| ²é¿´: 1745 | »Ø¸´: 11 | ||||
| µ±Ç°Ö÷ÌâÒѾ´æµµ¡£ | ||||
[½»Á÷]
·Ç¼òгЧӦ--Éù×ÓÈȵ¼
|
||||
|
×î½üͶµÄƪÎÄÕÂÓйØÓÚ¾§ÌåÈȵ¼ÂʵĽâÊÍÓиöÉó¸åÈ˾õµÃºÍʵÑé½á¹û²»·ûºÏ£¬ÊµÑé½á¹ûÆäʵÊÇËæÎ¶ÈÉý¸ß£¬Èȵ¼ÂÊÂÔ΢±äС£¬²»ÊǺÜÃ÷ÏÔ£¬µ«ÊÇÔÚ¸ßΣ¨550K£©²¿·Ö£¬Èȵ¼ÂÊÂÔ΢Ôö¼Ó£¬¸ÃÉó¸åÈËÈÏΪ²»ÊʺÏÓÐÕâ¸öЧӦ½âÊÍ£¬ÏÂÃæÊÇËû¶ÔÕâ¸öµÄ»Ø¸´ I do not agree on the relevance of anharmonic effects in determining the thermal conductivity (page 4, line 57): Fig. 8 shows no clear temperature dependence, while in case of anharmonic phonon phonon scattering, k should decrease with the temperature. ÓмÆËã±íÃ÷¸Ã¾§ÌåÖдæÔÚ¹âѧÉù×ÓÈí»¯£¬¹âѧºÍÉùѧģʽƵÂÊÏà½ü£¬Ä£Ê½¼äÄÜÁ¿×ª»¯ÈÝÒס£ÓÉÓڷǼòгЧӦ×÷Óã¬ÔØÈȵÄÉùƵ֧½«±»µÍƵµÄ¹âƵ֧ɢÉäµ¼Ö¼«µÍµÄÈȵ¼ÂÊ¡£ ÓÉÓÚÎÒÊÇѧ²ÄÁϵ쬶ÔÎïÀíÖ®ÀàµÄ¶«Î÷²»ÊǺÜÇå³þ£¬Ò»°ãµÄ·Ç¼òгЧӦÊÇÉùѧÉù×ÓÖ®¼äµÄÏ໥×÷Óã¬ÕâÖÖ¹âѧÉù×ÓÈí»¯¿ÉÒÔ½âÊÍÕâ¸öÂð |
» ÊÕ¼±¾ÌûµÄÌÔÌûר¼ÍƼö
µÚÒ»ÔÀí/¹ÌÌåÎïÀí»ù´¡ÀíÂÛ֪ʶ |
» ²ÂÄãϲ»¶
0703»¯Ñ§µ÷¼Á
ÒѾÓÐ12È˻ظ´
0703»¯Ñ§ 305Çóµ÷¼Á
ÒѾÓÐ4È˻ظ´
0703»¯Ñ§µ÷¼Á£¬Çó¸÷λÀÏʦÊÕÁô
ÒѾÓÐ10È˻ظ´
271²ÄÁϹ¤³ÌÇóµ÷¼Á
ÒѾÓÐ5È˻ظ´
281Çóµ÷¼Á£¨0805£©
ÒѾÓÐ16È˻ظ´
304Çóµ÷¼Á
ÒѾÓÐ6È˻ظ´
²ÄÁϹ¤³Ìר˶µ÷¼Á
ÒѾÓÐ6È˻ظ´
Ò»Ö¾Ô¸Ìì´ó²ÄÁÏÓ뻯¹¤£¨085600£©×Ü·Ö338
ÒѾÓÐ4È˻ظ´
085700×ÊÔ´Óë»·¾³308Çóµ÷¼Á
ÒѾÓÐ3È˻ظ´
Çó²ÄÁϵ÷¼Á
ÒѾÓÐ8È˻ظ´
» ±¾Ö÷ÌâÏà¹ØÉ̼ÒÍÆ¼ö: (ÎÒÒ²ÒªÔÚÕâÀïÍÆ¹ã)

xiamg
Ìú¸Ëľ³æ (ÖøÃûдÊÖ)
- Ó¦Öú: 14 (СѧÉú)
- ½ð±Ò: 11292.1
- É¢½ð: 1033
- ºì»¨: 6
- Ìû×Ó: 1112
- ÔÚÏß: 226Сʱ
- ³æºÅ: 441447
- ×¢²á: 2007-10-27
- רҵ: Äý¾Û̬ÎïÐÔI:½á¹¹¡¢Á¦Ñ§ºÍ
2Â¥2010-03-15 16:34:18
|
ÎÄÏ×£¨PRB 77£¬245203£¨2008£©£©First-principles calculations of the electronic, optical, and lattice vibrational properties of ** were performed with the generalized gradient approximation GGA and the screened-exchange local-density approximation sx-LDA method, which successfully corrects the band-gap problem found with GGA. ÓÐÁíһƪÎÄÏ×רÃÅÌáµ½ÓÉÓÚÔÚÆä×îµÍ¾§¸ñÈȵ¼£¨77K£©µÄʱºòÉù×ÓÆ½¾ù×ÔÓɳ̴ﵽÔ×Ó¼ä¾à£¬1/TµÄÈȵ¼¹ØÏµÒѾ²»³ÉÁ¢ÁË |

