During the last lecture we looked at N-N scattering in the low-energy regime, and determined what square well potentials were required to reproduce the data. We found that the potential had very different depths and ranges, but had a volume integral that was approximately the same. Also, for homework this week you are looking at the low energy phase shifts induced by a Yukawa potential of range and coupling of . The phase shift will be the same for spin triplet and singlet channels by construction.
In the extreme low energy limit, we would expect that the long-range part
of the potential between
nucleons is dominated by the exchange of the lightest strongly interacting
particle (as we are requiring all interactions are local), which we know to be the
Let us consider the dynamics of non-relativistic nucleons with 's.
As we are dealing with low energy processes, with a characteristic momentum
transfer of order
we expect that virtual pair production of nucleons is
production doesn't occur for energies
Therefore, we can use, honest to god, two-component spinors to describe
the theory and use a lagrange density
of the form
We are interested in the long-range behavour of the nuclear force and this will be induced by the exchange of 's. Let us construct the potential arising from one-pion exchange (OPE), it arises from the tree-level graphs with four external nucleons and an off-shell pion, as shown in fig. ().
The matrix element for nucleons scattering by pion exchange is
given by the graph, using our
usual Feynman rules, at lowest order in perturbation theory
(and recalling that a derivative acting on a scalar
field with incoming momentum q gives
The spatial potential
is recovered from the momentum
via a fourier
Let us start by doing the integral, without all the factors out the front,
This looks like a fairly innocent expression, but now we have to evaluate the
partial derivatives acting on .
Lets set up the partial derivatives so that it is clear where the
various parts of the final expression come
from, we have that
The final result for the potential between two nucleons induced by
the exchange of a virtual pion is given
Notice that we have recovered the function we discussed earlier, however, it was a bit subtle, as these things usually are! We had to add it in by hand in order to ensure that the action of the laplacian is reproduced. As we are not attempting to describes the short-distance part of the potential at this stage, and will not ask questions about operators that depend on short distance physics we can forget about the contribution. This gets renormalized away into the short distance part of the potential, described by and , which in the language of meson exchange models correspond to and exchange. In these models, which have many free parameters fit to reproduce nucleon-nucleon scattering, the singular part of the pion potential is "renormalized away" by the fitting of the heavy meson parameters. This fact is usually not stated in this way, but this is infact what is going on.
Let us now examine the behavour of each of the components of the pion exchange potential. The potential is strongly isospin dependent due to the factor (where is the total isospin of the N-N system). The interactions is 3 times stronger in the channel than in the channel.
The contribution from the operator depends on which angular momentum states are involved, it is a non-central force. Notice that is a traceless and symmetric tensor with 2 indices, and as such must transform as a object under rotations. For a more pedestrian view of this consider inserting different values for . For we have , and or gives . Both of which are written entirely in terms of the tensors. Therefore, this term can only contribute when the angular momentum of the initial and final states differs by . So for, initial and final state S-waves, it doesn't contribute. However, in the case of the deuteron, where we have a total state, this operator can induce and admixture of into our initially state. It is now clear that we must consider both components from the beginning and perform a coupled channels analysis. Physically, the form of this potential indicates that it is strongest when the separation vector is aligned or antialigned in the direction of the spins. The sign of the contribution depends upon the isospin channel under consideration, but for the deuteron with isospin , the noncentral force deforms the deuteron to be cigar-shaped. We should note that this form of interaction preserves spin, i.e. it commutes with the operator. It is this interaction that is responsible for the quadrupole moment of the deuteron.
The central part of the potential induced by pion exchange (preserves angular momentum by definition) depends on the spin and isospin channel. It is attractive for , but repulsive for the and channels, to name a few.