[go: up one dir, main page]

CN101726362B - Terahertz polarization analyzer and terahertz polarization measurement method - Google Patents

Terahertz polarization analyzer and terahertz polarization measurement method Download PDF

Info

Publication number
CN101726362B
CN101726362B CN2009102387323A CN200910238732A CN101726362B CN 101726362 B CN101726362 B CN 101726362B CN 2009102387323 A CN2009102387323 A CN 2009102387323A CN 200910238732 A CN200910238732 A CN 200910238732A CN 101726362 B CN101726362 B CN 101726362B
Authority
CN
China
Prior art keywords
light
terahertz
optical path
detection
crystal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
CN2009102387323A
Other languages
Chinese (zh)
Other versions
CN101726362A (en
Inventor
张亮亮
钟华
邓朝
张存林
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Capital Normal University
Original Assignee
Capital Normal University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Capital Normal University filed Critical Capital Normal University
Priority to CN2009102387323A priority Critical patent/CN101726362B/en
Publication of CN101726362A publication Critical patent/CN101726362A/en
Application granted granted Critical
Publication of CN101726362B publication Critical patent/CN101726362B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

一种太赫兹偏振分析器以及一种采用太赫兹偏振分析器的太赫兹偏振测量方法,偏振分析器包括发出激光的激光光源;分束片,设于所述激光光源的光路后方,将激光分为泵浦光和探测光;产生太赫兹波的太赫兹产生装置,设于所述分束片后方泵浦光的光路上;石英晶体,设置于所述太赫兹产生装置后方的光路上,所述石英晶体的光轴与水平方向成45°设置;光路调整装置,设于所述石英晶体后方的光路上和探测光的光路上,使所述太赫兹波和探测光同向共线;探测晶体,设于所述光路调整装置后方的光路上;探测装置,设于所述探测晶体后方的光路上。

Figure 200910238732

A terahertz polarization analyzer and a terahertz polarization measurement method using the terahertz polarization analyzer, the polarization analyzer includes a laser light source emitting laser light; a beam splitter is arranged behind the optical path of the laser light source to split the laser light It is the pumping light and the detection light; the terahertz generating device for generating terahertz waves is arranged on the optical path of the pumping light behind the beam splitter; the quartz crystal is arranged on the optical path behind the terahertz generating device, and the The optical axis of the quartz crystal is set at 45° to the horizontal direction; the optical path adjustment device is arranged on the optical path behind the quartz crystal and the optical path of the detection light, so that the terahertz wave and the detection light are collinear in the same direction; The crystal is arranged on the optical path behind the optical path adjustment device; the detection device is arranged on the optical path behind the detection crystal.

Figure 200910238732

Description

太赫兹偏振分析器及太赫兹偏振测量方法Terahertz polarization analyzer and method for measuring terahertz polarization

技术领域technical field

本发明涉及太赫兹辐射偏振方向的测量装置和测量方法,具体地说本发明涉及一种利用石英晶体并且只进行一次测量就可以测量出太赫兹辐射偏振方向的太赫兹偏振分析器及太赫兹偏振测量方法。The present invention relates to a measuring device and a measuring method for the polarization direction of terahertz radiation. Specifically, the present invention relates to a terahertz polarization analyzer and a terahertz polarization analyzer which can measure the polarization direction of terahertz radiation by using a quartz crystal and performing only one measurement. Measurement methods.

背景技术Background technique

太赫兹辐射由于其具有瞬态性、低能性和相干性等独特的性质,而在卫星通信、无损检测、军用雷达等方面具有重大的科学价值和广阔的应用前景。为了对太赫兹辐射的特性、产生机理等深入的理解以及对所测量样品的信息进行正确的提取,都需要对太赫兹辐射的偏振方向进行测量。Due to its unique properties such as transient, low energy and coherence, terahertz radiation has great scientific value and broad application prospects in satellite communications, nondestructive testing, and military radar. In order to have a deep understanding of the characteristics and mechanism of terahertz radiation and to extract the information of the measured sample correctly, it is necessary to measure the polarization direction of terahertz radiation.

通过研究由双频激光激发空气等离子体所产生的太赫兹辐射的偏振方向,可以知道通过改变基频光和二次谐波之间的相对相位可以控制辐射的太赫兹偏振方向。By studying the polarization direction of the terahertz radiation generated by the dual-frequency laser excitation of air plasma, it can be known that the terahertz polarization direction of the radiation can be controlled by changing the relative phase between the fundamental frequency light and the second harmonic.

但现有的对太赫兹辐射的偏振方向进行测量的方法是通过旋转偏振片来找出透过率最大的方向,这种方法需要旋转太赫兹偏振片最少180度来计算太赫兹辐射的偏振方向;或是旋转探测晶体来测量,这种方法需要对探测晶体处于最大值和最小值方向分别测量太赫兹辐射的电场来计算太赫兹辐射的偏振方向。这两种方法不仅操作复杂,而且测量过程会耗费大量时间。However, the existing method of measuring the polarization direction of terahertz radiation is to find the direction of maximum transmittance by rotating the polarizer. This method needs to rotate the terahertz polarizer at least 180 degrees to calculate the polarization direction of terahertz radiation. ; Or rotate the detection crystal to measure, this method needs to measure the electric field of the terahertz radiation respectively for the detection crystal in the maximum and minimum directions to calculate the polarization direction of the terahertz radiation. These two methods are not only complicated to operate, but also the measurement process will consume a lot of time.

