US2017310068A1PendingUtilityA1
Giant-chirp oscillator
Est. expiryJun 14, 2032(~5.9 yrs left)· nominal 20-yr term from priority
H01S 3/1618H01S 3/1112H01S 3/06791H01S 3/06725H01S 3/06712H01S 3/06783
40
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Claims
Abstract
A laser apparatus operable to generate giant chirp pulses. The pulses have a centre frequency comprising an arrangement of components connected or connectable to form a closed ring cavity. The components comprise a first gain medium, an optical isolator, a length of single mode fibre, a mode locking device, an output coupler, and an optical filter. Each of the components are optical fibre based components.
Claims
exact text as granted — not AI-modified1 - 32 . (canceled)
33 . A laser apparatus operable to generate giant chirp pulses having a center frequency, comprising an arrangement of components connected, or connectable to form a cavity, the components comprising a first gain medium, an optical isolator, a length of single mode fibre, a passive mode locking device, an output coupler, and an optical filter, wherein each of the components are optical fibre based components.
34 . A laser as claimed in claim 33 , wherein the optical fibre components are polarization maintaining components.
35 . A laser as claimed in claim 33 , wherein the components have, or substantially have, a normal dispersion relative to the center frequency.
36 . A laser as claimed in claim 33 , wherein the components have a net normal dispersion relative to the center frequency.
37 . A laser as claimed in claim 33 , wherein the mode locking device is a nonlinear amplified loop mirror comprising at least an optical coupler operable to provide and input and an output, and a second gain medium operable to provide energy to a propagating pulse.
38 . A laser as claimed in claim 33 , wherein the mode locking device is operable to mode lock the laser by varying the energy of the light from the second pump source.
39 . A laser as claimed in claim 33 , wherein the length of single mode fibre is operable in the cavity to receive light from the first gain medium and output light to the second gain medium.
40 . A laser as claimed in claim 33 , wherein the length of single mode fibre is operable to impart broadening to a pulse propagating within it.
41 . A laser as claimed in claim 33 , wherein the laser is operable to generate giant chirp pulses comprising a chirp that is substantially linear and positive.
42 . A laser as claimed in claim 33 , wherein varying the length of the single mode fibre varies at least one or more of the pulse repetition rate, the pulse energy or the pulse duration.
43 . A laser as claimed in claim 33 , wherein the optical filter has an operating bandwidth centered at or approximately at a desired pulse wavelength.
44 . A laser operable as a giant chirp oscillator, comprising a loop of substantially polarization maintaining, substantially normal dispersion, optical fibre based components including a gain medium, a section of single mode fibre, and an nonlinear amplifying optical loop mirror.
45 . A laser operable as a giant chirp oscillator, comprising:
a first lasing section comprising all normal dispersion optical components and a second lasing section comprising a nonlinear amplifying loop mirror, wherein the first and second lasing sections are operable to generate giant chirp pulses.
46 . A laser as claimed in claim 45 wherein the first and second lasing sections each comprise a loop of polarization maintaining, all normal dispersion optical fibre, wherein a first loop comprises a polarization maintaining normal dispersion first gain medium, a polarization maintaining normal dispersion optical filter, a polarization maintaining normal dispersion optical isolator, and a length of polarization maintaining normal dispersion single mode fibre, and a second loop comprises a polarization maintaining normal dispersion second gain medium, and the first loop is optically coupled to the second loop by a wavelength division multiplexing optical coupler.
47 . A laser as claimed in claim 46 wherein the first loop further comprises wavelength division multiplexing optical coupler to couple a source of pump light into the first gain medium, the second loop further comprises wavelength division multiplexing optical coupler to couple a source of pump light into the second gain medium, and at least one of the sources of pump light are operable to mode lock the oscillator.Join the waitlist — get patent alerts
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