本征广义琼斯矩阵方法 下载: 689次
1 Introduction
Jones calculus is a simple and general method for modelling several optical phenomena, such as those of liquid crystal displays[1-2], diffraction gratings[3], Šolc filters[4-6], holographic imaging[7-8], quantum communication[9] in classical and quantum optical fields, radio telescope image calibrators[10], radio polarimeters[11] in astronomical observation, human retinal imaging[12], human brain tissues[13], and biological specimens[14] in the biomedical imaging. Moreover, when applied in three dimensions, the Jones vector changes into the generalized Jones vector[15] and can be used to describe light propagating through a high-numerical-aperture focus lens[16], light interacting with nanoparticles[17], and optical coherence tomography[18].
Jones matrix calculus was first proposed by R. Clark Jones in the 1940s to describe the change in phase and polarization in a matrix or in vector forms for media or light[19]. It is a basic and widely used calculation method for describing the polarization of light transmitting in media. However, it has only been applied to normally or paraxially incident light. Zhang et al. introduced a Generalized Jones Vector (GJV), also called a 3D Jones vector to describe the polarization effect of light and optical media or systems[20-24]. Yeh et al. extended the method to treat the transmission of off-axis light through an anisotropic medium with an arbitrary optical axis orientation[25]. Azzam et al. invented the Generalized Jones Matrix (GJM) to describe the interaction between the fully polarized beam and its linear transformations in three dimensions[26]. Recently, Ortega-Quijano and colleagues proposed the differential Generalized Jones Matrix (dGJM) method to derive the GJM to model uniaxial and biaxial crystals with arbitrary orientations[27-28]. However, our repeated and precise calculations showed that the dGJM method is not applicable to samples with an arbitrary optical axis orientation or when the light is obliquely incident. The reason for this limitation is that the dGJM method tries to get the GJM of an arbitrarily oriented anisotropic crystal in the laboratory coordinate system through the rotation of the GJM consisting of the principle index in principle coordinate system. However, when the light has oblique incidence, the principle index should be replaced by the eigen refraction index, which can be calculated with the n-face equation of the crystal and the direction of the beam in the principle coordinate. Meanwhile, the eigen refraction index can be used to calculate the phase difference of the two eigen polarization lights.
In this paper, we propose a new method for calculating the phase and polarization of fully polarized light propagating in an arbitrarily oriented anisotropic crystal. The method overcomes the limitations of the dGJM method. In Sec. 2, an eigen Generalized Jones Matrix (eGJM) is derived that can be used in uniaxial and biaxial crystals. In Sec. 3, the eGJM is extended to describe the light refraction in the crystal interface. Then, we use the proposed method to simulate the polarization distribution of the cross-section for a light beam with a vortex and compare the results to an image obtained in an experiment[29-30]. The results demonstrate that our method is effective.
2 Eigen generalized Jones matrix method
2.1 Eigen generalized Jones matrix method
To overcome the limitations of the dGJM method, three coordinate systems are necessary: the laboratory coordinate system (S), which describes the position of the crystal; the principal axis coordinate system (Z), which describes the orientation of the optical axis; and the eigen coordinate system (B), which describes the direction of the polarized beam's. In addition, only one eigen coordinate system is required when the light beam transfers in the crystal without any refraction and that only two eigen coordinate systems are required for the two different wave vectors. These coordinates are illustrated in
图 1.
Fig. 1. Schematic diagram of the three coordinate systems. The black, blue, and red axes represent the laboratory, principal, and eigen coordinates, respectively. z 1 and z 2 are the optical axes.
We define the rotation relationship between them as
To obtain the eigen dGJM, we first calculate the eigen indices n1 and n2 from Eq. (1) and Eq. (2) using the principal coordinates:
where n is the refractive index,
Second, we can directly write the eGJM in B:
where δ=2π(n1d1−n2d2)/λ describes the phase difference. d1 and d2 are the propagation path lengths of the wave vector for the two eigen lights in the crystal. They must be calculated with different refractions at oblique incidents and identical refrations at normal incidents.
According to the relationship between B and S, the GJM in S is
where
The electric field vector
where
The physical meaning of Eq. (6) is easily understood.
2.2 Uniaxial crystal
We use the eGJM method to calculate the polarization distribution of the light beam in anisotropic crystals.
(1) Beam direction perpendicular to the optical axis
Consider a situation where the direction of the beam is perpendicular to the optical axis. The principal coordinate system is then in the superposition of the eigen coordinate system; thus,
where
In this case, there is no walk-off angle between the two eigen beams. Assuming the initial polarization direction is 45° from the x-axis, according to the eGJM method, we can calculate the polarization after a length d. The polarization distribution of the cross-section of the beam is presented in
图 2.
