| Deconvolution analysis of thermoluminescent glow curves in various commercial dosimeters using two different approaches in the framework of the one-trap, one-recombination model | Eren ŞAHİNER | 477–490 |
| Optical visible wavelength region selective reflector design for photovoltaic cells using photonic crystal | Veysel KORKMAZ, Ali ÇETİN | 491–497 |
| Monte Carlo simulation of a medical linear accelerator for filtered and FFF systems | Çağri YAZĞAN, Yiğit ÇEÇEN | 498–506 |
| Temperature measurements in a manufactured RF plasma jet in various Ar/N$_{2}$ mixtures | Mohammad Nasir Rostami RAVARI, Alireza GANJOVI, Farideh SHOJAEI, Amir FALAHAT | 507–519 |
| Elastic scattering analysis of $^{12}$C+$^{24}$Mg by WKB method | Orhan BAYRAK | 520–525 |
| Calculation of the frequency shifts and damping constant for the Raman modes (A$_{1g}$, B$_{1})$ near the tetragonal-cubic transition in SrTiO$_{3}$ | Ali KİRACI, Hasan Hamit YURTSEVEN | 526–535 |
| Synthesis of Ni-Fe thin films by electrochemical deposition technique and characterization of their microstructures and surface morphologies | Umut SARAÇ, Malik KAYA, Mevlana Celalettin BAYKUL | 536–544 |
| Quark shapes of most modern parton distribution functions | Hasan OĞUL | 545–550 |
| Analytical solution of the local fractional Klein-Gordon equation for generalized Hulthen potential | Hasibe Hale KARAYER, Ahmet Doğan DEMİRHAN, Fevzi BÜYÜKKILIÇ | 551–559 |
| Applying a self-feedback method to control chaos in the Buck converter | Mei Mei JIA | 560–575 |