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CN112082652B - An integrated array polarization imaging detector stacked with multilayer transparent black phosphorus sheets and a corresponding polarization information calculation method - Google Patents

An integrated array polarization imaging detector stacked with multilayer transparent black phosphorus sheets and a corresponding polarization information calculation method Download PDF

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CN112082652B
CN112082652B CN202010963096.7A CN202010963096A CN112082652B CN 112082652 B CN112082652 B CN 112082652B CN 202010963096 A CN202010963096 A CN 202010963096A CN 112082652 B CN112082652 B CN 112082652B
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black phosphorus
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CN112082652A (en
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张然
段斌
褚金奎
樊元义
金仁成
崔岩
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Dalian University of Technology
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
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    • G01J4/04Polarimeters using electric detection means

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Abstract

本发明公开了一种多层透明黑磷片堆叠的集成阵列式偏振成像探测器以及相应的偏振信息计算方法。偏振成像探测器由多个探测器单元排列而成,每个探测器单元由三层功能层和基底支撑层构成,功能层结构以透明黑磷片作为光敏层和导电沟道层,辅以电极和保护绝缘介质,并加以外围电路。以功能层为结构单元,沿光路方向堆叠多层可实现实时高分辨率的偏振探测。当偏振光照射器件时,由于黑磷片本身的特性,只对沿黑磷片的AC方向(Armchair)的偏振光吸收最大,其他方向会存在透射,所以多个角度的黑磷片的堆叠结构,可以在同一位置实时测量得到多个方向的光强信息。在黑磷片内载流子在外加电势驱动下单向运动,产生响应信号并实现偏振光光强的探测,并通过特定的算法求解出目标光束信息。该探测器解决了现有偏振探测空间不一致的问题,具有高度集成化、无分辨率损失、实时性好等特点,适用于偏振探测成像、导航等领域。

Figure 202010963096

The invention discloses an integrated array polarization imaging detector stacked with multilayer transparent black phosphorus sheets and a corresponding polarization information calculation method. The polarization imaging detector is composed of a plurality of detector units. Each detector unit is composed of three functional layers and a substrate support layer. The functional layer structure uses a transparent black phosphorus sheet as a photosensitive layer and a conductive channel layer, supplemented by electrodes. And protective insulating medium, and add peripheral circuits. Taking the functional layer as the structural unit, stacking multiple layers along the direction of the optical path can realize real-time high-resolution polarization detection. When polarized light illuminates the device, due to the characteristics of the black phosphorus sheet itself, only the polarized light along the AC direction (Armchair) of the black phosphorus sheet is absorbed the most, and there will be transmission in other directions, so the stacking structure of black phosphorus sheets with multiple angles , the light intensity information in multiple directions can be obtained by real-time measurement at the same position. The carriers in the black phosphorus sheet move unidirectionally under the driving of an applied potential, generate a response signal and realize the detection of the intensity of polarized light, and solve the target beam information through a specific algorithm. The detector solves the problem of inconsistency in the existing polarization detection space, and has the characteristics of high integration, no resolution loss, and good real-time performance, and is suitable for polarization detection imaging, navigation and other fields.

Figure 202010963096

Description

Integrated array type polarization imaging detector with multilayer transparent black phosphorus sheet stacking and corresponding polarization information calculation method
Technical Field
The invention relates to the technical field of polarization measurement, in particular to an integrated array type polarization imaging detector with stacked multilayer transparent black phosphorus sheets and a corresponding polarization information calculation method, which are designed by utilizing the polarization sensitivity, the light transmittance and the dichroism of the black phosphorus sheets.
Background
With the great development of industrialization, the photoelectric detection technology is more and more widely applied in the military and industrial fields of modern society, the photoelectric detection process is a process of acquiring light wave information, the light wave is an electromagnetic wave, and the utilization degree of information carried by the light wave determines whether a more accurate result can be obtained. The traditional detection means focuses on the detection of light intensity and wavelength, and ignores the polarization of another important inherent property of the light wave. Compared with most adopted intensity detection, the realization of polarization detection can expand information from an information set of light intensity, spectrum and space to a more comprehensive information set of light intensity, spectrum, space, polarization degree and polarization azimuth angle, and can obtain more accurate and effective results, thereby improving the precision of target detection and geographic substance identification. Currently, polarization detection is widely applied to a plurality of key fields such as meteorological detection, biological tissue detection, integrated navigation, underwater detection, geological exploration, soil analysis and the like.
