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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2019-10-03 14:36:51 -0400 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2019-10-03 14:36:51 -0400 |
commit | c24a328928d700da3be71b126d750fe224c1633b (patch) | |
tree | 04c9ff7f76b00ff32987b2867f5c4ef0f2e63579 | |
parent | f8a257b5b36b7887ccbdba8b4c7e93976ed2512b (diff) | |
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added note on experiments with doping
-rw-r--r-- | main.tex | 8 |
1 files changed, 5 insertions, 3 deletions
@@ -462,9 +462,11 @@ ever-closer commensurate values in the style of the devil's staircase \cite{bak_commensurate_1982}. This motivates future \rus\ experiments done at pressure, where the depth of the cusp in the $\Bog$ stiffness should deepen (perhaps with these commensurability jumps) at low pressure and approach zero -like $q_*^4\sim(c_\perp/2D_\perp)^2$ near the Lifshitz point. The presence of -spatial commensurability is not expected to modify the critical behavior -otherwise \cite{garel_commensurability_1976}. +like $q_*^4\sim(c_\perp/2D_\perp)^2$ near the Lifshitz point. Alternatively, +\rus\ done at ambient pressure might examine the heavy fermi liquid to \afm\ +transition by doping. The presence of spatial commensurability is not +expected to modify the critical behavior otherwise +\cite{garel_commensurability_1976}. There are two apparent discrepancies between the orthorhombic strain in the phase diagram presented by \cite{choi_pressure-induced_2018} and that predicted |