[Wien] DOS of slab

2017-04-29 Thread emami seyyed amir abbas
Dear users.

I am trying to calculate the electronic and magnetic properties of a thin film. 
I created a slab of 5 monolayer and run the scf. I desire to obtain the DOS of 
the just  top monolayer but there is no option in DOS program for this task. In 
DOS program i can plot DOS just for specific atom not layer.

best regards.

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[Wien] optic (transitions)

2016-10-15 Thread emami seyyed amir abbas
Dear users

I obtained dielectric function curve (both real and imaginary). There are some 
peaks in imaginary part of dielectric function which correspond to transition 
on its band structure. How can i specify which transition in bands correspond 
to those peaks? 

Thanks in advance.
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[Wien] intra-band contribution

2016-06-28 Thread emami seyyed amir abbas
Dear users

I am interested in obtaining dielectric curve as a function of energy by 
considering intra-band contribution for a half metal compound. I follow these 
steps:
1- x joint (mode=6) --- obtaining plasma frequencies for both spin up and down 
which is written in .ouputjoint (up/dn)
2- x joint (mode=4)
3- addjoint-updn
4- x kram (putting plasma frequencies from step 1)

but in step 4, we should insert just one plasma frequency while for half metals 
the value of plasma frequency for spin up and dn are differnt. Now what is the 
appropriated value for this input.

thank you in advance. 
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[Wien] optic-tetra value

2016-06-22 Thread emami seyyed amir abbas

Dear users.

I  am trying to obtain optical properties of a half-metal compound. As i  know 
for metallic systems we should put tetra/with value=101. But in  half-metal 
systems one spin channel has metallic behavior and other has  insulator or 
semiconductor behavior. Accordingly, which value will be  appropriated for this 
input.
 
Thank you in advance for your attention to this matter  ___
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[Wien] changing EXC-POT

2016-01-27 Thread emami seyyed amir abbas
dear users


I am trying to obtain electronic properties of a compound by using two exchange 
potential (pbe and engel-vosko). I first run a calculation by use GGA now is it 
possible to i just save the calculation, change the potential in case.in0 and 
re-run the calculation. i mean is it possible to use the old calculation and 
old .CLM for new potential. 
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[Wien] lattice change mBJ+SO

2015-12-25 Thread emami seyyed amir abbas
Dear users 

I am trying to run mBJ+SO for a cubic structure. Also i need to investigate the 
effect of lattice change on its magnetic properties. As i know for GGA 
calculation, i can just change the lattice and again run_lapw. But for mBJ we 
need some initialization. By this explanation, is it possible for mBL+SO to 
just change the lattice and again run_lapw without re-initializing. 

regards
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[Wien] spin-polarize BoltzTraP

2015-11-28 Thread emami seyyed amir abbas

 
 
 
 
 Dear users

I am trying to obtain transport properties of a half metal by Boltztrap. As it 
has been reported in the following article
  J. Phys. D: Appl. Phys. 42 (2009) 084003 (11pp)
for this calculation, they used a modified Boltztrap code to handle both spin 
up and dn simultaneously. Now i am wondering how can i do this? 

Thank you in advance for any help you can provide
 

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Re: [Wien] gather_energy

2015-11-26 Thread emami seyyed amir abbas

 
 Thank you dears Elias and Gavin.
 

 

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[Wien] #case.intranse

2015-11-26 Thread emami seyyed amir abbas

 
 
 
 Dear users

I am trying to obtain transport properties of a magnetic material by BoltZtrap. 
 In case.intrans need to specify the valence electron. Now in spin polarize 
calculation,what did it mean the valence electron? As i know for every spin i 
must run boltztrap separately. the valence electron in case.intrans must be the 
total of spin up and dn or for every spin calculation it must insert the 
corresponding number of spin electron.  ___
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[Wien] BoltzTraP

2015-11-25 Thread emami seyyed amir abbas

 
 Dear users


I am trying to obtain transport properties of a magnetic material by BoltZtrap. 
In case.intrans need to specify the valence electron.
Now in spin polarize calculation, the valence electron must split to up and dn 
or the total valence electron must insert.


thanks. 