发明内容Contents of the invention

本发明所要解决的技术问题在于,提供一种太赫兹偏振分析器及太赫兹偏振测量方法,在太赫兹偏振方向分析中采用石英晶体并且只进行一次测量,即可对太赫兹波的偏振方向进行测量的方法和装置,从而克服利用传统的太赫兹线栅偏振片对偏振方向进行测量过程中需要最少旋转偏振片180度的缺点。The technical problem to be solved by the present invention is to provide a terahertz polarization analyzer and a terahertz polarization measurement method. In the analysis of the terahertz polarization direction, a quartz crystal is used to measure the polarization direction of the terahertz wave. The measurement method and device overcome the disadvantage that the traditional terahertz wire grid polarizer needs to rotate the polarizer at least 180 degrees in the process of measuring the polarization direction.

为解决上述技术问题,本发明的一种太赫兹偏振分析器,包括发出激光的激光光源;分束片,设于所述激光光源的光路后方,将激光分为泵浦光和探测光;产生太赫兹波的太赫兹产生装置,设于所述分束片后方泵浦光的光路上;石英晶体,设置于所述太赫兹产生装置后方的光路上,所述石英晶体的光轴与水平方向成45°设置;光路调整装置,设于所述石英晶体后方的光路上和探测光的光路上,使所述太赫兹波和探测光同向共线;探测晶体,设于所述光路调整装置后方的光路上;探测装置,设于所述探测晶体后方的光路上。In order to solve the above-mentioned technical problems, a terahertz polarization analyzer of the present invention includes a laser light source emitting laser light; a beam splitter is arranged behind the optical path of the laser light source, and divides the laser light into pump light and probe light; The terahertz generating device of the terahertz wave is arranged on the optical path of the pumping light behind the beam splitter; the quartz crystal is arranged on the optical path behind the terahertz generating device, and the optical axis of the quartz crystal and the horizontal direction set at 45°; the optical path adjustment device is arranged on the optical path behind the quartz crystal and the optical path of the detection light, so that the terahertz wave and the detection light are in the same direction and collinear; the detection crystal is arranged on the optical path adjustment device The optical path at the rear; the detection device is arranged on the optical path at the rear of the detection crystal.

其中,所述太赫兹产生装置包括在泵浦光光路上依次设置的透镜、偏硼酸钡晶体和聚四氟乙烯板。Wherein, the terahertz generating device includes a lens, a barium metaborate crystal and a polytetrafluoroethylene plate sequentially arranged on the optical path of the pumping light.

其中,所述探测装置包括在光路上依次设置的四分之一波片、渥拉斯顿棱镜和差分探头。Wherein, the detection device includes a quarter-wave plate, a Wollaston prism and a differential probe arranged sequentially on the optical path.

其中,所述探测晶体为电光晶体。Wherein, the detection crystal is an electro-optic crystal.

一种采用太赫兹偏振分析器的太赫兹偏振测量方法,包括如下步骤:(1)产生同源的太赫兹波和探测光;(2)将所述太赫兹波通过光轴与水平方向成45°的石英晶体,使所述太赫兹波在时域上分为o光和e光;(3)调整探测光和分开后的太赫兹波的光路,使探测光和太赫兹波同向共线通过探测晶体,使探测光的偏振方向发生变化;(4)探测从所述探测晶体出射的探测光的水平偏振光和竖直偏振光的光强差;(5)根据探测结果得到太赫兹电场波形,计算得出太赫兹波的偏振角度。A method for measuring terahertz polarization using a terahertz polarization analyzer, comprising the following steps: (1) generating homologous terahertz waves and probe light; ° quartz crystal, so that the terahertz wave is divided into o light and e light in the time domain; (3) adjust the optical path of the probe light and the separated terahertz wave, so that the probe light and the terahertz wave are collinear in the same direction By detecting the crystal, the polarization direction of the detection light is changed; (4) detecting the light intensity difference between the horizontally polarized light and the vertically polarized light of the detection light emitted from the detection crystal; (5) obtaining the terahertz electric field according to the detection result Waveform, the polarization angle of the terahertz wave is calculated.

其中,步骤(4)中的探测水平偏振光和竖直偏振光的光强差,是先将探测光进行调零,使得开始时探测光束的水平偏振光和竖直偏振光的光强相等,然后将探测光的水平偏振光和竖直偏振光分开,由差分探头进行探测。Wherein, the detection of the light intensity difference between the horizontally polarized light and the vertically polarized light in step (4) is to first zero-adjust the detection light, so that the light intensity of the horizontally polarized light and the vertically polarized light of the detection beam are equal at the beginning, Then the horizontally polarized light and the vertically polarized light of the probe light are separated and detected by a differential probe.

其中,步骤(1)中的产生的太赫兹波和探测光,是将激光脉冲分为泵浦光和探测光,泵浦光经太赫兹产生装置产生太赫兹波。Wherein, the terahertz wave and the probe light generated in the step (1) are divided into the pump light and the probe light from the laser pulse, and the pump light is passed through the terahertz generating device to generate the terahertz wave.

其中,所述泵浦光经太赫兹产生装置产生太赫兹波的步骤为,将泵浦进行倍频,产生倍频光,所述倍频光与未被倍频的基频光被聚焦而在焦点处相混频,产生等离子体,激发太赫兹波,完成产生太赫兹波步骤。Wherein, the step of generating the terahertz wave by the pump light through the terahertz generating device is to perform frequency doubling on the pump to generate frequency-doubled light, and the frequency-doubled light and the fundamental frequency light that has not been frequency-multiplied are focused to form a Phase mixing at the focal point generates plasma, excites terahertz waves, and completes the step of generating terahertz waves.

其中,所述泵浦光具有入射激光的绝大部分能量,所述探测光为低功率激光。Wherein, the pumping light has most of the energy of the incident laser light, and the detection light is a low-power laser light.

通过上述的技术方案,本发明的太赫兹偏振分析器及太赫兹偏振测量方法,使得测量过程无需旋转偏振片,只进行一次测量就可以测量出太赫兹辐射偏振方向,测量更为简单方便,达到了有益的技术效果。Through the above-mentioned technical solution, the terahertz polarization analyzer and the terahertz polarization measurement method of the present invention make it possible to measure the polarization direction of the terahertz radiation without rotating the polarizer in the measurement process, and the measurement is simpler and more convenient, achieving beneficial technical effect.

