METHOD OF FABRICATING TUBULAR LASER LIGHT SOURCE, TUBULAR LASER LIGHT SOURCE AND DETECTION DEVICE USING TUBULAR LASER LIGHT SOURCE

Abstract

A tube preparation step of preparing a resin tube that has a tube wall impregnable with a solution including a fine substance and is made of a light-transmitting resin material, a solution preparation step of preparing a solution that includes a fine fluorescent substance that emits fluorescence or a fine scattering substance that scatters light as an oscillation material and an impregnation step of causing the resin tube to be immersed in the solution and causing the tube wall of the resin tube to be impregnated with the oscillation material, are included.

Claims

1. A method of fabricating a tubular laser light source that oscillates laser light outwardly of a tube wall based on light emitted from a fluorescent substance or scattered by a scattering substance, including: a tube preparation step of preparing a resin tube that has the tube wall impregnable with a solution including a fine substance and is made of a light-transmitting resin material; a solution preparation step of preparing a solution that includes a fine fluorescent substance that emits fluorescence or a fine scattering substance that scatters light as an oscillation material; and an impregnation step of causing the resin tube to be immersed in the solution and causing the tube wall of the resin tube to be impregnated with the oscillation material.

2. The method of fabricating a tubular laser light source according to claim 1, wherein a refractive index adjusting substance for adjusting a refractive index in the tube wall is included in the solution in the solution preparation step, and the tube wall is impregnated with the refractive index adjusting substance together with the oscillation material in the impregnation step.

3. The method of fabricating a tubular laser light source according to claim 1, wherein the resin tube is an acrylic acid tube.

4. A tubular laser light source configured to oscillate laser light outwardly of a tube wall from an inside of the tube wall based on light emitted from a fluorescent substance or scattered by a scattering substance, wherein the tube wall is impregnable with a solution including a fine substance, and the tube wall, of a resin tube that is made of a light-transmitting resin material, is impregnated with a fine fluorescent substance that emits fluorescence or a fine scattering substance that scatters light together with the fluorescent substance as an oscillation material.

5. The tubular laser light source according to claim 4, wherein the tube wall is impregnated with a refractive index adjusting substance for adjusting a refractive index in the tube wall together with the oscillation material.

6. The tubular laser light source according to claim 4, wherein the oscillation material is an organic EL material, and the tubular laser light source includes a voltage applier that applies a voltage for exciting the organic EL material to a portion between an inner surface and an outer surface of the resin tube.

7. The tubular laser light source according to claim 4, wherein the resin tube is an acrylic acid tube.

8. A detection device comprising: a measurement cell configured such that a sample flows through an inner flow path of the tubular laser light source according to claim 4; an oscillator that causes the tubular laser light source to oscillate laser light; a detector that detects measurement light emitted outwardly of a tube wall of the tubular laser light source; and a calculator configured to obtain concentration of a component of the sample flowing through the inner flow path of the tubular laser light source based on intensity or a wavelength of the measurement light detected by the detector.

9. The detection device according to claim 8, wherein the measurement cell is configured such that a plurality of the tubular laser light sources configured to oscillate laser light rays that are different from one another are in fluid connection with one another in series or in parallel, the detector has a detection element that detects measurement light from each of the plurality of the tubular laser light sources, and the calculator is configured to obtain concentration of a component or a type of component of a sample flowing through an inner flow path of the tubular laser light source based on intensity or a wavelength of each measurement light detected by the detection element of the detector.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0028] FIG. 1 is a schematic diagram showing the configuration of one inventive example of a detection device using a tubular laser light source.

[0029] FIG. 2 is a cross sectional view of the tubular laser light source of the same inventive example.

[0030] FIG. 3 is a diagram showing a method of fabricating the tubular laser light source in each step.

[0031] FIG. 4(A) is a graph showing an oscillation wavelength spectrum of the tubular laser light source fabricated by impregnation of a tube wall of a resin tube with DCM, and FIG. 4(B) is a graph showing the energy required for laser oscillation.

