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conductors_generic.jl
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conductors_generic.jl
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##########################################################################################################
#
# Conductors for normal extensions of normal fields
#
##########################################################################################################
function tame_conductors_degree_2(O::AbsSimpleNumFieldOrder, bound::ZZRingElem; unramified_outside::Vector{ZZRingElem} = ZZRingElem[])
K = nf(O)
d = degree(O)
b1 = Int(iroot(bound,d))
ram_primes = ramified_primes(O)
sort!(ram_primes)
filter!(x -> x!=2, ram_primes)
list = squarefree_up_to(b1, coprime_to = vcat(ram_primes,2), prime_base = unramified_outside)
extra_list = Tuple{Int, ZZRingElem}[(1,ZZRingElem(1))]
for q in ram_primes
tr = prime_decomposition_type(O, Int(q))
e = tr[1][2]
nq = ZZRingElem(q)^(divexact(d,e))
if nq > bound
break
end
l=length(extra_list)
for i = 1:l
n = extra_list[i][2]*nq
if n > bound
continue
end
push!(extra_list, (extra_list[i][1]*q, n))
end
end
final_list=Tuple{Int,ZZRingElem}[]
l = length(list)
for (el,norm) in extra_list
for i=1:l
if ZZRingElem(list[i])^d*norm>bound
continue
end
push!(final_list, (list[i]*el, ZZRingElem(list[i])^d*norm))
end
end
return final_list
end
function squarefree_for_conductors(O::AbsSimpleNumFieldOrder, n::Int, deg::Int; coprime_to::Vector{ZZRingElem}=ZZRingElem[], prime_base::Vector{ZZRingElem} = ZZRingElem[])
sqf = trues(n)
primes = trues(n)
#remove primes that can be wildly ramified or
#that are ramified in the base field
for x in coprime_to
if x > n
continue
end
el = Int(x)
t = el
while t <= n
@inbounds sqf[t]=false
@inbounds primes[t]=false
t += el
end
end
#sieving procedure
if !(2 in coprime_to)
dt = prime_decomposition_type(O,2)
if isone(gcd(2^dt[1][1]-1, deg))
j = 2
while j <= n
@inbounds sqf[j] = false
@inbounds primes[j] = false
j += 2
end
else
i=2
s=4
while s <= n
@inbounds primes[s] = false
s+=2
end
s=4
while s <= n
@inbounds sqf[s] = false
s+=4
end
end
end
i = 3
b = isqrt(n)
while i <= b
if primes[i]
if gcd(i-1, deg) != 1 && (!isempty(prime_base) && (i in prime_base))
j = i
while j <= n
@inbounds primes[j] = false
j += i
end
j = i^2
t = j
while j <= n
@inbounds sqf[j] = false
j += t
end
else
dt = prime_decomposition_type(O, i)
if gcd(deg, i^dt[1][1]-1) == 1 || (!isempty(prime_base) && !(i in prime_base))
j = i
while j <= n
@inbounds primes[j] = false
@inbounds sqf[j] = false
j+=i
end
else
j=i
while j <= n
@inbounds primes[j]=false
j+=i
end
j=i^2
t=j
while j<= n
@inbounds sqf[j]=false
j+=t
end
end
end
end
i+=2
end
while i<=n
if primes[i] && gcd(i-1, deg) == 1
dt=prime_decomposition_type(O,i)
if gcd(deg, i^dt[1][1]-1) == 1 || (!isempty(prime_base) && !(i in prime_base))
@inbounds sqf[i]=false
j=i
while j <= n
@inbounds sqf[j]=false
j+=i
end
end
end
i+=2
end
if degree(O)==1
i=2
while i<=length(sqf)
@inbounds sqf[i]=false
i+=4
end
end
return Int[i for i=1:length(sqf) if sqf[i]]
end
function conductors_tame(O::AbsSimpleNumFieldOrder, n::Int, bound::ZZRingElem; unramified_outside::Vector{ZZRingElem} = ZZRingElem[])
if n == 2
return tame_conductors_degree_2(O, bound, unramified_outside = unramified_outside)
