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CN113008839B - Organic semiconductor microcavity vitreous color-Einstein condensation vortex generation device - Google Patents

Organic semiconductor microcavity vitreous color-Einstein condensation vortex generation device Download PDF

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CN113008839B
CN113008839B CN202110191385.4A CN202110191385A CN113008839B CN 113008839 B CN113008839 B CN 113008839B CN 202110191385 A CN202110191385 A CN 202110191385A CN 113008839 B CN113008839 B CN 113008839B
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任元
吴昊
熊振宇
刘政良
刘通
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Abstract

本发明涉及一种有机物半导体微腔玻色‑爱因斯坦凝聚涡旋产生装置。它主要包括激发光产生、玻色‑爱因斯坦凝聚涡旋产生以及采集探测终端三部分,第一部分主要包括飞秒激光器、光学参量放大器和涡旋波片,第二部分主要包括激发光路和有机物样品仓,第三部分主要包括采集光路和图像分析终端。首先,飞秒激光器产生飞秒激光,飞秒激光通过激光器控制端控制后波长被调制为405nm,并通过涡旋波片转化为飞秒涡旋光束;随后,光束被照射到样品表面,激发产生玻色‑爱因斯坦凝聚;然后,利用电荷耦合传感器相机和光谱仪分别采集样品受激自发辐射光信号;最后,根据电荷耦合传感器相机观察到的有机物样品所产生的激射现象,并配合光谱仪从而判断有机物半导体微腔玻色‑爱因斯坦凝聚激发的产生。本装置结构简单,操作方便,开辟了一种有机物半导体微腔玻色‑爱因斯坦凝聚涡旋产生的新装置。

Figure 202110191385

The invention relates to an organic semiconductor microcavity Bose-Einstein condensed vortex generating device. It mainly includes three parts: excitation light generation, Bose-Einstein condensate vortex generation and acquisition and detection terminal. The first part mainly includes femtosecond laser, optical parametric amplifier and vortex wave plate, and the second part mainly includes excitation light path and organic matter The sample chamber, the third part mainly includes the acquisition optical path and the image analysis terminal. First, the femtosecond laser generates a femtosecond laser, the wavelength of the femtosecond laser is modulated to 405 nm after being controlled by the laser control terminal, and converted into a femtosecond vortex beam by a vortex wave plate; then, the beam is irradiated on the surface of the sample, and the excitation produces Bose-Einstein condensate; then, the stimulated spontaneous emission light signal of the sample is collected by the charge-coupled sensor camera and the spectrometer; finally, according to the lasing phenomenon produced by the organic sample observed by the charge-coupled sensor camera, and the spectrometer is used to Determining the Generation of Bose-Einstein Condensation Excitation in Organic Semiconductor Microcavities. The device has simple structure and convenient operation, and opens up a new device for generating organic semiconductor microcavity Bose-Einstein condensed vortex.

Figure 202110191385

Description

一种有机物半导体微腔玻色-爱因斯坦凝聚涡旋产生装置An organic semiconductor microcavity Bose-Einstein condensate vortex generator

技术领域technical field

本发明主要涉及有机物半导体微腔、凝聚态、光电、信号处理领域,尤其是有机物半导体微腔中的玻色-爱因斯坦凝聚激发的形成、涡旋光束的产生、自发辐射图像的检测等技术方法。The invention mainly relates to the fields of organic semiconductor microcavity, condensed matter, optoelectronics and signal processing, in particular to the formation of Bose-Einstein condensation excitation in organic semiconductor microcavity, generation of vortex beam, detection of spontaneous radiation image and other technologies method.

