Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region...
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Transcript of Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region...
Spectroscopy of NCNCS at the Canadian Light Source:
the far-infrared spectrum of the ν7 region from 60-140 cm-1
(and beyond…)Dennis W. Tokaryk, Stephen C. Ross
Department of Physics and Centre for Laser, Atomic, and Molecular Sciences
University of New Brunswick, Fredericton, NB Canada
Brenda Winnewisser, Manfred Winnewisser, F. C. De Lucia
Department of Physics, The Ohio State University, Columbus, OH USA
Brant E. BillinghurstCanadian Light Source, Inc., Saskatoon, SK Canada
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Background: the energy-momentum map ofNCNCS presented in the previous talkhas been calculated, not measured.
Genera
te p
ara
mete
rs d
esc
ribin
g t
he
pote
nti
al by fi
ttin
g B
eff,
Deff f
rom
each
ro
tati
onal vb/K
a s
eri
es.
Calc
ula
te e
nerg
ies
from
fitt
ed
pote
nti
al
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Objective: to measure the (vb, J=Ka) levels on this maprelative to one another using the far-infrared
rotation-vibration spectraobtained at the CLS
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Objective: to locate the (vb, J=Ka) levels on this maprelative to one another using the far-infrared
rotation-vibration spectraobtained at the CLS
b-type sub-bands
a-type sub-bands
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Phase 1: the spectrum of the ν7 low-frequency high-amplitude bending mode
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Phase 1: the spectrum of the ν7 low-frequency high-amplitude bending mode
v b 1
-0 K
a =
0
An
Inte
ract
ive
Lo
om
is-w
oo
d P
acka
ge
for
Sp
ectr
al A
ssig
nm
ent
in Ig
or
Pro
.N
eese
, C. F
.F
ifty-
sixt
h O
hio
Sta
te U
nive
rsity
Inte
rnat
iona
l Sym
posi
um o
n M
olec
ular
Spe
ctro
scop
yC
olum
bus,
Ohi
o, J
une
11-1
5, 2
001.
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Phase 1: the spectrum of the ν7 low-frequency high-amplitude bending mode
Mask
Data
Correlation spectrum
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Phase 1: the spectrum of the ν7 low-frequency high-amplitude bending mode
Up to
Ka = 10
Ka = 10
Ka = 12
Ka = 12
Origins of 68 a-type sub-bands of the ν7 spectrumdetermined in ~1.5 hours with the correlation
procedure!
But no b-type sub-bands were found… : (
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Phase 2: the spectrum of the ν3 hybrid band stretching mode
PGOPHER, a Program for Simulating Rotational Structure, C. M. Western, University of Bristol, http://pgopher.chm.bris.ac.uk
a-type sub-bands
b-type sub-bandsb-type sub-bands
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Phase 2: the spectrum of the ν3 hybrid band stretching mode
Ka
Ka
Ka+1
Ka-1
ν3=1
ν3=0
v 3
Ka =
6
a-ty
pe
• identify a-type sub-bands the hard way fora given value of Ka.
• calculate term energies in the ν3 level.
• create mask spectrum from upper state termenergies and calculated levels for v=0, Ka ±1.
• correlate the mask spectrum with the data.
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Phase 2: the spectrum of the ν3 hybrid band stretching mode
Ka’-Ka’’
3-2
4-3 5-
46-
57-
6
6-7 5-6
4-5
3-4
7-8
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
The energy-momentum map so far…
Up to
Ka = 10
Ka = 10
Ka = 12
Ka = 12
The relative energy of all states connected by arrowsare now known…. : )
But the stacks with Ka=0and Ka=1 still float relativeto the others… : (
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Where to next?
FAAAST Rotational spectrum: correlator failed to turn up the b-type sub-bands that would connect Ka 1-0 and 2-1.
Hybrid bands in 400-460 cm-1 range: lots of b-type Q-branches among the a-type spectra. The data potentially contain the two missing connections needed to complete the energy-momentum map.
69th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014
Conclusions
A directly measured energy-momentum map for the bending mode of NCNCS is nearly complete!
The potential function for the bending motion, obtained by fitting only Beff and Deff constants from pure rotational data with Stephen Ross’ Generalized Semi-Rigid Bender program, predicted vibrational level positions relative to one another to within ~2 cm-1 (for the levels I’ve
checked – not an exhaustive list). The physics that underlies quantum monodromy imprints itself on the large-amplitude bending motion (and a wide selection of other physical properties) of molecules…
… and the GSRB Hamiltonian captures that physics very nicely.
(DWT thanks Damien Forthomme and Colin Sonnichsen for help with the experiments, and NSERC for research funds.)
1 2 3 4 5
Welcome to the world where vibration and rotation can not be separated and the
eigenfunctions can not be factored: Dynamics of large amplitude motion
Quantum monodromy
in a Champagne bottle potential function