The existing polarized light imaging detector mostly adopts an integrated array structure of a sub-focal plane, the sub-focal plane polarization detection means that a polarization element array is integrated on a focal plane of the detector, and a single unit of the array corresponds to a single pixel of the focal plane. The minimum period unit of the polarization element array is composed of 2 multiplied by 2 polarization units, and a super pixel is formed. In the polarization element array, one super pixel is composed of a plurality of polarizing plates, wave plates or polarization rotators, wherein the polarization direction, the angle of the wave plates, the retardation of the wave plates and the angle of polarization rotation of the polarizing plates are different. Therefore, a plurality of units in one super pixel can form measurement of different polarization states of incident light, the Stokes vector of the measured light can be reconstructed, and polarization imaging can be further realized. However, the polarization detection system of the sub-focal plane performs simultaneous polarization detection through grating structures of different focal planes at different angles in a two-dimensional plane, interpolation calculation needs to be performed by using an algorithm, the real-time performance is good, but the spatial resolution of the measured information is low, and the problem of spatial inconsistency exists.
Under the condition of ensuring the integration level, the key technology of the polarized light detection detector capable of simultaneously ensuring the time resolution and the space resolution is to realize that the light intensity information of multiple angles can be simultaneously measured at one point in the space, so that the design and development of a new polarized detection detector structure are required. However, the traditional photoelectric detection method relying on the metal nano-grating relies on the high light transmittance TM and the high extinction ratio of the grating, and does not have the basis for realizing new idea. Therefore, it is urgent to search for new semiconductor materials and new functional structures to realize polarization detection with higher accuracy. In the aspect of new materials, the black phosphorus is found to have strong intrinsic plane anisotropy, and can be used for polarized light detection in multiple wave bands such as ultraviolet, terahertz, visible light, infrared and the like; compared with other materials, the black phosphor plate has considerable advantage of light transmittance in a visible light band. Based on the advantages, the integrated array type polarization real-time imaging detector with the multilayer transparent black phosphorus plate stack is provided and designed for solving the problem of space inconsistency of the existing polarization detector, the time resolution can be guaranteed, the detection space resolution can be guaranteed, and the integration level is higher than that of the traditional imaging detector.
Disclosure of Invention
In view of the defects of the prior art, the invention provides an integrated array type polarization imaging detector with stacked multilayer transparent black phosphorus sheets and a corresponding polarization information calculation method, which solve the problem of inconsistent space of the traditional polarization detector, can ensure the time resolution and the space resolution simultaneously, and provide a polarized light detection scheme with higher precision.
The invention provides an integrated array type polarization real-time imaging detector with stacked multilayer transparent black phosphorus sheets, wherein a detection unit of the polarization light detector sequentially comprises a top protective layer, a top metal electrode pair, a top 0-degree black phosphorus sheet, a first dielectric layer, a middle layer metal electrode pair, a middle layer 60-degree black phosphorus sheet, a second dielectric layer, a bottom metal electrode pair, a bottom 120-degree black phosphorus sheet and a bottom supporting layer from top to bottom, wherein the top protective layer, the top metal electrode pair, the top 0-degree black phosphorus sheet and the first dielectric layer are manufactured on the top 0-degree black phosphorus sheet, the middle layer metal electrode pair, the middle layer 60-degree black phosphorus sheet and the second.
In some embodiments, the top protective layer, the first dielectric layer, the second dielectric layer, and the bottom supporting layer may be optical thin film layers of silicon dioxide, zinc sulfide selenide, zinc oxide, yttrium oxide, cerium oxide, niobium oxide, titanium dioxide, titanium trioxide, titanium monoxide, tantalum pentoxide, silicon carbide, silicon nitride, or the like; further, the combination of the above-described optional optical material thin film layers may be used.
In some embodiments, the top, middle, and bottom metal electrode pairs are gold, titanium, or chromium electrodes.
In some embodiments, the top 0 ° black phosphor, the middle 60 ° black phosphor and the bottom 120 ° black phosphor refer to 0 ° directions of the XY plane of the spatial coordinate system with the AC direction of the top black phosphor as the space coordinate system, and the middle and bottom black phosphors correspond to black phosphors placed in 60 ° and 120 ° directions of the XY plane of the AC direction spatial coordinate system, and further, the above angles are not fixed to 0 °, 60 ° and 120 °, and may be any different angles.
