1257101 MP2 Mia PaCa-2 2 1257098 MP2 MiaPaca-2 2 1257121 MP2 micrococcin P2 2 1257116 MP2 midgut peptide 2 2 1257097 MP2 Moller-Pleset 2 2 1257092 MP2 M06-2X (DFT), ROB2-PLYP and DuT-D3 (DHDFT), and G3X 1 1257091 MP2 M06-2X, were compared with benchmark G3 1 1257090 MP2 MA Plesset 2nd order perturbation theory 1 1257095 MP2 MammaPrint High 2 1 1257124 MP2 mapping by ab initio calculations at the G2 1 1257120 MP2 master equation calculations that employ new G2 1 1257089 MP2 MCQDPT2, G3, G2+ 1 1257119 MP2 measurement period 2 1 1257118 MP2 measuring point 2 1 1257117 MP2 medium polyamine conjugated protein peak 2 1 1257094 MP2 Megasphaera phylotype 2 1 1257123 MP2 methods RHF, RMP2, and G3 1 1257122 MP2 methyl nitrate (1) were evaluated computationally at the Gaussian 2 1 1257102 MP2 MHP...(H(2)O)(n), (n=1-5) are performed at second order Moller-Plesset 1 1257115 MP2 mobile phase 2 1 1257114 MP2 mol(-1) (B3LYP/6-311++G(2d,2p)) or 15.6 kJ mol(-1) 1 1257113 MP2 mol, respectively at the G2 1 1257126 MP2 Moller-Plesset perturbation theory, SAPT-F12 1 1257111 MP2 MP2 and G2 1 1257106 MP2 MP2 interaction energies, denoted delta 1 1257105 MP2 MP2 stabilization energies and the Delta E(CCSD(T)) - Delta E 1 1257103 MP2 MP2, and ONIOM-based methods, as well as G3 1 1257104 MP2 MP2, G3 1 1257109 MP2 MP2-based basis-set-correction term in the G4 1 1257110 MP2 MP2-R12 1 1257108 MP2 MP2/3-21G*, CBS-4M, and G2 1 1257107 MP2 MP2/6-31+G(d), and G3 1 1257093 MP2 MP2/6-311G(d), B3LYP/6-311G(d), and G2 1 1257100 MP2 MP2/GTMP2Large and G3 1 1257099 MP2 MP2Full/6-31G(d) and G3 1 1257096 MP2 MPC and 2% PPI 1 1257112 MP2 myelopeptide 2 1 1257125 MP2 RI-MP2 method; that is, the second-order Moller-Plesset 1