Quantum integers #
This file develops the symmetric quantum integers associated to a generic nonzero parameter in a field. Besides the quotient definition, it provides a denominator-free Laurent sum, the sign and three-term recurrence identities, and the nonvanishing result needed for the ladder coefficients of generic rank-one quantum-group representations.
An element of a field is a generic quantum parameter if it is nonzero and none of its positive natural powers is one.
Instances For
A generic quantum parameter is nonzero.
No positive natural power of a generic quantum parameter is one.
The natural powers of a generic quantum parameter are pairwise distinct.
The integer powers of a generic quantum parameter are pairwise distinct.
At a generic parameter in a field of characteristic not two, a signed power ε q ^ m is an
integral power of q only for the positive sign.
At a generic parameter in a field of characteristic not two, a signed power ε q ^ m
determines both the sign ε and the exponent m.
A generic quantum parameter is not equal to its inverse.
The denominator in the symmetric quantum-integer formula is nonzero at a generic parameter.
The inverse of a generic quantum parameter is generic.
A positive natural power of a generic quantum parameter is generic.
For nonzero c, the multiples q ^ n * c of a generic quantum parameter q are pairwise
distinct.
The symmetric quantum integer [r]_q = (q^r - q⁻ʳ) / (q - q⁻¹).
Instances For
The zeroth quantum integer is zero.
Negating the index negates the quantum integer.
Replacing the parameter by its inverse leaves every quantum integer unchanged.
The symmetric quantum integers satisfy the usual three-term recurrence.
The addition formula [a + b]_q = q^a [b]_q + q^(-b) [a]_q.
The difference of two quantum integers as a determinant of neighbouring quantum integers:
[a - b]_q = [a]_q [b + 1]_q - [a + 1]_q [b]_q.
Every nonzero-index quantum integer is nonzero at a generic parameter.
For q ≠ 0, the quantum integer [r]_q vanishes exactly when q^(2r) = 1. When
q - q⁻¹ = 0, that is q = ±1, both sides hold: [r]_q = 0 by the field convention.