摘要
采用高温固相反应,以NaF作助熔剂,在1000°C的温度下合成了锕系元素Pu的模拟固化体(Gd1–xCex)2Zr2O7+x(0≤x≤0.7).研究了模拟固化体的物相、热膨胀系数(TEC)、热导率(TC)随温度及组成的变化规律.粉末X射线衍射(XRD)测试结果表明:Gd2Zr2O7基质本身呈弱有序烧绿石结构,而用Ce4+取代Gd3+的模拟固化体都呈缺陷萤石结构.(Gd1–xCex)2Zr2O7+x的Ce(3d)X射线光电子能谱(XPS)有六个峰,结合能分别位于881.7,888.1,897.8,900.4,907.1,916.1 e V处,与Ce O2的XPS图谱非常相似,说明Ce为四价.随着温度的升高,所有样品的热膨胀系数总体上呈增大趋势.在室温至750°C附近,大部分样品的热导率随温度的升高而降低,之后热导率又呈小幅上升.在相同温度下,固化体(Gd1–xCex)2Zr2O7+x(0≤x≤0.7)的热膨胀系数及热导率随组成变化呈相同趋势:在0≤x≤0.1范围内随x的增大而增大,随后在x=0.1–0.7时逐渐减小.
Polycrystalline samples of(Gd1-x Cex)2Zr2O7+x(0 ≤ x ≤ 0.7) were synthesized by solid-state reaction using NaF as a flux at 1000 °C to simulate Pu-immobilization in the Gd2Zr2O7 matrix. Phase transformation and variation of the thermal expansion coefficients(TECs) and thermal conductivities(TCs)of the samples with temperature and composition were investigated. Powder X-ray diffraction(XRD)patterns show that pure Gd2Zr2O7 has a weakly ordered pyrochlore structure, whereas Ce-containing samples(i.e., the Pu-simulated solidified samples) exhibit a defect fluorite structure even if x is as low as0.1. When x reaches 0.7, the XRD peaks of these samples widen. In the Ce 3d X-ray photoelectron spectrum(XPS) of(Gd1-x Cex)2Zr2O7+x there are six peaks located at binding energies of 881.7, 888.1,897.8, 900.4, 907.1, and 916.1 e V, which are almost the same as the peaks of Ce O2. The Ce 3d XPS reveals that the Ce species in(Gd1-x Cex)2Zr2O7+x are tetravalent. The TECs of(Gd1-x Cex)2Zr2O7+x(0 ≤ x ≤0.7) generally increase with increasing temperature. At the same temperature, the TECs and TCs exhibit the same variation trend with the composition of the simulated solidified forms: they decrease from x = 0 to0.1 and then linearly increase from x = 0.1 to 0.7.
出处
《物理化学学报》
SCIE
CAS
CSCD
北大核心
2015年第9期1810-1814,共5页
Acta Physico-Chimica Sinica
基金
supported by NSAF(11176014)
National Natural Science Foundation of China(21471088)~~
关键词
核废料固化
烧绿石结构
萤石结构
热膨胀系数
热导率
Immobilization of nuclear waste
Pyrochlore structure
Defect fluorite structure
Thermal expansion coefficient
Thermal conductivity