M. Blankenhorn

When spin-orbit-entangled $d$ -electrons reside on a honeycomb lattice, rich quantum states are anticipated to emerge, as exemplified by the $d^{5}$ Kitaev materials. Distinct yet equ…

cond-mat.str-el2020★ 4 cited

Design of opposed-anvil-type high-pressure cell for precision magnetometry and its application to quantum magnetism

Naoka Hiraoka, Kelton Whiteaker, Marian Blankenhorn +4

We have developed a much sensitve technique to conduct magnetometry under ultrahigh pressures up to 6.3~GPa, which can detect a weak volume susceptibilities as small as $\sim 10^{-…

cond-mat.str-el2020★ 32 cited

Quantum Paraelectricity in the Kitaev Quantum-Spin-Liquid Candidates H $_{3}$ LiIr $_{2}$ O $_{6}$ and D $_{3}$ LiIr $_{2}$ O $_{6}$

K. Geirhos, P. Lunkenheimer, M. Blankenhorn +7

H3LiIr2O6 is the first honeycomb-lattice system without any signs of long-range magnetic order down to the lowest temperatures, raising the hope for the realization of an ideal Kit…

cond-mat.str-el2014★ 14 cited

ESR studies on the spin-liquid candidate $κ$ -(BEDT-TTF) $_{2}$ Cu $_{2}$ (CN) $_{3}$ : anomalous response below $T = 8$ K

K. G. Padmalekha, M. Blankenhorn, T. Ivek +3

The organic conductor $κ$ -(BEDT-TTF) $_{2}$ Cu $_{2}$ (CN) $_{3}$ seems to form a quantum spin liquid, although at low temperatures unusual properties are seen in the charge, spin and latti…

Competing spin-orbital singlet states in the 4d4 honeycomb ruthenate Ag3​LiRu2​O6​

Design of opposed-anvil-type high-pressure cell for precision magnetometry and its application to quantum magnetism

Quantum Paraelectricity in the Kitaev Quantum-Spin-Liquid Candidates H3​LiIr2​O6​ and D3​LiIr2​O6​

ESR studies on the spin-liquid candidate κ-(BEDT-TTF)2​Cu2​(CN)3​: anomalous response below T=8 K

Competing spin-orbital singlet states in the 4 $d^{4}$ honeycomb ruthenate Ag $_{3}$ LiRu $_{2}$ O $_{6}$

Quantum Paraelectricity in the Kitaev Quantum-Spin-Liquid Candidates H $_{3}$ LiIr $_{2}$ O $_{6}$ and D $_{3}$ LiIr $_{2}$ O $_{6}$

ESR studies on the spin-liquid candidate $κ$ -(BEDT-TTF) $_{2}$ Cu $_{2}$ (CN) $_{3}$ : anomalous response below $T = 8$ K