Ultrathin and ordered stacking of silica nanoparticles

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ultrafiltration membranes. 4 ... Ultrafiltration (UF) membranes composed of an ultrathin and ordered layer of silica .... solution was pressurized to 2.5 bar.
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Ultrathin and ordered stacking of silica nanoparticles

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via spin-assisted layer-by-layer assembly under

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dehydrated

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ultrafiltration membranes

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Daisuke Saeki and Hideto Matsuyama*

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Center for Membrane and Film Technology, Department of Chemical Science and Engineering,

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Kobe University, 1-1 Rokkodai, Nada, Kobe 657-8501, Japan.

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E-mail address of Daisuke Saeki: [email protected]

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*

conditions

for

the

fabrication

of

Corresponding author. E-mail: [email protected]; Tel.: +81-78-803-6180; Fax: +81-78-803-6180.

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ABSTRACT

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Ultrafiltration (UF) membranes composed of an ultrathin and ordered layer of silica nanoparticles

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(NPs) was fabricated via spin-assisted layer-by-layer (LbL) assembly in dehydrated conditions.

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Anionic silica NPs and cationic sacrificial polymers were alternately stacked on an anodic

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aluminum oxide support membrane via electrostatic interactions. The assembly was then

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calcinated to remove the sacrificial polymers and form a stacked-NP membrane. The structure of

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the NP layers was controlled by altering the number of stacked-NP layers formed during the LbL

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assembly processes and performing an ethanol-based dehydration treatment. Increasing the

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number of NP layers increased the total thickness of the stacked-NP layer and decreased the water

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permeability. The rejection performance against dextran was improved by increasing the number

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of NP layers, indicating a decrease in the number of defects. The ethanol-based dehydration

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treatment successfully decreased the total thickness of the stacked-NP layer and improved the

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rejection performance against dextran. The surface morphology of the NP layers became smoother

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by the ethanol-based treatment. These results indicate that the ethanol-based treatment produces

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dense NP layers with an ordered structure by removing water molecules adsorbed on the sacrificial

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polymers and NPs. The performance of the stacked-NP membranes was superior to that of

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commercial UF membranes.

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Keywords: layer-by-layer assembly; stacked-nanoparticle membrane; ultrafiltration membrane,

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dehydration.

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1. INTRODUCTION

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Membrane separation has attracted much attention for water purification applications

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because of the high space and energy efficiencies compared to heat-based processes, such as

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distillation. Ultrafiltration (UF) is widely applied to separate dispersed materials, such as particles

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and colloids, from a solvent. The uniformity of the pores and low film thickness of an active

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separation layer are important factors for improving the solvent permeability and selective

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rejection of targets. Polymeric UF membranes are used because of their low fabrication costs and

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easy fabrication processes. Such membranes are fabricated from various polymers via phase

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separation methods, which is induced by a change in temperature or the addition of non-solvents

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[1]. Ceramic UF membranes are also used because of their high chemical and thermal stability,

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and are mainly fabricated via sol-gel methods [2, 3].

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Layer-by-layer (LbL) assembly methods have been used to easily fabricate well-controlled,

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thin, polymeric films on various substrates through molecular interactions, such as electrostatic

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interactions [4], hydrophobic interactions [5], hydrogen bonding [6, 7], and covalent bonding [8,

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9]. In the case of LbL assembly by electrostatic interactions, a substrate is alternately immersed in

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aqueous solutions/dispersions of oppositely charged materials, such as polyelectrolytes, and an

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extremely thin film is obtained. The film thickness can be controlled at the nanometer scale. LbL

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assembly has been applied to the preparation of microcapsules [10], surface coatings [11], and

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membranes for liquid [12-16] and gas separation [17]. LbL assembly of nanotubes [18-21] and

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nanosheets [22-26] is also attracted for the fabrication of functional thin structures.

