Light generating device, and carbon isotope analyzing device and carbon isotope analyzing method employing same

Patent metadata

Field	Value
Publication number	US-11025028-B2
Application number	US-201816640921-A
Country	US
Kind code	B2
Filing date	Aug 24, 2018
Priority date	Aug 24, 2017
Publication date	Jun 1, 2021
Grant date	Jun 1, 2021

Abstract

Provided is a carbon isotope analysis device including a carbon dioxide isotope generator provided with a combustion unit that generates gas containing carbon dioxide isotope from carbon isotope, and a carbon dioxide isotope purifying unit; a spectrometer including optical resonators having a pair of mirrors, and a photodetector that determines intensity of light transmitted from the optical resonators; and a light generator including a single light source, a first optical fiber that transmits first light from the light source, a second optical fiber that generates second light of a longer wavelength than the first light, the second optical fiber splitting from the first optical fiber and coupling therewith downstream, a first amplifier on the first optical fiber, a second amplifier on the second optical fiber, different in band from the first amplifier, and a nonlinear optical crystal.

First claim

The invention claimed is:

1. A carbon isotope analysis device comprising:
a carbon dioxide isotope generator provided with a combustion unit that generates gas containing carbon dioxide isotope from carbon isotope, and a carbon dioxide isotope purifying unit;
a spectrometer comprising an optical resonator having a pair of mirrors, and a photodetector that determines intensity of light transmitted from the optical resonator; and
a light generator comprising a single light source, a first optical fiber that transmits first light from the light source, a second optical fiber that generates second light of a longer wavelength than the first light, the second optical fiber splitting from a splitting node of the first optical fiber and coupling with the first optical fiber at a coupling node downstream, a first amplifier that is disposed between the splitting node and the coupling node of the first optical fiber, a second amplifier that is disposed between the splitting node and the coupling node of the second optical fiber and that is different in band from the first amplifier, and a nonlinear optical crystal that allows a plurality of light beams different in frequency to propagate through to thereby generate a mid-infrared optical frequency comb of a wavelength range from 4.5 μm to 4.8 μm, from the difference in frequency, as light at an absorption wavelength of the carbon dioxide isotope,
wherein the first optical fiber further comprises a third amplifier between the first amplifier and the coupling node, and
the second optical fiber further comprises a second wavelength-shifting fiber between the splitting node and the second amplifier.

2. The carbon isotope analysis device according to claim 1 , wherein the light source is a 1.55-μm ultrashort pulsed-laser light source, the first amplifier is an Er-doped optical fiber amplifier and the second amplifier is a Tm-doped optical fiber amplifier, in the light generator.

3. The carbon isotope analysis device according to claim 2 , wherein
the first optical fiber further comprises a first wavelength-shifting fiber between the third amplifier and the coupling node.

4. The carbon isotope analysis device according to claim 3 , wherein the first wavelength-shifting fiber is a dispersion shifted fiber (DSF).

5. The carbon isotope analysis device according to claim 2 , wherein
the second optical fiber further comprises a third wavelength-shifting fiber between the second amplifier and the coupling node.

6. The carbon isotope analysis device according to claim 5 , wherein light of a wavelength range of 1.8 μm to 2.0 μm is emitted through the second wavelength-shifting fiber, and
light of a wavelength range of 2.3 μm to 2.4 μm is emitted through the third wavelength-shifting fiber.

7. The carbon isotope analysis device according to claim 5 , wherein the second wavelength-shifting fiber is a small core fiber, and
the third wavelength-shifting fiber is a highly nonlinear dispersion shifted fiber (HN-DSF).

8. The carbon isotope analysis device according to claim 1 , wherein the light generator applies light of a wavelength range of 1.3 μm to 1.7 μm through the first optical fiber and applies light of a wavelength range of 1.8 μm to 2.4 μm through the second optical fiber.

9. The carbon isotope analysis device according to claim 1 , wherein a distance in a flow direction of light, of the nonlinear optical crystal, is longer than 11 mm.

