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Flow of Vibrational Energy in Polyatomic Molecules:Using Acetylenic Anharmonic Couplings to Follow
Vibrational Dynamics
Steven T. Shipman and Brooks H. Pate
Department of ChemistryUniversity of Virginia
BrightState
FirstTier
Bath StatesSecondTier
Tier Model of IVR
Solvent Accommodates Energy Difference at Each Step of the Relaxation “Cascade”
IR Pump
C-H StretchSolute Vibrational Levels
Vibrational Energy Relaxation (VER) of Polyatomic Molecules in Solution
Watching Localized Energy Transport
Many IVR studies follow the departure of energy from an initially prepared state rather than the arrival of energy elsewhere in the molecule.
Exceptions: Time-Resolved IR-Raman (Dlott)IR pump - UV probe (Crim, Abel)
A few difficulties: most low-frequency modes are delocalized across the entire molecule and are hard to directly monitor.
Terminal acetylenes have several nice features:
CC-H bend is at low frequency (625 cm-1) but localizedStretch-bend coupling larger than linewidths in RT sol’n phaseCC-H stretch is very intense
Using Anharmonic Couplings to Follow Dynamics
Following late-stage relaxation dynamics is hindered because directly probing low-frequency modes is difficult.
So let’s indirectly probe them…
E(v1,v2,v3,…) = ∑ i (vi + 1/2) + ∑ ∑ xij (vi + 1/2) (vj + 1/2) + …i i j ≥ i
Anharmonic interaction between acetylenic C–H stretch (3330 cm-1) and acetylenic C–H bend (600 cm-1) is -20 cm-1.
The transient absorption signal at 3330, 3310, and 3290 cm-1 allows us to extract the dynamics of the low-frequency bending mode.
Two Color Transient Absorption Spectroscopy
OPA 2
PUMP
OPA 1
PROBE
Variable Delay Stage
CaF2 lens
Sample
λ/2 plate
Chopper
ProbeReference
PumpReference
InSb
InSb InSb
Monochrom
ator
1 kHz repetition rateIndependently tunable OPAsTuning range ~1–6 µm, ~5–10 µJ/pulseGas and liquid samples
Transmitted Intensity
Polarizer
Vibrational Transitions of Terminal Acetylenes
Ground StatePump
v = 1–C–H
v = 1=C–H
3100
cm
-1
2950
cm
-1
Probe
v = 1≡C–H
v = 0bend
v = 1bend
v = 2bend
3310
cm
-1
3290
cm
-1
3270
cm
-1
What States are Being Prepared?
Ultrafast pulses are broad!High-resolution data is necessary to know what states are prepared.
mbey 202-101 (13567.966 MHz)1.5 ps pulse (20 cm-1 FWHM)
Molecular Beam Data – Butyne
GSD-DP Measurements202 – 101 (17259.905 MHz)10.8 cm-1 / hr, 20 averages
Butyne – C–H Stretch Identification
3007.13000.32943.32929.82914.5
Scaled Harm2982.92979.32911.22969.12920.0
Anharm2984.22983.12912.62986.62939.5
Cubic Rediagasym –CH3
asym –CH3 asym –CH2
sym –CH3
sym –CH2
Mode Description Intensity26.830.96.7
32.120.0
2827 cm-1
4.9 ps
3290 cm-1
16.9 / 29.7 ps
Butyne in CCl4 – The 2941 cm-1 Band
v = 0
v = 1
v = 2
v = 0
v = 1v = 1
Molecular Beam Data – Methylbutenyne
GSD-DP Measurements202 – 101 (13567.966 MHz)10.8 cm-1 / hr, 20 averages
Methylbutenyne in CCl4 – The 3101 cm-1 Band
vbend = 1
vbend = 2
3290 cm-1
3270 cm-1
18.4 / 31.0 ps
15.3 / 32.1 ps
vbend = 1
vbend = 2
Methylbutenyne in CCl4 – The 2925 cm-1 Band420
-2
0 50 100 150 200-50Delay Time (ps)
420
-2420
-2
Tra
nsie
nt A
bsor
ptio
n (m
OD
) 3310 cm-1
3290 cm-1
3270 cm-1
vbend = 0
10.7 / 34.6 ps
16.1 / 32.0 ps
9.9 / 21.0 ps
Pump 2925 cm-1 Pump 3101 cm-1
Pump
2925
3101
Probe
331032903270
32903270
Bend
012
12
Fast
10.7 (1.1)16.1 (1.3)9.9 (2.2)
18.4 (3.4)15.3 (5.9)
Slow
34.6 (5.4)32.0 (1.9)21.0 (5.1)
31.0 (4.6)32.1 (8.2)
2925 2925 3.7 (0.5)0 N/A
Methylbutenyne Results
Butyne and Methylbutenyne – Relaxation Tiers
BrightState
FirstTier
Bath StatesSecondTier
t = 0 ps
t = 5 ps t = 15 pst = 30 ps
–C–H stretches –C–H bends ≡C–H bends Solvent modes
Summary
The strong stretch-bend coupling of the acetylenic C–H stretch can be exploited to probe late stages of the vibrational relaxation process.
