Top Banner
Today Ch.36 (Diffraction) Next week, Dec.6, Review This week off. hours: Th: 2:00-3:15pm; F: 1:00-3:00pm Next week off. hours: Tu:2-3:15pm,W:1-3pm,Th:1-3pm Webct homework is due by Dec.12. Check your Midterm Exams Grades on elearning! Final Exam: (Ch.21-25, 27-29, 32,33,35,36) Secs.511-515: December 9, Friday: 12:30-2:30 pm Secs.521-525, 528: December 12,
29

Today Ch.36 (Diffraction) Next week, Dec.6, Review This week off. hours:

Feb 03, 2016

Download

Documents

magar

Today Ch.36 (Diffraction) Next week, Dec.6, Review This week off. hours: Th: 2:00-3:15pm; F: 1:00-3:00pm Next week off. hours: Tu:2-3:15pm,W:1-3pm,Th:1-3pm Webct homework is due by Dec.12. Check your Midterm Exams Grades on elearning! Final Exam: (Ch.21-25, 27-29, 32,33,35,36). - PowerPoint PPT Presentation
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Today Ch.36 (Diffraction) Next week, Dec.6, ReviewThis week off. hours: Th: 2:00-3:15pm; F: 1:00-3:00pmNext week off. hours:Tu:2-3:15pm,W:1-3pm,Th:1-3pmWebct homework is due by Dec.12.Check your Midterm Exams Grades on elearning!

Final Exam: (Ch.21-25, 27-29, 32,33,35,36)

Secs.511-515: December 9, Friday: 12:30-2:30 pmSecs.521-525, 528: December 12, Monday, 8-10 am

Page 2: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Lecture 24 (Ch. 36)

Diffraction1. Huygen’s principle, bending of the rays2. Fraunhofer’s diffraction3. Single slit4.Two slits with a finite width5. Resolution of the lens6. Diffraction grating7.Spectroscopy8. x-ray diffraction9. e diffraction

Page 3: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Huygen’s principle and bending of the rays

Page 4: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

1788 – 1827

Augustin-Jean Fresnel

Joseph von Fraunhofer (1787 – 1826)

Page 5: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Single slit diffraction

How to describe the real picture?

Page 6: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Single slit diffraction

ma

xy

x

ysmallfor

axistoparallelraysallm

mNBmma

asta

m

:min,tansin;

)max!00(

!0:,...)2,1(sin:min

sinmin)1(2

sin2

r

sinar

Page 7: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:
Page 8: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Intensity distribution

1st max 0

sin

2ark

)12(:max

)0(sin2:min

}

2

2sin

{,

2

2sin

,,2

sin2

200

0

m

mmam

IIEER

ER

E

R=

E

21st min: 1st max: 3

E

Page 9: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

)0(sin2:min;}

2

2sin

{ 20 mmamII

Page 10: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

a

1

Narrowing of the first fringe with increase of the slit width

Page 11: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Circular hole diffraction

Page 12: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

The photographs of four very small sources of light taken made with a circular aperture in front of the lens

Page 13: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

)7.4(650:

)7.0(780:

gigabytesnmDVD

gigabytesnmCD

Rayleigh’s criterion for resolution of two point objects: Two objects are barely resolved if the center of one diffraction pattern coincides with the first minimum if the other.

L

DLS

22.1sin

For a microscop

1842 – 1919John William Strutt, 3rd Baron Rayleigh

Page 14: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Hubble vs Arecibo

Hubble: D=2.4m, nm500Arecibo: D=300m, cm75

kmDkmS

kmss

myearcly

CentaurystarnearestlyL

sizecraterkmSmS

moonthetomL

DLS

JupiterH

AH

57

1378

8

10,10

101010311

),(4

)(1000,77

)(108.3

22.1sin

Page 15: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Giant Magellan Telescope (2016)

D1=8.5m, Deq=24m nm500

Page 16: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Interferometry: Arrays of telescopes

Page 17: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Two slits with a finite width

2cos}

2

2sin

{4

sin,

2

2sin

)(:

sin,2

cos)(2:

220

00

0

II

kaEEfactorDifraction

kdEEfactornceInterefere

Page 18: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Diffraction grating

mdm sin2:max

!02

0 ININEE otot

tE0

Page 19: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

N-1 minima

Page 20: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

With increase of N principal maxima becomes narrower

and their amplitude grows as 2N

Page 21: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:
Page 22: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Grating spectroscopySpectrum of sunlight produced by a diffraction grating has dark absorption lines due to absorption of the corresponding wavelength by the solar atmosphere. It allows to find out a chemical composition of the solar atmosphere.

Page 23: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

x-ray diffraction

Wilhelm Röntgen (1845 – 1923)The 1st Nobel Prize,1901

nm101.0~

Page 24: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Bragg condition

nd sin2

An x-ray scattering pattern of DNA recorded by Rosalind Franklin led Watson and Crick to discovery of the DNA double helix structure

Page 25: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Louis de Broglie (1892 – 1987)

Page 26: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:
Page 27: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Electromagnetically induced transparency (EIT)

Two undistinguishable absorption passes for light result in cancellation of absorption (transparency).An electron has the wave property. It may be in a superposition of states 1 and 1’. Monohromatic light with a frequency resonant either to one or another atomic transition is absorbed.Bichromatic light containing two resonant frequencies goes through.

11’

1 2

O.K., Y.I.Khanin, JETP, 1986; O.K., P. Mandel, Phys. Rev. A. 1990. theory S.E. Harris, PRL, 1991. experiment

Page 28: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours:

Electromagnetically induced transparency (EIT)Two undistinguishable absorption passes for light result in cancellation of absorption (transparency).An electron has the wave property. It may be in a superposition of states 1 and 1’. A circular polarized light interacts only with 1-2 (or 1’-2) state and absorbed. A linear polarized light interacts with both 1-2 and 1-2’ states and goes through the medium without absorption. To make medium transparent for light with given circular polarization send through the medium simultaneously light with another circular polarization.

The same is true for two beams of different frequenciesWhen the frequency difference coincides with the frequency of the atomic transition 1-1’.

1

1’

2

1

1’

1 2

O.K., Y.I.Khanin, JETP, 1986; O.K., P. Mandel, Phys. Rev. A. 1990. theory S.E. Harris, PRL, 1991. experiment

Page 29: Today Ch.36 (Diffraction)  Next week, Dec.6, Review This week off. hours: