An elliptic curve is given by a Weierstrass model

y^2 + a_{1} xy + a_{3} y = x^3 + a_{2} x^2 + a_{4} x + a_{6},

whose discriminant is non-zero. Affine points on `E`

are represented as
two-component vectors `[x,y]`

; the point at infinity, i.e. the identity
element of the group law, is represented by the one-component vector
`[0]`

.

Given a vector of coefficients [a_{1},a_{2},a_{3},a_{4},a_{6}], the function
`ellinit`

initializes and returns an *ell* structure. An additional
optional argument allows to specify the base field in case it cannot be
inferred from the curve coefficients. This structure contains data needed by
elliptic curve related functions, and is generally passed as a first argument.
Expensive data are skipped on initialization: they will be dynamically
computed when (and if) needed, and then inserted in the structure. The
precise layout of the *ell* structure is left undefined and should never
be used directly. The following member functions are available,
depending on the underlying domain.

**All domains.**

***** `a1`

, `a2`

, `a3`

, `a4`

, `a6`

: coefficients of the
elliptic curve.

***** `b2`

, `b4`

, `b6`

, `b8`

: b-invariants of the curve; in
characteristic != 2, for Y = 2y + a_1x+a3, the curve equation becomes
Y^2 = 4 x^3 + b_{2} x^2 + 2b_{4} x + b_{6} = : g(x).

***** `c4`

, `c6`

: c-invariants of the curve; in characteristic !=
2,3, for X = x + b_{2}/12 and Y = 2y + a_1x+a3, the curve equation becomes
Y^2 = 4 X^3 - (c_{4}/12) X - (c_{6}/216).

***** `disc`

: discriminant of the curve. This is only required to be
non-zero, not necessarily a unit.

***** `j`

: j-invariant of the curve.

These are used as follows:

? E = ellinit([0,0,0, a4,a6]); ? E.b4 %2 = 2*a4 ? E.disc %3 = -64*a4^3 - 432*a6^2

**Curves over ℂ.**

This in particular includes curves defined over ℚ. All member functions in
this section return data, as it is currently stored in the structure, if
present; and otherwise compute it to the default accuracy, that was fixed
*at the time of ellinit* (via a `t_REAL`

D domain argument, or
`realprecision`

by default). The function `ellperiods`

allows to
recompute (and cache) the following data to *current*
`realprecision`

.

***** `area`

: volume of the complex lattice defining E.

***** `roots`

is a vector whose three components contain the complex
roots of the right hand side g(x) of the attached b-model Y^2 = g(x).
If the roots are all real, they are ordered by decreasing value. If only one
is real, it is the first component.

***** `omega`

: [ω_{1},ω_{2}], periods forming a basis of the
complex lattice defining E. The first component ω_{1} is the
(positive) real period, in other words the integral of the Néron
differential dx/(2y+a_1x+a_{3})
over the connected component of the identity component of E(ℝ).
The second component ω_{2} is a complex period, such that
τ = (ω_{1})/(ω_{2}) belongs to Poincaré's
half-plane (positive imaginary part); not necessarily to the standard
fundamental domain. It is normalized so that Im(ω_{2}) < 0
and either Re(ω_{2}) = 0, when `E.disc > 0`

(E(ℝ) has two connected
components), or Re(ω_{2}) = ω_{1}/2

***** `eta`

is a row vector containing the quasi-periods η_{1} and
η_{2} such that η_{i} = 2ζ(ω_{i}/2), where ζ is the
Weierstrass zeta function attached to the period lattice; see
`ellzeta`

. In particular, the Legendre relation holds: η_{2}ω_{1} -
η_{1}ω_{2} = 2π i.

**Warning.** As for the orientation of the basis of the period lattice,
beware that many sources use the inverse convention where ω_{2}/ω_{1}
has positive imaginary part and our ω_{2} is the negative of theirs. Our
convention τ = ω_{1}/ω_{2} ensures that the action of PSL_{2} is the natural
one:
[a,b;c,d].τ = (aτ+b)/(cτ+d)
= (a ω_{1} + bω_{2})/(cω_{1} + dω_{2}),
instead of a twisted one. (Our tau is -1/τ in the above inverse
convention.)

**Curves over ℚ _{p}.**

We advise to input a model defined over ℚ for such curves. In any case,
if you input an approximate model with `t_PADIC`

coefficients, it will be
replaced by a lift to ℚ (an exact model "close" to the one that was
input) and all quantities will then be computed in terms of this lifted
model.

For the time being only curves with multiplicative reduction (split or
non-split), i.e. v_{p}(j) < 0, are supported by non-trivial functions. In
this case the curve is analytically isomorphic to ℚ_{p}^{*}/q^ℤ :=
E_{q}(ℚ_{p}), for some p-adic integer q (the Tate period). In
particular, we have j(q) = j(E).

***** `p`

is the residual characteristic

***** `roots`

is a vector with a single component, equal to the p-adic
root e_{1} of the right hand side g(x) of the attached b-model Y^2
= g(x). The point (e_{1},0) corresponds to -1 ∈ ℚ_{p}^{*}/q^ℤ
under the Tate parametrization.

***** `tate`

returns [u^2,u,q,[a,b],L, Ei] in the notation of Henniart-Mestre
(CRAS t. 308, p. 391--395, 1989): q is as above, u ∈ ℚ_{p}(sqrt{-c_{6}})
is such that φ^{*} dx/(2y + a_1x+a3) = u dt/t, where φ: E_{q} → E
is an isomorphism (well defined up to sign) and dt/t is the canonical
invariant differential on the Tate curve; u^2 ∈ ℚ_{p} does not depend on
φ. (Technicality: if u ∉ ℚ_{p}, it is stored as a quadratic
`t_POLMOD`

.)
The parameters [a,b] satisfy 4u^2 b.agm(sqrt{a/b},1)^2 = 1
as in Theorem 2 (*loc. cit.*).
`Ei`

describes the sequence of 2-isogenous curves (with kernel generated
by [0,0]) E_{i}: y^2 = x(x+A_{i})(x+A_{i}-B_{i}) converging quadratically towards
the singular curve E_ oo . Finally, L is Mazur-Tate-Teitelbaum's
ℒ-invariant, equal to log_{p} q / v_{p}(q).

**Curves over 𝔽 _{q}.**

***** `p`

is the characteristic of 𝔽_{q}.

***** `no`

is #E(𝔽_{q}).

***** `cyc`

gives the cycle structure of E(𝔽_{q}).

***** `gen`

returns the generators of E(𝔽_{q}).

***** `group`

returns [`no`

,`cyc`

,`gen`

], i.e. E(𝔽_{q})
as an abelian group structure.

**Curves over ℚ.**

All functions should return a correct result, whether the model is minimal or
not, but it is a good idea to stick to minimal models whenever
gcd(c_{4},c_{6}) is easy to factor (minor speed-up). The construction

E = ellminimalmodel(E0, &v)

replaces the original model E_{0} by a minimal model E,
and the variable change v allows to go between the two models:

ellchangepoint(P0, v) ellchangepointinv(P, v)

respectively map the point P_{0} on E_{0} to its image on
E, and the point P on E to its pre-image on E_{0}.

A few routines — namely `ellgenerators`

, `ellidentify`

,
`ellsearch`

, `forell`

— require the optional package `elldata`

(John Cremona's database) to be installed. In that case, the function
`ellinit`

will allow alternative inputs, e.g. `ellinit("11a1")`

.
Functions using this package need to load chunks of a large database in
memory and require at least 2MB stack to avoid stack overflows.

***** `gen`

returns the generators of E(ℚ), if known (from John
Cremona's database)

**Curves over number fields.**

***** `nf`

return the *nf* structure attached to the number field
over which E is defined.

***** `bnf`

return the *bnf* structure attached to the number field
over which E is defined or raise an error (if only an *nf* is available).

***** `omega`

, `eta`

, `area`

: vectors of complex periods,
quasi-periods and lattice areas attached to the complex embeddings of E,
in the same order as `E.nf.roots`

.

Let E be a curve defined over ℚ_{p} given by a p-integral model;
if the curve has good reduction at p, we may define its reduction
~{E} over the finite field 𝔽_{p}:

? E = ellinit([-3,1], O(5^10)); \\ E/ℚ_{5}? Et = ellinit(E, 5) ? ellcard(Et) \\ ~{E}/𝔽_{5}has 7 points %3 = 7 ? ellinit(E, 7) *** at top-level: ellinit(E,7) *** ^ — — — — *** ellinit: inconsistent moduli in ellinit: 5 != 7

Likewise, if a curve is defined over a number field K and 𝔭 is a
maximal ideal with finite residue field 𝔽_{q}, we define the reduction
~{E}/𝔽_{q} provided E has good reduction at 𝔭.
E/ℚ is an important special case:

? E = ellinit([-3,1]); ? factor(E.disc) %2 = [2 4] [3 4] ? Et = ellinit(E, 5); ? ellcard(Et) \\ ~{E} / 𝔽_{5}has 7 points %4 = 7 ? ellinit(E, 3) \\ bad reduction at 3 %5 = []

General number fields are similar:

? K = nfinit(x^2+1); E = ellinit([x,x+1], K); ? idealfactor(K, E.disc) \\ three primes of bad reduction %2 = [ [2, [1, 1]~, 2, 1, [1, -1; 1, 1]] 10] [ [5, [-2, 1]~, 1, 1, [2, -1; 1, 2]] 2] [[5, [2, 1]~, 1, 1, [-2, -1; 1, -2]] 2] ? P = idealprimedec(K, 3); \\ a prime of good reduction ? idealnorm(K, P) %4 = 9 ? Et = ellinit(E, P); ? ellcard(Et) \\ ~{E} / 𝔽_{9}has 4 points %6 = 4

If the model is not locally minimal at 𝔭, the above will fail:
`elllocalred`

and `ellchangecurve`

allow to reduce to that case.

Some functions such as `ellap`

, `ellcard`

, `ellgroup`

and
`ellissupersingular`

even implicitly replace the given equation by
a local minimal model and consider the group of non-singular points
~{E}^{ns} so they make sense even when the curve has bad reduction.

Returns the value at s = 1 of the derivative of order r of the L-function of the elliptic curve E.

? E = ellinit("11a1"); \\ order of vanishing is 0 ? ellL1(E) %2 = 0.2538418608559106843377589233 ? E = ellinit("389a1"); \\ order of vanishing is 2 ? ellL1(E) %4 = -5.384067311837218089235032414 E-29 ? ellL1(E, 1) %5 = 0 ? ellL1(E, 2) %6 = 1.518633000576853540460385214

The main use of this function, after computing at *low* accuracy the
order of vanishing using `ellanalyticrank`

, is to compute the
leading term at *high* accuracy to check (or use) the Birch and
Swinnerton-Dyer conjecture:

? \p18 realprecision = 18 significant digits ? E = ellinit("5077a1"); ellanalyticrank(E) time = 8 ms. %1 = [3, 10.3910994007158041] ? \p200 realprecision = 202 significant digits (200 digits displayed) ? ellL1(E, 3) time = 104 ms. %3 = 10.3910994007158041387518505103609170697263563756570092797 [...]

The library syntax is `GEN `

.**ellL1_bitprec**(GEN E, long r, long bitprec)

Sum of the points z1 and z2 on the elliptic curve corresponding to E.

The library syntax is `GEN `

.**elladd**(GEN E, GEN z1, GEN z2)

Computes the coefficient a_{n} of the L-function of the elliptic curve
E/ℚ, i.e. coefficients of a newform of weight 2 by the modularity theorem
(Taniyama-Shimura-Weil conjecture). E must be an `ell`

structure
over ℚ as output by `ellinit`

. E must be given by an integral model,
not necessarily minimal, although a minimal model will make the function
faster.

? E = ellinit([1,-1,0,4,3]); ? ellak(E, 10) %2 = -3 ? e = ellchangecurve(E, [1/5,0,0,0]); \\ made not minimal at 5 ? ellak(e, 10) \\ wasteful but works %3 = -3 ? E = ellminimalmodel(e); \\ now minimal ? ellak(E, 5) %5 = -3

If the model is not minimal at a number of bad primes, then the function will be slower on those n divisible by the bad primes. The speed should be comparable for other n:

? for(i=1,10^6, ellak(E,5)) time = 699 ms. ? for(i=1,10^6, ellak(e,5)) \\ 5 is bad, markedly slower time = 1,079 ms. ? for(i=1,10^5,ellak(E,5*i)) time = 1,477 ms. ? for(i=1,10^5,ellak(e,5*i)) \\ still slower but not so much on average time = 1,569 ms.

The library syntax is `GEN `

.**akell**(GEN E, GEN n)

Computes the vector of the first n Fourier coefficients a_{k}
corresponding to the elliptic curve E defined over a number field.
If E is defined over ℚ, the curve may be given by an
arbitrary model, not necessarily minimal,
although a minimal model will make the function faster. Over a more general
number field, the model must be locally minimal at all primes above 2
and 3.

The library syntax is `GEN `

.
Also available is **ellan**(GEN E, long n)`GEN `

, which
returns a **ellanQ_zv**(GEN e, long n)`t_VECSMALL`

instead of a `t_VEC`

, saving on memory.

Returns the order of vanishing at s = 1 of the L-function of the
elliptic curve E and the value of the first non-zero derivative. To
determine this order, it is assumed that any value less than `eps`

is
zero. If `eps`

is omitted, 2^{-b/2} is used, where b
is the current bit precision.

? E = ellinit("11a1"); \\ rank 0 ? ellanalyticrank(E) %2 = [0, 0.2538418608559106843377589233] ? E = ellinit("37a1"); \\ rank 1 ? ellanalyticrank(E) %4 = [1, 0.3059997738340523018204836835] ? E = ellinit("389a1"); \\ rank 2 ? ellanalyticrank(E) %6 = [2, 1.518633000576853540460385214] ? E = ellinit("5077a1"); \\ rank 3 ? ellanalyticrank(E) %8 = [3, 10.39109940071580413875185035]

The library syntax is `GEN `

.**ellanalyticrank_bitprec**(GEN E, GEN eps = NULL, long bitprec)

Let `E`

be an `ell`

structure as output by `ellinit`

, attached
to an elliptic curve E/K. If the field K = 𝔽_{q} is finite, return the
trace of Frobenius t, defined by the equation #E(𝔽_{q}) = q+1 - t.

For other fields of definition and p defining a finite residue field
𝔽_{q}, return the trace of Frobenius for the reduction of E: the argument
p is best left omitted if K = ℚ_ℓ (else we must have p = ℓ) and
must be a prime number (K = ℚ) or prime ideal (K a general number field)
with residue field 𝔽_{q} otherwise. The equation need not be minimal
or even integral at p; of course, a minimal model will be more efficient.

For a number field K, the trace of Frobenius is the a_{p}
coefficient in the Euler product defining the curve L-series, whence
the function name:
L(E/K,s) = ∏_{bad p} (1-a_{p} (Np)^{-s})^{-1}
∏_{good p} (1-a_{p} (Np)^{-s} + (Np)^{1-2s})^{-1}.

When the characteristic of the finite field is large, the availability of
the `seadata`

package will speed up the computation.

