CN104729998A - Atmosphere visibility measurement device based on optical cavity ring down spectroscopy technology - Google Patents
Atmosphere visibility measurement device based on optical cavity ring down spectroscopy technology Download PDFInfo
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- 238000005259 measurement Methods 0.000 title claims abstract description 30
- 238000005516 engineering process Methods 0.000 title claims abstract description 11
- 238000000180 cavity ring-down spectroscopy Methods 0.000 title claims description 10
- 230000003287 optical effect Effects 0.000 title abstract description 17
- 238000002834 transmittance Methods 0.000 claims description 3
- 230000007423 decrease Effects 0.000 claims 1
- 238000007747 plating Methods 0.000 claims 1
- 238000002310 reflectometry Methods 0.000 abstract description 31
- 230000008033 biological extinction Effects 0.000 abstract description 21
- 239000000443 aerosol Substances 0.000 abstract description 14
- 238000010168 coupling process Methods 0.000 abstract description 8
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- 230000005540 biological transmission Effects 0.000 description 16
- 239000000835 fiber Substances 0.000 description 12
- 238000010521 absorption reaction Methods 0.000 description 8
- 239000013307 optical fiber Substances 0.000 description 5
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Abstract
本发明提供一种基于光腔衰荡光谱技术的大气能见度测量装置,涉及气象观测装置。它包括呈马鞍状的壳体,一对高反射率腔镜位于壳体凹口两侧形成衰荡腔,激光发射器发出激光依次穿过偏振片、1/4波片和耦合透镜射入第一面高反射率腔镜后,一路由第一面高反射率腔镜反射通过1/4波片射入偏振片反射输出,另一路在衰荡腔中振荡后穿过第二面高反射率腔镜传输给光电倍增管,通过数据采集卡传输给计算机。本发明解决了现有技术中对大气能见度的测量待测样本取样与实际有偏差造成测量误差的技术问题。本发明的有益效果为:开放式衰荡腔与大气直接接触,可综合测量气体分子、气溶胶、雨水导致的大气消光系数变化,实现对大气能见度的准确测量。
The invention provides an atmospheric visibility measurement device based on optical cavity ring-down spectrum technology, and relates to a meteorological observation device. It consists of a saddle-shaped housing, a pair of high-reflectivity cavity mirrors are located on both sides of the housing notch to form a ring-down cavity, and the laser emitter emits laser light through the polarizer, 1/4 wave plate and coupling lens in turn and enters the first After one high-reflectivity cavity mirror, one route is reflected by the first high-reflectivity cavity mirror through the 1/4 wave plate and enters the polarizer reflection output, and the other route passes through the second high-reflectivity after oscillating in the ring-down cavity The cavity mirror is transmitted to the photomultiplier tube and transmitted to the computer through the data acquisition card. The invention solves the technical problem in the prior art that there is a deviation between the sampling of the sample to be tested and the actual measurement of the atmospheric visibility, which causes measurement errors. The beneficial effect of the present invention is that: the open ring-down cavity is in direct contact with the atmosphere, and can comprehensively measure changes in atmospheric extinction coefficients caused by gas molecules, aerosols, and rain, thereby realizing accurate measurement of atmospheric visibility.
Description
技术领域technical field
本发明涉及气象观测装置,尤其是设计一种利用光腔衰荡光谱技术对大气能见度的测量装置。The invention relates to a meteorological observation device, in particular to a device for measuring atmospheric visibility by using optical cavity ring-down spectrum technology.
背景技术Background technique
作为气象观测的要素之一,大气能见度是表征大气透明度的物理量。大气能见度的测量不仅用于日常气象部门的天气分析,更广泛用于高速公路、航空、航海等交通运输部门、军事等领域。同时根据《QX/T 113-2010霾的观测和预报等级》,大气能见度是雾霾等级的主要判断依据,因此研究大气能见度测量装置具有十分重要的意义。As one of the elements of meteorological observation, atmospheric visibility is a physical quantity that characterizes the transparency of the atmosphere. The measurement of atmospheric visibility is not only used in the weather analysis of the daily meteorological department, but also widely used in highways, aviation, navigation and other transportation departments, military and other fields. At the same time, according to "QX/T 113-2010 Haze Observation and Forecast Grades", atmospheric visibility is the main basis for judging haze grades, so it is of great significance to study atmospheric visibility measurement devices.
