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128 results about "Laser resonance" patented technology

2-micrometer high-pulse energy thulium-doped optical fiber laser of hybrid pump

The invention discloses a 2-micrometer high-pulse energy thulium-doped optical fiber laser of a hybrid pump. The 2-micrometer high-pulse energy thulium-doped optical fiber laser comprises a first fiber grating, a first fiber beam combiner, a second fiber beam combiner, a gain fiber and a second fiber grating, which are connected in sequence, wherein a first pumping source is connected with a second input end of the first fiber beam combiner through a first optical isolator, a second pumping source is connected with a second input end of the second fiber beam combiner through a second optical isolator, the first fiber gating and the second fiber gating form a laser resonance cavity, the first pumping source is a continuous laser diode, the second pumping source is a pulsed laser, and the gain fiber is a thulium-doped fiber. The 2-micrometer high-pulse energy thulium-doped optical fiber laser is reduced in the threshold valve energy of a pumping pulsed light in a gain switch technology, is capable of obtaining pulse with higher energy compared with other laser pulse producing technologies such as regulating Q and mode locking, has the characteristics of full-fiber connection, simple structure and the like, and brings convenience for application and popularization.
Owner:SHANGHAI JIAO TONG UNIV

LD pumping cogain double cavity very-large frequency difference double frequency Nd:YAG laser

InactiveCN1905294ASolve the problem of relatively small frequency differenceOptical resonator shape and constructionActive medium materialFiberPrism
The invention discloses an LD pumped co-gain double-cavity very large frequency difference double-frequency Nd:YAG laser, comprising: LD, LD controller, LD tail fiber, collecting optical system and laser resonance cavities, where the left end face of the Nd:YAG crystal and a first output coupling mirror compose a straight line cavity, KTP frequency doubling crystal and polarizing light splitting prism are arranged in order behind the Nd:YAG crystal in the straight line, a second output coupling mirror is arranged in the direction vertical to the axis of the straight line cavity and in the position corresponding to the polarizing light splitting prism, the left end surface of the Nd:YAG crystal and the second output coupling mirror compose a right angle cavity, the two resonance cavities contain the same Nd:YAG crystal and birefracting filter plate composed of polarizing light splitting prism and KTP frequency doubling crystal, making them both operate in single longitudinal mode; the straight line cavity and the right angle cavity can contain two KTP frequency doubling crystals which compose two birefracting filter plates with the polarizing light splitting prism, thus making the two resonance cavities both operate in single longitudinal mode. And two single-frequency green lights outputted by the straight line cavity and the right angle cavity are merged into orthotropic linear polarizing double frequency 532 green light whose maximum frequency difference can reach 360GHz.
Owner:XIAN UNIV OF TECH

Dual-wavelength Q-switched pulse fiber laser

The invention provides a dual-wavelength Q-switched pulse fiber laser comprising a first laser pump source, a second laser pump source, a light beam combination device, a diachronic mirror, a coupling lens, a dual-cladding Er <3+>-doped ZBLAN fiber, a first collimating lens, a focusing lens, an equivalent saturable absorber, a second collimating lens, and a high reflector. The light beam combination device, the diachronic mirror, the coupling lens, the dual-cladding Er <3+>-doped ZBLAN fiber, the first collimating lens, the focusing lens, the equivalent saturable absorber, the second collimating lens, and the high reflector are connected in sequence. The first laser pump source and the second laser pump source are connected with the light beam combination device. The reflection wavelength of the high reflector is 3 to 5 microns. The high reflector and the front end surface of the dual-cladding Er <3+>-doped ZBLAN fiber form a laser resonance cavity; and in the dual-cladding Er <3+>-doped ZBLAN fiber, the energy level transition of the Er <3+> ion corresponds to transition radiation of the wavelength of 3.2 to 3.9 microns, thereby realizing output of high-power pulse laser with the wavelength larger than 3 microns. On the basis of the way, a problem that the traditional fiber laser uses a single wavelength pump source and thus laser with the wavelength larger than 3 microns can not be generated easily can be solved.
Owner:UNIV OF ELECTRONICS SCI & TECH OF CHINA

Laser resonance Raman method for extra-high-voltage corona discharge early diagnosis

The invention discloses a laser resonance Raman method for extra-high-voltage corona discharge early diagnosis. A diagnosis system adopted in the method is composed of a remote laser resonance Raman testing system (1) and a rotary lifting adjusting support (19). The remote laser resonance Raman testing system is composed of a main control analysis subsystem (10), a visible light imaging system (9), an ultraviolet source subsystem (12), a cassette telescope (21), an ultraviolet spectrograph (4) and an optical accessory. Corona discharge early diagnosis can be achieved by carrying out laser resonance Raman spectrum detection on extremely tiny amounts of ozone, nitrogen oxide and nitric oxide gas molecules produced in the early-stage corona discharge chemical effect. According to the laser resonance Raman method for extra-high-voltage corona discharge early diagnosis, remote visible spectrum detection operation is achieved through the visible light imaging and laser resonance Raman spectrum detection optical path sharing and automatic focusing technology, ozone molecule molecular resonance Raman spectrum detection with extremely high sensitivity is achieved, and nitric oxide and nitrogen dioxide Raman spectra are effectively detected.
Owner:STATE GRID CORP OF CHINA +1

