Martin Höglund1, Jonas Garemark1, Mathias Nero2, Tom Willhammar2, Sergei Popov3, Lars A Berglund1. 1. Department of Fibre and Polymer Technology, Wallenberg Wood Science Center, KTH Royal Institute of Technology, SE-100 44 Stockholm, Sweden. 2. Department of Materials and Environmental Chemistry, Stockholm University, SE-106 91 Stockholm, Sweden. 3. Department of Applied Physics, KTH Royal Institute of Technology, 114 19 Stockholm, Sweden.
Abstract
Wood is an eco-friendly and abundant substrate and a candidate for functionalization by large-scale nanotechnologies. Infiltration of nanoparticles into wood, however, is hampered by the hierarchically structured and interconnected fibers in wood. In this work, delignified wood is impregnated with gold and silver salts, which are reduced in situ to plasmonic nanoparticles via microwave-assisted synthesis. Transparent biocomposites are produced from nanoparticle-containing wood in the form of load-bearing materials with structural color. The coloration stems from nanoparticle surface plasmons, which require low size dispersity and particle separation. Delignified wood functions as a green reducing agent and a reinforcing scaffold to which the nanoparticles attach, predesigning their distribution on the surface of fibrous "tubes". The nanoscale structure is investigated using scanning transmission electron microscopy (STEM), energy-dispersive spectroscopy (EDS), and Raman microscopy to determine particle size, particle distribution, and structure-property relationships. Optical properties, including response to polarized light, are of particular interest.
Wood is an eco-friendly and abundant substrate and a candidate for functionalization by large-scale nanotechnologies. Infiltration of nanoparticles into wood, however, is hampered by the hierarchically structured and interconnected fibers in wood. In this work, delignified wood is impregnated with gold and silver salts, which are reduced in situ to plasmonic nanoparticles via microwave-assisted synthesis. Transparent biocomposites are produced from nanoparticle-containing wood in the form of load-bearing materials with structural color. The coloration stems from nanoparticle surface plasmons, which require low size dispersity and particle separation. Delignified wood functions as a green reducing agent and a reinforcing scaffold to which the nanoparticles attach, predesigning their distribution on the surface of fibrous "tubes". The nanoscale structure is investigated using scanning transmission electron microscopy (STEM), energy-dispersive spectroscopy (EDS), and Raman microscopy to determine particle size, particle distribution, and structure-property relationships. Optical properties, including response to polarized light, are of particular interest.
Plasmonic nanoparticles
(PNPs) are of great interest as constituents
in complex nanomaterials and can provide functions exemplified by
photonic materials for e.g., optoelectronic devices,[1] solar energy management,[2] or
provision of structural color.[3] Although
sophisticated films and coatings with highly ordered PNP structures
have been produced,[4] they tend to be mechanically
delicate, and the challenge of large-scale processing needs to be
addressed for plasmonic nanomaterials in general.[5] Recently, wood was suggested as a substrate in large-scale
nanotechnologies,[6] as exemplified by structural
EMI-shielding,[7] since it is a low-cost,
eco-friendly structural material with a sophisticated hierarchical
structure. Combinations of chemical modification and embedding of
inorganic nanoparticles can add new functionalities to wood, in an
attractive combination with its structural properties. In the present
study, a processing method for load-bearing wood biocomposites with
PNPs is reported, and the resulting nanocomposites are investigated
for their optical properties and structural color effects.Transparent
wood (TW) is a new form of wood biocomposites, which
has garnered interest as a material combining optical transmittance
with mechanical performance and lightweight.[8,9] This
top-down approach utilizes the existing, oriented cellulose structures
in wood, as a simpler alternative to bottom-up freeze-dried cellulose
structures,[10] where processing-related
energy demands will be much higher. TW is created by chemical removal
of lignin chromophores, followed by impregnation and polymerization
of a polymer with a matching refractive index to the wood structure.