end
#
# First, conductors coprime to the ramified primes and to the
# degree of the extension we are searching for.
#
d = degree(O)
K = nf(O)
wild_ram = collect(keys(factor(ZZRingElem(n)).fac))
ram_primes = ramified_primes(O)
filter!(x -> !is_divisible_by(ZZRingElem(n),x), ram_primes)
sort!(ram_primes)
coprime_to = vcat(ram_primes, wild_ram)
m = minimum(wild_ram)
k = divexact(n, m)
e = Int((m-1)*k)
b1 = Int(iroot(bound, degree(O)*e))
list = squarefree_for_conductors(O, b1, n, coprime_to = coprime_to, prime_base = unramified_outside)
extra_list = Tuple{Int, ZZRingElem}[(1, ZZRingElem(1))]
for q in ram_primes
if !isempty(unramified_outside) && !(q in unramified_outside)
continue
end
tr = prime_decomposition_type(O, Int(q))
f = tr[1][1]
nq = q^f
if is_coprime(nq - 1, ZZRingElem(n))
continue
end
nq = nq^(length(tr)*e)
if nq > bound
continue
end
l = length(extra_list)
for i=1:l
no = extra_list[i][2]*nq
if no > bound
continue
end
push!(extra_list, (extra_list[i][1]*q, no))
end
end
final_list = Tuple{Int, ZZRingElem}[]
l = length(list)
e = Int((m-1)*k)
for (el,norm) in extra_list
for i=1:l
if (list[i]^(e*d)) * norm > bound
continue
end
push!(final_list, (list[i]*el, (ZZRingElem(list[i])^(e*d))*norm))
end
end
return final_list
end
function conductors(O::AbsSimpleNumFieldOrder, a::Vector{Int}, bound::ZZRingElem, tame::Bool=false; unramified_outside::Vector{ZZRingElem} = ZZRingElem[])
#Careful: I am assuming that a is in snf!
K = nf(O)
d = degree(O)
n = prod(a)
expo = a[end]
wild_ram = collect(keys(factor(n).fac))
#
# First, conductors for tamely ramified extensions
#
bound_tame = iroot(bound, divexact(n, expo))
list = conductors_tame(O, expo, bound_tame, unramified_outside = unramified_outside)
if tame
reverse!(list)
return Tuple{Int, Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}}[(x[1], Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}()) for x in list]
end
#
# now, we have to multiply the obtained conductors by proper powers of wildly ramified ideals.
#
wild_list = Tuple{Int, Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}, ZZRingElem}[(1, Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}(), ZZRingElem(1))]
for q in wild_ram
if !isempty(unramified_outside) && !(q in unramified_outside)
continue
end
lp = prime_decomposition(O, Int(q))
FqPolyRepFieldElem = divexact(d, lp[1][2]*length(lp))
l = length(wild_list)
sq = q^(divexact(d,lp[1][2])) #norm of the squarefree part of the integer q
#=
we have to use the conductor discriminant formula to understand the maximal possible exponent of q.
Let ap be the exponent of p in the relative discriminant, let m be the conductor and h_(m,C) the cardinality of the
quotient of ray class group by its subgroup C.
Then
ap= v_p(m)h_(m,C)- sum_{i=1:v_p(m)} h_(m/p^i, C)
Since m is the conductor, h_(m/p^i, C)<= h_(m,C)/q.
