2020
DOI: 10.4310/joc.2020.v11.n1.a7
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Kostant’s weight multiplicity formula and the Fibonacci and Lucas numbers

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Cited by 8 publications
(11 citation statements)
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“…Note that specializing Theorem 1.2 to = 1 and µ = 0 recovers the result presented in [3,Theorem 3.1], which shows that the cardinality of the associated Weyl alternation set is given by a Fibonacci number. Extending our results to the remaining pairs of weights listed in List A and List B is much more difficult since the Weyl group action on the highest weight of these representations is not as straightforward to describe.…”
Section: Introductionsupporting
confidence: 71%
See 1 more Smart Citation
“…Note that specializing Theorem 1.2 to = 1 and µ = 0 recovers the result presented in [3,Theorem 3.1], which shows that the cardinality of the associated Weyl alternation set is given by a Fibonacci number. Extending our results to the remaining pairs of weights listed in List A and List B is much more difficult since the Weyl group action on the highest weight of these representations is not as straightforward to describe.…”
Section: Introductionsupporting
confidence: 71%
“…In this case, Harris, Insko, and Williams established that the cardinalities of the Weyl alternation sets A(λ, 0) are given by linear recurrences with constant coefficients [7,8,12]. In 2017, Chang, Harris, and Insko described the sets A(β, µ), where β is the sum of all of the simple roots in a classical Lie algebra and µ is an integral weight, and showed that the cardinality of these sets are given by the Fibonacci numbers or multiples of the Lucas numbers [3].…”
Section: Introductionmentioning
confidence: 99%
“…In [2] #getting coefficients bigToSmall = { "A" : {"a", "d", "j"}, "B" : {"b", "d", "j"}, "C" : {"a", "e", "j"}, "D" : {"a", "d", "l"}, "E" : {"c", "e", "j"}, "F" : {"b", "f", "j"}, "G" : {"a", "g", "l"}, "H" : {"b", "d", "l"}, "I" : {"a", "e", "o"}, "J" : {"c", "f", "j"}, "K" : {"b", "h", "l"}, "L" : {"a", "i", "o"}, "M" : {"b", "f", "p"}, "N" : {"c", "e", "o"}, "O" : {"a", "g", "q"}, "P" : {"c", "f", "p"}, "Q" : {"a", "i", "q"}, } #contradictions of type III zeroToOne = { "b":{"a"}, "c":{"a", "b", "f"}, "e":{"d"}, "f":{"d", "e"}, "g":{"d","e"}, "h":{"d","e","f","g"}, "i":{"d","e","g"}, "l":{"j"}, "o":{"j","l"}, "p":{"j","l","o"}, "q":{"j","l","o","i"}, "a":set(), "d": set(), "j": set(), "p": set(), A", "B", "C", "D", "E", "F", "G", "H", "I", "J", "K", "L", "M", "N", "O", "P", "Q "A" : {"a", "d", "j"}, "B" : {"b", "d", "j"}, "C" : {"a", "e", "j"}, "D" : {"a", "d", "l"}, "E" : {"c", "e", "j"}, "F" : {"b", "f", "j"}, "G" : {"a", "g", "l"}, "H" : {"b", "d", "l"}, "I" : {"a", "e", "o"}, "J" : {"c", "f", "j"}, "K" : {"b", "h", "l"}, "L" : {"a", "i", "o"}, "M" : {"b", "f", "p"}, "N" : {"c", "e", "o"}, "O" : {"a", "g", "q"}, "P" : {"c", "f", "p"}, "Q" : {"a", "i", "q"} {"a"}, "c":{"a", "b", "f"}, "e":{"d"}, "f":{"d", "e"}, "g":{"d","e"}, "h":{"d","e","f","g"}, "i":{"d","e","g"}, "l":{"j"}, "o":{"j","l"}, "p":{"j","l","o"}, "q":{"j","l","o","i"}, "a":set(), "d": set(), "j": set(), "p": set(), A", "B", "C", "D", "E", "F", "G", "H", "I", "J", "K", "L", "M", "N", "O", "P", "Q "A" : {"a", "d", "j"}, "B" : {"b", "d", "j"}, "C" : {"a", "e", "j"}, "D" : {"a", "d", "l"}, "E" : {"c", "e", "j"}, "F" : {"b", "f", "j"}, "G" : {"a", "g", "l"}, "H" : {"b", "d", "l"}, "I" : {"a", "e", "o"}, "J" : {"c", "f", "j"}, "K" : {"b", "h", "l"}, "L" : {"a", "i", "o"}, "M" : {"b", "f", "p"}, "N" : {"c", "e", "o"}, "O" : {"a", "g", "q"}, "P" : {"c", "f", "p"}, "Q" : {"a", "i", "q"} :{"a"}, "c":{"a", "b", "f"}, "e":{"d"}, "f":{"d", "e"}, "g":{"d","e"}, "h":{"d","e","f","g"}, "i":{"d","e","g"}, "l":{"j"}, "o":{"j","l"}, "p":{"j","l","o"}, "q":{"j","l","o","i"}, "a":set(), "d": set(), "j": set(), "p": set(), } allElementList = ["A", "B", "C", "D", "E", "F", "G", "H", "I", "J", "K", "L", "M", "N", "O", "P", "Q…”
Section: } Allelementlist = ["unclassified
“…with the goal of describing and enumerating the sets A(λ, µ) as the weights λ and µ vary among the (dominant) fundamental weight lattice. Work to describe and enumerate the Weyl alternation sets has considered cases where λ is the highest root or a sum of the simple roots of a simple Lie algebra of types A r , B r , C r , and D r , see [2,4,[6][7][8][9]. The Weyl alternation sets of A 2 , A 3 , and all other simple Lie algebras of rank 2 have been described in [11,12].…”
Section: Introductionmentioning
confidence: 99%
“…Previous work concerning Weyl alternation sets includes determining and enumerating A(α, 0) when α is the highest root of the simple Lie algebras [4,7] and A(λ, 0) when λ is the sum of the simple roots of the classical Lie algebras [2]. In these cases the size of the Weyl alternation sets are given by constant coefficient homogeneous relations.…”
Section: Introductionmentioning
confidence: 99%