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CYCLOPROPYLACETYLENE STUDIED IN COLD FREE JET EXPANSION, ROOM TEMPERATURE
GAS, AND DILUTE SOLUTION: TIER MODEL IVR
PAM L. CRUM, GORDON G. BROWN, KEVIN O. DOUGLASS, BRIAN C. DIAN JAMES E. JOHNS, PRADEEP
M. NAIR, HYUN S. YOO, AND BROOKS H. PATE
Department of Chemistry, University of Virginia, McCormick Rd., P.O. Box 400319, Charlottesville, VA 22904
CC
C
C
C
H
H
H
H
H
H
Spectroscopic Techniques for Range of Molecular Environments
Frequency Domain
Isolated molecule
MW-IR Double
Resonance
Time Domain
Isolated molecule
FS Transient Absorption
Spectroscopy
Solvated molecule
FS Transient Absorption
Spectroscopy
Vibrational Dynamics of Isolated and Solvated Molecules
Intramolecular Vibrational Energy Redistribution (IVR) and Solvent-Induced Vibrational Energy Relaxation (VER)
IVR– Total amount of vibrational energy constant– Threshold density of states ~10 states/cm-1
– Only pathway for energy flow in isolated molecule– Rate is molecule dependent
VER– Energy removed from molecule (solute)– Rate is solvent dependent
E kIVR
kVER
v=1
v=0
Acetylenic C-H Stretch Fundamental Measurements:kTOT = kIVR + kVER
Acetylenic C-H Stretch Fundamental Measurements:kTOT = kIVR + kVER
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
Vibrational Dynamics in Solution
[≡C―H]
[≡C―H]
Intensity (V)
Fre
quen
cy (
cm-1
)
Nor
mal
spe
cies
13C
_413C
_213C
_1
3310
3320
3330
3340
13C
_5
2
5
14
2
Cyclopropylacetylene (CPA)
Exceptionally fast CCl4 relaxation time (sub ps)
What made this molecule different from the other Terminal Acetylenes studied?
2 TOOLS TO GET AT THE DYNAMICSMW-IR DR : FS TAS : t
Pulsed-IR FTMW Detector
• Advantages– Scan rate = 18 cm-1/hr– No hot bands– Sensitive
• Limitations– Linewidth ~ 0.03 cm-1 – Can’t tell where energy goes
OPO/OPA4 mJ/pulse
of 3 m light0.03 cm-1 bandwidth
Pulsed IRNd:YAG
Laser
CPA Ground State Depletion
Frequency (cm-1)3320 3340 3360
Inte
nsity
(V
)
0.2
0.4
0.6
FTMW monitor 13103.80 MHz
101
202
CC
C
C
C
H
H
H
H
H
H
Slow Scans of CPA
Frequency (cm-1)3336 3337 3338
C.
3332 3333 3334
B.
3327 3328 3329 3330
Inte
nsity (
V)
A.
3316 3317 3318 3319
D. R(1)
P(2)
P(1)
R(2)
101
202
FTMW Monitor13103.80 MHz
0 50 100 150
Sur
viva
l Pro
babi
lity
0.0
0.2
0.4
0.6
0.8
1.0 CPA Survival Probability
= 70 ps
time (ps)
0 5 10 15
Sur
viva
l Pro
babi
lity
0.0
0.2
0.4
0.6
0.8
1.0CPA Survival Probability
= 1.5 ps
= 7 ps
Timescales for IVR in CPA
Frequency DomainFTMW-IR
1 ~ 1 ps
2 = 7 ps
3 = 70 ps
(Single Rotational Level Analysis)
Tier Model of IVRState Specific Dynamics of Ultracold CPA
BrightState
FirstTier
Bath States
1 1 ps 2 = 7 ps
SecondTier
3 = 70 ps
Direct information on the identity of the interacting states is unavailable from IR spectrum
Two ColorTransient Absorption Spectroscopy
TOPAS 1
PUMP
TOPAS 2
PROBE
Variable Delay Stage
CaF2 lens
Sample
/2 plate