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Recently, structures composed of stacked nanoparticles (NPs) have been applied to the

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fabrication of both thin films for functional coatings [27-32] and porous membranes for liquid

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separation [33-38]. The well-packed structure of the NPs produces a uniform surface structure with

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uniform pores between the NPs. Stacked-NP structure in the previous studies are formed by

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vacuum filtration [33, 34, 36, 37], dip- or rod-coating [35, 39], LbL assembly [28-30, 32, 38], and

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spin-assisted LbL assembly [15, 27, 31, 40-42], etc. In particular, spin-assisted LbL assembly is

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effective at controlling the uniformity and density of stacked structures. This is because the

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centrifugal force caused by the spinning process removes adsorbed water molecules from the

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materials stacked on a substrate, which results in the densification of the stacked materials [27].

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Therefore, stacked-NP structures formed via spin-assisted LbL assembly have great potential for

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the fabrication of porous membranes with well-controlled pore diameters and a thin active

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separation layer for water purification applications.

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In this study, we fabricated UF membranes composed of an extremely thin stacked-NP

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layer via spin-assisted LbL assembly. Anionic silica NPs were alternately stacked with cationic

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sacrificial polymers on a porous support membrane via spin-assisted LbL assembly and

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electrostatic interactions. After a calcination process, a stacked-NP layer was formed on the

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support membrane. The performance of the stacked-NP layer as a UF membrane was evaluated

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based on its water permeability and rejection of various molecular weights of dextran. On LbL

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assembly processes in aqueous conditions, polyelectrolytes have a large free volume caused by the

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adsorption of water molecules, and prevent well packing of NPs. For further improvement of the

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packing density of the stacked-NP layer and membrane performance, we examined the dehydration

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of the sacrificial polymers by performing an ethanol-based treatment to remove water molecules

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adsorbed on the sacrificial polymers and NPs during the LbL assembly processes.

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2. EXPERIMENTAL

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2.1. Materials

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All chemicals were purchased from Wako Pure Chemical Industries (Osaka, Japan) unless

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otherwise specified, and used as received. Aqueous solutions were prepared with Milli-Q water (>

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18.2 MΩ⋅cm, Merck Millipore, Billerica, MA, USA). An anodic aluminum oxide membrane

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(Anodisc, pore diameter = 0.02 μm, Whatman, Maidstone, England) was used as a support

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membrane.

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Polydiallyldimethylammonium chloride (PDDA; molecular weight (Mw) = 400–500 kDa) was

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purchased from Sigma-Aldrich (St. Louis, MO, USA), and used to form sacrificial layers as

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polycations. Dextran was purchased from Nakarai Tesque (20 kDa; Kyoto, Japan), and Sigma-

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Aldrich (6, 40, 100, and 500 kDa) to evaluate the rejection performance and pore diameter of the

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membranes. Ethanol was used to dehydrate membrane surfaces because it is a water-miscible,

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volatile solvent and is a non-solvent for silica NPs and PDDA. The chemical structures of TEOS

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and PDDA, and the surface morphology of an anodic aluminum oxide support membrane are

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shown in Fig. 1.

Tetraethyl orthosilicate (TEOS) was used

to

prepare the silica NPs.

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Fig. 1. Chemical structures of (A) TEOS and (B) PDDA. (C) Field emission scanning electron

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microscopy (FE-SEM) image of the surface of an anodic aluminum oxide support membrane.

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2.2. Preparation of silica NPs

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A suspension of silica NPs was prepared by a sol-gel method [29]. TEOS (2.23 mL) was

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added to 992.5 mL of Milli-Q water and magnetically stirred at 400 rpm for 2 h. Then, 5.63 mL of

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aqueous sodium hydroxide (0.05 mol) was added to the TEOS solution and stirred for 2 days. The

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prepared suspension was filtered through a MILLEX-AP syringe filter (pore diameter = 2.0 µm,

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Merck Millipore, Billerica, MA, USA) to remove large aggregates. The diameter of the as-

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prepared NPs was evaluated via dynamic light scattering (DLS; ELSZ-1000ZS, Otsuka

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Electronics, Osaka, Japan). The morphology of the as-prepared NPs was observed with field

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emission scanning electron microscopy (FE-SEM; JSF-7500F, JEOL, Tokyo, Japan). For the FE-

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SEM observations, the samples were freeze-dried under vacuum conditions (FDU-1200; Tokyo

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Rikakikai, Tokyo, Japan) and then coated with osmium (Neoc; Meiwafosis, Tokyo, Japan).

