Theoretical Investigation on the Homoleptic [(NO)2Fe(NO)2]and Related Dinitrosyl-iron Complexe Department of Biological Science and Technology Institute of Bioinformatics and Systems Biology National Chiao Tung University TAIWAN Jen-Shiang K. Yu at PACCON 2013 (PCC-IV) The Tide Resort, Chunburi, Thailand January 25, 2013 * Chonburi Taiwan: 36,000 km2 with 22 millions populations. Similar climate to Thailand Taipei - Capital, 1,555 nautical miles from BKK. 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MO diagram of stable free radical •NO Biological Significance of Nitrogen Monoxides •NO is isoelectronic with the dioxygen monocation (O2+), and NO+ is isoelectronic with CO and CN-, while NO- is isoelectronic with O2 with a triplet ground state. Accounts for the continuing interest in the study of certain types of metal nitrosyl complexes which have structural and electronic analogies with biological oxygen activators. Medical application regarding NO include vasodilation, neuronal transmission, inflammation, immune system response and cancer remedy. Possible resonance forms of Metal-NO bonds J. A. McCleverty, Chem. Rev. 104, 403-418, (2004). The p-backbonding electron donation The dp—p* interaction bonding description is very similar to that between CO and metals. However, as NO is more electronegative than CO, it is a better electron acceptor than CO. Furthermore, within the M—N—O group, the metal-nitrogen bond is usually strong. Target Dinitrosyl-iron complexes (DNIC) [(NO)2Fe(NO)2][(N3)2Fe(NO)2][ I2Fe(NO)2]- [1] [2] [3] DNIC DNIC DNIC DNIC [1] Lin, Z.-S.; Chiou, T.-W.; Liu, K.-Y.; Hsieh, C.-C.; Yu, J.-S. K.; Liaw, W.-F. Inorg. Chem. 2012, 51, 10092-10094. [2] Tsai, M.-L.; Hsieh, C.-H.; Liaw, W.-F. Inorg. Chem. 2007, 46, 5110-5117. [3] Bryar, T.R.; Eaton, D.R. Can. J. Chem. 1992, 70, 1917-1926. Experimental Syntheses of DNICs • [(NO)2Fe(NO)2]- • [(N3)2Fe(NO)2]- • [(I)2Fe(NO)2][Fe(CO)3(NO)]- + MeI + cyclo-octatetraene → [(I-)2Fe(NO)2] - Computational aims • To reproduce the geometrical features of DNIC compounds in X-ray crystals. • Charge and spin analyses based on the above converged structures. • Vibrational frequencies, especially the N-O vibration modes. • Spectral assignments to experimental UV absorptions. Methodologies • Broken-Symmetry Density Functional Theories (BS-DFT) • SAC-CI • Multi-configuration methods (CASSCF) Dinitrosyl Iron Complexes Relevant to Rieske Cluster Nitrosylation: A Broken-Symmetry DFT Study Zachary J. Tonzetich, Loi H. Do, and Stephen J. Lippard, J. Am. Chem. Soc. 2009, 131, pp.7964–7965. “Broken Symmetry” DFT Study on Fe(NO)2(nacnac) model nacnac=[(phenyl)NC(Me)2]2CH- Comparison among functionals S. Ye and F. Neese, J. Am. Chem. Soc. 2010, 132, pp.3646–3647. Geometry optimizations of [(NO)2Fe(NO)2]Direct SAC-CI SD-R / LANL2DZ ECP on Fe, aug-cc-pVDZ on N, O. v.s. “Broken-Symmetry” TPSSh/def2-TZVP [(NO)2Fe(NO)4]- Symmetry Fe1-N1 Fe1-N2 Fe1-N3 Fe1-N4 N1-O1 N2-O2 N3-O3 N4-O4 Fe1-N1-O1 Fe1-N2-O2 Fe1-N3-O3 Fe1-N4-O4 Exptl.