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Update descriptions for Wishart Instances.
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francisjchen authored Apr 14, 2023
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"$$ H = -\\sum_{1\\leq i \\leq j \\leq N} J_{ij}\\sigma_i \\sigma_j$$\n",
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"where we have an $N \\times N$ matrix for $J$ (which is our spin coupling matrix) and an $N$-dimensional vector $h$ (which serves as our external field terms), along with each spin $\\sigma_i \\in \\{ -1, 1\\}$. \n",
"where we have an $N \\times N$ matrix for $J$ (which is our spin coupling matrix) specifying quadratic terms in the cost potential, along with each spin $\\sigma_i \\in \\{ -1, 1\\}$. \n",
"\n",
"We provide three implementations of the CIM: chaotic amplitude control (CAC), amplitude-heterogeneity correction (AHC), and amplitude-heterogeneity correction with external field terms (AHC). The first two solvers do not have an external field, while the latter requires an external field $h$.\n",
"\n",
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