I am chemist and ask for apologies for all my mathematical inabilities when asking this question in advance, but after quite a bit of searching I found that this problem could be "open" or at least hard enough to find addressed in the literature and also advanced enough that it's possibly suitable to be asked here.

I work over a subset of the finite groups called point groups these are all the ((essentially) finite) subgroups of $O(3)$. The "degeneracies" arising in those groups are of importance in Chemistry so I started to investigate them. With "degeneracy" the dimensions of the irreps over $\mathbb R$, (this is of essential importance) occurring for the group under consideration is meant. Whenever a group is represented by an irrep of dimension $n>1$ we speak about $n$-fold degeneracy.

The term degeneracy in this context relates to the fact that the quantum mechanical eigenstates of (symmetric) systems/molecules form such $n$-dimensional sub spaces of the Hilbert space. Since the Hamilton operator is self-adjunct it makes sense to regard representations over $\mathbb R$ instead of over the usually more elegant $\mathbb C$.

My first question is, under which conditions in terms of group elements degeneracy can occur in a group? And the second question is how is the maximal dimension $n_{\max}$ of real irreps, over all irreps of the group, determined by the structure of the group?

My primary observation is that groups that contain exactly one generator $y$ of order $m=3$, like a group $\langle x,y,...| x^2=y^m = 1 = ...\rangle $ have $n_{\max}=2$

Then there are just a very few point groups with $n_{\max} > 2$. We call them "high symmetry groups". Basically its the symmetry groups of the tetrahedron, the octahedron and the icosahedron (with 2 or 3 certain subgroups of theirs), where the former two have $n_{\max}=3$, the latter $n_{\max}=5$.

These high symmetry groups all have two generators, the tetrahedral groups one of order $m=3$, the octahedral groups one of order $m=4$ and the icosahedral groups one of order $5$.

So I would assume that there is a connection between the order of the generators and the degeneracies that can occur in a group. What it is exactly remains very obscure to me. So I would be very grateful about any hints also to the literature.


Since the audience is so fantastically knowledgeable, I can't resist to make a small comment on the motivation of my research in the hope it might ring some bell and give rise to more inspiring comments:

The motivation of my question is, that you can see certain interesting physical properties in the states (of physical systems) if they are degenerate. "States" are some manifestations of irreps where we have direct numerical access to and a good intuition about their visual representations. It happens that there are certain, it seems, deep connections between the angular momentum operator, which is essentially an infinitesimal rotation in the (physical space) $\mathbb R^3$, and the occurrence of degeneracy (at least if it's 2-fold). At the same time we see that these states which are instances of degenerate representations are transformed into each others by (finite) rotations. Such that the question was arising if all such degeneracies are related to rotations, or if there is at least something in the structure of rotations that is general in $d>1$ dimensional representations.

There was recently a result that suggested that there is a "hidden" anti-unitary symmetry (state transforming operator) at the basis of any $2$-fold degeneracy of the form

$$ \mathcal{O} = i \begin{pmatrix} 0 & 1 \\ -1 & 0 \end{pmatrix} \mathcal{K}$$ (with $\mathcal{K}$ as complex conjugation operator) that transforms between the two degenerate irreps. Such an operator can be easily constructed from the angular momentum operator, for example, but not only, constructions of operators like {\mathcal{O}} based on spin or time reversal and others are possible if one considers more general "parametrizations" of physical systems then only $\mathbb R^3$. Anyway, as far as symmetries of the real space $\mathbb R^3$ are concerned it seems that rotation (and infintesimal rotation) are crucial and I aim to understand what "crucial" here exactly means.

What I find in particular intriguing in the light of the answer from @QiaochuYuan is the connection with "non-Abelianess", because the defining relation of $J$, the angular momentum or also spin operator is the so called "angular momentum algebra", that is a commutator relation between its components

$$ [J_i,J_j] = i \varepsilon_{ijk} J_k$$

(with the Levi-Civita symbol $\varepsilon$). So this seems to suggest that angular momentum is an essential source of non-commutativity somehow. I like then to understand what types of sources else there might be, for this non-commutativity in quantum mechanical systems, especially if only representations of states in $\mathbf{R}^3$ are considered. One thing which complicates the question is that in most systems rotational symmetry "is broken" but degeneracy can nevertheless occur. Then my question would be, what is the explicit form of the $\mathcal{O}$ operator and if it can be continuously related to angular momentum if one views the "symmetry breaking" as a continuous process.