技术背景technical background

玻色爱因斯坦凝聚体(Bose–Einstein condensate,BEC)是上世纪20年代由玻色和爱因斯坦提出的气体凝聚态,1995年康奈尔和威曼及其助手在天体物理实验室联合研究所成功实现真正的BEC。近年来人们发现有机物半导体微腔中的激子极化激元系统能够在常温下实现BEC,这一发现极大地激发了人们对有机物半导体微腔激子极化激元的研究热情,其常温超流特性展现出巨大的科研与应用价值,但新型有机物半导体中光子-激子耦合的研究还处于初级阶段。在有机物半导体中,激子极化激元的拉比分裂可以达到上百meV,所以有机物激子极化激元的发射波长可调的范围也非常大,耦合强、成本低、波长可调谐的有机物半导体激子极化激元在玻色-爱因斯坦凝聚中有着重要的应用前景。此外由于激子极化激元的陀螺效应,使用带轨道角动量的涡旋光激发产生的激子极化激元对研究新型陀螺也有着重大意义。Bose–Einstein condensate (BEC) is a gas condensate proposed by Bose and Einstein in the 1920s. The Institute succeeds in realizing a true BEC. In recent years, it has been discovered that the exciton polariton system in the organic semiconductor microcavity can realize BEC at room temperature. Flow properties show great scientific and application value, but the research on photon-exciton coupling in new organic semiconductors is still in its infancy. In organic semiconductors, the Rabi splitting of exciton polaritons can reach hundreds of meV, so the emission wavelength range of organic exciton polaritons is also very large, strong coupling, low cost, and wavelength tunable. Organic semiconductor exciton polaritons have important application prospects in Bose-Einstein condensation. In addition, due to the gyroscopic effect of exciton polariton, the use of exciton polariton generated by vortex light excitation with orbital angular momentum is also of great significance for the study of new gyroscopes.

发明内容SUMMARY OF THE INVENTION

本发明的技术解决问题是:针对当前有机物半导体微腔中激子极化涡旋的难以直接、简便的制备的问题,本发明已在通过设计实验光路,使得涡旋光的制备与激子极化激元的激发装置有机结合,并通过光谱仪验证激子极化激元的产生。The technical problem solved by the present invention is: in view of the difficulty of direct and simple preparation of exciton polarized vortex in the current organic semiconductor microcavity, the present invention has designed an experimental optical path to make the preparation of vortex light and exciton polarized vortex. The excitation device of the exciton is organically combined, and the generation of the exciton polariton is verified by a spectrometer.

