Geometric & Radiometric Vignetting Associated with a 72-Facet, Off-Axis, Polygon Mirror for Swept Source Optical Coherence Tomography (SS-OCT)

被引:5
|
作者
Everson, Michael [1 ]
Duma, Virgil-Florin [2 ,3 ,4 ]
Dobre, George [1 ]
机构
[1] Univ Kent, Sch Phys Sci, AOG, Canterbury CT2 7NH, Kent, England
[2] Aurel Vlaicu Univ Arad, Optomechatron Grp 3OM, 77 Revolutiei Ave, Arad 310130, Romania
[3] Polytech Univ Timisoara, Doctoral Sch, 1 Mihai Viteazu Ave, Timisoara 300222, Romania
[4] West Univ Timisoara, Sch Phys, 4 Vasile Parvan Ave, Timisoara 300223, Romania
来源
TIM15-16 PHYSICS CONFERENCE | 2017年 / 1796卷
基金
英国工程与自然科学研究理事会;
关键词
SEMICONDUCTOR-LASER; WAVELENGTH FILTER; SCANNER;
D O I
10.1063/1.4972382
中图分类号
O59 [应用物理学];
学科分类号
摘要
Optical Coherence Tomography (OCT) has a broad range of applications in 2D and volumetric imaging of micron scale structures typically used on inaccessible objects such as the retina of the eye. This report focuses on Swept Source OCT (SS-OCT), favoured for its faster scanning speeds and therefore faster data acquisition (highly favourable when imaging live patients). SS-OCT relies on the scanning of a narrow laser line at speeds typically in excess of 100 kHz. We have employed Zemax (TM) ray tracing software to simulate one method of splitting the spectrum of a broadband, near-infrared source, into its component wavelengths by reflecting the spectrum from an off-axis, 72-facet polygon mirror at a frequency of 48 kHz. We specifically addressed the geometric and radiometric vignetting associated with the reflected spectrum off an individual mirrored facet and how this may impose limitations to the incident beam size and hence lead to a loss in the power available from the source. It was found that for certain configurations up to 44% of the light was lost at the edges of the spectrum due to both radiometric and geometric vignetting, which may result in an effective swept range of <50 nm from an initial bandwidth of 100 nm. Our simulations account for real refractive errors and losses in the beam caused by lens aberrations, and produce a model of the sampling function of wavelength against time.
引用
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页数:9
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