3Â¥2010-03-15 18:07:34
xiamg
Ìú¸Ëľ³æ (ÖøÃûдÊÖ)
- Ó¦Öú: 14 (СѧÉú)
- ½ð±Ò: 11292.1
- É¢½ð: 1033
- ºì»¨: 6
- Ìû×Ó: 1112
- ÔÚÏß: 226Сʱ
- ³æºÅ: 441447
- ×¢²á: 2007-10-27
- רҵ: Äý¾Û̬ÎïÐÔI:½á¹¹¡¢Á¦Ñ§ºÍ
Ä«Ïã(½ð±Ò+5):ллָµ¼ 2010-03-16 21:03
|
¡°ÓмÆËã±íÃ÷¸Ã¾§ÌåÖдæÔÚ¹âѧÉù×ÓÈí»¯£¬¹âѧºÍÉùѧģʽƵÂÊÏà½ü£¬Ä£Ê½¼äÄÜÁ¿×ª»¯ÈÝÒס£ÓÉÓڷǼòгЧӦ×÷Óã¬ÔØÈȵÄÉùƵ֧½«±»µÍƵµÄ¹âƵ֧ɢÉäµ¼Ö¼«µÍµÄÈȵ¼ÂÊ¡£¡±ÎªÊ²Ã´Ëµ¡°Ä£Ê½¼äÄÜÁ¿×ª»¯ÈÝÒס±£¿Éó¸åÈËÒѾÌáµ½Éù×Ó-Éù×ÓÏ໥×÷ÓÃÓ¦¸ÃÒýÆðÈȵ¼ÂÊËæÎ¶ÈÔö¼Ó¶ø¼õСµÄ£¬¶øÄãÎÄÖеÄͼÏßÏÔʾÈȵ¼ÂÊÓëζÈûÓйØÏµ£¬ËùÒÔÄã¸ø³öµÄÉù×ÓÉù×ÓÏ໥×÷Ó㨼´·Ç¼òгЧӦ£©²»ÄܽâÊÍÄãµÄ½á¹û¡£ ÔÙÓÐÒ»µã£¬¡°·Ç¼òгЧӦÊÇÉùѧÉù×ÓÖ®¼äµÄÏ໥×÷Óá±ÕâÖÖ˵·¨ÊDz»¶ÔµÄ£¬·Ç¼òгЧӦ¼´Éù×Ó-Éù×ÓÏ໥×÷Óã¬ÓÐÈýÉù×Ó¡¢ËÄÉù×Ó¹ý³Ì£¬ÆäÖÐÈýÉù×Ó¹ý³ÌÒ»°ã·ÖÕý³£É¢Éä¹ý³ÌºÍµ¹Äæ¹ý³Ì£¬ËûÃÇÐèÒªÂú×ãÒ»¶¨µÄÌõ¼þ²Å¿ÉÒÔ·¢Éú¡£±ÈÈ磬ÈýÉù×Ó¹ý³ÌÖм´¿ÉÄÜÊÇÒ»¸öÉùѧÉù×ÓÉ¢Éä³É¶þ¸öÉùѧÉù×Ó£¬Ò²¿ÉÄÜÉ¢Éä³ÉÒ»¸öÉùѧÉù×ÓºÍÒ»¸ö¹âѧÉù×Ó£¬»¹¿ÉÄÜÊǶþ¸ö¹âѧÉù×Ó£»·´¹ýÀ´Ò²¿ÉÄÜ¡£ 1/TµÄÈȵ¼ÆðÔ´ÓÚʲôÉù×ÓÄØ£¿1/TµÄÈȵ¼¹ØÏµÒѾ²»³ÉÁ¢±íʾÕâ¸öÉù×Ó¶ÔÈȵ¼µÄ¹±Ïײ»ÔÙÆðÖ÷µ¼×÷Ó㬶øÊÇÆäËûÉù×ÓÆðÖ÷Òª×÷ÓÃÁË¡£ |
4Â¥2010-03-16 09:36:30
|
¡°Ä£Ê½¼äÄÜÁ¿×ª»¯ÈÝÒס±ÔÎÄÊÇ£ºThe closeness between the frequencies of the optic modes and the acoustic modes means that energy transfer between these modes is easy. 1/TµÄÈȵ¼ÆðÔ´ÓÚÉùѧÉù×Ó£¬1/TµÄÈȵ¼¹ØÏµ²»³ÉÁ¢±íʾÕâ¸öÉù×Ó¶ÔÈȵ¼µÄ¹±Ïײ»ÔÙÆðÖ÷µ¼×÷Ó㬶øÊÇÆäËûÉù×ÓÆðÖ÷Òª×÷Óã¬ÄÇôÕâ¸öËùνµÄÆäËûÉù×Ó¶ÔÈȵ¼µÄ×÷ÓÃÒ²ÊÇËæÎ¶ȵÄÉý¸ßÈȵ¼½µµÍµÄÂ𣿼´Ê¹ÊÇÔÚÉù×ÓÆ½¾ù×ÔÓɳÌΪÔ×Ó¼ä¾à? ÈõÈõµÄÎÊÒ»¾ä£¬ËùνµÄÉù×ÓÉù×Ó£¨²»ÂÛʲôÉù×Ó£©µÄÏ໥×÷Óö¼ÓзǼòгЧӦÂ𣿠[ Last edited by Ä«Ïã on 2010-3-16 at 10:31 ] |

