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Neutron transmutation of 10{sup left}B doped diamond

机译:10 {sup left} B掺杂钻石的中子trans变

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Free standing 10{sup left}B isotope doped diamond films deposited by chemical vapor deposition in a microwave chamber were irradiated to thermal neutron fluence values of 0.32 × 10{sup}19, 0.65 × 10{sup}19, 1.3 × 10{sup}19, and 2.6 × 10{sup}19 n/cm{sup}2. Cooling of the diamond films was maintained during irradiation. In a separate experiment, neutron irradiation to a total fluence of 2.4 × 10{sup}20 n/cm{sup}2 with equal fast and thermal neutrons was also performed on a diamond epilayer without cooling during irradiation. The formation of defects in the diamond films was characterized using Raman, FTIR, photoluminescence, electron paramagnetic resonance spectroscopy, and X-ray diffraction. It was found that defect configurations in diamond responsible for an increase in continuum background in the one-phonon region of Raman spectrum were absent in the films that have been cooled. The FTIR peak at 1530 cm{sup}(-1) annealed in the sample irradiated to a fluence of 2.6 × 10{sup}19 n/cm{sup}2 indicating that the sample reached a temperature of 300℃ during irradiation. Absence of characteristic infrared absorption peaks that were observed only upon annealing neutron irradiated diamond is used to conclude that the temperature of the sample during neutron irradiation to a fluence of 2.6 × 10{sup}19 n/cm{sup}2 was well below 650℃ needed for mobility of defects and accumulation of stable unrecoverable damage. On the other hand, results from diamond epilayer subjected to equal thermal and fast neutron fluence of 2.4 × 10{sup}20 n/cm{sup}2 and without cooling showed that defects formed from displaced carbon atoms became mobile and formed complex configurations of irrecoverable damage. Electrical conductance of the unirradiated and irradiated diamond samples was measured as a function of temperature to determine the compensation of the p-type by the n-type charge carriers.
机译:在微波室中通过化学气相沉积法沉积的自立式10 {supleft} B掺杂同位素的金刚石薄膜被辐照到0.32×10 {sup} 19、0.65×10 {sup} 19、1.3×10 {sup的热中子注量值} 19和2.6×10 {sup} 19 n / cm {sup} 2。辐照期间保持金刚石膜的冷却。在一个单独的实验中,在金刚石外延层上也进行了中子辐照,辐照度为2.4×10 {sup} 20 n / cm {sup} 2,具有相同的快中子和热中子,辐照期间没有冷却。使用拉曼光谱,FTIR,光致发光,电子顺磁共振波谱和X射线衍射对金刚石膜中缺陷的形成进行了表征。已经发现,在冷却的膜中不存在导致拉曼光谱的单声子区域中的连续谱背景增加的金刚石中的缺陷构型。样品在1530 cm {sup}(-1)处进行了FTIR峰退火,辐照量为2.6×10 {sup} 19 n / cm {sup} 2,表明样品在辐照过程中达到了300℃的温度。仅在对中子辐照金刚石进行退火后才能观察到特征红外吸收峰的缺乏,可以得出结论:在中子辐照至2.6×10 {sup} 19 n / cm {sup} 2的通量时,样品的温度远低于650 ℃所需的缺陷迁移率和积累的稳定不可恢复的损伤。另一方面,金刚石外延层在2.4×10 {sup} 20 n / cm {sup} 2的条件下受到相等的热中子通量和快速中子通量并且没有冷却的结果表明,由置换的碳原子形成的缺陷变得可移动并形成了复杂的结构。不可挽回的损害。测量未辐照和辐照金刚石样品的电导随温度的变化,以确定n型电荷载流子对p型的补偿。

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