| ²é¿´: 1214 | »Ø¸´: 1 | |||
[½»Á÷]
¡¾ÇóÖú¡¿Çë½Ìһϸ÷λ¶þÁò»¯îѵľ§¸ñ³£Êý¼°»ùʸÊǶàÉÙ£¬·Ç³£¸Ðл£¡£¡£¡
|
| Çë½Ìһϸ÷λ¶þÁò»¯îѵľ§¸ñ³£Êý¼°»ùʸÊǶàÉÙ£¬·Ç³£¸Ðл£¡£¡£¡ |
» ²ÂÄãϲ»¶
±¾ÈË¿¼085602 »¯Ñ§¹¤³Ì ר˶
ÒѾÓÐ23È˻ظ´
Çóµ÷¼ÁԺУÐÅÏ¢
ÒѾÓÐ4È˻ظ´
085600²ÄÁÏÓ뻯¹¤306
ÒѾÓÐ4È˻ظ´
286Çóµ÷¼Á
ÒѾÓÐ10È˻ظ´
328Çóµ÷¼Á£¬Ó¢ÓïÁù¼¶551£¬ÓпÆÑоÀú
ÒѾÓÐ9È˻ظ´
Ò»Ö¾Ô¸±±¾©»¯¹¤´óѧ070300 ѧ˶336Çóµ÷¼Á
ÒѾÓÐ4È˻ظ´
286·ÖÈ˹¤ÖÇÄÜרҵÇëÇóµ÷¼ÁÔ¸Òâ¿ç¿¼£¡
ÒѾÓÐ8È˻ظ´
×ÊÔ´Óë»·¾³ µ÷¼ÁÉêÇë(333·Ö)
ÒѾÓÐ5È˻ظ´
280Çóµ÷¼Á
ÒѾÓÐ12È˻ظ´
269ר˶Çóµ÷¼Á
ÒѾÓÐ5È˻ظ´
» ±¾Ö÷ÌâÏà¹Ø¼ÛÖµÌùÍÆ¼ö£¬¶ÔÄúͬÑùÓаïÖú:
·Ç³£ÖØÒª£¬¹«ÅÉÁôѧ¶Á²©×Éѯ
ÒѾÓÐ6È˻ظ´
Çë½ÌÒ»¸öÇ׺˷´Ó¦
ÒѾÓÐ4È˻ظ´
Çë½Ì¸÷λ´óÏÀÏ©±ûλÑõ»¯³öôÊ»ùÔõô×ö±È½ÏºÃ£¬·Ç³£¸Ðл£¡£¡
ÒѾÓÐ7È˻ظ´
Ϊʲô²ÉÓÃCASTEP¼ÆËãCaTiO3µÄ¹âѧÐÔÖÊÆäÖеľ²Ì¬½éµç³£ÊýÓëʵÑéÖµÏà²îºÜ´ó
ÒѾÓÐ14È˻ظ´
ÇóÎÊÓÃX-ray diffraction Äܶ¨Á¿µÄ²â¶¨³ö¾§ÌåµÄ¾§¸ñ²ÎÊýÂð£¿
ÒѾÓÐ5È˻ظ´
Ï¡ÍÁÑõ»¯ÎïÑõ»¯îƵľ§¸ñ½á¹¹ºÍ³£Êý
ÒѾÓÐ6È˻ظ´
VASPÒ»´ÎÐÔÓÅ»¯ÈñîÑ¿óTiO2¾§¸ñ³£Êýʱ³ö´í£¡£¡
ÒѾÓÐ6È˻ظ´
¡¾ÇóÖú¡¿Çë½ÌÊÖ¶¯½øÐо§¸ñ³£ÊýµÄÓÅ»¯
ÒѾÓÐ4È˻ظ´
¡¾Çë½Ì¡¿Çë½Ìµ¥¾§SeµÄ¾§ÌåÀàÐͺ;§¸ñ³£Êý
ÒѾÓÐ12È˻ظ´
¡¾Çë½Ì¡¿Cu2O ºÍTiO2 ÄÇЩ¾§ÃæÄܹ»¾§¸ñÆ¥Åä
ÒѾÓÐ7È˻ظ´
¡¾Çë½Ì¡¿¹ØÓÚ¾§ÌåµÄ¾§¸ñ³£Êý
ÒѾÓÐ4È˻ظ´
¡¾ÇóÖú¡¿ºîÀÏʦµÄvaspÈëÃŵľ§¸ñÓÅ»¯²¿·Öû¿´¶®£¬ÎÊÒ»ÏÂ
ÒѾÓÐ25È˻ظ´
» ÇÀ½ð±ÒÀ²£¡»ØÌû¾Í¿ÉÒԵõ½:
ũҵÐÅÏ¢¹¤³Ì¼¼Êõ£¨×¨Ë¶£©ÕÐÊÕµ÷¼Á ÉòÑôũҵ´óѧ
+1/182
Ç󹺵羵ÉϵÄÒºµª¹Þ
+5/180
ÄϾ©Ò½¿Æ´óѧÉúֳҽѧÓë×Ó´ú½¡¿µ¹úÖØÊµÑéÊÒ-¶·Éºê¿ÎÌâ×é-ѧÊõ˶ʿÕÐÉú
+1/93
ÖйúµçÆø×°±¸¼¯ÍÅÑо¿ÔºÕÐÊÕAI+²ÄÁϵÈÏà¹Ø¸ÚλʵϰÉú
+1/88
