Saikat Nandi

most citedObservation of a gapped phase in the one-dimensional

S = \frac{1}{2}

Heisenberg antiferromagnetic chain Cu(Ampy)ClBr

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

collaborators

3 papers

cond-mat.str-el2026

Novel Quantum Spin Liquid States in the $S = \frac{1}{2}$ Three-Dimensional Compound Y $_{3}$ Cu $_{2}$ Sb $_{3}$ O $_{14}$

Saikat Nandi, Rounak Das, M. Hemmida +10

The three-dimensional $S = \frac{1}{2}$ system Y $_{3}$ Cu $_{2}$ Sb $_{3}$ O $_{14}$ consists of two inequivalent Cu $^{2 +}$ sites, each forming an edge shared triangular lattice. Our m…

cond-mat.str-el2026★ 2 cited

Observation of a gapped phase in the one-dimensional $S = \frac{1}{2}$ Heisenberg antiferromagnetic chain Cu(Ampy)ClBr

Saikat Nandi, Monika Jawale, Sanjay Bachhar +9

Spin-1/2 Heisenberg antiferromagnetic frustrated spin chain systems display exotic ground states with unconventional excitations and distinct quantum phase transitions as the ratio…

cond-mat.str-el2025

Frustration-driven unconventional magnetism in the Mn $^{2 +}$ ( $S = \frac{5}{2}$ ) based two-dimensional triangular-lattice antiferromagnet Ba $_{3}$ MnTa $_{2}$ O $_{9}$

Romario Mondal, Sk. Soyeb Ali, Saikat Nandi +11

A triple perovskite oxide Ba $_{3}$ MnTa $_{2}$ O $_{9}$ has been synthesized and its magnetic properties have been investigated through dc and ac magnetization, specific heat, electron…

Novel Quantum Spin Liquid States in the S=21​ Three-Dimensional Compound Y3​Cu2​Sb3​O14​

Observation of a gapped phase in the one-dimensional S=21​ Heisenberg antiferromagnetic chain Cu(Ampy)ClBr

Frustration-driven unconventional magnetism in the Mn2+ (S=25​) based two-dimensional triangular-lattice antiferromagnet Ba3​MnTa2​O9​

Novel Quantum Spin Liquid States in the $S = \frac{1}{2}$ Three-Dimensional Compound Y $_{3}$ Cu $_{2}$ Sb $_{3}$ O $_{14}$

Observation of a gapped phase in the one-dimensional $S = \frac{1}{2}$ Heisenberg antiferromagnetic chain Cu(Ampy)ClBr

Frustration-driven unconventional magnetism in the Mn $^{2 +}$ ( $S = \frac{5}{2}$ ) based two-dimensional triangular-lattice antiferromagnet Ba $_{3}$ MnTa $_{2}$ O $_{9}$