CN211700921U - 324-powered 500nm continuous laser triple frequency laser - Google Patents
324-powered 500nm continuous laser triple frequency laser Download PDFInfo
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- CN211700921U CN211700921U CN202020293263.7U CN202020293263U CN211700921U CN 211700921 U CN211700921 U CN 211700921U CN 202020293263 U CN202020293263 U CN 202020293263U CN 211700921 U CN211700921 U CN 211700921U
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Abstract
A triple frequency laser of 324-plus-500 nm continuous laser comprises a high-power fundamental frequency laser and a triple frequency module, wherein the output wavelength range of the fundamental frequency light is 972-plus-1500 nm, the triple frequency module consists of a single-pass frequency doubling module and a resonance sum frequency module, the high-power fundamental frequency laser generates watt-level double frequency laser (466-plus-750 nm) through the single-pass frequency doubling module, the high-power fundamental frequency laser once passes through a nonlinear crystal in a resonance sum frequency cavity, and the high-power triple frequency laser (324-plus-500 nm) is obtained by summing the frequency of the high-power fundamental frequency laser and a double frequency laser in the nonlinear sum frequency crystal. The resonance and frequency cavity only needs to lock the resonance and frequency cavity to the double frequency laser to obtain the light intensity gain. The utility model discloses can output stable, reliable and high beam quality 324-.
Description
Technical Field
The utility model relates to a 324-doped 500nm continuous laser, in particular to a triple frequency laser of a 324-doped 500nm continuous laser.
Background
The high-power continuous ultraviolet laser is widely applied to the fields of high-resolution laser spectrum analysis, single-photon rydberg state excitation of neutral atoms, quantum physics, optical data storage, optical disk control, photochemical reaction, atmospheric detection, coherent laser detection, biomedicine, advanced manufacturing, semiconductor industry and the like. Ultraviolet laser has the characteristics of short wavelength and high single photon energy, and is commonly used for ultraviolet-induced photochemical reaction and cold treatment. In the field of micromachining, ultraviolet lasers have the following advantages: first, the diffraction limit is small, the beam diffraction limit is an important factor limiting the minimum size to be processed, and the shorter the corresponding wavelength is, the smaller the minimum focal point diameter can be reached; secondly, the high-energy single photon can directly break the chemical bond of the material molecule, namely, the cold treatment process, and compared with the method that the frequency doubling light and the fundamental laser melt the material of the processing part by utilizing the collected heat, the heat influence of the ultraviolet laser is very small; thirdly, most materials can absorb ultraviolet light in nature, and the characteristic of the ultraviolet laser enables the ultraviolet laser to process a plurality of materials which can not be processed by frequency doubling laser and fundamental frequency laser.
At present, the technical scheme for obtaining the high-power continuously tunable all-solid-state ultraviolet laser mainly comprises the following steps:
firstly, a femtosecond laser is obtained by doping titanium sapphire in a green light pump, and then frequency multiplication is carried out on the femtosecond laser to obtain ultraviolet laser output (high-power green light is difficult to obtain and high in cost);
secondly, the frequency of the near-fundamental laser output by the laser diode is directly doubled (the efficiency is very low);
and thirdly, triple frequency or quadruple frequency of the fundamental frequency all-solid-state laser.
Among them, the triple frequency technique by fundamental laser can be generally used to obtain ultraviolet and double frequency band laser. Taking 355nm laser as an example, the high-power 355nm laser mainly comprises pulse or quasi-continuous laser which is currently put out in the laser market. For example, a 355nm UV laser with 30kHz repetition rate and 12w maximum power, as proposed by the United states Spectroscopy physical company; the United states coherent company provides a birefringence compensation technology for series connection of LD pump double rods, and realizes a 355nm ultraviolet laser with a repetition rate of 8kHz and power of 160W. No 355nm continuous laser with a compact structure and above the watt level is reported at present, the maximum output power of continuous 355nm frequency tripling which can be found in the literature is 410 milliwatts [ see Conference on laser and Electro-Optics 1996, ISBN: 1-55752-. Another frequency tripling technical scheme for generating continuous 355nm laser is frequency tripling by adopting a single-pass two cascaded PPSLT crystals (see Advanced Solid-State Photonics 2012,29 January-1 February2012, ISBN: 978-1-55752-933-6), and the scheme has the advantages of simple and compact structure and good output power stability, but is limited by the damage threshold of the second-stage sum frequency crystal, and only about 50mW of stable output of 355nm laser can be obtained at present.
Disclosure of Invention
An object of the utility model is to provide a triple frequency laser of 324-.
