1983
DOI: 10.1063/1.525695
|View full text |Cite
|
Sign up to set email alerts
|

Exact solutions to the valley problem in inverse scattering

Abstract: Standard approximate methods involving the Abel integral equation do not allow the ionospheric electron density to be determined in the ‘‘valley’’ between two electron density peaks. Here we present analytic solutions to the Gel’fand–Levitan equation, which occurs in the exact full-wave inverse scattering theory. These exact analytic solutions exhibit multiple peaks in the electron density as a function of height and provide a solution to the valley problem.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
7
0

Year Published

1983
1983
2014
2014

Publication Types

Select...
3
2
1

Relationship

0
6

Authors

Journals

citations
Cited by 7 publications
(7 citation statements)
references
References 8 publications
0
7
0
Order By: Relevance
“…This is shown in Figure 10. Of additional interest is the fact that if the pole positions are chosen to all be located in the same neighborhood but with displacement  , thus avoiding multiplicity which would void the inverse-scattering technique 17 , then the threepole, five-pole and seven-pole cases demonstrate similar values of waveguide dispersion 2 D and dispersion curvature 4 D but significant reduction of dispersion slope as shown in Table 1. Associated with this change in dispersion slope is an expansion and exaggeration of the core, ring and trench as shown in Figure 11.…”
Section: Five-pole and Seven-pole Rational Reflection Coefficientsmentioning
confidence: 85%
See 2 more Smart Citations
“…This is shown in Figure 10. Of additional interest is the fact that if the pole positions are chosen to all be located in the same neighborhood but with displacement  , thus avoiding multiplicity which would void the inverse-scattering technique 17 , then the threepole, five-pole and seven-pole cases demonstrate similar values of waveguide dispersion 2 D and dispersion curvature 4 D but significant reduction of dispersion slope as shown in Table 1. Associated with this change in dispersion slope is an expansion and exaggeration of the core, ring and trench as shown in Figure 11.…”
Section: Five-pole and Seven-pole Rational Reflection Coefficientsmentioning
confidence: 85%
“…Conservation of energy, ( ) 1 rk  for all real k , dictates that the parameter space is limited. Previous authors 6 , 7 have identified and considered the allowable region bounded above by the line 2 0.5 c  and to the right by the lemniscate of Bernoulli 17 . The allowable region can be extended past these points as is illustrated in Figure 2 below which shows the dispersion 2 D , dispersion slope 3 D and dispersion curvature 4 D associated with the allowable region.…”
Section: Three-pole Rational Reflection Coefficientsmentioning
confidence: 99%
See 1 more Smart Citation
“…since the condition |r(k)| ≤ 1 holds for real k in this case To solve integral equation (24), we use the method described in [6], which yields the following result:…”
Section: Exact Model Solutions Of the Inverse Problem Of Electromagnementioning
confidence: 99%
“…There exist exact analytical solutions of this equation for the reflection coefficients in the form of fractional rational functions which can be used as model approximations of the electron number density [5,6].…”
Section: Introductionmentioning
confidence: 99%