| Class / Patent application number | Description | Number of patent applications / Date published |
|---|
| 359305000 | Acousto-optic | 47 |
| 20080204857 | Bragg mirror optimized for shear waves - In an embodiment, set forth by way of example and not limitation, a Bragg mirror includes a first bi-layer of a first thickness and a second bi-layer of a second thickness which is different from the first thickness. In this exemplary embodiment, the first bi-layer consists essentially of a first high impedance layer and a first low impedance layer, and the second bi-layer of a second thickness which is different from the first thickness, the second bi-layer consisting essentially of a second high impedance layer and a second low impedance layer. Preferably, the first bi-layer is configured to substantially reflect a first wavelength and the second bi-layer is configured to substantially reflect a second wavelength different from the first wavelength. | 08-28-2008 |
| 20080231940 | Laser drawing method and apparatus - A method of laser drawing includes steps of causing laser light from a light source to be incident to an acousto-optical diffraction element, and deflecting the light incident to the element by changing a frequency of a high frequency signal to be inputted to the element to diffract the light, thereby changing a diffraction angle of the diffracted light, and condensing the diffracted light emerging from the element on an object to be processed as an optical spot, thereby scanning the object with the optical spot. A diffracted light intensity control table for controlling a light intensity of the diffracted light so as to be constant independent of the diffraction angle of the diffracted light is prepared in advance, and in the deflecting step, the light intensity of the diffracted light is controlled based on the diffracted light intensity control table. | 09-25-2008 |
| 20080247030 | LOW COST SYSTEM AND METHOD THAT IMPLEMENTS ACOUSTO-OPTIC (AO) RF SIGNAL EXCITATION - An acousto-optic modulator includes an acousto-optic bulk medium. A transducer is attached to the acousto-optic bulk medium and formed as a linear array of electrodes. A transducer driver is connected to each electrode and comprises a plurality of amplifiers connected to the electrodes such that each electrode is driven by a respective amplifier as a means to provide a low cost alternative to the use of higher power hybrid amplifiers in conventional AO device applications. | 10-09-2008 |
| 20080247031 | ACOUSTO-OPTIC DEVICES HAVING EXTENDED TEMPERATURE RELIABILITY - An acousto-optic modulator includes an acousto-optic bulk medium and transducer attached to the acousto-optic bulk medium. The transducer includes an electrode circuit and plurality of piezoelectric platelet segments attached to the bulk medium and supporting the electrode circuit. The piezoelectric platelet segments are configured for reducing shear stress and susceptibility to fracture due to temperature extremes. | 10-09-2008 |
| 20080310009 | Device for trapping or stretching microscopic substance and method thereof - The present invention provides a device for trapping or stretching a microscopic substance comprising (a) a light source for irradiating laser beam; (b) an acousto-optic modulator (AOM) for regulating the direction of said laser beam irradiating from said light source; (c) a beam-expander for expanding and collimating the light beam emitting from said AOM; (d) an object lens for focusing the laser beam passing through said beam-expander; and (e) an incoherent light source for imaging said microscopic substance. | 12-18-2008 |
| 20090073543 | HIGH FREQUENCY ACOUSTO-OPTIC FREQUENCY SHIFTER HAVING WIDE ACCEPTANCE ANGLE - An acousto-optic (AO) frequency shifter includes an anisotropic crystal having an optical axis and an input face, and an acoustic transducer having electrodes affixed to the face for receiving an electrical signal and projecting an acoustic wave into the crystal. The anisotropic crystal is cut relative to the face so that the transducer is at an acoustic angle (θ | 03-19-2009 |
| 20090073544 | Device for the optical splitting and modulation of electromagnetic radiation - A device for the optical splitting and modulation of monochromatic coherent electromagnetic radiation, in particular light beams and/or laser beams, contains a beam source, an acousto-optical element disposed downstream of the latter and serving for splitting the beam generated by means of the beam source into a number of partial beams, a modulator and also a signal generator for applying to the acusto-optical element an electrical signal for splitting the beam. The device is intended to be developed to the effect that in conjunction with a simple and functionally reliable construction and independently of the number of beams emitted by the beam source, the intensity of the individual split partial beams can be kept constant. For this purpose, it is proposed that the modulator is embodied as an acusto-optical modulator disposed downstream of the acusto-optical element, and that the acusto-optical modulator is fed the split partial beams for modulation, and the acusto-optical modulator can be driven with additional high-frequency electrical signals. | 03-19-2009 |
