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山本 卓; 小野田 忍; 大島 武; 磯谷 順一*; 寺地 徳之*; 谷口 尚*; 渡邊 賢司*; 小泉 聡*; 梅田 享英*; Jelezko, F.*; et al.
no journal, ,
Nイオン照射で生成した高純度C濃縮ダイヤモンド中のNV中心について、単一スピンの光学的検出磁気共鳴を測定した。詳細な光学的検出磁気共鳴測定から、Nイオン照射によってNVとNVが[NV]/[NV] 1の比で生成され、収率(イオン照射量に対する生成したNV中心の割合)は70-100%であることがわかった。スピンコヒーレンス時間は室温で2msと長く、これまで報告されているイオン照射試料の中で最も長いことがわかった。これらの結果は、イオン照射で生成したNVスピンを用いた応用が十分期待できると結論できた。
小川 修一*; 山田 貴壽*; 石塚 眞治*; 吉越 章隆; 長谷川 雅考*; 寺岡 有殿; 高桑 雄二*
no journal, ,
The behavior of C atoms in vacuum annealing/cooling processes for a graphene/Cu(111) has been investigated using synchrotron radiation photoelectron spectroscopy (SR-XPS). The sample structure is graphene/Cu(111)/AlO(0001), in which graphene was grown by a thermal CVD method at 1273 K. The C 1s, O 1s, and Cu 3s SR-XPS spectra were measured in situ during annealing/cooling in vacuum. The graphene coverage at a low temperature region below 873 K is almost 1 monolayer (ML), but it decreased with increasing temperature. At 1223 K, the coverage reached 0.4 ML. This indicates the graphene decomposed and C atoms diffused into the Cu substrate. It was also found from SIMS measurement that the amount of diffused C atoms in the thermal CVD process is smaller than that after vacuum annealing. These results suggest that the C atom diffusion into the Cu occurs frequently, but the diffused C atoms do not contribute to the graphene growth on the Cu surface.