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21Â¥2009-07-24 11:54:52
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xirainbow

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freshgirl(½ð±Ò+1,VIP+0):лл²ÎÓë~ 7-24 23:15
ÊìϤESPRESSOµÄÅóÓѶ¼ÖªµÀØÍÊÆÎļþµÄºó׺ÊÇUPF
ÎÒÒÔǰÒÔΪUPFÊÇultro-soft-pseudoµÄËõд
ËùÒÔÒ»Ö±ºÜÄÉÃÆÎªÊ²Ã´ºó׺ÊÇUPFµÄØÍÊÆÖмÈÓг¬Èí£¬ÓÖÓÐÄ£ÊØºã

½ñÌì¿´ÕâÆªÎÄÏ×£¬ÖÕÓÚÖªµÀÁËUPFµÄÈ«³ÆÊÇ
Unified Pseudopotential File (UPF).

ESPRESSOÈçÊÇ˵£º¡°Another problem affecting interoperability of PW-PP codes is the availability of data files containing atomic PP¡¯s ¡ª one of the basic ingredients of the calculation. There are many different types of PP¡¯s, many different codes generating PP¡¯s (see e.g. Ref [75, 76, 77]), each one with its own format. Again, the choice has fallen on a simple solution that makes it easy to write converters from and to the format used by QUANTUM ESPRESSO. Each atomic PP is contained in a formatted file (efficiency is not an issue here), described by a XML-like syntax. The resulting format has been named Unified Pseudopotential File (UPF). Several converters from other formats to the UPF format are available in QUANTUM ESPRESSO.¡±


[ Last edited by xirainbow on 2009-7-24 at 21:09 ]
22Â¥2009-07-24 21:06:48
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xirainbow

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fegg7502(½ð±Ò+2,VIP+0):thank you very much! 7-26 21:48
ESPRESSO´ÓÎïÀí²ãÃæÉÏÊÇÈçºÎʵÏÖ²¢ÐеÄÄØ£¿
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1£¬image parallelizaton£º½«ËùÓд¦ÀíÆ÷·ÖΪn_image×éimage(ÿ×éÖаüº¬Èô¸É¸öimage)¡£
2£¬pool parallelizaton£º½«Ã¿×éÖеĴ¦ÀíÆ÷½ø¶ø·ÖΪn_pool¸öpool£¬Ã¿¸öpool±»ÓÃÀ´´¦ÀíÈô¸É¸ökµã¡£
3£¬plane-wave parallelizaton£º½«Ã¿¸öpoolÖеĴ¦ÀíÆ÷·ÖΪn_pw×顣Ȼºó½«Êµ¿Õ¼äºÍµ¹¿Õ¼äÖеÄÍø¸ñ·ÖÅ䏸Õân_pw×é¡£
4£¬task-group parallelizaton£º´¦ÀíÆ÷½ø¶øÔÙ±»·ÖΪn_task×顣ÿһ¸ö×é±»ÓÃÀ´´¦ÀíÒ»¸öµç×Ó̬µÄ×éºÏ¡£Ã¿Ò»¸öµç×Ó̬µÄ×éºÏ½«±»ÓÃÓÚ¸µÁ¢Ò¶±ä»»£¬¶ø¸µÁ¢Ò¶±ä»»ÔÚÿһ¸ön_taskÖÐʽ±»²¢Ðл¯µÄ¡£

Îҵķ­ÒëºÍѧÊõˮƽ̫µÍ£¬´ó¼Ò¿´ÆðÀ´»á±È½ÏÄÑÊÜ£¬ÄǾÍÖ±½Ó¿´Ô­Îİɣ»£©Èç¹ûÎÒÉÏÃæÐ´µÄÓв»Í×Ö®´¦£¬»¹Çë¶à¶àÖ¸Õý£»P
¡°In this hierarchy, groups implementing coarser-grained parallel tasks are split into groups implementing finer-grained parallel tasks. The first level is image parallelization, implemented by dividing processors into nimage groups, each taking care of one or more images (i.e. a point in the configuration space, used by the NEB method). The second level is pool parallelization, implemented by further dividing each group of processors into npool pools of processors, each taking care of one or more k-points . The third level is plane-wave parallelization, implemented by distributing real- and reciprocal-space grids across the nPW processors of each pool. The final level is task group parallelization [79], in which processors are divided into ntask task groups of nFFT = nPW=ntask processors, each one taking care of different groups of electron states to be Fourier-transformed, while each FFT is parallelized inside a task group. A further paralellization level, linear-algebra, coexists side-to-side with plane-wave parallelization, i.e. they take care of different sets of operations, with different data distribution.¡±

[ Last edited by xirainbow on 2009-7-25 at 11:55 ]
23Â¥2009-07-25 11:54:18
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xirainbow

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¡°Both separable NC-PPs and US-PPs are implemented; recently,also the projector augmented-wave method [37] has been added, largely following the lines of Ref [84] for its implementation.

