supersonic jet spectroscopy on tio 2 millimeter-wave spectroscopy of titanium monoxide and titanium...
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![Page 1: Supersonic Jet Spectroscopy on TiO 2 Millimeter-wave Spectroscopy of Titanium Monoxide and Titanium Dioxide 63 rd International Symposium on Molecular](https://reader038.vdocument.in/reader038/viewer/2022110401/56649e115503460f94afcf41/html5/thumbnails/1.jpg)
Supersonic Jet Spectroscopy on TiO2
Millimeter-wave Spectroscopy of
Titanium Monoxide and Titanium Dioxide
63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
PATRIK KANIA, THOMAS F. GIESEN, HOLGER S. P. MÜLLER, STEPHAN SCHLEMMERI. Physikalisches Institut, Universität zu Köln
SANDRA BRÜNKENHarvard-Smithsonian Center for Astrophysics, Cambridge
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• TiO abundant in M & S stars; absorption used for classification
• TiO2 important ingredient of O-rich grains
• transition metal compounds important as catalysts
• TiO2 common substrate for surface science
• Ti abundant transition metal; Ti/H ≈ 3 × 10−8
Astrophysical Interest
• small molecules with transition metals of fundamental interest
Quantum Chemical Interest
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63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
• Optical : A – X band system study,
R. S. Ram, P. F. Bernath, M. Dulick, and L.Wallace, ApJS, 122, 331 (1999)
• Infrared: No rotationally resolved data available
• Millimeter wave: 220 – 460 GHz 48TiO main isotope K. Namiki, S. Saito, J.S. Robinson, and T.C. Steimle, J. Mol. Spectrosc. 191, 176-182 (1998)
Titanium monoxide TiO
3 Electronic Ground State
Isotopes of Titanium 46Ti: 8.25 %47Ti: 7.44 % (I = 5/2)48Ti: 73.72 %49Ti: 5.41 % (I = 7/2)50Ti: 5.18 %
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New Measurements
• 46TiO, 50TiO First pure rotational transitions
• Extended measurements on 48TiO
• Data for the 31 32 states
Titanium monoxide TiO
3 Electronic Ground State
Isotopes of Titanium 46Ti: 8.25 %47Ti: 7.44 % (I = 5/2)48Ti: 73.72 %49Ti: 5.41 % (I = 7/2)50Ti: 5.18 %
63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
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PLL
beam splitter
Rb-reference
BWO-supply
BWO
harmonic mixer
He
pulse generator
valve
l-He
digital lock-In
PC
synthesizer
pu
mp
250 – 350 GHz
Nd:YaGlaser
63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
Cologne Supersonic Jet Spectrometer for Terahertz Applications (SuJeSTA)
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Pulsed Laser
Laser Ablation Source for TiO and TiO2
backing pressure 2 – 2,5 bar
chamber pressure 5·10 5 bar
buffer gas He
laser energy per pulse 35 - 40 mJ
width of laser pulse 6 ns
repetition rate 30 Hz
Multipass
10 passes
• path length 30 cm
Pulsed Nozzle
rotating Ti rod
for TiO+ 1 % O2
for TiO2
+ 2-3 % O2
63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
Nd:YaG1064 nm
TiO2
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J : 10 ← 9
63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
Spectra of 48TiO and 46TiO in natural abundance
Frequency [GHz] Frequency [GHz]
Inte
nsity
[a.
u.]
Inte
nsity
[a.
u.]
