2007
DOI: 10.1016/j.susc.2007.07.025
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Dopant control over the crystal morphology of ceramic materials

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Cited by 26 publications
(27 citation statements)
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“…For the Ni only doped (no Er) sample, broad emission band ranging from 1300 nm to 1600 nm originated from the 3 T 2 ( 3 F) / 3 A 2 ( 3 F) transition of Ni 2+ was observed. [26][27][28][29][30][31][32][33] However, by introducing Er 3+ (Li + ) co-dopants, the Ni 2+ emission almost disappeared and Er 3+ emissions at around 1550 nm ( 4 I 13/2 / 4 I 15/2 ) and 980 nm ( 4 I 11/2 / 4 I 15/2 ) appeared (see Fig. S5 † for 1180 nm excited UC at 980 nm).…”
Section: Resultsmentioning
confidence: 99%
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“…For the Ni only doped (no Er) sample, broad emission band ranging from 1300 nm to 1600 nm originated from the 3 T 2 ( 3 F) / 3 A 2 ( 3 F) transition of Ni 2+ was observed. [26][27][28][29][30][31][32][33] However, by introducing Er 3+ (Li + ) co-dopants, the Ni 2+ emission almost disappeared and Er 3+ emissions at around 1550 nm ( 4 I 13/2 / 4 I 15/2 ) and 980 nm ( 4 I 11/2 / 4 I 15/2 ) appeared (see Fig. S5 † for 1180 nm excited UC at 980 nm).…”
Section: Resultsmentioning
confidence: 99%
“…[24][25][26][27][28][29][30][31] It has been demonstrated that six coordinated Ni 2+ ions located at the centers of octahedrons have substantial absorption around 1100-1400 nm that can further be tuned in a wide range by manipulating the crystal eld strength around the Ni 2+ ions. 26,30,32 Accordingly, its NIR emission band is also wide ranging from 1200 nm to longer than 1700 nm with extremely high quantum yield reaching unity in some crystals such as LiGa 5 O 8 .…”
Section: Materials Designmentioning
confidence: 99%
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“…The surface energies of the doped surfaces were calculated from the surface energies of the undoped surfaces and the surface segregation energy of the dopant as follows (per Ref. [33]):…”
Section: Methodsmentioning
confidence: 99%
“…This process between particles tends to form threedimensional architectures, resulting in energy loss. Thus, the process reduces accumulated energies associated with incomplete surfaces at random distances and, by converging, eliminates the mineral-air or mineral-fluid interfaces [32]. The interaction between components of self-organized systems are controlled by hydrogen bonds, Van der Waals forces, and electrostatic or hydrophobic interactions.…”
Section: Fe-sem Analysismentioning
confidence: 99%