| Initial electron beam polarization measurement in e-$\gamma$ collisions | Gökhan ÜNEL | 169–177 |
| Initial electron beam polarization measurement in e-$gamma$ collisions | Gökhan ÜNEL | 169–177 |
| Initial Electron Beam Polarization Measurement in e-g Collisions | Gökhan ÜNEL | 169–177 |
| Fourth SM Family Manifestations at CLIC | R. ÇİFTÇİ,A.K. ÇİFTÇİ,E. RECEPOĞLU,S. SULTANSOY | 179–186 |
| Nuclear Matrix Elements of Double Beta Decay in Deformed Nuclei | Cevat SELAM,ATALAY KÜÇÜKBURSA,HASAN BİRCAN,HASAN ALİ AYGÖR,TAHSİN BABACAN,İSMAİL MARAŞ,ALİ KÖKCE | 187–193 |
| High-Pressure Phase Transition in Some Alkali Halides Using Interatomic Potential Model | Harun Reşit YAZAR | 195–199 |
| Clebsch-Gordan Equalities that imply the Vanishing of Particular 6j Symbols | Harry A. MAVROMATIS | 201–203 |
| Electron Transport Mechanism in GaN/AlGaN HEMT Structures | SİBEL GÖKDEN | 205–210 |
| Characterization of $In_4Te_3$ single crystals | M. DONGOL,M. M. NASSARY,M. K. GERGES,M. A. SEBAG | 211–218 |
| Characterization of In4Te3 Single crystals | M. DONGOL, M. M. NASSARY, M. K. GERGES, M. A. SEBAG | 211–218 |
| Variation in thickness of copper films deposites at various distances and angles using the thermionic vacuum arc | TAMER AKAN,Naci EKEM | 219–224 |
| Variation in Thickness of Copper Films Deposited at Various Distances and Angles Using the Thermionic Vacuum Arc | Tamer AKAN, Naci EKEM | 219–224 |
| Study of the Structure and Some Physical Properties of Sodium-Boro-Phosphate Glasses Containing Antimony and Iron Oxides | Karam Abdel-Aati ALI,Ahmed Gamal El-Din MOSTAFA | 225–233 |