Source: https://patents.google.com/patent/CN102064462B/en
Timestamp: 2019-04-19 15:59:08+00:00

Document:
The invention provides an optical parametric oscillator with wide tuning range and dual wavelength output. The oscillator comprises a pumping source, an optical coupling lens group, a planar input mirror, a periodically poled nonlinear crystal, a temperature control furnace and a vertical double-arm output mirror, wherein the vertical double-arm output mirror is formed by two plane mirrors which are vertical with each other; the temperature control furnace is sleeved outside the periodically poleddomain nonlinear crystal to form a temperature-control nonlinear crystal; the planar input objective and the vertical double-arm output mirror form an oscillating cavity of the optical parametric oscillator; the structures are arranged on the same optical path in sequence; after pumping light emitted by the pumping source is focused through an optical coupling lens group and is transmitted from the planar input objective, the light first enters a certain period of the periodically poleddomainnonlinear crystal to generate first idle light with a certain wavelength; and after the rest pumping light is reflected through the vertical double-arm output mirror, the rest pumping light enters the other period of the periodically poleddomain nonlinear crystal to generate second idle light with the other wavelength. Therefore, dual wavelength output is obtained to form a dual wavelength optical parametric oscillator.
 (5)使用两束激光分别通过多周期极化晶体的两个不同周期实现双信号光运转的光学参量产生器：Pu Zhao 等人发表在J. Opt. A ：PureAppl. Opt. (vol (9)，2007 :235-238)上的文章使用声光分束器将泵浦激光分为两束激光后，分别通过多周期极化PPLN晶体两个不同极化周期产生双波长信号光输出。  (5) using two laser beams, respectively, to achieve dual optical parametric signal light generated by the operation of two different multi-cycle periods poled crystals: Pu Zhao et al in J. Opt A:... PureAppl Opt ( vol (9), 2007: the article was used on the sound 235-238) the beam splitter pump laser into two laser beams, respectively, generated by two-wavelength multiple signal light periodically poled two distinct poling period PPLN crystal output. 该方法中泵浦光单次通过PPLN晶体，只具有单程增益，激光输出功率受到限制。 This method of pump light in a single pass PPLN crystal, only a single pass gain, the laser output power is limited.
 为了解决背景技术中的问题，本发明的目的是要提供一种调谐范围宽、输出功率高、装置结构简单紧凑、光路易于调节的宽调谐范围双波长输出光参量振荡器。  In order to solve the problems of the background art, an object of the present invention is to provide a wide tuning range, high output power, device simple and compact structure, easy to adjust the optical path wide tuning range dual-wavelength output optical parametric oscillator.
 其中泵浦源发出的泵浦光经光学耦合透镜组聚焦再从平面输入镜透射后，先入射到周期极化非线性晶体的某一周期上产生某一波长的第一闲频光，第一闲频光由垂直双臂输出镜的上臂透射出去；剩余泵浦光经垂直双臂输出镜反射后，再入射到周期极化非线性晶体的另一周期上产生另一波长的第二闲频光，第二闲频光经平面输入镜反射后再由垂直双臂输出镜的下臂透射出去，由此获得双波长输出，构成双波长输出光参量振荡器。 Generating a first wavelength on Busy  where the pumping light is a pumping source optically coupled to the lens group and then emitted from the focal plane of the input mirror transmission, the first incident of a periodically poled nonlinear crystal optical frequency period of the first light transmitting idler arm out from the vertical arms of the output mirror; residual pump light that is generated by the vertical arms of another wavelength output mirror, is incident to the other cycle periodically poled nonlinear crystal of two idler, the second idler light input via the plane mirror and then passes through to the lower arm from the vertical arms of the output mirror, thereby obtaining a dual wavelength output, constituting the dual-wavelength output optical parametric oscillator.
 本发明的优点在于双波长闲频光的输出波长调谐范围宽、输出功率高，整套装置结构简单紧凑，光路易于调节。  The advantage of the present invention is that the output wavelength of the idler light wavelength bis wide tuning range, high output power, the entire apparatus simple and compact structure, easy to adjust the optical path.
 图9是本发明使用侧泵激光头的泵浦源的示意图。  FIG. 9 is a schematic diagram of the laser pump source side of the pump head of the present invention.
 平面输入镜13，所述的平面输入镜13的材料为石英（JGSl);其表面镀对泵浦光高透射率和对信号光、闲频光高反射率膜，其中高透射率T为97. 2% @1. 064 μ m,高反射率R> 99. 7% §1. 3-1. 6 μ m&R > 98. 2% §3. 6-4. 8 μ m。  The flat input mirror 13, the material of the flat input mirror 13 of quartz (JGSl); coating the surface of the pump light transmittance and high light reflectance of the film of high light signal, idler, wherein a high transmittance of T is 97. 2% @ 1. 064 μ m, a high reflectance R> 99. 7% §1. 3-1. 6 μ m & R> 98. 2% §3. 6-4. 8 μ m.