It was first investigated in anatomical studies of wood,[11] but the recent focus is on multifunctional biocomposites,
including stretchable/conductive,[12] magnetic,[13] heat shielding,[14] and thermal energy storing TW,[15] smart
windows,[16] and in solar energy applications.[17,18] Further studies have shown their potential as a photonic nanomaterial,
by incorporation of luminescent dyes,[19−21] quantum dots[22] and photochromic[23] or photo/thermochromic compounds.[24] Interesting
optical effects have been observed such as anisotropic light scattering,[25,26] wave guiding,[20] polarization effects,[27] and wood cells functioning as optical gain cavities
for lasing.[21] Chemical stability is a concern
for PNPs,[28] but the present thiol-ene polymer
improves chemical stability by antioxidative properties,[29] and reduces particle agglomeration problems.[30]A class of interesting optical functions,
not investigated for
TW, is structural coloration. Structural colors are renowned for their
vibrancy, iridescence, and photostability. Brilliant colors found
in butterfly wings, beetle shells, fish scales, and bird feathers
all stem from their micro to nanoscale structures.[31] Structural colors are related to micro- and nanoscale structures,
which interact with light, contrary to dyes which rely on absorption
by their specific molecular spectra. In plasmonic materials, conduction
band electrons oscillate coherently in response to external illumination,
generating a responding electric field at the surface. The modes of
oscillation are known as surface plasmons. Incident electromagnetic
waves which resonate with the surface plasmons are strongly absorbed
or scattered, observed as absorption bands originating from surface
plasmon resonance (SPR).[32] SPRs depend
on the dielectric character of the material, as well as the spatial
confinement in terms of size and geometry of the nanoparticles,[32−34] and is therefore considered a subset of structural coloring.[35] Gold and silver nanoparticles have SPRs within
the range of visible light and produce brilliant structural colors,
and exhibit molar extinction coefficients, which are several times
higher than common organic pigments.[32,36] In addition,
common pigments suffer from photodegradation, which noble metals avoid
due to their excellent stability and different origin of the coloring
response.[32,35] Plasmonic color does, however, require careful
control of particle size dispersion, and geometry, to produce narrow
SPR bands.PNPs have been used empirically throughout history
to produce brilliant
colors in ceramic glazes,[37] stained church
windows,[38] and in early photography.[39] Today, interest in PNPs is due to their photostability
and strong response to the exciting light, which could decrease colorant
load and remove the need for re-coloration. PNPs have therefore been
proposed for textile coloration,[40−43] and are of interest for photonic
biocomposites. Furthermore, PNPs have shown potential as active species
in optical filters and polarizers for information technology, in nonlinear
optics, for surface-enhanced fluorescence, and for improved photovoltaic
devices for solar cell applications.[44,45]Wood
has been functionalized with PNPs for water treatment applications,
either as filters[46] or for solar steam
generation,[47,48] but never for coloration purposes
where low particle size variation and good dispersion are required.[32] To the best of our knowledge, structural coloration
of wood has only been proposed as surface coatings of photonic crystals[49,50] or alternating layers of mica and titania.[51] Such structures display angle-dependent colors, unlike PNP coloration.Studies on water treatment applications focused primarily on bactericidal[46] and steam generation functions, with limited
analysis of nanostructural features.[47,48] Harmful reducing
agents were often added to convert metal salts to nanoparticles. An
interesting, more eco-friendly approach is suggested, where wood-derived
compounds are utilized as green reducing agents. Cellulose hydrogels,[52] cellulose derivatives,[53] lignocellulosic fibers,[54] cellulose nanocrystals,[55] wood powders,[56] and
bleached pulp[40] have been used to reduce
metal salts. To our knowledge, only palladium particles have been
precipitated in wood without reducing agents,[57] where wood lignin served as a reducing agent. Lignin is, however,
commonly removed during TW preparation,[8,9] since it contains
wood chromophores.[58] In the present study,
delignified wood is by itself reducing silver and gold salts to PNPs.Hydrothermal synthesis of metal nanoparticles often requires reaction
times of several hours when heated by standard means.[40,47,52,55,57] In microwave-assisted synthesis, inverted
heat gradients are efficiently and rapidly heating bulk solutions.[59,60] Reaction times are drastically reduced (5–10 min for gold
and silver nanoparticles) and dispersions of smaller particle size
are obtained due to improved nucleation.[60] The porous structure of wood is believed to improve electromagnetic
absorption and conversion to thermal energy,[61] and biomass-derived materials have been used for electromagnetic
shielding.[62,63] In previous investigations, iron
oxide particles were formed inside wood.[64] A variety of metal nanoparticles were precipitated on bacterial
cellulose fibrils, and combined into multifunctional laminate structures;[65] a related approach was demonstrated for wood-based
aerogels.[66]The hierarchical and
anisotropic wood structure is a specific characteristic
of TW biocomposites, resulting in mechanical[67] and optical anisotropy.[25−27] Functional anisotropy can also
be designed by selective deposition of nanoparticles on nanofibers,[68] and/or on cell walls in a wood substrate. The
particle distribution becomes predesigned by the wood structure and,
thus, mimics its anisotropy. In a previous study,[69] magnetic nanoparticles were found to decorate the inside
of wood fibers, but anisotropic predesign of TW using nanoparticles
has not been investigated in detail. In the present study, the distribution
of PNPs is scrutinized and related to enhanced anisotropic optical
effects.TW with structural color requires well-dispersed PNPs
with nanostructurally
controlled sizes, since the SPR scattering bands are sensitive to
particle aggregation.[32] The main objectives
are therefore to tailor and control the processes during both in situ
synthesis of PNPs and TW fabrication. In addition, relationships between
composition/structure and physical properties are investigated. The
mechanisms of particle formation and separation are explored, in particular
the role of delignified wood as a green reducing agent and scaffold
for controlled PNP nanoparticle distribution. After TW fabrication,
the resulting brilliantly colored TW nanocomposites combine load-bearing
and also functional properties, in the form of anisotropic optical
properties and polarization effects.
