wave propagation II Flashcards

1
Q

For the Fresnel approximation z is small but still

A

z&raquo_space; (x0-u)+(y0-v)

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2
Q

Fraunhofer Propagation known as

A

Also known as ‘Far field’ approximation

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3
Q

replace which wavefronts to what

A

Replace spherical wavefronts of Huygens principle or parabolic wavefronts of Fresnel propagation with planar wavefronts

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4
Q

fraunhofer model holds if

A

F = a*a/(lambda * z) &laquo_space;1
ie. z is large

fixed a: is the resolution you want to archive
fixed lambda: is the wavelength you use
variable z: is the distance of detector to sample

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5
Q

Rayleigh resolution criterion

A

Just resolved if maximum of first Airy disk falls on
first zero of second Airy disk

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6
Q

Sparrow resolution criterion

A

Just resolved if there is a vanishing derivative
in the center of the sum of the first and second Airy disk

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7
Q

The atmosphere is a major problem for

A

ground-based telescopes because of atmospheric turbulence (changing refractive index)

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8
Q

Fraunhofer propagation implies a Fourier transform relationship between the

A

complex field at the aperture and focal plane

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9
Q

fraunhofer: Measured intensity is absolute value of

A

complex field squared

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10
Q

x ray:
+ at higher energies …… absorption (……. dose)
+ and …… cross section ~1000 times bigger (better …….

A

+ at higher energies less absorption (lower dose)
+ and phase shift cross section ~1000 times bigger (better contrast

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11
Q

Fresnel Regime to small z
typically at least two unknowns:

A

attenuation and phase

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12
Q

Two propagation distances – a direct solution
The result is called

A

Transport of Intensity Equation” (TIE)

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13
Q

one propagation distance steps

A
  1. Take the Intensity at distance z=d
  2. Divide by the incident intensity (normalize)
  3. Take the Fourier transform
  4. Multiply by a filter term in Fourier space ( )
  5. Take the inverse Fourier transform
  6. Scale the answer to make it quantitative

filter term:
Inverse proportional to distance from origin (ie. low-pass filter)
* Tuned to sample material (d,µ) and propagation distance (d)
* Acting more strongly when phase (d) is large compared to attenuation
(µ), or when the propagation distance (z=d) is large.

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14
Q

Fraunhofer (far field) propagation
Intensity is squared Fourier transform of the wave at

A

the aperture

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15
Q

Propagation based Phase Contrast:;

Measured intensities > Equation
Two unknowns <–>
Paganin‘s one distance method with…… filter

A

Measured intensities > Transport of Intensity Equation
Two unknowns <–> two distances
Paganin‘s one distance method with d/µ filter

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16
Q

True or false?
The propagation-based phase-contrast imaging is a far-field imaging method.

A

False

17
Q

T or F?
phase contrast uses the phase shift due to vphase > cvacuum inside the object as contrast mechanism

A

True

18
Q

What is the additional assumption for the single distance method?

A

It is assumed that for homogeneous samples the ratio delta/mu is constant.

no coherence/no isolation assumption