Consequently, we get
v_p(m)<= (q*ap)/(h_(m,C)*(q-1))
=#
v = valuation(expo, q)
# First, we compute the bound coming from the bound on the discriminant
boundsubext = iroot(bound, Int(divexact(n, q^v))) #The bound on the norm of the discriminant on the subextension
# of order q^v
#Bound coming from the bound on the discriminant
obound = ZZRingElem(flog(boundsubext, sq))
#Bound coming from the analysis on the different in a local extension
nbound = q^v + lp[1][2] * v * q^v - 1
bound_max_ap = min(nbound, obound) #bound on ap
bound_max_exp = div(bound_max_ap, (q-1)*q^(v-1)) #bound on the exponent in the conductor
#Ramification groups bound
max_nontrivial_ramification_group = div(lp[1][2]*(q^v), q-1)
if v > 1
ram_groups_bound = max_nontrivial_ramification_group - sum(q^i for i = 1:v-1) + v
else
ram_groups_bound = max_nontrivial_ramification_group + 1
end
bound_max_exp = min(ram_groups_bound, bound_max_exp)
#The prime may be also tamely ramified!
nisc = gcd(q^(FqPolyRepFieldElem)-1, ZZRingElem(expo))
if nisc != 1
fnisc=minimum(keys(factor(nisc).fac))
nq=sq^((fnisc-1)*(divexact(n, fnisc)))
for s=1:l
nn=nq*wild_list[s][3]
if nn>bound
continue
end
push!(wild_list, (q*wild_list[s][1], wild_list[s][2], nn))
end
end
for i=2:bound_max_exp
d1=Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}()
for j=1:length(lp)
d1[lp[j][1]]=i
end
exp1 = i*(q-1)*divexact(n,q)
nq= sq^(exp1)
for s=1:l
nn=nq*wild_list[s][3]
if nn>bound
continue
end
d2 = merge(max, d1, wild_list[s][2])
if nisc!=1
push!(wild_list, (q*wild_list[s][1], d2, nn))
else
push!(wild_list, (wild_list[s][1], d2, nn))
end
end
end
end
#the final list
final_list=Tuple{Int, Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}}[]
for (el, nm) in list
for (q,d,nm2) in wild_list
if nm*nm2 > bound
continue
end
push!(final_list, (el*q,d))
end
end
reverse!(final_list)
return final_list
end
###############################################################################
#
# Conductors over QQ
#
###############################################################################
function squarefree_for_conductorsQQ(O::AbsSimpleNumFieldOrder, n::Int, a::Vector{Int}; coprime_to::Vector{ZZRingElem}=ZZRingElem[], unramified_outside::Vector{ZZRingElem} = ZZRingElem[])
G = map(Int, snf(abelian_group(a))[1].snf)
sqf= trues(n)
primes= trues(n)
deg = G[end]
#remove primes that can be wildly ramified
for x in coprime_to
if x > n
continue
end
el = Int(x)
t=el
while t <= n
@inbounds sqf[t] = false
@inbounds primes[t] = false
t += el
end
end
single = Vector{Int}()
push!(single, 1)
multiple = Vector{Int}()
#sieving procedure
#First, I can remove all the multiples of 2
if !(2 in coprime_to)
i=2
while i<=length(sqf)
@inbounds sqf[i] = false
i+=2
end
end
i=3
b = isqrt(n)
while i <= b
if primes[i]
if gcd(deg, i-1) == 1 || (!isempty(unramified_outside) && !(i in unramified_outside))
@inbounds primes[i]=false
@inbounds sqf[i]=false
j=i
while j<= n
@inbounds primes[j]=false
@inbounds sqf[j]=false
j+=i
end
else
j=i
while j<= n
@inbounds primes[j]=false
j+=i
end
j=i^2
t=2*j
while j<= n
@inbounds sqf[j]=false
j+=t
end
end
end
i+=2
end
while i<=n
if primes[i]
if gcd(deg,i-1) == 1 || (!isempty(unramified_outside) && !(i in unramified_outside))
@inbounds primes[i] = false
@inbounds sqf[i]=false
j = i
while j <= n
@inbounds sqf[j]=false
j += i
end
end
end
i += 2
end
if length(G) > 1
i = 3
while i <= n
if primes[i]
push!(single, i)
elseif sqf[i]
push!(multiple, i)
end
i += 2
end
elseif !is_prime(deg)
i = 3
while i <= n
if primes[i]
if rem(i-1, deg) == 0
push!(multiple, i)
else
push!(single, i)
end
elseif sqf[i]
push!(multiple, i)
end
i += 2
end
else
multiple = Int[i for i = 2:length(sqf) if sqf[i]]
end
return single, multiple
end
function conductors_tameQQ(O::AbsSimpleNumFieldOrder, a::Vector{Int}, bound::ZZRingElem; unramified_outside::Vector{ZZRingElem} = ZZRingElem[])
