Supercontinuum light source
US-10441158-B2 · Oct 15, 2019 · US
US11154189B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11154189-B2 |
| Application number | US-201916581912-A |
| Country | US |
| Kind code | B2 |
| Filing date | Sep 25, 2019 |
| Priority date | Jun 1, 2012 |
| Publication date | Oct 26, 2021 |
| Grant date | Oct 26, 2021 |
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A supercontinuum light source can include a seed laser arranged to provide seed pulses with a pulse frequency F seed ; a pulse frequency multiplier (PFM) arranged to multiply the seed pulses by converting pulses having the pulse frequency F seed to pump pulses with a pulse frequency F pump , where F pump is larger than F seed ; and a non-linear element arranged to receive said pump pulses and convert said pump pulses to pulses of supercontinuum light. The PFM can further include a splitter for splitting pulses into first and second sub beams each having the same pulse frequency, where the PFM is configured such that the sub beams experience different delays; and a combiner for combining said first and second sub beams into a beam having the pulse frequency that is greater than said same pulse frequency. The splitter can have an uneven splitter ratio.
Opening claim text (preview).
The invention claimed is: 1. A supercontinuum light source comprising: a seed laser configured to provide seed pulses with a pulse frequency F seed ; a pulse frequency multiplier (PFM) configured to multiply the seed pulses by converting seed pulses having the pulse frequency F seed to pump pulses with a pulse frequency F pump , where F pump is larger than F seed ; a non-linear element configured to receive said pump pulses and convert said pump pulses to pulses of supercontinuum light; and first and second amplifiers, one of the amplifiers configured to amplify pulses having the pulse frequency F seed and the other of the amplifiers configured to amplify pulses having the pulse frequency F pump , wherein said PFM is located between the amplifiers. 2. The supercontinuum light source of claim 1 , wherein said PFM comprises an attenuator configured to attenuate pulses of light having a pulse frequency that is less than F pump . 3. The supercontinuum light source of claim 1 , wherein said non-linear element comprises a microstructured optical fiber. 4. The supercontinuum light source of claim 1 , wherein F pump is 150 MHz or more. 5. The supercontinuum light source of claim 1 , wherein said seed laser is configured to provide seed pulses with a pulse duration t seed that is longer than about 1 ps. 6. The supercontinuum light source of claim 5 , wherein t seed is shorter than about 50 ps. 7. The supercontinuum light source of claim 1 , wherein the supercontinuum light source is configured such that the total average optical power in the range 400 nm-850 nm is less than 100 mW. 8. The supercontinuum light source of claim 1 , wherein the amplifiers provide an increase in pulse energy and peak power relative to an output from the seed laser. 9. The supercontinuum light source of claim 1 , wherein the supercontinuum light source is configured such that peak power of the pulses out of the first amplifier is constant. 10. The supercontinuum light source of claim 1 , wherein the supercontinuum light source is configured such that peak power of the pulses out of the second amplifier is constant. 11. The supercontinuum light source of claim 1 , wherein said seed laser comprises a mode locked Yb laser. 12. The supercontinuum light source of claim 11 , wherein said mode locked Yb laser comprises a fiber laser that is passively mode locked via a SESAM (Semiconductor Saturable Absorber Mirror).
Non-linear optics · CPC title
in an optical waveguide structure (G02F1/377, {G02F1/395} take precedence) · CPC title
Systems for changing the beam intensity distribution, e.g. Gaussian to top-hat · CPC title
for producing a supercontinuum · CPC title
provided with illuminating means (A61B3/117, A61B3/14 take precedence) · CPC title
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