vadim l. stakhursky *, lily zu †, jinjun liu, terry a. miller laser spectroscopy facility,...
TRANSCRIPT
VADIM L. STAKHURSKY*, LILY ZU†, JINJUN LIU, TERRY A. MILLER
Laser Spectroscopy Facility, Department of Chemistry, The Ohio State University
120 W. 18th Avenue, Columbus OH 43210.
CONFORMATIONAL ANALYSIS
OF SECONDARY ALKOXIES
VIA HIGH-RESOLUTION B-X LIF SPECTROSCOPY~ ~
* Present address
Radiation Oncology, Duke University Clinic,
P.O. , NC, 27710
† Present address
Department of Chemistry
Beijing Normal University
Motivation
Alkoxy radicals (RO·) are important intermediates in the combustion of hydrocarbon fuels and play important role in the balance of ozone in the atmosphere.
Rotational structure of large number of primary alkoxy radicals (CnH2n+1O·, n=3-7) was analyzed in our lab.
Until recently good rotational analysis of secondary alkoxies is not achieved yet.
ExcimerLaser(XeCl)
Pulse Amplifier
PMT
PD
Ar Laser 20WCW ringDye Laser
Computer
XeFPhotolysis
Laser
PD
I 2
+
5-10 mJ~120 MHz
DoublingCrystal
0.5mJ
Experimental Setup of High-Resolution LIF
2-Butoxy Conformers (ab initio Studies)
G+T G-
Gaussian 03 UHF(6-31G) calculations for ground state
Energy (cm-1)
Torsion Angle
18060 -60
Prediction of Molecular Parameters
G+ T G-For each stable conformer rotational constants were calculated in the ground
electronic state (UHF, B3LYP, CISD) and in the excited electronic state (CIS). Different basis sets were tested for convergence (6-31 to 6-311++G**).
Quantum chemistry calculations were done to predict transition dipole moments and components of the spin-rotation tensor. The experimentally determined parameters of ethoxy were used as a reference at the beginning. After parameters of one of the 2-butoxy conformers were obtained, they were used as a reference to predict parameters of the other two.
Vibrational frequencies were calculated for all three stable geometries to identify vibrationally excited bands in the 2-butoxy spectrum.
Relative energies of the conformers and isomerization barriers were estimated to understand the population and dynamics of the conformers in the jet.
H = HRot + HSR
HRot = ANa2 + BNb
2 + CNc2
HSR = ½ (S + S)
ParametersRotation Spin-Rotation
A', B', C'A", B", C" aa
", bb", cc
"
½(ab" + ba
")
½(ac" + ca
")½(bc
" + cb
")
H = HRot
Ground state Excited state
Hamiltonian Model
Negligible effect on spectra
Simulation of Band A
and A, exp.
and A, exp.
G+, Hrot Only, c type
T, Hrot Only, c type
G-, Hrot Only, c type
Frequency/cm-1
T=1.2K
Asym. rotor,ab initio, c-type
Asym. rotor,fit, c-type
Asym. rotor &spin-rotation, fit, c-type
Asym. rotor &spin-rotation, a,b-type
Final fita:b:c=0.05:0.35:1
Band A, exp.
Rotational Analysis of Band A (G+ conformer)
Frequency/cm-1
T=1.2K
Selectivity of the Spectroscopic Method, Band A
ground state calculations by Gaussian 03, UHF (6-31+g*) excited state calculations by Gaussian 03, CIS(6-31g)
Experimental G+ conformer T conformer G- conformer
A’ 8.106(3) 8.280 7.768 6.496
B’ 3.495(3) 3.460 3.478 3.863
C’ 2.775(4) 2.700 2.653 3.199
A” 8.627(5) 8.685 7.923 6.905
B” 3.471(4) 3.447 3.553 3.857
C” 2.781(4) 2.715 2.706 3.254
εaa 0.8(5) 0.3 -1.5 0.2
ε bb -1.4(7) -1.2 -0.4 -1.1
ε cc -0.0(1) -0.12 -0.04 -0.22
½(εab+ ε ba) <0.2 0.1 1.3 -0.3
½(εbc+ εcb) 0.38 -0.11 0.73
½(εac+ εca) -0.06 0.22 -0.13
Unit: GHz
Rotational Analysis of Band a
G -, asym. rotor,ab-initio, c-type
Band a, exp.