10. The carbon isotope analysis device according to claim 1 , wherein the light generator further comprises a delay line comprising a wavelength filter that separates the light from the light source to a plurality of spectral components, and a wavelength filter that adjusts the relative time delays of the plurality of spectral components and focuses the spectral components on the nonlinear crystal.

11. The carbon isotope analysis device according to claim 1 , wherein the nonlinear optical crystal is a PPMgSLT crystal or a PPLN crystal, or a GaSe crystal.

12. The carbon isotope analysis device according to claim 1 , wherein the spectrometer further comprises a cooler that cools the optical resonator.

13. The carbon isotope analysis device according to claim 1 , wherein the spectrometer further comprises a vacuum device that accommodates the optical resonator.

14. A carbon isotope analysis method, comprising:
providing a light generator that includes a single light source, a first optical fiber that transmits first light from the light source, a second optical fiber that generates second light of a longer wavelength than the first light, the second optical fiber splitting from a splitting node of the first optical fiber and coupling with the first optical fiber at a coupling node downstream, a first amplifier that is disposed between the splitting node and the coupling node of the first optical fiber, a second amplifier that is disposed between the splitting node and the coupling node of the second optical fiber and that is different in band from the first amplifier, and a nonlinear optical crystal;
generating carbon dioxide isotope from carbon isotope;
feeding the carbon dioxide isotope into an optical resonator having a pair of mirrors;
generating a plurality of light beams different in frequency, from the single light source, and amplifying intensities of the plurality of light beams obtained, by use of the first amplifier and the second amplifier;
allowing the plurality of light beams to propagate through the nonlinear optical crystal to thereby generate a mid-infrared optical frequency comb of a wavelength range from 4.5 μm to 4.8 μm, as irradiation light at an absorption wavelength of the carbon dioxide isotope, due to the difference in frequency;
measuring the intensity of the transmitted light generated by resonance of carbon dioxide isotope excited by the irradiation light; and
calculating the concentration of the carbon isotope from the intensity of the transmitted light,
wherein the first optical fiber further comprises a third amplifier between the first amplifier and the coupling node, and
wherein the second optical fiber further comprises a wavelength-shifting fiber between the splitting node and the second amplifier.

15. The carbon isotope analysis method according to claim 14 , wherein a light beam of a shorter wavelength is light of a wavelength range of 1.3 μm to 1.7 μm and a light beam of a longer wavelength is light of a wavelength range of 1.8 μm to 2.4 μm, among the light beams amplified.

16. The carbon isotope analysis method according to claim 14 , wherein the irradiation light is applied to radioactive carbon dioxide isotope 14 CO 2 .

17. A light generator comprising:
a single light source;
a first optical fiber that transmits light from the light source;
a second optical fiber that transmits light of a longer wavelength than the first optical fiber, the second optical fiber splitting from a splitting node of the first optical fiber and coupling with the first optical fiber at a coupling node downstream;
a first amplifier that is disposed between the splitting node and the coupling node of the first optical fiber;
a second amplifier that is disposed between the splitting node and the coupling node of the second optical fiber and that is different in band from the first amplifier;
a third amplifier between the first amplifier and the coupling node;
a wavelength-shifting fiber between the splitting node and the second amplifier; and
a nonlinear optical crystal through which a plurality of light beams different in frequency are allowed to propagate through to thereby g

Assignees

• Univ Nagoya Nat Univ Corp
• Sekisui Medical Co Ltd

Inventors

• Iguchi Tetsuo
• Tomita Hideki
• Nishizawa Norihiko
• SONNENSCHEIN Volker
• Terabayashi Ryohei
• Satou Atsushi

Classifications

• G01N2201/0697

  Pulsed lasers · CPC title

• H01S3/06758

  Tandem amplifiers · CPC title

• H01S3/0092

  Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity (nonlinear frequency conversion per se G02F1/35) · CPC title

• H01S3/1608

  erbium · CPC title

• G02F1/3551 Primary

  Crystals · CPC title