You Lai

Electronic landscape of the <i>f</i> -electron intermetallics with the ThCr ₂ Si ₂ structure

Anisotropy of the T vs. H phase diagram and the HO/LMAFM phase boundary in URu2−xFexSi2

Spectroscopic evidence for the direct involvement of local moments in the pairing process of the heavy-fermion superconductor <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>CeCoIn</mml:mi><mml:mn>5</mml:mn></mml:msub></mml:math>

An_1.33T₄Al₈Si₂ (An = Ce, Th, U, Np; T = Ni, Co): Actinide Intermetallics with Disordered Gd_1+<i>x</i>Fe₄Si_{10–<i>y</i>} Structure Type Grown from Metal Flux

Scale-invariant magnetic anisotropy in RuCl3 at high magnetic fields

Superstructures and Superconductivity Linked with Pd Intercalation in Nb₂Pd<i>_x</i>Se₅

Pressure-induced suppression of ferromagnetism in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>CePd</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">P</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>

Zeeman-Induced Valley-Sensitive Photocurrent in Monolayer <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>MoS</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>

Enhanced thermoelectric performance of heavy-fermion compounds Yb <i>TM</i> ₂ Zn ₂₀ ( <i>TM</i> = Co, Rh, Ir) at low temperatures

U_1.33T₄Al₈Si₂ (T = Ni, Co): Complex Uranium Silicides Grown from Aluminum/Gallium Flux Mixtures

Instability of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>f</mml:mi></mml:math>-electron state in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>URu</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Si</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 mathvariant="normal">P</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math> probed using high magnetic fields

Fermi surface of the flat-band intermetallics <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>A</mml:mi><mml:mi mathvariant="normal">P</mml:mi><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:mrow></mml:math> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mo>(</mml:mo><mml:mrow><mml:mi>A</mml:mi><mml:mo>=</mml:mo><mml:mi>Pb</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.28em"/><mml:mi>Sn</mml:mi></mml:mrow><mml:mo>)</mm

Bulk Fermi Surfaces of the Dirac Type-II Semimetallic Candidates <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>M</mml:mi><mml:msub><mml:mrow><mml:mi>Al</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math> (Where <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>M</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="normal">V</mml:mi></mml:mrow></mml:math>, Nb, and Ta)

Ferromagnetic quantum critical point in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>CePd</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">P</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math> with Pd <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mo>→</mml:mo></mml:math> Ni substitution

U₈Al₁₉Si₆, A Uranium Aluminide Silicide with a Stuffed Supercell Grown from Aluminum Flux

Tuning the ferromagnetic tri-critical point and quantum critical point in Ce(Pd&lt;sub&gt;1-&lt;em&gt;x&lt;/em&gt;&lt;/sub&gt;Ni&lt;sub&gt;&lt;em&gt;x&lt;/em&gt;&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;P&lt;sub&gt;2&lt;/sub&gt; under high magnetic fields [Poster]

Bulk Fermi surface of the Weyl type-II semimetallic candidate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>γ</mml:mi><mml:mo>−</mml:mo><mml:msub><mml:mi>MoTe</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>

Possible devil's staircase in the Kondo lattice CeSbSe

Correlated electron state in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>CeCu</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Si</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math> controlled through Si to P substitution

Temperature Dependent Magnetoresistance of CeCu2Si2 up to 60 T [Proposal: P14728]