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Quantum Statistical Theory of Superconductivity in MgB2

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Figure

Figure 1. An orthogonal unit cell (white solid lines) viewed from the top for graphite
Figure 2. Electron’s (phonon’s) motions are represented by solid (dotted) lines, and the time is measured upwards
Figure 3. Fluxon’s motion is represented by dot-dashed lines. The phonon exchange processes (a) and (b) generate the momenta change from the initial (electron, fluxon) state (k,−k′) to the final states (k+q,−k′−q
Figure 4. The molar heat capacity C for 2D free massless bosons (after Ref. 14, Figure 6.3)
+2

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