In some embodiments, the black phosphorus sheet has a thickness of 5 to 60 nanometers.
In some embodiments, the detector unit is composed of three functional layers and a substrate support layer, the functional layer structure takes transparent black phosphorus sheets as a photosensitive layer and a conductive channel layer, is supplemented with electrodes and protective insulating media, and is added with peripheral circuits, and pixels of the polarization imaging detector of the detector unit array correspond to pixels of the polarization imaging detector one by one.
The invention provides a corresponding polarization information calculation method of an integrated array type polarization imaging detector stacked by multilayer transparent black phosphorus sheets, which is characterized in that the information measured by the detector is calculated by the following steps:
assume that the Stokes vector of the incident light is S0=(I,Q,U,V)TWherein I is unpolarized light intensity, Q and U respectively represent linearly polarized light in two directions, V represents circularly polarized light, circularly polarized light component can be ignored in the detectable range of the instrument, so it is 0 to take V here, that is S0=(I,Q,U,0)T
The AC (X) direction of the black phosphorus of the first layer is set to be a 0-degree direction in an XY plane in a space coordinate system, the AC (X) direction of the black phosphorus of the second layer is set to be a 60-degree direction in the XY plane, and the AC (X) direction of the black phosphorus of the third layer is set to be a 120-degree direction in the XY plane.
The phase delay caused by the black phosphor can be expressed as
Figure GDA0003052957290000031
Here, d denotes a black phosphor sheet thickness, n denotes a real part of a complex refractive index, and λ denotes an incident light wavelength.
Let P1And P2Amplitude transmittances in the AC (X) and ZZ (Y) directions, respectively, the Mueller matrix of the black phosphor sheet can be expressed as
Figure GDA0003052957290000032
Further, the black phosphor patch rotated by the angle θ can be expressed as a black phosphor patch using a Mueller matrix
Figure GDA0003052957290000041
And further can show the conversion process of the Stokes vectors of incidence and emergence of each layer, namely the incident light S0=(I,Q,U,0)TThe transformation through the first layer of black phosphorus can be expressed as
S1=MΔ,0S0=(I',Q',U',0)T
Wherein, I ' is the unpolarized light intensity after passing through the first layer of black phosphorus, and Q ' and U ' are linearly polarized light respectively representing two directions after passing through the first layer of black phosphorus; similarly, the transformation of the second layer may be expressed as
S2=MΔ,60S1=MΔ,60MΔ,0S0=(I”,Q”,U”,0)T
Wherein, I ' is the unpolarized light intensity after passing through the second layer of black phosphorus, and Q ' and U ' are respectively linearly polarized light in two directions after passing through the second layer of black phosphorus;
the light intensity values corresponding to the black phosphorus sheets at different angles can be calculated according to the current variation collected by each layer of the detector
Figure GDA0003052957290000042
Four parameters I, Q and U of the Stokes vector of the incident light can be obtained, and the degree of linear polarization (DoLP) and the polarization angle (AoP) of the polarized light can be obtained
Figure GDA0003052957290000043
Figure GDA0003052957290000044
The invention has the following advantages:
the multi-directional polarization information acquisition device has the advantages that the multi-layer detection structure is adopted, multi-directional polarization information can be measured in real time according to the anisotropic light transmittance and anisotropic polarization absorption of the detection material, the time resolution can be guaranteed, and the detection spatial resolution can be guaranteed.
And the black phosphorus which is a novel low-dimensional material is used as a detection core, has stronger intrinsic plane anisotropy and has the advantages of high carrier mobility, quick response and the like.
The polarized light high-precision detector adopting the black phosphorus plate can directly detect the polarized light by utilizing the intrinsic anisotropy of the material and can detect the polarized light in multiple wave bands such as ultraviolet, terahertz, visible light, infrared and the like.
Based on the reasons, the invention solves the problem of inconsistent space of the existing detector, can ensure the time resolution and the detection spatial resolution at the same time, and has higher integration level than the prior detector.
Drawings
FIG. 1 is a schematic perspective view of the detector of the present invention;
FIG. 2 is a perspective view of a detector detection unit of the present invention;
FIG. 3 is a graph of the intensity of absorbed light versus incident light for example 1.
