wave propagation Flashcards

1
Q

(near field) propagation

A

fresnel

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2
Q

(far field) propagation

A

fraunhofer

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3
Q

First order approximation to propagation problem:

A

Geometric Optics

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4
Q

the phase velocity changes in matter
compared to vacuum by a factor

A

n: refraction index

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5
Q

for visible light: n1 ?? 1
for X-rays: n1 ?? 1

A

for visible light: n1 > 1
for X-rays: n1 < 1

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6
Q

n is complex and for X-rays often written as

A

n = 1- delta + i*beta

delta: phase shift of wave in matter
beta: attenuation

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7
Q

The direction of the waves is given
by the

A

wavevector: kn

kn = 2pi / (lambda n)

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8
Q

snells law

A

n0 * sin(theta0) = n1 * sin(theta1)

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9
Q

Huygens-Fresnel principle

A

Optical field in observation plane can be expressed as sum of spherical waves

exp(ikr)/abs(r)

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10
Q

Corpuscular Theory

A

particle theory of light

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11
Q

Interference of light
Double Slit Experiment done by

A

1804 Thomas Young

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12
Q

1804 Intensity of interference
1815 Polarisation done by

A

Augustin Jean Fresnel

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13
Q

Collimated work on electricity and magnetism
of Michael Faraday and André-Marie Ampère done by

A

1864 james clark maxwell

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14
Q

For isotropic media the polarization does not ………and we restrict ourself to …….. waves

A

For isotropic media the polarization does not change and we restrict ourself to scalar waves

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15
Q

à for electromagnetic waves of the velocity c

A

c = lambda * v
c = 1/sqrt(mu0*eps0)

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16
Q

Gauss’ theorem

A

connects the flux of the vector field
through a closed surface surrounding a volume
with the diverence of this field in the volume

divergence of a vector field
within a volume is equal to flux of the vector field
through surface with
normal vector n

17
Q

the integral theorem of Helmholtz and Kirchhoff

A

it allows to calculate the field at point P0 by integrating over a closed surface around P0

18
Q

Geometric optics ………… to describe diffraction and interference

A

insufficient

19
Q

Scalar Theory:

A

only a single component of E or B
and no polarization

20
Q

What are the components of the Fresnel-Kirchhoff diffraction integral

A

Wave Source:

Integration Variables:
two integration variables: one representing the coordinates of the points on the diffracting aperture or obstacle, and the other representing the observation point in the far-field region where the diffracted wave is being analyzed.

Amplitude Factor:

Phase Factor:

Aperture Function:

Geometrical Factor:

21
Q

Paraxial ray is a ray that makes

A

small angle to optical axis

22
Q

With paraxial & Taylor assumptions
* Free space propagation impulse response becomes

A

parabolic shape

23
Q

When to use Fresnel propagation?
Fresnel propagation is valid if

A

Fresnel number F = a*a/(lambda * z) >= 1

24
Q

Fresnel propagation also known as

A

near field

25
Q

Huygens principle assumes

A

spherical wavefronts

26
Q

Propagated wavefront with Fresnel propagation is given by

A

by the iFT of the product of Fourier transform of wavefront multiplied by the Fresnel kernel

27
Q

Geometric Optics vs Diffraction

A

Geometric Optics:
straight light rays
refraction at surfaces
snells law

Diffraction:
wave propagation
diffraction at apertures
fresnel-kirchoff integral

28
Q

How do we propagate a wave to the Fresnel regime?

A

By convolving with a Fresnel propagator (multiplying in Fourier space)

29
Q

Which wavefront shape is assumed by Fresnel diffraction?

A

parabolic

30
Q

If you propagate the TUM logo with a Fresnel propagator, what would you expect to see?

A

Slighly higher intensity at the edges of the TUM Logo.