The technical solution of the utility model is as follows:
a triple frequency laser of 324-activated 500nm continuous laser is characterized in that: the wavelength range of the high-power fundamental frequency laser and the triple frequency module are 972-1500nm, the triple frequency module comprises a single-pass frequency doubling module and a resonance sum frequency module, the single-pass frequency doubling module is used for frequency doubling of the high-power fundamental frequency light through the periodically polarized crystal once, and the wavelength range of the generated double frequency light covers 466-750 nm; the resonance sum frequency cavity in the resonance sum frequency module only resonates with the double-frequency laser, the residual high-power fundamental frequency light passes through the intracavity nonlinear crystal in the resonance cavity once, the resonant double-frequency light and the single-pass fundamental frequency light sum frequency obtain high-power triple-frequency continuous laser, and the wavelength range of the triple-frequency continuous laser is 324-500 nm.
The triple frequency laser of 324-activated 500nm continuous laser comprises a high-power fundamental frequency laser with a wavelength range of 972-activated 1500nm and a triple frequency module, wherein the triple frequency module comprises a single-pass frequency doubling and resonance sum frequency, and specifically comprises a first half-wavelength phase retarder, a second half-wavelength phase retarder, a third half-wavelength phase retarder, a single-pass frequency doubling crystal, a first harmonic filtering mirror, a first high-reflection mirror, a third high-reflection mirror, a fourth high-reflection mirror, a first mode matching lens, a second mode matching lens, a third mode matching lens, a resonance sum frequency cavity and a harmonic wave filter, wherein a nonlinear crystal is arranged in the resonance sum frequency cavity, and the components are distributed along an optical path as follows:
the first half-wavelength phase retarder, the first mode matching lens and the single-pass frequency doubling crystal are sequentially arranged along the direction of fundamental frequency light output by the high-power fundamental frequency laser, the single-pass frequency doubling crystal outputs double-frequency light and residual fundamental frequency light, the first harmonic filtering mirror is arranged in the directions of the double-frequency laser and the residual fundamental frequency light and is divided into residual fundamental frequency light in the transmission direction and double-frequency light in the reflection direction, the third high reflector, the fourth high reflector, the third half-wavelength phase retarder, the third mode matching lens group and the 2 ports of the resonance sum frequency cavity are sequentially arranged along the direction of the residual fundamental frequency light, the first high reflector, the second half-wavelength phase retarder, the second mode matching lens group and the 1 port of the resonance sum frequency cavity enter the resonance sum frequency cavity and are enhanced along the direction of the double-frequency light, and the residual fundamental frequency light generate triple-frequency light through the nonlinear crystal of fundamental frequency, the triple frequency light, the double frequency light and the residual fundamental frequency light are separated by the harmonic wave filter and then output triple frequency light through the harmonic wave filter.
The triple frequency laser of 324-activated 500nm continuous laser comprises a high-power fundamental frequency laser with the wavelength range of 972-activated 1500nm and a triple frequency module, wherein the triple frequency module comprises a single-pass frequency doubling and resonance sum frequency, and specifically comprises a first half-wavelength phase retarder, a second half-wavelength phase retarder, a third half-wavelength phase retarder, a single-pass frequency doubling crystal, a first harmonic filtering mirror, a first high-reflection mirror, a second high-reflection mirror, a third high-reflection mirror, a fourth high-reflection mirror, a first mode matching lens, a second mode matching lens, a third mode matching lens, a resonance sum frequency cavity and a harmonic wave filter, wherein a nonlinear crystal is arranged in the resonance sum frequency cavity, and the triple frequency laser further comprises a polarization splitter and a light collector, and the components are distributed along the light path as follows:
the first half-wavelength phase retarder and the polarization beam splitter are arranged along the direction of the fundamental frequency light output by the high-power fundamental frequency laser in sequence, the polarization beam splitter takes the input fundamental frequency light as transmitted fundamental frequency light and reflected fundamental frequency light,
the first high reflecting mirror, the third high reflecting mirror, the fourth high reflecting mirror, the third half-wavelength phase retarder, the third mode matching lens group and the 2 ports of the resonant sum frequency cavity are arranged along the direction of reflecting fundamental frequency light in sequence;
the first mode matching lens and the single-pass frequency doubling crystal are arranged along the direction of the transmission fundamental frequency light in sequence, the single-pass frequency doubling crystal outputs double-frequency light and residual fundamental frequency light, a first harmonic filtering mirror is arranged in the direction of the double-frequency light and the residual fundamental frequency light, the first harmonic filtering mirror is divided into residual fundamental frequency light in the transmission direction and double-frequency light in the reflection direction, the residual fundamental frequency light enters the light collector, the double-frequency light in the reflection direction enters the resonance sum frequency cavity through the first high reflecting mirror, the second half-wavelength phase retarder, the second mode matching lens group and the 1 port of the resonance sum frequency cavity in sequence and is subjected to resonance enhancement, the double-frequency light and the reflected fundamental frequency light generate triple-frequency light through the nonlinear crystal, and the triple-frequency light and the residual of the double-frequency light and the reflected fundamental frequency light are separated through the harmonic filter, the triple-frequency light (12) is transmitted through the harmonic filter and output.
