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Isn't Higgs a sneutrino dressed as a man?

Related LHC news: Both ATLAS and CMS released lots of new papers and preprints today. Perhaps most interestingly, ATLAS' measurement of the WW cross section still shows a uniform 2-sigmish excess in all channels after the 20/fb of the 2012 data which keeps the idea of light stops alive. Note that the paper is based on a set of collisions that is disjoint from the previous collisions that also showed an excess. In another ATLAS paper on \(t\bar t\), Monte Carlo models underestimate multijet events (another excess). Also, CMS is seeing a non-signal-like 2.6-sigma (locally) excess in the search for a sub-200-GeV higgsino, in the 30-90 GeV transverse energy channel of trileptons and tetraleptons. It really does seem like the interesting, non-SM-like LHC papers were being delayed.
Carla Biggio wrote a serious paper about a question that is so playful and ambitious that it may look silly to most particle physicists:
Is the standard model scalar the first discovered SUSY particle?
Supersymmetry predicts the doubling of the spectrum of all particles. Each fermion has a bosonic superpartner and vice versa. The traditional lore is that all the "old" particles that have to exist even without SUSY have been seen, while exactly the new particles predicted by SUSY (the superpartners) haven't been seen.

A new pictogram near Boskovice. Police isn't brave enough to accuse the extraterestrial aliens yet (especially because they seem to be NATO members) but hundreds of tourists probably beg to differ. ;-)

But isn't it possible that we have already seen a superpartner? Can't two of the particle species that experimenters already know be superpartners of each other? Let's look at all the possible combinations.

First, we can't have seen the superpartner of the graviton, the gravitino, because its spin is \(j=3/2\) and we haven't seen such an elementary particle yet. That was easy.

However, we couldn't have seen any gauginos, superpartners of the gauge bosons, either, because gauge bosons transform in the adjoint representation (the symmetry works well and we can't ignore it) while all the known candidate superpartners of the gauge bosons i.e. all the known elementary fermions transform in different representations of the gauge groups.

In particular, they transform as doublets under the electroweak \(SU(2)\) while the gauge bosons have to transform as a triplet. The quarks transform as triplets under \(SU(3)\) while the gluons form an octet. At most, the hypercharge \(U(1)\) gauge boson, the \(B^0\)-boson, could be the superpartner of another "complete singlet". But the only singlets we have really seen, the left-handed charged leptons, are charged so they can't be a superpartner of the neutral \(B^0\)-boson.

Can the leptons and quarks have a known superpartner? Those superpartners couldn't be the gauge bosons; this option was already killed in the previous paragraph. But the superpartners have to be bosons and the only remaining elementary boson we know is the Higgs boson. So can the Higgs boson have a known fermionic superpartner?

The Higgs boson transforms as a doublet, carries no color, and one of the components of the Higgs doublet is electrically neutral which fixes the hypercharge. Yes, it's the same arrangement as the lepton doublets.

The Higgs boson could be the sneutrino while the remaining eaten Goldstone bosons in the Higgs doublets could include charged sleptons etc.

Those who have attended a course of "basic conversations in Italian" must know that "a sneutrino" is translated as "a little cute scalar supersymmetric neutral elementary thingie" from Italian to English. If you have also read Aristotle's work, a "sneutrino" is translated as a "sneutrinum" to Latin.

For you to train the "-ino" suffix, you may listen to this song "Beautiful World" by the Bambini di Praga. How many people understand their English? It sounds Korean to me! ;-) But why an English-titled song by an Italian-styled Czech choir would be Korean is beyond me. Probably because they performed it in Korea LOL.

So can the relatively heavy \(125.7\GeV\) Higgs boson we know be nothing else than the superpartner of the light, nearly invisible neutrino? Probably the tau-like neutrino?

Well, there's one obvious sacrifice we have to make. The lightest superpartner is often assumed to be the dark matter particle. Such a particle is stable due to the conservation of R-parity. The R-parity should be \(+1\) for all the known particles and \(-1\) for all the others.

If the R-parity were conserved, the leptons would have to have \(R=+1\) because they can decay to other things with \(R=+1\). So it's the Higgs, the sneutrino, that would have to have \(R=-1\). But particles with \(R=-1\) may only be produced in pairs. On the contrary, the LHC has repeatedly created an isolated Higgs boson which didn't come in pairs.

