Optical imaging device and method for imaging a sample
US-2015366451-A1 · Dec 24, 2015 · US
US9683830B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9683830-B2 |
| Application number | US-201414565900-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 10, 2014 |
| Priority date | Oct 29, 2014 |
| Publication date | Jun 20, 2017 |
| Grant date | Jun 20, 2017 |
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A fiber light source comprises a laser pump configured to generate a pump laser beam at a predetermined wavelength; a first segment of rare earth doped fiber; a second segment of rare earth doped fiber; and an optical coupler coupled to a first end of the first segment and a first end of the second segment. The optical coupler is configured to split the pump laser beam based on a power coupling ratio. The first segment generates a first stimulated emission having a first mean wavelength sensitivity to pump laser power fluctuations and the second segment generates a second stimulated emission having a second mean wavelength sensitivity to pump laser power fluctuations such that a combined stimulated emission is approximately insensitive to pump laser power fluctuations.
Opening claim text (preview).
What is claimed is: 1. A fiber light source comprising: a pump laser configured to generate a pump laser beam at a predetermined wavelength; a first segment of rare earth doped fiber; a second segment of rare earth doped fiber; and an optical coupler coupled to a first end of the first segment and a first end of the second segment, the optical coupler configured to split the pump laser beam based on a power coupling ratio such that a first portion of the pump laser beam is coupled to the first segment at a first power level and a second portion of the pump laser beam is coupled to the second segment at a second power level; wherein the first segment of rare earth doped fiber generates a first stimulated emission having a first mean wavelength sensitivity to pump laser power fluctuations and the second segment of rare earth doped fiber generates a second stimulated emission having a second mean wavelength sensitivity to pump laser power fluctuations such that, when the first stimulated emission is combined with the second stimulated emission, a combined stimulated emission is approximately insensitive to pump laser power fluctuations. 2. The fiber light source of claim 1 , wherein the first segment of rare earth doped fiber has a first length and the second segment of rare earth doped fiber has a second length different from the first length. 3. The fiber light source of claim 1 , wherein the optical coupler is a first optical coupler and the power coupling ratio is a first power coupling ratio, the fiber light source further comprising a second optical coupler coupled to a second end of the first segment and to a second end of the second segment; wherein the second optical coupler is configured to combine the first stimulated emission and the second stimulated emission based on a second power coupling ratio. 4. The fiber light source of claim 3 , wherein the second power coupling ratio is different from the first power coupling ratio. 5. The fiber light source of claim 3 , wherein the second coupler comprises one of a polarization beam combiner configured to combine the first stimulated emission and the second stimulated emission with different polarization states or a wavelength division multiplexer configured to combine the first stimulated emission and the second stimulated emission with different wavelengths. 6. The fiber light source of claim 1 , wherein a second end of the first segment of rare earth doped fiber is coupled to a first termination fiber and the second end of the second segment of rare earth doped fiber is coupled to a second termination fiber; wherein the optical coupler is configured to combine the first stimulated emission and the second stimulated emission based on the power coupling ratio. 7. The fiber light source of claim 6 , wherein the first segment of rare earth doped fiber has a first length and the second segment of rare earth doped fiber has a second length different from the first length. 8. The fiber light source of claim 1 , wherein the first segment of rare earth doped fiber and the second segment of rare earth doped fiber are doped with one of the same rare earth ions or different rare earth ions such that the first and second segments of rare earth doped fiber generate respective emissions with one of different polarization states or different wavelengths. 9. A method of reducing mean wavelength sensitivity of a fiber light source to pump power fluctuations, the method comprising: generating a pump laser beam at a predetermined wavelength; splitting the pump laser beam into a first portion of the pump laser beam and a second portion of the pump laser beam based on a power coupling ratio, the first portion of the pump laser beam having a first power level and the second portion of the pump laser beam having a second power level; providing the first portion of the pump laser beam to a first segment of rare earth doped fiber, the first segment of rare earth doped fiber configured to generate a first stimulated emission having a first mean wavelength sensitivity to pump power fluctuations based on the first portion of the pump laser beam; providing the second portion of the pump laser beam to a second segment of rare earth doped fiber, the second segment of rare earth doped fiber configured to generate a second stimulated emission having a second mean wavelength sensitivity to pump power fluctuations based on the second portion of the pump laser beam; and combining the first stimulated emission with the second stimulated emission such that a combined stimulated emission is approximately insensitive to pump laser power fluctuations. 10. The method of claim 9 , wherein splitting the pump laser beam comprises splitting the pump laser beam with a first optical coupler based on a first power coupling ratio; and wherein combining the first stimulated emission with the second stimulated emission comprises combining the first stimulated emission with the second stimulated emission in the first optical coupler based on the first power coupling ratio. 11. The method of claim 9 , wherein splitting the pump laser beam comprises splitting the pump laser beam with a first optical coupler based on a first power coupling ratio; and wherein combining the first stimulated emission with the second stimulated emission comprises combining the first stimulated emission with the second stimulated emission in a second optical coupler based on a second power coupling ratio. 12. The method of claim 9 , wherein at least one of the first segment of rare earth doped fiber and the second segment of rare earth doped fiber comprises an erbium doped fiber.
Two or more frequencies or sources used for interferometric measurement (using only beat G01B9/02003) · CPC title
by particular optical compensation or alignment elements, e.g. dispersion compensation · CPC title
Fibre lasers · CPC title
Stabilisation of laser output parameters, e.g. frequency or amplitude · CPC title
the pumped medium being a fibre · CPC title
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