An introduction to crystals¶
Informally, a crystal \(\mathcal{B}\) is an oriented graph with edges colored in some set \(I\) such that, for each \(i\in I\), each node \(x\) has:
at most one \(i\)-successor, denoted \(f_i x\);
at most one \(i\)-predecessor, denoted \(e_i x\).
By convention, one writes \(f_i x=\emptyset\) and \(e_i x=\emptyset\) when \(x\) has no successor resp. predecessor.
One may think of \(\mathcal{B}\) as essentially a deterministic automaton whose dual is also deterministic; in this context, the \(f_i\)’s and \(e_i\)’s are respectively the transition functions of the automaton and of its dual, and \(\emptyset\) is the sink.
A crystal comes further endowed with a weight function \(\operatorname{wt} : \mathcal{B} \to L\) which satisfies appropriate conditions.
In combinatorial representation theory, crystals are used as combinatorial data to model representations of Lie algebra.
Axiomatic definition¶
Let \(C\) be a Cartan type (CartanType
) with index set \(I\),
and \(L\) be a realization of the weight lattice of the type \(C\).
Let \(\alpha_i\) and \(\alpha^{\vee}_i\) denote the simple roots and
coroots respectively.
A type \(C\) crystal is a non-empty set \(\mathcal{B}\) endowed with maps \(\operatorname{wt} : \mathcal{B} \to L\), \(e_i, f_i : \mathcal{B} \to \mathcal{B} \cup \{\emptyset\}\), and \(\varepsilon_i, \varphi_i : \mathcal{B} \to \ZZ \cup \{-\infty\}\) for \(i \in I\) satisfying the following properties for all \(i \in I\):
for \(b, b^{\prime} \in \mathcal{B}\), we have \(f_i b^{\prime} = b\) if and only if \(e_i b = b^{\prime}\);
if \(e_i b \in \mathcal{B}\), then:
\(\operatorname{wt}(e_i b) = \operatorname{wt}(b) + \alpha_i\),
\(\varepsilon_i(e_i b) = \varepsilon_i(b) - 1\),
\(\varphi_i(e_i b) = \varphi_i(b) + 1\);
if \(f_i b \in \mathcal{B}\), then:
\(\operatorname{wt}(f_i b) = \operatorname{wt}(b) - \alpha_i\),
\(\varepsilon_i(f_i b) = \varepsilon_i(b) + 1\),
\(\varphi_i(f_i b) = \varphi_i(b) - 1\);
\(\varphi_i(b) = \varepsilon_i(b) + \langle \alpha^{\vee}_i, \operatorname{wt}(b) \rangle\),
if \(\varphi_i(b) = -\infty\) for \(b \in \mathcal{B}\), then \(e_i b = f_i b = \emptyset\).
Some further conditions are required to guarantee that this data indeed models a representation of a Lie algebra. For finite simply laced types a complete characterization is given by Stembridge’s local axioms [Ste2003].
EXAMPLES:
We construct the type \(A_5\) crystal on letters (or in representation theoretic terms, the highest weight crystal of type \(A_5\) corresponding to the highest weight \(\Lambda_1\)):
sage: C = crystals.Letters(['A',5]); C
The crystal of letters for type ['A', 5]
It has a single highest weight element:
sage: C.highest_weight_vectors()
(1,)
A crystal is an enumerated set (see EnumeratedSets
); and we
can count and list its elements in the usual way:
sage: C.cardinality()
6
sage: C.list()
[1, 2, 3, 4, 5, 6]
as well as use it in for loops:
sage: [x for x in C]
[1, 2, 3, 4, 5, 6]
Here are some more elaborate crystals (see their respective documentations):
sage: Tens = crystals.TensorProduct(C, C)
sage: Spin = crystals.Spins(['B', 3])
sage: Tab = crystals.Tableaux(['A', 3], shape = [2,1,1])
sage: Fast = crystals.FastRankTwo(['B', 2], shape = [3/2, 1/2])
sage: KR = crystals.KirillovReshetikhin(['A',2,1],1,1)
One can get (currently) crude plotting via:
sage: Tab.plot()
Graphics object consisting of 52 graphics primitives
If dot2tex is installed, one can obtain nice latex pictures via:
sage: K = crystals.KirillovReshetikhin(['A',3,1], 1,1)
sage: view(K, pdflatex=True) # optional - dot2tex graphviz, not tested (opens external window)
or with colored edges:
sage: K = crystals.KirillovReshetikhin(['A',3,1], 1,1)
sage: G = K.digraph()
sage: G.set_latex_options(color_by_label={0:"black", 1:"red", 2:"blue", 3:"green"})
sage: view(G, pdflatex=True) # optional - dot2tex graphviz, not tested (opens external window)
For rank two crystals, there is an alternative method of getting
metapost pictures. For more information see C.metapost?
.
Todo
Vocabulary and conventions:
For a classical crystal: connected / highest weight / irreducible
…
Layout instructions for plot() for rank 2 types
RestrictionOfCrystal
The crystals library in Sage grew up from an initial implementation in MuPAD-Combinat (see <MuPAD-Combinat>/lib/COMBINAT/crystals.mu).
- class sage.combinat.crystals.crystals.CrystalBacktracker(crystal, index_set=None)¶
Bases:
sage.combinat.backtrack.GenericBacktracker
Time complexity: \(O(nF)\) amortized for each produced element, where \(n\) is the size of the index set, and \(F\) is the cost of computing \(e\) and \(f\) operators.
Memory complexity: \(O(D)\) where \(D\) is the depth of the crystal.
Principle of the algorithm:
Let \(C\) be a classical crystal. It’s an acyclic graph where each connected component has a unique element without predecessors (the highest weight element for this component). Let’s assume for simplicity that \(C\) is irreducible (i.e. connected) with highest weight element \(u\).
One can define a natural spanning tree of \(C\) by taking \(u\) as the root of the tree, and for any other element \(y\) taking as ancestor the element \(x\) such that there is an \(i\)-arrow from \(x\) to \(y\) with \(i\) minimal. Then, a path from \(u\) to \(y\) describes the lexicographically smallest sequence \(i_1,\dots,i_k\) such that \((f_{i_k} \circ f_{i_1})(u)=y\).
Morally, the iterator implemented below just does a depth first search walk through this spanning tree. In practice, this can be achieved recursively as follows: take an element \(x\), and consider in turn each successor \(y = f_i(x)\), ignoring those such that \(y = f_j(x^{\prime})\) for some \(x^{\prime}\) and \(j<i\) (this can be tested by computing \(e_j(y)\) for \(j<i\)).
EXAMPLES:
sage: from sage.combinat.crystals.crystals import CrystalBacktracker sage: C = crystals.Tableaux(['B',3],shape=[3,2,1]) sage: CB = CrystalBacktracker(C) sage: len(list(CB)) 1617 sage: CB = CrystalBacktracker(C, [1,2]) sage: len(list(CB)) 8