| Materials anddevices for integrated room temperature quantum spintronics | Mehmet Cengiz ONBAŞLI | 74–81 |
| Materials anddevices for integrated room temperature quantum spintronics | Mehmet Cengiz ONBAŞLI | 74–81 |
| Hollow-core optical fiber with eight-pointed star cladding structure for low-loss transmission in telecom bands | Mustafa ORDU | 82–89 |
| Hollow-core optical fiber with eight-pointed star cladding structure for low-losstransmission in telecom bands | Mustafa ORDU | 82–89 |
| ψ(2S) and J/ψ production in pp collisions at √s= 7, 8 and 13 TeV | Yasir ALI,Uzma TABASSAM,Syed Uzair AHMED SHAH,Atif ARIF,Mais SULEYMANOV,Zain KHAIRONIZAM | 90–104 |
| ψ(2S) and J/ψ production in pp collisions at √s= 7, 8 and 13 TeV | Yasir ALI, Zain ZAİN, Uzma TABASSAM, Syed Uzair AHMED SHAH, Atif ARIF, Mais SULEYMANOV | 90–104 |
| The effect of Sn doping on the electronic and mechanical properties ofTi3Al1−xSnxC2MAX phases | Ayşenur GENCER,Aytac ERKİSİ | 105–117 |
| The effect of Sn doping on the electronic and mechanical properties ofTi3Al1−xSnxC2MAX phases | Ayşenur GENCER, Aytaç ERKİŞİ | 105–117 |
| Hydrogen sensing properties of Pd loaded TiO2 nanorods | Serkan BÜYÜKKÖSE | 118–130 |
| Hydrogen sensing properties of Pd loaded TiO2 nanorods | Serkan BÜYÜKKÖSE | 118–130 |