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Korthals Altes","submitted_at":"2017-12-29T19:13:38Z","abstract_excerpt":"One loop corrections to the magnetostatic QCD action are evaluated to dimension six in the magnetostatic fields.The result is remarkably simple $${1\\over 4}\\int d\\vec x (F^a_{ij})^2 - {g_M^2 N \\over {32\\pi m_E^3}} \\int d\\vec x\\Bigg({1\\over{60}}(D_m^{ab} F^b_{mr})^2 + {1\\over 180} f^{abc} F^a_{mn} F^b_{nr }F^c_{rm} \\Bigg)(1+\\mathcal{O}(g_M^2)).$$ In all of the deconfined phase the correction is quite small. The term of $\\mathcal{O}(g^2_M)$ is the dimension eight contribution and is only presented in a covariant derivative basis. 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