The mid-infrared AC Hall effect in optimally-doped BSCCO
| dc.creator | Schmadel, D. C. | |
| dc.creator | Tu, J. J. | |
| dc.creator | Rigal, L. B. | |
| dc.creator | Romero, D. B. | |
| dc.creator | Grayson, M. | |
| dc.creator | Gu, G. D. | |
| dc.creator | Drew, H. D. | |
| dc.date | 2002-10-14 | |
| dc.date | 2002-11-21 | |
| dc.date.accessioned | 2026-07-07T02:47:44Z | |
| dc.date.available | 2026-07-07T02:47:44Z | |
| dc.description | A novel heterodyne polarimetry system determines the frequency dependence from 900 to 1100 cm^-1 and temperature dependence from 35 to 330 K of the Hall transport in single crystal, optimally doped BSCCO. The results show a significant disconnect from the behavior of the Hall angle in the existing data for YBCO in the far-infrared, which indicate a negative value for the real part of the Hall angle above 250 cm^-1, whereas that of the current work at 1000 cm^-1 is positive. The current work when analyzed using an extended Drude formalism results in a Hall mass comparable to the ARPES Fermi mass and a scattering rate comparable to the low frequency conductivity and Hall effect scattering rates, which, however, are only 1/4 of the ARPES values. | |
| dc.description | Changed format | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0210304 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0210304 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/20119 | |
| dc.subject | Superconductivity | |
| dc.title | The mid-infrared AC Hall effect in optimally-doped BSCCO | |
| dc.type | text |