²é¿´: 7303  |  »Ø¸´: 175
¡¾½±Àø¡¿ ±¾Ìû±»ÆÀ¼Û143´Î£¬×÷Õߺ£ÌìÌìÒâÔö¼Ó½ð±Ò 111.8 ¸ö
µ±Ç°Ö»ÏÔʾÂú×ãÖ¸¶¨Ìõ¼þµÄ»ØÌû£¬µã»÷ÕâÀï²é¿´±¾»°ÌâµÄËùÓлØÌû

º£ÌìÌìÒâ

Ìú¸Ëľ³æ (ÕýʽдÊÖ)


[×ÊÔ´] ×îР2012 science ¹ØÓÚʯīϩµÄ¼¸ÆªÎÄÕÂ

·îÉϼ¸Æª2012 science ÉÏÓйØgrapheneµÄÎÄÏ×£¬Çë´ó¼ÒÅõ³¡£¡·ÅÐÄÏÂÔØ£¬²»Ðè½ð±Ò¹þ£¡
ÏÂÔØÁË£¬¶¥Ò»ÏÂok£¡
1¡¢Electromechanical Properties of Graphene Drumheads £»Science 336, 1557 (2012);
We determined the electromechanical properties of a suspended graphene layer by scanning tunneling microscopy (STM) and scanning tunneling spectroscopy (STS) measurements, as well as computational simulations of the graphene-membrane mechanics and morphology. A graphene membrane was continuously deformed by controlling the competing interactions with a STM probe tip and the electric field from a back-gate electrode. The probe tip¨Cinduced deformation created a localized strain field in the graphene lattice. STS measurements on the deformed suspended graphene display an electronic spectrum completely different from that of graphene supported by a substrate. The spectrum indicates the formation of a spatially confined quantum dot, in agreement with recent predictions of confinement by strain-induced pseudomagnetic fields.
2¡¢Dislocation-Driven Deformations in Graphene £»Science 337, 209 (2012);
The movement of dislocations in a crystal is the key mechanism for plastic deformation in all materials. Studies of dislocations have focused on three-dimensional materials, and there is little experimental evidence regarding the dynamics of dislocations and their impact at the atomic level on the lattice structure of graphene. We studied the dynamics of dislocation pairs in graphene, recorded with single-atom sensitivity. We examined stepwise dislocation movement along the zig-zag lattice direction mediated either by a single bond rotation or through the loss of two carbon atoms. The strain fields were determined, showing how dislocations deform graphene by elongation and compression of C-C bonds, shear, and lattice rotations.
3¡¢Field-Effect Tunneling Transistor Based on Vertical Graphene Heterostructures£»Science 335, 947 (2012);
An obstacle to the use of graphene as an alternative to silicon electronics has been the absence of an energy gap between its conduction and valence bands, which makes it difficult to achieve low power dissipation in the OFF state. We report a bipolar field-effect transistor that exploits the low density of states in graphene and its one-atomic-layer thickness. Our prototype devices are graphene terostructures with atomically thin boron nitride or molybdenum disulfide acting as a vertical
transport barrier. They exhibit room-temperature switching ratios of ¡Ö50 and ¡Ö10,000, respectively. Such devices have potential for high-frequency operation and large-scale integration.[ Last edited by º£ÌìÌìÒâ on 2012-7-26 at 23:30 ]
»Ø¸´´ËÂ¥