(Sorry for the post-answer edit, I hope it complies with the MO rules!)

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    $\begingroup$ There aren't that many subgroups of $O(3)$, so if that's all you're ultimately interested in, an explicit list is probably the most helpful. For more general finite groups I don't think it's easy to deduce $n_{\mathrm{max}}$ directly from, say, a presentation, but representation theory says a lot (for example, the character table directly gives some inequalities). For an introduction, I recommend Serre's "Linear representations of finite groups". $\endgroup$ – Achim Krause Oct 10 at 10:29
  • $\begingroup$ @AchimKrause thank you for your comment. Ultimately I would be interested in the general principle that underlies degeneracies so I have put the (finite) in parentheses. Then the lists all are "countable inifinit lists" where induction is not immediate. As well in the former sense an extension to $O(n)$ with $n>3$ would be also interesting for me. $\endgroup$ – Rudi_Birnbaum Oct 10 at 10:35
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    $\begingroup$ I'm still not sure if I quite understand the terminology. When you say "under which conditions degeneracy can occur in a group", do you mean "under which conditions does a group have irreps of dimension $n>1$"? In that case, that happens precisely if your group is nonabelian (or, I guess, if you're working with real irreps, if your group is not of the form $C_2^{\times n}$). $\endgroup$ – Achim Krause Oct 10 at 10:38
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    $\begingroup$ The general principle that governs the dimensions (and other properties) of irreps is definitely given by character theory. I recommend looking into Serre's book! $\endgroup$ – Achim Krause Oct 10 at 10:41
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    $\begingroup$ Yes this is a good one if I remember rightly. I think the important thing is to have multiple books open at once on the table as it were, because each one has its eccentricities and weaknesses, so it's easier to get an intuitive picture for what is happening if you can see a few different books at once, see where they use the same examples, try to figure why they don't always use the same examples for the same theorem and so on. I normally try to come up with counterexamples to test the theorems and see how strong they are, this also increases my appreciation for the good theorems. $\endgroup$ – Hollis Williams Oct 12 at 12:45

Your question touches on many issues in group representation theory, and I can only give a few general remarks which may point you in interesting directions for further reading.

As to your question regarding the maximal real irreducible representation of a finite group, there is an interesting connection with the Frobenius Schur indicator.

If $\chi$ is a (complex) irreducible character of a finite group $G$, the Frobenius-Schur indicator of $\chi$ is denoted by $\nu(\chi)$ defined to be $0$ if $\chi$ is not real-valued, to be $-1$ if $\chi$ is real-valued, but $\chi$ may NOT be afforded by a representation over $\mathbb{R}$, and to be $1$ if $\chi$ is afforded by a representation over $\mathbb{R}.$ For example, the unique irreducible complex character of degree $2$ of the quaternion group of order $8$ has Frobenius-Schur indicator $-1$, and the unique irreducible character of degree $2$ of the dihedral group of order $8$ ( I mean the one with $8$ elements) has Frobenius-Schur indicator $1$.

The number of solutions of $x^{2}=1 $ in the finite group $G$ is equal to $\sum_{\chi} \nu(\chi) \chi(1)$, where $\chi$ runs over the complex irreducible characters of $G$.

This is especially useful if all irreducible characters $\chi$ of $G$ have $\nu(\chi) = 1$, which is always the case for $G = S_{n}$ (the symmetric group).

The FS-indicator may (in principle at least) be calculated via the formula $\nu(\chi) = \frac{1}{|G|} \sum_{g \in G} \chi(g^{2}).$

In the case of the alternating group of degree $5$, for example, all irreducible characters $\chi$ have $\nu(\chi) = 1$, the irreducible characters have degree $1,3,3,4,5$. Hence we get $\sum_{\chi} \nu(\chi)\chi(1) = 16$, and there are indeed $16$ solutions of $x^{2} = 1$ in $G$ (the identity and fifteen elements of order $2$).