本发明的技术解决方案是:本发明涉及一种有机物半导体微腔玻色-爱因斯坦凝聚涡旋产生装置,如图1所示,其主要部件包括:飞秒激光器(1)、激光器控制端(2)、光学参量放大器(3)、平面反射镜(4)、线偏振片1(5)、四分之一波片(6)、涡旋波片(7)、线偏振片2(8)、分光镜1(9)、样品仓(10)、显微物镜(11)、分光镜2(12)、准直透镜1(13)、短波通滤波片(14)、准直透镜2(15)、电荷耦合传感器相机(16)、图像采集处理终端(17)、陷波片(18)、光谱仪(19)、分束镜3(20)、白光光源(21)。首先,通过使用白光光源(21),将样片仓(10)中的样品调整至电荷耦合传感器相机(16)视野中的合适位置,关掉白光光源(21),打开飞秒激光器(1)产生飞秒激光束,通过激光器控制端(2),控制飞秒激光器(1)和光学参量放大器(2)使得飞秒激光束转换为设定功率和频率的飞秒激光束,光束经过平面反射镜(4)后经过线偏振片1(5)、四分之一波片(6)和涡旋波片(7),出射光束再经过线偏振片2(8)转换为飞秒涡旋光束。光束通过分束镜2(12)后经显微物镜(11)照射在有机物样品仓(10)。此时,样品表面会产生自发辐射图样。图样通过显微物镜(11)和分光镜2(12),随后依次通过准直透镜1(13)、准直透镜2(14)和滤波片(15)滤去泵浦光后,经过分束镜3(20)分为两束,分别被电荷耦合传感器相机(16)和光谱仪(19)采集并传输数据至图像采集处理终端(17)分析处理。通过对激光器控制端(2)的参数控制实时调节激发光的功率和频率,当功率低于产生玻色-爱因斯坦凝聚的阈值时,样品仅观察到荧光现象;进一步增大功率时样品会发生激射现象,观察到明显的光强变化;而当继续增大功率时,样品将会被烧蚀损毁。装置不仅产生涡旋光并通过光路照射到样品上,而且还可利用图像采集处理终端的信息实时观测玻色-爱因斯坦凝聚激发的现象。The technical solution of the present invention is: the present invention relates to an organic semiconductor microcavity Bose-Einstein condensed vortex generating device, as shown in FIG. 1 , the main components of which include: a femtosecond laser (1), a laser control terminal (2), optical parametric amplifier (3), plane mirror (4), linear polarizer 1 (5), quarter wave plate (6), vortex wave plate (7), linear polarizer 2 (8) ), beam splitter 1 (9), sample chamber (10), microscope objective lens (11), beam splitter 2 (12), collimating lens 1 (13), short-wave pass filter (14), collimating lens 2 ( 15), a charge-coupled sensor camera (16), an image acquisition and processing terminal (17), a notch plate (18), a spectrometer (19), a beam splitter 3 (20), and a white light source (21). First, by using a white light source (21), adjust the sample in the sample chamber (10) to an appropriate position in the field of view of the charge-coupled sensor camera (16), turn off the white light source (21), and turn on the femtosecond laser (1) to generate The femtosecond laser beam, through the laser control terminal (2), controls the femtosecond laser (1) and the optical parametric amplifier (2) so that the femtosecond laser beam is converted into a femtosecond laser beam with a set power and frequency, and the beam passes through the plane mirror (4) After passing through the linear polarizer 1 (5), the quarter wave plate (6) and the vortex wave plate (7), the outgoing beam is converted into a femtosecond vortex beam through the linear polarizer 2 (8). The light beam passes through the beam splitter 2 (12) and then is irradiated on the organic sample chamber (10) through the microscope objective lens (11). At this time, a spontaneous emission pattern will be generated on the surface of the sample. The pattern passes through the microscope objective lens (11) and the beam splitter 2 (12), and then passes through the collimating lens 1 (13), the collimating lens 2 (14) and the filter (15) in order to filter out the pump light, and then passes through the beam splitting The mirror 3 (20) is divided into two beams, which are respectively collected by a charge-coupled sensor camera (16) and a spectrometer (19) and transmit data to an image collection and processing terminal (17) for analysis and processing. The power and frequency of the excitation light are adjusted in real time by controlling the parameters of the laser control terminal (2). When the power is lower than the threshold for generating Bose-Einstein condensation, only fluorescence is observed in the sample; when the power is further increased, the sample will A lasing phenomenon occurs, and a significant change in light intensity is observed; and when the power continues to increase, the sample will be destroyed by ablation. The device not only generates vortex light and irradiates the sample through the optical path, but also can use the information of the image acquisition and processing terminal to observe the phenomenon of Bose-Einstein condensation excitation in real time.

本发明的原理是:The principle of the present invention is:

(1)基于超流特性的激子极化激元产生(1) Generation of exciton polaritons based on supercurrent properties

超流(Super Fluidity)是一种宏观范围内的量子效应。由于玻色-爱因斯坦凝聚,原子会形成一个紧密的集体,超流正是这种现象的具体表现。物理学界对超流、量子涡旋的研究持续了近一个世纪,超冷原子凝聚的发展为此领域的研究提供了极具可操控性的理想平台。P.Kapitza首次观测到玻色液体的超流现象,并因此获得1978年诺贝尔物理学奖;L.Landau提出了超流体的量子理论,解释并预言了超流体的许多重要性质,获得1962年诺贝尔物理学奖;A.A.Abrikosov通过求解Ginzburg–Landau方程,发现量子涡旋会遵循能量最低原则,排列成周期性的晶格结构;A.Leggett提出了一种新的量子理论,揭示了液氦-3费米超流的机理,他们因此分享了2003年诺贝尔物理学奖。Super fluidity is a quantum effect on a macroscopic scale. Superfluidity is a concrete manifestation of this phenomenon, in which atoms form a tight group due to Bose-Einstein condensation. The research on superfluid and quantum vortex in the field of physics has lasted for nearly a century, and the development of ultracold atomic condensation provides an ideal platform for research in this field. P.Kapitza first observed the superfluid phenomenon of Bose liquid, and won the Nobel Prize in Physics in 1978; L.Landau proposed the quantum theory of superfluid, explained and predicted many important properties of superfluid, won the 1962 Nobel Prize in Physics; A.A.Abrikosov discovered by solving the Ginzburg–Landau equation that quantum vortices follow the principle of the lowest energy and are arranged in a periodic lattice structure; A. Leggett proposed a new quantum theory, revealing liquid helium -3 Mechanism of Fermi superfluid, they shared the 2003 Nobel Prize in Physics.