#
# First, conductors coprime to the ramified primes and to the
# degree of the extension we are searching for.
#
n = prod(a)
wild_ram = collect(keys(factor(ZZRingElem(n)).fac))
m = minimum(wild_ram)
k = divexact(n, m)
b1 = Int(iroot(ZZRingElem(bound),Int((m-1)*k)))
return squarefree_for_conductorsQQ(O, b1, a, coprime_to = wild_ram, unramified_outside = unramified_outside)
end
function conductorsQQ(O::AbsSimpleNumFieldOrder, a::Vector{Int}, bound::ZZRingElem, tame::Bool=false; unramified_outside::Vector{ZZRingElem} = ZZRingElem[])
K = nf(O)
d = degree(O)
n = prod(a)
expo = a[end]
wild_ram = collect(keys(factor(ZZRingElem(n)).fac))
#
# First, conductors for tamely ramified extensions
#
single, multiple = conductors_tameQQ(O, a, bound, unramified_outside = unramified_outside)
if tame
return multiple
end
#
# now, we have to multiply the obtained conductors by proper powers of wildly ramified ideals.
#
wild_list=Tuple{Int, Int, ZZRingElem}[(1, 1, 1)]
for q in wild_ram
if !isempty(unramified_outside) && !(q in unramified_outside)
continue
end
l = length(wild_list)
#=
we have to use the conductor discriminant formula to understand the maximal possible exponent of q.
Let ap be the exponent of p in the relative discriminant, let m be the conductor and h_(m,C) the cardinality of the
quotient of ray class group by its subgroup C.
Then
ap= v_p(m)h_(m,C)- sum_{i=1:v_p(m)} h_(m/p^i, C)
Since m is the conductor, h_(m/p^i, C)<= h_(m,C)/q.
Consequently, we get
v_p(m)<= (q*ap)/(h_(m,C)*(q-1))
To find ap, it is enough to compute a logarithm.
=#
v = valuation(expo, q)
#I don't need to give a bound for a_p on the big extension but only on the maximum extension of q-power order
#This is the only thing that matters for the exponent of the conductor
nisc = gcd(q-1,n)
nbound = q^v + v * q^v - 1
boundsubext = iroot(bound, Int(divexact(n, q^v)))
obound = flog(boundsubext, q)
nnbound = valuation_bound_discriminant(n, q)
bound_max_ap = min(nbound, obound, nnbound) #bound on ap
bound_max_exp = div(bound_max_ap, (q^(v-1))*(q-1)) #bound on the exponent in the conductor
if q == 2
bound_max_exp = min(bound_max_exp, valuation(expo, q)+2)
else
bound_max_exp = min(bound_max_exp, valuation(expo, q)+1)
end
if nisc != 1
fnisc=minimum(keys(factor(nisc).fac))
nq=ZZRingElem(q)^((fnisc-1)*(divexact(n, fnisc)))
for s=1:l
nn=nq*wild_list[s][3]
if nn>bound
continue
end
push!(wild_list, (q*wild_list[s][1], wild_list[s][2], nn))
end
end
t=(q-1)*divexact(n,q)
for i=2:bound_max_exp
nq= q^(i*t)
for s=1:l
nn=nq*wild_list[s][3]
if nn>bound
continue
end
push!(wild_list, (wild_list[s][1], wild_list[s][2]*q^i, nn))
end
end
end
#the final list
final_list = Int[]
exps = Int((minimum(wild_ram)-1)*divexact(n, minimum(wild_ram)))
for el in multiple
for (q,d,nm2) in wild_list
if (ZZRingElem(el)^exps)*nm2 > bound
continue
end
push!(final_list, (el*q*d))
end
end
for el in single
for j = 2:length(wild_list)
q,d,nm2 = wild_list[j]
if (ZZRingElem(el)^exps)*nm2 > bound
continue
end
push!(final_list, (el*q*d))
end
end
return final_list
end