As to the question of what you term degeneracy, there is some ambiguity (related to the Frobenius-Schur indicator and also the Schur index). For example, the quaternion group of order $8$ has a $4$-dimensional representation which is irreducible as a real representation, but which is equivalent to the sum of two equivalent $2$-dimensional complex irreducible representations. An absolutely irreducible real representation is a real irreducible representation which remains irreducible as a complex representation. This is a representation whose character $\chi$ is irreducible as a complex character and has $\nu(\chi) = 1.$

A real irreducible representation which is not absolutely irreducible is one which is not irreducible as a complex representation. Such a representation may afford a character of the form $2\chi$ where $\chi$ is a complex irreducible character with $\nu(\chi) = -1$, or it may afford a character of the form $\chi + \overline{\chi}$, where $\chi$ is a complex irreducible character with $\nu(\chi) = 0$ (ie $\chi$ is not real-valued).

In terms of complex irreducible representations, it is one of the earliest theorems in group theory (due to C. Jordan) that if a finite group $G$ has a complex representation of degree $n$ (irreducible or not), then $G$ has an Abelian normal subgroup whose index is bounded in terms of $n$. This also applies to real irreducible representations.

If we restrict to complex irreducible representations which are primitive (that is, can not be induced from a representation of a proper subgroup), this tells us that if $G$ has a primitive complex irreducible representation of degree $n$, then the number of possibilities for $G/Z(G)$ is bounded in terms of $n$.

On the other hand, the symmetric group $S_{n+1}$ always has a real irreducible representation of degree $n$, and has order $(n+1)!$, yet has no non-identity Abelian normal subgroup if $n >3.$ This is related to the "generic" worst case bound for Jordan's Theorem, and is genuinely an upper bound for that Theorem if $n$ is large enough.

I think that in general, it is very difficult to relate the order of generators of a finite group $G$ with the largest degree of its real (or complex) irreducible representations. For example, there are arbitrarily large finite simple groups $G$ which may be generated by an element of order $2$ and an element of order $3$, and there is therefore no upper bound on the dimensions of the real irreducible representations of finte groups which may be generated by an element of order $2$ and an element of order $3$.

Later edit: Another general fact which is often useful, is a result of N. Ito, which states that if the finite group $G$ has an Abelian normal subgroup $A$, then the degree of any complex irreducible representation of $G$ is a divisor of the index $[G:A].$

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  • $\begingroup$ Thank you very much! This is indeed very interesting, I will check these things also in Serres book. On degeneracy: It is basically all about the dimension of the eigenspaces of the self-adjunct Hamilton operator. Whenever their dimension is $>1$ its degeneracy. Since the groups under consideration acts on the Hamiltonian, one can associate IRREPS directly with the "energy" (= eigenvalue of the Hamiltonian) related eigenspaces. $\endgroup$ – Rudi_Birnbaum Oct 10 at 12:14
  • $\begingroup$ So its the dimensons of the eigenspaces of the Hamiltonian which commutes with the group elements (or so to say the elements of a faithful representation of the group in $\mathbb R^3$). Does that clarify it? $\endgroup$ – Rudi_Birnbaum Oct 10 at 12:15
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    $\begingroup$ I was speaking not just of the three dimensional case, but in general. An example of what I meant is the quaterion group of order $8$ which has an irreducible real representation of degree $4$, but there are non-scalar matrices which commute with all group elements of that representation, so the representation is not irreducible when considered as a complex representation. $\endgroup$ – Geoff Robinson Oct 10 at 12:23

A simple bound on the largest dimension of a complex irreducible representation (which is either equal to or half of the largest dimension of a real irreducible representation) is the following: we know that

  • $|G| = \sum d_i^2$ where $d_i$ are the dimensions of the irreducibles,
  • the number of (complex) irreducibles is the number $c(G)$ of conjugacy classes, and
  • the size $a(G) = |G^{ab}|$ of the abelianization is the number of $1$-dimensional irreducibles (so the number of $d_i$ terms equal to $1$).

