lecture 3 the born-oppenheimer approximation · 2012. 6. 21. · born-oppenheimer (or adiabatic)...
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Lecture 3
The Born-Oppenheimer approximation
Learning outcomes
• Separate molecular Hamiltonians to electronic and nuclear partsaccording to the Born-Oppenheimer approximation
• Be able to manipulate expressions involving electronic wavefunctions,taking into account spin and space coordinates and antisymmetry
C.-K. Skylaris
CHEM3023 Spins, Atoms and Molecules
CHEM3023: Spins, Atoms and Molecules
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Separating electronic from nuclear coordinates
Nuclei are much heavier than electrons (e.g. Proton mass1800 times the massof an electron => compare kinetic energy operators of proton and electron).
As a result nuclei move much slower than electrons. To a very goodapproximation, we can assume that the electronic motions are instantaneously“equilibrated” at each nuclear position.
Example: Vibration of diatomic molecule:
Wrong picture: “electron cloud”trails behind moving nuclei
Correct picture: “electron cloud” instantaneously re-arranges itself around moving nuclei
electrons
Atomic nucleus
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Hamiltonian operator for water moleculeWater contains 10 electrons and 3 nuclei. We will use the symbols “O” for the oxygen (atomic numberZO=8) nucleus, “H1” and “H2” (atomic numbers ZH1=1 and ZH2=1) for the hydrogen nuclei.
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Kinetic energy of O
Kinetic energy of H1
Kinetic energy of H2
Kinetic energy of electron i
Electron attraction to O
Electron attraction to H1
Electron attraction to H2
Electron-electron repulsion
nucleus-nucleus repulsion
E.g. AssumeZ1 =ZO
Z2=ZH1
Z3=ZH2
![Page 4: Lecture 3 The Born-Oppenheimer approximation · 2012. 6. 21. · Born-Oppenheimer (or adiabatic) approximation CHEM3023 Spins, Atoms and Molecules 6. Potential Energy Surface (PES)](https://reader033.vdocuments.site/reader033/viewer/2022060915/60a89a934f3dcd360325d9e6/html5/thumbnails/4.jpg)
Hamiltonian operator for water moleculeWater contains 10 electrons and 3 nuclei. We will use the symbols “O” for the oxygen (atomic numberZO=8) nucleus, “H1” and “H2” (atomic numbers ZH1=1 and ZH2=1) for the hydrogen nuclei.
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Kinetic energy of O
Kinetic energy of H1
Kinetic energy of H2
Kinetic energy of electron i
Electron attraction to O
Electron attraction to H1
Electron attraction to H2
Electron-electron repulsion
nucleus-nucleus repulsion
E.g. AssumeZ1 =ZO
Z2=ZH1
Z3=ZH2
B.O.B.O.B.O.
CHEM3023 Spins, Atoms and Molecules
B.O.
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Example: Nuclear attraction potential for one O and two H
H2O OH + H
O + H2
• How does the Hamiltonian operator differ between these examples?
• Can you suggest how you may model the reaction OH+H H2O
CHEM3023 Spins, Atoms and Molecules
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The resulting wavefunctions andenergies have a parametric dependencein the coordinates of the nuclei
• Central to Chemistry: allows to find reactants, products, transition states,reaction paths
• We will use the Born-Oppenheimer approximation throughout this course
Solve Schrödinger's equation only in the electronic coordinates for each set ofgiven (fixed) nuclear coordinates.
Born-Oppenheimer (or adiabatic) approximation
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Potential Energy Surface (PES)
The electronic energy is a function of the nuclear positions. So is theinternuclear repulsion energy. Their sum is the “total energy” of a moleculeunder the B.O. approximation. One can represent this as a surface, which iscalled the potential energy surface (PES).
Repulsion energy between nuclei I and J
Electronic energyExample: PES of a diatomic
d
Equilibrium geometry de
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Reactants, products, transition states, reaction paths
Chemical reactions can be represented as paths followed on a PES
• Reactants and products areminimum energy points onthe PES
• Transition states are pointson the PES where theenergy is maximum alongone direction and minimumalong all other directions
• We can locate reactants, products and transition states by following pathson the PES until a minimum (or maximum in one direction for TS) is reached(zero partial derivative of energy with respect to each atomic coordinate)
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Spin, antisymmetry and the Pauli principle
• Each electron has a “spin”, an intrinsic property which has the characteristicsof rotational motion, and is quantised
• Electronic spin is described by a spin angular momentum quantum numbers=½, and its z-component ms = ½ (“up” spin) or -½ (“down” spin)
• We represent the two spin states of the electron by two spin wavefunctionsa(w) and b(w) which are orthonormal:
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• Particles whose spin quantum number s is a half-integer (e.g. 1/2, 3/2,5/2, etc ) are called Fermions
• Electrons and protons are examples of Fermions
• Particles whose spin quantum number s is an integer (e.g. 1, 2, 3) arecalled Bosons. Photons are examples of Bosons
• To describe the spin of an electron we therefore include an extra “spin-coordinate”
• Therefore, an electron is described not only by the three spatialcoordinates x,y,z (=r) but also by its spin coordinate w
• We will denote these four coordinates collectively by x
Spatial and spin coordinates
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Antisymmetry of electronic wavefunctions
•Wavefunctions of Fermions change sign when the coordinates (space andspin) of any two particles are exchanged.
•This property is called antisymmetry:
•Electrons are Fermions, therefore electronic wavefunctions must beantisymmetric
•We need to include antisymmetry in all approximate wavefunctions weconstruct
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Summary / Reading assignment
• Born-Oppenheimer approximation (Cramer, page 110)
• Many-electron wavefunctions (Cramer, pages 119-122)
• Antisymmetry of electronic wavefunctions (Cramer, pages 122-126)