| 20090219607 | METHOD AND APPARATUS FOR ENHANCED RESOLUTION MICROSCOPY OF LIVING BIOLOGICAL NANOSTRUCTURES - The present invention is a method and apparatus that utilizes an inertia-free diffraction mechanism to control both phase and rotation of the standing wave pattern that results in super-resolution at unparalleled imaging speeds. In some embodiments of the present inventions, AODs are utilized to control period, phase, and rotation of the SW pattern in contrast to the commonly used mechano-optical principles. This allows 2D (and 3D) super-resolution imagining at high stability and speed not limited by mechanical constraints. The present invention can be utilized, for example, for real time observations of dynamic processes in living cells. | 09-03-2009 |
| 20090290209 | LASER MICROSCOPE - It is an object to perform high-precision observation by compensating group-velocity-delay dispersion and angular dispersion with a simple structure. The invention provides a laser microscope | 11-26-2009 |
| 20100123948 | Bragg Mirror and Method for Making Same - In an embodiment, set forth by way of example and not limitation, a Bragg mirror includes a first bi-layer of a first thickness and a second bi-layer of a second thickness which is different from the first thickness. In this exemplary embodiment, the first bi-layer consists essentially of a first high impedance layer and a first low impedance layer, and the second bi-layer of a second thickness which is different from the first thickness, the second bi-layer consisting essentially of a second high impedance layer and a second low impedance layer. Preferably, the first bi-layer is configured to substantially reflect a first wavelength and the second bi-layer is configured to substantially reflect a second wavelength different from the first wavelength. | 05-20-2010 |
| 20100177375 | BEAM COMBINER AND A LIGHT SOURCE WITH SUCH A BEAM COMBINER - A beam combiner for combining at least two light beams ( | 07-15-2010 |
| 20100182676 | VARIABLE- BEAMWIDTH ANGLE ENCODING LASER SCANNER - A laser apparatus includes a laser capable of generating a laser signal; means for conditioning the laser signal; and means for varying the beamwidth of the laser signal as it is scanned into the field of view. | 07-22-2010 |
| 20100232011 | APPARATUS AND METHOD FOR OPERATING AN ACOUSTO-OPTICAL COMPONENT - An apparatus for controlling an acousto-optical component influencing at least one of illumination light and detection light in a microscope is described. The apparatus comprises a radio-frequency generator for supplying the acousto-optical component with a radio frequency. The radio-frequency generator is configured to compensate deviations in the characteristics of the light due to temperature fluctuations in the acousto-optical component by adapting the radio frequency. The apparatus can be operated by generating a control signal for controlling the radio frequency of the radio-frequency generator; measuring the temperature of the acousto-optical component; adapting the control signal depending on the measured temperature; and sending the adapted control signal into the radio-frequency generator for compensating deviations in the characteristics of the light due to temperature fluctuations and can be used in optical coherence tomography, particularly white light interferometry, optical tweezers in lithography, and distance measurement. | 09-16-2010 |
| 20120218623 | ACOUSTO-OPTIC DEFLECTORS OVER ONE OCTAVE - The technology described applies an extended frequency range of over one octave to drive an acousto-optic deflector, thereby defying a design rule of thumb that limited bandwidth to just under one octave. A combination of extended frequency range and well-timed beam blanking reduces the proportion of a so-called chirp signal that is consumed by beam blanking. This increases the working, effective portion of the sweep signal. | 08-30-2012 |
| 20120250140 | ACOUSTO-OPTIC SCANNER - An acousto-optic laser beam scanner of improved scanning angle scope is provided by introducing a controllable compound acoustic waveform into a light transmissive body wherein at least binary and binary diffraction grating patterns of both positive and negative sense can be introduced into the body, the period of the waveform determining the refraction angle magnitude and the order of the pulses determining the refraction angle direction. | 10-04-2012 |