Wherein: 1 top metal electrode pair, 2 top protective layer, 3 top 0 degree black phosphorus sheet, 4 medium layer I, 5 middle layer metal electrode pair, 6 middle layer 60 degree black phosphorus sheet, 7 medium layer II, 8 bottom metal electrode pair, 9 bottom 120 degree black phosphorus sheet, 10 bottom supporting layer.
Detailed Description
The following detailed description of embodiments of the present patent refers to the accompanying drawings.
As shown in fig. 1-3, the detection unit of the polarized light detector is sequentially, as viewed from top to bottom, a top protective layer 2, a top metal electrode pair 1, a top 0 ° black phosphor sheet 3, a first dielectric layer 4, a middle metal electrode pair 5, a middle 60 ° black phosphor sheet 6, a second dielectric layer 7, a bottom metal electrode pair 8, a bottom 120 ° black phosphor sheet 9 and a bottom support layer 10, which are fabricated on the top 0 ° black phosphor sheet.
In some embodiments, the top protective layer 2, the dielectric layer one 4, the dielectric layer two 7, and the bottom support layer 10 may be optical thin film layers of silicon dioxide, zinc sulfide selenide, zinc oxide, yttrium oxide, cerium oxide, niobium oxide, titanium dioxide, titanium oxide, titanium sesquioxide, titanium oxide, titanium monoxide, tantalum pentoxide, silicon carbide, silicon nitride, or the like; further, the combination of the above-described optional optical material thin film layers may be used.
In some embodiments, the top layer metal electrode pair 1, the middle layer metal electrode pair 5, and the bottom layer metal electrode pair 8 are gold, titanium, or chromium electrodes.
In some embodiments, the top 0 black phosphor patch 3, the middle 60 black phosphor patch and 6 and the bottom 120 black phosphor patch 9 refer to 0 directions in the XY plane of the spatial coordinate system with the AC direction of the top black phosphor patch as the 0 direction, and the middle and bottom black phosphor patches correspond to the black phosphor disposed in the 60 and 120 directions in the XY plane of the AC direction spatial coordinate system, and further the angles are not fixed at 0 °, 60 ° and 120 °, and can be any of various angles.
In some embodiments, the black phosphorus sheet has a thickness of 5-60 nanometers.
In some embodiments, each dielectric layer has a thickness of 1-90 microns.
In some embodiments, the detector unit is composed of three functional layers and a substrate supporting layer, the functional layer structure takes transparent black phosphorus sheets as a photosensitive layer and a conductive channel layer, is supplemented with electrodes and protective insulating media and is added with peripheral circuits, and pixels of the polarization imaging detector of the detector unit array correspond to pixels of the polarization imaging detector one by one
The invention provides a corresponding polarization information calculation method of an integrated array type polarization imaging detector stacked by multilayer transparent black phosphorus sheets, which is characterized in that the information measured by the detector is calculated by the following steps:
assume that the Stokes vector of the incident light is S0=(I,Q,U,V)TWherein I is unpolarized light intensity, Q and U respectively represent linearly polarized light in two directions, V represents circularly polarized light, circularly polarized light component can be ignored in the detectable range of the instrument, so it is 0 to take V here, that is S0=(I,Q,U,0)T
The AC (X) direction of the black phosphorus of the first layer is set to be a 0-degree direction in an XY plane in a space coordinate system, the AC (X) direction of the black phosphorus of the second layer is set to be a 60-degree direction in the XY plane, and the AC (X) direction of the black phosphorus of the third layer is set to be a 120-degree direction in the XY plane.
The phase delay caused by the black phosphor can be expressed as
Figure GDA0003052957290000061
Here, d denotes a black phosphor sheet thickness, n denotes a real part of a complex refractive index, and λ denotes an incident light wavelength.
