The most stringent constraint on the so-called effective electron neutrino mass from the present neutrinoless double beta decay experiments is |M_{ee}| < 0.2 eV, while the planned next generation experiment GENIUS is anticipated to reach a considerably more stringent limit |M_{ee}|< 0.001 eV. We investigate the constraints these bounds set on the neutrino masses and mixings of neutrinos in four-neutrino models where there exists a sterile neutrino along with the three ordinary neutrinos. We find that the GENIUS experiment would be sensitive to the electron neutrino masses down to the limit m_{\nu_e}\lsim 0.024 eV in such a scenario
The recent analysis of the normalization of reactor antineutrino data, the calibration data of solar...
AbstractWe present new limits on mixing between active and sterile neutrinos using more than 11 year...
Considering the scheme with mixing of three neutrinos and a mass hierarchy that can accommodate the ...
All existing data on neutrino oscillations (including those from the LSND experiment) imply a four n...
All existing data on neutrino oscillations (including those from the LSND experiment) imply a four n...
We show that, in the framework of a general model with mixing of three Majorana neutrinos and a neut...
It is shown that at least four massive neutrinos are needed in order to accommodate the evidences in...
We investigate the predictions for neutrinoless double beta ((ββ)0ν -) decay effective Majorana mass...
We study the possible structure of the neutrino mass matrix taking into consideration the solar and ...
Neutrinoless double beta decay belongs to the most sensitive tools for thesearch of new physics beyo...
AbstractWe study the possible structure of the neutrino mass matrix taking into consideration the so...
Double beta decay is indispensable to solve the question of the neutrino mass matrix together with n...
The relations between the effective Majorana mass of the electron neutrino, $m_{ee}$, responsible fo...
AbstractAssuming positive observation of neutrinoless double bata decay together with the CHOOZ reac...
In order to accommodate the neutrino oscillation signals from the solar, atmospheric, and LSND data,...
The recent analysis of the normalization of reactor antineutrino data, the calibration data of solar...
AbstractWe present new limits on mixing between active and sterile neutrinos using more than 11 year...
Considering the scheme with mixing of three neutrinos and a mass hierarchy that can accommodate the ...
All existing data on neutrino oscillations (including those from the LSND experiment) imply a four n...
All existing data on neutrino oscillations (including those from the LSND experiment) imply a four n...
We show that, in the framework of a general model with mixing of three Majorana neutrinos and a neut...
It is shown that at least four massive neutrinos are needed in order to accommodate the evidences in...
We investigate the predictions for neutrinoless double beta ((ββ)0ν -) decay effective Majorana mass...
We study the possible structure of the neutrino mass matrix taking into consideration the solar and ...
Neutrinoless double beta decay belongs to the most sensitive tools for thesearch of new physics beyo...
AbstractWe study the possible structure of the neutrino mass matrix taking into consideration the so...
Double beta decay is indispensable to solve the question of the neutrino mass matrix together with n...
The relations between the effective Majorana mass of the electron neutrino, $m_{ee}$, responsible fo...
AbstractAssuming positive observation of neutrinoless double bata decay together with the CHOOZ reac...
In order to accommodate the neutrino oscillation signals from the solar, atmospheric, and LSND data,...
The recent analysis of the normalization of reactor antineutrino data, the calibration data of solar...
AbstractWe present new limits on mixing between active and sterile neutrinos using more than 11 year...
Considering the scheme with mixing of three neutrinos and a mass hierarchy that can accommodate the ...