Quantum Mechanics for Engineers 

© Leon van Dommelen 

5.3 TwoState Systems
Twostate systems are systems in which only two quantum states are of
importance. That makes such systems the simplest nontrivial quantum
systems. A lot of qualitative understanding can be obtained from
them. Among others, this section will shed some light on the reason
why chemical bonds tend to involve pairs of electrons.
As seen in chapter 4.6, the protons in the H hydrogen
molecular ion are held together by a single shared electron. However,
in the H neutral hydrogen molecule of the previous section, they
are held together by a shared pair of electrons. In both cases a
stable bond was formed. So why are chemical bonds involving a single
electron relatively rare, while bonds involving pairs of shared
electrons are common?
The unifying concept relating the two bonds is that of twostate
systems. Such systems involve two intuitive basic states and
.
For the hydrogen molecular ion, one state,
, described that the electron was in the ground
state around the left proton. A physically equivalent state,
, had the electron in the ground state
around the right proton. For the hydrogen molecule,
had electron 1 around the left proton and
electron 2 around the right one. The other state
was physically the same, but it had the
electrons reversed.
There are many other physical situations that may be described as two
state systems. Covalent chemical bonds involving atoms other than
hydrogen would be an obvious example. Just substitute a positive ion
for one or both protons.
As another example of a twostate system, consider the
CH “benzene molecular ring.” This molecule consists of a hexagon of
6 carbon atoms that are held together by 9 covalent bonds. The
logical way that 9 bonds can be arranged between the atoms of a 6 atom
ring is to make every second bond a double one. However, that still
leaves two possibilities; the locations of the single and double bonds
can be swapped. So there are once again two different but equivalent
states and .
The NH “ammonia molecule” consists of an nitrogen atom bonded to three
hydrogen atoms. By symmetry, the logical place for the nitrogen atom
to sit would surely be in the center of the triangle formed by the
three hydrogen atoms. But it does not sit there. If it was in the
center of the triangle, the angles between the hydrogen atoms,
measured from the nitrogen nucleus, should be 120 each.
However, as discussed later in chapter 5.11.3, valence bond
theory requires that the angles should be about 90, not
120. (The actual angles are about 108
because of reasons similar to those for water as discussed in chapter
5.11.3.) The key point here is that the nitrogen must sit to
the side of the triangle, and there are two sides, producing once
again two different but equivalent physical states and
.
In each case described above, there are two intuitive physical states
and . The peculiarities of the quantum
mechanics of twostate systems arise from states that are combinations
of these two states, as in
Note that according to the ideas of quantum mechanics, the square
magnitude of the first coefficient of the combined state,
, represents the probability of being in state
and the probability of being in state . Of
course, the total probability of being in one of the states should be
one:
(This is only true if the and states are
orthonormal. In the hydrogen molecule cases, orthonormalizing the
basic states would change them a bit, but their physical nature would
remain much the same, especially if the protons are not too close.)
The key question is now what combination of states has the lowest
energy. That will be the ground state of the
twostate system. The expectation value of energy is
This can be multiplied out, taking into account that numerical factors
come out of the left of an inner product as complex conjugates. The
result is
using the shorthand notation
Note that and are real,
(2.16). They are the expectation energies of the states
and . The states will be ordered so that
is less or equal to .
(In all the examples mentioned so far, and
are equal because the two states are physically
equivalent.) Normally, and are not real but complex
conjugates, (2.16). However, you can always change the
definition of, say, by a complex factor of magnitude one to
make equal to a real and negative number, and then
will be that same negative number.
The above expression for the expectation energy consists of two kinds
of terms, which will be called:
Each of those contributions will be discussed in turn.
The averaged energy is the energy that you would intuitively expect
the combined wave function to have. It is a straightforward sum
of the expectation energies of the two component states and
times the probabilities of being in those states. In
particular, in the important case that the two states have the same
energy, the averaged energy is that energy. What is more logical than
that any mixture of two states with the same energy would have that
energy too?
But the twilight terms throw a monkey wrench in this simplistic
thinking. It can be seen that they will always make the ground state
energy lower than the lowest energy of the component
states . (To see that, just take and
positive real numbers and small enough that can be
neglected.) This lowering of the energy below the lowest component
state comes out of the mathematics of combining states; absolutely no
new physical forces are added to produce it. But if you try to
describe it in terms of classical physics, it really looks like a
mysterious new twilight force
is in operation here.
It is no new force; it is the weird mathematics of quantum mechanics.
So, what are these twilight terms physically? If you mean,
what are they in terms of classical physics, there is simply no
answer. But if you mean, what are they in terms of normal language,
rather than formulae, it is easy. Just have another look at the
definition of the twilight terms; they are a measure of the inner
product . That is the energy you
would get if nature was in state if nature was in state
. On quantum scales, nature can get really, really
ethereal, where it moves beyond being describable by classical
physics, and the result is very concrete, but weird, interactions.
For, at these scales twilight is real, and classical physics is not.
For the twilight terms to be nonzero, there must be a region where the
two states overlap, i.e. there must be a region where both
and are nonzero. In the simplest case of the hydrogen
molecular ion, if the atoms are far apart, the left and right wave
functions do not overlap and the twilight terms will be zero. For the
hydrogen molecule, it gets a bit less intuitive, since the overlap
should really be visualized in the sixdimensional space of those
functions. But still, the terms are zero when the atoms are far
apart.
The twilight terms are customarily referred to as “exchange terms,” but everybody seems to have a different idea
of what that is supposed to mean. The reason may be that these terms
pop up all over the place, in all sorts of very different settings.
This book prefers to call them twilight terms, since that most clearly
expresses what they really are. Nature is in a twilight zone of
ambiguity.
The lowering of the energy by the twilight terms produces more stable
chemical bonds than you would expect. Typically, the effect of the
terms is greatest if the two basic states and are
physically equivalent, like for the mentioned examples. Then the two
states have the same expectation energy, call it
. For such symmetric systems, the
ground state will occur for an equal mixture of the two states,
, because then the
twilight terms are most negative. (Complex coefficients do not really
make a physical difference, so and can be assumed to be
real numbers for convenience.) In the ground state, the lowest energy
is then an amount below the energy of the
component states:

