Three-dimensional quantitative phase imaging via tomographic deconvolution phase microscopy

被引:61
作者
Jenkins, Micah H. [1 ]
Gaylord, Thomas K. [1 ]
机构
[1] Georgia Inst Technol, Sch Elect & Comp Engn, Atlanta, GA 30332 USA
基金
美国国家科学基金会;
关键词
OPTICAL DIFFRACTION TOMOGRAPHY; RESIDUAL-STRESS RELAXATION; PERIOD FIBER GRATINGS; REFRACTIVE-INDEX; RECONSTRUCTION ALGORITHMS; LIVE CELLS; INVERSION; ILLUMINATION; PROPAGATION; RESOLUTION;
D O I
10.1364/AO.54.009213
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
The field of three-dimensional quantitative phase imaging (3D QPI) is expanding rapidly with applications in biological, medical, and industrial research, development, diagnostics, and metrology. Much of this research has centered on developing optical diffraction tomography (ODT) for biomedical applications. In addition to technical difficulties associated with coherent noise, ODT is not congruous with optical microscopy utilizing partially coherent light, which is used in most biomedical laboratories. Thus, ODT solutions have, for the most part, been limited to customized optomechanical systems which would be relatively expensive to implement on a wide scale. In the present work, a new phase reconstruction method, called tomographic deconvolution phase microscopy (TDPM), is described which makes use of commercial microscopy hardware in realizing 3D QPI. TDPM is analogous to methods used in deconvolution microscopy which improve spatial resolution and 3D-localization accuracy of fluorescence micrographs by combining multiple through-focal scans which are deconvolved by the system point spread function. TDPM is based on the 3D weak object transfer function theory which is shown here to be capable of imaging "nonweak" phase objects with large phase excursions. TDPM requires no phase unwrapping and recovers the entire object spectrum via object rotation, mitigating the need to fill in the "missing cone" of spatial frequencies algorithmically as in limited-angle ODT. In the present work, TDPM is demonstrated using optical fibers, including single-mode, polarization-maintaining, and photonic-crystal fibers as well as an azimuthally varying CO2-laser-induced long-period fiber grating period as test phase objects. (C) 2015 Optical Society of America
引用
收藏
页码:9213 / 9227
页数:15
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