能见度作为一个复杂的物理量,主要取决于大气消光系数。消光系数是光波在大气传输过程中,由于各种因素造成的能量衰减,是由大气对光辐射吸收、散射所引起的,包括分子吸收、分子散射、气溶胶吸收、气溶胶散射、雨水吸收和雨水散射。As a complex physical quantity, visibility mainly depends on the atmospheric extinction coefficient. The extinction coefficient is the energy attenuation caused by various factors during the transmission of light waves in the atmosphere, which is caused by the absorption and scattering of light radiation by the atmosphere, including molecular absorption, molecular scattering, aerosol absorption, aerosol scattering, rain absorption and Rain scatter.
目前大气能见度测量装置主要有透射式能见度仪和散射式能见度仪。透射式能见度仪是基于光辐射在大气传输中的透过率测量。透射仪一般分为双端式和单端式两种。双端式是将发射器和接收器装于基线的两端。单端式是将发射器和接收器装于基线的通端,在基线的另一端装有反射器,从而使得测量光路变为往返式光程。透射式能见度仪直接测量大气消光系数,但是为保证测量准确度,往往需要较长的基线,同时为了能测量低能见度和高能见度,需要采用双基线系统,因此透射式能见度仪对场地要求较高。散射式能见度仪发出红外光辐射,并探测某一方向散射信号,并根据具体角度上散射信号与总散射量的关系来确定总散射系数,最后按公式反演能见度。散射式能见度仪可分为前向散射仪和后向散射仪。散射式能见度仪是目前使用最广泛的能见度仪,但是散射式能见度仪只测量大气散射系数,没有测量大气吸收系数;而在我国不同地区,大气吸收系数和大气散射系数的比值都不同的,并且有时候大气吸收系数是可与大气散射系数相比拟的,因此散射式能见度仪存在较大的测量误差。At present, the atmospheric visibility measurement devices mainly include the transmission type visibility meter and the scattering type visibility meter. Transmissive visibility meters are based on the measurement of the transmittance of light radiation in the atmosphere. Transmissometers are generally divided into two types: double-ended and single-ended. The double-ended type is to install the transmitter and receiver at both ends of the baseline. The single-ended type is to install the transmitter and receiver on the open end of the baseline, and install a reflector on the other end of the baseline, so that the measurement optical path becomes a round-trip optical path. The transmission-type visibility meter directly measures the atmospheric extinction coefficient, but in order to ensure the measurement accuracy, a longer baseline is often required. At the same time, in order to measure low visibility and high visibility, a double-baseline system is required, so the transmission-type visibility meter has higher requirements for the site . The scattering visibility meter emits infrared light radiation, detects the scattering signal in a certain direction, and determines the total scattering coefficient according to the relationship between the scattering signal and the total scattering amount at a specific angle, and finally inverts the visibility according to the formula. Scattering visibility meter can be divided into forward scatter meter and back scatter meter. The diffuse visibility meter is the most widely used visibility meter at present, but the diffuse visibility meter only measures the atmospheric scattering coefficient and does not measure the atmospheric absorption coefficient; in different regions of my country, the ratio of the atmospheric absorption coefficient to the atmospheric scattering coefficient is different, and Sometimes the atmospheric absorption coefficient can be compared with the atmospheric scattering coefficient, so the scattering visibility meter has a large measurement error.
