Subscriber access provided by University of Sunderland
Interfaces: Adsorption, Reactions, Films, Forces, Measurement Techniques, Charge Transfer, Electrochemistry, Electrocatalysis, Energy Production and Storage
Free-Standing Metal Films Prepared via Electroless Plating at Liquid-Liquid Interfaces Toshihiko Tsuneyoshi, Yu Yohaze, Takaichi Watanabe, and Tsutomu Ono Langmuir, Just Accepted Manuscript • DOI: 10.1021/acs.langmuir.8b02822 • Publication Date (Web): 16 Oct 2018 Downloaded from http://pubs.acs.org on October 17, 2018
Just Accepted “Just Accepted” manuscripts have been peer-reviewed and accepted for publication. They are posted online prior to technical editing, formatting for publication and author proofing. The American Chemical Society provides “Just Accepted” as a service to the research community to expedite the dissemination of scientific material as soon as possible after acceptance. “Just Accepted” manuscripts appear in full in PDF format accompanied by an HTML abstract. “Just Accepted” manuscripts have been fully peer reviewed, but should not be considered the official version of record. They are citable by the Digital Object Identifier (DOI®). “Just Accepted” is an optional service offered to authors. Therefore, the “Just Accepted” Web site may not include all articles that will be published in the journal. After a manuscript is technically edited and formatted, it will be removed from the “Just Accepted” Web site and published as an ASAP article. Note that technical editing may introduce minor changes to the manuscript text and/or graphics which could affect content, and all legal disclaimers and ethical guidelines that apply to the journal pertain. ACS cannot be held responsible for errors or consequences arising from the use of information contained in these “Just Accepted” manuscripts.
is published by the American Chemical Society. 1155 Sixteenth Street N.W., Washington, DC 20036 Published by American Chemical Society. Copyright © American Chemical Society. However, no copyright claim is made to original U.S. Government works, or works produced by employees of any Commonwealth realm Crown government in the course of their duties.
Page 1 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
Free-Standing Metal Films Prepared via Electroless Plating at Liquid-Liquid Interfaces Toshihiko Tsuneyoshi, Yu Yohaze, Takaichi Watanabe, Tsutomu Ono* Department of Applied Chemistry, Graduate School of Natural Science and Technology, Okayama University, 3-1-1, Tsushima-Naka, Kita-Ku, Okayama 700-8530, Japan *E-mail:
[email protected] ACS Paragon Plus Environment
1
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 2 of 54
GRAPHICAL ABSTRACT
ACS Paragon Plus Environment
2
Page 3 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
ABSTRACT
We report a simple preparation of free-standing metal films via electroless plating (ELP)
at the liquid-liquid (L-L) interface between an aqueous electroless plating solution and an
organic solvent. The use of ELP does not require any external energy in the form of heating
and stirring. We find that the affinity of the organic solvent for the palladium nanoparticles
(PdNPs) as catalysts and the vertical position of the organic and aqueous phases in the
biphasic system are important considerations for synthesizing a robust copper film.
Specifically, 1,2-dichloroethane which has an appropriate affinity for PdNPs and higher
density than water was found to be a good candidate for use as the organic phase in this
system. However, a poor-quality copper film was obtained in the system with 1-hexanol
as the organic phase. We also controlled the micro-scale surface structure of the copper
films by using different concentrations of the injected PdNP dispersion. A high density of
ACS Paragon Plus Environment
3
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 4 of 54
PdNPs caused smaller regions of metal growth, which contributed to the formation of
smoother metal films. Moreover, under the optimal synthesis condition we confirmed the
electrical conductivity of the obtained copper film to be 1.16107 m. We believe that
this metal film preparation represents a promising way to produce a range of metal film
structures through the use of flexible L-L interfaces as templates.
ACS Paragon Plus Environment
4
Page 5 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
INTRODUCTION
Electroless plating (ELP) is a wet chemical process, which involves deposition of a metal
film onto a substrate surface through in-situ chemical reduction of metal ions [1, 2]. ELP
is widely used to prepare various surface-modified materials such as composite fibers [3-
5] and flexible electronics [6, 7], which have hybrid-functionalities owing to the
combination of substrate materials (e.g., polymers and ceramics) and deposited metals.
In addition, ELP allows colloidal materials to be coated with metal films, which is difficult
to achieve by electroplating methods that require a connection to an external electronic
source [2]. Indeed, many metal-composite colloidal materials, including core-shell
particles and microcapsules synthesized by ELP, have been studied for decades owing to
their high performance as catalysts and conductive materials [8-19]. We have recently
reported on the synthesis of metal-coated microcapsules with tunable magnetic
properties, which contained a liquid core and metallic shell [18]. The microcapsules
ACS Paragon Plus Environment
5
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 6 of 54
showed a magnetic response induced by the ELP. This response enabled the phase change
materials to act as a heat-pump system in an external magnetic field.
In ELP processes, in-situ metal precipitation is initiated by activation of reductants
by a dehydrogenation reaction, which is catalyzed by noble metal like palladium at the
substrates surface [1, 2]. Catalytic nanoparticles are necessary for ELP and the conditions
of the catalytic NPs adsorption onto the substrate are important. The deposition of
catalytic NPs on substrate surfaces should be sufficiently dense and durable to form a
continuous metal film on the surface. The NPs strongly adsorb to the solid surface by
chemical or physical bonding to catalytically promote the formation of a dense and
durable layer by ELP. However, unstable substrates, such as L-L interfaces that cannot
support catalytic have not been considered as candidates for substrates of metal film
formation by ELP.
ACS Paragon Plus Environment
6
Page 7 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
Particle adsorption at interfaces has been studied for the last century, because
particles adsorbed at interfaces represent a good platform for novel materials synthesis.
The droplets stabilized by adsorbed particles, known as Pickering emulsions, were discovered at the beginning of the 20th century by Pickering and Ramsden [20, 21].
Approximately 100 years later, Dinsmore et al. synthesized microcapsules consisting of
adsorbed particles denoted as colloidosomes, which derived from Pickering emulsions
[22-26]. Colloidosomes are functional microcapsules with size-selective permeability
owing to the spaces between particles packed at the interface. In these materials,
micrometer-sized particles are used owing to their high adsorption stability at interface
[27-29]. NPs adsorption at interfaces has also been studied recently, because of the high
potential of NPs in electronic, optical, and magnetic applications [30-40]. Mohwald et al.
reported that surface-functionalized gold nanoparticles strongly adsorb at L-L interfaces
and the resulting films have a metallic luster [36, 37]. Reincke et al. also presented
ACS Paragon Plus Environment
7
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 8 of 54
spontaneous assembly and structural control of NPs at water-oil interface by changing
the electrical charge of the particles, which could be applied to the fabrication of 2D and
3D materials for optoelectrical or magnetic applications [38]. In addition, metal
nanoparticles films prepared via Langmuir–Blodgett films are good substrates for Raman-
imaging [39, 40].