| 20120281271 | Method and Device Scanning a Two-Dimensional Brush Through an Acousto-Optic Deflector (AOD) Having an Extended Field in a Scanning Direction - The technology disclosed relates to improved acousto-optic deflectors (AODs). In particular, it relates to compensation for subtle effects not previously addressed by AOD designers. A shifting center of gravity is described and addressed using advanced power equalisation strategies. Denser writing brushes are provided by using a two-dimensional array of beams with corrections for factors such as angle of incidence at the AOD interface. The compensation and dense brush features can be used separately or in combination. | 11-08-2012 |
| 20120281272 | TUNABLE ACOUSTIC GRADIENT INDEX OF REFRACTION LENS AND SYSTEM - A tunable acoustic gradient index of refraction (TAG) lens and system are provided that permit, in one aspect, dynamic selection of the lens output, including dynamic focusing and imaging. The system may include a TAG lens and at least one of a source and a detector of electromagnetic radiation. A controller may be provided in electrical communication with the lens and at least one of the source and detector and may be configured to provide a driving signal to control the index of refraction and to provide a synchronizing signal to time at least one of the source and the detector relative to the driving signal. Thus, the controller is able to specify that the source irradiates the lens (or detector detects the lens output) when a desired refractive index distribution is present within the lens, e.g. when a desired lens output is present. | 11-08-2012 |
| 20130010349 | SYSTEMS AND METHODS FOR PROVIDING TEMPERATURE STABILITY OF ACOUSTO-OPTIC BEAM DEFLECTORS AND ACOUSTO-OPTIC MODULATORS DURING USE - The invention provides a method of laser processing that includes the steps of: generating a sequence of RF pulses corresponding to a sequence of laser pulses having a laser pulse repetition rate, the RF pulses including transmitting RF pulses at transmitting RF frequencies and non-transmitting RF pulses at non-transmitting RF frequencies for causing the sequence of laser pulses to be deflected in respective transmitting and non-transmitting directions, each RF pulse comprising an RF frequency, an RF amplitude and a duration; controlling each RF pulse such that the sequence of RF pulses provides a modulated RF drive signal that is modulated to provide a balanced thermal loading on the acousto-optic deflector; applying the modulated RF drive signal to the acousto-optic deflector; and deflecting at least one laser pulse with the acousto-optic deflector using the modulated RF drive signal to irradiate a selected target position with a predetermined pulse energy. | 01-10-2013 |
| 20130148188 | METHODS AND APPARATUS TO CONTROL ACOUSTO-OPTIC DEFLECTORS - Methods and apparatus for optimising, improving or maximising the efficiency of an acousto-optic lens (AOL) system are disclosed. Data relating to efficiency is used to select drive frequencies of the acousto-optic devices (AODs) forming the AOL, thereby both increasing the usable field of view and reducing a prior art patternation problem. Preferably according to the invention, drive frequencies are selected that maximise efficiency of transmission through the AOL. When scanning, the centre of each scan is optimised to be of maximum efficiency. | 06-13-2013 |
| 20130301114 | ACOUSTO-OPTIC IMAGING DEVICE - An acousto-optic imaging device disclosed in the present application includes: an acoustic wave source; an acoustic lens system for converting a scattered wave produced by irradiation of an object with an acoustic wave emitted from the acoustic wave source into a predetermined converged state; an acousto-optic medium section which is arranged such that a scattered wave transmitted through the acoustic lens system is incident on the acousto-optic medium section; a light source for emitting a light beam which is formed by a plurality of superposed monochromatic light rays traveling in different directions; an image formation lens system for condensing diffracted light of a plurality of the monochromatic plane wave light rays produced at the acousto-optic medium section; and an image receiving section for detecting light condensed by the image formation lens system to output an electric signal. | 11-14-2013 |
