Vibrational wave packets in the C 1
u state of Cs2: Two color pump–probe experiments
J. Chem. Phys. 103, 10473 (1995); doi:10.1063/1.469897
Issue Date: 22 December 1995
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Two color, pump–probe laser experiments on the ~100 fs time scale have been applied to examining the dynamics of vibrational wave packets in the C 1
u state of Cs2. Wave packets consisting of more than 20 C state vibrational levels are produced with an initial pulse having a central wavelength between ~620 and 680 nm. The temporal history of the wave packet is inferred from the time and energy-integrated photoelectron signal produced when the excited state is photoionized by a time-delayed pulse centered at 605, 610, 615, 617, or 620 nm. Because of the difference in equilibrium internuclear separations for the Cs2(C) and Cs
(X) states (
Re
0.75 Å), wave packets are readily observed (signal-to-noise ratio
10) without the need to resort to mass selection techniques. Frequency analysis of the wave packet data shows a dominant (fundamental) component that decreases from 29 to ~28.3 cm−1 as the pump wavelength is tuned from 627 to 641 nm. Other spectral modes at ~23.5 and ~34 cm−1 and a weaker term at twice the fundamental frequency are also observed and quantum mechanical calculations of the wavepacket motion are in accord with the experimental results. ©1995 American Institute of Physics.
u state of Cs2. Wave packets consisting of more than 20 C state vibrational levels are produced with an initial pulse having a central wavelength between ~620 and 680 nm. The temporal history of the wave packet is inferred from the time and energy-integrated photoelectron signal produced when the excited state is photoionized by a time-delayed pulse centered at 605, 610, 615, 617, or 620 nm. Because of the difference in equilibrium internuclear separations for the Cs2(C) and Cs
Re
0.75 Å), wave packets are readily observed (signal-to-noise ratio
10) without the need to resort to mass selection techniques. Frequency analysis of the wave packet data shows a dominant (fundamental) component that decreases from 29 to ~28.3 cm−1 as the pump wavelength is tuned from 627 to 641 nm. Other spectral modes at ~23.5 and ~34 cm−1 and a weaker term at twice the fundamental frequency are also observed and quantum mechanical calculations of the wavepacket motion are in accord with the experimental results. ©1995 American Institute of Physics.
| History: | Received 10 August 1995; accepted 11 September 1995 |
| Permalink: |
http://link.aip.org/link/?JCPSA6/103/10473/1 |
KEYWORDS and PACS
BOUND STATES,
CESIUM,
DIATOMIC MOLECULES,
DIMERS,
DYNAMICS,
ELECTRONIC STRUCTURE,
FS RANGE,
PHOTOELECTRON SPECTROSCOPY,
PROBES,
PUMPING,
TIME DELAY,
TIME RESOLUTION,
VIBRATIONAL STATES,
WAVE PACKETS
- 33.20.Tp
Molecular properties and interactions with photons Molecular spectra Vibrational analysis - 33.60.Cv
Molecular properties and interactions with photons Photoelectron spectra Ultraviolet and vacuum ultraviolet photoelectron spectra - 39.30.+w
Instrumentation and techniques for atomic and molecular physics Spectroscopic techniques - YEAR: 1995
RELATED DATABASES
PUBLICATION DATA
0021-9606 (print)
1089-7690 (online)
REFERENCES (49)
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- M. Dantus, M. J. Rosker, and A. H. Zewail, J. Chem. Phys. 87, 2395 (1987).
- T. S. Rose, M. J. Rosker, and A. H. Zewail, J. Chem. Phys. 88, 6672 (1988).
- M. J. Rosker, M. Dantus, and A. H. Zewail, J. Chem. Phys. 89, 6113 (1988).
- T. S. Rose, M. J. Rosker, and A. H. Zewail, J. Chem. Phys. 91, 7415 (1989).
- J. Misewich, J. H. Glownia, J. E. Rothenberg, and P. P. Sorokin,
Chem. Phys. Lett. 150, 374 (1988 ). - M. Dantus, R. M. Bowman, M. Gruebele, and A. H. Zewail, J. Chem. Phys. 91, 7437 (1989).
- R. M. Bowman, M. Dantus, and A. H. Zewail,
Chem. Phys. Lett. 161, 297 (1989 ). - J. Misewich, J. H. Glownia, and P. P. Sorokin, J. Chem. Phys. 92, 3335 (1990).
- M. Gruebele, G. Roberts, R. M. Bowman, and A. H. Zewail,
Chem. Phys. Lett. 166, 459 (1990 ). - L. R. Khundkar and A. H. Zewail,
Ann. Rev. Phys. Chem. 41, 15 (1990 ). - T. Baumert, B. Bühler, R. Thalweiser, and G. Gerber, Phys. Rev. Lett. 64, 733 (1990).
- M. Gruebele, G. Roberts, and A. H. Zewail, Philos. Trans. R. Soc. London, Ser. A 332, 35 (1990).
