We study fluctuation-induced interaction in confined fluids above the isotropic-lamellar transition. At an ideally continuous transition, the disjoining pressure has the asymptotic form Π(d → ∞) ≈ −CkBT q 2 0 /d, where d is the interwall distance, q0 is the wavenumber of the scattering peak, and C = 1/(4π) in the strong anchoring limit. The long-rangedness is enhanced due to continuous distribution of soft modes in the q-space. An unconventionally strong Casimir force with a range of several lamella thicknesses is realistic above the transition. We also find an oscillatory force profile near a surface-induced transition.PACS numbers: 68.15.+e, 64.60.Cn, 61.25.Hq, Fluids in confined geometries show a variety of phenomena that are not observed in bulk. Among them, thermal-fluctuation-induced interactions between boundary walls or objects immersed in the fluid have attracted much attention. They are called the Casimir forces by analogy with the quantum original [1]. The forces are long-ranged in systems with soft modes, such as critical simple fluids [2,3] and liquid crystals [4,5], with the decay law and amplitude modulated by various surface effects [3,6,7]. Recent evidence [8,9,10] supports the view that the interaction is ubiquitous in correlated fluids [11].In this Letter, we address the effect in structured fluids above the isotropic-lamellar (I-L) transition. The model system we consider has two characteristic lengths, which describe decay and oscillation of the correlation function. Physical realizations of the model include block copolymers in the disordered phase and bicontinuous microemulsions. Films of block copolymers have constituted the subject of numerous papers [12,13,14,15,16]. Most of them focus on the lamellar phase, while a few theoretical works treat the system above the I-L transition [15,16]. The latter works discuss the effect of a surface field, which induces a mean-field interaction between boundary walls. In comparison to the case of copolymers, much less is known about confined fluids containing short-chain surfactants [17,18,19]. A meanfield study with a standard Ginzburg-Landau model of microemulsions found a surface-induced I-L transition that preempts the bulk transition [17].The bulk property of the system we assume is described by the Hamiltonianwhere ǫ is a constant, φ is the order parameter, and p 0 and q 0 are characteristic wavenumbers that generally depend on the temperature. This and similar types of Hamiltonians, with or without additional nonlinear terms, have been applied to various kinds of complex fluids [20,21,22,23]. For symmetric AB-block copolymer melts, for instance, φ represents the excess of Amonomer's (say) volume fraction with respect to its spatial average, and the parameters are given by ǫ = 0.0327k B T R g /N 1/2 , q 0 = 1.95/R g , and1/4 /R g . Here, R g is the chain's gyration radius, N is the polymerization index, χ is the Flory interaction parameter, and χ c = 10.5/N locates the mean-field I-L transition [20]. To be general, we shall use the ratio p 0 /q...