光腔衰荡光谱技术可直接测量消光系数,目前光腔衰荡光谱技术已被用于测量气溶胶的消光系数,是通过将大气中气溶胶抽入衰荡腔进行测量。中国专利申请公布号CN103616334A,申请公布日2014年3月5日,名称为“一种光腔衰荡气溶胶消光仪”和中国专利申请公布号CN103712914A,申请公布日2014年4月9日,名称为“一种同时检测气溶胶消光和散射系数的激光光腔衰荡光谱仪”的公开方案,都是通过将大气中气溶胶抽入衰荡腔进行气溶胶消光系数的测量的技术方案。能见度与大气总的消光系数相关,大气总的消光系数不只气溶胶消光系数,还应包含气体分子消光系数和雨水导致的消光系数,因此用气溶胶消光仪测量能见度存在一定的测量误差。中国专利申请公布号CN104062236A,申请公布日2014年9月24日,名称为“一种基于腔衰荡技术的大气能见度检测装置”的发明专利公开文件,提供了另外一种装置。该装置包括依次设置的光源、导入光纤、光纤谐振腔、导出光纤、光电探测器以及用于将光损耗数据进行计算得到被探测样本能见度值的数据处理单元。导入光纤与光纤谐振腔之间设置有导入准直器,光纤谐振腔和导出光纤之间设置有导出准直器,光纤谐振腔包括第一耦合器、特种光纤以及第二耦合器,第一耦合器的输入端与导入光纤连接,第一耦合器的输出端与特种光纤的输入端连接;特种光纤的输出端与第二耦合器的输入端连接;第二耦合器的输出端分别与第一耦合器的输入端和光学探测器连接;特种光纤用于使光波与外界环境中的待测样本接触和吸收。数据处理单元按照谐振腔的特性得出光波在谐振腔内的损耗,通过光损耗最终确定被测样本的能见度数值。该装置在光源和谐振腔之间、谐振腔和光学探测器之间用光纤连接,并采用特种光纤用于使光波与外界环境中的待测样本接触和吸收。但是存在以下问题:需要利用特种光纤,不但成本高,而且使用也不方便;外界环境中的待测样本通过特种光纤吸收还是与实际的待测样本有偏差,造成测量误差。Optical cavity ring-down spectroscopy technology can directly measure the extinction coefficient. At present, optical cavity ring-down spectroscopy technology has been used to measure the extinction coefficient of aerosols, which is measured by pumping aerosols in the atmosphere into the ring-down cavity. Chinese patent application publication number CN103616334A, application publication date March 5, 2014, titled "An optical cavity ring-down aerosol extinction instrument" and Chinese patent application publication number CN103712914A, application publication date April 9, 2014, title The public scheme of "a laser cavity ring-down spectrometer for simultaneous detection of aerosol extinction and scattering coefficient" is a technical scheme for measuring the aerosol extinction coefficient by pumping the aerosol in the atmosphere into the ring-down cavity. Visibility is related to the total extinction coefficient of the atmosphere. The total extinction coefficient of the atmosphere is not only the aerosol extinction coefficient, but also includes the extinction coefficient of gas molecules and the extinction coefficient caused by rain. Therefore, there is a certain measurement error in measuring visibility with an aerosol extinction meter. Chinese patent application publication number CN104062236A, the application publication date is September 24, 2014, and the invention patent publication titled "An Atmospheric Visibility Detection Device Based on Cavity Ring-Down Technology" provides another device. The device includes sequentially arranged light source, lead-in fiber, fiber resonator, lead-out fiber, photodetector and a data processing unit for calculating the light loss data to obtain the visibility value of the detected sample. A lead-in collimator is set between the lead-in fiber and the fiber resonator, a lead-out collimator is set between the fiber resonator and the lead-out fiber, the fiber resonator includes a first coupler, a special fiber and a second coupler, the first coupler The input end of the coupler is connected to the input fiber, the output end of the first coupler is connected to the input end of the special fiber; the output end of the special fiber is connected to the input end of the second coupler; the output end of the second coupler is respectively connected to the first The input end of the coupler is connected with the optical detector; the special optical fiber is used to make the light wave contact and absorb the sample to be measured in the external environment. The data processing unit obtains the loss of the light wave in the resonator according to the characteristics of the resonator, and finally determines the visibility value of the measured sample through the light loss. The device is connected by optical fibers between the light source and the resonant cavity, between the resonant cavity and the optical detector, and uses a special optical fiber to make the light wave contact and absorb the sample to be measured in the external environment. However, there are the following problems: the need to use special optical fibers, which is not only costly, but also inconvenient to use; the absorption of the sample to be tested in the external environment through the special optical fiber still deviates from the actual sample to be tested, resulting in measurement errors.
