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Next: 11.4 Quantum Substances Up: 11. Two Stages of Previous: 11.2 Actual and Virtual Subsections
It is only with virtual events that interactions occur, as actual events are purely selections of a wave function that already includes all possible interactions. If we consider interactions as they are presumed to occur by quantum theory, then it is notable that there are many ways of describing their possibilities, ways which turn out to be describing essentially the same interactions, as they result in the same propensities of actualising, and hence in exactly the same probabilities for actual events. There are several features of interactions which behave in this way:
Despite our relational view of space and time, the manybody wave function was still defined over the configuration space as if the coordinates defined absolute positions in an absolute space. It is certainly more convenient in practice to work with coordinates rather than relative distances in defining places, but if we insist on doing so, we must be careful to define our propensity fields only on certain equivalence classes of configuration spaces. Barbour [1982, 1986] describes how this might be done.
It makes no difference to any interaction or event if the whole universe
were to be shifted over in space, rotated about any axis, or delayed
arbitrarily in time. According to the relational view of space and time,
these cannot be physical changes: if we have only relational distances,
they cannot even be described. If, however, we insist on using the
coordinates and t, then they do make a difference.
Given all pairs of relational distances, for example, those coordinates
are determined (in the nonrelativistic case) only up to a sevenparameter
`gauge transformation'
where R is an orthogonal 3 3 matrix, g is a 3component vector, and h is a scalar. The matrix R describes rotations of the coordinate system, the vector g describes translations of its origin, and h sets the origin of the time coordinate. Furthermore, different rotations and translations can be used at different times: which allows the universe as a whole to be described by a coordinate system in which it (apparently) has an angular momentum and/or a linear velocity. Barbour also considers the case where the `time shift' h varies with time: this is equivalent to replacing the time coordinate t by any other coordinate subject only to the requirement of monotonic increases: Similar laws of transformation hold for relativistic spacetime, based on the inhomogeneous Lorentz group. These transformations are all those allowed which do not change a given physical situation. The set of all ordered pairs which can be transformed among themselves by equations (11.4) and (11.6) therefore form an equivalence class. It is the specification of which equivalence class which describes the physical situation, and all physical laws should depend only on the equivalence class, not on any preferred members of the class. That is, it should not make any difference to physical processes or physical laws if the universe as a whole were described by new coordinates which were translated and/or rotated compared with any other coordinate system. Absolute positions and rotations have no significance. We say then, that the physical laws must be invariant under the transformations (11.4) and (11.6). The relational view of spacetime can therefore be expressed either as extensiveness being purely a relation between places, and places not being individuated beyond their extensive relations, or as spacetime being labelled by configuration coordinates with there being additional laws of `gauge invariance' which state that all physical laws and probabilities should be invariant under the transformations of equations (11.4) and (11.6).
However, as explained in any textbook on electromagnetic theory, the potentials A and V are not uniquely determined by the equations (11.7). For B is left the same if A changes by the gradient of some function: while E is then also unchanged if V changes by Since, in the Maxwell theory, the physically measurable quantities are E and B, and these do not change under the transformations (11.9) and (11.10), we have an invariance of the theory. The transformations (11.9) and (11.10) are called gauge transformations, and are an essential feature of Maxwellian electromagnetic theory. Furthermore, the function may be an arbitrary function of space and time: The timederivative of , for example, acts like the origin of potential scale V. It is well known in physics that only differences of potentials have any physical significance, and that absolute values of potential fields are not strictly meaningful. This fact can be expressed more formally by the requirement that all the laws of physics, and all event probabilities, are invariant under the gauge transformations (11.9) and (11.10). Not only do we have a global invariance of the physical laws under changes in the meaning of V = 0 in electrostatics, but the gauge transformations express a local invariance of the laws under potential changes that may differ at every point in space and time. Local invariance imposes a much more stringent condition on physical laws. In the previous section, equation (11.4) expresses a global invariance, whereas equation (11.6) expresses an invariance that is local at least in time (though not in space), and hence has more physical content.
