted in the direction of the Cerenkov radiation angle out of all the diffracted light generated from a circular aperture irradiated by light having the amplitude distribution J 0 (Ur) 2 . Therefore, it is necessary that the Cerenkov radiation angle exist in the main lobe of the diffracted image to obtain a high conversion efficiency. As apparent from Fig. 2, the main or most power intensity P 2ω is obtained within from the peak to the first trough (from 0 to 3.8327 on the ak G sin axis) in the property curve of the power of the second harmonic wave. Therefore the angle of Cerenkov radiation  in the range satisfying the following inequality sin<3.8327/ak G preferably suffices a requirement to obtain the main power of the second harmonic wave. The effective refractive index N ω in the core extending direction is expressed by the following equation N ω = n G 2ω cos Using the equations 13a and 17, the relationship between the refractive indexes, the wavelength of the fundamental wave and the core radius is expressed by the following inequality (n G 2ω ) 2 - (N ω ) 2 < 0.093(λ/a) 2 Since effective refractive index in the waveguide mode to the fundamental wave is therefore defined by the refractive indexes of the clad optical glass and the core material to the fundamental wave as shown in equation 4, the second harmonic wave is easily generated at a high efficiency by selecting the core materials, the wavelength of the fundamental wave, the core radius and the clad materials so as to satisfy the above inequality (1). Furthermore, the factor G(2β) should be considered in order to obtain other conditions for a higher conversion efficiency. For this, it is preferable that the SHG suffices not only the requirement of equation 1 but also that of factor G(2β), which should be increased. The factor G(2β) comprises a function including the γ and δ, which complicatedly changes in accordance with both the refractive indexes of the core with respect to the second harmonic wave n G 2ω and that of the clad with respect to the second harmonic wave n S 2ω as parameters for designing of the wavelength converter. Therefore, the change of the factor G(2β) have been investigated by changing n G 2ω and n S 2ω . The tendency of G(2β) is calculated through the following equations 19 and 20. ζ 2 | K =2β = (2 k ) 2 (( n 2ω G ) 2 -( N ω ) 2 ) η 2 | K =2β = (2 k ) 2 (( n 2ω S ) 2 -( N ω ) 2 ) Fig. 4 shows a graph of an isarithm or contour map prepared on the basis of these equations in which the abscissa indicates an increase ratio of the refractive index of the core with respect to the second harmonic wave from the effective refractive index of the optical fiber (n G 2ω ) 2 - (N ω ) 2 , and the ordinate indicates an increase ratio of the refractive index of the clad with respect to the second harmonic wave from the effective refractive index of the optical fiber (n S 2ω ) 2 - (N ω ) 2 , the curves being plotted along the equivalent values G(2β) in the plane containing the two coordinate axes. The direction indicating the high value G(2β) corresponds to a vertical direction to such a plane. It is analyzed that, when the refractive indexes of the core and clad with respect to the second harmonic wave are equal to each other, G(2β) = 1 is obtained as shown by the dots line C of Fig 4. Particularly, it will be understood that an envelope of the curves of G(2β) in a vertical plane has a plurality of peaks, the maximum of each being marked by P in several places along the abscissa and that such peaks follows to ridges extending parallel to the ordinate, the vertical plane being parallel to the abscissa and vertical to the ordinate of the isarithm map showing the equivalent values of the factor G(2β). Namely, the G(2β) values at the peaks and ridges are greater than those at other places. The G(2β) value is sufficient within a full width at half maximum of the envelope cut out in the vertical plane so that a high conversion efficiency is obtained in the SHG. The generation of these peaks should be used for the designing of an SHG with a high conversion efficiency. Thus the SHG with a high conversion efficiency is obtained by selecting a wavelength of the fundamental wave corresponding to a value of the factor G(2β) within the full width at half maximum, preferably an adjacent value of one peak of a curve of the factor G(2β) including a plurality of peaks. Fig. 5 shows a property of the conversion efficiency depending on the wavelength of the fundamental wave, in which the curve A shows a property of an SHG comprising a core made of DMNP and a clad made of SF11 glass, and the curve B shows a property of an SHG comprising a core made of DMNP and a clad made of SF15 glass. As seen from the graphs, the conversion efficiencies of the SHG surge and increase in accordance with the peaks. In these cases, the wavelength converting efficiencies (the power of an second harmonic wave / the power of the second harmonic wave) are obtained through equation 11 with parameter λ under conditions of the power of the fundamental wave being 40 mW and the SHG length being 1 mm. As shown in Fig. 5 (curve A ), high conversion efficiency is obtained when SF11 glass is selected for the clad material and 960 nm is selected for the wavelength of the fundamental wave. When this selection of SF11 glass for the clad and of 960 nm for the fundamental wave, such a wavelength corresponds to one of peaks in the curve of G(2β) as shown in Fig. 4. When SF15 glass is selected for the clad and 890 nm is selected for the fundamental wave as shown with curve B of Fig. 5, such a wavelength corresponds to one of peaks in the curve of G(2β) as shown in Fig. 4. In this way, by scanning the wavelengths of the fundamental waves and selecting a pertinent one from the clad materials, a high conversion efficiency can be found out for the SHG, although the refractive index does change due to the refractive index dispersion of the wavelength of the fundamental wave entering the fiber comprising the core and clad. Accordingly, it is useful to satisfy the above equation 1 by the selected combination of a core radius, a glass material for the clad and a nonlinear optical material for the core and, at the same time, to select parameters, i.e., a clad glass and a wavelength for the fundamental wave for generating the peaks of the curve of G(2β) for designing of an SHG with a high conversion efficiency.