The high-power fundamental frequency laser with the wavelength range of 972-1500nm comprises but is not limited to a solid laser, an ytterbium-doped fiber laser, an erbium-doped fiber laser, a Raman fiber laser or a semiconductor laser.
The single-pass frequency multiplication of the single-pass periodically polarized crystal and the output end of the high-power fundamental frequency laser are integrated on a nonadjustable light path through precise alignment, and the high-power fundamental frequency laser has the advantages of compact structure and stable light path;
the resonance sum frequency cavity comprises traveling wave cavities such as a double-mirror FP standing wave cavity, a three-cavity mirror, a four-cavity mirror and a five-cavity mirror; the modes of resonance and frequency cavity locking include, but are not limited to, dither frequency stabilization [ see Optics Express 15(21) 14213-.
The resonant and intracavity nonlinear crystal includes but is not limited to lithium triborate (LBO), barium metaborate (BBO), cesium triborate (CLBO), and Periodically Poled Lithium Niobate (PPLN), periodically poled lithium tantalate (pplst), periodically poled potassium titanyl phosphate (PPKTP); the resonance and the frequency cavity only need to be locked to the wavelength of the double frequency light, and the high-power fundamental frequency light passes through the nonlinear crystal in the cavity once; the double frequency light is enhanced in resonance and frequency cavity resonance, and high-power fundamental frequency laser passes through the double frequency light and the frequency cavity once in the nonlinear crystal to obtain 324-500nm triple frequency laser.
The utility model discloses compare with current triple frequency scheme as follows advantage:
1. compared with a frequency tripling scheme of single-pass two cascaded periodically poled crystals, the laser output power is improved by two orders of magnitude.
2. Compared with the triple frequency technical scheme of resonance and frequency cavity dual wavelength locking, the utility model only needs one locking loop and only needs one set of high-power fiber laser, wherein, the single pass frequency cavity only needs to lock frequency doubling laser, the locking is easier, and the anti-interference performance is better; only a single set of high-power single-frequency fiber laser is needed, so that the cost is lower.
In a word, the utility model discloses reduced the cost of laser instrument, enlarged practical scope.
Drawings
FIG. 1 is a schematic diagram of a triple frequency laser for 324-doped 500nm continuous laser of the present invention
Fig. 2 is a schematic structural diagram of a triple-frequency laser of a hundred milliwatts 355nm continuous ultraviolet laser according to the embodiment of the present invention.
Fig. 3 is a schematic structural diagram of a triple-frequency laser of a watt-level 355nm continuous ultraviolet laser according to the embodiment of the present invention.
Detailed Description
Referring to fig. 1, fig. 1 is a schematic diagram of a triple frequency laser of 324-plus 500nm continuous laser according to the present invention, as can be seen from the figure, the triple frequency laser of 324-plus 500nm continuous laser according to the present invention, a high-power fundamental frequency laser 1 and a triple frequency module 2 with a wavelength range of 972-plus 1500nm, wherein the triple frequency module 2 includes a one-way frequency doubling module 201 and a resonant frequency doubling module 202, the one-way frequency doubling module 201 is used for frequency doubling of the high-power fundamental frequency light 3 by a single-pass periodically polarized crystal, and the wavelength range of the generated double frequency light 4 covers 466-plus 750 nm; the resonant cavity in the resonant sum frequency module 202 only resonates with the frequency-doubled laser 4, the remaining high-power fundamental frequency light 5 passes through the nonlinear sum frequency crystal in the resonant cavity once, and the frequency sum of the resonated frequency-doubled light 4 and the once-passed fundamental frequency light 5 obtains the high-power triple-frequency continuous laser 6, wherein the wavelength range of the triple-frequency continuous laser 6 is 324-.
The characteristics and advantages of the invention will become more apparent from reading the detailed description of a non-limiting example given with reference to fig. 2 and 3.
