Femtosecond-laser-induced modifications on the surface of a single-crystalline diamond

2017 ◽  
Vol 56 (11) ◽  
pp. 112701
Author(s):  
Tatsuya Okada ◽  
Takuro Tomita ◽  
Tomoyuki Ueki ◽  
Yuki Masai ◽  
Yota Bando ◽  
...  
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pp. 662-672 ◽  
Author(s):  
Graham C.B. Lee ◽  
Shi Su ◽  
Jiangling Li ◽  
Kate Sugden ◽  
Nima Roohpour ◽  
...  

2006 ◽  
Vol 34 (11) ◽  
pp. 773-778 ◽  
Author(s):  
Yusaku IZAWA ◽  
Shigeki TOKITA ◽  
Masaki HASHIDA ◽  
Masayuki FUJITA ◽  
Yasukazu IZAWA

Nanomaterials ◽  
2018 ◽  
Vol 8 (8) ◽  
pp. 631 ◽  
Author(s):  
Dongshi Zhang ◽  
Wonsuk Choi ◽  
Yugo Oshima ◽  
Ulf Wiedwald ◽  
Sung-Hak Cho ◽  
...  

There are few reports on zero-field-cooled (ZFC) magnetization measurements for Fe@FeOx or FeOx particles synthesized by laser ablation in liquids (LAL) of Fe, and the minimum blocking temperature (TB) of 120 K reported so far is still much higher than those of their counterparts synthesized by chemical methods. In this work, the minimum blocking temperature was lowered to 52 K for 4–5 nm α-Fe2O3 particles synthesized by femtosecond laser ablation of Fe in acetone. The effective magnetic anisotropy energy density (Keff) is calculated to be 2.7–5.4 × 105 J/m3, further extending the Keff values for smaller hematite particles synthesized by different methods. Large amorphous-Fe@α-Fe2O3 and amorphous-Fe@C particles of 10–100 nm in diameter display a soft magnetic behavior with saturation magnetization (Ms) and coercivities (Hc) values of 72.5 emu/g and 160 Oe at 5 K and 61.9 emu/g and 70 Oe at 300 K, respectively, which mainly stem from the magnetism of amorphous Fe cores. Generally, the nanoparticles obtained by LAL are either amorphous or polycrystalline, seldom in a single-crystalline state. This work also demonstrates the possibility of synthesizing single-crystalline α-Fe2O3 hematite crystals of several nanometers with (104), (113), (116) or (214) crystallographic orientations, which were produced simultaneously with other products including carbon encapsulated amorphous Fe (a-Fe@C) and Fe@FeOx core-shell particles by LAL in one step. Finally, the formation mechanisms for these nanomaterials are proposed and the key factors in series events of LAL are discussed.


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