[0032] FIG. 5(A) is a graph showing an oscillation wavelength spectrum of a tubular laser light source fabricated by impregnation of a tube wall of a resin tube with DCM and 5CB, and FIG. 5(B) is a graph showing the energy required for laser oscillation.

[0033] FIG. 6 is an oscillation wavelength spectrum of a tubular laser light source (random laser) fabricated by impregnation of a tube wall of a resin tube with DCM and 5CB.

[0034] FIG. 7 is a schematic diagram showing the configuration of another inventive example of a detection device using a tubular laser light source.

DESCRIPTION OF EMBODIMENTS

[0035] FIG. 1 shows one inventive example of a detection device using a tubular laser light source.

[0036] The detection device of this inventive example uses the tubular laser light source 2 as a measurement cell through which a sample passes. As shown in FIG. 2, the tubular laser light source 2 has a tube wall 2b, of a resin tube made of a light-transmitting material, that is impregnated with an oscillation material. The oscillation material includes a fine fluorescent substance that emits fluorescence or a fine scattering substance that scatters light.

[0037] In a case where the oscillation material is a fluorescent substance, when the fluorescent substance in the tube wall 2b is excited, the light having a specific wavelength of the fluorescence emitted from the fluorescent substance repeats total reflection at the interface between the tube wall 2b of the tubular laser light source 2 and an air layer, thereby being oscillated. As a result, when the fluorescent substance is irradiated with excitation light having certain intensity or higher, the light having the specific wavelength is oscillated outwardly from the inside of the tube wall of the tubular laser light source 2 as laser light. On the other hand, in a case where the oscillation material is a scattering substance, when the scattering substance in the tube wall 2b is irradiated with light from the outside, the fluorescence excited by the light is scattered by the scattering substance. Further, the light having the specific wavelength is repeatedly reflected from the interface between the tube wall 2b of the tubular laser light source 2 and an air layer or repeats multiple scattering in the tube, thereby being oscillated. As a result, in a case where the scattering substance is irradiated with light having certain intensity or higher, the light having the specific wavelength is oscillated outwardly from the inside of the tube wall 2b of the tubular laser light source 2 as laser light.

[0038] Returning to FIG. 1, an oscillator 4 causes the tubular laser light source 2 to oscillate laser light by utilizing the oscillation material in the tube wall 2b of the tubular laser light source 2. In a case where the oscillation material with which the tube wall 2b is impregnated is a fluorescent substance, an excitation light source that emits excitation light for exciting the fluorescent substance is cited as the oscillator 4.

[0039] While one example of the fluorescent substance is DCM (4-(dicyanomethylene)-2-methyl 6-(4-dimethylaminostyryl)-4H-pyran), any fine substance that emits fluorescence when being excited can be used.

[0040] An organic EL material such as DOO-PPV (2,5-dioctyloxy poly (p-phenylene vinylene)) can also be used as a fluorescent substance. The oscillator 4 in this case includes a voltage applier configured to apply a voltage from both of the inner surface and the outer surface of the tubular laser light source 2 to excite the organic EL material by using a current injection system.

[0041] On the other hand, in a case where the oscillation material with which the tube wall 2b is impregnated is a scattering substance, a light source for irradiating a scattering substance with light having any wavelength can be used as the oscillator 4. Although one example of a scattering substance includes submicron to micron-order bubbles present inside of the tube, fogging caused by intentional degradation of resin, and nanoparticles of a size (100 nm or less in diameter) with which the resin tube can be impregnated, any substance can be used as long as the substance is fine and scatters light.

[0042] A detector 6 is used to detect the measurement light emitted from the tubular laser light source 2. Although being realized by a photodiode, for example, the detector 6 may include a filter for extracting the light serving as the measurement light, a spectrometer and the like.