Example 1
Fig. 2 is a schematic diagram of a frequency tripling structure of a hundred milliwatts 355nm continuous ultraviolet laser according to the embodiment of the present invention. It can be seen from the figure that the triple frequency laser of the 324-plus-500 nm continuous laser in this embodiment includes a high-power fundamental frequency laser 1 with a wavelength range of 972-plus-1500 nm and a triple frequency module, where the triple frequency module includes a single-pass frequency doubling 4 and a resonant sum frequency cavity 8, and specifically includes a first half-wavelength phase retarder 201, a second half-wavelength phase retarder 202, a third half-wavelength phase retarder 203, a single-pass frequency doubling crystal 401, a first harmonic filtering mirror 501, a first high-reflection mirror 502, a second high-reflection mirror 503, a third high-reflection mirror 504, a first mode matching lens 701, a second mode matching lens 702, a third mode matching lens 703, a resonant sum frequency cavity 8, and a harmonic wave splitter 9, and a nonlinear crystal 805 is disposed in the resonant sum frequency cavity 8, and the components are distributed along the optical path as follows:
the first half-wavelength phase retarder 201, the first mode matching lens 701 and the single-pass frequency doubling crystal 401 are sequentially arranged along the direction of the fundamental frequency light 10 output by the high-power fundamental frequency laser 1, and the output frequency doubling light 11 and the residual fundamental frequency light 10 of the single-pass frequency doubling crystal 401 are sequentially arranged along the direction of the fundamental frequency light 10 output by the high-power fundamental frequency laser 1*In the frequency-doubled laser 11 and the residual fundamental frequency light 10*The direction is a first harmonic filtering mirror 501, and the first harmonic filtering mirror 501 is divided into residual fundamental frequency light 10 in the transmission direction*And a reflection direction of the light 11 of double frequency along said residual fundamental frequency 10*The direction is sequentially a second high reflection mirror 503, a third high reflection mirror 504, a third half-wavelength phase retarder 203, a third mode matching lens group 703 and a 2 port of a resonance sum frequency cavity 8, the direction of the frequency doubling light 11 is sequentially a first harmonic filtering mirror 501 and a second high reflection mirror 502, the direction of the second half-wavelength phase retarder 202, the direction of the second mode matching lens group 702 and a 1 port of the resonance sum frequency cavity 8 enter the resonance sum frequency cavity 8 and are resonantly enhanced, and the frequency doubling light 11 and the residual base frequency light 10*The frequency of the nonlinear crystal 805 is summed to generate triple frequency light 12, the double frequency light 11 and the residual fundamental frequency light 10*After being separated by the harmonic filter 9, the light passes through the harmonic filter 9 and outputs triple-frequency light 12.
Wherein, single-pass doubling of frequency part 4 includes:
the focusing lens 701: and 1064nm fundamental frequency light is collected.
Periodically poled crystal 401: adopting a periodically poled crystal with high damage threshold and high nonlinear conversion efficiency; the heat sink temperature of the crystal is accurately controlled, and the crystal is wrapped by special high-temperature-resistant engineering plastics, so that the long-term temperature drift of the crystal is reduced.
The harmonic filtering mirror 501 is used for filtering out 1064nm fundamental frequency light remaining in 532nm frequency doubling light, and guiding 532nm laser into the resonance sum frequency cavity 8.
The resonance sum frequency part comprises:
the second mode matching lens 702: a mode matching lens group of 532nm frequency doubling light is optimally designed by utilizing a transmission matrix of Gaussian beams, so that the mode matching lens group is matched with a local oscillation mode of a resonance frequency cavity.
Four-mirror resonance sum frequency cavity 8: the ring cavity is locked to 532nm green light generated by the first stage through a PDH frequency stabilization technology, the power of 532nm laser in the cavity is improved, and other resonant cavities with gain effects can be used for replacing the ring cavity, such as a double-mirror FP cavity, a three-mirror ring cavity, a five-mirror ring cavity and the like; the frequency stabilization technology can be a common frequency stabilization scheme such as PDH frequency stabilization, HC frequency stabilization, jitter frequency stabilization and the like; wherein 801-804 is a resonant cavity mirror used for 532nm laser to form a resonance condition.
Nonlinear crystal 805: nonlinear crystals for 1064nm and 532nm sum frequency, and the crystals can be LBO, BBO, CLBO and other nonlinear crystals. The cutting mode comprises normal incidence on two surfaces, parallel Brewster angle cutting on two surfaces and single Brewster angle cutting on an emergent end.
Harmonic separator 9: to filter out the residual 1064nm and 532nm laser light in 355 nm.
Fundamental frequency light 10: the laser 1 generates high-power 1064nm fundamental frequency light.
The frequency-doubled light 11 is 532nm frequency-doubled light generated by the fundamental frequency light 10 passing through the single-pass frequency doubling crystal 401.
