| Symmetry and the order of events in time: description of a reversible thermal energy converter composed of negative mass | Randy WAYNE | 1–21 |
| Thermodynamic properties of the noncommutative black hole in (z = 3)-Horava Lifshitz gravity | Mourad NACH,Khadija BILAL,My Brahim SEDRA,Abderrahman EL BOUKILI | 22–29 |
| Thermodynamic properties of the noncommutative black hole in (z = 3)-Horava-Lifshitz gravity | Mourad NACH, Khadija BILAL, My Brahim SEDRA, Abderrahman El BOUKILI | 22–29 |
| Temperature dependence for the synthetic magnetization of a rotating Bose gas in harmonic trap | M. Azza El BADRY | 30–38 |
| One proton emission with structural effects in medium mass nuclei | Chandrasekaran Anu RADHA,Velayudham RAMASUBRAMANIAN | 39–48 |
| Spin assignment and behavior of superdeformed bands in A∼150 mass region | Ali KHALAF,Manal SIRAG,Mahmoud TAHA | 49–62 |
| Spin assignment and behavior of superdeformed bands in A\\sim 150 mass region | Ali KHALAF, Manal SIRAG, Mahmoud TAHA | 49–62 |
| Spin-one DKP equation in the presence of nonminimal vector Woods Saxon potential in (1 + 1) dimensions | Hassan HASSANABADI,Zahra MOLAEE,Saber ZARRINKAMAR | 63–73 |
| Spin-one DKP equation in the presence of nonminimal vector Woods-Saxon potential in (1 + 1) dimensions | Hassan HASSANABADI, Zahra MOLAEE, Saber ZARRINKAMAR | 63–73 |
| The nonrelativistic molecular Tietz potential | Hossein NIKOOFARD,Elham MAGHSOODI,Saber ZARRINKAMAR,Mohsen FARHADI,Hassan HASSANABADI | 74–82 |
| DKP equation under scalar and vector Kratzer potentials | Bentol Hoda YAZARLOO,Hassan HASSANABADI,Saber ZARRINKAMAR | 83–89 |
| Empirical rule for the pair break mechanism in three-quasiparticle rotational bands | Sukhjeet Singh DHINDSA,Sushil KUMAR,Jatinder Kumar SHARMA | 90–98 |
| Investigation of dominant states in the collisions of Ar VII and Kr XXIV with $H_2$ and He targets |