Pseudopotential calculations of Porphyrin Complexes…
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Transcript of Pseudopotential calculations of Porphyrin Complexes…
Japan Advanced Institute of Science and Technology,
Kanazawa, Japan.
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Kanazawa
Tokyo
Pseudopotential calculations of Porphyrin Complexes…
TTI2007@Tuscany, Italy.
Ryo Maezono
School of Information Science,
Aim
N
N
N
N
TM = Ni, Cu, Zn
TM
Establish procedures for pseudo-pot. QMC calculations.
Porphyrin, Phthalocyanine etc.
- Actively studied in Nano/Bio research field. - Interplay between TM site and Side-chains.
- prepare trial/guiding WF in pseudo-pot. calc.
- Basis set re-optimization.
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suitable for stable DMC accumulation.
People involved…
- Mr. Jun Koseki
QMC code implementation.
- Prof. Richard Needs group
(CASINO ; QMC code.)
- Prof. Masanori Tachikawa
- Ryo MAEZONO.QuickTime˛ Ç∆TIFFÅià≥èkǻǵÅj êLí£ÉvÉçÉOÉâÉÄǙDZÇÃÉsÉNÉ`ÉÉÇ å©ÇÈÇΩÇflÇ…ÇÕïKóvÇ≈Ç∑ÅB
Gaussian SCF calc./ structure optimization.
Basis set optimization / QMC calc.
Background (1)
John’s Pseudo potential studies.- Non-diverging, non-local pseudo potentials.
avoiding eN-cusp. Fock exchange.
- Transition metal ions…s-electrons coexist with d-electrons.→ Difficulty!
John investigated long-range tail.
Asymptotic behavior of orbital functions.
Valence electron but not HOMO
…then wrong behavior…
Trail-Needs ( 2005) , Dolg ( 2005)
Lee-Needs ( 2002)
Ovacharenko-Lester ( 2001)
‘QMC_pp’
Pathology due to Non-locality
€
rcNorm-conserving
Fock non-locality
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Vlpp r→ ∞( ) ~
Zeffr
€
Zeff +δ l( )
r+η l
Pseudo orb.
AE orbital
John investigated …Asymptotic behavior of orbital functions.
Valence electron but not HOMO…then wrong behavior…
J. Trail et.al., JCP 122, 174109 (2005).
→ continuously taken over by outside.Zeff r
‘4s’-orb. of TM ion.3d is HOMO above 4s
N
N
N
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TM = Ni, Cu, Zn
TM
Interesting test case
Establish procedures for pseudo-pot. calculations.
Porphyrin, Phthalocyanine etc.
- Actively studied in Nano/Bio Science. - Interplay between TM site and Side-chains.
- Generate trial/guiding WF in pseudo-pot. calc. - Basis set re-optimization.
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suitable for stable DMC accumulation.
Gaussian basis set with JRT pseudo.
commonly used in Molecular Science, Bio-molecule bussiness as well.
MDT has rich experiences on this.
‘Billy’ utility (his first script with mysterious name)
Conventional pseudo pot. provided with preset basis set.
(such as LANL2DZ etc.)
not fully optimized but well calibrated. ‘This basis set can be reliable upto XXX digit’
→ Basis set optimization by ourselves.
How to setup the basis set for JRT pseudo?
preparation of proper basis set.
Gaussian basis calculation with JRT pseudo.
Lighter Ions.
Practical calculations after JRT2005
I. Gurtubay et.al., JCP 124, 024318 (2006).
She used ‘Billy’ utility for basis set optimization.
→ Basis set optimization manually.
TM Ions.
- Porphyrin calculations.
- See how’s going on TM pseudo by John’s remedy.
The system is too large to be dealt with ‘Billy’.
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TM = Ni, Cu, Zn
TM
<Aim>
ProcedureLANL1DZ the same core size as JRT pseudo.
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<Porphin>
Re-optimize H,C,N basis set @ porphin.
TM = Ni, Cu, Zn
TMN
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N
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<Porphyrin>Replace TM Pseudo (from LANL to JRT)
QMC_pp(TM)
Re-optimize TM basis set
Structure optimization in B3LYP
H,C,N are treated as AE (6-31G**).
