zdepth¼
p
2 dk
¼
Mp
2 Dk
¼
M
4
k^2
Dk
¼
M
2
lc ð 10 : 15 Þ
wherelcis the coherence length of the source andΔk=2πΔλ/λ^2.
The A-scanaxial resolutionΔzis
Dzgaussian¼
4ln2
DkFWHM
¼
4ln2
2 pDk=k^2
ð 10 : 16 Þ
when using a Gaussian source that has a full-width half-maximum bandwidth
kFWHM. For a rectangular source the axial resolution is
zrect¼
p
Dk
ð 10 : 17 Þ
Example 10.6Consider an SS-OCT system for which M = 220,
λ= 1308 nm, andΔλ= 87 nm. (a) What is the scan depth range? (b) What is
the axial resolution when using a Gaussian source?
Solution: (a) Using Eq. (10.15) yields the following scan depth range
zdepth¼
M
4
k^2
Dk
¼
220
4
ð1308 nmÞ^2
87 nm
¼ 1 :08 mm
(b) Using Eq. (10.16) yields the following axial resolution for a Gaussian
source
Dzgaussian¼
4ln2
2 pDk=k^2
¼4ln2
ð1308 nmÞ^2
2 pð87 nmÞ
¼ 8 : 7 lm
Tissue
sample
Fixed
mirror
Reference arm
Optical splitter
SMF
Tunable SMF
laser
source
(^12)
3
AD converter PC
Photodetector
Optical circulator
Fig. 10.8 Schematic of the setup for a swept source OCT system
302 10 Optical Imaging Procedures