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chuzhaonan

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2Â¥2013-06-25 14:39:50
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KalaShayminS

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¡ï ¡ï ¡ï ¡ï ¡ï
Сľ³æ: ½ð±Ò+0.5, ¸ø¸öºì°ü£¬Ð»Ð»»ØÌû
souledge: ½ð±Ò+2, It is quite interesting! 2013-06-25 21:05:21
souledge: ½ð±Ò+2, The new beta version (2.1.22) has been uploaded since June 27th. 2013-06-30 17:58:14
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3Â¥2013-06-25 17:00:43
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ÒýÓûØÌû:
3Â¥: Originally posted by KalaShayminS at 2013-06-25 17:00:43
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ELKÒ²ÄÜÓÐSVN·¢²¼µÄNighty°æ£¿´ÓÄĶùÄÜŪµ½°¡£¿¹Ù·½ÍøÕ¾Ã»¿´µ½ÈκεÄ˵Ã÷°¡¡«
4Â¥2013-06-25 21:05:08
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû

gongjijun

ľ³æ (ÕýʽдÊÖ)


¡ï ¡ï
Сľ³æ: ½ð±Ò+0.5, ¸ø¸öºì°ü£¬Ð»Ð»»ØÌû
souledge: ½ð±Ò+1, The new beta version (2.1.22) has been uploaded since June 27th. 2013-06-30 17:58:26
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5Â¥2013-06-25 22:31:56
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ÒýÓûØÌû:
5Â¥: Originally posted by gongjijun at 2013-06-25 22:31:56
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6Â¥2013-06-25 22:45:03
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gongjijun

ľ³æ (ÕýʽдÊÖ)


ÒýÓûØÌû:
6Â¥: Originally posted by souledge at 2013-06-25 22:45:03
Ö±½ÓÓÃelk.sourceforge.netÊǵÄÈ·¹úÄÚÉϲ»È¥µÄ£¬µ«ÊÇwww.sourceforge.netȴûÓÐÈκÎÎÊÌ⣬˵Ã÷²»ÊDZ»Ç½£¬¶øÊÇDNSÓÐ벡£¬²»ÄÜÕýÈ·½âÎö×ÓÓòÃû¡«
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7Â¥2013-06-27 10:46:42
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gongjijun

ľ³æ (ÕýʽдÊÖ)


ÒýÓûØÌû:
6Â¥: Originally posted by souledge at 2013-06-25 22:45:03
Ö±½ÓÓÃelk.sourceforge.netÊǵÄÈ·¹úÄÚÉϲ»È¥µÄ£¬µ«ÊÇwww.sourceforge.netȴûÓÐÈκÎÎÊÌ⣬˵Ã÷²»ÊDZ»Ç½£¬¶øÊÇDNSÓÐ벡£¬²»ÄÜÕýÈ·½âÎö×ÓÓòÃû¡«
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8Â¥2013-06-27 11:18:54
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ifmc1234

ľ³æ (ÖøÃûдÊÖ)


¡ï ¡ï ¡ï ¡ï ¡ï ¡ï
Сľ³æ: ½ð±Ò+0.5, ¸ø¸öºì°ü£¬Ð»Ð»»ØÌû
souledge: ½ð±Ò+3, It's a heartening news! 2013-06-28 21:53:43
souledge: ½ð±Ò+2, The new beta version (2.1.22) has been uploaded since June 27th. 2013-06-30 17:58:01
Dear All,

In anticipation of the upcoming CECAM Elk Tutorial, we are releasing a
beta version 2. This is a test version that is unsuitable for
production, but may be used to test the new features of the code.

The main new addition is linear-response phonons using density
functional perturbation theory. This has been under intense development
for over a year, and is nearly ready for production. There are a few
remaining problems with the implementation which will be hopefully
resolved prior to the Tutorial.

Also new, is the full magnetic response tensor chi(G,G',q,w) which
works with all LSDA functionals as well as spin-orbit coupling,
non-collinear magnetism and spin-spirals.

We'd also like to welcome Oscar Grånäs as a new main author of the
code.

Best wishes,
Kay Dewhurst, Sangeeta Sharma, Lars Nordstrom, Francesco Cricchio,
Fredrik Bultmark, Oscar Grånäs and Hardy Gross

-------------------------------

elk-2.1.22
-Important: this is a beta version and should not be used for
production work; a production release will be made in a few weeks
-Important: this version is not backwards compatible; calculations will
have to be converged from scratch
-density functional perturbation theory (DFPT) phonons now available;
only for spin-unpolarised calculations at the moment; spin-polarisation
will be added for the next release; use with task=205; still
experimental and generates incorrect results for certain symmetries -
we're still working on this; see the example 'Al-phonon-DFPT'
-full frequency-dependent magnetic response function now available;
works with non-collinear magnetism, etc.; use task=330; see example
'Ni-magnetic-response'
-iterative diagonalisation greatly improved; now uses the method of P.
Blaha, et al., J. Comp. Phys. 229, p453 (2010)
-upgraded code to handle libxc version 2
-hybrid functionals should now work with libxc (experimental)
-upgraded LAPACK to version 3.4.2
-block name dos changed to wplot; changed variable 'nwdos' to 'nwplot'
-variable 'gmaxrpa' changed to 'gmaxrf'; this is the response function
G-vector cut-off
-BSE and TDDFT now faster, more accurate and memory efficient; thanks
to M. Meinert for discussions
-task 188 changed to 320
-reintroduced the variables 'lmaxinr' and 'fracinr'; this improves
stability
-lots of optimisations
-added more MPI parallelism
-various minor bug fixes
-conduction state local-orbitals can now be switched on; use
'lorbcnd=.true.'; this can improve both ground-state and response
function calculations; this is switched on automatically when
'highq=.true.'
-most species files have been changed; mostly larger muffin-tin radii
-Important: Markus Meinert suggested a change to 'nempty'; this
variable now represents the number of states per atom and spin; this
scales automatically as the number of atoms is increased
-default 'nempty' is now 4
-M. Meinert changed the default Broyden parameters after extensive
testing
-LN fixed bug in XCrysDen Fermi surface plotting
-LN also reduced the number of states which contribution to the Fermi
surface plot to the minimum
-supercell phonon calculations can now be restarted with 'task=202'
-Frank Wagner discovered a bug which affects certain types of
symmetries in rare instances; this has now been fixed
-Important: default smearing function is now Fermi-Dirac (stype=3)
-entropy contribution now added to the total energy
-default smearing width reduced to 0.001 Ha, corresponding to room
temperature
-M. Meinert added a blocks-to-columns script; this is in the
'utilities' directory
-Oscar Grånäs added to list of main authors


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9Â¥2013-06-28 09:56:30
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû
ÓÐûÓÐÈËÓÐÐËȤ°ÑеÄ2.1.22±àÒë³ÉWindows°æ°¡£¿½üÀ´ÊÖÍ·µÄµçÄÔûÓа²×°Visual Studio£¬ÎÞ·¨±àÒëµÄ˵¡«
10Â¥2013-07-02 18:22:48
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû

hezhu

½ð³æ (СÓÐÃûÆø)


¡ï
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  • 2013-08-09 18:39:17, 3.01 M
11Â¥2013-08-09 18:39:59
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû

hezhu

½ð³æ (СÓÐÃûÆø)


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