[1] C1 1.695 1.719 2.008 2.045 1.175 1.154 1.387 1.281 163.1 161.0 106.8 113.2 TPSSh SAC-CI (A') C1 1.739 1.637 1.928 1.750 1.197 1.187 1.205 1.198 152.1 179.0 122.8 154.8 Cs 1.688 1.688 1.987 1.970 1.175 1.175 1.296 1.278 162.9 162.9 104.6 100.5 Linear Radical Bent Anion Charge and spin analyses of [(NO)2Fe(NO)2]Direct SAC-CI SD-R / LANL2DZ ECP on Fe, aug-cc-pVDZ on N, O. v.s. “Broken-Symmetry” TPSSh/def2-TZVP TPSSh/def2-TZVP Fe1 N1 O1 N1 + O1 N2 O2 N2 + O2 N3 O3 N3 + O3 N4 O4 N4 + O4 Charge 0.239 0.036 -0.336 -0.300 0.028 -0.348 -0.320 -0.018 -0.289 -0.307 0.021 -0.333 -0.312 Spin Density (e ) -0.849 0.605 0.371 0.975 -0.169 -0.074 -0.243 -0.032 -0.006 -0.037 0.723 0.430 1.153 SAC-CI Charge 0.846 0.290 -0.558 -0.269 0.290 -0.558 -0.269 -0.027 -0.650 -0.678 -0.067 -0.564 -0.631 Spin Density (e ) 0.000 0.053 0.040 0.094 0.053 0.040 0.094 0.027 0.004 0.031 0.002 0.005 0.008 Linear Radical Bent Anion Charge analysis based on SP calculation at CASSCF(7,7)/aug-cc-PVDZ (SAC-CI geometry) Fe1 N1 O1 N1 + O1 N2 O2 N2 + O2 N3 O3 N3 + O3 N4 O4 N4 + O4 Fe1 N1 O1 TPSSh/def2-TZVP Charge Spin Density (e ) 0.239 -0.849 0.036 0.605 -0.336 0.371 -0.300 0.975 0.028 -0.169 -0.348 -0.074 -0.320 -0.243 -0.018 -0.032 -0.289 -0.006 -0.307 -0.037 0.021 0.723 -0.333 0.430 -0.312 1.153 Charge 0.846 0.290 -0.558 -0.269 0.290 -0.558 -0.269 -0.027 -0.650 -0.678 -0.067 -0.564 -0.631 SAC-CI Spin Density (e ) 0.000 0.053 0.040 0.094 0.053 Linear 0.040 Radical 0.094 0.027 0.004 0.031 0.002 Bent 0.005 Anion 0.008 s 6.50174 3.74704 4.03185 p 11.82088 3.01564 4.44513 d 6.02086 0.04240 0.07491 f 0.10630 0.00000 0.00000 g 0.00000 0.00000 0.00000 Total 24.44979 6.80508 8.55189 3.74704 4.03185 3.01564 4.44513 0.04240 0.07491 0.00000 0.00000 0.00000 0.00000 6.80508 8.55189 3.81184 4.07795 3.34175 4.60341 0.03329 0.04202 0.00000 0.00000 0.00000 0.00000 7.18687 8.72338 3.76909 4.07807 3.32817 4.66756 0.04116 0.04198 0.00000 0.00000 0.00000 0.00000 7.13842 8.78761 N1 + O1 N2 O2 N2 + O2 N3 O3 N3 + O3 N4 O4 N4 + O4 Charge 1.55021 0.19492 -0.55189 -0.35697 0.19492 -0.55189 -0.35697 -0.18687 -0.72338 -0.91025 - 0.13842 -0.78761 -0.92603 Electron occupation in the active space: occ= occ= occ= occ= occ= occ= occ= 1.4550 1.1829 1.0108 0.9984 0.9534 0.8715 0.5281 E= -0.0254 E= -0.0476 E= 0.0274 E= 0.0617 E= 0.0741 E= 0.0126 E= 0.1439 However, CASSCF failed to optimize for the geometry of [(NO)2Fe(NO)2]- • Although CASSCF charge analysis is correct and the digits are significantly better than SAC-CI, the geometry optimization at CASSCF cannot converge. • Optimization at CASSCF level tends to dissociate three of the Fe—NO bonds. • Higher order of MC correlation