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Albert Einstein (1879-1955)

“ Imagination is more

important than knowledge.

For knowledge is limited to all we now know and understand, while imagination embraces the entire world, and all there ever will be to know and

understand. ”

Einstein

Einstein

(2)

Stimulated Emission Stimulated Emission

( ) ( )

i ij j ji ji

N B u ν = N ⎡ ⎣ A + B u ν ⎤ ⎦

At equilibrium

(3)

Stimulated Emission Stimulated Emission

( ) / /

3 3

/

( ) ( )

( ) /

1

8 /

( )

1

j i B B

B

i ij j ji ji

ji ji

i ij

j ji

E E k T h k T

i j

ij h k T

ji

N B u N A B u A B

u N B

N B

N e e

N

h c

u B

B e

ν

ν

ν ν

ν

ν π ν

⎡ ⎤

= ⎣ + ⎦

= ⎛ ⎞⎛ ⎞

⎜ ⎟⎜ ⎟ −

⎜ ⎟⎜ ⎟

⎝ ⎠⎝ ⎠

= =

= ⎛ ⎞

⎜ ⎟ −

⎜ ⎟

⎝ ⎠

Boltzmann factors

Planck’s distribution

(4)

Emission’s A, B Coefficients Emission’s A, B Coefficients

3 3

8

ij ji

ji ji

B B B

A A h B

c π ν

= ≡

≡ =

Stimulated emission should exist!

(5)

( )

0

0

3 3

internal energy of 1kilomole of soild : Avogadro's number

3 3

B

V

V

V

E N k T RT

N c dE

dT d RT

c R

dT

= =

⎛ ⎞

= ⎜ ⎟

⎝ ⎠

= =

Specific Heat of Solids Specific Heat of Solids

Dulong-Petit law

(6)

( )

/

0

2 /

/ 2

1 3

3

1

B

B

B

h k T

h k T

V h k T

V B

h e

E N

dE h e

c R

dT k T e

ν

ν ν

ε ν

ε

ν

= −

=

⎛ ⎞

⎛ ⎞

= ⎜ ⎟ = ⎜ ⎟

⎝ ⎠ ⎝ ⎠ −

Einstein’s Theory of Specific Heat of Solids

Einstein’s Theory of Specific Heat of Solids

(7)

Coupled harmonic oscillators

Debye’s Theory of Specific Heat of Solids Debye’s Theory of Specific Heat of Solids

Phonons

(8)

Fermi-Dirac Distribution

Fermi-Dirac Distribution

(9)

( )

( )

3/ 2 3

/

0 0 /

( )

8 2

( ) 1

( ) 1

F B

F B

E E k T

E E k T

g E dE D EdE D m

h

D EdE n E dE

e

N EdE

n E dE D

V e

π

∞ ∞

=

=

= +

= =

∫ ∫ +

Density of States in 3D Structure (Metal)

Density of States in 3D Structure (Metal)

(10)

3/ 2 0

2 / 3 2

At 0

2 3 (0) 3

2 8

E

F

F

F

T K

N D EdE DE V

h N

E m π V

=

= =

⎛ ⎞

= ⎜ ⎝ ⎟ ⎠

Fermi Energy in Metal

Fermi Energy in Metal

(11)

9.2

페르미 에너지

eV

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