Are the bonding orbitals in methane equivalent - photoelectron spectrum

The low energy portion (the part dealing with the $\ce{2s}$ and $\ce{2p}$ electrons) of the photoelectron (PE) spectrum of methane is reproduced below.

The reaction being examined is the following one-photon process $$\ce{CH4 + ~h\nu~ -> [CH4]^{+} + ~e^-}$$

The fact that 2 peaks in roughly 1:3 intensity are observed is often used to argue against the $\ce{sp^3}$ hybridization model for methane. Simply put, how can a model with 4 equivalent $\ce{sp^3}$ bonds produce 2 peaks in the PE spectrum. The argument then goes on to point out that, according to MO theory, methane has one triply degenerate bonding MO and a second single bonding MO and these two nonequivalent orbitals would explain the 2 peaks in the PE spectrum with their 1:3 ratio (see p. 827 here for an example of such an MO-based explanation).

The PE spectrum of methane shows 2 transitions with 1:3 intensity. How does one know that it is the methane ground state that is responsible for producing two peaks with a 1:3 ratio in the PE spectrum? Why couldn't one argue that it is $\ce{[CH4]^+}$, where we clearly have 3 $\ce{C-H}$ bonds containing a pair of electrons and one $\ce{C-H}$ bond with one electron - two different types of $\ce{C-H}$ bonds in a 1:3 ratio - that is responsible for the two peaks in the PE spectrum?

Can the PE spectrum of methane really be used as evidence to argue against the hybridization model?

EDIT:

Poking around on the internet, I came across this Wikipedia article on Orbital Hybridization - Photoelectron Spectroscopy.

It says,

"There is a popular misconception that the concept of hybrid orbitals incorrectly predicts the ultraviolet photoelectron spectra of many molecules. While this is true if Koopmans' theorem is applied to localized hybrids, quantum mechanics requires that the (in this case ionized) wavefunction obey the symmetry of the molecule which implies resonance in valence bond theory. For example, in methane, the ionized states (CH4+) can be constructed out of four resonance structures attributing the ejected electron to each of the four sp3 orbitals. A linear combination of these four structures, conserving the number of structures, leads to a triply degenerate T2 state and a A1 state.[16] The difference in energy between each ionized state and the ground state would be an ionization energy, which yields two values in agreement with experiment." (emphasis mine)

The bold face portion seems to support my contention (if I'm understanding it correctly) that it is the energy differences between the ground state and the excited state that is responsible for the spectrum. Therefore, orbital splitting and orbital degeneracies in the excited state are likely an explanation for the observed spectrum.

• That's not how I'd interpret the VB discussion in the book. If you want to preserve the idea of hybrid orbitals, then ssavec's answer is the one you want - cast the wavefunction into a linear combination of hybrid orbitals. But I disagree completely that $\ce{[CH4]+}$ is involved - it's an entirely different species with a completely different PES. May 27, 2015 at 17:07
• As the question gradually evolves, I would need more time to medidate on this topic. Although you do not measure spectrum of $\ce{[CH_4]^+}$ (which is different, as you pointed out in your comment), $\ce{[CH_4]^+}$ is the final state of the process (non particle conserving, alas). To be honest, I did not yet came across of rigorous enough QM description of this process (but I did not actually tried that much). May 27, 2015 at 17:43

This question goes along the line of what does it mean when it is said that an sp3 orbital has 25% s-character. It also intrigued me so I have tried to find answer, which would not break my hybridised orbital view.

What you clearly see from the spectrum is that there are two bands, corresponding to different energy levels in the molecule and their intensity is 3:1. You can say, it is $3\times 2p : 1 \times 2s$ and you are done. Not at all. The most important thing to deal with is the $T_{d}$ symmetry of the molecule. That means, all four $\ce{C-H}$ bonds are equivalent.

But it is this symmetry which has the answer. Leaving out the $1s$ orbital of carbon, the occupied orbitals must have the following symmetries: $1\times A_1$ and $3\times T_2$. And this is what you see in the spectrum.

