US2005215985A1PendingUtilityA1
Method of generating an ultra-short pulse using a high-frequency ring oscillator
Est. expiryAug 11, 2023(expired)· nominal 20-yr term from priority
A61B 18/20
41
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Abstract
The present invention provides a method of generating an ultra-short pulse in a ring oscillator by amplifying a series of wavelength-swept-with time pulses using one or more amplifiers, compressing the amplified wavelength-swept-with time pulses, reducing the compressed pulses to sub-picosecond pulses, stretching the sub-picosecond pulses into wavelength-swept-with time pulses and returning the stretched pulses to the one or more amplifiers.
Claims
exact text as granted — not AI-modified1 . A method of generating an ultra-short pulse in a ring oscillator, comprising the steps of:
amplifying a series of wavelength-swept-with time pulses using one or more amplifiers; compressing the amplified wavelength-swept-with time pulses; reducing the compressed pulses to sub-picosecond pulses; stretching the sub-picosecond pulses into wavelength-swept-with time pulses; and returning the stretched pulses to the one or more amplifiers.
2 . The method of claim 1 , wherein the one or more of the one or more amplifiers comprise one or more semiconductor optical amplifiers.
3 . The method of claim 1 , wherein the compressing is preformed by one or more gratings.
4 . The method of claim 3 , wherein the one or more gratings comprise a chirped fiber Bragg grating.
5 . The method of claim 1 , wherein the reducing is preformed by one or more nonlinear optical elements.
6 . The method of claim 5 , wherein the one or more nonlinear optical elements comprise a carbon nanotube saturable absorber.
7 . The method of claim 1 , wherein the stretching is preformed by one or more gratings.
8 . The method of claim 7 , wherein the one or more gratings comprise a chirped fiber Bragg grating.
9 . The method of claim 1 , wherein the ring oscillator is coupled through an output coupler.
10 . The method of claim 9 , wherein a portion of each of the amplified pulses are coupled out through the output coupler.
11 . The method of claim 9 , wherein a portion of each of the compressed pulses are coupled out through the output coupler.
12 . The method of claim 1 , wherein the oscillator runs at a repetition rate of at least 25 MHz.
13 . The method of claim 12 , wherein the oscillator further comprises a pulse selector to give a pulse-selector output with a repetition rate of less than one-tenth the oscillator repetition rate.
14 . The method of claim 13 , further comprising the step of synchronizing the oscillator and the pulse selector, wherein an electrical impulse generator is used to activate a device in the oscillator.
15 . The method of claim 14 , wherein the electrical impulse generator is used to activate one or more semiconductor optical amplifiers.
16 . The method of claim 14 , wherein the electrical impulse generator is used to activate an electro-optic modulator to produce a temporal window of net positive pulse amplification within the oscillator.
17 . The method of claim 1 , wherein the oscillator contains one or more polarization controllers.
18 . The method of claim 1 , wherein the step of stretching and the step of compressing are preformed by one or more chirped fiber Bragg gratings.
19 . The method of claim 1 , wherein one or more optical connections between components are made through optical fiber.Cited by (0)
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