Date post: | 11-Jan-2016 |
Category: |
Documents |
Upload: | ira-sullivan |
View: | 219 times |
Download: | 0 times |
A First-Principles Model of Fermi Resonance in the Alkyl CH Stretch Region: Application to
Hydronaphthalenes, Indanes, and Cyclohexane
Funded by NSF and DOE
Molecular Spectroscopy Symposium, June, 2014
Nathanael Kidwell, Tim Zwier, Danny Tabor, and Ned Sibert
DPE C2h
DPOE C2h
DPE C2
DPOE C2
Probing molecular structure with CH chromophoreswith the Zwier Group at Purdue
Our goal is to develop theoretical models that will enable us to use the CH stretch as a probe of environment. Initial work focuses on developing Hamiltonians that allow us to predicting spectra of the molecules based on input from electronic structure theory and couplings that are scaled to the DPE C2h spectrum.
so/ss so
so/ssso/ss
ss/so as
asas
ss/so
ss as
asss/so
Background
CH2 Scissor CH Sym Stretch CH Asym Stretch 1450 cm-1 2960 cm-1 2980 cm-1
Images from Molecular Vibration; Wikipedia, the free encyclopedia
1500 3000
Wavenumber (cm-1)
A
/ /
ss asso
2900 3000
ss as
2900 3000
1) Calculate Ess, Eas, Eso and W with DFT.
2) Scale the results using a, b, and c.
3) For different X-CH2-Y species use the same a, b, and c.
The Strategy
The Hamiltonian
Stretch-Bend Fermi Coupling
An Aside
One can use either a symmetrized representation
Or one can use a localized representation
Complication No. 1 The spectra are extremely congested.
SolutionFind a good experimentalist.
Complication No. 2Normal modes are sensitive to small potential changes.
SolutionUse local modes.
Local modes are insensitive to small potential changes.Local modes potentials are transferrable.The local mode picture is approximate.
1476 cm-1
1479 cm-1
The CH2 Scissor Vibrations of TetralinNM picture hides interactions with scissor modes
1466 cm-1
The Scaled & Localized CH2 Scissor Vibrations of Tetralin
Enough with the preliminaries.
Onto the main event.
THNI2M
tetralin
A
C
AB
14DHN A
A
B
A
indane
A
B
A
indene 12DHN
B
A
B
A
A
Comparison to Normal Mode Results
Model HamiltonianStart with a zero order Hamiltonian and dipole
N
iii nH
1
)0( )2
1(
N
iiiq
1
)0(
Add some Fermi coupling terms
kjikjiikl chaaafH
,,
)1( .).(
Pick a basis, diagonalize the H matrix, and calculate the spectrum.
B3LYP/6-311+G(d,p)
12DHN Spectra
With anharmonic terms included.
12DHN Spectra
CH2 Decoupling Approximation
CH2 Decoupling Approximation
Calculate bilinear terms in dipole
14DHN Spectra
Comparison of Model Results to Experimental Results
CH2 Decoupling Approximation
Concluding Remarks
• Developed a model for CH2 stretches.• Hamiltonian has parameters that are fit to one
member of a group of similar species.• Working to extend to CH3 groups.• Working to better parameterize the
Hamiltonian.• Would like to add waters.
On to CH3 groups!
CH3-CD3 R1
F2
F1
R2
R3 F3