Abstract: A method for making a microchip laser includes preparing a laser-cavity chip assembly comprising a gain media, a first substantially flat surface, and a second substantially flat surface parallel to the first substantially flat surface. The method also includes forming a first reflective film on the first substantially flat surface to form a first cavity mirror, forming a second reflective film on the second substantially flat surface to form a second cavity mirror, and patterning at least one of the first reflective film or the second reflective film by removing at least a portion of the reflective film in the outer portion to form a center reflective portion in the one of the first reflective film or the second reflective film. The first cavity mirror and the second cavity mirror can suppress higher order transverse modes and produce a single TEM00 mode in the lasing light.

Abstract: A method for making a microchip laser includes preparing a laser-cavity chip assembly comprising a gain media, a first substantially flat surface, and a second substantially flat surface parallel to the first substantially flat surface. The method also includes forming a first reflective film on the first substantially flat surface to form a first cavity mirror, forming a second reflective film on the second substantially flat surface to form a second cavity mirror, and patterning at least one of the first reflective film or the second reflective film by removing at least a portion of the reflective film in the outer portion to form a center reflective portion in the one of the first reflective film or the second reflective film. The first cavity mirror and the second cavity mirror can suppress higher order transverse modes and produce a single TEM00 mode in the lasing light.

Abstract: A single longitudinal-mode laser includes a first mirror and a second mirror that define a laser cavity therein that does not include a linear polarizer. A birefringent gain medium can generate a lasing light at a lasing wavelength along a light propagation direction in response to a pump light at a pumping wavelength. The birefringent gain medium has an optical axis substantially perpendicular to the light propagation direction. A first wave plate positioned between the first mirror and the birefringent gain medium is a quarter wave plate at the lasing wavelength and a whole wave plate at the pumping wavelength. A second wave plate is positioned between the birefringent gain medium and the second mirror. The first wave plat and the second wave plate in part produce a single longitudinal mode in the lasing light.

Abstract: A single longitudinal-mode laser includes a first mirror and a second mirror that define a laser cavity therein that does not include a linear polarizer. A birefringent gain medium can generate a lasing light at a lasing wavelength along a light propagation direction in response to a pump light at a pumping wavelength. The birefringent gain medium has an optical axis substantially perpendicular to the light propagation direction. A first wave plate positioned between the first mirror and the birefringent gain medium is a quarter wave plate at the lasing wavelength and a whole wave plate at the pumping wavelength. A second wave plate is positioned between the birefringent gain medium and the second mirror. The first wave plat and the second wave plate in part produce a single longitudinal mode in the lasing light.

Abstract: This invention discloses an apparatus for skin treatments. The apparatus comprising a chamber placed on a skin target which is formed with an aperture on the distal end thereof; means for applying vacuum to said chamber, therefore the skin target is able to be treated upon the applied vacuum; and/or means for supplying negative ion into said chamber; and c) at least one light source with one wavelength or multi-wavelength, wherein the light source is arranged inside the chamber to provide optical energy in the predetermined wavelength(s) through the aperture to the skin target. With the assistance of negative ion as well as vacuum, the skin treatment will be improved because it purifies the air and relieves stress to enhance activation of skin cell, accelerate blood cycle.

Abstract: Method and system for flattening tilt gain with a digital title gain equalizer (“DTGE”) constructed with a linear tilt optical filter (“LTOF”). In a first embodiment, a DTGE flattens tilt gain with a combination of LTOF and a rotative half-wave plate. In a second embodiment, a DTGE flattens tilt gain with a combination of LTOF and variable Faraday rotators.

Abstract: A Micro-Electro-Mechanical System (MEMS) and double-layer nozzle based high efficiency, lightweight, low cost, compact, portable fiber-optic connector cleaning apparatus useful for various fiber optic communications applications such as fiber optic cable plant maintenance. The double-layer nozzle design enables the delivery of compressed, filtered air and solvent to connector surfaces. A built-in MEMS pump sucks the air and solvent back to remove particles and contaminations without leaving residues and without scratching the connector surfaces. An interchangeable external needle allows the cleaner to quickly adapt to all kinds of fiber optic connectors. No disassembly is required. The connector cleaner is therefore both fast and effective at cleaning various male and female fiber optic connectors. The fiber optic connector cleaner with 3–5 cc solvent weighs less than half a pound and can be held and operated by one hand.

Abstract: Method and system for flattening tilt gain with a digital title gain equalizer (“DTGE”) constructed with a linear tilt optical filter (“LTOF”). In a first embodiment, a DTGE flattens tilt gain with a combination of LTOF and a rotative half-wave plate. In a second embodiment, a DTGE flattens tilt gain with a combination of LTOF and variable Faraday rotators.

Abstract: Method and system for flattening tilt gain with a digital title gain equalizer (“DTGE”) constructed with a linear tilt optical filter (“LTOF”). In a first embodiment, a DTGE flattens tilt gain with a combination of LTOF and a rotative half-wave plate. In a second embodiment, a DTGE flattens tilt gain with a combination of LTOF and variable Faraday rotators.

Abstract: A Micro-Electro-Mechanical System (MEMS) and double-layer nozzle based high efficiency, lightweight, low cost, compact, portable fiber-optic connector cleaning apparatus useful for various fiber optic communications applications such as fiber optic cable plant maintenance. The double-layer nozzle design enables the delivery of compressed, filtered air and solvent to connector surfaces. A built-in MEMS pump sucks the air and solvent back to remove particles and contaminations without leaving residues and without scratching the connector surfaces. An interchangeable external needle allows the cleaner to quickly adapt to all kinds of fiber optic connectors. No disassembly is required. The connector cleaner is therefore both fast and effective at cleaning various male and female fiber optic connectors. The fiber optic connector cleaner with 3-5 cc solvent weighs less than half a pound and can be held and operated by one hand.

