Weak Charge-Lattice Coupling Requires Reinterpretation of Stripes of Charge Order in ${\mathrm{L}\mathrm{a}}_{1-x}{\mathrm{C}\mathrm{a}}_x{\mathrm{M}\mathrm{n}\mathrm{O}}_3$

Modulations in manganites attributed to stripes of charge/orbital/spin order are thought to result from strong electron-lattice interactions that lock the superlattice and parent lattice periodicities. Surprisingly in ${\mathrm{L}\mathrm{a}}_{1-x}{\mathrm{C}\mathrm{a}}_x{\mathrm{M}\mathrm{n}\mathrm{O}}_3$ ($x>0.5,90\mathrm{K}$), convergent beam (3.6 nm spot) electron diffraction patterns rule out charge stacking faults and indicate a superlattice with uniform periodicity. Moreover, large area electron diffraction peaks are sharper than simulations with stacking faults. Since the electron-lattice coupling does not lock the two periodicities (to yield stripes) it may be too weak to strongly localize charge.