chapter 10 diffraction - seoul national universityshhong.snu.ac.kr/lecture/2014_02/2014 chapter...
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Chapter 10 Diffraction
Reading Assignment:1. D. Sherwood, Crystals, X-rays, and
Proteins-chapter 6http://www.matter.org.uk/diffraction/Default.htm
Contents
Diffraction and Information
Mathematics of Diffraction
Fourier Transform
3
1
2
4
Diffraction
5 Experimental Limitations
Interaction of waves with obstacles- interaction of waves with obstacles
infinite plane wave with wave vector and frequency
obstacle- perturb the wave motion in some way
-scattering- wave-obstacle interaction such that the
dimensions of obstacles and wavelength are comparable
diffraction- wave-obstacle interaction such that the
dimensions of obstacles are much larger than the
wavelength of the wave motion
( )i k r wtoeψ ψ −=
k
w
X-ray (~1Å)
crystal (~10mm)
atom (~1nm) scattering-microscopic
diffraction-macroscopic
Diffraction of X-rays
D. Sherwood, Crystals, X-rays, and Proteins
Diffraction of Water Waves
- ripple tankrule-periodic dipping plane water wave
long-no reflection
- transparent base-light shadow on the screen
- synchronize light withwave motion- frozen in stroboscopic ripple
tank
D. Sherwood, Crystals, X-rays, and Proteins
Diffraction of Water Waves
- obstacle- plane wavecurved wave
D. Sherwood, Crystals, X-rays, and Proteins
D. Halliday, Fundamentals of Physics
Diffraction of Water Waves
- when slit width is wide compared to the wavelengthof the wave motion, the diffraction effects are masked
D. Sherwood, Crystals, X-rays, and Proteins
Diffraction and Information
- plane wave obstacle semi-circulardiffracted wave contains additional
information about obstacle
- When a wave interacts with an obstacle, diffractionoccurs. The detailed behavior depends solely on thediffracting obstacles, and so the diffracted waves maybe regarded as containing information on the structureof the obstacles.
- ex) X-ray
crystal
diffracted pattern
information about nature of moleculesand the way they are packed
reconstructobstacle
Diffraction of Light
D. Halliday, Fundamentals of Physics
Poisson’s Bright Spot
http://www.richmond.edu/~ebunn/phys205/cache/poisson.html
Diffraction of X-rays
crystal: well-defined, 3D orderedarray
X-ray
atom, molecule
well-defined phase relationshipbetween scattered waves
clear and precisediffraction pattern
* liquid- diffuse and impreciseD. Sherwood, Crystals, X-rays, and Proteins
Mathematics of Diffraction
-assumption-structure and all physical properties ofthe diffracting obstacle are known.
(diffraction pattern-recipe)-plane electromagnetic waves of a single
frequency and wavelength are incident normally on the obstacle.
(a) frequency and wavelength
w λ
incident wave
diffracted wave
E w w
w
electrons in the moleculeoscillate
free
Mathematics of Diffraction
(a) frequency and wavelength
in any medium, velocity of electromagnetic radiationis constantwavelength is also unchanged
* diffracted waves have the same frequency andwavelength as the incident waves.
* electrons in the molecules are not really free
* during one cycle of the X-radiation, the electron has hardly changed its position relative to thenucleus electron forget the presence of nucleus electrons behave as if it were free
λ
19
16
X-ray : 0.1 nm, 10 Hzorbital motion of an electron: 10 Hz
ww
λ = =
=
Mathematics of Diffraction
(b) spatial consideration
frequency and wavelength unchangedsome other effect
plane wave spatially different wave* information of the wave is somehow contained in the
way in which they are spread out in space.
