Detection of Two Glass Transitions on Triton X100 under Connement Esther G. Merino, Paulo D. Neves, , Isabel M. Fonseca, Florence Dane ́ de, § Abdenacer Idrissi, C. J. Dias, Madalena Dionísio,* , and Nata ́ lia T. Correia* ,,§ REQUIMTE/CQFB, Departamento de Química, Faculdade de Ciê ncias e Tecnologia, Universidade Nova de Lisboa, 2829-516 Caparica, Portugal CENIMAT/I3N, Departamento de Ciê ncia dos Materiais, Faculdade de Ciê ncias e Tecnologia, FCT, Universidade Nova de Lisboa, 2829-516 Caparica, Portugal § Unite ́ Mate ́ riaux Et Transformations (UMET), UMR CNRS 8207, UFR de Physique, BAT P5, Universite ́ Lille Nord de France, F-59655 Villeneuve dAscq Cedex, France Laboratoire de Spectrochimie Infrarouge et Raman (LASIR), UMR CNRS 8516, BAT C5, Universite ́ Lille Nord de France, F-59655 Villeneuve dAscq Cedex, France ABSTRACT: Because of the strong tendency of Triton X-100 to crystallize, inclusion in a SBA-15 matrix of 5.7 nm in pore diameter was used as a means to suppress crystallization. Clear evidence that Triton X-100 exists under connement in the amorphous and supercooled state is given by X-ray diraction supported by dierential scanning calorimetry and dielectric relaxation spectroscopy. From the thermogravimetric analysis, a loading degree of 50% (wt) was estimated; the decomposition of conned Triton X-100 follows a two-step prole, indicating that molecules are partitioned between bulklike and adsorbed, the latter fraction being in a higher proportion. This allowed the unequivocal detection by DSC of two well-resolved glass transitions (20 K apart), which is a remarkable result obtained by conventional calorimetric analysis in conned systems. The two molecular populations have dierent mobilities giving rise to two dierent dielectric relaxation processes: an α Tr/SBA bulklike process associated with molecules located more in the center of the pores, slightly slowed down relative to bulk α-relaxation, and an S-process due to molecules absorbed at the walls with signicantly hindered mobility. Moreover, an MWS process is detected due to interfacial polarization that builds up between the adsorbed Triton X-100 molecules and SBA pore walls whose temperature dependence seems to be correlated with the one of the S-process. The inclusion in SBA-15 revealed to be a good strategy to simultaneously avoid crystallization and achieve a long-term stabilization of the disordered form. 1. INTRODUCTION Connement studies emerged recently as an attractive means to explore fundamental concepts concerning condensed matter physics. In this context, particular attention is given to the inuence of connement on the glass transition: 1,2 for polymer thin lms, the studies concern mainly the thickness dependence of the glass transition temperature (T g ), whereas, for molecular guests conned to nanosized porous restricted geometries, the focus is given to the inuence of the host pore dimensions (refs 1, 3, and 4, and references therein); recently, a correlation between the glass transition temperature and the interfacial free volume has been proposed. 5 In systems exhibiting a distribution of the glass transition as multilayered polymer thin lms, sophisticated techniques are needed, such as neutron reectivity, to reveal multiple T g s, 6,7 instead of thermal techniques as calorimetry. Even for glass formers conned to nanogeometries, which have been extensively studied in the literature, the calorimetric detection of two glass transitions is not trivial. A few examples are provided as polystyrene/o-terphenyl solutions in controlled pore glasses (CPGs), 8 salol in silica mesopores, 9 propylene glycol in CPG, 10 and acetaminophen in nanoporous Vycor glass. 11 In the present work, evidence of a bimodal behavior concerning the glass transition of the water-soluble, liquid surfactant Triton X-100 entrapped in a nanoporous matrix is investigated by dierential scanning calorimetry (DSC) and dielectric relaxation spectroscopy (DRS). These techniques were employed in previous works by some of us 12,13 to evaluate the temperature-driven phase transformations and dynamical Received: May 1, 2013 Revised: September 18, 2013 Published: September 18, 2013 Article pubs.acs.org/JPCC © 2013 American Chemical Society 21516 dx.doi.org/10.1021/jp404306a | J. Phys. Chem. C 2013, 117, 2151621528