2016
DOI: 10.1364/boe.7.003140
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Aperture scanning Fourier ptychographic microscopy

Abstract: Fourier ptychographic microscopy (FPM) is implemented through aperture scanning by an LCOS spatial light modulator at the back focal plane of the objective lens. This FPM configuration enables the capturing of the complex scattered field for a 3D sample both in the transmissive mode and the reflective mode. We further show that by combining with the compressive sensing theory, the reconstructed 2D complex scattered field can be used to recover the 3D sample scattering density. This implementation expands the s… Show more

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Cited by 43 publications
(29 citation statements)
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“…Phase information can also be retrieved by using computational algorithms [8]. For example, Fourier ptychographic microscopy (FPM) takes a series of images captured under different illumination angles [9][10][11][12][13] or different overlapped apertures [14][15][16] to iteratively recover a sample's phase and amplitude; transport of intensity phase imaging [17][18][19][20] uses images captured at different defocused planes to solve the transport of intensity equation (TIE) and retrieve phase. The large number of measurements needed is a disadvantage of these methods.…”
Section: Introductionmentioning
confidence: 99%
“…Phase information can also be retrieved by using computational algorithms [8]. For example, Fourier ptychographic microscopy (FPM) takes a series of images captured under different illumination angles [9][10][11][12][13] or different overlapped apertures [14][15][16] to iteratively recover a sample's phase and amplitude; transport of intensity phase imaging [17][18][19][20] uses images captured at different defocused planes to solve the transport of intensity equation (TIE) and retrieve phase. The large number of measurements needed is a disadvantage of these methods.…”
Section: Introductionmentioning
confidence: 99%
“…Increased resolution/SBP Aperture synthesis [1,[21][22][23][24] Phase imaging Phase retrieval [25][26][27][28][29] Digital refocusing Phase retrieval [1,27,30] Aberration correction EPRY [24,[31][32][33] Long working distance low NA objective [34,35] Sub-λ imaging high-angle illumination [21][22][23]34,36,37] Multimodal imaging scanning illumination angle [24,34,38] High-speed LED & camera multiplexing [26,[39][40][41][42][43][44][45] Compact and portable Novel hardware [33,46,47] 3D imaging light field, 1st Born, multislice [48][49][50][51][52][53][54][55][56] computation using low numerical aperture (NA) op...…”
Section: Achieved By Referencesmentioning
confidence: 99%
“…The maximum synthesized NA that can be expected for an FP system in air is 2 -when NA ill and NA obj are both one. With scanning [27,30,76] and multi-aperture [42] FP setups, the synthetic NA may be defined via a similar process and its extent in Fourier space also defines the system's final resolution.…”
Section: Resolutionmentioning
confidence: 99%
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“…There also have been numerous efforts in improving the Fourier ptychographic (FP) reconstruction by adopting more noise-robust algorithms [15][16][17][18]. Alternative FPM modalities involving aperture scanning instead of angular illuminations were demonstrated, which allowed for imaging the complex field of a thick specimen [19,20] and estimating optical aberrations [21]. Imaging a thick specimen with angular illuminations also became possible by employing the first Born approximation [22] or multislice coherent model [23].…”
Section: Introductionmentioning
confidence: 99%