...aside from supersymmetry...
Apologies if the title was too dramatic. Supersymmetry and its possible looming discovery at the LHC has been discussed many times. But let's look at a different portion of modern model building in particle physics, Grand Unification. Grand Unified Theories (GUTs) are those that embed the Standard Model group\[
SU(3)_c\times SU(2)_W\times U(1)_Y
\] into a larger group, typically "simpler" (having fewer factors), ideally "simple" group in the technical sense (one factor). If it is possible, and it possible, the advantage is that the quarks and leptons may arise in a smaller number of multiplets (representations of the gauge group) and the lower number of factors in the gauge group implies a smaller number of adjustable coupling constants. So the GUTs are more constrained.
If they're verifiably right, they're more beautiful. But because they're more predictive, one may also be worried that they're less flexible and therefore less resilient towards falsification – a characteristic you may consider good or bad. However, the flexibility may be restored by adding various stuff and potentials at the GUT scale so the "qualitative difference" is somewhat debatable. At any rate, from a purely theoretical or aesthetic topdown perspective, it's rather natural to expect that Nature may want to unify the forces near the fundamental scale if She can.
And yes, She can. Many grand unified theories are naturally compatible with everything we may observe at low energies of doable experiments.
Grand unification has been discussed many times on this blog. In this text, I want to be somewhat more specific about the possible choices of the gauge groups and representations and possible particles that could show up at the accelerators (which is generally unlikely as the GUTs are associated with an insanely high energy scale, the GUT scale, which is not far from the Planck scale linked to quantum gravity).
\(SU(5)\): GeorgiGlashow model
The simplest gauge group we may pick is \(SU(5)\). Note that the rank – the maximum number of mutually commuting independent \(U(1)\) subgroups – is equal to four, much like for the Standard Model group. The GeorgiGlashow gauge group has dimension equal to \(d=5^21=24\). The adjoint representation, which is therefore 24dimensional, may be decomposed into representations of the Standard Model subgroup:\[
24\rightarrow (8,1)_0\oplus (1,3)_0\oplus (1,1)_0\oplus (3,2)_{\frac{5}{6}}\oplus (\bar{3},2)_{\frac{5}{6}}
\] In the parentheses, the first number represents the representation in which the piece transforms under the \(SU(3)_c\) colorful group of QCD. It may be a singlet (doesn't transform at all), a triplet (like quarks), antitriplet (like antiquarks), or octet (like gluons, the adjoint representation). More complicated representations may appear, too.
The second number in the parentheses is the representation under the \(SU(2)_W\) electroweak group. Note that the doublet \({\bf 2}\) is equivalent to its complex conjugate representation in this case – because the representation is pseudoreal (there's only one inequivalent spinor representation in 3 dimensions). The adjoint representation is 3dimensional. The subscripts indicate the hypercharge i.e. charge under the \(U(1)_Y\) factor of the Standard Model gauge group.
You see that on the right hand side of the equation above, you find the adjoint representations of \(SU(3)_c\), \(SU(2)_W\), and \(U(1)_Y\). There are two new pieces that are complex conjugate to each other – they come with new gauge bosons that should however be insanely heavy (not accessible at the LHC) if the proton is supposed to preserve its longevity we know and love. The new bosons transform as color triplets as well as electroweak doublets. The latter fact implies that they have charges like an exotic quark doublet. We sometimes talk about new Xbosons and Ybosons.
It's equally interesting to find out whether the leptons and quarks may be rearranged into representations of \(SU(5)\). The answer is YES and this fact is nontrivial. Let's look at all lefthanded twocomponent complex spinor fields that are associated with a single generation of quarks and leptons (the whole field content or particle content is tripled at the end because there are three generations; and the Hermitian conjugate fields are added as well).
We find 15 such spinor fields in total: 2 (up, down: organized as an electroweak doublet) lefthanded quarks, each in three colors (6 in total), 2 lefthanded antiquarks (separate electroweak singlets), each in 3 colors (their Hermitian conjugates are righthanded quarks; again 6), lefthanded electron and lefthanded neutrino (they form a doublet), and a lefthanded positron (an electroweak singlet). In total, \(6+6+2+1=15\). We may also add the lefthanded antineutrino (so far unobserved and insanely feebly interacting if it exists) to raise fifteen to sixteen.
