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Volumn 80, Issue 24, 2009, Pages

Low-energy collective electronic excitations in Pd metal

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EID: 77954717738     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.245114     Document Type: Article
Times cited : (25)

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    • Note that at this q, the peak B in Im [Ε (q,ω ) ] is too weak in order to have any significance, although as it is shown below the corresponding peak for the momentum transfers q 's along the 110 direction is much more pronounced producing an additional acoustic plasmon mode.
    • Note that at this q, the peak B in Im [Ε (q, ω)] is too weak in order to have any significance, although as it is shown below the corresponding peak for the momentum transfers q 's along the 110 direction is much more pronounced producing an additional acoustic plasmon mode.
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    • From Fig. and Table it is clear that acoustic plasmons in Pd have too high group velocities to induce any effect on superconductivity in this material. This is because the large value of the group velocity reduces the phase space for virtual transitions involving acoustic plasmons, leading to a small value of the coupling constant for the pairing and to inability to overcome direct static Coulomb repulsion. This is in accord with absence of superconductivity in this metal.
    • From Fig. and Table it is clear that acoustic plasmons in Pd have too high group velocities to induce any effect on superconductivity in this material. This is because the large value of the group velocity reduces the phase space for virtual transitions involving acoustic plasmons, leading to a small value of the coupling constant for the pairing and to inability to overcome direct static Coulomb repulsion. This is in accord with absence of superconductivity in this metal.


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