PESMO Flashcards
Describe the fundamental principles behind MO theory.
Each electron is describe by a one-electron spatial wavefunction, φi, know as the MO. The electron itself is indistingushable and only represents a share of the electron density.
The MOs are polycentric and stretch across many atoms. Each MO is defined by a set of quantum numbers which also define their shape and energy, εi.
Each electron has a spin of ms = ±1.
Describe how the spacial wavefunction is affected by the individual atoms with an equation and what are the requirements for the atomic orbitals to combine as such?
φ = c1χA + c2χB where χ are the atomic one-electron orbitals.
They may combine effectively if they have comparable energies, they have resonable overlap and they have the same symmetry.
Define a basis set and describe it for a 2nd row diatomic.
The basis set is a set of equations which describe the bonding orbitals of the electrons in a molecule. They generally only describe the valence orbitals that can engage in bonding so this is typically the 2p and 2s orbitals.
Describe the effects and draw diagrams showing the change in MO shape from weak to strong sp mixing of a 2nd row diatomic.
This is summerised by combinding each of the wavefunctions,
φσ = c12sA + c22sB + c32pz A + c42pz B
Outline, for the 2nd row diatomics, how sp mixing changes.
Starting from Li2 the orbitals are close in energy so there is very strong sp mixing. This decreases down to N2 which is still mixed but only closely. The next diatomic, O2, is weakly mixed so the MO energies change but the 1π is above the 3σ.
Briefly describe the photoelectric effect and the associated graph and equation.
Electrons are emitted from a metal when light is shone onto it. Photolelectrons are only released after a threshold frequency is reached and the kinetic energy of the photoelectrons increases linearly with photon frequency. This is described by hv = ½mev2 + Φ.
Describe the way that photoelectron spectroscopy was developed from the observation of the photoelectron effect.
Much higher energy light sources were developed using x-rays to ionise core electrons and deep UV rays to ionise valence electrons. The UV source was a He(I) lamp with a very specific source wavelength of 21.22 eV.
Describe generally how PES occurs and Koopmans theorem for how it can be analysed.
The electrons are ionised from the valence bands and the kinetic energies are measured. The rest of the photons energy is assumed to have been used in the ionisation of the electron from its band.
Koopmans theorem states that ‘For a closed shell molecule, the ionisation energy for an electron in a particular orbital is approximately equal to the negative of the orbtial energy.’ However this relies on the theory of one electron orbitals and neglets eletron reorganisation such as the repulsion been electrons. It also cannot be used for open shell molecules.
Why must the monochromatic light source be carefully selected.
It must have an appropriate amount of energy and have a wavelength that will propagate in air. It must also only produce light from one transition.
How is the kinetic energy of the emitted photonelectron analysed and how can it be adapted?
Using a magnetic or electric field, the photoelectron can be curved around a path between hemispherical plates where the number of photoelectrons that have the correct kinetic energy can be detected. A small range of energies being detected at once is desireable.
The resolution, the range of energies, can be determined by ES/2R where E is the kinetic energy, R is the radius of the path and S is the slit width at the start and end of the path.
Describe the origin and meaning of the vibrational structure produced when an ionisation takes place.
Assuming the Born-Oppenheimer approximation, the electron movement will be much faster than nuclei movement. Hence the molecular structure will electronically and structurally reorganise after the transition.
If the electron is removed from a non-bonding orbital, the bond length will be the same in both species and a sharp peak will be seen for the transition to the v = 0 level in the product as this will have the greatest overlap with the ground species.
If the electron is removed from a bonding orbital, the bond is weakened, and will vibrate outwards since the best overlap is with upper vibration states of the cation produced. Hence a vibrational progression is seen in the spectra.
If the electron is removed from an anti-bonding orbital, the bond is strengthened and the progession will be shorter as the potential energy curve for the cation will be narrower.
For F2, weak sp mixing, describe the change in bond length and the progressions for each of the MO ionisations.
- π* orbital - bond is shortened as the bonding energy increases. Short progression with middle peak highest as PE curve narrows.
- π orbital - bond is lengthened as the bonding energy decreases. Long progression.
- σ orbital - bond is even more lengthened as the bonding energy is more significantly reduced. Long progression.
The intensity of the bands decreases the deeper they are.
What does the Λ symbol represent and how can it cause complications to the spectra?
Λ represents the quantum number l (angular momentum) associated with the symmetry of the species produced. Π labelled species have a value of 1 and Σ labelled species have a value of 0.
This can the couple to the electron spin, called spin orbit coupling and they add together to give the total angular momentum of the species. Ω = |Λ| + Ms. For Π this gives states of 3/2 and 1/2 where the higher value is lower energy.
This causes 2 peaks to form at each vibrational level and the effect increases with z4. For I2, there is 2 distinct, seperate bands.
Describe the PES spectrum and the change in bond length associated with N2.
The orbital ordering of N2 is sp mixed and the occupancy is up to 3σ.
- 3σ (sp mixed to weakly bonding) - small increase in bond length. Short progression.
- 1π bonding orbital - strongly bonding so large increase in bond length with long progression.
- 2σ* slightly anti-bonding - small decrease in bond length, short vibrational structure.
Describe the complexities in the PES spectrum of O2.
The state where both unpaired electrons are spin up is favoured. For the first band, one is ionised, one band is formed.
For the other bands, where an additional unpaired electron is produced, two resultant states can form, where the unpaired electron can either go with or against the spin of the other unpaired electrons. The state where the unpaired electrons are the same spin is lower in energy and has a multiplicity of 4. The states are a multiplicity of either doublet or quartet, hence a band is formed for each.
The bond lengths will change but the amount that it does is quite complex.