The technique of in-situ metal deposition at L-L interface has been studied for long
time since Faraday reported reduction of metal at the water-carbon disulfide interface
[41-45]. Recently, Nishi et al. reported synthesis of Au and Pt nanofiber at ionic liquid-
water interface [42-44]. Although these studies have presented smart way to prepare
various shape of metal at L-L interface, few reports are available on the fabrication of
continuous and robust metal film. Several groups have reported on the synthesis of
continuous metal films at soft fluid interfaces by interfacial crystallization of metals, cross-
linking of NPs and liquid phase deposition (LPD) [46-51]. Rao et al. reported the in-situ
ACS Paragon Plus Environment
8
Page 9 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
crystallization of metals at organic solvent-water interfaces, in which reactants in both
phases contacted and reacted at the interface [46-48]. The obtained metal films were
ultrathin and lacked free-standing character; however, high metal-like conductivities were
achieved by the formation of pure metal films. Russell et al. successfully synthesized free-
standing films containing gold NPs, which were prepared via cross-linking of
nanoparticles assembled at air-liquid interfaces [49]. However, these metal films, showed
weak metallic properties owing to the high content of polymer in the films. The LPD
approach reported by Mizuhata et al. addressed the trade-off between durability and
purity in metal films prepared at L-L interfaces but their approach was limited to forming
metal oxide films, such as TiO2 and SnO2 [51]. Therefore, the formation of free-standing
films of pure-metals at an L-L interface has yet to be achieved, without several reports
using the electrode connected to fluid interface that needs complex equipment [52].
ACS Paragon Plus Environment
9
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 10 of 54
Here we describe the formation of free-standing metal films by ELP at catalytic
nanoparticles adsorbed to a L-L interface. The L-L interface in a biphasic system consisted
of electroless plating solution and an appropriate organic solvent, which enabled the
synthesis of continuous and robust metal films. They were formulated by the continuous
reduction of metal precursors provided from plating solution. This is quite different from
the previous challenges for metal film formation using interfacial reaction requiring
reactants feeding from both phases [41-45]. We report on the appearance, surface
structure, and characteristics of metal-films fabricated under different synthesis
conditions, organic solvents, and catalytic NP concentrations. This report provides insight
into the mechanism of ELP at L-L interfaces and highlights the potential applications of
these novel metal films.
ACS Paragon Plus Environment
10
Page 11 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
EXPERIMENTAL SECTION
Materials. Sodium tetrachloropalladate (II) (Na2PdCl4), 1,2-dichloroethane (DCE), 1-
hexanol, copper (II) sulfate, formaldehyde aqueous solution (37wt%), potassium sodium
(+)- tartrate tetrahydrate and sodium hydroxide solution (5 N) were obtained from Wako
Pure Chemicals. A triblock copolymer, poly(ethyleneglycol)-block-poly(propyleneglycol)-
block-poly(ethyleneglycol) with an average molecular weight of 5800 g/mol (Pluronic P-
123) was obtained from Sigma-Aldrich. All reagents were used as received. Elix water,
obtained from a Milli-Q system (Millipore), was used in all experiments. Sample bottles
used for film synthesis were hydrophobized with trimethoxy (octadecyl) silane (Sigma-
Aldrich) to prevent undesirable adsorption of nanoparticles and precipitated metals to the
glass wall. Sample bottles were dried at 110°C for 1 day after immersion in 1 wt%
trimethoxy (octadecyl) silane in toluene solution for 4 h. These sample bottles were used
after washing with ethanol and hexane (Wako Pure Chemicals).
ACS Paragon Plus Environment
11
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 12 of 54
Synthesis of PdNPs. Pluronic stabilized palladium nanoparticles (PdNPs) were
synthesized according to a procedure reported by Piao et al. [53]. The PdNPs were
obtained in a 1-day reaction starting with rapid injection of 1 mL of a sodium
tetrachloropalladate aqueous solution (1 M) into a vigorously stirred 100 mL Pluronic P-
123 aqueous solution (2 wt%) at room temperature. We changed the particle
concentration of this dispersion by controlling the molar ratio of Na2PdCl4 and Pluronic.
The concentrations of the injected Na2PdCl4 solutions (1 mL) were 3.4510−2, 6.9010−2,
0.345, 1.73, and 3.45 M, which gave a range of molar ratios against Pluronic (0.345 mol,
[Na2PdCl4]: [Pluronic]) in the reaction system, namely, 1:1000, 1:50, 1:100, 1:20, and 1:10,
respectively. The obtained PdNP dispersions were used as prepared without any
purification.
Observation of morphologies and adsorption behaviors of PdNPs. The size and
morphology of the prepared PdNPs were observed with a transmission electron
ACS Paragon Plus Environment
12
Page 13 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
microscope (TEM) (JEM-2100F; JEOL). We observed the assembly behavior of PdNPs at
DCE-water and 1-hexanol-water interfaces according to the method presented by
Kutuzov et al. [54] to reproduce and confirm the behavior of PdNPs at the organic solvent–
plating solution interfaces under actual experimental conditions without a subsequent
plating reaction (Supporting Information Scheme S1). A TEM grid supporting organic
solvent was immersed gently into the dilute PdNP aqueous dispersion for 1 min. The TEM
grid was carefully pulled out and then dried overnight. The TEM grids used for all the
samples in these measurements were copper grids with a collodion membrane (200 mesh,
Nisshin EM).