The triple-frequency light 12 is a fundamental light 10*And 355nm frequency tripled light generated by the frequency doubling light 11 passing through resonance and the frequency summation 8.
The fundamental frequency power required to generate 355nm of hundred milliwatts is relatively low, and the 1064nm fundamental frequency light 10 remained after single-pass frequency doubling*The fundamental power required for resonance and sum frequencies can already be met. The single-frequency 1064nm fiber laser amplifier 1 outputs a high-power 1064nm continuous fundamental frequency light 10 of about 30 watts. 1064nm enters the periodically poled crystal 401 through the first mode matching lens group 701 with proper beam waist and polarization, and the heat sink of the periodically poled crystal 401 is wrapped by engineering plastics with high temperature resistance and excellent heat preservation. Outgoing double frequency light 11 and residual fundamental frequency light 10*Separation of residual 1064nm fundamental light 10 by harmonic filtering mirror 501*Wherein, 532nm frequency doubling light 11 with 10W magnitude is reflected by the first high reflecting mirror 502 and then guided into the next stage resonance and frequency cavity 8. Residual approximately 20 watts of 1064nm fundamental frequency light 10*Through the secondThe high reflection mirror 504, the third high reflection mirror 505, is guided into the resonance sum frequency cavity 8 and passes a single time through a nonlinear crystal 805 inside the cavity. The phase retarder 203 is used for changing 1064nm polarization to meet the phase matching condition required by sum frequency. The third lens group 703 is used to focus the 1064nm laser light to the center of the nonlinear crystal 805.
According to Boyd and Kleinman's theory on the sum frequency of Gaussian light, the relationship between the sum frequency power and the two fundamental frequency optical powers can be written as P theoreticallySFG＝γSFGP1P2In which P isSFGIs sum frequency power, P1And P2For two fundamental powers, gammaSFGFor normalization and frequency conversion efficiency, this value is typically at 3.0x10 after selection of optimal focusing conditions for a typical nonlinear crystal- 4W-1Left and right. The 1064nm fundamental frequency light 10 of about 20W is used here*The power of 532nm in the nonlinear crystal 805 is increased by a single pass through the nonlinear crystal 805 and the resonance gain of the 532nm frequency-doubled light 11 of 10W in the resonance and frequency cavity 8 to the hundred watt level. The power of 355nm frequency tripled laser 12 generated by sum frequency can reach hundreds of milliwatts according to theoretical calculation. The generated 355nm triple frequency ultraviolet light 12 is output through the cavity mirror 804, and 1064nm and 532nm laser light is finally filtered by the harmonic separator 9.
Example 2
Fig. 3 is a schematic structural diagram of a triple-frequency laser of a watt-level 355nm continuous ultraviolet laser according to embodiment 2 of the present invention.
As can be seen from the figure, the embodiment includes a high-power 1064nm fiber laser amplifier 1, a first half-wavelength phase retarder 201, a second half-wavelength phase retarder 202, a third half-wavelength phase retarder 203, a polarization beam splitter 3, a single-pass frequency doubling module 4, a harmonic filtering mirror 501, a first high-reflection mirror 502, a second high-reflection mirror 503, a third high-reflection mirror 504, a fourth high-reflection mirror 505, a light collector 6, a first mode matching lens group 701, a second mode matching lens group 702, a third mode matching lens group 703, and a resonant sum frequency cavity 8.
The first half-wavelength phase delayer 201 is arranged along the direction of the fundamental frequency light 10 output by the high-power fundamental frequency laser 1A polarization beam splitter 3 for splitting the input fundamental frequency light into a transmission fundamental frequency light and a reflection fundamental frequency light 10 by the polarization beam splitter 3**，
Along the reflected fundamental light 10**The direction is sequentially the second high reflection mirror 503, the third high reflection mirror 504, the fourth high reflection mirror 505, the third half-wavelength phase retarder 203, the third mode matching lens group 703, the resonance and 2 ports of the frequency cavity 8;
the first mode matching lens 701 and the single-pass frequency doubling crystal 401 are arranged along the direction of the transmission fundamental frequency light in sequence, and the single-pass frequency doubling crystal 401 outputs frequency doubling light 11 and residual fundamental frequency light 10*At said frequency-doubled light 11 and residual fundamental frequency light 10*The direction is a first harmonic filtering mirror 501, and the first harmonic filtering mirror 501 is divided into transmission direction residual fundamental frequency light 10*And a reflection direction of a second frequency light 11, said residual fundamental frequency light 10*The light enters the light collector 601, the frequency-doubled light 11 in the reflection direction sequentially passes through the first high-reflection mirror 502, the second half-wavelength phase retarder 202, the second mode matching lens group 702 and the port 1 of the resonance sum frequency cavity 8 to enter the resonance sum frequency cavity 8 and be resonantly enhanced, and the frequency-doubled light 11 and the reflected fundamental frequency light 10**The frequency of the nonlinear crystal 805 is summed to generate triple frequency light 12, the double frequency light 11 and the reflected fundamental frequency light 10**After the residue is separated by the harmonic filter 9, the triple frequency light 12 is transmitted through the harmonic filter 9 and output.