Band a, exp.
T, asym. rotor,ab-initio, a, b-type
G -, asym. rotor,ab-initio, a-b-type
T, asym. rotor,ab-initio, c-type
Rotational Analysis of Band a (G- Conformer)
Asym. rotor,Ab-initio
Asym. Rotor & spin-rotation, fit
Band a, exp.
Band a, exp.
Selectivity of the Spectroscopic Method, Band a
ground state calculations by Gaussian 03, UHF (6-31+g*) excited state calculations by Gaussian 03, CIS(6-31g)
Experimental G+ conformer T conformer G- conformer
A’ 6.427(14) 8.280 7.768 6.496
B’ 3.896(11) 3.460 3.478 3.863
C’ 3.188(11) 2.700 2.653 3.199
A” 6.83(2) 8.685 7.923 6.905
B” 3.903(17) 3.447 3.553 3.857
C” 3.216(11) 2.715 2.706 3.254
εaa 0.1(1) 0.3 -1.5 0.2
ε bb -0.93(7) -1.2 -0.4 -1.1
ε cc -0.23(6) -0.12 -0.04 -0.22
½(εab+ ε ba) -0.53(27) 0.1 1.3 -0.3
½(εbc+ εcb) 0.38 -0.11 0.73
½(εac+ εca) -0.06 0.22 -0.13
Unit: GHz
Simulation of Band B (T conformer)
Band B, exp.
asym. rotor & spin-rotation ab initio
A-X energy separation =55(10)cm-1 (from dispersed
fluorescence experiment).
Quasi-degenerate electronic states A and X render
Hamiltonian model used inadequate.
A-X energy separation =55(10)cm-1 (from dispersed
fluorescence experiment).
Quasi-degenerate electronic states A and X render
Hamiltonian model used inadequate.
Moderate-Resolution LIF Spectrum of 2-Butoxy
26600 26800 27000 27200 27400 27600 27800 28000
26740.7
26761.9
27069.1
27321.027679.8
21.2
559.1
610.7
a
DC
B
A
Frequency/cm-1
a
G- G+T
G- G+T
Conformer Frequency (cm-1)
(Band)
Assignment Obs. Freq. Separation
(cm-1)
Calc. Freq. Separation
(cm-1)
G+ 26761.9 (A)
Origin
G+ 27321.0 (C)
C-O stretch 559.1 532
T 27069.1 (B)
Origin
T 27679.8 (D)
C-O stretch 610.7 536
G- 26740.7 (a) Origin 738
Vibrational Assignment of Bands in 2-Butoxy
Band A, exp.
Convolution of two bands(Band A used, δ=5.95GHz)
Band C, exp.
Simulation of Band C (G+ conformer)
Conclusions and Future work
All three theoretically predicted conformers, G+, G- and T, are identified in the spectrum based on comparison of experimentally “extracted” rotational constants with ab-initio predictions, establishing spectroscopic “fingerprinting” of 2-butoxy conformers.
Quantum chemistry prediction of transition dipole moment and spin-rotation tensor elements significantly simplifies the analysis of fine structure of radicals.
All three theoretically predicted conformers, G+, G- and T, are identified in the spectrum based on comparison of experimentally “extracted” rotational constants with ab-initio predictions, establishing spectroscopic “fingerprinting” of 2-butoxy conformers.
Quantum chemistry prediction of transition dipole moment and spin-rotation tensor elements significantly simplifies the analysis of fine structure of radicals.
The effective Hamiltonian model should be refined to consider the effect of quasi-degeneracy of two lowest states on rotational structure of T conformer.
Other secondary alkoxies to be analyzed.
The effective Hamiltonian model should be refined to consider the effect of quasi-degeneracy of two lowest states on rotational structure of T conformer.
Other secondary alkoxies to be analyzed.