These 15 spinor fields are reorganized as the following representation of \(SU(5)\):\[
\mathbf{\bar{5}}\oplus\mathbf{10}\oplus\mathbf{1}
\] The decomposition of these pieces under the Standard Model group is\[
\eq{
\bar{5}&\rightarrow (\bar{3},1)_{\frac{1}{3}}\oplus (1,2)_{\frac{1}{2}}\\
10&\rightarrow (3,2)_{\frac{1}{6}}\oplus (\bar{3},1)_{\frac{2}{3}}\oplus (1,1)_1\\
1&\rightarrow (1,1)_0
}
\] The last line, the lefthanded antineutrino (whose Hermitian conjugate is the righthanded neutrino), is optional or uncertain, as we have mentioned. The first line contains the lepton doublet and the \(d\)antiquark singlet (\(d^c\) and \(\ell\), to use some symbols) on the right hand side. The second line has \(q\), \(u^c\), and \(e^c\). The \(c\) superscript refers to the antiparticles (it stands for "charge conjugation"). Let me emphasize in advance that the clumping of the particles into these larger representations is inequivalent in flipped \(SU(5)\) models.
The \(SU(5)\) grand unified group may be broken down to the Standard Model if you realize that the Standard Model group is exactly the subgroup that commutes with the generator \(U(1)_Y\), the hypercharge. Up to an overall normalization (that sometimes omits the factor of \(1/2\)), it is given by the following traceless \(5\times 5\) matrix:\[
\frac{Y}{2} = \left(\begin{array}{rrr}
\frac 13&0&0&0&0\\
0&\frac 13&0&0&0\\
0&0&\frac 13&0&0\\
0&0&0&+\frac 12&0\\
0&0&0&0&+\frac 12
\end{array}\right)
\] Equivalently, it is the subgroup that keeps a \(Y\)like vev of a new GUT Higgs field transforming in \({\bf 24}\), the adjoint of \(SU(5)\), invariant. One may also achieve the breaking by Wilson lines (monodromies around noncontractible loops, to be more accurate) in stringy models with extra dimensions and by other means.
The minimum grand unified model predicted a rather slow but not too slow proton decay. Within a year or so, the prediction was ruled out. The simplest grand unified theory has been falsified. The broader concept hasn't been falsified and it has way too many positive features so that we shouldn't think we will kill it too quickly.
Flipped \(SU(5)\) i.e. \(SU(5)\times U(1)\)
The flipped \(SU(5)\) models are the "most comparable ones" to the GeorgiGlashow model. They're associated with the names Dimitri Nanopoulos, Stephen Barr, Ignatios Antoniadis, John Ellis, and John Hagelin and their research in the early 1980s. The realization of this previously overlooked possibility was linked to some string theory research in the 1980s and the 1990s: string theory arguably makes the flipped \(SU(5)\) models more natural than the GeorgiGlashow model.
Note that Sheldon Glashow had already omitted a \(U(1)\) factor once when he tried to construct a purely \(SU(2)\) theory of the electroweak force so it wouldn't be shocking if he has displayed the same excessive fanaticism for minimalism together with Howard Georgi again. ;)
You could think that that \(SU(5)\times U(1)\) must be just a complicated extension of the original \(SU(5)\) in which we add possibilities and allow things to be deformed. You could think that the GeorgiGlashow model is a special case of the flipped \(SU(5)\) models. But you would be wrong. The flipped \(SU(5)\) models are qualitatively different from their unflipped cousins – and they're "equally robust", in some sense. Their arrangement of quarks and leptons into the \(SU(5)\) multiplets is permuted – therefore "flipped" – relatively to the GeorgiGlashow model.
To mention a visible example of the differences, note that the righthanded neutrino \(SU(5)\) singlet was optional in the GeorgiGlashow model. In the flipped \(SU(5)\) models you also have to use \(\bar{5}\oplus 10 \oplus 1\) but the last, singlet piece isn't optional at all. For a simple reason: it is not a neutrino. It is actually the lefthanded positron! We surely need it. So the actual fermionic content we have to add in the flipped \(SU(5)\) models comes in the representation\[
\bar{5}_{3}+10_{1}+1_{5}
\] where the subscripts indicate the charges under the \(U(1)\) factor of the flipped \(SU(5)\) gauge group. These subscripts are extremely natural from the viewpoint of an \(SO(10)\) or \(Spin(10)\) group in which \(SU(5)\times U(1)\) may be embedded. In that group, the three pieces combine to a 16dimensional complex spinor representation; the \(U(1)\) charge is proportional to the sum of all the five weights. It is fair to say that the flipped \(SU(5)\) models become more natural than the ordinary GeorgiGlashow \(SU(5)\) if you look "beyond \(SU(5)\)" e.g. at the \(SO(10)\) models.