[ Last edited by xirainbow on 2009-7-26 at 16:47 ]
24Â¥2009-07-26 16:38:48
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xirainbow

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fegg7502(½ð±Ò+2,VIP+0):thank you very much! 7-26 21:48
US-PPµÄecutwfcÓ¦¸ÃÊÇecutrhoµÄ6~12±¶¡£
ÎҼǵÃÒÔÇ°ÔøÔÚÄÄÀï¿´µ½¹ý£¬ecutrhoºÃÏñÒ²ÐèÒª½øÐÐÊÕÁ²²âÊԵġ£
¹ØÓÚÏÂÃæµÄÁ½×é²ÎÊý£¬ÎÒÒÔǰ´ÓûעÒâ¹ý¡£ÎÄÕÂÖÐÒ²¸ø³öÁËÏàÓ¦µÄ½âÊÍ¡£
nr1, nr2, nr3         INTEGER
    three-dimensional FFT mesh (hard grid) for charge
    density (and scf potential). If not specified
    the grid is calculated based on the cutoff for
    charge density (see also "ecutrho"

nr1s, nr2s, nr3s         INTEGER
    three-dimensional mesh for wavefunction FFT and for the smooth
    part of charge density ( smooth grid ).
    Coincides with nr1, nr2, nr3 if ecutrho = 4 * ecutwfc ( default )

            
Ô­ÎÄ£ºIn the case of US-PPs, the electronic wave functions can be made smoother at the price of having to augment their square modulus with additional contributions to recover the actual physical charge densities. For this reason, the charge density is more structured than the square of the wavefunctions, and requires a larger energy cutoff for its plane wave expansion (typically, 6 to 12 times larger; for a NC-PP, a factor of 4 would be mathematically sufficient). Hence, different real-space Fourier grids are introduced - a "soft" one that represents the square of electronic wave functions, and a "hard" one that represents the charge density [82, 85].
The augmentation terms can be added either in reciprocal space (using an exact but expensive algorithm) or directly in real space (using an approximate but faster algorithm that exploits the local character of the augmentation charges).


   Variable:       tqr

   Type:           LOGICAL
   Default:        .FALSE.
   Description:    If .true., use the (VERY EXPERIMENTAL) real-space algorithm
                   for augmentation charges in ultrasoft pseudopotentials.
                   Must faster execution of ultrasoft-related calculations,
                   but numerically less accurate than the default algorithm.
                   Use with care and after testing!


[ Last edited by xirainbow on 2009-7-27 at 19:30 ]
25Â¥2009-07-26 16:51:58
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xirainbow

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fegg7502(½ð±Ò+2,VIP+0):thank you very much! 7-26 21:48
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Crystal symmetries are automatically detected and exploited to reduce computational costs, by restricting the sampling of the BZ to the irreducible wedge alone.

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When only the gama point (k = 0) is used, advantage is taken of the real character of the orbitals, allowing to store just half of the Fourier components.

ÓÃFermi-Dirac smearingÀ´¿¼ÂÇζÈЧӦ£¬ÒÔǰ¿´¹ýһƪÓйصļÆËã¡£
The finite-temperature effects on the electronic properties can be easily accounted for by using the Fermi-Dirac smearing not as a mathematical device, but as a practical way of implementing the Mermin density-functional approach

Èýά¾§Ìå¿ÉÒÔ¼Óºê¹Ûµç³¡½øÐмÆËã¡£µ«Õâ¸ö¸úBerry phaceÓÐʲô¹ØÏµ£¿
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The effects of finite macroscopic electric fields on the electronic structure of the ground state can be accounted for either through the method of Ref [106, 107] based on the Berry phase, or (for slab geometries only) through a sawtooth external potential [108, 109].
26Â¥2009-07-26 16:58:51
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xirainbow

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ATOMIC Ä£¿é£º
atomicÄ£¿éÍê³ÉÈýÏîÈÎÎñ:
1) solution of the self-consistent all-electron radial Kohn-Sham equations (with a Coulomb nuclear potential and spherically symmetric charge density);
2) generation of NC PPs, of US PPs, or of PAW data-sets;
3) test of the above PPs and data-sets.


ÔÚÉú³ÉØÍÊÆÊ±£¬ÓÐÈý¸öÈ«µç×Ó·½³Ì±¸Ñ¡£º
1) the non relativistic radial Kohn and Sham equations,
2) the scalar relativistic approximation to the radial Dirac equations  
3) the radial Dirac-like equations derived within relativistic density functional theory .

The generation of fully relativistic NC and US PPs including spin-orbit coupling effects is also available.
27Â¥2009-07-27 13:05:12
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Neoo

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[ Last edited by Neoo on 2011-3-24 at 22:27 ]
28Â¥2011-03-24 22:26:27
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