Table 1.
TD-OCT | SD-OCT | SS-OCT | |
---|---|---|---|
1. Commercial Availability | 1996 [4] | 2006 [4] | 2012 [4] |
2. Principle of Operation | A beam splitter splits incident light into a reference wavelength which is adjusted for different depths while the sample light is reflected from the observed tissue and recombined at a sensor to give a single profile of the tissue [5]. | Based on FD-OCT. It has similar principles to TD-OCT, but the sensor is upgraded to a spectrometer to split the reflected light into wavelengths (λ) using a diffractor. A combination of the individual images provided by the λs produces a Fourier transform to obtain depth information (A-scan) [6]. | Also based on FD-OCT like SD-OCT. It possesses a sweeping tunable laser as its light source. A photoreceiver transduces the relayed signals into noise (images) [7]. |
3. Bandwidth | 20 nm [8] | 150 nm [8] | ~1040–1080 nm [8] |
4. Wavelength Frequency |
810 nm [8] | 840 nm [8] | ~1050 nm [9] |
5. Axial resolution | 8–10 µm [9] | 5–7 µm [9] | 5.3 µm [10] |
6. Scan Speeds | 400 A-scans per second [11] | 20,000–52,000 A-scans per second [11] | 100,000–236,000 A-scans per second [11,12] |