 周期极化非线性晶体14，所述的周期极化非线性晶体14，其尺寸为30mmX 13mmX lmm,其极化结构为扇形周期极化结构，极化周期从26. 9-29. 5 μ m连续变化，该周期极化非线性晶体14两端面镀对信号光、闲频光和泵浦光减反射率膜，其中减反射率R < 1% §1. 3-1. 6 μ m&R < I. 5% §3. 3-4. 8 μ m&R < 2% il. 064 μ m。  periodically poled nonlinear crystal 14, a periodically poled nonlinear crystal 14, having dimensions of 30mmX 13mmX lmm, its polarization periodically poled structure of a fan structure, poling period from 26. 9-29. 5 μ m varies continuously, periodically poled nonlinear crystal 14 the both end surfaces plated with the signal light, idler light and pumping light reflectance reducing film, wherein the antireflection of R <1% §1. 3-1. 6 μ m & R <I. 5% §3. 3-4. 8 μ m & R <2% il. 064 μ m. 所述的周期极化非线性晶体14 的材料是PPLN、PPLT, PPKTP, PPKTA, PPRTA, MgOiPPLN 或MgO:PPLT ;所述的非线性晶体的极化结构是扇形周期极化结构或多周期极化结构； 控温炉15，所述的控温炉15用来控制周期极化非线性晶体14的工作温度，控制精度为±0. rc ;周期极化非线性晶体14的外部套置控温炉15，形成控温非线性晶体100 ； 垂直双臂输出镜16，所述的垂直双臂输出镜16由两个互相垂直的平面镜构成，两个平面镜是垂直双臂输出镜16的双臂；所述的垂直双臂输出镜16的材料为CaF2 ;所述的垂直双臂输出镜16的表面镀对泵浦光、信号光高反射率和对闲频光高透射率膜，其中高反射率R> 98. 7% il. 064 μ m&R > 98. 7% il. 3_1· 6 μ m，高透射率T > 95. 7% §3. 6-4. 8 μ m,皆为45°入射角。 The material of the periodically poled nonlinear crystal 14 is PPLN, PPLT, PPKTP, PPKTA, PPRTA, MgOiPPLN or MgO: PPLT; polarization of the nonlinear crystal structure is a fan or a periodically poled periodically poled structure structure;  the temperature control oven 15, the temperature of the furnace 15 is used to control the operating temperature periodically poled nonlinear crystal 14, the control precision is ± 0 rc;. sleeved outside periodically poled nonlinear crystal 14 furnace temperature control 15, temperature of the nonlinear crystal 100 is formed;  the output mirror 16 vertical arms, said vertical arms output mirror 16 is constituted by two mutually perpendicular plane mirror, two mirrors is perpendicular to the plane output mirror arms the arms 16; the material of the vertical arms of the output mirror 16 is in CaF2; arms perpendicular to the surface of the output mirror 16 is coated pump light, the signal light and high reflectance of light transmittance of the film high idler pairs wherein the high reflectance R> 98. 7% il. 064 μ m & R> 98. 7% il. 3_1 · 6 μ m, a high transmittance T> 95. 7% §3. 6-4. 8 μ m, are an incident angle of 45 °. 所述的垂直双臂输出镜16与平面输入镜13组成光参量振荡器的振荡腔；所述的光参量振荡器的振荡腔或是由平面输入镜83、平面输出镜86和直角全反射棱镜87构成。 The output mirror 16 is perpendicular to the plane of the arms enter the cavity mirrors oscillation of the optical parametric oscillator 13; said optical parametric oscillator cavity or oscillation input by a plane mirror 83, at right angles to a plane output mirror and a total reflection prism 86 87 constitute.
 其中泵浦源11发出的泵浦光经光学耦合透镜组12聚焦再从平面输入镜13透射后，先入射到周期极化非线性晶体14的某一周期上产生第一闲频光II，第一闲频光Il由垂直双臂输出镜16上臂透射出去；剩余泵浦光经垂直双臂输出镜16反射后，入射到周期极化非线性晶体14的另一周期上产生第二闲频光12，第二闲频光12经平面输入镜13反射后再由垂直双臂输出镜16的下臂透射出去，由此获得双波长输出构成双波长输出光参量振荡器。  wherein the pump light is optically coupled to the focusing lens group 12 and then the pump source 11 emitted from the flat input mirror 13 transmitting, to generate a first incident light at a certain period idler 14 periodically poled nonlinear crystal II, the first idler arms Il transmissive output mirror out by the vertical arm 16; the remaining pump light reflected by the vertical arms output mirror 16, is incident to the other periodically poled nonlinear crystal 14 cycles generating a second idler 12, the second idler 12 via the input plane mirror 13 and then passes through to the lower arm by a vertical arms output mirror 16, thereby obtaining dual wavelength output constituting the dual-wavelength output optical parametric oscillator.
 其中第一闲频光Il和第二闲频光12的波长调谐方式是通过改变周期极化非线性晶体14的温度实现温度调谐，或通过平移控温非线性晶体100实现周期调谐，或通过平移垂直双臂输出镜16实现腔镜调谐。  Il wherein the first and second idler idler light wavelength tuning mode 12 is achieved by changing the temperature of the periodically poled nonlinear crystal 14 is temperature tuned, or by translating the temperature cycle to achieve tuning of the nonlinear crystal 100, or tuning achieved by translating mirror output mirror 16 perpendicular arms.
 其中光参量振荡器的振荡腔是以信号光作为振荡光而输出双波长闲频光，信号光在光参量振荡器的振荡腔内沿U形路径往返振荡；或是以闲频光作为振荡光而输出双波长信号光，闲频光在光参量振荡器的振荡腔内沿U形路径往返振荡。  wherein the optical parametric oscillator cavity is oscillating light signal light as an oscillation output of the dual idler wavelength, the signal light and from the cavity of the oscillation in the oscillating U-shaped path along the optical parametric oscillator; or to idler as a dual-wavelength oscillation output light of the signal light, and from the idler oscillation in the oscillating U-shaped path along the cavity optical parametric oscillator.
 请参见图I和图2所示。  Referring to FIG. I and 2. 各光学器件的具体参数如下：半导体激光器21在25°C时中心波长808nm，光纤芯径为400 μ m，数值孔径为O. 22，自带温度控制和冷却系统。 Specific parameters of the optical device is as follows: the semiconductor laser 21 at 25 ° C, the center wavelength of 808nm, optical fiber core diameter of 400 μ m, a numerical aperture O. 22, temperature control and cooling system built. 光学耦合系统23为I : I耦合系统，把光纤22输出的808nm激光耦合进Nd = YVO4晶体24，聚焦光斑直径为400 μ m。 The optical coupling system 23 is a I: I coupling system, the 808nm laser 22 is coupled into the output fiber Nd = YVO4 crystal 24, the focusing spot diameter of 400 μ m. 1064nm激光腔采用结构简单的平-平腔结构，半导体激光器21输出的808nm激光经过耦合系统23后泵浦Nd = YVO4晶体24，NdiYVO4晶体24前端面镀HTi808nm&HRil064nm薄膜，作为1064nm激光谐振腔的输入镜，后端面镀HT@808nm&1064nm薄膜，NdiYVO4晶体24尺寸3X3X 10mm3，掺杂浓度为O. 3atm%，采用恒温水冷机将温度控制在18°C。 1064nm laser cavity with a simple structure flat - flat cavity structure, 808nm laser beam 21 outputted from the semiconductor laser after 23 pumped Nd coupling system = YVO4 crystal 24, NdiYVO4 crystal 24 front end surface plating HTi808nm & HRil064nm film, as a 1064nm laser resonator input mirror rear end surface plating film HT @ 808nm & 1064nm, NdiYVO4 crystal size of 24 3X3X 10mm3, a doping concentration of O. 3atm%, constant temperature water cooling unit controlling the temperature at 18 ° C. 为了获得脉冲激光输出，腔内加入声光Q开关25，重复频率l-50kHz可调。 In order to obtain the pulsed laser output, added intracavity acousto-optic Q-switch 25, l-50kHz repetition frequency is adjustable. 输出耦合镜26对1064nm的透过率为10%，腔长约为100mm。 26 pairs of 1064nm output mirror transmittance of 10%, the cavity length is about 100mm.
