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Www.soran.edu.iq 1. 2 Example: Diamond in air What is the critical angle c for light passing from diamond (n 1 = 2.41) into air (n 2 = 1)? Rearranging.

Dec 17, 2015

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Page 1: Www.soran.edu.iq 1. 2 Example: Diamond in air What is the critical angle  c for light passing from diamond (n 1 = 2.41) into air (n 2 = 1)? Rearranging.

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Example: Diamond in air• What is the critical angle c for light passing from diamond (n1 =

2.41) into air (n2 = 1)?

n1

n2

sin 2

sin1

Rearranging the equation

• Solution: At the critical angle,

1 c

2 90and

sin1 sinc n2

n1

sin(90 ) n2

n1

Substitution gives

sinc 1

2.41c 24.5

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• Incident light is reflected, absorbed, scattered, and/or transmitted:

I0 IT IA IR IS

Light Interactions with Solids

• Optical classification of materials:

Adapted from Fig. 21.10, Callister 6e. (Fig. 21.10 is by J. Telford, with specimen preparation by P.A. Lessing.)

single crystal

polycrystalline dense

polycrystalline porous

TransparentTranslucent

Opaque

Incident: I0

Absorbed: IA

Transmitted: IT

Scattered: IS

Reflected: IR

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• Absorption of photons by electron transitions:

• Unfilled electron states are adjacent to filled states• Near-surface electrons absorb visible light.

Adapted from Fig. 21.4(a), Callister & Rethwisch 8e.

Optical Properties of Metals: Absorption

Energy of electron

Incident photon

Planck’s constant

(6.63 x 10-34 J/s)

freq. of incident light

filled states

unfilled states

E = h required!

of energy h

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Light Absorption

e0IIT

The amount of light absorbed by a material is calculated using Beer’s Law

= absorption coefficient, cm-1

= sample thickness, cm = incident light intensity = transmitted light intensity0I

TI

ln0I

IT

Rearranging and taking the natural log of both sides of the equation leads to

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Adapted from Fig. 21.4(b), Callister & Rethwisch 8e.

Reflection of Light for Metals• Electron transition from an excited state produces a photon.

photon emitted from metal surface

Energy of electron

filled states

unfilled states

Electron transition

IR “conducting” electron

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Reflection of Light for Metals (cont.)

• Reflectivity = IR /I0 is between 0.90 and 0.95.• Metal surfaces appear shiny• Most of absorbed light is reflected at the same

wavelength• Small fraction of light may be absorbed• Color of reflected light depends on wavelength

distribution– Example: The metals copper and gold absorb light in blue

and green => reflected light has gold color

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Reflectivity of Nonmetals• For normal incidence and light passing into a solid having

an index of refraction n:

R reflectivity n 1

n1

2

17.0141.2

141.22

R

reflectedislightof%17

• Example: For Diamond n = 2.41

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Scattering of Light in Polymers

• For highly amorphous and pore-free polymers– Little or no scattering– These materials are transparent

• Semicrystalline polymers– Different indices of refraction for amorphous and crystalline

regions– Scattering of light at boundaries– Highly crystalline polymers may be opaque

• Examples:– Polystyrene (amorphous) – clear and transparent– Low-density polyethylene milk cartons – opaque

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Absorption of light of frequency by by electron transition occurs if h > Egap

• If Egap < 1.8 eV, all light absorbed; material is opaque (e.g., Si, GaAs)

• If Egap > 3.1 eV, no light absorption; material is transparent and colorless (e.g., diamond)

Selected Light Absorption in Semiconductors

• If 1.8 eV < Egap < 3.1 eV, partial light absorption; material is colored

Adapted from Fig. 21.5(a), Callister & Rethwisch 8e.

blue light: h = 3.1 eVred light: h = 1.8 eV

incident photon energy h

Energy of electron

filled states

unfilled states

Egap

Examples of photon energies:

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Ge(min) hc

Eg (Ge)

(6.63 x 10 34 Js)(3 x 108 m/s)

(0.67 eV)(1.60 x 10 19 J/eV)

Computations of Minimum Wavelength Absorbed

Note: the presence of donor and/or acceptor states allows for light absorption at other wavelengths.

Solution:

(a) What is the minimum wavelength absorbed by Ge, for which Eg = 0.67 eV?

Ge(min) 1.86 x 10-6 m 1.86 m

(b) Redoing this computation for Si which has a band gap of 1.1 eV

Si(min) 1.13 m

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• Color determined by the distribution of wavelengths: -- transmitted light -- re-emitted light from electron transitions

• Example 1: Cadmium Sulfide (CdS), Eg = 2.4 eV -- absorbs higher energy visible light (blue, violet) -- color results from red/orange/yellow light that is transmitted

Color of Nonmetals

• Example 2: Ruby = Sapphire (Al2O3) + (0.5 to 2) at% Cr2O3

-- Sapphire is transparent and colorless (Eg > 3.1 eV) -- adding Cr2O3 : • alters the band gap • blue and orange/yellow/green light is absorbed • red light is transmitted • Result: Ruby is deep red in color

Adapted from Fig. 21.9, Callister & Rethwisch 8e. (Fig. 21.9 adapted from "The Optical Properties of Materials" by A. Javan, Scientific American, 1967.)

40

60

70

80

50

0.3 0.5 0.7 0.9

Tra

nsm

ittan

ce (

%)

ruby

sapphire

wavelength, (= c/)(m)