5Â¥2010-03-16 10:29:17
xiamg
Ìú¸Ëľ³æ (ÖøÃûдÊÖ)
- Ó¦Öú: 14 (СѧÉú)
- ½ð±Ò: 11292.1
- É¢½ð: 1033
- ºì»¨: 6
- Ìû×Ó: 1112
- ÔÚÏß: 226Сʱ
- ³æºÅ: 441447
- ×¢²á: 2007-10-27
- רҵ: Äý¾Û̬ÎïÐÔI:½á¹¹¡¢Á¦Ñ§ºÍ
¡ï
Ä«Ïã(½ð±Ò+1):лл²ÎÓë
Ä«Ïã(½ð±Ò+4):ллָµ¼ 2010-03-16 21:04
Ä«Ïã(½ð±Ò+1):лл²ÎÓë
Ä«Ïã(½ð±Ò+4):ллָµ¼ 2010-03-16 21:04
|
×÷ÓÃÒ²ÊÇËæÎ¶ȵÄÉý¸ßÈȵ¼½µµÍµÄÂ𣿼´Ê¹ÊÇÔÚÉù×ÓÆ½¾ù×ÔÓɳÌΪÔ×Ó¼ä¾à? £¨1£©ÊÇ£¬£¨2£©Éù×ÓÆ½¾ù×ÔÓɳÌΪÔ×Ó¼ä¾àʱ£¬Éù×Ó´«ÊäÓ¦¸ÃΪµ¯µÀ´«Ê䷽ʽ£¬Õâʱ²£¶ú×ÈÂü´«Êä²»ÊÊÓÃÁË¡£ 1/TµÄÈȵ¼Ó¦¸ÃÊǸßÎÂÇé¿öÏÂÈýÉù×Ó¹ý³Ì£¨»¹ÓÐ1/T^2µÄ£©£¬ËæÎ¶ÈÉý¸ßÈȵ¼Ó¦¸Ã³öÏÖ1/T^2ÏҲ¾ÍÊÇÆäÈȵ¼-ζÈͼÏßÖÐбÂʱÈ1/T»¹Òª´ó£¨ÇúÏßϽµ»¹Òª¿ì£©£¬¶øÄãµÄ½á¹ûÊÇÈȵ¼ËæÎ¶ÈûÓйØÏµÁË£¬¼´Î¶ÈÔö¼ÓÈȵ¼¼¸ºõ²»±ä£¡ ·Ç¼òгЧӦ¾ÍÊÇÖ¸Éù×Ó-Éù×ÓÏ໥×÷Óᣠ![]() [ Last edited by xiamg on 2010-3-16 at 19:35 ] |
6Â¥2010-03-16 19:29:03

7Â¥2010-03-16 21:04:47
xiamg
Ìú¸Ëľ³æ (ÖøÃûдÊÖ)
- Ó¦Öú: 14 (СѧÉú)
- ½ð±Ò: 11292.1
- É¢½ð: 1033
- ºì»¨: 6
- Ìû×Ó: 1112
- ÔÚÏß: 226Сʱ
- ³æºÅ: 441447
- ×¢²á: 2007-10-27
- רҵ: Äý¾Û̬ÎïÐÔI:½á¹¹¡¢Á¦Ñ§ºÍ
8Â¥2010-03-17 16:28:32
9Â¥2010-03-17 16:31:29
|
Éó¸åÒâ¼û£ºI do not agree on the relevance of anharmonic effects in determining the thermal conductivity (page 4, line 57): Fig. 8 shows no clear temperature dependence, while in case of anharmonic phonon phonon scattering, k should decrease with the temperature. In some samples it even increases (x=54), thus signifying that k is mainly determined by impurity, disorder or grain boundary scattering. ÎÒ¸ÃÔõô»Ø´ð±È½ÏºÃ£¬Í¬ÒâËû˵µÄÊÇimpurity, disorder or grain boundary scattering. Ó°ÏìµÄ£¿ |

10Â¥2010-03-18 10:50:16













»Ø¸´´ËÂ¥

