|
|
|
|
LEADER |
01731 am a22002653u 4500 |
001 |
51049 |
042 |
|
|
|a dc
|
100 |
1 |
0 |
|a Shu, G. J.
|e author
|
100 |
1 |
0 |
|a Massachusetts Institute of Technology. Department of Physics
|e contributor
|
100 |
1 |
0 |
|a Lee, Patrick A.
|e contributor
|
100 |
1 |
0 |
|a Lee, Patrick A.
|e contributor
|
700 |
1 |
0 |
|a Huang, F.-T.
|e author
|
700 |
1 |
0 |
|a Chu, M.-W.
|e author
|
700 |
1 |
0 |
|a Lin, J.-Y
|e author
|
700 |
1 |
0 |
|a Lee, Patrick A.
|e author
|
700 |
1 |
0 |
|a Chou, F. C.
|e author
|
245 |
0 |
0 |
|a Staging model of the ordered stacking of vacancy layers and phase separation in layered NaxCoO2 (x≳0.71) single crystals
|
260 |
|
|
|b American Physical Society,
|c 2010-01-29T20:20:06Z.
|
856 |
|
|
|z Get fulltext
|u http://hdl.handle.net/1721.1/51049
|
520 |
|
|
|a Phase diagram of Na[subscript x]CoO[subscript 2](x≳0.71) has been reinvestigated using electrochemically fine-tuned single crystals. Both phase-separation and staging phenomena as a result of sodium multivacancy cluster ordering have been found. Phase-separation phenomenon is observed in the narrow ranges of 0.76≲x≲0.82 and 0.83≲x≲0.86. While x=0.820 shows A-type antiferromagnetic (A-AF) ordering below 22 K, x=0.833 is confirmed to have a magnetic ground state of A-AF ordering below ∼8 K and is only reachable through slow cooling. In addition, x=0.859 is found to be responsible for the highest A-AF transition temperature at about 29 K. Staging model based on ordered stacking of multivacancy layers is proposed to explain the hysteretic behavior and A-AF correlation length for x ∼0.82-0.86.
|
520 |
|
|
|a Department of Energy
|
520 |
|
|
|a National Science Council of Taiwan
|
546 |
|
|
|a en_US
|
655 |
7 |
|
|a Article
|
773 |
|
|
|t Physical Review B
|