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國立中正大學 化學暨生物化學研究所 博士論文口試 孫翊倫 (Yi-Lun Sun) 指導教授:胡維平 (Wei-Ping Hu) 中華民國 101 年 7 月 10 日. Content. Chapter 1 Accurate Multi-Coefficient Electronic Structure Methods MLSE( C n )-DFT for Thermochemical Kinetics Chapter 2 - PowerPoint PPT Presentation
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Content• Chapter 1
Accurate Multi-Coefficient Electronic Structure Methods MLSE(Cn)-DFT for Thermochemical Kinetics
• Chapter 2A New Set of Accurate Multi-level Methods Including Parameterization for Heavy Elements
• Chapter 3 Theoretical Prediction of Stable Noble-Gas Anions XeNO2
- and XeNO3
- with very Short Xenon-Nitrogen Bond Lengths
2博士論文口試
Content• Chapter 4
Theoretical Prediction of A New Class of Xenon Containing Molecules and Anions NXeOnFm
• Chapter 5Theoretical Study on the Excited State Dynamics of Phenol Chromophores
Chapter 6Theoretical Prediction of A New Type Xe Polymer
博士論文口試
• Chapter 2A New Set of Accurate Multi-level Methods Including Parameterization for Heavy Elements
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Tyrosine
博士論文口試
Tyrosine, one of the 22 amino acids that are used by cells to synthesize proteins.
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Fluorescence?
博士論文口試
The so-called photostability prevents the undesired photochemical reactions for these molecules upon the irradiation with ultraviolet photons.
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methods
• Geometry:B3LYP/6-311+G**
• PES: TD B3LYP/6-311+G**CAS/6-31+G**
• Program:Gaussian 03/09Molpro 2010
博士論文口試 9
Conclusions• Recent theoretical
calculations suggested that the low fluorescence quantum yield for phenol was due to dissociation from an excited electronic state potential energy surface.
博士論文口試 21
Sobolewski, A. L.; Domcke, W. Chem. Phys. 2000, 259, 181.
Conclusions• For various conformers of HBA
and HAP without intramolecular hydrogen bonding, the second excited state is a repulsive state. It crosses 2A' at short O-H bond distance and crosses 1A' at large O-H bond distance.
• Hydrogen atom elimination can occur easily on this repulsive potential energy surface.
博士論文口試 23
Conclusions• For all the MOBA, the second
excited state is a repulsive state. It crosses 2A' at short O-C bond distance and crosses 1A' at large O-C bond distance.
• CH3 group elimination can occur easily on this repulsive potential energy surface.
博士論文口試 24
Conclusions• For conformers of 2-HBA and 2-
HAP with intramolecular hydrogen bonding, the formation of intramolecular hydrogen bonding reduces the ground state (1A') energy significantly at large O-H distances due to the formation of zwitterionic species and avoids the intersecting with the 1A" state.
