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4. Molecular many electron systems: electronic & nuclear movement
Hamiltonian for a polyatomic molecule treated as Coulomb system with N nuclei
(coordinates {R}) and n electrons (coordinates {ri}) :
In atomic units i.e. ~ = qe = me = 1
Kinetic energy operator for nuclei
Kinetic energy operator for electrons
Nuclei-electron interaction operator
Electron-electron interaction operator
Nuclei-nuclei interaction operator
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IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
(3N + 3n)-dimensional problem:
Born-Oppenheimer Approximation: separate treatment of electronic and nuclear
motion allows the total wavefunction of a molecule to be broken into its electronic
and nuclear
components:
Does not depend on {ri} =
constant for given nuclear
geometry
Decomposition of Hamiltonian:
= adiabatic potential energy surfaces
Schrödinger equation for complete problem:
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IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
Multiplication with
and integration over electron coordinates
Schrödinger equation for nuclear motion:
C describe coupling between nuclear and electron motion thus the resulting
coupling of electronic states (non-adiabatic coupling)
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IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
Born-Oppenheimer approx. neglects coupling between nuclear and electron motion
C = 0
Electrons adjust immediately or adiabatically to any nuclear motion:
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displays the potential for nuclear motion
Born-Oppenheimer:
nuclear motion is described on adiabatic potential energy surfaces
IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
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IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
Atmomic Orbitals:
main quantum number (n)
1s
2s
orbital quantum
number (l=s,p,d,f)
2p
http://en.wikipedia.org/wiki/Atomic_orbital
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IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
Atomic Orbitals:
m= -l ... l
Energy
sequence:
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http://en.wikipedia.org/wiki/Atomic_orbital
IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
Bond types (orbital symmetry):
Orbitals:
2 x 2p = pp-p
Bonds:
plane of symmetry
Free Pairs: n
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http://en.wikipedia.org/wiki/Pi_bond
IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
Binding orbitals to explain the structure of molecules:
Hybridization (Valence Bond Theory)
useful for molecules with C, N, O, (S, P)
limits noticeable for d-orbitals involved in binding
Carbon Ground state: 1s2 2s2 2px1 2py1
Carbon usually binds 4 hydrogen (Methane). Why?:
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http://en.wikipedia.org/wiki/Hybrid_orbital
IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
Influence of the Hydrogen:
linear mix of s and p: sp3 hybrid orbitals
sp3 orbital binding with 1s:
s - Bond
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http://en.wikipedia.org/wiki/Hybrid_orbital
IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
C – C double Bonds (Ethene):
p - Bond
s - Bond
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http://en.wikipedia.org/wiki/Hybrid_orbital
IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
C – C double Bonds (Ethene), sp2:
s - Bond
p - Bond
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http://en.wikipedia.org/wiki/Double_bond
IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
Molecular orbital or electronic configuration (z.B. Formaldehyd)
Energetic order of transitions:
p* ← n < p* ← p < s* ← n < p* ← s < s* ← s
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IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
spin multiplicity
LUMO
HOMO
• Total spin quantum number S = ∑ si
with si = +½ or - ½
• Multiplicity M = 2S + 1
• M = 1: Singulet
• M = 2: Dublet
• M = 3: Triplet
Triplet T1: usually lower energy than S1
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4. Molecular many electron systems: electronic & nuclear movement
Molecular
orbital
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Electronic
configuration
Electronic
states
UV/Vis-absorption spectrum
IPC Friedrich-Schiller-Universität Jena
4. Molecular many electron systems: electronic & nuclear movement
Jablonski-Scheme
Excitation [10-15 s]
v=1
Rotational levels
J=4
v=0
Microwavespectroscopy
J=3
J=2
J=1
J=0
UV-VIS-spectroscopy
S4
S3
Internal conversion
[10-14 s]
Tn
S2
IR- & NIRspectroscopy
Intersystem crossing
v=4
v=3
Vibrational levels
S1
T1
Fluorescence Phosphorescence
[10-9 s]
[10-3 s]
v=1
v=0
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S0
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5. UV-Vis-Absorption
5.1 Franck-Condon principle
Interpret electronic absorption spectra based on
||2 of the vibrational levels
electronic transitions (~10-16s)
are much faster than the vibrational
period (~10-13s)
of a given molecule
thus nuclear coordinates do not
change during transition
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IPC Friedrich-Schiller-Universität Jena
5. UV-Vis-Absorption
5.1 Franck-Condon principle
Transition dipole moment for a transition between the states |i and |f:
For excitation
follows:
B.O.-approximation
Electronic transition dipole moment
is developed in a rapidly converging Taylor
expansion about nuclear displacements from the equilibrium position
Condon approximation neglects higher order terms i.e. electronic transition dipole
moment
is assumed to be constant i.e. nuclear coordinates correspond to
equilibrium geometry
Condon approximation:
Transition dipole moment:
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IPC Friedrich-Schiller-Universität Jena
5. UV-Vis-Absorption
5.2 Franck-Condon principle
= degree of redistribution of electron density during transition
= degree of similarity of nuclear configuration between vibrational
wavefunctions of initial and final states.
Intensity of a vibronic transition is direct proportional to the square modulus of the
overlap integral between vibrational wavefunctions of the two electronic states =
Franck-Condon-Factor:
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IPC Friedrich-Schiller-Universität Jena
5. UV-Vis-Absorption
5.1 Franck-Condon principle
|f
|f
|i
|i
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