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2.3. Fabrication of stacked silica-NP membranes

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Stacked silica-NP membranes were prepared via spin-assisted LbL assembly with or

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without a dehydration process (Fig. 2). First, an anodic aluminum oxide membrane was placed on

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the stage of the spin-coater (MS-A100, Mikasa, Tokyo, Japan). A sacrificial cationic PDDA layer

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was then formed on the surface of the support membrane. An aqueous solution of PDDA (0.25

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wt.%) was dropped on the support membrane and spun at 3000 rpm for 15 s. Then, Milli-Q water

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was dropped and spun to wash the membrane surface ten times. For some of the membranes

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fabricated, ethanol was dropped and spun to dehydrate the membrane surface ten times. Next, a

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layer of stacked silica NPs was formed on the sacrificial PDDA layer. The silica-NP suspension

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was dropped, spun, and washed under the same conditions as the PDDA layer. This stacking cycle

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was repeated 3, 5, or 7 times. The PDDA/stacked-NP membranes were calcinated at 500 οC for 5

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h to remove the sacrificial PDDA layers and bind the NPs each other [2, 29], and the membranes

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composed of 3, 5, or 7 layers of stacked NPs were obtained.

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Fig. 2. Schematic diagram of the spin-assisted layer-by-layer (LbL) method.

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2.4. Characterization of the surface properties of the fabricated membranes

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The surface morphology of the fabricated membranes was observed via FE-SEM and

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atomic force microscopy (AFM; SPA-400, Hitachi High-Tech Science, Tokyo, Japan). The total

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thickness of the NP layer was measured from cross-sectional FE-SEM images. The AFM

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observations were carried out with a SI-DF40P2 cantilever (Hitachi High-Tech Science) in tapping

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mode. The ζ-potentials of the silica-NP and PDDA surfaces were measured with an electrophoretic

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light-scattering apparatus (ELSZ-1000ZS) using a flat quartz cell in aqueous sodium chloride (10

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mmol) at a pH of 6.7. The chemical composition of the membrane surfaces was analyzed with X-

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ray photoelectron spectroscopy (XPS; JPS-9010, JEOL). For the AFM observations, FE-SEM

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observations, and XPS analyses, the samples were freeze-dried under vacuum conditions.

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2.5. Membrane performance

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The membrane performance was evaluated with a cross-flow membrane filtration system,

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the details of which were previously reported by our group [43]. The effective diameter of each

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membrane sample was 10.0 mm. The water permeability of the fabricated membranes was

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evaluated using Milli-Q water as a feed solution, and calculated from the weight gain of the

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permeate solution. Aqueous solutions containing 1.0 g/L of one of five molecular weights of

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dextran (6, 20, 40, 100, and 500 kDa) and 1.0 g/L of ethylene glycol as a reference material were

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used as the feed solutions to evaluate the rejection performance of the membranes. The feed

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solution was pressurized to 2.5 bar. The dextran concentration in the permeate solution was

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analyzed via gel permeation chromatography (GPC) at 1.0 mL/min and 40 οC with a refractive

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index detector (RID-10A, Shimadzu, Kyoto, Japan) and a Shodex SB-805HQ column (Showa

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Denko, Tokyo, Japan). The rejection of dextran, R, was calculated from the peak-area ratios with

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the following equation: R = 1 − (AP,d/AP,r)/(AF,d/AF,r), where AP,d, AP,r, AF,d, and AF,r indicate the

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peak areas of dextran and ethylene glycol in the permeate and feed solutions, respectively. The

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standard deviations were calculated from the measurements for at least three samples

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independently fabricated. For comparison purposes, the performance of commercial organic UF

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membranes (polyethersulfone membrane, molecular weight cut-off = 30 kDa; regenerated

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cellulose membranes, molecular weight cut-off = 30, 100, and 300 kDa; Millipore) and ceramic

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UF membranes (molecular weight cut-off = 15, 50, 150, and 300 kDa; Sterlitech, Kent, WA, USA)

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was also evaluated.

