In the latest theories of the nucleus, Anapole magnetic fields are produced by monopole field magnetic generation by quark/antiquark pairs inside nuclear subatomic particles. In the latest standard model theories of the nucleus, quarks are monopoles.
This idea comes from the newly developing theory of quantum chromodynamics called the dual superconductor model. For more background on this theory see as follows: http://ccdb5fs.kek.jp/tiff/2012/1227/1227046.pdf Non-Abelian dual superconductivity and Gluon propagators in the deep IR region for SU(3) Yang-Mills theory. In this theory of quantum chromodynamics, the dual superconductor model attempts to explain confinement of quarks in terms of an electromagnetic dual theory of superconductivity. According to this theory,the strong force is just works in reverse of electromagnetic behavior when EMF is active inside the nucleus of the atom. In this electromagnetic dual theory, the roles of electric and magnetic fields are interchanged. In standard EMF theory, the BCS theory of superconductivity explains superconductivity as the result of the condensation of electric charges into Cooper pairs. In a dual superconductor nuclear model, an analogous effect occurs through the condensation of magnetic charges generated by quarks (also called magnetic monopoles). In ordinary electromagnetic theory, no monopoles have been shown to exist. However, in quantum chromodynamics — the theory of color charge which explains the strong interaction between quarks — the color charges can be viewed as (non-abelian) analogues of electric charges and corresponding magnetic monopoles are known to exist. Dual superconductor models posit that condensation of these magnetic monopoles in a superconductive state explains color confinement — the phenomenon that only neutrally colored bound states are observed at low energies. Color confinement is the area of nuclear activity where the LENR reaction operates. Qualitatively, confinement in dual superconductor models can be understood as a result of the dual to the Meissner effect. The Meissner effect says that a superconducting metal will try to expel magnetic field lines from its interior. If a magnetic field is forced to run through the superconductor, the electric field lines are compressed in magnetic flux tubes. In a dual superconductor the roles of magnetic and electric fields are exchanged and the Meissner effect tries to expel electric field lines. Quarks and antiquarks carry opposite color charges, and for a quark–antiquark pair 'electric' field lines run from the quark to the antiquark. In a pion, the quark–antiquark pair is immersed in a vacuum based dual superconductor (aka the Higgs field), and then the electric field lines get compressed into a flux tube. The confinement energy carried by the tube is proportional to its length, and the potential energy of the quark–antiquark is proportional to their separation. The energy of colored objects gets large if quark/antiquark pair moves apart by any significant distance. A quark–antiquark will therefore always bind regardless of their separation, which explains why no unbound quarks are ever found. Dual superconductors are described by (a dual) the Landau–Ginzburg model, which is equivalent to the Abelian Higgs model. The MIT bag model boundary conditions for gluon fields are those of the dual color superconductor. Based on these theories, it is posited that a monopole field (aka anapole) will disrupt the duel superconductive mechanism that keeps the nucleus and the nucleons that make it up together. How can this monopole magnetic field disrupt a nucleus? The Higgs theory is a superconductive magnetic mechanism of QCD and states that quarks are monopoles. The pions can be interpreted as the magnetic gauge boson. http://phys.cts.ntu.edu.tw/si2012/files%5CRyuichiroKitano.ppt.pdf Hadron physics as Seiberg dual of QCD Ryuichiro Kitano (Tohoku U.) see also http://arxiv.org/pdf/1206.7114.pdf Origins of Mass by Frank Wilczek Page 12: One cannot tolerate, for example, anomalous color magnetic moments, for either quarks or gluons. If anomalous quantum chromodynamic magnetic Moments can be induced inside the nucleus, we can perturb inner workings of the nuclear mechanism. This is what the Ni/H reactor does; it introduces anomalous color magnetic moments, for both quarks and gluons through projecting a briefly formed monopole field into the nucleus. One type pion that keeps the nucleus together is made of one up quark and one down antiquark. If we can find a source(s) of a monopole field in the Ni/H reactor, we may be able to explain transmutation of elements via disruption of the strong force mechanism. The duration of this anaopole field is a few picoseconds in length before the hotspot decomposes. By that is more than enough time for nuclear disruption to occur.