» ±¾Ìû¸½¼þ×ÊÔ´Áбí

» ÊÕ¼±¾ÌûµÄÌÔÌùר¼­ÍƼö

ʯīϩ֪ʶ»ã×Ü ÏȽø²ÄÁÏ Ó¢ÎÄÎÄÏ×»òÕß½Ì²Ä Ê¯Ä«Ï©Óë̼ÄÉÃ×¹Ü
ʯīϩС°Ù¿Æ ¿ÆÑРʯīϩ̼ÄÉÃ׹ܼ¼Êõ¶¥¼¶²Î¿¼ ʯīϩÁ¿×Óµã
¿ÆÑг£Ê¶ ÎÞ»úÄÉÃײÄÁÏ ÉêÇëÁôѧ ¹ØÓÚ﮵çµç³ØµÄ×ÊÔ´ºÏ¼¯
ʯīϩ-¸ß·Ö×Ó¸´ºÏ²ÄÁÏ Ê¯Ä«Ï© »·¾³ÄÜÔ´¿Æѧ ﮵çºÏ³É·½ÃæµÄÎÄÏ×
ʯīϩ¹¦ÄÜÐÞÊμ°Æ临ºÏ²ÄÁϵÄÖƱ¸¼°±íÕ÷ »¯Ñ§½Ì²Ä ¼ÆËã»úÄ£Äâ ÓîÖ泬¼¶ÎÞµÐÅùö¨‡åËÀÈ˲»³¥ÃüÄÉÃײÄÁÏ£¨Ê¯
GSÎÄÏ× µÈÀë×ÓÌå¼¼Êõ¡¢±¡Ä¤¼°Ð²ÄÁÏ µãµÎ ¾«»ª
weiweipengµÄר¼­ ¿ÆÑÐÓëÉú»î Graphene ѧϰ×ÊÁÏ
comeµÄ×ÊԴСվ Science and Nature

» ²ÂÄãϲ»¶

» ±¾Ö÷ÌâÏà¹ØÉ̼ÒÍƼö: (ÎÒÒ²ÒªÔÚÕâÀïÍƹã)

» ±¾Ö÷ÌâÏà¹Ø¼ÛÖµÌùÍƼö£¬¶ÔÄúͬÑùÓаïÖú:

ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû

lfb2008

½ð³æ (ÕýʽдÊÖ)