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3. RESULTS AND DISCUSSION

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3.1. Stacked silica-NP membranes fabricated via spin-assisted LbL assembly

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The average diameter of the as-prepared silica NPs was approximately 8.2 nm (standard

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deviation (S.D.) = 0.7 nm), which was measured by DLS. An FE-SEM image of the NPs (Fig. S1

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of the Supplementary Material) also shows that the diameter of the NPs is approximately 10 nm.

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The ζ-potentials of the silica-NP and PDDA surfaces were −17.5 and 21.2 mV, respectively. Table

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1 shows the chemical compositions of the membrane surfaces, which were determined via XPS

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analysis. When the surface of the support membrane is coated with PDDA, carbon, nitrogen, and

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chlorine are detected. The subsequent coating of the membrane with silica NPs increases and

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decreases the relative concentrations of silicon and aluminum, respectively. Nitrogen was not

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detected in the membrane surface after the calcination process because the sacrificial PDDA layers

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decompose during this process. The FE-SEM images (Fig. S2 of the Supplementary Material)

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show the same trends, i.e., a large number of silica NPs are present on the support membrane

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coated with NPs after the sacrificial PDDA layer was formed, while only a few NPs are present

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without the PDDA layer. This result indicates that the silica NPs interact with the PDDA-coated

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support membrane via electrostatic interactions, and LbL assembly enables the alternate stacking

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of layers of silica NPs and sacrificial PDDA on the support membrane.

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Table 1. Chemical compositions of the surfaces of the stacked-NP membranes, which were

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determined via XPS analysis (all values in atomic %).

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a

Membranes

Al

O

Si

C

N

Cl

Pristine membrane

30.43

69.57

-a

-

-

-

PDDA-coated membrane

28.40

57.47

-

10.34

0.82

2.97

PDDA- and NP-coated membrane (3 layer)

8.42

61.12

24.59

4.68

1.19

-

PDDA- and NP-coated membrane (3 layer) after calcination

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60.59

27.60

2.70

-

-

- = element was not detected.

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Fig. 3 shows FE-SEM images of the membranes coated with different numbers of NP

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layers after calcination. For the fabrication of these membranes, the ethanol-based dehydration

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treatment was not carried out. The surfaces of all the fabricated membranes are not flat, and there

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is a large amount of aggregates that are greater than 20 nm in diameter (Figs. 3(A−C)). Therefore,

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the stacking of the NPs on the support membranes is not well-ordered. The surface of the support

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membrane coated with 3 layers of NPs is not fully covered with the NPs (Fig. 3(A)). On the other

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hand, the surfaces of the membranes coated with 5 and 7 layers are completely covered (Figs. 3(B)

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and (C), respectively). In addition, the total thickness of the stacked-NP layer increases as the

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number of NP layers increases (Figs. 3(D−F)), indicating that the NPs were stacked by the LbL

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assembly processes. The surface morphology did not change before and after the membrane

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performance evaluations.

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Fig. 3. FE-SEM images of the membranes coated with different numbers of NP layers and without

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the ethanol-based dehydration treatment. (A−C) Surface views. (D−F) Cross-sectional views.

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Fig. 4 shows the performance of the membranes coated with different numbers of NP

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layers. The support membrane did not reject any molecular weight of dextran, and its water

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permeability was determined to be 4.6 × 103 L/(m2⋅h⋅bar). The water permeability of the stacked-

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NP membranes is drastically lower than that of the pristine support membrane, and it decreases as

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the number of NP layers increases. The increase of the water permeability did not occur during the

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permeation experiments, indicating the high stability of the fabricated membranes. The rejection

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of the 3-layer stacked-NP membrane for 500-kDa dextran is approximately 50%. This result could

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be explained by the fact that the pores of this membrane are not completely covered with NPs,

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which agrees with the FE-SEM image shown in Fig. 3(A). The rejection of the 5-layer stacked-NP

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membrane for 500-kDa dextran is over 90%, while that of the 7-layer stacked-NP membrane for

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100-kDa dextran is nearly 90%. Therefore, the rejection performance is improved by increasing

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the number of NP layers because of the more complete coverage of the pores of the support

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membrane with NPs.