附图说明Description of drawings

图1a为自由空间的太赫兹波形;Figure 1a is the terahertz waveform in free space;

图1b为太赫兹波通过光轴与水平方向的夹角固定为45度的石英晶体后的时域波形图;Figure 1b is a time-domain waveform diagram of a terahertz wave passing through a quartz crystal whose angle between the optical axis and the horizontal direction is fixed at 45 degrees;

图2a为石英晶体方向示意图;Figure 2a is a schematic diagram of the direction of the quartz crystal;

图2b为入射的太赫兹波方向示意图;Figure 2b is a schematic diagram of the direction of the incident terahertz wave;

图2c为透射的太赫兹波方向示意图;Figure 2c is a schematic diagram of the transmitted terahertz wave direction;

图3为太赫兹偏振分析器的示意图;3 is a schematic diagram of a terahertz polarization analyzer;

图4为通过本发明和现有技术分别计算得出的太赫兹波的偏振方向随着的基频波和倍频波之间相位差的变化而改变的角度。Fig. 4 is the angle at which the polarization direction of the terahertz wave changes with the change of the phase difference between the fundamental frequency wave and the double frequency wave calculated by the present invention and the prior art respectively.

附图标记说明Explanation of reference signs

1-透镜;2-BBO晶体;3-聚四氟乙烯板;4-抛面镜;5-石英晶体;6-导电玻璃;7-ZnTe晶体;8-四分之一波片;9-沃拉斯顿棱镜;10-差分探测器;11-反射镜。1-lens; 2-BBO crystal; 3-PTFE plate; 4-parabolic mirror; 5-quartz crystal; 6-conductive glass; 7-ZnTe crystal; 8-quarter wave plate; Raston prism; 10-differential detector; 11-mirror.

具体实施方式Detailed ways

以下通过具体对双频激光激发空气等离子体所产生的太赫兹波的偏振方向的测量进行的描述,对本发明的一次测量计算太赫兹波的偏振方向的方法作进一步的说明。The method for calculating the polarization direction of the terahertz wave in one measurement of the present invention will be further described by describing the measurement of the polarization direction of the terahertz wave generated by the air plasma excited by the dual-frequency laser.

本发明的太赫兹偏振测量方法其原理为,太赫兹波通过光轴与水平方向的夹角固定为45度的石英晶体后,由于双折射现象而被分解为两束光:寻常光(以下简称为o光)与非寻常光(以下简称为e光)。如图1a所示为自由空间的太赫兹波形。图1b为太赫兹波通过光轴与水平方向的夹角固定为45°的石英晶体后,在其时域上波形出现两处振幅最大值,分别代表被分开的o光和e光。The principle of the terahertz polarization measurement method of the present invention is that after the terahertz wave passes through the quartz crystal whose angle between the optical axis and the horizontal direction is fixed at 45 degrees, it is decomposed into two beams of light due to birefringence: ordinary light (hereinafter referred to as For o light) and extraordinary light (hereinafter referred to as e light). The terahertz waveform in free space is shown in Figure 1a. Figure 1b shows that after the terahertz wave passes through the quartz crystal whose angle between the optical axis and the horizontal direction is fixed at 45°, two amplitude maxima appear in the waveform in the time domain, representing the separated o-light and e-light respectively.

图2a为xoy平面内的石英晶体,其光轴方向与水平方向(ox方向)的夹角为45°,图2b为入射的太赫兹波,其偏振方向与水平方向的夹角为θ。该太赫兹波经石英晶体后,被分解为o光和e光,两束光的偏振方向分别为沿石英晶体的光轴方向和垂直于光轴方向。由于石英晶体5的光轴与水平方向成45°设置,分解后的o光和e光强度基本相等,因此当太赫兹波的偏振方向发生改变时,能够更清楚的显示出来。Figure 2a is a quartz crystal in the xoy plane, the angle between the optical axis direction and the horizontal direction (ox direction) is 45°, and Figure 2b is the incident terahertz wave, and the angle between the polarization direction and the horizontal direction is θ. After the terahertz wave passes through the quartz crystal, it is decomposed into o light and e light, and the polarization directions of the two beams are along the optical axis of the quartz crystal and perpendicular to the optical axis, respectively. Since the optical axis of the quartz crystal 5 is set at 45° to the horizontal direction, the intensity of the decomposed o-light and e-light is basically equal, so when the polarization direction of the terahertz wave changes, it can be displayed more clearly.

如图2c所示,分解后的两束光的振幅分别为ein(t)cos(45°-θ)和ein(t)sin(45°-θ),则分解后的两束光振幅在水平方向的分量分别为

Figure G2009102387323D00031
ein(t)cos(45°-θ)和
Figure G2009102387323D00032
Figure G2009102387323D00033
Figure G2009102387323D00034
来表示。As shown in Figure 2c, the amplitudes of the two beams of light after decomposition are e in (t)cos(45°-θ) and e in (t)sin(45°-θ) respectively, then the amplitudes of the two beams of light after decomposition are The components in the horizontal direction are
Figure G2009102387323D00031
e in (t)cos(45°-θ) and
Figure G2009102387323D00032
by
Figure G2009102387323D00033
and
Figure G2009102387323D00034
To represent.

