Multiphoton ionization of SiH3 and SiD3 radicals: Electronic spectra, vibrational analyses of the ground and Rydberg states, and ionization potentials
J. Chem. Phys. 91, 3340 (1989); doi:10.1063/1.456909
Issue Date: 15 September 1989
You are not logged in to this journal. Log in
The electronic spectra of silyl radicals, SiH3 and SiD3, were observed between 310 and 430 nm (46 000–64 000 cm−1) by resonance enhanced multiphoton ionization (REMPI) mass spectroscopy. The spectra were generated through a 2+1 REMPI mechanism. Two Rydberg series originating from planar, D3h point group states were observed. One series, of quantum defect
=1.45(2), is comprised of the
2A
(4p),
2A
2(5p), and
2A
2(6p) Rydberg states which have origins at
0–0 =48 438, 56 929, and 60 341 cm−1 in SiH3 and at
0–0 =48 391, 56 874, and 60 267 cm−1 in SiD3. In SiD3 the
2A
2(7p) Rydberg origin was observed at
0–0 =62 002 cm−1. The
,
, and
states observed in the SiD3 spectrum comprise the second Rydberg series,
=2.09, and were tentatively assigned as ns 2A
Rydberg states (n=5, 6, 7). The
and
origins were observed at
0–0 =58 417 and 61 005 cm−1. A fit of the Rydberg formula to the np 2A
2(n
5) origins found the adiabatic ionization potential of the SiH3 and SiD3 radicals to be IPa=8.135(+5,−2) eV and IPa=8.128(1) eV, respectively. Detailed vibrational analyses of these Rydberg states are presented. Analysis showed that in the
2A
(4p) state of the SiH3 radical 
(a
symmetric bend)=796(7) and 2
/2(e
degenerate bend)=870(5) cm−1 and that in SiD3 radical 
(a
SiH3 symmetric stretch)=1576(3), 
=589(3), and 2
/2=635(6) cm−1. The REMPI spectra exhibited 
hot bands from vibrational levels as high as Ev =2073 cm−1 in the
2A1state. Modeling calculations, which fit the numerous 
2 hot bands, predicted barriers to inversion of Binv=1935 cm−1 and Binv =1925 cm−1 for SiH3 and SiD3
2A1 radicals, respectively.
The Journal of Chemical Physics is copyrighted by The American Institute of Physics.
=1.45(2), is comprised of the
0–0 =48 438, 56 929, and 60 341 cm−1 in SiH3 and at
0–0 =48 391, 56 874, and 60 267 cm−1 in SiD3. In SiD3 the
0–0 =62 002 cm−1. The
=2.09, and were tentatively assigned as ns 2A
0–0 =58 417 and 61 005 cm−1. A fit of the Rydberg formula to the np 2A
5) origins found the adiabatic ionization potential of the SiH3 and SiD3 radicals to be IPa=8.135(+5,−2) eV and IPa=8.128(1) eV, respectively. Detailed vibrational analyses of these Rydberg states are presented. Analysis showed that in the 






| History: | Received 3 April 1989; accepted 8 June 1989 |
| Permalink: |
http://link.aip.org/link/?JCPSA6/91/3340/1 |
KEYWORDS and PACS
SILANES,
DEUTERIUM COMPOUNDS,
ABSORPTION SPECTRA,
MULTI&minus,
PHOTON PROCESSES,
PHOTOIONIZATION,
MASS SPECTROSCOPY,
RYDBERG STATES,
VIBRATIONAL STATES,
SPECTRAL FUNCTIONS,
RADICALS,
ELECTRONIC STRUCTURE,
IONIZATION POTENTIAL
- 33.80.Rv
Molecular spectra and interactions of molecules with photons Photon interactions with molecules Multiphoton ionization and excitation to highly excited states (e.g., Rydberg states) - 35.20.Wg
Experimentally derived information on atoms and molecules; instrumentation and techniques Molecules Mass spectra - 35.20.Pa
Experimentally derived information on atoms and molecules; instrumentation and techniques Molecules Rotation, vibration, and vibration
rotation constants
- 35.20.Vf
Experimentally derived information on atoms and molecules; instrumentation and techniques Molecules Ionization potentials, electron affinities, molecular core binding energy - YEAR: 1988-89
PUBLICATION DATA
0021-9606 (print)
1089-7690 (online)
REFERENCES (48)
For access to fully linked references, you need to log in.
For access to fully linked references, you need to Log in.
- G. Herzberg and J. Shoosmith, Can. J. Phys. 34, 523 (1956).
- G. Herzberg, Proc. R. Soc. London Ser. A 262, 291 (1961).
- (a) G. Herzberg and R. D. Verma, Can. J. Phys. 42, 395 (1964);
- (b) G. Herzberg, A. Lagerqvist, and B. J. McKenzie, ibid. 47, 1889 (1970).
- R. D. Verma, Can. J. Phys. 43, 2136 (1965).
- I. Dubois, Can. J. Phys. 46, 2485 (1968).
- J. W. Hudgens, in Advances in Multi-photon Processes and Spectroscopy, edited by S. H. Lin (World Scientific, Singapore, 1988), Vol. 4.
- T. G. DiGiuseppe, J. W. Hudgens, and M. C. Lin, J. Chem. Phys. 76, 3338 (1982).
- J. W. Hudgens, T. G. DiGiuseppe, and M. C. Lin, Chem. Phys. 79, 571 (1983).
- R. D. Johnson III and J. W. Hudgens, Chem. Phys. Lett. 141, 163 (1987).
- R. D. Johnson III, B. P. Tsai, and J. W. Hudgens, Resonance Ionization Spectroscopy 1988, Institute of Physics Conference Series No. 94, edited by T. B. Lucatorto and J. E. Parks (Institute of Physics, Bristol, Philadelphia, 1988), p. 133.