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Fig. 4. Performance of the stacked-NP membranes. (A) Water permeability of the membranes and

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total thickness of the stacked-NP layer as functions of the number of NP layers. The filled and

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empty symbols indicate the water permeability and total thickness of the stacked-NP layer,

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respectively. (B) Rejection of the membranes against different molecular weights of dextran. The

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diamonds, squares, and triangles indicate the 3-, 5-, and 7-layer stacked-NP membranes,

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respectively.

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3.2. Effects of the ethanol-based dehydration treatment on the membrane performance

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In conventional LbL assembly methods that use electrostatic interactions in aqueous

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conditions, cationic and anionic polymers are stacked in a hydrated state, i.e., the polymers have a

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large free volume because of the presence of water molecules. In this study, to achieve a higher

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packing density of the NP layers, we examined the dehydration of the stacked polymers by

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performing an ethanol-based treatment between the alternate stacking of the NP layers and

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sacrificial polymeric layers. Fig. 5 shows FE-SEM images of the stacked-NP membranes that were

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subjected to the ethanol-based dehydration treatment. The membrane surfaces are completely

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covered with the NPs under all stacking conditions, and are flatter than the corresponding untreated

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membranes (Figs. 3(A−C)). In addition, the total thickness of the stacked-NP layer increases as

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the number of NP layers increases (Figs. 5(D−F)), which indicates that the ethanol-based treatment

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is applicable to the LbL assembly processes of the stacked-NP layers.

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Fig. 5. FE-SEM images of the membranes coated with different numbers of NP layers and

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subjected to the ethanol-based dehydration treatment. (A−C) Surface views. (D−F) Cross-sectional

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views.

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The performance of the stacked-NP membranes subjected to the ethanol-based treatment

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is shown in Fig. 6. The water permeability decreases as the number of NP layers increases. In

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addition, the water permeability of each ethanol-treated membrane is lower than that of the

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corresponding untreated membrane (Fig. 4(A)). The dextran rejection of the ethanol-treated

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membranes is much higher than that of the untreated membranes, and the molecular-weight cut-

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off curves of the ethanol-treated membranes are very sharp, as shown in Fig. 6(B). The dextran

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rejection of the ethanol-treated, 3-layer, stacked-NP membrane is the same as that of the untreated,

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7-layer, stacked-NP membrane. Furthermore, the rejection of the ethanol-treated, 7-layer, stacked-

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NP membrane for 6-kDa dextran is nearly 90%. These results indicate that the NPs are more

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densely packed after the ethanol-based dehydration treatment, and the pores between the NPs are

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more uniform.

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Fig. 6. Performance of the stacked-NP membranes subjected to the ethanol-based dehydration

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treatment. (A) Water permeability of the membranes and total thickness of the stacked-NP layer

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as functions of the number of NP layers. The filled and empty symbols indicate the water

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permeability and total thickness of the stacked-NP layer, respectively. (B) Rejection of the

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membranes against different molecular weights of dextran. The diamonds, squares, and triangles

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indicate the 3-, 5-, and 7-layer stacked-NP membranes.

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We compared the performance of the fabricated stacked-NP membranes to that of

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commercial organic and inorganic membranes. Fig. 7 shows the relationship between the water

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permeability of the membranes and rejection against 100-kDa dextran. The upper right region of

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Fig. 7 indicates a high membrane performance, with both a high water permeability and high

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rejection. The stacked-NP membranes fabricated in this study have higher water permeabilities

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compared to the commercial membranes at the same rejection value. In addition, the ethanol-based

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dehydration treatment improves the membrane performance. The thickness of the active separation

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layer of commercial UF membranes is generally several hundred nanometers to several

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micrometers. The stacked layers of NPs on the fabricated membranes are extremely thin, i.e.,

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several tens of nanometers, compared to the active separation layer of commercial membranes.

