scholarly journals Large Negative Photoresistivity in Amorphous NdNiO3 Film

Coatings ◽  
2021 ◽  
Vol 11 (11) ◽  
pp. 1411
Author(s):  
Alexandr Stupakov ◽  
Tomas Kocourek ◽  
Natalia Nepomniashchaia ◽  
Marina Tyunina ◽  
Alexandr Dejneka

A significant decrease in resistivity by 55% under blue lighting with ~0.4 J·mm−2 energy density is demonstrated in amorphous film of metal-insulator NdNiO3 at room temperature. This large negative photoresistivity contrasts with a small positive photoresistivity of 8% in epitaxial NdNiO3 film under the same illumination conditions. The magnitude of the photoresistivity rises with the increasing power density or decreasing wavelength of light. By combining the analysis of the observed photoresistive effect with optical absorption and the resistivity of the films as a function of temperature, it is shown that photo-stimulated heating determines the photoresistivity in both types of films. Because amorphous films can be easily grown on a wide range of substrates, the demonstrated large photo(thermo)resistivity in such films is attractive for potential applications, e.g., thermal photodetectors and thermistors.

Author(s):  
J. L. Batstone ◽  
D.A. Smith

Recrystallization of amorphous NiSi2 involves nucleation and growth processes which can be studied dynamically in the electron microscope. Previous studies have shown thatCoSi2 recrystallises by nucleating spherical caps which then grow with a constant radial velocity. Coalescence results in the formation of hyperbolic grain boundaries. Nucleation of the isostructural NiSi2 results in small, approximately round grains with very rough amorphous/crystal interfaces. In this paper we show that the morphology of the rccrystallizcd film is dramatically affected by variations in the stoichiometry of the amorphous film.Thin films of NiSi2 were prepared by c-bcam deposition of Ni and Si onto Si3N4, windows supported by Si substrates at room temperature. The base pressure prior to deposition was 6 × 107 torr. In order to investigate the effect of stoichiomctry on the recrystallization process, the Ni/Si ratio was varied in the range NiSi1.8-2.4. The composition of the amorphous films was determined by Rutherford Backscattering.


2013 ◽  
Vol 2013 (CICMT) ◽  
pp. 000014-000018 ◽  
Author(s):  
M. Osada ◽  
T. Sasaki

We present a novel procedure for ceramic nanocoating using oxide nanosheet as a building block. A variety of oxide nanosheets (such as Ti1−δO2, MnO2 and perovsites) were synthesized by delaminating appropriate layered precursors into their molecular single sheets. These nanosheets are exceptionally rich in both structural diversity and electronic properties, with potential applications including conductors, semiconductors, insulators, and ferromagnets. Another attractive aspect is that nanosheets can be organized into various nanoarchitectures by applying solution-based synthetic techniques involving electrostatic layer-by-layer assembly and Langmuir-Blodgett deposition. It is even possible to tailor superlattice assemblies, incorporating into the nanosheet galleries with a wide range of materials such as organic molecules, polymers, and inorganic/metal nanoparticles. Sophisticated functionalities or paper-like devices can be designed through the selection of nanosheets and combining materials, and precise control over their arrangement at the molecular scale.