发明内容Contents of the invention
为了解决现有技术存在的对大气能见度的测量待测样本取样与实际有偏差造成测量误差的技术问题,本发明提供一种基于光腔衰荡光谱技术的大气能见度测量装置,衰荡腔为开放式结构,直接与大气接触,综合测量气体分子、气溶胶、雨水导致的大气消光系数变化,实现对大气能见度的准确测量。In order to solve the technical problem in the prior art that there is a deviation between the sampling of the sample to be tested and the actual measurement error in the measurement of atmospheric visibility, the present invention provides an atmospheric visibility measurement device based on optical cavity ring-down spectroscopy. The ring-down cavity is an open It is in direct contact with the atmosphere, comprehensively measures changes in the atmospheric extinction coefficient caused by gas molecules, aerosols, and rain, and realizes accurate measurement of atmospheric visibility.
本发明的技术方案是:一种基于光腔衰荡光谱技术的大气能见度测量装置,它包括呈马鞍状密封腔体结构的壳体,壳体腔体内设有激光发射器、偏振片、1/4波片、耦合透镜、高反射率腔镜、光电倍增管和数据采集卡,高反射率腔镜有一对位于壳体凹口两侧形成衰荡腔,激光发射器发出的激光依次穿过偏振片、1/4波片和耦合透镜射入第一面高反射率腔镜,激光分成两路,一路激光由第一面高反射率腔镜反射通过1/4波片射入偏振片反射输出,另一路激光在衰荡腔中来回振荡后穿过第二面高反射率腔镜传输给光电倍增管,光电倍增管通过数据采集卡电连接有计算机。采用开放式衰荡腔,与大气直接接触,综合测量气体分子、气溶胶、雨水导致的大气消光系数变化,实现对大气能见度的准确测量。The technical solution of the present invention is: an atmospheric visibility measurement device based on optical cavity ring-down spectroscopy, which includes a housing with a saddle-shaped sealed cavity structure, and a laser transmitter, a polarizer, a 1/4 Wave plate, coupling lens, high-reflectivity cavity mirror, photomultiplier tube and data acquisition card. A pair of high-reflectivity cavity mirrors are located on both sides of the housing notch to form a ring-down cavity. The laser emitted by the laser transmitter passes through the polarizer in turn , 1/4 wave plate and coupling lens are injected into the first high-reflectivity cavity mirror, and the laser is divided into two paths. One path of laser light is reflected by the first high-reflectivity cavity mirror and injected into the polarizer through the 1/4 wave plate to reflect and output. The other laser beam oscillates back and forth in the ring-down cavity and transmits it to the photomultiplier tube through the second high-reflectivity cavity mirror, and the photomultiplier tube is electrically connected to the computer through the data acquisition card. It adopts an open ring-down cavity, which is in direct contact with the atmosphere, and comprehensively measures the changes in the atmospheric extinction coefficient caused by gas molecules, aerosols, and rainwater to achieve accurate measurement of atmospheric visibility.
作为优选,壳体还设有腔镜盒,腔镜盒相对应的侧壁分别设有Ⅰ透光口和Ⅱ透光口,高反射率腔镜固定腔镜盒腔体内位于Ⅰ透光口和Ⅱ透光口之间。避免高反射率腔镜受大气污染,确保测量精确。Preferably, the casing is also provided with a cavity mirror box, and the corresponding side walls of the cavity mirror box are respectively provided with I light transmission port and II light transmission port, and the high reflectivity cavity mirror is fixed in the cavity of the cavity mirror box. Ⅱ Between the light-transmitting ports. Prevent the high reflectivity cavity mirror from being polluted by the atmosphere to ensure accurate measurement.