| 20130321898 | SYSTEM AND METHOD FOR DIRECT IMAGING - A direct imaging system comprises an illumination unit comprising a plurality of light sources, the plurality of light sources configured to emit a plurality of beams, an optical system for forming the plurality of beams to be aligned in position or angle, an acoustic optical modulator positioned to receive the plurality of beams aligned in one of position or angle and to consecutively diffract different portions of the plurality of beams as an acoustic wave propagates in an acoustic direction, and a scanning element adapted to scan an exposure plane with the plurality of beams modulated by the acoustic optical modulator at a scanning velocity, wherein the scanning velocity is selected to incoherently unite the different portions of the plurality of beams into a single exposure spot. | 12-05-2013 |
| 20140036346 | Tunable Acoustic Gradient Index of Refraction Lens and System - A tunable acoustic gradient index of refraction (TAG) lens and system are provided that permit, in one aspect, dynamic selection of the lens output, including dynamic focusing and imaging. The system may include a TAG lens and at least one of a source and a detector of electromagnetic radiation. A controller may be provided in electrical communication with the lens and at least one of the source and detector and may be configured to provide a driving signal to control the index of refraction and to provide a synchronizing signal to time at least one of the source and the detector relative to the driving signal. Thus, the controller is able to specify that the source irradiates the lens (or detector detects the lens output) when a desired refractive index distribution is present within the lens, e.g. when a desired lens output is present | 02-06-2014 |
| 20140078578 | FOCUSING ELECTROMAGNETIC RADIATION WITHIN A TURBID MEDIUM USING ULTRASONIC MODULATION - The present disclosure provides various systems and methods for focusing electromagnetic radiation (EMR) within a diffusion medium, such as a turbid medium. A diffusion medium is irradiated with EMR. The EMR may be modulated by an acoustical wave focused on a focus volume within the diffusion medium. The EMR may be modulated by a beat frequency or other function of multiple focused acoustical waves. The EMR may be modulated at a harmonic of a fundamental frequency of one or more acoustical waves. A filter may filter the emerging EMR to remove all but specifically modulated EMR scattered from the focus volume. The modulated EMR may be focused and/or used for various purposes, including imaging. In some embodiments, the modulated EMR may be reflected and/or amplified by a phase conjugating mirror. Furthermore, in some embodiments, acoustical phase conjugation may be used to focus an acoustical wave on a focus volume. | 03-20-2014 |
| 20140168752 | TUNABLE ACOUSTIC GRADIENT INDEX OF REFRACTION LENS AND SYSTEM - A tunable acoustic gradient index of refraction (TAG) lens and system are provided that permit, in one aspect, dynamic selection of the lens output, including dynamic focusing and imaging. The system may include a TAG lens and at least one of a source and a detector of electromagnetic radiation. A controller may be provided in electrical communication with the lens and at least one of the source and detector and may be configured to provide a driving signal to control the index of refraction and to provide a synchronizing signal to time at least one of the source and the detector relative to the driving signal. Thus, the controller is able to specify that the source irradiates the lens (or detector detects the lens output) when a desired refractive index distribution is present within the lens, e.g. when a desired lens output is present. | 06-19-2014 |
| 20140168753 | APPARATUS AND METHOD FOR OPERATING AN ACOUSTO-OPTICAL COMPONENT - An apparatus for controlling an acousto-optical component influencing at least one of illumination light and detection light in a microscope is described. The apparatus comprises a radio-frequency generator for supplying the acousto-optical component with a radio frequency. The radio-frequency generator is configured to compensate deviations in the characteristics of the light due to temperature fluctuations in the acousto-optical component by adapting the radio frequency. The apparatus can be operated by generating a control signal for controlling the radio frequency of the radio-frequency generator; measuring the temperature of the acousto-optical component; adapting the control signal depending on the measured temperature; and sending the adapted control signal into the radio-frequency generator for compensating deviations in the characteristics of the light due to temperature fluctuations and can be used in optical coherence tomography, particularly white light interferometry, optical tweezers in lithography, and distance measurement. | 06-19-2014 |
