OBSERVATIONS OF ROTATIONAL MAGNETIC-MOMENTS IN THE GROUND AND SOME EXCITED VIBRATIONAL SIGMA-STATES OF C2H2, C2HD, AND C2D2 BY MAGNETIC VIBRATIONAL CIRCULAR-DICHROISM
Cn. Tam et al., OBSERVATIONS OF ROTATIONAL MAGNETIC-MOMENTS IN THE GROUND AND SOME EXCITED VIBRATIONAL SIGMA-STATES OF C2H2, C2HD, AND C2D2 BY MAGNETIC VIBRATIONAL CIRCULAR-DICHROISM, The Journal of chemical physics, 104(5), 1996, pp. 1813-1824
Magnetic vibrational circular dichroism (MVCD) spectra of acetylene an
d its deuterated isotopomers have been recorded for the following Sigm
a symmetry combination and overtone bands of C2H2: nu(4)+nu(5); C2HD:
nu(4)+nu(5); 2 nu(4), 2 nu(5); C2D2: nu(4)+nu(5): the nu(3) fundamenta
l for C2HD and C2D2; and the nu(4)-->2 nu(4)+nu 5 and nu(5)-->nu(4)+2
nu(5) hot bands for C2H2. For a Sigma(g)-->Sigma(u) transition, the MV
CD A terms observed must arise primarily from the rotational Zeeman ef
fect. These negative A(1)/D-0 values for low J '' transitions confirm
that the sign of the rotational g-value for acetylene is positive. The
rotational magnetic moments in both the lower and upper vibrational s
tates were determined by comparison of moment analyses of experimental
and simulated MVCD spectra obtained with a model Hamiltonian for acet
ylene. The g(J) values in all the excited bending combination and over
tone vibrational levels observed are smaller than those in the ground
and the first excited stretching vibrational levels. This observation
has been confirmed by theoretical simulation of the MVCD spectra of th
e nu(4)+nu(5) combination band of C2H2. From these MVCD results, for C
2H2, g(J)(ground) = +0.0535+/-0.0033 and Delta g(nu(4)+nu(5)) = -0.006
1+/-0.0004; for C2HD, g(J)(ground)similar to g(J)(nu(3)) = +0.0363+/-0
.0048, Delta g(nu(4)+nu(5)) = -0.0052+/-0.0031; and for C2HD, g(J)(gro
und)similar to g(J)(nu(3)) = +0.0409 +/- 0.0069. These are the first q
uantitative, MVCD determinations of nondegenerate excited state g valu
es distinctly different from the ground state. The decrease in g value
correlates with off-axis deformation of the linear C2H2 rotation. (C)
1996 American Institute of Physics.