Survey
* Your assessment is very important for improving the work of artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the work of artificial intelligence, which forms the content of this project
Vibrational cooling of large molecules
in supersonic expansions: The case of
C60 and pyrene
Bradley M. Gibson and Jacob T. Stewart, Department
of Chemistry, University of Illinois at Urbana-Champaign
Benjamin J. McCall, Departments of Chemistry and Astronomy,
University of Illinois at Urbana-Champaign
Why study C60?
Symmetry
Figure from:
Astrochemical Relevance
J. Cami, J. Bernard-Salas, E. Peeters, and S.E. Malek. Science 329, 1180 (Sep. 2010)
{2}
How do we look for C60?
β’ High- temperatureC(~850
K) Pressure
oven
Vapor
60
β’ Cooling via continuous
supersonic expansion
β’ CW-CRDS detection, ~1185 cm-1
Figures from: B. Brumfield. Development of a quantum cascade laser based spectrometer for high-resolution spectroscopy of
gas phase C60. UIUC, 2011.
{3}
What do we expect to see?
β’ Branch heads possible
S/N=
ππ§ ππ β² πΏπππ‘
βπ£(πππΈπ΄ )
βB
β’ Pinhole nozzle: ~2
β’ Slit nozzle: ~40
Figure from:
J. T. Stewart, B. Brumfield, B. M. Gibson, B. J. McCall. In preparation.
{4}
What did we actually see?
Estimated:
Observed:
(NEA ~0.6 ppm)
Figures from: J. T. Stewart, B. Brumfield, B. M. Gibson, B. J. McCall. In preparation.
{5}
Why didnβt we see anything?
High-Temperature
Ground State Oven
Population
Alignment
1.0
Fraction in Ground State
0.8
0.6
0.4
0.2
0.0
0
Figure from:
50
100
200
150
Vibrational Temperature (K)
250
300
B. Brumfield. Development of a quantum cascade laser based spectrometer for high-resolution spectroscopy of
gas phase C60. UIUC, 2011.
{6}
Do other molecules cool efficiently?
Pyrene
β’ Oven temp ~430 K
β’ Estimated from absorption depth
β’ Tvib 60-90 K
D2O
β’ Oven temp ~800 K
β’ Estimated from hot band
β’ Tvib > 1000 K
{7}
How does vibrational cooling work?
V-T Transfer
v=2
v=1
kBT
kBT
v=0
Translational Energy: β
Vibrational Energy: β
See also:
M. E. Sanz, M. C. McCarthy and P. Thaddeus. J. Chem. Phys. 122, 194319 (2005)
{8}
How does vibrational cooling work?
V-T Transfer
v=2
kBT
v=1
kBT
v=0
Translational Energy: β
Vibrational Energy: β
See also:
M. E. Sanz, M. C. McCarthy and P. Thaddeus. J. Chem. Phys. 122, 194319 (2005)
{9}
How does vibrational cooling work?
V-T Transfer
-4
10
-6
Fraction in Ground State
(After Cooling)
10
-8
10
-10
10
-12
10
-14
10
-16
10
-18
10
-20
10
300
400
500
600
Initial Temperature (K)
700
800
{10}
How does vibrational cooling work?
Intramode Relaxation
v=2
v=1
v=0
See also:
M. E. Sanz, M. C. McCarthy and P. Thaddeus. J. Chem. Phys. 122, 194319 (2005)
{11}
How does vibrational cooling work?
Intermode Relaxation
Bend
See also:
Stretch
M. E. Sanz, M. C. McCarthy and P. Thaddeus. J. Chem. Phys. 122, 194319 (2005)
{12}
How does vibrational cooling work?
Cluster Predissociation
Bend
See also:
Intermolecular
Stretch
G. Ewing. Chem. Phys. 29, 253 (Apr. 1978)
{13}
How can we produce colder vapor?
Laser Ablation
β’ Initial temperature >1900K
Laser Desorption
β’ Initial temperature uncertain
β’ Ground state detectable by R2PI
See also:
E. E. B. Campbell, I. V. Hertel, Ch. Kusch, R. Mitzner, and B. Winter. Synth. Mat. 77, 173 (1996)
R. E. Haufler, L-S. Wang, L. P. F. Chibante, C. Jin, J. Conceicao, Y. Chai, and R. E. Smalley. Chem. Phys. Lett. 179, 449
(1991)
{14}
How can we produce colder vapor?
Supercritical Fluid Expansion
β’ Initial temperature solvent dependent (~450 K)
β’ CO2 w/ toluene co-solvent β aids cooling
β’ Low vapor flux (~1013 molecules s-1)
See also:
C. H. Sin, M. R. Linford, and S. R. Goates. Anal. Chem. 64, 233 (1992)
{15}
Conclusions
β’
β’
β’
β’
C60 signal not yet observed
Lack of signal likely due to poor vibrational cooling
Efficient cooling highly dependent upon initial temperature
New vaporization technique required
{16}
Acknowledgements
β’ McCall Group
β’ Brian Brumfield
β’ Claire Gmachl
{17}