In a five-page-long highly efficient paper, Nosratollah Jafari and Ahmad Shariati show that the rules of the so-called "doubly special relativity" (DSR) to transform the energy-momentum vectors are nothing else than the ordinary rules of special relativity translated to awkward variables that parameterize the energy and the momentum.

In fact, there have been two main "subspecies" of DSR proposed in the literature, and our Iranian friends trivialize both of them. The DSR by Magueijo and Smolin is the simpler one.

Magueijo and Smolin demystified

Jafari and Shariati start with the realization that much like

- "p
^{m}p^{n}g_{mn}"

- "p
^{m}p^{n}g_{mn}/ ( 1 - L p^{0})^{2}"

- "pi
^{m}= p^{m}/ ( 1 - L p^{0})"

^{m}", the DSR Lorentz transformations of the 4-vector reduce to the standard Lorentz transformations of special relativity. Note that all components of the energy-momentum vector have the same denominator in the redefinition which is why the direction in spacetime (or velocity) is preserved - it is only the overall magnitude of the 4-vector that is redefined.

Amelino-Camelia DSR

They also show that another version of the transformation rules, one that involves a lot of "sinh" and "cosh", is equivalent to ordinary special relativity, too. In this particular case, they find a non-linear redefinition of the generators of boosts instead of the energy-momentum vector itself. So far I have not checked this portion of the paper at all but I have not found a good reason to doubt that they are correct either.

In this Amelino-Camelia case, it is somewhat unclear whether the physical system is supposed to be invariant under the modified or unmodified boosts and what it exactly means for the system to be invariant under the modified boosts. But I guess that whatever answer we choose, we either obtain something that is equivalent to the conventional theories or inconsistent.

Conclusions

Consequently, there is no new physics in doubly special relativity, and the concept of doubly special relativity can't be used to explain why some physically sick theories such as loop quantum gravity fail to be Lorentz-invariant. Of course, this is no surprise for most physicists because everyone has always known that there can't be any fundamentally new theories that are just "partially" Lorentz-invariant. But still, it is useful to have an explicit set of formulae that prove that there is no new physics behind the papers about DSR. Note that the required field redefinitions are given by non-polynomial functions of the momenta which is why physics would look non-local in the coordinates that are dual to the bizarre DSR momenta instead of the standard ones.

What I still find a bit confusing is that I thought that the Amelino-Camelia DSR had the Poincare group that was a contraction of the quantum deformed AdS or dS symmetry. Quantum deformation looks like something different from a cheap redefinition of variables (or generators). But maybe this difference goes away in the limit of a vanishing cosmological constant, i.e. because of the contraction.

These doubts aside, DSR is certainly not the only example of an overhyped idea that is sold almost as a competitor to the whole field of high-energy physics or string theory but whose emptiness can be shown on one page or two.

## snail feedback (2) :

This paper just duplicates simple derivations that were already made by Amelino-Camellia in a 2002 paper on DSR theories (gr-qc/0210063 on arxiv.org). The question raised by Jafari and Shariati's paper is raised and addressed in that paper. Jafari and Shariati don't even bother to answer the question, by the way--they just say their derivation "probably" means that DSR theories are just restatements of conventional SR in new coordinates, but they don't discuss at all the deeper issues involved, which Amelino-Camellia's paper does. Given that Jafari and Shariati's paper gives no new result and suggests no new interpretation of any result, I'm not even sure why it deserved to be published.

Dear Peter Donis, could you please be more specific what deeper issues do you exactly see there? I, for one, think that there are no deeper issues here at all.

If you can rewrite the theories in conventional coordinates (and dispersion relations), it just means that you don't have any new theories, unless you would have some new prescription what theories are "natural" using the curved coordinates. But because there is no such a description, the field redefinition is completely uninteresting.

A generic "simple" theory in the curved coordinates is just a generic non-local (in x-space) theory in the normal coordinates.

Would you argue that a field redefinition in any theory to any random complicated coordinates raises deep issues? If you don't, what's the difference in the DSR situation?

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