? E = ellinit([0,1]); \\ y^2 = x^3 + 0.x + 1, defined over Q ? ellap(E, 7) \\ 7 necessary here %2 = -4 \\ #E(F_{7}) = 7+1-(-4) = 12 ? ellcard(E, 7) %3 = 12 \\ OK ? E = ellinit([0,1], 11); \\ defined over F_11 ? ellap(E) \\ no need to repeat 11 %4 = 0 ? ellap(E, 11) \\ ... but it also works %5 = 0 ? ellgroup(E, 13) \\ ouch, inconsistent input! *** at top-level: ellap(E,13) *** ^ — — — -- *** ellap: inconsistent moduli in Rg_to_Fp: 11 13 ? a = ffgen(ffinit(11,3), 'a); \\ defines F_{q}:= F_{11^3}? E = ellinit([a+1,a]); \\ y^2 = x^3 + (a+1)x + a, defined over F_{q}? ellap(E) %8 = -3

If the curve is defined over a more general number field than ℚ,
the maximal ideal p must be explicitly given in `idealprimedec`

format. There is no assumption of local minimality at p.

? K = nfinit(a^2+1); E = ellinit([1+a,0,1,0,0], K); ? fa = idealfactor(K, E.disc) %2 = [ [5, [-2, 1]~, 1, 1, [2, -1; 1, 2]] 1] [[13, [5, 1]~, 1, 1, [-5, -1; 1, -5]] 2] ? ellap(E, fa[1,1]) %3 = -1 \\ non-split multiplicative reduction ? ellap(E, fa[2,1]) %4 = 1 \\ split multiplicative reduction ? P17 = idealprimedec(K,17)[1]; ? ellap(E, P17) %6 = 6 \\ good reduction ? E2 = ellchangecurve(E, [17,0,0,0]); ? ellap(E2, P17) %8 = 6 \\ same, starting from a non-miminal model ? P3 = idealprimedec(K,3)[1]; ? ellap(E, P3) \\ OK: E is minimal at P3 %10 = -2 ? E3 = ellchangecurve(E, [3,0,0,0]); ? ellap(E3, P3) \\ not integral at P3 *** at top-level: ellap(E3,P3) *** ^ — — — — *** ellap: impossible inverse in Rg_to_ff: Mod(0, 3).

**Algorithms used.** If E/𝔽_{q} has CM by a principal imaginary
quadratic order we use a fast explicit formula (involving essentially
Kronecker symbols and Cornacchia's algorithm), in O(log q)^2 bit
operations.
Otherwise, we use Shanks-Mestre's baby-step/giant-step method, which runs in
time Õ(q^{1/4}) using Õ(q^{1/4}) storage, hence becomes
unreasonable when q has about 30 digits. Above this range, the `SEA`

algorithm becomes available, heuristically in Õ(log q)^4, and
primes of the order of 200 digits become feasible. In small
characteristic we use Mestre's (p = 2), Kohel's (p = 3,5,7,13), Satoh-Harley
(all in Õ(p^{2} n^2)) or Kedlaya's (in Õ(p n^3))
algorithms.

The library syntax is `GEN `

.**ellap**(GEN E, GEN p = NULL)

Deprecated alias for `ellheight(E,P,Q)`

.

The library syntax is `GEN `

.**bilhell**(GEN E, GEN z1, GEN z2, long prec)

The object E being an elliptic curve over a number field, returns a real
number c such that the BSD conjecture predicts that
L_{E}^{(r)}(1)/r != c R S where r is the rank, R the regulator and
S the cardinal of the Tate-Shafarevich group.

? e = ellinit([0,-1,1,-10,-20]); \\ rank 0 ? ellbsd(e) %2 = 0.25384186085591068433775892335090946105 ? lfun(e,1) %3 = 0.25384186085591068433775892335090946104 ? e = ellinit([0,0,1,-1,0]); \\ rank 1 ? P = ellheegner(e); ? ellbsd(e)*ellheight(e,P) %6 = 0.30599977383405230182048368332167647445 ? lfun(e,1,1) %7 = 0.30599977383405230182048368332167647445 ? e = ellinit([1+a,0,1,0,0],nfinit(a^2+1)); \\ rank 0 ? ellbsd(e) %9 = 0.42521832235345764503001271536611593310 ? lfun(e,1) %10 = 0.42521832235345764503001271536611593309

The library syntax is `GEN `

.**ellbsd**(GEN E, long prec)

Let `E`

be an `ell`

structure as output by `ellinit`

, attached
to an elliptic curve E/K. If K = 𝔽_{q} is finite, return the order of the
group E(𝔽_{q}).

? E = ellinit([-3,1], 5); ellcard(E) %1 = 7 ? t = ffgen(3^5,'t); E = ellinit([t,t^2+1]); ellcard(E) %2 = 217

For other fields of definition and p defining a finite residue field
𝔽_{q}, return the order of the reduction of E: the argument p is best
left omitted if K = ℚ_ℓ (else we must have p = ℓ) and must be a
prime number (K = ℚ) or prime ideal (K a general number field) with
residue field 𝔽_{q} otherwise. The equation need not be minimal
or even integral at p; of course, a minimal model will be more efficient.
The function considers the group of non-singular points of the reduction
of a minimal model of the curve at p, so also makes sense when the curve
has bad reduction.

? E = ellinit([-3,1]); ? factor(E.disc) %2 = [2 4] [3 4] ? ellcard(E, 5) \\ as above ! %3 = 7 ? ellcard(E, 2) \\ additive reduction %4 = 2

When the characteristic of the finite field is large, the availability of
the `seadata`

package will speed the computation. See also `ellap`

for the list of implemented algorithms.

The library syntax is `GEN `

.
Also available is **ellcard**(GEN E, GEN p = NULL)`GEN `

where p is not
**ellcard**(GEN E, GEN p)`NULL`

.

Changes the data for the elliptic curve E
by changing the coordinates using the vector `v = [u,r,s,t]`

, i.e. if x'
and y' are the new coordinates, then x = u^2x'+r, y = u^3y'+su^2x'+t.
E must be an `ell`

structure as output by `ellinit`

. The special
case v = 1 is also used instead of [1,0,0,0] to denote the
trivial coordinate change.

The library syntax is `GEN `

.**ellchangecurve**(GEN E, GEN v)

Changes the coordinates of the point or
vector of points x using the vector `v = [u,r,s,t]`

, i.e. if x' and
y' are the new coordinates, then x = u^2x'+r, y = u^3y'+su^2x'+t (see also
`ellchangecurve`

).

? E0 = ellinit([1,1]); P0 = [0,1]; v = [1,2,3,4]; ? E = ellchangecurve(E0, v); ? P = ellchangepoint(P0,v) %3 = [-2, 3] ? ellisoncurve(E, P) %4 = 1 ? ellchangepointinv(P,v) %5 = [0, 1]

The library syntax is `GEN `

.
The reciprocal function **ellchangepoint**(GEN x, GEN v)`GEN `

inverts the coordinate change.**ellchangepointinv**(GEN x, GEN ch)

Changes the coordinates of the point or vector of points x using
the inverse of the isomorphism attached to `v = [u,r,s,t]`

,
i.e. if x' and y' are the old coordinates, then x = u^2x'+r,
y = u^3y'+su^2x'+t (inverse of `ellchangepoint`

).

? E0 = ellinit([1,1]); P0 = [0,1]; v = [1,2,3,4]; ? E = ellchangecurve(E0, v); ? P = ellchangepoint(P0,v) %3 = [-2, 3] ? ellisoncurve(E, P) %4 = 1 ? ellchangepointinv(P,v) %5 = [0, 1] \\ we get back P0

The library syntax is `GEN `

.**ellchangepointinv**(GEN x, GEN v)

Converts an elliptic curve name, as found in the `elldata`

database,
from a string to a triplet [*conductor*, *isogeny class*,
*index*]. It will also convert a triplet back to a curve name.
Examples:

? ellconvertname("123b1") %1 = [123, 1, 1] ? ellconvertname(%) %2 = "123b1"

The library syntax is `GEN `

.**ellconvertname**(GEN name)

n-division polynomial f_{n} for the curve E in the
variable v. In standard notation, for any affine point P = (X,Y) on the
curve, we have
[n]P = (φ_{n}(P)ψ_{n}(P) : ω_{n}(P) : ψ_{n}(P)^3)
for some polynomials φ_{n},ω_{n},ψ_{n} in
ℤ[a_{1},a_{2},a_{3},a_{4},a_{6}][X,Y]. We have f_{n}(X) = ψ_{n}(X) for n odd, and
f_{n}(X) = ψ_{n}(X,Y) (2Y + a_1X+a_{3}) for n even. We have
f_{1} = 1, f_{2} = 4X^3 + b_2X^2 + 2b_{4} X + b_{6}, f_{3} = 3 X^4 + b_{2} X^3 + 3b_{4} X^2 + 3 b_{6} X + b8,
f_{4} = f_{2}(2X^6 + b_{2} X^5 + 5b_{4} X^4 + 10 b_{6} X^3 + 10 b_{8} X^2 +
(b_2b_{8}-b_4b_{6})X + (b_8b_{4} - b_{6}^2)),...
For n ≥ 2, the roots of f_{n} are the X-coordinates of points in E[n].

The library syntax is `GEN `

where **elldivpol**(GEN E, long n, long v = -1)`v`

is a variable number.

k being an even positive integer, computes the numerical value of the
Eisenstein series of weight k at the lattice w, as given by
`ellperiods`

, namely

(2i π/ω_{2})^k
(1 + 2/ζ(1-k) ∑_{n ≥ 1} n^{k-1}q^n / (1-q^n)),

where q = exp(2iπ τ) and τ := ω_{1}/ω_{2} belongs to the
complex upper half-plane. It is also possible to directly input w =
[ω_{1},ω_{2}], or an elliptic curve E as given by `ellinit`

.

? w = ellperiods([1,I]); ? elleisnum(w, 4) %2 = 2268.8726415508062275167367584190557607 ? elleisnum(w, 6) %3 = -3.977978632282564763 E-33 ? E = ellinit([1, 0]); ? elleisnum(E, 4, 1) %5 = -47.999999999999999999999999999999999998

When *flag* is non-zero and k = 4 or 6, returns the elliptic invariants g_{2}
or g_{3}, such that
y^2 = 4x^3 - g_{2} x - g_{3}
is a Weierstrass equation for E.

The library syntax is `GEN `

.**elleisnum**(GEN w, long k, long flag, long prec)

Returns the quasi-periods [η_{1},η_{2}]
attached to the lattice basis *w* = [ω_{1}, ω_{2}].
Alternatively, *w* can be an elliptic curve E as output by
`ellinit`

, in which case, the quasi periods attached to the period
lattice basis `E.omega`

(namely, `E.eta`

) are returned.

? elleta([1, I]) %1 = [3.141592653589793238462643383, 9.424777960769379715387930149*I]

The library syntax is `GEN `

.**elleta**(GEN w, long prec)

Let ω := dx / (2y+a_1x+a_{3}) be the invariant differential form
attached to the model E of some elliptic curve (`ellinit`

form),
and η := x(t)ω. Return n terms (`seriesprecision`

by default)
of f(t),g(t) two power series in the formal parameter t = -x/y such that
ω = f(t) dt, η = g(t) dt:
f(t) = 1+a_{1} t + (a_{1}^2 + a_{2}) t^2 +...,
g(t) = t^{-2} +...

? E = ellinit([-1,1/4]); [f,g] = ellformaldifferential(E,7,'t); ? f %2 = 1 - 2*t^4 + 3/4*t^6 + O(t^7) ? g %3 = t^-2 - t^2 + 1/2*t^4 + O(t^5)

The library syntax is `GEN `

where **ellformaldifferential**(GEN E, long precdl, long n = -1)`n`

is a variable number.

The elliptic formal exponential `Exp`

attached to E is the
isomorphism from the formal additive law to the formal group of E. It is
normalized so as to be the inverse of the elliptic logarithm (see
`ellformallog`

): `Exp`

o L = Id. Return n terms of this
power series:

? E=ellinit([-1,1/4]); Exp = ellformalexp(E,10,'z) %1 = z + 2/5*z^5 - 3/28*z^7 + 2/15*z^9 + O(z^11) ? L = ellformallog(E,10,'t); ? subst(Exp,z,L) %3 = t + O(t^11)

The library syntax is `GEN `

where **ellformalexp**(GEN E, long precdl, long n = -1)`n`

is a variable number.

The formal elliptic logarithm is a series L in t K[[t]]
such that d L = ω = dx / (2y + a_1x + a_{3}), the canonical invariant
differential attached to the model E. It gives an isomorphism
from the formal group of E to the additive formal group.

? E = ellinit([-1,1/4]); L = ellformallog(E, 9, 't) %1 = t - 2/5*t^5 + 3/28*t^7 + 2/3*t^9 + O(t^10) ? [f,g] = ellformaldifferential(E,8,'t); ? L' - f %3 = O(t^8)

The library syntax is `GEN `

where **ellformallog**(GEN E, long precdl, long n = -1)`n`

is a variable number.

If E is an elliptic curve, return the coordinates x(t), y(t) in the
formal group of the elliptic curve E in the formal parameter t = -x/y
at oo :
x = t^{-2} -a_{1} t^{-1} - a_{2} - a_{3} t +...
y = - t^{-3} -a_{1} t^{-2} - a_2t^{-1} -a_{3} +...
Return n terms (`seriesprecision`

by default) of these two power
series, whose coefficients are in ℤ[a_{1},a_{2},a_{3},a_{4},a_{6}].

? E = ellinit([0,0,1,-1,0]); [x,y] = ellformalpoint(E,8,'t); ? x %2 = t^-2 - t + t^2 - t^4 + 2*t^5 + O(t^6) ? y %3 = -t^-3 + 1 - t + t^3 - 2*t^4 + O(t^5) ? E = ellinit([0,1/2]); ellformalpoint(E,7) %4 = [x^-2 - 1/2*x^4 + O(x^5), -x^-3 + 1/2*x^3 + O(x^4)]

The library syntax is `GEN `

where **ellformalpoint**(GEN E, long precdl, long n = -1)`n`

is a variable number.

Return the formal power series w attached to the elliptic curve E,
in the variable t:
w(t) = t^3 + a_{1} t^4 + (a_{2} + a_{1}^2) t^5 +...+ O(t^{n+3}),
which is the formal expansion of -1/y in the formal parameter t := -x/y
at oo (take n = `seriesprecision`

if n is omitted). The
coefficients of w belong to ℤ[a_{1},a_{2},a_{3},a_{4},a_{6}].

? E=ellinit([3,2,-4,-2,5]); ellformalw(E, 5, 't) %1 = t^3 + 3*t^4 + 11*t^5 + 35*t^6 + 101*t^7 + O(t^8)

The library syntax is `GEN `

where **ellformalw**(GEN E, long precdl, long n = -1)`n`

is a variable number.