由于o光和e光的传播速度不同,因此在水平方向上会先后探测到

Figure G2009102387323D00041
Figure G2009102387323D00042
故根据
Figure G2009102387323D00043
则可以算出太赫兹光的偏振方向与水平方向的夹角θ。现有技术中太赫兹波的振幅方向与水平方向的夹角θ的计算方法为
Figure G2009102387323D00044
其中
Figure G2009102387323D00045
为太赫兹波沿水平方向的振幅,
Figure G2009102387323D00046
为太赫兹波振幅的最大值。由该公式与本发明的公式
Figure G2009102387323D00047
比较,并结合图2a-2c的几何关系可知,本发明与现有技术的方法测量与计算的结果是一致的。Since o light and e light travel at different speeds, they will be detected successively in the horizontal direction
Figure G2009102387323D00041
and
Figure G2009102387323D00042
Therefore according to
Figure G2009102387323D00043
Then the angle θ between the polarization direction of the terahertz light and the horizontal direction can be calculated. In the prior art, the calculation method of the angle θ between the amplitude direction of the terahertz wave and the horizontal direction is
Figure G2009102387323D00044
in
Figure G2009102387323D00045
is the amplitude of the terahertz wave along the horizontal direction,
Figure G2009102387323D00046
is the maximum amplitude of the terahertz wave. By this formula and the formula of the present invention
Figure G2009102387323D00047
Comparing and combining with the geometric relationship of Figs. 2a-2c, it can be known that the measurement and calculation results of the method of the present invention and the prior art are consistent.

图3所示为太赫兹偏振分析器的示意图。本发明的太赫兹偏振分析器包括激光光源,在本实施例中,该激光光源可以选用美国光谱物理公司生产的飞秒激光放大器,其激光脉冲平均输出功率为3.5W,重复频率1KHz,中心波长800nm,脉宽50fs。激光光源还可以选用产生其他波长激光的激光器,在此不再赘述。Figure 3 shows a schematic diagram of a terahertz polarization analyzer. The terahertz polarization analyzer of the present invention includes a laser light source. In this embodiment, the laser light source can be a femtosecond laser amplifier produced by American Spectrum Physics Corporation. The average output power of the laser pulse is 3.5W, the repetition rate is 1KHz, and the center wavelength 800nm, pulse width 50fs. The laser light source can also choose lasers that generate lasers with other wavelengths, which will not be repeated here.

该激光光源光路后方同轴设置有分束片,产生的激光脉冲经过分束片后,被分为两束光,泵浦光L1和探测光L2。泵浦L1具有入射激光的绝大部分能量,经太赫兹产生装置产生太赫兹波。探测L2为低功率激光,作为探测光束。A beam splitter is arranged coaxially behind the optical path of the laser light source, and the generated laser pulses are divided into two beams after passing through the beam splitter, pumping light L1 and probe light L2. The pump L1 has most of the energy of the incident laser, and the terahertz wave is generated by the terahertz generating device. The detection L2 is a low-power laser as the detection beam.

泵浦光L1经太赫兹产生装置产生的太赫兹波,由太赫兹产生装置后方光路上设置的抛面镜4准直后,聚焦于后方光路上的石英晶体5处。该石英晶体5的光轴与水平方向成45°设置,经由该石英晶体5的双折射作用,将太赫兹波在时域上分为两个振幅大致相等且相互垂直的o光和e光。The terahertz wave generated by the pump light L1 through the terahertz generating device is collimated by the parabolic mirror 4 arranged on the optical path behind the terahertz generating device, and then focused on the quartz crystal 5 on the optical path behind the terahertz generating device. The optical axis of the quartz crystal 5 is set at 45° to the horizontal direction. Through the birefringence of the quartz crystal 5, the terahertz wave is divided into two o-rays and e-rays with approximately equal amplitudes and perpendicular to each other in the time domain.

探测光L2作为探测光束和分开后的太赫兹波,分别经设于各自光路上的光路调整装置调整其光路后,同向共线到达探测晶体7处。The detection light L2 is used as the detection light beam and the separated terahertz waves, and after the optical paths are adjusted by the optical path adjustment devices arranged on the respective optical paths, they arrive at the detection crystal 7 in the same direction and collinearly.

在图3所示的实施例中,光路调整装置实施为:分开后的太赫兹波经抛面镜4的准直和聚焦后,由抛面镜4后方的导电玻璃6反射到探测晶体7处。该探测晶体7选用如ZnTe的电光晶体,该导电玻璃6可选用ITO。探测光束经反射镜11和透镜1调整光路并聚焦后,透过导电玻璃6与通过石英晶体的太赫兹波同向共线通过探测晶体7。In the embodiment shown in FIG. 3 , the optical path adjustment device is implemented as follows: After the separated terahertz wave is collimated and focused by the parabolic mirror 4, it is reflected by the conductive glass 6 behind the parabolic mirror 4 to the detection crystal 7. . The detection crystal 7 is an electro-optic crystal such as ZnTe, and the conductive glass 6 is ITO. After the detection beam is adjusted and focused by the mirror 11 and the lens 1, it passes through the conductive glass 6 and passes through the detection crystal 7 in the same direction as the terahertz wave passing through the quartz crystal.

由于泵浦光L1和探测光L2为同源光,故在同向共线通过探测晶体7时,太赫兹波和探测光束在探测晶体上重合。在探测晶体7内,太赫兹电场改变晶体的折射率椭球,从而使出射的探测光束的偏振态发生改变,使原本水平偏振的800nm探测光束的偏振方向发生变化。探测装置设于该探测晶体7光路后方,可探测得出太赫兹电场波形。Since the pump light L1 and the probe light L2 are homologous light, when the same direction collinearly passes through the probe crystal 7, the terahertz wave and the probe beam overlap on the probe crystal. In the detection crystal 7, the terahertz electric field changes the refractive index ellipsoid of the crystal, thereby changing the polarization state of the outgoing detection beam and changing the polarization direction of the originally horizontally polarized 800nm detection beam. The detection device is arranged behind the optical path of the detection crystal 7, and can detect and obtain the terahertz electric field waveform.

