My Library

But I lost sight of all of them except Puthoff. Even my humble self ceased to be a body, becoming a yellow haze with eyes in it. Those eyes focused on Puthoff, whom I asked: "How the fuck am I supposed to influence something I can't see???" But Puthoff was ready for me. "Now, Ingo," he began, "you wanted an experiment that has no loopholes in it. Well, here it is." And he then went on to explain. And I now explain here. First of all, since the equipment was buried in concrete, no one could say that anyone could have an opportunity to fool around with it. The quark detector, the magnetometer inside it, had been subjected to tests with large electromagnets, and no signals had been induced in the shielded portion. Prior to our arrival, a decaying magnetic field had been set up inside the shielded chamber. Its steady, slow decay with time provided a background calibration signal that registered as a sine wave output on an x-y recorder, the frequency of the sine wave corresponding to the decay rate of the calibration field. Further, this system had been running for something on the order of an hour before our arrival with no "noise" showing up in the sine wave. The quark-detecting function of this instrument was not in operation, and so the experiment would pertain only to the operating magnetometer housed deep within the various shieldings. Puthoff explained that if I were to affect the magnetic field in the magnetometer, evidence of the effect would show up as a change in the output sine wave recording. This would be seen as some kind of variation in the sine wave -- which was slowly moving up and down in a wavy line with an obvious equal rhythm.