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005 | 20250311141806.0 | ||
008 | 250311b |||||||| |||| 00| 0 eng d | ||
022 | _a09743626 | ||
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_aMSU _bEnglish _cMSU _erda |
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050 | 0 | 0 | _aQD31 JOU |
100 | 1 |
_aGoswami, Soumyabrata _eauthor |
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245 | 1 | 0 |
_aExploration of the structural features and magnetic behaviour in a novel 3-dimensional interpenetrating Co(II)-based framework / _ccreated by Soumyabrata Goswami, A. Mondal, Sanjit Konar |
264 | 1 |
_aBangalore : _bSpringer, _c2015. |
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336 |
_2rdacontent _atext _btxt |
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337 |
_2rdamedia _aunmediated _bn |
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338 |
_2rdacarrier _avolume _bnc |
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_aJournal of chemical sciences _vVolume 127, number 2, |
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520 | 3 | _aA new Co(II)-based three-dimensional (3D) framework having the molecular formula [Co(C4O4)(4-bpmh))H2O)2]n·2nH2O·2nMeOH·(1) (4-bpmh=N, N-bis-pyridin-4-ylmethylene-hydrazine) has been syn-thesized using a mixed ligand system and characterized by elemental analysis, IR spectroscopy, thermogravi-metric analysis, single crystal X-ray diffraction and variable temperature magnetic study. The framework isconstructed by the bridging squarate (C4O2−4)and N, N-bis-pyridin-4-ylmethylene-hydrazine (4-bpmh) ligandsand interpenetration of the 2D grid-like frameworks at definite angles gives rise to 2D→3D inclined polycate-nation with sql/Shubnikov tetragonal plane net topology. Extensive non-covalent interactions (H-bonding aswell asπ···πinteractions) are also observed which stabilises the 3D arrangement. Additionally, complex1contains 1D channels of large dimensions (10.91×11.78 Å2)that runs along theb-axis. Variable temperatureDC magnetic susceptibility study reveals dominant spin–orbit coupling effect typical of the4T1gground stateof octahedral high-spin Co(II) ion at a higher temperature range. | |
650 |
_aMixed ligand system _vCo(II)-based 3D framework _xInterpenetrated structure |
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700 | 1 |
_aMondal, A. _eco author |
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700 | 1 |
_aKonar, Sanjit _eco author |
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856 | _uhttps://doi.org/10.1007/s12039-015-0771-8 | ||
942 |
_2lcc _cJA |
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_c169253 _d169253 |