################################################################################
#
# Conductors generic
#
################################################################################
function conductors_generic(K::AbsSimpleNumField, gtype::Vector{Int}, absolute_bound::ZZRingElem; only_tame::Bool = false)
return conductors_generic(lll(maximal_order(K)), gtype, absolute_bound; only_tame = only_tame)
end
function conductors_generic(OK::AbsSimpleNumFieldOrder, gtype::Vector{Int}, absolute_bound::ZZRingElem; only_tame::Bool = false)
#I am assuming that gtype is in "SNF"
conds_tame = conductors_generic_tame(OK, gtype, absolute_bound)
if only_tame
return Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}[(x[1], Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}()) for x in conds_tame]
end
wild = collect(keys(factor(gtype[end]).fac))
n = prod(gtype)
bound = div(absolute_bound, abs(discriminant(OK))^n)
wild_primes = Vector{Tuple{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, UnitRange{Int}}}()
@vprintln :AbExt 1 "Computing wild conductors ... "
for p in wild
lp = prime_decomposition(OK, p)
for (P, v) in lp
starting_power = 2
ending_power = 2
nP = norm(P)
if nP > bound
continue
end
gn = gcd(nP-1, gtype[end])
if !isone(gn)
starting_power = 1
end
vp = valuation(gtype[end], p)
# First, we compute the bound coming from the bound on the discriminant
boundsubext = iroot(bound, Int(divexact(n, p^vp))) #The bound on the norm of the discriminant on the subextension
# of order q^v
#Bound coming from the bound on the discriminant
obound = flog(boundsubext, nP)
#Bound coming from the analysis on the different in a local extension
nbound = p^vp + v * vp * p^vp - 1
bound_max_ap = min(nbound, obound) #bound on ap
ending_power = Int(div(bound_max_ap, (p-1)*p^(vp-1)))
if ending_power >= starting_power
push!(wild_primes, (P, starting_power:ending_power))
end
end
end
#create now a sublist with just the wild ramified primes.
conds_wild = Vector{Tuple{Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}, ZZRingElem}}()
push!(conds_wild, (Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}(), ZZRingElem(1)))
# For each p in wild_primes, p[2] describes the possible exponent
# range. Of course, not every prime needs to appear, so we add
# 0 to the list of possible exponents.
it = cartesian_product_iterator(Array{Int}[push!(collect(x[2]), 0) for x in wild_primes], inplace = true)
for I in it
if all(x->x<2, I)
# Exclude exponents (0, 0, ..., 0)
# Note that all exponents are >= 2 by if they are nonzero
continue
end
D = Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}()
nD = ZZRingElem(1)
for j = 1:length(I)
if iszero(I[j])
continue
end
P = wild_primes[j][1]
nP = norm(P, copy = false)
p = minimum(P, copy = false)
vp = minimum([valuation(gtype[i], p) for i = 1:length(gtype)])
nD *= nP^((p^vp-p^(vp-1))*I[j])
if nD > bound
break
end
D[P] = I[j]
end
if nD > bound
continue
end
push!(conds_wild, (D, nD))
end
@vprintln :AbExt 1 "... done"
@vprintln :AbExt 1 "Merging tame and wild conductors ..."
