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Combined with the experimental implementation, we have applied a solution to the forward problem appropriate to our imaging geometry so that we were able to compare model predictions with the measured phase change near focus and with the reflectivity and phase of the field reflected from a calibration sphere.
Optical pathlength changes (op = φλ/(4π)) in the sample are induced by light absorption of oxy- and deoxy-hemoglobin in blood, where φ is measured phase change at a specific depth and λ = 1328 nm is central wavelength of the DWP-OCT system.
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To compare with the experimentally measured phase changes, the displacements along the dotted line in Figure 3b are extracted and superposed in Figure 2c (red dashed line).
While measuring phase change traits, the height to each transition was also recorded to enable direct comparisons with previous studies (Jordan et al. 1999, 2000).
ODT is a functional extension of OCT that measures phase change due to Doppler frequency shift of light backscattered from red blood cells (RBCs) moving through the functional vessel lumen [ 28].
We used multiple antennas to measure phase changes over different path lengths to get a bearing on a selected FM radio station.
Coda-wave interferometry is a technique to detect slight changes in medium properties by measuring phase changes or waveform changes in coda waves from repetitive similar sources (e.g., Poupinet et al. 1984; Snieder et al. 2002; Snieder 2006).
Atom interferometry measures the phase change caused by the difference in two trajectories of an atom in space.
This paper measures the phase change temperature, latent heat, and specific heat of the samples using a differential scanning calorimeter (DSC), the thermal diffusivity using a laser flash method, and derives the thermal conductivity of each sample.
It measures the phase change per atom in units of rad/atom.
Doppler OCT is a blood flow detection method based on measuring the phase change of the light back-scattered from red blood cells.
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