28 August 2022 to 1 September 2022
Serbian Academy of Sciences and Arts – SASA
Europe/Belgrade timezone

Session

S07 Optics and Photonics

S07-OP
29 Aug 2022, 14:30
Serbian Academy of Sciences and Arts – SASA

Serbian Academy of Sciences and Arts – SASA

Knez Mihailova St. 35, Belgrade

Conveners

S07 Optics and Photonics

  • Milutin Stepić (Vinča Institute of Nuclear Sciences)

Presentation materials

There are no materials yet.

  1. Jose Ordonez-Miranda (Institute of Industrial Science, The University of Tokyo, Tokyo 153-8505, Japan; LIMMS, CNRS-IIS UMI 2820, The University of Tokyo, Tokyo 153-8505, Japan)
    29/08/2022, 14:30
    S07 Optics and Photonics
    Invited talk

    Thermal waves generated by the periodic fluctuations on time of a temperature field are widely used to determine thermal properties of macro-, micro-, and nanomaterials via standard photothermal techniques (thermoreflectance, radiometry, 3w, photoacoustics, and resonant cavity), and they usually do not carry a net heat flux in materials with constant thermal properties. By contrast, in...

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  2. Dr Vadim Sirkeli (Faculty of Physics and Engineering, Moldova State University, Chisinau, Moldova)
    29/08/2022, 15:00
    S07 Optics and Photonics
    Oral presentation (virtual)

    Zinc selenide is a wide bandgap semiconductor which is attractive for the fabrication of many optoelectronic devices, including ultraviolet (UV) photodetectors, due to its large bandgap energy (2.67 eV at 300 K), high electric breakdown field strength (~ 1 MV/cm), as well as high resistance to intense UV and X-ray radiation. Most commercial UV-photodetectors are based on Si or GaAs...

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  3. Prof. Alexander Dreischuh (Sofia University "St. Kliment Ohridski, Bulgaria)
    29/08/2022, 15:15
    S07 Optics and Photonics
    Oral presentation

    One of the processes that is assumed to be well understood, is that any fundamental Gaussian light beam experiences an axial phase shift of $π$ radians with respect of a reference plane wave when passing through its focus. For a higher-order Hermite-Gaussian mode with mode indices ($m,n$) this phase is multiplied by a factor of ($1+m+n$). For a higher-order Laguerre-Gaussian mode with mode...

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