spectroscopy of cun in the near infrared by intracavity laser absorption spectroscopy leah c....
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![Page 1: Spectroscopy of CuN in the Near Infrared by Intracavity Laser Absorption Spectroscopy Leah C. O'Brien and Kaitlin A. Womack, Department of Chemistry, Southern](https://reader035.vdocument.in/reader035/viewer/2022073103/56649ce35503460f949aef39/html5/thumbnails/1.jpg)
Spectroscopy of CuN in the Near Infrared by Intracavity Laser Absorption Spectroscopy
Leah C. O'Brien and Kaitlin A. Womack, Department of Chemistry, Southern Illinois University, Edwardsville, IL 62026-1652;
James J. O'Brien,Department of Chemistry and Center for Nanoscience, University of Missouri, St. Louis, MO 63121
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Previous Work on CuN
No previous experimental work
Several papers on ground state bond length and symmetry, 3Σ-
Ground and excited potential energy curves calculated by A. Daoudi, A. Touimi Benjelloun, J.P. Flament, and G. Berthier, J. Mol. Spectrosc. 194 (1999) 8-16
• X 3Σ-
• A 3Π at 1.5 eV
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MO Energy Level Diagram for CuN
Fenske-Hall Calculation
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Intracavity Laser Absorption Spectroscopy
Absorption spectra recorded using intracavity laser spectrometer at the University of Missouri – St. Louis
Configured with a copper hollow cathode plasma discharge operating at high current, 1.5 A, from DCG power supply
Pressures of 1.5 Torr of oxygen was employed
Generation times (tg) up to 200 µs were used, the copper hollow cathode was 50 mm long, the overall laser cavity length was 2.30 m
Spectra are recorded as a series of overlapping spectral segments, each segment being ; 6 cm−1 wide
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Copper Hollow Cathode Discharge
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ResultsNew spectrum with red-degraded band heads at
13004.6, 12962.9, 12957.4, and 12947.9 cm-1
13004.6 cm-1 band Shows a single P- and R-branch
Identified line positions in each branch
Used Excel to graph line positions and the difference between peaks
Possibly (0,0) band of A 3Π0 – X 3Σ-0?
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Portion of the CuN spectrum associated with the 13004.6 cm-1 band
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Unusual line spacing in both branches
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Useful to get J assignments!
5. H.D. Babcock and L. Herzberg, Ap. J. 108 (1948) 167-190.
One and only one assignment gives unperturbed ground state!
Cm
-1
J
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Partial line list for 13004.6 cm-1 band
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Ground state Δ2F values for 13004.6 cm-1 band
Δ2F = 4B (J + 0.5)
• x-intercept should go through J = -0.5
• y-intercept should be 2B
Confirms that J is integer
Not CuO! (also checked Δ2F values for X 2Π3/2 , X 2Π3/2)
EJ = B J(J+1) – D J2(J+1)2
Fit to get molecular constantsB0 D0 x 106 r0 (Å)
Ground state
0.442845(35) 0.687(14) 1.823
Ab initio re=1.811
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X 3Σ-1 X
3Σ-0
A 3Π0
40 cm-1
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12957.4 cm-1 band
1 R- and P-branch• Branches have regular spacing
Fit as Ω=0 – Ω=0 transitionPossibly (1,1) bandhead?
Tv Bv Dv x 106
Excited state x + 12954.333
0.402133(63) 0.896(68)
Lower state x 0.439722(63) 0.899(57)
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Wavenumber (cm-1)
12948 12950 12952 12954 12956 12958
Tra
nsm
itta
nce
(%)
75
80
85
90
95
100
Angstrom (Å)7715771777197721
97
100
I2
CuN
RR36 34 32
26 24 14162022 18
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Spectrum of CuN?
Pros
“Ok” match with predicted ground state bond length
Not CuO, not O3
A 3Π0 - X 3Σ-0 should be a
single P- and R-branch
Other nearby bandheads could be related to A3Π0 - X 3Σ-
1 transition
• Work in progress!!
b 1Δ state predicted near A 3Π – could be perturbing state
Isoelectronic NiO has X 3Σ-
with λss = 25 cm-1
Cons
Only “Ok” match with ground state bond length
Calculation predicts A 3Π – X 3Σ- should be blue-degraded
• Re” = 3.426 a0 = 1.812 Å
• Re’ = 3.372 a0 = 1.784 Å
• However, calculation did not include spin-orbit effects
• Perturbing states near excited state
No evidence of 63Cu/65Cu isotope structure
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SummaryFour newly-observed bandheads are tentatively
assigned to CuN
13004.6 cm-1 band contained single P- and R-branch
• Perturbations in excited state
• Ground state Δ2F values fitted
• Molecular constants for ground state obtained
12957.4 cm-1 band contained single P- and R-branch
• No perturbations in excited state, molecular constants obtained for both states
• (1,1) band?
Work in progress on other bandheads
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Acknowledgements
National Science Foundation
Kaitlin Womack, undergraduate student at SIU Edwardsville
Thank you for your attention!
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Beff (J)= EJ/[J(J+1)]