Preparation of metal films at L-L interface. The reaction field, liquid-liquid (L-L)
interface was composed of organic solvents (DCE, 1-hexanol; oil phase) and electroless
plating solutions (aqueous phase) in a sample bottle. The composition of the copper
electroless plating solution was as follows: 7.5 g/L of copper (II) sulfate, 22 mL/ L of
ACS Paragon Plus Environment
13
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 14 of 54
formaldehyde aqueous solution, 85 g/L of potassium sodium (+)- tartrate tetrahydrate,
(the pH of the plating solution was adjusted to be 12.5 by addition of sodium hydroxide
solution). An organic solvent (DCE or 1-hexanol) contacted the plating solution (2 mL
each) in a hydrophobized sample bottle to form a biphasic system. The PdNP aqueous
dispersion (20 L) was then injected gently onto the L-L interface with the use of a
micropipette. After injection, the plating reaction immediately started at the L-L interface
because of the high catalytic activity of PdNPs for the copper electroless plating reaction
(Supporting Information Scheme S2). The obtained metal films were collected with a pair
of tweezers after 60 min of reaction. We studied the effects of organic solvents and
concentration of the PdNP dispersion on the metal film formation and its characteristics.
Characterization of the obtained PdNP dispersions. The particle concentration of
obtained PdNP dispersion was calculated based on diameters measured from TEM images
and the weight of deposited nanoparticles after ultracentrifugation. The obtained PdNPs
ACS Paragon Plus Environment
14
Page 15 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
were centrifuged (20°C, 60 min, 30000 rpm; 72,260 G) three times in an ultracentrifugation
machine (HIMAC CP100MX with angle rotor P100AT2; Hitachi Koki). The deposited
nanoparticles were dried under reduced pressure and weighed with a balance. The particle
concentration was calculated by the following equations:
𝑊𝑑𝑝
𝑁𝑝 = 𝑊𝑝 × 𝑣,
6𝑊𝑑𝑝
= 𝜋𝑑
𝑎𝑣
3
,
𝜌𝑣
where 𝑁𝑝 is the particle concentration (particles/mL), 𝑊𝑑𝑝 is the total weight of
deposited nanoparticles after centrifugation (g), 𝑊𝑝 is the weight of one palladium
nanoparticle estimated from the average diameter (𝑑𝑎𝑣, nm) of nanoparticles measured from TEM images and the density of palladium (12.0 g/cm3 at r.t.), and 𝑣 is the volume of
the dispersion that originally contained these nanoparticles (mL).
ACS Paragon Plus Environment
15
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 16 of 54
Characterization of the prepared metal films. The obtained metal films were
characterized in terms of their morphology, material composition, surface roughness,
crystalline character and electrical conductivity as follows.
The morphology of the obtained metal films was examined with a field-emission
scanning electron microscope (FE-SEM) (S4700; Hitachi) operating at an applied voltage
of 1.0 kV.
The elemental surface composition of the prepared metal films was determined by
X-ray photoelectron spectroscopy (XPS). XPS measurements were performed with an S-
Probe ESCA apparatus (Fusion Instruments) equipped with a monochromated 𝐴𝑙𝐾𝛼 X-ray
source, after Ar-ion sputtering of samples dried for 10 s.
The surface roughness of the metal films was studied with an atomic force microscope
(AFM, SPA-400; Seiko Instruments Inc.). The AFM measurements were conducted in contact
ACS Paragon Plus Environment
16
Page 17 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
mode with a micro-cantilever (SI-DF3; Seiko Instruments Inc.) over a 5 m 5 m area on the
metal films. The height change of a line scan of the sample surface was also examined in contact
mode and the average roughness was calculated according to the equation below:
1
𝑛
𝑅𝑎 = 𝑛∑1|𝑍(𝑖) ― 𝑍𝑐|,
where 𝑅𝑎 is the average roughness (nm), 𝑛 is the number of measured points, 𝑍(𝑖)
is the height, and 𝑍𝑐 is average height on the measured line (nm).
The crystallinity of the obtained metal films was examined by X-ray diffraction
(XRD) with the use of a RINT-2500 diffractometer (Rigaku). Measurements were
conducted at an applied voltage of 40 kV and a current of 200 mA under CuK radiation.
A reflection-free Si sample holder was used for all XRD studies. The size of the copper
crystals was estimated from the XRD peaks corresponding to Cu (111) crystal with the
Scherrer equation [55]:
ACS Paragon Plus Environment
17
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 18 of 54
𝐾𝜆
𝐷 = 𝐵cos 𝜃,
where 𝐷 is the single crystal diameter, 𝜆 is the wavelength of CuK radiation (1.54056 Å),
𝐵 is the full width at half maximum (FWHM) of an XRD peak, and 𝐾 is the Scherrer constant
(0.9).
The electric conductivities of the obtained metal films were studied by a four-terminal
method with an electrical resistance meter (RM3545; HIOKI). The measurements were conducted
for the dried metal films at room temperature.
ACS Paragon Plus Environment
18
Page 19 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
RESULTS AND DISCUSSION
An aqueous dispersion of PdNPs was obtained (Supporting Information Figure S1, S2 and
Table S1) and used as the initiator for metal film preparation. The addition of the PdNP
dispersion to the organic-water interface of the biphasic system is shown in Figure 1(a)
and (d). After injection of the PdNP dispersion, the nanoparticles stabilized by amphiphilic
block copolymer adsorbed at the L-L interface to reduce the surface energy of the system
(Supporting Information Table S2) [27]. As shown in Figure 1(b) and (e), there was a
difference in the assembly behavior of PdNPs on the interfaces between the DCE-water
and 1-hexanol-water. At the DCE-water interface, PdNPs slightly aggregated whereas for
at the 1-hexanol-water interface PdNPs were well-dispersed. We attribute this difference
to the affinities of poly(ethylene oxide) (PEO) chains, which created hydrophilic corona
that surrounded the PdNPs [56]. The PdNPs surrounded by the PEO chains achieved a
uniform dispersion at the interface between the water and 1-hexanol, which dissolved and
ACS Paragon Plus Environment
19
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 20 of 54
dispersed the PEO chains more easily than did DCE. We explain these difference
solubilities in terms of Hansen solubility parameters of the components (Supporting
Information, Table S3) [57]. Hence, the Pluronic stabilized PdNPs formed aggregates at
the DCE-water interface but were finely dispersed in 1-hexanol. This manner of PdNP
assembly at the L-L interface might influence the characteristics of the resulting metal
films, as will be discussed later. After the plating reaction proceeded for 60 min,
continuous films with a metallic luster were formed at L-L interfaces in both biphasic
systems with DCE and 1-hexanol as the organic phase [Figure 1(c) and (f)]. The metal film
obtained at the DCE-water interface showed both mechanical robustness and some
brittleness owing to its metallic nature. This metal film could be picked up with a pair of
tweezers, indicating successful preparation of a free-standing metal film at the L-L
interface. In contrast, metal films obtained at the 1-hexanol-water interface lacked
mechanical toughness owing to the formation of a thinner metal film at the interface. We
ACS Paragon Plus Environment
20
Page 21 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
attribute this difference to the condition of PdNPs at the interface. The highly disperse
nature of PdNPs at the 1-hexanol phase was disadvantageous for metal film formation
because of the low particle density caused by steric repulsion between each nanoparticle.
