### Session T41: Focus Session: Search for New Superconductors - Nanotubes and Fullerides

2:30 PM–5:18 PM, Wednesday, March 17, 2010
Room: F152

Chair: Anvar Zakhidov, University of Texas at Dallas

Abstract ID: BAPS.2010.MAR.T41.7

### Abstract: T41.00007 : Superconducting state of metallic clusters: Potential for room temperature superconductivity, nano-based tunneling networks

4:06 PM–4:42 PM

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Nanoclusters form a new family of high temperature superconductors. We focus on small metallic nanoclusters M$_{n}$ (n is the number of atoms) which contain delocalized electrons. These electrons form energy shells similar to those in atoms or nuclei (e.g., s,p,d,..). The presence of the shell structure and the corresponding orbital degeneracy 2(2L+1) leads to an increase in the effective density of states and to a great strengthening of the pairing interaction. It turns out that under special, but perfectly realistic conditions, the superconducting pairing is very strong and leads to high T$_{c}$. For some specific clusters (e.g., Al$_{56}$, Zn$_{83}$) T$_{c}$ reaches $\sim$150 K and the energy spectrum becomes strongly modified. With a realistic sets of parameters, it should be possible to raise T$_{c}$ up to room temperature. Specific experiments capable of detecting this phenomenon can be identified (spectroscopic, magnetic and thermodynamic measurements). The observation of a heat capacity jump for Al$_{45}^{-}$ and Al$_{47}^{-}$ clusters at T$_{c}\sim$200K (Cao et al.,2008) yielded first experimental support for the phenomenon: the amplitude, width and position of the jumps are in good agreement with the theory. Pairing also raises the possibility of observing intercluster Josephson tunneling. The discrete nature of the spectrum makes the analysis very different from that for conventional superconductors. Especially interesting is the case of resonant tunneling. The effect is promising for the creation of superconducting tunneling networks at high T$_{c}$ (potentially at room temperatures), and with current densities greatly exceeding those of usual superconductors.