Audio_part2
May 18, 2026 08:41
· 6:11
· English
· Whisper Turbo
· 2 Konuşmacılar
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Speaker 1 (Audio_part2)
So here is the structure.
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So the top silicon
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cubet that comes to silicon cubet and these
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are fabricated and the glass substrate.
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The deformation
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is given here
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in both in every side of the center cubet.
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whereas the corner cuvette adjust their
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side length to maintain the rotational symmetry
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so this is the periodicity so we have
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fixed the design parameter periodicity is for 70
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nanometer height of the silicon nano disk at 250 nanometer
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and this is and so we have employed
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3d a 3d method to investigate
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the electromagnetic properties so this is when there
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is this blue line this this is a transmission spectrum for
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symmetric and the part of system
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and when there is no perturbation and
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so it is we see no resonance and but when there is 10
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nanometer so we see two obrc arise if
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you want and p2 and this
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is so two resonance arise at 840 nanometer and
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1005 nanometer and
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so the q factor variation as a function of deviation
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is characterized here where it's
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following this classical final formula and
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so which shows exhibit the inverse square law which
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is the standard hallmark of quasi
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-bse structure
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So, this is the dependence of transmission spectra and
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this is on polarization.
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Speaker 2 (Audio_part2)
So,
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this was the polarization.
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You see that both the resonance exhibit
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very polarization in sensitivity and this is the variation
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with the deviation and you see that when there is no
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deviation, so with the deviation we see two resonance
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one at P1 and there is P2.
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so we said the resonance at here it actually
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change with the deviation the resonance wavelength but
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whereas the resonance at p2 fixed
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with the most fixed with the deviation
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so
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It gives,
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so the resonance at P2 gives very stable
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resonance against the perturbation to the
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system.
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This is the variation of height and this is the variation of
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periodicity and both shows very extensive
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Speaker 1 (Audio_part2)
attunability to change
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the, for tuning the.
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spectral response of the resonance this is
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the inclined electric field distribution and
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we see that the
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electric field distribution we see that the mainly electric field and this also shows
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the field line it shows that
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there is a strong electric dipole
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dipolar contribution
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and whereas this shows the some
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kind of electric waterfall contribution and in
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case of here also we see that there is a magnetic field which
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mainly contribute mainly localized in
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the corner and it exhibits some strong and
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the field lines shows the strong magnetic
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dipolar
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and there is also it
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is also seen in strong negative diploid
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to further investigate the properties
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we have calculated the total scattering cross section so the
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total scattering cross section can be expressed by
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this by contribution to the dipolar magnetic
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dipole electric dipole magnetic quadrupole and electric quadrupole system
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and this can be further expressed
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following this formula so we have plotted the
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formula so this gives the
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effect of multiple decomposition active
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resonances so it sees that it is only at a 40
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nanometer the main contribution is coming from electric
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dipole and magnetic dipole contribution whereas in that case the
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main contribution is coming from magnetic
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dipole and electric quadrupole
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The distinct multipolar composition highlight the fundamental different radiation
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mechanism underlying the two QVIC modes.
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In summary,
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we have demonstrated and all directed at a surface that exhibits dual
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-band QVIC,
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and both the VIC exhibits polarization and
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sensitivity, and PHRP2 exhibits strong
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wave -band robustness against system perturbation.
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So, the simple structure of design provides a sensibility of
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web -and -block privacy and privacy for a wide range of applications including
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sensing,
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online optics,
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quantum technologies.
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Speaker 2 (Audio_part2)
Thank you.
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