| ²é¿´: 3150 | »Ø¸´: 2 | |||
| µ±Ç°Ö»ÏÔʾÂú×ãÖ¸¶¨Ìõ¼þµÄ»ØÌû£¬µã»÷ÕâÀï²é¿´±¾»°ÌâµÄËùÓлØÌû | |||
Azure001½ð³æ (³õÈëÎÄ̳)
|
[ÇóÖú]
ÇóÖúÌû¡£µ½µ×ʲôÊÇGÐÍ·´Ìú´Å ÒÑÓÐ1È˲ÎÓë
|
||
| ÎÄÏ×ÉÏÒ»Ö±½²ÌúËáîéÊÇGÐÍ·´Ìú´Å£¬Í¬Ê±¾ßÓÐÒ»¸ö62nmµÄÂÝÐý×ÔÐýµ÷ÖÆ½á¹¹¡£ÏëÇóÖúһϸ÷λ¿ÆÑÐǰ±²·´Ìú´Åµ½µ×ÊÇÔõô·ÖÀàΪA¡¢B¡¢C¡¢GÐ͵ġ£·Á˺ܶà´ÅѧµÄÊ黹ÊÇûÕÒµ½£¬ºÜÊÇ¿àÄÕ¡£Çóǰ±²ÃÇÖ¸ÌõÃ÷·£¬½²½²Ò²ºÃ£¬¹²Ïíµã×ÊÁÏÒ²ºÃ£¬°Ýл |
» ÊÕ¼±¾ÌûµÄÌÔÌûר¼ÍƼö
¸ÆîÑ¿óÏà¹ØÀíÂÛ |
» ²ÂÄãϲ»¶
»¯¹¤Ñ§Ë¶294·Ö£¬Çóµ¼Ê¦ÊÕÁô
ÒѾÓÐ29È˻ظ´
Çóµ÷¼Á
ÒѾÓÐ10È˻ظ´
¿¼ÑÐÇóµ÷¼Á
ÒѾÓÐ13È˻ظ´
Çóµ÷¼Á
ÒѾÓÐ3È˻ظ´
È˹¤ÖÇÄÜ320µ÷¼Á08¹¤À໹Óлú»áÂð
ÒѾÓÐ17È˻ظ´
¿¼ÑÐÓ¢Ò»ÊýÒ»338·Ö
ÒѾÓÐ10È˻ظ´
ÇóÖúµ÷¼Á£¬¿çµ÷
ÒѾÓÐ15È˻ظ´
085600²ÄÁÏÓ뻯¹¤329·ÖÇóµ÷¼Á
ÒѾÓÐ20È˻ظ´
085600²ÄÁÏÓ뻯¹¤349·ÖÇóµ÷¼Á
ÒѾÓÐ15È˻ظ´
Çóµ÷¼Á
ÒѾÓÐ13È˻ظ´
³È×Ó150
гæ (³õÈëÎÄ̳)
- Ó¦Öú: 0 (Ó×¶ùÔ°)
- ½ð±Ò: 52.4
- Ìû×Ó: 11
- ÔÚÏß: 12.4Сʱ
- ³æºÅ: 6353110
- ×¢²á: 2017-04-19
- רҵ: Äý¾Û̬ÎïÐÔ II £ºµç×ӽṹ
¡¾´ð°¸¡¿Ó¦Öú»ØÌû
|
a collinear bipartite antiferromagnet composed of two interpenetrating square lattices A and B possessing antiferromagnetically aligned moments [see Fig. 1(a), the extension to three dimensions is straightforward]. This configuration is usually referred to as a G-type or checkerboard antiferromagnet, i.e.,when both intraplane and interplane couplings are antiferromagnetic (other collinear bipartite spin structures exist, such as the A-type structure when intraplane coupling is ferromagnetic and inter lane coupling is antiferromagnetic, or the C-type structure when intraplane coupling is antiferromagnetic and interplane coupling is ferromagnetic.) ÎÄÏ×ÉÏ¿´µ½µÄ£¬·ÒëһϾÍÊÇ£ºGÐÍÊÇÃæÄÚºÍÆ½Ãæ¼äñîºÏ¶¼ÊÇ·´Ìú´ÅÐÔ£»AÐÍÊÇÃæÄÚñîºÏÊÇÌú´ÅÐÔ£¬Æ½Ãæ¼äñîºÏÊÇ·´Ìú´Å£»CÐÍÊÇÃæÄÚñîºÏÊÇ·´Ìú´ÅÐÔ£¬Æ½Ãæ¼äñîºÏÊÇÌú´ÅÐÔ¡£ |
3Â¥2019-07-24 21:19:15
wd12309812
ͳæ (ÕýʽдÊÖ)
- Ó¦Öú: 3 (Ó×¶ùÔ°)
- ½ð±Ò: 66.2
- É¢½ð: 80
- ºì»¨: 3
- Ìû×Ó: 386
- ÔÚÏß: 173.7Сʱ
- ³æºÅ: 3028207
- ×¢²á: 2014-03-08
- ÐÔ±ð: GG
- רҵ: Äý¾Û̬ÎïÐÔ II £ºµç×ӽṹ
2Â¥2017-12-08 16:08:17














»Ø¸´´ËÂ¥