# US 10,770,860 B2 · Lookthrough compression arrangement > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 10,770,860 B2 - Document ID: US10770860B2 - Status: Granted - Kind: B2 - Application number: 15/788,429 - Filed: 2017-10-19 - Published: 2018-05-03 - Granted: 2020-09-08 - Earliest claimed: 2016-10-31 - Applicants: Innoven Energy LLC - Inventors: Robert O. Hunter, Jr. - Web page: https://patentgrep.com/patent/US10770860B2 ## CPC - H01S 3/305: {in a gas} - G21B 1/03: with inertial plasma confinement - H01S 3/0057: {Temporal shaping, e.g. pulse compression, frequency chirping (soliton generation and propagation G02F1/3513, H01S3/063 and H01S3/108)} - H01S 3/2391: {emitting at different wavelengths} - H01S 3/005: {Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping (shaping laser beam for working metal or other materials B23K26/06; optical elements, systems or apparatus in general G02B)} - H01S 3/0071: {Beam steering, e.g. whereby a mirror outside the cavity is present to change the beam direction} - H01S 3/2316: {Cascaded amplifiers} - H01S 2301/02: ASE (amplified spontaneous emission), noise; Reduction thereof - Y02E 30/10: Nuclear fusion reactors - 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 - G21B: FUSION REACTORS (uncontrolled reactors G21J) - Y02E: REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION ## Abstract An apparatus and process for pumping laser media by an optical pump over a 10 nanosecond period and thereafter time compressing the energy into an extraction pulse and focusing onto a target with a final 1 nanosecond irradiation time are disclosed. The exciting pump pulses are directed into a lookthrough compression arrangement wherein they energize a stimulated scattering process in low pressure (about 1 atmosphere) gaseous media and impinge in an off axis backward geometry. The extraction pulse is formed and directed towards the target with the appropriate information (color, phase, desired irradiance pattern) impressed on it at relatively low energy by manipulation with conventional, solid material optical elements. Once formed, it traverses the gaseous media, is amplified, and proceeds through a vacuum transition section and onto the target. After the injection of the extraction pulse into the lookthrough compression arrangement, it is amplified in the gaseous media by conversion of the pump energy, coupled through the scattering process. The media and the pump and extraction pulses are tailored to give high energy gain to the input optical pulse, high output fluence, good beam quality (high fidelity amplification to the desired temporal and spatial shape), and time compression. Once injected into the entrance to the first section by the material elements, the extraction pulse proceeds through shutter areas that separate different media regions and encounter no further solid material optical elements as it travels to the target. The focus on the target is impressed before amplification and time compression from the pump pulses and results in a very high brightness irradiance of the target. The desired spatial pattern of irradiance on the target is likewise formed with material elements and then imaged onto the target. Fluences some 2-3 orders of magnitude above those available under the conventional art may be thus obtained with an output brightness better by some six orders of magnitude. ## Claims ### Claim 1 A system for amplifying an output fluence in a stimulated scattering system, the system comprising: an input extraction pulse module comprising: an optical pulse; and one or more optical elements positioned to direct said optical pulse toward a fast compression stage; said fast compression stage comprising: one or more sections that each correspond to a distinct medium and positioned within a propagation media without intervening permanent optical materials between sections; wherein said propagation media is a gaseous media within a total pressure range of 0.5-2 atmospheres; one or more pump pulses, each impinging upon one of the one or more sections, wherein said optical pulse is shorter than the pump pulse and is amplified as it interacts with the pump pulse; a transition section having a transition medium to receive the optical pulse; and a target chamber to hold a target within a vacuum, wherein said target interacts with and is energized by said optical beam. ### Claim 2 (depends on 1) The system of claim 1, further comprising: two or more sections each with corresponding distinct mediums; two or more pump pulses, wherein a pump pulse corresponds with each of the sections; and wherein an index matching medium lies within each of the sections. ### Claim 3 (depends on 1) The system of claim 1, further comprising: two or more sections each with corresponding distinct mediums; two or more pump pulses, wherein a pump pulse corresponds with each of the sections; and wherein an index and density matching medium lies within each of the sections. ### Claim 4 (depends on 1) The system of claim 1, further comprising: two or more sections each with corresponding mediums; two or more pump pulses, wherein a pump pulse corresponds with each of the sections; and wherein a different medium lies within each of the sections. ### Claim 5 (depends on 1) The system of claim 1, further comprising: two or more contiguous sections each with corresponding mediums; and two or more pump pulses, wherein a pump pulse corresponds with each of the sections. ### Claim 6 (depends on 1) The system of claim 1, wherein the medium is selected from one of the following: noble gases, N2 isotopes, H2 isotopes and mixtures thereof. ### Claim 7 (depends on 1) The system of claim 1, wherein the one or more optical elements further comprises a polarization modulating element to control the angle of polarization of the optical beam relative to the pump beam and/or a polarization modulating element to control the angle of polarization of the pump beam. ### Claim 8 (depends on 1) The system of claim 1, wherein the one or more optical elements further comprises an active adaptive optical element or a passive scattering element to compensate for phase distortions. ### Claim 9 (depends on 1) The system of claim 1, wherein the one or more optical elements comprises active optics. ### Claim 10 (depends on 1) The system of claim 1, wherein the one or more pump pulses emits a single pump color. ### Claim 11 (depends on 1) The system of claim 1, wherein the one or more pump pulses emits a multi-color pump color. ### Claim 12 (depends on 1) The system of claim 1, wherein the one or more pump pulses each emit a unique color. ### Claim 13 (depends on 1) The system of claim 1, wherein the one or more pump pulses