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IUGG XXIV General Assembly July 2-13, 2007 Perugia, Italy<br />

(S) - <strong>IASPEI</strong> - International Association of Seismology and Physics of the Earth's<br />

Interior<br />

JSS008 Oral Presentation 1991<br />

Understanding Electromagnetic Properties of Dry and Wet, Stressed and<br />

Unstressed Igneous Rocks: Progress Report<br />

Prof. Friedemann Freund<br />

Earth Science Division, Code SGE NASA Ames Research Center IAGA<br />

Vern Vanderbilt, Akihiro Takeuchi, Bobby W.S. Lau, Milton Bose<br />

The discovery of a new type of electric currents that can be stress-activated in igneous rocks (1) opens<br />

a window of opportunity for controlled laboratory experiments and for considering source generation<br />

mechanisms. Laboratory experiments demonstrate that the propagation of the electronic charge carriers<br />

is not impeded by water films in water-soaked rock, though cm-thick layers of liquid water reverse the<br />

direction of the current flow. The charge carriers that propagate through rocks are defect electrons in<br />

the oxygen anion sublattice (positive holes or pholes for short). They are introduced into the matrix of<br />

nominally anhydrous minerals during cooling from magmatic or high-grade metamorphic temperatures<br />

when hydroxyl pairs (traces of dissolved H2O) split off H2 molecules and convert to peroxy links. The<br />

oxygens in the peroxy links thereby change from the 2- to the 1- valence state. Stress causes<br />

dislocations to move, breaking peroxy links and activating pholes alongside with loosely bound<br />

electrons. The electron-phole pairs are long-lived (hrs to days). Our hypothesis is that the boundary<br />

between stressed and unstressed rock acts analogous to a semiconductor pn junction, impeding<br />

electron flow across the boundary in one direction while promoting flow of pholes. Whereas pholes can<br />

stream out of the stressed rock into the unstressed rock, electrons need an n-type contact to flow. We<br />

report on the magnitude of the transient currents that can be expected, when pholes and electrons both<br />

flow out of the stressed rock volume and reconnect, thereby closing the electric circuit. (1) Freund et al.<br />

2006, Phys. Chem. Earth 31, 389-396; Freund & Sornette, 2007, Tectonophys. 431, 33-47.<br />

Keywords: pre earthquake signals, telluric currents, electromagnetic emissions

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