Enhanced angular domain imaging in turbid media using Gaussian line illumination

被引:9
作者
Chapman, Glenn H. [1 ]
Rao, Josna [1 ]
Liu, Ted C. K. [1 ]
Chan, Paulman K. Y. [1 ]
Vasefi, Fartash [1 ]
Kaminska, Bozena [1 ]
Pfeiffer, Nick [1 ]
机构
[1] Simon Fraser Univ, Sch Engn Sci, 8888 Univ Ave, Burnaby, BC V5A 1S6, Canada
来源
OPTICAL INTERACTIONS WITH TISSUE AND CELLS XVII | 2006年 / 6084卷
关键词
optical tomography; tissue optics; collimating optics; micromachining; lasers;
D O I
10.1117/12.650457
中图分类号
Q2 [细胞生物学];
学科分类号
071009 ; 090102 ;
摘要
Coherence or Time Domain Optical tomography within highly scattering media observes the shortest path photons over the dominant randomly scattered background light. Angular Domain Imaging employs micromachined collimators detecting photons within small angles of aligned laser light sources. These angular filters are micromachined silicon collimator channels 51 microns wide by 10 mm long on 102 micron spacing, giving an acceptance angle of 0.29 degrees at a CMOS detector array. Phantom test objects were observed in scattering media 5 cm thick at effective scattered to ballistic ratios from 1 1 to greater than 1E8:1. Line and space test objects detection limits are set by detector pixel size (5.5 microns) not collimator hole spacing. To maximize the ballistic/quasi-ballistic photons observed, a line of light aligned with the collimator holes increases detectability by reducing the amount of scattered background light. A Cylindrical Spherical Cylindrical beam expander/shrinker creates a 16 mm by 0.35 mm line of light. Best results Occur when the scattering medium, collimator and detector are within 3X the Rayleigh Range of the beam's narrow vertical axis. allowing imaging of 51 micron lines/spaces at 3E8:1 scattering ratios. Restricting the light to a I mm line extends this to 8E9:1. Carbon coating the SMCA to reduce reflectivity shows that at high scattering levels absorbing walls will reduce background light, improving contrast. ADI has also been shown to work when the illumination is unaligned with the detector. This allows for side illumination with detection of structures at depths of 3mm with a scattering ratio of 1E6:1.
引用
收藏
页数:12
相关论文
共 15 条
[1]  
[Anonymous], SPIE IS
[2]  
BOAS DA, 2003, J ELECT IMAGING, V12
[3]   Angular domain image detectability with changing turbid medium scattering coefficients [J].
Chapman, GH ;
Chan, PKY ;
Dudas, J ;
Rao, J ;
Pfeiffer, N .
Optical Interactions with Tissue and Cells XVI, 2005, 5695 :160-171
[4]   Angular domain optical imaging of structures within highly scattering material using silicon micromachined collimating arrays [J].
Chapman, GH ;
Trinh, M ;
Lee, D ;
Pfeiffer, N ;
Chu, G .
OPTICAL TOMOGRAPHY AND SPECTROSCOPY OF TISSUE V, 2003, 4955 :462-473
[5]   Angular domain imaging of objects within highly scattering media using silicon micromachined collimating arrays [J].
Chapman, GH ;
Trinh, M ;
Pfeiffer, N ;
Chu, G ;
Lee, D .
IEEE JOURNAL OF SELECTED TOPICS IN QUANTUM ELECTRONICS, 2003, 9 (02) :257-266
[6]   Optical imaging of objects within highly scattering media using silicon micromachined collimating arrays [J].
Chapman, GH ;
Tank, MS ;
Chu, G ;
Trinh, MT .
OPTICAL FIBERS AND SENSORS FOR MEDICAL APPLICATIONS II, 2002, 4616 :187-198
[7]  
CHU G, 2000, THESIS SIMON FRASER
[8]  
INABA H, 1993, SPIE I ADV OPTICAL T, V11, P317
[9]  
JACQUES S, 2001, INTRO BIOMEDICAL OPT
[10]  
Jacques S. L., 1987, Lasers in the Life Sciences, V1, P309