# US 11,307,086 B2 · Measuring device and methods for characterization of a radiation field > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 11,307,086 B2 - Document ID: US11307086B2 - Status: Granted - Kind: B2 - Application number: 17/159,205 - Filed: 2021-01-27 - Published: 2021-06-10 - Granted: 2022-04-19 - Earliest claimed: 2021-01-27 - Assignees: LaVision BioTec GmbH - Applicants: LaVision BioTec GmbH - Inventors: Frank Killich; Uwe Engeland - Web page: https://patentgrep.com/patent/US11307086B2 ## CPC - G01J 1/4257: {applied to monitoring the characteristics of a beam, e.g. laser beam, headlamp beam (monitoring arrangements for lasers in general H01S3/0014)} - G01J 1/0266: {Field-of-view determination; Aiming or pointing of a photometer; Adjusting alignment; Encoding angular position; Size of the measurement area; Position tracking; Photodetection involving different fields of view for a single detector} - G01J 1/0411: {using focussing or collimating elements, i.e. lenses or mirrors; Aberration correction} - G01J 1/0414: {using plane or convex mirrors, parallel phase plates, or plane beam-splitters} - G01J 1/4228: {arrangements with two or more detectors, e.g. for sensitivity compensation} - G02B 5/001: {Axicons, waxicons, reflaxicons} - G01J 1/0425: {using optical fibers} - G01J: MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY (light sources F21, H01J, H01K, H05B; investigating properties of materials by optical means G01N) - G02B: OPTICAL ELEMENTS, SYSTEMS OR APPARATUS ## Abstract A radiation field measuring device for the characterization of a radiation comprises a detector device and a reconstruction device. The detector device may have at least one detector camera, which contains at least one detector array arranged for the image recording of scattered radiation in a multiplicity of lateral directions that deviate from the longitudinal direction. The reconstruction device may be configured for the tomographic reconstruction of a field density of the scattered radiation in the radiation field. ## Claims ### Claim 1 A radiation field measuring device (100), which is configured for characterizing a radiation field (1) that passes through a medium (2) in a longitudinal direction (z), comprising: a detector device (10) having at least one detector camera (11), which contains at least one detector array (12) arranged for the image recording of scattered radiation (3) that is generated in the medium by the radiation field (1) and is directed in at least 3 lateral directions, that deviate from the longitudinal direction (z), and a reconstruction device (20), which is configured for characterizing the radiation field (1) on the basis of image signals of the detector device (10) by means of a tomographic reconstruction of a field density of the scattered radiation (3) in the radiation field (1), characterized in that the detector device (10) comprises a plurality of detector cameras (11), each having at least one detector array (12) in which an associated detector camera is provided for each lateral direction in which a scattered radiation image is to be recorded or the detector device (10) comprises a single detector camera (11), which contains a plurality of detector arrays (12) that are each arranged for the image recording of scattered radiation (3) in one of the lateral directions, the detection device (10) is configured for a spectrally selective image recording of the scattered radiation (3), and the reconstruction device (20) is configured for the statistical or algebraic tomographic reconstruction of the field density of the scattered radiation (3) in the radiation field (1). ### Claim 2 (depends on 1) The radiation field measuring device according to claim 1, in which the reconstruction device (20) is configured for statistical tomographic reconstruction of the field density of the scattered radiation (3) based on an objective function to be minimized, wherein the objective function contains a tomographic data mismatch term which accounts for the noise characteristics of the measurement data, and the objective function contains at least an Lp-norm term with (0≤p<2) and a Bayesian regularization term. ### Claim 3 (depends on 1) The radiation field measuring device according to claim 1, wherein the reconstruction device (20) is configured for the tomographic reconstruction of a layer section of the field density of the scattered radiation (3), which can be converted into a two-dimensional intensity distribution of the radiation field (1). ### Claim 4 (depends on 1) The radiation field measuring device according to claim 1, wherein the reconstruction device (20) is configured for the tomographic reconstruction of the field density of the scattered radiation (3) in a three-dimensional volume section, which comprises at least two juxtaposed layer sections. ### Claim 5 (depends on 1) The radiation field measuring device according to claim 1, wherein a deflector device (30) is provided, which is arranged for deflecting the scattered radiation (3) along the multiplicity of lateral directions onto the at least one detector camera (11), and wherein the deflector device (30) comprises at least one catoptric element (31, 32, 33) or at least one dioptric element (35) and the at least one catoptric element comprises a plurality of reflector sections (31, 33), which are each arranged for deflecting the scattered radiation (3) along one of the lateral directions towards one of the detector arrays (12). ### Claim 6 (depends on 5) The radiation field measuring device according to claim 5, wherein the detector device (10) comprises a single detector camera (11), and the at least one catoptric element comprises a collection reflector (32), which is arranged for deflecting the scattered radiation (3) from the reflector sections (31, 33) to the detector camera (11). ### Claim 7 (depends on 1) The radiation field measuring device according to claim 1, comprising a beam rotator (40) having a rotatable prism, in particular a Dove prism (41), and/or mirrors, which is configured for rotating the radiation field (1) about the longitudinal direction (z), wherein the detector device (10) comprises a single detector camera (11), which is arranged for the image recording of scattered radiation (3), and wherein for the image recording of scattered radiation (3) in the multiplicity of lateral directions, the radiation field (1) can be rotated with the beam rotator into different rotational positions relative to