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The controlled thickness of the active separation layer and uniform pores between the NPs are

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responsible for the superior performance of the stacked-NP membranes. The stacked-NP

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membranes have advantages of high water permeability, precisely-controlled pore size, and high

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chemical and thermal stability as inorganic membranes over commercial membranes, although

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they require multi-step processes for fabricating.

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Fig. 7. Relationship between the water permeability and rejection against 100-kDa dextran for the

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commercial and fabricated membranes. The filled and empty diamonds, circles, and squares

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indicate the fabricated stacked-NP membranes without and with the ethanol-based dehydration

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treatment, commercial organic membranes, and commercial inorganic membranes, respectively.

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3.3. Effects of the ethanol-based dehydration treatment on the membrane structure

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To investigate the effects of the ethanol-based dehydration treatment on the membrane

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structure, we observed the surface structure of the membranes via AFM (Fig. 8). The average

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surface roughness (Ra) of the untreated and ethanol-treated, 3-layer, stacked-NP membranes is

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19.0 and 4.5 nm, respectively. Thus, the surface of the stacked-NP membrane is smoothed by the

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ethanol-based treatment. The surface roughness of the untreated stacked-NP membrane is much

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larger than the average NP radius, while that of the ethanol-treated membrane is nearly equal to

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the average NP radius of 4.1 nm. This indicates that the stacking of NPs on the membrane becomes

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more ordered by the ethanol-based dehydration treatment.

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Fig. 8. AFM images of the surfaces of the (A) untreated and (B) ethanol-treated, 3-layer, stacked-

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NP membranes. The average surface roughness (Ra) of (A) and (B) is 19.0 and 4.5 nm,

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respectively.

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Table 2 shows a summary of the total thickness and pore diameter of the NP layer of the

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fabricated membranes. The pore diameter was calculated from the molecular-weight cut-off for

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dextran, i.e., the molecular weight of dextran at which 90% of the solute was retained by the

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membrane, and the hydrodynamic diameter of dextran (Ddextran), which was calculated with the

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following equation: Ddextran = 0.066 × Mw0.463 [44]. The theoretical values for the NP-layer

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thickness and pore diameter were estimated from the NP diameter when assuming a simple cubic

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packing: Single NP layers are stacked onto each other keeping their two-dimensional structure,

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when sacrificial polymeric layers are removed by the calcination (Fig. S3). Increasing the number

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of NP layers decreases the pore diameter, the values of which are close to the theoretical values

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because of the decreased number of defects. The defects are caused by areas of the support

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membrane that are not covered with NPs. The ethanol-based dehydration treatment clearly

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decreases the total thickness and pore diameter of the NP layer, and the values of the

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aforementioned parameters for the ethanol-treated membranes are close to the theoretical values.

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From these results, the ethanol-based treatment is effective at enhancing the density and uniformity

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of the NP layers. The improved membrane performance shown in Fig. 7 is considered to be due to

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structural changes in the stacked-NP layers that result in a more ordered structure. The solutes and

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solvent were separated by the uniform pores between the NPs. The stacked-NP membranes have

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been reported for UF and NF membranes by controlling the particle diameter [33]. The membrane

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performance could be controlled by altering the diameter of the NPs.

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Table 2. Total thickness and pore diameter of the NP layer of the fabricated membranes. Number of NP layers

2

a

3

b

4

c

3

5

7

Untreated membranes

Total thicknessa [nm]

42.3

71.4

85.8

Pore diameterb [nm]

-

28.7

13.6

Ethanol-treated membranes

Total thicknessa [nm]

36.7

47.6

63.5

Pore diameterb [nm]

28.7

8.9

3.7

Theoretical valuesc

Total thickness [nm]

24.6

41.0

57.4

Pore diameter [nm]

3.4

Evaluated from FE-SEM images. Calculated from the molecular-weight cut-off for dextran.

