Добавил:
Upload Опубликованный материал нарушает ваши авторские права? Сообщите нам.
Вуз: Предмет: Файл:

VLE 3 Wave optics

.pdf
Скачиваний:
9
Добавлен:
12.03.2015
Размер:
3.44 Mб
Скачать

9. Double slit and grating

71

Prof. M. Schmidt

Institute of Photonic Technologies, Univ. Erlangen, Germany

Young‘s double slit experiment

The Young’s double slit is a further experiment to prove light is a wave.

Setup: single slit to generate coherent beam

The two close slits:

72

Prof. M. Schmidt

Institute of Photonic Technologies, Univ. Erlangen, Germany

Double slit (1)

After the double slit there are two cylinder waves which interfere.

The observation is done in the distance d behind the double slit.

r2

r1

73

Prof. M. Schmidt

Institute of Photonic Technologies, Univ. Erlangen, Germany

Double slit (2)

Most of the time s >> a (a few thousand times)

The optical path difference

 

 

 

 

 

 

 

 

 

 

 

between

S1 P and S2 P can be approximated

with

 

 

 

 

 

 

 

 

 

S1 B

S1 P

S

or with

 

S1B r1 r2

With this approximation sin r1 r2

a

With

r1 r2

m

there is constructive interference (m = 0, 1, 2 …).

Thus

sin m

m

(At the maxima in 0 as the zeros fringe)

a

 

 

 

 

74

Prof. M. Schmidt

Institute of Photonic Technologies, Univ. Erlangen, Germany

Double slit (3)

 

 

 

y

 

 

 

 

 

 

m

Furthermore: tan

 

Therefore:

y

m

s tan arcsin

 

 

 

 

 

 

 

s

 

 

 

a

 

 

 

 

 

m

 

 

 

 

 

For small angles:

ym s

 

 

 

 

 

 

 

a

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

Distance between two fringes:

ym 1 ym as m 1 as m

Or: y as

Conclusion: Width and distance of the fringes are a function of the wavelength

(red fringes are wider than blue)

source: http://www.tf.uni-kiel.de, 09.12.2008

75

Prof. M. Schmidt

Institute of Photonic Technologies, Univ. Erlangen, Germany

Comparison of interference patters of diffrent apertures

1 slit

2 slits

3 slits

4 slits

5 slits

source: Hecht, E. „Optik“

76

Prof. M. Schmidt

Institute of Photonic Technologies, Univ. Erlangen, Germany

Grating

Gratings are regular arrangements of diffraction elements. They are grouped as followed:

Transmissions-

Transmissions-

Reflection-phase

Amplitude grating

phase-grating

grating

Multiple slits

Incised glass

Incised mirror

77

Prof. M. Schmidt

Institute of Photonic Technologies, Univ. Erlangen, Germany

Transmission-Amplitude-grating

Calculation is the same as for the double slit:

sin m m a

But: The maxima have a higher contrast.

Maximal order:

mmax a

Gratings are described with the line density [1/mm] grating constant (= line distance) in [µm]

78

Prof. M. Schmidt

Institute of Photonic Technologies, Univ. Erlangen, Germany

Blazed grating

With a normal grating most of the energy is diffracted in the zeros' order.

A blazed grating is a reflection grating, which is optimised to diffract a certain wavelength best.

The reflection which has the most energy is shifted to higher orders.

For the angle :

12 arcsin m a

Blazed gratings are used for making a beam monochromatic in spectrometer

79

Prof. M. Schmidt

Institute of Photonic Technologies, Univ. Erlangen, Germany

Questions

1.Which parameters describe a harmonic wave?

2.How big the phase difference has to be, so that the intensity doubles (f1 = f2, A1 = A2)?

3.What is the maximal shift you can measure with a Michelson-Interferometer?

4.What is the connection between speed of light and refractive index?

5.Which methods are suited to measure the wavelength of a laser?

6.How does the diffraction pattern look after an obstacle?

80

Prof. M. Schmidt

Institute of Photonic Technologies, Univ. Erlangen, Germany