Figure 3
From: Quantum magnetisms in uniform triangular lattices Li2AMo3O8 (A = In, Sc)
TOF neutron scattering results on Li2InMo3O8. Low-energy inelastic neutron scattering intensity maps at (a) 4.6 K and (b) 13.5 K measured with Ei = 11.9 meV. (c) High-energy inelastic neutron scattering intensity map at 4.6 K measured with Ei = 22.0 meV. (d) Calculated inelastic neutron scattering intensity map at 4.6 K using the optimum parameters as described in the main text. Calculated energy resolution for Ei = 11.9 meV was convoluted. (e) Elastic neutron scattering intensities at 4.6 and 18.7 K with energy window of [−0.15, 0.15] meV. Solid lines represent the fitting result using the Gaussian function with linear background. (f) Energy spectra integrated over Q = [0.69, 0.77] Å−1 at 4.6 and 13.5 K measured with Ei = 11.9 meV. (g) Q dependences of the neutron scattering intensities at several energy windows. Each energy window was [1.5, 2.0], [2.0, 2.5], [2.5, 3.0], [3.0, 3.5], and [3.5, 4.0] meV with Ei = 11.9 meV (red), [4.0, 4.5] and [4.5, 5.0] meV with Ei = 15.8 meV (blue), [5.0, 6.0] and [6.0, 7.0] meV with Ei = 22.0 meV (green), and [7.0, 8.0] meV with Ei = 32.7 meV (black), respectively. Constant background was subtracted from each Q dependence. Solid lines are calculated results using the optimum parameters in Eq. (5).
