Patent Application
20100054296
This application is based on and claims priority under 35 U.S.C. §119 to Japanese Patent Application 2008-217050, filed on Aug. 26, 2008, the entire content of which is incorporated herein by reference.
The present invention relates to a terahertz wave generating apparatus and a terahertz wave generating method for generating high-intensified terahertz waves.
Terahertz waves are electromagnetic waves having frequency in a range between 0.1 and 10 THz and having wavelength in a range between 30 and 3000 μm, which approximately correspond to a range between a microwave band and a light. Taking advantage of this characteristic, the terahertz wave has been expected to be applied to various areas such as telecommunication, examination and the like.
A device and a method for generating terahertz waves are disclosed in a non-patent document 1: Kiyomi Sakai “terahertz time-domain spectroscopy (THz-TDS)”, spectroscopy kenkyu, Vol. 50, No. 6, 2001, p. 261-273, and a non-patent document 2: Hoffman et al., “Efficient terahertz generation by optical rectification at 1035 nm”, OPTICS EXPRESS, Vol. 15, No. 18, 3 Sep. 2007, pp. 11706-11713.
In the non-patent document 1, several technologies for generating terahertz waves are disclosed. As one example, a terahertz wave is generated by use of an antenna element such as a voltage-biased antenna having a micro antenna structure. Specifically, the terahertz wave is generated by using the antenna irradiated with an ultra short pulse laser. As another example, a terahertz wave is generated on the basis of a nonlinear effect. Specifically, the terahertz wave is generated on the basis of light rectification effect by using a certain material having a reversal symmetry X(2) irradiated with ultra short pulse laser. Furthermore, a surface semiconductor and an application of magnetic field are used in order to generate the terahertz wave.
In the non-patent document 2, a technology for generating high-intensified terahertz waves, on the basis of the Cherenkov radiation theory, within LN(LiNbO3: lithium niobate) crystal, in such a way that wavefront of an incident laser is tilted by use of diffraction grating, is disclosed.
According to the non-patent document 1, because the intensity of the obtained terahertz wave (output) is relatively low, such terahertz wave may not be used for areas other than spectroscopic measurement.
Further, according to the non-patent document 2, because the wavefront of the incident laser needs to be tilted, an optical system for propagating a beam image focused on the diffraction grating, by use of the diffraction grating and a lens, is used. In this configuration, the light tilted at the diffraction grating may be dispersed at areas other than the vicinity of the focal point of the lens, accordingly, a positional alignment of the optical system needs to be adjusted very precisely.
A need thus exists for a terahertz wave generating apparatus and a terahertz wave generating method, which are not susceptible to the drawback mentioned above.
According to an aspect of the present invention, a terahertz wave generating apparatus includes an excitation light source for outputting an excitation light at a predetermined wavelength, an optical crystal being excited by an irradiation with the excitation light in order to generate a terahertz wave and terahertz wave amplifying means for repeatedly performing an optical parametric amplification for the terahertz wave by use of the excitation light, wherein the terahertz wave amplifying means includes an optical waveguide having the optical crystal serving as a core and a medium serving as a clad whose refractive index is smaller than a refractive index of the optical crystal, and the inputted excitation light is propagated within the optical waveguide with fulfilling a condition for a total reflection.
According to another aspect of the present invention, a terahertz wave generating method includes steps of; outputting an excitation light toward an optical crystal at a predetermined wavelength, generating a terahertz wave by exciting the optical crystal and propagating the inputted excitation light with performing a total reflection within the optical waveguide having the optical crystal as a core, and repeatedly performing an optical parametric amplification for the terahertz wave by use of the excitation light.
The foregoing and additional features and characteristics of the present invention will become more apparent from the following detailed description considered with the reference to the accompanying drawings, wherein:
A terahertz wave generating apparatus related to the present invention will be explained in accordance with a drawing in
The excitation light source 11 is a semiconductor laser equipment serving as a light source for emitting an excitation light 13 serving as a toward the nonlinear optical crystal 12 serving as an optical crystal. In the embodiment, the excitation light 13 is set at 780 nm of its wavelength, and a polarization direction of the excitation light 13 is set so as to be parallel to an axis Z in
The nonlinear optical crystal 12 generates terahertz waves by process of an optical parametric generation on the basis of a nonlinear optical principle for an incident light such as a laser light. In the embodiment, LN (LiNbO3: lithium niobate) crystal is used as the nonlinear optical crystal 12, and an optic axis of the nonlinear optical crystal 12 is in parallel with the axis Z in
As illustrated in
The nonlinear optical crystal 12 includes an incident plane 12c (e.g., a tapered surface) through which the excitation right 13 enters the nonlinear optical crystal 12. The incident plane 12c is formed so as to form an angle θ between the incident plane 12c and principle surfaces (total reflection planes 12a and 12b formed parallel to each other) of the nonlinear optical crystal 12. The angle θ is set so as to fulfill a condition where the excitation light 13 is total-reflected on the total reflection planes 12a and 12b. In the embodiment, the angle θ is set to 30°, and an exit plane 12d through which the excitation light 13 and the terahertz wave 15 exit the nonlinear optical crystal 12 is formed so as to be vertical relative to each of the total reflection planes 12a and 12b.
