schrödinger equation for hydrogen molecule ion · lecture 13: molecular structure ... schrödinger...

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PY3004 Lecture 13: Molecular structure Lecture 13: Molecular structure o Hydrogen molecule ion (H 2 + ) o Overlap and exchange integrals o Bonding/Anti-bonding orbitals o Molecular orbitals PY3004 Schrödinger equation for hydrogen molecule ion Schrödinger equation for hydrogen molecule ion o Simplest example of a chemical bond is the hydrogen molecule ion (H 2 + ) . o Consists of two protons and a single electron. o If nuclei are far from each another, electron is localised on one nucleus. Wavefunctions are then those of atomic hydrogen. r ab r b r a + + - a b o ! a is the hydrogen atom wavefunction of electron belonging to nucleus a. Must therefore satisfy and correspondingly for other wavefunction, ! b . The energies are therefore PY3004 Schrödinger equation for hydrogen molecule ion Schrödinger equation for hydrogen molecule ion o If atoms are brought into close proximity, electron localised on b will now experience and attractive Coulomb force of nucleus a. o Must therefore modify Schrödinger equation to include Coulomb potentials of both nuclei: where o To find the coefficients c a and c b , substitute into Eqn. 2: (2) PY3004 Solving the Schrödinger equation Solving the Schrödinger equation o Can simplify last equation using Eqn. 1 and the corresponding equation for H a and H b . o By writing E a 0 ! a in place of H a ! a gives o Rearranging, o As E a 0 = E b 0 by symmetry, we can set E a 0 - E = E b 0 - E = -!E, (3)

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Page 1: Schrödinger equation for hydrogen molecule ion · Lecture 13: Molecular structure ... Schrödinger equation for hydrogen molecule ion ... oSee Chapter 24 of Haken & Wolf for further

PY3004

Lecture 13: Molecular structureLecture 13: Molecular structure

o Hydrogen molecule ion (H2+)

o Overlap and exchange integrals

o Bonding/Anti-bonding orbitals

o Molecular orbitals

PY3004

Schrödinger equation for hydrogen molecule ionSchrödinger equation for hydrogen molecule ion

o Simplest example of a chemical bond is the

hydrogen molecule ion (H2+).

o Consists of two protons and a single electron.

o If nuclei are far from each another, electron is

localised on one nucleus. Wavefunctions are then

those of atomic hydrogen.

rab

rbra

++

-

ab

o !a is the hydrogen atom wavefunction of electron belonging to nucleus a. Must therefore

satisfy

and correspondingly for other wavefunction, !b. The energies are therefore

PY3004

Schrödinger equation for hydrogen molecule ionSchrödinger equation for hydrogen molecule ion

o If atoms are brought into close proximity, electron localised on b will now experience and

attractive Coulomb force of nucleus a.

o Must therefore modify Schrödinger equation to include Coulomb potentials of both nuclei:

where

o To find the coefficients ca and cb, substitute into Eqn. 2:

(2)

PY3004

Solving the Schrödinger equationSolving the Schrödinger equation

o Can simplify last equation using Eqn. 1 and the corresponding equation for Ha and Hb.

o By writing Ea0 !a in place of Ha !a gives

o Rearranging,

o As Ea0 = Eb

0 by symmetry, we can set Ea0 - E = Eb

0 - E = -!E,

(3)

Page 2: Schrödinger equation for hydrogen molecule ion · Lecture 13: Molecular structure ... Schrödinger equation for hydrogen molecule ion ... oSee Chapter 24 of Haken & Wolf for further

PY3004

Overlap andOverlap and exchange integralsexchange integrals

o !a and !b depend on position, while ca and cb do not. Now we know that for orthogonal

wavefunctions

o But !a and !b are not orthoganal, so

o If we now multiply Eqn. 3 by !b and integrate the results, we obtain

o As -e|!a|2 is the charge density of the electron => Eqn. 4 is the Coulomb interaction energy

between electron charge density and nuclear charge e of nucleus b.

o The -e!a !b in Eqn. 5 means that electron is partly in state a and partly in state b => an

exchange between states occurs. Eqn. 5 therefore called an exchange integral.

Normalisation integral

Overlap integral

(4)

(5)

PY3004

Overlap andOverlap and exchange integralsexchange integrals

o Eqn. 4 can be visualised via figure at right.

o Represents the Coulomb interaction energy of an

electron density cloud in the Coulomb field on the

nucleus.

o Eqn. 5 can be visualised via figure at right.

o Non-vanishing contributions are only possible

when the wavefunctions overlap.

o See Chapter 24 of Haken & Wolf for further

details.

PY3004

Orbital energiesOrbital energies

o If we mutiply Eqn 3 by !a and integrate we get

o Collecting terms gives,

o Similarly,

o Eqns. 6 and 7 can be solved for c1 and c2 via the matrix equation:

o Non-trivial solutions exist when determinant vanishes:

(6)

(7)

PY3004

Orbital energiesOrbital energies

o Therefore

o This has two solutions: (8)

and (9)

o From Eqn. 8,

o Substituting this into Eqn. 6 => cb = -ca = -c

o The total wavefunction is thus

o Similarly solving for !E in Eqn. 9 and substituting into Eqn. 6 => ca = cb = c, giving

Anti-bonding orbital

Bonding orbital

Page 3: Schrödinger equation for hydrogen molecule ion · Lecture 13: Molecular structure ... Schrödinger equation for hydrogen molecule ion ... oSee Chapter 24 of Haken & Wolf for further

PY3004

Bonding and anti-bonding Bonding and anti-bonding orbitalsorbitals

o If two nuclei approach each other, the

electronic energy E slits depending on whether

dealing with a bonding or an anti-bonding

wavefunction.

o For symmetric case (top right), occupation

probability for " is positive.

o Not the case for a asymmetric wavefunctions

(bottom right).

PY3004

Bonding and anti-bonding Bonding and anti-bonding orbitalsorbitals

o The energy E of the hydrogen molecular ion can finally be written

o ‘+’ correspond to anti-bonding orbital energies, ‘-’ to bonding.

o Energy curves below are plotted to show their dependence on rab

PY3004

Molecular Molecular orbitalsorbitals

PY3004

Molecular Molecular orbitalsorbitals

Page 4: Schrödinger equation for hydrogen molecule ion · Lecture 13: Molecular structure ... Schrödinger equation for hydrogen molecule ion ... oSee Chapter 24 of Haken & Wolf for further

PY3004

Molecular Molecular orbitalsorbitals

o Energies of bonding and anti-bonding

molecular orbitals for first row diatomic

molecules.

o Two electrons in H2 occupy bonding

molecular orbital, with anti-parallel spins.

If irradiated by UV light, molecule may

absorb energy and promote one electron

into its anti-bonding orbital.

PY3004

Molecular Molecular orbitalsorbitals