¡ï¡ï¡ï ÈýÐǼ¶,Ö§³Ö¹ÄÀø

thank
34Â¥2012-07-30 11:05:37
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû
Ïà¹Ø°æ¿éÌøת ÎÒÒª¶©ÔÄÂ¥Ö÷ º£ÌìÌìÒâ µÄÖ÷Ìâ¸üÐÂ
¡î ÎÞÐǼ¶ ¡ï Ò»ÐǼ¶ ¡ï¡ï¡ï ÈýÐǼ¶ ¡ï¡ï¡ï¡ï¡ï ÎåÐǼ¶
×î¾ßÈËÆøÈÈÌûÍƼö [²é¿´È«²¿] ×÷Õß »Ø/¿´ ×îºó·¢±í
[ÂÛÎÄͶ¸å] Ï£ÍûµÕ³¤×Ó˳Àû³ö³¡£¡ +4 C¿¯°ÔÍõ 2024-05-31 5/250 2024-06-02 19:21 by kangshisan
[»ù½ðÉêÇë] ÈëÖ°¸ßУ3Äê·¢±í10+SCI£¬¾¡ÈËÊÂÌýÌìÃü +33 kaoyan250 2024-05-27 48/2400 2024-06-02 19:17 by kaoyan250
[»ù½ðÉêÇë] Èý¸öÆÀίÊÕµ½µÄ»ù½ð°üÀïÃæµÄÏîÄ¿ÊÇÏàͬµÄÂ𣿠+5 ºÓÂí¤ÎÊ·Ê« 2024-06-02 5/250 2024-06-02 19:05 by 328838485
[ÂÛÎÄͶ¸å] Ñ¡ÆÚ¿¯ 5+3 jfdhj 2024-05-29 4/200 2024-06-02 13:30 by bobvan
[¿¼²©] ÇóÉúÎïѧµÄ²©µ¼ÊÕÁô +5 É격³É¹¦¹¦³É²©É 2024-06-01 5/250 2024-06-02 13:19 by С³æ×ÓßÇßÇ
[˶²©¼ÒÔ°] ÂÛ´ó¼Ò¶Ô6070ºóÆÕͨ½ÌÊÚµ¼Ê¦µÄ¿´·¨ +7 SNaiL1995 2024-05-28 11/550 2024-06-02 13:16 by С³æ×ÓßÇßÇ
[¿¼²©] µ¼Ê¦²»ÈÃ˶ת²©£¬ÈÃÎÒÈ¥¹úÍâ¶Á²©£¬ÄÜÀí½âÂ𣿠+12 ÏôɽÓÄ¹È 2024-05-29 20/1000 2024-06-02 12:01 by yuan0806
[¿¼²©] Çó25²©µ¼£¬½ðÊôÔö²ÄÖÆÔì·½Ïò +3 22»úе 2024-06-01 3/150 2024-06-02 11:17 by Napoleonsky
[¿¼²©] 24Ä격ʿÕÐÉú +8 abinit432 2024-05-27 10/500 2024-06-01 17:38 by czp97
[ÂÛÎÄͶ¸å] ÇóSciÆÚ¿¯ÍƼö 10+4 ÕçСÓã 2024-05-30 7/350 2024-06-01 10:41 by bobvan
[»ù½ðÉêÇë] ²©ºóÌرð×ÊÖú״̬±ä»¯ +24 ËæÃζø·É2017 2024-05-30 35/1750 2024-06-01 10:10 by ÇൺÑô×Ð
[¿¼²©] É격ÇóÖú?±¾Ë¶Ë«·ÇһƪÈýÇøºÍËÄÇøÈ¥985¹¤¿Æ·ÇÌì¿ÓרҵÓÐûÓÐÏ£Íû£¿ +4 LYS1200 2024-05-29 6/300 2024-06-01 08:50 by ѧÊõÔüÔüÉñ
[¸ß·Ö×Ó] MMAÔ¤¾ÛÌå¹â¹Ì»¯·¢ÎíÎÊÌâÇóÖú +3 »ÝÑǽð×Ü 2024-05-29 10/500 2024-05-31 14:59 by »ÝÑǽð×Ü
[˶²©¼ÒÔ°] ÇóÎÊendnoteÉÏWileyÒýÓøñʽÔÚÄÄÏÂÔØ +3 Elon. 2024-05-30 3/150 2024-05-31 10:13 by crazy peng
[ÎÄѧ·¼²ÝÔ°] ¶Ô¶Ô×Ó°¡ +5 ÌìÈô¹Â¶À 2024-05-29 7/350 2024-05-31 09:00 by wjykycg
[ÂÛÎÄͶ¸å] ¸ßÊÖÅóÓÑÍƼö±È½ÏÈÝÒ×Ͷ¸åºÍ¼ÓõÄSCIÆÚ¿¯£¬²»Í¶¸åÊÕ·ÑSC£¬¶Ô·ÖÇøûÓÐÒªÇó 5+3 xintangren 2024-05-28 4/200 2024-05-29 10:46 by xintangren
[ÂÛÎÄͶ¸å] ºËÐijõÉ󱻾ܣ¬ÀíÓÉÊÇ¡°Ñ¡ÌâµÄÒâÒå²»Ã÷È·£¬ÎÄÕÂдµÃ²»ÏñÊǿƼ¼ÂÛÎÄ¡±£¬Ôõô¸Ä 5+3 ¹¤ÌÙÀ×»¨Ó£ 2024-05-27 8/400 2024-05-29 10:09 by topedit
[ÂÛÎÄͶ¸å] EIѧ±¨£¬Ò»Éó·µÐÞºó£¬ÎªÉ¶²»ÔÙËÍÉó£¬Ö±½ÓÖÕÉóÖÐ? +4 qweasd12345 2024-05-27 6/300 2024-05-29 00:02 by dut_ameng
[»ù½ðÉêÇë] E05Çà»ùÓм¸¸öÆÀÉó +4 KYXY123 2024-05-28 4/200 2024-05-28 19:25 by popt2t
[»ù½ðÉêÇë] ÃæÉÏ»ù½ð»áÆÀר¼Ò£¬ÓлرܻúÖÆÂ𣿠+4 huang1991js 2024-05-27 4/200 2024-05-27 19:08 by ÐÇ»ð12
ÐÅÏ¢Ìáʾ
ÇëÌî´¦ÀíÒâ¼û