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MPCVD growth of C-13-enriched diamond single crystals with nitrogen addition

机译:添加氮的MPCVD生长富含C-13的金刚石单晶

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This study describes the growth of C-13-enriched (100)-oriented diamond single crystals by the MPCVD (microwave plasma chemical vapour deposition) process. All crystals are at least 6 x 6 mm(2) in area and 0.5-1.0 mm in thickness. The samples with nominal C-13 percentages (R = [C-13] [C-13 + C-12]) of 0.011 (natural abundance), 0.10, 0.21, 0.24 and 034 were obtained by controlling the flow of the carbon-13 and carbon-12 methane feed gases. To obtain thicker and near -colourless quality C-13-enriched diamond, 190 ppm of nitrogen was added into the gas mixture. The shift towards lower frequency in the Raman peak positions and decrease in the thermal conductivities of the near -colourless crystals with increasing C-13 percentages are similar to previous studies of isotopically-controlled diamond grown with no nitrogen additive. The images of the structural defects associated with C-13-enrichment obtained by spatially-resolved X-ray rocking curve measurement show distinct patterned structures that runs parallel to the < 100 > direction. Moreover, the broadening in the line width of the nuclear magnetic resonance (NMR) peak from sp(3) C-13 correlates with increasing R. We also expand the study by injecting 500 ppm of nitrogen. Higher nitrogen concentration leads to the formation of brown crystals. The brown crystals show far greater C-13 NMR peak intensity than the near-colourless. This suggests that paramagnetic nitrogen impurities in the brown crystals hasten the spin-lattice relaxation time of the C-13 nuclear spin that resulted in higher intensity. The isotopic splitting observed for the localized vibrational mode of the NVH0 defect in brown crystals is attributed to the co-existence of both the C-13 (3114.2 cm(-1)) and C-12 (3123.5 cm(-1)). Unlike the isotopic splitting observed for NVH0 defect, the peak position of the NS defect shifts towards lower frequency as R increases. Not only have we demonstrate the growth of bigger isotopically-controlled diamond single crystals, the results shown here have provided a framework to further investigate the interplay between C-13 atoms and nitrogen impurity. (C) 2015 Elsevier B.V. All rights reserved.
机译:这项研究描述了通过MPCVD(微波等离子体化学气相沉积)工艺生长的富含C-13(100)的金刚石单晶。所有晶体的面积至少为6 x 6 mm(2),厚度至少为0.5-1.0 mm。通过控制碳流量,可以得到标称C-13百分比(R = [C-13] [C-13 + C-12])为0.011(自然丰度),0.10、0.21、0.24和034的样品。 13和碳12甲烷进料气。为了获得更厚且几乎无色的富含C-13的钻石,将190 ppm的氮气添加到混合气体中。随着C-13百分比的增加,拉曼峰位置朝着较低的频率移动,以及近无色晶体的热导率降低,这与以前没有氮添加剂的同位素控制金刚石的研究相似。通过空间分辨X射线摇摆曲线测量获得的与C-13富集相关的结构缺陷的图像显示出与<100>方向平行的独特图案结构。此外,sp(3)C-13的核磁共振(NMR)峰的线宽变宽与R的增加相关。我们还通过注入500 ppm的氮扩大了研究范围。较高的氮浓度导致形成棕色晶体。棕色晶体比几乎无色的C-13 NMR峰强度高得多。这表明棕色晶体中的顺磁性氮杂质会加速C-13核自旋的自旋晶格弛豫时间,从而导致强度更高。观察到的棕色晶体中NVH0缺陷的局部振动模式的同位素分裂归因于C-13(3114.2 cm(-1))和C-12(3123.5 cm(-1))的共存。与NVH0缺陷观察到的同位素分裂不同,NS缺陷的峰值位置随着R的增加而向较低的频率移动。我们不仅证明了较大的同位素控制的金刚石单晶的生长,而且此处显示的结果为进一步研究C-13原子与氮杂质之间的相互作用提供了框架。 (C)2015 Elsevier B.V.保留所有权利。

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