Optimisation of a polygon mirror-based spectral filter for swept source optical coherence tomography (SS-OCT)

Medical imaging using Optical Coherence Tomography (OCT) provides clinicians with 3D, high resolution reconstructions of microscopic structures, in depth. It has been initially developed for ophthalmology, in order to scan the retinas of patients to diagnose illness. The quality of the images depends upon their axial and lateral resolutions and the properties of the light being used. Research using a polygon mirror (PM) as a spectral filter in Swept Source OCT (SS-OCT) has resulted in a variety of different experimental arrangements. Although the application of PM-based SS-OCT sources has been successfully demonstrated, the combination of their components’ fundamental properties and the overall impact they have on imaging performance is rarely reported. A more detailed examination of these properties would lead to a full description of their operation and to the best methods to employ if system performance is to be maximised. This work presents our current findings of on-going research into the optimisation of PM-based SS-OCT systems. A swept source spectral filter, consisting of a collimator, a transmission grating, a two-lens telescope and an off-axis PM with an end reflector mirror has been evaluated experimentally and compared with theoretical predictions. The system’s performance has been compared for two different fibre collimators. Although the beam width on the grating is different for each of the two collimators, the spot size at the PM facet is made the same by selecting appropriate focal lengths. An improvement in the signal roll-off at the interferometer output of ~1.0 dB/mm was obtained when using a 3.4 mm collimator compared to a 1.5 mm collimator.

[1]  Victor X. D. Yang,et al.  Simultaneous 6-channel optical coherence tomography using a high-power telescope-less polygon-based swept laser in dual-amplifier configuration , 2010, BiOS.

[2]  S. Yun,et al.  115 kHz tuning repetition rate ultrahigh-speed wavelength-swept semiconductor laser. , 2005, Optics letters.

[3]  Adrian Gh. Podoleanu,et al.  Polygon mirror scanners in biomedical imaging: a review , 2013, Photonics West - Optoelectronic Materials and Devices.

[4]  S. M. R. Motaghiannezam,et al.  Differential phase-contrast, swept-source optical coherence tomography at 1060 nm for in vivo human retinal and choroidal vasculature visualization. , 2012, Journal of biomedical optics.

[5]  Feng Gao,et al.  Phase and amplitude correction in polygon tunable laser-based optical coherence tomography , 2017 .

[6]  N. Lippok,et al.  Simple and versatile long range swept source for optical coherence tomography applications , 2015 .

[7]  Adrian Mariampillai,et al.  Real-time speckle variance swept-source optical coherence tomography using a graphics processing unit , 2012, Biomedical optics express.

[8]  M. Kuznetsov,et al.  Analysis of a spinning polygon wavelength swept laser , 2015, 1501.07003.

[9]  N. Munce,et al.  High-power wavelength-swept laser in Littman telescope-less polygon filter and dual-amplifier configuration for multichannel optical coherence tomography. , 2009, Optics letters.

[10]  B. Vakoc,et al.  >400 kHz repetition rate wavelength-swept laser and application to high-speed optical frequency domain imaging. , 2010, Optics letters.

[11]  Wolfgang Wieser,et al.  Fully automated 1.5 MHz FDML laser with 100 mW output power at 1310 nm , 2015 .

[12]  S. Sherif,et al.  High performance wavelength-swept laser with mode-locking technique for optical coherence tomography , 2009 .