Abstract
The Kramers-Kronig relation (KKR) is widely used to determine optical parameters of the bulk materials. It allows to restore amplitude reflectance from the energy reflection coefficient measured in a wide spectral band and thus to receive at every wavelength two simple equations for refractive index real and imaginary parts determination1. In the case of reflection from bulk material surface correctness of the KKR is the sequence of the fundamental physical properties.2 These properties prescribe that amplitude reflectance zeros must be located in the lower half-plane.
© 1992 Optical Society of America
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