4 research outputs found

    Theoretical Modeling of the Magnetic Behavior of Thiacalix[4]arene Tetranuclear Mn<sup>II</sup><sub>2</sub>Gd<sup>III</sup><sub>2</sub> and Co<sup>II</sup><sub>2</sub>Eu<sup>III</sup><sub>2</sub> Complexes

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    In view of a wide perspective of 3dā€“4f complexes in single-molecule magnetism, here we propose an explanation of the magnetic behavior of the two thiacalix[4]Ā­arene tetranuclear heterometallic complexes Mn<sup>II</sup><sub>2</sub>Gd<sup>III</sup><sub>2</sub> and Co<sup>II</sup><sub>2</sub>Eu<sup>III</sup><sub>2</sub>. The energy pattern of the Mn<sup>II</sup><sub>2</sub>Gd<sup>III</sup><sub>2</sub> complex evaluated in the framework of the isotropic exchange model exhibits a rotational band of the low-lying spin excitations within which the LandeĢ intervals are affected by the biquadratic spinā€“spin interactions. The nonmonotonic temperature dependence of the Ļ‡<i>T</i> product observed for the Mn<sup>II</sup><sub>2</sub>Gd<sup>III</sup><sub>2</sub> complex is attributed to the competitive influence of the ferromagnetic Mnā€“Gd and antiferromagnetic Mnā€“Mn exchange interactions, the latter being stronger (<i>J</i>(Mn, Mn) = āˆ’1.6 cm<sup>ā€“1</sup>, <i>J</i><sub>s</sub>(Mn, Gd) = 0.8 cm<sup>ā€“1</sup>, <i>g</i> = 1.97). The model for the Co<sup>II</sup><sub>2</sub>Eu<sup>III</sup><sub>2</sub> complex includes uniaxial anisotropy of the seven-coordinate Co<sup>II</sup> ions and an isotropic exchange interaction in the Co<sup>II</sup><sub>2</sub> pair, while the Eu<sup>III</sup> ions are diamagnetic in their ground states. Best-fit analysis of Ļ‡<i>T</i> versus <i>T</i> showed that the anisotropic contribution (arising from a large zero-field splitting in Co<sup>II</sup> ions) dominates (weak-exchange limit) in the Co<sup>II</sup><sub>2</sub>Eu<sup>III</sup><sub>2</sub> complex (<i>D</i> = 20.5 cm<sup>ā€“1</sup>, <i>J</i> = āˆ’0.4 cm<sup>ā€“1</sup>, <i>g</i><sub>Co</sub> = 2.22). This complex is concluded to exhibit an easy plane of magnetization (arising from the Co<sup>II</sup> pair). It is shown that the low-lying part of the spectrum can be described by a highly anisotropic effective spin-<sup>1</sup>/<sub>2</sub> Hamiltonian that is deduced for the Co<sup>II</sup><sub>2</sub> pair in the weak-exchange limit

    Enhanced Pseudocapacitive Performance of Ī±ā€‘MnO<sub>2</sub> by Cation Preinsertion

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    Although the theoretical capacitance of MnO<sub>2</sub> is 1370 F g<sup>ā€“1</sup> based on the Mn<sup>3+</sup>/Mn<sup>4+</sup> redox couple, most of the reported capacitances in literature are far below the theoretical value even when the material goes to nanoscale. To understand this discrepancy, in this work, the electrochemical behavior and charge storage mechanism of K<sup>+</sup>-inserted Ī±-MnO<sub>2</sub> (or K<sub><i>x</i></sub>MnO<sub>2</sub>) nanorod arrays in broad potential windows are investigated. It is found that electrochemical behavior of K<sub><i>x</i></sub>MnO<sub>2</sub> is highly dependent on the potential window. During cyclic voltammetry cycling in a broad potential window, K<sup>+</sup> ions can be replaced by Na<sup>+</sup> ions, which determines the pseudocapacitance of the electrode. The K<sup>+</sup> or Na<sup>+</sup> ions cannot be fully extracted when the upper cutoff potential is less than 1 V vs Ag/AgCl, which retards the release of full capacitance. As the cyclic voltammetry potential window is extended to 0ā€“1.2 V, enhanced specific capacitance can be obtained with the emerging of new redox peaks. In contrast, the K<sup>+</sup>-free Ī±-MnO<sub>2</sub> nanorod arrays show no redox peaks in the same potential window together with much lower specific capacitance. This work provides new insights on understanding the charge storage mechanism of MnO<sub>2</sub> and new strategy to further improve the specific capacitance of MnO<sub>2</sub>-based electrodes

    Single-Ion Magnet Et<sub>4</sub>N[Co<sup>II</sup>(hfac)<sub>3</sub>] with Nonuniaxial Anisotropy: Synthesis, Experimental Characterization, and Theoretical Modeling

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    In this article we report the synthesis and structure of the new CoĀ­(II) complex Et<sub>4</sub>NĀ­[Co<sup>II</sup>Ā­(hfac)<sub>3</sub>] (<b>I</b>) (hfac = hexafluoroacetylacetonate) exhibiting single-ion magnet (SIM) behavior. The performed analysis of the magnetic characteristics based on the complementary experimental techniques such as static and dynamic magnetic measurements, electron paramagnetic resonance spectroscopy in conjunction with the theoretical modeling (parametric Hamiltonian and ab initio calculations) demonstrates that the SIM properties of <b>I</b> arise from the nonuniaxial magnetic anisotropy with strong positive axial and significant rhombic contributions

    A new member of the cationic dinitrosyl iron complexes family incorporating N-ethylthiourea is effective against human HeLa and MCF-7 tumor cell lines

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    <p>A new analog of the active site of mononuclear dinitrosyl [1Feā€“2S] proteins, [C<sub>3</sub>N<sub>2</sub>H<sub>8</sub>SFe(NO)<sub>2</sub>Cl][Fe(NO)<sub>2</sub>(C<sub>3</sub>N<sub>2</sub>H<sub>8</sub>S)<sub>2</sub>]<sup>+</sup>Cl<sup>āˆ’</sup> (<b>I</b>), has been synthesized by reacting NO with an aqueous mixture of iron(II) sulfate and N-ethylthiourea in acidic medium. The structure and properties of the complex were studied by X-ray diffraction, IR, Mƶssbauer, and EPR spectroscopy, in addition to quantum chemical calculations. Complex <b>I</b> spontaneously generates NO in protic media. The cytotoxicity of <b>I</b> was investigated against human cervical carcinoma (HeLa), breast cancer (MCF7), and non-immortalized (FetMCS) cell lines. The cytotoxicity of <b>I</b> against HeLa is similar to that of anticancer agents currently used clinically (platinum complexes), but <b>I</b> is 10 times less toxic in normal cells. The cytotoxicity of MCF7 cells to <b>I</b> is low.</p
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