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Techniques to find approximate solutions to the Schrodinger equation 1. The perturbation theory 2. The variational principle 3. The WKB approximation
21

WKB approx.ppt

Nov 08, 2014

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Page 1: WKB approx.ppt

Techniques to find approximate solutions

to the Schrodinger equation

1. The perturbation theory

2. The variational principle

3. The WKB approximation

Page 2: WKB approx.ppt

The WKB approximationWentzel- Kramers - Brillouin

Hendrik Kramers

Dutch1894- 1952

Leon Brillouin

French1889- 1969

GregorWentzel

German1898- 1978

Page 3: WKB approx.ppt

The WKB approximation

The WKB approximation is based on the idea thatfor any given potential, the particle can be locally

seen as a free particle with a sinusoidal wave function,but whose wavelength varies very slowly in space.

ikxx Ae

Page 4: WKB approx.ppt

The free particle

ikxx Ae

Infinite space

sinx A kx

2mEk

2p mE

Finite box

Page 5: WKB approx.ppt

Flat potential

ikxx Ae 2m E V

k

xx Ae

Scattering state E V

Bound state E V 2m V E

E

V

Page 6: WKB approx.ppt

Varying potentialThe WKB approximation

V(x)

E

Classical region (E>V)

Turning points

Page 7: WKB approx.ppt

The WKB approximation

V(x)

E

Classical region (E>V)

Locally constantor varying very slowly

In respect to wavelength

Page 8: WKB approx.ppt

The WKB approximationClassical region

2 2

22

dV x E

m dx

2 2

2 2

d p

dx

2p x m E V x with

Page 9: WKB approx.ppt

The WKB approximationClassical region

solution i xx A x e

2

2

2" '

pA x A x

2 'A x x cste

real part

imaginary part

Page 10: WKB approx.ppt

The WKB approximationClassical region

solution i xx A x e

( )

CA x

p x

p xd

dx

2"

'A x

A xassumption

2

2

p

and

Page 11: WKB approx.ppt

The WKB approximationClassical region

solution i xx A x e

( )

( )

ip x dxC

x ep x

where

2p x m E V x

22

( )C

xp x

Incidentally

Page 12: WKB approx.ppt

Quiz 17a

In the WKB approximation,what can we say about the solution

for the wave function ?

A. The amplitude and the wavelength are fixed

B. The amplitude is fixed but the wavelength varies

C. The wavelength varies but the amplitude is fixed

D. Both the wavelength and the amplitude vary

E. There are multiple wavelengths for a given position

Page 13: WKB approx.ppt

The WKB approximationClassical region

solution i xx A x e

0

( ') '

( )

xip x dxC

x ep x

Phase is a function of x

Page 14: WKB approx.ppt

The WKB approximationClassical region

/if xx e

Another way to write the solution:

where f(x) is a complex function

Develop the function as power of f x

Page 15: WKB approx.ppt

The WKB approximationClassical region

1( ') 'x p x dx

1( ') '

b

a

b a p x dx

When the phase is known at specific points:

Gives informationon the allowed

energies

i xx A x e

Page 16: WKB approx.ppt

Quiz 17b

A. For any type of potential and any energy value

B. Only when

C. Only when

D. Only when the potential exhibits 1 turning point

E. Only when the potential exhibits 2 turning points

In which situation can we apply the formula

? 1( ') '

b

a

b a p x dx

E V x E V x

Page 17: WKB approx.ppt

Example

Infinite Square well

sinx A x x

2p mE

The WKB approximationClassical region

0 0 a n

0

1' '

a

a p x dx n

Page 18: WKB approx.ppt

2p m E V x

The WKB approximationClassical region

0 0 a n

0

1' '

a

a p x dx n 0V

Page 19: WKB approx.ppt

The WKB approximationat turning points

V(x)

E

Classical region (E>V)

Turning points

E V x 0p x

Page 20: WKB approx.ppt

The WKB approximationat turning points

V(x)

E

Classical region (E>V)

1x 2x

2

1

1( )

2

x

x

p x dx n

Connection formula (eq 8.51)

Page 21: WKB approx.ppt

The WKB approximationat turning points

2

1

1( )

2

x

x

p x dx n

Pb 8.7

Harmonic Oscillator

Pb 8.14

Hydrogenatom

2 21

2V x m x

2 2

20

1 ( 1)

4 2eff

e l lV r

r m r