• No H atom elimination analogous to that of phenol was observed
博士論文口試 25
SchrödingerEquation
Electron correlation →
Basis set Type
3-21G
6-31+G**
aug-cc-pVDZ
aug-cc-pVTZ
aug-cc-pVQZ
HF MP2 MP3 MP4 QCISD(T) … Full CI
… … … … … … …
∞
Quantum Chemical Calculations
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●●
博士論文口試
• Example:MP2/aug-cc-pVDZQCISD(T)/aug-cc-pVTZ
• Deficiencies:1. Low accuracy2. Cost expensive
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Single Level Methods
博士論文口試
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Error of the reaction energy :CH4 + Cl2 → CH3Cl + HCl, Erxn = -23.1 kcal/molMP2/aug-cc-pVDZ : 8.1 kcal/molQCISD(T)/aug-cc-pVTZ : 1.9 kcal/mol
CH4 → C + 4 H (atomization energy) , Erxn = 420.1 kcal/molMP2/aug-cc-pVDZ : 25.6 kcal/molQCISD(T)/aug-cc-pVTZ : 6.0 kcal/mol
MP2/aug-cc-pVDZ > 5 kcal/molQCISD(T)/aug-cc-pVTZ > 1 kcal/mol
Single Level Methods
博士論文口試
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Cost :MP2/aug-cc-pVDZTime : 1 unit
QCISD(T)/aug-cc-pVTZTime : 288 units~ couple hours
Single Level Methods
博士論文口試
Popular Multi-level Methods: G1, G2, G3, G4
Multi-level Methods with Scaled Energies: (Multi-coefficient Method)
MCG3, G3S, G3SX , MLSEn+d
Multi-level Methods
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G3 & G3S• Geometry:MP2(full)/6-31G(d)• Ebase : MP4/6-31G(d)• ΔE+ : MP4/6-31+G(d) - Ebase• Δ E2df,p : MP4/6-31G(2df,p) – Ebase• Δ EQCI : QCISD(T)/6-31G(d) – Ebase• Δ EG3Large : MP2(full)/G3Large – [ MP2/6-31G(2df,p) +MP2/6-
31+G(d) – MP2/6-31G(d) ]• Δ EHLC : – Anβ – B(nα – nβ)
E(G3)= Ebase + ΔE+ + ΔE2df,p + ΔEQCI + ΔEG3Large + ΔEHLC + EZPE
Journal of Chemical Physics, 1998, 109, 7764-7776 32
C1 C2 C3 C4
博士論文口試
The MLSE(C1)-DFT Method• E(MLSE(C1)-DFT) = CWF { E(HF/pdz) +
CE2 [E2/pdz] +CE34SDQ [E(MP4SDQ/pdz) – E(MP2/pdz)] +CQCID [E(QCISD/pdz) – E(MP4SDQ/pdz)] +CQCI [E(QCISD(T)/pdz) – E(QCISD/pdz)] +CB1E2 [E2/ptz – E2/pdz] +CHF+ [E(HF/apdz) – E(HF/pdz]) +CE2+ [E2/apdz – E2/pdz] +CB2E2 [E2/aptz – E2/apdz] +CB1E34 [E(MP4D/ptz) – E(MP4D/pdz)] } +(1 - CWF ) { E(DFTX/pdz) + CDFT+ [E(DFTX/apdz – DFTX/pdz] } .
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Chem. Phys. Lett. 2009, 475, 141. 博士論文口試
Database
MGAE109 Database. 109 atomization energies (AEs).
IP13 and EA13 Database. 13 IPs and 13 EAs
HTBH38 Database. 38 transition state barrier heights for hydrogen transfer (HT) reactions.
Training sets
NHTBH38 Database. 38 transition state barrier heights for non-hydrogentransfer(NHT) reactions.
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Computational Cost
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Cost MUE (kcal/mol)
MP2/aug-cc-pVDZ 1 15.1
MLSE(C1)-M06-2X 70 0.56
MLSE(C2)-M06-2X 50 0.59
MLSE(C3)-B3LYP 25 0.62
MLSE-TS 25 0.61
QCISD(T)/aug-cc-pVTZ 288 6.11
M06-2X/aug-cc-pVTZ 16 1.89
博士論文口試
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CH4 + Cl2 → CH3Cl + HCl , Erxn = -23.1 kcal/mol
MP2/aug-cc-pVDZ : 8.1 kcal/molQCISD(T)/aug-cc-pVTZ : 1.9 kcal/molMLSE(C1)-M06-2X : 1.0 kcal/mol
CH4 → C + 4 H (atomization energy) , Erxn = 420.1 kcal/mol
MP2/aug-cc-pVDZ : 25.6 kcal/molQCISD(T)/aug-cc-pVTZ : 6.0 kcal/molMLSE(C1)-M06-2X : 0.13 kcal/mol
Accuracy
博士論文口試
For Heavy Elements?
