12.3 General Structure Models Interaction of Laser Radiation with a Biotissue
185
Study of the Optical Characteristics of Thin Layer of the Biological Sample for
Case In vitro
Input parameters:
n j (λ) + iχ j (λ) is refractive index of the jth layer,
d j is thickness jth layer,
M 1 ,M 2 are the radii of mirrors,
L is the mirror distance.
σ is the standard deviation of the profile of the rough boundary from the unperturbed
boundary
Output parameters:
ω = ω(d j , n j , iχ j , σ )are frequencies of the resonator eigenmodes
Experimental measurement:
χ j (λ) is dependence of the imaginary part of the refractive index
on simulated biological structures for jth layer.
Calculate:
1. n j (λ) is dependence of the real part of the refractive index epidermis
2. χ j (λ) is dependence of the imaginary part of the refractive index epidermis
Simulation of the Thermal Processes for Case In vivo
Input parameters:
n j (λ) + iχ j (λ)is refractive index of the jth layer,
d j is thickness jth layer,
m
k
1 is refractive index of the cytoplasm
m
k
2 is refractive index of the plasma membrane
a
k
1 is the radius of the cytoplasm of kth particle,
a
k
2 is the radius of the plasma membrane of kth particle,
c
j
0 is specific heat capacity jth layer,
Λ
j is heat conductivity coefficient jth layer,
ρ
j is density jth layer,
μ is absorption coefficient,
E o is radiant energy density,
τ p is pulse duration,
ρ blood is density blood,
T blood is temperature blood,
f (t, T ) is the density of the flow of blood into the tissues,
is the reduced heat-transfer coefficient,
T 0 is the initial temperature,
ΔH is enthalpy of activation,
ΔS is entropy of activation,
185
Study of the Optical Characteristics of Thin Layer of the Biological Sample for
Case In vitro
Input parameters:
n j (λ) + iχ j (λ) is refractive index of the jth layer,
d j is thickness jth layer,
M 1 ,M 2 are the radii of mirrors,
L is the mirror distance.
σ is the standard deviation of the profile of the rough boundary from the unperturbed
boundary
Output parameters:
ω = ω(d j , n j , iχ j , σ )are frequencies of the resonator eigenmodes
Experimental measurement:
χ j (λ) is dependence of the imaginary part of the refractive index
on simulated biological structures for jth layer.
Calculate:
1. n j (λ) is dependence of the real part of the refractive index epidermis
2. χ j (λ) is dependence of the imaginary part of the refractive index epidermis
Simulation of the Thermal Processes for Case In vivo
Input parameters:
n j (λ) + iχ j (λ)is refractive index of the jth layer,
d j is thickness jth layer,
m
k
1 is refractive index of the cytoplasm
m
k
2 is refractive index of the plasma membrane
a
k
1 is the radius of the cytoplasm of kth particle,
a
k
2 is the radius of the plasma membrane of kth particle,
c
j
0 is specific heat capacity jth layer,
Λ
j is heat conductivity coefficient jth layer,
ρ
j is density jth layer,
μ is absorption coefficient,
E o is radiant energy density,
τ p is pulse duration,
ρ blood is density blood,
T blood is temperature blood,
f (t, T ) is the density of the flow of blood into the tissues,
is the reduced heat-transfer coefficient,
T 0 is the initial temperature,
ΔH is enthalpy of activation,
ΔS is entropy of activation,