97. 2% §1. 064 μ m)和对信号光、闲频光高反射率膜(R > 99. 7% §1. 3-1. 6 μ m&R > 98. 2%@3. 6-4. 8 μ m)(垂直入射条件)，垂直双臂输出镜16材料为CaF2,表面镀对泵浦光、信号光高反射率（R = 98. 7% §1. 064 μ m&R > 98. 7 % il. 3-1. 6 μ m)和对闲频光高透射率膜（T>95.7% §3. 6-4. 8 μ m) (45°角入射条件）。 97. 2% §1. 064 μ m) and high light reflectance film (R> signal light, idler 99. 7% §1. 3-1. 6 μ m & R> 98. 2% @ 3. 6- 4. 8 μ m) (normal incidence), the vertical arms of the output mirror 16 in CaF2 material, plated pump light, signal light having a high reflectance (R = 98. 7% §1. 064 μ m & R> 98. 7% il. 3-1. 6 μ m) and the idler light on the high transmittance of the film (T> 95.7% §3. 6-4. 8 μ m) (45 ° angle of incidence condition). 这样，光参量振荡器的振荡腔对信号光单谐振。 Thus, the optical parametric oscillator cavity resonance oscillations of the single light signal. 在平面输入镜13和双臂垂直输出镜16之间设置的周期极化非线性晶体14的材料为MgO:PPLN,其尺寸为30mm(长)X 13mm(宽)X Imm(厚),其极化结构为扇形周期极化结构，极化周期从26. 9-29. 5 μ m连续变化，周期极化非线性晶体14两端面镀对信号光、闲频光和泵浦光减反射率膜(R < 1% §1. 3-1. 6 μ m&R < I. 5% §3. 3-4. 8 μ m&R < 2 % il. 064 μ m)。 Periodically poled nonlinear crystal material between a plane perpendicular to the input mirror 13 and output mirror 16 disposed arms 14 of MgO: PPLN, a size of 30mm (length) X 13mm (width) X Imm (thick), which is very a fan structure periodically poled structure, the poling period changes continuously from 26. 9-29. 5 μ m, periodically poled nonlinear crystal 14 on both end surfaces plated with the signal light, idler light and pumping light reflectance reducing film (R <1% §1. 3-1. 6 μ m & R <I. 5% §3. 3-4. 8 μ m & R <2% il. 064 μ m). 周期极化非线性晶体14工作温度由控温炉15控制，工作温度范围为20-200°C，控温炉15采用Pt 100作为温度传感器，控制精度为±0. 1°C。 Periodically poled nonlinear crystal 14 is controlled by the operating temperature of the furnace temperature control 15, temperature range of 20-200 ° C, the furnace temperature 15 Pt 100 employed as a temperature sensor, control precision is ± 0. 1 ° C.
 下面为了叙述方便，在周期极化非线性晶体14端面宽度方向加上均匀刻度（如图I所示），刻度范围为0-13mm，其中Omm刻度对应极化周期26. 9 μ m处，13mm刻度对应极化周期29. 5 μ m处，刻度与周期极化非线性晶体14同步移动；谐振腔右端加上坐标轴，X轴方向沿周期极化非线性晶体14的长度方向，Y轴方向沿周期极化非线性晶体14的宽度方向，Y轴坐标值范围为0-13mm,坐标轴固定不动。  For convenience of description below, plus a uniform scale in the width direction of the end face 14 periodically poled nonlinear crystal (shown in FIG. I), scale range of 0-13mm, wherein Omm poling period corresponding to the scale 26. 9 μ m at 13mm poling period corresponding to the scale 29. 5 μ m, the scale and the periodically poled nonlinear crystal 14 the synchronous mobile; plus right end of the resonator axis, the longitudinal direction 14 along the X-axis direction periodically poled nonlinear crystal, Y-axis direction along a periodically poled nonlinear crystal 14 in the width direction, Y-axis coordinate value in the range of 0-13mm, stationary axis.
 1064nm泵浦光从平面输入镜13透射后，先入射到周期极化非线性晶体14某一周期上，产生第一闲频光II，第一闲频光Il从垂直双臂输出镜16上臂透射出去；剩余泵浦光再经垂直双臂输出镜16反射后，入射到周期极化非线性晶体14另一周期，产生第二闲频光12，第二闲频光12经平面输入镜13反射后由垂直双臂输出镜16下臂透射出去。  1064nm pump light from the plane mirror 13 transmitting input, a first period 14 is incident on the periodically poled nonlinear crystal to generate a first idler II, the first idler arms Il from the vertical output mirror 16 out of the transmission arm; then the remaining pump light reflected by the vertical arms 16 output mirror is incident on another cycle periodically poled nonlinear crystal 14 to produce a second idler beam 12, the second idler 12 via the input plane after the mirror 13 passes through to the lower arm vertical arms 16 output mirror. 为了保证泵浦光经过垂直双臂输出镜16反射进入周期极化非线性晶体14的另一周期后具有足够的功率密度，泵浦光聚焦在周期极化非线性晶体14另一周期沿X轴方向的中心，光斑半径约为100 μ m。 In order to ensure the pumping light through the vertical arms into the output mirror 16 periodically poled nonlinear crystal 14 after a further cycle has a sufficient power density, pump light is focused on another periodically poled nonlinear crystal 14 along the X-axis cycle center direction, the spot radius of about 100 μ m.