Given a genus 1 plane curve, defined by the affine equation f(x,y) = 0,
return the coefficients [a_{1},a_{2},a_{3},a_{4},a_{6}] of a Weierstrass equation
for its Jacobian. This allows to recover a Weierstrass model for an elliptic
curve given by a general plane cubic or by a binary quartic or biquadratic
model. The function implements the f ` ⟼ `

f^{*} formulae of Artin, Tate
and Villegas (Advances in Math. 198 (2005), pp. 366--382).

In the example below, the function is used to convert between twisted Edwards coordinates and Weierstrass coordinates.

? e = ellfromeqn(a*x^2+y^2 - (1+d*x^2*y^2)) %1 = [0, -a - d, 0, -4*d*a, 4*d*a^2 + 4*d^2*a] ? E = ellinit(ellfromeqn(y^2-x^2 - 1 +(121665/121666*x^2*y^2)),2^255-19); ? isprime(ellcard(E) / 8) %3 = 1

The elliptic curve attached to the sum of two cubes is given by

? ellfromeqn(x^3+y^3 - a) %1 = [0, 0, -9*a, 0, -27*a^2]

**Congruent number problem:.**
Let n be an integer, if a^2+b^2 = c^2 and a b = 2 n,
then by substituting b by 2 n/a in the first equation,
we get ((a^2+(2 n/a)^2)-c^2) a^2 = 0.
We set x = a, y = a c.

? En = ellfromeqn((x^2 + (2*n/x)^2 - (y/x)^2)*x^2) %1 = [0, 0, 0, -16*n^2, 0]

For example 23 is congruent since the curve has a point of infinite order, namely:

? ellheegner( ellinit(subst(En, n, 23)) ) %2 = [168100/289, 68053440/4913]

The library syntax is `GEN `

.**ellfromeqn**(GEN P)

Returns the coefficients [a_{1},a_{2},a_{3},a_{4},a_{6}] of a fixed elliptic curve
with j-invariant j.

The library syntax is `GEN `

.**ellfromj**(GEN j)

If E is an elliptic curve over the rationals, return a ℤ-basis of the
free part of the Mordell-Weil group attached to E. This relies on
the `elldata`

database being installed and referencing the curve, and so
is only available for curves over ℤ of small conductors.
If E is an elliptic curve over a finite field 𝔽_{q} as output by
`ellinit`

, return a minimal set of generators for the group E(𝔽_{q}).

**Caution.** When the group is not cyclic, of shape ℤ/d_{1}ℤ x
ℤ/d_{2}ℤ with d_{2} | d_{1}, the points [P,Q] returned by ellgenerators
need not have order d_{1} and d_{2}: it is true that
P has order d_{1}, but we only know that Q is a generator of
E(𝔽_{q})/ <P> and that the Weil pairing w(P,Q) has order d_{2},
see `??ellgroup`

.
If you need generators [P,R] with R of order d_{2}, find
x such that R = Q-[x]P has order d_{2} by solving
the discrete logarithm problem [d_{2}]Q = [x]([d_{2}]P) in a cyclic group of
order d_{1}/d_{2}. This will be very expensive if d_{1}/d_{2} has a large
prime factor.

The library syntax is `GEN `

.**ellgenerators**(GEN E)

Let E be an `ell`

structure as output by `ellinit`

attached
to an elliptic curve defined over a number field. This function calculates
the arithmetic conductor and the global Tamagawa number c.
The result [N,v,c,F,L] is slightly different if E is defined
over ℚ (domain D = 1 in `ellinit`

) or over a number field
(domain D is a number field structure, including `nfinit(x)`

representing ℚ !):

***** N is the arithmetic conductor of the curve,

***** v is an obsolete field, left in place for backward compatibility.
If E is defined over ℚ, v gives the coordinate change for E to the
standard minimal integral model (`ellminimalmodel`

provides it in a
cheaper way); if E is defined over another number field, v gives a
coordinate change to an integral model (`ellintegralmodel`

provides it
in a cheaper way).

***** c is the product of the local Tamagawa numbers c_{p}, a quantity
which enters in the Birch and Swinnerton-Dyer conjecture,

***** F is the factorization of N,

***** L is a vector, whose i-th entry contains the local data
at the i-th prime ideal divisor of N, i.e.
`L[i] = elllocalred(E,F[i,1])`

. If E is defined over ℚ, the local
coordinate change has been deleted and replaced by a 0; if E is defined
over another number field the local coordinate change to a local minimal
model is given relative to the integral model afforded by v (so either
start from an integral model so that v be trivial, or apply v first).

The library syntax is `GEN `

.**ellglobalred**(GEN E)

Let `E`

be an `ell`

structure as output by `ellinit`

, attached
to an elliptic curve E/K. We first describle the function when the field
K = 𝔽_{q} is finite, it computes the structure of the finite abelian group
E(𝔽_{q}):

***** if *flag* = 0, return the structure [] (trivial group) or [d_{1}]
(non-trivial cyclic group) or [d_{1},d_{2}] (non-cyclic group) of
E(𝔽_{q}) ~ ℤ/d_{1}ℤ x ℤ/d_{2}ℤ, with d_{2} | d_{1}.

***** if *flag* = 1, return a triple [h,*cyc*,*gen*], where
h is the curve cardinality, *cyc* gives the group structure as a
product of cyclic groups (as per *flag* = 0). More precisely, if d_{2} > 1,
the output is [d_1d_{2}, [d_{1},d_{2}], [P,Q]] where P is
of order d_{1} and [P,Q] generates the curve.
**Caution.** It is not guaranteed that Q has order d_{2}, which in
the worst case requires an expensive discrete log computation. Only that
`ellweilpairing`

(E, P, Q, d_{1}) has order d_{2}.

For other fields of definition and p defining a finite residue field
𝔽_{q}, return the structure of the reduction of E: the argument
p is best left omitted if K = ℚ_ℓ (else we must have p = ℓ) and
must be a prime number (K = ℚ) or prime ideal (K a general number field)
with residue field 𝔽_{q} otherwise. The curve is allowed to have bad
reduction at p and in this case we consider the (cyclic) group of
non-singular points for the reduction of a minimal model at p.

If *flag* = 0, the equation not be minimal or even integral at p; of course,
a minimal model will be more efficient.

If *flag* = 1, the requested generators depend on the model, which must then
be minimal at p, otherwise an exception is thrown. Use
`ellintegralmodel`

and/or `ellocalred`

first to reduce to this case.

? E = ellinit([0,1]); \\ y^2 = x^3 + 0.x + 1, defined over Q ? ellgroup(E, 7) %2 = [6, 2] \\ Z/6 x Z/2, non-cyclic ? E = ellinit([0,1] * Mod(1,11)); \\ defined over F_11 ? ellgroup(E) \\ no need to repeat 11 %4 = [12] ? ellgroup(E, 11) \\ ... but it also works %5 = [12] ? ellgroup(E, 13) \\ ouch, inconsistent input! *** at top-level: ellgroup(E,13) *** ^ — — — — -- *** ellgroup: inconsistent moduli in Rg_to_Fp: 11 13 ? ellgroup(E, 7, 1) %6 = [12, [6, 2], [[Mod(2, 7), Mod(4, 7)], [Mod(4, 7), Mod(4, 7)]]]

Let us now consider curves of bad reduction, in this case we return the
structure of the (cyclic) group of non-singular points, satisfying
#E_{ns}(𝔽_{p}) = p - a_{p}:

? E = ellinit([0,5]); ? ellgroup(E, 5, 1) %2 = [5, [5], [[Mod(4, 5), Mod(2, 5)]]] ? ellap(E, 5) %3 = 0 \\ additive reduction at 5 ? E = ellinit([0,-1,0,35,0]); ? ellgroup(E, 5, 1) %5 = [4, [4], [[Mod(2, 5), Mod(2, 5)]]] ? ellap(E, 5) %6 = 1 \\ split multiplicative reduction at 5 ? ellgroup(E, 7, 1) %7 = [8, [8], [[Mod(3, 7), Mod(5, 7)]]] ? ellap(E, 7) %8 = -1 \\ non-split multiplicative reduction at 7

The library syntax is `GEN `

.
Also available is **ellgroup0**(GEN E, GEN p = NULL, long flag)`GEN `

, corresponding
to **ellgroup**(GEN E, GEN p)*flag* = 0.

Let E be an elliptic curve over the rationals, assumed to be of (analytic) rank 1. This returns a non-torsion rational point on the curve, whose canonical height is equal to the product of the elliptic regulator by the analytic Sha.

This uses the Heegner point method, described in Cohen GTM 239; the complexity is proportional to the product of the square root of the conductor and the height of the point (thus, it is preferable to apply it to strong Weil curves).

? E = ellinit([-157^2,0]); ? u = ellheegner(E); print(u[1], "\n", u[2]) 69648970982596494254458225/166136231668185267540804 538962435089604615078004307258785218335/67716816556077455999228495435742408 ? ellheegner(ellinit([0,1])) \\ E has rank 0 ! *** at top-level: ellheegner(E=ellinit *** ^ — — — — — — -- *** ellheegner: The curve has even analytic rank.

The library syntax is `GEN `

.**ellheegner**(GEN E)

Let E be an elliptic curve defined over K = ℚ or a number field,
as output by `ellinit`

; it needs not be given by a minimal model
although the computation will be faster if it is.

***** Without arguments P,Q, returns the Faltings height of the curve E
using Deligne normalization. For a rational curve, the normalization is such
that the function returns `-(1/2)*log(ellminimalmodel(E).area)`

.

***** If the argument P ∈ E(K) is present, returns the global
Néron-Tate height h(P) of the point, using the normalization in
Cremona's *Algorithms for modular elliptic curves*.

***** If the argument Q ∈ E(K) is also present, computes the value of
the bilinear form (h(P+Q)-h(P-Q)) / 4.

The library syntax is `GEN `

.
Also available is **ellheight0**(GEN E, GEN P = NULL, GEN Q = NULL, long prec)`GEN `

(Q omitted).**ellheight**(GEN E, GEN P, long prec)

x being a vector of points, this
function outputs the Gram matrix of x with respect to the Néron-Tate
height, in other words, the (i,j) component of the matrix is equal to
`ellbil(E,x[i],x[j])`

. The rank of this matrix, at least in some
approximate sense, gives the rank of the set of points, and if x is a
basis of the Mordell-Weil group of E, its determinant is equal to
the regulator of E. Note our height normalization follows Cremona's
*Algorithms for modular elliptic curves*: this matrix should be divided
by 2 to be in accordance with, e.g., Silverman's normalizations.

The library syntax is `GEN `

.**ellheightmatrix**(GEN E, GEN x, long prec)

Look up the elliptic curve E, defined by an arbitrary model over ℚ,
in the `elldata`

database.
Return `[[N, M, G], C]`

where N is the curve name in Cremona's
elliptic curve database, M is the minimal model, G is a ℤ-basis of
the free part of the Mordell-Weil group E(ℚ) and C is the
change of coordinates from E to M, suitable for `ellchangecurve`

.

The library syntax is `GEN `

.**ellidentify**(GEN E)

Initialize an `ell`

structure, attached to the elliptic curve E.
E is either

***** a 5-component vector [a_{1},a_{2},a_{3},a_{4},a_{6}] defining the elliptic
curve with Weierstrass equation
Y^2 + a_{1} XY + a_{3} Y = X^3 + a_{2} X^2 + a_{4} X + a_{6},

***** a 2-component vector [a_{4},a_{6}] defining the elliptic
curve with short Weierstrass equation
Y^2 = X^3 + a_{4} X + a_{6},

***** a character string in Cremona's notation, e.g. `"11a1"`

, in which
case the curve is retrieved from the `elldata`

database if available.

The optional argument D describes the domain over which the curve is defined:

***** the `t_INT`

1 (default): the field of rational numbers ℚ.

***** a `t_INT`

p, where p is a prime number: the prime finite field
𝔽_{p}.

***** an `t_INTMOD`

`Mod(a, p)`

, where p is a prime number: the
prime finite field 𝔽_{p}.

***** a `t_FFELT`

, as returned by `ffgen`

: the corresponding finite
field 𝔽_{q}.

***** a `t_PADIC`

, O(p^n): the field ℚ_{p}, where p-adic quantities
will be computed to a relative accuracy of n digits. We advise to input a
model defined over ℚ for such curves. In any case, if you input an
approximate model with `t_PADIC`

coefficients, it will be replaced by a lift
to ℚ (an exact model "close" to the one that was input) and all quantities
will then be computed in terms of this lifted model, at the given accuracy.

***** a `t_REAL`

x: the field ℂ of complex numbers, where floating
point quantities are by default computed to a relative accuracy of
`precision`

(x). If no such argument is given, the value of
`realprecision`

at the time `ellinit`

is called will be used.

***** a number field K, given by a `nf`

or `bnf`

structure; a
`bnf`

is required for `ellminimalmodel`

.

***** a prime ideal 𝔭, given by a `prid`

structure; valid if
x is a curve defined over a number field K and the equation is integral
and minimal at 𝔭.

This argument D is indicative: the curve coefficients are checked for
compatibility, possibly changing D; for instance if D = 1 and
an `t_INTMOD`

is found. If inconsistencies are detected, an error is
raised:

? ellinit([1 + O(5), 1], O(7)); *** at top-level: ellinit([1+O(5),1],O *** ^ — — — — — — -- *** ellinit: inconsistent moduli in ellinit: 7 != 5

If the curve coefficients are too general to fit any of the above domain categories, only basic operations, such as point addition, will be supported later.

If the curve (seen over the domain D) is singular, fail and return an empty vector [].

? E = ellinit([0,0,0,0,1]); \\ y^2 = x^3 + 1, over Q ? E = ellinit([0,1]); \\ the same curve, short form ? E = ellinit("36a1"); \\ sill the same curve, Cremona's notations ? E = ellinit([0,1], 2) \\ over F2: singular curve %4 = [] ? E = ellinit(['a4,'a6] * Mod(1,5)); \\ over F_{5}[a4,a6], basic support !

The result of `ellinit`

is an *ell* structure. It contains at least
the following information in its components:

a_{1},a_{2},a_{3},a_{4},a_{6},b_{2},b_{4},b_{6},b_{8},c_{4},c_{6},Δ,j.

All are accessible via member functions. In particular, the discriminant is
`E.disc`

, and the j-invariant is `E.j`

.

? E = ellinit([a4, a6]); ? E.disc %2 = -64*a4^3 - 432*a6^2 ? E.j %3 = -6912*a4^3/(-4*a4^3 - 27*a6^2)

Further components contain domain-specific data, which are in general dynamic: only computed when needed, and then cached in the structure.

? E = ellinit([2,3], 10^60+7); \\ E over F_{p}, p large ? ellap(E) time = 4,440 ms. %2 = -1376268269510579884904540406082 ? ellcard(E); \\ now instantaneous ! time = 0 ms. ? ellgenerators(E); time = 5,965 ms. ? ellgenerators(E); \\ second time instantaneous time = 0 ms.

See the description of member functions related to elliptic curves at the beginning of this section.

The library syntax is `GEN `

.**ellinit**(GEN x, GEN D = NULL, long prec)

Let E be an `ell`

structure over a number field K or ℚ_{p}.
This function returns an integral model. If v is present, sets
v = [u,0,0,0] to the corresponding change of variable: the return value is
identical to that of `ellchangecurve(E, v)`

.

