M. Padmanabhan

Single crystalline and polycrystalline samples of $S = 1/2$ Kagomé lattices {[Cu $_{3}$ (CO $_{3}$ ) $_{2}$ $(b p e)_{3}$ ](ClO $_{4}$ ) $_{2}$ } $_{n}$ and {[Cu $_{3}$ (CO $_{3}$ ) $_{2}$ $(b p y)_{3}$ ](Cl…

cond-mat.mtrl-sci2014★ 30 cited

Quasi-two-dimensional $S = 1/2$ magnetism of Cu[C $_{6}$ H $_{2}$ (COO) $_{4}$ ][C $_{2}$ H $_{5}$ NH $_{3}$ ] $_{2}$

R. Nath, M. Padmanabhan, S. Baby +5

We report structural and magnetic properties of the spin- $\frac{1}{2}$ quantum antiferromagnet Cu[C $_{6}$ H $_{2}$ (COO) $_{4}$ ][C $_{2}$ H $_{5}$ NH $_{3}$ ] $_{2}$ by means of single-crystal x-ray diffractio…

Tuning of magnetic frustration in S=1/2 Kagomé lattices {[Cu3​(CO3​)2​(bpe)3​](ClO4​)2​}n​ and {[Cu3​(CO3​)2​(bpy)3​](ClO4​)2​}n​ through rigid and flexible ligands

Quasi-two-dimensional S=1/2 magnetism of Cu[C6​H2​(COO)4​][C2​H5​NH3​]2​

Tuning of magnetic frustration in $S = 1/2$ Kagomé lattices {[Cu $_{3}$ (CO $_{3}$ ) $_{2}$ $(b p e)_{3}$ ](ClO $_{4}$ ) $_{2}$ } $_{n}$ and {[Cu $_{3}$ (CO $_{3}$ ) $_{2}$ $(b p y)_{3}$ ](ClO $_{4}$ ) $_{2}$ } $_{n}$ through rigid and flexible ligands

Quasi-two-dimensional $S = 1/2$ magnetism of Cu[C $_{6}$ H $_{2}$ (COO) $_{4}$ ][C $_{2}$ H $_{5}$ NH $_{3}$ ] $_{2}$