[0043] A calculator 8 is configured to obtain absorbance, the refractive index, Raman scattering light intensity, etc. of the sample flowing through an inner flow path 2a of the tubular laser light source 2 based on a measurement value of intensity of the measurement light detected by the detector 6. The calculator 8 is the function obtained when an arithmetic element executes a predetermined program in a dedicated computer or a general-purpose personal computer.

[0044] In a case where the light that has the specific wavelength and has been oscillated in the tubular laser light source 2 is detected by the detector 6 as the measurement light, and a change amount (an amount of decrease) is obtained, the absorbance of the sample flowing through the inner flow path 2a of the tubular laser light source 2 can be obtained.

[0045] Further, it is possible to obtain the Raman scattering light intensity of the sample by using the light having the same wavelength as that of the light oscillated in the tubular laser light source 2 as the excitation light and measuring the light having a wavelength different from the oscillation wavelength generated from the component of the excited sample.

[0046] Next, the method of fabricating the tubular laser light source 2 will be described with reference to FIG. 2.

[0047] A resin tube 2 (FIG. 2(A)) that can be impregnated with the solution including a fine oscillation material such as a fluorescent substance or a scattering substance and is made of a light-transmitting material, and the solution 10 (FIG. 2(B)) including an oscillation material, are prepared. Here, light transmissivity means that it does not absorb the light having the wavelength used for measurement (transmittance of 99% or more, for example). An acrylic acid tube or a PMMA (methyl molymethacrylate) tube can be used as the resin tube 2, for example. The solution 10 including an oscillation material is the mixture of an oscillation material such as DCM or DOO-PPV with a solvent such as 2-ethoxyethyl acetate or acetone. The solution 10 may include a plurality of types of oscillation materials. It is possible to make a tube be bendable by fabricating the tube using acrylic acid or the like. In a case where being used for analysis with a flow path such as a liquid chromatograph, the present laser can be installed in more places (the laser can also be used as a pipe).

[0048] The resin tube 2 is immersed in the solution 10 including an oscillation material for a certain period of time (one hour, for example) (FIG. 2(C)), and the tube wall 2b of the resin tube 2 is impregnated with the oscillation material (FIG. 2(D)).

[0049] The oscillation material with which the tube wall 2b is to be impregnated is selected such that the light having a wavelength corresponding to the measurement purpose is oscillated in the tubular laser light source 2. The wavelength of the light oscillated in the tubular laser light source 2 is determined based on the inner and outer diameters of the tubular laser light source 2, the refractive index in the tube wall 2b and so on in addition to the type of the oscillation material. The refractive index in the tube wall 2b can be adjusted by impregnation of the tube wall 2b with a nematic liquid crystal (5CB:4-cyano-4A-npentylbiphenyl), for example, as a refractive index adjusting substance together with the oscillation material. As the refractive index adjusting substance, a smectic liquid crystal, a polymer liquid having a high viscosity or the like can be used in addition to the nematic liquid crystal.

[0050] In a case where the refractive index in the tube wall 2b is increased by impregnation of the tube wall 2b with a refractive index adjusting substance such as a liquid crystal, a Q value of a resonator is increased. Thus, a threshold value for oscillating laser light can be lowered. Further, it is possible to change the wavelength of the laser light oscillated in the tubular laser light source 2 without changing the type of a fluorescent substance or the dimension of the resin tube.

[0051] Each of FIGS. 4 and 5 shows the measurement data of the tubular laser light source (FIG. 4) that is fabricated by impregnation of the tube wall 2b with DCM as an oscillation material, and the measurement data of the tubular laser light source (FIG. 5) fabricated by impregnation of the tube wall 2b with a liquid crystal (5CB) as a refractive index adjusting substance. Each of FIGS. 4(A) and 5(A) shows the oscillation wavelength spectrum, and each of FIGS. 4(B) and 5(B) shows the energy required for laser oscillation.

