Mononuclear and three-dimensional metal complexes based on a multidentate hydrazone ligand

Liu, Yanfei; Liu, Yaping; Zhang, Ke-Ke; Ren, Qing-Ling; Qin, Jie

doi:10.1107/s2053229615000698

Cited by 5 publications

(3 citation statements)

References 21 publications

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“…The title comlex is a mononuclear coordination compound in which the six coordinated Cu 2+ is surrounded by two crystallogaphically dependent acylhydrazones giving a distorted octahedral geometry. The bond lengths of Cu-O and Cu-N (2.066(3)−2.204(4) Å) in the title complex are comparable with those found in our previous work [7] and there is a structurally related manganese complex [8].…”

Section: Discussionsupporting

confidence: 86%

Crystal structure of bis(N-(1-(pyrazin-2-yl)ethylidene)nicotinohydrazonato-κ³ N,N′,O)copper(II) C₂₄H₂₀N₁₀O₂Cu

Jiao

2018

Zeitschrift Für Kristallographie - New Crystal Structures

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Section: Discussionsupporting

confidence: 86%

Crystal structure of bis(N-(1-(pyrazin-2-yl)ethylidene)nicotinohydrazonato-κ³ N,N′,O)copper(II) C₂₄H₂₀N₁₀O₂Cu

Jiao

2018

Zeitschrift Für Kristallographie - New Crystal Structures

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“…Very recently, a one‐dimensional coordination polymer of copper(II) with both acetate and tridentate aroylhydrazone bridges was published . However, to the best of our knowledge, only a few aroylhydrazone‐bridged coordination polymers or MOFs with higher 2D or 3D dimensionalities have been reported . Similarly, aroylhydrazones were only very recently successfully implemented as linkers in 2D covalent organic frameworks (COFs) …”

Section: Introductionmentioning

confidence: 99%

Carboxylate–Hydrazone Mixed‐Linker Metal–Organic Frameworks: Synthesis, Structure, and Selective Gas Adsorption

Roztocki

Senkovska²,

Kaskel³

et al. 2016

Eur J Inorg Chem

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New mixed-linker metal-organic framework (MOF) materials incorporating both carboxylate and hydrazone linkers were prepared. The zinc-based 3D MOFs were obtained by utilizing a presynthesized aroylhydrazone [4-pyridinecarbaldehyde isonicotinoyl hydrazone (PCIH)] and para-dicarboxylic acids [1,4-benzenedicarboxylic acid (H 2 BDC) and 4,4′-biphenyldicarboxylic acid (H 2 BPDC)]. Single-crystal X-ray diffraction revealed the interpenetrated, pillar-layered structures of the MOFs, including

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“…Atom positions in different RCS dispersed throughout the thickness may be uncorrelated, but diffraction from these pairs still contributes to the total diffracted intensity. This fact, and the complication of dynamical diffraction, means that, in general, the features in diffraction patterns from amorphous materials cannot be interpreted naively on the basis of a particular RCS [2,3]. Despite these difficulties, END patterns have been used to fingerprint local structure at the length scale of nearest-neighbour clusters [4,5] and map these subtle symmetries to [4] access any extended range order.…”

mentioning

confidence: 99%

Statistical Analyses of Electron Nanodiffraction Patterns to Examine Order and Structural Variability in Amorphous Materials

et al. 2017

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The information contained in an ensemble of scanning electron nanodiffraction (END) patterns from amorphous materials is extremely rich and yet notoriously hard to interpret. By focussing the electron probe, the lateral size of the diffracting volume can be restricted to that of the "regions of correlated structure" (RCS) [1] and the otherwise isotropic diffuse amorphous rings in the diffraction pattern break up into areas of diffracted intensity that are related to the local structure. In reality, the diffracting volume has a finite thickness, spanning some tens of RCS. Atom positions in different RCS dispersed throughout the thickness may be uncorrelated, but diffraction from these pairs still contributes to the total diffracted intensity. This fact, and the complication of dynamical diffraction, means that, in general, the features in diffraction patterns from amorphous materials cannot be interpreted naively on the basis of a particular RCS [2,3]. Despite these difficulties, END patterns have been used to fingerprint local structure at the length scale of nearest-neighbour clusters [4,5] and map these subtle symmetries to [4] access any extended range order.The correlations and symmetries found in these END patterns are weak, and interpretation has relied upon significant prior knowledge from related equilibrium crystal phases and atomistic modeling [4,5]. In this contribution we present more "order agnostic" approaches to decomposing these END data sets using a range of statistical analyses. In an isotropic material, such as an amorphous material, the local RCS can take any orientation with respect to the electron beam. Thus, one way to reduce the dimensionality of the data set is to remove the azimuthal dependence of the scattering angle by calculating the set of Fourier coefficients of the angular symmetries [4,5]. These Fourier coefficients can be compared to or decomposed into calculated fingerprints from ideal nearest-neighbour clusters [5].Another approach is to calculate, without prior assumptions of structure, raw statistical measurements from this reduced data set of Fourier coefficients. For example, the covariance matrix can be calculated to investigate how different angular symmetries vary with respect to each other (Figure 1 (a)). The Pearson correlation coefficient can be mapped (Figure 1 (b)) or calculated from the whole ensemble of END patterns (Figure 1 (c)) to examine variability in the local structure from volume to volume. A Principal Component Analysis (Figure 1 (d)) can reveal the number of distinct orthogonal components required to encompass the data set and to identify the features that best describe the variance in the data. These measures can be compared for different specimens, providing more clues about the nature of local RCS and the variability and distribution of RCS. In some cases these measurements could provide an efficient and direct link to the underlying physics of how these materials form and behave, without requiring precise identification of local structure geometry. ...

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Mononuclear and three-dimensional metal complexes based on a multidentate hydrazone ligand

Cited by 5 publications

References 21 publications

Crystal structure of bis(N-(1-(pyrazin-2-yl)ethylidene)nicotinohydrazonato-κ³ N,N′,O)copper(II) C₂₄H₂₀N₁₀O₂Cu

Crystal structure of bis(N-(1-(pyrazin-2-yl)ethylidene)nicotinohydrazonato-κ³ N,N′,O)copper(II) C₂₄H₂₀N₁₀O₂Cu

Carboxylate–Hydrazone Mixed‐Linker Metal–Organic Frameworks: Synthesis, Structure, and Selective Gas Adsorption

Statistical Analyses of Electron Nanodiffraction Patterns to Examine Order and Structural Variability in Amorphous Materials

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Mononuclear and three-dimensional metal complexes based on a multidentate hydrazone ligand

Cited by 5 publications

References 21 publications

Crystal structure of bis(N-(1-(pyrazin-2-yl)ethylidene)nicotinohydrazonato-κ3 N,N′,O)copper(II) C24H20N10O2Cu

Crystal structure of bis(N-(1-(pyrazin-2-yl)ethylidene)nicotinohydrazonato-κ3 N,N′,O)copper(II) C24H20N10O2Cu

Carboxylate–Hydrazone Mixed‐Linker Metal–Organic Frameworks: Synthesis, Structure, and Selective Gas Adsorption

Statistical Analyses of Electron Nanodiffraction Patterns to Examine Order and Structural Variability in Amorphous Materials

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Crystal structure of bis(N-(1-(pyrazin-2-yl)ethylidene)nicotinohydrazonato-κ³ N,N′,O)copper(II) C₂₄H₂₀N₁₀O₂Cu

Crystal structure of bis(N-(1-(pyrazin-2-yl)ethylidene)nicotinohydrazonato-κ³ N,N′,O)copper(II) C₂₄H₂₀N₁₀O₂Cu