Chopper
Probe Reference
Pump Reference
Transmitted Intensity
InSb
InSb InSb
v=2
v=0
v=1
X-H – 100cm-1
X-H
νpump1 ~ 3320cm-1
νprobe ~ 3220cm-1
~ 10μJ~ 12μJ
v=0
v=1 X-H – 40cm-1
X-H
νpump1 ~ 3320cm-1
νprobe ~ 3280cm-1
~ 10μJ~ 10μJ
300K Gas Phase Dynamics by Femtosecond Transient Absorption Spectroscopy
Time (ps)
0 20 40 60 80 100
Nor
mal
ized
Abs
orpt
ion
Cha
nge
(OD
)
0.0
0.2
0.4
0.6
0.8
1.0CPA (g)
v = 2-1 probe1 = 0.6 ps
2 = 6.0 ps
3 = 38 ps
-2 0 2 4 6 8 10 12 14
0.0
0.2
0.4
0.6
0.8
1.0CPA (g)
v = 2-1 probe
1 = 0.6 ps
2 = 6.0 ps
3 = 38 ps
Initial Decay, Recurrences, and Oscillations: Data Agreement
Time (ps)
0 10 20 30 40 50
Nor
ma
lize
d A
bso
rptio
n C
ha
nge
(O
D)
0.0
0.2
0.4
0.6
0.8
1.0 CPA (g)v = 2-1 probe
Survival Probability
0 10 20 30 40 50
-0.05
0.00
0.05
0.10 Residuals
Gas Phase Measurement of Population Relaxation into CH Bend Overtone Levels
CPA (g)PS Measurement
Time (ps)
0 50 100 150 200 250 300
0
2
4
6
8
rise ~ 1 ps (laser limited)fall1 ~ 7 psfall2 ~ 40 ps
Normal Vibrational Mode Shifts due to 13C
Isotope Shift (cm-1)
-60 -50 -40 -30 -20 -10 0 10
Nor
mal
Mod
e F
requ
ency
of
Nor
mal
Spe
cies
(cm
-1)
0
500
1000
1500
2000
2500
3000
3500
C5C4C3C2 and C1
Inte
nsity
(V
)
Frequency (cm-1)
Normal species
13C_4
13C_2
13C_1
3310 3320 3330 3340
13C_5
2
5
1
4
2
C5C4C1C2
GSD IR Spectra of CPA:
Normal Species and 13C
(Natural Abundance)
Inte
nsi
ty (
V)
Frequency (cm-1)
Normal species
13C_4
13C_2
13C_1
3310 3320 3330 3340
13C_5
2
5
1
4
2
13C Isotopomers:Effect on Dynamics
time (ps)
0 5 10 15 20
Inte
nsity
0.0
0.2
0.4
0.6
0.8
1.0NS13C_213C_5
Inte
nsity
(V
)
Frequency (cm-1)
Normal species
13C_4
13C_2
13C_1
3310 3320 3330 3340
13C_5
2
5
1
4
2
Vibrational Dynamics of CPA in 300K Gas
Acetylenic CH StretchBrightState
Acetylenic CH Bend Overtone
Excitation (1200 cm-1)
Third Tier
1 ~ 1 ps 2 = 7 ps
SecondTier
3 = 40 ps
Comparison of 300K Gas and Dilute Solution Dynamics (0.05 M CCl4)
Initial rates are the samein gas and solution butsolution relaxation ismore efficient
Solution relaxation is not single exponential and “breaks off” at about 1/5 of the full amplitude
Vibrational Dynamics of CPA in Dilute Solution
Acetylenic CH StretchBrightState
Acetylenic CH Bend Overtone
Excitation (1200 cm-1)
Third Tier
1 ~ 1 ps 2 = 7 ps
SecondTier
3 = 40 ps
Solution Phase Bleach Recovery and 300K Gas Dynamics
CPAGas v = 2-1 ProbeCCl4 v = 1-0 Probe
Time (ps)0 50 100 150 200
Nor
mal
ized
Abs
orpt
ion
Cha
nge
(OD
)
0.0
0.4
0.8
1.2
0 10 20 30
0.0
0.4
0.8
1.2
CCl4: 1 = 0.6 ps 2 = 7 ps 3 = 41 ps
Gas: 1 = 0.6 ps 2 = 6 ps 3 = 38 ps
Summary of CPA Dynamics
Free jet expansion (FTMW):
1 ~ 1 ps
2 = 7 ps
3 = 70 ps
300K Gas phase fs data:
1 ~ 0.6 ps
2 = 7 ps
3 = 38 ps
Dilute Solution fs data:
1 ~ 0.6 ps
2 = 7 ps
3 = 40 ps
Thermal rate enhancement in the final IVR time scale is typicallyobserved (coupled modes are thermally populated).
