Notes:

Isotopes of Palladium

• 102 - 0+ - 0.0102
• 104 - 0+ - 0.1114
• 105 - 5/2+ - 0.2233
• 106 - 0+ - 0.2733
• 108 - 0+ - 0.2646
• 110 - 0+ - 0.1172

Pd·D and Pd·H are superconductive at 10K and 8K

"semiconductive" Pd·D at relative high (>50%) concentrations

micro - nano - pico - femto

Proposed process:

Deuterium is absorbed into Palladium (fcc) lattice. Octahedral holes are filled from 0% to 2% as single D₂ atoms/ions in the Pd·D alpha phase. As additional Deuterium is added, the Pd·D (expanded lattice) beta phase is fully reached at 58% saturation. Above 50% saturation, the electron structure of the palladium lattice is altered significantly becoming a semiconductor. Normal atmospheric pressure saturation is at 70% of the octahedral holes filled.

The number of deuterium atoms per unit volume (partial pressure) appears to be much higher in the metal lattice than as gas. The metal lattice is isolating the atoms from one another until the conductivity is changed.  As the metallic conductivity is lost, interaction between atoms increases. Pauli Exclusion can be used to describe this form of pressure.

The number of atoms can be increased by adding sufficient energy to alter some percentage of the atom/ions (NMR). The higher energy deuterium would normally drop back to base levels. The amount of excess deuterium would be limited by the time some of the deuterium would be flipped. The low/high time ratio can be moderated the structure of the lattice. Using a careful arraignment of spin zero and spin five halves palladium, some of the deuterium can find octahedral holes where the potential forces to revert to low energy is somewhat less attractive.

Current flow through the Pd·D will induce a motion in the deuterium. A string of quark gravy (quark soup is already used), which is the nucleus, occurs as the deuterium ions move from one hole to the next. As the strings move about, two with opposing spin can have their wave functions intersect.

D₂^↓ + D₂^↑ ↔ He₄^↑ (bi-directional with high energy He)

He₄^↑ → He₄^↓ + energy

Questions:

How to coerce the energy from the He₄^↑ in a form that does not distort the palladium lattice.

How to get the He₄^↓ out of the palladium lattice.

States of normal matter vs. states of ionized matter vs. states of completely ionized matter

Behavior of composites/mixtures/solutions of different states and ionizations

Elastic interactions

Electron flow without using magnets and coils; thermocouples and piezoelectric.

Magnetism and "strain-induced martensite"

Ferromagnetic, paramagnetic, and diamagnetic