The Harada–Norton group HN\mathrm{HN} is the by the fixed pair of 133×133133\times133 A,BA,B in ATLAS dataset HNG1-f5r133B0:

HN=⟨A,B⟩≤GL133(F5).\mathrm{HN}=\langle A,B\rangle\leq\mathrm{GL}_{133}(\mathbb F_{5}).

The files HNG1-f5r133B0.m1 and HNG1-f5r133B0.m2 specify AA and BB, respectively; their entries are part of this concrete definition. Here F5=Z/5Z\mathbb F_{5}=\mathbb Z/5\mathbb Z is the , GL133(F5)\mathrm{GL}_{133}(\mathbb F_{5}) consists of invertible matrices, and the group operation is matrix multiplication over that field. The exact generator files are linked in References.

Order and structure

This is a nonabelian finite , with

∣HN∣=273030912000000=214⋅36⋅56⋅7⋅11⋅19.|\mathrm{HN}|=273030912000000=2^{14}\cdot3^{6}\cdot5^{6}\cdot7\cdot11\cdot19.

It belongs to the Monster display block of the sporadic groups. This grouping records the ATLAS organization, without asserting a direct embedding into another displayed group.

The concrete matrix model

This gives a on F5133\mathbb F_{5}^{133}. The matrix degree 133133 is distinct from the number of group elements. The two specified matrices determine the group; tests on the orders of unspecified generators would not constitute this definition.

References
  1. ATLAS, Harada–Norton group, order heading and “Representations.”
  2. ATLAS, matrix model HNG1-f5r133B0, “About this representation” and “Download”; exact matrices A and B.