Abstract

Author(s): Fishkin, JB; Fantini, S; vandeVen, MJ; Gratton, E | Abstract: The predictions of the frequency-domain standard diffusion equation (SDE) model for light propagation in an infinite turbid medium diverge from the more complete [Formula Presented] approximation to the linear Boltzmann transport equation at intensity modulation frequencies greater than several hundred MHz. The [Formula Presented] approximation is based on keeping only the terms l=0 and l=1 in the expansion of the angular photon density in spherical harmonics, and the nomenclature [Formula Presented] approximation is used since the spherical harmonics of order l=1 can be written in terms of the first order Legendre polynomial, which is traditionally represented by the symbol [Formula Presented]. Frequency-domain data acquired in a quasi-infinite turbid medium at modulation frequencies ranging from 0.38 to 3.2 GHz using a superheterodyning microwave detection system were analyzed using expressions derived from both the [Formula Presented] aproximation equation and the SDE. This analysis shows that the [Formula Presented] approximation provides a more accurate description of the data over this range of modulation frequencies. Some researchers have claimed that the [Formula Presented] approximation predicts that a light pulse should propagate with an average speed of c/ √3 in a thick turbid medium. However, an examination of the Green’s function that we obtained from the frequency-domain [Formula Presented] approximation model indicates that a photon density wave phase velocity of c/ √3 is only asymptotically approached in a regime where the light intensity modulation frequency aproaches infinity. The Fourier transform of this frequency-domain result shows that in the time domain, the [Formula Presented] approximation predicts that only the leading edge of the pulse (i.e., the photons arriving at the detector at the earliest time) approaches a speed of c/√3. © 1996 The American Physical Society.

Highlights

  • Frequency-domain methods, in which the light source intensity is modulated at radio frequency, have been successfully applied to spectroscopy studies of turbid media [1,2,3,4]

  • These expressions are based on the standard di6'usion equation

  • We discuss the limiting phase velocity of the photon density wave predicted by the frequency-domain solution of the P, approximation to the Boltzmann transport equation

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Summary

INTRODUCTION

Frequency-domain methods, in which the light source intensity is modulated at radio frequency, have been successfully applied to spectroscopy studies of turbid media [1,2,3,4]. In this paper we discuss the range of optical parameters that can be recovered from the measurement of a single quantity, i.e., the phase of the photon density wave in a range of modulation frequencies. Another reason for doing measurements at GHz modulation frequencies is to perform localized tissue spectroscopy. We discuss the limiting phase velocity of the photon density wave predicted by the frequency-domain solution of the P, approximation to the Boltzmann transport equation. We describe how this limiting phase velocity relates to the leading edge of pulse propagation in a turbid medium

THEORY
Limiting value of the phase velocity
AND METHOD
Superheterodyning electronics
Measurement protocol in the turbid medium
RESULTS
Full Text
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