method such as CASPT2 is not computationally faster than direct SAC-CI. CASSCF: out of OPT cycles (50) The geometry tends to deform from tetrahedral into trigonal pyramidal. SAC-CI calculation for open-shell radicals Four schemes to treat doublet radicals: CationDoublet (Ⅰ) RHF SAC AnionDoublet (Ⅱ) SAC-CI CationDoublet, AddElectron, ROHF (Ⅲ) ROHF SAC SAC-CI RHF SAC SAC-CI AnionDoublet,SubElectron,ROHF (Ⅳ) ROHF SAC SAC-CI Key-point: ・ Use SAC to calculate the closed-shell molecule. ・ Doublet radical is computed by anionize the SAC wavefunction. This electron-attached state is computed by SAC-CI method. ・ These four approaches are numerically equivalent. Geometry optimizations of [(N3)2Fe(NO)2]Direct SAC-CI SD-R / LANL2DZ ECP on Fe, aug-cc-pVDZ on N, O. v.s. “Broken-Symmetry” TPSSh/def2-TZVP [(N3)2Fe(NO)2]Symmetry Fe-N1 Fe-N1A Fe-N2 Fe-N2A N1-O1 N1A-O1A N2-N3 N3-N4 O1-N1-Fe Fe-N2-N3 N4-N3-N2 Exptl.[2] C2 1.693 1.693 1.948 1.948 1.172 1.172 1.160 1.067 160.7 141.9 174.3 TPSSh SAC-CI (A) C1 1.728 1.728 1.976 1.977 1.180 1.180 1.200 1.156 164.3 129.4 176.2 C2 1.660 1.660 1.974 1.974 1.164 1.164 1.170 1.088 161.0 141.9 174.5 [2] Tsai, M.-L.; Hsieh, C.-H.; Liaw, W.-F. Inorg. Chem. 2007, 46, 5110-5117. Charge and spin analyses of [(N3)2Fe(NO)2]Direct SAC-CI SD-R / LANL2DZ ECP on Fe, aug-cc-pVDZ on N, O. v.s. “Broken-Symmetry” TPSSh/def2-TZVP TPSSh/def2-TZVP Charge Fe1 0.420 N1 0.076 O1 -0.281 N1 + O1 -0.204 N1A 0.077 O1A -0.281 N1A + O1A -0.204 N2 -0.463 N3 0.337 N4 -0.380 N2 + N3 + N4 -0.506 N2A -0.464 N3A 0.338 N4A -0.380 N2A + N3A + N4A -0.506 Spin Density (e ) 2.902 -0.636 -0.455 -1.091 -0.636 -0.455 -1.091 0.021 -0.019 0.138 0.140 0.021 -0.019 0.137 0.140 SAC-CI Charge 0.962 0.258 -0.467 -0.209 0.258 -0.467 -0.209 -0.573 0.309 -0.507 -0.772 -0.573 0.309 -0.507 -0.772 Spin Density (e ) 0.000 0.009 0.007 0.016 0.009 0.007 0.016 0.005 -0.001 0.002 0.007 0.005 -0.001 0.002 0.007 Geometry optimizations of [(I)2Fe(NO)2]Direct SAC-CI SD-R / LANL2DZ ECP on Fe, aug-cc-pVDZ on N, O. v.s. “Broken-Symmetry” TPSSh/def2-TZVP [(I)2Fe(NO)2]Symmetry Fe-N1 Fe-N2 Fe-I1 Fe-I2 N1-O1 N2-O2 Fe-N1-O1 Fe-N2-O2 [3] Exptl.[3] C1 1.679 1.683 2.584 2.596 1.141 1.149 167.7 164.1 TPSSh SAC-CI (A1) C1 1.702 1.710 2.646 2.649 1.173 1.175 171.188 163.352 C 2v 1.643 1.643 2.649 2.649 1.145 1.145 167.6 167.6 Bryar, T.R.; Eaton, D.R. Can. J. Chem. 1992, 70, 1917-1926. Charge and spin analyses of [(I)2Fe(NO)2]Direct SAC-CI SD-R / LANL2DZ ECP on Fe, aug-cc-pVDZ on N, O. v.s. “Broken-Symmetry” TPSSh/def2-TZVP TPSSh/def2-TZVP Fe N1 O1 N1 + O1 N2 O2 N2 + O2 I1 I2 Charge 0.071 0.093 -0.192 -0.099 0.080 -0.197 -0.117 -0.431 -0.424 Spin Density (e ) 2.711 -0.546 -0.410 -0.956 -0.566 -0.422 -0.987 0.118 0.115 SAC-CI Charge 0.267 0.378 -0.462 -0.084 0.378 -0.462 -0.084 -0.549 -0.549 Spin Density (e ) 0.000 0.006 0.004 0.010 0.006 0.004 0.010 0.000 0.000 DFT: Comparison among different functionals and relativistic effects of [(I)2Fe(NO)2]- [(I)2Fe(NO)2]Symmetry Fe-N1 Fe-N2 Fe-I1 Fe-I2 N1-O1 N2-O2 Fe-N1-O1 Fe-N2-O2 [(I)2Fe(NO)2]Symmetry Fe-N1 Fe-N2 Fe-I1 Fe-I2 N1-O1 N2-O2 Fe-N1-O1 Fe-N2-O2 Exptl.