| 20140204454 | CONFIGURATION OF ACOUSTO-OPTIC DEFLECTORS FOR LASER BEAM SCANNING - A first acousto-optic deflector receives a laser beam. The first acousto-optic deflector diffracts the received laser beam along a first axis. A second acousto-optic deflector receives the diffracted laser beam. The second acousto-optic deflector diffracts the received diffracted laser beam along a second axis. | 07-24-2014 |
| 20150301428 | TUNABLE ACOUSTIC GRADIENT INDEX OF REFRACTION LENS AND SYSTEM - A tunable acoustic gradient index of refraction (TAG) lens and system are provided that permit, in one aspect, dynamic selection of the lens output, including dynamic focusing and imaging. The system may include a TAG lens and at least one of a source and a detector of electromagnetic radiation. A controller may be provided in electrical communication with the lens and at least one of the source and detector and may be configured to provide a driving signal to control the index of refraction and to provide a synchronizing signal to time at least one of the source and the detector relative to the driving signal. Thus, the controller is able to specify that the source irradiates the lens (or detector detects the lens output) when a desired refractive index distribution is present within the lens, e.g. when a desired lens output is present. | 10-22-2015 |
| 20150338718 | ACOUSTO-OPTIC DEFLECTOR WITH MULTIPLE TRANSDUCERS FOR OPTICAL BEAM STEERING - An acousto-optic deflector with multiple acoustic transducers is described that is suitable for use in substrate processing. In one example a method includes transmitting an optic beam through an acousto-optic deflector, applying an acoustic signal with a phase delay across multiple transducers of the acousto-optic deflector to deflect the beam along a first axis by the acousto-optic deflector, and directing the deflected beam onto a workpiece. | 11-26-2015 |
| 20160139488 | LASER OSCILLATION MECHANISM - A laser oscillation mechanism includes a pulse laser oscillator which oscillates a pulse laser beam, and an optical path changing unit which changes an angle of an optical path of the pulse laser beam oscillated by the pulse laser oscillator. The optical path changing unit is configured from an acousto-optic deflection unit including an acousto-optic device for changing the optical path of the pulse laser beam oscillated by the pulse laser oscillator within an effective region, and a volume Bragg grating which excludes, from among pulse laser beams obtained by changing the angle of the optical path of the pulse laser beam by passing through the acousto-optic device, a pulse laser beam desired to be eliminated by refraction from within the effective region. | 05-19-2016 |
| 359307000 | Utilizing optical feedback | 4 |
| 20090244691 | APPARATUS FOR PROVIDING MULTIPLE TIME-DIVISION MULTIPLEXED INDEPENDENTLY CONTROLLABLE PULSED BEAMS FROM A SINGLE, PULSED LASER OUTPUT-BEAM - An output beam from a laser is directed into an acousto-optic cell. The laser beam includes repeated sequences of two or more pulses. The acousto-optic cell is sequentially driven by RF voltages at two or more frequencies. A portion of the laser output beam is diffracted by the acousto-optic cell at two or more different angles to the laser output beam. This provides two or more secondary beams. One of the secondary beams includes only the first pulses of the sequences; the other includes only the second pulses of the sequences. The duration of the pulses in the laser beam is controlled to control time-averaged power in the secondary beams. | 10-01-2009 |
| 20100177376 | TUNABLE ACOUSTIC GRADIENT INDEX OF REFRACTION LENS AND SYSTEM - A tunable acoustic gradient index of refraction (TAG) lens and system are provided that permit, in one aspect, dynamic selection of the lens output, including dynamic focusing and imaging. The system may include a TAG lens and at least one of a source and a detector of electromagnetic radiation. A controller may be provided in electrical communication with the lens and at least one of the source and detector and may be configured to provide a driving signal to control the index of refraction and to provide a synchronizing signal to time at least one of the source and the detector relative to the driving signal. Thus, the controller is able to specify that the source irradiates the lens (or detector detects the lens output) when a desired refractive index distribution is present within the lens, e.g. when a desired lens output is present. | 07-15-2010 |