 温度调谐过程中，如图I所示，保持平面输入镜13中心、周期极化非线性晶体14沿Y轴方向中心和垂直双臂输出镜16中心都在Y = 6. 5mm直线（图中虚线）上，周期极化非线性晶体14初始温度为20°C。  The temperature of the tuning process, as shown in FIG. I, the hold input center plane mirror 13, periodically poled nonlinear crystal 14 in the Y-axis direction center of the output mirror 16 and the center of the vertical arms are in a straight line Y = 6. 5mm ( the broken line in FIG.), the initial temperature of 14 periodically poled nonlinear crystal is 20 ° C. 泵浦光从平面输入镜13透射后，入射到周期极化非线性晶体14宽度方向5. 5mm刻度位置处（对应极化周期28. O μ m)，产生第一闲频光Il波长为4. 352 μ m，泵浦光经垂直双臂输出镜16反射后，入射到周期极化非线性晶体14宽度方向7. 5mm刻度位置处（对应极化周期28. 4 μ m)，产生的第二闲频光12波长为4. 219 μ m，第一闲频光Il和第二闲频光12双波长间隔为133nm，若对该双波长闲频光使用差频过程可以获得频率为2. 173THZ的信号。 From the plane of the pump light transmissive input mirror 13, is incident to the 14 position of the width direction of the scale 5. 5mm periodically poled nonlinear crystal (corresponding to the poling period 28. O μ m), to generate a first idler light having a wavelength of 4 Il . 352 μ m, the reflected pump light 16 through the vertical arms output mirror 14 in the width direction of the scale positions on the incident 7. 5mm periodically poled nonlinear crystal (corresponding to the poling period 28. 4 μ m), produced by the first two idler light having a wavelength of 12 4. 219 μ m, the first idler and the second idler Il dual wavelength interval of light 12 133nm, if the two-wavelength light using the idle frequency difference frequency generation frequency of 2 can be obtained. 173THZ signal. 当周期极化非线性晶体14温度为200°C时，产生的第一闲频光Il和第二闲频光12的波长分别为4. 135 μ m和3. 992 μ m，双波长间隔为143nm，若对该双波长闲频光使用差频过程可以获得频率为2. 599THZ的信号。 When periodically poled nonlinear crystal 14 temperature of 200 ° C, first idler light generated frequency and a second idler Il wavelength light 12, respectively, and 4. 135 μ m 3. 992 μ m, double wavelength spacing 143nm, if the two-wavelength light using the difference frequency during idle frequency signal of frequency can be obtained in 2. 599THZ. 当周期极化非线性晶体14的温度从20°C连续变化到200°C时，第一闲频光Il波长从4. 352 μ m连续变化到4. 135 μ m,第二闲频光12波长从4. 219 μ m连续变化到3. 992 μ m,第一闲频光Il和第二闲频光12的双波长间隔从133nm变化到143nm，理论计算结果如图3所示。 When the temperature periodically poled nonlinear crystal 14 is continuously changed from 20 ° C to 200 ° C, a first idler light wavelength Il continuously changed from to 4. 352 μ m 4. 135 μ m, a second idler 12 wavelength varies continuously from the 4. 219 μ m 3. 992 μ m, the first idler and the second idler light Il dual wavelength interval 12 143nm, 133nm to change the theoretical calculation from the results shown in Fig. 若使用差频过程可以获得太赫兹信号频率变化的相应范围为2. 173-2. 599THz。 If the process can be obtained using difference frequency THz range corresponding to the frequency change 2. 173-2. 599THz.
 周期调谐过程中，如图4a所示，保持平面输入镜43、双臂垂直输出镜46中心在Y=6. 5直线上，保持泵浦光入射位置在Y = 5. 5直线上，保持周期极化非线性晶体44工作温度为20°C。  Cycle tuning process, shown in Figure 4a, the input holding plane mirror 43, an output mirror 46 vertical arms centered on Y = 6. 5 straight, holding the pump light incident position on a straight line Y = 5. 5 , periodically poled nonlinear crystal 44 to maintain an operating temperature of 20 ° C. 沿平行于Y轴方向平移控温非线性晶体400，改变与泵浦光发生相互作用的周期极化非线性晶体44的极化周期。 Direction parallel to the Y-axis direction translation temperature of the nonlinear crystal 400, the pump light polarization changes and period of the periodic polarization interaction nonlinear crystal 44 occurs. 当泵浦光从周期极化非线性晶体44宽度方向O. 5mm刻度位置处入射时，参与相互作用的周期极化非线性晶体44极化周期为27. O μ m，产生第一闲频光Il波长为4. 672 μ m ;剩余泵浦光经垂直双臂输出镜46反射后，入射至周期极化非线性晶体44宽度方向2. 5mm刻度位置处，参与相互作用的周期极化非线性晶体44极化周期为27. 4 μ m，产生第二闲频光12波长为4. 546 μ m，第一闲频光Il和第二闲频光12双波长间隔为126nm，若对该双波长闲频光使用差频过程可以获得频率为I. 780THz的信号。 When the pumping light is incident from the periodically poled nonlinear crystal 44 in the width direction O. 5mm scale position, involved in the interaction of the periodically poled nonlinear crystal 44 poling period is 27. O μ m, to generate a first idler Periodic linear polarization perpendicular to the residual pump light is output arms reflection mirror 46, is incident to the periodically poled nonlinear crystal 44 the width direction of the scale at the position of 2. 5mm, involved in the interaction of; IL wavelength 4. 672 μ m poling period of crystal 44 27. 4 μ m, to produce a second idler beam 12 having a wavelength of 4. 546 μ m, the first idler and the second idler Il dual wavelength interval of light 12 126nm, if the bis idler wavelength difference frequency generation can be obtained using a frequency of a signal I. 780THz. 如图4b所示，平移控温非线性晶体400'后，当泵浦光从周期极化非线性晶体44'宽度方向10. 5mm刻度位置处入射时，参与相互作用的周期极化非线性晶体44'极化周期为29. O μ m，产生第一闲频光Il波长为4. 015 μ m，剩余泵浦光经垂直双臂输出镜46'反射后，入射至周期极化非线性晶体44'宽度方向12. 5mm刻度位置处，参与相互作用的周期极化非线性晶体44'极化周期为29. 4 μ m，产生第二闲频光12波长为3. 873 μ m,第一闲频光Il和第二闲频光12双波长间隔为142nm，若对该双波长闲频光使用差频过程可以获得频率为2.740THZ信号。 4b, 'later, when the pump light from the periodically poled nonlinear crystal 44' translational temperature of the nonlinear crystal 400 is incident at a position of the width direction of the scale 10. 5mm, involved in the interaction of the periodically poled nonlinear crystal 44 'poling period is 29. O μ m, to generate a first idler light having a wavelength of Il 4. 015 μ m, the residual pump light is output mirror vertical arms 46' after reflection, is incident to the periodically poled nonlinear crystal 'at the position of the scale 12. 5mm width direction, the polarization of the cycle involved in the interaction of the nonlinear crystal 44' 44 poling period is 29. 4 μ m, to produce a second idler beam 12 having a wavelength of 3. 873 μ m, a first a second idler Il and 12 pairs of idler light wavelength interval of 142nm, if the two-wavelength light using the difference frequency during idle frequency signal 2.740THZ frequency can be obtained. 沿Y轴方向平移控温非线性晶体400'，当泵浦光入射位置从周期极化非线性晶体44'宽度方向O. 5_刻度位置变化至10. 5_刻度位置时，第一闲频光Il的波长变化范围为4. 672-4. 015 μ m,第二闲频光12的波长变化范围为4. 546-3. 873 μ m,闲频光双波长间隔变化范围为126-142nm，理论计算结果如图5所示。 Translation along the Y axis temperature of the nonlinear crystal 400 ', when the pump light is incident from the position of the periodically poled nonlinear crystal 44' is O. 5_ widthwise position change to the scale 10. The scale position 5_, a first idler Il wavelength range of light to 4. 672-4. 015 μ m, the second idler light wavelength range is 12 4. 546-3. 873 μ m, double idler light wavelength range of 126-142nm interval theoretical results shown in Fig. 若使用差频过程可以获得太赫兹信号频率变化的相应范围为I. 780-2. 740THz。 If the process can be obtained using difference frequency THz range corresponding to the frequency change I. 780-2. 740THz.
