11 research outputs found
Highly Controllable Surface Plasmon Resonance Property by Heights of Ordered Nanoparticle Arrays Fabricated <i>via</i> a Nonlithographic Route
Perfectly ordered nanoparticle arrays are fabricated on large-area substrates (>cm<sup>2</sup>) <i>via</i> a cost-effective nonlithographic route. Different surface plasmon resonance (SPR) modes focus consequently on their own positions due to the identical shape and uniform size and distance of these plasmonic metallic nanoparticles (Ag and Au). On the basis of this and FDTD (finite-difference time-domain) simulation, this work reveals the variation of all SPR parameters (position, intensity, width, and mode) with nanoparticle heights, which demonstrates that the effect of heights are different in various stages. On increasing the heights, the major dipole SPR mode precisely blue-shifts from the near-infrared to the visible region with intensity strengthening, a peak narrowing effect, and multipole modes excitation in the UV–vis range. The intensity of multipole modes can be manipulated to be equal to or even greater than the major dipole SPR mode. After coating conformal TiO<sub>2</sub> shells on these nanoparticle arrays by atomic layer deposition, the strengthening of the SPR modes with increasing the heights results in the multiplying of the photocurrent (from ∼2.5 to a maximum 90 μA cm<sup>–2</sup>) in this plasmonic-metal–semiconductor-incorporated system. This simple but effective adjustment for all SPR parameters provides guidance for the future design of plasmonic metallic nanostructures, which is significant for SPR applications
Carrier Mobility-Dominated Gas Sensing: A Room-Temperature Gas-Sensing Mode for SnO<sub>2</sub> Nanorod Array Sensors
Adsorption-induced
change of carrier density is presently dominating
inorganic semiconductor gas sensing, which is usually operated at
a high temperature. Besides carrier density, other carrier characteristics
might also play a critical role in gas sensing. Here, we show that
carrier mobility can be an efficient parameter to dominate gas sensing,
by which room-temperature gas sensing of inorganic semiconductors
is realized via a carrier mobility-dominated gas-sensing (CMDGS) mode.
To demonstrate CMDGS, we design and prepare a gas sensor based on
a regular array of SnO<sub>2</sub> nanorods on a bottom film. It is
found that the key for determining the gas-sensing mode is adjusting
the length of the arrayed nanorods. With the change in the nanorod
length from 340 to 40 nm, the gas-sensing behavior changes from the
conventional carrier-density mode to a complete carrier-mobility mode.
Moreover, compared to the carrier density-dominating gas sensing,
the proposed CMDGS mode enhances the sensor sensitivity. CMDGS proves
to be an emerging gas-sensing mode for designing inorganic semiconductor
gas sensors with high performances at room temperature
Integration of Cointercalation and Adsorption Enabling Superior Rate Performance of Carbon Anodes for Symmetric Sodium-Ion Capacitors
Carbon
materials have been the most common anodes for sodium-ion
storage. However, it is well-known that most carbon materials cannot
obtain a satisfactory rate performance because of the sluggish kinetics
of large-sized sodium-ion intercalation in ordered carbon layers.
Here, we propose an integration of co-intercalation and adsorption
instead of conventional simplex-intercalation and adsorption to promote
the rate capability of sodium-ion storage in carbon materials. The
experiment was demonstrated by using a typical carbon material, reduced
graphite oxide (RGO400) in an ether-solvent electrolyte. The ordered
and disordered carbon layers efficiently store solvated sodium ions
and simplex sodium ions, which endows RGO400 with enhanced reversible
capacity (403 mA h g–1 at 50 mA g–1 after 100 cycles) and superior rate performance (166 mA h g–1 at 20 A g–1). Furthermore, a symmetric
sodium-ion capacitor was demonstrated by employing RGO400 as both
the anode and cathode. It exhibits a high energy density of 48 W h
g–1 at a very high power density of 10,896 W kg–1. This work updates the sodium-ion storage mechanism
and provides a rational strategy to realize high rate capability for
carbon electrode materials
Dibenzothiophene Derivatives: From Herringbone to Lamellar Packing Motif
It is generally believed that π−π stacking would be much more efficient than herringbone stacking for the transporting of charge carriers. The electron-withdrawing group sulphone unit was introduced into dibenzothiophene (DBT) derivatives, and lamellar structures were observed in the single crystals of the products along with strong, long-range π−π intermolecular interactions. As a contrast, the reduced materials adopted herringbone packing. We contributed this change of packing motif to the polarity of the sulphone unit. These results are meaningful to the molecular design to obtain π−π stacking
Dibenzothiophene Derivatives: From Herringbone to Lamellar Packing Motif
