Solitons in Nonlocal Media
Solitons in Nonlocal Media
Solitons in Nonlocal Media
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LIST OF FIGURES<br />
3.2 (a,b) Perturbation profiles versus ξ for 〈ξ〉 = 0.5, 0.63, 0.76 and 0.9 (solid<br />
l<strong>in</strong>e, squares, stars and triangles, respectively) for (a) ω = 0.001 and (b)<br />
ω = 0.09. The profile <strong>in</strong> (a) is very similar to the Green function, as<br />
the soliton is much narrower than the sample width. (c) Calculated<br />
α (squares) and α s for 〈ξ〉 = 0.54 (no symbols), 〈ξ〉 = 0.72 (stars)<br />
and 〈ξ〉 = 0.86 (triangles), respectively, versus normalized waist ω. (d)<br />
Calculated α g for the same set of soliton positions. . . . . . . . . . . . . 40<br />
3.3 Calculated V ξ m(ξ) for ω = 0.02 and 〈ξ〉 = 0.5(solid l<strong>in</strong>e), ω = 0.02 and<br />
〈ξ〉 = 0.75 (asterisks), ω = 0.1 and 〈ξ〉 = 0.5 (triangles), ω = 0.1 and<br />
〈ξ〉 = 0.75 (squares), respectively. The numerical results are <strong>in</strong> complete<br />
agreement with the theoretical approximation. (b, c) Calculated degree<br />
of nonlocality along x and (d) along t for 〈ξ〉 = 0.5 (circles), 〈ξ〉 = 0.54<br />
(solid l<strong>in</strong>e), 〈ξ〉 = 0.68 (squares) and 〈ξ〉 = 0.81 (triangles), respectively. 45<br />
3.4 Perturbation profiles for (a,c) ω = 0.01 and (b,d) ω = 0.1 for (a,b)<br />
〈ξ〉 = 0.5 and (c,d) 〈ξ〉 = 0.75. The dashed (solid) l<strong>in</strong>es correspond<br />
to profiles along υ(ξ − 〈ξ〉). The profiles are chosen such to conta<strong>in</strong><br />
the perturbation peak. Squares (triangles) are the correspond<strong>in</strong>g values<br />
computed with a full numerical approach, which completely agree with<br />
the theoretical predictions from eq. (3.20). . . . . . . . . . . . . . . . . . 46<br />
3.5 Calculated figure of nonlocality αx for Gaussian <strong>in</strong>tensity profiles (curves<br />
for αt and α g/s<br />
x/t are nearly identical) versus ω for 〈ξ〉 = 0.5 and (a,b)<br />
µ/κ = 102 or (c,d) µ/κ = 104 . In this range for µ/κ, the nonlocality<br />
does not depend on beam position. When αx = 1, perturbation and<br />
excitation have the same profile, i.e. the medium is local. (b) - (d):<br />
perturbation profile along υ(symbols) and ξ−〈ξ〉(solid l<strong>in</strong>e) for µ/κ = 10 2<br />
and µ/κ = 10 4 , respectively, when ω = 0.035 and 〈ξ〉 = 0.5; <strong>in</strong> both cases<br />
the perturbation possesses radial symmetry. In (b) the perturbation is<br />
wider due to a higher ratio µ/κ. . . . . . . . . . . . . . . . . . . . . . . . 49<br />
3.6 Plots of g1 (a,d) and g2 (b,e) for 〈ξ〉 = 0.5. The correspond<strong>in</strong>g profiles<br />
are plotted <strong>in</strong> (c) and (f) versus ξ (g1 solid l<strong>in</strong>e, g2 squares) and υ (g1<br />
dashed l<strong>in</strong>e, g2 triangles), normalized to one (the cross sections are <strong>in</strong><br />
υ = 0 and ξ = 0.5, respectively). Results for g1 and g2 perfectly overlap.<br />
Excitation waists are ω = 0.03 (a,b,c) and ω = 0.1 (d,e,f), respectively. . 53<br />
x