Wherein, single-pass doubling of frequency part 4 includes:
the focusing lens 701: and 1064nm fundamental frequency light is collected.
Periodically poled crystal 401: adopting a periodically poled crystal with high damage threshold and high nonlinear conversion efficiency; the heat sink temperature of the crystal is accurately controlled, and the crystal is wrapped by special high-temperature-resistant engineering plastics, so that the long-term temperature drift of the crystal is reduced.
The light ray collector 601: the residual 1064nm fundamental frequency light was collected.
The resonance sum frequency part comprises:
wherein 801-
Second pattern matching lens group 702: a mode matching lens group of 532nm frequency doubling light is optimally designed by utilizing a transmission matrix of Gaussian beams, so that the mode matching lens group is matched with a local oscillation mode of a resonance frequency cavity.
Four-mirror resonance sum frequency cavity 8: the ring cavity is locked to 532nm green light generated by the first stage through a PDH frequency stabilization technology, the power of 532nm laser in the cavity is improved, and other resonant cavities with gain effects can be used for replacing the ring cavity, such as a double-mirror FP cavity, a three-mirror ring cavity, a five-mirror ring cavity and the like; the frequency stabilization technology can be a common frequency stabilization scheme such as PDH frequency stabilization, HC frequency stabilization, jitter frequency stabilization and the like; wherein 801-804 is a resonant cavity mirror used for 532nm laser to form a resonance condition.
Nonlinear crystal 805: nonlinear crystals for 1064nm and 532nm sum frequency, and the crystals can be LBO, BBO, CLBO and other nonlinear crystals. The cutting mode comprises normal incidence on two surfaces, parallel Brewster angle cutting on two surfaces and single Brewster angle cutting on an emergent end.
Harmonic separator 9: to filter out the residual 1064nm and 532nm laser light in 355 nm.
The fundamental light 10 is a high-power 1064nm fundamental light generated by the laser 1.
The frequency-doubled light 11 is 532nm frequency-doubled light generated by the single-pass frequency doubling crystal 401.
The triple-frequency light 12 is a fundamental light 10**And 355nm frequency tripled light generated by the resonance and the sum frequency 8 of the frequency doubled light 11.
As illustrated in fig. 2, the present invention obtains a frequency tripling laser of a watt-level 355nm continuous laser, wherein the frequency tripling part comprises a single-pass frequency doubling 4 and a resonant frequency 8.
Considering the damage threshold of the single-pass frequency doubling crystal 401, the single-frequency 1064nm fiber laser amplifier 1 outputs 100W 1064nm continuous fundamental frequency light 10It needs to be divided into two paths through the phase retarder 201 and the polarization beam splitter 3. The first path of 1064nm of about 30 w is incident into the periodically polarized crystal 401 through the focusing lens 701 with proper beam waist and polarization, and the heat sink of the periodically polarized crystal 401 is wrapped by engineering plastics with excellent high temperature resistance and heat preservation. 532nm double frequency light 11 and residual fundamental frequency light 10*Filtering out residual 1064nm fundamental frequency light 10 by the harmonic filtering mirror 501*Wherein the residual 1064nm fundamental frequency light 10*Collected by the light collector 601, the 532nm double frequency light 11 obtained by this method is reflected by the high reflection mirror 502 and guided to the next stage resonance and frequency cavity 8.
The resonant sum frequency cavity 8 is exemplified by a four-cavity mirror annular cavity, wherein the phase retarder 202 is used for changing the polarization state of the 532nm double frequency light 11 to satisfy the phase matching condition required by the sum frequency, and the mode matching lens group 702 is used for mode conversion of the 532nm double frequency light 11 to satisfy the mode matching condition required by the resonant cavity. Second path of 1064nm fundamental laser 10 about 70W**And is guided to the resonance and frequency cavity by harmonic filtering mirrors 503, 504 and 505, and passes through the intracavity nonlinear crystal 805 in a single pass. The phase retarder 203 is used for changing the 1064nm fundamental frequency light 10**To satisfy the phase matching condition required for sum frequency. The lens group 703 is used for converting 1064nm fundamental frequency light 10**Converging to the center of the nonlinear crystal 805.
