JETCOOLED LASERINDUCED FLUORESCENCE SPECTROSCOPY OF LARGE SECONDARY ALKOXY

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JET-COOLED LASER-INDUCED FLUORESCENCE SPECTROSCOPY OF LARGE SECONDARY ALKOXY RADICALS JINJUN LIU, MING-WEI CHEN, AND

JET-COOLED LASER-INDUCED FLUORESCENCE SPECTROSCOPY OF LARGE SECONDARY ALKOXY RADICALS JINJUN LIU, MING-WEI CHEN, AND TERRY A. MILLER Laser Spectroscopy Facility Department of Chemistry The Ohio State University 06/21/10

Motivation I: Hydrocarbon oxidation * J. J. Orlando, G. S. Tyndall, T. J. Wallington,

Motivation I: Hydrocarbon oxidation * J. J. Orlando, G. S. Tyndall, T. J. Wallington, Chem. Rev. 103, 4657 (2003)

Motivation II: Jahn-Teller and pseudo-Jahn-Teller effects CH 2 DO ethoxy 1 -propoxy …… methoxy

Motivation II: Jahn-Teller and pseudo-Jahn-Teller effects CH 2 DO ethoxy 1 -propoxy …… methoxy CH 3 O CD 3 O CHD 2 O iso-propoxy 2 -butoxy …… * J. Liu et al. , JCP, 130, 074302 (2009). * D. Melnik et al. , JCP, submitted * X. Q. Tan et al. , JCP, 97, 9311 (1993) * J. Liu et al. , 65 th MSS, TG 14 (2010). * S. Gopalakrishnan et al. , JCP, 118, 4954 (2003). * V. Stakhursky et al. , JCP, 125, 094316 (2006)

Motivation III: Conformers of alkoxy radicals For secondary alkoxy radicals, N=3(n-3) N: number of

Motivation III: Conformers of alkoxy radicals For secondary alkoxy radicals, N=3(n-3) N: number of conformers; n: number of carbon atoms. N=3 N=9 N=27 Φ 1=O-C 1 -C 2 -C 3; Φ 2=C 1 -C 2 -C 3 -C 4; Φ 3=C 2 -C 3 -C 4 -C 5 … G+= gauche clockwise (Φ ~ 60 o) T= trans (Φ ~ 180 o) G-= gauche counterclockwise (Φ ~ -60 o)

Experimental apparatus I: Low-resolution LIF PMT Doubling Crystal Vacuum Chamber (SHG) Δν~3 GHz Photolysis

Experimental apparatus I: Low-resolution LIF PMT Doubling Crystal Vacuum Chamber (SHG) Δν~3 GHz Photolysis Excitation RONO +He/Ne T~1 K

Low-resolution LIF spectra

Low-resolution LIF spectra

Low-resolution LIF spectra

Low-resolution LIF spectra

Low-resolution LIF spectra

Low-resolution LIF spectra

Experimental apparatus II: High-resolution LIF PMT Doubling Crystal Δν~100 MHz Pulse Dye Amplifier Excimer

Experimental apparatus II: High-resolution LIF PMT Doubling Crystal Δν~100 MHz Pulse Dye Amplifier Excimer Laser (Xe. Cl) Xe. F Photolysis Laser RONO+He Etalon Box. Car Δν~1 MHz Ar+ Laser Computer CW Ring Dye Laser I 2 Lockin PD PD

High-resolution LIF spectra of 2 -pentoxy Type I: A, C 1, C 2 Type

High-resolution LIF spectra of 2 -pentoxy Type I: A, C 1, C 2 Type II: B, C 3, D 1 D 2, D 3 Type II (overlapping): D 4, 5 D 6, 7

High-resolution LIF spectra of 2 -hexoxy Type I: A, C 1 Type I (overlapping):

High-resolution LIF spectra of 2 -hexoxy Type I: A, C 1 Type I (overlapping): C 2, 3 C 4, 5 Type II: B, D

High-resolution LIF spectra 2 -pentoxy 2 -hexoxy Type II

High-resolution LIF spectra 2 -pentoxy 2 -hexoxy Type II

Spectroscopic model ground state (X) excited state (B) Hamiltonian H = HRot + HSR

Spectroscopic model ground state (X) excited state (B) Hamiltonian H = HRot + HSR H = HRot = ANa 2 + BNb 2 + CNc 2 HSR = ½ ab (Na. Sb + Sb. Na) a, b molecular constants rotational constants A", B", C" A', B', C' spin-rotation constants* aa", bb", cc" ½( ab" + ba") transition types* ½( ac" + ca") a: b: c ½( bc" + cb") * Predicted based on the experimental results of iso-propoxy.

Quantum chemistry calculations 2 -pentoxy 2 -hexoxy ~ ~ A and X states: B

Quantum chemistry calculations 2 -pentoxy 2 -hexoxy ~ ~ A and X states: B 3 LYP/6 -31+G(d) ~ B state: CIS/6 -31+G(d) * Scaled by 0. 76. [G. Tarczay, S. Gopalakrishnan, and T. A. Miller, J. Mol. Spectrosc. 220, 276 (2003). ]

Simulation with calculated/predicted parameters 2 -pentoxy

Simulation with calculated/predicted parameters 2 -pentoxy

Simulation using evolutionary algorithm (EA)* 2 -pentoxy * W. L. Meerts and M. Schmitt

Simulation using evolutionary algorithm (EA)* 2 -pentoxy * W. L. Meerts and M. Schmitt Int. Rev. Phys. Chem. , 25(3), 353– 406 (2006)

Fit parameters 2 -pentoxy G+T: from global fit of Bands A, C 1 and

Fit parameters 2 -pentoxy G+T: from global fit of Bands A, C 1 and C 2 (Type I); TT: from global fit of Bands B and C 3 (Type II). [ ]: discrepancy between cal. and expt. ; ( ): one standard deviation.

Simulation of overlapping bands 2 -pentoxy, Band D 4, 5 (CO stretch band of

Simulation of overlapping bands 2 -pentoxy, Band D 4, 5 (CO stretch band of TT conformer) Frequency interval: δν~0. 03 cm-1 D 3

Low-resolution LIF spectra Origin CO stretch B D + T G + GA B

Low-resolution LIF spectra Origin CO stretch B D + T G + GA B C D CO TCO +T TT G+T GA B C D CO TTCO G+A B C D TT TTT G+TTCO TTTCO +TTT G+TTT TTTT G A B C D CO TTT CO +TTTT G+TTTT TTTTT G A B C D CO TTTT CO TTTTTT TTTTT A B C D CO G+TTTTT G +TTTTTCO TTTTTTT TTTTTT CO A B C D G+TTTTTT G +TTTTTTCO

Summary and Future work High-resolution rotationally resolved spectra of 2 -pentoxy and 2 -hexoxy

Summary and Future work High-resolution rotationally resolved spectra of 2 -pentoxy and 2 -hexoxy have been obtained and simulated. n Evolutionary algorithm was used for global fitting successfully. n These spectra were assigned to all-Trans conformers or conformers with a G+ OCCC dihedral angle. 2 -pentoxy: G+T, TT; 2 -hexoxy: G+TT, TTT. n Good agreement between experimentally determined and calculated/predicted parameters has been found. n n n Quantitative understanding of the pseudo-Jahn-Teller effect in secondary alkoxy radicals; Study of cyclic alkoxy radicals.

Acknowledgements Miller Group Prof. Dr. W. Leo Meerts Radboud University Nijmegen The Netherlands Thank

Acknowledgements Miller Group Prof. Dr. W. Leo Meerts Radboud University Nijmegen The Netherlands Thank you all!