不同于宏观物体,微观粒子除了坐标空间的动量外,还有一种“内部”角动量——即自旋。具有半整数自旋的粒子称为费米子,如电子、夸克、中微子,它们的自旋为1/2。具有整数自旋的粒子叫玻色子、如胶子、光子、引力子、W及Z玻色子,它们的自旋为1。对于费米子,由于泡利不相容原理的缘故,每个状态只允许填一个粒子。而对于玻色子,粒子在各状态上的填充数不受限制。温度降到一个特定值后,越来越多的玻色子处于能量最低的,也就是动量为零的状态,而这个现象就是玻色-爱因斯坦凝聚。Unlike macroscopic objects, microscopic particles have an "internal" angular momentum, namely spin, in addition to the momentum in the coordinate space. Particles with half-integer spins are called fermions, such as electrons, quarks, neutrinos, and their spin is 1/2. Particles with integer spins are called bosons, such as gluons, photons, gravitons, W and Z bosons, and their spin is 1. For fermions, due to the Pauli exclusion principle, only one particle is allowed to fill each state. For bosons, however, there is no limit to the number of particles that fill each state. After the temperature drops to a certain value, more and more bosons are in the lowest energy state, that is, their momentum is zero, and this phenomenon is called Bose-Einstein condensation.

(2)基于下支激子极化激元的玻色-爱因斯坦凝聚(2) Bose-Einstein Condensation Based on Lower Branch Exciton Polariton

激子极化激元是由激子场和光子场相互耦合而形成的准粒子,由于激子-光子的耦合问题是二次型的,所以可以解析得出对角化激子极化激元的Hamilton量H为:The exciton polariton is a quasiparticle formed by the mutual coupling of the exciton field and the photon field. Since the exciton-photon coupling problem is quadratic, the diagonalized exciton polariton can be obtained analytically. The Hamilton quantity H is:

Figure BDA0002944324380000031
Figure BDA0002944324380000031

其中,

Figure BDA0002944324380000041
为约化普朗克常量,k表示波矢,ωX(k)和ωC(k)分别表示激子场和光子场的色散,而激子与光子间的耦合就可以用矩阵中的元素ΩR描述,称之为Rabi劈裂。in,
Figure BDA0002944324380000041
In order to reduce Planck's constant, k represents the wave vector, ω X (k) and ω C (k) represent the dispersion of the exciton field and the photon field, respectively, and the coupling between the excitons and photons can be determined by the elements in the matrix Ω R description, called Rabi splitting.

这个矩阵的本征值由下述方程给出,即:The eigenvalues of this matrix are given by the following equations, namely:

Figure BDA0002944324380000042
Figure BDA0002944324380000042

显然从上式,我们可以得到激子极化激元的两支色散关系,即:Obviously, from the above formula, we can obtain the two-branch dispersion relation of the exciton polariton, namely:

Figure BDA0002944324380000043
Figure BDA0002944324380000043

上式中的ωUP(k)和ωLP(k)分别表示激子极化激元的上支和下支两支色散关系,激子极化激元的Bose-Einstein凝聚就是指下支激子极化激元的凝聚,激子极化激元的涡旋叠加态也是由下支激子极化激元形成的。In the above formula, ω UP (k) and ω LP (k) represent the dispersion relation of the upper branch and the lower branch of the exciton polariton, respectively, and the Bose-Einstein condensation of the exciton polariton refers to the lower branch excitation. The condensation of the subpolariton, the vortex superposition state of the exciton polariton is also formed by the lower branch exciton polariton.