the detector camera (11). ### Claim 8 (depends on 1) The radiation field measuring device according to claim 1, further comprising an analyzer device (21), which is configured for determining at least one beam parameter of the radiation field (1) on the basis of the field density of the scattered radiation (3) in which the at least one of the beam parameter comprises pulse energy or pulse energy density of the radiation field (1) in the case of a pulsed radiation field (1), field density of the radiation field (1) in the case of a continuous radiation field (1), geometric properties of the radiation field (1), in particular beam diameter, divergence angle and/or beam shape, properties of the beam waist of the radiation field (1), in particular radius, position along the longitudinal direction (z), and/or shape of the focus in transaxial section, spatial location of the radiation field (1) in the medium (2), coherence properties of the radiation field (1), wave fronts of the radiation field (1), Rayleigh lengths of the radiation field (1), and diffraction indexes, M2 and beam propagation factors k of the radiation field (1). ### Claim 9 (depends on 8) The radiation field measuring device according to claim 8, wherein the analyzer device (21) is configured for calculating a beam propagation, in particular by means of a wave front analysis, and the analyzer device (21) is configured for calculating a focus position of the radiation field (1). ### Claim 10 A method for characterizing a radiation field (1) that passes through a medium (2) in a longitudinal direction (z), using a radiation field measuring device (100), comprising the steps: recording an image by means of a detector device (10), of scattered radiation (3), which is generated in the medium (2) by the radiation field (1) and is directed in at least 3 lateral directions, that deviate from the longitudinal direction (z), and characterizing the radiation field (1) with a reconstruction device (20) using image signals of the detector device (10), wherein the reconstruction device (20) carries out a tomographic reconstruction of a field density of the scattered radiation (3) in the radiation field (1) characterized in that the detector device (10) comprises a plurality of detector cameras (11), each having at least one detector array (12) in which an associated detector camera is provided for each lateral direction in which a scattered radiation image is to be recorded or the detector device (10) comprises a single detector camera (11), which employs a plurality of detector arrays (12) that are each arranged for the image recording of scattered radiation (3) in one of the lateral directions, and wherein the image recording is carried out spectrally selectively, and the reconstruction device (20) carries out a non-analytical, in particular statistical or algebraic, tomographic reconstruction of the field density of the scattered radiation (3). ### Claim 11 (depends on 10) The method according to claim 10, wherein the reconstruction device (20) carries out the tomographic reconstruction of the field density of the scattered radiation (3) by means of an iterative algorithm, wherein the iterative algorithm carries out a statistical tomographic reconstruction, and the statistical tomographic reconstruction is based on a statistical model with an objective functional to be minimized, the tomographic data mismatch term of which accounts for the noise characteristics of the measurement data, and the objective functional contains an Lp-norm term with (0≤p<2) and/or a Bayesian regularization term. ### Claim 12 (depends on 10) The method according to claim 10, wherein the field density of the scattered radiation (3) is reconstructed in the forward and backward projection process of the tomographic reconstruction, with an illumination background of the radiation field (1) taken into account, and wherein deflection of the scattered radiation (3) along the multiplicity of lateral directions with the deflector device (30) onto the at least one detector camera (11), and wherein rotation of the radiation field (1) about the longitudinal direction (z) with the beam rotator, and image recording of the scattered radiation (3) with a single detector camera (11), wherein for the image recording of scattered radiation (3) in the multiplicity of lateral directions, the radiation field (1) is rotated with the beam rotator into different rotational positions relative to the detector camera (11), and wherein the field density of the scattered radiation (3) is reconstructed with particles in the medium taken into account, which particles would lead to artefacts of the reconstructed field density if they were not taken into account. ### Claim 13 (depends on 10) The method according to claim 10, further comprising at least one of the steps tomographic reconstruction of a layer section of the field density of the scattered radiation (3), and conversion of the field density of the scattered radiation (3) into a two-dimensional intensity distribution of the radiation field (1), and tomographic reconstruction of a field density of the scattered radiation (3) in a three-dimensional volume section, which comprises at least two juxtaposed layer sections. ### Claim 14 (depends on 10) The method according to claim 10, further comprising the step of capturing at least one beam parameter, wherein the at least one beam parameter is at least one of pulse energy or pulse energy density of the radiation field (1) in the case of a pulsed radiation field (1), field density of the radiation field (1) in the case of a continuous radiation field (1), geometric properties of the radiation field (1), in particular beam diameter, divergence angle and/or beam shape, properties of the beam waist of the radiation field (1), in particular radius, position along the longitudinal direction (z), and/or shape of the focus in transaxial section, spatial location of the radiation field (1) in the medium (2), coherence properties of the radiation field (1), wave fronts of the radiation field (1), Rayleigh lengths of the radiation field (1), diffraction indexes, M2 and beam propagation factors k of the radiation field (1). ### Claim 15 (depends on 14) The method according to claim 14, where the capturing of the at least one beam parameter comprises at least one of the steps calculation of a beam propagation, in particular by means of wave front analysis, and calculation of focus position of the radiation field (1).