| ²é¿´: 963 | »Ø¸´: 5 | |||
| µ±Ç°Ö÷ÌâÒѾ´æµµ¡£ | |||
| µ±Ç°Ö»ÏÔʾÂú×ãÖ¸¶¨Ìõ¼þµÄ»ØÌû£¬µã»÷ÕâÀï²é¿´±¾»°ÌâµÄËùÓлØÌû | |||
ÕÅÊéö©Òø³æ (СÓÐÃûÆø)
|
[½»Á÷]
¡¾ÇóÖú¡¿¹ØÓÚpseudogapµÄÎÊÌâ
|
||
|
ÎÒÊÇ»¯Ñ§³öÉíµÄ,ÏëÇë½ÌÎïÀí·½ÃæµÄ¸ßÊÖ,pseudogapÊÇʲôÒâ˼Ŷ?×îºÃÄÜÓñȽÏͨË×µÄÓïÑÔ½âÊÍÒ»ÏÂ,ÎÒ¸üÈÝÒ×Àí½â,ºÇºÇ [ Last edited by ddx-k on 2008-12-14 at 20:00 ] |
» ²ÂÄãϲ»¶
Ã÷ÌìÓ¦¸Ã¿É²éÁË£¡£¿
ÒѾÓÐ5È˻ظ´
Èç¹û´Ë¿ÌÄãÕýÔÚΪ¹ú»ù¸Ðµ½½¹ÂÇ£¬²»·ÁÀ´ÌýÌýÕâÊס¶»ù½ðÖ®Íâ¡·
ÒѾÓÐ7È˻ظ´
ûÓÐÈκÎÏûÏ¢-ÊDz»ÊǾÍÁ¹ÁË
ÒѾÓÐ8È˻ظ´
ÊÛSCI-T0PÎÄÕ£¬ÎÒ:8O.5.5.1.O.54,¿ÆÄ¿ÆëÈ«,¿É+¼±
ÒѾÓÐ3È˻ظ´
ÊÛSCIÒ»ÇøÎÄÕ£¬ÎÒ:8.O.551.O.5.4,¿ÆÄ¿È«,¿ÉÙ¤¼±
ÒѾÓÐ5È˻ظ´
ÈËÆø²»ÐÐÁË
ÒѾÓÐ10È˻ظ´
ÎÒÃæÉÏÍêµ°ÁË
ÒѾÓÐ10È˻ظ´
ÄÜ·ñÍ˳ö²ÎÓëµÄÃæÉÏÏîÄ¿½â³ýÏÞÏî
ÒѾÓÐ24È˻ظ´
filecode£¬4¸öjtjcÁË
ÒѾÓÐ17È˻ظ´
2026¹ú×ÔÈ»º¯ÆÀ·Ñµ½ÕË
ÒѾÓÐ19È˻ظ´
fleeting
ͳæ (³õÈëÎÄ̳)
- Ó¦Öú: 0 (Ó×¶ùÔ°)
- ½ð±Ò: 138
- Ìû×Ó: 17
- ÔÚÏß: 44·ÖÖÓ
- ³æºÅ: 532442
- ×¢²á: 2008-03-25
- רҵ: Äý¾Û̬ÎïÀí
|
Â¥ÉÏ˵µÄºÜºÃ£¬²»¹ý¹ØÓÚØÍÄÜ϶µÄ»úÀíĿǰ»¹Ã»ÓÐÒ»¸öͳһµÄÈÏʶ£¬Ô¤Åä¶ÔÖ»ÊÇ´ó¼ÒÆÕ±é½ÓÊܵÄÒ»¸öÖ÷Á÷¹Ûµã£¬Õâ¸ö»¹ÓÐÕùÒ飬¿ÉÒÔ¿´Ò»ÏÂÕâÆª×ÛÊöÎÄÕ Physics Reports 431 (2006) 231 ¨C 259 ÖÁÓÚelectronic stripesµÄÎÊÌ⣬ÆäʵÔںܶàÇ¿¹ØÁªÌåϵÀïÃæ¶¼·¢ÏÖÁËÀàËÆµÄelectronic phase separationÎÊÌ⣬Õâ¸öÊǵçºÉ£¨×ÔÐý£©ÔÚʵ¿Õ¼äµÄÖÜÆÚÐÔÅÅÁУ¬¹«¶Èµ÷ÖÆµÄÇé¿öÏ£¬½á¹¹±È½ÏÎȶ¨¡£Õâ¸ö¿ÉÒÔÓÃÑÜÉä¼¼Êõ²âÁ¿µ½µÄ£¬ÓÐÈËÈÏΪÌõÎÆÏà½á¹¹ÊǸß㬵¼µÄ»ù̬֮һ£¬ÁíÒ»¸ö±È½ÏÎȶ¨µÄÏàÊÇ×î¼Ñ²ôÔӵij¬µ¼×é·Ö¡£µ«ÊǶÔÓÚ¶¯Ì¬µÄÌõÎÆÏàĿǰÈÏʶµÄ»¹²»¹»Çå³þ£¬Èç¹û¸ÐÐËȤµÄ»°¿ÉÒԲο¼ÕâÆªÎÄÏ× REVIEWS OF MODERN PHYSICS, VOLUME 75 £¨2003£© 1201 |
6Â¥2008-03-29 11:41:04
gaoky2008
ľ³æ (ÖøÃûдÊÖ)
- Ó¦Öú: 0 (Ó×¶ùÔ°)
- ½ð±Ò: 6742.6
- Ìû×Ó: 1564
- ÔÚÏß: 139.7Сʱ
- ³æºÅ: 472596
- ×¢²á: 2007-12-04
- ÐÔ±ð: GG
- רҵ: ¸ß·Ö×Ӻϳɻ¯Ñ§
¡ï ¡ï
zt970831(½ð±Ò+2,VIP+0):лл£º£©
zt970831(½ð±Ò+2,VIP+0):лл£º£©
|
Pseudogap From Wikipedia, the free encyclopedia A pseudogap is a term from the field of high-temperature superconductivity which describes an energy (normally near the Fermi energy) which has very few states associated with it. This is very similar to a 'gap', which is an energy that has no allowed states. Such gaps open up, for example, when electrons interact with the lattice. Interestingly only certain electrons `see' this gap. The gap, which should be associated with an insulating state, only exists for electrons travelling parallel to the copper-oxygen bonds. Electrons travelling at 45 degrees to this bond can move freely throughout the crystal. The Fermi surface therefore consists of Fermi Arcs forming pockets centred on the corner of the Brillouin zone. In the pseudogap phase these arcs gradually disappear as the temperature is lowered until only four points on the diagonals of the Brillouin zone remain ungapped. On one