Let P1And P2Amplitude transmittances in the AC (X) and ZZ (Y) directions, respectively, the Mueller matrix of the black phosphor sheet can be expressed as
Figure GDA0003052957290000062
Further, the black phosphor patch rotated by the angle θ can be expressed as a black phosphor patch using a Mueller matrix
Figure GDA0003052957290000071
Further, the incident and emergent Stokes of each layer can be shownProcess of conversion of the Gaussian vector, incident light S0=(I,Q,U,0)TThe transformation through the first layer of black phosphorus can be expressed as
S1=MΔ,0S0=(I',Q',U',0)T
Wherein, I ' is the unpolarized light intensity after passing through the first layer of black phosphorus, and Q ' and U ' are linearly polarized light respectively representing two directions after passing through the first layer of black phosphorus;
similarly, the transformation of the second layer may be expressed as
S2=MΔ,60S1=MΔ,60MΔ,0S0=(I”,Q”,U”,0)T
Wherein, I ' is the unpolarized light intensity after passing through the second layer of black phosphorus, and Q ' and U ' are respectively linearly polarized light in two directions after passing through the second layer of black phosphorus;
the light intensity values corresponding to the black phosphorus sheets at different angles can be calculated according to the current variation collected by each layer of the detector
Figure GDA0003052957290000072
Four parameters I, Q and U of the Stokes vector of the incident light can be obtained, and the degree of linear polarization (DoLP) and the polarization angle (AoP) of the polarized light can be obtained
Figure GDA0003052957290000073
Figure GDA0003052957290000074
As shown in fig. 1, the present invention integrates a plurality of polarization detection units in an array on a quartz glass substrate. As shown in FIG. 2, each detection unit has a structure of three layers of black phosphor polarization absorption structures with different angles, which are made by stacking multiple layers of transparent black phosphors. Three layers of 38-nanometer black phosphorus sheets with different angles are vertically arranged on the quartz glass substrate 10, the included angles of the black phosphorus sheets are respectively 0 degree, 60 degrees and 120 degrees, the detection wavelength is 400 nanometers, the dielectric layer is silicon dioxide, and the thicknesses of the black phosphorus sheets are 91 nanometers, 258 nanometers and 283 nanometers from top to bottom in sequence. On the basis, the current variation is obtained by combining a detection circuit, and then the light intensity value is calculated, and further the polarization information is solved. As shown in fig. 3, it is depicted that in this configuration, the absorption intensity values of the respective layers of the detection unit vary with the angle of the incident light. The curve described by the rectangle is the light intensity value absorbed by the first layer of black phosphorus, the curve described by the circular frame is the light intensity value absorbed by the second layer of black phosphorus, and the curve described by the triangular frame is the light intensity value absorbed by the third layer of black phosphorus.
The above description is only a preferred embodiment of the present invention, but the scope of the present invention is not limited thereto, and those skilled in the art can easily conceive of changes or substitutions within the technical scope of the present invention. The protection scope of the present invention shall be subject to the protection scope of the claims.

Claims (7)

