files / problems / simon-lieb-thirring / compute / record.json
{
"classical": {
"formula": "2^{-d} pi^{-d/2} Gamma(gamma+1)/Gamma(gamma+1+d/2)",
"Lcl_1_1": 0.21220659078919374,
"Lcl_1_1_closed": "2/(3pi)",
"Lcl_1_1_closed_value": 0.2122065907891938,
"Lcl_3_2_1": 0.18750000000000003,
"Lcl_3_2_1_closed": "3/16",
"Lcl_3_2_1_closed_value": 0.1875,
"Lcl_1_3": 0.0067547455761558526
},
"published": {
"fhjn_theorem_1_ratio": 1.456,
"fhjn_finer_ratio": 1.455786,
"one_bound_state_over_classical_1d_gamma1": 1.1547005383792517,
"citation": "Frank\u2013Hundertmark\u2013Jex\u2013Nam, arXiv:1808.09017 / JEMS 23 (2021)"
},
"sech2_witnesses": [
{
"nu": 1,
"gamma": 1.0,
"n_bound": 1,
"moment": 1.0,
"integral": 4.442882938158366,
"ratio": 0.22507907903927651,
"ratio_over_classical": 1.0606601717798214
},
{
"nu": 2,
"gamma": 1.0,
"n_bound": 2,
"moment": 5.0,
"integral": 23.085896942913553,
"ratio": 0.21658244478713226,
"ratio_over_classical": 1.0206207261596578
},
{
"nu": 3,
"gamma": 1.0,
"n_bound": 3,
"moment": 14.0,
"integral": 65.29677711243184,
"ratio": 0.21440568155291914,
"ratio_over_classical": 1.0103629710818454
},
{
"nu": 4,
"gamma": 1.0,
"n_bound": 4,
"moment": 30.0,
"integral": 140.49629462081452,
"ratio": 0.2135287630251531,
"ratio_over_classical": 1.0062305898749055
},
{
"nu": 1,
"gamma": 1.25,
"n_bound": 1,
"moment": 1.0,
"integral": 4.836056776129937,
"ratio": 0.20678003718563695,
"ratio_over_classical": 1.0405562256273813
},
{
"nu": 2,
"gamma": 1.25,
"n_bound": 2,
"moment": 6.656854249492381,
"integral": 33.0714766470665,
"ratio": 0.2012868769221666,
"ratio_over_classical": 1.01291360505182
},
{
"nu": 3,
"gamma": 1.25,
"n_bound": 3,
"moment": 22.245311517612276,
"integral": 111.23874463866059,
"ratio": 0.1999780884787242,
"ratio_over_classical": 1.0063275342618696
}
],
"note": "Witness ratios are lower bounds on L(gamma,1), not upper bounds. They do not improve 1.456."
}