 腔镜调谐过程中，如图6a所示，保持平面输入镜66和周期极化非线性晶体64的Y轴方向中心在Y = 6. 5直线上，保持周期极化非线性晶体64工作温度为20°C，保持泵浦光从Y = O. 5_直线（对应周期极化非线性晶体64宽度方向O. 5_刻度位置处）入射。  Endoscopic tuning process, shown in Figure 6a, the input mirror 66 and the holding plane periodically poled nonlinear crystal Y-axis direction center 64 in a straight line Y = 6.5 on, periodically poled nonlinear crystal 64 held operating temperature is 20 ° C, holding the pump light from the straight line Y = O. 5_ (corresponding to the periodically poled nonlinear crystal 64 the width direction of the scale position O. 5_) is incident. 当垂直双臂输出镜66中心在Y = I. Omm直线上时，泵浦光从平面输入镜63透射后入射到周期极化非线性晶体64宽度方向O. 5_刻度位置处，参与作用的极化周期为27. Oym,产生第一闲频光Il的波长为4. 672 μ m ;剩余泵浦通光经垂直双臂输出镜66反射后，入射到周期极化非线性晶体64宽度方向I. 5_刻度位置处，参与作用的极化周期为27. 2 μ m,产生第二闲频光12的波长为4. 609 μ m，第一闲频光Il和第二闲频光12双波长间隔为63nm，若对该双波长闲频光使用差频过程可以获得频率为O. 878THz信号。 When the vertical center of the output mirror 66 on the arms in a straight line Y = I. Omm, the pump light incident on the mirror 63 after being transmitted at O. 5_ scale positions periodically poled nonlinear crystal 64 from the width direction of the input plane, the role participation poling period is 27. Oym, generate a first idle frequency wavelength of light Il 4. 672 μ m; after the residual pump light through the output mirror 66 vertical arms reflected incident periodically poled nonlinear crystal 64 in the width direction I. 5_ at scale position, is involved in the role of the poling period 27. 2 μ m, to produce a second idler light having a wavelength of 12 4. 609 μ m, the first idler and the second idler Il 12 dual wavelength interval of 63nm, when the dual-wavelength idler frequency generation can be obtained using a differential frequency signal O. 878THz. 如图6b所示，沿Y轴方向移动双臂垂直输出镜66'，当垂直双臂输出镜66'中心在Y = 6. 5mm直线上时，泵浦光从平面输入镜63'透射后入射到周期极化非线性晶体64'宽度方向O. 5mm刻度位置处，参与作用的极化周期为27. O μ m，产生第一闲频光Il的波长为4. 672 μ m ;剩余泵浦通光经垂直双臂输出镜66'反射后，入射到周期极化非线性晶体64'宽度方向12. 5_刻度位置处，参与作用的极化周期为29. 4 μ m，产生第二闲频光12的波长为3. 873 μ m，第一闲频光Il和第二闲频光12双波长间隔为799nm，若对该双波长闲频光使用差频过程可以获得频率为13. 247THz信号。 6b, is moved in the Y-axis direction perpendicular to the output mirror arms 66 ', the vertical arms when the output mirror 66' is centered on a straight line Y = 6. 5mm, the input pump light from the plane mirror 63 'is incident after transmission to the periodically poled nonlinear crystal 64 'O. 5mm width direction of the scale position, is involved in the role of the poling period 27. O μ m, to generate a first wavelength of the idler beam Il 4. 672 μ m; residual pump 'after reflection, is incident on the periodically poled nonlinear crystal 64' of the light passing through the output mirror 66 perpendicular to the width direction of the arms 12. 5_ scale position, is involved in the role of the poling period 29. 4 μ m, to generate a second idle frequency wavelength of light 12 is 3. 873 μ m, the first idler and the second idler Il dual wavelength interval of light 12 799nm, if the two-wavelength light using the idle frequency difference frequency generation frequency can be obtained 13. 247THz signal. 沿Y轴方向平移双臂垂直输出镜66'，当双臂垂直输出镜66'中心从Y= I.Omm移至Y = 6. 5mm位置处时，第一闲频光Il的波长保持4. 672 μ m不变，第二闲频光12的波长从4. 609 μ m连续变化至3. 873 μ m,闲频光双波长间隔从63nm变化到799nm,理论计算结果如图9所示。 Translating the arms along the Y-axis direction perpendicular to the output mirror 66 ', the vertical arms when the output mirror 66' is moved from the center of Y = Y = I.Omm 6. 5mm at a position, a first wavelength of light Il holding idler 4. 672 μ m unchanged, the second idler light wavelength is changed from 12 [mu] m 609 consecutive to 4. 3. 873 μ m, double idler light wavelength interval 799nm, 63nm to change from a theoretical calculation result is shown in FIG. 若对双波长闲频光使用差频过程可以获得太赫兹信号频率变化的相应范围为O.878-13. 247THz。 If dual wavelength idler light can be obtained using difference frequency generation THz frequency variation range corresponds O.878-13. 247THz.
98. 7% il. 3-1. 5 μ m)和对闲频光高透射率膜（T > 95. 7 % @4. 0-4. 8 μ m) (45°角入射条件)，直角全反射棱镜87材料为CaF2，斜面抛光后镀对信号光、闲频光和泵浦光减反射率膜(R < 1% §1. 3-1. 5 μ m&R < I. 5% @4. 0-4. 8 μ m&R < 2 % il. 064 μ m)。 98. 7% il. 3-1. 5 μ m) of the idler light and the high transmittance of the film (T> 95. 7% @ 4. 0-4. 8 μ m) (45 ° angle of incidence condition), at right angles total reflection prism 87 in CaF2 material, plating the bevel polishing signal light, idler light and pumping light reflectance reducing film (R <1% §1. 3-1. 5 μ m & R <I. 5% @ 4. 0-4. 8 μ m & R <2% il. 064 μ m). 这样，光参量振荡器的振荡腔对信号光单谐振。 Thus, the optical parametric oscillator cavity resonance oscillations of the single light signal. 在平面输入镜83和平面输出镜86之间设置的周期极化非线性晶体14的材料为MgO:PPLN，其尺寸为30mm(长）X 13mm(宽）X Imm(厚），其极化结构为多周期极化结构，极化周期从27. 5变化到28. 3 μ m，每两个相邻周期相差O. I μ m，每个周期区域的宽度为1_，相邻周期区域相隔0.5_。 Periodically poled nonlinear crystal material between the planar mirror 83 and the input plane output mirror 86 is provided to 14 MgO: PPLN, a size of 30mm (length) X 13mm (width) X Imm (thick), which polarization structure periodically poled structure of a multi-polarization. 5 to 27. a cycle from 28. 3 μ m, each two adjacent periods differ O. I μ m, the width of each region is 1_ period, the adjacent periodic areas spaced 0.5 _. 多周期极化非线性晶体84两端面镀对信号光、闲频光和泵浦光高透射率膜（R< 1% @1.3-1. 5 μ m&R < I. 5% §4. 0-4. 8 μ m&R < 2% @1.064μπι)。 Multi-cycle nonlinear crystal polarization plate 84 both end faces of the optical signal, high idler light and pumping light transmittance of the film (R <1% @ 1.3-1. 5 μ m & R <I. 5% §4. 0-4 . 8 μ m & R <2% @ 1.064μπι). 周期极化非线性晶体84工作温度由控温炉85控制，工作温度范围为20-200°C，控温炉85采用PtlOO作为温度传感器，控制精度为±0. 1°C。 Periodically poled nonlinear crystal 84 by the operating temperature of the furnace temperature control 85, temperature range of 20-200 ° C, the furnace temperature PtlOO employed as the temperature sensor 85, the control precision is ± 0. 1 ° C.