According to Boyd and Kleinman's theory on the sum frequency of Gaussian light, the relationship between the sum frequency power and the two fundamental frequency optical powers can be written as P theoreticallySFG＝γSFGP1P2In which P isSFGIs sum frequency power, P1And P2For two fundamental powers, gammaSFGFor normalization and frequency conversion efficiency, this value is typically at 3.0x10 after selection of optimal focusing conditions for a typical nonlinear crystal- 4W-1Left and right. The 1064nm fundamental frequency light 10 of about 70W is used here**The power of 532nm in the nonlinear crystal 805 is increased by a single pass through the nonlinear crystal 805 and the resonance gain of the 532nm frequency-doubled light 11 of 10W in the resonance and frequency cavity 8 to the hundred watt level. According to theoretical calculation, the laser power of 355nm frequency tripling 12 generated by sum frequency can reach wattAnd (4) stages. The generated 355nm triple frequency ultraviolet light 12 is output through the cavity mirror 804, and 1064nm and 532nm laser light is finally filtered by the harmonic separator 9.
The technical effects of the utility model:
the utility model discloses can only realize the continuous ultraviolet output of powerful 355nm with the triple frequency of one set of 1064nm, wherein change the resonance doubling of frequency of first order into the one-way doubling of frequency 4 back, can realize the stable output of powerful 532nm doubling of frequency light, its line width is narrower, and the beam quality is better than the doubling of frequency light that the resonance doubling of frequency produced. The resonance and frequency cavity 8 of the second stage only needs to be locked to 532nm laser, the locking loop is simpler, and the stability of the continuous operation of the laser can be better.
Compared with the scheme of singly passing through two cascade period polarized crystals, the utility model greatly improves the ultraviolet output power; compared with the common technical scheme of resonance and frequency cavity dual-wavelength locking, the method has the advantages of no need of multiple sets of resonance and lasers, simpler light path structure, more stable output power and lower cost.
Claims (6)
1. A triple frequency laser of 324-activated 500nm continuous laser is characterized in that: the wavelength range of the high-power fundamental frequency laser (1) and the triple frequency module (2) is 972-1500nm, the triple frequency module (2) comprises a single-pass frequency doubling module and a resonance sum frequency module, the single-pass frequency doubling module is used for periodically polarizing a frequency doubling crystal through single pass of high-power fundamental frequency light, and the wavelength range of the generated double frequency light covers 466-750 nm; the resonance sum frequency cavity (8) in the resonance sum frequency module only resonates with the double-frequency laser, the residual high-power fundamental frequency light passes through the intracavity nonlinear crystal (805) in the resonance cavity once, the resonant double-frequency light and the single-pass fundamental frequency light sum frequency obtain high-power triple-frequency laser (6), and the wavelength range of the triple-frequency laser (6) is 324-500 nm.
2. The triple frequency laser for 324-activated 500nm continuous laser as claimed in claim 1, wherein: the high-power fundamental frequency laser comprises a high-power fundamental frequency laser (1) with the wavelength range of 972-1500nm and a triple frequency module (2), wherein the triple frequency module (2) comprises a single-pass frequency doubling (4) and a resonant sum frequency cavity (8), and specifically comprises a first half-wavelength phase retarder (201), a second half-wavelength phase retarder (202), a third half-wavelength phase retarder (203), a single-pass frequency doubling crystal (401), a first harmonic filtering mirror (501), a first high-reflection mirror (502), a second high-reflection mirror (503), a third high-reflection mirror (504), a first mode matching lens (701), a second mode matching lens (702), a third mode matching lens (501), a resonant sum frequency cavity (703) and a harmonic wave splitter (9), and a nonlinear crystal (805) is arranged in the resonant sum frequency cavity (8);
the first half-wavelength phase retarder (201), the first mode matching lens (701) and the single-pass frequency doubling crystal (401) are sequentially arranged along the direction of the fundamental frequency light (10) output by the high-power fundamental frequency laser (1), and the output double-frequency light (11) and the residual fundamental frequency light (10) of the single-pass frequency doubling crystal (401) are*) At said second harmonic light (11) and residual fundamental light (10)*) The direction is a first harmonic filtering mirror (501), and the first harmonic filtering mirror (501) is divided into transmission direction residual fundamental frequency light (10)*) And light (11) of double frequency in the reflection direction, along said residual fundamental frequency (10)*) The direction is sequentially a third high reflecting mirror (504), a fourth high reflecting mirror (505), a third half-wavelength phase retarder (203), a third mode matching lens (703) and a 2 port of a resonance sum frequency cavity (8), along the direction of the frequency doubling light (11), a 1 port of the first high reflecting mirror (502), the second half-wavelength phase retarder (202), the second mode matching lens (702) and the resonance sum frequency cavity (8) enters the resonance sum frequency cavity (8) and is enhanced in resonance, and the frequency doubling light (11) and the residual frequency base light (10)*) Generating a frequency tripled light (12) by said nonlinear crystal (805), said frequency tripled light and frequency doubled light (11) and residual fundamental light (10)*) After being separated by the harmonic wave sub-filter (9), the triple frequency light (12) is output by penetrating through the harmonic wave sub-filter (9).
