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324 Handbook on the Physics and Chemistry of Rare Earths FIG. 18 High field phase diagrams for CeRhIn5. Upper panel: Temperature vs field phase diagram down to 0.5 K and up to 50 T, illustrating the change from a small Fermi surface in AFMS to large Fermi surface in AFML. PL represents a large Fermi surface paramagnet. Lower panel: Proposed pressure vs field phase diagram at T 1⁄4 0. Note the coexistence of superconductiv- ity (SC) and antiferromagnetism (AFM). According to Jiao, L., Chen, Y., Kohama, Y., Graf, D., Bauer, E.D., Singleton, J., Zhu, J.X., Weng, Z., Pang, G., Shang, T., et al., 2015. Fermi surface reconstruction and multiple quantum phase transitions in the antiferromagnet CeRhIn5. Proc. Natl. Acad. Sci. 112 (3), 673-678. is well-known as the hidden order (HO) material which shows a mysterious CPT at 17.5 K. The origin of this transition is neither magnetic nor structural and still persists after 30 years as unclarified, thus its designation as HO. Only within the HO phase does unconventional SC exists below Tc 1⁄4 1.5 K. Much has been published, both experimentally and theoretically, in relation to the HO state and its formation (Mydosh and Oppeneer, 2011, 2014). From an experimental point of view, the HO has stimulated the develop- ments of novel methods to detect its origin. In Fig. 19, we show an “elephant” cartoon of these many techniques utilized to characterize the HO. There has been significant progress in developing exotic evaluations of the HO beyond the bulk studies. For the first time, ARPES, STM/STS,PDF Image | HANDBOOK ON THE PHYSICS AND CHEMISTRY OF RARE EARTHS
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