It seems that the R-parity has to be broken or non-existent. The supersymmetric model building of this form may lose a dark matter candidate – I think that this issue isn't discussed by Biggio – and the broken discrete symmetry may guarantee a lethal rapid proton decay as well as huge neutrino masses.

Biggio proposes a solution to these problems. Instead of a \(\ZZ_2\) R-parity group, she proposes a whole new \(U(1)_R\) continuous R-symmetry. She seems to assign nonzero R-charges even to things like the gauge bosons. I have no idea how it may work because it's so easy to produce another gauge boson (e.g. a photon) out of nothing.

At any rate, if she knows what she's doing, there is a reason why this may work and she concludes that such models are viable. Third-generation sfermions like the stop and sbottom are expected to be light in the model. The model itself seems to be even "more minimal" than the minimal supersymmetric standard model. Because I don't understand why the nonzero R-charges are OK, I would currently bet against this cute possibility.

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reader Ron Maimon said...

This is an ancient idea, easily dismissed, because the Yukawa couplings are forbidden by SUSY. See the intro to Grant and Kakushadze's paper here:

reader Luboš Motl said...

You really meant what I wrote above, didn't you? Yukawa couplings are perfectly allowed by SUSY - they come from the cubic terms in the superpotential - they just break the R-parity in these models. This Carla physicist realizes that R-parity is broken.

Moreover, as the paper you mentioned says, many couplings not allowed by the R-parity are generated after SUSY breaking from the Kähler potential.

reader Sneutrino said...

Not so easily dismissed!! Some Yukawas can appear from the superpotential preserving the R-symmetry and some others can be generated after breaking susy (as it should). This is discussed in the paper. Try then to find a better reason to kill it!

reader Uncle Al said...

"The Higgs boson could be the sneutrino while the remaining eaten Goldstone bosons in the Higgs doublets could include charged sleptons etc." but you will not champion a 90-day geometric Eötvös experiment as a definitiive empirical alternative that requires zero curve fitting. "And why beholdest thou the mote that is in thy brother's eye, but considerest not the beam that is in thine own eye?"

reader kashyap vasavada said...

Interesting speculation. But the currently known Higgs field
plays such a prominent role in giving masses to quarks and leptons and also in
electro-weak symmetry breaking that such a correspondence may require a major
revision of theories. What do you think?

reader Luboš Motl said...

I don't think that the word "speculation" is appropriate. It's a model, or at least a candidate model.

Higgs may play a "prominent" role but the "Higgs boson" is just a name given to the particle of the field playing this role. It doesn't mean that the particle can't have other identities, names, and roles as well. If you can write down the model and things work, it just works and complaints would be irrational.

Not to mention the fact that supersymmetry plays a more prominent role in physics than the Higgs mechanism, so a more logical way to formulate your objection would really be upside down.

reader Luboš Motl said...

Thanks a lot for the insightful comment, A. It is clever.

reader Fred said...

Are your algorithms parametrised and you change the parameters to optimise the score? Or do the algorithms differ in more fundamental ways ? If so how many parameters do you need. Or is this top secret?

reader Luboš Motl said...

There are dozens of pretty much arbitrary numbers - parameters - in my code and in principle, changing them in some ways might improve the score except that most changes one may try seem to make things worse and one doesn't have any deep enough arguments that to change them in one way or another should dramatically improve the final score.

There are also lots of discrete changes being made all the time. It's in no way true that my 220+ submissions are just the same code with different values of parameters. If you divide the submissions to classes whose elements only differ by numbers, there are at least 70 classes. ;-)

Some of these qualitative changes are minor, some of them are conceptual and "huge" but sometimes arguably clever, but most of these would-be clever inventions haven't led to a detectable improvement of the score in most cases when they were applied separately, so the advantages are often theoretical in character. But maybe my above-the-average score may be viewed as circumstantial evidence that collectively, many of these seemingly minor additions work, after all.

If I had to write a paper about all the ideas I've tried, the "inequivalent distinct ideas" would make at least 10-20 sections at this moment.

reader Fred said...

OK. By the way, why did you do it on the Nokia Lumia. Surely a PC would be much faster ?

reader Luboš Motl said...

Sorry, I was assuming you would understand it was a joke. You can't simulate a Universe - or Windows or Ubuntu, for that matter - on Windows Phone.