ANALYSIS OF SF-6 QUASI-CONTINUUM STATES .2.

被引:13
作者
ANGELIE, C
机构
[1] Commissariat À l'Energie Atomique, Centre d'Etudes Nucléaires Saclay, DSM/DRECAM/SPAM, 91191 Gif sur Yvette, Cedex
关键词
D O I
10.1063/1.464138
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The IR fluorescence data of SF6 excited in its quasicontinuum (QC), reported in paper I [C. Angelie, J. Chem. Phys. %, 8072 (1992)], are analyzed in comparison with IR multiphoton absorption (IRMPA) data, either in the nanosecond or in the picosecond regimes. A general description of the QC transition matrix elements is first derived. All the following features must be taken into account: multiple rovibrational transitions, perturbative redistribution onto secondary resonances, dissipative redistribution onto the whole energy shell, and intramolecular mode inhomogeneity producing a frequency dispersion. The intramolecular couplings obey a hierarchy V(k) versus the number k of quanta exchanged, with an effective density of couplings rho(k). A model without arbitrary parameters settles that the parameter gamma = pirho[V2] can be shared between a dissipative part gamma(d) approximately 1-1.5 cm-1 (for E approximately 10 000-15 000 cm-1), corresponding to the orders k greater-than-or-equal-to 5, and a perturbative part gamma(p) approximately 2-15 cm-1, corresponding to the lowest orders k congruent-to 3 and 4, i.e., the strongest couplings cannot produce the dissipative relaxation. The same model explains that the QC threshold is at E approximately 4000 cm-1, as demonstrated by Raman experiments, with a half-width gamma(d) approximately 0.21 cm-1, in excellent agreement with picosecond spectroscopy giving a T1 relaxation time of approximately 11 ps. The parameter gamma is also extracted from IRMPA cross sections. It is found from these data that gamma(E) increases from 0.25 to 15 cm-1 when E increases from 4000 to 34000 cm-1. Finally, picosecond data, showing a spectacular enhancement of the number of photons absorbed for short pulses of duration tau(L) approximately 30 ps, are fully explained by the previous QC description: Energy is mainly absorbed selectively in the nu3 mode, producing a dramatic enhancement of the Rabi width. Then, all known data on the SF6 QC can be incorporated in a unique framework, likely generalizable to other molecules.
引用
收藏
页码:2541 / 2563
页数:23
相关论文
共 48 条
[2]   MULTIPHOTON ABSORPTION OF 12CF3L, 13CF3L, CF3BR AND SF6 BY A HIGH-PRESSURE CO2-LASER [J].
ANGELIE, C ;
CAPITINI, R ;
GIRARD, P .
LASER CHEMISTRY, 1987, 7 (5-6) :305-331
[3]   THEORETICAL-STUDY OF THE SF6 QUASI-CONTINUUM - HOMOGENEOUS LINEWIDTH, ISOTOPIC SELECTIVITY, ROTATIONAL HEATING [J].
ANGELIE, C ;
MILLIE, P .
CHEMICAL PHYSICS, 1983, 82 (1-2) :171-197
[4]   OUT OF RESONANCE INFRARED FLUORESCENCE OF SF6, (CF3I)-C-12, (CF3I)-C-13 IN QUASI-CONTINUUM STATES .1. [J].
ANGELIE, C .
JOURNAL OF CHEMICAL PHYSICS, 1992, 96 (11) :8072-8085
[5]  
Bagratashvili V. N., 1979, SOV PHYS JETP, V50, P1075
[6]   STOCHASTIZATION LIMIT OF VIBRATIONAL-ENERGY IN SF6 AND CF3I MOLECULES AT IR MULTIPLE PHOTON EXCITATION [J].
BAGRATASHVILI, VN ;
DOLJIKOV, VS ;
LETOKHOV, VS ;
MAKAROV, AA ;
MALJAVKIN, LP ;
RYABOV, EA ;
SILKIS, EG ;
VAINER, YG .
OPTICS COMMUNICATIONS, 1981, 38 (01) :31-34
[7]  
BAGRATASHVILI VN, 1989, MULTIPLE PHOTON INFR
[8]  
BAGRATASHVILI VN, 1981, SOV PHYS JETP, V53, P512
[9]   INTRAMOLECULAR RADIATIONLESS TRANSITIONS [J].
BIXON, M ;
JORTNER, J .
JOURNAL OF CHEMICAL PHYSICS, 1968, 48 (02) :715-&
[10]   COLLISIONLESS MULTI-PHOTON ENERGY DEPOSITION AND DISSOCIATION OF SF6 [J].
BLACK, JG ;
KOLODNER, P ;
SHULTZ, MJ ;
YABLONOVITCH, E ;
BLOEMBERGEN, N .
PHYSICAL REVIEW A, 1979, 19 (02) :704-716