1.一种多层透明黑磷片堆叠的集成阵列式偏振成像探测器,探测器探测单元结构包括金属电极对(1)、顶层保护层(2)、顶层0°黑磷片(3)、介质层一(4)、中间层金属电极对(5)、中间层60°黑磷片(6)、介质层二(7)、底层金属电极对(8)、底层120°黑磷片(9)和底部支撑层(10),其特征在于:1. An integrated array polarization imaging detector stacked with multilayer transparent black phosphorus sheets, wherein the detector detection unit structure comprises a metal electrode pair (1), a top protective layer (2), a top 0° black phosphorus sheet (3), Dielectric layer one (4), intermediate layer metal electrode pair (5), intermediate layer 60° black phosphorus sheet (6), dielectric layer two (7), bottom metal electrode pair (8), bottom layer 120° black phosphorus sheet (9) ) and a bottom support layer (10), characterized in that: 所述偏振成像探测器的探测单元从上向下观察,依次是制作在顶层0°黑磷片上的顶层保护层(2)、顶层金属电极对(1)、顶层0°黑磷片(3)、介质层一(4)、制作在中间层60°黑磷片上的中间层金属电极对(5)、中间层60°黑磷片(6)、介质层二(7)、制作在底层120°黑磷片上的底层金属电极对(8)、底层120°黑磷片(9)和底部支撑层(10)。The detection unit of the polarization imaging detector is observed from top to bottom, and the top protective layer (2), the top metal electrode pair (1), and the top 0° black phosphorus sheet (3) are formed on the top 0° black phosphorus sheet in order. , dielectric layer one (4), intermediate layer metal electrode pair (5) made on the intermediate layer 60° black phosphorus sheet, intermediate layer 60° black phosphorus sheet (6), dielectric layer two (7), made on the bottom layer 120° Bottom metal electrode pair (8), bottom 120° black phosphorus sheet (9) and bottom support layer (10) on the black phosphorus sheet. 2.根据权利要求1所述的集成阵列式偏振成像探测器,其特征在于,所述顶层保护层(2)、介质层一(4)、介质层二(7)和底部支撑层(10)为二氧化硅、硫化锌硒化锌、氧化锌、氧化钇、氧化铈、氧化铌、二氧化钛、五氧化三钛、三氧化二钛、一氧化钛、五氧化二钽、碳化硅、氮化硅光学薄膜层;或者,为上述任意光学薄膜层的组合。2. The integrated array polarization imaging detector according to claim 1, wherein the top protective layer (2), the first dielectric layer (4), the second dielectric layer (7) and the bottom support layer (10) For silicon dioxide, zinc sulfide, zinc selenide, zinc oxide, yttrium oxide, cerium oxide, niobium oxide, titanium dioxide, titanium pentoxide, titanium dioxide, titanium monoxide, tantalum pentoxide, silicon carbide, silicon nitride An optical film layer; or, a combination of any of the above optical film layers. 3.根据权利要求1所述的集成阵列式偏振成像探测器,其特征在于,所述顶层金属电极对(1)、中间层金属电极对(5)和底层金属电极对(8)为金、钛或者铬电极。3. The integrated array polarization imaging detector according to claim 1, wherein the top metal electrode pair (1), the middle layer metal electrode pair (5) and the bottom metal electrode pair (8) are made of gold, Titanium or chromium electrodes. 4.根据权利要求1所述的集成阵列式偏振成像探测器,其特征在于,所述顶层0°黑磷片(3)、中间层60°黑磷片(6)与底层120°黑磷片(9)指以顶层黑磷片AC方向为空间坐标系XY平面的0°方向,中间层以及底层黑磷片相当于将黑磷置于片AC方向空间坐标系XY平面的60°和120°方向上。4. The integrated array polarization imaging detector according to claim 1, characterized in that the top layer 0° black phosphorus sheet (3), the middle layer 60° black phosphorus sheet (6) and the bottom layer 120° black phosphorus sheet (9) refers to the 0° direction of the XY plane of the space coordinate system with the AC direction of the top black phosphorus sheet as the 0° direction of the XY plane of the space coordinate system, and the middle layer and the bottom black phosphorus sheet are equivalent to placing the black phosphorus at 60° and 120° of the XY plane of the space coordinate system in the AC direction of the sheet direction. 5.根据权利要求1所述的集成阵列式偏振成像探测器,其特征在于,所述顶层0°黑磷片(3)、中间层60°黑磷片(6)与底层120°黑磷片(9)厚度为5-60纳米。5. The integrated array polarization imaging detector according to claim 1, wherein the top layer 0° black phosphorus sheet (3), the middle layer 60° black phosphorus sheet (6) and the bottom layer 120° black phosphorus sheet (9) The thickness is 5-60 nm. 6.根据权利要求1所述的集成阵列式偏振成像探测器,其特征在于,探测器单元由三层功能层和基底支撑层构成,功能层结构以透明黑磷片作为光敏层和导电沟道层,辅以电极和保护绝缘介质,并加以外围电路,探测器单元阵列的偏振成像探测器的像素一一对应。6 . The integrated array polarization imaging detector according to claim 1 , wherein the detector unit is composed of three functional layers and a substrate support layer, and the functional layer structure uses a transparent black phosphorus sheet as the photosensitive layer and the conductive channel. 7 . layer, supplemented by electrodes and protective insulating medium, and with peripheral circuits, the pixels of the polarized imaging detector of the detector unit array correspond one by one. 7.