Collective noise model for focal plane modulated single-pixel imaging

Abstract Single-pixel imaging, also known as computational ghost imaging, provides an alternative method to perform imaging in various applications which are difficult for conventional cameras with pixelated detectors, such as multi-wavelength imaging, three-dimensional imaging, and imaging through turbulence. In recent years, many improvements have successfully increased the signal-to-noise ratio of single-pixel imaging systems, showing promise for the engineering feasibility of this technique. However, many of these improvements are based on empirical findings. In this work we perform an investigation of the noise from each system component that affects the quality of the reconstructed image in a single-pixel imaging system based on focal plane modulation. A collective noise model is built to describe the resultant influence of these different noise sources, and numerical simulations are performed to quantify the effect. Experiments have been conducted to verify the model, and the results agree well with the simulations. This work provides a simple yet accurate method for evaluating the performance of a single-pixel imaging system, without having to carry out actual experimental tests.

[1]  Dongfeng Shi,et al.  Two-wavelength ghost imaging through atmospheric turbulence. , 2013, Optics express.

[2]  K. Petermann Laser Diode Modulation and Noise , 1988 .

[3]  Ling-An Wu,et al.  Thermal light subwavelength diffraction using positive and negative correlations , 2016 .

[4]  J. Dainty Laser speckle and related phenomena , 1975 .

[5]  V. Vilnrotter,et al.  Symbol-Error Probabilities for Pulse-Position Modulation Signaling With an Avalanche Photodiode Receiver and Gaussian Thermal Noise , 1998 .

[6]  A. Gatti,et al.  Differential ghost imaging. , 2010, Physical review letters.

[7]  Ling-An Wu,et al.  Nonlocal imaging of a reflective object using positive and negative correlations. , 2015, Applied optics.

[8]  Zukang Lu,et al.  Speckle suppression with a rotating light pipe , 2010 .

[9]  Graham M. Gibson,et al.  Simultaneous real-time visible and infrared video with single-pixel detectors , 2015, Scientific Reports.

[10]  Charles C. Harb,et al.  Understanding and controlling laser intensity noise , 1999 .

[11]  Aswin C. Sankaranarayanan,et al.  CS-MUVI: Video compressive sensing for spatial-multiplexing cameras , 2012, 2012 IEEE International Conference on Computational Photography (ICCP).

[12]  Shih,et al.  Optical imaging by means of two-photon quantum entanglement. , 1995, Physical review. A, Atomic, molecular, and optical physics.

[13]  D. L. Donoho,et al.  Compressed sensing , 2006, IEEE Trans. Inf. Theory.

[14]  Jeffrey H. Shapiro,et al.  Ghost imaging in reflection: resolution, contrast, and signal-to-noise ratio , 2010, Optical Engineering + Applications.

[15]  Shree K. Nayar,et al.  Multiplexing for Optimal Lighting , 2007, IEEE Transactions on Pattern Analysis and Machine Intelligence.

[16]  Graham M. Gibson,et al.  Single-pixel three-dimensional imaging with time-based depth resolution , 2016, Nature Communications.

[17]  M. Padgett,et al.  3D Computational Imaging with Single-Pixel Detectors , 2013, Science.

[18]  Thomas B. Moeslund,et al.  Super-resolution: a comprehensive survey , 2014, Machine Vision and Applications.

[19]  Y. Shih,et al.  Turbulence-free ghost imaging , 2011 .

[20]  Ting Sun,et al.  Single-pixel imaging via compressive sampling , 2008, IEEE Signal Process. Mag..

[21]  Jeffrey H. Shapiro,et al.  Computational ghost imaging , 2008, 2009 Conference on Lasers and Electro-Optics and 2009 Conference on Quantum electronics and Laser Science Conference.

[22]  Kevin J. Mitchell,et al.  Single-pixel infrared and visible microscope , 2014 .

[23]  R. Boyd,et al.  "Two-Photon" coincidence imaging with a classical source. , 2002, Physical review letters.

[24]  Ming-Jie Sun,et al.  A sur-pixel scan method for super-resolution reconstruction , 2013 .

[25]  Shengmei Zhao,et al.  Fast reconstructed and high-quality ghost imaging with fast Walsh–Hadamard transform , 2016 .

[26]  Jahja I. Trisnadi Hadamard speckle contrast reduction. , 2004, Optics letters.

[27]  M. Chekhova,et al.  High-visibility, high-order lensless ghost imaging with thermal light. , 2009, Optics letters.

[28]  Chun-xi Zhang,et al.  Third-order lensless ghost diffraction with classical fully incoherent light. , 2010, Optics letters.

[29]  Wenlin Gong,et al.  Scalar-matrix-structured ghost imaging , 2016 .

[30]  Wenlin Gong,et al.  Ghost imaging lidar via sparsity constraints , 2012, 1203.3835.

[31]  H. Andrews,et al.  Hadamard transform image coding , 1969 .

[32]  J. Shapiro,et al.  Signal-to-noise ratio of Gaussian-state ghost imaging , 2008, 2009 Conference on Lasers and Electro-Optics and 2009 Conference on Quantum electronics and Laser Science Conference.

[33]  N J Sloane,et al.  Masks for Hadamard transform optics, and weighing designs. , 1976, Applied optics.

[34]  Graham M Gibson,et al.  Improving the signal-to-noise ratio of single-pixel imaging using digital microscanning. , 2016, Optics express.

[35]  Jingang Zhong,et al.  Single-pixel imaging by means of Fourier spectrum acquisition , 2015, Nature Communications.

[36]  O. Katz,et al.  Ghost imaging with a single detector , 2008, 0812.2633.