In methylbutenyne, a comparison of the dynamics of states with vbend = 1 and vbend = 2 indicates that the methylic and ethylenic stretches explore qualitatively different relaxation pathways.
Gas phase measurements need to be made for comparison, but the solvent contribution to the relaxation is no faster than 30 ps.
Acknowledgements
NSF - Chemistry
Current and former Pate Lab members
GSD-DP Measurements202 – 101 (17259.905 MHz)10.8 cm-1 / hr, 20 averages
Weak Butyne Bands Near 2981
32903310 (x –1.05)
Methylbutenyne
pump 2941probe 2941
1.4 (0.4) ps recovery
Butyne one-color measurement
One-color measurements hindered by stimulated emission.
Vibrational Dynamics in Solution
Acetylenic C-H Stretch Fundamental Measurements:kTOT = kIVR + kVER
E kIVR
kVER
v=1
v=0
Yoo, H.S. et al. J. Phys. Chem A 2004 108(8) 1348-1364Yoo, H.S. et al. J. Phys. Chem A 2004 108(8) 1365-1379Yoo, H.S. et al. J. Phys. Chem A 2004 108(8) 1380-1387
Fre
quen
cy (
cm)
-1
500
1000
1500
2000
2500
3000
3500
CHstretch and (CCstretch + 2CHbend)
v=2 CHbend
CCstretch
CHbend
H
C
C
RAcetylenic CH stretch is a local mode oscillator with motion dominated by the terminal H-atom.
This atom extends approximately 3A from the R group.-CH2CH3
-CHFCH3
-C(CH3)=CH2
-CH(CH3)2
-CH2Br
-CH2Cl
-CH2F
-CH3
-C(CH3)3
-Si(CH3)3
R group structure
Properties of Acetylenic Compounds
Bright State
W
C-H
Dark StatesMolecular
Eigenstates
Bright States vs. Eigenstates
Pulsed-IR FTMW Detector
OPO/OPA0.02 cm-1 bandwidth
Pulsed IRNd:YAG
Laser
10 Hz repetition rateTuning range ~1 – 4 µm, ~5 – 10 mJ/pulseMolecular Beam Samples – No Hot Bands!
The Molecules Under Study
1-butyne methylbutenyne
tert-butyl acetylene trimethyl silylacetylene
2973 / 2973 cm-1
15.4 ps2964 / 2964 cm-1
8.4 ps
Preliminary Data – TBA and TMSA in CCl4
Long lifetime of bright state implies that couplings are not large.
2982 cm-1
13.4 ps
Butyne – Coupling to Other C–H Bends
5 cm-1 resolution makes identification of probed band difficult…… But the bleach indicates a frequency shift of at least that amount.
From Xij, most likely couplings are to bending modes near 1470 cm-1.(Couplings on the order of 20 cm-1 to all –CH3-based stretches.)
Pump
2941
Probe
3290
Bend
1
Fast
16.9 (2.2)
Slow
29.7 (2.9)
294128272982
29414.9 (0.7)
13.4 (0.7)
1.4 (0.4)00
0N/AN/A
N/A
Butyne Results
3290 time constants are in agreement with methylbutenyne results.
Same general relaxation pathways? Need to check at 3270…
Difficult to say if 2982 and 3290 time constants are in fact identical.