作为优选,腔镜盒设有镀高透膜的窗口片,窗口片覆盖Ⅰ透光口。Preferably, the cavity mirror box is provided with a window plate coated with a high-transparency film, and the window plate covers the light transmission port I.
作为优选,腔镜盒顶部靠近Ⅱ透光口设有进气口;通过向进气口充入高纯氮气,在高反射率腔镜表面形成气帘,保护高反射率腔镜不受大气污染。As a preference, an air inlet is provided on the top of the cavity mirror box close to the light transmission port II; by filling the inlet with high-purity nitrogen, an air curtain is formed on the surface of the high-reflectivity cavity mirror to protect the high-reflectivity cavity mirror from atmospheric pollution.
与现有技术相比,本发明的有益效果是:衰荡腔为开放式结构,与大气直接接触,可综合测量气体分子、气溶胶、雨水导致的大气消光系数变化,实现对大气能见度的准确测量。Compared with the prior art, the beneficial effect of the present invention is that the ring-down cavity is an open structure, directly in contact with the atmosphere, and can comprehensively measure the change of the atmospheric extinction coefficient caused by gas molecules, aerosols, and rainwater, and realize accurate measurement of atmospheric visibility. Measurement.
附图说明Description of drawings
附图1为本发明示意图;Accompanying drawing 1 is schematic diagram of the present invention;
附图2为腔镜盒剖视图。Accompanying drawing 2 is a sectional view of the endoscope box.
图中:1-激光发射器;2-反射镜;3-偏振片;4-1/4波片;5-耦合透镜;6-腔镜盒;7-高反射率腔镜;8-光电倍增管;9-数据采集卡;10-计算机;11-壳体;61-Ⅰ透光口;62-Ⅱ透光口;63-进气口;64-窗口片;111-衰荡腔。In the figure: 1-laser transmitter; 2-mirror; 3-polarizer; 4-1/4 wave plate; 5-coupling lens; 6-cavity mirror box; 7-high reflectivity cavity mirror; 8-photoelectric multiplier Tube; 9-data acquisition card; 10-computer; 11-housing; 61-I light transmission port; 62-II light transmission port; 63-air inlet; 64-window; 111-ring ring.
具体实施方式Detailed ways
下面通过实施例,并结合附图,对本发明的技术方案作进一步具体的说明。The technical solutions of the present invention will be further specifically described below through the embodiments and in conjunction with the accompanying drawings.
实施例1:Example 1:
如图1和2所示,图纸虚线表示光路,箭头表示光路方向;细实线表示电连接。一种基于光腔衰荡光谱技术的大气能见度测量装置,它包括呈马鞍状密封腔体结构的壳体11,壳体11为密封腔体结构。壳体11下部有一凹口,凹口向壳体11腔内凹进。壳体11腔体内设有一对高反射率腔镜7,高反射率腔镜7位于壳体11凹口两侧。一对高反射率腔镜7形成衰荡腔111。衰荡腔111为开放式结构,位于壳体11的密封腔体外,与大气直接接触。为免避高反射率腔镜7受大气污染,导致测量误差,壳体11还设有腔镜盒6。腔镜盒6有两个,每一个腔镜盒6腔体内固定一面高反射率腔镜7。腔镜盒6为圆柱状腔体结构。腔镜盒6的侧壁分别设有Ⅰ透光口61和Ⅱ透光口62,Ⅰ透光口61和Ⅱ透光口62以腔镜盒6中轴线为对称轴对称布置。高反射率腔镜7位于Ⅰ透光口6和Ⅱ透光口62之间。腔镜盒6侧壁外表面设有窗口片64,窗口片64外表面镀有高透膜。窗口片64覆盖Ⅰ透光口61。腔镜盒6顶部靠近Ⅱ透光口62设有进气口63。从进气口63充入高纯氮气再由Ⅱ透光口62出来,在高反射率腔镜7表面形成气帘,从而防止大气污染高反射率腔镜7。壳体11腔体内还设有激光发射器1、反射镜2、偏振片3、1/4波片4、耦合透镜5、光电倍增管8、数据采集卡9和计算机10。反射镜2有两面,激光发射器1与偏振片3之间连接有第一面反射镜2,1/4波片4与耦合透镜5之间连接有第二面反射镜2。激光发射器1、第一面反射镜2、偏振片3、1/4波片4、第二面反射镜2、耦合透镜5、第一面高反射率腔镜7、第二面高反射率腔镜7和光电倍增管8依次排列。光电倍增管8与数据采集卡9、数据采集卡9与计算机10分别通过导线电连接。