# US 2008/0187010 A1 · Laser Device Triggered by a Photonic Fibre > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 2008/0187010 A1 - Document ID: US20080187010A1 - Status: Published application - Kind: A1 - Application number: 11/912,894 - Filed: 2006-04-27 - Published: 2008-08-07 - Earliest claimed: 2005-04-28 - Assignees: Eolite Systems - Inventors: Philippe Metivier; Philippe Yvernault; Sebastien Ermeneux - Web page: https://patentgrep.com/patent/US20080187010A1 ## CPC - H01S 3/067: Fibre lasers - H01S 3/117: using intracavity acousto-optic devices - H01S 3/06729: {Peculiar transverse fibre profile} - H01S 3/06741: {Photonic crystal fibre, i.e. the fibre having a photonic bandgap} - H01S: DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL ## Abstract A device producing laser pulses of durations smaller than 30 ns, and including along its internal optical axis: a laser resonator of optical length smaller than 2 m including two reflecting ends and incorporating an MPF photonic fibre pumped continuously by at least one pump wave with laser diodes, the laser medium being a medium where the laser wave is guided and has a gain with very weak signal greater than 10 per passage, the resonator also incorporating an optical modulator. The optical modulator may deflect the internal laser axis via an electric control along two stable directions, the first direction corresponding to an axis along which the internal laser beam undergoes sufficient losses to prevent the laser effect, the second direction corresponding to an axis along which the laser beam is reflected towards itself at least partially by an optical return element. ## Claims ### Claim 1 A device for cyclically generating short duration laser pulses typically smaller than 30 ns, the device including a laser resonator of optical length smaller than 2 m including two reflecting ends and incorporating an MPF photonic fibre pumped continuously by at least one pump wave derived from power semi-conductive laser diodes focussed by optical means for collimating the fibre, the MPF fibre including a medium where an internal laser beam is guided and having a gain with very weak signal greater than 10 per passage through the gain medium. the laser resonator also incorporating an optical modulator, the optical modulator being able to deflect the axis of the internal laser beam, said optical modulator is actuated by an electric control, along two stable directions, the first direction corresponding to an axis along which the internal laser beam undergoes sufficient losses to prevent the laser effect from being triggered, the device then being in an open cavity mode, and the second direction corresponding to an axis along which the internal laser beam is reflected towards itself at least partially by an optical return means closing the resonator at a first one of its ends, the device then being in a closed cavity mode, the second end of the laser resonator being closed by a means at least partially reflecting situated on the other side of the amplifying medium, characterised in that the device generates a peak power of at least 33 KW, and that the modulator possesses a switching time greater than the time taken by light to travel through the cavity and that it is used in a configuration, where the loss factor introduced in the state corresponding to the open cavity mode is greater than the gain with very weak signal of the resonator and in that the amplifying medium preserves the state of polarisation. ### Claim 2 (depends on 1) A device according to claim 1, characterised in that the modulator ensures directly the closing of the resonator in activated mode. ### Claim 3 (depends on 1) A device according to claim 1, characterised in that the optical modulator is an acousto-optical modulator. ### Claim 4 (depends on 3) A device according to claim 3, characterised in that the optical return means used for closing the resonator is positioned so that the angle formed by its normal and the laser beam at the output of the non-activated modulator is equal to the angle between the order 0 and the order 1 or −1 of the acousto-optical modulator. ### Claim 5 (depends on 3) A device according to claim 3, characterised in that the acousto-optical modulator draws practically no electrical control energy during the locked mode of the laser. ### Claim 6 (depends on 1) A device according to claim 1, characterised in that it is monolithic, the members of the optical cavity being made of silica and/or of glass and being attached to one another. ### Claim 7 (depends on 1) A device according to claim 1, characterised in that the optical modulator is mechanical and that it acts by moving mechanically an optical means. ### Claim 8 (depends on 1) A device according to claim 1, characterised in that it comprises means enabling to generate laser pulses of duration smaller than 30 ns at rates above 50 kHz with a beam quality better than 1.5 times the diffraction. ### Claim 9 (depends on 1) A device according to claim 1, characterised in that one of the ends of the MPF fibre is tilted relative to the normal to the longitudinal axis of the fibre. ### Claim 10 (depends on 1) A device according to claim 1, characterised in that the MPF fibre is pumped at both its ends. ### Claim 11 A device for cyclically generating short duration laser pulses, typically smaller than 30 ns, the device including a laser resonator of optical length smaller than 2 m including two reflecting ends and incorporating an MPF photonic fibre pumped continuously by at least one pump wave derived from power semi-conductive laser diodes focussed by optical means for collimating the fibre, the MPF fibre including a medium where an internal laser beam is guided and having a gain with very weak signal greater than 10 per passage through the gain medium, the laser resonator also incorporating an optical modulator, the optical modulator being able to deflect the axis of the internal laser beam, said optical modulator is actuated by an electric control, along two stable directions, the first direction corresponding to an axis along which the internal laser beam undergoes sufficient losses to prevent the laser effect from being triggered, the device then being in an open cavity mode, and the second direction corresponding to an axis along which the internal laser beam is reflected towards itself at least partially by an optical return means closing the resonator at a first one of its ends, the device then being in a closed cavity mode, the second end of the laser resonator being closed by a means at least partially reflecting situated on the other side of the amplifying medium, characterised in that the modulator possesses a switching time greater than the time taken by light to travel through the cavity, and that it is used in a configuration where the loss factor introduced in the state corresponding to the open cavity mode is greater than the gain with very weak signal of the resonator, in that the amplifying medium preserves the state of polarisation, and in that it includes means for generating harmonic radiation with non-linear crystals. ### Claim 12 (depends on 4) A device according to claim 4, characterised in that the acousto-optical modulator draws practically no electrical control energy during the locked mode of the laser. ### Claim 13 (depends on 2) A device according to claim 2, characterised in that the optical modulator is mechanical and that it acts by moving mechanically an optical means.