ÎÄÏ×·ÖÏí£¬»¶ÓÒýÓÃ
+1/84
Ô¸Óö¼ûÄ㣬Óö¼û²»Ö¹²Á¼ç¶ø¹ýµÄÔµ·Ö
+1/74
É¢½ð±Ò£¬ÇóºÃÔË£¬×£ÃæÉÏ˳Àû£¡
+2/66
ÖйúÒ©¿Æ´óѧ211-¿ÎÌâ×éÕÐÊÕ2026²©Ê¿/˶ʿ-Óлú»¯Ñ§
+1/48
ÏæÌ¶´óѧ¡°¹ý³ÌÇ¿»¯ÓëÂÌÉ«»¯¹¤¡±´´ÐÂÍŶӲ¹ÕÐ2026ÄêÇïÈëѧ²©Ê¿Éú
+1/35
ÉϺ£½»Í¨´óѧÉòµÀÖǸ±½ÌÊÚÕÐÊÕ2026ÄêÁªÅ಩ʿ/˶ʿÑо¿Éú£¨Î¢ÄÉÆ÷¼þÓëÖÆÔì·½Ïò£©
+1/33
ÕÐÊÕרҵ´úÂë08µÄѧ˶£¡
+1/15
±±¾©Ä³Ñо¿ÔºÉúÎﻯѧÓë·Ö×ÓÉúÎïѧÏà¹Ø×¨ÒµÉêÇ뿼ºËÖÆ²©Ê¿ÕÐÉú£¨´º¼¾£©
+1/11
ÐÂ¼ÓÆÂ¹úÁ¢´óѧҩѧϵ»¯Ñ§ÉúÎïѧ¿ÎÌâ×éÕÐPhD
+1/6
ºþ±±´óѧ²ÄÁÏѧÕÐ26¼¶Ë¶Ê¿Ñо¿ÉúÈô¸ÉÃû
+1/6
ÖйúÅ©¿ÆÔºÀ¼ÖÝÄÁÒ©ËùÊÞÒ©´´ÐÂÓëÄÍÒ©ÐÔ¿ÆÑÐÍŶӯ¸¿ÆÑÐÖúÀí£¬¼±¼±¼±£¡
+1/5
Ïã¸ÛÖÐÎÄ´óѧ»¯Ñ§ÏµÎâ»ùÅà½ÌÊÚÕÐļ2026ÄêÇï¼¾£¨2026Äê8ÔÂ1ÈÕ£©Èëѧȫ½±²©Ê¿Ñо¿Éú
+1/5
»¶ÓÉúÎïÓëÒ½Ò©¡¢Ò©Ñ§¡¢»¯Ñ§µÈÏà¹Ø×¨ÒµµÄͬѧ
+1/4
¡¾¿ÆÑиɻõ¡¿ÄÉÃ׿¹ÌåÆ¾Ê²Ã´³ÉΪʵÑéÊÒ¡°Ð³衱£¿¸½ÓÅÖÊÖÆ±¸·þÎñÉ̲ο¼
+1/3
ÖпÆÔºÉϺ£Î¢ÏµÍ³Ëù²ÄÁÏÉú³¤ÀíÂÛÓë·ÂÕæ¿ÎÌâ×é-²©Ê¿ºóÕÐÆ¸£¨²ÄÁϼÆËãÓëAI4S£©
+1/1
À¥Ã÷Àí¹¤´óѧ³Â½ÕÕ½ÌÊÚÍŶӲ©Ê¿ÕÐÉú
+1/1
¡ï ¡ï ¡ï
youzhizhe(½ð±Ò+3): лл½»Á÷¡£ 2011-03-16 08:54:32
ÊñÖÐɽӥ(½ð±Ò+5): 2011-03-16 12:27:20
youzhizhe(½ð±Ò+3): лл½»Á÷¡£ 2011-03-16 08:54:32
ÊñÖÐɽӥ(½ð±Ò+5): 2011-03-16 12:27:20
|
*data for ICSD #91579 Coll Code 91579 Rec Date 2002/10/01 Mod Date 2006/04/01 Chem Name Titanium Sulfide Structured Ti S2 Sum S2 Ti1 ANX AX2 D(calc) 3.24 Title Structural analysis of the layered compounds Cux Ti S2 Author(s) Kusawake, T.;Takahashi, Y.;Ohshima, K.I. Reference Mol. Cryst. and Liq. Cryst. (2000), 341, 93-98 Golden Book of Phase Transitions, Wroclaw (2002), 1, 1-123 Journal of Physics: Condensed Matter (2001), 13, 9913-9921 Unit Cell 3.4097(5) 3.4097(5) 5.7052(5) 90. 