Figures from    ftrue_higuchi.for      program and also for Alsop's Figure 13

Name of file:lat_scat_test_081209.html
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Created on:8/12/09 (5:40 AM)
Revised on:8/13/09 (1:20AM)
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Key Reference email(s):
1) Los Angeles, 3:26 PM Monday, August 10, 2009
2) Los Angeles, 3:24 PM Tuesday, August 11, 2009

A. Figures for Higuchi Model

A.1 Exact solutions for R/T coefficients for HIGUCHI model when the "fundamental assumption" is applied.

a. (v_R_11)_Higuchi = (v_R_11)_latave        Here, "EXACT" = "DIRECT" in the output.

b. (v_T_11)_Higuchi = (v_T_11)_latave        Here, "EXACT" = "DIRECT" in the output.

The "scattering ratio" that you see besides the "Fractional energy" in the lowermost panel is actually the    RATIOE(I)     that you computed in ftrue_f13_enbal.for 

         RATIOE(I) = ( OMEGA(I) * K_LEFT(I) * LSHLFT(I) * RLFRHD(I)**2 +
     1                 OMEGA(I) * KRIGHT(I) * LSHRHT(I) * TLFRHD(I)**2 )
     2               / 
     3               ( OMEGA(I) * K_LEFT(I) * LSHLFT(I) * 1.000D+00**2 )

A.2 Other parameters for HIGUCHI model when the "fundamental assumption" is applied. In the upper panel, the wavenumber    k     is always increasing as frequency increases. In the second and third panels, the subtraction of LEFT side and RIGHT will equal to parameter in the CENTER.

A.3 Ratio

 

B. Figures for Alsop's Figure 13

A.1 Exact solutions for R/T coefficients from laterally-averaged Alsop's Figure 13. The method where we used

( v_R_11 )_latave = (1 - a)/(1 + a )     and       ( v_T_11 )_latave = 2/(1 + a)

produces the same results.

The "scattering ratio" that you see besides the "Fractional energy" in the lowermost panel is actually the    RATIOE(I)     that you computed in ftrue_f13_enbal.for 

         RATIOE(I) = ( OMEGA(I) * K_LEFT(I) * LSHLFT(I) * RLFRHD(I)**2 +
     1                 OMEGA(I) * KRIGHT(I) * LSHRHT(I) * TLFRHD(I)**2 )
     2               / 
     3               ( OMEGA(I) * K_LEFT(I) * LSHLFT(I) * 1.000D+00**2 )

A.2 Other parameters. In the upper panel, the wavenumber    k     is always increasing as frequency increases. In the second and third panels, the subtraction of LEFT side and RIGHT will equal to parameter in the CENTER.

A.3

A.4 | Direct - Exact | .

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