mirror of https://gitlab.com/QEF/q-e.git
Documentation update. PLEASE CHECK IF THE CHANGES TO THE SPIN-POLARIZED
CASES ARE CORRECT. What is the difference between "multiplicity" and "tot_magnetization", by the way ? git-svn-id: http://qeforge.qe-forge.org/svn/q-e/trunk/espresso@3081 c92efa57-630b-4861-b058-cf58834340f0
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Doc/CREDITS
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Doc/CREDITS
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@ -29,7 +29,6 @@ The web site for PWSCF and related codes is: http://www.pwscf.org/
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The CP code is based on the original code written by
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Roberto Car and Michele Parrinello.
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CP was developed by Alfredo Pasquarello (IRRMA, Lausanne), Kari
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Laasonen (Oulu), Andrea Trave (LLNL), Roberto Car (Princeton),
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Nicola Marzari (MIT), Paolo Giannozzi, and others.
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@ -47,6 +46,13 @@ the original code by Paolo Giannozzi.
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The input/output toolkit "iotk" (http://www.s3.infm.it/iotk)
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was written by Giovanni Bussi (S3 Modena).
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The calculation of the finite (imaginary) frequency molecular
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polarizability using the approximated Thomas-Fermi + von Weizaecker
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scheme was contributed by Huy-Viet Nguyen (Sissa),
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The BlueGene porting was done by Costas Bekas and Alessandro Curioni
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(IBM Zurich).
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A list of further contributors includes:
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Dario Alfe', Francesco Antoniella, Mauro Boero, Nicola Bonini,
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Claudia Bungaro, Paolo Cazzato, Davide Ceresoli, Gabriele Cipriani,
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@ -54,7 +60,7 @@ Matteo Cococcioni, Cesar Da Silva, Alberto Debernardi, Gernot Deinzer,
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Oswaldo Dieguez, Andrea Ferretti, Ralph Gebauer, Martin Hilgeman,
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Eyvaz Isaev, Yosuke Kanai, Axel Kohlmeyer, Konstantin Kudin,
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Michele Lazzeri, Sergey Lisenkov, Kurt Maeder, Francesco Mauri,
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Nicolas Mounet, Huy-Viet Nguyen, Pasquale Pavone, Mickael Profeta, Guido Roma,
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Nicolas Mounet, Pasquale Pavone, Mickael Profeta, Guido Roma,
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Manu Sharma, Alexander Smogunov, Kurt Stokbro, Pascal Thibaudeau,
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Antonio Tilocca, Paolo Umari, Renata Wentzcovitch, Malgorzata Wierzbowska,
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Xiaofei Wang, Yudong Wu, and let us apologize to everybody we have forgotten.
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57
Doc/INPUT_PW
57
Doc/INPUT_PW
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@ -267,16 +267,6 @@ nosym LOGICAL ( default = .FALSE. )
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of the lattice. Use with care in low-symmetry large cells
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if you cannot afford a k-point grid with the correct symmetry.
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starting_magnetization(i)
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REAL
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starting spin polarization (values between -1 and 1)
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on atomic type 'i' in a lsda calculation. Breaks the
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symmetry and provides a starting point for self-consistency.
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The default value is zero, BUT a value MUST be specified for
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AT LEAST one atomic type in spin polarized calculations.
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If zero starting magnetization is specified, zero final
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magnetization will be obtained.
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occupations CHARACTER
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'smearing': gaussian smearing for metals
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requires a value for degauss
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@ -305,17 +295,45 @@ smearing CHARACTER
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'fermi-dirac', 'f-d', 'fd':
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smearing with Fermi-Dirac function
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nelup, neldw REAL
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number of spin-up and spin-down electrons, respectively
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The sum must yield nelec that must also be specified
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explicitly in this case.
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nspin INTEGER
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nspin = 1 : non-polarized calculation (default)
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nspin = 2 : spin-polarized calculation
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nspin = 2 : spin-polarized calculation, LSDA
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(magnetization along z axis)
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nspin = 4 : spin-polarized calculation, noncolinear
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(magnetization in generic direction)
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DO NOT specify nspin in this case;
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specify "noncolin=.TRUE." instead
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noncolin LOGICAL
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if .true. the program will perform a noncollinear calculation.
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DEFAULT: .false.
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starting_magnetization(i)
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REAL
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starting spin polarization (values between -1 and 1)
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on atomic type 'i' in a spin-polarized calculation.
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Breaks the symmetry and provides a starting point for
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self-consistency. The default value is zero, BUT a value
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MUST be specified for AT LEAST one atomic type in spin
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polarized calculations. Note that if start from zero
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initial magnetization, you will get zero final magnetization
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in any case. If you desire to start from an antiferromagnetic
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state, you may need to define two different atomic species
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corresponding to sublattices of the same atomic type.
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If you fix the magnetization with "nelup/neldw" or with
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"multiplicity" or with "tot_magnetization", you should
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not specify starting_magnetization
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nelup, neldw REAL
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number of spin-up and spin-down electrons, respectively
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Note that this fixes the final value of the magnetization.
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The sum must yield nelec that must also be specified
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explicitly in this case. Not valid for spin-unpolarized
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or noncolinear calculations, only for LSDA. Obsolescent.
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multiplicity INTEGER ( default = 0 [unspecified] )
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spin multiplicity (2s+1). 1 is singlet, 2 for doublet etc.
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Note that this fixes the final value of the magnetization.
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if unspecified or a non-zero value is specified in nelup/neldw
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then multiplicity variable is ignored.
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@ -399,17 +417,16 @@ eamp REAL ( default = 0.001 a.u. )
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Amplitude of the electric field (in a.u.)
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( 1 a.u. = 51.44 10^10 V/m )
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noncolin LOGICAL
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if .true. the program will perform a noncollinear calculation.
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DEFAULT: .false.
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angle1(i) REAL
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The angle expressed in degrees between the initial
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magnetization and the z-axis. I runs over the atom types.
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magnetization and the z-axis. For noncolinear calculations
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only. I runs over the atom types.
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angle2(i) REAL
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The angle expressed in degrees between the projection
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of the initial magnetization on x-y plane and the x-axis.
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For noncolinear calculations only.
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constrained_magnetization CHARACTER ( defalt = 'none' )
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Used to perform constrained calculations in magnetic systems
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@ -195,6 +195,9 @@ The calculation of the finite (imaginary) frequency molecular
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polarizability using the approximated Thomas-Fermi + von Weiz\"acker
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scheme was contributed by Huy-Viet Nguyen (Sissa),
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The BlueGene porting was done by Costas Bekas and Alessandro Curioni
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(IBM Zurich).
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\hyphenation{fran-ce-sco}
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\hyphenation{ce-re-so-li}
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An alphabetical list of further contributors includes:
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