nitric oxide adsorption
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2021 ◽  
Author(s):  
Julia Oktawiec ◽  
Henry Z. H. Jiang ◽  
Ari B Turkiewicz ◽  
Jeffrey R. Long

Nitric oxide (NO) is an important signaling molecule in biological systems, and as such, the ability of porous materials to reversibly adsorb NO is of interest for potential medical applications....



2021 ◽  
Author(s):  
Julia Oktawiec ◽  
Henry Z. H. Jiang ◽  
Ari B. Turkiewicz ◽  
Jeffrey R. Long

Correction for ‘Influence of the primary and secondary coordination spheres on nitric oxide adsorption and reactivity in cobalt(ii)–triazolate frameworks’ by Julia Oktawiec et al., Chem. Sci., 2021, DOI: 10.1039/d1sc03994f.



2020 ◽  
Author(s):  
Julia Oktawiec ◽  
Henry Z. H. Jiang ◽  
Ari Turkiewicz ◽  
Jeffrey R. Long

<p>Nitric oxide (NO) is an important signaling molecule in biological systems, and as such the ability of certain porous materials to reversibly adsorb NO is of interest for medical applications. Metal–organic frameworks have been explored for their ability to reversibly bind NO at coordinatively-unsaturated metal sites, however the influence of metal coordination environment on NO adsorption has yet to be studied in detail. Here, we examine NO adsorption in the frameworks Co<sub>2</sub>Cl<sub>2</sub>(bbta) and Co<sub>2</sub>(OH)<sub>2</sub>(bbta) (H<sub>2</sub>bbta = 1<i>H</i>,5<i>H</i>-benzo(1,2-<i>d</i>:4,5-<i>d</i>′)bistriazole) via gas adsorption, infrared spectroscopy, powder X-ray diffaction, and magnetometry measurements. While NO adsorbs reversibly in Co<sub>2</sub>Cl<sub>2</sub>(bbta) without electron-transfer, adsorption of low pressures of NO in Co<sub>2</sub>(OH)<sub>2</sub>(bbta) is accompanied by charge transfer from the cobalt(II) centers to form a cobalt(III)–NO<sup>−</sup> adduct, as supported by diffraction and infrared spectroscopy data. At higher pressures of NO, characterization data support additional uptake of the gas and disproportionation of the bound NO to form a cobalt(III)–nitro (NO<sub>2</sub><sup>−</sup>) species and N<sub>2</sub>O gas, a transformation that appears to be facilitated in part by stabilizing hydrogen bonding interactions between the bound NO<sub>2</sub><sup>−</sup> and framework hydroxo groups. This reactivity represents a rare example of reductive NO-binding in a metal–organic framework and demonstrates that NO binding can be tuned by changing the coordination environment of the framework metal centers.</p>



2020 ◽  
Author(s):  
Julia Oktawiec ◽  
Henry Z. H. Jiang ◽  
Ari Turkiewicz ◽  
Jeffrey R. Long

<p>Nitric oxide (NO) is an important signaling molecule in biological systems, and as such the ability of certain porous materials to reversibly adsorb NO is of interest for medical applications. Metal–organic frameworks have been explored for their ability to reversibly bind NO at coordinatively-unsaturated metal sites, however the influence of metal coordination environment on NO adsorption has yet to be studied in detail. Here, we examine NO adsorption in the frameworks Co<sub>2</sub>Cl<sub>2</sub>(bbta) and Co<sub>2</sub>(OH)<sub>2</sub>(bbta) (H<sub>2</sub>bbta = 1<i>H</i>,5<i>H</i>-benzo(1,2-<i>d</i>:4,5-<i>d</i>′)bistriazole) via gas adsorption, infrared spectroscopy, powder X-ray diffaction, and magnetometry measurements. While NO adsorbs reversibly in Co<sub>2</sub>Cl<sub>2</sub>(bbta) without electron-transfer, adsorption of low pressures of NO in Co<sub>2</sub>(OH)<sub>2</sub>(bbta) is accompanied by charge transfer from the cobalt(II) centers to form a cobalt(III)–NO<sup>−</sup> adduct, as supported by diffraction and infrared spectroscopy data. At higher pressures of NO, characterization data support additional uptake of the gas and disproportionation of the bound NO to form a cobalt(III)–nitro (NO<sub>2</sub><sup>−</sup>) species and N<sub>2</sub>O gas, a transformation that appears to be facilitated in part by stabilizing hydrogen bonding interactions between the bound NO<sub>2</sub><sup>−</sup> and framework hydroxo groups. This reactivity represents a rare example of reductive NO-binding in a metal–organic framework and demonstrates that NO binding can be tuned by changing the coordination environment of the framework metal centers.</p>



2019 ◽  
Vol 26 (06) ◽  
pp. 1850202
Author(s):  
ZHICHENG YU ◽  
XIURONG ZHANG ◽  
KUN GAO ◽  
PEIYING HUO

Geometric and electronic properties of nitric oxide adsorption on WmMon ([Formula: see text] 6) clusters have been systematically calculated by density functional theory (DFT) at the generalized gradient approximation (GGA) level for ground-state structures. NO molecule prefers top site with nitrogen-end bridging a tungsten atom for W[Formula: see text]Mo[Formula: see text] and W3Mo2 clusters. While NO tends to locate on the hollow site for WMo5, W2Mo4 and W3Mo3 clusters, and dissociation of NO molecule happens on W3Mo, N–O bond lengths expand in accordance with the variation of adsorption energy with the increasing number of tungsten atoms, originating from metal [Formula: see text] back-donation. Electron transfer occurs among 4d state of Mo, 5d state of W, 2p state of N and 2p state of O.



2019 ◽  
Vol 123 (7) ◽  
pp. 4299-4307 ◽  
Author(s):  
Arafat Hossain Khan ◽  
Katharina Peikert ◽  
Frank Hoffmann ◽  
Michael Fröba ◽  
Marko Bertmer


2019 ◽  
Vol 55 (19) ◽  
pp. 2825-2828 ◽  
Author(s):  
Jia-Ge Jia ◽  
Jian-Shen Feng ◽  
Xin-Da Huang ◽  
Song-Song Bao ◽  
Li-Min Zheng

Homochiral nanotubular metal phosphonates (R)-or (S)-[Fe(pemp)(H2O2)2] [pemp2− = (R)- or (S)-(1-phenylethylamino) methylphonate] are reported which are the first examples of metal–organic nanotubes combining chirality, metamagnetism and highly selective nitric oxide absorption in the same molecular composite.



2018 ◽  
Vol 122 (24) ◽  
pp. 12723-12730 ◽  
Author(s):  
Arafat Hossain Khan ◽  
Benjamin Barth ◽  
Martin Hartmann ◽  
Jürgen Haase ◽  
Marko Bertmer


2018 ◽  
Vol 20 (23) ◽  
pp. 15871-15875 ◽  
Author(s):  
Z. Y. Li ◽  
M. Jibran ◽  
X. Sun ◽  
A. Pratt ◽  
B. Wang ◽  
...  

The spin polarization of the Fe3O4(100) surface is greatly enhanced by NO adsorption through the filling of the spin-down 2π* states.



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