Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

14
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel

Transcript of Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

Page 1: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

Physics 452

Quantum mechanics II

Winter 2012

Karine Chesnel

Page 2: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

Homework

Phys 452

Wed Feb 16: assignment # 10Pb 7.8, 7.9, 7.13, 7.17

Friday Feb 18: assignment # 118.1, 8.2, 8.7, 8.14

Announcements

Monday: Holiday

Next class: Tuesday at 1pm

Page 3: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

H atom

Hydrogen molecule ion H2+

Phys 452

H atom

electron

1r

2r

R

Page 4: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

Hydrogen molecule ion H2+

Phys 452

electron

1r

2r

R

2 2

0 1 2

1 1

2 4

p eH

m r r

Step 1: Hamiltonian

Step 2: trial wave function 0 1 0 2A r r

Overlap integral: 0 1 0 2r r

Normalization: 1/2

2/1 1

1 132

R a R RA e

a a

Page 5: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

0 1r

R

0 2r

Hydrogen molecule ion H2+

Phys 452

0 1 0 2A r r

Use the trial wave function:

2 2

0 1 0 20 1 2

1 1

2 4

p eH A r r

m r r

2 22 2 2 2

0 1 0 2 0 1 0 20 1 0 2 0 2 0 1

1 1 1 1

2 4 2 4 4 4

p pe e e eH A r r r r

m r m r r r

Hydrogen Hamiltonianwith first nucleus

Hydrogen Hamiltonianwith second nucleus

Cross terms

Step 3: expectation value of H

Page 6: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

0 1r

R

0 2r

Hydrogen molecule ion H2+Phys 452

2

1 0 1 0 20 2 1

1 1

4n

eH E A r r

r r

2

2

1 0 1 0 1 0 2 0 2 0 1 0 2 0 2 0 10 2 1 1 2

1 1 1 1

4n

eH H E A r r r r r r r r

r r r r

2

2

1 0 1 0 1 0 1 0 20 2 1

1 12

4n

eH H E A r r r r

r r

Direct integral D exchange integral X

Pb. 7.8

Eigenstates of Individual hydrogen atoms

00 1 0nH E

Page 7: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

0 1r

R

0 2r

Hydrogen molecule ion H2+

Phys 452

11 2

1

D XH E

I

where

2/ 1

13

R a R RI e

a a

2 /1 R aa aD e

R R

/1 R aaX e

R

directintegral

exchangeintegral

Finally…!

Page 8: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

0 1r

R

0 2r Hydrogen molecule ion H2

+Phys 452

1 1

21 2

1

D X aH E E

I R

Step 4: Minimization

First include the proton-proton interaction !

2

0

1

4pp

eV

R

2 2

21

1 (2 / 3) 121

1 1 1/ 3

x x

x

x e x eHF x

E x x x e

wherex = R/a

Page 9: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

0 1r

R

0 2r Hydrogen molecule ion H2

+Phys 452

Step 4: Minimization

Rx

a

1

H

E

Presence of a minimum:Evidence of bonding

Equilibrium separation distance:

2.4 1.3eqR a

Page 10: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

Quiz 15

Phys 452

The binding energy for the hydrogen molecule ion H2+

is experimentally found to be 2.8eV.What can we predict about the binding energy E

estimated with the variational principle?

A. E > 2.8 eV

B. E < 2.8 eV

C. E = 2.8 eV

D. Can be any value

E. Can not tell

Page 11: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

0 1r

R

0 2r

Hydrogen molecule ion H2+

Phys 452

Pb 7.8

Calculation of

Direct integral 0 1 0 12

1D r r

r

0 1 0 21

1X r r

r

Exchange integral

Page 12: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

0 1r

R

0 2r Hydrogen molecule ion H2

+Phys 452

Pb 7.9

Rx

a

1

H

E

Presence of a minimum:Evidence of bonding

For symmetrical state

0 1 0 2A r r

What about antisymmetrical state?

0 1 0 2A r r

Page 13: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

0 r Hydrogen atom H

Phys 452

Pb 7.13

Another trial wave function

2brr Ae

Hamiltonian 2

2

pH V r

m

Calculate H …and minimize it

use spherical coordinates

Page 14: Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

0 2r Helium - like systemPhys 452

Pb 7.17

“Rubber – band” model for He

0 1r

2 2

22 2 2 21 21 2 1 2

1

2 2 2 4

p pH m r r m r r

m m

a) Change of variable

b) Exact solution (harmonic oscillators)

c) Evaluate with ground state of 3D HO 0 0H 0