added new citations for wavevector

1 files changed, 4 insertions, 3 deletions

diff --git a/main.tex b/main.tex
index 1839913..3928eae 100644
--- a/main.tex
+++ b/main.tex
@@ -444,15 +444,16 @@ $q_*$ should continuously vanish. Far from the Lifshitz point we expect the
 wavevector to lock into values commensurate with the space group of the
 lattice, and moreover that at zero pressure, where the \rus\ data here was
 collected, the half-wavelength of the modulation should be commensurate with
-the lattice, or $q_*\simeq0.328\,\A^{-1}$ \cite{meng_imaging_2013}. In between
+the lattice, or $q_*\simeq0.328\,\A^{-1}$ \cite{meng_imaging_2013,
+broholm_magnetic_1991, wiebe_gapped_2007, bourdarot_precise_2010}. In between
 these two regimes, the ordering wavevector should shrink by jumping between
 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}.
+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