具体的,该探测装置主要由在光路上依次设置的四分之一波片8、渥拉斯顿棱镜9和差分探头10组成。从该探测晶体7出射的探测光束,经过四分之一波片8调零,使得开始时探测光束的水平偏振光和竖直偏振光的光强相等。然后经渥拉斯顿棱镜9将水平偏振光和竖直偏振光分开,分开的两束光由差分探头10进行探测。Specifically, the detection device is mainly composed of a quarter-wave plate 8 , a Wollaston prism 9 and a differential probe 10 sequentially arranged on the optical path. The detection beam emitted from the detection crystal 7 is zeroed through the quarter-wave plate 8, so that the intensity of the horizontally polarized light and the vertically polarized light of the detection beam are equal at the beginning. Then the horizontally polarized light and the vertically polarized light are separated by the Wollaston prism 9 , and the two separated beams are detected by the differential probe 10 .

分开的水平偏振光和竖直偏振光的光强差正比于太赫兹电场,使用差分探头10可以将这两束偏振光的光强差转换为电流差,经计算机软件计算,从而探测到太赫兹电场随时间变化的时域光谱来,得到如图1b的太赫兹电场波形。然后根据图中测到的

Figure G2009102387323D00051
Figure G2009102387323D00052
即可计算得出太赫兹偏振的θ角。The light intensity difference between the separated horizontally polarized light and vertically polarized light is proportional to the terahertz electric field. Using the differential probe 10, the light intensity difference between the two beams of polarized light can be converted into a current difference, and calculated by computer software, so as to detect the terahertz electric field. From the time-domain spectrum of the electric field changing with time, the terahertz electric field waveform as shown in Figure 1b is obtained. Then according to the measured
Figure G2009102387323D00051
and
Figure G2009102387323D00052
The θ angle of the terahertz polarization can be calculated.

本发明的太赫兹产生装置是采用双频激光激发空气产生等离子体,从而产生太赫兹波的方法产生的。太赫兹产生装置包括在泵浦光光路上依次设置的透镜1、偏硼酸钡晶体2和聚四氟乙烯板3。The terahertz generating device of the present invention is produced by using a dual-frequency laser to excite air to generate plasma, thereby generating terahertz waves. The terahertz generating device includes a lens 1 , a barium metaborate crystal 2 and a polytetrafluoroethylene plate 3 arranged in sequence on the optical path of the pumping light.

泵浦光L1通过分束片后方所设的透镜1后,经BBO(偏硼酸钡)晶体2进行倍频,部分光被倍频为400nm的倍频光,部分光从BBO晶体透过后仍为800nm的基频光。该倍频光与基频光于距BBO晶体距离d处聚焦相混频,产生等离子体,从而激发太赫兹波。BBO晶体后方光路上设有聚四氟乙烯板3,产生的太赫兹波能够从聚四氟乙烯板3透过,从而滤去其他光波,得到实验所需太赫兹波。After the pump light L1 passes through the lens 1 set behind the beam splitter, it is frequency-doubled by the BBO (barium metaborate) crystal 2, and part of the light is frequency-doubled to 400nm frequency-doubled light, and part of the light is still transmitted through the BBO crystal. 800nm fundamental frequency light. The frequency doubled light and the fundamental frequency light are focused and mixed at a distance d from the BBO crystal to generate plasma, thereby exciting terahertz waves. There is a polytetrafluoroethylene plate 3 on the optical path behind the BBO crystal, and the generated terahertz wave can pass through the polytetrafluoroethylene plate 3, thereby filtering out other light waves and obtaining the terahertz wave required for the experiment.

基于双频激光激发空气产生等离子体产生太赫兹波的机制中,当基频光是线偏振光时,激发的太赫兹波也是线偏振的。随着基频光和倍频光的相对相位的变化太赫兹波的偏振方向会连续变化。基频光和倍频光的相对相位随着BBO晶体到等离子体的距离d的不同而发生变化,并且基频光和倍频光的相对相位的变化正比于BBO晶体的位置的变化。In the mechanism based on dual-frequency laser excitation of air to generate plasma to generate terahertz waves, when the fundamental frequency light is linearly polarized, the excited terahertz waves are also linearly polarized. The polarization direction of the terahertz wave will change continuously with the change of the relative phase of the fundamental frequency light and the double frequency light. The relative phase of the fundamental frequency light and the double frequency light changes with the distance d from the BBO crystal to the plasma, and the change of the relative phase of the fundamental frequency light and the double frequency light is proportional to the change of the position of the BBO crystal.

当BBO晶体的位置连续发生变化时,太赫兹波的偏振方向也会连续发生变化,通过探测通过石英晶体的太赫兹波所分开的两个脉冲,再进行计算,就可以只通过一次测量得到太赫兹波的偏振方向。图4显示了改变BBO晶体2的位置时,太赫兹波的偏振角度随之发生的变化。从图4中可知,用本发明太赫兹偏振分析器测量得到的结果,与采用现有技术直接测量得到的结果能够很好的吻合。When the position of the BBO crystal changes continuously, the polarization direction of the terahertz wave will also change continuously. By detecting the two pulses separated by the terahertz wave passing through the quartz crystal and performing calculations, the terahertz wave can be obtained by only one measurement. The polarization direction of the Hertzian waves. Fig. 4 shows the change of the polarization angle of the terahertz wave when the position of the BBO crystal 2 is changed. It can be seen from FIG. 4 that the results obtained by using the terahertz polarization analyzer of the present invention are in good agreement with the results obtained by direct measurement using the prior art.