It is generally believed that π−π stacking would be much more efficient than herringbone stacking for the transporting of charge carriers. The electron-withdrawing group sulphone unit was introduced into dibenzothiophene (DBT) derivatives, and lamellar structures were observed in the single crystals of the products along with strong, long-range π−π intermolecular interactions. As a contrast, the reduced materials adopted herringbone packing. We contributed this change of packing motif to the polarity of the sulphone unit. These results are meaningful to the molecular design to obtain π−π stacking
Dibenzothiophene Derivatives: From Herringbone to Lamellar Packing Motif
It is generally believed that π−π stacking would be much more efficient than herringbone stacking for the transporting of charge carriers. The electron-withdrawing group sulphone unit was introduced into dibenzothiophene (DBT) derivatives, and lamellar structures were observed in the single crystals of the products along with strong, long-range π−π intermolecular interactions. As a contrast, the reduced materials adopted herringbone packing. We contributed this change of packing motif to the polarity of the sulphone unit. These results are meaningful to the molecular design to obtain π−π stacking
Extended π‑Conjugated System for Fast-Charge and -Discharge Sodium-Ion Batteries
Organic sodium-ion batteries (SIBs)
are potential alternatives
of current commercial inorganic lithium-ion batteries for portable
electronics (especially wearable electronics) because of their low
cost and flexibility, making them possible to meet the future flexible
and large-scale requirements. However, only a few organic SIBs have
been reported so far, and most of them either were tested in a very
slow rate or suffered significant performance degradation when cycled
under high rate. Here, we are focusing on the molecular design for
improving the battery performance and addressing the current challenge
of fast-charge and -discharge. Through reasonable molecular design
strategy, we demonstrate that the extension of the π-conjugated
system is an efficient way to improve the high rate performance, leading
to much enhanced capacity and cyclability with full recovery even
after cycled under current density as high as 10 A g<sup>–1</sup>
Rational Design of a Hierarchical Candied-Haws-like NiCo<sub>2</sub>O<sub>4</sub>@Ni,Co-(HCO<sub>3</sub>)<sub>2</sub> Heterostructure for the Electrochemical Performance Enhancement of Supercapacitors
Designing core–shell heterostructures with multicomponents,
more electroactive sites, hierarchical structures, and stable geometrical
configurations is an effective approach to enhance the electrochemical
properties of supercapacitors. Herein, we report the fabrication of
a hierarchical candied-haws-like NiCo2O4@NiCo-hydrocarbonate
heterostructure on Ni foam (NiCo2O4@NiCo-HCs),
which consists of NiCo2O4 nanowires acting as
“rebars” that are tightly strung with NiCo-HC nanoparticles.
The strong interfacial reaction between the NiCo2O4 “core” and the NiCo-HC “shell”
accelerates the charge transfer within the heterostructure, while
the hierarchical structure containing quantities of paths and pores
provides fast ion diffusion throughout the whole electrode, hence
remarkably boosting the electrochemical performance of a NiCo2O4@NiCo-HC electrode. As expected, the NiCo2O4@NiCo-HC electrode shows a high specific capacitance
of 3216.4 F g–1 at a current density of 1 A g–1 and 2259.9 F g–1 even at 20 A g–1 (1.6-fold that of the NiCo2O4 electrode and 5.5-fold that of NiCo-HCs). In addition, an assembled
asymmetric supercapacitor NiCo2O4@NiCo-HCs//AC
delivers a high energy density of 47.46 Wh kg–1 at
a power density of 708.94 W kg–1, together with
96.2% capacitance retention after 6000 cycles, surpassing most of
the reported analogues. These results suggest that our hierarchical
candied-haws-like heterostructure design is potential for the performance
enhancement of supercapacitors
Highly Ordered Three-Dimensional Ni-TiO<sub>2</sub> Nanoarrays as Sodium Ion Battery Anodes
Sodium ion batteries (SIBs) represent
an effective energy storage
technology with potentially lower material costs than lithium ion
batteries. Here, we show that the electrochemical performance of SIBs,
especially rate capability, is intimately connected to the electrode
design at the nanoscale by taking anatase TiO<sub>2</sub> as an example.
Highly ordered three-dimensional (3D) Ni-TiO<sub>2</sub> core–shell
nanoarrays were fabricated using nanoimprited AAO templating technique
and directly used as anode. The nanoarrays delivered a reversible
capacity of ∼200 mAh g<sup>–1</sup> after 100 cycles
at the current density of 50 mAh g<sup>–1</sup> and were able
to retain a capacity of ∼95 mAh g<sup>–1</sup> at the
current density as high as 5 A g<sup>–1</sup> and fully recover
low rate capacity. High ion accessibility, fast electron transport,
and excellent electrode integrity were shown as great merits to obtain
the presented electrochemical performance. Our work demonstrates the
possibility of highly ordered 3D heterostructured nanoarrays as a
promising electrode design for Na energy storage to alleviate the
reliance on the materials’ intrinsic nature and provides a
versatile and cost-effective technique for the fabrication of such
perfectly ordered nanostructures
