siena, settembre 2005 (i) 1 theory of electron transport in semiconductor materials and structures...

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Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on Nano-Structures and Bio-Systems Laboratory S3 Università di Modena e Reggio Emilia, Italy Tel. 059-205.5278 [email protected] I

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Page 1: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 1

Theory of electron transportin semiconductor materials and structures

Carlo Jacoboni

INFM-CNR National Research Center on Nano-Structures and Bio-Systems Laboratory S3

Università di Modena e Reggio Emilia, Italy

Tel. [email protected]

I

Page 2: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 2

CONTENTS1. Un po’ di storia2. Le origini della meccanica quantistica3. La fisica quantistica ed effetti quantistici4. Cristalli, stati di Bloch, bande di energia5. Dinamica pseudo-classica6. Metalli, isolanti e semiconduttori.7. Semiconduttori intrinseci ed estrinseci. Statistica degli elettroni

nei semiconduttori8. Modello semplice del trasporto in semiconduttori9. Funzione di distribuzione ed equazione di Boltzmann10. Scattering elettronici11. Strutture a semiconduttore – Giunzioni, diodi e mosfet12. Quantum wells, wires, dots e super-reticoli 13. Strutture mesoscopiche (Landauer)

Page 3: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 3

Some history Some history

1630 – Galileo, Dialogo sopra i due massimi sistemi del mondo1638 – Galileo, Discorsi e dimostrazioni matematiche intorno a due nuove scienze1687 – Newton, Principia1788 – Lagrange equations 1792 – Wedgwood: all bodies in the oven become incandescent at the same temp.1814 – Fraunhofer discovers the black lines in the solar spectrum1843 – Hamilton equations1855 – Maxwell equations1859 – Kirchhoff explains the black lines in the solar sp. and founds spectroscopy1879 – Stefan law: Etot=T4

1887 – Hertz confirms experimentally the propagation of the e.m. waves1887 – Michelson-Moreley experiment1896 – Mme Curie discovers radioactivity1897 – Thomson discovers the electron (cathodic rays)1900 – Reilaigh-Jeans law1900 – Planck law, photon quantization

Page 4: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 4

Some Some history (2)history (2)1902 – Measurements of the photoelectric effect – Lénard

1905 – Golden year of Einstein1911 – Rutherford experimets1912 – X-ray diffraction from crystals (von Laue)1913 – Bohr atom1916 – Bohr-Sommerfeld quantization conditions1923 – de Broglie hypothesis1926 – Schroediger and Heisenberg equations1927 – Electron diffraction from crystals – Davisson e Germer (1925)1928 – Dirac equation

Page 5: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 5

Luce: onde Luce: onde elettromagnetiche o elettromagnetiche o fotoni ?fotoni ?

Radiazione termica

Effetto fotoelettrico

Interferenza

Plack:

Einstein:

// hkcp

Page 6: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 6

Interference

Page 7: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 7

Luce: onde Luce: onde elettromagnetiche o elettromagnetiche o fotoni ?fotoni ?

Radiazione termica

Effetto fotoelettrico

Interferenza a singolo fotone

Page 8: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 8

Single-photon Single-photon interferenceinterference

Page 9: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 9

Atomo di Bohr: perché Atomo di Bohr: perché non collassa ?non collassa ?

nL

Page 10: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 10

Electrons: Electrons: particles or particles or waves ?waves ?

rn 2

/hp

nL Bohr!!

Page 11: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 11

Electron Electron interferenceinterference

Electrons are in superposition of states. The measurement …Theory predicts PROBABILITY

I

Page 12: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 12

Schroedinger equationSchroedinger equationE= ; p = k

(x,t) = A ei(kx-t)

For given energy and momentum: plane wave

Dx2(x) = -k2 (x)

Dt(x) = -i (x) m

k

m

p

22

222

Schroedinger equation

2

22

2 xmti

V

Page 13: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 13

Schroedinger equation-Forma operatorialeSchroedinger equation-Forma operatoriale

Vxmt

i2

22

2

A f = g ; (AB) f = A (B f) ; (A+B) f = Af+ (B f)

Vm

pH

mm

p

pip

222

2222

222

Ht

i

Page 14: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 14

Time-independent Schroedinger equationTime-independent Schroedinger equation

H

Hii

er

Ht

i

ti

)(

Page 15: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 15

Wave Wave packetspackets

(x,t) = A(k) ei(kx-t) dk

v

x p ½

Page 16: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 16

Energy eigenstates Energy eigenstates States with well defined energyStates with well defined energy

Ground state

First excited state

Second excited state

Infinitepotentialwell

Page 17: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 17

Energy eigenstates Energy eigenstates States with well defined energyStates with well defined energy

Localized state

Extended state

Finitepotentialwell

Resonant state

Page 18: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 18

Quantum effects: Total reflectionQuantum effects: Total reflection

V(x)

v

v

Vo

< Vo

Page 19: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 19

Quantum effects: Quantum effects: Partial reflectionPartial reflection

V(x)

v

v

> Vo

v

Page 20: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 20

Quantum effects: Quantum effects: TunnelTunnel

V(x)

v

v

<Vo

v

Page 21: Siena, settembre 2005 (I) 1 Theory of electron transport in semiconductor materials and structures Carlo Jacoboni INFM-CNR National Research Center on

Siena, settembre 2005 (I) 21

Pauli exclusion Pauli exclusion principleprinciple

Coulomb potential well Periodic table

Identical particles

Electron spin 1/2

Atoms