• Chinese Optics Letters
  • Vol. 23, Issue 1, 011101 (2025)
Liyuan Xu1, Zizhuo Lin1, Ruijian Li1, Yin Wang1..., Tong Liu1,**, Zhengliang Liu2, Linlin Chen1 and Yuan Ren2,*|Show fewer author(s)
Author Affiliations
  • 1Department of Aerospace Science and Technology, Space Engineering University, Beijing 101416, China
  • 2Department of Basic Course, Space Engineering University, Beijing 101416, China
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    DOI: 10.3788/COL202523.011101 Cite this Article Set citation alerts
    Liyuan Xu, Zizhuo Lin, Ruijian Li, Yin Wang, Tong Liu, Zhengliang Liu, Linlin Chen, Yuan Ren, "Computational ghost holography with Laguerre-Gaussian modes," Chin. Opt. Lett. 23, 011101 (2025) Copy Citation Text show less

    Abstract

    Computational ghost holography is a single-pixel imaging technique that has garnered significant attention for its ability to simultaneously acquire both the amplitude and phase images of objects. Typically, single-pixel imaging schemes rely on real-value orthogonal bases, such as Hadamard, Fourier, and wavelet bases. In this Letter, we introduce a novel computational ghost holography scheme with Laguerre–Gaussian (LG) modes as the complex orthogonal basis. It is different from the traditional methods that require the number of imaging pixels to exactly match the number of modulation modes. Our method utilizes 4128 distinct LG modes for illumination. By employing the second-order correlation (SOC) and TVAL3 compressed sensing (CS) algorithms, we have successfully reconstructed the amplitude and phase images of complex objects, and the actual spatial resolution obtained by the experiments is about 70 µm. Due to the symmetry of the LG modes, objects with rotational symmetry can be recognized and imaged using fewer modes. The difference between bucket detection and zero-frequency detection is analyzed theoretically and verified experimentally. Moreover, in the process of object reconstruction, the advanced image processing function can be seamlessly integrated via the preprocessing of the LG modes. As such, it may find a wide range of applications in biomedical diagnostics and target recognition.
    LGlp(r,φ)=2p!π(p+|l|)!1ω0(r2ω0)|l|×exp(r2ω02)Lp|l|(2r2ω02)exp(ilφ),

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    O(r,φ)=A(r,φ)exp[iϕ(r,φ)]=lBl(r)exp(ilφ)=l,pAl,pLGlp(r)exp(ilφ),

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    Bl(r)=02πO(r,φ)[exp(ilφ)]*dφ,

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    Al,p=02πdφ0+O(r,φ)[LGlp(r)exp(ilφ)]*rdr.

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    In=|[O(r,φ)LGlp(r,φ)*·exp(inπ/2)+O(r,φ)·R(r,φ)]k=0|2rdrdφ,n=0,1,2,3,

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    In=|O(r,φ)LGlp(r,φ)*|2rdrdφ+α2+2rdrdφ|O(r,φ)LGlp(r,φ)*|α·cos[ϕ(r,φ)+ϕα+n·π2],n=0,1,2,3,

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    Al,p(I0I2)+i(I1I3)=4αeiϕαO(r,φ)LGlp(r,φ)*rdrdφ.

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    In=|O(r,φ)|2|LGlp(r,φ)*·exp(inπ/2)+R(r,φ)|2rdrdφ,n=0,1,2,3.

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    Al,p(I0I2)+i(I1I3)=4|O(r,φ)|2LGlp(r,φ)*R(r,φ)*rdrdφ.

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    SSIM(O,O¯)=(2μOμO¯+c1)(σOO¯+c2)(μO2+μO¯2+c1)(σO2+σO¯2+c2),

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    c1=(K1L)2,c2=(K2L)2,

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    LGlp(r,φ)r+LGlp(r,φ)rφ=[|l|r2rω024rω02Lp1|l|+1(2r2ω02)Lp|l|(2r2ω02)+ilr]LGlp(r,φ).

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    Liyuan Xu, Zizhuo Lin, Ruijian Li, Yin Wang, Tong Liu, Zhengliang Liu, Linlin Chen, Yuan Ren, "Computational ghost holography with Laguerre-Gaussian modes," Chin. Opt. Lett. 23, 011101 (2025)
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