Ultra Low Energy Nuclear Synthesis via Three-Body Resonances in Cuboctahedron CsH2Pd12 Cluster

The three-body nuclear and molecular resonances for 135 55 Cs+ 21 H+ 21 H, and 133 55 Cs+ 31 H+ 31 H systems are calculated in "cuboctahedron 135 55 Cs21H2 A46Pd12 and 133 55 Cs31H2 A46Pd12 clusters" in a very wide range from 0.01[fm] to several hundreds of nm in "one stretch" with more than "100 significant figures", where the mass number A of Pd could be 102, 104, 105, 106, 108, 110 but neglected hereafter, because Pd isn't concerned directly with the nuclear reaction. We obtained several new "three-ion resonance states" between the expected molecular CsH2 ground state and the first excited state in cuboctahedron CsH2Pd12 cluster, where H represents either a 11 H, a 21 H, or a 31 H, respectively. The molecular "ground and the first excited states" in the cluster are derived by the Kohn-Sham equation or the ADF package which could mainly describe many electrons rather than cores of ions. We found that the E2 transition times from some CsH2 (7/2+) resonance states (or the IOS states) to the nuclear 139 57 La (7/2+) ground state are about t = 10(-1) similar to 10-6sec for five traditional potentials, and t = 10(-2) similar to 10-8sec for six potentials with our long range three-body force (3BLF) where the "molecular resonances" can strongly interfere with the "nuclear resonances". The thermal nuclear "critical reaction value" (or fusion constant) and/or ultra low energy corresponding value: Chigh/low=(duration time)x(density)x(energy or temperature) are compared. It was found that Clow is almost the same order as Chigh or more. Finally, an ignition method for the synthesis will be discussed.