QMC_pp(all)
Replace AE by JRT-Pseudo.
TM
Basis Set optimization (TM)
<Ni@NiPo
>
Initial -1020.612(LANL1DZ)
- From inner most to outer, d(inner) most effective.
-1021.036Optimized (hartree)
- Gaussian exponents are optimized in HFSCF.
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N
N
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<Porphyrin>
Ni
s(3), p(2), and d(5)
-1020.970Uncontracted 3*s(1), 2*p(1), and 5*d(1)
(hartree)
Basis Set optimization (C, N, H)
<Lighter atoms @ Porphin>
Initial -154.242(6-31G**)
-155.612Optimized (hartree)
(※LANL1D2)
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N
Energy difference“Not depending on Core size ”
€
ΔE
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-0.16894
0.22476Optimized
JRT pseudoInitial with LANL1DZ
(c.f. 0.29691 by AE)
of NiPo
€
ΔE
(hartree)
TM
TM… similar as ‘binding energy’
QMC calculations
(hartree)
HFSCF
Variational
-206.4994
B3LYP-212.7404
MP2-210.2612
Non-variational
VMC-210.693(1)
DMC-211.5698(9)
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N
N
NCu
Cu-Porphyrin [QMC_pp(all)]
Jastrow Functions…
JrR( ) ~F u( )
rR( )+ F χ( )
rR( )+ F f( )
rR( )
<ee> <en> <een>
- Fixed cutoff lengths ; Lu=5.0 a.u./ Lχ=4.0 a.u./ Lf=3.0 a.u./
- N.D.Drummond, M.D.Towler and R.J.Needs; Phys. Rev. B, 70, 235119 (2004)
- Optimization ; Unreweighted SC Variance Minimization. - N.D.Drummond and R.J.Needs; Phys. Rev. B, 72, 085124 (2005)
Energy differences
N
N
N
NCu
Cu-Porphyrin
Cu
0.39517
0.28371
0.21771
0.26160
AE
LANLsmall
LANLlarge
QMC_pp(TM)
0.42870
0.18091
0.17061
0.33397
0.25533 0.33404QMC_pp(all)
NotYet
NotYet
Unstable
0.249(2)
NotYet
NotYet
0.063(2)
0.178(2)
0.230(1) 0.170(1)
0.35248
0.20359
0.19622
0.29338
0.29309
B3LYP MP2 DMC OPTVMC HFSCF
(hartree)
reduced time step, Casula’s scheme, frequent updating.
Tendencies
Absolute values of energy
2 ha. (all) / 4 ha. (TM)B3LYP < DMC < MP2
Energy Diff. ( ‘binding’ )
MP2 < B3LYP < DMC
[TMPo/Atom/Po] [QMCpp(TM)/QMCpp(all)]
€
⊗
MP2 < DMC <B3LYP
Only for NiPo,
※ QMC not variational here.
B3LYP, DMC, MP2
Notes
- Atomic calculation of Zn with LANL.
VARMIN (CASINO v 1.8.2)
→ Try with latest CASINO with emin/madmin??
Though it is QUITE simple system,
won’t run even with reduced parameters into one.
SummaryReplacing procedure of QMC pseudo potentials
suitable for stable DMC accumulation.
LANL pseudo/basis set … easy to get and calculate in SCF.
No stable DMC
as it is
Stable DMC accumulation.
replace with JRT pseudo re-optimization of basis set
δE~0.001 hartree
High Performance Computing Facilities…
* Cray; T3E,XT3
* SGI; Origin2000,Origin3000,Altix3700,Altix4700
* Clusters; Pentium3,Opteron,Macintosh(Xeon)
* IBM; SP3, p690.
* HP; GS320, ES40, ES45, GS1280
* Hitachi; SR11000
* Fujitsu; PrimePower,PrimeQuest
Architectures
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@JAIST (360 procs) - SGI Altix
Itanium2, 24GB/4cpu
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- Cray XT3Opteron150, 32GB/4cpu
@JAIST (128 procs)
- Hitachi SR11000IBM Power5+, 128GB/16cpu
@Hokkaido Univ. (640 procs)
- Macintosh @JAIST (96 procs, my own!)
Xeon, 16GB/4cpu