Conversely, the PdNPs in the plating solution-DCE interface were densely aggregated at
the interface such that a thicker metal film formed with many points capable of initiating
the catalytic reaction.
ACS Paragon Plus Environment
21
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 22 of 54
Figure 1. Preparation of metal films at planar L-L interfaces in biphasic systems. PdNPs
were injected into biphasic systems with (a) DCE-water and (d) 1-hexanol-water interfaces.
The aqueous phase contained Cu electroless plating solution. TEM images of the assembly
behavior of the PdNPs at (b) DCE-water and (e) 1-hexanol-water interfaces. The assembly
behavior of PdNPs at DCE-water and 1-hexanol-water interfaces was observed to
reproduce and confirm the behavior of PdNPs at the organic solvent–plating solution
ACS Paragon Plus Environment
22
Page 23 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
interfaces under actual experimental conditions without a subsequent plating reaction.
Photographs of continuous metal films formed at (c) DCE-water and (f) 1-hexanol-water
interfaces after a 60-min electroless plating reaction.
ACS Paragon Plus Environment
23
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 24 of 54
The morphologies of the obtained metal films in each system were observed by
FE-SEM (Figure 2). We found distinct differences in the surface structure of metal films
prepared with DCE and 1-hexanol as the organic phase [Figure 2(a) and (d)]. The metal
films formed at the DCE-water interface had a rough surface with some holes and
adsorbed particles, which we assumed were caused by the spherical-shaped growth of
the deposited continuous metal film. Conversely, we observed dendritic structures on the
surface of the metal films obtained at the 1-hexanol-water interface. These differences in
the surface structure directly affected the appearance of metal films; the metal films had
a relatively smooth surface when prepared with DCE and exhibited a metallic luster;
however, films prepared with 1-hexanol had a rough surface and showed no luster. The
films also had different thicknesses. The metal film formed at the DCE-water interface
grew thicker than that formed at the 1-hexanol-water interface (Film thickness: 40827
nm vs. 374 nm) [Figure 2(b) and (e)]. From these results, we proposed two mechanisms
ACS Paragon Plus Environment
24
Page 25 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
of metal film formation [Figure 2(c) and (f)]. In the system with DCE-water, the metal film
formation started with in-situ metal precipitation, followed by growth of metallic copper
from the desorbed catalytic PdNPs [Figure 2c (i)]. In addition, reduced and copper metal
in the bulk solution then deposited on the L-L interface. This deposition strongly
contributed to the formation of a metal film through a mechanism analogous to the phase
separation of melamine-formaldehyde resin used for microencapsulation [58] [Figure 2(c)
(ii) and (iii)]. The deposited metal grew continuously to form a thick metal membrane by
in-situ metal growth [Figure 2(c) (iv)]. Conversely, for the film formed in the system with
1-hexanol, precipitated metal settled at the bottom of the sample bottle, which did not
deposit onto the L-L interface [Figure 2(f) (i’)-(iii)]. The in-situ metal growth without any
other deposition resulted in poor quality films with dendritic metal precipitation. We
found that in-situ metal precipitation at the L-L interface with 1-hexanol proceeded by
dendritic growth (Supporting Information, Figure S3). In general, dendritic growth of
ACS Paragon Plus Environment
25
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 26 of 54
crystals occurs under diffusion-limited reaction conditions, when a highly-active agent is
present in a relatively dilute solution [60]. The large number of PdNPs might have caused
an absence of copper ions around the L-L interface and induced dendritic growth under
the diffusion-limited conditions.
ACS Paragon Plus Environment
26
Page 27 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
Figure 2. SEM images of surface structure (a) and (d) and cross-section (b) and (e), and
schematic illustration of metal film formation (c) and (f) in systems with DCE and 1-hexanol
as the organic phase, respectively. Insert photographs in (a) and (d) show the appearance
of metal films with scale bars showing 1 cm.
ACS Paragon Plus Environment
27
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 28 of 54
Metal films synthesized at the oil-water interface had different surface structures
on both sides. Photographs of the metal films from each side prepared at the DCE-water
interface are shown in Figure 3(a). Although both sides had a macroscopically similar
appearance, XPS spectra from each side of the metal film clearly showed the presence of
palladium only on the side adjacent to the organic phase [Figure 3(b)]. This result supports
the mechanism we proposed above; the metal films formed by adsorption of PdNPs at
the DCE-water interface and the following metal growth was directing into the aqueous
phase, which contained the metal and reductant source. FE-SEM images of the surface
structures of both sides of the film also indicated this mechanism of film formation [Figure
3(c) and (d)]. The film surface adjacent to the aqueous phase had a relatively rough surface
due to deposition of precipitated particles from bulk solution. Conversely, the organic
phase of the metal film had a smooth and compressed surface, which indicates that metal
growth toward the organic phase was prevented.
ACS Paragon Plus Environment
28
Page 29 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
Figure 3. A metal film formed at L-L interface with Cu plating solution and DCE; (a)
appearance of the obtained metal film and both sides of the collected film. (b) XPS spectra
of both sides of the obtained film from SEM images of these surfaces [(c) plating solution
side, (d) DCE side]. In the XPS spectrum of the surface contacted to the DCE, peaks at 335
and 340 eV were detected corresponding to Pd 3d.
ACS Paragon Plus Environment
29
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 30 of 54
ACS Paragon Plus Environment
30
Page 31 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
The surface roughness of the metal films was affected by the particle concentration
of the injected PdNP dispersions. Table 1 summarizes the synthesis conditions of the
PdNP dispersion and the characteristics of the PdNP dispersion in terms of particle size
and particle concentration. There were no notable differences in the size of the PdNPs
among these conditions (Supporting Information, Figure S4). However, particle
concentrations of each PdNP dispersion (𝑁𝑝) increased as the concentration of metal
precursor in Na2PdCl4 solution was increased from 6.51015 to 2.11017 particles/mL. In
this nanoparticle synthesis, Pluronic acted not only as a stabilizer of the obtained PdNPs
but also as a reducing agent of the palladium precursors [56]. Therefore, the palladium
precursors were immediately reduced for nucleation in Pluronic-rich conditions and few
precursor ions were used for the following particles growth. Pluronic-rich conditions also
ensured the stability of the PdNPs and contributed to the formation of uniform
nanoparticles. Notably, when the molar ratio of [Na2PdCl4]: [Pluronic] was 1:10, we could
ACS Paragon Plus Environment
31
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 32 of 54
not measure the particle size because the obtained particles were severely aggregated
owing to the lack of Pluronic to reduce and stabilize all the injected palladium.