We now look at how gauge invariance is incorporated into quantum
mechanics.
For a particle of mass m and charge q, the familiar
nonrelativistic Schrödinger's equation (11.1) becomes
If Maxwell's theory and quantum mechanics are not to be in conflict, there must not be any observable effects on the wave function of the gauge transformations (11.9) and (11.10). The equation (11.11) remains the same if, when the gauge transformations are performed, the wave function is also transformed according to where we see explicitly that the local nature of the gauge transformations is to change the phase of the wave function by a correspondingly suitable amount. The transformation (11.12) is also perfectly valid for relativistic wave functions. The conclusion is that the local choice of the phase of the wave function is linked to the choice of the vector potential (V,A). One could at this point take a positivistic attitude, and say that the potentials V and A. were `theoretical constructs', as the empirically measurable quantities are the field vectors E and B. This argument would be reinforced by the unobservability of phases in quantum mechanics: all probabilities depend on the square moduli with only relative phases having any observable consequence. The response to this argument is to note that relative phase are observable, just as are relative potentials, but that does not make them any the less real. If we attribute reality to the equivalence classes of potential/phase combinations, with the equivalence classes being defined by the possibility of gauge transformations between all members of each class, then potentials and phases have this new kind of `relational reality'. The situation is exactly analogous to the spatiotemporal invariances of the previous section. Although the absolute position, time, velocity and angular momentum of the universe are physically unobservable, relative positions, times, velocities and angular momenta are still perfectly real and definable. The point at issue is (interestingly) not merely philosophical. For sometimes the field potentials B and E can be vanishingly small even though the potentials V and A may be significant. Because it is V and A which enter into the Schrö.dinger's equation (11.11), the propensities of particles can still be affected in those situations. Such is the case with the AharanovBohm effect (Aharanov & Bohm [1959]), where an electron affected by the relative changes in the vector potentials on either side of a long thin solenoid. There is hence a phase change between the two paths, and this leads to observable interference patterns. Furthermore, these effects persist even when the fields E and B become vanishingly small, so if reality was only to be granted to these fields, then there would be an unusually disproportionate ratio between causes and effects in this case (see Berry [1980, 1986] for more discussion here). Taking V and A as causally efficacious produces a better `balance' between the magnitudes of causes and of effects. 3. Equivalent `Infinitesimal' Sizes of Virtual EventsIn quantum field theory, virtual processes such as those shown in 11.3 contribute to the effective mass and charge of the particles involved. If the theory is naively extended to include virtual events of smaller and smaller extensions, down to the limit of point events, then there is the embarrassing consequence of infinite contributions to the apparent masses and charges. Physicists have come up with a process called `renormalisation', which involves essentially putting in corrections to these effects so that the final masses and charges come out to be what we observe them to be. The trouble is that, strictly speaking, these corrections have to be infinite! Noone has been very happy with this method  Feynman [1985] says that `no matter how clever the word, it is what I would call a dippy process!'. However, physicists have grown accustomed to the idea, and even make it a necessary feature of the new theories they are constructing to describe the weak and strong nuclear interactions. The WeinbergSalaam and quantum chromodynamics (quark) theories are attractive to them precisely because they do allow a renormalisation process to be performed, and finite results obtained. All the infinite changes come essentially because virtual events are considered to have proximities and sizes of all values, down to and including zero distances. Physicists feel that `one should be able to go down to zero distance in order to be mathematically consistent' (Feynman [1985]), but that is where the trouble is. Then, instead of including all possible coupling points [i.e. virtual events] down to a distance of zero, if one stops the calculation when the distance between coupling points is very small  say, 10^{30} centimeters, [very much] smaller than anything observable in experiment (presently 10^{16} centimeters)  then there are definite values for n and j [the initial mass and charge numbers] that we can use so tha the calculated mass comes out to match the mass m observed in experiments, and the calculated charge matches the observed charge, e Now, here's the