| ²é¿´: 1539 | »Ø¸´: 2 | ||
| µ±Ç°Ö»ÏÔʾÂú×ãÖ¸¶¨Ìõ¼þµÄ»ØÌû£¬µã»÷ÕâÀï²é¿´±¾»°ÌâµÄËùÓлØÌû | ||
hui0087ľ³æ (ÕýʽдÊÖ)
|
[ÇóÖú]
³¬µ¼½üÁÚЧӦ
|
|
|
×î½üÔÚÑо¿³¬µ¼½üÁÚЧӦ£¬Óм¸¸öÎÊÌâÓÐЩÀ§»ó£¬»¹Çë¸÷λ³æÓÑÄܹ»¸øÓèÖ¸µ¼°ïÖú£¬²»Éõ¸Ð¼¤£¡ ÔõÑù²ÅÄÜ´ÓdI/dV-VÇúÏßÉÏÖ¤Ã÷´æÔÚÓÉÓÚ½üÁÚЧӦÔÚ½çÃæÓÕµ¼³öµÄÒ»¸öеij¬µ¼Ì¬£¬ÊDz»ÊDzâÊԵõ½ZBCP¾Í¿ÉÒÔ£¿ËùνµÄAndreev reflection£¬pair currentºÍAndreev Bound StatesÓÖ·Ö±ðÖ¸µÄÊÇʲô£¬ÔÚdI/dV-VÇúÏßÉÏÓÐÊ²Ã´Çø±ð£¿ ¿´µ½Nature Communication 3 (2012) 1056 ÖÐÓÐÒ»¶Î»° ¡°Specifically, our differential conductance measurements reveal a very wide central Andreev feature, which is almost independent of the bias. This is consistent with Andreev reflection in the normal material from an induced gap and is completely different from an Andreev-bound state.¡± лл£¡ |
» ²ÂÄãϲ»¶
ѧ˶274Çóµ÷¼Á
ÒѾÓÐ11È˻ظ´
Ò»Ö¾Ô¸Ö£´ó²ÄÁϹ¤³Ì290Çóµ÷¼Á
ÒѾÓÐ12È˻ظ´
»·¾³¹¤³Ì 085701£¬267Çóµ÷¼Á
ÒѾÓÐ8È˻ظ´
083000ѧ˶274Çóµ÷¼Á
ÒѾÓÐ10È˻ظ´
Ò»Ö¾Ô¸085600ÖпÆÔºÄþ²¨Ëù276·ÖÇóµ÷¼Á
ÒѾÓÐ4È˻ظ´
²ÄÁÏרҵÉ격
ÒѾÓÐ3È˻ظ´
307Çóµ÷¼Á
ÒѾÓÐ20È˻ظ´
285Çóµ÷¼Á
ÒѾÓÐ8È˻ظ´
²ÄÁÏÓ뻯¹¤£¨0856£©304ÇóBÇøµ÷¼Á
ÒѾÓÐ8È˻ظ´
370Çóµ÷¼Á
ÒѾÓÐ3È˻ظ´
hui0087
ľ³æ (ÕýʽдÊÖ)
- Ó¦Öú: 0 (Ó×¶ùÔ°)
- ½ð±Ò: 4012.6
- É¢½ð: 84
- ºì»¨: 2
- Ìû×Ó: 671
- ÔÚÏß: 163.8Сʱ
- ³æºÅ: 519394
- ×¢²á: 2008-03-06
- ÐÔ±ð: GG
- רҵ: Äý¾Û̬ÎïÐÔ II £ºµç×ӽṹ
3Â¥2015-12-23 21:33:46














»Ø¸´´ËÂ¥