3. The triple frequency laser of 324-1500 nm continuous laser according to claim 1, comprising a high power fundamental frequency laser (1) with a wavelength range of 972-1500nm and a triple frequency module (2), wherein the triple frequency module (2) comprises a single-pass frequency doubling (4) and a resonant sum frequency cavity (8), and specifically comprises a first half-wavelength phase retarder (201), a second half-wavelength phase retarder (202), a third half-wavelength phase retarder (203), a single-pass frequency doubling crystal (401), a first harmonic rejection mirror (501), a first high-reflection mirror (502), a second high-reflection mirror (503), a third high-reflection mirror (504), a fourth high-reflection mirror (505), a first mode matching lens (701), a second mode matching lens (702), a third mode matching lens (703), a resonant sum frequency cavity (8), and a harmonic filter (9), a nonlinear crystal (805), a polarization beam splitter (3) and a light collector (601) are arranged in the resonance sum frequency cavity (8);
the first half-wavelength phase retarder (201) and the polarization beam splitter (3) are sequentially arranged along the direction of the fundamental frequency light (10) output by the high-power fundamental frequency laser (1), and the polarization beam splitter (3) takes the input fundamental frequency light as transmitted fundamental frequency light and reflected fundamental frequency light (10)**)，
Along the reflected fundamental light (10)**) The direction is sequentially 2 ports of the second high-reflection mirror (503), the third high-reflection mirror (504), the fourth high-reflection mirror (505), the third half-wavelength phase retarder (203), the third mode matching lens (703) and the resonant sum frequency cavity (8);
the first mode matching lens (701) and the single-pass frequency doubling crystal (401) are arranged in sequence along the direction of the transmitted fundamental frequency light, and the single-pass frequency doubling crystal (401) outputs double-frequency light (11) and residual fundamental frequency light (10)*) At said second harmonic light (11) and residual fundamental light (10)*) The direction is a first harmonic filter mirror (501), the first harmonic filter mirror (501) is divided into residual fundamental frequency light (10) in the transmission direction*) And light (11) of double frequency in the reflection direction, said residual fundamental light (10)*) Enters the light collector (601), the frequency doubling light (11) in the reflection direction sequentially enters the resonance sum frequency cavity (8) through the first high-reflection mirror (502), the second half-wavelength phase retarder (202), the second mode matching lens (702) and the 1 port of the resonance sum frequency cavity (8) and is resonantly enhanced, and the frequency doubling light (11) and the reflection fundamental frequency light (10)**) Generating a frequency tripled light (12) by said nonlinear crystal (805), said frequency tripled light and frequency doubled light (11) and reflected fundamental light (10)**) The residual menstrual period ofAfter the harmonic wave sub-filter (9) is separated, the triple frequency light (12) is transmitted through the harmonic wave sub-filter (9) to be output.
4. The triple frequency laser of 324-activated 500nm continuous laser as claimed in claim 1, 2 or 3, wherein: the high-power fundamental frequency laser (1) with the wavelength range of 972-1500nm comprises but is not limited to a solid laser, an ytterbium-doped fiber laser, an erbium-doped fiber laser, a Raman fiber laser or a semiconductor laser.
5. The triple frequency laser of 324-doped 500nm continuous laser according to claim 1, 2 or 3, characterized in that the resonance sum frequency cavity (8) includes but is not limited to a double-mirror FP standing wave cavity, a triple cavity mirror, a four-cavity mirror and a five-cavity mirror iso-traveling wave cavity; the modes of resonance and frequency cavity locking include, but are not limited to, jitter stabilization, PDH stabilization, and HC stabilization.
6. The triple frequency laser of 324-doped 500nm continuous laser according to claim 1, 2 or 3, characterized in that the intracavity nonlinear crystal (805) comprises lithium triborate (LBO), barium metaborate (BBO), cesium triborate (CLBO) and Periodically Poled Lithium Niobate (PPLN), periodically poled lithium tantalate (pplst), periodically poled potassium titanyl phosphate (PPKTP).
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