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ANION PHOTOELECTRON SPECTROSCOPIC STUDIES OF NbCr(CO) n ‾ (n = 2,3) HETEROBIMETALLIC CARBONYL COMPLEXES Melissa A. Baudhuin, Praveenkumar Boopalachandran, and Doreen G. Leopold University of Minnesota – Chemistry Department June 25 th, 2015 1
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2 SAFETY MOMENT Gas Cylinder Safety ALWAYS wear safety glasses: ▫ When connecting/disconnecting regulators Do NOT leave gas cylinder: ▫ Uncapped without a regulator
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3 METAL CARBONYL COMPLEXES Motivation Transition metal carbonyl complex ▫ Used for CO-releasing molecules (CORMs) as a therapeutic agent Method Anion Photoelectron Spectroscopy ▫ Obtain electron affinities, vibrational frequencies, and excited state energies ▫ Provide benchmark values for computational studies Garcia-Gallego, S.; Bernardes, G. J. L. Angew. Chem. Int. Ed. 2014, 53, 9712
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Flowing Afterglow Ion-Molecule Reactor Magnetic Sector Mass Analyzer Photoelectron Spectroscopy Chamber Slits Argon Ion Laser Electron Kinetic Energy Analyzer Chamber 1 Chamber 2 Chamber 3 Chamber 4 Chamber 5 hν (488 or 514 nm) 4 Electron Detector MINNESOTA ANION PHOTOELECTRON SPECTROMETER (MAPELS)
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5 INTERPRETING DATA (eKE) Electron Kinetic Energy (eBE) Electron Binding Energy eBE = hν - eKE X+ e ‾ ←X‾X‾ +hνhν X*+ e ‾ ←X‾X‾ +hνhν X‾X‾ X X* 1 eV ≈ 8065 cm -1
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6 MASS SPECTRUM OF FLOW TUBE REACTION PRODUCTS: Nb + Cr(CO) 6
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7 PHOTOELECTRON SPECTRUM OF NbCr(CO) 2 ‾ AT 488 nm A
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8 Neutral moleculeTransition A Electron affinity (eV)1.668 ± 0.007 ν 1 (cm -1 )1935 ± 20 ν 2 (cm -1 )395 ± 20 AnionTransition A ν 2 (cm -1 )380 ± 20 A 395 cm -1 1935 cm -1 380 cm -1 PHOTOELECTRON SPECTRUM OF NbCr(CO) 2 ‾ AT 488 nm
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Complexes have small number of active modes ▫ Expect high symmetry structures ▫ Small geometry changes between anion and neutral states DFT – B3LYP/gen ▫ Identify the isomeric structure ▫ Determine anion and neutral electronic states ▫ Compare calculated values to our experimental measurements 9 gen: Nb & Cr → SDD C & O → 6-311++G(df,pd) NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS
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10 NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS Geometry & Frequency Calculations: ▫ NbCr(CO) 2 ‾ Spin Multiplicity (2S + 1): 1, 3, & 5 states ▫ NbCr(CO) 2 Spin Multiplicity: 2, 4, & 6 states Calculated Franck-Condon Progression: ▫ NbCr(CO) 2 ← NbCr(CO) 2 ‾ Spin allowed transitions 1 electron transitions Isomers Tested:
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11 NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS Isomers Tested: ISOMERS ELIMINATED DUE TO: 1)Calculated Franck-Condon progression did not match experimental spectrum 2)Imaginary frequencies in the anionic state 3)Convergence failure in the geometry optimization
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12 NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS
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13 NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS Anion State 1 A 1 ← Neutral State 2 A 1 π back bonding σ bonding