Because the wavelength of the excitation light 13 is different from that of the terahertz wave 15, the excitation light 13 and the terahertz wave 15 propagate within the nonlinear optical crystal 12 at different speeds. In the embodiment, the propagation speed of the terahertz wave 15 is set so as to be a half of the propagation speed of the excitation light 13.
In this configuration, the nonlinear optical crystal 12, serving as a core, and air 16, serving as a clad, configure an optical waveguide.
The optical system 17 is an optical system such as a lens provided between the excitation light source 11 and the nonlinear optical crystal 12. The optical system 17 is illustrated in the diagram of
Only main components of the terahertz wave generating apparatus 10 are explained above and illustrated in the diagram in
An actuation of the terahertz wave generating apparatus 10 structured as mentioned above will be explained.
As illustrated in the drawing in
The excitation light 13 entering the nonlinear optical crystal 12 generates an idler wave 14 and a terahertz wave 15 by process of optical parametric generation. On the basis of law of conservation of energy, a relation among an angular frequency of the excitation light 13 (ω1), an angular frequency of the idler wave 14 (ω2) and an angular frequency of the terahertz wave 15 (ω3) is expressed by a formula: ω1=ω2+ω3. Further, on the basis of law of conservation of momentum, a relation among a light vector of the excitation light 13 (k1), a light vector of the idler wave 14 (k2) and a light vector of the terahertz wave 15 (k3) is expressed by a formula: k1=k2+k3.
Then, the excitation light 13 is total-reflected on the total reflection planes 12a and 12b, each of which configures principle surfaces of the nonlinear optical crystal 12. Because a refractive index of LN crystal used for the nonlinear optical crystal 12 is set to 2.15, and a refractive index of the air is 1.0003, the optical waveguide fulfills a condition of the total reflection of the excitation light 13 at an angle θ of 30°. Accordingly, the excitation light 13 propagates within the nonlinear optical crystal 12 by repeating several times the total reflections on the total reflection planes 12a and 12b at the incident angle θ of 30°.
The terahertz wave 15 propagates within the nonlinear optical crystal 12 at a single mode in a direction indicated by an arrow illustrated in the diagram in
A relationship between the excitation light 13 and the terahertz wave 15 will be explained in detail in accordance with the drawing of
After entering the nonlinear optical crystal 12 through the incident plane 12c and generating the terahertz wave 15 and the idler wave 14, the excitation light 13-1 propagates toward the total reflection plane 12a after being total-reflected on the total reflection plane 12b. The terahertz wave 15 generated within the nonlinear optical crystal 12 is propagated in the direction indicated by an arrow in
As indicated in the drawing of
Then, an interaction between the excitation light 13-1 and the terahertz wave 15-1 occurs at the point S1. A phase matching condition of the optical parametric amplification between the excitation light 13 and the terahertz wave 15 is fulfilled in this interaction. Accordingly, the terahertz wave 15-1 is optical-parametrically amplified to be the terahertz wave 15-2, which has an intensity that is higher than the intensity of the terahertz wave 15-1, and the amplified terahertz wave 15-2 is further propagated within the nonlinear optical crystal 12. On the other hand, the intensity of the excitation light 13-1 is reduced by the amplification of the terahertz wave 15-1 so as to be the excitation light 13-2, whose intensity is lower than that of the excitation light 13-1, and the excitation light 13-2 is further propagated within the nonlinear optical crystal 12.
The excitation light 13-2 total-reflected on the total reflection plane 12a and the terahertz wave 15-2 interact with each other at the point S2 repetitively, so that the terahertz wave 15-2 is amplified to be the terahertz wave 15-3, and the intensity of the excitation light 13-2 is reduced so as to be an excitation light 13-3 whose intensity is lower than that of the excitation light 13-2.
After “n” times of the interaction (at the point Sn), the terahertz wave 15 has been amplified by the excitation light 13 “n” times so as to be the terahertz wave 15out, whose intensity is relatively highest, and the terahertz wave 15out exits the nonlinear optical crystal 12 through the exit plane 12d. An object to be examined is irradiated with the outputted terahertz wave 15out in order to obtain, for example image information of the object, by means of a detecting means of the examination apparatus.