The decomposition of the relevant flipped \(SU(5)\) representations under the Standard Model group is\[
\eq{
\bar{5}_{3}&\rightarrow (\bar{3},1)_{\frac{2}{3}}\oplus (1,2)_{\frac{1}{2}}\\
10_{1}&\rightarrow (3,2)_{\frac{1}{6}}\oplus (\bar{3},1)_{\frac{1}{3}}\oplus (1,1)_0\\
1_{5}&\rightarrow (1,1)_1\\
24_0&\rightarrow (8,1)_0\oplus (1,3)_0\oplus (1,1)_0\oplus (3,2)_{\frac{1}{6}}\oplus (\bar{3},2)_{\frac{1}{6}}
}
\] The subscripts on the right hand side are the values of the hypercharge. The last line is the adjoint representation again; there is an extra generator of the \(U(1)\) aside from this line, too. The first line describes the upantiquark lefthanded singlet and the lepton lefthanded doublet. The second line describes the quark lefthanded doublet, the downantiquark lefthanded singlet; and the lefthanded antineutrino (unobserved). The third line is the lefthanded positron singlet and can't be omitted.
Not too grand unified groups
Let me mention that there are other GUTlike gauge groups that are far from simple and that have been proposed with various justifications. The electroweak gauge group only treats the lefthanded particles as doublets. One may add another \(SU(2)\) under which the righthanded particles are doublets. These leftright models have the gauge group \(SU(3)_c\times SU(2)_L\times SU(2)_R\times U(1)_{BL}\).
The PatiSalam model has the gauge group \(SU(4)\times SU(2)\times SU(2)\). The two \(SU(2)\) factors are analogous to those in the previous paragraph. However, \(SU(3)_c\) is embedded into an \(SU(4)\) where the "quark of the fourth color" is identified with a lepton.
Also, \(SO(10)\) models may be flipped to \(SO(10)\times U(1)\). The electroweak \(SU(2)_W\) may be extended to another \(SU(3)\) in the 331 models (Paul Frampton was a pioneer). \(SU(6)\) models have been constructed, too.
Trinification has a gauge group composed of three equal pieces, \(SU(3)\times SU(3)\times SU(3)\).
Truly large and simple GUT groups
However, the truly motivated "master gauge groups" are \(SO(10)\) and \(E_6\), an exceptional group. Note that the \(E_6\) group is the only exceptional group that has complex representations at all – something we need to treat lefthanded and righthanded fermions separately.
This \(E_6\) is naturally embedded into the \(E_8\) that arises in the heterotic string and heterotic Mtheory and it contains pretty much all the GUT groups above as a subgroup, including the group of trinification. The decompositions of all the representations under various subgroups are interesting and you should try to find all of them if you haven't done so. Also, \(SO(10)\times U(1)\) – where the \(U(1)\) may participate or not, depending on whether we have flipped models – may be embedded into \(E_6\).
The fermionic content of \(SO(10)\) models combines into the 16dimensional spinor representation of \(Spin(10)\) I have already mentioned. But it's even more interesting to see what happens for \(E_6\) because the minimum nontrivial representation is the 27dimensional fundamental representation, \({\bf 27}\). This inevitably contains some new spinor fields aside from the quark and leptons we know (and different from the righthanded neutrino, too)!
The decomposition of this representation under \(SO(10)\times U(1)\) is\[
27\rightarrow 16_{1}+10_{2}+1_4.
\] Note that the trace of this \(U(1)\) in this 27dimensional representation is \(16\times 110\times 2+ 1\times 4 = 0\). It has to vanish because it's the trace of a generic generator of a nonAbelian group, \(E_6\).
Now, the \(U(1)\) labels are funny. You may notice that only the 16dimensional spinor of quarks and leptons has an odd label. If you correlated this \(U(1)\) charge with the Rparity in supersymmetric models (instead of using \(BL\), and this is my idea), you could say that we will easily observe fermions from the 16dimensional representation (we do) but bosons from the remaining, 10 and 1dimensional representations!
So it's funny to ask what are the Standard Model charges of the additional representations. If you use the flipped \(SU(5)\) models, you will find out that \({\bf 10}\) decomposes into \({\bf 5}\oplus \bar{\bf 5}\) and these pieces contain both Higgs doublets of the MSSM (but this field content is tripled because there's a pair of Higgs doublets in each of the three generations!) plus a new electroweak singlet squark with the charges of the downsquark.
Symmetry has been a powerful tool in our successful efforts to understand Nature at least for a century. Supersymmetry tells us that we may expect superpartners of all known particles – although some of them may be much less accessible than others. But we could actually find traces of another, ordinary "bosonic" symmetry, by finding the (broken) symmetry partners of the known quarks and leptons.
For example, if the LHC ultimately started to find the new Higgs doublets predicted above as well as an exotic quark or three, it would be a huge hint of an underlying greater symmetry operating in Nature. Many of these models are heavily constrained and virtually all models with new light charged particles destroy the simplest "intriguing accident" of gauge coupling unification. But I view the simplest match for the MSSM gauge coupling unification to be just a 2sigma intriguing bump. It may still be a misleading guide and there may be many more fascinating things we may discover if we sacrifice this one. Of course, it's up to us what we believe but on a sunny day in the future, Nature may very well force us to sacrifice the belief in the simplest scenario of gauge coupling unification.