2021 ◽  
Author(s):  
Preeti Jain ◽  
Oleg N. Antzutkin

<p>We report a comparative analysis of non-halogenated surface-active ionic liquids (SAILs), which consists of the surface-active anion, 2-ethylhexyl sulfate, and the phosphonium, and imidazolium cations <i>i.e.,</i> tetrabutylphosphonium ([P<sub>4444</sub>]<sup>+</sup>), trihexyl(tetradecyl)phosphonium ([P<sub>66614</sub>]<sup>+</sup>), and 1-methyl-3-hexylimidazolium ([C<sub>6</sub>C<sub>1</sub>IM]<sup>+</sup>). We explored the thermal and electrochemical properties, <i>i.e.</i>, degradation, melting and crystallization temperatures, and ionic conductivity of this new class of IL. These SAILs were tested as an electrolyte in a multi-walled carbon nanotubes (MWCNTs)-based supercapacitor at various temperatures from 253 to 373 K. The electrochemical performance of different SAILs by varying the cationic core as a function of temperature were compared, in the same MWCNT-based supercapacitor. We found that the supercapacitor cell with [C<sub>6</sub>C<sub>1</sub>IM][EHS] shown high specific capacitance (<i>C<sub>elec</sub></i> in F g<sup>-1</sup>), a high energy density (<i>E</i> in Wh kg<sup>-1</sup>), and a high power density (<i>P</i> in kW kg<sup>-1</sup>) when compared to those for the other SAILs <i>i.e.</i> [P<sub>4444</sub>][EHS], [P<sub>66614</sub>][EHS], and [N<sub>8888</sub>][EHS] at all temperatures. The supercapacitor with an MWCNT-based electrode and [C<sub>6</sub>C<sub>1</sub>IM][EHS], [P<sub>4444</sub>][EHS], and [P<sub>66614</sub>][EHS] as an electrolyte showed a specific capacitance of 148, 90, and 47 F g<sup>-1</sup> (at the scan rate of 2 mV s<sup>-1</sup>) with an energy density of 82, 50, and 26 Wh kg<sup>-1</sup> (at 2 mV s<sup>-1</sup>) respectively, at 298 K. The temperature effect can be seen by the three to four-fold increase in the specific capacitance of the cell and the energy density values, <i>i.e.</i>, 290, 198, and 114 F g<sup>-1</sup> (at 2 mV s<sup>-1</sup>) and 161, 110, and 63 Wh kg<sup>-1</sup> (at 2 mV s<sup>-1</sup>), respectively, at 373 K. This study reveals that these new SAILs specifically [C<sub>6</sub>C<sub>1</sub>IM][EHS] and [P<sub>4444</sub>][EHS] can potentially be used as electrolytes in the wide range of temperature. The solution resistance (<i>R<sub>s</sub></i>), charge transfer resistance (<i>R<sub>ct</sub></i>), and equivalent series resistance (ESR) also decreased with an increase in temperature for all SAILs as electrolytes. These new SAILs can explicitly be used for high-temperature (wide range of temperature) electrochemical applications, such as efficient supercapacitors for high energy storage due to enhanced specific capacitance, energy, and power density at elevated temperatures. </p>


2021 ◽  
Author(s):  
Preeti Jain ◽  
Oleg N. Antzutkin

<p>We report a comparative analysis of non-halogenated surface-active ionic liquids (SAILs), which consists of the surface-active anion, 2-ethylhexyl sulfate, and the phosphonium, and imidazolium cations <i>i.e.,</i> tetrabutylphosphonium ([P<sub>4444</sub>]<sup>+</sup>), trihexyl(tetradecyl)phosphonium ([P<sub>66614</sub>]<sup>+</sup>), and 1-methyl-3-hexylimidazolium ([C<sub>6</sub>C<sub>1</sub>IM]<sup>+</sup>). We explored the thermal and electrochemical properties, <i>i.e.</i>, degradation, melting and crystallization temperatures, and ionic conductivity of this new class of IL. These SAILs were tested as an electrolyte in a multi-walled carbon nanotubes (MWCNTs)-based supercapacitor at various temperatures from 253 to 373 K. The electrochemical performance of different SAILs by varying the cationic core as a function of temperature were compared, in the same MWCNT-based supercapacitor. We found that the supercapacitor cell with [C<sub>6</sub>C<sub>1</sub>IM][EHS] shown high specific capacitance (<i>C<sub>elec</sub></i> in F g<sup>-1</sup>), a high energy density (<i>E</i> in Wh kg<sup>-1</sup>), and a high power density (<i>P</i> in kW kg<sup>-1</sup>) when compared to those for the other SAILs <i>i.e.</i> [P<sub>4444</sub>][EHS], [P<sub>66614</sub>][EHS], and [N<sub>8888</sub>][EHS] at all temperatures. The supercapacitor with an MWCNT-based electrode and [C<sub>6</sub>C<sub>1</sub>IM][EHS], [P<sub>4444</sub>][EHS], and [P<sub>66614</sub>][EHS] as an electrolyte showed a specific capacitance of 148, 90, and 47 F g<sup>-1</sup> (at the scan rate of 2 mV s<sup>-1</sup>) with an energy density of 82, 50, and 26 Wh kg<sup>-1</sup> (at 2 mV s<sup>-1</sup>) respectively, at 298 K. The temperature effect can be seen by the three to four-fold increase in the specific capacitance of the cell and the energy density values, <i>i.e.</i>, 290, 198, and 114 F g<sup>-1</sup> (at 2 mV s<sup>-1</sup>) and 161, 110, and 63 Wh kg<sup>-1</sup> (at 2 mV s<sup>-1</sup>), respectively, at 373 K. This study reveals that these new SAILs specifically [C<sub>6</sub>C<sub>1</sub>IM][EHS] and [P<sub>4444</sub>][EHS] can potentially be used as electrolytes in the wide range of temperature. The solution resistance (<i>R<sub>s</sub></i>), charge transfer resistance (<i>R<sub>ct</sub></i>), and equivalent series resistance (ESR) also decreased with an increase in temperature for all SAILs as electrolytes. These new SAILs can explicitly be used for high-temperature (wide range of temperature) electrochemical applications, such as efficient supercapacitors for high energy storage due to enhanced specific capacitance, energy, and power density at elevated temperatures. </p>