catch: if somebody else comes along and stops their calculation at a different distance  say, 10^{40} centimeters  their values for n and j to get the same m and e come out different! I do not wish to condone an ad hoc process which may eventually be done away with (e.g. if `superstring' theories^{11.2} become tractable), but it does seem to me that a fundamental misunderstanding is obstructing the way to a possible realistic interpretation of what quantum field theory could be about. The problem goes back to the question of chapter 6 of whether space (and time) are actually composed of points of zero size (albeit in a transfinite number), or whether the continuity and point structure of space and time should be seen as a process of ever more possibilities for subdivision, without there being a definite end. Perhaps there is a difference between a continuum of a bounded (though transfinite) number of points, and a continuum of a unbounded possibilities for division. If we adopt the latter view, virtual events (or `coupling points') should not be seen as necessarily occurring at all separations down to zero, but they should be seen as occurring in regions which are arbitrarily small, without there being a minimum size. We do not want a minimum size, whether it is zero (as Feynman wants), or nonzero (as if space were made of finite `lumps'). We therefore want physical laws to be independent of this precise arbitrariness, and so can allow a physical theory to be a particular equivalence class of combinations of arbitrarilysmall virtual events with correspondingly suitable initial coupling constants (such as the `bare' mass n and `bare' charge j). It would be interesting to speculate at this point as to whether there would be any new physical content in the requirement of `local renormalisability'. This is the requirement that all virtual events are independent in their arbitrariness of size, and that physical laws should be unaffected by all these variabilities. In this way, the door is opened for a possible realistic understanding of the renormalisation process, should it prove to be a permanent feature of physical theories. I am not claiming that it is necessarily part of physics, as our philosophy of nature is only providing a general framework in which quantumlike theories can be formulated realistically, and is not deriving them specifically.
Leinas et al. show that if space has three or more dimensions, and if
is an analytic
function of its variables, then the wave function must be either
symmetric
or antisymmetric
nder the process of exchanging identical particles. This is because, in
three or more dimensions, the trajectory of the process of exchanging
particles any even number of times can be continuously deformed and
contracted into the `identity' process of zero exchanges. The trajectory
for any odd number of exchanges can be similarly deformed into a trajectory for just
one exchange. This means that the , as a multivalued analytic
function, falls into one of the categories (11.13) or (11.15) above.
These are the categories of bosons and fermions respectively.
For fermions, the Pauli Exclusion Principle follows from equation
(11.15). One can see immediately, for example, that the wave function
must be zero if two fermions are in the same place:
Leinas emphasises that within this formulation, the two possibilities (of bosons or fermions) are singled out in a natural way, and not as the consequence of any symmetrisation postulate. SummaryWhat we have done in this section is to point out that the space of `virtual events', and the fields of propensities that thereby result, are not definite functions over Newtonian configuration spaces to complexvalued field functions for definite masses and charges. If we do want to keep these features of our description, all these `spaces' and field descriptions should be seen as simply particular (arbitrary) members of certain equivalence classes. It is the specification of particular equivalence classes which really describes the spaces and propensities for virtual events. From modern physics, it appears to be as essential feature of the `space' of possibilities for virtual events that it is defined in this way. I am not claiming to have found reasons why nature should be like this, only to have put the four features above (usually regarded as some of the more mysterious parts of physics) on a uniform footing. When actual and virtual events are distinguished in a twostage process, with virtual events being the production of propensities for actual events, we can allow that the two kinds of events occur in different `spaces': different sets of possibilities. With the help of the arguments in the previous chapters, we can begin to see the manner in which events, possibilities and propensities etc. can be said to exist. The philosophy of nature is useful as it shows how these things can exist, and thus provides an ontological framework in which quantum physics (and quantum field theory) can be interpreted realistically. Next: 11.4 Quantum Substances Up: 11. Two Stages of Previous: 11.2 Actual and Virtual Prof Ian Thompson 20030225 
