How can two-time theories be compactified to 3+1 without any Kaluza-Klein remnants?

Question

I have recently been looking into the two-time theories and the implied concepts.

For me this seems slightly hard to grasp.

How can I see the basic concept in this theory in a fundamental way based on its implied interaction with normal 3+1 dimension?

I am interested specifically in how gauge symmetries that effectively reduce 2T-physics in 4+2 dimensions to 1T-physics in 3+1 dimensions without any Kaluza-Klein remnants.

This article here possibly says something about it, in particular the papers explained therein. But I have just detected and not yet read it. — Dilaton, Dec 09 '12 at 23:00
"slightly hard to grasp." My friend, if you have understood one time dimension, you are already a king among physicists. — kηives, Dec 10 '12 at 01:19

score 2 · Answer 1 · answered Jun 29 '13 at 23:15

In this blog post, a paper that derives by dimensional reduction well known super Yang-Mills (SYM) theories, such as N=1 SYM in 9+1 dimensions and N=4 SYM in 3+1 dimensions among other things using a SYM theory in 10+2 dimensions as a common more fundamental underlying theory.

As can be seen from looking at figure 1 of that paper

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As stated below equation (3.1), if applying the method of deriving shadows of two time physics to obtain lower dimensional theories, Kaluza-Klein are avoided.

How can two-time theories be compactified to 3+1 without any Kaluza-Klein remnants?

1 Answers1