同步辐射消除癌细胞的潜力:hartree- fok方法分析质子化菱锰矿晶体

R. Gobato, Marcia Regina Risso Gobato, A. Heidari, A. Mitra
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引用次数: 11

摘要

红锰矿(MnCO3)与菱铁矿(FeCO3)呈完全固溶体,其中可能含有大量的Zn、Mg、Co、Ca。利用红锰矿晶体组织吸收和同步辐射消除肿瘤组织,消除这些受影响的组织,治疗肿瘤组织尚无文献先例。这些被发现的研究是这个团队的研究论文。通过不受限制的hartrei - fock (UHF)计算模拟,利用原子极性张量(APT)和Mulliken两种常用的方法研究了质子化红铬石晶体CH19Mn6O8的紧凑有效势(CEP)、红外光谱以及单位分子的负载分布。结构为CMn6O8的菱铁矿晶体单元胞,在UHF CEP-4G(有效核心电位(ECP)最小基)、UHF CEP-31G (ECP分裂价)和UHF CEP-121G (ECP三分裂基)下验证了分子的负载分布。在CEP-121G基组中,APT和Mulliken方法的负荷变化最大,δ = 2.922 e δ = 2.650 u. a, δAPT > δMulliken。CEP-4G、CEP-31G和CEP-121G基组的最大吸光度峰出现在2172.23 cm-1频率处,归一化强度为0.65;2231.4 cm-1和0.454;和2177.24 cm-1和1.0。采用小角x射线散射(SAXS)、超小角x射线散射(USAXS)、涨落x射线散射(FXS)、广角x射线散射(WAXS)、掠射小角x射线散射(GISAXS)、掠射广角x射线散射(GIWAXS)、小角中子散射(SANS)、掠入射小角中子散射(GISANS)、x射线衍射(XRD)、粉末x射线衍射(PXRD)、广角x射线衍射(WAXD)、掠入射x射线衍射(GIXD)和能量色散x射线衍射(EDXRD)。后来的研究可以通过同步辐射检查红锰矿在治疗癌症方面的优缺点,例如一个振荡器晶体。研究rhodocrossite的作用位点可以更好地了解其在健康和/或肿瘤组织中的吸收情况,从而更好地将同步辐射应用于肿瘤以消除它们。
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Potential in the elimination of cancer cells through synchrotron radiation: A hartree-fock methods analysis protonated rhodochrosite crystal
The rhodochrosite (MnCO3) shows complete solid solution with siderite (FeCO3), and it may contain substantial amounts of Zn, Mg, Co, and Ca. There is no precedent in the literature on the treatment of tumor tissues by eliminating these affected tissues, using rhodocrosite crystals in tissue absorption and eliminating cancerous tissues by synchrotron radiation. The studies that are found are the research papers of this team. Through an unrestricted Hartree-Fock (UHF) computational simulation, Compact effective potentials (CEP), the infrared spectrum of the protonated rhodochrosite crystal, CH19Mn6O8, and the load distribution by the unit molecule by two widely used methods, Atomic Polar Tensor (APT) and Mulliken, were studied. The rhodochrosite crystal unit cell of structure CMn6O8, where the load distribution by the molecule was verified in the UHF CEP-4G (Effective core potential (ECP) minimal basis), UHF CEP-31G (ECP split valance) and UHF CEP-121G (ECP triple-split basis). The largest load variation in the APT and Mulliken methods were obtained in the CEP-121G basis set, with δ = 2.922 e δ = 2.650 u. a., respectively, being δAPT > δMulliken. The maximum absorbance peaks in the CEP-4G, CEP-31G and CEP-121G basis set are present at the frequencies 2172.23 cm-1, with a normalized intensity of 0.65; 2231.4 cm-1 and 0.454; and 2177.24 cm-1 and 1.0, respectively. An in-depth study is necessary to verify the absorption by the tumoral and non-tumoral tissues of rhodochrosite, before and after irradiating of synchrotron radiation using Small–Angle X–Ray Scattering (SAXS), Ultra–Small Angle X–Ray Scattering (USAXS), Fluctuation X–Ray Scattering (FXS), Wide–Angle X–Ray Scattering (WAXS), Grazing–Incidence Small–Angle X–Ray Scattering (GISAXS), Grazing–Incidence Wide–Angle X–Ray Scattering (GIWAXS), Small–Angle Neutron Scattering (SANS), Grazing–Incidence Small–Angle Neutron Scattering (GISANS), X–Ray Diffraction (XRD), Powder X–Ray Diffraction (PXRD), Wide–Angle X–Ray Diffraction (WAXD), Grazing– Incidence X–Ray Diffraction (GIXD) and Energy–Dispersive X–Ray Diffraction (EDXRD). Later studies could check the advantages and disadvantages of rhodochrosite in the treatment of cancer through synchrotron radiation, such as one oscillator crystal. Studying the sites of rhodocrosite action may lead to a better understanding of its absorption by healthy and/or tumor tissues, thus leading to a better application of synchrotron radiation to the tumors to eliminate them.
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