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curve #216

y2 + xy = x3 − 292164008972198360516541x + 60777760375298123458072491954931825
a-invariants
[1, 0, 0, -292164008972198360516541, 60777760375298123458072491954931825]
rank (lower bound)
≥ 17
conductor (N)
8229621766982592642433268362527136439092061141374442470
naive height
173.7084
Faltings height
12.1714
discriminant (Δ)
319660562013917792358156721464086339946753006672777251625449427814400
primes of bad reduction
2, 5, 11, 29, 37, 41, 61, 257, 2467, 4177, 40298971, 453713587, 575746473701180535499
regulator
605706094414059953.433928438056900702744283818617694394403423434391605716
submitted by
Edgar Costa
last updated
2026-07-01 22:35:41

Witness: 17 independent points

Commentary

Specialization at T = -2407/2 of the Mestre/Fermigier family y^2 = r(x,T), where r is the degree-<=4 remainder in p6(x-T)*p6(x+T) = g(x)^2 - r (g monic of degree 6), p6(x) = prod_i(x-a_i) on the sextuple (a) = (-44, -60, -6, 110, 94, -94). Located by a Mestre-Nagao sieve of this family for small-conductor high-rank specializations. Seventeen independent rational points were found by rational-x enumeration on the quartic plus a direct minimal-model x = n/q^2 sieve; rank >= 17 follows from the positive-definiteness of their 17x17 Neron-Tate height-pairing matrix, computed independently in Sage and Magma. Conductor by Tate's algorithm. Proven lower bound on the Mordell-Weil rank (no exact-rank, Selmer, or BSD claim).

last edited by Edgar Costa at 2026-06-25 21:52:44 · history

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