apeiron said:
So do we just extrapolate this mental image of a 2D tube to a 6D "tube" which moves a writhing CY space, a tangle of wriggles? This would seem to follow from Tom's description.
No, hopefully not!
Let's discuss the geometrical ideas in more detail:
We start by reducing the 10d spacetime of ST to 3d in order to have a chance to visualize things; that means we have a 2d space and 1d for time. Geometrically the string is (in STs with only closed strings) a closed loop with a coordinate
s labelling the loop and a coordinate
t labelling time; for each
t you have a loop = a "deformed" circle, as
t changes the loop itself changes, e.g. it can vibrate or twist or something like that.
The string is a field
Xm(s,t), where
m is now labelling the spacetime dimension
m=0..2. Attention: these coordinates labelled by
m are different from
s and
t;
s and
t are not labelled by
m. Instead these coordinates are labelling the spacetime the string
X lives in.
In our low-dimensional example we can start with a flat, euclidean space
R2 and a time coordinate. The entire 3d spacetime is now a stack of R
2 spaces on top of each other, one
R2 space for each time
X0. In this picture we identify the time coordinate
t of the string with the time coordinate
X0 of the 3d spacetime. This is slightly misleading if you want to start calculations in string theory, but for our purpose it's OK.
Now you can draw a loop in each
R2 space of the whole stack. So the string lives in an
R2 space and it moves in the third dimension as time evolves. For each time
t you have a new
R2. The coordinate
s is a coordinate along the loop, the coordinates
X1 and
X2 are simply the coordinates within one
R2.
If you now look at the whole
R3, the spacetime, your string will draw a world-tube as it moves through
t=X0.
Now we change to a picture where spacetime is poartially compactified. Instead of
R2 we use a cylinder
R1 * S1. There is one compactified dimension
S1, which is topologically a circle.
Now you can draw a loop on a cyclinder which is again the string seen at one instance of time
t=X0; you are still identifying these to time coordinates. As time evolves you have to draw a stack of cylinders. You can do that by wrapping one cylinder at time
X0 by a new cylinder at time
X0'. If you would do that by a sheet of paper your cylinders (more exactly the dimension labelled by
X2) grew, but that is only due to the limitation of using sheets of paper. Physically this dimension does not grow (in the
R2 case the shape was constant).
Looking at this stack of cylinders is harder to visualize, but still you have a 2d world-tube generated by the string as it moves through this stack of cylinders. Using the sheets of paper wrapping each other you have one closed loop on each sheet.
So it should be clear that changing the shape of one dimension does not chnage the topology of the world tube. If you replace the 1d spatial dimension of the cylinder by a 3d space and if you replace the 1d circular dimension by a CY, the visualization of the wrapped cylinders breaks down, but the 2d world-tube survives mathematically.
The last difficulty is that the length of the string (the loop) can be (much) larger that the length of the circular dimension
S1. That means that the string can wind around the cylinder. You can compare this to a rubber band that fixes a poster. You can wind the rubber band once, twice, ... around the poster. So the rubber band can vibrate (like a violine string) and it can wind around the cylinder. The difference between types of elementary particles is partially due to different windings.
Again this difficulty does not change the topology of the 2d world-tube.