| 20140098410 | SYSTEMS AND METHODS FOR PROVIDING TEMPERATURE STABILITY OF ACOUSTO-OPTIC BEAM DEFLECTORS AND ACOUSTO-OPTIC MODULATORS DURING USE - The invention provides a method of laser processing with a thermally stabilized acousto-optic beam deflector. The method includes the steps of: generating a sequence of RF pulses corresponding to a sequence of laser pulses having a laser pulse repetition rate, the RF pulses including transmitting RF pulses at transmitting RF frequencies and non-transmitting RF pulses at non-transmitting RF frequencies for causing the sequence of laser pulses to be deflected in respective transmitting and non-transmitting directions, each RF pulse comprising an RF frequency, an RF amplitude and a duration; controlling each RF pulse such that the sequence of RF pulses provides a modulated RF drive signal that is modulated to provide a balanced thermal loading on the acousto-optic deflector; applying the modulated RF drive signal to the acousto-optic deflector; and deflecting at least one laser pulse with the acousto-optic deflector using the modulated RF drive signal to irradiate a selected target position with a predetermined pulse energy. | 04-10-2014 |
| 20140211299 | TUNABLE ACOUSTIC GRADIENT INDEX OF REFRACTION LENS AND SYSTEM - A tunable acoustic gradient index of refraction (TAG) lens and system are provided that permit, in one aspect, dynamic selection of the lens output, including dynamic focusing and imaging. The system may include a TAG lens and at least one of a source and a detector of electromagnetic radiation. A controller may be provided in electrical communication with the lens and at least one of the source and detector and may be configured to provide a driving signal to control the index of refraction and to provide a synchronizing signal to time at least one of the source and the detector relative to the driving signal. Thus, the controller is able to specify that the source irradiates the lens (or detector detects the lens output) when a desired refractive index distribution is present within the lens, e.g. when a desired lens output is present. | 07-31-2014 |
| 359308000 | Filter | 4 |
| 20090080061 | METHOD AND DEVICE FOR HIGH RESOLUTION ACOUSTO-OPTIC PROGRAMMABLE FILTERING IN THE INFRARED REGION - The subject matter of the invention is a method of high-resolution acousto-optic programmable filtering in the infrared region of an incident optical wave. To that end it proposes the use of a birefringent acousto-optic crystal whereof the propagation speed of acoustic waves is slow, such as compounds of mercury, which acousto-optic crystal comprises, on one of its faces, a piezoelectric transducer designed to generate a transverse acoustic wave with wave vector whereof the energy propagates according to the same axis but in the opposite direction to the energy of the incident optical wave, knowing that the optical wave resulting from the acousto-optic interaction between the incident optical wave and the acoustic wave with wave vector is diffracted perpendicularly or almost perpendicularly to the direction of the incident optical wave. | 03-26-2009 |
| 20090284826 | Acousto-Optic Devices - An acousto-optic module is provided, including a number of partially coupled optical resonators distributed within a dielectric medium and at least one acoustic transducer mounted on a surface of the dielectric medium for injecting an acoustic wave into the optical resonators so as to diffract light passing therethrough by means of Bragg diffraction. This acousto-optic module has been applied in particular to an improved tuneable optical filter in which an acoustic shear wave is generated and which travels through the acousto-optic module in a direction substantially parallel with a polarised light signal passing therethrough. The acousto-optic module is also applied to an improved optical frequency shifter. | 11-19-2009 |
| 20100214648 | OPTICAL WAVELENGTH TUNABLE FILTER - An acousto-optical tunable filter is disclosed. The filter includes a medium having one or more indices of refractions alterable by the application of acoustic waves to the medium. The filter also includes an acoustic transducer coupled to the medium to generate the acoustic waves Altering the frequency of the acoustic wave selects among the different wavelengths in the incident light ray. The device also includes an optical mirror for reflecting a wave diffracted by the medium back to the medium so that it can again be diffracted. The first diffracted wave has its frequency shifted in one direction by the frequency of the acoustic wave while the second diffracted wave has its frequency shifted in the opposite direction, thereby compensating for the first shift. The result is an output ray with little or no frequency shift. | 08-26-2010 |