emits a modulated pump beam. ### Claim 14 (depends on 1) The system of claim 1, wherein the one section is segmented into four or more different segments arranged in parallel and wherein said one or more pump pulses further comprises: four or more different pump pulses arranged to impinge upon each of the four segments. ### Claim 15 (depends on 1) The system of claim 1, wherein the input extraction pulse is shaped as a pattern. ### Claim 16 (depends on 1) The system of claim 1, wherein said transition section is a vacuum transition section without a permanent material surface. ### Claim 17 (depends on 1) The system of claim 1, wherein the input extraction pulse module and the pump pulse are positioned on an off-axis propagation path. ### Claim 18 (depends on 1) The system of claim 1, wherein the input extraction pulse module and the pump pulse are positioned on a common propagation path. ### Claim 19 A method for amplifying an output fluence in a stimulated scattering process, the method comprising: directing an optical pulse through one or more optical elements towards a fast compression stage, wherein said fast compression stage comprises one or more sections that correspond to a distinct medium and positioned within a propagation media that is a gaseous media within a total pressure range of 0.5-2 atmospheres; directing one or more pump pulses towards a fast compression stage and impinging upon one of the one or more sections without impinging upon intervening permanent optical materials between sections, wherein said optical pulse is shorter than the pump pulse; amplifying the optical pulse as it interacts with the one or more sections and the one or more pump pulses; directing the optical pulse through a transition section having a transition medium; and energizing a target held within a vacuum of a target chamber by interacting with the optical beam. ### Claim 20 (depends on 19) The method of claim 19, further comprising: directing two or more pump pulses towards two or more sections each with corresponding distinct mediums, wherein the sections comprise an index matching medium. ### Claim 21 (depends on 19) The method of claim 19, further comprising: directing two or more pump pulses towards two or more sections each with corresponding distinct mediums, wherein the sections comprise an index and density matching medium. ### Claim 22 (depends on 19) The method of claim 19, further comprising: directing two or more pump pulses towards two or more sections each with corresponding distinct mediums, wherein the sections comprise a different index medium. ### Claim 23 (depends on 19) The method of claim 19, further comprising: directing two or more pump pulses towards two or more contiguous sections each with corresponding distinct mediums. ### Claim 24 (depends on 19) The method of claim 19, further comprising selecting the medium from one of the following: noble gases, N2 isotopes, H2 isotopes and mixtures thereof. ### Claim 25 (depends on 19) The method of claim 19, further comprising controlling the angle of polarization of the optical beam relative to the pump beam and/or an angle of polarization of the pump beam. ### Claim 26 (depends on 19) The method of claim 19, further comprising compensating for phase distortions with an active adaptive optic system of a passive scattering element. ### Claim 27 (depends on 19) The method of claim 19, further comprising directing the optical pulse through active optics. ### Claim 28 (depends on 19) The method of claim 19, further comprising emitting a single pump color from each of the one or more pump pulses. ### Claim 29 (depends on 19) The method of claim 19, further comprising emitting a multi-color pump color from each of the one or more pump pulses. ### Claim 30 (depends on 19) The method of claim 19, further comprising emitting a unique pump color from each of the one or more pump pulses. ### Claim 31 (depends on 19) The method of claim 19, further comprising emitting modulated pump pulses from each of the one or more pump pulses. ### Claim 32 (depends on 19) The method of claim 19, wherein the one section is segmented into four different segments and arranged in parallel and further comprising emitting four different pump pulses upon each of the four segments. ### Claim 33 (depends on 19) The method of claim 19, further comprising emitting a patterned shaped input extraction pulse. ### Claim 34 (depends on 1) The system of claim 1, wherein said transition section is a vacuum transition section without a permanent material surface. ### Claim 35 (depends on 19) The method of claim 19, further comprising emitting the input extraction pulse and the pump pulse on an off-axis propagation path. ### Claim 36 (depends on 19) The method of claim 19, further comprising emitting the input extraction pulse and the pump pulse on a common propagation path. ### Claim 37 A system for amplifying an output fluence in a stimulated scattering system, the system comprising: a lookthrough compression arrangement configured to convert an entrance pulse having an entrance fluence εENT to an exit pulse having an exit fluence εEXIT; wherein the ratio of the exit fluence εEXIT to the entrance fluence εEXIT is greater than 103; wherein the efficiency η of conversion of the entrance pulse to the exit pulse is greater than 0.8; and wherein the lookthrough compression arrangement has a small signal gain exponent G less than 30. ### Claim 38 (depends on 37) The system of claim 37, further comprising a parameter for time compression. ### Claim 39 (depends on 37) The system of claim 37, wherein the conversion of the entrance pulse to the exit pulse is effecting by Raman scattering. ### Claim 40 (depends on 37) The system of claim 37, wherein the conversion of the entrance pulse to the exit pulse is effecting by Brillouin scattering. ### Claim 41 A method for amplifying an output fluence in a stimulated scattering system, the method comprising: converting an entrance pulse having an entrance fluence εENT to an exit pulse having an exit fluence εEXIT; wherein the ratio of the exit fluence εEXIT to the entrance fluence εENT is greater than 103; wherein the efficiency η of conversion of the entrance pulse to the exit pulse is greater than 0.8; and wherein a small signal gain exponent G less than 30. ### Claim 42 (depends on 41) The method of claim 41, further comprising adjusting for time compression. ### Claim 43 (depends on 41) The method of claim 41, wherein the conversion of the entrance pulse to the exit pulse is effecting by Raman scattering. ### Claim 44 (depends on 41) The method of claim 41, wherein the conversion of the entrance pulse to the exit pulse is effecting by Brillouin scattering.