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[Wien] gather_energy

2015-11-25 Thread emami seyyed amir abbas

 Dear users

I am trying to construct the case.energy as an input file for BlotZtraP. My 
normal calculations were performed in parallel. Now I want to use 
gather_energy.pl to generate case.energy. Now, how can i run this program. What 
is the command for doing this?

thanks
 

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[Wien] error-irrep

2015-10-29 Thread emami seyyed amir abbas

  Dear users

I  am trying to represent band structures in irreducible  representation.  The 
space group of compound is 221 and spin-orbit interaction is  included (RLO is 
not included). I run the following sequence of programs for obtaining band  
structures:

x lapw1 -band -up -p
x lapw1 -band -up -p
x lapwso -up -p
x irrep -up -so -p
x spaghetti -up -so -p

but  in the output only case.outputirsoup was ceated and within this file  this 
expression "X not equal for all elements in the class" was  appeared. Also when 
I run spaghetti this error "ERROR: irrep  inconsistency:no of egval 1" was 
appeared. For more details i attached  the case.outputirsoup file. 

Thank you in advance 

### 2015-10-27  15:59:39

 Title   
 Plattice
 Symmorphic crystal with inversion symmetry
 Complex eigenfunctions
 Spin-orbit eigenfunctions (->;time inversion)
 Spin-polarization


 Transformations:
 From k-list in lapw1 to Cartesian coord. system (BR1)
 1. 0. 0.
 0. 1. 0.
 0. 0. 1.

 From k-list in lapw1 to prim. reciprocal space  (DB1)
 1. 0. 0.
 0. 1. 0.
 0. 0. 1.

 

SYMMETRY OPERATIONS Pi={Ri|taui+tm}
  Ri taui   inv(Ri) Ri(Cartesian coord)  Eulers angles  spin transf.

 1 0 0   0.000   1 0 0   1.000 0.000 0.000   0.000
 0 1 0   0.000   0 1 0   0.000 1.000 0.000   0.000  ( 1.000 0.000)( 0.000 0.000)
 0 0 1   0.000   0 0 1   0.000 0.000 1.000   0.000  ( 0.000 0.000)( 1.000 0.000)
   1 (E)
unity op.   
rotation through ( 1.000, 0.000, 0.000)
 
-1 0 0   0.000  -1 0 0  -1.000 0.000 0.000   0.000
 0-1 0   0.000   0-1 0   0.000-1.000 0.000   3.142  ( 0.000 1.000)( 0.000 0.000)
 0 0 1   0.000   0 0 1   0.000 0.000 1.000   0.000  ( 0.000 0.000)( 0.000-1.000)
   2 (C2)
180-degree rotation
rotation through ( 0.000, 0.000, 1.000)
 
 0-1 0   0.000   0 1 0   0.000-1.000 0.000   0.000
 1 0 0   0.000  -1 0 0   1.000 0.000 0.000   4.712  ( 0.707-0.707)( 0.000 0.000)
 0 0 1   0.000   0 0 1   0.000 0.000 1.000   0.000  ( 0.000 0.000)( 0.707 0.707)
   3 (C4)
90-degree rotation
clockwise rotation through ( 0.000, 0.000, 1.000)
 
 0 1 0   0.000   0-1 0   0.000 1.000 0.000   0.000
-1 0 0   0.000   1 0 0  -1.000 0.000 0.000   1.571  ( 0.707 0.707)( 0.000 0.000)
 0 0 1   0.000   0 0 1   0.000 0.000 1.000   0.000  ( 0.000 0.000)( 0.707-0.707)
   4 (C4)
90-degree rotation
counterclockwise rotation through ( 0.000, 0.000, 1.000)
 
-1 0 0   0.000  -1 0 0  -1.000 0.000 0.000   0.000
 0-1 0   0.000   0-1 0   0.000-1.000 0.000   0.000  ( 1.000 0.000)( 0.000 0.000)
 0 0-1   0.000   0 0-1   0.000 0.000-1.000   0.000  ( 0.000 0.000)( 1.000 0.000)
   5 (I)
inverse op. 
rotation through ( 1.000, 0.000, 0.000)
 
 1 0 0   0.000   1 0 0   1.000 0.000 0.000   0.000
 0 1 0   0.000   0 1 0   0.000 1.000 0.000   3.142  ( 0.000 1.000)( 0.000 0.000)
 0 0-1   0.000   0 0-1   0.000 0.000-1.000   0.000  ( 0.000 0.000)( 0.000-1.000)
   6 (IC2)
180-degree rotation times inversion
rotation through ( 0.000, 0.000, 1.000)
 
