均匀偏振cosh-Pearcey-Gauss光束的远场坡印廷矢量，自旋与轨道角动量

廖赛; 程科; 黄宏伟; 杨嶒浩; 梁梦婷; 孙望轩

doi:10.37188/CO.EN.2022-0022

均匀偏振cosh-Pearcey-Gauss光束的远场坡印廷矢量，自旋与轨道角动量

成都信息工程大学光电工程学院, 四川成都 610225

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中图分类号: TN929.1;
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出版历程
- 收稿日期: 2022-11-11
- 录用日期: 2023-01-30
- 网络出版日期: 2023-02-28

The Poynting vectors, spin and orbital angular momentums of uniformly polarized cosh-Pearcey-Gauss beams in the far zone

doi: 10.37188/CO.EN.2022-0022

College of Optoelectronic Engineering, Chengdu University of Information Technology, Chengdu 610225, P.R. China

Funds: Supported by Sichuan Science and Technology Program of China (No. 23NSFSC1097)

More Information

Author Bio:
LIAO Sai (1998—), M.E, College of Optoelectronic Engineering, Chengdu University of Information Technology. His research interests are in the vector structures of catastrophe beams. E-mail: 1399417658@qq.com

CHENG Ke (1979—), Ph.D, Professor, College of Optoelectronic Engineering, Chengdu University of Information Technology. His research interests are in the propagation and control of High-Power Lasers. E-mail: ck@cuit.edu.cn

Corresponding author: E-mail: ck@cuit.edu.cn

摘要

摘要:
我们提出了均匀偏振cosh-Pearcey-Gauss 光束，其主要由双曲余弦函数(n, Ω)和偏振相关角度(α, δ)所调制。基于矢量角谱法和稳相法，研究了该光束的远场坡印廷矢量、自旋角动量和轨道角动量。研究结果表明：较大的双曲余弦函数值能将远场坡印廷矢量、自旋角动量和轨道角动量分割成多瓣抛物线结构。虽然左旋和右旋椭圆偏振不能影响整个光束结构，但却可通过调节TE和TM项的左半边和右半边的分布权重，进而分辨出光束的远场坡印廷矢量和角动量分布。本文结果对信息存储与偏振成像技术领域有着潜在的应用价值。
- cosh-Pearcey-Gauss光束 /
- 自旋角动量密度 /
- 轨道角动量密度 /
- 坡印廷矢量
Abstract:
We propose cosh-Pearcey-Gauss beams with uniform polarization, which are mainly modulated by a hyperbolic cosine function (n, Ω) and the angles related to uniform polarization (α, δ). Based on angular spectrum representation and the stationary phase method, the Poynting vector, spin and orbital angular momentum in the far zone are studied. The results show that a larger n or Ω in the hyperbolic cosine function can partition the longitudinal Poynting vectors, SAMs and OAMs into more multi-lobed parabolic structures. Different polarizations described by (α, δ) can distinguish their Poynting vectors and angular momentums between the TE and TM terms, though this does not affect the patterns of the whole beam. Furthermore, the weight of the left and right sides of longitudinal Poynting vectors, SAMs and OAMs in TE and TM terms can be modulated by left-handed or right-handed elliptical polarization, respectively. The results in this paper may be useful for information storage and polarization imaging.
- cosh-Pearcey-Gauss beams /
- spin angular momentum /
- orbital angular momentum /
- Poynting vector

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Figure 1. The initial intensity and angular spectrum of the cPeG beams with different initial polarization states for n=1, 2 and 4. (a1), (a2): α=π/4, δ=π/8; (b1), (b2): α=0, δ=0; (c1), (c2): α=π/4, δ=−3π/4; The phase distribution and polarization states are described in the top left and right in Figs.1 (a1)−(c1). Blue: left-handed elliptical polarization; Red: right-handed elliptical polarization; Black: linear polarization. The parameters are x₀=y₀=100 μm and Ω=1.4.

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Figure 2. The theoretical design of the cPeG beams with uniform polarization. BS: beam splitter; SLM: spatial Light Modulator.

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Figure 3. Normalized longitudinal Poynting vector (backgrounds) and transversal Poynting vector (arrows) of cPeG beams for different uniform polarizations (α, δ) at z=50z₀. (a1)−(c1): TE term; (a2)−(c2): TM term; (a3)−(c3): whole beam. The parameters are n=2 and Ω=1.4. The red point symbolizes topological charge l=+1, and the white point denotes l=−1

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Figure 4. Normalized longitudinal Poynting vector (backgrounds) and transverse Poynting vector (arrows) of cPeG beams for different n and Ω at z=50z₀, where the uniform polarization is (α, δ)=(π/4, π/8).

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Figure 5. Normalized longitudinal SAM (3D and 2D) and transverse SAM (arrows) of cPeG beams at z=50z₀. (a1)−(a3): α=π/4, δ=π/8; (b1)−(b3): α=π/4, δ=−3π/4. The other parameters are the same as those in Fig. 3.

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Figure 6. Normalized longitudinal (3D and 2D) SAM and transverse SAM (arrows) of cPeG beams (n=1, 4) at z=50z₀. The other parameters are the same as those in Figs. 5 (a1)−(b3): α=π/4, δ=π/8.

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Figure 7. Normalized longitudinal OAM (3D and 2D) and transverse OAM (arrows) of cPeG beams (Ω=1.4) at z=50z₀. (a1)−(a3): α=π/4, δ=π/8; (b1)-(b3): α= 0, δ= 0; (c1)−(c3): α=π/4, δ=−3π/4; The other parameters are the same as those in Fig. 3. n=2

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Figure 8. Normalized longitudinal and transverse (arrows) OAM of cPeG beams (n=1, 4) at z=50z₀. The other parameters are the same as those in Fig. 4.

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