TY - JOUR
T1 - Reflection statistics of weakly disordered optical medium when its mean refractive index is different from an outside medium
AU - Pradhan, Prabhakar
AU - John Park, Daniel
AU - Capoglu, Ilker
AU - Subramanian, Hariharan
AU - Damania, Dhwanil
AU - Cherkezyan, Lusik
AU - Taflove, Allen
AU - Backman, Vadim
N1 - Funding Information:
This work was partly supported by NIH grants (Nos. R01EB003682, R01EB016983, R01CA128641 and U54CA143869), a NSF grant no CBET-0937987, a FedEx Institute of Technology Grant, and a Faculty Research Grant from the University of Memphis.
Publisher Copyright:
© 2017 Elsevier B.V.
PY - 2017/6/15
Y1 - 2017/6/15
N2 - Statistical properties of light waves reflected from a one-dimensional (1D) disordered optical medium [n(x) = n0 + dn(x), =0] have been well studied, however, most of the studies have focused on the situation when the mean refractive index of the optical medium matched with the outside medium, i.e., n0 = nout =1. Further, considering dn(x) as a Gaussian color noise refractive index medium with exponential spatial correlation decay length lc and k as the incident wave vector, it has been shown that for smaller correlation length limit, i.e., klc <<1, both the mean reflection coefficient and std of r, σ(r), have same value, and they follow the relation = σ(r) ∝ 2> lc. However, when the refractive index of the sample medium is different from the outside medium, the reflection statistics may have interesting features, which has not been well studied or understood. We studied the reflection statistics of a 1D weakly disordered optical medium with the mean background refractive index n0 being different from the outside medium nout (≠n0), to see the effect of mismatching (i.e., value of n0 - nout) on the reflection statistics. In the mismatched case, the results show that the mean reflection coefficient follows a form similar to that of the matched refractive-index case, i.e., c)>∝ 2> lc, with a linear increased shift, which is due to 1D uniform background reflection from a slab. However, σ(r) is shown to be σ(r) ∝ (2>lc)1/2, which is different from the matched case. This change in std of r is attributed to the interference between the mismatched-crerated edge mediated multiple scattering that are coupled with the random scattering. Applications to light scattering from random layered media and biological cells are discussed.
AB - Statistical properties of light waves reflected from a one-dimensional (1D) disordered optical medium [n(x) = n0 + dn(x), =0] have been well studied, however, most of the studies have focused on the situation when the mean refractive index of the optical medium matched with the outside medium, i.e., n0 = nout =1. Further, considering dn(x) as a Gaussian color noise refractive index medium with exponential spatial correlation decay length lc and k as the incident wave vector, it has been shown that for smaller correlation length limit, i.e., klc <<1, both the mean reflection coefficient and std of r, σ(r), have same value, and they follow the relation = σ(r) ∝ 2> lc. However, when the refractive index of the sample medium is different from the outside medium, the reflection statistics may have interesting features, which has not been well studied or understood. We studied the reflection statistics of a 1D weakly disordered optical medium with the mean background refractive index n0 being different from the outside medium nout (≠n0), to see the effect of mismatching (i.e., value of n0 - nout) on the reflection statistics. In the mismatched case, the results show that the mean reflection coefficient follows a form similar to that of the matched refractive-index case, i.e., c)>∝ 2> lc, with a linear increased shift, which is due to 1D uniform background reflection from a slab. However, σ(r) is shown to be σ(r) ∝ (2>lc)1/2, which is different from the matched case. This change in std of r is attributed to the interference between the mismatched-crerated edge mediated multiple scattering that are coupled with the random scattering. Applications to light scattering from random layered media and biological cells are discussed.
KW - Backscattering
KW - Cancer detection
KW - Scattering theory
KW - Weakly disordered biological media
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U2 - 10.1016/j.optcom.2017.02.041
DO - 10.1016/j.optcom.2017.02.041
M3 - Article
AN - SCOPUS:85013664295
VL - 393
SP - 185
EP - 190
JO - Optics Communications
JF - Optics Communications
SN - 0030-4018
ER -