brillouin

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Free electron bands for fcc structure G – center of the BZ X – [100] intercept; G - X path D K – [110] intercept; G - K path S L – [111] intercept; G - L path L

description

primeira zona de brillouin

Transcript of brillouin

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Free electron bands for fcc structureG – center of the BZ

X – [100] intercept; G - X path D

K – [110] intercept; G - K path S

L – [111] intercept; G - L path L

Band structure of Al (fcc)

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Free Electron Bands

Ene

rgy

k

Ek = Ek k + G( )

1D : E =h2

2mk +

n2pa

Ê

Ë Á

ˆ

¯ ˜

2

; n = 0, ±1, ± 2 ...n=1

n=-2

n=-1

n=0

Brillouin zones - 2DBZ construction•reciprocal lattice

•bisect vectors to the nearest neighbors

•area defined by bisecting linesrepresents 1BZ

Zonas de brillouin en red cuadrada

Zonas de brillouin (red cúbica simple)

1 2 3

Zonas de brillouin (red bcc)

1 2 3

Zonas de brillouin (red fcc)

1 2 3

Zonas de Brillouin y Superficie de Fermi

* Red cuadrada* Aprox. e libres

(densidad arbitraria)

Ejemplo:

Esquema de zona extendida

Segunda zona de BrillouinEsquema de zona repetida:

Tercera zona de BrillouinEsquema de zona repetida:

Cuarta zona de BrillouinEsquema de zona repetida:

Superficie de Fermi en esquema de zona reducida

1 2 3 4

The Fermi surface ofalkali metals

kF = (3p2n)1/3,n = 2/a3

à kF = (3/4p)1/3(2p/a)GN=(2p/a)[(1/2)2+(1/2)2]1/2

\ kF = 0.877 GN

First BZ (of a bcc lattice) andthe Fermi sphere

The Fermi surface of copper (similar for Ag and Au)

Band structure

(Cu is amonovalent metalwith fcc lattice)

Fermi surface

(a cross-section)

Periodic zone scheme

The Fermi surface of Al

(Al is a trivalent metalwith fcc lattice)

Empty lattice result

Actual Fermi surface

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Distorting the Fermi Surface

2nd zone 3rd zone 3rd zone in periodic zone scheme

Distortion due to weak periodic potential

2nd zone 3rd zone

3D Fermi Surface

web page: http://www.phys.ufl.edu/fermisurface/

Na Ca Al

1 valence e- 2 valence e- 3 valence e-

Periodic Table of the Fermi Surfaces of Elemental Solids http://www.phys.ufl.edu/fermisurface

Ferromagnets:

Alternate Structures :

Tat-Sang Choy, Jeffery Naset , Selman Hershfield, and Christopher StantonPhysics Department, University of Florida

Seagate TechnologyJian Chen

Source of tight binding parameters (except for fcc Co ferromagnet): D.A. Papaconstantopoulos, Handbook of the band structure of elemental solids, Plenum 1986.This work is supported by NSF, AFOSR, Research Corporation, and a Sun Microsystems Academic Equipment Grant.

(15 March, 2000)

Co_fcc Co_fcc