S. S. Islam

activity

20242026

most citedPressure-Induced Enhancement of Superfluid Density in Transition Metal Dichalcogenides with and without Charge Density Wave

2 citations · 4 across the 15 of their papers we have counts for

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Showing 2025Show all

7 papers · 1 filter

cond-mat.mtrl-sci2025

Inhomogeneous dynamic state in the double trillium lattice antiferromagnet KBaFe $_{2}$ (PO $_{4}$ ) $_{3}$

S. J. Sebastian, S. S. Islam, R. Kolay +11

The three-dimensional (3D) magnet KBaFe $_{2}$ (PO $_{4}$ ) $_{3}$ hosts a double-trillium lattice of Fe $^{3 +}$ (spin, $S = 5/2$ ) ions offering a prototypical platform to study the frustration…

cond-mat.supr-con2025

Distinct Uniaxial Stress and Pressure Fingerprint of Superconductivity in the 3D Kagome Lattice Compound CeRu2

O. Gerguri, D. Das, V. Sazgari +16

The exploration of tunable superconductivity in strongly correlated electron systems is a central pursuit in condensed matter physics, with implications for both fundamental unders…

cond-mat.supr-con2025

Discovery of High-Temperature Charge Order and Time-Reversal Symmetry-Breaking in the Kagome Superconductor YRu3Si2

P. Kràl, J. N. Graham, V. Sazgari +21

The identification of high-temperature unconventional charge order and superconductivity in kagome quantum materials is pivotal for deepening our understanding of geometrically fru…

cond-mat.supr-con2025

Competing Quantum Orders in 6R-TaS $_{2}$ : Unconventional Superconductivity, Charge Order, and an Anomalous Hall Effect phase

V. Sazgari, J. N. Graham, S. S. Islam +13

The transition metal dichalcogenide 6R-TaS $_{2}$ offers a natural platform for studying the interplay among charge density wave (CDW) order, superconductivity, and transport anomal…

cond-mat.supr-con2025★ 1 cited

Contrasting $c$ -axis and in-plane uniaxial stress effects on superconductivity and stripe order in La $_{1.885}$ Ba $_{0.115}$ CuO $_{4}$

S. S. Islam, V. Sazgari, J. N. Graham +16

The cuprate superconductor La $_{2 - x}$ Ba $_{x}$ CuO $_{4}$ (LBCO) near $x = 0.125$ is a striking example of intertwined electronic orders, where 3D superconductivity is anomalously suppresse…

cond-mat.str-el2025

Magnetic order and spin dynamics across the ferromagnetic quantum critical point in Ni\boldmath{ $_{1 - x}$ }Mo\boldmath{ $_{x}$ }

H. K. Dara, S. S. Islam, A. Magar +5

Realizing a quantum critical point (QCP) in clean ferromagnetic (FM) metals has remained elusive due to the coupling of magnetization to the electronic soft modes that drive the tr…

cond-mat.str-el2025

Emergence of a Fluctuating Ground State in Y-kapellasite under Pressure

Dipranjan Chatterjee, Petr Doležal, Federico Abbruciati +17

Y-kapellasite (Y $_{3}$ Cu $_{9}$ (OH) $_{19}$ Cl $_{8}$ ), which hosts an original anisotropic kagome sublattice, is a promising candidate for studying elusive and complex correlated physics. I…

Inhomogeneous dynamic state in the double trillium lattice antiferromagnet KBaFe2​(PO4​)3​

Distinct Uniaxial Stress and Pressure Fingerprint of Superconductivity in the 3D Kagome Lattice Compound CeRu2

Discovery of High-Temperature Charge Order and Time-Reversal Symmetry-Breaking in the Kagome Superconductor YRu3Si2

Competing Quantum Orders in 6R-TaS2​: Unconventional Superconductivity, Charge Order, and an Anomalous Hall Effect phase

Contrasting c-axis and in-plane uniaxial stress effects on superconductivity and stripe order in La1.885​Ba0.115​CuO4​

Magnetic order and spin dynamics across the ferromagnetic quantum critical point in Ni\boldmath{1−x​}Mo\boldmath{x​}

Emergence of a Fluctuating Ground State in Y-kapellasite under Pressure

Inhomogeneous dynamic state in the double trillium lattice antiferromagnet KBaFe $_{2}$ (PO $_{4}$ ) $_{3}$

Competing Quantum Orders in 6R-TaS $_{2}$ : Unconventional Superconductivity, Charge Order, and an Anomalous Hall Effect phase

Contrasting $c$ -axis and in-plane uniaxial stress effects on superconductivity and stripe order in La $_{1.885}$ Ba $_{0.115}$ CuO $_{4}$

Magnetic order and spin dynamics across the ferromagnetic quantum critical point in Ni\boldmath{ $_{1 - x}$ }Mo\boldmath{ $_{x}$ }