? e = ellinit([1/17,1/42]); ? e = ellintegralmodel(e,&v); ? e[1..5] %3 = [0, 0, 0, 15287762448, 3154568630095008] ? v %4 = [1/714, 0, 0, 0]

The library syntax is `GEN `

.**ellintegralmodel**(GEN E, GEN *v = NULL)

Given E/K a number field and P in E(K)
return 1 if P = [n]R for some R in E(K) and set Q to one such R;
and return 0 otherwise. The integer n ≥ 0 may be given as
`ellxn(E,n)`

, if many points need to be tested.

? K = nfinit(polcyclo(11,t)); ? E = ellinit([0,-1,1,0,0], K); ? P = [0,0]; ? ellorder(E,P) %4 = 5 ? ellisdivisible(E,P,5, &Q) %5 = 1 ? lift(Q) %6 = [-t^7-t^6-t^5-t^4+1, -t^9-2*t^8-2*t^7-3*t^6-3*t^5-2*t^4-2*t^3-t^2-1] ? ellorder(E, Q) %7 = 25

The algebraic complexity of the underlying algorithm is in
O(n^4), so it is advisable to first factor n, then use a chain of checks
attached to the prime divisors of n: the function will do it itself unless
n is given in `ellxn`

form.

The library syntax is `long `

.**ellisdivisible**(GEN E, GEN P, GEN n, GEN *Q = NULL)

Given an elliptic curve E, a finite subgroup G of E is given either
as a generating point P (for a cyclic G) or as a polynomial whose roots
vanish on the x-coordinates of the non-zero elements of G (general case
and more efficient if available). This function returns the
[a_{1},a_{2},a_{3},a_{4},a_{6}] invariants of the quotient elliptic curve E/G and
(if *only_image* is zero (the default)) a vector of rational
functions [f, g, h] such that the isogeny E → E/G is given by (x,y)
`: — >`

(f(x)/h(x)^2, g(x,y)/h(x)^3).

? E = ellinit([0,1]); ? elltors(E) %2 = [6, [6], [[2, 3]]] ? ellisogeny(E, [2,3], 1) \\ Weierstrass model for E/<P> %3 = [0, 0, 0, -135, -594] ? ellisogeny(E,[-1,0]) %4 = [[0,0,0,-15,22], [x^3+2*x^2+4*x+3, y*x^3+3*y*x^2-2*y, x+1]]

The library syntax is `GEN `

where **ellisogeny**(GEN E, GEN G, long only_image, long x = -1, long y = -1)`x`

, `y`

are variable numbers.

Given an isogeny of elliptic curves f:E' → E (being the result of a call
to `ellisogeny`

), apply f to g:

***** if g is a point P in the domain of f, return the image f(P);

***** if g:E" → E' is a compatible isogeny, return the composite
isogeny f o g: E" → E.

? one = ffgen(101, 't)^0; ? E = ellinit([6, 53, 85, 32, 34] * one); ? P = [84, 71] * one; ? ellorder(E, P) %4 = 5 ? [F, f] = ellisogeny(E, P); \\ f: E->F = E/<P> ? ellisogenyapply(f, P) %6 = [0] ? F = ellinit(F); ? Q = [89, 44] * one; ? ellorder(F, Q) %9 = 2 ? [G, g] = ellisogeny(F, Q); \\ g: F->G = F/<Q> ? gof = ellisogenyapply(g, f); \\ gof: E -> G

The library syntax is `GEN `

.**ellisogenyapply**(GEN f, GEN g)

Given an elliptic curve E defined over a number field, compute
representatives of the isomorphism classes of elliptic curves ℚ-isogenous
to E. For any such curve E_{i}, let f_{i}: E → E_{i} be a rational isogeny
of minimal degree and let g_{i}: E_{i} → E be the dual isogeny; and let M
be the matrix such that M_{i,j} is the minimal degree for an isogeny E_{i}
→ E_{j}.

The function returns a vector [L,M] where L is a list of triples
[E_{i}, f_{i}, g_{i}] (*flag* = 0), or simply the list of E_{i} (*flag* = 1,
which saves time). The curves E_{i} are given in [a_{4},a_{6}] form and the
first curve E_{1} is isomorphic to E by f_{1}.

If p is set, it must be a prime number; in this which case only isogenies of degree a power of p are considered.

Over a number field, the possible isogeny degrees are determined by Billerey algorithm. As a consequence, CM curves over a number field are not fully supported.

? E = ellinit("14a1"); ? [L,M] = ellisomat(E); ? LE = apply(x->x[1], L) \\ list of curves %3 = [[215/48,-5291/864],[-675/16,6831/32],[-8185/48,-742643/864], [-1705/48,-57707/864],[-13635/16,306207/32],[-131065/48,-47449331/864]] ? L[2][2] \\ isogeny f_{2}%4 = [x^3+3/4*x^2+19/2*x-311/12, 1/2*x^4+(y+1)*x^3+(y-4)*x^2+(-9*y+23)*x+(55*y+55/2),x+1/3] ? L[2][3] \\ dual isogeny g_{2}%5 = [1/9*x^3-1/4*x^2-141/16*x+5613/64, -1/18*x^4+(1/27*y-1/3)*x^3+(-1/12*y+87/16)*x^2+(49/16*y-48)*x +(-3601/64*y+16947/512),x-3/4] ? apply(E->ellidentify(ellinit(E))[1][1], LE) %6 = ["14a1","14a4","14a3","14a2","14a6","14a5"] ? M %7 = [1 3 3 2 6 6] [3 1 9 6 2 18] [3 9 1 6 18 2] [2 6 6 1 3 3] [6 2 18 3 1 9] [6 18 2 3 9 1]

The library syntax is `GEN `

.**ellisomat**(GEN E, long p, long fl)

Gives 1 (i.e. true) if the point z is on the elliptic curve E, 0 otherwise. If E or z have imprecise coefficients, an attempt is made to take this into account, i.e. an imprecise equality is checked, not a precise one. It is allowed for z to be a vector of points in which case a vector (of the same type) is returned.

The library syntax is `GEN `

.
Also available is **ellisoncurve**(GEN E, GEN z)`int `

which does not
accept vectors of points.**oncurve**(GEN E, GEN z)

Given an elliptic curve E defined over ℚ or a set of
ℚ-isogenous curves as given by `ellisomat`

, return a pair [L,M] where

***** L lists the minimal models of the isomorphism classes of elliptic
curves ℚ-isogenous to E (or in the set of isogenous curves),

***** M is the adjacency matrix of the prime degree isogenies tree:
there is an edge from E_{i} to E_{j} if there is an isogeny E_{i} → E_{j} of
prime degree such that the Néron differential forms are preserved.

? E = ellinit("14a1"); ? [L,M] = ellisotree(E); ? M %3 = [0 0 3 2 0 0] [3 0 0 0 2 0] [0 0 0 0 0 2] [0 0 0 0 0 3] [0 0 0 3 0 0] [0 0 0 0 0 0] ? [L2,M2] = ellisotree(ellisomat(E,2,1)); %4 = [0 2] [0 0] ? [L3,M3] = ellisotree(ellisomat(E,3,1)); ? M3 %6 = [0 0 3] [3 0 0] [0 0 0]

Compare with the result of `ellisomat`

.

? [L,M]=ellisomat(E,,1); ? M %7 = [1 3 3 2 6 6] [3 1 9 6 2 18] [3 9 1 6 18 2] [2 6 6 1 3 3] [6 2 18 3 1 9] [6 18 2 3 9 1]

The library syntax is `GEN `

.**ellisotree**(GEN E)

Return 1 if the elliptic curve E defined over a number field, ℚ_{p}
or a finite field is supersingular at p, and 0 otherwise.
If the curve is defined over a number field, p must be explicitly given,
and must be a prime number, resp. a maximal ideal, if the curve is defined
over ℚ, resp. a general number field: we return 1 if and only if E
has supersingular good reduction at p.

Alternatively, E can be given by its j-invariant in a finite field. In this case p must be omitted.

? setrand(1); \\ make the choice of g deterministic ? g = ffprimroot(ffgen(7^5)) %1 = 4*x^4 + 5*x^3 + 6*x^2 + 5*x + 6 ? [g^n | n <- [1 .. 7^5 - 1], ellissupersingular(g^n)] %2 = [6] ? K = nfinit(y^3-2); P = idealprimedec(K, 2)[1]; ? E = ellinit([y,1], K); ? ellissupersingular(E, P) %5 = 1 ? Q = idealprimedec(K,5)[1]; ? ellissupersingular(E, Q) %6 = 0

The library syntax is `GEN `

.
Also available is
**ellissupersingular**(GEN E, GEN p = NULL)`int `

where j is a j-invariant of a curve
over a finite field.**elljissupersingular**(GEN j)

Elliptic j-invariant. x must be a complex number with positive imaginary part, or convertible into a power series or a p-adic number with positive valuation.

The library syntax is `GEN `

.**jell**(GEN x, long prec)

Calculates the Kodaira type of the local fiber of the elliptic curve
E at p. E must be an `ell`

structure as output by
`ellinit`

, over ℚ_ℓ (p better left omitted, else equal to ℓ)
over ℚ (p a rational prime) or a number field K (p
a maximal ideal given by a `prid`

structure).
The result is a 4-component vector [f,kod,v,c]. Here f is the exponent of
p in the arithmetic conductor of E, and kod is the Kodaira type which
is coded as follows:

1 means good reduction (type I_{0}), 2, 3 and 4 mean types II, III and IV
respectively, 4+ν with ν > 0 means type I_ν;
finally the opposite values -1, -2, etc. refer to the starred types
I_{0}^{*}, II^{*}, etc. The third component v is itself a vector [u,r,s,t]
giving the coordinate changes done during the local reduction;
u = 1 if and only if the given equation was already minimal at p.
Finally, the last component c is the local Tamagawa number c_{p}.

The library syntax is `GEN `

.**elllocalred**(GEN E, GEN p = NULL)

Given two points P and G on the elliptic curve E/𝔽_{q}, returns the
discrete logarithm of P in base G, i.e. the smallest non-negative
integer n such that P = [n]G.
See `znlog`

for the limitations of the underlying discrete log algorithms.
If present, o represents the order of G, see Section se:DLfun;
the preferred format for this parameter is `[N, factor(N)]`

, where N
is the order of G.

If no o is given, assume that G generates the curve. The function also assumes that P is a multiple of G.

? a = ffgen(ffinit(2,8),'a); ? E = ellinit([a,1,0,0,1]); \\ over F_{2^8}? x = a^3; y = ellordinate(E,x)[1]; ? P = [x,y]; G = ellmul(E, P, 113); ? ord = [242, factor(242)]; \\ P generates a group of order 242. Initialize. ? ellorder(E, G, ord) %4 = 242 ? e = elllog(E, P, G, ord) %5 = 15 ? ellmul(E,G,e) == P %6 = 1

The library syntax is `GEN `

.**elllog**(GEN E, GEN P, GEN G, GEN o = NULL)

This function is deprecated, use `lfun(E,s)`

instead.

E being an elliptic curve, given by an arbitrary model over ℚ as output
by `ellinit`

, this function computes the value of the L-series of E at
the (complex) point s. This function uses an O(N^{1/2}) algorithm, where
N is the conductor.

The optional parameter A fixes a cutoff point for the integral and is best
left omitted; the result must be independent of A, up to
`realprecision`

, so this allows to check the function's accuracy.

The library syntax is `GEN `

.**elllseries**(GEN E, GEN s, GEN A = NULL, long prec)

E being an elliptic curve defined over a number field output by
`ellinit`

, return the minimal discriminant ideal of E.

The library syntax is `GEN `

.**ellminimaldisc**(GEN E)

Let E be an `ell`

structure over a number field K. This function
determines whether E admits a global minimal integral model. If so, it
returns it and sets v = [u,r,s,t] to the corresponding change of variable:
the return value is identical to that of `ellchangecurve(E, v)`

.

Else return the (non-principal) Weierstrass class of E, i.e. the class of
∏ 𝔭^{(v𝔭{Δ} - δ_{𝔭}) / 12} where
Δ = `E.disc`

is the model's discriminant and
𝔭 ^ δ_{𝔭} is the local minimal discriminant.
This function requires either that E be defined
over the rational field ℚ (with domain D = 1 in `ellinit`

),
in which case a global minimal model always exists, or over a number
field given by a *bnf* structure. The Weierstrass class is given in
`bnfisprincipal`

format, i.e. in terms of the `K.gen`

generators.

The resulting model has integral coefficients and is everywhere minimal, the
coefficients a_{1} and a_{3} are reduced modulo 2 (in terms of the fixed
integral basis `K.zk`

) and a_{2} is reduced modulo 3. Over ℚ, we
further require that a_{1} and a_{3} be 0 or 1, that a_{2} be 0 or ±
1 and that u > 0 in the change of variable: both the model and the change
of variable v are then unique.

? e = ellinit([6,6,12,55,233]); \\ over Q ? E = ellminimalmodel(e, &v); ? E[1..5] %3 = [0, 0, 0, 1, 1] ? v %4 = [2, -5, -3, 9]

? K = bnfinit(a^2-65); \\ over a non-principal number field ? K.cyc %2 = [2] ? u = Mod(8+a, K.pol); ? E = ellinit([1,40*u+1,0,25*u^2,0], K); ? ellminimalmodel(E) \\ no global minimal model exists over Z_{K}%6 = [1]~

The library syntax is `GEN `

.**ellminimalmodel**(GEN E, GEN *v = NULL)

Let E be an elliptic curve defined over ℚ, return
a discriminant D such that the twist of E by D is minimal among all
possible quadratic twists, i.e. if *flag* = 0, its minimal model has minimal
discriminant, or if *flag* = 1, it has minimal conductor.

In the example below, we find a curve with j-invariant 3 and minimal conductor.

? E = ellminimalmodel(ellinit(ellfromj(3))); ? ellglobalred(E)[1] %2 = 357075 ? D = ellminimaltwist(E,1) %3 = -15 ? E2 = ellminimalmodel(ellinit(elltwist(E,D))); ? ellglobalred(E2)[1] %5 = 14283

In the example below, *flag* = 0 and *flag* = 1 give different results.

? E = ellinit([1,0]); ? D0 = ellminimaltwist(E,0) %7 = 1 ? D1 = ellminimaltwist(E,1) %8 = 8 ? E0 = ellminimalmodel(ellinit(elltwist(E,D0))); ? [E0.disc, ellglobalred(E0)[1]] %10 = [-64, 64] ? E1 = ellminimalmodel(ellinit(elltwist(E,D1))); ? [E1.disc, ellglobalred(E1)[1]] %12 = [-4096, 32]

The library syntax is `GEN `

.
Also available are
**ellminimaltwist0**(GEN E, long flag)`GEN `

for **ellminimaltwist**(E)*flag* = 0, and
`GEN `

for **ellminimaltwistcond**(E)*flag* = 1.

e being an elliptic curve defined over ℚ output by `ellinit`

,
compute the modular degree of e divided by the square of
the Manin constant c. It is conjectured that c = 1 for the strong Weil
curve in the isogeny class (optimal quotient of J_{0}(N)) and this can be
proven using `ellweilcurve`

when the conductor N is moderate.

