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Exact zero transmission during the Fano resonance phenomenon in non-symmetric waveguides. / Chesnel, Lucas; Nazarov, Sergei A.
в: Zeitschrift fur Angewandte Mathematik und Physik, Том 71, № 3, 82, 04.05.2020.Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
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TY - JOUR
T1 - Exact zero transmission during the Fano resonance phenomenon in non-symmetric waveguides
AU - Chesnel, Lucas
AU - Nazarov, Sergei A.
PY - 2020/5/4
Y1 - 2020/5/4
N2 - We investigate a time-harmonic wave problem in a waveguide. We work at low frequency so that only one mode can propagate. It is known that the scattering matrix exhibits a rapid variation for real frequencies in a vicinity of a complex resonance located close to the real axis. This is the so-called Fano resonance phenomenon. And when the geometry presents certain properties of symmetry, there are two different real frequencies such that we have either R= 0 or T= 0 , where R and T denote the reflection and transmission coefficients. In this work, we prove that without the assumption of symmetry of the geometry, quite surprisingly, there is always one real frequency for which we have T= 0. In this situation, all the energy sent in the waveguide is backscattered. However in general, we do not have R= 0 in the process. We provide numerical results to illustrate our theorems.
AB - We investigate a time-harmonic wave problem in a waveguide. We work at low frequency so that only one mode can propagate. It is known that the scattering matrix exhibits a rapid variation for real frequencies in a vicinity of a complex resonance located close to the real axis. This is the so-called Fano resonance phenomenon. And when the geometry presents certain properties of symmetry, there are two different real frequencies such that we have either R= 0 or T= 0 , where R and T denote the reflection and transmission coefficients. In this work, we prove that without the assumption of symmetry of the geometry, quite surprisingly, there is always one real frequency for which we have T= 0. In this situation, all the energy sent in the waveguide is backscattered. However in general, we do not have R= 0 in the process. We provide numerical results to illustrate our theorems.
KW - Fano resonance
KW - Scattering matrix
KW - Waveguides
KW - Zero transmission
KW - TRAPPED MODES
KW - EIGENVALUE
KW - REFLECTION
KW - COMPLEX RESONANCES
KW - ENFORCED STABILITY
KW - CONTINUOUS-SPECTRUM
UR - http://www.scopus.com/inward/record.url?scp=85084189822&partnerID=8YFLogxK
U2 - 10.1007/s00033-020-01305-9
DO - 10.1007/s00033-020-01305-9
M3 - Article
AN - SCOPUS:85084189822
VL - 71
JO - Zeitschrift fur Angewandte Mathematik und Physik
JF - Zeitschrift fur Angewandte Mathematik und Physik
SN - 0044-2275
IS - 3
M1 - 82
ER -
ID: 60873423