 下面为了叙述方便，在周期极化非线性晶体84端面宽度方向加上均匀刻度（如图8所示），刻度范围为0-13mm，其中Omm刻度对应极化周期27. 5 μ m处，13mm刻度对应极化周期28. 3 μ m处，刻度与周期极化非线性晶体84同步移动；谐振腔右端加上坐标轴，X轴方向沿周期极化非线性晶体84的长度方向，Y轴方向沿周期极化非线性晶体84的宽度方向，坐标轴固定不动，其中使用的周期极化非线性晶体84的极化结构为多周期极化结构。  For convenience of description below, plus a uniform scale (Figure 8) in the end face width direction of the nonlinear crystal 84 periodically poled, scale range of 0-13mm, wherein Omm poling period corresponding to the scale 27. 5 μ m at 13mm poling period corresponding to the scale 28. 3 μ m, the scale and the periodically poled nonlinear crystal 84 the synchronous mobile; plus right end of the resonator axis, X-axis direction along the longitudinal direction 84 of the periodically poled nonlinear crystal, Y-axis direction along a periodically poled nonlinear crystal 84 in the width direction of the coordinate axis is fixed, wherein a periodically poled nonlinear crystal polarization structure 84 is a multi-periodically poled structure.
 1064nm泵浦光从平面输入镜83透射后，先入射到周期极化非线性晶体84某一周期上，产生第一闲频光II，第一闲频光Il从平面输出镜86透射出去；剩余泵浦光再经直角全反射棱镜87反射后，入射到周期极化非线性晶体84另一周期，产生第二闲频光12，第二闲频光12经平面输入镜83反射后，由平面输出镜86透射出去。  After the 1064nm pump light is transmitted from the input plane mirror 83, is incident on the first 84 cycles a periodically poled nonlinear crystal to generate a first idler II, the first idler Il transmission from the plane output mirror 86 after the remaining pump light reflected at a right angle and then by the total reflection prism 87, is incident on the periodic cycle of the nonlinear crystal 84 the other polarized light 12 generates a second idler, the second idler light 1283 reflected by the input mirror plane; out transmissive output mirror 86 out of the plane. 泵浦光经过光学耦合透镜组82，聚焦到周期极化非线性晶体84另一周期的X轴方向的中心，光斑半径约为200 μ m。 Pump light through the optical coupling lens group 82, a focus to another cycle period of the nonlinear crystal 84 poled central X-axis direction, the spot radius of about 200 μ m.
 温度调谐过程中，调整光路，使泵浦光从平面输入镜83透射后，先入射到周期极化非线性晶体84宽度方向5_刻度位置处（对应极化周期27. 8 μ m)，产生第一闲频光Il ；剩余泵浦光经直角全反射棱镜87反射后，入射到周期极化非线性晶体84宽度方向8_刻度位置处（对应极化周期28.0 μ m)，产生第二闲频光12。  The temperature of the tuning process, the optical path to adjust the position of the scale at a 5_ pump light input from the transmission plane mirror 83, is incident on the first periodically poled nonlinear crystal 84 in the width direction (corresponding to the poling period 27. 8 μ m ), generating a first idler Il; remaining pump light reflected by the right angle reflection prism 87, is incident to the periodically poled nonlinear crystal 84 in the width direction of the scale positions 8_ (poling period corresponding to 28.0 μ m), produced The second idler 12. 改变周期极化非线性晶体84工作温度，当周期极化非线性晶体84工作温度从20°C变化到200°C时，第一闲频光11波长从4. 417 μ m变化到4. 205 μ m,第二闲频光12波长从4. 352 μ m变化到4. 135 μ m,第一闲频光Il和第二闲频光12双波长间隔从65nm变化到70nm。 Periodically poled nonlinear crystal 84 to change the operating temperature when the periodically poled nonlinear crystal 84 the operating temperature from 20 ° C to 200 ° C, a first idler light 11 from a change in wavelength to 4. 417 μ m 4.205 μ m, the second idler light 12 from a change in wavelength to 4. 352 μ m 4. 135 μ m, the first idler and the second idler Il dual wavelength interval of light 12 changes from 65nm to 70nm.
