Electrical conductivity and spin crossover: Towards the first achievement with a metal bis dithiolene complex

2006 ◽  
Vol 142 (3-4) ◽  
pp. 261-266 ◽  
Author(s):  
Christophe Faulmann ◽  
Stéphane Dorbes ◽  
José A. Real ◽  
Lydie Valade
2020 ◽  
Vol 49 (15) ◽  
pp. 5601-5638 ◽  
Author(s):  
Víctor Rubio-Giménez ◽  
Sergio Tatay ◽  
Carlos Martí-Gastaldo

This review aims to reassess the progress, issues and opportunities in the path towards integrating conductive and magnetically bistable coordination polymers and metal–organic frameworks as active components in electronic devices.


2008 ◽  
Vol 130 (21) ◽  
pp. 6688-6689 ◽  
Author(s):  
Kazuyuki Takahashi ◽  
Heng-Bo Cui ◽  
Yoshinori Okano ◽  
Hayao Kobayashi ◽  
Hatsumi Mori ◽  
...  

2015 ◽  
Vol 3 (5) ◽  
pp. 945-949 ◽  
Author(s):  
Yan-Cong Chen ◽  
Yan Meng ◽  
Zhao-Ping Ni ◽  
Ming-Liang Tong

A flexible heterostructure is reported herein, which elastically couples the volumetric variation during SCO to the electrical conductivity of a strain-sensitive metallic conductor, thereby resulting in synergistic electrical bistability.


2007 ◽  
Vol 46 (21) ◽  
pp. 8548-8559 ◽  
Author(s):  
Christophe Faulmann ◽  
Kane Jacob ◽  
Stéphane Dorbes ◽  
Stéphane Lampert ◽  
Isabelle Malfant ◽  
...  

2007 ◽  
Vol 142 (3-4) ◽  
pp. 265-270 ◽  
Author(s):  
Christophe Faulmann ◽  
Stéphane Dorbes ◽  
José A. Real ◽  
Lydie Valade

2020 ◽  
Vol 6 (3) ◽  
pp. 31
Author(s):  
Andrei-Cristian Gheorghe ◽  
Yurii S. Bibik ◽  
Olesia I. Kucheriv ◽  
Diana D. Barakhtii ◽  
Marin-Vlad Boicu ◽  
...  

We studied the spin-state dependence of the electrical conductivity of two nanocrystalline powder samples of the spin crossover complex [Fe(pyrazine){Au(CN)2}2]. By applying an external pressure (up to 3 kbar), we were able to tune the charge transport properties of the material from a more conductive low spin state to a crossover point toward a more conductive high spin state. We rationalize these results by taking into account the spin-state dependence of the activation parameters of the conductivity.


2012 ◽  
Vol 48 (35) ◽  
pp. 4163-4165 ◽  
Author(s):  
Aurelian Rotaru ◽  
Il'ya A. Gural'skiy ◽  
Gábor Molnár ◽  
Lionel Salmon ◽  
Philippe Demont ◽  
...  

2021 ◽  
Vol 7 (5) ◽  
pp. 72
Author(s):  
Scott S. Turner ◽  
Joanna Daniell ◽  
Hiroki Akutsu ◽  
Peter N. Horton ◽  
Simon J. Coles ◽  
...  

Two novel salts containing the anion [Ni(mnt)2]− (mnt = maleonitriledithiolate) have been synthesized. The counter-ions, [Fe(II)(L1 or L2)2], are cationic complexes where L1 and L2 are methylated derivatives of 2,6-bis(pyazolyl)pyridine or pyrazine, which are similar to ligands found in a series of spin-crossover (SCO) complexes. Both salts are characterized by variable temperature single crystal X-ray diffraction and bulk magnetization measurements. Compound 1, [Fe(II)(L1)2][Ni(mnt)2]2 displays an incomplete and gradual SCO up to 300 K, followed by a more rapid increase in the high-spin fraction between 300 and 350 K. Compound 2, [Fe(II)(L2)2][Ni(mnt)2]2.MeNO2, shows a gradual, but more complete SCO response centered at 250 K. For compound 2, the SCO is confirmed by variable temperature Mössbauer spectroscopy. In both cases, the anionic moieties are isolated from each other and so no electrical conductivity is observed.


Author(s):  
John C. Russ ◽  
Nicholas C. Barbi

The rapid growth of interest in attaching energy-dispersive x-ray analysis systems to transmission electron microscopes has centered largely on microanalysis of biological specimens. These are frequently either embedded in plastic or supported by an organic film, which is of great importance as regards stability under the beam since it provides thermal and electrical conductivity from the specimen to the grid.Unfortunately, the supporting medium also produces continuum x-radiation or Bremsstrahlung, which is added to the x-ray spectrum from the sample. It is not difficult to separate the characteristic peaks from the elements in the specimen from the total continuum background, but sometimes it is also necessary to separate the continuum due to the sample from that due to the support. For instance, it is possible to compute relative elemental concentrations in the sample, without standards, based on the relative net characteristic elemental intensities without regard to background; but to calculate absolute concentration, it is necessary to use the background signal itself as a measure of the total excited specimen mass.


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