? E = ellinit("11a1"); \\ from Cremona table: strong Weil curve and c = 1 ? [v,smith] = ellweilcurve(E); smith \\ proof of the above %2 = [[1, 1], [5, 1], [1, 1/5]] ? ellmoddegree(E) %3 = 1 ? [ellidentify(e)[1][1] | e<-v] %4 = ["11a1", "11a2", "11a3"] ? ellmoddegree(ellinit("11a2")) %5 = 5 ? ellmoddegree(ellinit("11a3")) %6 = 1/5

The modular degree of `11a1`

is 1 (because
`ellweilcurve`

or Cremona's table prove that the Manin constant
is 1 for this curve); the output of `ellweilcurve`

also proves
that the Manin constants of `11a2`

and `11a3`

are 1 and 5
respectively, so the actual modular degree of both `11a2`

and `11a3`

is 5.

The library syntax is `GEN `

.**ellmoddegree**(GEN e)

Given a prime N < 500, return a vector [P,t] where P(x,y)
is a modular equation of level N, i.e. a bivariate polynomial with integer
coefficients; t indicates the type of this equation: either
*canonical* (t = 0) or *Atkin* (t = 1). This function requires
the `seadata`

package and its only use is to give access to the package
contents. See `polmodular`

for a more general and more flexible function.

Let j be the j-invariant function. The polynomial P satisfies
the functional equation,
P(f,j) = P(f | W_{N}, j | W_{N}) = 0
for some modular function f = f_{N} (hand-picked for each fixed N to
minimize its size, see below), where W_{N}(τ) = -1 / (N τ) is the
Atkin-Lehner involution. These two equations allow to compute the values of
the classical modular polynomial Φ_{N}, such that Φ_{N}(j(τ),
j(Nτ)) = 0, while being much smaller than the latter. More precisely, we
have j(W_{N}(τ)) = j(N τ); the function f is invariant under
Γ_{0}(N) and also satisfies

***** for Atkin type: f | W_{N} = f;

***** for canonical type: let s = 12/gcd(12,N-1), then
f | W_{N} = N^s / f. In this case, f has a simple definition:
f(τ) = N^s (η(N τ) / η(τ) )^{2 s},
where η is Dedekind's eta function.

The following GP function returns values of the classical modular polynomial
by eliminating f_{N}(τ) in the above functional equation,
for N ≤ 31 or N ∈ {41,47,59,71}.

classicaleqn(N, X='X, Y='Y)= { my([P,t] = ellmodulareqn(N), Q, d); if (poldegree(P,'y) > 2, error("level unavailable in classicaleqn")); if (t == 0, \\ Canonical my(s = 12/gcd(12,N-1)); Q = 'x^(N+1) * substvec(P,['x,'y],[N^s/'x,Y]); d = N^(s*(2*N+1)) * (-1)^(N+1); , \\ Atkin Q = subst(P,'y,Y); d = (X-Y)^(N+1)); polresultant(subst(P,'y,X), Q) / d; }

The library syntax is `GEN `

where **ellmodulareqn**(long N, long x = -1, long y = -1)`x`

, `y`

are variable numbers.

Computes [n]z, where z is a point on the elliptic curve E. The exponent n is in ℤ, or may be a complex quadratic integer if the curve E has complex multiplication by n (if not, an error message is issued).

? Ei = ellinit([1,0]); z = [0,0]; ? ellmul(Ei, z, 10) %2 = [0] \\ unsurprising: z has order 2 ? ellmul(Ei, z, I) %3 = [0, 0] \\ Ei has complex multiplication by Z[i] ? ellmul(Ei, z, quadgen(-4)) %4 = [0, 0] \\ an alternative syntax for the same query ? Ej = ellinit([0,1]); z = [-1,0]; ? ellmul(Ej, z, I) *** at top-level: ellmul(Ej,z,I) *** ^ — — — — -- *** ellmul: not a complex multiplication in ellmul. ? ellmul(Ej, z, 1+quadgen(-3)) %6 = [1 - w, 0]

The simple-minded algorithm for the CM case assumes that we are in characteristic 0, and that the quadratic order to which n belongs has small discriminant.

The library syntax is `GEN `

.**ellmul**(GEN E, GEN z, GEN n)

Opposite of the point z on elliptic curve E.

The library syntax is `GEN `

.**ellneg**(GEN E, GEN z)

Given an elliptic curve E/ℚ (more precisely, a model defined over ℚ of a curve) and a rational point P ∈ E(ℚ), returns the pair [R,n], where n is the least positive integer such that R := [n]P has good reduction at every prime. More precisely, its image in a minimal model is everywhere non-singular.

? e = ellinit("57a1"); P = [2,-2]; ? ellnonsingularmultiple(e, P) %2 = [[1, -1], 2] ? e = ellinit("396b2"); P = [35, -198]; ? [R,n] = ellnonsingularmultiple(e, P); ? n %5 = 12

The library syntax is `GEN `

.**ellnonsingularmultiple**(GEN E, GEN P)

Gives the order of the point z on the elliptic curve E, defined over a finite field or a number field. Return (the impossible value) zero if the point has infinite order.

? E = ellinit([-157^2,0]); \\ the "157-is-congruent" curve ? P = [2,2]; ellorder(E, P) %2 = 2 ? P = ellheegner(E); ellorder(E, P) \\ infinite order %3 = 0 ? K = nfinit(polcyclo(11,t)); E=ellinit("11a3", K); T = elltors(E); ? ellorder(E, T.gen[1]) %5 = 25 ? E = ellinit(ellfromj(ffgen(5^10))); ? ellcard(E) %7 = 9762580 ? P = random(E); ellorder(E, P) %8 = 4881290 ? p = 2^160+7; E = ellinit([1,2], p); ? N = ellcard(E) %9 = 1461501637330902918203686560289225285992592471152 ? o = [N, factor(N)]; ? for(i=1,100, ellorder(E,random(E))) time = 260 ms.

The parameter o, is now mostly useless, and kept for backward
compatibility. If present, it represents a non-zero multiple of the order
of z, see Section se:DLfun; the preferred format for this parameter is
`[ord, factor(ord)]`

, where `ord`

is the cardinality of the curve.
It is no longer needed since PARI is now able to compute it over large
finite fields (was restricted to small prime fields at the time this feature
was introduced), *and* caches the result in E so that it is computed
and factored only once. Modifying the last example, we see that including
this extra parameter provides no improvement:

? o = [N, factor(N)]; ? for(i=1,100, ellorder(E,random(E),o)) time = 260 ms.

The library syntax is `GEN `

.
The obsolete form **ellorder**(GEN E, GEN z, GEN o = NULL)`GEN `

should no longer be
used.**orderell**(GEN e, GEN z)

Gives a 0, 1 or 2-component vector containing the y-coordinates of the points of the curve E having x as x-coordinate.

The library syntax is `GEN `

.**ellordinate**(GEN E, GEN x, long prec)

Returns the value (or r-th derivative) on a character χ^s of
ℤ_{p}^{*} of the p-adic L-function of the elliptic curve E/ℚ, twisted by
D, given modulo p^n.

**Characters.** The set of continuous characters of
Gal(ℚ(μ_{p oo })/ ℚ) is identified to ℤ_{p}^{*} via the
cyclotomic character χ with values in ℚ_{p}^{*}. Denote by
τ:ℤ_{p}^{*} → ℤ_{p}^{*} the Teichmüller character, with values
in the (p-1)-th roots of 1 for p != 2, and {-1,1} for p = 2;
finally, let
`<`

χ`>`

= χ τ^{-1}, with values in 1 + 2pℤ_{p}.
In GP, the continuous character of
Gal(ℚ(μ_{p oo })/ ℚ) given by `<`

χ`>`

^{s1}
τ^{s2} is represented by the pair of integers s = (s_{1},s_{2}), with s_{1}
∈ ℤ_{p} and s_{2} mod p-1 for p > 2, (resp. mod 2 for p = 2); s
may be also an integer, representing (s,s) or χ^s.

**The p-adic L function.**
The p-adic L function L_{p} is defined on the set of continuous
characters of Gal(ℚ(μ_{p oo })/ ℚ), as ∫_{ℤp*}
χ^s d μ for a certain p-adic distribution μ on ℤ_{p}^{*}. The
derivative is given by
L_{p}^{(r)}(E, χ^s) = ∫_{ℤp*} log_{p}^r(a) χ^s(a) dμ(a).
More precisely:

***** When E has good supersingular reduction, L_{p} takes its
values in D := H^1_{dR}(E/ℚ) ⨂ _ℚ ℚ_{p} and satisfies
(1-p^{-1} F)^{-2} L_{p}(E, χ^0) = (L(E,1) / Ω).ω
where F is the Frobenius, L(E,1) is the value of the complex L
function at 1, ω is the Néron differential
and Ω the attached period on E(ℝ). Here, χ^0 represents
the trivial character.

The function returns the components of L_{p}^{(r)}(E,χ^s) in
the basis (ω, F ω).

***** When E has ordinary good reduction, this method only defines
the projection of L_{p}(E,χ^s) on the α-eigenspace,
where α is the unit eigenvalue for F. This is what the function
returns. We have
(1- α^{-1})^{-2} L_{p,α}(E,χ^0) = L(E,1) / Ω.

Two supersingular examples:

? cxL(e) = bestappr( ellL1(e) / e.omega[1] ); ? e = ellinit("17a1"); p=3; \\ supersingular, a3 = 0 ? L = ellpadicL(e,p,4); ? F = [0,-p;1,ellap(e,p)]; \\ Frobenius matrix in the basis (omega,F(omega)) ? (1-p^(-1)*F)^-2 * L / cxL(e) %5 = [1 + O(3^5), O(3^5)]~ \\ [1,0]~ ? e = ellinit("116a1"); p=3; \\ supersingular, a3 != 0~ ? L = ellpadicL(e,p,4); ? F = [0,-p; 1,ellap(e,p)]; ? (1-p^(-1)*F)^-2*L~ / cxL(e) %9 = [1 + O(3^4), O(3^5)]~

Good ordinary reduction:

? e = ellinit("17a1"); p=5; ap = ellap(e,p) %1 = -2 \\ ordinary ? L = ellpadicL(e,p,4) %2 = 4 + 3*5 + 4*5^2 + 2*5^3 + O(5^4) ? al = padicappr(x^2 - ap*x + p, ap + O(p^7))[1]; ? (1-al^(-1))^(-2) * L / cxL(e) %4 = 1 + O(5^4)

Twist and Teichmüller:

? e = ellinit("17a1"); p=5; \\ ordinary \\ 2nd derivative at tau^1, twist by -7 ? ellpadicL(e, p, 4, [0,1], 2, -7) %2 = 2*5^2 + 5^3 + O(5^4)

We give an example of non split multiplicative reduction (see
`ellpadicbsd`

for more examples).

? e=ellinit("15a1"); p=3; n=5; ? L = ellpadicL(e,p,n) %2 = 2 + 3 + 3^2 + 3^3 + 3^4 + O(3^5) ? (1 - ellap(e,p))^(-1) * L / cxL(e) %3 = 1 + O(3^5)

This function is a special case of `mspadicL`

and it also appears
as the first term of `mspadicseries`

:

? e = ellinit("17a1"); p=5; ? L = ellpadicL(e,p,4) %2 = 4 + 3*5 + 4*5^2 + 2*5^3 + O(5^4) ? [M,phi] = msfromell(e, 1); ? Mp = mspadicinit(M, p, 4); ? mu = mspadicmoments(Mp, phi); ? mspadicL(mu) %6 = 4 + 3*5 + 4*5^2 + 2*5^3 + 2*5^4 + 5^5 + O(5^6) ? mspadicseries(mu) %7 = (4 + 3*5 + 4*5^2 + 2*5^3 + 2*5^4 + 5^5 + O(5^6)) + (3 + 3*5 + 5^2 + 5^3 + O(5^4))*x + (2 + 3*5 + 5^2 + O(5^3))*x^2 + (3 + 4*5 + 4*5^2 + O(5^3))*x^3 + (3 + 2*5 + O(5^2))*x^4 + O(x^5)

These are more cumbersome than `ellpadicL`

but allow to
compute at different characters, or successive derivatives, or to
twist by a quadratic character essentially for the cost of a single call to
`ellpadicL`

due to precomputations.

The library syntax is `GEN `

.**ellpadicL**(GEN E, GEN p, long n, GEN s = NULL, long r, GEN D = NULL)

Given an elliptic curve E over ℚ, its quadratic twist E_{D}
and a prime number p, this function is a p-adic analog of the complex
functions `ellanalyticrank`

and `ellbsd`

. It calls `ellpadicL`

with initial accuracy p^n and may increase it internally;
it returns a vector [r, L_{p}] where

***** L_{p} is a p-adic number (resp. a pair of p-adic numbers if
E has good supersingular reduction) defined modulo p^N, conjecturally
equal to R_{p} S, where R_{p} is the p-adic regulator as given by
`ellpadicregulator`

(in the basis (ω, F ω)) and S is the
cardinal of the Tate-Shafarevich group for the quadratic twist E_{D}.

***** r is an upper bound for the analytic rank of the p-adic
L-function attached to E_{D}: we know for sure that the i-th
derivative of L_{p}(E_{D},.) at χ^0 is O(p^N) for all i < r
and that its r-th derivative is non-zero; it is expected that the true
analytic rank is equal to the rank of the Mordell-Weil group E_{D}(ℚ),
plus 1 if the reduction of E_{D} at p is split multiplicative;
if r = 0, then both the analytic rank and the Mordell-Weil rank are
unconditionnally 0.

Recall that the p-adic BSD conjecture (Mazur, Tate, Teitelbaum, Bernardi,
Perrin-Riou) predicts an explicit link between R_{p} S and
(1-p^{-1} F)^{-2}.L_{p}^{(r)}(E_{D}, χ^0) / r!
where r is the analytic rank of the p-adic L-function attached to
E_{D} and F is the Frobenius on H^1_{dR}; see `ellpadicL`

for definitions.

