Carbon isotope analysis device and carbon isotope analysis method
US-2016349177-A1 · Dec 1, 2016 · US
US2022190547A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2022190547-A1 |
| Application number | US-202117555901-A |
| Country | US |
| Kind code | A1 |
| Filing date | Dec 20, 2021 |
| Priority date | May 26, 2016 |
| Publication date | Jun 16, 2022 |
| Grant date | — |
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A pulsed light generation device, includes: a first optical fiber through which first pulsed light and second pulsed light, having an intensity that decreases while an intensity of the first pulsed light increases, and increases while the intensity of the first pulsed light decreases, having been multiplexed and entered therein, are propagated; and a second optical fiber at which the first pulsed light, having exited the first optical fiber and entered therein, is amplified while being propagated therein, wherein: at the first optical fiber, phase modulation occurs in the first pulsed light due to cross phase modulation caused by the second pulsed light; and self-phase modulation occurring in the first pulsed light at the second optical fiber is diminished by the phase modulation having occurred at the first optical fiber.
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What is claimed is: 1 . A light amplification device, comprising: a first optical fiber to receive first pulsed light and second pulsed light, the second pulsed light having a peak intensity greater than a peak intensity of the first pulsed light; and a second optical fiber to receive the first pulsed light from the first optical fiber and to amplify the first pulsed light, wherein nonlinearity of the first optical fiber is greater than nonlinearity of the second optical fiber, and a length of the first optical fiber is longer than a length of the second optical fiber. 2 . A light amplification device, comprising: a first optical fiber to receive first pulsed light and second pulsed light, the second pulsed light having a peak intensity greater than a peak intensity of the first pulsed light; and a second optical fiber to receive the first pulsed light from the first optical fiber and to amplify the first pulsed light, wherein a mode field diameter of the first optical fiber is smaller than a mode field diameter of the second optical fiber, and a length of the first optical fiber is longer than a length of the second optical fiber.
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