本发明采用上述太赫兹偏振分析器的太赫兹偏振测量方法,包括如下步骤:The present invention adopts the terahertz polarization measurement method of the above-mentioned terahertz polarization analyzer, comprising the following steps:

(1)产生同源的太赫兹波和探测光L2,探测光L2作为探测光束;(1) Generate homologous terahertz waves and probe light L2, and probe light L2 is used as a probe beam;

(2)将太赫兹波利用抛面镜准直和聚焦,通过光轴与水平方向成45°的石英晶体,使太赫兹波在时域上分为两个振幅大致相等的o光和e光;(2) The terahertz wave is collimated and focused by a parabolic mirror, and passes through a quartz crystal whose optical axis is 45° to the horizontal direction, so that the terahertz wave is divided into two o-rays and e-rays with roughly equal amplitudes in the time domain ;

(3)调整探测光束和分开后的太赫兹波的光路,使太赫兹波与探测光束同向共线通过探测晶体,通过太赫兹电场改变探测晶体的折射率椭球,从而使原本水平偏振的800nm探测光束的偏振方向发生变化,该探测晶体7可选用如ZnTe的电光晶体;(3) Adjust the optical path of the detection beam and the separated terahertz wave, so that the terahertz wave and the detection beam pass through the detection crystal in the same direction, and the refractive index ellipsoid of the detection crystal is changed by the terahertz electric field, so that the original horizontally polarized The polarization direction of the 800nm detection beam changes, and the detection crystal 7 can be an electro-optic crystal such as ZnTe;

(4)利用探测装置探测从该探测晶体出射的该探测光束水平偏振光和竖直偏振光的光强差,从而探测得出太赫兹电场波形。(4) Using a detection device to detect the light intensity difference between the horizontally polarized light and the vertically polarized light of the detection beam emitted from the detection crystal, so as to detect and obtain a terahertz electric field waveform.

步骤(1)中产生太赫兹波和探测光束,是将激光光源产生的激光脉冲经过分束片后,被分为两束光,泵浦光L1和探测光L2。泵浦光L1具有入射激光的绝大部分能量,经太赫兹产生装置产生太赫兹波,探测光L2为低功率激光,作为探测光束。该激光光源可以选用美国光谱物理公司生产的飞秒激光放大器,其激光脉冲平均输出功率为3.5W,重复频率1KHz,中心波长800nm,脉宽50fs。本实施例中选用800nm的激光光源,还可以选用其他波长的激光,在此不再赘述。The generation of terahertz wave and probe beam in step (1) is to divide the laser pulse generated by the laser light source into two beams, pumping light L1 and probe light L2, after passing through the beam splitter. The pumping light L1 has most of the energy of the incident laser light, and the terahertz wave is generated by the terahertz generating device, and the detection light L2 is a low-power laser as the detection beam. The laser light source can be selected from the femtosecond laser amplifier produced by American Spectrophysics Corporation. The average output power of the laser pulse is 3.5W, the repetition frequency is 1KHz, the center wavelength is 800nm, and the pulse width is 50fs. In this embodiment, a laser light source of 800 nm is selected, and lasers of other wavelengths may also be selected, which will not be repeated here.

太赫兹波可以通过双频激光激发空气产生等离子体,从而产生太赫兹波的方法产生。具体为将800nm的泵浦光L1进行倍频,产生波长为400nm的光,可选用BBO晶体进行倍频。该倍频光与未被倍频的基频光被聚焦而在聚焦处相混频,产生等离子体,从而激发太赫兹波。激发的太赫兹波从聚四氟乙烯板透过,滤去其他光波,得到实验所需太赫兹波。BBO晶体与等离子体之间的距离d的变化,正比于基频光和倍频光的相对相位的变化,从而使太赫兹波的偏振方向也发生变化。Terahertz waves can be generated by exciting air with dual-frequency lasers to generate plasma, thereby generating terahertz waves. Specifically, to double the frequency of the 800nm pump light L1 to generate light with a wavelength of 400nm, a BBO crystal can be selected for frequency doubling. The frequency-doubled light and the undoubled fundamental-frequency light are focused and mixed at the focal point to generate plasma and excite terahertz waves. The excited terahertz wave passes through the polytetrafluoroethylene plate, filters out other light waves, and obtains the terahertz wave required for the experiment. The change of the distance d between the BBO crystal and the plasma is proportional to the change of the relative phase of the fundamental frequency light and the double frequency light, so that the polarization direction of the terahertz wave also changes.

步骤(4)中该探测光束先通过四分之一波片进行调零,使得开始时探测光束的水平偏振光和竖直偏振光的光强相等。然后经渥拉斯顿棱镜将水平偏振光和竖直偏振光的光路分开,由差分探头进行探测。分开的水平偏振光和竖直偏振光的光强差正比于太赫兹电场,使用差分探头可以将这两束偏振光的光强差转换为电流差,经计算机软件计算,从而探测到太赫兹电场随时间变化的时域光谱来,得到如图1b的太赫兹电场波形图。然后根据图中测到的

Figure G2009102387323D00061
Figure G2009102387323D00062
即可计算得出太赫兹偏振的θ角。In step (4), the detection beam is first zero-adjusted through a quarter-wave plate, so that the light intensity of the horizontally polarized light and the vertically polarized light of the detection beam are equal at the beginning. Then the optical paths of horizontally polarized light and vertically polarized light are separated by a Wollaston prism, and detected by a differential probe. The light intensity difference between the separated horizontally polarized light and vertically polarized light is proportional to the terahertz electric field. Using a differential probe, the light intensity difference between the two beams of polarized light can be converted into a current difference, and calculated by computer software to detect the terahertz electric field. From the time-domain spectrum changing with time, the terahertz electric field waveform shown in Figure 1b is obtained. Then according to the measured
Figure G2009102387323D00061
and
Figure G2009102387323D00062
The θ angle of the terahertz polarization can be calculated.

利用上述方法可以只通过一次测量得到太赫兹波的偏振方向,且其测量得到的结果,与采用现有技术直接测量得到的结果能够很好的吻合。Using the above method, the polarization direction of the terahertz wave can be obtained by only one measurement, and the result obtained by the measurement is in good agreement with the result obtained by direct measurement using the prior art.