? E = ellinit("11a1"); p = 7; n = 5; \\ good ordinary ? ellpadicbsd(E, 7, 5) \\ rank 0, %2 = [0, 1 + O(7^5)] ? E = ellinit("91a1"); p = 7; n = 5; \\ non split multiplicative ? [r,Lp] = ellpadicbsd(E, p, n) %5 = [1, 2*7 + 6*7^2 + 3*7^3 + 7^4 + O(7^5)] ? R = ellpadicregulator(E, p, n, E.gen) %6 = 2*7 + 6*7^2 + 3*7^3 + 7^4 + 5*7^5 + O(7^6) ? sha = Lp/R %7 = 1 + O(7^4) ? E = ellinit("91b1"); p = 7; n = 5; \\ split multiplicative ? [r,Lp] = ellpadicbsd(E, p, n) %9 = [2, 2*7 + 7^2 + 5*7^3 + O(7^4)] ? ellpadicregulator(E, p, n, E.gen) %10 = 2*7 + 7^2 + 5*7^3 + 6*7^4 + 2*7^5 + O(7^6) ? [rC, LC] = ellanalyticrank(E); ? [r, rC] %12 = [2, 1] \\ r = rC+1 because of split multiplicative reduction ? E = ellinit("53a1"); p = 5; n = 5; \\ supersingular ? [r, Lp] = ellpadicbsd(E, p, n); ? r %15 = 1 ? Lp %16 = [3*5 + 2*5^2 + 2*5^5 + O(5^6), \ 5 + 3*5^2 + 4*5^3 + 2*5^4 + 5^5 + O(5^6)] ? R = ellpadicregulator(E, p, n, E.gen) %17 = [3*5 + 2*5^2 + 2*5^5 + O(5^6), 5 + 3*5^2 + 4*5^3 + 2*5^4 + O(5^5)] \\ expect Lp = R*#Sha, hence (conjecturally) #Sha = 1 ? E = ellinit("84a1"); p = 11; n = 6; D = -443; ? [r,Lp] = ellpadicbsd(E, 11, 6, D) \\ Mordell-Weil rank 0, no regulator %19 = [0, 3 + 2*11 + O(11^6)] ? lift(Lp) \\ expected cardinal for Sha is 5^2 %20 = 25 ? ellpadicbsd(E, 3, 12, D) \\ at 3 %21 = [1, 1 + 2*3 + 2*3^2 + O(3^8)] ? ellpadicbsd(E, 7, 8, D) \\ and at 7 %22 = [0, 4 + 3*7 + O(7^8)]

The library syntax is `GEN `

.**ellpadicbsd**(GEN E, GEN p, long n, GEN D = NULL)

If p > 2 is a prime and E is an elliptic curve on ℚ with good
reduction at p, return the matrix of the Frobenius endomorphism ϕ on
the crystalline module D_{p}(E) = ℚ_{p} ⨂ H^1_{dR}(E/ℚ) with respect to
the basis of the given model (ω, η = x ω), where
ω = dx/(2 y+a_{1} x+a_{3}) is the invariant differential.
The characteristic polynomial of ϕ is x^2 - a_{p} x + p.
The matrix is computed to absolute p-adic precision p^n.

? E = ellinit([1,-1,1,0,0]); ? F = ellpadicfrobenius(E,5,3); ? lift(F) %3 = [120 29] [ 55 5] ? charpoly(F) %4 = x^2 + O(5^3)*x + (5 + O(5^3)) ? ellap(E, 5) %5 = 0

The library syntax is `GEN `

.**ellpadicfrobenius**(GEN E, long p, long n)

Cyclotomic p-adic height of the rational point P on the elliptic curve E (defined over ℚ), given to n p-adic digits. If the argument Q is present, computes the value of the bilinear form (h(P+Q)-h(P-Q)) / 4.

Let D := H^1_{dR}(E) ⨂ _ℚ ℚ_{p} be the ℚ_{p} vector space
spanned by ω
(invariant differential dx/(2y+a_1x+a3) related to the given model) and
η = x ω. Then the cyclotomic p-adic height h_{E} associates to
P ∈ E(ℚ) an element f ω + g η in D.
This routine returns the vector [f, g] to n p-adic digits.
If P ∈ E(ℚ) is in the kernel of reduction mod p and if its reduction
at all finite places is non singular, then g = -(log_{E} P)^2, where
log_{E} is the logarithm for the formal group of E at p.

If furthermore the model is of the form Y^2 = X^3 + a X + b and P = (x,y),
then
f = log_{p}(`denominator`

(x)) - 2 log_{p}(σ(P))
where σ(P) is given by `ellsigma`

(E,P).

Recall (*Advanced topics in the arithmetic of elliptic
curves*, Theorem 3.2) that the local height function over the complex numbers
is of the form
λ(z) = -log (|`E.disc`

|) / 6 + Re(z η(z)) - 2 log(
σ(z)).
(N.B. our normalization for local and global heights is twice that of
Silverman's).

? E = ellinit([1,-1,1,0,0]); P = [0,0]; ? ellpadicheight(E,5,3, P) %2 = [3*5 + 5^2 + 2*5^3 + O(5^4), 5^2 + 4*5^4 + O(5^5)] ? E = ellinit("11a1"); P = [5,5]; \\ torsion point ? ellpadicheight(E,19,6, P) %4 = [0, 0] ? E = ellinit([0,0,1,-4,2]); P = [-2,1]; ? ellpadicheight(E,3,3, P) %6 = [2*3^2 + 2*3^3 + 3^4 + O(3^5), 2*3^2 + 3^4 + O(3^5)] ? ellpadicheight(E,3,5, P, elladd(E,P,P)) %7 = [3^2 + 2*3^3 + O(3^7), 3^2 + 3^3 + 2*3^4 + 3^5 + O(3^7)]

***** When E has good ordinary reduction at p or non split multiplicative
reduction, the "canonical" p-adic height is given by

s2 = ellpadics2(E,p,n); ellpadicheight(E, p, n, P) * [1,-s2]~

Since s_{2} does not depend on P, it is preferable to
compute it only once:

? E = ellinit("5077a1"); p = 5; n = 7; \\ rank 3 ? s2 = ellpadics2(E,p,n); ? M = ellpadicheightmatrix(E,p, n, E.gen) * [1,-s2]~; ? matdet(M) \\ p-adic regulator on the points in E.gen %4 = 5 + 5^2 + 4*5^3 + 2*5^4 + 2*5^5 + 2*5^6 + O(5^7)

***** When E has split multiplicative reduction at p (Tate curve),
the "canonical" p-adic height is given by

Ep = ellinit(E[1..5], O(p^(n))); \\ E seen as a Tate curve over Qp [u2,u,q] = Ep.tate; ellpadicheight(E, p, n, P) * [1,-s2 + 1/log(q)/u2]]~

where s_{2} is as above. For example,

? E = ellinit("91b1"); P =[-1, 3]; p = 7; n = 5; ? Ep = ellinit(E[1..5], O(p^(n))); ? s2 = ellpadics2(E,p,n); ? [u2,u,q] = Ep.tate; ? H = ellpadicheight(E,p, n, P) * [1,-s2 + 1/log(q)/u2]~ %5 = 2*7 + 7^2 + 5*7^3 + 6*7^4 + 2*7^5 + O(7^6)

These normalizations are chosen so that p-adic BSD conjectures
are easy to state, see `ellpadicbsd`

.

The library syntax is `GEN `

.**ellpadicheight0**(GEN E, GEN p, long n, GEN P, GEN Q = NULL)

Q being a vector of points, this function returns the "Gram matrix"
[F,G] of the cyclotomic p-adic height h_{E} with respect to
the basis (ω, η) of D = H^1_{dR}(E) ⨂ _ℚ ℚ_{p}
given to n p-adic digits. In other words, if
`ellpadicheight`

(E,p,n, Q[i],Q[j]) = [f,g], corresponding to
f ω + g η in D, then F[i,j] = f and G[i,j] = g.

? E = ellinit([0,0,1,-7,6]); Q = [[-2,3],[-1,3]]; p = 5; n = 5; ? [F,G] = ellpadicheightmatrix(E,p,n,Q); ? lift(F) \\ p-adic entries, integral approximation for readability %3 = [2364 3100] [3100 3119] ? G %4 = [25225 46975] [46975 61850] ? [F,G] * [1,-ellpadics2(E,p,n)]~ %5 = [4 + 2*5 + 4*5^2 + 3*5^3 + O(5^5) 4*5^2 + 4*5^3 + 5^4 + O(5^5)] [ 4*5^2 + 4*5^3 + 5^4 + O(5^5) 4 + 3*5 + 4*5^2 + 4*5^3 + 5^4 + O(5^5)]

The library syntax is `GEN `

.**ellpadicheightmatrix**(GEN E, GEN p, long n, GEN Q)

Given E defined over K = ℚ or ℚ_{p} and P = [x,y] on E(K) in the
kernel of reduction mod p, let t(P) = -x/y be the formal group
parameter; this function returns L(t), where L denotes the formal
logarithm (mapping the formal group of E to the additive formal group)
attached to the canonical invariant differential:
dL = dx/(2y + a_1x + a_{3}).

? E = ellinit([0,0,1,-4,2]); P = [-2,1]; ? ellpadiclog(E,2,10,P) %2 = 2 + 2^3 + 2^8 + 2^9 + 2^10 + O(2^11) ? E = ellinit([17,42]); ? p=3; Ep = ellinit(E,p); \\ E mod p ? P=[114,1218]; ellorder(Ep,P) \\ the order of P on (E mod p) is 2 %5 = 2 ? Q = ellmul(E,P,2) \\ we need a point of the form 2*P %6 = [200257/7056, 90637343/592704] ? ellpadiclog(E,3,10,Q) %7 = 3 + 2*3^2 + 3^3 + 3^4 + 3^5 + 3^6 + 2*3^8 + 3^9 + 2*3^10 + O(3^11)

The library syntax is `GEN `

.**ellpadiclog**(GEN E, GEN p, long n, GEN P)

Let E/ℚ be an elliptic curve. Return the determinant of the Gram
matrix of the vector of points S = (S_{1},..., S_{r}) with respect to the
"canonical" cyclotomic p-adic height on E, given to n (p-adic)
digits.

When E has ordinary reduction at p, this is the expected Gram
deteterminant in ℚ_{p}.

In the case of supersingular reduction of E at p, the definition
requires care: the regulator R is an element of
D := H^1_{dR}(E) ⨂ _ℚ ℚ_{p}, which is a two-dimensional
ℚ_{p}-vector space spanned by ω and η = x ω
(which are defined over ℚ) or equivalently but now over ℚ_{p}
by ω and Fω where F is the Frobenius endomorphism on D
as defined in `ellpadicfrobenius`

. On D we
define the cyclotomic height h_{E} = f ω + g η
(see `ellpadicheight`

) and a canonical alternating bilinear form
[.,.]_{D} such that [ω, η]_{D} = 1.

For any ν ∈ D, we can define a height h_ν := [ h_{E}, ν ]_{D}
from E(ℚ) to ℚ_{p} and `<`

.,.`>`

_ν the attached
bilinear form. In particular, if h_{E} = f ω + gη, then
h_η = [ h_{E}, η ]_{D} = f and h_ω = [ h_{E}, ω ]_{D} = - g
hence h_{E} = h_η ω - h_ω η.
Then, R is the unique element of D such that
[ω,ν]_{D}^{r-1} [R, ν]_{D} = det(`<`

S_{i}, S_{j} `>`

_{ν})
for all ν ∈ D not in ℚ_{p} ω. The `ellpadicregulator`

function returns R in the basis (ω, Fω), which was chosen
so that p-adic BSD conjectures are easy to state, see `ellpadicbsd`

.

Note that by definition
[R, η]_{D} = det(`<`

S_{i}, S_{j} `>`

_{η})
and
[R, ω+η]_{D} = det(`<`

S_{i}, S_{j} `>`

_{ω+η}).

The library syntax is `GEN `

.**ellpadicregulator**(GEN E, GEN p, long n, GEN S)

If p > 2 is a prime and E/ℚ is an elliptic curve with ordinary good
reduction at p, returns the slope of the unit eigenvector
of `ellpadicfrobenius(E,p,n)`

, i.e., the action of Frobenius ϕ on
the crystalline module D_{p}(E) = ℚ_{p} ⨂ H^1_{dR}(E/ℚ) in the basis of
the given model (ω, η = x ω), where ω is the invariant
differential dx/(2 y+a_{1} x+a_{3}). In other words, η + s_{2}ω
is an eigenvector for the unit eigenvalue of ϕ.

? e=ellinit([17,42]); ? ellpadics2(e,13,4) %2 = 10 + 2*13 + 6*13^3 + O(13^4)

This slope is the unique c ∈ 3^{-1}ℤ_{p} such that the odd solution
σ(t) = t + O(t^2) of
- d((1)/(σ) (d σ)/(ω))
= (x(t) + c) ω
is in tℤ_{p}[[t]].

It is equal to b_{2}/12 - E_{2}/12 where E_{2} is the value of the Katz
p-adic Eisenstein series of weight 2 on (E,ω). This is
used to construct a canonical p-adic height when E has good ordinary
reduction at p as follows

s2 = ellpadics2(E,p,n); h(E,p,n, P, s2) = ellpadicheight(E, [p,[1,-s2]],n, P);

Since s_{2} does not depend on the point P, we compute it
only once.

The library syntax is `GEN `

.**ellpadics2**(GEN E, GEN p, long n)

Let w describe a complex period lattice (w = [w_{1},w_{2}]
or an `ellinit`

structure). Returns normalized periods [W_{1},W_{2}] generating
the same lattice such that τ := W_{1}/W_{2} has positive imaginary part
and lies in the standard fundamental domain for SL_{2}(ℤ).

If *flag* = 1, the function returns [[W_{1},W_{2}], [η_{1},η_{2}]], where
η_{1} and η_{2} are the quasi-periods attached to
[W_{1},W_{2}], satisfying η_{2} W_{1} - η_{1} W_{2} = 2 i π.

The output of this function is meant to be used as the first argument given to ellwp, ellzeta, ellsigma or elleisnum. Quasi-periods are needed by ellzeta and ellsigma only.

? L = ellperiods([1,I],1); ? [w1,w2] = L[1]; [e1,e2] = L[2]; ? e2*w1 - e1*w2 %3 = 6.2831853071795864769252867665590057684*I ? ellzeta(L, 1/2 + 2*I) %4 = 1.5707963... - 6.283185307...*I ? ellzeta([1,I], 1/2 + 2*I) \\ same but less efficient %4 = 1.5707963... - 6.283185307...*I

The library syntax is `GEN `

.**ellperiods**(GEN w, long flag, long prec)

If E/ℂ ~ ℂ/Λ is a complex elliptic curve (Λ =
`E.omega`

), computes a complex number z, well-defined modulo the
lattice Λ, corresponding to the point P; i.e. such that
P = [℘_Λ(z),℘'_Λ(z)] satisfies the equation
y^2 = 4x^3 - g_{2} x - g_{3},
where g_{2}, g_{3} are the elliptic invariants.

If E is defined over ℝ and P ∈ E(ℝ), we have more precisely, 0 ≤ Re(t) < w1 and 0 ≤ Im(t) < Im(w2), where (w1,w2) are the real and complex periods of E.

? E = ellinit([0,1]); P = [2,3]; ? z = ellpointtoz(E, P) %2 = 3.5054552633136356529375476976257353387 ? ellwp(E, z) %3 = 2.0000000000000000000000000000000000000 ? ellztopoint(E, z) - P %4 = [2.548947057811923643 E-57, 7.646841173435770930 E-57] ? ellpointtoz(E, [0]) \\ the point at infinity %5 = 0

If E is defined over a general number field, the function returns the
values corresponding to the various complex embeddings of the curve
and of the point, in the same order as `E.nf.roots`

:

? E=ellinit([-22032-15552*x,0], nfinit(x^2-2)); ? P=[-72*x-108,0]; ? ellisoncurve(E,P) %3 = 1 ? ellpointtoz(E,P) %4 = [-0.52751724240790530394437835702346995884*I, -0.090507650025885335533571758708283389896*I] ? E.nf.roots %5 = [-1.4142135623730950488016887242096980786, \\ x-> -sqrt(2) 1.4142135623730950488016887242096980786] \\ x-> sqrt(2)

If E/ℚ_{p} has multiplicative reduction, then E/ℚ_{p} is analytically
isomorphic to ℚ_{p}^{*}/q^ℤ (Tate curve) for some p-adic integer q.
The behavior is then as follows:

***** If the reduction is split (E.`tate[2]`

is a `t_PADIC`

), we have
an isomorphism φ: E(ℚ_{p}) ~ ℚ_{p}^{*}/q^ℤ and the function returns
φ(P) ∈ ℚ_{p}.

