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Electronic Transitions of Palladium Monoboride and Platinum Monoboride Y.W. Ng, H.F. Pang, Y. S. Wong, Yue Qian, and A. S-C. Cheung Department of Chemistry University of Hong Kong June 2012 67th OSU International Symposium on Molecular Spectroscopy 1
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Acknowledgments The work described here was supported by grants from the Research Grants Council of the Hong Kong SAR, China. (Project numbers 701008P). 2
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Contents Introduction Experimental Setup Results Summary 3
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Introduction Interest in transition metal monoboride Spectroscopic Interest Molecular & electronic structure Synthesizing metal monoboride in gas phase Pervious study Limited studies on metal boride 4
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Introduction Pd and Pt are elements from same Group (Group 10) Same outermost shell electronic configuration Likely to have same ground state symmetry on PdB & PtB Similar chemical properties Catalysts for hydrogenation, dehydrogenation, reductive alkylation, hydrogenation of carbonyl and selective hydrogenation of nitro compound Likely to have similar reaction towards B 2 H 6 5
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Introduction Pervious Works on PdB Knight et al (J Chem. Phys. 97 2987 (1992)) Studying PdB by electron spin resonance (ESR) spectroscopy Performing ab initio calculations on PdB using unrestriced Hartree-Fock method and limited STO-3G basis set PdB X 2 Σ + state r o =1.608 Å Kharat et al (Int. J Quant. Chem. 109 1103 (2009)) Studying 4d transition metal monoboride by density functional theory (DFT) calculations PdB X 2 Σ + state r o = 1.856 Å ω e = 725.6cm -1 6
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Introduction Pervious Works on PtB Kalamse et al (Bull. Mater. Sci. 33 233 (2010)) Using DFT calculated the ground state symmetry, bond length and vibrational frequency of 5d transition metal mononitrides and monoborides ranging from La to Hg: PtBX 2 Σ + state r o = 1.809 Å ω e = 906cm -1 7 No experimental observation of electronic transition of palladium monoboride and platinum monoboride
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Laser ablation/reaction free jet expansion Molecule production: Pd (Pt) + B 2 H 6 (0.5% in Ar) → PdB (PtB) + etc. Ablation Laser : Nd:YAG, 10Hz, 532nm, 5mJ Free Jet Expansion : i) backing pressure: 6 atm B 2 H 6 (0.5% in Ar) ii) background pressure: 1x10 -5 Torr LIF spectrum in the visible region Laser system: Optical Parametric Oscillator laser Gas-Phase PdB (PtB ) Production Method 8
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Experiment Schematic Diagram of Laser Vaporization/ LIF Experimental Setup Pulsed Nd: YAG laser 9 Metal rod
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Monochromator Fix the wavelength of the OPO laser Scan the grating in monochromator Wavelength resolved fluorescence spectrum 10 v’ v” 0 0 1 2 Δ G 3/2 Δ G 1/2 Excitation Laser Scanning grating Δ G 1/2 Δ G 3/2 Wavelength resolved fluorescence spectrum
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Monochromator Serve as an optical filter Set the grating at a particular wavelength Small spectral region is detected by PMT 11 Total fluorescence spectrum Without monochromator filtering Filtered fluorescence spectrum With monochromator filtering
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Experiment The pulsed valve, ablation laser, excitation laser and oscilloscope are synchronized appropriately by a delay generator 12 Pulsed Nd: YAG laser