- M. Dantus, M. H. M. Janssen, and A. H. Zewail,
Chem. Phys. Lett. 181, 281 (1991 ). - M. Gruebele, I. R. Sims, E. D. Potter, and A. H. Zewail, J. Chem. Phys. 95, 7763 (1991).
- M. Dantus, M. J. Rosker, and A. H. Zewail, J. Chem. Phys. 89, 6128 (1988).
- M. H. M. Janssen, R. M. Bowman, and A. H. Zewail,
Chem. Phys. Lett. 172, 99 (1990 ). - T. Baumert, M. Grosser, R. Thalweiser, and G. Gerber, Phys. Rev. Lett. 67, 3753 (1991).
- G. Rodriguez and J. G. Eden,
Chem. Phys. Lett. 205, 371 (1993 ). - F. W. Loomis and P. Kusch, Phys. Rev. 46, 292 (1934).
- R. P. Benedict, D. L. Drummond, and L. A. Schlie, J. Chem. Phys. 66, 4600 (1977).
- R. Gupta, W. Happer, J. Wagner, and E. Wennmyr, J. Chem. Phys. 68, 799 (1978).
- P. Kusch and M. M. Hessel,
J. Mol. Spectrosc. 25, 205 (1968 ). - P. Kusch and M. M. Hessel,
J. Mol. Spectrosc. 32, 181 (1969 ). - M. Raab, G. Hönig, W. Demtröder, and C. R. Vidal, J. Chem. Phys. 76, 4370 (1982).
- C. Amiot, W. Demtröder, and C. R. Vidal, J. Chem. Phys. 88, 5265 (1988).
- C. B. Collins, F. W. Lee, J. A. Anderson, P. A. Vicharelli, D. Popescu, and I. Popescu, J. Chem. Phys. 74, 1067 (1981).
- H. Weickenmeier, U. Diemer, M. Wahl, M. Raab, W. Demtröder, and W. Müller, J. Chem. Phys. 82, 5354 (1985).
- This state is occasionally labeled b 3

or (2)3

in the literature.
- E. K. Kraulinya, S. M. Papernov, and M. L. Janson,
Chem. Phys. Lett. 63, 531 (1979 ). - H. Katô, K. Yokoyama, M. Baba, N. Tamai, I. Yamazaki, and S. Nagakura, J. Chem. Phys. 87, 1987 (1987).
- M. Baba, T. Nakahori, T. Iida, and H. Katô, J. Chem. Phys. 93, 4637 (1990).
- R. S. Mulliken, J. Chem. Phys. 33, 247 (1960).
- K. Yokoyama, M. Baba, and H. Katô, J. Chem. Phys. 89, 1209 (1988).
- H. Katô, T. Kobayashi, M. Chosa, T. Nakahori, T. Iida, S. Kasahara, and M. Baba, J. Chem. Phys. 94, 2600 (1991).
- T. Kobayashi, T. Usui, T. Kamauchi, M. Baba, K. Ishikawa, and H. Katô, J. Chem. Phys. 98, 2670 (1993).
- R. L. Fork, C. V. Shank, and R. T. Yen, Appl. Phys. Lett. 41, 223 (1982).
- H. Suemitsu, H. Kitaura, and K. Seki,
J. Phys. Soc. Jpn. 62, 3425 (1993 ), and references cited therein. - M. Lapp and L. P. Harris,
J. Quant. Spectrosc. Radiat. Trans. 6, 169 (1966 ). - M. Gruebele and A. H. Zewail, J. Chem. Phys. 98, 883 (1993).
- T. Baumert, B. Bühler, M. Grosser, R. Thalweiser, V. Weiss, E. Wiedenmann, and G. Gerber,
J. Phys. Chem. 95, 8103 (1991 ). - T. Baumert, V. Engel, C. Röttgermann, W. T. Strunz, and G. Gerber,
Chem. Phys. Lett. 191, 639 (1992 ). - V. Engel, H. Metiu, R. Almeida, R. A. Marcus, and A. H. Zewail,
Chem. Phys. Lett. 152, 1 (1988 ). - V. Engel and H. Metiu, J. Chem. Phys. 90, 6116 (1989);
- H. Metiu and V. Engel, J. Chem. Phys. 93, 5693 (1990).
- M. D. Feit and J. A. Fleck, J. Chem. Phys. 78, 301 (1983).
- M. D. Feit and J. A. Fleck,
J. Chem. Phys. 80, 2078 (1984 ). - L. Von Szentpaly, P. Fuentealba, H. Preuss, and H. Stoll,
Chem. Phys. Lett. 93, 555 (1982 ). - M. Krauss and W. J. Stevens, J. Chem. Phys. 93, 4236 (1990).
- A. Wetmore, F. K. Men, M. Kimura, and R. E. Olson (unpublished).








