Orders of elements and cardinalities #
Let g have finite order n and let f divide n. The order of g ^ k is n / gcd n k, so
f divides it exactly when f * gcd n k divides n. That condition is decided one prime of f
at a time: it fails at p exactly when k is divisible by p ^ (v_p n - v_p f + 1), the room
n leaves at p after f, plus one.
In a finite additive group with one, the cardinality casts to 0, as Mathlib's
Nat.cast_card_eq_zero records, so the cardinality minus one casts to -1.
By Euler's theorem, raising an n-th root of unity to the power q ^ φ(n), for q prime to n,
does nothing.
An element squaring to 1 only sees the parity of its exponent, so identities between products
of powers of such elements reduce to congruences modulo 2 between the exponents.
If conjugation by s raises an element t of finite order to a power q, then q is
prime to the order of t, since conjugation preserves orders, and so s normalizes the cyclic
subgroup ⟨t⟩. This is the finite shadow of a relation s t s⁻¹ = t ^ q, such as the one between
Frobenius and tame inertia.
Main results #
IsOfFinOrder.dvd_orderOf_pow_iff, and its additive counterpart: divisibility of the order of a power as non-divisibility of its exponent by a prime power at each prime off.TauCeti.natCast_natCard_sub_one_eq_neg_one: in a finite additive group with one of cardinalityq, the cast ofq - 1is-1, a companion of Mathlib'sNat.cast_card_eq_zero.TauCeti.pow_pow_totient_eq_self:x ^ q ^ φ(n) = xwheneverx ^ n = 1andqis prime ton.TauCeti.mul_pow_eq_of_sq_eq_one: in a commutative monoid, exponents of elements squaring to1only matter modulo2.TauCeti.coprime_orderOf_of_mul_mul_inv_eq_pow,TauCeti.mem_normalizer_zpowers_of_mul_mul_inv_eq_pow: ifs * t * s⁻¹ = t ^ qwithtof finite order, thenqis prime to the order oftandsnormalizes⟨t⟩.
When a number divides the order of a power. Let g have finite order and let f divide
that order. Then f divides the order of g ^ k exactly when, for every prime p of f, the
exponent k is not divisible by p ^ (v_p (orderOf g) - v_p f + 1).
The exponent is the room orderOf g leaves at p after f has taken v_p f, plus one: the
order of g ^ k is orderOf g / gcd (orderOf g) k, so k may absorb at most
v_p (orderOf g) - v_p f powers of p; the first forbidden exponent is that room plus one.
When a number divides the additive order of a multiple. Let g have finite additive order
and let f divide that order. Then f divides the additive order of k • g exactly when, for
every prime p of f, the exponent k is not divisible by
p ^ (v_p (addOrderOf g) - v_p f + 1).
In a finite additive group with one of cardinality q, the cast of q - 1 is -1.
Only parities matter for 2-torsion exponents. In a commutative monoid whose elements
u, v, w, z square to 1, an identity between products of their powers holds as soon as the
exponents agree modulo 2: here S * (u * v) ^ A * (w * z) ^ B * w ^ C * u ^ D regroups as
S * z * (v * w) ^ E * u ^ F. This is the sign bookkeeping behind induction steps on products
of quaternion symbols with binomial exponents.
A conjugate power is a coprime power. If conjugation by s sends an element t of finite
order to t ^ q, then q is prime to the order of t: conjugation preserves orders,
and the order of t ^ q is orderOf t / gcd (orderOf t) q.
A conjugate power normalizes the cyclic subgroup. If conjugation by s sends an element
t of finite order to t ^ q, then s normalizes the cyclic subgroup generated by
t. Since q is prime to the order of t, conjugation by s⁻¹ is a power map on it as well.