We prepared metal films at the interface of the plating solution and DCE using
these PdNP dispersions. The surface structure of the obtained metal films for each
dispersion was studied by SEM and AFM. The surface structures formed from the use of
different particle densities at the interface suggested that a higher particle density led to
smaller metal precipitates [Figure 4(a)-(c)]. For the metal precipitates formed at a high
PdNP density the metal precursors were mainly consumed for nucleation, and formed
many small metal precipitate domains in the films. At the lowest particle density (i.e.,
6.51015 particles/mL), a metal film was not formed because an insufficient amount of
PdNPs was supplied to L-L interface. AFM images of the film surfaces also showed that
the surface roughness decreased as the PdNP concentration in the dispersions increased
[Figure 4(d)-(f)]. The change in height of the white line in each AFM image was measured
ACS Paragon Plus Environment
32
Page 33 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
and the results are plotted in Figure 4(g). We confirmed that the surface roughness
decreased as the PdNP concentration at the interface increased. The average roughness
(𝑅𝑎) calculated from these height changes also showed slight decrease; the 𝑅𝑎 values were
26, 22, and 20 nm when the concentrations of PdNPs were 1.61016, 5.31016, and 2.11017
particles/mL, respectively [Figure 4(h)].
ACS Paragon Plus Environment
33
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 34 of 54
Table 1. Diameter, stability, and calculated particle concentration 𝑁𝑝 of PdNP aqueous
dispersion obtained under the same synthesis conditions, with [Na2PdCl4]: [Pluronic]
molar ratios of 1: 1000, 1: 500, 1: 100, 1: 20, and 1: 10.
Entr y
1
2
3
4
5
Na2PdCl4 (A) (mol)
Pluronic (B) (mol)
3.45×104
6.90×104
3.45×103
1.73×102
3.45×102
0.345
Molar ratio A: B
Diamete r (nm)
Particle Concentration 𝑁𝑝 (particles/mL)
1: 1000
4.4
6.5×1015
1: 500
3.7
1.6×1016
1: 100
4.1
5.3×1016
1: 20
4.2
2.1×1017
1: 10
N/D
N/D
ACS Paragon Plus Environment
34
Page 35 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
ACS Paragon Plus Environment
35
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 36 of 54
Figure 4. SEM and AFM images of the surface of metal films exposed to the organic phase,
which were obtained with PdNP dispersions having different particle concentrations 𝑁𝑝:
(a, d) 1.61016, (b, e) 5.31016, and (c, f) 2.11017 particles/mL. (g) Line profiles of the height
of the surface scanned along the white lines in the AFM images [purple, blue, and black
lines corresponds to (d), (e) and (f)]. Scale bars show 1 m. Average roughness, 𝑅𝑎 of the
metal films calculated from the line profiles (g) is shown in (h).
ACS Paragon Plus Environment
36
Page 37 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
We conducted an XRD study of the metal films prepared with different PdNP
dispersion particle concentrations. Figure 5 shows peaks at 2 43.3 corresponding to
the Cu (111) crystal in metal films, which had similar peak shapes. We calculated the
crystallite diameter in the metal films from the FWHM of the Cu (111) XRD peaks using
the Scherrer equation (Table 2, Supporting Information, Figure S4). The diameters of Cu
(111) crystals decreased from 35.9 to 30.0 nm as the PdNP concentration was increased
from 1.61016 to 5.31016 particles/mL. The size change of the crystals corresponded with
the roughness change of the metal films described above. A higher density of PdNPs lead
to smaller metal crystallites. In addition, we measured the electrical conductivities of these
metal films by the four-terminal method with an electrical resistance meter (Table 2). The
electrical conductivities of metal films prepared with 𝑁𝑝: 5.31016 and 2.11017
particles/mL (Entries 3 and 4) were 1.16107 and 6.62107 m respectively, whereas the
electrical conductivity for the metal film prepared with 𝑁𝑝: 1.61016 (Entry 2) was too brittle
ACS Paragon Plus Environment
37
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 38 of 54
to be measured under the pressure of the measurement probes. We attribute the
brittleness of the metal film to the low content of Pluronic polymers, which stabilized the
PdNPs. The Pluronic content of the metal films might provide mechanical durability to the
film owing to the flexible nature of the polymers. These values for the electric
conductivities are comparable to those of composite copper membranes (electrical
conductivity of pure copper: 1.68108 m [60]), which indicates successful preparation
of electrically conductive metal films by our process. In this preparation, the electrical
conductivities increased as the concentration of catalytic PdNPs was increased. We
attribute this trend to the small size of the copper crystallites and the amount of
composite materials included in the metal films. The metal film consisted of a large
number of small Cu (111) crystals, which were produced from numerous PdNPs, and had
many crystal interfaces. The many interfaces prevented transfer of electrons and
ACS Paragon Plus Environment
38
Page 39 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
contributed to the high electrical conductivities. Moreover, the PdNPs and Pluronic
polymers included in the metal films might decrease the electric conductivity.
Figure 5. XRD patterns for obtained metal films, which were obtained with different
particle concentrations for the PdNP dispersion 𝑁𝑝: (a) 1.61016, (b) 5.31016, and (c)
ACS Paragon Plus Environment
39
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 40 of 54
2.11017 particles/mL. Peaks corresponding to the Cu (111) crystals were detected at 2
43.3 with a Cu-K radiation source.
