±±¾©Ê¯ÓÍ»¯¹¤Ñ§Ôº2026ÄêÑо¿ÉúÕÐÉú½ÓÊÕµ÷¼Á¹«¸æ
²é¿´: 322  |  »Ø¸´: 2
¡¾½±Àø¡¿ ±¾Ìû±»ÆÀ¼Û2´Î£¬×÷ÕßstaphleeÔö¼Ó½ð±Ò 2 ¸ö
µ±Ç°Ö÷ÌâÒѾ­´æµµ¡£

staphlee

½ð³æ (ÕýʽдÊÖ)


[×ÊÔ´] һƪÓйØUeq(displacement parameter,ζÈÒò×Ó)µÄÎÄÏ×(×÷Õß½¨×h²»Òª·QËüœØ¶ÈÒò×Ó)

һƪÓйØUeq(atomic displacement parameter (ADP), or ζÈÒò×Ó)µÄÎÄÏ×
ÕâÆªÖ÷Òª½²µ½ÓйØUeqÏÖÔÚµÄÃüÃûºÏ²»ºÏÊÊ...ÓÐºÜ¶à¼ÆËã....ÎÒ°Ñ×îÖ÷Òª×ܽáµÄµØ·½¸øcopy³öÀ´¸ø¸÷λ³æÓÑ....¶Ô¼ÆËãÓÐÐËȤµÄ×Ô¼ºÈ¥ÏÂÔØÈ«ÎİÉ....ÆäÖÐÔÚµÚ6.µÄµØ·½ÓÐÌÖÂÛµ½²»ÊʺϳÆÕâ¸ötermΪζÈÒò×Ó...ÕâÒ²ÊÇ×÷ÕßµÄÒâ¼ûÀ²...»¹ÊÇÂú¶àÈËÔÙÓÃÕâ¸öÃû´ÊµÄ...´ó¼Ò¿´¿´. ...²Î¿¼Ò»ÏÂ.....


from Acta Cryst. (1996). A52, 770-781.
http://d.namipan.com/d/aa88c4255 ... e4ff079c2bbb6f71300

4. Recommendations
1. The term anisotropic displacement parameters (abbreviated
ADPs) should be used in referring to the
individual atomic coefficients in the exponent of the
factor that describes the effects of atomic motion and
static displacement.

2. The elements of the tensors U and/5 should always
be superscripted when the refinement is referred to a
crystal system rather than to a Cartesian system. This
definition follows from the definition of the elements
of U and /5 as contravariant tensor components (see
¡ì2.1). The frequent use of subscripts for the ADPs, and
specifically for those not referred to Cartesian systems,
is inconsistent with their tensorial properties.

3. With the common Gaussian approximation, use
either the quantities U ij, which have dimension (length) 2,
defined in (25), or the dimensionless/3/j, defined in (22).

4. When the Gaussian approximation to the probability
density function is not deemed valid, the use of
the Gram-Charlier expansion of (62) is recommended,
although other formalisms may sometimes be advantageous
for special problems.

5. Standard uncertainties of ADPs obtained from a
full-matrix refinement are valid within the system in
which the refinement is made. If ADPs are transformed
to any other axial system, Cartesian or not, then the
uncertainties may also be calculated by transforming
the original variance-covariance matrix to this new
axial system and taking the square roots of its
diagonal elements, i.e. the variances. The required
variance-covariance matrix is usually not available
for ADPs taken from the literature. Hence, although
ADPs can still be transformed, their uncertainties cannot
be. Calculations involving published ADPs and their
(published) uncertainties should therefore be referred to
the same system of coordinates as the original refinement
in order to retain the significance of the published
uncertainties.

6. Avoid using the term 'temperature factor', both
because the phenomenon represented may not be due
entirely to thermal motion and because that phrase has
in the past been used in several quite distinct senses
(see ¡ì1.5).

7. Avoid using the Gaussian anisotropic parameters
that are now usually symbolized as B ij and are defined
in (26). These quantities are directly proportional to the
recommended U ij, the ratio being 87r 2.

8. Avoid using ADPs that do not represent matrix elements.
In some early references and computer programs,
cross terms were sometimes doubled in magnitude, being
represented, for example, as hk~ 12 instead of 2hk~ 12 for
programming convenience. This was possible because
the matrix representing the ADP is symmetric, with only
six independent terms. This practice is not found in
modern crystallographic software.

9. Published values of Ueq should always be accompanied
by their standard uncertainties. The ratio
of the minimum to the maximum eigenvalues of the
corresponding anisotropic displacement tensors should
also be published, either in the primary publication itself
or in the secondary (deposition) publication.
Authors of crystallographic software and crystallographers
who maintain their own software are encouraged
to introduce the minor modifications that are required
for the implementation of these Recommendations.