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CH4 + I2 → CH3I + HI , Erxn= 13.1 kcal/molQCISD(T)/aug-cc-pVTZ : 4.7 kcal/molMLSE(C1)-M06-2X : 2.7 kcal/mol
I2 → 2 I , Erxn= 35.9 kcal/molQCISD(T)/aug-cc-pVTZ : 5.4 kcal/molMLSE(C1)-M06-2X : 4.3 kcal/mol
博士論文口試
New Database
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unit:kcal/mol AE AE IP
I2 35.87 HBr 90.51 I 241.01
HI 73.79 NOBr 181.64 Br 272.43
IBr 42.27 CH3I 369.12 EA
ICl 50.19 CH3Br 380.94 I 70.54
Br2 45.90 C2H5I 662.69 Br 77.60
博士論文口試
MLSE(C1)-M062X
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(unit : kcal/mol) MUE(225)
HHAE(10)
HHIP(2)
HHEA(2)
MLSE(C1)-M062X(Eso) 0.66 1.84 1.22 2.21
MLSE(C1)-M062X-HA 0.66 1.66 1.21 2.30
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SCS-MP2
CE2S[(E2aa+E2bb)/pdz] +CE2O [(E2ab)/pdz] +CE2+S [(E2aa+E2bb)/apdz] +CE2+O [(E2ab)/apdz] +CB1E2S [(E2aa+E2bb)/ptz] +CB1E2O [(E2ab)/ptz] +CB2E2S [(E2aa+E2bb)/aptz] +CB2E2O [(E2ab)/aptz] +
The different scaling factors were used to the same spin and opposite spin perturbational terms (MP2).
博士論文口試
New Database
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unit : kcal/mol AE AE IP
I2 35.87 HBr 90.51 I 241.01
HI 73.79 NOBr 181.64 Br 272.43
IBr 42.27 CH3I 369.12 EA
ICl 50.19 CH3Br 380.94 I 70.54
Br2 45.90 C2H5I 662.69 Br 77.60
博士論文口試
Accuracy
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(unit : kcal/mol) MUE(225)
HHAE(10)
HHIP(2)
HHEA(2)
MLSE(C1)-M062X(Eso) 0.66 1.84 1.22 2.21
MLSE(C1)-M062X-HA 0.66 1.66 1.21 2.30
MLSE(HA-1) 0.58 0.87 0.49 1.07
MLSE(HA-2) 0.64 0.98 0.48 1.04
博士論文口試
Computational Cost
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(unit : kcal/mol) Cost MUE(211)
MUE(225)
HHAE(10)
MLSE(C1)-M062X 100% 0.56 0.66 1.66
MLSE(HA-1) 162% 0.56 0.58 0.87
MLSE(HA-2) 104% 0.62 0.64 0.98
博士論文口試
Results
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CH4 + I2 → CH3I + HI , Erxn= 13.1 kcal/molQCISD(T)/aug-cc-pVTZ : 4.7 kcal/molMLSE(C1)-M06-2X : 2.7 kcal/molMLSE(HA-1) : 0.5 kcal/molMLSE(HA-2) : 1.0 kcal/mol
I2 → 2 I , Erxn= 35.9 kcal/molQCISD(T)/aug-cc-pVTZ : 5.4 kcal/molMLSE(C1)-M06-2X : 4.3 kcal/molMLSE(HA-1) : 0.7 kcal/molMLSE(HA-2) : 0.6 kcal/mol博士論文口試
Conclusions
• The MLSE(C1)-M06-2X method provided the lowest overall MUE of 0.56 kcal/mol on the training set.
• Both MLSE(C1)-M06-2X (Eso) and MLSE(C1)-M06-2X-HA methods performed unsatisfactorily on the 10 heavy halogen containing atomization energies(>1 kcal/mol).
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Conclusions• MLSE(HA-1) and MLSE(HA-2) performed 0.58 and
0.64 kcal/mol on the MUE(225), with the MUE of HHAE(10) both less than 1 kcal/mol.
• MLSE(HA-1) method required 62% cost more than the MLSE(C1)-M06-2X method. But MLSE(HA-2) method only cost 4% more than the MLSE(C1)-M06-2X method.
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Acknowledgement• Prof. Wei-Ping Hu• Our group members.
(Tsung-Hui Li, Jien-Lian Chen et al.)• Department of Chemistry & Biochemistry,
National Chung Cheng University• National Science Council• National Center for High-Performance
Computing
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