一种如权利要求1-6任一项所述的集成阵列式偏振成像探测器相应的偏振信息计算方法,其特征在于,对于探测器测得的信息运算步骤如下:7. A corresponding polarization information calculation method of the integrated array polarization imaging detector according to any one of claims 1-6, characterized in that, the information operation steps measured for the detector are as follows: 假定入射光的斯托克斯矢量是S0=(I,Q,U,V)T,其中I为非偏振光强,Q和U分别代表两个方向上的线偏振光,V代表圆偏振光,圆偏振分量在仪器可以检测的范围内忽略,故此处取V=0,即S0=(I,Q,U,0)TAssume that the Stokes vector of the incident light is S 0 =(I,Q,U,V) T , where I is the unpolarized light intensity, Q and U represent the linearly polarized light in the two directions, and V represents the circularly polarized light Light, the circularly polarized component is ignored within the range that the instrument can detect, so take V=0 here, that is, S 0 =(I,Q,U,0) T ; 第一层黑磷的AC(X)方向设置为空间坐标系中XY平面内的0°方向、第二层黑磷的AC(X)方向设置为XY平面内的60°方向、第三层黑磷的AC(X)方向设置为XY平面内的120°方向;The AC(X) direction of the first layer of black phosphorus is set to be the 0° direction in the XY plane in the spatial coordinate system, the AC(X) direction of the second layer of black phosphorus is set to the 60° direction in the XY plane, and the third layer of black phosphorus is set to the 0° direction in the XY plane. The AC(X) direction of phosphorus is set to the 120° direction in the XY plane; 黑磷片造成的相位延迟,可以表示为The phase delay caused by the black phosphorus sheet can be expressed as
Figure FDA0003052957280000021
Figure FDA0003052957280000021
此处,d表示黑磷片厚度,n表示复折射率实部,λ表示入射光波长;Here, d represents the thickness of the black phosphorus sheet, n represents the real part of the complex refractive index, and λ represents the wavelength of the incident light; 设P1和P2分别为AC(X)、ZZ(Y)方向的振幅透射率,则黑磷片的米勒矩阵可以表示为Assuming that P 1 and P 2 are the amplitude transmittances in the AC(X) and ZZ(Y) directions, respectively, the Miller matrix of the black phosphorus sheet can be expressed as
Figure FDA0003052957280000022
Figure FDA0003052957280000022
进而,旋转了角度θ的黑磷片,使用米勒矩阵可以表示为MΔ,θ=Tθ·MΔ,0·T Furthermore, the black phosphorus sheet rotated by the angle θ can be expressed as M Δ, θ =T θ ·M Δ, 0 ·T using the Miller matrix
Figure FDA0003052957280000023
Figure FDA0003052957280000023
进而可以表示出各层入射和出射的斯托克斯矢量的变换过程,入射光S0=(I,Q,U,0)T经过第一层黑磷的变换可以表示为Furthermore, the transformation process of the incoming and outgoing Stokes vectors of each layer can be expressed. The transformation of the incident light S 0 =(I,Q,U,0) T through the first layer of black phosphorus can be expressed as S1=MΔ,0S0=(I',Q',U',0)T S 1 =M Δ,0 S 0 =(I',Q',U',0) T 其中,I′为经过第一层黑磷后的非偏振光强,Q′和U′分别为经过第一层黑磷后的分别代表两个方向上的线偏振光;Among them, I' is the unpolarized light intensity after passing through the first layer of black phosphorus, Q' and U' are the linearly polarized light in two directions after passing through the first layer of black phosphorus respectively; 同理,第二层的变换可以表示为Similarly, the transformation of the second layer can be expressed as S2=MΔ,60S1=MΔ,60MΔ,0S0=(I”,Q”,U”,0)T S 2 =M Δ,60 S 1 =M Δ,60 M Δ,0 S 0 =(I”,Q”,U”,0) T 其中,I″为经过第二层黑磷后的非偏振光强,Q″和U″分别为经过第二层黑磷后的分别代表两个方向上的线偏振光;Wherein, I" is the unpolarized light intensity after passing through the second layer of black phosphorus, and Q" and U" are the linearly polarized light in two directions after passing through the second layer of black phosphorus respectively; 探测器每层所采集到的电流变化量可以计算出不同角度黑磷片所对应的光强值,并根据The current variation collected by each layer of the detector can calculate the light intensity value corresponding to the black phosphorus sheet at different angles, and according to the
Figure FDA0003052957280000031
Figure FDA0003052957280000031
可以求出入射光斯托克斯矢量的四个参量I、Q和U,同时可以求出偏振光的线偏振度(DoLP)以及偏振角(AoP)The four parameters I, Q and U of the Stokes vector of the incident light can be obtained, and the degree of linear polarization (DoLP) and the angle of polarization (AoP) of the polarized light can be obtained at the same time
Figure FDA0003052957280000032
Figure FDA0003052957280000032
Figure FDA0003052957280000033
Figure FDA0003052957280000033
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