It follows that the largest dimension $d_{max}$ satisfies $a(G) + d_{max}^2 \le |G| \le a(G) + (c(G) - a(G)) d_{max}^2$, and rearranging these gives

$$\sqrt{ \frac{|G| - a(G)}{c(G) - a(G)} } \le d_{max} \le \sqrt{|G| - a(G)}.$$

$c(G)$ is a measure of "how abelian" $G$ is; it's a nice exercise to show that $\frac{c(G)}{|G|}$ is the probability that two random elements of $G$ commute. Roughly speaking this means that $d_{max}$ is a measure of "how nonabelian" $G$ is. For example, if $G = A_5$ is the icosahedral group then $|G| = 60, a(G) = 1, c(G) = 5$ gives

$$ \sqrt{ \frac{59}{4} } \approx 3.84 \dots \le d_{max} \le \sqrt{59} \approx 7.68 \dots $$

so $4 \le d_{max} \le 7$, and since we also know that the dimensions $d_i$ divide $|G|$ we have $4 \le d_{max} \le 6$, and the true value $d_{max} = 5$ is right in the middle. Loosely speaking this says that $A_5$ is "more nonabelian" than, say, a dihedral group, which satisfies $d_{max} = 2$.

This bound is most useful when the abelianization is large. A different bound useful when the center $Z$ is large is the following: we know that

  • by Schur's lemma every irreducible representation has a central character, and if $\lambda : Z \to \mathbb{C}^{\times}$ is a central character, then the irreducibles with central character $\lambda$ can be identified with simple modules over the twisted group algebra obtained by quotienting $\mathbb{C}[G]$ by the relations $z = \lambda(z)$ for $z \in Z(G)$,
  • every twisted group algebra as above has dimension $|G/Z|$, so the dimensions $d_i(\lambda)$ of the irreducibles with central character $\lambda$ satisfy $|G/Z| = \sum d_i(\lambda)^2$,
  • the number of irreducibles with a fixed central character is the number of conjugacy classes of $G/Z$ satisfying a certain condition, and in particular is at most the number of conjugacy classes of $G/Z$.

Now it follows that the largest dimension $d_{max}$ satisfies $d_{max}^2 \le |G/Z| \le c(G/Z) d_{max}^2$, which gives

$$\sqrt{ \frac{|G/Z|}{c(G/Z)} } \le d_{max} \le \sqrt{|G/Z|}.$$

For example, the upper bound is tight for a finite Heisenberg group $H_3(\mathbb{F}_p)$, which satisfies $|G/Z| = p^2$ and has $p^2$ one-dimensional characters and $p - 1$ irreducibles of dimension $p$. The lower bound actually produces $1$ here which shows that it can be worse than the previous lower bound (which applied here gives $\sqrt{ \frac{p^3 - p^2}{p^2 + p - 1} } \approx \sqrt{p}$). The size of the center is another measure of "how abelian" $G$ is so this gives another sense in which $d_{max}$ measures "how nonabelian" $G$ is.

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    $\begingroup$ This is not quite relevant to the OP, but when I was a wee lad I asked MO how small a group with an irreducible representation of dimension $n$ could be, as a function of $n$. The answer appears to depend delicately on an open number-theoretic question: if you can find a prime $q \equiv 1 \bmod n$ of size $O(n^{1 + \varepsilon})$ then you can take $|G| = nq = O(n^{2 + \varepsilon})$. Unconditionally in the worst case it's unclear how to beat $|G| \approx n^3$. Link: mathoverflow.net/questions/530/… $\endgroup$ – Qiaochu Yuan Oct 10 at 21:13
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    $\begingroup$ Thank you very much for this extremely inspiring answer! Unfortunately I understand only 2/3 at most (especially the "twisted group algebra" is something I never came across before, yet) but this further motivates me to delve deeper into group and representation theory. $\endgroup$ – Rudi_Birnbaum Oct 11 at 10:40

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