The intensity of the excitation light 13 has been reduced so as to be the excitation light 13out, whose intensity is relatively the lowest, and exits the nonlinear optical crystal 12 through the exit plane 12d. The outputted excitation light 13out and the idler wave 14 are absorbed by an absorving apparatus or the like.
Because the positive integer “n” is increased in accordance with the size of the nonlinear optical crystal 12 in a propagation direction, the intensity of the terahertz wave 15 may be appropriately increased depending on the size of the nonlinear optical crystal 12 by means of the interaction between the terahertz wave 15 and the excitation light 13. However, because the intensity of the excitation light 13 is reduced by repeating the amplification of the terahertz wave 15, the excitation light 13 is fogged as the propagation thereof proceeds. Therefore, the size of the nonlinear optical crystal 12 in the propagation direction may be set appropriately in consideration with the intensity of the excitation light 13 entering the nonlinear optical crystal 12.
In the embodiment, the total reflection of the excitation light is repeated within the nonlinear optical crystal 12, which configures the optical waveguide, at the same time, the terahertz wave generated within the nonlinear optical crystal by process of the optical parametric generation interacts with the excitation light so as to fulfill the phase matching condition of the optical parametric amplification. Accordingly, using a single excitation light, the terahertz wave may be parametrically amplified several times, in other words, a terahertz wave with high intensity may be generated by a device whose configuration is relatively simple.
The terahertz wave generating apparatus and method in the embodiment may be modified or may be applied to another apparatus.
For example, in the embodiment, the angle θ indicated in the drawing of
Further, in the embodiment, the optical waveguide is comprised of the nonlinear optical crystal 12 serving as a core and the air 16 serving as clad, however, the medium may be changed, regardless of vapor or solid substance, as long as it fulfills the condition for the total reflection of the excitation light 13.
In the embodiment, the terahertz wave generating apparatus 10 is mounted to an imaging examination apparatus, however, the device may be applied to another apparatus such as a spectroscopic measurement apparatus, a telecommunication apparatus, a chemical analysis apparatus and the like.
As described in the embodiment, a terahertz wave generating apparatus includes an excitation light source for outputting an excitation light at a predetermined wavelength, an optical crystal being excited by an irradiation with the excitation light in order to generate a terahertz wave and terahertz wave amplifying means for repeatedly performing an optical parametric amplification for the terahertz wave by use of the excitation light, wherein the terahertz wave amplifying means includes an optical waveguide having the optical crystal serving as a core and a medium serving as a clad whose refractive index is smaller than a refractive index of the optical crystal, and the inputted excitation light is propagated within the optical waveguide with fulfilling a condition for a total reflection.
Further, the optical crystal is formed in a plate shape body having a predetermined thickness and having first and second principle surfaces formed so as to be parallel to each other and a tapered surface, a predetermined angle is set between each of the first and second principle surfaces and the tapered surface, the excitation light vertically enters the optical crystal through the tapered surface, the clad including a layer of the medium having a predetermined refractive index is arranged so as to contact at least one of the first and second principle surfaces of the optical crystal, the terahertz wave amplifying means is structured so as to perform a total reflection on an interfacial surface between the first principle surface and the clad and on an interfacial surface between the second principle surface and the clad, and the predetermined thickness of the optical crystal is set so as to fulfill a phase matching condition of the optical parametric amplification between the excitation light and the terahertz wave propagated within the optical crystal and so as to fulfill a condition where a propagation mode of the terahertz wave is in a single mode.
Furthermore, the optical crystal is a LiNbO3 crystal, and a terahertz wave generating method includes steps of; outputting an excitation light toward an optical crystal at a predetermined wavelength, generating a terahertz wave by exciting the optical crystal and propagating the inputted excitation light with performing a total reflection within the optical waveguide having the optical crystal as a core, and repeatedly performing an optical parametric amplification for the terahertz wave by use of the excitation light.
Thus, high-intensified terahertz waves are generated by repeatedly performing the optical parametric amplification of the terahertz waves, generated by use of the optical crystal excited by the irradiation with the excitation light, by use of the excitation light propagating with performing the total reflection within the optical waveguide including the optical crystal serving as a core.
The principles, preferred embodiment and mode of operation of the present invention have been described in the foregoing specification. However, the invention which is intended to be protected is not to be construed as limited to the particular embodiments disclosed. Further, the embodiments described herein are to be regarded as illustrative rather than restrictive. Variations and changes may be made by others, and equivalents employed, without departing from the spirit of the present invention. Accordingly, it is expressly intended that all such variations, changes and equivalents which fall within the spirit and scope of the present invention as defined in the claims, be embraced thereby.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2008-217050 | Aug 2008 | JP | national |
