files / problems / hilbert16-limit-cycles / compute / q1 / b-cubic-fourteen / certificate.json
{
"abelian_integral": {
"I_h": "pi*mu*h*(2 - h)",
"I_over_pi_mu_coeffs_h_high_to_low": [
"-1",
"2",
"0"
],
"I_prime_at_2": "-2*pi*mu",
"methods_agree": [
"trig_parametrization",
"green_disk_flux"
],
"note": "A simple zero of the first-order Abelian integral gives a unique hyperbolic cycle near the circle of radius 2 for sufficiently small \u03bc>0 (Poincar\u00e9\u2013Pontryagin). Uniqueness for every \u03bc>0 is the Li\u00e9nard theorem, not this integral.",
"perturbation_P1": "0",
"perturbation_Q1": "-(x**2 - 1)*y",
"positive_zeros": [
"2"
],
"simple_at_h2": true,
"unperturbed_H": "(x**2 + y**2)/2"
},
"energy": {
"cartesian_dE_dt": "-mu*(x**2 - 1)*y**2",
"closed_orbit_must_meet_both_strips": true,
"lienard_dW_dt": "-x*F(x)",
"lienard_dW_dt_expanded": "-mu*x**2*(x**2/3 - 1)"
},
"equilibrium": {
"charpoly_lambda": "lambda**2 - mu*lambda + 1",
"det_at_0": "1",
"jacobian_at_0": [
[
"0",
"1"
],
[
"-1",
"mu"
]
],
"origin_is_source": true,
"trace_at_0": "mu",
"unique_equilibrium": [
0,
0
]
},
"exact_statement": "For every real mu>0 the cubic van der Pol field dx/dt=y, dy/dt=-x-mu*(x**2-1)*y satisfies the hypotheses of Lienard's uniqueness theorem, hence has exactly one periodic orbit, and that orbit is asymptotically stable. Separately, its first-order Abelian integral on the ovals of H=(x**2+y**2)/2 is I(h)=pi*mu*h*(2-h), with exactly one positive simple zero, at h=2.",
"field": {
"P": "y",
"Q": "-x - mu*(x**2 - 1)*y",
"deg_P": 1,
"deg_Q": 3,
"degree": 3
},
"h3_lower_bound_claimed": false,
"hn_moved": false,
"imagined_claim": "An explicit real cubic planar field with 14 isolated periodic orbits, beating Li\u2013Liu\u2013Yang H(3)>=13.",
"isolated_periodic_orbits": 1,
"lienard_hypotheses": {
"F": "mu*(x**3/3 - x)",
"F_factored": "(mu/3)*x*(x**2 - 3)",
"F_negative_on": "(0, sqrt(3))",
"F_odd": true,
"F_positive_on": "(sqrt(3), oo)",
"F_prime_at_0": "-mu",
"F_prime_at_sqrt3": "2*mu",
"F_prime_positive_on_tail": true,
"F_tends_to_plus_infinity": true,
"G": "x**2/2",
"G_tends_to_plus_infinity": true,
"f": "mu*(x**2 - 1)",
"g": "x",
"g_odd": true,
"positive_zero_of_F": "sqrt(3)",
"theorem": "Li\u00e9nard uniqueness for \u1e8b=y-F(x), \u1e8f=-x with F odd, one positive zero a, F<0 on (0,a), F>0 and F'>0 on [a,\u221e), F\u2192\u221e. Conclusion: exactly one periodic orbit, asymptotically stable.",
"xg_positive_off_zero": true
},
"line": "B",
"not_the_radial_family": {
"distinct_from_radial_family": true,
"radial_P": "y - x*(x**2 + y**2 - rho**2)",
"radial_Q": "-x - y*(x**2 + y**2 - rho**2)",
"this_P": "y",
"this_Q": "-x - mu*(x**2 - 1)*y"
},
"parameter": "mu>0",
"published_record": "H(3)>=13, Li\u2013Liu\u2013Yang, J. Differ. Equations 246 (2009). Not replayed (paywalled). Not beaten.",
"status": "fork",
"what_this_is_not": [
"not a dent of H(3)",
"not a claim that H(3)>=14",
"not a replay of Li\u2013Liu\u2013Yang's 13 cycles",
"not a lower bound from numerics"
]
}