Optical resonant cavity mode and loss measurement device and method based on optical cavity ring-down method

The invention belongs to the technical field of measurement and particularly relates to an optical resonant cavity mode and loss measurement device based on an optical cavity ring-down method. The measurement device comprises a laser, an acousto-optic switch, a first spherical reflector, a plane reflector, a second spherical reflector, a polarizer, a resonant cavity fixing platform, a spectroscope, a high-resolution CCD telescoping collimation system, an image acquisition card, a high-speed detector, a high-speed data acquisition card, a master control computer, an acousto-optic switch driver and a manual piezoelectric ceramic driver. According to the device, by monitoring the specified intrinsic mode in the optical resonant cavity and the light intensity attenuation characteristic time in the cavity, the intrinsic mode and the loss of the optical resonant cavity can be accurately measured at the same time, the measurement accuracy is high, and operation is convenient to perform. Through the device, the loss in the installing and adjusting process of an annular laser resonance cavity can also be well completed, and the device has important significance in improving the performance of laser gyroscopes and the percent of pass in production.
Owner:NAT UNIV OF DEFENSE TECH

Intermediate infrared femtosecond mode-locked laser

InactiveCN102570270AStable continuous femtosecond laser pulse outputAvoid expensive pricesLaser detailsSemiconductor lasersMode-lockingChemical vapor deposition
The invention relates to an intermediate infrared femtosecond mode-locked laser which comprises a collimating mirror, a focusing mirror, an input spherical surface mirror, a laser medium and a spherical surface high-reflection mirror which are sequentially arranged along a direction of a pumping light beam outputted by a laser diode, wherein lasers in a five-mirror laser resonance cavity formed by the input spherical surface mirror, the spherical surface high-reflection mirror, the spherical surface high-reflection focusing mirror, an output coupling mirror and a graphene mode-locking element is reflected onto the high-reflection focusing mirror through the input spherical surface mirror, is focused on the graphene mode-locking element, returns back along the original path by sequentially passing through the spherical surface high-reflection focusing mirror, the input spherical surface mirror, a laser crystal and the spherical surface high-reflection mirror, is deflected and reflected to a dispersion compensation prism pair by the spherical surface high-reflection mirror, and is output from the output coupling mirror through a slit. According to the intermediate infrared femtosecond mode-locked laser, graphene growing by adopting a CVD (Chemical Vapor Deposition) method is transferred to a laser wavelength high-reflection mirror, and is protected by using inert gas, and thus stable mode-locked laser pulse output is realized in an intermediate infrared band. The intermediate infrared femtosecond mode-locked laser has the advantages of being simple in regulation, low in manufacture cost, and easy to realize single layer (little non-saturated loss).
Owner:SHANGHAI JIAO TONG UNIV

Double-resonance vertical-cavity surface-emitting laser structure for generating terahertz wave and microwave

The invention discloses a double-resonance vertical-cavity surface-emitting laser structure for generating terahertz wave and microwave and relates to the field of optoelectronic devices. The structure comprises a lower metal electrode, an n-type substrate, a lower distributed feedback Bragg reflector, an n-type phase matching layer, a gain area, a p-type phase matching layer, an upper distributed feedback Bragg reflector, a passivation layer and an upper metal electrode which are sequentially arranged from bottom to top; the structure is characterized in that the length d of a laser resonance cavity is formed by the optical thickness of the n-type phase matching layer, the optical thickness of the gain area, the optical thickness of the p-type phase matching layer, and energy transmission depth of laser in the lower distributed feedback Bragg reflector and the upper distributed feedback Bragg reflector; the length d of the resonance cavity is required to meet the equation as follows: d=c/2omega; if the omega is greater than 0.1THz and smaller than 10THz, the terahertz wave is generated; if the omega is greater than 300MHz and smaller than 300GHz, the microwave is generated. Compared with the existing terahertz light source, the double-resonance vertical-cavity surface-emitting laser structure for generating the terahertz wave and the microwave has the advantages of integration, miniaturization, working at room temperature and easiness in formation of two-dimensional arrays.
Owner:BEIJING UNIV OF TECH