Conclusions
• Dynamics in all cases dominated by intramolecular processes
• CPA IVR dynamics follow Tier Model
• Strong coupling to first tier– States with two quanta in C-H bend
Acknowledgements
Pate Lab Group Members
Funding:• NSF Chemistry• SELIM Program• University of Virginia• John D. and Catherine T. Macarthur Foundation• The Jeffress Trust
Quantum DecoherenceModel Calculation: Coupled Degenerate States
H = Hmol(Q1,Q2) + Hbath({qi}) + Hmol-bath
Hmol = H1(Q1) + H2(Q2) + W12 : E1 = E2
Hmol-bath kQn2qi : Only pure dephasing terms included
The dynamics are modeled using random matrix methods:
W12E1 + Ebath
H =W12
E2 + Ebath
The dephasing interactions for the two coupled intramolecular states are assumed to be uncorrelated.
N = 24 N = 24 N1 = 9 N2 = 40
Extending the Quantum Decoherence Model to Other Common IVR Models
I. IVR in a Sparse II. IVR Dominated III. Tier ModelIntramolecular Bath by a Single, Strong
Resonance
Solvent Dephasing Effects for Tier Model IVR
Solvent Dephasing Effects for Tier Model IVR
GSD Slow Scans of CPA
frequency (cm-1)
3335 3336 3337 33383331 3332 3333 3334
3327 3328 3329 3330
Inte
nsity
(V
)
3316 3317 3318
P(1)R(1)
P(2) R(2)
Inte
nsity
(V
)
0.2
0.3
0.4
0.5
0.6
Frequency (cm-1)
3320 3330 3340 3350
0.01
0.02
0.03
0.04
12C species
13C species
GSD of 13C Species
CC
C
13C
C
H
H
H
H
H
H
Dynamics from frequency-domain spectrum:
All Bands
Bands 6-13
Bands 9-13
Frequency (cm-1)
3320 3330 3340
Calc.1.5ps6 ps
time (ps)
0 5 10 15
Free jet expansion timescales:
1 ~ 1.5 ps
2 ~ 6 ps
Comparing ultracold free jet expansion to gas-phase room-temperature
Gas-Phase Ultrafast Time-Domain
Isolated molecule
Room-Temp Dynamics of all
thermally populated levels (vibrational hot bands and rotational)
fs transient absorption spectroscopy
Free Jet Expansion Frequency-Domain
Isolated molecule
Ultracold Dynamics of a
single rotational level (State-Resolved)
MW-IR Double-Resonance
Frequency (cm-1)3300 3320 3340 3360
Inte
nsi
ty
0.2
0.4
0.6
0.8
1.0
frequency spectrumfs pulse (norm)
~ 300 fs pulse
~ 100 cm-1 bandwidth
0 50 100 150
Sur
viva
l Pro
babi
lity
0.0
0.2
0.4
0.6
0.8
1.0 CPA Survival Probability
= 70 ps
time (ps)
0 5 10 15
Sur
viva
l Pro
babi
lity
0.0
0.2
0.4
0.6
0.8
1.0CPA Survival Probability
= 1.5 ps
= 7 ps
0 50 100 150
Sur
viva
l Pro
babi
lity
0.0
0.2
0.4
0.6
0.8
1.0 CPA Survival Probability
= 70 ps
time (ps)
0 5 10 15
Sur
viva
l Pro
babi
lity
0.0
0.2
0.4
0.6
0.8
1.0CPA Survival Probability
= 1.5 ps
= 7 ps
Timescales for IVR in CPA
Frequency DomainFTMW-IR
1 = 1.5 ps
2 = 7 ps
3 = 70 ps
Time DomainGas Phase
1 = 0.1 (0.02) ps
2 = 7 (0.9) ps
3 = 50 (15) ps
Time (ps)
0 5 10 15 20
No
rma
lized
Ab
sorp
tion
Ch
ang
e (
OD
)
0.0
0.2
0.4
0.6
0.8
1.0 CPA (g)v = 2-1 probe
1 = 0.6 ps
2 = 7.0 ps
3 = 42 ps
0 50 100 150
Sur
viva
l Pro
babi
lity
0.0
0.2
0.4
0.6
0.8
1.0 CPA Survival Probability
