Patent classifications
H01S3/00
SYSTEMS, METHODS, AND DEVICES FOR SPECTROCHROME LASER OUTPUT
In one aspect, an example handheld device for providing a spectrochrome output includes (a) an enclosed chamber containing one or more substances; (b) a light source; (c) an electromagnetic coil; (d) one or more magnets; and (e) a housing, wherein the housing is configured to: (i) secure the enclosed chamber; (ii) secure the light source such that an output of the light source is substantially aligned to pass through the enclosed chamber in one or more directions; and (iii) secure the electromagnetic coil around the enclosed chamber such that an electromagnetic field is created in a substantially same direction of the output of the light source through the enclosed chamber.
Compact laser source with frequency modulators generating multiple lines
A compact laser source and a single sideband modulator used therein is disclosed. The compact laser source includes a seed laser and one or more channels, with each channel generating one or more output laser beams having corresponding different wavelengths. The compact laser source can be formed in whole or in part on a single optical motherboard to thereby minimize space and power requirements. By employing the disclosed single sideband modulator, harmonics in the generated output laser beams can be minimized. The compact laser source finds application in an atom interferometer (AI) system, which may be used to measure gravity, acceleration, or rotation of the AI system.
GAS PURGE SYSTEMS FOR A LASER SOURCE
A laser source includes a laser chamber configured to generate a first laser beam. The laser source further includes an optical system coupled to the laser chamber and configured to receive the first laser beam and output an output laser beam. The laser source also includes a gas purge system. According to some aspects, the gas purge system is configured to supply a nitrogen gas into the optical system at a pressure less than atmospheric pressure. According to some aspects, the gas purge system is configured to supply a helium gas into the optical system.
OPTICAL COUPLER AND LIGHT OUTPUT DEVICE
An optical coupler includes: input-type optical fibers; an output-type optical fiber; and radiant light processing units. The input-type optical fibers are bundled at leading end side to form a fiber bundle portion, and leading end portion of the fiber bundle portion is connected to the output-type optical fiber. In at least either the input-type optical fibers or the output-type optical fiber, a tapered portion is formed in which cross-sectional area is tapered to become narrower in light traveling direction indicating direction from the input-type optical fibers toward the output-type optical fiber. The number of the tapered portion is equal to or greater than two. Each radiant light processing unit is disposed to mutually overlap with one of the tapered portions or away from one of the tapered portions in the light traveling direction, and is disposed on outer periphery of the input-type optical fibers or the output-type optical fiber.
BEAM SHUTTER, LASER ARRANGEMENT AND ASSOCIATED OPERATING METHOD
A beam shutter for a laser beam includes a main body, a magnetic field sensor, a holding arm having release and closure positions, a reflecting optical unit and a permanent magnet producing a magnetic field having reduced strength upon heating above a limit temperature. The magnet is closer to the sensor in the closure than the release position. A controller deactivates a laser light source at reduced magnetic field measured by the sensor, when passing a predefined strength and/or gradient magnetic field threshold. A laser arrangement includes a laser light source and beam shutter. The laser beam strikes the reflecting unit in the closure position. An operating method includes bringing the holding arm into closure position, operating the laser light source, measuring magnetic field strength and/or gradient using the sensor, deactivating the laser light source when the magnetic field drops and passes the predefined magnetic field threshold.
METHOD AND SYSTEM FOR THE TEMPORAL AND SPECTRAL CHARACTERIZATION OF THE AMPLITUDE AND PHASE OF ULTRASHORT LASER PULSES
The method comprises A method includes steps for creating at least two replicas of an input pulse to be characterised, varying the relative amplitude of the two replicas within a range, creating a nonlinear signal at each case of said amplitude variation, measuring the spectra of the nonlinear signals and recovering the spectral amplitude and phase of the input pulse with a proper algorithm. The system includes a replicator for creating at least two replicas of the input pulse and varying their relative amplitude within a range of relative amplitudes, a nonlinear medium, which obtains a nonlinear signal for each relative amplitude, and an analyzer, associated to the nonlinear signal for measuring and characterising spectrally each nonlinear signal.
Fractional handpiece with a passively Q-switched laser assembly
A fractional handpiece and systems thereof for skin treatment include a passively Q-switched laser assembly operatively connected to a pump laser source to receive a pump laser beam having a first wavelength and a beam splitting assembly operable to split a solid beam emitted by the passively Q-switched laser assembly and form an array of micro-beams across a segment of skin. The passively Q-switched laser assembly generates a high power sub-nanosecond pulsed laser beam having a second wavelength.
OPTICAL SYSTEM FOR INCREASING THE CONTRAST OF PULSED LASER RADIATION, LASER SYSTEM AND METHOD FOR INCREASING THE CONTRAST OF PULSED LASER RADIATION
An optical system for increasing contrast of pulsed laser radiation includes a first polarization setting optical unit for setting an elliptical polarization state of the pulsed laser radiation, and a multipass cell having at least two opposing mirrors. The pulsed laser radiation passes the multipass cell with formation of a plurality of intermediate focus zones. The multipass cell is filled with a gas having an optical nonlinearity that causes an intensity-dependent rotation of an alignment of the elliptical polarization state of the pulsed laser radiation, such that the multipass cell outputs beam portions having differently aligned elliptical polarization states on account of the intensity-dependent rotation. The optical system further includes an optical beam splitting system for splitting the beam portions having differently aligned elliptical polarization states.
COHERENT PHOTONICS IMAGER WITH OPTICAL CARRIER SUPPRESSION AND PHASE DETECTION CAPABILITY
A coherent imaging system including a transmitter and a receiver. The transmitter includes a coherent source and a power splitter for splitting the electromagnetic radiation into a reference and a signal beam. The receiver includes an image forming device and an array of pixels. Each of the pixels include means for collecting at least a portion of the signal beam imaged on the pixel by an image forming device, as a collected signal; means for splitting the collected signal into a plurality of collected signals each having different phase shifts; means for mixing each of the collected signals with the reference beam so as to form a plurality of mixed signals; and means for detecting the mixed signals and outputting a plurality of output electrical signals in response to the mixed signals.
TWO-PHOTON MICROSCOPY AND PULSE WIDTH CORRECTION METHOD USING THE SAME
Provided is a two-photon spectroscopy including a light source configured to generate first laser light having a pulse, a pulse width correction device configured to receive the first laser light to output a second laser light, an optical system through which the second laser light passes, a first two-photon sensor configured to measure a first pulse width of the first laser light generated from the light source, and a second two-photon sensor configured to measure a second pulse width of the second laser light passing through the optical system, wherein the pulse width correction device corrects a difference between the first pulse width and the second pulse width.