#Now, the final merge.
conds = Vector{Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}}()
for i in 1:length(conds_wild)
for j in 1:length(conds_tame)
if conds_wild[i][2]*conds_tame[j][2] <= bound
push!(conds, merge(conds_wild[i][1], conds_tame[j][1]))
end
end
end
@vprintln :AbExt 1 "... done"
return conds
end
function conductors_generic_tame(K::AbsSimpleNumField, gtype::Vector{Int}, absolute_bound::ZZRingElem)
return conductors_generic_tame(lll(maximal_order(K), gtype, absolute_bound))
end
function conductors_generic_tame(OK::AbsSimpleNumFieldOrder, gtype::Vector{Int}, absolute_bound::ZZRingElem)
n = prod(gtype)
wild = collect(keys(factor(n).fac))
pmin = Int(minimum(wild))
bound = div(absolute_bound, abs(discriminant(OK))^n)
@vprintln :AbExt 1 "Tame conductors: Computing prime ideals ... "
lp = prime_ideals_up_to(OK, Int(iroot(bound, pmin-1)))
@vprintln :AbExt 1 "Tame conductors: found $(length(lp)) "
filter!(x -> !(minimum(x, copy = false) in wild), lp)
lf = Vector{Tuple{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, ZZRingElem}}()
dummy = Int[]
for P in lp
nP = norm(P)
gn = gcd(nP-1, gtype[end])
if isone(gn)
continue
end
fgn = factor(gn)
k = minimum(keys(fgn.fac))
kp, cpk = ppio(gtype[end], Int(k))
dP = nP^(div(n, gtype[end])*(k-1)*cpk)
if dP > bound
continue
end
push!(lf, (P, dP))
end
#Now, I have to merge them.
new_conds = Vector{Tuple{Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}, ZZRingElem}}()
# All possible conductors are the squarefree products of the elements in lf with norm bounded
# P1
# P1, P2, P1*P2
# P1, P2, P1*P2, P3, P3*P1, P3*P2, P3*P1*P2
# ...
# We iteratively construct all those products.
# To be efficient, the list must always be ordered.
# Thus we need an ordered list with
# - in-order iteration
# - fast random insertion
# We use a tree to keep track of the indices for the ordering induced by the norm.
# Our AVL implementation cannot handle ordering with are not anti-symmetric
# (We keep track of the indicies, but compare them by comparing the corresponding norm.
# This is not anti-symmetric).
# To cicrumvent this, we keep an array of indices per norm.
conds = Vector{Tuple{Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}, ZZRingElem}}()
push!(conds, (Dict{AbsNumFieldOrderIdeal{AbsSimpleNumField, AbsSimpleNumFieldElem}, Int}(), ZZRingElem(1)))
if isempty(lf)
return conds
end
A = AVLTree{Tuple{Vector{Int}, ZZRingElem}}((i, j) -> i[2] < j[2], (i, j) -> i[2] == j[2])
push!(A, ([1], ZZ(1)))
@vprintln :AbExt 1 "Tame conductors: Computing all tame conductors ..."
for i = 1:length(lf)
empty!(new_conds)
if i % 10000 == 1
@vprintln :AbExt 1 "Tame conductors: ... $(length(lf) - i) left"
end
P = lf[i][1]
dP = lf[i][2]
for j in A
Dd = dP*j[2]
if Dd > bound
break
end
for k in j[1]
D = copy(conds[k][1])
D[P] = 1
push!(new_conds, (D, Dd))
end
end
for j in 1:length(new_conds)
newnorm = !haskey(A, (dummy, new_conds[j][2]))
push!(conds, new_conds[j])
if newnorm
push!(A, ([length(conds)], new_conds[j][2]))
else
node = search_node(A, (dummy, new_conds[j][2]))
@assert node.data[2] == new_conds[j][2]
push!(node.data[1], length(conds))
end
end
end
@vprintln :AbExt 1 "Tame conductors: found $(length(conds))"
sort!(conds, by = x -> x[2])
return conds
end