K. Chaturvedi

The $(β^{+} β^{+})_{0 ν}$ and $(ε β^{+})_{0 ν}$ modes of $^{96}$ Ru, $^{102}$ Pd, $^{106}$ Cd, $^{124}$ Xe, $^{130}$ Ba and $^{156}$ Dy isotopes are studied in the Projected Hartr…

nucl-th2008★ 59 cited

Nuclear deformation and neutrinoless double- $β$ decay of $^{94, 96}$ Zr, $^{98, 100}$ Mo, $^{104}$ Ru, $^{110}$ Pd, $^{128, 130}$ Te and $^{150}$ Nd nuclei in mass mechanism

K. Chaturvedi, R. Chandra, P. K. Rath +2

The $(β^{-} β^{-})_{0 ν}$ decay of $^{94, 96}$ Zr, $^{98, 100}$ Mo, $^{104}$ Ru, $^{110}$ Pd, $^{128, 130}$ Te and $^{150}$ Nd isotopes for the $0^{+} \to 0^{+}$ transition is studied in the P…

Deformation effects and neutrinoless positron ββ decay of 96Ru, 102Pd, 106Cd, 124Xe, 130Ba and 156Dy isotopes within Majorona neutrino mass mechanism

Nuclear deformation and neutrinoless double-β decay of 94,96Zr, 98,100Mo, 104Ru, 110Pd, 128,130Te and 150Nd nuclei in mass mechanism

Deformation effects and neutrinoless positron $β β$ decay of $^{96}$ Ru, $^{102}$ Pd, $^{106}$ Cd, $^{124}$ Xe, $^{130}$ Ba and $^{156}$ Dy isotopes within Majorona neutrino mass mechanism

Nuclear deformation and neutrinoless double- $β$ decay of $^{94, 96}$ Zr, $^{98, 100}$ Mo, $^{104}$ Ru, $^{110}$ Pd, $^{128, 130}$ Te and $^{150}$ Nd nuclei in mass mechanism