Expand this Topic clickable element to expand a topic
Skip to content
Optica Publishing Group

Synthetic aperture superresolution by speckle pattern projection

Open Access Open Access

Abstract

We propose a method for increasing the resolution of an aperture limited optical system by illuminating the input with a speckle pattern. The high resolution of the projected speckle pattern demodulates the high frequencies of the sample and permits its passage through the system aperture. A decoding provides the superresolved image. The speckle pattern can be generated in a simple manner in contrast with other structured light superresolution methods. The method is demonstrated in microscopy test images.

©2005 Optical Society of America

Full Article  |  PDF Article
More Like This
Superresolved imaging based on wavelength multiplexing of projected unknown speckle patterns

Omer Wagner, Ariel Schwarz, Amir Shemer, Carlos Ferreira, Javier García, and Zeev Zalevsky
Appl. Opt. 54(13) D51-D60 (2015)

Aberration-free superresolution imaging via binary speckle pattern encoding and processing

Eyal Ben-Eliezer and Emanuel Marom
J. Opt. Soc. Am. A 24(4) 1003-1010 (2007)

Synthetic aperture superresolution with multiple off-axis holograms

Vicente Mico, Zeev Zalevsky, Pascuala García-Martínez, and Javier García
J. Opt. Soc. Am. A 23(12) 3162-3170 (2006)

Supplementary Material (2)

Media 1: AVI (1376 KB)     
Media 2: AVI (888 KB)     

Cited By

Optica participates in Crossref's Cited-By Linking service. Citing articles from Optica Publishing Group journals and other participating publishers are listed here.

Alert me when this article is cited.


Figures (4)

Fig. 1.
Fig. 1. Scheme of the experimental setup.
Fig. 2.
Fig. 2. (a) Encoding speckle pattern. (b) Autocorrelation of the encoding pattern.
Fig. 3.
Fig. 3. (a) Low pass image. (b) Reconstruction from the image set (1.34 MB).
Fig. 4.
Fig. 4. Incoherent case. (a) Low pass image (b) Reconstruction from the image set (888 KB).

Equations (10)

Equations on this page are rendered with MathJax. Learn more.

o ξ ( x ) = [ g ( x ) s ( x ξ ) ] h ( x ) = [ g ( x ) s ( x ξ ) ] h ( x x ) dx ,
o ( x ) = o ξ ( x ) s ( x ξ ) = { [ g ( x ) s ( x ξ ) ] h ( x x ) } s ( x ξ ) dx .
γ ( x x ) = s ( x ξ ) s ( x ξ ) = s ( ν ) s ( ν + ( x x ) ) .
o ( x ) = g ( x ) h ( x x ) γ ( x x ) dx = g ( x ) h ( x x ) dx = g ( x ) h ( x ) .
h ( x ) = h ( x ) γ ( x ) .
h ( x ) h ( x ) δ ( x ) = h ( 0 ) δ ( x ) .
γ ( x ) = sin c 2 ( Lx λz )
o incoh ( x ) = I g ( x ) [ I h ( x ) Γ ( x ) ] ,
Γ ( x ) = [ 1 + sin c 2 Lx λz ] .
o incoh ( x ) = I g ( x ) I h ( x ) + I g ( x ) .
Select as filters


Select Topics Cancel
© Copyright 2024 | Optica Publishing Group. All rights reserved, including rights for text and data mining and training of artificial technologies or similar technologies.