spectra, structures, and dynamics of weakly bound clusters from dimers to nonamers
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Spectra, Structures, and Dynamics of Weakly Bound Clusters from Dimers to Nonamers. Wolfgang Jäger Department of Chemistry, University of Alberta. Potential Energy Curves for H-Cl and Kr-Xe. Significance of van der Waals Interactions. Significance, continued …. - PowerPoint PPT PresentationTRANSCRIPT
Spectra, Structures, and Dynamics of Weakly Bound Clusters from
Dimers to Nonamers
Wolfgang Jäger
Department of Chemistry, University of Alberta
Potential Energy Curves for H-Cl and Kr-Xe
Significance of van der Waals Interactions
Significance, continued …
Fourier Transform Microwave Spectrometer
Frequency range: 4 – 26 GHz (ca. 0.1 – 1 cm-1)
microwave cavity
nozzle
Fourier Transform Microwave Spectrometer
Outline for Remainder of Talk
• large amplitude motions in van der Waals complexes
• three-body effects in ternary and quaternary clusters
• successive micro-solvation of molecules with helium atoms
Ne-Ethylene in its Principal Inertial Axis System
Energy Level Diagram of Ne-trans-C2D2H2
(Out-of-Plane Motion)
Energy Level Diagram of Ne-trans-C2D2H2
(In-Plane Motion)
RGN-NH3 Complexes
Ne, Ar,a Kr NH3 Ne, Ar NH3 Ne, Ar NH3
15NH3 15NH3 15NH3
ND3 ND3 ND3
ND2H ND2H ND2HNDH2 NDH2 NDH2
a Ar-NH3, Ar-15NH3 by D. D. Nelson Jr. et al., JCP 85, 512 (1986); E. Zwart et al., JCP 95, 793 (1991); and many others.
J=4-3 Transitions of Deuterated Ar3-Ammonia
Ammonia internal rotation in RGN-NH3 clusters
14N nuclear quadrupole coupling constants in MHz
14N nuclear quadrupole coupling constant in free ammonia: =-4.0898 MHz
M. D. Marshall and J. S. Muenter, JMS 85, 322 (1981).
Three-Body Interactions
Three-body interactions
crystal structures of solid rare gases
face-centered cubic
(observed)hexagonal close-packed
(predicted using pairwise additivity)
NeAr
Ne2Ar
NeAr2
Ne3Ar
Ne2Ar2
NeAr3
Pure Rare Gas Clusters
Survey Scan with Ne/Ar Sample Gas Mixture
Transitions JKaKc = 202-101 of Ne2Ar
Rotational Energy Level DiagramsNe2Ar NeAr2
Comparison with Theoretical Calculations
Rotational
ConstantExperiment
pairwise
additive
pairwise +
AT term
A (MHz) 4724.1(8) 4742.30 4730.61
B (MHz) 2484.64(6) 2488.88 2486.92
C (MHz) 1597.88(6) 1592.57 1590.09
References:
1. Ernesti & Hutson, JCP 103, 3386 (1995).
2. Aziz & Slaman, Chem. Phys. 130, 187 (1989). Ne-Ne PES ~ viscosity data & high energy total cross sections
3. Barrow & Aziz, JCP 89, 6189 (1988). Ne-Ar PES ~ low energy total cross section data & low temperature second virial coefficients & room temperature diffusion coefficients & high energy total cross sections modified (scaled re) to fit MW data [JCP 102, 1181 (1995)].
Helium – Molecule Complexes
very weak interactions
high zero point energy spectra sample significant portion of PES attractive systems for ab initio calculations
relevant wrt spectroscopy of doped helium droplets
possibility to measure Hen-molecule systems?
S. Grebenev, J. P. Toennies, and A. F. Vilesov, Science 279, 2083 (1998).
Helium Nanodroplet Isolation Spectroscopy (Background)
Grebenev, Toennies, Vilesov, Science 279, 2083 (1998).
Helium Nanodroplet Isolation Spectroscopy (more Background)
Grebenev, Toennies, Vilesov, Science 279, 2083 (1998).