Fig. 2. Spatial distributions of the polarization state. (a) Original linear polarization. (b) Left(right) polarization. (c) Circular polarization. (d) Right(left) polarization. (e) Opposite linear polarization.
(2) Arbitrary angle between the beam and optical axis
When the angle between the beam and optical axis is arbitrary, the eigen refractive indices for the extraordinary ray will no longer be ne, but they should be calculated from Eq. (10)[30].
Then, the eGJM for the electric displacement vector
where
For the extraordinary beam, the array direction is not the same as the wave vector direction, so the eGJM for the electric field vector
where
The walk-off angle should be calculated before we obtain the polarization distribution of the cross-section of the beam. For a potassium dideuterium phosphate (KDDP) crystal, no=1.494 2, ne=1.460 3. The change in walk-off angle with θz from 0 to π/2 is shown in
图 4.
Fig. 4. Spatial distributions of the polarization state with a right direction walk-off effect. (a) Original linear polarization. (b) Left (right) polarization. (c) Circular polarization. (d) Right (left) polarization. (e) Opposite linear polarization.
2.3 Biaxial crystal
In biaxial crystals, there is always a walk-off effect for the light beam so the transmission of light is in the direction of the optical axis and its conical refraction effect is not considered a special situation. The eigen refractive indices for the two eigen linear polarization light beams can be calculated from Eq. (1) and Eq. (2). The eGJM for the electric field vector can immediately be written as
where
The eGJM for the electric displacement vector can be written as
where
To calculate the polarization distribution of the cross-section of the light beam, we also need to calculate the walk-off angle. We define the light direction as (θ, φ) in principal coordinates, and the change in walk-off angle is shown in
In
图 6.
Fig. 6. Spatial distributions of the polarization state with a upward-right direction walk-off effect. (a) Original linear polarization. (b) Left(right) polarization. (c) Circular polarization. (d) Right(left) polarization. (e) Opposite linear polarization.
3 Extended eigen generalized Jones matrix
We extend the eGJM to a more general case of refraction on the interface.
图 7.
Fig. 7. Phase difference and polarization. (a) Phase difference of the refracted light beam in birefringent crystals. (b) Polarization of reflection and refracted light beam at the interface in birefringent crystals.
The results indicate that the two phase changes are identical. They are equivalent to either the energy flow direction or the wave vector direction of the extraordinary light.
where δ1=(necosθe−nocosθo)dω/c and δ2=(ne/cosθe+no/cosθo)dω/c. Ignoring the phase factor
If we extend Eq. (24) to three dimensions, we have
In applications, we calculate the phase distribution for a vector vortex light beam with a singularity transference through the KDP crystal and compare the simulation results to the experimental results of Flossmann[28], as shown in
The black squares indicate the singularities of the light beam. The colored circles represent the circular polarization state points and the yellow lines represent the linear polarization states in the cross-section of the output vector beam. There is a small difference in the bottom and middle areas between these two images because of experimental error and simulation method. However, the polarization distribution and positions of the special points are almost identical, which clearly indicates that the eGJM method is practical.
4 Conclusions
In this study, we analyzed the GJM method, which provides a convenient way to establish the Jones matrix for anisotropic crystals whose optical axis is oriented arbitrarily in three-dimensional space. We proposed the eGJM method to overcome the limitation of the dGJM, which is effective only when the light has perpendicular incidence and the optical axis is perpendicular or parallel to the incidence face. The calculation results indicate that our method can be used to construct the Jones matrix when the directions of the light beam and optical axis are both arbitrary. The eGJM can also be extended to include cases where the light refraction is on the interface when light travels through the crystal, so that its polarization and phase can be precisely calculated. Finally, we use this method to simulate the polarization distribution of the cross-section for a fully polarized light beam with a vortex transmitting through an anisotropic crystal, and we compare the results to those of an experiment. The results demonstrate that our method is effective. Thus, the eGJM method has potential applications in simulating the space evolution of vector beams. Optional optical crystal instruments can be calculated based on the requirement beams. Factors like the electro-photon effect, magnetic-photon effect and optical rotation should be further studied to fully develop the eGJM method for applications like light propagation in crystals in electromagnetic fields.
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Article Outline
宋东升, 郑远林, 刘虎, 胡维星, 张志云, 陈险峰. 本征广义琼斯矩阵方法[J]. 中国光学, 2020, 13(3): 637. Dong-sheng SONG, Yuan-lin ZHENG, Hu LIU, Wei-xing HU, Zhi-yun ZHANG, Xian-feng CHEN. Eigen generalized Jones matrix method[J]. Chinese Optics, 2020, 13(3): 637.