Online Supplementary Material: Low temperature vortex liquid in $\rm La_{2-x}Sr_xCuO_4$

dc.creatorLi, Lu
dc.creatorCheckelsky, J. G.
dc.creatorKomiya, Seiki
dc.creatorAndo, Yoichi
dc.creatorOng, N. P.
dc.date2007-03-13
dc.date.accessioned2026-07-07T07:59:51Z
dc.date.available2026-07-07T07:59:51Z
dc.descriptionWe report here the supplementary material for Ref. [1]. Using torque magnetometry, we measured the magnetization anisotropy of 7 crystals of $\rm La_{2-x}Sr_xCuO_4$ (LSCO). In optimally-doped cuprates, the bulk susceptibility is dominated by the paramagnetic van-Vleck orbital term $χ_{orb}$ which has a significant anisotropy ($χ^{orb}_c>χ^{orb}_{ab}$) that changes weakly with $T$ (subscripts $c$ and ${ab}$ identify quantities measured with $\bf H||c$ and $\bf H\perp c$, respectively). Moreover, in the lightly-doped regime, the paramagnetic spin susceptibilities $χ^s_c$ and $χ^s_{ab}$ become significantly large below the interval 40-60 K. However, the spin susceptibility is very nearly isotropic (except below 10 K where its anisotropy becomes measurable). Against the large orbital and spin terms, the weak diamagnetic signal is very difficult to resolve using standard bulk magnetometry in lightly-doped cuprates. By contrast, torque magnetometry selectively detects the orbital diamagnetism generated by supercurrents confined to the CuO$_2$ layers while ignoring the large spin contribution when it is isotropic. The orbital van-Vleck contribution is also detected, but as a ``background'' that is $H$-linear to intense fields and only mildly $T$ dependent.
dc.description11 pages, 9 figures, Supplement to cond-mat/0702121, Nature Physics, in press
dc.identifierhttps://arxiv.org/abs/cond-mat/0703348
dc.identifierhttp://arxiv.org/abs/cond-mat/0703348
dc.identifierOnline Supplement to Nature Physics 3, 311-314 (2007)
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/128528
dc.subjectSuperconductivity
dc.subjectStrongly Correlated Electrons
dc.titleOnline Supplementary Material: Low temperature vortex liquid in $\rm La_{2-x}Sr_xCuO_4$
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