Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region...

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Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 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. Billinghurst Canadian Light Source, Inc., Saskatoon, SK Canada 69 th International Symposium on Molecular Spectroscopy Champaign-Urbana, IL USA June 19, 2014

Transcript of Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region...

Page 1: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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

Page 2: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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

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Page 3: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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

Page 4: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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

Page 5: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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

Page 6: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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

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Page 7: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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

Page 8: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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… : (

Page 9: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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

Page 10: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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.

Page 11: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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

Page 12: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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… : (

Page 13: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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.

Page 14: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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.)

Page 15: Spectroscopy of NCNCS at the Canadian Light Source: the far-infrared spectrum of the ν 7 region from 60-140 cm -1 (and beyond…) Dennis W. Tokaryk, Stephen.

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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