Chirped laser pulses provide sufficient electric and magnetic fields that easily cause fission fusion and all decay products known. Holmlid uses laser pulses.
________________________________ From: Adrian Ashfield <a.ashfi...@verizon.net> Sent: Friday, April 28, 2017 9:26 AM To: vortex-l@eskimo.com Subject: Re: [Vo]:The Kerr effect Axil Axil, Lattice QCD in strong magnetic Fields is too dense for me by an order of magnitude. I subscribe to the theory that if one truly understands the situation they can explain it in relatively simple terms. So what would you propose as a demonstration of LENR with a parameter that could be altered to prove your theory? -----Original Message----- From: Axil Axil <janap...@gmail.com> To: vortex-l <vortex-l@eskimo.com> Sent: Tue, Apr 25, 2017 7:29 pm Subject: Re: [Vo]:The Kerr effect IMHO, Holmlid's recent experiments using a fast high electric field to induce meson production has proved the theory. This result shows that the SPP requires an electrostatic field stimulus to produce the super strong magnetism necessary to activate nucleon decay. Also, the use of anisotropic magnets (SmCo5) to induce LENR shows that magnetism disrupts the gluon condensate inside the proton and neutron. Even through there is a difference between a monopole fundamental particle, a synthetic monopole quasiparticle like the SPP, and an anisotropic magnetic field formatted by a pertinent magnet to support monopole flux lines, the magnetic field produces the same effect. The SmCo5 magnet produces a magnetic field that is anisotropic field (almost a monopole formated magnetic field). This SmCo5 type magnetic supports monopole flux lines of force. That is why the SmCo5 magnet can produce a LENR reaction. To refresh your memory, see http://www.mail-archive.com/vortex-l@eskimo.com/msg108069.html The details of what a strong monopole magnetic field does to the insides of the proton and neutron is yet to be determined. I am trying to understand this: See http://www.slac.stanford.edu/econf/C0906083/pdf/25.pdf Lattice QCD in strong magnetic flelds<http://www.slac.stanford.edu/econf/C0906083/pdf/25.pdf> www.slac.stanford.edu Lattice QCD in strong magnetic flelds P.V.Buividovichab, M.N.Chernodubcdb x, E.V.Luschevskayab, M.I.Polikarpovb a JIPNR \Sosny", National Academy of Science, Krasin ... Lattice QCD in strong magnetic Fields On Tue, Apr 25, 2017 at 6:31 PM, Adrian Ashfield <a.ashfi...@verizon.net<mailto:a.ashfi...@verizon.net>> wrote: AXil Axil, As usual you have come up with a very imaginative theory that sounds just as likely or unlikely as myriads of others. My question is how can it be proved or falsified? -----Original Message----- From: Axil Axil <janap...@gmail.com<mailto:janap...@gmail.com>> To: vortex-l <vortex-l@eskimo.com<mailto:vortex-l@eskimo.com>> Sent: Tue, Apr 25, 2017 4:29 pm Subject: Re: [Vo]:The Kerr effect LENR in a nutshell LENR is an optical based process where light is trapped in a waveform called a soliton. Think of this structure as Nano sized ball lightning. This ball of light can form in many ways: inside ultra-dense hydrogen, on the surface of rough metal surfaces, inside cracks in metal, on nanoparticles and microparticles, between nanoparticles, and in dusty plasma. But critically, this soliton is not active until it is triggered through the electrostatic effects of a stimulating emission. When this soliton first form, light rotates around inside the soliton and supports two degenerate propagating-wave modes: clockwise (CW) and counterclockwise (CCW) waves, manifesting the symmetry of this system. This counter rotation of the light negates any organization of the spin of the light from generating any meaningful magnetic effect. But when the symmetry of this counter rotating light is broken by this electrostatic stimulant, like a magnet all spin of the light ceases to interfere with each other and a newly organized super intense magnetic beam projects out of the soliton in an highly organized mode. The soliton then becomes a synthetic analog monopole quasiparticle. When this beam of magnetism enters inside protons and neutrons that move into its path, the quarks that make up these protons and neutrons change their type(color) and the protons and neutrons transform into exotic mesons made up of strange and beauty quark types. Energy is also produced in these subatomic particle decays and is feed back into the solitons of light thereby increasing their intensity. In this way, this infusion of incoming subatomic energy allows the soliton to survive for an extended period in a self-sustaining mode while the electrostatic stimulant continues to maintain the organization of the photonic spin. Leif Holmlid has been using a laser pulse as the stimulator but yesterday Sveinn Olafsson just told me this: “Leif has applied fast high electric field and sees meson signal” On Sun, Apr 23, 2017 at 9:47 PM, Axil Axil <janap...