Area of research
Condensed Matter Physics · Electronic, Optical and Magnetic Materials
Research interest
Research interests include Advanced Condensed Matter Physics, Magnetic and transport properties of perovskites and related materials, Multiferroics and related materials, and Physics of Superconductivity and Magnetism.
Vacancies tailoring lattice anharmonicity of Zintl-type thermoelectrics
Strong low-energy rattling modes enabled liquid-like ultralow thermal conductivity in a well-ordered solid
Nonlinear magnons and exchange Hamiltonians of the delafossite proximate quantum spin liquid candidates <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mtext>KYbSe</mml:mtext><mml:mn>2</mml:mn></mml:msub></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mtext>NaYbSe</mml:mtext><mml:mn>2</mml:mn></mml:msub></mml:math>
Magnetic properties of the quasi-XY Shastry-Sutherland magnet <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Er</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Be</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>SiO</mml:mi><mml:mn>7</mml:mn></mml:msub></mml:mrow></mml:math>
Accurate HER2 determination in breast cancer: a prominent COF-immobilized enzyme-enhanced electrochemical aptasensor employing 4-acetamidophenol as an efficient mediator
Extreme phonon anharmonicity underpins superionic diffusion and ultralow thermal conductivity in argyrodite Ag8SnSe6
Discovery of the High‐Entropy Carbide Ceramic Topological Superconductor Candidate (Ti<sub>0.2</sub>Zr<sub>0.2</sub>Nb<sub>0.2</sub>Hf<sub>0.2</sub>Ta<sub>0.2</sub>)C
Secondary phase effect on the thermoelectricity by doping Ag in SnSe
Magnetic field effects on the quantum spin liquid behaviors of NaYbS2
Successive Phase Transitions and Multiferroicity in Deformed Triangular-Lattice Antiferromagnets Ca <sub>3</sub> MNb <sub>2</sub> O <sub>9</sub> (M=Co, Ni) with Spatial Anisotropy
A cost-effective and humidity-tolerant chloride solid electrolyte for lithium batteries
Topological magnon insulators in two-dimensional van der Waals ferromagnets CrSiTe <sub>3</sub> and CrGeTe <sub>3</sub> : Toward intrinsic gap-tunability
Evolution of magnetic field induced ordering in the layered quantum Heisenberg triangular-lattice antiferromagnet <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Ba</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi>CoSb</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>9</mml:mn></mml:msub></mml:mrow></mml:math>
Experimental evidence for a valence-bond glass in the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mn>5</mml:mn><mml:msup><mml:mi>d</mml:mi><mml:mn>1</mml:mn></mml:msup></mml:mrow></mml:math> double perovskite <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Ba</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>YWO</mml:mi><mml:mn>6</mml:mn></mml:msub></mml:mrow></mml:math>
Magnetoelectric effect arising from a field-induced pseudo Jahn-Teller distortion in a rare-earth magnet
Negative Thermal Expansion of Ni-Doped MnCoGe at Room-Temperature Magnetic Tuning
Author Correction: The nature of spin excitations in the one-third magnetization plateau phase of Ba3CoSb2O9
The nature of spin excitations in the one-third magnetization plateau phase of Ba3CoSb2O9
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Ba</mml:mi><mml:mn>8</mml:mn></mml:msub><mml:msub><mml:mi>CoNb</mml:mi><mml:mn>6</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>24</mml:mn></mml:msub></mml:mrow></mml:math>: A spin-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mfrac><mml:mn>1</mml:mn><mml:mn>2</mml:mn></mml:mfrac></mml:math>triangular-lattice Heisenberg antiferromagnet in the two-dimensional limit
Magnetic properties of the triangular lattice magnets <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mn>4</mml:mn></mml:msub><mml:msup><mml:mi>B</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:msub><mml:mi>B</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>12</mml:mn></mml:msub></mml:mrow></mml:math> (<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>A</mml:mi><mml:mo>=</mml:mo><mml:mi>Ba</
Ferroelectricity of structural origin in the spin-chain compounds <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Ca</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi>Co</mml:mi><mml:mrow><mml:mn>2</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi>Mn</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>6</mml:mn></mml:msub></mml:mrow></mml:math>
Magnetic and electric properties of triangular lattice antiferromagnets Ba3ATa2O9 (A= Ni and Co)
Static and Dynamical Properties of the Spin-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mn>1</mml:mn><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:math>Equilateral Triangular-Lattice Antiferromagnet<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>Ba</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>CoSb</m
Rylene and Rylene Diimides: Comparison of Theoretical and Experimental Results and Prediction for High-Rylene Derivatives
Magnetism and multiferroicity of an isosceles triangular lattice antiferromagnet Sr<sub>3</sub>NiNb<sub>2</sub>O<sub>9</sub>
Twisting phonons in complex crystals with quasi-one-dimensional substructures
Competition between the inter- and intra-sublattice interactions in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Yb</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">V</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>7</mml:mn></mml:msub></mml:mrow></mml:math>
Magnetic phase diagram and multiferroicity of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi mathvariant="normal">Ba</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">MnNb</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>9</mml:mn></mml:msub></mml:math>: A spin-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mfrac><mml:mn>5</mml:mn><mml:mn>2</mml:mn></mml:mfrac></mml:math>triangular la
Series of phase transitions and multiferroicity in the quasi-two-dimensional spin-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mfrac><mml:mn>1</mml:mn><mml:mn>2</mml:mn></mml:mfrac></mml:math>triangular-lattice antiferromagnet<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>Ba</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi>CoNb</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>9</mml:mn></mml:msub></mm
Magnetic and structural phase transitions in the spinel compound<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mrow><mml:mi>Fe</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mrow><mml:mi>Cr</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math><mml:math xmlns:mml="http://