Fixed-point-free low-order traces on the two rotation tori #
The nonparabolic low-order trace set omits the global parabolic set and uses only eigenvalues whose square is not one. Inversion is therefore fixed-point-free on both the split and norm-one sources, giving
2 * |nonparabolic low traces| ≤ (bound - 1) * M.
noncomputable def
BGS.Markoff.nonparabolicConcreteLowOrderTraceSet
(p : ℕ)
[Fact (Nat.Prime p)]
(bound : ℕ)
:
Nonparabolic bounded-order traces represented in either the split torus or the quadratic norm-one torus.
Equations
- One or more equations did not get rendered due to their size.
Instances For
theorem
BGS.Markoff.mem_nonparabolicConcreteLowOrderTraceSet_of_rotationOrder_lt
{p : ℕ}
[Fact (Nat.Prime p)]
(hpTwo : p ≠ 2)
(t : ZMod p)
(bound : ℕ)
(hnonparabolic : t ^ 2 ≠ 4)
(hsmall : rotationOrder t < bound)
:
Every nonparabolic trace of small rotation order lies in the fixed-point-free concrete trace set.
theorem
BGS.Markoff.two_mul_nonparabolicConcreteLowOrderTraceSet_card_le
{p : ℕ}
[Fact (Nat.Prime p)]
(bound : ℕ)
:
2 * (nonparabolicConcreteLowOrderTraceSet p bound).card ≤ (bound - 1) * maximalDivisorCountSum p bound
The exact fixed-point-free maximal-divisor trace count.