以上对本发明的描述是说明性的,而非限制性的,本专业技术人员理解,在权利要求限定的精神与范围之内可对其进行许多修改、变化或等效,但是它们都将落入本发明的保护范围内。The above description of the present invention is illustrative rather than restrictive. Those skilled in the art understand that many modifications, changes or equivalents can be made to it within the spirit and scope of the claims, but they will all fall into within the protection scope of the present invention.

Claims (7)

1.一种太赫兹偏振分析器,其特征在于,包括1. A terahertz polarization analyzer, characterized in that, comprising 发出激光的激光光源;a laser light source that emits laser light; 分束片,设于所述激光光源的光路后方,将激光分为泵浦光和探测光;A beam splitter, arranged behind the optical path of the laser light source, divides the laser light into pump light and probe light; 产生太赫兹波的太赫兹产生装置,设于所述分束片后方泵浦光的光路上;A terahertz generating device for generating terahertz waves is arranged on the optical path of the pump light behind the beam splitter; 石英晶体,设置于所述太赫兹产生装置后方的光路上,所述石英晶体的光轴与水平方向成45°设置;A quartz crystal is arranged on the optical path behind the terahertz generating device, and the optical axis of the quartz crystal is arranged at 45° to the horizontal direction; 光路调整装置,设于所述石英晶体后方的光路上和探测光的光路上,使所述太赫兹波和探测光同向共线;The optical path adjustment device is arranged on the optical path behind the quartz crystal and the optical path of the detection light, so that the terahertz wave and the detection light are collinear in the same direction; 探测晶体,设于所述光路调整装置后方的光路上;The detection crystal is arranged on the optical path behind the optical path adjustment device; 探测装置,设于所述探测晶体后方的光路上;所述探测装置包括在光路上依次设置的四分之一波片、渥拉斯顿棱镜和差分探头。The detection device is arranged on the optical path behind the detection crystal; the detection device includes a quarter-wave plate, a Wollaston prism and a differential probe arranged in sequence on the optical path. 2.如权利要求1所述的太赫兹偏振分析器,其特征在于,所述太赫兹产生装置包括在泵浦光光路上依次设置的透镜、偏硼酸钡晶体和聚四氟乙烯板。2 . The terahertz polarization analyzer according to claim 1 , wherein the terahertz generating device comprises a lens, a barium metaborate crystal and a polytetrafluoroethylene plate arranged in sequence on the optical path of the pumping light. 3.如权利要求1或2所述的太赫兹偏振分析器,其特征在于,所述探测晶体为电光晶体。3. The terahertz polarization analyzer according to claim 1 or 2, wherein the detection crystal is an electro-optic crystal. 4.一种采用太赫兹偏振分析器的太赫兹偏振测量方法,其特征在于,包括如下步骤:4. A method for measuring terahertz polarization using a terahertz polarization analyzer, comprising the steps of: (1)产生同源的太赫兹波和探测光;(1) Generate homologous terahertz waves and probe light; (2)将所述太赫兹波通过光轴与水平方向成45°的石英晶体,使所述太赫兹波在时域上分为o光和e光;(2) passing the terahertz wave through a quartz crystal whose optical axis is 45° from the horizontal direction, so that the terahertz wave is divided into o light and e light in the time domain; (3)调整探测光和分开后的所述太赫兹波的光路,使探测光和太赫兹波同向共线通过探测晶体,使探测光的偏振方向发生变化;(3) adjusting the optical path of the detection light and the separated terahertz wave, so that the detection light and the terahertz wave pass through the detection crystal in the same direction and collinearly, so that the polarization direction of the detection light changes; (4)探测从所述探测晶体出射的探测光的水平偏振光和竖直偏振光的光强差:先将探测光进行调零,使得开始时探测光束的水平偏振光和竖直偏振光的光强相等,然后将探测光的水平偏振光和竖直偏振光分开,由差分探头进行探测;(4) Detect the light intensity difference between the horizontally polarized light and the vertically polarized light of the probing light emitted from the probing crystal: the probing light is first zeroed, so that at the beginning the horizontally polarized light and the vertically polarized light of the probing beam The light intensity is equal, and then the horizontally polarized light and the vertically polarized light of the probe light are separated, and detected by the differential probe; (5)根据探测结果得到太赫兹电场波形,计算得出太赫兹波的偏振角度。(5) Obtain the terahertz electric field waveform according to the detection results, and calculate the polarization angle of the terahertz wave. 5.如权利要求4所述的太赫兹偏振测量方法,其特征在于,步骤(1)中的产生同源的太赫兹波和探测光,是将激光脉冲分为泵浦光和探测光,泵浦光经太赫兹产生装置产生太赫兹波。5. The method for measuring terahertz polarization as claimed in claim 4, wherein the generation of homologous terahertz waves and probe light in step (1) is to divide the laser pulse into pump light and probe light, and pump The Pu light passes through the terahertz generating device to generate terahertz waves. 6.如权利要求5所述的太赫兹偏振测量方法,其特征在于,所述泵浦光经太赫兹产生装置产生太赫兹波的步骤为,将泵浦进行倍频,产生倍频光,所述倍频光与未被倍频的基频光被聚焦而在焦点处相混频,产生等离子体,激发太赫兹波,完成产生太赫兹波步骤。6. The method for measuring terahertz polarization according to claim 5, wherein the step of generating terahertz waves through the terahertz generating device of the pump light is to double the frequency of the pump to generate frequency-doubled light. The frequency doubled light and the undoubled fundamental frequency light are focused and mixed at the focal point to generate plasma, excite terahertz waves, and complete the step of generating terahertz waves. 7.如权利要求5所述的太赫兹偏振测量方法,其特征在于,所述泵浦光具有入射激光的绝大部分能量,所述探测光为低功率激光。7. The terahertz polarization measurement method according to claim 5, wherein the pumping light has most of the energy of the incident laser light, and the detection light is a low-power laser.
CN2009102387323A 2009-11-23 2009-11-23 Terahertz polarization analyzer and terahertz polarization measurement method Expired - Fee Related CN101726362B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN2009102387323A CN101726362B (en) 2009-11-23 2009-11-23 Terahertz polarization analyzer and terahertz polarization measurement method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN2009102387323A CN101726362B (en) 2009-11-23 2009-11-23 Terahertz polarization analyzer and terahertz polarization measurement method