Claims: A fiber type optical wavelength converter (3) comprising an optical fiber including a core (10) made of a nonlinear optical crystal and a clad (20) surrounding the core, in which a fundamental wave having a wavelength λ entering and propagating in the direction of the center axis of the core is converted into a second harmonic wave having a half wavelength λ/2, wherein said core (10) and said clad (20) are made of a nonlinear optical material and an optical glass satisfying the following inequality respectively: (n G 2ω ) 2 - (N ω ) 2 < 0.093(λ/a) 2 where n G 2ω represents a refractive index of said core to the second harmonic wave corresponding to a dielectric tensor effectively utilized in the conversion, N ω represents an effective refractive index of the optical fiber, λ represents the wavelength of the fundamental wave and a represents the radius of said core in the cross-section in such a manner that the core radius satisfies inequality 1; and characterized in that: the output power P 2ω of said second harmonic wave is defined by the following equation 11 P 2ω = 4π 2 ω 3 µ 0 ε 0 2 d 2 C 2 LG(2β)F(2β) where ω denotes the angular frequency of the fundamental wave; µ 0 denotes the permeability of vacuum; ε 0 denotes the dielectric constant of vacuum; d denotes a constant of a nonlinear polarization tensor effectively utilized in the wavelength conversion; C denotes a constant number based on the fundamental wave; G(2β) denotes a factor influencing an interface reflection that the second harmonic wave undergoes at the boundary between the core and clad due to a refractive index difference therebetween which corresponds to a Fresnel coefficient of transmittance and is defined by the following equation 10 ϒ = (4ω 2 µ 0 ε G 2ω -κ 2 ) 1/2 η = (4ω 2 µ 0 ε S 2ω -κ 2 ) 1/2 where ε G 2ω denotes a dielectric constant of the core with respect to the second harmonic wave; ε S 2ω denotes a dielectric constant of the clad with respect to the second harmonic wave; N 0 and N 1 denote the zeroth and the first Neumann functions respectively; J 1 and J 0 denote the first and the zeroth Bessel functions of the first kind respectively; and H 1 and H 0 denote the first and the zeroth deformation Hankel functions respectively; F(2β) denotes a factor influencing a so-called overlap integral between the distribution of a nonlinear polarization and an electric field; β denotes a propagation constant of the fundamental wave propagating in the fiber; and L denotes the length of core crystal; and in that said wavelength λ is a selected wavelength of the fundamental wave corresponding to a value of the factor G(2β) within the full width at half maximum of one peak of a curve of said factor G(2β) including a plurality of peaks in a contour map prepared on the basis of the following equations 19 and 20 ζ 2 | K=2β = (2k) 2 ((n G 2ω ) 2 -(N ω ) 2 ) η 2 | K=2β = (2k) 2 ((n S 2ω ) 2 -(N ω ) 2 ) in which the abscissa indicates an increasing ratio of the refractive index of the core with respect to the second harmonic wave from the effective refractive index of the optical fiber (n G 2ω ) 2 - (N ω ) 2 , and the ordinate indicates an increasing ratio of the refractive index of the clad with respect to the second harmonic wave from the effective refractive index of the optical fiber (n S 2ω ) 2 - (N ω ) 2 , the curves being plotted along the equivalent values of G(2β) in the plane containing the two coordinate axes, such that the direction indicating the high value of G(2β) corresponds to a vertical direction to such a plane. A fiber type optical wavelength converter according to claim 1, wherein said effective refractive index of the fiber is the root of the following characteristic equation 4: UJ 1 (U)/J 0 (U) = WK 1 (W)/K 0 (W) U = k 0 a[(n G ω ) 2 -(N ω ) 2 ] 1/2 W = k 0 a[(N ω ) 2 -(n S ω ) 2 ] 1/2 where J 1 and J 0 denote the first and the zeroth Bessel functions of the first kind respectively; K 1 and K 0 denote the first and the zeroth deformation Hankel functions respectively; n G ω represents the refractive index of the core with respect to the fundamental wave; n S ω represents the refractive index of the clad with respect to the fundamental wave; and k 0 denotes the propagation constant 2π/λ in vacuum. A fiber type optical wavelength converter according to claim 1 or 2, wherein said constant number based on the fundamental wave C is approximated by the following formula 3: C α 2(µ 0 /ε 0 ) 1/2 W 2 P ω πa 2 N ω (U 2 + W 2 ) where a denotes the core radius; N ω denotes an effective refractive index in an LP 01 mode for propagating a fundamental wave with the propagation constant β in the fiber; P ω denotes the power of the fundamental wave. A fiber type optical wavelength converter according to claim 1, 2 or 3 wherein the angle of Cerenkov radiation  is in the range satisfying the following inequality:- sin < 3.8327/ak G where k G represents a normalization frequency expressed by the following equation: k G = 4πn G 2ω /λ A fiber type optical wavelength converter according to any one of the preceding claims, wherein the wavelength λ is a selected wavelength of the fundamental wave corresponding to a value of the factor G(2β) adjacent one peak of said curve of said factor G(2β).

Inventors: CHIKUMA KIYOFUMI, OKAMOTO SOTA, CHIKUMA, KIYOFUMI, OKAMOTO, SOTA
Applicants: PIONEER ELECTRONIC CORP, PIONEER ELECTRONIC CORPORATION
Application year: 1992
Main classification: G02F1
IPC codes: G02F1