For room-temperature superconductivity, abruptly diverging <i>T<sub>c</sub></i> over a transition pressure, 225 GPa, explained by Brinkman-Rice picture
ORAL
Abstract
For discovered room-temperature superconductivity of 287.7±12 K at 267±10 GPa in a H-S-C compound, Tc-discontinuity around Ptransition=225 GPa and Tc-divergence over Ptransition were observed [1]. Explaining Tc-divergence is a core problem for the mechanism of room-temperature superconductivity. ~~The Tc-divergence results from 3D-density of states, N(0)*, with diverging behavior of m* induced by a large correlation strength of κBR=U/Uc near ρ≈1 [2].
This was analyzed by the strong-coupling-limit BCS Tc=(4/b)ΘD*exp(-1/λ*)(1-exp(-2/λ*))-1=(4/b)ρ1/3ΘDexp(-1/Aλ)(1-exp(-2/Aλ))-1 with b≥3.5. Effective parameterts, ΘD*=ρ1/3ΘD, λ*≡Aλ=A(N(0)Ve-phonon), A≡N(0)*/N(0)=ρ1/3/(1-ρ4) from N(0)*∝m*n1/3, m*=m/(1-ρ4) [2] are given.
~~Here, n=ρntot, 0<ρ=n/ntot<1 of band-filling factor, ntot of the number of atoms in the measurement region are defined in an inhomogeneous system such as compounds with metal and insulator phases[2]. m* is the effective mass obtained from the correlation strength in the Brinkman-Rice(BR) picture.
Moreover, with increasing pressure, n, ρ, Tc increase by insulator-metal transition, which is caused by the extension of the metal region (percolation). [1] Nature586(2020)373(Fig.1c). [2] arXiv/1710.07754.
This was analyzed by the strong-coupling-limit BCS Tc=(4/b)ΘD*exp(-1/λ*)(1-exp(-2/λ*))-1=(4/b)ρ1/3ΘDexp(-1/Aλ)(1-exp(-2/Aλ))-1 with b≥3.5. Effective parameterts, ΘD*=ρ1/3ΘD, λ*≡Aλ=A(N(0)Ve-phonon), A≡N(0)*/N(0)=ρ1/3/(1-ρ4) from N(0)*∝m*n1/3, m*=m/(1-ρ4) [2] are given.
~~Here, n=ρntot, 0<ρ=n/ntot<1 of band-filling factor, ntot of the number of atoms in the measurement region are defined in an inhomogeneous system such as compounds with metal and insulator phases[2]. m* is the effective mass obtained from the correlation strength in the Brinkman-Rice(BR) picture.
Moreover, with increasing pressure, n, ρ, Tc increase by insulator-metal transition, which is caused by the extension of the metal region (percolation). [1] Nature586(2020)373(Fig.1c). [2] arXiv/1710.07754.
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Presenters
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Hyun-Tak Kim
Electronics & Telecommunications Research Institute, Metal-Insulator Transition Laboratory, ETRI, Metal-Insulator Transition Laboratory, Electronics and Telecommunications Research Institute, MIT Lab, ETRI in Korea
Authors
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Hyun-Tak Kim
Electronics & Telecommunications Research Institute, Metal-Insulator Transition Laboratory, ETRI, Metal-Insulator Transition Laboratory, Electronics and Telecommunications Research Institute, MIT Lab, ETRI in Korea