@gmail.com<mailto:janap...@gmail.com>> wrote: A post that might hold some insights as follows: 1. Giuseppe April 23, 2017 at 3:37 PM<http://www.journal-of-nuclear-physics.com/?p=892&cpage=230#comment-1276782> Dear Andrea, seems that to activate the E-Cat you need heat, does the QuarkX need heat to be activated? Best regards, Giuseppe 2. Andrea Rossi April 23, 2017 at 3:48 PM<http://www.journal-of-nuclear-physics.com/?p=892&cpage=230#comment-1276783> Giuseppe: Not exactly. The mechanism is much more complex and is based on electromagnetic fields. Warm Regards, A.R. ================ The nature of the LENR reaction has evolved when the gas envelope is in the plasma state to depend solely on optical mechanisms. An EMF trigger is the factor can gets the LENR reaction going. not heat. As stated in the Rossi patent, very high voltage electrostatic potential is that trigger. The name of the triggering effect is "kerr effect". The minimum voltage at which the kerr effect is triggered is 30,000 volts. This trigger applies to both Rossi's low temperature reactions and his plasma based reactions. Kerr electro-optic effect The Kerr electro-optic effect, or DC Kerr effect, is the special case in which a slowly varying external electric field is applied by, for instance, a voltage<https://en.wikipedia.org/wiki/Voltage> on electrodes across the sample material. Under this influence, the sample becomes birefringent<https://en.wikipedia.org/wiki/Birefringent>, with different indices of refraction for light polarized<https://en.wikipedia.org/wiki/Polarization_(waves)> parallel to or perpendicular to the applied field. The difference in index of refraction is controlled by the strength of the applied electric field. [1-physicistsob.jpg] Birefringence modifies how light behaves inside a whispering gallery wave. Birefringence is the optical<https://en.wikipedia.org/wiki/Optics> property of a material having a refractive index<https://en.wikipedia.org/wiki/Refractive_index> that depends on the polarization<https://en.wikipedia.org/wiki/Polarization_(waves)> and propagation direction of light<https://en.wikipedia.org/wiki/Light>. These optically anisotropic<https://en.wikipedia.org/wiki/Anisotropic> materials are said to be birefringent (or birefractive). The birefringence is often quantified as the maximum difference between refractive indices exhibited by the material. Crystals<https://en.wikipedia.org/wiki/Crystal> with non-cubic crystal structures<https://en.wikipedia.org/wiki/Crystal_structure> are often birefringent, as are plastics<https://en.wikipedia.org/wiki/Plastic> under mechanical stress<https://en.wikipedia.org/wiki/Mechanical_stress>. The kerr effect produces a change in stated of the optical properties that underpin the LENR reaction. Research should be directed at finding where that change of state sets in. As in Holmlid's experiments, a laser can produce the kerr effect Optical Kerr effect The optical Kerr effect, or AC Kerr effect is the case in which the electric field is due to the light itself. This causes a variation in index of refraction which is proportional to the local irradiance<https://en.wikipedia.org/wiki/Irradiance> of the light. This refractive index variation is responsible for the nonlinear optical<https://en.wikipedia.org/wiki/Nonlinear_optics> effects of self-focusing<https://en.wikipedia.org/wiki/Self-focusing>, self-phase modulation<https://en.wikipedia.org/wiki/Self-phase_modulation> and modulational instability<https://en.wikipedia.org/wiki/Modulational_instability>, and is the basis for Kerr-lens modelocking<https://en.wikipedia.org/wiki/Kerr-lens_modelocking>. This effect only becomes significant with very intense beams such as those from lasers<https://en.wikipedia.org/wiki/Laser>. The optical Kerr effect has also been observed to dynamically alter the mode-coupling properties in multimode fibre, a technique that has potential applications for all-optical switching mechanisms.
