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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2019-12-18 17:12:43 -0500 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2019-12-18 17:12:43 -0500 |
commit | e3140ea3be1a42178ce34012a5a6d8f14f28cf7a (patch) | |
tree | 695554d1e24e95eb71df7f50a678818d4a5c0bc6 | |
parent | 7b444f163a155d85eaf9e6db8e278493c11d056e (diff) | |
parent | 2781b05409a1360b062e613ae9daa608b43adc4a (diff) | |
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Merge commit '2781b05'
-rw-r--r-- | main.tex | 8 |
1 files changed, 3 insertions, 5 deletions
@@ -119,7 +119,7 @@ rau_hidden_2012, riggs_evidence_2015, hoshino_resolution_2013, ikeda_theory_1998, chandra_hastatic_2013, harrison_hidden_nodate, ikeda_emergent_2012} propose associating any of a variety of broken symmetries with \ho. This work analyzes a phenomenological model with order parameters of -general symmetry, linearly coupled to strain. Of these, only one is compatible +general symmetry that couple linearly to strain. Of these, only one is compatible with two experimental observations: first, the $\Bog$ ``nematic" elastic susceptibility $(C_{11}-C_{12})/2$ softens anomalously from room temperature down to $T_{\text{\ho}}=17.5\,\K$;\cite{de_visser_thermal_1986} and second, a @@ -546,10 +546,8 @@ pressure, where the depth of the cusp in the $\Bog$ modulus should deepen as $q_*^4\sim(c_\perp/2D_\perp)^2$ near the Lifshitz point. Alternatively, \rus\ done at ambient pressure might examine the heavy Fermi liquid to \afm\ transition by doping. Though previous \rus\ studies have doped -\urusi\ with Rhodium,\cite{yanagisawa_ultrasonic_2014} the magnetic nature of -Rhodium ions likely artificially promotes magnetic phases. A dopant like -phosphorous that only exerts chemical pressure might more faithfully explore -the pressure axis of the phase diagram. Our work also motivates experiments +\urusi\ with Rhodium,\cite{yanagisawa_ultrasonic_2014} the magnetic rhodium dopants likely promote magnetic phases. A non-magnetic dopant such as phosphorous may more faithfully explore +the transition out of the HO phase. Our work also motivates experiments that can probe the entire correlation function---like x-ray and neutron scattering---and directly resolve its finite-$q$ divergence. The presence of spatial commensurability is known to be irrelevant to critical behavior at a |