ACS Paragon Plus Environment
40
Page 41 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
Table 2. Calculated crystal diameters of Cu (111) crystals and electric conductivities of the
metal films, which were obtained with different PdNP concentrations 𝑁𝑝: (a) 1.61016, (b)
5.31016, and (c) 2.11017 particles/mL. The crystal diameters were calculated with the
Scherrer equation based on the XRD peaks detected at 2 43.3 with a Cu-K radiation
source. Entr y
Particle Concentration 𝑁𝑝 (particles/mL)
Crystal Diameter (nm)
Electric Conductivity (m)
2
1.6×1016
35.9
N/D
3
5.3×1016
35.6
1.16107
4
2.1×1017
30.0
6.62107
ACS Paragon Plus Environment
41
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 42 of 54
CONCLUSIONS
We successfully prepared free-standing metal film via electroless plating at L-L interfaces
composed of an organic solvent and aqueous plating solution. The affinity of the organic
solvent for the catalytic PdNPs and the vertical position of the organic phase and aqueous
phase in the biphasic system were important factors affecting the synthesis of robust
metal films. Slightly aggregated PdNPs formed thin metal films with a large number of
total adsorbed nanoparticles in the DCE-water system. Conversely, well-dispersed PdNPs
were poorly adsorbed at the L-L interface, owing to the high affinity of the solvent (1-
hexanol) for the PdNPs. This system led to the formation of thin metal films without free-
standing ability. For film formation in the biphasic system, it is important to use higher
density organic solvent like DCE than aqueous plating solution, which promotes
deposition from the bulk solution induced by gravity. Therefore, organic solvents with an
appropriate affinity for the catalytic nanoparticles and a density higher than water are
ACS Paragon Plus Environment
42
Page 43 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
good candidates for the organic phase in this system. We could also control the surface
morphology of the metal films by changing the concentration of the injected catalytic
nanoparticle dispersion. A high density of PdNPs induced growth of small metal
crystallites, which contributed to the formation of smooth metal films. Moreover, we
confirmed the electrical conductivities of metal films obtained under the optimal synthesis
condition to be 1.16107 m. Conductivity also varied with the PdNP density.
This simple preparation of metal films is an important expansion of the usage of soft L-L
interfaces as templates. Various L-L interfaces might be used as templates for such metal films.
For example, metal microcapsules can be prepared through encapsulation of oil droplets with a
metallic shell by this technique. This metal film preparation might also enable mass production of
commercial metal films with low-energy costs and no need for external thermal or mechanical
energy.
ACS Paragon Plus Environment
43
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 44 of 54
ASSOCIATED CONTENT
Supporting Information.
The Supporting Information is available free of charge on the @@@.
ACS Paragon Plus Environment
44
Page 45 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
AUTHOR INFORMATION
Corresponding Author
*E-mail:
[email protected] Tel: +81-86-251-8072, Fax: +81-86-251-8072.
Author Contributions
T.T., Y.Y., T.W. and T.O. designed the experiments. Y.Y. performed the experiments and
analyzed the data. T.T., Y.Y., T.W., and T.O. interpreted the results and wrote the
manuscript. T.T. and T.O. designed the research.
Notes
The authors declare no competing financial interest.
ACS Paragon Plus Environment
45
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 46 of 54
ACKNOWLEDGMENT
We thank S. Matsumoto for assistance conducting XPS measurements and useful discussions, M.
Yoneda for assistance conducting TEM measurements, and M. Nakanishi for assistance with XRD
measurements and other useful advice. This work was supported by the JSPS KAKENHI (Grant
number: 16K1445908, 26289291).
ACS Paragon Plus Environment
46
Page 47 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
REFERENCES
[1] Ohno, I., Electrochemistry of electroless plating. Mater. Sci. Eng., A 1991, 146 (1-2), 3349. [2] Schlesinger, M.; Paunovic, M.; Snyder, D. D.; Dini, W. J. et al., Modern Electroplating, Fifth Edition, Schlesinger, M.; Paunovic, M., Ed.; John Wiley & Sons, Inc., 2011. [3] Jiang, S. Q.; Kan, C. W.; Yuen, C. W. M.; Wong, W. K., Electroless nickel plating of polyester fiber. J. Appl. Polym. Sci. 2008, 108 (4), 2630-2637. [4] Liu, X.; Chang, H.; Li, Y.; Huck, W. T.; Zheng, Z., Polyelectrolyte-bridged metal/cotton hierarchical structures for highly durable conductive yarns. ACS. Appl. Mater. Interfaces 2010, 2 (2), 529-35. [5] Xu, C. J.; Zhou, R. H.; Chen, H. Y.; Hou, X.; Liu, G. L.; Liu, Y. Q., Silver-coated glass fibers prepared by a simple electroless plating technique. J. Mater. Sci. - Mater. Electron. 2014, 25 (10), 4638-4642. [6] Cheng, K.; Yang, M. H.; Chiu, W. W. W.; Huang, C. Y.; Chang, J.; Ying, T. F.; Yang, Y., Inkjet printing, self-assembled polyelectrolytes, and electroless plating: Low cost fabrication of circuits on a flexible substrate at room temperature. Macromol. Rapid Commun. 2005, 26 (4), 247-264. [7] Hao, Z. X.; Chen, H. W.; Ma, D., Preparation of Micro Gold Devices on Poly(dimethylsiloxane) Chips with Region-Selective Electroless Plating. Anal. Chem. 2009, 81 (20), 8649-8653.
ACS Paragon Plus Environment
47
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 48 of 54
[8] Jang, S. G.; Kim, S.-H.; Lee, S. Y.; Jeong, W. C.; Yang, S.-M., Facile synthesis of core-shell and Janus particles via 2-D dendritic growth of gold film. J. Colloid Interface Sci. 2010, 350 (2), 387-395. [9] Sanles-Sobrido, M.; Bañobre-López, M.; Salgueiriño, V.; Correa-Duarte, M. A.; Rodríguez-González, B.; Rivas, J.; Liz-Marzán, L. M., Tailoring the magnetic properties of nickel nanoshells through controlled chemical growth. J. Mater. Chem. 2010, 20 (35), 7360. [10] Shibata, N.; Nagao, D.; Ishii, H.; Konno, M., Preparation of various Janus composite particles with two components differently combined. Colloid. Polym. Sci. 2013, 291 (1), 137-142. [11] Wang, K.; Zhang, X. L.; Niu, C. Y.; Wang, Y. Q., Template-Activated Strategy toward One-Step Coating Silica Colloidal Microspheres with Sliver. ACS Appl. Mater. Interfaces 2014, 6 (2), 1272-1278. [12] Patchan, M. W.; Baird, L. M.; Rhim, Y.-R.; LaBarre, E. D.; Maisano, A. J.; Deacon, R. M.; Xia, Z.; Benkoski, J. J., Liquid-Filled Metal Microcapsules. ACS Appl. Mater. Interfaces 2012, 4 (5), 2406-2412. [13] Hitchcock, J. P.; Tasker, A. L.; Baxter, E. A.; Biggs, S.; Cayre, O. J., Long-Term Retention of Small, Volatile Molecular Species within Metallic Microcapsules. ACS Appl. Mater. Interfaces 2015, 7 (27), 14808-14815. [14] Tasker, A. L.; Hitchcock, J.; Baxter, E. A.; Cayre, O. J.; Biggs, S., Understanding the Mechanisms of Gold Shell Growth onto Polymer Microcapsules to Control Shell Thickness. Chem. Asian. J. 2017, 12 (13), 1641-1648.
