Spin Ice
| dc.creator | Gingras, Michel J. P. | |
| dc.date | 2009-03-16 | |
| dc.date.accessioned | 2026-07-07T12:52:53Z | |
| dc.date.available | 2026-07-07T12:52:53Z | |
| dc.description | Geometric frustration usually arises in systems that comprise magnetic moments (spins) which reside on the sites of a lattice made up of elementary triangular or tetrahedral units and which interact via antiferromagnetic nearest-neighbor exchange. Albeit much less common, geometric frustration can also arise in systems with strong non-collinear single-ion easy-axis (Ising-like) anisotropy and ferromagnetically} coupled spins. This is what happens in some pyrochlore oxide materials where Ising-like magnetic rare earth moments (Ho$^{3+}$, Dy$^{3+}$) sit on a lattice of corner-shared tetrahedra and are coupled via effectively ferromagnetic (dipolar) interactions. These systems possess a macroscopic number of quasi-degenerate classical ground states and display an extensive low-temperature entropy closely related to the extensive proton disorder entropy in common water ice. For this reason, these magnetic systems are called {\it spin ice}. This chapter reviews the essential ingredients of spin ice phenomenology in magnetic pyrochlore oxides. | |
| dc.description | 33 pages, 6 figures. Lecture notes for Trieste Summer School, August 2007. To appear as a chapter in "Highly Frustrated Magnetism", Eds. C. Lacroix, P. Mendels, F. Mila | |
| dc.identifier | https://arxiv.org/abs/0903.2772 | |
| dc.identifier | http://arxiv.org/abs/0903.2772 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/223444 | |
| dc.subject | Statistical Mechanics | |
| dc.subject | Other Condensed Matter | |
| dc.title | Spin Ice | |
| dc.type | text |