One atomic unit of magnetic field is defined for a Bohr magneton in a B field which has the energy of 13.6 eV.
Thus 1 a.u. of magnetic field = *2.35x10^^**5 *Tesla On Thu, Dec 19, 2013 at 1:15 PM, Axil Axil <[email protected]> wrote: > The magnetic field is atomic level. The next step in the research that the > Ni/H reactor developers need to do is measure the magnetic fields that they > are developing in their reactions. This can be done using sub-micron hall > effect probes. > > > On Thu, Dec 19, 2013 at 1:10 PM, John Franks <[email protected]> wrote: > >> What's the magnitutde magnetic field and how do heavy hadrons display >> these collective properties like light leptons? >> >> >> >> On Thu, Dec 19, 2013 at 6:05 PM, Axil Axil <[email protected]> wrote: >> >>> FQHE reduces the inherent charge of fermions as a function of increasing >>> magnetic field. >>> >>> The nucleus is a fermion, the protons and neutrons are fermions and so >>> are quarks. >>> >>> Why should a magnetic field make a distinction in the way it >>> reduces charge is the various types of fermions? I won't. >>> >>> >>> On Thu, Dec 19, 2013 at 12:59 PM, John Franks <[email protected]> wrote: >>> >>>> "Is like or maybe is" >>>> >>>> How so? Once again, QHE or FQHE is to do with cooperative properties of >>>> light leptons. So how does this carry over to heavy hadrons and what does >>>> that have to do with CF? >>>> >>>> >>>> On Thu, Dec 19, 2013 at 5:53 PM, Axil Axil <[email protected]> wrote: >>>> >>>>> Cold fusion is like(or maybe is) the Factional Quantum Hall >>>>> Effect(FQHE). Science did not believe that something like the FQHE was >>>>> possible until it was shown experimentally. Cold fusion is the FQHE moved >>>>> over to the fermions of the fermions of the atomic nucleus. >>>>> >>>>> >>>>>> >>>>>> If you are suggesting BEC, well electrons are leptons and light, how >>>>>> can you get heavy hadrons into one coherent state at room temperature? If >>>>>> this is the case, has CF been observed to occur spontaneously in liquid >>>>>> H2? >>>>>> >>>>> >>>> >>> >> >
