화학공학소재연구정보센터
Journal of Physical Chemistry B, Vol.103, No.50, 11016-11020, 1999
Third-order nonlinear optical properties of donor-acceptor organometallic compounds in films and solution
The third-order nonlinear optical susceptibilities, chi((3))(-3 omega; omega, omega, omega), of push-pull organobimetallic Mo/Fe compounds of the type [Mo(Tp(An))(NO)(Cl){(HN-pi-bridge)(4-Fc)}] {Tp(An) = hydrotris(3-p-methoxyphenylpyrazol-1 -yl)borate; Fc= (eta(5)-C5H4)Fe(eta(5)-C5H5); bridge = C6H4 (1), C6H3(3-R)-4-[N=N-C6H3(3-R')] [R= R'= H (2); R= CH3, R'= H (3); R= R'= CH3 (4)], C6H4-4-[CH=CH-C6H4] (7)} ("straight" compounds) and [Mo(Tp(An))(NO)(Cl){HNC6H3(3-CH3)[-N=N-C6H3(5-CH3) -2-{(eta(5)-C5H5)}]-4}](5) ("bent" compound) have been measured in both chloroform solutions (at lambda = 1907 nm) and dispersed into spin-coated poly(methyl methacrylate) films (at lambda = 1907 nm and lambda = 1064 nm). For comparison, THC measurements were carried out on films containing two related organometallic compounds, [4-O2NC6H3(2-CH3)N=NC6H3(5'-CH3)-2'-{(eta(5)-C5H4)Fe(eta(5)-C5H5)}](6) ("bent" derivative) and [4-O2NC6H4CH=CHC6H4-4'-{(eta(5)-C5H4)Fe(eta(5)-C5H5)}] (8) ("Straight" derivative), where the nitro group has been substituted for the [Mo(Tp(An))(NO)(Cl)] one as the acceptor moiety. Some trends for the role of conjugation length, substituents in the bridge, and molecular characteristics ("straight" or "bent") have been identified. From the solution data the real and imaginary components of the molecular cubic hyperpolarizability gamma(3 omega; omega, omega, omega) have been determined for 1-5 and 8. The real cubic hyperpolarizability gamma(r) is negative for the compounds 1-5, whereas it becomes positive for the compound 8. Highest values \y\ congruent to 5 x 10(-33) esu have been obtained for "straight" aza-bridged derivatives 2-4 having the [Mo(Tp(An))(NO)(Cl)] fragment as acceptor group. They are comparable to those reported for highly conjugated planar phthalocyanines and other related compounds. The susceptibilities chi((3))(3 omega; omega, omega, omega) measured at lambda = 1907 nm for the spin-coated films show similar trends as those derived for the hyperpolarizabilities. For the "straight" organobimetallic compounds 1-4 and 7 the chi((3))(3 omega; omega, omega, omega) values at;l = 1907 nm are higher than those measured at a = 1064 nm. On the other hand, for the "bent" organobimetallic compound 5 and the two nitro derivatives 6 and 8 having the acceptor NO2 group, the wavelength behavior is just opposite.