High-resolution FTIR study of the (ν3+ν4,ν1+ν4) interacting system of rovibrational bands of PF3 between 1100 and 1300 cm-1

被引:14
作者
Ben Sari-Zizi, N
Najib, H
Sebihi, R
Pracna, P
机构
[1] Univ Mohammed 5, Fac Sci, Lab Spect Phys Appl, Rabat, Morocco
[2] J Heyrovsky Inst Phys Chem, Prague 18223 8, Czech Republic
关键词
D O I
10.1006/jmsp.1998.7568
中图分类号
O64 [物理化学(理论化学)、化学物理学]; O56 [分子物理学、原子物理学];
学科分类号
070203 ; 070304 ; 081704 ; 1406 ;
摘要
With a resolution of 4.4 x 10(-3) cm(-1), we were able to identify in this range the very weak nu(2) + 2 upsilon(4)(0 )(A(1)) component near 1180 cm(-1), the upsilon(3) + upsilon(4) band around 1205 cm(-1) with its (A(1) + A(2)) and E very intermixed components, and the upsilon(1) + upsilon(4) (E) band centered at 1238 cm(-1). Three thousand six hundred transitions belonging to the (upsilon(3) + upsilon(4), upsilon(1) + upsilon(4)) interacting system were fitted together with a model taking into account l(2, 2) interactions inside upsilon(1) + upsilon(4)( )and between (A(1 )+ A(2)) and E components of upsilon(3) + upsilon(4), the l-vibrational resonance inside upsilon(3) + upsilon(4)(A(1) + A(2)), and the Coriolis interactions between upsilon(1) + upsilon(4) and upsilon(3) + upsilon(4 )(A(1) + A(2)) On one hand and between upsilon(1) + upsilon(4) and upsilon(3) + upsilon(4) (E) on the other. Four available MW transitions were also included in the fit. A rms of 0.76 x 10(-3) cm(-1) was obtained with 34 free parameters among 38. Normally the Fermi resonance, which links upsilon(3) to upsilon(2) + upsilon(4) with a coupling term W-234 = 2.86 cm must connect each component of upsilon(3) + upsilon(4) with each component of upsilon(2 )+ 2 upsilon(4). But since we have only little experiment information about the weak upsilon(2) + 2 upsilon(4)(0) component (120 assigned lines) and none about the dark upsilon(2 )+ 2 upsilon(4)(+/-2 )component It was not possible to introduce this resonance in the fit. However, the bandcenters' shifts were calculated since the basic coupling term W-234 and the anharmonic constant x(24) are well known. Therefore, according to this approximation, the very sensitive anharmonic constants x(34) and g(34) could be deduced. Of course the x(14) Fermi-independent constant, derived directly from the (upsilon(1) + upsilon(4))(0) bandcenter given by the fit, was certainly more accurate. (C) 1998 Academic Press.
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页码:15 / 27
页数:13
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