Abstract: A GTIFR interferometer, for use in an interleaver or in a deinterleaver, wherein the GTIFR interferometer includes a Gires-Toutnois interferometer with a 45 degree Faraday rotator between the mirrors of the Gires-Tournois interferometer and further includes a 22.5 degree Faraday rotator in the light path to the Gires-Tournois interferometer and an interleaver or deinterleaver that contains one GTIFR. A dispersion compensated GTIFR interleaver includes a second Gires-Tournois interferometer for providing chromatic dispersion compensation.

Abstract: A deinterleaver includes three polarization interferometers and a dispersion compensator, the input light beam containing all channels passing through the dispersion compensator and the first polarization interferometer, the light beam being separated by a polarization beam splitter into an even channel beam and an odd channel beam with the even channel beam passing through a second polarization interferometer and the odd channel beam passing through a third polarization interferometer. A dispersion compensated deinterleaver as above in which all three polarization interferometers have pass bands corresponding to all channels and in which there are two output ports. A dispersion compensated deinterleaver in which the first polarization interferometer has pass bands for all channels, the second polarization interferometer has pass bands for even channels, the third polarization interferometer has pass bands for odd channels and in which there are four output ports.

Abstract: An optical de-interleaver for de-interleaving light beams of odd and even channel signals having channel spacing S into light beams of odd channel signals having channel spacing 2S and light beams of even channel signals having channel spacing 2S is provided which has only one polarization interferometer and one optical dispersion compersator. A 50/100 GHz de-interleaver and a 50/200 GHz de-interleaver with high isolation and dispersion compensation are provided by applying this unique arrangement. The optical de-interleaver has a 0.5 dB passband width of about 30 GHz and a −25 dB isolation stopband width of about 30 GHz.

Abstract: A GTIFR interferometer, for use in an interleaver or in a deinterleaver, wherein the GTIFR interferometer includes a Gires-Toutnois interferometer with a 45 degree Faraday rotator between the mirrors of the Gires-Tournois interferometer and further includes a 22.5 degree Faraday rotator in the light path to the Gires-Tournois interferometer and an interleaver or deinterleaver that contains one GTIFR. A dispersion compensated GTIFR interleaver includes a second Gires-Tournois interferometer for providing chromatic dispersion compensation.

Abstract: A GTIFR interferometer, for use in an interleaver or in a deinterleaver, wherein the GTIFR interferometer includes a Gires-Toutnois interferometer with a 45 degree Faraday rotator between the mirrors of the Gires-Tournois interferometer and further includes a 22.5 degree Faraday rotator in the light path to the Gires-Tournois interferometer and an interleaver or deinterleaver that contains one GTIFR. A dispersion compensated GTIFR interleaver includes a second Gires-Tournois interferometer for providing chromatic dispersion compensation.

Abstract: An etalon includes a tuning plate in the air-gap between the etalon mirrors. The method of tuning includes selecting a tuning plate that makes the optical length of the etalon slightly less than required for ITU and then rotating the tuning plate through a small angle until tuning is complete. The tuning plate material is selected to provide dispersion compensation and to compensate for thermal expansion of the mirror spacers.

Abstract: The present invention provides an optical dispersion compensator with relatively small size and low insertion loss comprising a Fabry-Perot etalon and a dual-fiber collimator having a dual-fiber pigtail and a GRIN lens. The dual-fiber pigtail has an input fiber and an output fiber. An optical signal is coupled into the input fiber and then collimated by the GRIN lens into a collimated incident beam that is incident on the Fabry-Perot etalon with an incident angle. The collimated incident beam is reflected back by the Fabry-Perot etalon into a collimated reflected beam that is collected by the GRIN lens and coupled into the output fiber. By adjusting the separation between the input fiber and the output fiber of the dual-fiber pigtail, the collimated incident beam will change its incident angle and reflected angle. By tuning this angle, the group delay pattern of the output optical signal through the output fiber will shift along with wavelength, therefore dispersion compensation can be achieved.

Abstract: An optical de-interleaver for de-interleaving light beams of odd and even channel signals having channel spacing S into light beams of odd channel signals having channel spacing 2S and light beams of even channel signals having channel spacing 2S is provided which has only one polarization interferometer and one optical dispersion compersator. A 50/100 GHz de-interleaver and a 50/200 GHz de-interleaver with high isolation and dispersion compensation are provided by applying this unique arrangement. The optical de-interleaver has a 0.5 dB passband width of about 30 GHz and a −25 dB isolation stopband width of about 30 GHz.

Abstract: An etalon includes a tuning plate in the air-gap between the etalon mirrors. The method of tuning includes selecting a tuning plate that makes the optical length of the etalon slightly less than required for ITU and then rotating the tuning plate through a small angle until tuning is complete. The tuning plate material is selected to provide dispersion compensation and to compensate for thermal expansion of the mirror spacers.

Abstract: A deinterleaver includes three polarization interferometers and a dispersion compensator, the input light beam containing all channels passing through the dispersion compensator and the first polarization interferometer, the light beam being separated by a polarization beam splitter into an even channel beam and an odd channel beam with the even channel beam passing through a second polarization interferometer and the odd channel beam passing through a third polarization interferometer. A dispersion compensated deinterleaver as above in which all three polarization interferometers have pass bands corresponding to all channels and in which there are two output ports. A dispersion compensated deinterleaver in which the first polarization interferometer has pass bands for all channels, the second polarization interferometer has pass bands for even channels, the third polarization interferometer has pass bands for odd channels and in which there are four output ports.