 周期调谐过程中，保持周期极化非线性晶体84工作温度为20°C。  during the tuning period, periodically poled nonlinear crystal 84 to maintain an operating temperature of 20 ° C. 调整光路，使泵浦光从平面输入镜83透射后，先入射到周期极化非线性晶体84宽度方向O. 5mm刻度位置处（对应极化周期27. 5 μ m)，产生第一闲频光Il波长为4. 513 μ m ;剩余泵浦光经直角全反射棱镜87反射后，入射到周期极化非线性晶体84宽度方向3. 5_刻度位置处（对应极化周期27. 7 μ m)，产生第二闲频光12波长为4. 449 μ m。 Adjust the optical path, the pump light input from the transmission plane mirror 83, is incident at the first periodically poled nonlinear crystal 84 O. 5mm width direction of the scale positions (corresponding to the poling period 27. 5 μ m), to generate a first idler Il light having a wavelength of 4. 513 μ m; the remaining pump light reflected by the right angle reflection prism 87, the incident position of the scale 3. 5_ periodically poled nonlinear crystal 84 in the width direction (corresponding to the poling period 27. 7 μ m), generates a second idler beam 12 having a wavelength of 4. 449 μ m. 沿Y轴方向平移控温非线性晶体800，使泵浦光从平面输入镜83透射后，先入射到周期极化非线性晶体84宽度方向9. 5mm刻度位置处（对应极化周期28. I μ m)，产生第一闲频光Il波长为4. 319 μ m ;剩余泵浦光经直角全反射棱镜87反射后，入射到周期极化非线性晶体84宽度方向12. 5_刻度位置处（对应极化周期28. 3 μ m)，产生第二闲频光12波长为4. 253 μ m。 Translation along the Y axis temperature of the nonlinear crystal 800, so that the pumping light is transmitted from the input plane mirror 83, is incident on the first periodically poled nonlinear crystal 84 in the width direction at a position 9. 5mm scale (corresponding to the poling period 28. I μ m), to generate a first idler light having a wavelength of Il 4. 319 μ m; the remaining pump light reflected by the right angle reflection prism 87, incident on the periodic nonlinear polarization direction of the crystal 12. the width 84 of the scale positions 5_ (corresponding to the poling period 28. 3 μ m), to generate a second idler beam 12 having a wavelength of 4. 253 μ m. 周期调谐时，第一闲频光Il波长从4. 513 μ m变化到4. 319 μ m,第二闲频光12波长从4. 449 μ m变化到4. 253 μ m,第一闲频光Il和第二闲频光12双波长间隔从64nm变化到66nm。 When tuning cycle, a first idler light wavelength Il changed from to 4. 513 μ m 4. 319 μ m, 12 second idler light wavelength is changed from the 4. 449 μ m 4. 253 μ m, a first idler Il idler light and the second light 12 is changed from the two-wavelength spacing 64nm to 66nm. 整个周期调谐过程中，控温非线性晶体800的位置不能连续变化，需要具体设定控温非线性晶体800的位置，使泵浦光从平面输入镜83透射后，入射到周期极化非线性晶体84的不同极化周期区域位置Y轴方向的中心。 The entire cycle of the tuning process, the position of the temperature of the nonlinear crystal 800 can not be continuously changed, it is necessary to set the position of the specific temperature of the nonlinear crystal 800, so that the input pump light is transmitted from the plane mirror 83, is incident on the periodically poled nonlinear Y-axis direction position of the central region of the crystal 84 in different poling period.
 腔镜调谐过程中，保持周期极化非线性晶体84工作温度为20°C。  Endoscopic tuning process, periodically poled nonlinear crystal 84 to maintain an operating temperature of 20 ° C. 调整光路，使泵浦光从平面输入镜83透射后，先入射到周期极化非线性晶体84宽度方向O. 5mm刻度位置处（对应极化周期27. 5 μ m)，产生第一闲频光Il波长为4. 513 μ m ;剩余泵浦光经直角全反射棱镜87反射后，入射到周期极化非线性晶体84宽度方向2_刻度位置处（对应极化周期27. 6 μ m)，产生第二闲频光12波长为4. 481 μ m。 Adjust the optical path, the pump light input from the transmission plane mirror 83, is incident at the first periodically poled nonlinear crystal 84 O. 5mm width direction of the scale positions (corresponding to the poling period 27. 5 μ m), to generate a first idler Il light having a wavelength of 4. 513 μ m; the remaining pump light reflected by the right angle reflection prism 87, the incident position of the scale 84 in the width direction 2_ periodically poled nonlinear crystal (corresponding to the poling period 27. 6 μ m) generating a second idler beam 12 having a wavelength of 4. 481 μ m. 沿X轴方向平移直角全反射棱镜87，使剩余泵浦光经直角全反射棱镜87反射后，入射到周期极化非线性晶体84宽度方向12. 5mm刻度位置处（对应极化周期28. 3 μ m)，产生第二闲频光12波长为4. 253 μ m。 Translation along the X axis direction at a right angle reflection prism 87, the remaining pump light reflected by the right angle reflection prism 87, is incident to the periodically poled nonlinear crystal 84 in the width direction 12. 5mm scale positions (corresponding to the poling period 28.3 μ m), to generate a second idler beam 12 having a wavelength of 4. 253 μ m. 腔镜调谐时，第一闲频光Il波长保持4. 513 μ m不变，第二闲频光12波长从4. 481 μ m变化到4. 253 μ m，第一闲频光Il和第二闲频光12双波长间隔从32nm变化到260nm。 When tuning mirror, a first idler light wavelength Il remains unchanged 4. 513 μ m, 12 second idler light wavelength is changed from the 4. 481 μ m 4. 253 μ m, the first and second idler Il 12 pairs of two idler light wavelength interval varies from 32nm to 260nm. 整个腔镜调谐过程中，直角全反射棱镜87的位置不能连续变化，需要具体设定直角全反射棱镜87的位置，使剩余泵浦光从直角全反射棱镜87反射后，入射到周期极化非线性晶体84的不同极化周期区域位置Y轴方向的中心。 Endoscopic entire tuning process, the position of the right-angle reflection prism 87 can not change continuously, it is necessary to set the specific position of the right-angle reflection prism 87, the remaining pump light reflected at a right angle from the total reflection prism 87, is incident on the non-periodically poled a central region different from the Y-axis direction linear polarization of crystal 84 cycles.
 虽然本发明已以实施例揭露如上，然其并非用以限定本发明，任何所属技术领域中具有通常知识者，在不脱离本发明的精神和范围内，当可作些许的更动与润饰，故本发明的保护范围当视权利要求范围所界定的为准。  Although the present invention has been disclosed in the above embodiments, they are not intended to limit the present invention, any skilled in the art having ordinary knowledge, without departing from the spirit and scope of the present invention, various omissions, substitutions can be made to and variations, so that the scope of the present invention is best defined by the scope of the claims and their equivalents.