- R. D. Johnson III, B. P. Tsai, and J. W. Hudgens, J. Chem. Phys. 89, 4558 (1988).
- R. Robertson, D. Hils, H. Chatham, and A. Gallagher, Appl. Phys. Lett. 43, 544 (1983).
- W. D. Allen and H. F. Schaefer III, Chem. Phys. 108, 243 (1986).
- R. L. Morehouse, J. J. Christiansen, and W. Gordy, J. Chem. Phys. 45, 1751 (1966).
- G. S. Jackel and W. Gordy, Phys. Rev. 176, 443 (1968).
- The often reported internal angle in C3
species,
H-Si-H, is related to
by the equation
(H-A-H) = 2 sin−1[(3/4)1/2 cos
]. - D. S. Marynick, J. Chem. Phys. 74, 5186 (1981).
- K. Ohta, H. Nakatsuji, I. Maeda, and T. Yonezawa, Chem. Phys. 67, 49 (1982).
- J. A. Pople, B. T. Luke, M. J. Frisch, and J. S. Binkley, J. Phys. Chem. 89, 2198 (1985).
- J. Moc, Z. Latajka, and H. Ratajczak, J. Mol. Struct. (Theochem) 150, 189 (1987).
- J. Kalcher, Chem. Phys. 118, 273 (1987).
- G. Olbrich, Chem. Phys. 101, 381 (1986).
- Y. Ellinger, F. Pauzat, V. Barone, J. Douady, and R. Subra, J. Chem. Phys. 72, 6390 (1980).
- P. R. Bunker and F. Olbrich, Chem. Phys. Lett. 109, 41 (1984).
- M. R. Nimlos and G. B. Ellison, J. Am. Chem. Soc. 108, 6522 (1986).
- C. Yamada and E. Hirota, Phys. Rev. Lett. 56, 923 (1986).
- J. M. Dyke, N. Jonathan, A. Ridha, and M. J. Winter, Chem. Phys. 81, 481 (1983).
- J. A. Pople and L. A. Curtiss, J. Phys. Chem. 91, 155 (1987).
- J. Berkowitz, J. P. Greene, H. Cho, and B. Ruscic, J. Chem. Phys. 86, 1235 (1987).
- B. H. Boo and P. B. Armentrout, J. Am. Chem. Soc. 109, 3549 (1987).
- See G. Herzberg, Electronic Spectra of Polyatomic Molecules (Van Nostrand Reinhold, New York, 1966), p. 170.
- Certain commercial materials and equipment are identified in this paper in order to adequately specify the experimental procedure. In no case does such an identification imply recommendation or endorsement by the National Institute of Standards and Technology, nor does it imply that the material or equipment identified is necessarily the best available for the purpose.
- D. S. King, P. K. Schenck, K. C. Smyth, and J. C. Travis, Appl. Opt. 16, 2617 (1977).
- A. R. Striganov and N. S. Sventitskii, Table of Spectral Lines of Neutral and Ionized Atoms (Plenum, New York, 1968).
- Heats of formation were obtained from S. G. Lias, J. E. Bartmess, J. F. Liebman, J. L. Holmes, R. D. Levin, and G. Mallard, J. Chem. Phys. Ref. Data 17, Suppl. 1 (1988) from Ref.30.
- W. H. Duewer and D. W. Setser, J. Chem. Phys. 58, 2310 (1973).
- M. B. Robin, Higher Excited State of Polyatomic Molecules (Academic, New York, 1975).
- S. T. Manson, Phys. Rev. 182, 97 (1969).
- J. L. Dehmer, Rev. Mod. Phys. 48, 49 (1976).
- The isotopic ratio of vibrational frequencies expected between the SiH3 and SiD3 radical and cation species were calculated from G-matrix elements. G-matrix elements were computed using the method shown in F. A. Cotton, Chemical Applications of Group Theory, 2nd ed. (Wiley Interscience, New York, 1971), p. 324 and Appendix VIII. Using the
2A1 radical geometry given in Ref. 26, the SiH3/SiD3 vibrational ratios: 1.414, 1.350, 1.427, and 1.354 were found for the
1,
2,
3, and
4 modes of the radicals. Adopting the 1A
cation geometry of Ref. 19, the ratios 1.414, 1.350, 1.413, and 1.353 were computed.
- J. W. Hudgens, C. S. Dulcey, G. R. Long, and D. J. Bogan, J. Chem. Phys. 87, 4546 (1987).
-
ZPE itself is the difference between the zero point energies of the cation and radical, i.e.,
ZPE = ZPE(ion)−ZPE(radical). - No correction for the energy separation between the

= 0−1 levels was applied. This difference, ~0.3 cm−1, is much less than the measurement uncertainty.
- J. Laane, Appl. Spectrosc. 24, 73 (1970).
- The two point fits by Yamada and Hirota cannot provide meaningful error estimates for the estimated value of Binv.
- In the event that future measurements or high quality calculations change these Rydberg orbital assignments, we recommend that the letter designation of each REMPI band system remain unchanged. New letters or prime designations may need to be introduced. For example, in the event that the
state becomes assigned as the 3d2E state, then the reassigned state should be called
2E(3d), the 5s2A
state should acquire a primed letter designation (the letter determined by its energy), and the
designation should be discarded.
- Coriolis induced predissociation appears in the spectrum of the H3 radical. See I. Dabrowski and G. Herzberg, Can. J. Phys. 58, 1238 (1980);
- G. Herzberg and J. K. G. Watson, ibid. 58, 1250 (1980).
- C. Moore, Atomic Energy Levels, Natl. Bur. Stand. Circ. 467 (U.S. GPO, Washington, D.C., 1949), Vol. 1.