***** If the reduction is *not* split (E.`tate[2]`

is a
`t_POLMOD`

), we only have an isomorphism φ: E(K) ~ K^{*}/q^ℤ over
the unramified quadratic extension K/ℚ_{p}. In this case, the output
φ(P) ∈ K is a `t_POLMOD`

.

? E = ellinit([0,-1,1,0,0], O(11^5)); P = [0,0]; ? [u2,u,q] = E.tate; type(u) \\ split multiplicative reduction %2 = "t_PADIC" ? ellmul(E, P, 5) \\ P has order 5 %3 = [0] ? z = ellpointtoz(E, [0,0]) %4 = 3 + 11^2 + 2*11^3 + 3*11^4 + 6*11^5 + 10*11^6 + 8*11^7 + O(11^8) ? z^5 %5 = 1 + O(11^9) ? E = ellinit(ellfromj(1/4), O(2^6)); x=1/2; y=ellordinate(E,x)[1]; ? z = ellpointtoz(E,[x,y]); \\ t_POLMOD of t_POL with t_PADIC coeffs ? liftint(z) \\ lift all p-adics %8 = Mod(8*u + 7, u^2 + 437)

The library syntax is `GEN `

.**zell**(GEN E, GEN P, long prec)

Deprecated alias for `ellmul`

.

The library syntax is `GEN `

.**ellmul**(GEN E, GEN z, GEN n)

E being an integral model of elliptic curve , return a vector
containing the affine rational points on the curve of naive height less than
h. If *flag* = 1, stop as soon as a point is found; return either an empty
vector or a vector containing a single point.
See `hyperellratpoints`

for how h can be specified.

? E=ellinit([-25,1]); ? ellratpoints(E,10) %2 = [[-5,1],[-5,-1],[-3,7],[-3,-7],[-1,5],[-1,-5], [0,1],[0,-1],[5,1],[5,-1],[7,13],[7,-13]] ? ellratpoints(E,10,1) %3 = [[-5,1]]

The library syntax is `GEN `

.**ellratpoints**(GEN E, GEN h, long flag)

E being an `ell`

structure over ℚ as output by `ellinit`

,
this function computes the local root number of its L-series at the place
p (at the infinite place if p = 0). If p is omitted, return the global
root number and in this case the curve can also be defined over a number field.

Note that the global root number is the sign of the functional equation and conjecturally is the parity of the rank of the Mordell-Weil group. The equation for E needs not be minimal at p, but if the model is already minimal the function will run faster.

The library syntax is `long `

.**ellrootno**(GEN E, GEN p = NULL)

Let E be an *ell* structure as output by `ellinit`

, defined over
a finite field 𝔽_{q}. This low-level function computes the order of the
group E(𝔽_{q}) using the SEA algorithm; compared to the high-level
function `ellcard`

, which includes SEA among its choice of algorithms,
the `tors`

argument allows to speed up a search for curves having almost
prime order and whose quadratic twist may also have almost prime order.
When `tors`

is set to a non-zero value, the function returns 0 as soon
as it detects that the order has a small prime factor not dividing `tors`

;
SEA considers modular polynomials of increasing prime degree ℓ and we
return 0 as soon as we hit an ℓ (coprime to `tors`

) dividing
#E(𝔽_{q}):

? ellsea(ellinit([1,1], 2^56+3477), 1) %1 = 72057594135613381 ? forprime(p=2^128,oo, q = ellcard(ellinit([1,1],p)); if(isprime(q),break)) time = 6,571 ms. ? forprime(p=2^128,oo, q = ellsea(ellinit([1,1],p),1);if(isprime(q),break)) time = 522 ms.

In particular, set `tors`

to 1 if you want a curve with prime order,
to 2 if you want to allow a cofactor which is a power of two (e.g. for
Edwards's curves), etc. The early exit on bad curves yields a massive
speedup compared to running the cardinal algorithm to completion.

When `tors`

is negative, similar checks are performed for the quadratic
twist of the curve.

The following function returns a curve of prime order over 𝔽_{p}.

cryptocurve(p) = { while(1, my(E, N, j = Mod(random(p), p)); E = ellinit(ellfromj(j)); N = ellsea(E, 1); if (!N, continue); if (isprime(N), return(E)); \\ try the quadratic twist for free if (isprime(2*p+2 - N), return(ellinit(elltwist(E)))); ); } ? p = randomprime([2^255, 2^256]); ? E = cryptocurve(p); \\ insist on prime order %2 = 47,447ms

The same example without early abort (using `ellcard(E)`

instead of `ellsea(E, 1)`

) runs for about 5 minutes before finding a
suitable curve.

The availability of the `seadata`

package will speed up the computation,
and is strongly recommended. The generic function `ellcard`

should be
preferred when you only want to compute the cardinal of a given curve without
caring about it having almost prime order:

***** If the characteristic is too small (p ≤ 7) or the field
cardinality is tiny (q ≤ 523) the generic algorithm
`ellcard`

is used instead and the `tors`

argument is ignored.
(The reason for this is that SEA is not implemented for p ≤ 7 and
that if q ≤ 523 it is likely to run into an infinite loop.)

***** If the field cardinality is smaller than about 2^{50}, the
generic algorithm will be faster.

***** Contrary to `ellcard`

, `ellsea`

does not store the computed
cardinality in E.

The library syntax is `GEN `

.**ellsea**(GEN E, long tors)

This function finds all curves in the `elldata`

database satisfying
the constraint defined by the argument N:

***** if N is a character string, it selects a given curve, e.g.
`"11a1"`

, or curves in the given isogeny class, e.g. `"11a"`

, or
curves with given conductor, e.g. `"11"`

;

***** if N is a vector of integers, it encodes the same constraints
as the character string above, according to the `ellconvertname`

correspondance, e.g. `[11,0,1]`

for `"11a1"`

, `[11,0]`

for
`"11a"`

and `[11]`

for `"11"`

;

***** if N is an integer, curves with conductor N are selected.

If N codes a full curve name, for instance `"11a1"`

or `[11,0,1]`

,
the output format is [N, [a_{1},a_{2},a_{3},a_{4},a_{6}], G] where
[a_{1},a_{2},a_{3},a_{4},a_{6}] are the coefficients of the Weierstrass equation of
the curve and G is a ℤ-basis of the free part of the
Mordell-Weil group attached to the curve.

? ellsearch("11a3") %1 = ["11a3", [0, -1, 1, 0, 0], []] ? ellsearch([11,0,3]) %2 = ["11a3", [0, -1, 1, 0, 0], []]

If N is not a full curve name, then the output is a vector of all matching curves in the above format:

? ellsearch("11a") %1 = [["11a1", [0, -1, 1, -10, -20], []], ["11a2", [0, -1, 1, -7820, -263580], []], ["11a3", [0, -1, 1, 0, 0], []]] ? ellsearch("11b") %2 = []

The library syntax is `GEN `

.
Also available is **ellsearch**(GEN N)`GEN `

that only
accepts complete curve names (as **ellsearchcurve**(GEN N)`t_STR`

).

Computes the value at z of the Weierstrass σ function attached to
the lattice L as given by `ellperiods`

(,1): including quasi-periods
is useful, otherwise there are recomputed from scratch for each new z.
σ(z, L) = z ∏_{ω ∈ L*} (1 -
(z)/(ω))e^{(z)/(ω) + (z^2)/(2ω^2)}.
It is also possible to directly input L = [ω_{1},ω_{2}],
or an elliptic curve E as given by `ellinit`

(L = `E.omega`

).

? w = ellperiods([1,I], 1); ? ellsigma(w, 1/2) %2 = 0.47494937998792065033250463632798296855 ? E = ellinit([1,0]); ? ellsigma(E) \\ at 'x, implicitly at default seriesprecision %4 = x + 1/60*x^5 - 1/10080*x^9 - 23/259459200*x^13 + O(x^17)

If *flag* = 1, computes an arbitrary determination of log(σ(z)).

The library syntax is `GEN `

.**ellsigma**(GEN L, GEN z = NULL, long flag, long prec)

Difference of the points z1 and z2 on the elliptic curve corresponding to E.

The library syntax is `GEN `

.**ellsub**(GEN E, GEN z1, GEN z2)

The object E being an elliptic curve over a number field, returns the global Tamagawa number of the curve (including the factor at infinite places).

? e = ellinit([1, -1, 1, -3002, 63929]); \\ curve "90c6" from elldata ? elltamagawa(e) %2 = 288 ? [elllocalred(e,p)[4] | p<-[2,3,5]] %3 = [6, 4, 6] ? vecprod(%) \\ since e.disc > 0 the factor at infinity is 2 %4 = 144

The library syntax is `GEN `

.**elltamagawa**(GEN E)

Computes the modular parametrization of the elliptic curve E/ℚ,
where E is an `ell`

structure as output by `ellinit`

. This returns
a two-component vector [u,v] of power series, given to d significant
terms (`seriesprecision`

by default), characterized by the following two
properties. First the point (u,v) satisfies the equation of the elliptic
curve. Second, let N be the conductor of E and Φ: X_{0}(N) → E
be a modular parametrization; the pullback by Φ of the
Néron differential du/(2v+a_1u+a_{3}) is equal to 2iπ
f(z)dz, a holomorphic differential form. The variable used in the power
series for u and v is x, which is implicitly understood to be equal to
exp(2iπ z).

The algorithm assumes that E is a *strong* Weil curve
and that the Manin constant is equal to 1: in fact, f(x) = ∑_{n > 0}
`ellan`

(E, n) x^n.

The library syntax is `GEN `

.**elltaniyama**(GEN E, long precdl)

Computes the Tate pairing of the two points P and Q on the elliptic curve E. The point P must be of m-torsion.

The library syntax is `GEN `

.**elltatepairing**(GEN E, GEN P, GEN Q, GEN m)

If E is an elliptic curve defined over a number field or a finite field,
outputs the torsion subgroup of E as a 3-component vector `[t,v1,v2]`

,
where `t`

is the order of the torsion group, `v1`

gives the structure
of the torsion group as a product of cyclic groups (sorted by decreasing
order), and `v2`

gives generators for these cyclic groups. E must be an
`ell`

structure as output by `ellinit`

.

? E = ellinit([-1,0]); ? elltors(E) %1 = [4, [2, 2], [[0, 0], [1, 0]]]

Here, the torsion subgroup is isomorphic to ℤ/2ℤ x ℤ/2ℤ, with generators [0,0] and [1,0].

The library syntax is `GEN `

.**elltors**(GEN E)

Returns the coefficients [a_{1},a_{2},a_{3},a_{4},a_{6}] of the twist of the
elliptic curve E by the quadratic extension of the coefficient ring
defined by P (when P is a polynomial) or `quadpoly(P)`

when P is an
integer. If E is defined over a finite field, then P can be omitted,
in which case a random model of the unique non-trivial twist is returned.
If E is defined over a number field, the model should be replaced by a
minimal model (if one exists).

Example: Twist by discriminant -3:

? elltwist(ellinit([0,a2,0,a4,a6]),-3) %1 = [0,-3*a2,0,9*a4,-27*a6]

Twist by the Artin-Shreier extension given by x^2+x+T in characteristic 2:

? lift(elltwist(ellinit([a1,a2,a3,a4,a6]*Mod(1,2)),x^2+x+T)) %1 = [a1,a2+a1^2*T,a3,a4,a6+a3^2*T]

Twist of an elliptic curve defined over a finite field:

? E=ellinit([1,7]*Mod(1,19));lift(elltwist(E)) %1 = [0,0,0,11,12]

The library syntax is `GEN `

.**elltwist**(GEN E, GEN P = NULL)

If E' is an elliptic curve over ℚ, let L_{E'} be the
sub-ℤ-module of Hom_{Γ0(N)}(Δ_{0},ℚ) attached to E'
(It is given by x[3] if [M,x] = `msfromell`

(E').)

On the other hand, if N is the conductor of E and f is the modular form
for Γ_{0}(N) attached to E, let L_{f} be the lattice of the
f-component of Hom_{Γ0(N)}(Δ_{0},ℚ) given by the elements
φ such that φ({0,γ^{-1} 0}) ∈ ℤ for all
γ ∈ Γ_{0}(N) (see `mslattice`

).

Let E' run through the isomorphism classes of elliptic curves
isogenous to E as given by `ellisomat`

(and in the same order).
This function returns a pair `[vE,vS]`

where `vE`

contains minimal
models for the E' and `vS`

contains the list of Smith invariants for
the lattices L_{E'} in L_{f}. The function also accepts the output of
`ellisomat`

, i.e. the isogeny class. If the optional argument `ms`

is present, it contains the output of `msfromell(vE, 0)`

, i.e. the new
modular symbol space M of level N and a vector of triples [x^+,x^-, L]
attached to each curve E'.

In particular, the strong Weil curve amongst the curves isogenous to E is the one whose Smith invariants are [c,c], where c is the Manin constant, conjecturally equal to 1.

? E = ellinit("11a3"); ? [vE, vS] = ellweilcurve(E); ? [n] = [ i | i<-[1..#vS], vS[i]==[1,1] ] \\ lattice with invariant [1,1] %3 = [2] ? ellidentify(vE[n]) \\ ... corresponds to strong Weil curve %4 = [["11a1", [0, -1, 1, -10, -20], []], [1, 0, 0, 0]] ? [vE, vS] = ellweilcurve(E, &ms); \\ vE,vS are as above ? [M, vx] = ms; msdim(M) \\ ... but ms contains more information %6 = 3 ? #vx %7 = 3 ? vx[1] %8 = [[1/25, -1/10, -1/10]~, [0, 1/2, -1/2]~, [1/25,0; -3/5,1; 2/5,-1]] ? forell(E, 11,11, print(msfromell(ellinit(E[1]), 1)[2])) [1/5, -1/2, -1/2]~ [1, -5/2, -5/2]~ [1/25, -1/10, -1/10]~

The last example prints the modular symbols x^+ in M^+
attached to the curves `11a1`

, `11a2`

and `11a3`

.

The library syntax is `GEN `

.**ellweilcurve**(GEN E, GEN *ms = NULL)

Computes the Weil pairing of the two points of m-torsion P and Q on the elliptic curve E.

The library syntax is `GEN `

.**ellweilpairing**(GEN E, GEN P, GEN Q, GEN m)

Computes the value at z of the Weierstrass ℘ function attached to
the lattice w as given by `ellperiods`

. It is also possible to
directly input w = [ω_{1},ω_{2}], or an elliptic curve E as given
by `ellinit`

(w = `E.omega`

).

