Wu et al., 2011 - Google Patents
Achieving single-longitudinal-mode output about Tm: YAG laser at room temperatureWu et al., 2011
- Document ID
- 12261173777105664738
- Author
- Wu C
- Ju Y
- Zhou R
- Duan X
- Wang Y
- Publication year
- Publication venue
- Laser Physics
External Links
Snippet
We report on the single-longitudinal-mode Tm: YAG laser with a volume Bragg grating pumped by laser diode at room temperature. The maximum SLM power of 142 mW was achieved under incident pump power of 3.22 W. The central wavelength was 2012.6 nm …
- 238000001228 spectrum 0 abstract description 14
Classifications
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/09—Processes or apparatus for excitation, e.g. pumping
- H01S3/091—Processes or apparatus for excitation, e.g. pumping using optical pumping
- H01S3/094—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
- H01S3/0941—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light of a laser diode
- H01S3/09415—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light of a laser diode the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/05—Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/0602—Crystal lasers or glass lasers
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/05—Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
- H01S3/106—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling a device placed within the cavity
- H01S3/1063—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling a device placed within the cavity using a solid state device provided with at least one potential jump barrier
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/05—Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/07—Construction or shape of active medium consisting of a plurality of parts, e.g. segments
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/05—Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/0619—Coatings, e.g. AR, HR, passivation layer
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/05—Construction or shape of optical resonators; Accomodation of active medium therein; Shape of active medium
- H01S3/08—Construction or shape of optical resonators or components thereof
- H01S3/08018—Mode suppression
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
- H01S3/11—Pulse generation, e.g. Q-switching, mode locking
-
- G—PHYSICS
- G02—OPTICS
- G02F—DEVICES OR ARRANGEMENTS, THE OPTICAL OPERATION OF WHICH IS MODIFIED BY CHANGING THE OPTICAL PROPERTIES OF THE MEDIUM OF THE DEVICES OR ARRANGEMENTS FOR THE CONTROL OF THE INTENSITY, COLOUR, PHASE, POLARISATION OR DIRECTION OF LIGHT, e.g. SWITCHING, GATING, MODULATING OR DEMODULATING; TECHNIQUES OR PROCEDURES FOR THE OPERATION THEREOF; FREQUENCY-CHANGING; NON-LINEAR OPTICS; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating, or modulating; Non-linear optics
- G02F1/35—Non-linear optics
- G02F1/353—Frequency conversion, i.e. wherein a light beam with frequency components different from those of the incident light beams is generated
- G02F1/3544—Particular phase matching techniques
- G02F2001/3548—Quasi-phase-matching [QPM], e.g. using a periodic domain inverted structure
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S5/00—Semiconductor lasers
- H01S5/10—Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
- H01S5/14—External cavity lasers
- H01S5/146—External cavity lasers using a fiber as external cavity
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/30—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves using scattering effects, e.g. stimulated Brillouin or Raman effects
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01S—DEVICES USING STIMULATED EMISSION
- H01S3/00—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves
- H01S3/14—Lasers, i.e. devices for generation, amplification, modulation, demodulation, or frequency-changing, using stimulated emission, of infra-red, visible, or ultra-violet waves characterised by the material used as the active medium
- H01S3/16—Solid materials
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN101859974A (en) | Narrow linewidth thulium-doped fiber laser | |
Zhang et al. | Single longitudinal mode and continuously tunable frequency Tm, Ho: YLF laser with two solid etalons | |
Wu et al. | Achieving single-longitudinal-mode output about Tm: YAG laser at room temperature | |
Wu et al. | Injection-seeded Tm: YAG laser at room temperature | |
JP2017526975A (en) | Method and apparatus for generating cavity enhanced broadband intrapulse differential frequency | |
Li et al. | A linearly-polarized rubidium vapor laser pumped by a tunable laser diode array with an external cavity of a temperature-controlled volume Bragg grating | |
Dai et al. | Experimental study into single-longitudinal-mode Tm, Ho: YVO4 lasers | |
Deng et al. | A diode-pumped 1617 nm single longitudinal mode Er: YAG laser with intra-cavity etalons | |
Yang et al. | Q-switched Ho: YAlO 3 laser pumped by Tm: YLF laser at room temperature | |
Zhou et al. | A single-longitudinal-mode CW 0.25 mm Tm, Ho: GdVO 4 microchip laser | |
Fritsche et al. | Increased efficiency of Er: YAG lasers at 1645 nm using narrow bandwidth diode lasers and dual-wavelength resonant pumping | |
Chen et al. | Room temperature diode-pumped Tm, Ho: YAP laser with double etalons | |
Li et al. | Efficient continuous wave and Q-switched operation of a dual-end-pumped c-cut Tm: YAP laser | |
Yao et al. | Room temperature diode-pumped tunable single-frequency Tm: YAG ceramic laser | |
Vogelmann et al. | Transverse-pumping approach for a powerful single-mode Ti: sapphire laser for near infrared lidar applications | |
Ju et al. | Single-longitudinal-mode lasing of Tm, Ho: GdVO 4 using a filter of Fabry-Perot etalon and volume Bragg grating | |
Wang et al. | Stable and tunable single frequency Nd: GSAG laser around 943 nm | |
Wang et al. | A diode-pumped tunable single frequency Tm: YAG laser at room temperature using two etalons | |
Duan et al. | Efficient Tm: YLF laser with a volume Bragg grating recycle pumped by laser diode | |
You-Lun et al. | A single-longitudinal-mode dual-wavelength cw Tm, Ho: GdVO4 microchip laser | |
Zhu et al. | Effect of resonator length on ZnGeP 2 doubly resonant optical parametric oscillator pumped by a Tm, Ho: GdVO 4 laser | |
Li et al. | Tunable CW Tm, Ho: YLF laser at 2 microns | |
Lv et al. | High energy widely tunable narrow-linewidth Ti: sapphire laser using combined-cavity configuration | |
Yang et al. | A narrow linewidth continuous wave Ho: YAP laser with a volume Bragg grating | |
Du et al. | Absorption measurement of a 50-mm-long periodically poled lithium niobate optical parametric oscillator pumped at 1064 nm by a Nd: YAG laser |