[3] C1 1.679 1.683 2.584 2.596 1.141 1.149 167.7 164.1 Exptl.[3] C1 1.679 1.683 2.584 2.596 1.141 1.149 167.7 164.1 BP86/TZVP BP86/TZVP ZORA C1 1.664 1.664 2.640 2.639 1.186 1.186 165.256 165.005 C1 1.654 1.654 2.625 2.624 1.188 1.188 165.8 165.6 BP86/TZVP DKH BP86/aug-cc-pVTZ ZORA C1 1.646 1.646 2.620 2.619 1.187 1.187 169.6 169.4 B3LYP/aug-cc-pVTZ ZORA B3LYP/aug-cc-pVTZ DKH TPSSH/def2-TZVP C1 1.741 1.754 2.675 2.674 1.174 1.179 171.8 159.4 C1 1.535 1.539 2.550 2.530 1.153 1.155 165.5 162.2 C1 1.702 1.710 2.649 2.646 1.173 1.175 171.188 163.352 C1 1.648 1.648 2.625 2.623 1.185 1.185 165.8 166.0 Vibration frequencies of linear NO radicals Compound [(NO)2Fe(NO)2] [(N3)2Fe(NO)2] - - NO frequency (cm-1) TPSSh/def2-TZVP 1782, 1712 1751, 1691* 1755, 1698 1783, 1741 1775, 1719 1817, 1774 [(I)2Fe(NO)2] *Initial geometry is obtained from SAC-CI, and the frequencies are calculated by B3LYP. (Scaling factor 0.89 ) Tsai, M.-L.; Hsieh, C.-H.; Liaw, W.-F. Inorg. Chem. 2007, 46, 5110-5117. UV absorptions v.s SAC-CI excitation energies Direct SAC-CI - [(NO)2Fe(NO)2] Transition A' → A' A' → A' A' → A'' - [(N3)2Fe(NO)2] Transition A→B A→B - - [(I)2Fe(NO)2] Transition A1 → B1 A1 → B2 SAC-CI SD-R ∆E(eV) Wavelength(nm) Oscillator strength(f ) 2.859 453 0.010 3.407 380 0.006 1.757 729 0.015 UV Exptl.(nm) SAC-CI SD-R ∆E(eV) Wavelength(nm) Oscillator strength(f ) 3.192 388 0.003 2.205 562 0.012 - UV Exptl.(nm) [2] SAC-CI SD-R ∆E(eV) Wavelength(nm) Oscillator strength(f ) 2.362 525 0.013 3.128 396 0.004 UV Exptl.(nm) 473 385 744 397 502 701 [2] Tsai, M.-L.; Hsieh, C.-H.; Liaw, W.-F. Inorg. Chem. 2007, 46, 5110-5117. DFT orbitals among three DNICs ( TPSSh/def2-TZVP ) [(NO)2Fe(NO)2]- [(N3)2Fe(NO)2]- [(I)2Fe(NO)2]- Canonical orbitals among three DNIC systems (SAC-CI) [(NO)2Fe(NO)2]- [(N3)2Fe(NO)2]- [(I)2Fe(NO)2]- Energy Gaps among Anionic States anionic EA state [(NO)2Fe(NO)2][(N3)2Fe(NO)2](L)2Fe(NO)2 [(I)2Fe(NO)2]- 1st state 1st A' 5th A 3rd A1 2nd state 2nd A' 3rd A 2nd A1 3rd state 4th state 1st A 1st A1 2nd A - neutral state anionic EA state SAC Energy SAC-CI Energy 1st state 2nd state 3rd state 4th state -640.663096 -640.635223 - - -708.948369 -708.898150 -708.853320 -708.763387 -971.538079 -971.455814 -971.338311 - 1st state 2nd state 3rd state 4th state 0.0 0.0 0.0 0.8 1.4 2.2 2.6 5.4 5.0 - -640.564298 -708.753385 -971.328430 [(NO)2Fe(NO)2][(N3)2Fe(NO)2][(I)2Fe(NO)2]- anionic states neutral state ∆E (eV) -2.7 -5.3 -5.7 [(NO)2Fe(NO)2][(N3)2Fe(NO)2][(I)2Fe(NO)2]- Concluding Remark • SAC-CI method is very useful and precise to study the