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D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA , K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 u Σ 3 School of Chemistry, University of Sydney 62 nd International Symposium on Molecular Spectroscopy, June 21, 2007 RD03
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D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Dec 18, 2015

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Page 1: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

D.L. KOKKIN, N.J. REILLY, J.A. JOESTER,M. NAKAJIMA, K. NAUTA,

S.H. KABLE and T.W. SCHMIDT

Direct Observation of the c State of C2

uΣ3

School of Chemistry, University of Sydney

62nd International Symposium on Molecular Spectroscopy, June 21, 2007

RD03

Page 2: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Introduction

groundmeta-stable

Low-Lying Electronic State of C2

Page 3: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Previous Studies

Experimental Studies of the stateuc Σ3

#Perturbation partner of the state uA Π1

E.A. Ballik and D.A. Ramsay, Astrophys. J. 137, 84 (1963).

A.E. Bragg et al., Chem. Phys. Lett. 376, 767 (2003).

#Photoelectron spectroscopy of C2–

c(neutral)−X or B(anion) [vibrationally resolved]

L.J. Brug and M.C. Heaven, J. Chem. Phys. 87, 4235 (1987).

#LIF excitation spectroscopy (tentative assignment)

The A state is perturbed by the state.uc Σ3

transition of C2 (lower state is )?ΣΣ uc Σ3

Page 4: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Introduction

Theoretical Studies of the stateuc Σ3

D.L. Kokkin et al., J. Chem. Phys. 126, 084302 (2007).

Based on this high-level calculation, we surveyed an excitation spectrum of the d–c system!

Oscillator strength of the d←c transition is much smaller (~1/10) than that of d←a (Swan).

MR-CISD+Q/aug-cc-pV6Z[incl. core and core-valence correlation energies]

# Molecular constants in uc Σ3

# Oscillator strength of the transition ug cd Σ33

Page 5: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Experimental# Generation of C2

Pre-mixed gas of 1 % Acetylene in Ar Pulsed discharge by a pulsed-discharge nozzle

The state of C2 was produced in a jetuc Σ3

# Excitation light sourceA pulsed dye laser (~5 ns pulse, ~0.05 cm-1) Δ

# Experimental ConditionsStagnation pressure: ~5 barbackground pressure (chamber): 2×10-4 torr

# Detection methodLaser-induced fluorescence (LIF) technique

Page 6: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Experimental

#Experimental Scheme of LIF Excitation Spectrum

(Most fluorescence is observed as Swan emission.)

Swan (d−a) emission, caused by d←c excitation, was detected through a monochrometor.

Theoretical transition moment of d-c is ~1/10 of that of d-a.

Only a few percents of emission from the d-state terminates to the c-state.

Difficult to detect the d→c emission!

In LIF excitation measurements of d←c…

Page 7: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Survey Spectrum of jet-cooled C2

monitoring@~470 nm Swan emission

ug cd ΣΠ 33

7←3

3←0

4←1 5←2

6←3

Page 8: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Excitation/Emission 2D Image

Swan (4→5)

Swan (5→6)

& overlapping region1)(433 ug cd ΣΠ 8)(533 ug ad ΠΠ

We can separate “Swan” and “d-c” bands in emission!even if they are overlapping in an excitation spectrum.

Monochrometor slit ~1 mm 60 cm-1(~2 nm) bandpass

{

Selective detection of the Swan (4-5) emission through a monochrometor

d-c (4←1)

Swan (d-a: 5←8)

Page 9: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Rotationally Resolved d-c Bands

v' -v"

Page 10: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Rotationally Resolved 3-0 Band

0)(333 ug cd ΣΠ

Sim.

Obs.

Page 11: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Molecular Constants in the Stateuc Σ3

Form lower state combination differences…

v" B"v /cm-1 "v /cm-1 "v /cm-1

0123

1.92220(32)1.89751(32)1.88668(16)1.86616(14)

−0.3330(26)−0.3042(27)−0.3216(16)−0.3151(17)

0.0107(12) −0.01433(97) 0.01553(68) 0.00323(59)

Rotational levels in the v' = 4 level of the d-state have been reported to be perturbed even at low J levels.

Rotational analyses:3-0, 4-1, 5-2, and 7-3 bands of the transition. ug cd ΣΠ 33

A. Tanabashi et al. Astrophys. J. Suppl. Ser. 169, 472 (2007).

)/3(32 22 SSSNNB zˆˆˆˆˆ vvv 3 Hamiltonian:

Page 12: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Te (c-X) = 9171.84(49) cm-1

e = 2061.56(58) cm-1

exe = 14.73(14) cm-1

Molecular Constants in the Stateuc Σ3

A. Tanabashi et al. Astrophys. J. Suppl. Ser. 169, 472 (2007).S.P. Davis et al. J. Opt. Soc. Am. B 5, 1838 (1838).

Using… # Determined 3-0, 4-1, 5-2, & 7-3 band origins of the transition # Known term values of v = 3, 4, 5, & 7 levels in the d3g state

ug cd ΣΠ 33

Be = 1.9319(17)

e = 0.01855(68) cm-1

cm-1

Using determined Bv values…

Page 13: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Comparison with Ab Initio Values

*Ab initio work: D.L. Kokkin et al., J. Chem. Phys. 126, 084302 (2007).

Full-valence MR-CISD(+Q)/aug-cc-pV6Z [incl. core and core-valence correlations]

C2 molecular constants in the stateuc Σ3

Exp. / cm-1 *Theory / cm-1 Te

e

exe

Be

e

9171.84(49)

2061.56(58)

14.73(14)

1.9319(17)

0.01855(68)

9315

2061.3

13.54

1.9289

0.01695

–143 cm-1

+0.01%

+8.8%

+0.16%

+9.4%

Good Agreements!

Page 14: D.L. KOKKIN, N.J. REILLY, J.A. JOESTER, M. NAKAJIMA, K. NAUTA, S.H. KABLE and T.W. SCHMIDT Direct Observation of the c State of C 2 School of Chemistry,

Swan & …

“Swan” system

New band system

ug ad ΠΠ 33

ug cd 33Π

Duck Bands!