Now how it comes with the hybridisation? Upon simple HF/STO-3G calculation, the orbital populations are following:

• $A_1$: 0.62 C 2s + 4x 0.18 H 1s ... fully symmetric, great
• $T_2$: 0.57 C pz + 0.3 1H 1s + 0.3 2H 1s - 0.3 3H 1s - 0.3 4H 1s
• $T_2$: 0.57 C py + 0.3 1H 1s - 0.3 2H 1s - 0.3 3H 1s + 0.3 4H 1s
• $T_2$: 0.57 C px + 0.3 1H 1s - 0.3 2H 1s + 0.3 3H 1s - 0.3 4H 1s

Well, as if you would copy the symmetry table ;) The downside of this picture is that all the bonds are completely delocalised (as you would expect from canonical MOs). Although observable through PES, they do not allow you to draw line between any C and H atom.

Where do we get the hybridised orbitals? If we want to localize the orbitals, whatever scheme you choose, you just form linear combinations of the existing MOs so that you have least number of atoms involved in any bond. One of such methods is NBO and as a result you obtain:

C - H1  ( 52.55%)   0.7249* C    s( 25.00%)p 3.00( 75.00%)
( 47.45%)   0.6888* H  1 s(100.00%)
C - H2  ( 52.55%)   0.7249* C    s( 25.00%)p 3.00( 75.00%)
( 47.45%)   0.6888* H  2 s(100.00%)
C - H3  ( 52.55%)   0.7249* C    s( 25.00%)p 3.00( 75.00%)
( 47.45%)   0.6888* H  3 s(100.00%)
C - H4  ( 52.55%)   0.7249* C    s( 25.00%)p 3.00( 75.00%)
( 47.45%)   0.6888* H  4 s(100.00%)


All with 2 electron occupation and energy -0.63479 Eh.

So where is the truth? ... $\Psi$ is the answer and you can massage it to your will, depending what you want to see. You want localized bonds? You will get them. You want orbitals with the proper symmetry required by spectroscopy? As you wish.

Does the hybridisation concept have sense? In localized bond picture yes. Is it observable? No, and was never meant to be.

The short answer is that's not how photoelectron spectroscopy works. It's a one-photon spectroscopy.

You have a sample of $\ce{CH4}$ in this case, and you shoot different energy photons at the sample. At certain energies, the photon is absorbed and you get an electron off. Note, that's a single electron from one photon.

For you to have any significant amount of $\ce{[CH4]+}$ around, you'd have to hit it with two photons. The first would do:

$$\ce{CH4 + ~energy -> [CH4]^{+} + ~e^-}$$

Only then would you be able to hit that one single $\ce{[CH4]+}$ ion with another photon.

That's a two-photon process. Assuming the incident light intensity is small, that's extremely unlikely. It's much more likely that that second photon hits a different $\ce{CH4}$.

In other words, normal photoelectron spectroscopy gives a set of intensities when the species absorbs a single photon with enough energy to remove a single electron (i.e., orbital energies). This process happens on the femtosecond timescale, so it's essentially a "frozen orbital" technique. There's no time to sample the electronic structure of the resulting cation.

Also, the PES of $\ce{[CH4]+}$ is completely different (seen here), because of the Jahn-Teller distortion. The geometry is $C_{2v}$ and thus there are many more electronic transitions - it actually gets quite complicated.

• Geoff, thanks for your answer. I'm probably not being clear because I'm not very clear on my own question. I understand that PES is a one photon process. What I'm asking is, doesn't the energetics or MO description of the product ($\ce{[CH4]^+}$ in this case) play some role in determining the energetics of the ejected electron?
– ron
May 27, 2015 at 2:33
• @ron Nope. PES is a fast process. While it's possible to do time-resolved PES you need femtosecond pulses. The best description is the "frozen orbital" approximation. The electron is ejected before it can sample the ionized product. May 27, 2015 at 2:48
• @ron There are techniques where the ion matters. For example, in electrochemistry, such as cyclic voltammetry, the ionization process matters in determining the shape and peak potential. May 27, 2015 at 2:49
• I dug up a PES of $\ce{[CH4]+}$ which shows in Figure 11 the spectra is quite different. May 27, 2015 at 2:58

To begin with, I am not really well-versed in this area, so would appreciate any input/corrections.

