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xiaoxue7002(½ð±Ò+1,VIP+0):лл 3-31 09:41
xiaoxue7002(½ð±Ò+1,VIP+0):лл 3-31 09:41
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2Â¥2009-03-30 23:11:43
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6Â¥2009-04-02 11:51:27
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8Â¥2009-04-03 11:11:29
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zdhlover(½ð±Ò+1,VIP+0):лл 4-18 00:55
xiaoxue7002(½ð±Ò+1,VIP+0):лл¹Ø×¢ 4-22 16:04
xiaoxue7002(½ð±Ò+1,VIP+0): 4-22 16:04
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°Ñͼ´«ÉÏÀ´ÎÒ¿´¿´°É ¿ÉÄÜÊDzÙ×÷»òÕß±äÁ¿ÉèÖò»Ç¡µ±µÄÎÊÌ⣬ ÎÒÅöµ½¹ý [ Last edited by zxzj05 on 2009-4-17 at 18:02 ] |

9Â¥2009-04-17 18:01:03
y1ding
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zdhlover(½ð±Ò+2,VIP+0):лл 4-18 00:55
xiaoxue7002(½ð±Ò+1,VIP+0):thank you 4-22 16:06
zdhlover(½ð±Ò+2,VIP+0):лл 4-18 00:55
xiaoxue7002(½ð±Ò+1,VIP+0):thank you 4-22 16:06
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There is a good news about this result, and a bad news. The good news is that there are indeed three acoustic mode, with frequency rather close to zero (less than 1 cm^-1, which is rather good !). The bad news comes when the three other frequencies are compared with experimental results, or other theoretical results. Indeed, in the present run, one obtains three degenerate modes, while there should be a (2+1) splitting. This can be seen in the paper Ab initio calculation of phonon dispersions in semiconductors, by P. Giannozzi, S. de Gironcoli, P. Pavone and S. Baroni, Phys. Rev. B 43, 7231 (1991) , especially Fig. 2. Actually, we have forgotten to take into account the coupling between atomic displacements and the homogeneous electric field, that exists in the case of polar insulators, for so-called "Longitudinal Optic (LO) modes". A splitting appears between these modes and the "Transverse Optic (TO) modes". This splitting (Lyddane-Sachs-Teller LO-TO splitting) is presented in simple terms in standard textbooks, and should not be forgotten in doing Ab initio calculations of phonon frequencies. Thus we have now to treat correctly the homogeneous electric field type perturbation. |
10Â¥2009-04-17 19:39:46














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