wave propagation Flashcards
(near field) propagation
fresnel
(far field) propagation
fraunhofer
First order approximation to propagation problem:
Geometric Optics
the phase velocity changes in matter
compared to vacuum by a factor
n: refraction index
for visible light: n1 ?? 1
for X-rays: n1 ?? 1
for visible light: n1 > 1
for X-rays: n1 < 1
n is complex and for X-rays often written as
n = 1- delta + i*beta
delta: phase shift of wave in matter
beta: attenuation
The direction of the waves is given
by the
wavevector: kn
kn = 2pi / (lambda n)
snells law
n0 * sin(theta0) = n1 * sin(theta1)
Huygens-Fresnel principle
Optical field in observation plane can be expressed as sum of spherical waves
exp(ikr)/abs(r)
Corpuscular Theory
particle theory of light
Interference of light
Double Slit Experiment done by
1804 Thomas Young
1804 Intensity of interference
1815 Polarisation done by
Augustin Jean Fresnel
Collimated work on electricity and magnetism
of Michael Faraday and André-Marie Ampère done by
1864 james clark maxwell
For isotropic media the polarization does not ………and we restrict ourself to …….. waves
For isotropic media the polarization does not change and we restrict ourself to scalar waves
à for electromagnetic waves of the velocity c
c = lambda * v
c = 1/sqrt(mu0*eps0)