Tunneling spectroscopy of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Bi</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Sr</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">CaCu</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mrow><mml:mn>8</mml:mn><mml:mo>+</mml:mo><mml:mi>δ</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>:</mml:mo></mml:math> Eliashberg analysis of the spectral dip feature
Annotatsiya
Eliashberg strong-coupling theory, extended to a d-wave symmetric gap function, is used to fit quantitatively a published tunneling spectrum of ${\mathrm{Bi}}_{2}{\mathrm{Sr}}_{2}{\mathrm{CaCu}}_{2}{\mathrm{O}}_{8+\ensuremath{\delta}}$ near optimal doping. The shape, location, and strength of the high-bias spectral dip feature is adequately reproduced using a single-peak ${\ensuremath{\alpha}}^{2}F(\ensuremath{\omega})$ centered at 36.5 meV. ${\ensuremath{\alpha}}^{2}F(\ensuremath{\omega})$ also self-consistently determines the measured gap value $\ensuremath{\Delta}=32\mathrm{meV}.$ Possible origins of the bosonic spectrum that give rise to high-${T}_{C}$ superconductivity are discussed.
Hali tarjima qilinmagan