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Dive into the research topics where Asha Gupta is active.

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Featured researches published by Asha Gupta.


ACS Applied Materials & Interfaces | 2013

Sn–Cu Nanocomposite Anodes for Rechargeable Sodium-Ion Batteries

Yong-Mao Lin; Paul R. Abel; Asha Gupta; John B. Goodenough; Adam Heller; C. Buddie Mullins

Sn0.9Cu0.1 nanoparticles were synthesized via a surfactant-assisted wet chemistry method, which were then investigated as an anode material for ambient temperature rechargeable sodium ion batteries. The Sn0.9Cu0.1 nanoparticle-based electrodes exhibited a stable capacity of greater than 420 mA h g(-1) at 0.2 C rate, retaining 97% of their maximum observed capacity after 100 cycles of sodium insertion/deinsertion. Their performance is considerably superior to electrodes made with either Sn nanoparticles or Sn microparticles.


Advanced Materials | 2015

High‐Rate Oxygen Evolution Reaction on Al‐Doped LiNiO2

Asha Gupta; William D. Chemelewski; C. Buddie Mullins; John B. Goodenough

LiNi0.8 Al0.2 O2 with a higher Ni(3+) /Li(+) ordering, synthesized by the solution-combustion method, gives oxygen-evolution-reaction (OER) activity in alkaline solution that is comparable to that of IrO2 . This confirms that the octahedral-site Ni(IV) /Ni(III) couple in an oxide is an active redox center for the OER with -redox energy pinned at the top of the O-2p bands.


Inorganic Chemistry | 2015

Conditions for TaIV–TaIV Bonding in Trirutile LixMTa2O6

Asha Gupta; Preetam Singh; Hugo Celio; C. Buddie Mullins; John B. Goodenough

Stabilization of Ta-Ta bonding in an oxide across a shared octahedral-site edge of a Ta2 dimer is not known. Investigation of Li insertion into the trirutile structure of MTa2O6 with M = Mg, Cr, Fe, Co, and Ni indicates that Ta-Ta bonding across the shared octahedral-site edge of the dimer can be stabilized by a reversible electrochemical reduction of Ta(V) to Ta(IV) for M = Cr, Fe, Co, and Ni but not for M = Mg. Chemical reduction of MTa2O6 by n-butyl lithium only reduced NiTa2O6 to any significant extent. With M = Fe, Co, or Ni, electrochemical formation of the Ta-Ta bonds is accompanied by a partial reduction of the Fe(II), Co(II), or Ni(II) to Fe(0), Co(0), or Ni(0). For M = Cr, two Li per formula unit can be inserted reversibly with no displacement of Cr(0). For M = Mg, no Mg(II) are displaced by Li insertion, but a solid-electrolyte interphase (SEI) layer is formed on the oxide with no evidence of Ta-Ta bonding. Stabilization of Ta-Ta bonding across a shared octahedral-site edge in a dimer appears to require significant hybridization of the Ta(V) 5d(0) and M 4s(0) states.


Journal of Advanced Ceramics | 2014

Investigation of strong shock wave interactions with CeO 2 ceramic

V. Jayaram; Asha Gupta; K. P. J. Reddy

Strong shock wave interactions with ceramic material ceria (CeO2) in presence of O2 and N2 gases were investigated using free piston driven shock tube (FPST). FPST is used to heat the test gas to very high temperature of about 6800–7700 K (estimated) at pressure of about 6.8–7.2 MPa for short duration (2–4 ms) behind the reflected shock wave. Ceria is subjected to super heating and cooling at the rate of about 106 K/s. Characterization of CeO2 sample was done before and after exposure to shock heated test gases (O2 and N2). The surface composition, crystal structure, electronic structure and surface morphology of CeO2 ceramic were examined using X-ray photoelectron spectroscopy (XPS), X-ray diffraction (XRD), Fourier transform infrared (FTIR) spectrometry, scanning electron microscopy (SEM) and high resolution transmission electron microscopy (HRTEM). Results obtained from the experimental investigations show that CeO2 can withstand high pressure accompanied by thermal shock without changing its crystal structure. Reducible CeO2 releases lattice oxygen making it possible to shift between reduced and oxidized states upon the interaction with shock heated gas. Due to such reaction mechanism, CeO2 ceramic undergoes nitrogen doping with decrease in lattice parameter. Investigations reveal that CeO2 retains its crystal structure during strong shock interaction, even at elevated pressure.


Chemistry of Materials | 2010

Correlation of Oxygen Storage Capacity and Structural Distortion in Transition-Metal-, Noble-Metal-, and Rare-Earth-Ion-Substituted CeO2 from First Principles Calculation

Asha Gupta; Umesh V. Waghmare; M. S. Hegde


Journal of Physical Chemistry C | 2013

Nanocolumnar Germanium Thin Films as a High-Rate Sodium-Ion Battery Anode Material

Paul R. Abel; Yong Mao Lin; Tania De Souza; Chia Yun Chou; Asha Gupta; John B. Goodenough; Gyeong S. Hwang; Adam Heller; C. Buddie Mullins


Journal of Physical Chemistry C | 2009

High Oxygen Storage Capacity and High Rates of CO Oxidation and NO Reduction Catalytic Properties of Ce1−xSnxO2 and Ce0.78Sn0.2Pd0.02O2-δ

Tinku Baidya; Asha Gupta; Paraag A. Deshpandey; Giridhar Madras; M. S. Hegde


Chemistry of Materials | 2009

Origin of activation of Lattice Oxygen and Synergistic Interaction in Bimetal-Ionic Ce0.89Fe0.1Pd0.01O2−δ Catalyst

Asha Gupta; Anil Kumar; Umesh V. Waghmare; M. S. Hegde


Journal of Power Sources | 2012

Optimum lithium-ion conductivity in cubic Li7−xLa3Hf2−xTaxO12

Asha Gupta; Ramaswamy Murugan; M. Parans Paranthaman; Zhonghe Bi; Craig A. Bridges; Masahiro Nakanishi; Alexei P. Sokolov; Kee Sung Han; Edward W. Hagaman; Hui Xie; C. Buddie Mullins; John B. Goodenough


Chemistry of Materials | 2009

Structural Investigation of Activated Lattice Oxygen in Ce1−xSnxO2 and Ce1−x−ySnxPdyO2−δ by EXAFS and DFT calculation

Asha Gupta; M. S. Hegde; K. R. Priolkar; Umesh V. Waghmare; P. R. Sarode; S. Emura

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John B. Goodenough

University of Texas at Austin

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C. Buddie Mullins

University of Texas at Austin

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M. S. Hegde

Indian Institute of Science

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Umesh V. Waghmare

Jawaharlal Nehru Centre for Advanced Scientific Research

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Hui Xie

University of Texas at Austin

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Preetam Singh

University of Texas at Austin

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Adam Heller

University of Texas at Austin

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Alexei P. Sokolov

Oak Ridge National Laboratory

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Craig A. Bridges

Oak Ridge National Laboratory

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M. Parans Paranthaman

Oak Ridge National Laboratory

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