1. 一种宽调谐范围双波长输出光参量振荡器，包括： 泵浦源、光学耦合透镜组、平面输入镜、周期极化非线性晶体、控温炉和垂直双臂输出镜；所述垂直双臂输出镜由两个互相垂直的平面镜构成；所述周期极化非线性晶体的外部套置控温炉，形成控温非线性晶体；所述平面输入镜和垂直双臂输出镜构成光参量振荡器的振荡腔； 其中该泵浦源、光学耦合透镜组、平面输入镜、控温非线性晶体和垂直双臂输出镜依次排列于同一光路上； 其中泵浦源发出的泵浦光经光学耦合透镜组聚焦再从平面输入镜透射后，先入射到周期极化非线性晶体的某一周期上产生某一波长的第一闲频光，第一闲频光由垂直双臂输出镜的上臂透射出去；剩余泵浦光经垂直双臂输出镜反射后，再入射到周期极化非线性晶体的另一周期上产生另一波长的第二闲频光，第二闲频光经平 A wide tuning range of dual-wavelength output optical parametric oscillator, comprising: a pump source optically coupled to the lens group, the input mirror plane, periodically poled nonlinear crystal, and the vertical arms temperature furnace output mirror; the vertical output mirror consists of two arms perpendicular to each other plane mirror; furnace temperature sleeved outside the periodic polarization nonlinear crystal, nonlinear crystals forming temperature; the input mirror and the plane perpendicular to the arms constituting the optical parametric output mirror oscillation of the oscillator cavity; wherein the pump source, the optical coupling lens group, the input plane mirror, a nonlinear crystal temperature and the output mirror are sequentially arranged in the vertical arms on the same optical path; wherein pump light emitted by the pump source optically coupling the focusing lens group from the flat input mirror and then transmitting, to generate a first idle incident fundamental light of a certain wavelength on a period of the periodic polarization of the nonlinear crystal, a first idler arms by the vertical arm of the output mirror out transmission; residual pump light is reflected back vertical arms output mirror, is incident to generate a second pilot light of another wavelength busy on another cycle periodically poled nonlinear crystal, the second idler tricot 输入镜反射后再由垂直双臂输出镜的下臂透射出去，由此获得双波长输出，构成双波长输出光参量振荡器； 其中光参量振荡器的振荡腔是以信号光作为振荡光而输出双波长闲频光，信号光在光参量振荡器的振荡腔内沿U形路径往返振荡。 Input mirror and then transmitted by the lower vertical arm of the arms out of the output mirror, thereby obtaining a dual wavelength output, constituting the dual-wavelength output optical parametric oscillator; wherein the optical parametric oscillator cavity is an oscillation light signal as an oscillation light output idler dual-wavelength, the signal light and from the cavity of the oscillation in the oscillating U-shaped path along the optical parametric oscillator.
2.如权利要求I所述的宽调谐范围双波长输出光参量振荡器，其中平面输入镜材料为石英，表面镀对泵浦光高透射率和对信号光、闲频光高反射率膜，其中高透射率T为97. 2%§1. 064 μ m,高反射率R > 99. 7 % @1. 3-1. 6 μ m&R > 98. 2% §3. 6-4. 8 μ m。 2. I claim wide tuning range of the dual wavelength optical parametric oscillator output, wherein the input plane mirror material is quartz, plated high pump light and the signal light transmissivity, high reflectance idler film, wherein the high transmittance T of 97. 2% §1. 064 μ m, a high reflectance R> 99. 7% @ 1. 3-1. 6 μ m & R> 98. 2% §3. 6-4. 8 μ m.
3.如权利要求I所述的宽调谐范围双波长输出光参量振荡器，其中垂直双臂输出镜材料为CaF2，表面镀对泵浦光、信号光高反射率和对闲频光高透射率膜，其中高反射率R >98. 7% §1. 064 μ m&R > 98. 7% il. 3-1. 6 μ m,高透射率T > 95. 7% §3. 6-4. 8 μ m,皆为45。 3. I claim wide tuning range of the dual wavelength optical parametric oscillator output, wherein the output of the vertical arms is in CaF2 lens material, plated pump light, the signal light and a high reflectance for light having a high transmittance idle frequency film, wherein the high reflectivity R> 98. 7% §1. 064 μ m & R> 98. 7% il. 3-1. 6 μ m, a high transmittance T> 95. 7% §3. 6-4. 8 μ m, are all 45. 入射角。 Angle of incidence.
4.如权利要求I所述的宽调谐范围双波长输出光参量振荡器，其中在平面输入镜和双臂垂直输出镜之间设置的周期极化非线性晶体的材料为MgO:PPLN，其尺寸为30mmX 13mmX 1mm,其极化结构为扇形周期极化结构,极化周期从26. 9-29. 5 μ m连续变化，该周期极化非线性晶体两端面镀对信号光、闲频光和泵浦光减反射率膜，其中减反射率R< 1% §1. 3-1. 6 μ m&R < I. 5% §3. 3-4. 8 μ m&R < 2% il. 064 μ m。 4. I claim wide tuning range of the dual wavelength optical parametric oscillator output requirements, periodically poled nonlinear crystal material, wherein between the input mirror and the plane mirror is disposed in the vertical output arms to MgO: PPLN, the size is 30mmX 13mmX 1mm, its polarization periodically poled structure of a sector structure, the poling period changes continuously from 26. 9-29. 5 μ m, both end faces of the non-linear crystal polarized period plating signal light, idler light, of the pump light antireflection film, wherein the reflectance reducing R <1% §1. 3-1. 6 μ m & R <I. 5% §3. 3-4. 8 μ m & R <2% il. 064 μ m.
6.如权利要求I所述的宽调谐范围双波长输出光参量振荡器，其中第一闲频光和第二闲频光的波长调谐方式是通过改变周期极化非线性晶体的温度实现温度调谐，或通过平移控温非线性晶体实现周期调谐，或通过平移垂直双臂输出镜实现腔镜调谐。 6. I claim wide tuning range of the dual wavelength optical parametric oscillator output, wherein the first idler light and the wavelength tunable light idler second embodiment is achieved by changing the temperature of the temperature tuned periodically poled nonlinear crystal or cycle realized by the translational temperature tuned nonlinear crystal, or achieved by translating the vertical arms tuning mirror output mirror.
7.如权利要求I所述的宽调谐范围双波长输出光参量振荡器，其中的泵浦源是使用侧泵激光头或端泵激光晶体。 7. The wide tuning range I of the dual wavelength optical parametric oscillator output, wherein the pump source is a pump laser head or the use-side end pump laser crystal.
8.如权利要求I所述的宽调谐范围双波长输出光参量振荡器，其中的泵浦源波长为1064nm 或532nm。 I as claimed in claim 8. The wide tuning range of the dual-wavelength output optical parametric oscillator, wherein the pump source wavelength of 1064nm or 532nm.
9.如权利要求I所述的宽调谐范围双波长输出光参量振荡器，其中使用的周期极化非线性晶体的材料是PPLN、PPLT, PPKTP, PPKTA, PPRTA 或MgO:PPLT。 I as claimed in claim 9 wide tuning range of the dual wavelength optical parametric oscillator output, wherein the period of use of the nonlinear crystal material polarization is PPLN, PPLT, PPKTP, PPKTA, PPRTA or MgO: PPLT.
10.如权利要求I所述的宽调谐范围双波长输出光参量振荡器，其中使用的周期极化非线性晶体的极化结构为多周期极化结构。 I as claimed in claim 10. The wide tuning range of the dual-wavelength output optical parametric oscillator, wherein the periodic structure of the polarization of the nonlinear crystal is used for the polarization of the polarization structure of multi-cycle.

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