[ Last edited by staphlee on 2009-7-13 at 09:14 ]
»Ø¸´´ËÂ¥
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû

wangxj505

Ìú¸Ëľ³æ (ÕýʽдÊÖ)


¡ï¡ï¡ï¡ï¡ï ÎåÐǼ¶,ÓÅÐãÍÆ¼ö

¶àлÁË£¬ÕýÔÚ¿´Õâ¸ö·½ÃæµÄÎÄÏ×
2Â¥2009-11-18 22:39:26
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû

brilliant

¾èÖú¹ó±ö (Ö°Òµ×÷¼Ò)


¡ï¡ï¡ï¡ï¡ï ÎåÐǼ¶,ÓÅÐãÍÆ¼ö

thanks
3Â¥2009-11-19 13:06:19
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû
Ïà¹Ø°æ¿éÌø×ª ÎÒÒª¶©ÔÄÂ¥Ö÷ staphlee µÄÖ÷Ìâ¸üÐÂ
¡î ÎÞÐǼ¶ ¡ï Ò»ÐǼ¶ ¡ï¡ï¡ï ÈýÐǼ¶ ¡ï¡ï¡ï¡ï¡ï ÎåÐǼ¶
×î¾ßÈËÆøÈÈÌûÍÆ¼ö [²é¿´È«²¿] ×÷Õß »Ø/¿´ ×îºó·¢±í
[¿¼ÑÐ] 320Çóµ÷¼Á +3 ũҵ¹¤³ÌÓëÐÅÏ¢¼ 2026-04-03 3/150 2026-04-03 11:40 by ÍÁľ˶ʿÕÐÉú
[¿¼ÑÐ] 296²ÄÁÏר˶Çóµ÷¼Á +20 202451007219 2026-04-02 21/1050 2026-04-03 11:15 by wangjy2002
[¿¼ÑÐ] ÉúÎïѧÇóµ÷¼Á +3 15064154688 2026-04-03 3/150 2026-04-03 10:28 by macy2011
[¿¼ÑÐ] 070300»¯Ñ§Çóµ÷¼Á +10 Æð¸öÃûÕ¦ÕâôÄÑ 2026-03-27 11/550 2026-04-03 10:24 by macy2011
[¿¼ÑÐ] ±§Ç¸ +5 ÌïºéÓÐ 2026-03-30 5/250 2026-04-03 10:24 by linyelide
[¿¼ÑÐ] 260Çóµ÷¼Á +3 ÖìÜÆÁÕ 2026-04-02 3/150 2026-04-03 08:44 by yulian1987
[¿¼ÑÐ] 277Çóµ÷¼Á +3 12A3 2026-04-02 3/150 2026-04-02 21:30 by swb0218
[¿¼ÑÐ] 296Çóµ÷¼Á +4 sdhu 2026-04-02 4/200 2026-04-02 21:29 by baoball
[¿¼ÑÐ] Ò»Ö¾Ô¸085600ÖпÆÔºÄþ²¨Ëù276·ÖÇóµ÷¼Á +26 ²ÄÁÏѧ257Çóµ÷¼Á 2026-03-28 27/1350 2026-04-02 15:15 by chyhaha
[¿¼ÑÐ] ²ÄÁÏ¿ÆÑ§Ó빤³Ìµ÷¼Á +18 ÉîVËÞÉá°É 2026-03-30 19/950 2026-04-02 10:28 by sanrepian
[¿¼ÑÐ] 304Çóµ÷¼Á +12 ËØÄê¼ÀÓï 2026-03-31 15/750 2026-04-01 22:41 by peike
[¿¼ÑÐ] ²ÄÁÏÓ뻯¹¤£¨0856£©304ÇóBÇøµ÷¼Á +8 Çñgl 2026-03-30 16/800 2026-04-01 17:58 by Çñgl
[¿¼ÑÐ] Ò»Ö¾Ô¸»ªÄÏʦ·¶361·Ö£¬»¯Ñ§Çóµ÷¼Á +4 Nicole88888 2026-04-01 4/200 2026-04-01 10:08 by ÌÆãå¶ù
[¿¼ÑÐ] 339Çóµ÷¼Á +5 zjjkt 2026-03-31 5/250 2026-04-01 09:18 by JourneyLucky
[¿¼ÑÐ] 315Çóµ÷¼Á +6 akie... 2026-03-28 7/350 2026-03-31 16:48 by asdfzly
[¿¼ÑÐ] 327Çóµ÷¼Á +5 С¿¨²»¿¨. 2026-03-29 5/250 2026-03-30 19:30 by Wang200018
[¿¼ÑÐ] 0703»¯Ñ§321·ÖÇóµ÷¼Á +10 Èýdd. 2026-03-30 11/550 2026-03-30 19:24 by markhwc
[¿¼ÑÐ] 293Çóµ÷¼Á +3 ĩδmm 2026-03-30 5/250 2026-03-30 17:23 by Íõ±£½Ü33
[¿¼ÑÐ] 11408Èí¼þ¹¤³ÌÇóµ÷¼Á +3 Qiuѧing 2026-03-28 3/150 2026-03-28 21:50 by zhq0425
[¿¼ÑÐ] Ò»Ö¾Ô¸ÄϾ©º½¿Õº½Ìì´óѧ²ÄÁÏѧ˶Çóµ÷¼Á +3 @taotao 2026-03-28 3/150 2026-03-28 10:26 by JourneyLucky
ÐÅÏ¢Ìáʾ
ÇëÌî´¦ÀíÒâ¼û