From 3ecb26966a1c27bfe93efbc66db0a252b224db9d Mon Sep 17 00:00:00 2001 From: zmorrell <66835471+zmorrell@users.noreply.github.com> Date: Tue, 19 Mar 2024 10:04:21 -0400 Subject: [PATCH] RuCl image1 fix (#16) * Fixed Typo in file name for RuClLattices.jpg * Fix rendering issues for Image 2 and S_i --- notebooks/RuClExample.ipynb | 8 ++++---- 1 file changed, 4 insertions(+), 4 deletions(-) diff --git a/notebooks/RuClExample.ipynb b/notebooks/RuClExample.ipynb index 505b28b..b1de29e 100644 --- a/notebooks/RuClExample.ipynb +++ b/notebooks/RuClExample.ipynb @@ -18,7 +18,7 @@ "\\end{split}\n", "\\end{equation}\n", "\n", - "The terms $S^{x}_{i}$, $S^{y}_{i}$, and $S^{z}_{i}$ represent the Pauli operators acting on site $i$. The terms $K_{x}$, $K_{y}$, and $K_{z}$ represent the strength of the Kitaev interaction between two sites in a given direction. The bold terms $\\bf{S_i}$ $ = [S^x_i, S^y_i, S^z_i]$ are useful for defining the Heisenberg interaction terms with strength $J$. The terms $\\Gamma$ represent the strength of off-diagonal symmetric exchange interactions between nearest neighboring sites, and the terms $\\Gamma'$ represent the effect of trigonal distortion. Lastly, the term $A$ represents the effect of single-ion anisotropy. \n", + "The terms $S^{x}_{i}$, $S^{y}_{i}$, and $S^{z}_{i}$ represent the Pauli operators acting on site $i$. The terms $K_{x}$, $K_{y}$, and $K_{z}$ represent the strength of the Kitaev interaction between two sites in a given direction. The bold terms ${\\bf{S_i}} = [S^x_i, S^y_i, S^z_i]$ are useful for defining the Heisenberg interaction terms with strength $J$. The terms $\\Gamma$ represent the strength of off-diagonal symmetric exchange interactions between nearest neighboring sites, and the terms $\\Gamma'$ represent the effect of trigonal distortion. Lastly, the term $A$ represents the effect of single-ion anisotropy. \n", "\n", "The connectivity of the Hamiltonian is defined directionally, as shown in Figure 1 (obtained from [[1]](https://doi.org/10.1038/s41535-019-0203-y)). As a result of the experiment being performed on the material, we need to include a time-varying Hamiltonian component, corresponding to the time-varying Zeeman terms operating on the material. This Hamiltonian is\n", "\\begin{equation}\n", @@ -30,7 +30,7 @@ " H(t) = H_{material} + H_{field}(t)\n", "\\end{equation}\n", "\n", - "\"RuCl\n", + "![RuCl_Latticve](EmbeddedFigures/RuClLattice.jpg)\n", "\n", "##### Figure 1" ] @@ -910,7 +910,7 @@ "\n", "Once all of this has been done, the state has been prepared and the dynamics may be executed.\n", "\n", - "\"RuCl_Spin_Structure\"\n", + "![RuCl_Spin_Structure](EmbeddedFigures/RuCl3_spinstructure.jpeg)\n", "\n", "##### Figure 3" ] @@ -1381,7 +1381,7 @@ "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython3", - "version": "3.11.5" + "version": "3.9.13" } }, "nbformat": 4,