S. Hameed

collaborators

4 papers

cond-mat.mtrl-sci2025

Uniaxial strain tuning of polar lattice vibrations in KTaO $_{3}$ and SrTiO $_{3}$

I. Khayr, N. Somun, S. Hameed +11

The interplay of electronic and structural degrees of freedom is a prominent feature of many quantum materials and of particular interest in systems with strong ferroelectric fluct…

cond-mat.supr-con2025

Evolution of spin excitations in superconducting La $_{2 - x}$ Ca $_{x}$ CuO $_{4 - I^´}$ from the underdoped to the heavily overdoped regime

S. Hameed, Y. Liu, M. Knauft +8

We investigate high-energy spin excitations in hole-doped La $_{2 - x}$ Ca $_{x}$ CuO $_{4 - I^´}$ films across a broad Ca doping range $x = 0.05 - 0.50$ using resonant inelastic x-ray scatter…

cond-mat.supr-con2025

Coincident onset of charge order and pseudogap in a homogeneous high-temperature superconductor

D. Betto, S. Nakata, F. Pisani +10

Understanding high-temperature superconductivity in cuprates requires knowledge of the metallic phase it evolves from, particularly the pseudogap profoundly affecting the electroni…

cond-mat.str-el2025

Nature of the ferromagnet-paramagnet transition in Y $_{1 - x}$ Ca $_{x}$ TiO $_{3}$

S. Hameed, I. Khayr, J. Joe +8

Neutron scattering, magnetometry, and muon spin rotation ( $I^¼$ SR) measurements were performed to investigate the magnetic order and spin dynamics across the ferromagnet-to-paramagn…

Uniaxial strain tuning of polar lattice vibrations in KTaO3​ and SrTiO3​

Evolution of spin excitations in superconducting La2−x​Cax​CuO4−I^´​ from the underdoped to the heavily overdoped regime

Coincident onset of charge order and pseudogap in a homogeneous high-temperature superconductor

Nature of the ferromagnet-paramagnet transition in Y1−x​Cax​TiO3​

Uniaxial strain tuning of polar lattice vibrations in KTaO $_{3}$ and SrTiO $_{3}$

Evolution of spin excitations in superconducting La $_{2 - x}$ Ca $_{x}$ CuO $_{4 - I^´}$ from the underdoped to the heavily overdoped regime

Nature of the ferromagnet-paramagnet transition in Y $_{1 - x}$ Ca $_{x}$ TiO $_{3}$