Wikipedia is correct on the matter; the photoelectron spectrum of methane is not a proof that hybrid orbitals are incorrect. The same can be said of water, ammonia, and so on. When one says that two peaks in the PES are observed and that it must correspond to two different levels, Koopmans' theorem is being implicitly invoked:

$$\mathrm{IP} = -\varepsilon_i$$

Here, $\mathrm{IP}$ refers to the experimental ionisation potential, and $\varepsilon_i$ refers to the energy of a canonical orbital $|\chi_i\rangle$, which are obtained by solving the Hartree–Fock equations:

$$\hat{f}|\chi_i\rangle = \varepsilon_i|\chi_i\rangle$$

The problem with applying this theorem to hybrid orbitals is that hybrid orbitals are not eigenfunctions of the Fock operator; the hybrid orbitals $\phi_i$ are obtained by some unitary transformation of the canonical orbitals $\chi_i$.

$$\begin{pmatrix} \phi_1 \\ \phi_2 \\ \vdots \\ \phi_i \end{pmatrix} = \mathbf{U}\begin{pmatrix} \chi_1 \\ \chi_2 \\ \vdots \\ \chi_i \end{pmatrix}; \qquad \mathbf{U}^{-1} = \mathbf{U}^\mathrm{T}$$

and Koopmans' theorem does not apply after a unitary transformation, as has been explained in this question. So, the PES cannot be used as proof for the non-existence of hybrid orbitals, since the peaks in the PES cannot be linked to energies of hybrid orbitals.

How can hybrid orbitals explain the PES? Can they even do so? It is instructive to consider the "incorrect" way of doing it, first. This is adapted from Section 2.9 of The Chemical Bond – Fundamental Aspects of Chemical Bonding, edited by Gernot Frenking and Sason Shaik. Let's say we have four equivalent hybrid orbitals in methane, $\{\phi_i\}$ $(i = 1,2,3,4)$. Then the wavefunction of methane, ignoring core orbitals, can be written as a Slater determinant

$$\Psi(\ce{CH4}) = |\phi_1 \phi_2 \phi_3 \phi_4 \bar{\phi}_1 \bar{\phi}_2 \bar{\phi}_3 \bar{\phi}_4|$$

(no bar indicates spin up, a bar indicates spin down). Now, according to the wrong interpretation, one can remove an electron from any of these four orbitals. Without loss of generality we will remove a spin down electron. This supposedly would lead to four possible new wavefunctions:

\begin{align} \Psi_1(\ce{CH4+}) &= |\phi_1 \phi_2 \phi_3 \phi_4 \bar{\phi}_2 \bar{\phi}_3 \bar{\phi}_4| \\ \Psi_2(\ce{CH4+}) &= |\phi_1 \phi_2 \phi_3 \phi_4 \bar{\phi}_1 \bar{\phi}_3 \bar{\phi}_4| \\ \Psi_3(\ce{CH4+}) &= |\phi_1 \phi_2 \phi_3 \phi_4 \bar{\phi}_1 \bar{\phi}_2 \bar{\phi}_4| \\ \Psi_4(\ce{CH4+}) &= |\phi_1 \phi_2 \phi_3 \phi_4 \bar{\phi}_1 \bar{\phi}_2 \bar{\phi}_3| \\ \end{align}

In Koopmans' theorem, the ionisation potential is identified as the difference in energy between the ionised wavefunction and the unionised wavefunction. The theorem states that this is simply the negative of the energy of the orbital from which the electron was removed.

The problem is that these ionised wavefunctions, $\Psi_i(\ce{CH4+})$ $(i = 1,2,3,4)$, are not acceptable wavefunctions for the molecular ion, as they do not respect the $T_\mathrm{d}$ symmetry of the molecular ion (the equilibrium geometry of the molecular ion is not $T_\mathrm{d}$, but PES is a "fast" technique and the geometry must remain the same during ionisation - in other words, Franck–Condon principle).

I can make an educated guess about what exactly "respecting the symmetry" entails, but I'm not 100% sure, so it will be the subject of a separate question, and I will edit it in here if/when it gets answered. Anyway, according to Hiberty and Shaik (who wrote the chapter), a group theoretical analysis will show that the acceptable linear combinations transform as $\mathrm{A_1} + \mathrm{T_2}$, which have different energies. Hence, the PES can still be rationalised using a hybrid orbital approach.

A refutation of the "failures" of VB theory is given in much more detail by Hiberty and Shaik, in Chapter 5 of their other book A Chemist's Guide to Valence Bond Theory. But I'll have to leave that to somebody else to describe, as I don't fully understand it myself.

• Sounds like the sort of argument Professor Klapötke would make (that’s the guy with the tens of resonance structures for $\ce{H2}$). $+1$
– Jan
Sep 15, 2017 at 9:37