J π = 0 + states have been investigated in the actinide nucleus 240 Pu up to an excitation energy of 3 MeV with a high-resolution (p,t) experiment at Ep= 24 MeV. To test the recently proposed J π = 0 + 2 double-octupole structure, the phenomenological approach of the spdf-interacting boson model has been chosen. In addition, the total 0 + strength distribution and the 0 + strength fragmentation have been compared to the model predictions as well as to the previously studied (p,t) reactions in the actinides. The results suggest that the structure of the 0 + 2 states in the actinides might be more complex than the usually discussed pairing isomers. Instead, the octupole degree of freedom might contribute significantly. The signature of two close-lying 0 + states below the 2-quasiparticle energy is presented as a possible manifestation of strong octupole correlations in the structure of the 0 + 2 states in the actinides.The nature of the first excited2 ) states in the even-even actinides has been controversially discussed for decades. Extensive experimental studies had shown an asymmetry between the population in (p,t) and (t,p) reactions [1][2][3]. While large (p,t) cross sections were observed (σ 0/σ gs < 2%) were seen in the studies of Casten et al. [3]. Ragnarsson and Broglia proposed to interpret these states as pairing isomers having a smaller neutron pairing gap ∆ n than the ground state itself [4,5]. These isomers should be present in the case of an inhomogeneity of weakly coupled prolate and oblate levels around the Fermi surface for comparable monopole and quadrupole pairing strengths. The experimental signature of these pairing isomers would be large (p,t) cross sections and almost vanishing (t,p) cross sections [4]. Furthermore, Rij and Kahana predicted a negligible population of these states in single-neutron transfer reactions [5]. However, in 240 Pu a strong (d,p) population of the 0 + 2 state (σ 0 + 2 /σ gs ≈ 18%) was observed [6]. In addition to the peculiar situation of an inhomogeneous distribution of oblate and prolate single-particle orbitals around the Fermi surface, the octupole degree of freedom contributes significantly to the low-energy spectrum of the actinide nuclei [7,8]. The enhanced octupole collectivity, which has been observed in several experimental and theoretical studies, has been mainly attributed to the strong octupole interaction involving unique neutron and proton single-particle orbitals differing by ∆j = ∆l = 3. These are the j 15/2 and g 9/2 orbitals (N ∼ 134) for the neutrons, and the i 13/2 and f 7/2 orbitals (Z ∼ 88) in the case of the protons. One of the most striking signatures of * spieker@ikp.uni-koeln.de; Member of the Bonn-Cologne Gradu- ). In the even-even Pu isotopes the strongest octupole correlations have been found for 240 Pu by means of an alternating-parity band at high spins (J ∼ 20) [12]. Using two-center octupole wave functions in the framework of supersymmetric quantum mechanics, Refs. [13,14] explained the experimental data as a second-order phase tran...