activity
20102023
most citedLetter of Intent for KM3NeT 2.0

908 citations · 2.4k across the 44 of their papers we have counts for

collaborators

46 papers

quant-ph2023★ 1 cited

Zero-Point Energy Density at the Origin of the Vacuum Permittivity and Photon Propagation Time Fluctuation

Christophe Hugon, Vladimir Kulikovskiy

We give a vacuum description with zero-point density for virtual fluctuations. One of the goals is to explain the origin of the vacuum permittivity and permeability and to calculat…

nucl-ex2020★ 1 cited

Search for Periodic Modulations of the Rate of Double-Beta Decay of Mo in the NEMO-3 Detector

3 Collaboration, R. Arnold, C. Augier +105

Double-beta decays of Mo from the 6.0195-year exposure of a 6.914 kg high-purity sample were recorded by the NEMO-3 experiment that searched for neutrinoless double-beta de…

quant-ph2020

Paving Through the Vacuum

Christophe M. F. Hugon, Vladimir Kulikovskiy

Using the model in which the vacuum is filled with virtual fermion pairs we propose an effective description of photon propagation compatible with the wave-particle duality and the…

physics.ins-det2020★ 6 cited

Search for the double-beta decay of 82Se to the excited states of 82Kr with NEMO-3

3 collaboration, C. Augier, A. S. Barabash +104

The double-beta decay of 82Se to the 0+1 excited state of 82Kr has been studied with the NEMO-3 detector using 0.93 kg of enriched 82Se measured for 4.75 y, corresponding to an exp…

physics.ins-det2019★ 39 cited

Neutrino Physics with an Opaque Detector

A. Cabrera, A. Abusleme, J. dos Anjos +59

In 1956 Reines & Cowan discovered the neutrino using a liquid scintillator detector. The neutrinos interacted with the scintillator, producing light that propagated across transpar…

nucl-ex2019★ 6 cited

Detailed studies of Mo two-neutrino double beta decay in NEMO-3

3 Collaboration, R. Arnold, C. Augier +103

The full data set of the NEMO-3 experiment has been used to measure the half-life of the two-neutrino double beta decay of Mo to the ground state of Ru, $T_{1/2} =…