Scientific background Solving the Schroedinger equation for the nuclear motions in small polyatomic molecules has been and will remain one of the most challenging computational problems. Accurate solutions for the vibrational states of molecules which play a significant role in combustion and atmospheric chemistry as well as in biology are highly demanded since the recent advances in high resolution spectroscopy [1]. Unequivocally, the progress in experiment and theory of vibrational spectroscopy of the last twenty years is immense. Grid methods for the solution of the Schroedinger equation are nowadays of the most powerful and exploited tools both for the time independent (here mainly known as Discrete Variable Representation - DVR [2-4]) and time dependent pictures. Concerning the last one, it was the introduction of the Fourier Pseudospectral (PS) method which provided the necessary efficiency to compete with the traditional variational techniques and to make feasible the task [5,6]. Lately, the ideas of the Chebychev expansion of the time propagator for solving the time dependent Schroedinger equation have been extended to the energy domain, thus, producing the filtering techniques for diagonalizing the Hamiltonian matrix [7,8]. This allowed the extraction of accurate wave functions in triatomic molecules at high energies with large densities of states. The present computational algorithms and computer technology have made vibrational calculations on triatomic molecules relatively a routine job, even on small size computers [9], and feasible the calculations with the rotational degrees of freedom included [10] and on tetratomic molecules (six degrees of freedom) [11]. However, as the size of molecule increases or the density of vibrational states increases the goal of solving the Schroedinger equation remains unsatisfied. It is interesting that in our effort to surmount the above difficulties old techniques are revisited. For example, local methods such as the Finite Difference (FD) algorithms were the first to apply in problems of Molecular Dynamics [12]. The results obtained that time were rather unsatisfactory and the appearance of global methods such as the PS ones (DVR or Fourier) dominated in solving the vibrational problem in polyatomic molecules. However, new developments in the theory of Finite Differences [13] have led us to examine their efficiency in solving the Schroedinger equation. Thanks to new computer algorithms for computing the necessary weights in FD schemes, it was shown that the FD method may lead to a considerable saving in computer memory and time because of the local representation of the wave function [14,15]. Old ideas based on the hydrodynamic formulation of quantum mechanics going back to de Broglie and Bohm have been revived in a new scheme known as Quantum Trajectory Method (QTM) [16]. Again, the advances are due to the progress in numerical solutions of computational fluid dynamics [17]. These ideas replace the well known wave equation with trajectory - type (quantum) equations. The molecular vibrational problem is not only that of solving the Schroedinger equation. Even if that was possible, the huge amount of data would be useless without being able to assign the vibrational states and extract their physical meaning. Assigning the vibrationally highly excited states is also a difficult task because of the non linear mechanical behaviour of the molecule. Progress in this direction has been achieved by developing methods based on effective Hamiltonians, semiclassical theories and periodic orbits [18,19]. It turns out that up to now there has been no effort to face both problems (computation and assignment of vibrational states) simultaneously within the same theory.
Motivation and objectives The CECAM workshop on Spectroscopy and Computational Challenges in Vibrationally Highly Excited Polyatomic Molecules aims into examining techniques for solving the Schroedinger equation in conjunction to the interpretation of vibrational spectra in highly excited polyatomic molecules. It is believed, that instead of computing the whole spectrum in a range of energies the computation of those parts of the spectrum related to experimental or other type of theoretical information will help in circumventing the difficulties in computer memory and time. In the list of participants a few leading experimentalists are included. By bringing together theorists and experimentalists we hope to trace the problems better and stimulate new research projects. Through the presentations of the participants the currently used algorithms will be reviewed. During the discussion sessions ideas of designing algorithms which take in account previous experimental or theoretical information will be worked out. References {1}Molecular Dynamics and Spectroscopy by Stimulated Emission Pumping, edited by {H.-L.}~Dai and R.~Field, World Scientific, Singapore, (1995).} {2}{J. V. Lill, G. A. Parker and J. C. Light, {Chem. Phys. Lett.} { 89}, 483 (1982).} {3}{C. Iung and C. Leforestier, {J. Chem. Phys.} { 102}, 8453 (1995).} {4}{R. E. Wyatt, { J. Chem. Phys.} { 103}, 8433 (1995).} {5}{R. Kosloff, in Dynamics of Molecules and Chemical Reactions, R. E. Wyatt and J. Z. H. Zhang eds. Marcel Dekker Inc., New York, 1996.} {6}{R. Kosloff, {Ann. Rev. Phys. Chem.} { 45}, 145 (1994).} {7}{V. Mandelshtam and H. S. Taylor, { J. Chem. Phys.} { 106}, 5085 (1997).} {8}{R. Chen and H. Guo, { J. Chem. Phys.} {105}, 1311 (1996).} {9}{Ch. Beck, H.-M. Keller, S. Yu. Grebenshchikov, R. Schinke, S. C. Farantos, K. Yamashita and K. Morokuma, {\it J. Chem. Phys.} {\bf 107}, 9818 (1997).} {10}{H. Y. Mussa, J. Tennyson, C. J. Noble and R. J. Allan, { Comp. Phys. Comm.}, { 108}, 29 (1998).} {11}{C. Leforestier, L. B. Braly, K. Liu, M. J. Elrod and R. J. Saykally, { J. Chem. Phys.}, { 106}, 8527 (1997).} {12}{E. A. McCullough and R. E. Wyatt, { J. Chem. Phys.} { 51}, 1253 (1969).} {13}{B. Fornberg and D. M. Sloan, { Acta Numerica} (1994), pp. 203-267.} {14}{G. W. Wei, D. S. Zhang, D. J. Kouri and D. K. Hoffman, { Phys. Rev. Lett.} { 79}, 775 (1997).} {15}{R. Guantes and S. C. Farantos, {J. Chem. Phys.}, {111}, 10827, 1999.} {16}{C. L. Lopreore and R. E. Waytt, {Phys. Rev. Lett.}, {82}, 5190 (1999).} {17}{T. Belytschko, Y. Krongauz, D. Organ M. Fleming and P. Krysl, { Comput. Methods Appl. Mech. Eng.} { 139}, 3 (1996).} {18}{S. C. Farantos, { Comp. Phys. Comm.} {108}, 240 (1998).} {19}{H. Ishikawa, R. W. Field, S. C. Farantos, M. Joyeux, J. Koput, C. Beck and R. Schinke, { Ann. Rev. Phys. Chem.}, 50, 443 (1999).}