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Figure 1. Differential resistance, dV/dI, vs. bias voltage (left), and at zero-bias vs. temperature (right), across the boundary between ion-implanted and unimplanted regions of a CDW crystal, NbSe3 (as compared to a pristine sample, inset on the left and black triangles on the right). Note the abrupt drop in zero-bias resistance below 46 K, as shown by the red circles on the right. (12)

Collective quantum phenomena and their applications

John H. Miller, Jr., University of Houston (UH), from the Dept. of Physics and Texas Center for Superconductivity, explains collective quantum phenomena and their applications.
Department of Physics

Department of Physics & Texas Center for Superconductivity

Physical science research at the University of Houston encompasses a wide range of topics including collaborations with the Large Hadron Collider in Geneva and Relativistic Heavy Ion Collider at Brookhaven.
Magnet levitating above a high-temperature superconductor

Superconductivity and related macroscopic quantum phenomena

John H. Miller, Jr., from the University of Houston, Dept. of Physics and Texas Center for Superconductivity, walks us through superconductivity and related macroscopic quantum phenomena.

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