Discriminant coset minima of orthogonal sums #
Under the canonical identification A_(L ⊥ M) ≃ A_L × A_M, the norms in a discriminant
coset are exactly the sums of norms in its two component cosets. Consequently, attained
component minima add, and a vector attains their sum exactly when both components attain
their minima. Iterating this result combines shortest-coset calculations for root lattices
without losing attainment in the orthogonal sum.
The same holds for the orthogonal sum ⊥ i, L i of a finite family: under
A_(⊥ i, L i) ≃ Π i, A_(L i), attained least norms r i of the component cosets sum to the
attained least norm ∑ i, r i of the coset of the orthogonal sum, and a vector of that coset
attains ∑ i, r i exactly when each of its coordinates attains r i. This is the form in which
the shortest norm of a glue word is the sum of the shortest norms of its labels.
No positivity, evenness, or nondegeneracy assumption is required: the statements apply whenever the specified component cosets have least norms.
The construction uses discriminantGroupOrthogonalSumEquiv and
orthogonalSumDualCarrierEquiv, respectively discriminantGroupPiEquiv and piDualCarrierEquiv,
to keep the classes tied to the actual dual carriers.
References #
- J. H. Conway and N. J. A. Sloane, Sphere Packings, Lattices and Groups, Chapter 4, §6 and Chapter 16, §1.
The norms in a discriminant coset of an orthogonal sum are exactly the pairwise sums of norms in its component cosets.
Attained least norms in two discriminant cosets add to the attained least norm of the corresponding coset of the orthogonal sum.
A vector in a fixed discriminant coset attains the sum of component lower bounds exactly when both components attain their respective bounds.
Finite families #
Attained least norms r i in the discriminant cosets a i of a finite family of lattices
sum to the attained least norm of the corresponding coset of the orthogonal sum ⊥ i, N i.
A vector in a fixed discriminant coset of the orthogonal sum ⊥ i, N i attains the sum of
component lower bounds exactly when each of its coordinates attains its bound.