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有馬 寛*; 宮田 登*; 吉田 鉄生*; 笠井 聡*; 大内 啓一*; Zhang, S.*; 宮崎 司*; 青木 裕之
Review of Scientific Instruments, 91(10), p.104103_1 - 104103_7, 2020/10
被引用回数：9 パーセンタイル：56.16(Instruments & Instrumentation)We developed a novel humidity control system for neutron reflectivity measurements based on the two-way gas-flow method that can generate up to 85% relative humidity (RH) within a temperature range of 5-85
C. The system consists of a gas-flow-type humidity generator and a thermostatic sample chamber, each of which can independently control the temperature. The key features include rapid humidity response and long stable operation time. The humidity reaches equilibrium within 2 to 5 min during the humidity change, and the system exhibited acceptable stability over a three-day, nonstop experimental measurement duration, with a precision of 
1% RH at 85C and 85% RH. The sample chamber is capable of measuring substrate samples with dimensions of up to 2-in. in diameter and 5-mm in thickness. We demonstrate the reflectivity data measured at a pulsed neutron facility, MLF BL17, in the Japan Proton Accelerator Research Complex. The combined use of this system with neutrons permits in situ, time-resolved studies of the swelling process of polyvinyl alcohol and adhesive materials.
和泉 篤士*; 首藤 靖幸*; 柴山 充弘*; 吉田 鉄生*; 宮田 登*; 宮崎 司*; 青木 裕之
Macromolecules, 53(10), p.4082 - 4089, 2020/05
被引用回数：7 パーセンタイル：32.71(Polymer Science)The interfacial structure of a hexamethylenetetramine-cured phenolic resin on a silica surface was investigated by the complementary use of X-ray and neutron reflectivity (XRR and NR, respectively). The contrast-variation technique was applied using D
O for the NR analysis in which the coherent neutron scattering length density (SLD) largely changed owing to the DO absorption of the dry phenolic resin and the hydrogen-to-deuterium exchange of phenolic hydroxyl groups. The XRR profile indicated no clear interfacial structure in terms of the mass density, whereas the NR profile indicated the presence of an interfacial nanolayer on the native silica surface according to the SLD. The thickness of the interfacial layer was 1-2 nm, which was independent of the thickness of the bulk resin layer. The formation of the interfacial layer on the silica surface could be caused by preferential adsorption of the novolac resin on the silica surface via strong hydrogen bonding between phenolic units in the novolac resin and silica surface comprising silanol and silyl ether groups resulting in interfacial cross-link inhomogeneity of the phenolic resin on the silica surface in the thickness direction. To the best of our knowledge, this is the first report of an experimental elucidation of the buried interfacial structure between the phenolic resins on the silica surface at a nanometer level.
宮崎 司*; 宮田 登*; 吉田 鉄生*; 有馬 寛*; 津村 佳弘*; 鳥飼 直也*; 青木 裕之; 山本 勝宏*; 金谷 利治*; 川口 大輔*; et al.
Langmuir, 36(13), p.3415 - 3424, 2020/04
被引用回数：14 パーセンタイル：58.64(Chemistry, Multidisciplinary)We investigated in detail the structures in the poly(vinyl alcohol) (PVA) adsorption layers on a Si substrate, which remained on the substrate after immersing the relatively thick 30 - 50 nm films in hot water, by neutron reflectometry under humid conditions. For the PVA with a degree of saponification exceeding 98 mol %, the adsorption layer exhibits a three-layered structure in the thickness direction. The bottom layer is considered to be the so-called inner adsorption layer that is not fully swollen with water vapor. This may be because the polymer chains in the inner adsorption layer are strongly constrained onto the substrate, which inhibits water vapor penetration. The polymer chains in this layer have many contact points to the substrate via the hydrogen bonding between the hydroxyl groups in the polymer chain and the silanol groups on the surface of the Si substrate and consequently exhibit extremely slow dynamics. Therefore, it is inferred that the bottom layer is fully amorphous. Furthermore, we consider the middle layer to be somewhat amorphous because parts of the molecular chains are pinned below the interface between the middle and bottom layers. The molecular chains in the top layer become more mobile and ordered, owing to the large distance from the strongly constrained bottom layer; therefore, they exhibit a much lower degree of swelling compared to the middle amorphous layer. Meanwhile, for the PVA with a much lower degree of saponification, the adsorption layer structure consists of the two-layers. The bottom layer forms the inner adsorption layer that moderately swells with water vapor because the polymer chains have few contact points to the substrate. The molecular chains in the middle layer, therefore, are somewhat crystallizable because of this weak constraint.
