[Wien] Crystal field splitting in empty 3d band of Fe2O3

2009-09-17 Thread Hua Wu
Dear Y. Ding,

 For the material Fe2O3 having the formal high-spin Fe3+ and a closed 
up-spin shell, I think LDA (when giving an insulating solution) or LDA+U
partial d-DOS can well show the t2g-eg (if being eigenorbitals) crystal field 
splitting. 

Just a note: have you worked with a hexagonal lattice coordinate or a local 
octahedral coordinate ?  May the short Fe-Fe pair or a trigonal field distort 
too much the crystal field level diagram ?

best regards -- H. Wu

On Thursday 17 September 2009 07:51, Pavel Novak wrote:
  Dear Yang Ding,

 yesterday I forgot third point, which perhaps could give answer to your
 question. If U is chosen such that it put d-states close to the oxygen p-
 states, hybridization increases and it shifts the d-levels down if EdEp,
 or up if EdEp.
 Regards Pavel

 On Wed, 16 Sep 2009, Pavel Novak wrote:
  Dear Yang Ding,
 
  care is needed when estimating the crystal field splitting from the LDA+U
  calculation using the DOS. There are two reasons for it. First, the LDA+U
  lower the energy of more occupied states and increase the energy of less
  occupied states. Even if the bands are above Fermi energy, they contain
  nonzero fraction of electrons (cf :QTL in scf file), which is different
  for eg and t2g states, hence LDA+U distorts the splitting. Second, the
  selfinteraction of the d-electrons is present, again distorting the
  crystal field splitting.
 
  Regards
  Pavel Novak
 
  On Tue, 15 Sep 2009, Yang Ding wrote:
   Dear WIEN2k  users,
  
   I am really new to WIEN2k, and wondering if you could give your advice
   and experience on following question concerning the crystal filed
   splitting calculated from WIEN2k.
  
   In order to understand if the pre-edge splitting appearing in the Fe
   K-edge spectra (1s-4p transition) measured by emission-XANES on Fe2O3
   [Groot et al. J. Phys.: Condens. Matter 21 (2009) 104207
   http://www.iop.org/EJ/abstract/0953-8984/21/10/104207/], is linked to
   crystal-filed splitting in 3d empty band. We did a very preliminary
   ground state calculation using WIEN2k based on GGA+U (and LSDA+U) with
   U = 4 eV structure to check the crystal field splitting in empty d band
   above Fermi level.
  
   As a result, we found that above 2-6 eV above Fermi level, the energy
   of t2g is higher than that of eg. This result is similar to what
   reported by Rollsman et al (PHYSICAL REVIEW B 69, 165107 (2004)
   http://prola.aps.org/abstract/PRB/v69/i16/e165107) on Fe2O3. In his
   calculation (GGA/LSDA+U , U= 4eV), the energy of t2g is also higher
   than that of eg. So my question is why the t2g and eg are reversed in
   DFT, but the Multiplet calculation gives contradictory results (i.e
   from Groot et al.).
  
   I noticed that  Glatzel et al (PHYSICAL REVIEW B 77, 115133 (2008)
   http://prola.aps.org/abstract/PRB/v69/i16/e165107) reported that they
   obtained the right crystal field splitting using (LDA+U, U=6 eV) from
   WIEN2k.   So we wonder if we might missed something in the
   calculations?
  
   Thanks  in advance for your help,



[Wien] Crystal field splitting in empty 3d band of Fe2O3

2009-09-16 Thread Pavel Novak
Dear Yang Ding,

care is needed when estimating the crystal field splitting from the LDA+U 
calculation using the DOS. There are two reasons for it. First, the LDA+U 
lower the energy of more occupied states and increase the energy of less 
occupied states. Even if the bands are above Fermi energy, they contain 
nonzero fraction of electrons (cf :QTL in scf file), which is different 
for eg and t2g states, hence LDA+U distorts the splitting. Second, the 
selfinteraction of the d-electrons is present, again distorting the 
crystal field splitting.