(3)基于涡旋波片的涡旋光制备(3) Preparation of vortex light based on vortex wave plate

涡旋光是一种具有涡旋形光场分布的光束。涡旋光的传播具有柱对称性,这种光束中心区域的光场强度为零,该中心区域被称为光束奇点或相位奇点。在涡旋光传播过程中,奇点处光强始终保持为零。涡旋光的波前呈螺旋形,其波矢量有方位项,且绕着涡旋中心旋转,而因为这个旋转的存在使得涡旋光波携带了轨道角动量。涡旋光携带轨道角动量的特殊性质,使其不仅在物理学领域有着广泛的应用,而且在生物界和医学界也有着广阔的应用前景。涡旋波片是一种可以生成涡旋光束的光学元件,涡旋波片可以通过使用液晶、液晶聚合物配合先进的光配项技术实现。涡旋波片生成的涡旋光束在量子光学、光场调控、超分辨率成像、光束捕捉、激光加工等领域具有良好的应用前景。Vortex light is a light beam with a vortex-shaped light field distribution. The propagation of vortex light has cylindrical symmetry, and the optical field intensity is zero in the central region of the beam, which is called the beam singularity or phase singularity. During the propagation of vortex light, the light intensity at the singularity always remains zero. The wavefront of vortex light is spiral, and its wave vector has an azimuth term, and it rotates around the center of the vortex, and because of the existence of this rotation, the vortex light wave carries orbital angular momentum. The special properties of orbital angular momentum carried by vortex light make it not only have a wide range of applications in the field of physics, but also have broad application prospects in the biological and medical fields. Vortex wave plate is an optical element that can generate vortex beam. Vortex wave plate can be realized by using liquid crystal, liquid crystal polymer and advanced optical matching technology. Vortex beams generated by vortex wave plates have good application prospects in the fields of quantum optics, light field manipulation, super-resolution imaging, beam trapping, and laser processing.

涡旋波片的琼斯矩阵M可以表示为:The Jones matrix M of the vortex plate can be expressed as:

Figure BDA0002944324380000051
Figure BDA0002944324380000051

其中R(θ)是旋转矩阵:where R(θ) is the rotation matrix:

Figure BDA0002944324380000052
Figure BDA0002944324380000052

当入射光为左旋圆偏振光时,入射光场为

Figure BDA0002944324380000053
E0表示光场强度,则出射光场为:When the incident light is left-handed circularly polarized light, the incident light field is
Figure BDA0002944324380000053
E 0 represents the intensity of the light field, then the outgoing light field is:

Figure BDA0002944324380000054
Figure BDA0002944324380000054

当入射光为左旋圆偏振光时,入射光场为

Figure BDA0002944324380000055
则出射光场为:When the incident light is left-handed circularly polarized light, the incident light field is
Figure BDA0002944324380000055
Then the outgoing light field is:

Figure BDA0002944324380000056
Figure BDA0002944324380000056

其中,exp(i2θ(x,y))与exp(-i2θ(x,y))即为螺旋相位因子,可见,入射为左旋圆偏振光时候,经过涡旋波片后变成右旋圆偏振涡旋光束;入射为右旋圆偏振光时,经过涡旋波片后变成左旋圆偏振涡旋光束。Among them, exp(i2θ(x,y)) and exp(-i2θ(x,y)) are the helical phase factors. It can be seen that when the incident is left-handed circularly polarized light, it becomes right-handed circularly polarized after passing through the vortex wave plate. Vortex beam; when the incident is right-handed circularly polarized light, it becomes a left-handed circularly polarized vortex beam after passing through the vortex wave plate.

本发明的主要优点:The main advantages of the present invention:

(1)结构简单,各元器件位置固定,变量仅激光器控制端控制飞秒光束功率和频率,易于控制。(1) The structure is simple, the position of each component is fixed, and the variable is only controlled by the laser control end to control the power and frequency of the femtosecond beam, which is easy to control.