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Results (PdB) Low-resolution broad band spectrum of PdB 13 The analysis of the [19.7] 2 Σ + – X 2 Σ + transitions of PdB in the spectral region between 465 and 520 nm using laser induced fluorescence (LIF) spectroscopy
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Results (PtB) Low resolution broad band spectrum of PtB 14 The analysis of the [21.2] 2 Π 1/2 – X 2 Σ + and [20.2] 2 Π 3/2 – X 2 Σ + transitions of PtB in the spectral region between 455 and 520 nm using laser induced fluorescence (LIF) spectroscopy
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Confirmation of PdB and PtB Signal intensity is proportional to the abundance of the isotopes Abundance 11 B : 10 B ≈ 4:1 Intensity of two bands ≈ 4:1 B carrier Five peaks with similar intensity representing the five palladium isotopes 104 Pd (11.14%) 105 Pd (22.33%) 106 Pd (27.33%) 108 Pd (26.46%) 110 Pd (11.72%) Pd carrier Spectra of Pt isotopic species is observed 194 Pt (32.9%) 195 Pt (33.8%) 196 Pt (25.3%) 198 Pt (7.2%) Pt carrier 15
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Results (PdB) 16 R 1, R 2 branches and P 1, P 2 branches No Q branch 2 Σ + - 2 Σ + transition
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Results (PdB) Observed vibrational transitions of PdB 17 + +
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Results (PdB) 18 Molecular constants for Pd 11 B (cm -1 ) [19.7] 2 + X2+X2+ ∆G 1/2 541.12753.98 BoBo 0.47410.5353 r o (Å)1.8471.738
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Results (PtB) 19 2 P-branches (P 1 and P 12 ) doublet state Strong R and Q branches ΔΛ= +1 Ω’=0.5 – Ω”=0.5 transition 2 Π 1/2 - 2 Σ + transition 0.5 1.5 0.5 1.5 Ω” = 0.5 J Ω’ = 0.5 P 1 (1.5)R 1 (0.5) Q 1 (0.5) 0.5 1.5
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Results (PtB) 20 2 R-branches (R 2 and R 21 ) doublet state Strong R and Q branches ΔΛ= +1 Ω’=1.5 – Ω”=0.5 transition 2 Π 3/2 - 2 Σ + transition 1.5 0.5 1.5 2.5 Ω” = 0.5 J Ω’ = 1.5 P 2 (2.5)R 2 (0.5)Q 2 (1.5) 0.5 1.5 2.5
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Vibrational bands observed for PtB X2Σ+X2Σ+ [21.2] 2 П 1/2 [20.2] 2 П 3/2 0 1 0 1 2 0 1 v v v 21 Results (PtB)
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2 Π 3/2 is lower in energy than 2 Π 1/2 inverted Π state B o value of 2 Π 3/2 is larger than 2 Π 1/2 regular Π state [21.2] 2 Π 1/2 and [20.2] 2 Π 3/2 come from different 2 states 22 Molecular constants for Pt 11 B (cm -1 ) [21.2] 2 П 1/2 [20.2] 2 П 3/2 X2Σ+X2Σ+ ΔG 1/2 613.9636.26903.60 BoBo 0.46990.49950.5274 r o (Å)1.8561.8001.751
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Molecular orbital energy level diagram of PdB & PtB Electronic Configuration PdB (PtB) 1σ1σ 1π1π 2σ2σ 2π2π 3σ3σ Pd (Pt) B d s 2p 1δ1δ σ δ π σ σ π 23 Ground State: 1σ 2 1π 4 1δ 4 2σ 1 2 Σ + Excited State: 1σ 2 1π 4 1δ 4 2π 1 2 Π 1σ 2 1π 4 1δ 4 3σ 1 2 Σ + 1σ 2 1π 4 1δ 3 2σ 1 2π 1 2 Π
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Comparison of Group 10 monoboride 24 MoleculeNiBPdBPtB Ground state Symmetry 2+2+2+2+2+2+ r o (Å)1.6981.7381.751 ΔG 1/2 (cm -1 )768.2754.0903.6 Bond length increases down the group from NiB to PtB The larger ΔG 1/2 of PtB indicates a stronger bonding between Pt and B atoms
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Summary First experimental observation of electronic transition of the PdB and PtB molecule [19.7] 2 Σ + - X 2 Σ + of PdB [21.2] 2 Π 1/2 – X 2 Σ + and [20.2] 2 Π 3/2 – X 2 Σ + of PtB Ground state of PdB and PtB: 2 Σ + Bond length at ground state of PdB, r o = 1.738Å Bond length at ground state of PtB, r o = 1.751Å 25
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