multiconfiguration Fe(NO)4- anion, and in fact it is the only successful theory up to now that can describe this system correctly. Zong-Sian Lin, Tzung-Wen Chiou, Kuan-Yu Liu, Chang-Chih Hsieh, Jen-Shiang K. Yu*, and Wen-Feng Liaw*, A Dinitrosyliron Complex within the Homoleptic Fe(NO)4 Anion: NO as Nitroxyl and Nitrosyl Ligands within a Single Structure, Inorg. Chem., 51, 10092-10094 (2012). • Vibrational analysis for the N-O vibration is planned to use the ezPES. Kuan-Yu Liu 劉冠佑 Acknowledgements • National Science Council • ATU Plan, Minister of Education • National Chiao Tung University, Taiwan Thank you for your attentions. UV absorption of [(NO)2Fe(NO)2]- [(NO)2Fe(NO)2] Transition A' → A' A' → A' A' → A'' A' A'' SAC-CI SD-R ∆E(eV) Wavelength(nm) Oscillator strength(f ) 2.859 453 0.010 3.407 380 0.006 1.757 729 0.015 1 2 3 4 5 6 7 1 2 3 4 5 6 7 UV Exptl.(nm) 473 385 744 Excitation Energy nm Osc. Strength Excitation from this state. 0.8065 1604 0.0015 2.8566 453 0.0102 3.2113 403 0.0063 3.4049 380 0.0065 -1.7717 -730 0.0030 4.9708 260 0.0007 0.2812 4601 0.0000 0.9718 1331 0.0395 2.988 433 0.0058 1.4481 893 0.0066 1.7737 729 0.0146 4.7409 273 0.0006 5.8203 222 0.0000 Double excitation 1 4 0 0 0 4 0 1 1 0 3 1 0 0 Exptl. 473 385 744 UV absorption of [(N3)2Fe(NO)2]- [(N3)2Fe(NO)2] Transition A→B A→B A B SAC-CI SD-R ∆E(eV) Wavelength(nm) Oscillator strength(f ) 3.192 388 0.003 2.205 562 0.012 1 2 3 4 5 6 7 1 2 3 4 5 6 7 UV Exptl.(nm) 397 502 701 Excitation Energy nm Osc. Strength 2.5783 481 0 5.0109 247 0.0032 1.3644 909 0.0001 5.7847 214 0.0011 Excitation from this state. 7.011 177 0.0004 7.3249 169 0.0046 3.1919 388 0.0033 2.2048 562 0.0124 5.4551 227 0.0027 5.4754 226 0.0169 6.9979 177 0.0036 7.4919 165 0.0136 8.029 154 0.035 Double excitation 1 4 4 2 4 2 3 1 2 2 1 1 3 1 Exptl. 397 502 UV absorption of [(I)2Fe(NO)2]- SAC-CI SD-R ∆E(eV) Wavelength(nm) Oscillator strength(f ) 2.362 525 0.013 3.128 396 0.004 [(I)2Fe(NO)2] Transition A1 → B1 A1 → B2 A1 A2 B1 B2 1 2 3 4 5 1 2 3 4 5 1 2 3 4 5 1 2 3 4 5 UV Exptl.(nm) - Excitation Energy nm Osc. Strength (f ) 5.307 234 0.0001 2.1735 570 0.0012 Excitation from this state 6.061 205 0.0083 7.1264 174 0.0072 2.9194 425 0.0000 7.7967 159 0.0000 8.9584 138 0.0000 11.3277 109 0.0000 13.1297 94 0.0000 2.362 525 0.0128 5.8295 213 0.0037 7.3236 169 0.0097 8.4683 146 0.0144 9.0618 137 0.0019 3.1276 396 0.0038 5.8502 212 0.0003 7.4853 166 0.0002 8.5082 146 0.1119 8.9267 139 0.0049 Double excitation 1 3 7 0 0 1 0 0 0 12 1 0 0 2 16 2 1 1 15 0 Exptl. - Enemark−Feltham notation {Mn(NO)x}n x = the number of nitrosyls n = the total number of electrons associate with metal d and π* (NO) orbitals L1L2Fe(NO)2 x=2 n = 7 (d7 for FeI) + 2 (two π* e- for NO ) = 9 The notation for DNICs is {Fe(NO)2}9. J. H. Enemark; R. D. Feltham, Coord. Chem. Rev. 13, 339, (1974).