| 20120069427 | METHOD AND DEVICE FOR ACOUSTO-OPTIC FILTERING WITH LONG OPTICAL AND ACOUSTIC INTERACTION LENGTH - A method and a device for acousto-optic filtering with large optic and acoustic interaction length; includes the use of a birefringent acousto-optic crystal whereof the sound wave propagation speed is as low as possible, this acousto-optical crystal including, on one of its faces, a piezoelectric transducer intended to generate a transverse sound wave whereof the energy propagates collinearly to the energy of an incident light wave, all along the path of the incident light wave, in the aforementioned birefringent acousto-optic crystal, knowing that the transverse sound wave and the incident light wave travel a path including multiple reflections on one or the other of the reflective faces of the birefringent acousto-optic crystal perpendicular to the axes of symmetry shared by the acoustic slownesses curve and the curves of the ordinary and extraordinary optical indices of the acousto-optic crystal. | 03-22-2012 |
| 359309000 | Acting on polychromatic light | 1 |
| 20150029578 | Compensator System and Method for Compensating Angular Dispersion - The invention relates to a compensator system adapted to compensate for the angular dispersion of electromagnetic beams deflected by at least one acousto-optic deflector of an optical system, wherein the angular dispersion of each deflected beam is dependent on the deflection angle obtained by the deflecting acoustic frequency of the acousto-optic deflector, characterised in that the compensator system comprises: —a first lens group for spatially separating the deflected beams of different deflection angle and angular dispersion by focusing the beams substantially into the focal plane, —a compensator element having a first surface and a second surface, and being arranged such that the first surface of the compensator element lies substantially in the focal plane of the first lens group, and the first and second surfaces of the compensator element have nominal radiuses R | 01-29-2015 |
| 359310000 | Plural cell array | 7 |
| 20100328759 | IMAGING APPARATUS AND METHODS - Methods, systems and apparatus for manipulating electromagnetic radiation such as laser beams. A method and apparatus for correcting magnification chromatic aberration utilises one or more dispersive lenses such that long wavelength components are magnified less than short wavelength components. A telecentric relay is preferred to achieve this aim. Further, the use of polarisers to block the undesired zeroth order components of diffraction emanating from acousto-optic deflectors (AODs) is disclosed. Furthermore, specific designs of AOD including narrow transducer AODs which produce a diverging acoustic wave and AODs having two transducers and a selection switch are disclosed. Further, the invention provides methods, systems and apparatus for allowing the wavelength of radiation to be changed, for providing a user selectable degree of compensation, for providing a scanning and/or a pointing system and for providing a compact system that does not require telecentric relays between adjacent acousto-optic deflectors. | 12-30-2010 |
| 20130057946 | IMAGING APPARATUS AND METHODS - Methods, systems and apparatus for manipulating electromagnetic radiation such as laser beams. A method and apparatus for correcting magnification chromatic aberration utilises one or more dispersive lenses such that long wavelength components are magnified less than short wavelength components. A telecentric relay is preferred to achieve this aim. Further, the use of polarisers to block the undesired zeroth order components of diffraction emanating from acousto-optic deflectors (AODs) is disclosed. Furthermore, specific designs of AOD including narrow transducer AODs which produce a diverging acoustic wave and AODs having two transducers and a selection switch are disclosed. Further, the invention provides methods, systems and apparatus for allowing the wavelength of radiation to be changed, for providing a user selectable degree of compensation, for providing a scanning and/or a pointing system and for providing a compact system that does not require telecentric relays between adjacent acousto-optic deflectors. | 03-07-2013 |
| 20140029081 | METHODS AND APPARATUS TO CONTROL ACOUSTO-OPTIC DEFLECTORS - The invention is directed to an acousto-optic lens (AOL) and corresponding method. The AOL of the invention comprises a first and second acousto-optic deflector, each being arranged to support a respective acoustic wave. The AOL includes a driver for synthesizing first and second drive signals for the respective first and second acousto-optic deflectors. The driver is arranged to synthesize the drive signals so as to be phase-modulated by functions that can be expressed as a Taylor series having one or more coefficients greater than second order. The functions are preferably non-sinusoidal and have sufficient magnitude at the higher orders to effect one or more of fixed aberration correction, dynamic aberration correction and Z-scanning. | 01-30-2014 |
