G. Agnolet

most citedCharacteristic crossing point (

T_{*} \approx 2.7

K) in specific-heat curves of samples RuSr

_{2}

_{1.5}

_{0.5}

_{2}

_{10 - δ}

taken for different values of magnetic field

5 citations · 5 across the 3 of their papers we have counts for

collaborators

4 papers

cond-mat.dis-nn2020

Importance of Electronic Correlation in the Intermetallic Half-Heusler Compounds

Minjie Lu, Hao Chen, Glenn Agnolet

Low temperature scanning tunneling spectroscopy of HfNiSn shows a V^m(m < 1) zero bias anomaly around the Fermi level. This local density of states with a fractional power law shap…

physics.ins-det2020

Phonon-mediated High-voltage Detector with Background Rejection for Low-mass Dark Matter and Reactor Coherent Neutrino Scattering Experiments

H. Neog, R. Mahapatra, N. Mirabolfathi +6

We report the first demonstration of a phonon-mediated silicon detector technology that provides a primary phonon measurement in a low-voltage region, and a simultaneous indirect m…

physics.ins-det2020

Quantum Detection using Magnetic Avalanches in Single-Molecule Magnets

Hao Chen, Rupak Mahapatra, Glenn Agnolet +7

The detection of a single quantum of energy with high efficiency and low false positive rate is of considerable scientific interest, from serving as single quantum sensors of optic…

cond-mat.str-el2009★ 5 cited

Characteristic crossing point ( $T_{*} \approx 2.7$ K) in specific-heat curves of samples RuSr $_{2}$ Gd $_{1.5}$ Ce $_{0.5}$ Cu $_{2}$ O $_{10 - δ}$ taken for different values of magnetic field

B. I. Belevtsev, V. B. Krasovitsky, D. G. Naugle +3

Magnetic properties of polycrystalline samples of RuSr $_{2}$ (Gd $_{1.5}$ Ce $_{0.5}$ )Cu $_{2}$ O $_{10 - δ}$ , as-prepared (by solid-state reaction) and annealed (12 hours at 845 $^{\circ}$ C)…

Importance of Electronic Correlation in the Intermetallic Half-Heusler Compounds

Phonon-mediated High-voltage Detector with Background Rejection for Low-mass Dark Matter and Reactor Coherent Neutrino Scattering Experiments

Quantum Detection using Magnetic Avalanches in Single-Molecule Magnets

Characteristic crossing point (T∗​≈2.7 K) in specific-heat curves of samples RuSr2​Gd1.5​Ce0.5​Cu2​O10−δ​ taken for different values of magnetic field

Characteristic crossing point ( $T_{*} \approx 2.7$ K) in specific-heat curves of samples RuSr $_{2}$ Gd $_{1.5}$ Ce $_{0.5}$ Cu $_{2}$ O $_{10 - δ}$ taken for different values of magnetic field