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14 NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS Anion State 1 A 1 ← Neutral State 2 A 1 Electron Detached: sσ type MO π back bonding σ bonding
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15 NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS Anion State 1 A 1 ← Neutral State 2 A 1 r (Cr-Nb) = 1.991 Å r (C-O) = 1.175 Å r (Nb-C) = 2.115 Å r (Nb-C) = 2.160 Å r (Cr-Nb) = 2.014 Å r (C-O) = 1.149 Å 81° 83° π back bonding σ bonding v CO = 2040 cm -1 v CO = 1860 cm -1
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16 NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS Neutral moleculeTransition AB3LYP/gen Electron affinity (eV)1.668 ± 0.0071.509 ν 1 (cm -1 )1935 ± 202040 ν 2 (cm -1 )395 ± 20397 AnionTransition AB3LYP/gen ν 2 (cm -1 )380 ± 20432 ν 1 : CO stretch
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17 NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS Neutral moleculeTransition AB3LYP/gen Electron affinity (eV)1.668 ± 0.0071.509 ν 1 (cm -1 )1935 ± 202040 ν 2 (cm -1 )395 ± 20397 AnionTransition AB3LYP/gen ν 2 (cm -1 )380 ± 20432 ν 2 : M-M stretch + M-L bend
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18 PHOTOELECTRON SPECTRUM OF NbCr(CO) 3 ‾ AT 488 nm A
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19 Neutral moleculeTransition A Electron affinity (eV)1.162 ± 0.007 ν 1 (cm -1 )1910 ± 20 ν 2 (cm -1 )1445 ± 20 ν 3 (cm -1 )560 ± 20 ν 4 (cm -1 )260 ± 20 AnionTransition A ν 3 (cm -1 )560 ± 20 ν 4 (cm -1 )275 ± 20 PHOTOELECTRON SPECTRUM OF NbCr(CO) 3 ‾ AT 488 nm A
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20 NbCr(CO) 3 AND NbCr(CO) 3 ‾ DFT ANALYSIS Isomers Tested : Geometry & Frequency Calculations: ▫ NbCr(CO) 3 ‾ Spin Multiplicity: 1, 3, 5, & 7 states ▫ NbCr(CO) 3 Spin Multiplicity: 2, 4, & 6 states Calculated Franck-Condon Progression: ▫ NbCr(CO) 3 ← NbCr(CO) 3 ‾ Spin allowed transitions 1 electron transitions
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21 NbCr(CO) 3 AND NbCr(CO) 3 ‾ DFT ANALYSIS Isomers Tested: ALL ISOMERS AND SPIN STATES TESTED THUS FAR HAVE: 1)Calculated Franck-Condon progression did not match experimental spectrum 2)Imaginary frequencies in the anionic state 3)Convergence failure in the geometry optimization
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22 NbCr(CO) 3 AND NbCr(CO) 3 ‾ DFT ANALYSIS Isomers Tested: ISSUES COULD BE FROM: 1)Large deviations in the S 2 values Calculated complexes are spin contaminated DFT is not an appropriate treatment for these complexes 2)Multiple low-lying excited states Spin Multiplicity Calculated S 2 value True S 2 value S(S + 1) Singlet2.740.00 Doublet2.400.75 Triplet3.642.00 Quartet5.303.75
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Thank You 23 Current Group Members Doreen Leopold Melissa Baudhuin Alex Schnepper Previous Group Members Dr. Praveen Boopalachandran Dr. Steve Miller Dr. Ashfaq Bengali Srijay Rajan Funding NSF
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Questions 24
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25 MoleculeElectron Affinity (eV) Neutral State v CO stretch (cm -1 ) NbCr0.793 ± 0.003- CO2143 Cr(CO) 3 * 1.349 ± 0.0062000 ± 10 NbCr(CO) 2 1.668 ± 0.0071935 ± 20 NbCr(CO) 3 1.162 ± 0.0071910 ± 20 SUMMARY OF EXPERIMENTAL RESULTS *Bengali, A. A.; Casey S. M.; Cheng, C.-L.; Dick, J. P.; Fenn, T.; Villalta, P. W.; Leopold, D. G. J. Am. Chem. Soc. 1992, 114, 5257-5268