emit in all directions
superpositionemit in all directionsin space
emit in all directions
Mathematics of Diffraction
(c) significance of the wave vector k
( )o=
2magnitude :
direction: normal to the advancing wavefront
spatial information* total set of diffracted waves may be represented by a set of wave vectors all of which have th
i k r wte
k k
k
ψ ψπλ
−
= =
→
e same magnitude, equal to that of incident wave, but different directions
Mathematics of Diffraction(d) mathematical description
- assumption- structure and physical properties known- phenomenon- (1) waves are propagated through obstacle (2) obstacle perturb these waves
- arbitrary origin, position vector
11 1
1 1
( )
,
infinitesimal volume element centered on by
- volume element centered on
perturbing effect ( )
i k r wt
r
r d r
d r r
f r d r
e −→
D. Sherwood, Crystals, X-rays, and Proteins
Mathematics of Diffraction
1
1
1
1 1
1
1 1
1 1
( )
( )
( )
- two different way of combining and ( )
diffracted wave from volume element
( ) or
( )
- consider a pe
-
-
i k r wt
i k r wt
i k r wt
f r d r
dr
f r d r
f r d r
e
e
e
−
−
−
+
11 1 1
2
( )
rfectly absorbing obstacle ( ) 0 no diffracted wave second equation is correct
- wave diffracted from volume element ( )
- wave diffracted from volume element (
i k r wt
f r
d r f r d r
dr f r
e −
→ =→
=
=
22 1
( )) i k r wt d re −
Mathematics of Diffraction
1 2
3
1 21 1
3 3
( ) ( )
( )
- Principle of superposition
diffraction pattern = ( ) ( )
( )
i k r wt i k r wt
i k r wt
f r d r f r d r
f r d r
e e
e
− −
−
+
+
V
-
19 19
( ) = ( )
= ( )
- X-ray: ~0.1 nm, ~ 10 Hz, one cycle ~ 10 sec- no recording device is availabele- diffraction expe
iwt
V
i k r wt
ik r
f r d r
e f r d r
w E
e
e
λ −
−∫
∫
riment- time average of the intensity of the diffracted wave
Mathematics of Diffraction
- diffraction pattern = ( )
- limits on the integral
( ) : finite mathematically not well behaved
define ( ) over an infinite range dividing the values into two domains
diff
V
ik rf r d r
f r
f r
e
→
∫
all
raction pattern = ( )
( )
( ) : amplitude function- diffraction pattern of any obstacle is the Fourier transform of the ampli
Fourier
tude
trn
funct
asform of ( )
ion
ik r
r
f r
f
d r
f r
r
e∫
Significance of Fourier Transform
all
- diffraction pattern = ( )
1. integrand - function of and , integration - over
diffraction pattern ( )
information in the diffraction pattern-spatial k
2.
ik r
r
ik
f r d r
k r r
F k
e
e
→
←
∫
: wave, ( ) : amplitude type function passive scatterer replaced by active source identical
r f r→ →
Fourier Transform and Shape
1 2
1 1
0 0 1 1 2 2
- a linear array of scattering center in an obstacle- phase at point 0=0
2 phase at point 1= OA( cos )
- total scattered wave= ( ) ( ) ( )ik r ik r
r k r
f r d r f r e dr f r e dr
π θλ
= =
+ + +
= ( )
- exponential term-specifiy phase relationship between scattering centers and an arbitrary origin
obstacle
ik rf r e d r∫
Fourier Transform and Information
- ( ) ik rf r e
amplitude modulated
5
- AM radio radio frequency (of order 10 Hz) audio frequency (of order 500 Hz)
ik re ( )f r
D. Sherwood, Crystals, X-rays, and Proteins
Fourier Transform and Information
- diffraction pattern in terms of Fourier transform
(i) the description is, as required, a function of k (ii) the decription agrees with our physical knowledge of the interaction of wave w
ith obstacles (iii) the description represents a general solution of three-dimensional wave equation (iv) the description is capable of containing the required information
Inverse Transform
all
all
- diffraction pattern ( )
( )= ( )
( ) is Fourier transform of ( )- inverse transform
( )= ( )
- ( ) : diffraction pattern functio
ik r
r
ik r
k
F k
F k f r d r
F k f r
f r F k dk
F k
e
e−
∫
∫
2
n- information on spatial distribution of diffraction pattern
( ): information on the structure of obstacle
- diffraction experiment intensity ( ) ( ) ( )
f r
F k F k f r→ ∝ → →
Microscope
D. Sherwood, Crystals, X-rays, and Proteins
Experimental Limitation
all
- diffraction pattern ( )
( )= ( )
- information contained in all space physically impossible to scan all space to collect some information lost- phase problem measur
ik r
r
F k
F k f r d re∫
2
e only the intensity not the complex amplitude of diffraction pattern
( ) ( )
observe ( ) lost information on
iF k F k e
F k
δ
δ
=
→