(2)本装置适用范围广。根据设计装置可以看出,实验所用的飞秒激光波长可调,可以适用各个波长的泵浦光来激发玻色-爱因斯坦凝聚,并用来研究不同波长的泵浦光的激发阈值。(2) The device has a wide range of applications. According to the designed device, it can be seen that the wavelength of the femtosecond laser used in the experiment is adjustable, and the pump light of each wavelength can be used to excite the Bose-Einstein condensation, and it can be used to study the excitation threshold of the pump light of different wavelengths.

(3)本装置在制备涡旋光方面方式灵活,在光路中可以更换不同的涡旋波片以形成不同拓扑荷数的涡旋光,进而实现不同拓扑荷数涡旋光激发产生的激子极化激元凝聚的形成以及涡旋制备效果。(3) The device is flexible in the preparation of vortex light, and different vortex wave plates can be replaced in the optical path to form vortex lights with different topological charge numbers, thereby realizing exciton polarization excitation generated by vortex light excitation of different topological charge numbers. Formation of meta-agglomerates and effects of vortex preparation.

附图说明Description of drawings

图1为检测装置示意图;1 is a schematic diagram of a detection device;

图2涡旋光光场强度图;Figure 2. The intensity map of the vortex light field;

图3有机物样品示意图;Figure 3 is a schematic diagram of organic matter samples;

图4激子极化激元激射示意图;Fig. 4 Schematic diagram of exciton polariton lasing;

图5激射光谱示意图;Figure 5 is a schematic diagram of a lasing spectrum;

具体实施方案specific implementation

本发明以涡旋光与半导体微腔中的激子极化激元耦合形成的自发辐射干涉图样为测量载体,具体实施步骤如下:The present invention uses the spontaneous emission interference pattern formed by the coupling of the vortex light and the exciton polariton in the semiconductor microcavity as the measurement carrier, and the specific implementation steps are as follows:

首先,先将样品放置在样品仓中,利用白光光源(21)和电荷耦合传感器相机(16)观察样品的空间位置,结合图像采集处理终端(17)将样品调整至如图3的位置,使得样品在视野范围内有较好的观察区域后,关闭白光光源(21),打开飞秒激光器(1),通过激光器控制端(2)控制飞秒激光器(1)和光学参量放大器(3),使得从飞秒激光器中出射的基本光转换为特定功率和频率的飞秒光束。First, place the sample in the sample chamber, use the white light source (21) and the charge-coupled sensor camera (16) to observe the spatial position of the sample, and adjust the sample to the position shown in Figure 3 in conjunction with the image acquisition and processing terminal (17), so that After the sample has a good observation area within the field of view, turn off the white light source (21), turn on the femtosecond laser (1), and control the femtosecond laser (1) and the optical parametric amplifier (3) through the laser control terminal (2), The fundamental light emitted from the femtosecond laser is converted into a femtosecond beam of a specific power and frequency.

产生的飞秒光束通过平面镜(4)的反射先后通过线偏振片1(5)、四分之一波片(6)、涡旋波片(7)和线偏振片2(8)后转变为如图2的飞秒涡旋光束,经分束镜1(9)和分束镜2(12)后进入显微物镜(11),光束汇聚后照射到样片仓(10)中的样品上,激发产生有机物半导体微腔的玻色-爱因斯坦凝聚并放出激射光。The generated femtosecond beam is reflected by the plane mirror (4) and then successively passes through the linear polarizer 1 (5), the quarter wave plate (6), the vortex wave plate (7) and the linear polarizer 2 (8) and then converted into a The femtosecond vortex beam as shown in Figure 2 enters the microscope objective lens (11) after passing through the beam splitter 1 (9) and the beam splitter 2 (12), and the beam converges and irradiates the sample in the sample chamber (10), Bose-Einstein condensates that generate organic semiconductor microcavities are excited and emit lasing light.

