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Approaches to Quantum Gravity

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<strong>Quantum</strong> <strong>Gravity</strong> phenomenology 431<br />

theory is in principle able <strong>to</strong> make any definite predictions, since the formalism is<br />

so flexible, so capable of saying anything, that it is feared it will amount basically<br />

<strong>to</strong> saying nothing.<br />

Usually in physics the demand that a theory be falsifiable is of course the first<br />

and most important requirement, but it is also usually not a <strong>to</strong>ugh one: any reasonable,<br />

however naive, concept of theory should give rise <strong>to</strong> a falsifiable theory.<br />

Two known causes of failure for falsifiability are the lack of logical consistency<br />

(so basically the candidate theory was not a theory after all, since the piece of<br />

mathematics introduced did not combine <strong>to</strong> produce a logically consistent overall<br />

structure) or the presence of unlimited flexibility, i.e. the scenario feared for string<br />

theory. Of course a theory that in principle is falsifiable but presents us with practically<br />

unsurmountable computational challenges (which might be the case of loop<br />

quantum gravity, if a satisfac<strong>to</strong>ry description of the classical limit does not become<br />

available) is for our purposes not falsifiable.<br />

So concerning task two the situation does not look very healthy, but the problem<br />

resides on the theory side, not the phenomenology side. If they give us definite<br />

predictions we will do our best <strong>to</strong> honour them by killing their theories (which I<br />

still think should be the healthiest attitude <strong>to</strong> be adopted when doing phenomenology<br />

work). Presently, for most of the fashionable theories, no such honour can be<br />

given.<br />

If indeed, at least for now, we cannot falsify loop quantum gravity and string theory,<br />

can we at least falsify some other theory used in <strong>Quantum</strong> <strong>Gravity</strong> research?<br />

I believe it is extremely important for <strong>Quantum</strong> <strong>Gravity</strong> phenomenology <strong>to</strong> find<br />

one such example. If we do find a first example then we can legitimately hope<br />

that the falsifiability of more and more theories will gradually be achieved. And<br />

because of the importance I give <strong>to</strong> this objective I have invested a lot of effort in<br />

the study of one of the formalisms used in <strong>Quantum</strong> <strong>Gravity</strong> research, that of the<br />

κ-Minkowski noncommutative spacetime. I do not necessarily “favour” this formalism,<br />

but I have the intuition that it should be falsifiable. This intuition must,<br />

however, still find full support in the analysis. The logical consistency of theories<br />

in κ-Minkowski has still not really been shown, at least not <strong>to</strong> the level desired<br />

by physicists, and we are presently unable <strong>to</strong> do many computations in this framework,<br />

which may be a manifestation of a serious unsurmountable challenge for<br />

computations; but at present it is still legitimate <strong>to</strong> hope (in my view rather reasonable<br />

<strong>to</strong> expect) that we will soon be able <strong>to</strong> do these computations. There have,<br />

for many years, been results on κ-Minkowski providing weak links (the usual<br />

weak links from theory <strong>to</strong> effects in <strong>Quantum</strong> <strong>Gravity</strong> research) <strong>to</strong> effects such<br />

as deformed dispersion relations, deformed energy-momentum-conservation laws,<br />

and deformed boost transformations. Some of these links have become gradually<br />

somewhat more robust. I expect that progress in this direction will accelerate thanks

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