Cooper-pair distribution function $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) for superconducting $$\hbox {D}_3\hbox {S}$$ D 3 S and $$\hbox {H}_3\hbox {S}$$ H 3 S
Abstract Cooper-pair distribution function, $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) , is a recent theoretical proposal that reveals information about the superconductor state through the determination of the spectral regions where Cooper pairs are formed. This is built from the well-established Eli...
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Nature Portfolio
2021
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oai:doaj.org-article:64a5a8c7e5704536a7d4416d872431cf2021-11-21T12:17:26ZCooper-pair distribution function $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) for superconducting $$\hbox {D}_3\hbox {S}$$ D 3 S and $$\hbox {H}_3\hbox {S}$$ H 3 S10.1038/s41598-021-02081-w2045-2322https://doaj.org/article/64a5a8c7e5704536a7d4416d872431cf2021-11-01T00:00:00Zhttps://doi.org/10.1038/s41598-021-02081-whttps://doaj.org/toc/2045-2322Abstract Cooper-pair distribution function, $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) , is a recent theoretical proposal that reveals information about the superconductor state through the determination of the spectral regions where Cooper pairs are formed. This is built from the well-established Eliashberg spectral function and phonon density of states, calculated by first-principles. From this function is possible to obtain the $$N_{cp}$$ N cp parameter, which is proportional to the total number of Cooper pairs formed at a critical temperature $$T_c$$ T c . Herein, we reported $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) function of the compressed $$D_3S$$ D 3 S and $$H_3S$$ H 3 S high- $$T_c$$ T c conventional superconductors, including the effect of stable sulfur isotopes in $$H_3S$$ H 3 S . $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) suggests that the vibration energy range of 10–70 meV is where the Cooper pairs are possible for these superconductors, pointing out the possible importance of the low-energy region on the electron–phonon superconductivity. This has been confirmed by the fact that a simple variation in the low-frequency region induced for the substitution of S atoms in $$H_3S$$ H 3 S by its stable isotopes can lead to important changes in $$T_c$$ T c . The results also show proportionality between $$N_{cp}$$ N cp parameter and experimental or theoretical $$T_c$$ T c values.G. I. González-PedrerosJ. A. Camargo-MartínezF. MesaNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 11, Iss 1, Pp 1-7 (2021) |
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Medicine R Science Q G. I. González-Pedreros J. A. Camargo-Martínez F. Mesa Cooper-pair distribution function $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) for superconducting $$\hbox {D}_3\hbox {S}$$ D 3 S and $$\hbox {H}_3\hbox {S}$$ H 3 S |
| description |
Abstract Cooper-pair distribution function, $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) , is a recent theoretical proposal that reveals information about the superconductor state through the determination of the spectral regions where Cooper pairs are formed. This is built from the well-established Eliashberg spectral function and phonon density of states, calculated by first-principles. From this function is possible to obtain the $$N_{cp}$$ N cp parameter, which is proportional to the total number of Cooper pairs formed at a critical temperature $$T_c$$ T c . Herein, we reported $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) function of the compressed $$D_3S$$ D 3 S and $$H_3S$$ H 3 S high- $$T_c$$ T c conventional superconductors, including the effect of stable sulfur isotopes in $$H_3S$$ H 3 S . $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) suggests that the vibration energy range of 10–70 meV is where the Cooper pairs are possible for these superconductors, pointing out the possible importance of the low-energy region on the electron–phonon superconductivity. This has been confirmed by the fact that a simple variation in the low-frequency region induced for the substitution of S atoms in $$H_3S$$ H 3 S by its stable isotopes can lead to important changes in $$T_c$$ T c . The results also show proportionality between $$N_{cp}$$ N cp parameter and experimental or theoretical $$T_c$$ T c values. |
| format |
article |
| author |
G. I. González-Pedreros J. A. Camargo-Martínez F. Mesa |
| author_facet |
G. I. González-Pedreros J. A. Camargo-Martínez F. Mesa |
| author_sort |
G. I. González-Pedreros |
| title |
Cooper-pair distribution function $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) for superconducting $$\hbox {D}_3\hbox {S}$$ D 3 S and $$\hbox {H}_3\hbox {S}$$ H 3 S |
| title_short |
Cooper-pair distribution function $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) for superconducting $$\hbox {D}_3\hbox {S}$$ D 3 S and $$\hbox {H}_3\hbox {S}$$ H 3 S |
| title_full |
Cooper-pair distribution function $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) for superconducting $$\hbox {D}_3\hbox {S}$$ D 3 S and $$\hbox {H}_3\hbox {S}$$ H 3 S |
| title_fullStr |
Cooper-pair distribution function $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) for superconducting $$\hbox {D}_3\hbox {S}$$ D 3 S and $$\hbox {H}_3\hbox {S}$$ H 3 S |
| title_full_unstemmed |
Cooper-pair distribution function $$D_{cp}(\omega ,T_c)$$ D cp ( ω , T c ) for superconducting $$\hbox {D}_3\hbox {S}$$ D 3 S and $$\hbox {H}_3\hbox {S}$$ H 3 S |
| title_sort |
cooper-pair distribution function $$d_{cp}(\omega ,t_c)$$ d cp ( ω , t c ) for superconducting $$\hbox {d}_3\hbox {s}$$ d 3 s and $$\hbox {h}_3\hbox {s}$$ h 3 s |
| publisher |
Nature Portfolio |
| publishDate |
2021 |
| url |
https://doaj.org/article/64a5a8c7e5704536a7d4416d872431cf |
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