| 20140153081 | IMAGING APPARATUS AND METHODS - Methods, systems and apparatus for manipulating electromagnetic radiation such as laser beams. A method and apparatus for correcting magnification chromatic aberration utilises one or more dispersive lenses such that long wavelength components are magnified less than short wavelength components. A telecentric relay is preferred to achieve this aim. Further, the use of polarisers to block the undesired zeroth order components of diffraction emanating from acousto-optic deflectors (AODs) is disclosed. Furthermore, specific designs of AOD including narrow transducer AODs which produce a diverging acoustic wave and AODs having two transducers and a selection switch are disclosed. Further, the invention provides methods, systems and apparatus for allowing the wavelength of radiation to be changed, for providing a user selectable degree of compensation, for providing a scanning and/or a pointing system and for providing a compact system that does not require telecentric relays between adjacent acousto-optic deflectors. | 06-05-2014 |
| 20140313569 | Illumination Device and Method for Controlling the Illumination Device - An illumination device for illuminating a target to be combated includes a laser light source for emitting light along a beam path, a first modulator in the beam path and configured to manipulate a direction of the beam path in a first plane, a phase plate in the beam path having a variety of different optical thicknesses, and a control device connected to the light source and the first modulator and is configured to activate the first modulator using different frequencies, so that the beam path is deflected over a control period of time up to a first angle. | 10-23-2014 |
| 20150085346 | Method for Scanning Along a Continuous Scanning Trajectory With a Scanner System - The invention relates to a method for scanning along a continuous scanning trajectory with a scanner system ( | 03-26-2015 |
| 20160187761 | IMAGING APPARATUS AND METHODS - Methods, systems and apparatus for manipulating electromagnetic radiation such as laser beams include a first acousto-optic deflector optimised for efficient transmission at the input beam angle and a second acousto-optic deflector of lower peak efficiency than the first acousto-optic deflector but which accepts beams from a wider range of angles at better transmission efficiency than the first acousto-optic deflector by passing a beam optimised for efficient transmission through the first acousto-optic deflector at the input beam angle, deflecting the beam using the first acousto-optic deflector, passing the deflected beam through the second acousto-optic deflector, which has a lower peak efficiency than the first acousto-optic deflector and accepts beams from a wider range of angles at better transmission efficiency than the first acousto-optic deflector, and deflecting the beam using the second acousto-optic deflector. | 06-30-2016 |
| 359311000 | Plural transducers on single cell | 1 |
| 20130063805 | TUNABLE ACOUSTIC GRADIENT INDEX OF REFRACTION LENS AND SYSTEM - A tunable acoustic gradient index of refraction (TAG) lens and system are provided that permit, in one aspect, dynamic selection of the lens output, including dynamic focusing and imaging. The system may include a TAG lens and at least one of a source and a detector of electromagnetic radiation. A controller may be provided in electrical communication with the lens and at least one of the source and detector and may be configured to provide a driving signal to control the index of refraction and to provide a synchronizing signal to time at least one of the source and the detector relative to the driving signal. Thus, the controller is able to specify that the source irradiates the lens (or detector detects the lens output) when a desired refractive index distribution is present within the lens, e.g. when a desired lens output is present. | 03-14-2013 |
| 359313000 | Particular cell shape | 1 |
| 20130070329 | ACOUSTO-OPTIC MODULATOR - According to one embodiment, an acousto-optic modulator includes an acousto-optic medium and a piezoelectric transducer. The acousto-optic medium has a configuration of a hexahedron. The acousto-optic medium has surfaces D, E, F, G and H. The piezoelectric transducer is provided on a surface C of the acousto-optic medium. The surface D opposes the surface C and has respective four sides shared by the surfaces E, F, G and H. Four angles defined between the surface D and the surfaces E, F, G and H each is other than 90°. At least one of eight angles defined between each pair of the surfaces C, E, F, G and H is other than 90°. The each pair has one shared side. | 03-21-2013 |
