Two characteristic energies in the low-energy antiferromagnetic response of the electron-doped high-temperature superconductor Nd$_{2-x}$Ce$_x$CuO$_{4+δ}$
| dc.creator | Yu, G. | |
| dc.creator | Li, Y. | |
| dc.creator | Motoyama, E. M. | |
| dc.creator | Hradil, K. | |
| dc.creator | Mole, R. A. | |
| dc.creator | Greven, M. | |
| dc.date | 2008-03-22 | |
| dc.date | 2008-11-29 | |
| dc.date.accessioned | 2026-07-07T12:05:45Z | |
| dc.date.available | 2026-07-07T12:05:45Z | |
| dc.description | Inelastic neutron scattering for Nd$_{2-x}$Ce$_x$CuO$_{4+δ}$ near optimal doping ($x \approx 0.155$, $T_{c} = 25 \mathrm{K}$) reveals that the dynamic magnetic susceptibility at the antiferromagnetic zone center exhibits two characteristic energies in the superconducting state: $ω_1 \approx 6.4 \mathrm{meV}$ and $ω_2 \approx 4.5 \mathrm{meV}$. These two magnetic energies agree $quantitatively$ with the $B_{1g}$ / $B_{2g}$ and $A_{1g}$ features previously observed in electronic Raman scattering, where the former is believed to indicate the maximum electronic gap and the origin of the smaller $A_{1g}$ feature has remained unexplained. The susceptibility change upon cooling into the superconducting state is inconsistent with previous claims of the existence of a magnetic resonance mode near 10 meV, but consistent with a resonance at $ω_2$. | |
| dc.description | 5 pages, 3 figures | |
| dc.identifier | https://arxiv.org/abs/0803.3250 | |
| dc.identifier | http://arxiv.org/abs/0803.3250 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/208461 | |
| dc.subject | Superconductivity | |
| dc.title | Two characteristic energies in the low-energy antiferromagnetic response of the electron-doped high-temperature superconductor Nd$_{2-x}$Ce$_x$CuO$_{4+δ}$ | |
| dc.type | text |