2020
DOI: 10.7566/jpsj.89.073701
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Variation of Electronic Heat Capacity of κ-(BEDT-TTF)2Cu[N(CN)2]Br Induced by Partial Substitution of Donor Layers

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Cited by 3 publications
(2 citation statements)
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“…As discussed in Ref. [19], this is more likely due to the impurity scattering at superconducting gap nodes because the present superconductivity is classified into d-wave symmetry with line nodes [30]. For the higher x salts, a small amount of extrinsic contribution arising from some impurities are included, as displayed in Fig.…”
mentioning
confidence: 84%
“…As discussed in Ref. [19], this is more likely due to the impurity scattering at superconducting gap nodes because the present superconductivity is classified into d-wave symmetry with line nodes [30]. For the higher x salts, a small amount of extrinsic contribution arising from some impurities are included, as displayed in Fig.…”
mentioning
confidence: 84%
“…Physical pressure, on the other hand, enables tuning in arbitrary steps through the phase diagram, at the cost of more difficult experiments that have to be carried out in a pressure cell. The advantages of both approaches-flexible tuning and ambient pressure experiments-can be achieved by partial substitution of the constituents, either the donor molecules [16][17][18][19][20][21][22][23][24][25][26][27][28][29] or the anions [30][31][32][33], as depicted in Figure 1. So far, partial substitution has remained poorly investigated compared to pressure tuning, but, in addition to bandwidth tuning, it also enables the study of disorder effects on metal-insulator transitions and superconductivity [29].…”
Section: Introductionmentioning
confidence: 99%