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The proposed technique required high oversampling (i.e. the ratio between the sample beam width and the lateral sampling interval) along the slow axis.
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In our implementation, this matching is conveniently achieved by overlapping the zero-order reflection from the grating co-linearly with the sample beam, ensuring that the angle between the first-order diffracted beam and the sample beam equals the pulse front tilt induced by the grating.
The sample beam propagates through the experimental volume before recombining with the reference beam.
The reference beam is slightly tilted with respect to the sample beam to create a uniform fringe structure.
The surface of OB was perpendicularly illuminated by the sample beam of the OCT system.
THz transients are recorded point by point using a delay stage between the THz beam and the sampling beam.
The interferogram carries the information on the optical path variation between the varying sample beam and the still reference beam.
The telescope magnification also reduces the grating-induced pulse front tilt by a factor 5, matching it to the 2.4° angle between the reference and sample beam.
The fluorescence emission was directed into the detection module by a second dichroic mirror (DM2) placed between the fiber collimating optics of the OCT sample beam and DM1.
The angle between the reference and sample beams at the detector was set to θ x, θ y ≈ 6.25 mrad, yielding a fringe frequency of 1 cycle/ 4px at λ0 = 500 nm and 1 cycle/5.76 px at λ0 = 720 nm.
In the off-axis interferometry, there has a large angle between the reference and sample beams to separate the desired and undesired waves which will lose the sensitivity of interference measurement [ 12].
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