hand, this could indicate a completely new electronic phase which consumes available states, leaving only a few to pair up and superconduct. On the other hand, the similarity between this partial gap and that in the superconducting state could indicate that the pseudogap results from preformed cooper pairs. Mechanism The origin of the pseudogap is controversial and still subject to debate in the condensed matter community. Two main interpretations are emerging: 1. The scenario of preformed pairs In this scenario, electrons form pairs at a temperature T* that can be much larger than the critical temperature Tc where superconductivity appears. T* of the order of 300K have been measured in underdoped cuprates where Tc is about 80k. The superconductivity does not appear at T* because large phase fluctuations of the pairing field cannot order at this temperature. The pseudogap is then produced by non coherent fluctuations of the pairing field. 2. The scenario of a non superconducting related pseudogap In this class of scenarios, many different origins have been put forward: like the formation of electronic stripes, antiferromagnetic ordering, exotic order parameter competing with superconductivity. A pseudogap can be seen with several different experimental methods. One of the first observations was in specific heat measurements of YBa2Cu3O6+x by Loram et al.[1] The pseudogap is also apparent in ARPES (Angle Resolved Photoemission Spectroscopy) data, which can measure the density of states of the electrons in a material. References ^J. W. Loram, K. A. Mirza, J. R. Cooper, and W. Y. Liang (1993). "Electronic specific heat of YBa2Cu3O6+x'' from 1.8 to 300 K".Physical Review Letters71 (11): 1740-1743. doi:10.1103/PhysRevLett.71.1740. Emery et al. Physical Review B, Vol 56, Page 6120 (1997) Kyle McElroy, Nature Physics, Vol 2, Page 441 (2006) External links pseudogap in non-superconducting materials:http://www.physorg.com/news10505.html |

2Â¥2008-03-26 16:59:01
ÕÅÊéö©
Òø³æ (СÓÐÃûÆø)
- Ó¦Öú: 0 (Ó×¶ùÔ°)
- ½ð±Ò: 1685.4
- Ìû×Ó: 64
- ÔÚÏß: 102.2Сʱ
- ³æºÅ: 511209
- ×¢²á: 2008-02-25
- ÐÔ±ð: MM
- רҵ: ÆäËûÎÞ»ú·Ç½ðÊô²ÄÁÏ
3Â¥2008-03-26 20:32:12
supersolid226
Ìú¸Ëľ³æ (ÕýʽдÊÖ)
- Ó¦Öú: 4 (Ó×¶ùÔ°)
- ½ð±Ò: 7409.4
- ºì»¨: 1
- Ìû×Ó: 815
- ÔÚÏß: 183.6Сʱ
- ³æºÅ: 479871
- ×¢²á: 2007-12-15
- ÐÔ±ð: GG
- רҵ: Äý¾Û̬ÎïÐÔ II £ºµç×ӽṹ
¡ï
zt970831(½ð±Ò+1,VIP+0):ллÄúµÄ½»Á÷£º£©
zt970831(½ð±Ò+1,VIP+0):ллÄúµÄ½»Á÷£º£©
|
Èç¹ûÄãÓк«Èêɺ¡¶¸ß㬵¼ÎïÀí¡·£¬ÀïÃæÓкÜÏêϸµÄpsudogapµÄͼÏó£¬Äã¿ÉÒԲο¼ [ Last edited by supersolid226 on 2008-3-27 at 16:56 ] |
4Â¥2008-03-27 16:54:33









»Ø¸´´ËÂ¥
20