Estimated for a simple cubic packing.

5 6

When the sacrificial polymers and NPs are stacked on the support membrane by LbL

7

assembly, the sacrificial polymeric layers retain a large amount of water molecules, and thus, have

8

a large free volume, which causes the loose packing of the NPs (Fig. 9(A)). Chiarelli et al. [40]

9

reported that performing a heat treatment on the LbL assembly of oppositely charged

10

polyelectrolytes removes surface water molecules and results in a uniform surface. In this study,

11

the ethanol-based dehydration treatment also removed surface water molecules from the sacrificial

12

polymeric layers (Fig. 9(B)). As a result, the NPs were densely stacked and well-ordered, and the

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membrane performance was improved (Fig. 7). In addition, the ethanol-based dehydration method

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is milder than a heat treatment, and it has minimal effects on the structure of the NPs and sacrificial

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polymers. The formation of uniform, thin, well-packed NP layers onto porous substrates is

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important for fabricating membranes with high permeability and selectivity. The previously

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reported techniques like as vacuum filtration are generally difficult to expand the membrane size,

19

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although they can easily form well-packed structures onto porous substrates [33, 34, 36, 37]. Spin-

2

assisted LbL assembly could also barely expands the membrane size. The ethanol-based

3

dehydration treatment is effective to traditional dip-LbL assembly to obtain more thin and dense

4

stacked-NP layers. LbL assembly under dehydrated conditions would be able to form stacked-NP

5

layers onto various inorganic substrates including flat sheets, hollow fibers, and monolith

6

substrates for the expansion of the membrane size. Furthermore, the technique presented in this

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paper is applicable to the stacking of functional nanomaterials, such as nanotubes and nanosheets

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[21, 23, 45-47], for the membrane fabrication with highly controlled structures.

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Fig. 9. Schematic diagram showing a possible mechanism for the effect of the ethanol-based

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dehydration treatment on the stacking of NPs on porous substrates by spin-assisted LbL assembly.

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The cationic polyelectrolyte PDDA was dehydrated by the ethanol-based treatment.

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4. CONCLUSIONS

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In this study, we developed a fabrication technique of UF membranes that use NPs as the

3

separating elements via spin-assisted LbL assembly and a subsequent dehydration process. Silica

4

NPs were alternately stacked with cationic sacrificial polymers on an anodic aluminum oxide

5

support membrane. The total thickness of the stacked-NP layer increased as the number of NP

6

layers increased, and it was controlled to be less than 100 nm. The rejection performance against

7

dextran was also improved as the number of NP layers increased. The surface roughness of the

8

stacked-NP layer on the support membrane was larger than the NP diameter because of the low

9

packing density. To control the packing density of the NPs, we dehydrated the sacrificial polymer

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layers during the LbL assembly processes with an ethanol-based treatment. While the total

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thickness and water permeability of the stacked-NP layer decreased by the ethanol-based

12

treatment, the rejection performance was greatly increased. AFM measurements showed that the

13

surface of the stacked-NP layer was more uniform and smoother by the ethanol-based treatment,

14

indicating that the stacking of the NPs was more orderly. The membrane performance of the as-

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fabricated membranes was superior to that of commercial membranes because of their extremely

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thin active separation layer and well-ordered stacked-NP structure.

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SUPPLEMENTARY MATERIAL

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The supplementary material includes FE-SEM images of the prepared silica NPs (Fig. S1), the

20

surfaces of support membranes coated with silica NPs (Fig. S2(A)) and silica NPs after a sacrificial

21

PDDA layer was formed (Fig. S2(B)), and schematic images of the theoretical total thickness and

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pore diameter of the stacked-NP membranes when assuming a simple cubic packing (Fig. S3).

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ACKNOWLEDGMENTS

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This work was financially supported by a research grant from the Organization for Membrane and

3

Film Technology, Japan. We thank Mr. Yusuke Nakasuji for his help of XPS measurements and

4

Mr. Shinji Kawada, Tsuyoshi Yamashita, and Fumiya Sako for their encouragement.

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