? w = ellperiods([1,I]); ? ellwp(w, 1/2) %2 = 6.8751858180203728274900957798105571978 ? E = ellinit([1,1]); ? ellwp(E, 1/2) %4 = 3.9413112427016474646048282462709151389

One can also compute the series expansion around z = 0:

? E = ellinit([1,0]); ? ellwp(E) \\ 'x implicitly at default seriesprecision %5 = x^-2 - 1/5*x^2 + 1/75*x^6 - 2/4875*x^10 + O(x^14) ? ellwp(E, x + O(x^12)) \\ explicit precision %6 = x^-2 - 1/5*x^2 + 1/75*x^6 + O(x^9)

Optional *flag* means 0 (default): compute only ℘(z), 1: compute
[℘(z),℘'(z)].

For instance, the Dickson elliptic functions *sm* and *sn* can be
implemented as follows

smcm(z) = { my(a, b, E = ellinit([0,-1/(4*27)])); \\ ell. invariants (g2,g3)=(0,1/27) [a,b] = ellwp(E, z, 1); [6*a / (1-3*b), (3*b+1)/(3*b-1)]; } ? [s,c] = smcm(0.5); ? s %2 = 0.4898258757782682170733218609 ? c %3 = 0.9591820206453842491187464098 ? s^3+c^3 %4 = 1.000000000000000000000000000 ? smcm('x + O('x^11)) %5 = [x - 1/6*x^4 + 2/63*x^7 - 13/2268*x^10 + O(x^11), 1 - 1/3*x^3 + 1/18*x^6 - 23/2268*x^9 + O(x^10)]

The library syntax is `GEN `

.
For **ellwp0**(GEN w, GEN z = NULL, long flag, long prec)*flag* = 0, we also have
`GEN `

, and
**ellwp**(GEN w, GEN z, long prec)`GEN `

for the power series in
variable v.**ellwpseries**(GEN E, long v, long precdl)

In standard notation, for any affine point P = (v,w) on the
curve E, we have
[n]P = (φ_{n}(P)ψ_{n}(P) : ω_{n}(P) : ψ_{n}(P)^3)
for some polynomials φ_{n},ω_{n},ψ_{n} in
ℤ[a_{1},a_{2},a_{3},a_{4},a_{6}][v,w]. This function returns
[φ_{n}(P),ψ_{n}(P)^2], which give the numerator and denominator of
the abscissa of [n]P and depend only on v.

? E = ellinit([17,42]); ? T = ellxn(E, 2, 'X) %2 = [X^4 - 34*X^2 - 336*X + 289, 4*X^3 + 68*X + 168] ? P = [114,1218]; ellmul(E,P,2) %3 = [200257/7056, 90637343/592704] ? [x,y] = subst(T,'X,P[1]) \\ substitute P[1] in ellxn(E,2) %4 = [168416137, 5934096] \\ numerator and denominator of 2*P ? x/y \\ check we find ellmul(e,P,2)[1] %5 = 200257/7056

The library syntax is `GEN `

where **ellxn**(GEN E, long n, long v = -1)`v`

is a variable number.

Computes the value at z of the Weierstrass ζ function attached to
the lattice w as given by `ellperiods`

(,1): including quasi-periods
is useful, otherwise there are recomputed from scratch for each new z.
ζ(z, L) = (1)/(z) + z^2∑_{ω ∈ L*}
(1)/(ω^2(z-ω)).
It is also possible to directly input w = [ω_{1},ω_{2}],
or an elliptic curve E as given by `ellinit`

(w = `E.omega`

).
The quasi-periods of ζ, such that
ζ(z + aω_{1} + bω_{2}) = ζ(z) + aη_{1} + bη_{2}
for integers a and b are obtained as η_{i} = 2ζ(ω_{i}/2).
Or using directly `elleta`

.

? w = ellperiods([1,I],1); ? ellzeta(w, 1/2) %2 = 1.5707963267948966192313216916397514421 ? E = ellinit([1,0]); ? ellzeta(E, E.omega[1]/2) %4 = 0.84721308479397908660649912348219163647

One can also compute the series expansion around z = 0 (the quasi-periods are useless in this case):

? E = ellinit([0,1]); ? ellzeta(E) \\ at 'x, implicitly at default seriesprecision %4 = x^-1 + 1/35*x^5 - 1/7007*x^11 + O(x^15) ? ellzeta(E, x + O(x^20)) \\ explicit precision %5 = x^-1 + 1/35*x^5 - 1/7007*x^11 + 1/1440257*x^17 + O(x^18)

The library syntax is `GEN `

.**ellzeta**(GEN w, GEN z = NULL, long prec)

E being an *ell* as output by
`ellinit`

, computes the coordinates [x,y] on the curve E
corresponding to the complex or p-adic parameter z. Hence this is the
inverse function of `ellpointtoz`

.

***** If E is defined over a p-adic field and has multiplicative
reduction, then z is understood as an element on the
Tate curve Q_{p}^{*} / q^ℤ.

? E = ellinit([0,-1,1,0,0], O(11^5)); ? [u2,u,q] = E.tate; type(u) %2 = "t_PADIC" \\ split multiplicative reduction ? z = ellpointtoz(E, [0,0]) %3 = 3 + 11^2 + 2*11^3 + 3*11^4 + 6*11^5 + 10*11^6 + 8*11^7 + O(11^8) ? ellztopoint(E,z) %4 = [O(11^9), O(11^9)] ? E = ellinit(ellfromj(1/4), O(2^6)); x=1/2; y=ellordinate(E,x)[1]; ? z = ellpointtoz(E,[x,y]); \\ non-split: t_POLMOD with t_PADIC coefficients ? P = ellztopoint(E, z); ? P[1] \\ y coordinate is analogous, more complicated %8 = Mod(O(2^4)*x + (2^-1 + O(2^5)), x^2 + (1 + 2^2 + 2^4 + 2^5 + O(2^7)))

***** If E is defined over the complex numbers (for instance over ℚ),
z is understood as a complex number in ℂ/Λ_{E}. If the
short Weierstrass equation is y^2 = 4x^3 - g_2x - g_{3}, then [x,y]
represents the Weierstrass ℘-function
and its derivative. For a general Weierstrass equation we have
x = ℘(z) - b_{2}/12, y = ℘'(z)/2 - (a_{1} x + a_{3})/2.
If z is in the lattice defining E over ℂ, the result is the point at
infinity [0].

? E = ellinit([0,1]); P = [2,3]; ? z = ellpointtoz(E, P) %2 = 3.5054552633136356529375476976257353387 ? ellwp(E, z) %3 = 2.0000000000000000000000000000000000000 ? ellztopoint(E, z) - P %4 = [2.548947057811923643 E-57, 7.646841173435770930 E-57] ? ellztopoint(E, 0) %5 = [0] \\ point at infinity

The library syntax is `GEN `

.**pointell**(GEN E, GEN z, long prec)

Let PQ be a polynomial P, resp. a vector [P,Q] of polynomials, with
rational coefficients.
Determines the reduction at p > 2 of the (proper, smooth) genus 2
curve C/ℚ, defined by the hyperelliptic equation y^2 = P(x), resp.
y^2 + Q(x)*y = P(x).
(The special fiber X_{p} of the minimal regular model X of C over ℤ.)

If p is omitted, determines the reduction type for all (odd) prime divisors of the discriminant.

This function was rewritten from an implementation of Liu's
algorithm by Cohen and Liu (1994), `genus2reduction-0.3`

, see
`http://www.math.u-bordeaux.fr/~liu/G2R/`

.

**CAVEAT.** The function interface may change: for the
time being, it returns [N,*FaN*, T, V]
where N is either the local conductor at p or the
global conductor, *FaN* is its factorization, y^2 = T defines a
minimal model over ℤ[1/2] and V describes the reduction type at the
various considered p. Unfortunately, the program is not complete for
p = 2, and we may return the odd part of the conductor only: this is the
case if the factorization includes the (impossible) term 2^{-1}; if the
factorization contains another power of 2, then this is the exact local
conductor at 2 and N is the global conductor.

? default(debuglevel, 1); ? genus2red(x^6 + 3*x^3 + 63, 3) (potential) stable reduction: [1, []] reduction at p: [III{9}] page 184, [3, 3], f = 10 %1 = [59049, Mat([3, 10]), x^6 + 3*x^3 + 63, [3, [1, []], ["[III{9}] page 184", [3, 3]]]] ? [N, FaN, T, V] = genus2red(x^3-x^2-1, x^2-x); \\ X_{1}(13), global reduction p = 13 (potential) stable reduction: [5, [Mod(0, 13), Mod(0, 13)]] reduction at p: [I{0}-II-0] page 159, [], f = 2 ? N %3 = 169 ? FaN %4 = Mat([13, 2]) \\ in particular, good reduction at 2 ! ? T %5 = x^6 + 58*x^5 + 1401*x^4 + 18038*x^3 + 130546*x^2 + 503516*x + 808561 ? V %6 = [[13, [5, [Mod(0, 13), Mod(0, 13)]], ["[I{0}-II-0] page 159", []]]]

We now first describe the format of the vector V = V_{p} in the case where
p was specified (local reduction at p): it is a triple [p, *stable*,
*red*]. The component *stable* = [*type*, *vecj*] contains
information about the stable reduction after a field extension;
depending on *type*s, the stable reduction is

***** 1: smooth (i.e. the curve has potentially good reduction). The
Jacobian J(C) has potentially good reduction.

***** 2: an elliptic curve E with an ordinary double point; *vecj*
contains j mod p, the modular invariant of E. The (potential)
semi-abelian reduction of J(C) is the extension of an elliptic curve (with
modular invariant j mod p) by a torus.

***** 3: a projective line with two ordinary double points. The Jacobian
J(C) has potentially multiplicative reduction.

***** 4: the union of two projective lines crossing transversally at three
points. The Jacobian J(C) has potentially multiplicative reduction.

***** 5: the union of two elliptic curves E_{1} and E_{2} intersecting
transversally at one point; *vecj* contains their modular invariants
j_{1} and j_{2}, which may live in a quadratic extension of 𝔽_{p} and need
not be distinct. The Jacobian J(C) has potentially good reduction,
isomorphic to the product of the reductions of E_{1} and E_{2}.

***** 6: the union of an elliptic curve E and a projective line which has
an ordinary double point, and these two components intersect transversally
at one point; *vecj* contains j mod p, the modular invariant of E.
The (potential) semi-abelian reduction of J(C) is the extension of an
elliptic curve (with modular invariant j mod p) by a torus.

***** 7: as in type 6, but the two components are both singular. The
Jacobian J(C) has potentially multiplicative reduction.

The component *red* = [*NUtype*, *neron*] contains two data
concerning the reduction at p without any ramified field extension.

The *NUtype* is a `t_STR`

describing the reduction at p of C,
following Namikawa-Ueno, *The complete classification of fibers in
pencils of curves of genus two*, Manuscripta Math., vol. 9, (1973), pages
143-186. The reduction symbol is followed by the corresponding page number
or page range in this article.

The second datum *neron* is the group of connected components (over an
algebraic closure of 𝔽_{p}) of the Néron model of J(C), given as a
finite abelian group (vector of elementary divisors).

If p = 2, the *red* component may be omitted altogether (and
replaced by `[]`

, in the case where the program could not compute it.
When p was not specified, V is the vector of all V_{p}, for all
considered p.

**Notes about Namikawa-Ueno types.**

***** A lower index is denoted between braces: for instance,
`[I{2}-II-5]`

means `[I`

._{2}-II-5]

***** If K and K' are Kodaira symbols for singular fibers of elliptic
curves, then `[K-K'-m]`

and `[K'-K-m]`

are the same.

We define a total ordering on Kodaira symbol by fixing `I`

< `I*`

<
`II`

< `II*`

,.... If the reduction type is the same, we order by
the number of components, e.g. `I`

_{2} < `I`

_{4}, etc.
Then we normalize our output so that K ≤ K'.

***** `[K-K'--1]`

is `[K-K'-α]`

in the notation of
Namikawa-Ueno.

***** The figure `[2I`

in Namikawa-Ueno, page 159, must be denoted
by _{0}-m]`[2I`

._{0}-(m+1)]

The library syntax is `GEN `

.**genus2red**(GEN PQ, GEN p = NULL)

X being a non-singular hyperelliptic curve defined over a finite field, return the characteristic polynomial of the Frobenius automorphism. X can be given either by a squarefree polynomial P such that X: y^2 = P(x) or by a vector [P,Q] such that X: y^2 + Q(x) y = P(x) and Q^2+4 P is squarefree.

The library syntax is `GEN `

.**hyperellcharpoly**(GEN X)

Let X be the curve defined by y^2 = Q(x), where Q is a polynomial of
degree d over ℚ and q ≥ d is a prime such that X has good reduction
at q. Return the matrix of the Frobenius endomorphism ϕ on the
crystalline module D_{p}(X) = ℚ_{p} ⨂ H^1_{dR}(X/ℚ) with respect to the
basis of the given model (ω, x ω,...,x^{g-1} ω), where
ω = dx/(2 y) is the invariant differential, where g is the genus of
X (either d = 2 g+1 or d = 2 g+2). The characteristic polynomial of
ϕ is the numerator of the zeta-function of the reduction of the curve
X modulo q. The matrix is computed to absolute q-adic precision q^n.

Alternatively, q may be of the form [T,p] where p is a prime,
T is a polynomial with integral coefficients whose projection to
𝔽_{p}[t] is irreducible, X is defined over K = ℚ[t]/(T) and has good
reduction to the finite field 𝔽_{q} = 𝔽_{p}[t]/(T). The matrix of
ϕ on D_{q}(X) = ℚ_{q} ⨂ H^1_{dR}(X/K) is computed
to absolute p-adic precision p^n.

The library syntax is `GEN `

.
The functions
**hyperellpadicfrobenius0**(GEN Q, GEN q, long n)`GEN `

and
**hyperellpadicfrobenius**(GEN H, ulong p, long n)`GEN `

are also
available.**nfhyperellpadicfrobenius**(GEN H, GEN T, ulong p, long n)

X being a non-singular hyperelliptic curve given by an rational model,
return a vector containing the affine rational points on the curve of naive
height less than h.a If *flag* = 1, stop as soon as a point is found; return
either an empty vector or a vector containing a single point.

X is given either by a squarefree polynomial P such that X: y^2 = P(x) or by a vector [P,Q] such that X: y^2+Q(x) y = P(x) and Q^2+4 P is squarefree.

The parameter h can be

***** an integer H: find the points [n/d,y] whose abscissas x = n/d have
naive height ( = max(|n|, d)) less than H;

***** a vector [N,D] with D ≤ N: find the points [n/d,y] with
|n| ≤ N, d ≤ D.

***** a vector [N,[D_{1},D_{2}]] with D_{1} < D_{2} ≤ N find the points
[n/d,y] with |n| ≤ N and D_{1} ≤ d ≤ D_{2}.

The library syntax is `GEN `

.**hyperellratpoints**(GEN X, GEN h, long flag)