90. 120. Vol 57.44 Z 1 Space Group P -3 m 1 SG Number 164 Cryst Sys trigonal/rhombohedral Pearson hP3 Wyckoff d a R Value .04 Red Cell P 3.409 3.409 5.705 90 90 120 57.443 Trans Red 1.000 0.000 0.000 / 0.000 1.000 0.000 / 0.000 0.000 1.000 Comments Stable from 50 to 420 K (2nd ref., Tomaszewski) The structure has been assigned a PDF number (calculated powder diffraction data): 01-070-6204 The structure has been assigned a PDF number (experimental powder diffraction data): 15-853 Temperature factors available Structure type : CdI2/Mg(OH)2 X-ray diffraction from single crystal Atom # OX SITE x y z SOF H Ti 1 +4 1 a 0 0 0 1. 0 S 1 -2 2 d 0.3333 0.6667 0.24867(4) 1. 0 Lbl Type U11 U22 U33 U12 U13 U23 Ti1 Ti4+ 0.01146(66) 0.01146(6) 0.01626(10) 0.00573(3) 0 0 S1 S2- 0.00967(5) 0.00967(5) 0.01117(7) 0.00483(3) 0 0 Std. Notes Transformation Method: Tidy Std. Cell 3.4097 3.4097 5.7052 90 90 120 Std. Vol. 57.44 Std. Z 1 Std. SG P3-M1 Std. Atom Atom # OX SITE x y z SOF Ti 1 +4 1 a 0 0 0 1. S 1 -2 2 d .33333 .66667 .24867 1. *end for ICSD #91579 [ Last edited by lindlar0078 on 2011-3-15 at 23:17 ] |
2Â¥2011-03-15 23:16:03













»Ø¸´´ËÂ¥