So far, no official discovery of physics beyond the Standard Model has been announced by the LHC; just to be sure, the Higgs boson is almost as old physics as Peter Higgs himself. But this situation isn't guaranteed to last forever. It isn't even guaranteed to survive the Moriond 2013 conference in early March.
Stay tuned.
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Thanks for this nice extension of what Lenny Susskind said about (only) the SU(5) GUTs, I like this :)
finding supersymmetry does not mean string theory is correct but if supersymmetry exists there are more chances for string theory to work, right?
"The minimum grand unified model predicted a rather slow but not too slow proton decay." Yes, but the prediction was based upon possibly false assumptions.
According to Goffinet, “One of the main drawbacks of grand unification theories is the introduction of new gauge bosons which, in general, break up the lepton and baryon numbers and therefore allow the proton to decay. The current measurement settles firm constraints and has ruled out many of them
including the original SU(5). Another drawback, aesthetic this time, is related to the breaking of the grand unification group. Usually this breaking requires
several Higgs representations which imply a rather complex scalar sector with many physical scalar particles.”
http://cp3.irmp.ucl.ac.be/upload/theses/phd/goffinet.pdf “A bottomup approach to fermion masses”,
2008 doctoral thesis by François Goffinet
Consider three beliefs about the foundations of physics:
(A) The equivalence principle is 100% empirically valid.
(B) The universe is infinite.
(C) Supersymmetry predicts many new particles.
My guess is that the work of Milgrom, McGaugh, and Kroupa refutes belief (A).
http://astroweb.case.edu/ssm/mond/ “The MOND pages” by Stacy McGaugh
The equivalence principle might be 100% correct for measured energy and 100% wrong for nonmeasured energy. If 't Hooft is correct about the foundations of physics, then SU(5) physics needs to be reevaluated. Have most physicists underestimated Milgrom and 't Hooft?
More or less right, well, it depends on which arguments you find convincing. I think that with SUSY, string theory is also unavoidable because SUSY+gravity (gravity provably exists) implies SUGRA and to show that string theory is needed to make SUGRA work is a rather fast and convincing argument, too.
There are also people who say that most string theory vacua should have no lowenergy supersymmetry, which is why we shouldn't expect lowenergy SUSY if string theory is right. I disagree with those arguments.
thanks
Dear Lubos,
what is this sugra > string argument? Does it work in 4d?
Dear Rezso, the *fact* that our Universe can't really be 4D isn't just something you omitted, it's a key part of the argument.
Well, one derives that the charges under the SUGRA have to be quantized, via Dirac quantization rule, it implies that the noncompact symmetries if any are broken to a discrete subgroup, there is a moduli space, and in the extreme limits of the moduli space, one may derive that there are strings and/or other extended objects just like claimed in string theory and one may derive that they interact in the way string/Mtheory says, and the rest of derivation of string/Mtheory dynamics follows the actual derivation that were derived by string theorists in the actual history.
It applies more straightforwardly to highly supersymmetric vacua, such as N=8 in d=4 SUGRA which is a T7 compactification of 11D SUGRA, but the less supersymmetric SUGRA theories have more severe UV problems.
So the more wellbehaved a SUGRA theory is, the more you may hope that it could be consistent, but the more clearly you may also prove that it's actually just an approximation to string/Mtheory.
I very much hope your (Lumo's) disagreement turns our to be justified!
P.S. "Hoping" (which I take to be a relative of "hopping") is an extra adaptive behavior (a fairly fuzzily focused form of mental actention) if what one is hoping for not only helps one to avoid futile fretting or selfdefeating feelings of any sort but if it also keeps one alert and on the lookout for potential realistically exploitable and pleasingtopounce on opportunities.
The way you Lumo are prompted and keep on pointing out the best or most healthily conservative yet most up to date ways of knowing/understanding the laws of Nature (mainly but not only physicsrelated such) reminds me of the function of depleted uranium in a keel of a sailing boat in the midst of a rough and stormy sea! %)
At the risk of sounding ridiculous and naive (or naively ridiculous), I offer the following thought. If the big bang singularity can be seen as one supermassive particle, could you not test any of these models by their ability to predict such a state of matter/time/space/gravity? Is that not the direction these models point to, with particles of ever increasing energy levels?
How big accelerator would we need to test GUT scale physics?
Earth radius? Radius of the trajectory of Earth around Sun?
Minor typo in paragraph 10: "These 15 spinor fields are ... 5 + 10 +1" should probably say 16, not 15.
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