= 70 ps
time (ps)
0 5 10 15
Sur
viva
l Pro
babi
lity
0.0
0.2
0.4
0.6
0.8
1.0CPA Survival Probability
= 1.5 ps
= 7 ps
Timescales for IVR in CPA
Frequency DomainFTMW-IR
1 = 1.5 ps
2 = 7 ps
3 = 70 ps
Time DomainGas Phase
1 = 0.6 ps
2 = 7 ps
3 = 42 ps
Time (ps)
0 5 10 15 20
No
rma
lized
Ab
sorp
tion
Ch
ang
e (
OD
)
0.0
0.2
0.4
0.6
0.8
1.0 CPA (g)v = 2-1 probe
1 = 0.6 ps
2 = 7.0 ps
3 = 42 ps
Time DomainSolution Phase
1 = 0.6 ps
2 = 7 ps
3 = 60 ps
CPACCl4 v = 1-0 Probe
Time (ps)
0 50 100 150 200
No
rma
lize
dA
bso
rptio
n C
ha
ng
e (O
D)
0.0
0.4
0.8
1.2
0 10 20 30
0.0
0.4
0.8
1.2
Comparison of Solution Rate and Initial Gas-Phase IVR Rate
kTOT = kIVR + kVER
Dynamics of the Acetylenic C-H stretch for
Gas-Phase CPA
Time (ps)
0 5 10 15 20
No
rma
lized
Ab
sorp
tion
Ch
ang
e (
OD
)
0.0
0.2
0.4
0.6
0.8
1.0 CPA (g)v = 2-1 probe
1 = 0.6 ps
2 = 7.0 ps
3 = 42 ps
CPA (g)PS Measurementv=1 - v=0 Probe
0
4
8
12
16
CPA (g)PS Measurementv=2 - v=1 Probe
Abs
orba
nce
Cha
nge
(mO
D)
0
2
4
6
8
CPA (g)PS Measurement-40 cm-1 Probe
Time (ps)
0 50 100 150 200 250 300
0
2
4
6
8
Femtosecond Resolution Picosecond Resolution
Dynamics of the Acetylenic C-H stretch for Solution-Phase CPA
0.00
0.01
0.02
0.03 CPA (CCl4)
CPA (Gas)
Time (ps)
0 4 8 12 16 20
Abs
orpt
ion
Cha
nge
(OD
)
0.00
0.01
0.02
0.03 CPA (CCl4)
1 = 0.65 ps
CPA
Gas v = 2-1 Probe
CCl4 v = 1-0 Probe
Time (ps)
0 50 100 150 200
No
rmal
ized
Abs
orp
tion
Ch
ang
e (O
D)
0.0
0.4
0.8
1.2
0 10 20 30
0.0
0.4
0.8
1.2
13C Isotopomers:Effect on Dynamics
time (ps)
0 5 10 15 20
Inte
nsity
0.0
0.2
0.4
0.6
0.8
1.0NS13C_413C_5
Data Agreement
time (ps)
0 10 20 30 40 50
Inte
nsi
ty
0.0
0.2
0.4
0.6
0.8
1.0 Average of all speciesGas femto
time (ps)
0 5 10 15 20
Inte
nsity
0.0
0.2
0.4
0.6
0.8
1.0NS13C_113C_213C_413C_5
Average Survival Probability(all species)
FS Gas Dynamics
13C Isotopomers:Normal Vibrational Mode Shift &
Effect on Dynamics
The survival probability calculation for the normal species of CPA is compared to the same calculation for each of the 13C isotopomers.
time (ps)
0 5 10 15 20
Inte
nsity
0.0
0.2
0.4
0.6
0.8
1.0NS13C_113C_213C_413C_5
Isotope Shift (cm-1)
-60 -50 -40 -30 -20 -10 0 10
Nor
mal
Mod
e F
requ
ency
of
Nor
mal
Spe
cies
(cm
-1)
0
500
1000
1500
2000
2500
3000
3500
C5C4C3C2 and C1
Solution Phase Measurement of Population Relaxation into CH Bend
Overtone Levels
Time (ps)
-5 0 5 10 15 20 25 30
Abs
orpt
ion
Cha
nge
(OD
)
0.00
0.05
0.10
0.15
CPA (CCl4)
PS Measurementsv = 2-1 Probe
-40 cm-1 Probe
rise = 1.2 ps (laser limited)fall1 = 6.4 psfall2 = 45 ps
Transient Absorption Spectroscopy for
Terminal Acetylenes
v=2
v=0
v=1
0
0–108cm-1
1 2
Excited StateAbsorption
SEP
GSD
0– 40cm-1
vCHs = 0,
vCHb= 2
+ 2100 cm-1 in other modes
0
vCHs = 0,
vCHb= 0
+ 3300 cm-1 in other modes
1
1
1
2
2
Excited State Absorption
Bend Overtone Absorption
Bleach Recovery