16. dielectrics / metals

28
Institute of Solid State Physics Technische Universität Graz 16. Dielectrics / Metals Nov. 26, 2018

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Page 1: 16. Dielectrics / Metals

Institute of Solid State PhysicsTechnische Universität Graz

16. Dielectrics/ Metals

Nov. 26, 2018

Page 2: 16. Dielectrics / Metals

Dielectrics

Dielectrics used as electrical insulators should not conduct.

Large breakdown field.

Low AC losses.

Sometimes a low dielectric constant is desired (CMOS interconnects)

Sometimes a high dielectric constant is desired (supercapacitors).

Page 3: 16. Dielectrics / Metals

Breakdown field

Typically 105-106 V/cm

Page 4: 16. Dielectrics / Metals

AC losses - loss tangent

In an ideal capacitor, current leads voltage by 90o.

21 0 tan2V

Because the dielectric constant is complex, in real materials current leads voltage by 90o - .

Power loss =

Becomes more of an issue at high frequencies (microwaves)

0 0

Page 5: 16. Dielectrics / Metals

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Loss tangent

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Polarizability

• Orientation polarizability• Space charge polarizability

• Ionic polarizability• Electronic polarizability

Overdamped modes

Underdamped modes

Page 7: 16. Dielectrics / Metals

Orientation (dipolar) Polarizability

For materials (gases, liquids, solids) with a permanent dipole moment.

The theory is very similar to paramagnetism.

1T

Curie law

Page 8: 16. Dielectrics / Metals

Orientation Polarizability

Ion jumps.

doubly ionized

Page 9: 16. Dielectrics / Metals

Schematic dielectric function of water from Wikipedia

Water

Source: Classical Electrodynamics,J.D. Jackson

Page 10: 16. Dielectrics / Metals

Ionic Polarizability

Displacement of ions of opposite sign. Only in ionic substances.

This is an underdamped mode in the infrared.

Page 11: 16. Dielectrics / Metals

Electronic polarizability (all materials)

P Np N E

density

dipole moments

polarizability

Page 12: 16. Dielectrics / Metals

Polarizability

Kittel

Page 13: 16. Dielectrics / Metals

Inter- and intraband transitions

( ) ( )c vE k E k

When the bands are parallel, there is a peak in the absorption (")

Optical spectroscopy has developed into the most important experimental tool for band structure determination. - Kittel

Page 14: 16. Dielectrics / Metals

Ashcroft and Mermin

Page 15: 16. Dielectrics / Metals

Dielectric function of BaTiO3

Page 16: 16. Dielectrics / Metals

Dielectric function of silicon

absorption

extinction K

refractive index n

( ) ( ) ( )n iK

4 fKc

Page 17: 16. Dielectrics / Metals

AC Conductivity

For constant voltage, conductors conduct and insulators don't.

For low ac voltages in a conductor, electric field and the electron velocity are in-phase, electric field and electron position are out-of-phase.

For low ac voltages in an insulator, electric field and the electron position are in-phase, electric field and electron velocity are out-of-phase.

At high (optical) frequencies the in-phase and out-of-phase component of the response is described by the dielectric function.

Page 18: 16. Dielectrics / Metals

Conductivity / Dielectric function

0 0

P nexE E

0

1 1i

j nev i nexE E E

0i

v i x

Below about 100 GHz the frequency dependent conductivity is normally used.Above about 100 GHz the dielectric function is used (optical experiments).

, , i t i t i tv v e x x e E E e Harmonic dependence

Page 19: 16. Dielectrics / Metals

Diffusive transport (low frequencies)

sc

dvF ma eE m

scd

e E vm

e dE v

scme

2nenem

Page 20: 16. Dielectrics / Metals

Diffusive metal

n nm mj E

The current is related to the electric field

( ) ( ) ( )dv t ev tm eE tdt

The differential equation that describes how the velocity changes in time is:

n nm mv E

The impulse response function :

1( ) exp 0etg t tm m

Inertial term

Steady state solution

Page 21: 16. Dielectrics / Metals

Diffusive metal

( ) ( ) ( )dv t ev tm eE tdt

Assume a harmonic solution E()eit, v()eit

The differential equation is:

1 ( ) ( )i m v Ee

1

12 2

11 11

v ii m iE e

2 2

11

j v ine neE E

low ne 2

high inem

me Scattering time

Page 22: 16. Dielectrics / Metals

Diffusive metal

2 2

0 0

11

ne ii i

2 20

1 11

ne i

2

23 21 pi

Take the limit as goes to infinity

2

21 p

0 for 0 for 0

22

0p

nem

Page 23: 16. Dielectrics / Metals

low frequency metal / high frequency insulator

Ibach & Lueth

Aluminum

Conducting transparent contacts for LEDs and Solar cells

Windows that reflect infrared

Reflection of radio waves from ionosphere

22

0p

nem

ITO

Page 24: 16. Dielectrics / Metals

http://lamp.tu-graz.ac.at/~hadley/ss2/linearresponse/dmetal.php

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Ellipsometry

1 1 2 2sin sinn n

Page 27: 16. Dielectrics / Metals

Ellipsometry

Ellipsometry measures the change of polarization upon reflection. The measured signal depends on the thickness and the dielectric constant.

http://en.wikipedia.org/wiki/Ellipsometry

Page 28: 16. Dielectrics / Metals

Ellipsometry

The ratio of the two reflected polarizations is insensitive to instabilities of light source or atmospheric absorption.