## 1 Introduction  
Various glass-based systems have their own medical, industrial, and technological applications due to their intrinsic magnetic, optical, physical, structural, and mechanical features. These properties, in principle, can be measured in house-based laboratories due to their ease of modification and access for certain experimental setups [1; 2; 3; 4]. On the other hand, radiation-matter interactions may be best performed at synchrotron-based facilities such as the Deutsches Elektronen-Synchrotron (DESY) (Hamburg, Germany), European Synchrotron Radiation Facility (ESRF) (Grenoble, France), or National Synchrotron Light Source (NSLS) (Brookhaven, NY, USA). Unfortunately, access to these worldwide state-of-art laboratories is very restricted for users due to their tight beam time schedule. Therefore, theoretical calculations or numerical simulations may be used as one alternative to overcome these experimental deficiencies in order to shed light on X-ray or \(\gamma\)-ray radiation-matter interactions. For this purpose, the study will focus on calculations and simulations of SiO\({}_{2}\)-Na\({}_{2}\)O-CaO glasses with different contents of Sb\({}_{2}\)O\({}_{3}\) (see below), which have emerged in different applications [5]. Heavy metal oxide (HMO) glasses, such as Bi\({}_{2}\)O\({}_{3}\), Sb\({}_{2}\)O\({}_{3}\), and PbO, have been investigated due to their interesting properties in infrared and nonlinear optics [6]. Additionally, soda-lime-silica glasses are currently the subject of extensive research because of their various applications in medical and dental fields, in addition to their utilization in industrial applications [7; 8]. Moreover, soda-lime-silica glasses have been utilized as radiation-sensitive dosimeters and are desirable glasses for the preparation of cheap integrated optical amplifiers [9]. However, some studies have exemplified the different types of glass systems for their potential use as shielding materials. [PERSON] et al. [10] estimated several attenuation parameters of barium borate-flyash glass samples at different photon energies using an experimental setup. The authors reported that these samples are better photon shields in comparison to some types of concretes. [PERSON] et al. [11] evaluated the effective atomic number and other relevant quantities for borate glasses with Bi\({}_{2}\)O\({}_{3}\), PbO, CaO, and SrO, using photon interaction cross-sections. They found that the glass samples with both PbO and Bi\({}_{2}\)O\({}_{3}\) were promising photon shielding mediums due to the high \(Z_{\text{eff}}\) of these HMOs, which leads to a high absorption of photons. They also concluded that Bi\({}_{2}\)O\({}_{3}\) is an excellent alternative to PbO for radiological protection. [PERSON] and [PERSON] [12] have investigated the shielding factors of waste soda-lime-silica glasses with several amounts of SrO using a computer program called Phy-X. They found that the glass with 15 wt% of SrO had the highest attenuation factors (both mass and linear) and the lowest half-value thickness. [PERSON] et al. [13] fabricated bismuth borate glass samples doped with Ni, Cu, and Co using a traditional melting technique and reported the radiation shielding characteristics using an experimental method at four energies (between 662 and 1333 keV). They found that the addition of 0.7% of Ni, Cu, and Co to the bismuth borate glasses enhanced the fabricated samples' shielding ability because these transition metal oxides can have several valance numbers. [PERSON] and [PERSON] [14] applied Geant4 simulation to determine the gamma attenuation features for borosilicate systems doped with TiO\({}_{2}\), Bi\({}_{2}\)O\({}_{3}\), and BaO. They studied the influence of each of these three heavy metal oxides on the half-value layer of the samples at 0.347 and 1.275 MeV.