激射光经过显微物镜(11)、分束镜2(12)后进入采集光路,其中准直透镜1(13)、准直透镜2(15)将光路准直,短波通滤波片(14)将反射回的杂散波滤去,经分束镜3(20)后,一束光通过陷波片(18)滤去泵浦光后被电荷耦合传感器相机(16)接收,另一束光被光谱仪(19)传感接收,通过图像采集处理终端(17)观察产生的激射。其中电荷耦合传感器相机得到的图像如图4所示,可以明显看到激射区域的产生;光谱仪得到的图像如图5所示,在490nm附近观察到激射的出现,进而验证了激子极化激元凝聚的产生。The laser light enters the collection optical path after passing through the microscope objective lens (11) and the beam splitter 2 (12), wherein the collimating lens 1 (13) and the collimating lens 2 (15) collimate the optical path, and the short-wave pass filter (14) The reflected stray wave is filtered out, and after passing through the beam splitter 3 (20), one beam of light passes through the notch filter (18) to filter out the pump light and is received by the CCD camera (16), and the other beam of light is received by the CCD camera (16). It is sensed and received by the spectrometer (19), and the generated lasing is observed through the image acquisition and processing terminal (17). The image obtained by the charge-coupled sensor camera is shown in Figure 4, and the generation of the lasing region can be clearly seen; the image obtained by the spectrometer is shown in Figure 5, and the appearance of lasing is observed near 490 nm, which further verifies the exciton pole. The generation of excimer condensation.

本发明书中未作详细描述的内容属于本领域专业技术人员公知的现有技术。Contents not described in detail in the present invention belong to the prior art known to those skilled in the art.

Claims (2)

1. An organic semiconductor micro-cavity glass-Einstein condensation vortex generating device, comprising: the device comprises a femtosecond laser (1), a laser control end (2), an optical parametric amplifier (3), a plane reflector (4), a linear polarizer 1 (5), a quarter-wave plate (6), a vortex wave plate (7), a linear polarizer 2 (8), a beam splitter 1 (9), a sample bin (10), a microscope objective (11), a beam splitter 2 (12), a collimating lens 1 (13), a short-wave-pass filter (14), a collimating lens 2 (15), a charge coupled sensor camera (16), an image acquisition processing terminal (17), a trap plate (18), a spectrometer (19), a beam splitter 3 (20) and a white light source (21); the method comprises the steps that a femtosecond laser is utilized to generate a beam of femtosecond pulse laser, the generated femtosecond beam is reflected by a plane reflector (4) to be converted into a femtosecond vortex beam through a linear polarizer 1 (5), a quarter wave plate (6), a vortex wave plate (7) and a linear polarizer 2 (8), the femtosecond vortex beam enters a microscope objective (11) through a beam splitter 1 (9) and a beam splitter 2 (12), the beam is converged and then irradiated on a sample in a sample bin (10), and the vitrescence-einstein coagulation of an organic semiconductor microcavity is generated through excitation and emitted laser light is emitted; laser light enters a collection light path after passing through a microscope objective (11) and a beam splitter 2 (12), wherein the light path is collimated by a collimating lens 1 (13) and a collimating lens 2 (15), reflected stray waves are filtered by a short wave pass filter (14), after passing through a beam splitter 3 (20), one beam of light is received by a charge coupled sensor camera (16) after being filtered by pump light by a trap wave plate (18), the other beam of light is sensed and received by a spectrometer (19), and the generated laser is observed by an image collection processing terminal (17).
2. The organic semiconductor microcavity vitreous color-einstein condensed vortex generating device according to claim 1, wherein the device is characterized in that: the power and the frequency of the emergent femtosecond laser are changed by continuously changing the control coefficient of the laser control end, so that the femtosecond laser with different power and frequency is irradiated on the surface of a sample to generate stimulated radiation; the radiation light passes through the collection light path and passes through the beam splitter, one beam of the radiation light is collected by the charge coupled sensor camera, the other beam of the radiation light is collected by the spectrometer, the image collection processing terminal is used for carrying out real-time analysis processing on the collected signals, and whether the sample is stimulated to radiate or not and generate glass color-Einstein condensation is judged in real time by combining the spectrometer.
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