Author(s):  
Jian Shen ◽  
Bin Xu ◽  
Zifei Wang ◽  
Jing Zhang ◽  
Weiguang Zhang ◽  
...  

Optical multiplexing based on luminescent materials with tunable lifetime holds potential applications in information storage and security. However, most of these materials reported so far are still limited to microsecond...


RSC Advances ◽  
2020 ◽  
Vol 10 (33) ◽  
pp. 19353-19359 ◽  
Author(s):  
S. M. Nikam ◽  
A. Sharma ◽  
M. Rahaman ◽  
A. M. Teli ◽  
S. H. Mujawar ◽  
...  

Cobalt ferrite thin films were grown by PLD at different temperatures as an electrode material for supercapacitors. The films deposited at room temperature exhibited the best power density (3277 W kg−1) and energy density (17 W h kg−1) values.


1990 ◽  
Vol 200 ◽  
Author(s):  
M. R. Poor ◽  
A. M. Hurd ◽  
C. B. Fleddermann ◽  
A. Y. Wu

ABSTRACTPotential applications for ferroelectric thin films include both electronic and optoelectronic devices. In order to integrate a large number of devices on a single ceramic film or to incorporate ceramic devices with silicon-based integrated circuits, suitable film patterning techniques must be developed. In this study, the use of plasma etching for device patterning of PLT thin films has been explored using a dc hollow cathode discharge with HCl and CF4 etching gases. At room temperature, no etching of material is discernable. As the substrate temperature is increased, however, relatively rapid etching takes place. Etch rates for PLT thin films as high as 6500 Å/hour were measured. Etching occurred in both chlorinated and fluorinated plasmas, but at considerably different rates. The etch rate is enhanced by a factor of six by using a combination of HCl and CF4 in the plasma. After etching, the stoichiometry of the film, measured by energy dispersive spectroscopy (EDS), varied greatly with changes in substrate temperature. Although the removal rate for each element is different, all traces of lead, titanium, and lanthanum can be removed from the substrate over a wide range of plasma etching conditions.


2005 ◽  
Vol 475-479 ◽  
pp. 3843-3846
Author(s):  
Jiwei Chen ◽  
Jing Yang ◽  
Jian She Lian

The irradiation of a Nd-YAG pulsed laser on the CeO2 target in water was investigated. The CeO2 nanoparticles sized of 20-80 nm were formed in water, while the power density was larger than 32 kJ/cm2. The nanocrystalline films with grain sized of 50-150 nm were formed on the target with the energy density of 20 kJ/cm2-25 kJ/cm2. Finally, the amorphous films were formed with the energy density of 6 kJ/cm2-15 kJ/cm2. The formation mechanisms of the nanoparticles and the films were discussed.


2015 ◽  
Vol 51 (22) ◽  
pp. 4693-4696 ◽  
Author(s):  
Haodong Liu ◽  
Jing Xu ◽  
Chuze Ma ◽  
Ying Shirley Meng

A new O3–Na0.78Li0.18Ni0.25Mn0.583Ow is prepared as the cathode material for Na-ion batteries, delivering exceptionally high energy density and superior rate performance. No phase transformation happens through a wide range of sodium concentrations.


Author(s):  
Ernest L. Hall ◽  
J. B. Vander Sande

The present paper describes research on the mechanical properties and related dislocation structure of CdTe, a II-VI semiconductor compound with a wide range of uses in electrical and optical devices. At room temperature CdTe exhibits little plasticity and at the same time relatively low strength and hardness. The mechanical behavior of CdTe was examined at elevated temperatures with the goal of understanding plastic flow in this material and eventually improving the room temperature properties. Several samples of single crystal CdTe of identical size and crystallographic orientation were deformed in compression at 300°C to various levels of total strain. A resolved shear stress vs. compressive glide strain curve (Figure la) was derived from the results of the tests and the knowledge of the sample orientation.


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