ACS Paragon Plus Environment
48
Page 49 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
[15] Hitchcock, J. P.; Tasker, A. L.; Stark, K.; Leeson, A.; Baxter, E. A.; Biggs, S.; Cayre, O. J., Adsorption of Catalytic Nanoparticles onto Polymer Substrates for Controlled Deposition of Microcapsule Metal Shells. Langmuir 2018, 34 (4), 1473-1480. [16] Al-Shannaq, R.; Kurdi, J.; Al-Muhtaseb, S.; Farid, M., Innovative method of metal coating of microcapsules containing phase change materials. Sol. Energy 2016, 129, 54-64. [17] Roberts, N. S.; A-Shannaq, R.; Kurdi, J.; Al-Muhtaseb, S. A.; Farid, M. M., Efficacy of using slurry of metal-coated microencapsulated PCM for cooling in a micro-channel heat exchanger. Appl. Therm. Eng. 2017, 122, 11-18. [18] Tsuneyoshi, T.; Ono, T., Metal-coated microcapsules with tunable magnetic properties synthesized via electroless plating. Mater. Sci. Eng., B 2017, 222, 49-54. [19] Nocera, G. M.; Ben M'Barek, K.; Bazzoli, D. G.; Fraux, G.; Bontems-Van Heijenoort, M.; Chokki, J.; Georgeault, S.; Chen, Y.; Fattaccioli, J., Fluorescent microparticles fabricated through chemical coating of O/W emulsion droplets with a thin metallic film. RSC Adv. 2014, 4 (23), 11564-11568. [20] Pickering, S. U., CXCVI.-Emulsions. J. Chem. Soc. Trans. 1907, 91 (0), 2001-2021. [21] Ramsden, W., Separation of solids in the surface-layers of solutions and ‘suspensions’ (observations on surface-membranes, bubbles, emulsions, and mechanical coagulation). - Preliminary account. Proc. R. Soc. London 1904, 72 (477-486), 156-164. [22] Velev, O. D.; Furusawa, K.; Nagayama, K., Assembly of latex particles by using emulsion droplets as templates .1. Microstructured hollow spheres. Langmuir 1996, 12 (10), 2374-2384.
ACS Paragon Plus Environment
49
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 50 of 54
[23] Velev, O. D.; Furusawa, K.; Nagayama, K., Assembly of latex particles by using emulsion droplets as templates .2. Ball-like and composite aggregates. Langmuir 1996, 12 (10), 2385-2391. [24] Velev, O. D.; Nagayama, K., Assembly of latex particles by using emulsion droplets .3. Reverse (water in oil) system. Langmuir 1997, 13 (6), 1856-1859. [25] Aveyard, R.; Binks, B. P.; Clint, J. H., Emulsions stabilised solely by colloidal particles. Adv. Colloid Interface Sci. 2003, 100-102, 503-546. [26] Dinsmore, A. D.; Hsu, M. F.; Nikolaides, M. G.; Marquez, M.; Bausch, A. R.; Weitz, D. A., Colloidosomes: Selectively permeable capsules composed of colloidal particles. Science 2002, 298 (5595), 1006-1009. [27] Cayre, O. J.; Noble, P. F.; Paunov, V. N., Fabrication of novel colloidosome microcapsules with gelled aqueous cores. J. Mater. Chem. 2004, 14 (22), 3351-3355. [28] Fujii, S.; Yusa, S.; Nakamura, Y., DD Stimuli-Responsive Liquid Marbles: Controlling Structure, Shape, Stability, and Motion. Adv. Funct. Mater. 2016, 26 (40), 7206-7223. [29] Melle, S.; Lask, M.; Fuller, G. G., Pickering emulsions with controllable stability. Langmuir 2005, 21 (6), 2158-2162. [30] Cui, M. M.; Emrick, T.; Russell, T. P., Stabilizing Liquid Drops in Nonequilibrium Shapes by the Interfacial Jamming of Nanoparticles. Science 2013, 342 (6157), 460-463. [31] Fang, P. P.; Chen, S.; Deng, H. Q.; Scanlon, M. D.; Gumy, F.; Lee, H. J.; Momotenko, D.; Amstutz, V.; Cortes-Salazar, F.; Pereira, C. M.; Yang, Z. L.; Girault, H. H., Conductive Gold Nanoparticle Mirrors at Liquid/Liquid Interfaces. ACS Nano 2013, 7 (10), 9241-9248.
ACS Paragon Plus Environment
50
Page 51 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
[32] Maestro, A.; Deshmukh, O. S.; Mugele, F.; Langevin, D., Interfacial Assembly of Surfactant-Decorated Nanoparticles: On the Rheological Description of a Colloidal 2D Glass. Langmuir 2015, 31 (23), 6289-6297. [33] Russell, J. T.; Lin, Y.; Boker, A.; Su, L.; Carl, P.; Zettl, H.; He, J. B.; Sill, K.; Tangirala, R.; Emrick, T.; Littrell, K.; Thiyagarajan, P.; Cookson, D.; Fery, A.; Wang, Q.; Russell, T. P., Selfassembly and cross-linking of bionanoparticles at liquid-liquid interfaces. Angew. Chem. Int. Edit. 2005, 44 (16), 2420-2426. [34] Skaff, H.; Lin, Y.; Tangirala, R.; Breitenkamp, K.; Boker, A.; Russell, T. P.; Emrick, T., Crosslinked capsules of quantum dots by interfacial assembly and ligand crosslinking. Adv. Mater. 2005, 17 (17), 2082-2086. [35] Y. Lin, H. S., T. Emrick, A. D. Dinsmore, T. P. Russell, Nanoparticle Assembly and Transport at Liquid-Liquid Interfaces. Science 2003, 299. [36] Duan, H.; Wang, D.; Kurth, D. G.; Mohwald, H., Directing self-assembly of nanoparticles at water/oil interfaces. Angew. Chem. Int. Ed. 2004, 43 (42), 5639-42. [37] Wang, D. Y.; Duan, H. W.; Mohwald, H., The water/oil interface: the emerging horizon for self-assembly of nanoparticles. Soft Matter 2005, 1 (6), 412-416. [38] Reincke, F.; Hickey, S. G.; Kegel, W. K.; Vanmaekelbergh, D., Spontaneous assembly of a monolayer of charged gold nanocrystals at the water/oil interface. Angew. Chem. Int. Ed. 2004, 43 (4), 458-462. [39] Schwartz, H.; Harel, Y.; Efrima, S., Surface behavior and buckling of silver interfacial colloid films. Langmuir 2001, 17 (13), 3884-3892.
