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York City and you put energy on over here for two or three or Now if you think about this, it seems correct. four days, you don't have to take it off over there. It's okay; you He said, "Dave, what we really need is a material that totally can keep putting it in. When they want the energy in New York _ bends space-time; a material that has no gravitational attraction at they can resonant-frequency-tune the wire, apply voltage and suck _ all. Less than zero." it out. It gets a free ride from Portland all the way to New York It's what he called “exotic matter" in his papers. on this quantal wave of the superconductor—as light, not electric- I said, “Hal, do you realise that if you heat this material it has ity. No gravitational attraction at all?" How do you measure this light if it has no voltage in it? How is I'd been reading papers on the vacuum energy. Do you know it possible to get a machine that can measure this light? Guess that there is an overlap between the thermal spectrum and the what? It can't be done, ‘cause every piece of instrumentation man —_zero-point spectrum? The two of them overlap. So if you heat has ever figured out always uses a differential that it must reflect, | something, it should interact with the zero-point energy. Well, and yet a superconductor has no voltage. because this material is resonating in two dimensions, when you You literally start the superconductor flowing by applying a _ heat it, it literally loses all gravitational attraction. You know Magnetic field. It responds to the magnetic field by flowing light | what Hal Puthoff said to me? inside of it and building a bigger Meissner field around itself. He said, "Dave, at that point you shouldn't be able to see the You can put your magnet down and walk away. You cancome material." back a hundred years later and the supercon- ductor is still flowing exactly the same as when you left. It doesn't ever slow down. It excludes not 99.99999, but 100.00000 per cent of all external magnetic fields. There is absolutely no resistance in the sample; it is Perpetual motion. It runs for ever and ever and ever and ever. The Russian physicist Sakharov said in the 1960s that we are looking for gravity but we are never going to find it as a magnetic field. Gravity is what is produced when protons, neutrons and electrons interact with the vac- material only weighs uum energy—that energy that is everywhere Ry in the Universe, timeless; that energy 56) per cent of its. is not there, pass an arm through the that is there like the ether. When you sample pan. If it is there and resonat- pump out all heat and all matter, every- true mass, you do ing at a frequency that you don't per- thing, there still is energy there—the ceive, you knock it out of the pan— vacuum energy. If there is no matter, because when you cool it down and it there is no gravity. Interesting theory. : begins to reappear, it always appears in Everyone kind of ignored it fora while materia is actu ily the same shape and place it was in There's this fellow by the name of bending oe before it left. That's proof that it left Hal Puthoff, who worked over in the ‘ s these three dimensions." And he said, Bay Area in California doing distant- space-time?" "Dave, if you do that, you will never viewing experimentation and is now ever want for money." working down in Austin, Texas [at the In 1988 I not only filed a patent on Institute for Advanced Studies]. He ORMEs [Orbitally Rearranged actually developed the mathematics for Monatomic Elements], I filed patents Sakharov's theory of gravity and pub- on S-ORMEs, the resonant coupled lished it in one of the top science journals.' quantum oscillating system of many atoms of these ORMEs. I In the mathematics he shows that when matter begins to interact have 11 patents on ORMEs and another 11 patents on S-ORMEs. in two dimensions, as opposed to interacting in three dimensions _I have 22 patents. (by definition, a superconductor is a resonance-coupled quantum So, what are some of the other aspects of a superconductor? oscillator resonating in two dimensions, not three dimensions), it | How do you prove a superconductor is a superconductor? You should theoretically lose four-ninths of its gravitational weight. __ literally take a constant magnetic field and you pass the material I said, “Correct. You can look in the pan through the quartz tube and there is nothing in the pan. But the pan isn't weighing what it would weigh if the stuff wasn't in it.” Now I had mistakenly assumed that the material was just resonating at a frequency we didn't perceive. He said, "Dave, theoretically it should be withdrawing from these three dimensions. It should not even be in these three dimen- sions." I said, "Wow!" He said, "Dave, you have to devise an experiment where you can do this: while it Did you know that five-ninths is 56 per cent, exactly? into the constant magnetic field. I decided, "I've got to go down and see Hal Puthoff. I've got to If it's not a superconductor, if you apply a magnetic field you take all my data and go down and see Hal Puthoff.” get positive inductance. If you graph it—applied magnetic field So I did, and I said to him, "Hal, we have the experimental con- _-vs inductance; magnetic field vs inductance—and if it's a perfect firmation that, in fact, your mathematics are absolutely correct. In _ insulator, you'll run totally parallel. No matter how much magnet- addition, Sakharov's theory of gravity is absolutely correct, __ic field you apply, no inductance. If it's a perfect conductor, just because this material only weighs 56 per cent when it goes to the _the littlest amount of magnetic field on it will make the graph go superconducting state. straight up. Hal Puthoff said, “Dave, you do realise that gravity is what If it's a superconductor, as you apply a magnetic field it goes determines space-time? When this material only weighs 56 per _ negative. It literally eats the magnetic field. It feeds on the mag- cent of its true mass, you do realise that this material is actually _ netic field and takes it inside itself. Negative inductance in a pos- bending space-time?" itive-applied magnetic field is the proof of a superconductor. Now if you think about this, it seems correct. He said, "Dave, what we really need is a material that totally bends space-time; a material that has no gravitational attraction at all. Less than zero." It's what he called “exotic matter" in his papers. I said, “Hal, do you realise that if you heat this material it has no gravitational attraction at all?" I'd been reading papers on the vacuum energy. Do you know that there is an overlap between the thermal spectrum and the zero-point spectrum? The two of them overlap. So if you heat something, it should interact with the zero-point energy. Well, because this material is resonating in two dimensions, when you heat it, it literally loses all gravitational attraction. You know what Hal Puthoff said to me? He said, "Dave, at that point you shouldn't be able to see the material." 46 * NEXUS OCTOBER - NOVEMBER 1996