As shown in Figures 1 and 2, the dotted lines in the drawings indicate the optical path, and the arrows indicate the direction of the optical path; the thin solid lines indicate electrical connections. An atmospheric visibility measurement device based on optical cavity ring-down spectroscopy technology, which includes a housing 11 with a saddle-shaped sealed cavity structure, and the housing 11 is a sealed cavity structure. There is a notch in the lower part of the housing 11, and the notch is recessed into the cavity of the housing 11. A pair of high-reflectivity cavity mirrors 7 are arranged in the cavity of the casing 11 , and the high-reflectivity cavity mirrors 7 are located on both sides of the notch of the casing 11 . A pair of high-reflectivity cavity mirrors 7 form a ring-down cavity 111 . The ring-down cavity 111 is an open structure, located outside the sealed cavity of the casing 11, and directly in contact with the atmosphere. In order to prevent the high-reflectivity cavity mirror 7 from being polluted by the atmosphere, resulting in measurement errors, the casing 11 is also provided with a cavity mirror box 6 . There are two cavity mirror boxes 6, and a high reflectivity cavity mirror 7 is fixed in each cavity mirror box 6 cavity. The cavity mirror box 6 is a cylindrical cavity structure. The side wall of the cavity mirror box 6 is respectively provided with an I light transmission port 61 and a II light transmission port 62 , and the I light transmission port 61 and the II light transmission port 62 are symmetrically arranged with the central axis of the cavity mirror box 6 as a symmetrical axis. The cavity mirror 7 with high reflectivity is located between the I light-transmitting port 6 and the II light-transmitting port 62 . The outer surface of the side wall of the cavity mirror box 6 is provided with a window sheet 64, and the outer surface of the window sheet 64 is coated with a high-transparency film. The window 64 covers the I light-transmitting opening 61 . The top of the cavity mirror box 6 is provided with an air inlet 63 close to the II light transmission port 62 . Fill the high-purity nitrogen gas from the air inlet 63 and then come out from the II light-transmitting port 62 to form an air curtain on the surface of the high-reflectivity cavity mirror 7, thereby preventing atmospheric pollution of the high-reflectivity cavity mirror 7. A laser transmitter 1 , a mirror 2 , a polarizer 3 , a quarter wave plate 4 , a coupling lens 5 , a photomultiplier tube 8 , a data acquisition card 9 and a computer 10 are also arranged in the cavity of the housing 11 . The reflection mirror 2 has two sides, the first reflection mirror 2 is connected between the laser transmitter 1 and the polarizer 3 , and the second reflection mirror 2 is connected between the 1/4 wave plate 4 and the coupling lens 5 . Laser transmitter 1, first mirror 2, polarizer 3, 1/4 wave plate 4, second mirror 2, coupling lens 5, first high reflectivity cavity mirror 7, second high reflectivity The cavity mirror 7 and the photomultiplier tube 8 are arranged in sequence. The photomultiplier tube 8 is electrically connected to the data acquisition card 9, and the data acquisition card 9 is connected to the computer 10 through wires.