ACS Paragon Plus Environment
51
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 52 of 54
[40] Schultz, D. G.; Lin, X. M.; Li, D. X.; Gebhardt, J.; Meron, M.; Viccaro, P. J.; Lin, B. H., Structure, wrinkling, and reversibility of Langmuir monolayers of gold nanoparticles. J. Phys. Chem. B 2006, 110 (48), 24522-24529. [41] Faraday, M., X. The Bakerian Lecture. –Experimental relation of gold (and other metals) to light. Phil. Trans. R. Soc. Lond. 1857, 147, 145-181. [42] Nishi, N.; Kakinami, T.; Sakka, T., Dendritic nanofibers of gold formed by the electron transfer at the interface between water and a highly hydrophobic ionic liquid. Chem. Commun. 2015, 51 (71), 13638-13641. [43] Kakinami, T.; Nishi, N.; Amano, K.; Sakka, T., Preparation of Dendritic Gold Nanofibers Using a Redox Reaction at the Interface between an Ionic Liquid and Water: Correlation between Viscosity and Nanostructure. Bunseki Kagaku 2016, 65 (3), 157-161. [44] Zhang, Y.; Nishi, N.; Amano, K.; Sakka, T., One-dimensional Pt nanofibers formed by the redox reaction at the ionic liquidjwater interface. Electrochim Acta 2018, 282, 886891. [45] Dryfe, R. A. W.; Uehara, A.; Booth, S. G., Metal Deposition at the Liquid-Liquid Interface. Chem. Rec. 2014, 14 (6), 1013-1023. [46] Rao, C. N. R.; Kulkarni, G. U.; Thomas, P. J.; Agrawal, V. V.; Saravanan, P., Films of metal nanocrystals formed at aqueous-organic interfaces. J. Phys. Chem. B 2003, 107 (30), 73917395. [47] Gautam, U. K.; Ghosh, M.; Rao, C. N. R., Template-free chemical route to ultrathin single-crystalline films of CuS and CuO employing the liquid-liquid interface. Langmuir 2004, 20 (25), 10775-10778.
ACS Paragon Plus Environment
52
Page 53 of 54 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Langmuir
[48] Agrawal, V. V.; Kulkarni, G. U.; Rao, C. N. R., Nature and properties of ultrathin nanocrystalline gold films formed at the organic-aqueous interface. J. Phys. Chem. B 2005, 109 (15), 7300-7305. [49] Kosif, I.; Kratz, K.; You, S. S.; Bera, M. K.; Kim, K.; Leahy, B.; Emrick, T.; Lee, K. Y. C.; Lin, B. H., Robust Gold Nanoparticle Sheets by Ligand Cross-Linking at the Air-Water Interface. ACS Nano 2017, 11 (2), 1292-1300. [50] Sebastian, H. B.; Mayall, R. M.; Birss, V. I.; Bryant, S., Fabrication of a Self-Supported Nanoparticle-Decorated Amphipathic Film at a Liquid/Liquid Interphase. Langmuir 2017, 33 (39), 10125-10133. [51] Deki, S.; Nakata, A.; Sakakibara, Y.; Mizuhata, M., Deposition of metal oxide films at liquid-liquid interface by the liquid phase deposition method. J. Phys. Chem. C 2008, 112 (35), 13535-13539. [52] Kaneko, H.; Sakahara, H.; Taimatsu, H., Filmy growth of metal leaves electrodeposited at the metallic salt solution/organic liquid interface., Shigen To Sozai 1991, 107 (8), 4044. [53] Piao, Y. Z.; Jang, Y. J.; Shokouhimehr, M.; Lee, I. S.; Hyeon, T., Facile aqueous-phase synthesis of uniform palladium nanoparticles of various shapes and sizes. Small 2007, 3 (2), 255-260. [54] Kutuzov, S.; He, J.; Tangirala, R.; Emrick, T.; Russell, T. P.; Boker, A., On the kinetics of nanoparticle self-assembly at liquid/liquid interfaces. Phys. Chem. Chem. Phys. 2007, 9 (48), 6351-6358.
ACS Paragon Plus Environment
53
Langmuir 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 54 of 54
[55] Scherrer, P., Bestimmung der Größe und der inneren Struktur von Kolloidteilchen mittels Röntgenstrahlen. Nachrichten von der Gesellschaft der Wissenschaften zu Göttingen, Mathematisch-Physikalische Klasse 1918, 98-100. [56] Sakai, T.; Alexandridis, P., Mechanism of gold metal ion reduction, nanoparticle growth and size control in aqueous amphiphilic block copolymer solutions at ambient conditions. J. Phys. Chem. B 2005, 109 (16), 7766-7777. [57] Hansen, C., The Three Dimensional Solubility Parameter and Solvent Diffusion Coefficient and Their Importance in Surface Coating Formulation., Danish Technical Press, 1967. [58] Kamio, E.; Yonemura, S.; Ono, T.; Yoshizawa, H., Microcapsules with Macroholes Prepared by the Competitive Adsorption of Surfactants on Emulsion Droplet Surfaces. Langmuir 2008, 24 (23), 13287-13298. [59] Witten, T. A.; Sander, L. M., Diffusion-Limited Aggregation, a Kinetic Critical Phenomenon. Phys. Rev. Lett. 1981, 47 (19), 1400-1403. [60] Matula, R. A., Electrical-Resistivity of Copper, Gold, Palladium, and Silver. J. Phys. Chem. Ref. Data 1979, 8 (4), 1147-1298.
ACS Paragon Plus Environment
54