Publications (2)

Publication Number Publication Date
CN101726362A CN101726362A (en) 2010-06-09
CN101726362B true CN101726362B (en) 2011-08-17

Family

ID=42447585

Family Applications (1)

Application Number Title Priority Date Filing Date
CN2009102387323A Expired - Fee Related CN101726362B (en) 2009-11-23 2009-11-23 Terahertz polarization analyzer and terahertz polarization measurement method

Country Status (1)

Country Link
CN (1) CN101726362B (en)

Families Citing this family (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102192884B (en) * 2011-03-14 2013-06-19 首都师范大学 Method for imaging of samples by using polarization controllable terahertz waves
CN102192883B (en) * 2011-03-14 2013-04-03 首都师范大学 Imaging method by terahertz wave and system thereof
CN103901404B (en) * 2014-03-14 2016-05-11 中国工程物理研究院电子工程研究所 Be applicable to the MMAOP framework of Terahertz radar and communication system
CN104749131A (en) * 2015-03-09 2015-07-01 首都师范大学 Light path balance adjusting device used for TeraHertz wave detection system
CN106248615B (en) * 2015-06-05 2019-04-23 中国科学院苏州纳米技术与纳米仿生研究所 A terahertz wave analyzer
CN107015414A (en) * 2016-01-28 2017-08-04 首都师范大学 A kind of system and method for changing terahertz polarization state
CN106441557A (en) * 2016-08-17 2017-02-22 中国电子科技集团公司第四十研究所 Multi-purpose terahertz optical power probe
CN106248616B (en) * 2016-09-27 2017-10-24 深圳市太赫兹科技创新研究院有限公司 The full polarization state detection spectrometer of Terahertz
CN106483096B (en) * 2016-11-25 2023-04-25 首都师范大学 System and method for laser excitation of air plasma to generate high-intensity terahertz waves
CN106932357B (en) * 2017-03-09 2020-08-11 南开大学 Super-diffraction resolution limit terahertz spectral imaging system
CN108918457A (en) * 2018-04-27 2018-11-30 天津大学 The device and method that THz wave modulates laser spectral intensity measurement electro-optic coefficient
CN109238466B (en) * 2018-08-13 2020-09-29 首都师范大学 Characterization method of polarization state of terahertz wave and time-resolved focal plane imaging system
CN109900360B (en) * 2019-03-12 2021-04-13 中国工程物理研究院应用电子学研究所 Device and method for measuring free electron laser terahertz wave peak power
CN110768087B (en) * 2019-11-22 2020-08-18 北京航空航天大学 Polarization tunable terahertz wave radiation source
CN113720784B (en) * 2021-10-11 2023-03-24 阜阳师范大学 Chromium-based spinel test system based on terahertz waveband magneto-optical spectrum

Also Published As

Publication number Publication date
CN101726362A (en) 2010-06-09

Similar Documents

Publication Publication Date Title
CN101726362B (en) Terahertz polarization analyzer and terahertz polarization measurement method
CN101813619B (en) Method utilizing polarization-controllable T-Hz wave to measure optical axis direction of birefringent crystal
CN110376125B (en) Transient absorption spectroscopy measurement system and method
CN2874476Y (en) Terahertz time domain spectral instrument based on optical rectification
CN104236711B (en) The three-dimensional spectrum investigating system of a kind of femtosecond CARS for the research of molecule ultra-fast dynamics and detection method
CN103344623A (en) Coherent anti-stokes raman scattering optical comb spectrum detection method for improving precision
CN113655018B (en) Terahertz time-domain spectroscopy system for microstructure characterization of multiferroic material
CN114389125B (en) System and method for generating terahertz waves by circular airy three-color field laser
CN104792703B (en) Detection device for optical absorption coefficient of aerosol based on laser multiple reflections optoacoustic spectroscopy
US8759779B2 (en) Terahertz wave generation element, terahertz wave detection element, and terahertz time domain spectral device
CN107462849B (en) Device and method for measuring radio frequency line transmission factor based on atomic energy level
Chen et al. Systematic investigation of terahertz wave generation from liquid water lines
CN112098736A (en) Method for measuring phase of microwave electric field
CN105716756A (en) Accurate measuring device for microstress spatial distribution of optical material
CN106768335B (en) A Nonlinear Spectral Phase Measurement Method
Song et al. Enhance terahertz radiation and its polarization-control with two paralleled filaments pumped by two-color femtosecond laser fields
CN101963495A (en) Device and method for measuring physical parameters of anisotropic substance
CN105910995A (en) Transient polarization absorption spectrum measurement method and laser flash photolysis instrument system for realizing same
CN216483549U (en) an autocorrelator
CN114935696A (en) Portable power frequency electric field measuring device based on atomic spectrum
TWI464364B (en) Liquid crystal cell gap measurement device and measurement method thereof
CN109613456A (en) An all-optical atomic magnetometer and method
CN110749552B (en) System and method for determining second-order nonlinear polarizability of materials
CN110703532B (en) A method and device for generating and adjusting higher harmonics of circular or elliptical polarization
CN114460508A (en) Light path of atomic spectrum lamp pump magnetometer and design method thereof

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
C17 Cessation of patent right
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20110817

Termination date: 20131123