QFT of Charged n-Particle: Dynamics
Posted by Urs Schreiber
Given an -particle (a point, a string, a membrane, etc.) coupled to a -bundle with connection (an electromagnetic field, a Kalb-Ramond field, a 2-gerbe, etc.), what is the corresponding quantum theory?
The answer to this question has a kinematical and a dynamical aspect and up to now I had concentrated on the kinematics:
Definition, point particle, string on , open string on .
Here I start talking about dynamics. The right abstract point of view on the dynamics of quantum systems, as far as path integrals are concerned, is certainly that adopted for instance in
E. Lupercio, B. Uribe
Topological Quantum Field Theories, Strings, and Orbifolds
hep-th/0605255.
A parameter space , describing the shape of the quantum object (the point, the circle, the sphere, etc.) propagates along “worldvolumes” (graphs, surfaces, 3-manifolds, etc.), which are spaces whose boundaries look like , by pull-push along correspondences of the form
Here I formulate this in an arrow theoretic way (a little more arrow-theoretic than the discussion in the above text, that is) that fits into the context of kinematics that I discussed before.
While everything is categorical, a crucial point is that, as opposed to the kinematics, the dynamics requires the push-forward of a set at one point. In the absence of a notion of adjoint morphisms of sets, this requires extra structure on our sets: a measure. This is the infamous measure that appears in the path integral.
The following definition is taken from
Recall # that an -particle is something that looks like the ()-category (the point , or the interval , or the sphere, , etc.) and comes equipped with a choice of maps into some -category called “target space” (ordinarily, are -paths in some “spacetime” ).
Each such map is a configuration of the -particle: one of many ways for it to sit in spacetime.
If our -particle, however, does not just want to sit around, we get the same picture just slightly lifted in dimension: we look at -categories whose boundaries look like , and think of them as inducing interpolations between different configurations of the -particle.
Deinition. A worldvolume (or diagram) for our -particle is an -category together with a collection of embeddings and
Given a worldvolume, a space of histories or space of trajectories or space of paths is a choice of subcatgeory which is compatible with the above choice of configuration space in that and
For instance, for and the single point particle, the simplest worldvolume is the worldline, which is nothing but the interval with the only two possible injections In a simple standard example, we would take target space to be , the category of Moore paths (paths with a parameter length) in and would take the category of histories to be the discrete category on the set of paths of parameter length , say.
Not before long, we will need to equip the space of objects of this category with a measure. The canonical choice here would be the Wiener measure.
The interval in the above example is special, in that it is a cylinder over parameter space.
Definition. A worldvolume is a cylinder over parameter space if there is a unique transformation
Whenever we have a worldvolume which is a cylinder (not only then, but let us concentrate on this for the time being), the unique transformation it comes with induces for us a transformation filling the diagram
This is noteworthy, because this diagram can be regarded as a correspondence through which we may pull-push states of the -particle.
Recall that a state of the particle charged under the -bundle with parallel transport is a transformation of the form
Given the above -diagram, we may
- first pull such a state back along , “from the incoming -particle to the space of paths”
- then tranport it by composition with to the other end of the cylinder
- and finally push it forward along from the space of paths to the outgoing -particle.
The diagrams below illustrate this process, and its appearance in pasting diagrams, in full detail.
Remarkably, while everything in the theory of the charged -particle is completely canonical and based only on abstract arrow theory, here is one point where it seems as if the Dao does not yield an answer, and we need to intervene by hand:
in order to reproduce standard quantum theory, we need to interpret the above push-foward as a push-forward of measure spaces.
If we do this, we add to our definition of space of paths, , a measure on this space. Then the required push-forward is integration over the fiber with respect to this measure.
In our above example, with this measure chosen as the ordinary Wiener measure, the map which we get from the worldline of length is precisely the path integral propagator over time in standard quantum mechanics.
Re: QFT of Charged n-Particle: Dynamics
I just wrote a long reply to this post talking in a pretty general way about categories of spans, functors giving configuration spaces and state spaces, and the pull-push procedure for turning spans of configuration spaces into operators on state spaces, and then mistakenly hit the “cancel” button rather than “preview”. Ugh: never edit anything in a web browser. The bottom line can be summed up thus:
You have a span of configuration spaces - one for a cobordism, and one each for its input and output boundaries. Then you have a “state space” which is something like a space of functions on these configuration spaces (or, if the configuration spaces are categories, a category of presheaves). You want to take a function from input to output. You do this by pulling back the function (or presheaf) to the middle of the span (your space of histories) - then pushing forward onto the output. The result is a path integral.
There are a bunch of variations depending on two things: (1) what category the configuration spaces live in, and (2) what kind of algebraic structure the functions take values in. In particular, if configuration spaces are literally spaces, and functions are literally complex-valued function, then you find you need a measure to do the pushforward - which is then integration. But there are other cases where no extra structure is needed and the Tao remains un-intervened with - basically, if has infinitary “sums”. For example, as John has discussed in the “quantization and cohomology” seminar recently, if is one of these idempotent algebras using “min” instead of summation, you are taking an infemum rather than an integral - so no measure is needed. In a different vein, if we categorify things, and we’re taking presheaves valued in a category with infinite colimits, then again everything works internal to .
Some questions that occur to me, then: what combinations of and work automatically? What sorts of need what kinds of extra structure on to make the push-forward part work? How “canonical” are the choices? Etc.