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NCSA NEWS |
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Copper. Aluminum. Iron. These are the elements we typically think of as metals. Their atomic structures are orderly--often arrayed in compact lattices that are as uniform as the squares on a checkerboard. So close are these atoms that the successive energy levels at which the electrons orbit the nuclei become almost indistinguishable, with the outer high-energy bands forming into a conduction band in which electrons move easily throughout the crystal. This delocalized state of electrons is what imparts the conductivity we associate with a metal.
The propensity of all materials metallize when subjected to sufficient pressure was first recognized in the 1930s by Hungarian physicist Eugene P. Wigner. Using the newly penned Schrodinger equation, which governs the particle and wavelike behavior of subatomic matter, he calculated how pressure and volume conspire to push electrons into a delocalized state. His predictions of the pressure required for this transition, though, were off by 10-fold. The fault laid not in the basic ideas but in the overly simplistic numerical methods then available to him. At that time, computer were nothing more than glorified adding machines. Laboratory experiments for replicating these extreme conditions, too, were decades away. |
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