Cooling method for gain medium in solid laser and low interior heat solid laser

InactiveCN101505030AReduce the temperatureExcellent refrigeration efficiencyActive medium materialSequence signalFluorescence
The invention discloses a method for cooling a gain medium in a solid laser and a solid laser having lower internal heat. A laser pump light source and a refrigerating pump light source which can adjust light intensity, pulse width and repetition rate respectively are arranged. The gain medium corresponding to the laser pump light source and a refrigerating medium corresponding to the refrigerating pump light source are the same block of crystal mixed with rare earth ions. Two physical processes of laser refrigeration and laser oscillation are controlled to alternatively or synchronously operate by a sequence signal circuit and a gain switch so as to approximately counteract the refrigerating capacity of superradiance on the media and the heat generated by the laser oscillation, to make the laser in a laser resonance cavity transmitted along the crystal 'apyrexia' direction, and to reduce the thermal lens effect caused by a residual temperature gradient in the crystal . The method converts waste heat in the gain medium into an anti-Stocks scattering photon which has fast radiation and small residual temperature gradient. A main pump light beam and an auxiliary pump light beam (pulse) are used for inducing the crystal to emit the superradiance. The refrigerating efficiency of the superradiance is better than that of fluorescence in the prior laser refrigerators.
Owner:谭吉春

Inner-cavity single-resonance optical parametric oscillator of fiber laser pump

The invention discloses an inner-cavity single-resonance optical parametric oscillator of a fiber laser pump. A pump source emits single-mode gain optical fiber to absorb pump light in a band, and after being focused by a coupling lens and passing through a dichroic mirror, the pump light enters the single-mode gain optical fiber. After the single-mode gain optical fiber absorbs the pump light, population inversion is formed, and laser oscillation is formed in a laser resonance cavity which is composed of a laser fully-reflecting mirror, the dichroic mirror and an SRO output mirror. A non-linear crystal is arranged in the resonance cavity of an optical fiber laser device, and nonlinear gain is provided. Signal light oscillation is formed in an SRO resonance cavity which is composed of the SRO output mirror and the SRO fully-reflecting mirror and is output by the SRO output mirror. According to the inner-cavity single-resonance optical parametric oscillator of the fiber laser pump, the single-mode optical fiber laser device is used as the pump light of an inner-cavity SRO, the pump source of the SRO is forced to operate in a fundamental transverse mode through the structural features of the single-mode gain optical fiber, and therefore the problems that since the heat effect in a traditional inner-cavity SRO causes degradation of the quality of a pump light beam and the degradation is difficult to compensate, the conversion efficiency of the SRO and the quality of the output light beam are influenced are solved.
Owner:TIANJIN UNIV

Far-end pumping erbium-doped optical fiber amplifier

The invention provides a far-end pumping erbium-doped optical fiber amplifier. The amplifier comprises a pump light source and an erbium-doped optical fiber amplifier body which are connected through a pump transmission optical fiber, wherein the pump light source is a high-power laser with a wavelength being 1390nm, one end of the pump transmission optical fiber is connected with the pump light source through a high-reflectivity fiber bragg grating with a wavelength being 1480nm, and the other end of the pump transmission optical fiber is connected with the erbium-doped optical fiber amplifier body through a low-reflectivity fiber bragg grating with a wavelength being 1480nm. A laser resonance cavity is formed by the fiber bragg grating pair, and high-efficiency frequency shift from laser with the wavelength being 1390nm to laser with the wavelength being 1480nm is realized. The far-end pumping erbium-doped optical fiber amplifier overcomes the defect of low Raman frequency shifting efficiency in 1390nm laser transmission, sufficient 1480nm pump laser can be obtained after longer optical fiber transmission, the power of 1480nm pump laser obtained through the optical fiber amplifier is increased by more than 3dB than that of the 1480nm pump laser obtained in a traditional manner; with the adoption of the far-end pumping erbium-doped optical fiber amplifier, a larger signal gain can be obtained under the condition of the same distance, or a further pump transmission distance can be realized under the condition of the same signal gain.
Owner:NO 34 RES INST OF CHINA ELECTRONICS TECH GRP +2

Radial polarization beam laser

The invention discloses a radial polarization beam laser. The radial polarization beam laser comprises an output cavity mirror (101), a pumping source (102), a gain medium (103) and a symmetrical polarization selecting assembly (104). The output cavity mirror is a mirror plane reflecting one part of light emitted by the laser and transmitting the other part of the light emitted by the laser, and the output cavity mirror outputs one part of the laser generated by the laser in a coupling mode and reflects the other part of the light to the laser to maintain laser resonance. The pumping source provides energy for the laser gain medium, and the laser gain medium is excited to jump to a higher energy level. The radial polarization beam laser structurally comprises the pumping source, the gain medium and the symmetrical polarization selecting assembly, wherein the pumping source and the gain medium provide energy for the laser resonance, the symmetrical polarization selecting assembly is composed of a barrel-shaped polarization mold, a reflecting mirror and a conical reflector. Polarization of a beam in a cylindrical symmetry mode can be achieved through the symmetrical polarization selecting assembly, and thus beam output of the radial polarization laser is achieved. The radial polarization beam laser is clear in structure, high in stability and capable of achieving high-power output.
Owner:UNIV OF SCI & TECH OF CHINA
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