Regards
Pavel Novak

On Tue, 15 Sep 2009, Yang Ding wrote:

 Dear WIEN2k  users,
 
 I am really new to WIEN2k, and wondering if you could give your advice and
 experience on following question concerning the crystal filed splitting
 calculated from WIEN2k.
 
 In order to understand if the pre-edge splitting appearing in the Fe K-edge
 spectra (1s-4p transition) measured by emission-XANES on Fe2O3 [Groot et al.
 J. Phys.: Condens. Matter 21 (2009) 104207
 http://www.iop.org/EJ/abstract/0953-8984/21/10/104207/], is linked to
 crystal-filed splitting in 3d empty band. We did a very preliminary ground
 state calculation using WIEN2k based on GGA+U (and LSDA+U) with U = 4 eV
 structure to check the crystal field splitting in empty d band above Fermi
 level.
 
 As a result, we found that above 2-6 eV above Fermi level, the energy of t2g
 is higher than that of eg. This result is similar to what reported by Rollsman
 et al (PHYSICAL REVIEW B 69, 165107 (2004)
 http://prola.aps.org/abstract/PRB/v69/i16/e165107) on Fe2O3. In his
 calculation (GGA/LSDA+U , U= 4eV), the energy of t2g is also higher than that
 of eg. So my question is why the t2g and eg are reversed in DFT, but the
 Multiplet calculation gives contradictory results (i.e from Groot et al.).
 
 I noticed that  Glatzel et al (PHYSICAL REVIEW B 77, 115133 (2008)
 http://prola.aps.org/abstract/PRB/v69/i16/e165107) reported that they
 obtained the right crystal field splitting using (LDA+U, U=6 eV) from
 WIEN2k.   So we wonder if we might missed something in the calculations?
 
 Thanks  in advance for your help,
 

-- 


[Wien] Crystal field splitting in empty 3d band of Fe2O3

2009-09-15 Thread Yang Ding
Dear WIEN2k  users,

I am really new to WIEN2k, and wondering if you could give your advice 
and experience on following question concerning the crystal filed 
splitting calculated from WIEN2k.

In order to understand if the pre-edge splitting appearing in the Fe 
K-edge  spectra (1s-4p transition) measured by emission-XANES on Fe2O3 
[Groot et al. J. Phys.: Condens. Matter 21 (2009) 104207 
http://www.iop.org/EJ/abstract/0953-8984/21/10/104207/], is linked to 
crystal-filed splitting in 3d empty band. We did a very preliminary 
ground state calculation using WIEN2k based on GGA+U (and LSDA+U) with U 
= 4 eV structure to check the crystal field splitting in empty d band 
above Fermi level.

As a result, we found that above 2-6 eV above Fermi level, the energy of 
t2g is higher than that of eg. This result is similar to what reported 
by Rollsman et al (PHYSICAL REVIEW B 69, 165107 (2004) 
http://prola.aps.org/abstract/PRB/v69/i16/e165107) on Fe2O3. In his 
calculation (GGA/LSDA+U , U= 4eV), the energy of t2g is also higher than 
that of eg. So my question is why the t2g and eg are reversed in DFT, 
but the Multiplet calculation gives contradictory results (i.e from 
Groot et al.).

I noticed that  Glatzel et al (PHYSICAL REVIEW B 77, 115133 (2008) 
http://prola.aps.org/abstract/PRB/v69/i16/e165107) reported that they 
obtained the right crystal field splitting using (LDA+U, U=6 eV) from 
WIEN2k.   So we wonder if we might missed something in the calculations?

Thanks  in advance for your help,
-- 

Yang Ding 
http://www.aps.anl.gov/Users/Scientific_Interest_Groups/HPSynC/people/%7EYDing.html

Staff Scientist

RM-B3180/Blgd-401

HPSynC at Advanced Photon Source

Argonne National Laboratory

9700 S. Cass Avenue

Argonne, IL 60439

Phone: 630-252-6288

Email: yangding at aps.anl.gov

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