He-OCS in its Principal Inertial Axes System
Measured Rotational Transitions of He-OCS Is o to p o m er H e-O C S H e -O C 34S H e-O 13C S H e -O C 33SJ ' - J" νobs νob s νobs F'- F" νobs K a' , K c' K a" , K c" 1 0 ,1 - 0 0 ,0 9 1 6 1 . 8 1 2 0 a 8 9 5 8 .4 2 4 4 9 1 4 9 . 1 9 0 0 0 .5 -1 . 5 9 0 6 3 . 2 5 6 6 2 .5 -1 . 5 9 0 5 8 . 4 8 2 1 1 .5 -1 . 5 9 0 5 2 . 5 0 8 0
1 1 ,0 - 1 0 ,1 9 4 8 0 . 3 4 7 0 a 9 5 1 5 .6 5 4 0 9 4 4 8 . 8 0 0 3 1 .5 -2 . 5 9 4 9 9 . 9 7 3 5 0 .5 -1 . 5 9 4 9 9 . 4 0 1 6 2 .5 -2 . 5 9 4 9 6 . 3 4 1 2
1 1 ,1 - 0 0 ,0 1 6 8 4 1 . 2 6 8 0 1 6 7 4 6 .4 0 3 7 1 6 7 9 8 . 0 2 9 5 1 .5 -1 . 5 1 6 7 9 4 . 2 7 1 9 2 .5 -1 . 5 1 6 7 9 1 . 9 5 9 4 0 .5 -1 . 5 1 6 7 9 0 . 11 0 1
1 1 ,0 - 1 1 ,1 1 8 0 0 . 8 9 3 0 a - - 2 1 ,1 - 2 1 ,2 5 3 8 6 . 5 2 4 0 a - - 2 0 ,2 - 1 0 ,1 1 8 0 2 9 . 2 8 4 0 a 1 7 6 4 8 .0 8 5 6 1 8 0 0 3 . 6 3 9 8 1 .5 -1 . 5 1 7 8 3 8 . 3 6 7 6 3 .5 -2 . 5 1 7 8 3 4 . 1 0 9 4 2 .5 -1 . 5 1 7 8 3 4 . 0 8 3 8 0 .5 -0 . 5 1 7 8 3 3 . 6 1 7 3 2 .5 -2 . 5 1 7 8 2 8 . 1 0 8 2 1 .5 -0 . 5 1 7 8 2 7 . 6 1 9 9a K . H ig g in s a n d W . K lem p ere r , J . C h em . P h y s . 11 0 , 1 3 8 3 (1 9 9 9 ) .
J ' - J" νobs νob s νobs F'- F" νobs K a' , K c' K a" , K c"
He2-OCS in its Principal Inertial Axes System
JKaKc=101-000 Transitions of He2-OCS
Multidimensional Assignment Procedure
a) infrared predictions
b) sample conditions (pressure, temperature)
c) double resonance experiments
d) consistency of isotopic data
e) spectral fits
Effect of Nozzle Cooling on Cluster Formation
He6-OCS, J=3-2 at 11176.83 MHz, 0.01% OCS in He at 20.4 atm100 averaging cycles
nozzle at room temperatureS/N ~ 2
nozzle at dry ice temperature (-78.5 C)S/N ~ 40
Double Resonance Spectrometer
Double Resonance Spectrometer (Schematics)
Double Resonance Experiments on He6-OCS
signal: J-3-2, 11176.83 MHzpump: J=2-1, 7588.75 MHz20 averaging cycles
pump power(continuous)
off
-3 dBm
3 dBm
Vibrational Frequency Shifts of HeN-OCS Clusters
experimental valuesTang et al., Science, accepted.
values from Whaley and co-workers, JCP 115, 10225 (2001).
Moment-of-Inertia Shifts of Isotopomers
Proposed Structure of He8-OCS
Spectroscopic Constants of HeN-OCS ClustersMolecule B D
Free OCS 6081.59 1.31x10-5
He-OCS 13208.57
5504.18 4582.80
3661.42
0.950
He2-OCS 5803.39
4546.34 3782.81
3019.28
---
He3-OCS 3104.57 5.11
He4-OCS 2591.95 0.881
He5-OCS 2225.15 0.234
He6-OCS 1910.49 2.60
He7-OCS 1682.98 1.29
He8-OCS 1447.73 2.00
OCS in 4He droplet
(N~10,000)
2194.5(90) 11.4(3)
Rotational Constants of HeN-OCS Clusters
Potential Energy Surface of He-N2O
CCSD(T) level of theory, aug-cc-pVDZ basis set
Bound State Calculations
Transition Experiment Bound Difference
101 - 000 18560.5 MHz 18435.1 MHz 0.68 %
111 - 000 19743.3 MHz 19704.6 MHz 0.20 %
110 - 111 6295.0 MHz 6222.1 MHz 1.16 %
110 - 101 7477.5 MHz 7491.5 MHz -0.19 %
220 - 221 5035.0 MHz
211 - 212 18465.7 MHz
202 - 111 30342.8 MHz
211 - 110 30657.1 MHz
202 - 101 31612.3 MHz
211 - 110 42900.7 MHz
Wavefunction of Ground State
Wavefunctions of 1st and 2nd Excited States
J=1-0 Spectrum of He5-N2O
He6-N2O in its Principal Inertial Axes System
AcknowledgementsDr. Yunjie Xu (H31)Dr. Aiko Huckauf
Dean CourtDr. Yaqian Liu (H19)Dr. Jennifer van Wijngaarden (H15)Dr. Silas Ngari
Kai Brendel (H30)Hans OsthoffWendy Topic
Tobias KlemmerJames Song
Mike GerryBob McKellarPN Roy
NSERCASRACIPI