Abstract.
An experimental and theoretical study on the excited Ba\(\cdots\)FCH3(A) photodissociation yield as a function of the excitation laser fluence is reported. Experimentally, it was found that the two-photodissociation channel yields, i.e. the reactive BaF and non-reactive Ba* products, increased exhibiting a similar behaviour, as the laser fluence changed from 0.2 up to ca. 4 mJ/cm2. Beyond this value the BaF yield levels off and the Ba* decreases over the 4-7 mJ/cm2 range. The theoretical simulation of the excited state electron-ion dynamics within the time-dependent density functional theory revealed that the reactive channel dominated the photofragmentation dynamics as it occurs within a femtosecond time scale and became accelerated as the photodissociation laser fluence increased. By contrast, the non-reactive channel only manifested for low laser fluences at the nano/picosecond time regime resulted inactive as the laser fluence increased. A simple scheme to control the dynamics of the intracluster multichannel reaction is suggested in which the slowest the channel the easiest to close it as the excitation laser power increases.
Similar content being viewed by others
References
R.N. Zare, Science 279, 1875 (1998)
S.R. Rice, Nature 409, 422 (2000)
S. Shi, A. Woody, H. Rabitz, J. Chem. Phys. 88, 6870 (1988)
M. Shapiro, P.J. Brumer, J. Chem. Phys. 84, 4103 (1986)
M. Shapiro, P.J. Brumer, J. Chem. Phys. 97, 6259 (1992)
L.-C. Zhu, V. Kleiman, X.-N. Li, S.P. Lu, K. Trentelman, R.J. Gordon, Science 70, 77 (1995)
D. Tannor, S.A. Rice, J. Chem. Phys. 83, 5013 (1985)
T. Baumert, M. Grosser, R. Thalweiser, G. Gerber, Phys. Rev. Lett. 67, 3753 (1991)
A. Assion, T. Baumert, M. Bergt, T. Brixner, B. Kiefer, V. Seyfried, M. Strehle, G. Gerber, Science 282, 919 (1998)
C. Daniel, J. Full, L. González, C. Lupulescu, J. Manz, A. Merli, S. Vajda, L. Woste, Science 299, 536 (2003)
S. Skowronek, R. Pereira, A. González Ureña, J. Chem. Phys. 107, 1668 (1997)
S. Skowronek, R. Pereira, A. González Ureña, J. Phys. Chem. 101, 7468 (1997)
V. Stert, P. Farmanara, W. Radloff, F. Noack, S. Skowronek, J. Jimenez, A. González Ureña, Phys. Rev. A 59, 1727 (1999)
P. Farmanara, V. Stert, W. Radloff, S. Skowronek, A. González Ureña, Chem. Phys. Lett. 304, 127 (1999)
A. González Ureña, K. Gasmi, J. Jiménez, R.F. Lobo, Chem. Phys. Lett. 352, 369 (2002)
E.K.U. Gross, F.J. Dobson, M. Petersilka, Density Functional Theory (Springer, New York, 1996)
G. Onida, L. Reining, A. Rubio, Rev. Mod. Phys. 74, 601 (2002)
While the ionisation laser crosses the molecular beam perpendicularly, the excitation laser intersects the crossing point at an angle of about 5\(^\circ\) with respect to the ionisation laser. Care was taken to achieve complete overlap of the two lasers in the intersection region by using two complementary double-diaphragms at the entrance and the exit window of the detection chamber. Thus, the pump laser beam overlaps totally the packet of complexes that is to be ionised by the probe laser
S. Skowronek, A. González Ureña, in Atomic and Molecular beams: The state of the Art, edited by R. Campargue (Springer, 2000), p. 353
S. Skowronek, A. González Ureña, Progr. React. Kin. Mech. 24, 101 (1999)
The octopus project in aimed at describing by first-principles the electron-ion dynamics in finite and extended systems under the influence of arbitrary time-dependent electromagnetic fields. The program can be freely downloaded from http//:www.tddft.org/programs/octopus. For details see M.A.L. Marques, A. Castro, G.F. Bertsch, A. Rubio, Comp. Phys. Comm. 151, 60 (2003)
A. Castro, M.A.L. Marques, J.A. Alonso, G.F. Bertsch, A. Rubio, Eur. J. Phys. B (in press, 2003)
This technique, first introduced in K. Yabana, G.F. Bertsch, Phys. Rev. B 54, 4484 (1996) for the calculation of linear optical spectra of clusters, does not rely on perturbation theory, and is competitive with implementations in the frequency domain (A. Rubio, J.A. Alonso, X. Blase, L.C. Balbás, S.G. Louie, Phys. Rev. Lett. 77, 247 (1996)
N. Troullier, J. Martins, Phys. Rev. B 43, 1993 (1991). We used the core radii r c =1.4 and 1.29 a.u. for all the s, p pseudopotential components of C and F, respectively. For Ba we used a charged configuration including semicore states (5s 2(r c =1.73) 5p 6(r c =2)). Inclusion of scalar relativistic effects turn out to be crucial for the proper description of the excited state properties of the Ba atom
D.M. Ceperley, B.J. Alder, Phys. Rev. Lett. 45, 1196 (1980)
V. Stert, H.H. Ritze, P. Farnamara, W. Radloff, Phys. Chem. Chem. Phys. 3, 3939 (2001)
P. Piecuch, J. Mol. Struct. 503, 436 (1997)
V. Stert, P. Farnamara, H.H. Ritze, W. Radloff, K Gasmi, A. González Ureña, Chem. Phys. Lett. 337, 299 (2000)
A.E. Orel, W.H. Miller, J. Chem. Phys. 70, 4393 (1979)
T. Baumert, V. Engel, C. Meier, G. Gerber, Chem. Phys. Lett. 200, 488 (1992)
Author information
Authors and Affiliations
Corresponding author
Additional information
Received: 3 July 2003
PACS:
36.40.Jn Reactivity of clusters - 36.40.Qv Stability and fragmentation of clusters - 34.50.Rk Laser-modified scattering and reactions
Rights and permissions
About this article
Cite this article
González Ureña, A., Gasmi, K., Skowronek, S. et al. Laser-induced control of (multichannel) intracluster reactions. Eur. Phys. J. D 28, 193–198 (2004). https://doi.org/10.1140/epjd/e2003-00302-7
Published:
Issue Date:
DOI: https://doi.org/10.1140/epjd/e2003-00302-7