(5.13) 
On the other hand, if the lower energy state has
significantly less energy than state , then the minimum
energy will occur near the lower energy state. That means that
1 and 0. (This assumes that the
twilight terms are not big enough to dominate the energy.) In that
case 0 in the twilight terms (5.12), which
pretty much takes the terms out of the picture completely.
This happens for the singleelectron bond of the hydrogen molecular
ion if the second proton is replaced by another ion, say a lithium
ion. The energy in state , where the electron is around
the proton, will now be significantly less than that of state
, where it is around the lithium ion. For such
asymmetrical singleelectron bonds, the twilight terms are not likely
to help much in forging a strong bond. While it turns out that the
LiH ion is stable, the binding energy is only 0.14 eV or so,
compared to 2.8 eV for the H ion. Also, the LiH
bond seems to be best described as a Van der Waals attraction, rather
than a true chemical bond.
In contrast, for the twoelectron bond of the neutral hydrogen
molecule, if the second proton is replaced by a lithium ion, states
and will still be the same: both states will have
one electron around the proton and one around the lithium ion. The
two states do have the electrons reversed, but the electrons are
identical. Thus the twilight terms are still likely to be effective.
Indeed neutral LiH lithium hydride exists as a stable molecule with a
binding energy of about 2.5 eV at low pressures.
(It should be noted that the LiH bond is very ionic, with the
shared
electrons mostly at the hydrogen side, so the
actual ground state is quite different from the covalent hydrogen
model. But the model should be better when the nuclei are farther
apart, so the analysis can at least justify the existence of a
significant bond.)
For the ammonia molecule, the two states and differ
only in the side of the hydrogen triangle that the nitrogen atom is
at. Since these two states are physically equivalent, there is again
a significant lowering of the energy for the symmetric
combination . Similarly, there is a
significant raising of the energy for the antisymmetric
combination . Transitions between these two
energy states produce photons of a single energy in the microwave
range. It allows a maser (microwaverange laser) to be constructed.
The first maser was in fact an ammonia one. It gave rise to the
subsequent development of opticalrange versions. These were
initially called optical masers,
but are now known as
lasers.
Masers are important for providing a single
frequency reference, like in some atomic clocks. See chapter
7.7 for the operating principle of masers and lasers.
The ammonia molecule may well be the best example of how weird these
twilight effects are. Consider, there are two commonsense states in
which the nitrogen is at one side of the hydrogen triangle. What
physical reason could there possibly be that there is a state of lower
energy in which the atom is at both sides at the same time with a
50/50 probability? Before you answer that, recall that it only works
if you do the 50/50 case right. If you do it wrong, you end up
raising the energy. And the only way to figure out whether you do it
right is to look at the behavior of the sign of a physically
unobservable wave function.
It may finally be noted that in the context of chemical bonds, the
raisedenergy antisymmetric state is often called an “antibonding” state.
Key Points

 In quantum mechanics, the energy of different but physically
equivalent states can be lowered by mixing them together.

 This lowering of energy does not come from new physical forces,
but from the weird mathematics of the wave function.

 The effect tends to be much less when the original states are
physically very different.

 One important place where states are indeed physically the same
is in chemical bonds involving pairs of electrons. Here the
equivalent states merely have the identical electrons interchanged.
5.3 Review Questions

1.

The effectiveness of mixing states was already shown by the hydrogen molecule and molecular ion examples. But the generalized story above restricts the basis
states to be orthogonal, and the states used in the hydrogen examples were not.
Show that if and are not orthogonal states, but are normalized and produce a real and positive value for , like in the hydrogen examples, then orthogonal states can be found in the form
For normalized and the CauchySchwartz inequality implies that will be less than one. If the states do not overlap much, it will be much less than one and will be small.
(If and do not meet the stated requirements, you can always redefine them by factors and , with , , and real, to get states that do.)
Solution 2statea

2.

Show that it does not have an effect on the solution whether or not the basic states and are normalized, like in the previous question, before the state of lowest energy is found.
This requires no detailed analysis; just check that the same solution can be described using the nonorthogonal and orthogonal basis states. It is however an important observation for various numerical solution procedures: your set of basis functions can be cleaned up and simplified without affecting the solution you get.
Solution 2stateb