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26 NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS Anion State 1 A 1 ← Neutral State 2 A 1 1.991 Å 1.175 Å (1860 cm -1 ) 2.115 Å 2.160 Å 2.014 Å 1.149 Å (2040 cm -1 ) 81°83° Electron Detached: sσ type MO
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27 r1r1 r2r2 r3r3 α1α1 NbCr(CO) 2 & NbCr(CO) 2 ‾ B3LYP/gen Geometric Parameters Anion ( 1 A 1 )Neutral ( 2 A 1 ) r 1 (Å)1.9912.014 r 2 (Å)2.1152.160 r 3 (Å)1.1751.149 α 1 (°)8183 NbCr Experimental & B3LYP/SDD Geometric Parameters Anion ( 1 ∑ + )Neutral ( 2 ∆) Experiment r (Å)1.815 ± 0.011 a 1.8940 ± 0.0003 b B3LYP/SDD r (Å)1.8081.889 a Baudhuin, M. A.; Boopalachandran, P.; Rajan, S.; Leopold, D. G. (to be published) b Sickafoose, S. M.; Langenberg, J. D.; Morse, M. D. J. Phys. Chem. A. 2000, 104, 3521-3527 r NbCr(CO) 2 AND NbCr(CO) 2 ‾ DFT ANALYSIS
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28 NbCr(CO) 3 AND NbCr(CO) 3 ‾ DFT ANALYSIS Anion State 7 A Neutral State 6 A ← 2.026 Å 1.182 Å 2.803 Å2.717 Å 2.025 Å 1.171 Å
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29 r1r1 r2r2 r3r3 α1α1 NbCr(CO) 3 & NbCr(CO) 3 ‾ B3LYP/gen Geometric Parameters Anion ( 7 A)Neutral ( 6 A) r 1 (Å)2.8032.717 r 2 (Å)2.0262.025 r 3 (Å)1.1821.171 α 1 (°)49.750.2 NbCr Experimental & B3LYP/SDD Geometric Parameters Anion ( 1 ∑ + )Neutral ( 2 ∆) Experiment r (Å)1.815 ± 0.011 a 1.8940 ± 0.0003 b B3LYP/SDD r (Å)1.8081.889 a Baudhuin, M. A.; Boopalachandran, P.; Rajan, S.; Leopold, D. G. (to be published) b Sickafoose, S. M.; Langenberg, J. D.; Morse, M. D. J. Phys. Chem. A. 2000, 104, 3521-3527 r NbCr(CO) 2 AND NbCr(CO) 3 ‾ DFT ANALYSIS
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30 NbCr(CO) 3 AND NbCr(CO) 3 ‾ DFT ANALYSIS
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31 NbCr(CO) 3 AND NbCr(CO) 3 ‾ DFT ANALYSIS Neutral moleculeTransition AB3LYP/gen Electron affinity (eV)1.162 ± 0.0071.270 ν 1 (cm -1 )1910 ± 201923 ν 2 (cm -1 )1445 ± 20- ν 3 (cm -1 )560 ± 20603 ν 4 (cm -1 )260 ± 20405 AnionTransition AB3LYP/gen ν 3 (cm -1 )560 ± 20596 ν 4 (cm -1 )275 ± 20402
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Cr(CO) 2 ‾ PHOTOELECTRON SPECTRUM 32 Bengali, A. A. Ph.D. Thesis, University of Minnesota, Minneapolis, MN, 1992
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Cr(CO) 3 ‾ PHOTOELECTRON SPECTRUM 33 Bengali, A. A.; Casey S. M.; Cheng, C.-L.; Dick, J. P.; Fenn, T.; Villalta, P. W.; Leopold, D. G. J. Am. Chem. Soc. 1992, 114, 5257-5268
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Cr(CO) 3 ‾ DFT ANALYSIS 34 Bengali, A. A.; Casey S. M.; Cheng, C.-L.; Dick, J. P.; Fenn, T.; Villalta, P. W.; Leopold, D. G. J. Am. Chem. Soc. 1992, 114, 5257-5268
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35 Cr(CO) 3 AND Cr(CO) 3 ‾ DFT ANALYSIS Anion State 2 A 1 Neutral State 1 A 1 ← Electron Detached: sσ type MO 1.814 Å 1.170 Å 1.821 Å 1.154 Å
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Cr(CO) 3 ‾ DFT ANALYSIS 36 Bengali, A. A.; Casey S. M.; Cheng, C.-L.; Dick, J. P.; Fenn, T.; Villalta, P. W.; Leopold, D. G. J. Am. Chem. Soc. 1992, 114, 5257-5268 Neutral moleculeTransition AB3LYP/gen Electron affinity (eV)1.349 ± 0.0061.327 ν 1 (cm -1 ) 2000 ± 102069 ν 2 (cm -1 ) 680 ± 10702 ν 3 (cm -1 ) 480 ± 20468 AnionTransition AB3LYP/gen ν 2 (cm -1 )680 ± 10700
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