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For a transverse path of 1m for Cherenkov light emitted from a particle of normal incidence in fused silica, the time difference for $\beta$=1 and $\beta$=0.99 is only 61ps. However, due to dispersion both emission angle and speed of light in the medium are a function of the wavelength. For 300nm and 600nm photons the time difference is 0.5ns. $ n_{group} = n_{phase} - \lambda dn_{phase}/d\lambda $ <img src="%ATTACHURLPATH%/panda20a2.gif" alt="fused silica - n_phase and n_group" width="350" height="270" align=right /> To calculate the propagation speed of the photons inside the dispersive medium the group velocity has to be used. The dynamic range of the corresponding group velocity refractive index is about 3 times larger than that of the normal refractive index. The figure shows these velocities for fused silica. -- Main.KlausFoehl - 14 Sep 2005
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14 Sep 2005 - 18:07
KlausFoehl
fused silica - n_phase and n_group
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Topic revision: r1 - 14 Sep 2005,
KlausFoehl
Cerenkov/Pandacerenkov
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