The effect on the propagation characteristics due to a low-index buffer layer added over a lossy superconductive leaky waveguide in a high-index substrate is related to a transition from the guided modes to the leaky one. For a guided waveguide structure, neglecting the high-index substrate, the TM mode field amplitude is more confined within the core layer and in superconducting thin film and more evanescent in the air claddings than the corresponding TE mode profile. Moreover, both the TE and TM mode profiles of the buffered waveguide leaks out more into the high-index substrate in comparison with those of the waveguide with a larger buffer thickness. This behaviour is confirmed by the fraction of the power carried by the modes along of the propagation direction.

Determination of field profiles in buffer superconducting multilayer optical planar waveguides / Popescu, V. A.; Puscas, N. N.; Perrone, Guido. - In: JOURNAL OF OPTOELECTRONICS AND ADVANCED MATERIALS. - ISSN 1454-4164. - STAMPA. - 12:5(2010), pp. 994-999.

Determination of field profiles in buffer superconducting multilayer optical planar waveguides

PERRONE, Guido
2010

Abstract

The effect on the propagation characteristics due to a low-index buffer layer added over a lossy superconductive leaky waveguide in a high-index substrate is related to a transition from the guided modes to the leaky one. For a guided waveguide structure, neglecting the high-index substrate, the TM mode field amplitude is more confined within the core layer and in superconducting thin film and more evanescent in the air claddings than the corresponding TE mode profile. Moreover, both the TE and TM mode profiles of the buffered waveguide leaks out more into the high-index substrate in comparison with those of the waveguide with a larger buffer thickness. This behaviour is confirmed by the fraction of the power carried by the modes along of the propagation direction.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11583/2422317
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