激光发射器1发出p偏振光,为了不影响衰荡信号,激光脉冲宽度应足够短,本实施例激光波长为532nm、脉冲宽度为1ns,激光模式为基模。p偏振光射入第一面反射镜2折射后依次穿过偏振片3和1/4波片4后变成圆偏光。圆偏光射入第二面反射镜2折射后,由耦合透镜5耦合到衰荡腔111。圆偏光穿过覆盖第一个腔镜盒6的窗口片64,通过第一个腔镜盒6的Ⅰ透光口61射入第一面高反射率腔镜7分成两路。一路圆偏光由第一面高反射率腔镜7反射,再次通过第一个腔镜盒6的透光口61,穿过窗口片64,通过第二面反射镜2折射,射入1/4波片4后变成s偏振光,s偏振光射入偏振片3反射隔离输出,防止其重新入射到激光发射器1,造成激光发射器1损伤。另一路圆偏光穿过第一面高反射率腔镜7,从第一个腔镜盒6的Ⅱ透光口62出来与被测大气直接接触,穿过第二个腔镜盒6的Ⅱ透光口62,被第二面高反射率腔镜7反射,在第一面高反射率腔镜7与第二面高反射率腔镜7之间来回振荡,形成测量光路。然后穿过第二面高反射率腔镜7、第二个腔镜盒6的Ⅰ透光口61、窗口片64输出衰荡信号。衰荡信号被光电倍增管8探测到。数据采集卡9采集衰荡信号传输给计算机10。计算机10处理得到衰荡时间。分别测量空腔衰荡时间t0和大气衰荡时间t,由公式就可计算得到大气的消光系数β(公式中c为光速)。不同的衰荡时间对应不同的消光系数,由此可以计算大气消光系数和能见度。The laser transmitter 1 emits p-polarized light. In order not to affect the ring-down signal, the laser pulse width should be short enough. In this embodiment, the laser wavelength is 532 nm, the pulse width is 1 ns, and the laser mode is the fundamental mode. The p-polarized light enters the first reflector 2 and is refracted, then passes through the polarizer 3 and the 1/4 wave plate 4 in sequence, and becomes circularly polarized light. The circularly polarized light enters the second reflector 2 and is refracted, then is coupled to the ring-down cavity 111 by the coupling lens 5 . Circularly polarized light passes through the window plate 64 covering the first cavity mirror box 6, and enters the first high-reflectivity cavity mirror 7 through the I light transmission port 61 of the first cavity mirror box 6, and is divided into two paths. One path of circularly polarized light is reflected by the first high-reflectivity cavity mirror 7, passes through the light transmission port 61 of the first cavity mirror box 6, passes through the window 64, is refracted by the second reflector 2, and enters 1/4 After the wave plate 4 becomes s-polarized light, the s-polarized light enters the polarizer 3 to reflect and isolate the output, preventing it from entering the laser transmitter 1 again and causing damage to the laser transmitter 1 . The other circularly polarized light passes through the first high-reflectivity cavity mirror 7, comes out from the II light transmission port 62 of the first cavity mirror box 6, and directly contacts the atmosphere to be measured, and passes through the II transmittance port 62 of the second cavity mirror box 6. The optical port 62 is reflected by the second high-reflectivity cavity mirror 7 and oscillates back and forth between the first high-reflectivity cavity mirror 7 and the second high-reflectivity cavity mirror 7 to form a measurement optical path. Then pass through the second high-reflectivity cavity mirror 7, the I light-transmitting port 61 of the second cavity mirror box 6, and the window plate 64 to output the ring-down signal. The ringdown signal is detected by the photomultiplier tube 8 . The data acquisition card 9 collects the ring down signal and transmits it to the computer 10 . The computer 10 processes and obtains the ring down time. Measure the cavity ring-down time t 0 and the atmospheric ring-down time t respectively, by the formula The extinction coefficient β of the atmosphere can be calculated (c in the formula is the speed of light). Different ring down times correspond to different extinction coefficients, from which the atmospheric extinction coefficient and visibility can be calculated.
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