PMID-sentid Pub_year Sent_text comp_official_name comp_offsetprotein_name organism prot_offset 12298022-4 2002 In agreement with experiment, the chromium system requires a change from low- to high-spin in the catalytic cycle, whereas the manganese system can proceed either with spin inversion or entirely on the high-spin surface. Manganese 127-136 spindlin 1 Homo sapiens 168-172 12452719-5 2002 The Mn(II)-Ni(II) weak ferromagnetic coupling in the chain is interpreted in a spin delocalization mechanism as resulting from the weakness of the overlap between the magnetic orbitals centered on nickel and those centered on manganese which are only weakly delocalized on the ligands. Manganese 226-235 spindlin 1 Homo sapiens 79-83 12298022-4 2002 In agreement with experiment, the chromium system requires a change from low- to high-spin in the catalytic cycle, whereas the manganese system can proceed either with spin inversion or entirely on the high-spin surface. Manganese 127-136 spindlin 1 Homo sapiens 168-172 31940603-0 2020 Spin-phonon interaction increased by compressive strain in antiferromagnetic MnO thin films. Manganese 77-80 spindlin 1 Homo sapiens 0-4 16656699-1 1967 Changes in the intensity of the electron spin resonance signal of divalent manganese were found to occur in suspensions of wild-type Chlamydomonas reinhardi. Manganese 75-84 spindlin 1 Homo sapiens 41-45 33497240-8 2021 For this purpose, we used a prototypical bis-mu-oxo binuclear manganese complex ([Mn2O2(NH3)8]4+) and demonstrated that its antiferromagnetism (J < 0), calculated by using the active space composed of all valence pO and dMn orbitals, correlates well with the largest elements in the differential low-spin vs high-spin entanglement map. Manganese 62-71 spindlin 1 Homo sapiens 300-304 33497240-8 2021 For this purpose, we used a prototypical bis-mu-oxo binuclear manganese complex ([Mn2O2(NH3)8]4+) and demonstrated that its antiferromagnetism (J < 0), calculated by using the active space composed of all valence pO and dMn orbitals, correlates well with the largest elements in the differential low-spin vs high-spin entanglement map. Manganese 62-71 spindlin 1 Homo sapiens 313-317 11671322-1 1999 High-field and -frequency electron paramagnetic resonance (HFEPR) spectroscopy has been used to study two complexes of high-spin manganese(III), d(4), S = 2. Manganese 129-138 spindlin 1 Homo sapiens 124-128 9753446-1 1998 When acetate-inhibited photosystem II (PSII) membranes are illuminated at temperatures above 250 K and quickly cooled to 77 K, a 240 G-wide electron paramagnetic resonance (EPR) signal is observed at 10 K. This EPR signal arises from a reciprocal interaction between the spin 1/2 ground state of the S2 state of the Mn4 cluster, for which a multiline EPR signal with shifted 55Mn hyperfine peaks is observed, and the oxidized tyrosine residue, YZ*, for which a broadened YZ* EPR spectrum is observed. Manganese 316-319 spindlin 1 Homo sapiens 271-279 11669688-0 1997 Density Functional Calculations of Electronic Structure, Charge Distribution, and Spin Coupling in Manganese-Oxo Dimer Complexes. Manganese 99-108 spindlin 1 Homo sapiens 82-86 34330123-4 2021 This theoretical model is supported by the experimental measurements of the manganese spin relaxation time in the GaMnAs by means of spin-flip Raman scattering. Manganese 76-85 spindlin 1 Homo sapiens 86-90 34330123-4 2021 This theoretical model is supported by the experimental measurements of the manganese spin relaxation time in the GaMnAs by means of spin-flip Raman scattering. Manganese 76-85 spindlin 1 Homo sapiens 133-137 31976695-1 2020 We report on temperature dependent measurements of the longitudinal spin Seebeck effect (LSSE) in the mixed valent manganite La_{0.7}Ca_{0.3}MnO_{3}. Manganese 141-144 spindlin 1 Homo sapiens 68-72 25166407-1 2013 Optical pump-probe experiments reveal spin beats of manganese ions in (Cd,Mn)Te, due to hyperfine and crystal fields. Manganese 52-61 spindlin 1 Homo sapiens 38-42 27419390-2 2016 In agreement with experiment our calculations reveal that high spin (HS) state for Mn(4+) ion and low spin (LS) state for Co(4+) ion stabilize the magnetic structure of the respective compounds. Manganese 83-89 spindlin 1 Homo sapiens 63-67 27746891-0 2016 A Low Spin Manganese(IV) Nitride Single Molecule Magnet. Manganese 11-20 spindlin 1 Homo sapiens 6-10 26382137-0 2015 Atomic-like spin noise in solid-state demonstrated with manganese in cadmium telluride. Manganese 56-65 spindlin 1 Homo sapiens 12-16 25166407-6 2013 The manganese spin coherence time up to T(2)(Mn) 15 ns is measured for a manganese concentration x=0.0011. Manganese 4-13 spindlin 1 Homo sapiens 14-18 23383938-1 2013 High-spin paramagnetic manganese defects in polar piezoelectric zinc oxide exhibit a simple, almost axial anisotropy and phase coherence times of the order of a millisecond at low temperatures. Manganese 23-32 spindlin 1 Homo sapiens 5-9 25166407-6 2013 The manganese spin coherence time up to T(2)(Mn) 15 ns is measured for a manganese concentration x=0.0011. Manganese 74-83 spindlin 1 Homo sapiens 14-18 21673400-5 2011 First measurements of the electron spin polarization in the L(3)M(2, 3)V and L(3)VV Auger emission peaks from the manganese constituents in [Mn(6)(III)Cr(III)](3+) resonantly excited at the L(3)-edge near 640 eV by circularly polarized synchrotron radiation are reported. Manganese 114-123 spindlin 1 Homo sapiens 35-39 23000927-0 2012 Electron Spin Resonance and optical absorption spectroscopic studies of manganese centers in aluminium lead borate glasses. Manganese 72-81 spindlin 1 Homo sapiens 9-13 21780752-0 2011 Tuning manganese dopant spin interactions in single GaN nanowires at room temperature. Manganese 7-16 spindlin 1 Homo sapiens 24-28 21469891-0 2011 Long-lived ultrafast spin precession in manganese alloys films with a large perpendicular magnetic anisotropy. Manganese 40-49 spindlin 1 Homo sapiens 21-25 21814012-0 2009 Spin dynamics in the manganese tetramer compound alpha-MnMoO(4). Manganese 21-30 spindlin 1 Homo sapiens 0-4