 0 1 0   0.000   0-1 0   0.000 1.000 0.000   0.000
-1 0 0   0.000   1 0 0  -1.000 0.000 0.000   4.712  ( 0.707-0.707)( 0.000 0.000)
 0 0-1   0.000   0 0-1   0.000 0.000-1.000   0.000  ( 0.000 0.000)( 0.707 0.707)
   7 (IC4)
90-degree rotation times inversion
clockwise rotation through ( 0.000, 0.000, 1.000)
 
 0-1 0   0.000   0 1 0   0.000-1.000 0.000   0.000
 1 0 0   0.000  -1 0 0   1.000 0.000 0.000   1.571  ( 0.707 0.707)( 0.000 0.000)
 0 0-1   0.000   0 0-1   0.000 0.000-1.000   0.000  ( 0.000 0.000)( 0.707-0.707)
   8 (IC4)
90-degree rotation times inversion
counterclockwise rotation through ( 0.000, 0.000, 1.000)
 
-1 0 0   0.000  -1 0 0  -1.000 0.000 0.000   3.142
 0 1 0   0.000   0 1 0   0.000 1.000 0.000   0.000  ( 0.000 0.000)( 1.000 0.000)
 0 0-1   0.000   0 0-1   0.000 0.000-1.000   0.000  (-1.000 0.000)( 0.000 0.000)
   9 (C2)
180-degree rotation
rotation through ( 0.000, 1.000, 0.000)
 
 1 0 0   0.000   1 0 0   1.000 0.000 0.000   3.142
 0-1 0   0.000   0-1 0   0.000-1.000 0.000   3.142  ( 0.000 0.000)( 0.000-1.000)
 0 0-1   0.000   0 0-1   0.000 0.000-1.000   0.000  ( 0.000-1.000)( 0.000 0.000)
  10 (C2)
180-degree rotation
rotation through ( 1.000, 0.000, 0.000)
 
 0 1 0   0.000   0 1 0   0.000 1.000 0.000   3.142
 1 0 0   0.000   1 0 0   1.000 0.000 0.000   1.571  ( 0.000 0.000)( 0.707 0.707)
 0 0-1   0.000   0 0-1   0.000 0.000-1.000   0.000  (-0.707 0.707)( 0.000 0.000)
  11 (C2)
180-degree rotation
rotation through ( 0.707, 0.707, 0.000)
 
 0-1 0   0.000   0-1 0   0.000-1.000 0.000   3.142
-1 0 0   0.000  -1 0 0  -1.000 0.000 0.000   4.712  ( 0.000 0.000)(-0.707 0.707)
 0 0-1   0.000   0 0-1   0.000 0.000-1.000   0.000  ( 0.707 0.707)( 0.000 0.000)
  12 (C2)
180-degree rotation
rotation through ( 0.707,-0.707, 0.000)
 
 1 0 0   0.000   1 0 0   1.000 0.000 0.000   3.142
 0-1 0   0.000   0-1 0   0.000-1.000 0.000   0.000  ( 0.000 0.000)( 1.000 0.000)
 0 0 1   0.000   0 0 1   0.000 0.000 1.000   0.000  (-1.000 0.000)( 

Re: [Wien] Band labeling

2015-10-26 Thread emami seyyed amir abbas

  Thank you very much for your helpful responds.

What i realized is that for obtaining more details such as band labeling i need 
to run irrep. As you said for topological characterization, it is necessary to 
obtain band structures in irreducible representation. Is there any difference 
in shape of bands between normal band and ones obtained in irreducible? In 
other words why you mentioned it is requires to plot the bands in irreducible 
representations. I will be very grateful if i find my answer. 

Thanks
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[Wien] Band labeling

2015-10-25 Thread emami seyyed amir abbas
Dear users

I am trying to label the band structures (i.e. gamma 6, gamma 7 etc). In fact, 
for investigation of the topological properties of compounds, it is required to 
specify the band index. Now how can i label the band structures? Any 
suggestions will be appreciate in advanced.
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[Wien] Im_eps

2015-09-29 Thread emami seyyed amir abbas
ِDear users 

I am trying to obtain imaginary and real part of Dielectric function. As i know 
these information can be find in case.joint and case.epsilon but the  Im_eps_xx 
which is in both file have a different value. What is the reason of this 
discrepancy?

Regards
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