Abstract:Conventional superconductivity is inevitably suppressed in ultra-small metallic grains for characteristic sizes smaller than the Anderson limit. Experiments have shown that above the Anderson limit the critical temperature may be either enhanced or reduced when decreasing the particle size, depending on the superconducting material. In addition, there is experimental evidence that whether an enhancement or a reduction is found depends on the strength of the electron-phonon interaction in the bulk. We reveal ho… Show more
“…A future challenge is to correlate the changes in the phonon density of states at the nanoscale to changes in the superconducting behaviour. β-Sn is a low temperature superconductor with a bulk superconducting transition temperature (T C ) of 3.7 K. A substantial increase in (T C ) of Sn nanostructures has been experimentally observed [66][67][68] with origins in the subtle interplay of the quantum confinement for the electronic degrees of freedom and a phonon environment 69 . Our work enables further analysis of the role of phonon confinement in nanoscale superconductivity, and its precise account in Sn nanostructures.…”
To unravel the effects of phonon confinement, the influence of size and morphology on the atomic vibrations is investigated in Sn nano islands and cluster-assembled films. Nuclear resonant inelastic X-ray scattering is used to probe the phonon density of states of the Sn nanostructures which show significant broadening of the features compared to bulk phonon behaviour. Supported by ab initio calculations, the broadening is attributed to phonon scattering and can be described within the damped harmonic oscillator model. Contrary to the expectations based on previous research, the appearance of high-energy modes above the cut-off energy is not observed. From the thermodynamic properties extracted from the phonon density of states, it was found that grain boundary Sn atoms are bound by weaker forces than bulk Sn atoms.
“…A future challenge is to correlate the changes in the phonon density of states at the nanoscale to changes in the superconducting behaviour. β-Sn is a low temperature superconductor with a bulk superconducting transition temperature (T C ) of 3.7 K. A substantial increase in (T C ) of Sn nanostructures has been experimentally observed [66][67][68] with origins in the subtle interplay of the quantum confinement for the electronic degrees of freedom and a phonon environment 69 . Our work enables further analysis of the role of phonon confinement in nanoscale superconductivity, and its precise account in Sn nanostructures.…”
To unravel the effects of phonon confinement, the influence of size and morphology on the atomic vibrations is investigated in Sn nano islands and cluster-assembled films. Nuclear resonant inelastic X-ray scattering is used to probe the phonon density of states of the Sn nanostructures which show significant broadening of the features compared to bulk phonon behaviour. Supported by ab initio calculations, the broadening is attributed to phonon scattering and can be described within the damped harmonic oscillator model. Contrary to the expectations based on previous research, the appearance of high-energy modes above the cut-off energy is not observed. From the thermodynamic properties extracted from the phonon density of states, it was found that grain boundary Sn atoms are bound by weaker forces than bulk Sn atoms.
“…For Sn nanostructures an increase in T C of up to 10% has been observed [3][4][5][6][7][8][9][10] . The mechanism of this T C enhancement is not well understood and is suggested to be caused by changes in the phonon density of states 3,5,[11][12][13][14] , changes in the electron density of states [15][16][17][18][19][20][21][22][23] or a combination of these effects [24][25][26][27][28][29][30] .…”
Results and Discussion Structural characterisation. The structural characterisation using atomic force microscopy (AFM) and grazing incidence X-ray diffraction (XRD) of the Sn nanostructures shown here, was presented in detail in ref. 32. The relevant results of these measurements are summarised in Table 1 and Fig. 1. Figure 1 shows AFM images of the two types of nanostructures highlighting their different morphologies: Fig. 1(a) shows a 53 nm thick, granular cluster-assembled film grown on amorphous SiO 2 while Fig. 1(b) shows Sn islands, grown on Si(111), with an average island height of 68 ± 17 nm (Fig. 1(b)). To avoid oxidation the nanostructures were capped with Si and Ge respectively. Figure 1 shows clearly that the morphology of the two types of nanostructures is very different. While the Sn islands are textured, with a preferred orientation perpendicular to the substrate, the cluster-assembled film is polycrystalline, consisting of randomly oriented grains formed by coalescence of much smaller deposited clusters. These conclusions are further supported by XRD measurements (not shown). Further details on the sample fabrication and characterisation processes can be found in 32 .
“…As mentioned before, T c of weak-coupling superconductors increases upon size reduction while no impact or even a reduction of T c is observed in strong coupling materials. Note that, according to theoretical calculations, strongcoupling superconducting nanograins exhibit a larger broadening of single electron levels and a heavier electron mass than weak-coupling superconductors [52]. QSE are inversely proportional to the electron mass, thus making them more relevant in strong-coupling superconductors.…”
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