48TiO 73,8 %46TiO 8,0 %
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Data analysis using SPFIT/SPCAT including data from Namiki et al. (1998)
Molecular parameters for ground state TiO This work Namiki et al. (1998)
Parameter 46TiO 48TiO 50TiO 48TiO
B 16 177.070 26 (218) 16 003.552 79 (138) 15 843.788 18 (234) 16 003.408 14 (154)
D 0.0185032 (132) 0.0180560 (129) 0.0177302 (127) 0.0180606 (168)
H x 107 -1.64 (41) -1.64 (41) -1.64 (41) -1.53 (60)
1518483.66a 1518483.66a 1518483.66a 1518477.2
D - 0.81782 (122) - 0.79413 (54) - 0.77486 (132) - 0.79422 (70)
52381.8b 52381.8b 52381.8b 52380.0
D 0.0194825 (72) 0.0194825 (72) 0.0194825 (72) 0.01494 (100)
x 103 0.73 (46) 0.73 (46) 0.73 (46) 0.73 (46)
Analysis of TiO
Parameters are given in MHz. Standard deviations of all parameters given in parentheses are in units of the corresponding last digits.a, b Fixed to the value of R. S. Ram, P. F. Bernath, M. Dulick, and L.Wallace, ApJS, 122, 331 (1999)
eff 2 2 4 6 2 2 2 2 2 2 2 2 2Z Z Z Z Z
DZD ˆ
1 2 1ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ, (3 ) (3 ), ( )2 3 3
H L S L S N N N N SA A B S S S N SH o JD S J
63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
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• Asymmetry: = - 0.84
• Spin statistics: Ka + Kc even allowed
• Spectrum: b-type
63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
TiO2
dipole moment: 6.7D
Energy Level Diagram of TiO2
S. Brünken, H. S. P. Müller, K. M. Menten, M. C. McCarthy, and P. Thaddeus, ApJ 676, 1367 (2008)
Titanium dioxide (1A1)
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First pure rotational studies of TiO2
S. Brünken, H. S. P. Müller, K. M. Menten, M. C. McCarthy, and P. Thaddeus, ApJ 676, 1367 (2008)
27 observed transitions in the 7 – 42 GHz range for three isotopomers 46TiO2, 48TiO2, 50TiO2
63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
Inte
nsity
/ 1
0-8 n
m2 M
Hz
Frequency [GHz]
TiO2 rotational spectrum at 10 K
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000
202
404
606
808
10010
111
220
331
440
771
871
973
1073
1175
1275
1377
1479
1579
16711
880
982
1082
1184
1284
1386
1488
1588
660
762
862
964
1064
1166
1266
1368
1468
156 10
166 10
176 12
551
753
853
955
1055
1157
1257
1359
1459
155 11
165 11
175 13
175 13
651
744
844
946
1046
1148
1248
134 10
144 10
154 12
164 12
633
735
835
937
1037
1139
1239
133 11
143 11
153 13
642
542
Energy Level Diagram of TiO2
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000
202
404
606
808
10010
111
220
331
440
771
871
973
1073
1175
1275
1377
1479
1579
16711
880
982
1082
1184
1284
1386
1488
1588
660
762
862
964
1064
1166
1266
1368
1468
156 10
166 10
176 12
551
753
853
955
1055
1157
1257
1359
1459
155 11
165 11
175 13
175 13
651
744
844
946
1046
1148
1248
134 10
144 10
154 12
164 12
633
735
835
937
1037
1139
1239
133 11
143 11
153 13
642
542
Energy Level Diagram of TiO2
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JKa,Kc : 85,3 ← 74,4 JKa,Kc : 95,5 ← 84,4
63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
Example of the 48TiO2 measured spectra
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46TiO2 - 8,0 %47TiO2 - 7,3 %48TiO2 - 73,8 %49TiO2 - 5,5 %50TiO2 - 5,4 %
JKa,Kc : 75,3 ← 64,2
Stable isotopomers of titanium dioxide
63rd International Symposium on Molecular Spectroscopy, Ohio June 19, 2008
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Data fitted to A-reduced Watson Hamiltonian including data from (Brünken et al. 2008)
Analysis of TiO2
Ground state molecular constants for TiO2 This work Brünken et al.
Parameter 46TiO2 48TiO2
50TiO2 48TiO2
A 31 051.479 43 (168) 30 520.540 96 (132) 30 031.664 58 (164) 30 520.541 48 (165)
B 8 471.564 34 (36) 8 471.758 010 (305) 8 471.935 13 (41) 8 471.758 38 (54)
C 6 638.200 87 (48) 6613.587 28 (41) 6 590.319 30 (48) 6 613.587 31 (47)
J x 103 -8.379 51 (129) 8.348 07 (129) -8.319 21 (128) 8.363 2 (123)
JK x 103 -96.735 9 (267) -94.617 6 (261) -92.680 2 (255) -94.397 (110)
K x 103 757.404 (63) 732.662 (61) 710.238 (59) 732.445 (151)
J x 103 2.964 22 (66) 2.979 97 (66) 2.994 44 (66) 2.981 5 (40)
K x 103 17.283 (49) 16.798 (48) 16.345 (47) 16.819 (141)
K x 106 64.04 (80) 60.89 (76) 58.02 (73) 39.3 (85)
KJ x 106 -7.81 (37) -7.49 (35) -7.20 (34)
K x 106 5.89 (209) 5.64 (200) 5.42 (192)
Parameters are given in MHz. Standard deviations of all parameters given in parentheses are in units of the corresponding last digits
Isotopics ratios kept fixed for distortion parameters
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TiO
• First pure rotational transitions of 46TiO and 50TiO
• Isotopic invariant fit in progress
TiO2
• Extended measurements up to J = 22, Ka = 8 (T= 150 K)
• Higher order centrifugal parameters • Data for astronomical observations
Conclusion