A.S. BARABASH
Double-beta decay to the excited states (Experiment). .  /447-453/

A.S. BARABASH
Is the weak interaction constant really constant ? .  /455-461/

A.BOBYK, W.A.KAMIŃSKI, P. ZARĘBA
Comparison of various extensions of the QRPA formalism for the double-beta decay.  /463-470/

O. CIVITARESE
Isospin symmetry breaking in double-beta-decay processes.  /471-483/

A. GARCÍA
Electron-capture decays of ¹⁰⁰Tc and ¹¹⁶In and nuclear structure relevant for 2b decays. .  /485-487/

W.A. KAMIŃSKI, A. WODECKI, F. ŠIMKOVIC
Minimal supersymmetric standard model with the gauge mediated supersymmetry breaking and the. neutrinoless double-beta decay.  / 489-498/

G. PANTIS, F. ŠIMKOVIC
.The role of the induced currents in the mass mechanism of neutrinoless double-beta decay.  /499-507/

M.R. QUAGLIA, P.F. BORTIGNON, G. COLO, R.A. BROGLIA
Nuclear field theory and highly forbidden nuclear decays: the case of ¹²³Te.  /509-517/

O.A. RUMYANTSEV, M.H. URIN
On the hindrance of the two-neutrino bb-decay rate.  /529-535/

M. SAMBATARO
Multistep variational approach to collective excitations.  /537-544/

F. ŠIMKOVIC
Quasiparticle random phase approximation with the Pauli exclusion principle fully fulfilled.  /545-552/

I. ŠTEKL, P. ČERMÁK, P. BENEŠ, V.B. BRUDANIN, N.I. RUKHADZE, V.G. EGOROV V.E. KOVALENKO, A. KOVALÍK, A.V. SALAMATIN, V.V. TSOUPKO-SITNIKOV, Ts.VYLOV, Ch. BRIANCON, F. ŠIMKOVIC
Experiments TGV I (double-beta decay of ⁴⁸Ca) and TGV II (double-beta decay of ¹⁰⁶Cd and ⁴⁸Ca).  /553-559/

J. SUHONEN, O. CIVITARESE
Testing the single-state dominance in two-neutrino double-beta decay.  / 561-565/

J. SUHONEN, M. AUNOLA, M. KORTELAINEN, T. SIISKONEN, M. HJORTH-JENSEN
Refined shell-model matrix elements for muon capture processes.  /567-575/

A.V. TIKHOMIROV
Centrifugal enrichment of stable isotopes and modern physical experiments.  /577-580/

A.A. RADUTA
Theoretical results and experimental projects for 0n bb decay.  /581-586/

J. SUHONEN
Nuclear-structure aspects of rare and exotic weak decays.  /587-591/