Applications of Quantum Mechanics -
Solid state
Shreya Prasad
, SUMMARY
→ Classical theory ? Relaxation time
2
thermal velocity
=3km Drift velocity Vd=el
/
heard
R=
F- nerd J=rE
F-
S=£
↳ Mattheis entente :
f- fiefm metal G- R
{
_ -
) (
net impurity
→
Quantum theory :
KTF E Mtr
k¥p
k=nI
=
Ep Neff net
- __
a
Tomar
probability f-④
eE-Er!lk
=
factor
available
States
n =
¥§mµa "rE
'VE
stale
density
g = Efg)ˢ
Energy density NCE )=gE ) f- (E)-
n-t%E3dtfumivdou.ly
Nooffneeé
VF=j2EmI
Effective
f%¥yE_ =§Ef
→
man
Ewg=
h-2ci-E.im?-.)--EE.:.7E-oueD
M =
lorenz
1--4--2=-1,1%5
no He Ho
4- ¥ ) ]
-
. -
?⃝
, CLASSICAL ELECTRON THEORY
→ thermal
velocity
=
21mi =
3- KI ( %)
ruax-H-mier-fskm.TT I µ conductivity
nerd
velocity Vd=eE÷ I=neAVd
→ J= E-
Drift F- r
:
classical election
considered
theory
Mobility µ=eIm ¥
→ : =
manual
Boltzmann
theory
↳ Resistivity
:
^
✓
8=10 at T -0k Residual I is present
%
.
9=9,1 Pres
(
-
5- E-
g
r ,
Residual s E
S S E-
ne¥
T→ = - =
impunity
.
g- nerd
Ym
m m
!
=
net net nets litres impurities)
§ is dueto
&
'
I Eres II
=
B-
* CEFT DRAWBACKS :
1. Temperature dependence of S :
C- Vs s)
=÷a
f =
M "
not
s=
mn֖
S m
]3kyB
=
helps
3kBh =
need
safe
But in 8×7
reality
i.
,