[0052] When FIG. 4(A) and FIG. 5(A) are compared to each other, in a case where the tube wall 2b is not impregnated with 5CB (FIG. 4(A)), which is a refractive index adjusting substance, the oscillation wavelength is about 603 nm. On the contrary, in a case where the tube wall 2b is impregnated with 5CB (FIG. 5(A)), the oscillation wavelength is changed to about 617 nm. From this comparison, it is found that it is possible to adjust the oscillation wavelength by changing the refractive index in the tube wall 2b by using a refractive index adjusting substance.

[0053] Further, when FIG. 5(B) and FIG. 5(B) are compared to each other, in a case where the tube wall 2b is not impregnated with 5CB, the threshold value for laser oscillation is 38 J/mm.sup.2. On the contrary, in a case where the tube wall 2b is impregnated with 5CB, the threshold value for laser oscillation is lowered to 25 J/mm.sup.2. From this comparison, it is found that it is possible to lower the threshold value for laser oscillation by increasing the refractive index in the tube wall 2b by using a refractive index adjusting substance.

[0054] FIG. 6 shows the measurement data of the tubular laser light source that carries out random laser oscillation, the tubular laser light source being fabricated in a case where a tube having a tube wall 2b that is impregnated with DCM/5CB as an oscillation material is fabricated, resin is degraded such that transparency of the tube is reduced, and then resin becomes a scattering substance. The intensity of excitation light is 1350 J/mm.sup.2, and the excitation light having higher intensity is required as compared to that of the tubular laser of FIG. 5. This is the measurement data in regard to laser oscillation utilizing multiple scattering that occurs among scatters. Thus, a Q value is lower and the threshold value is higher as compared to the above-mentioned WGM laser.

[0055] Next, an application example in which a plurality of tubular laser light sources 2 are used will be described with reference to FIG. 7.

[0056] In this inventive example, three tubular laser light sources 2-1 to 2-3 are in fluid connection with one another in series to constitute a measurement cell through which a sample passes. The sample sequentially flows through respective inner flow paths from the most upstream tubular laser light source 2-1 to the most downstream tubular laser light source 2-3. The type of the oscillation material, and presence or absence of a refractive index adjusting substance, or the type of a refractive index adjusting substance are adjusted such that the tubular laser light sources 2-1 to 2-3 oscillate the laser light rays having wavelengths that are different from one another. The number of tubular laser light sources may be any number, and may be two, four or more than four.

[0057] Further, oscillators 4-1 to 4-3 for causing each of the tubular laser light sources 2-1 to 2-3 to carry out laser oscillation, and detectors 6-1 to 6-3 for detecting the measurement light from the tubular laser light sources 2-1 to 2-3 are provided. The signals obtained by the detectors 6-1 to 6-3 are configured to be acquired by a common calculator 8.

[0058] As described above, the measurement cell is constituted by the plurality of tubular laser light sources 2-1 to 2-3 that oscillate laser light rays having wavelengths that are different from one another. Thus, the measurement can be carried out at a time in regards to the light rays having a plurality of wavelengths. The inventive example of FIG. 7 is merely one example of an embodiment in which a plurality of tubular laser light sources 2 are used.

[0059] In this manner, the tubular laser light source 2 of the present invention, which is easily fabricated and simply configured, can be not only provided with the both functions of the light source and the measurement cell in the detection device but also can be used for various purposes using a combination of the plurality of tubular laser light sources 2.

[0060] While the description has been made on the assumption that the sample flowing through the inner flow path of the tubular laser light source 2 is irradiated with laser light oscillated by the tubular laser light source in the above-mentioned inventive example, the present invention is not limited to such a purpose. The present invention may be configured to irradiate another object with the laser light oscillated by the tubular laser light source 2.

DESCRIPTION OF REFERENCE NUMERALS

[0061] 2, 2-1, 2-2, 2-3 Tubular Laser Light Sources [0062] 2a Inner Flow Path [0063] 2b Tube Wall [0064] 4, 4-1, 4-2, 4-3 Oscillators [0065] 6, 6-1, 6-2, 6-3 Detectors [0066] 8 Calculator [0067] 10 Solution Including oscillation material