Experimental
Section
Materials
Rotary cut balsa veneers with a density of
90–110 kg m–3 was supplied by Material AB
(Sweden). Sodium acetate, silver nitrate (AgNO3), chloroauric acid
(HAuCl4), pentaerythritol tetrakis(3-mercaptoproponiate) (PETMP), 1,3,5-trially-1,3,5-trione-2,4,6(1H,3H,5H)-triazine (TATATO), and 1-hydroxycyclohexyl
phenyl ketone were all supplied by Merck. Acetone and ethanol absolute
were supplied from VWR. Acetic acid (Honey-well) and sodium chlorite
(Alfa Aesar) were supplied by other vendors.
Wood Delignification
Balsa veneers were cut with a
razor blade to 1.5 × 1.2 × 0.1 cm3 (for optical
characterization) or 5.0 × 0.5 × 0.1 cm3 (for
tensile testing) pieces. The pieces were delignified at 80 °C
in acetate buffer containing sodium chlorite (1 wt %), according to
a previously published method.[8] Delignification
continued until the pieces turned completely white. The delignified
substrates were subsequently washed in deionized water.
Microwave-Assisted
In Situ Synthesis of PNPs
Delignified
wood substrates were infiltrated under reduced pressure with aqueous
solutions (4 mL) of either silver nitrate (0.5 mM) or chloroauric
acid (0.1 mM) for 3 h. Infiltrated substrates were kept in metal salt
solutions during in situ synthesis, which was performed with a temperature-controlled
single-mode (2.45 GHz) microwave oven (Biotage Initiator). Samples
were heated to and kept at 120 °C during synthesis, followed
by cooling down to 50 °C. The reaction time was 5 min for chloroauric
solutions and 10 min for silver nitrate solutions.
Transparent
Wood Preparation
TW preparation followed
a fabrication method reported elsewhere.[70] Substrates were sequentially solvent exchanged from deionized water
to ethanol absolute and to acetone. A stoichiometric mixture, according
to functional groups, of TATATO and PETMP containing 1-hydroxycyclohexyl
phenyl ketone (0.5 wt %) was infiltrated into the substrates for at
least 4 h inside a fume hood. Impregnation was mediated by acetone,
which was then evaporated. UV illumination for 4 min using four 9W
365 nm UV-lamps, cured the thiol-ene thermoset, resulting in TW biocomposites.
Characterization
Wood content in finished TW composites
was calculated from the average density of delignified substrates
and the dimensions and weight of TW samples.A Universal Testing
Machine (Instron 5566) equipped with a video extensometer was used
to perform tensile tests with a 10 kN load cell, 5 mm min–1 piston speed, and a grip distance of 2.5 mm. Samples (5.0 ×
0.5 × 0.1 cm3) were conditioned at 22 °C and
50% relative humidity overnight prior to testing. The presented data
are averages of five samples per specific composite.Total transmittance
(ballistic and diffuse light) was measured
according to ASTM D1003-13.[71] TW samples
were placed at the opening port of an integrating sphere and exposed
to spectrally broadband light (quartz tungsten halogen light, model
66181, Oriel Instruments). The same set-up
was used to measure polarized transmittance by placing a polarizing
filter between the sample and the integrating sphere. The samples
were measured with the wood fibers oriented parallel and perpendicular
to the polarization direction of the filter. The ratio of polarization
split is the quotient of the two polarized measurements.Scanning
transmission electron microscopy (STEM) images of the
TW materials were acquired using a double aberration-corrected Thermo
Fisher Themis-Z transmission electron microscope. The microscope was
operated at an accelerating voltage of 300 kV. Annular dark-field
(ADF) STEM images were acquired using a beam current of 40 pA, a beam
convergence angle of 21 mrad, an inner collection angle of 39 mrad,
and a dwell time of 20 μs.To study the interior of the
TW material, ultra-thin transverse
sectioning was carried out using a Leica Ultracut UCT with a 45°
diamond knife from Diatome. A cutting speed of 1 mm s–1 was used and a clearance angle of 6°. The sections have estimated
thicknesses of ca. 100 nm. After cutting, the sections were transferred
to carbon coated copper grids (EMS CF400-CU-UL) for STEM analysis.
No staining or other contrast enhancing chemicals were used.Scanning electron microscopy (SEM) imaging and energy-dispersive
X-ray spectroscopy (EDS) were conducted with a field emission SEM
(FE-SEM) (Hitachi S-4800, Japan) with an attached EDX probe (X-MaxN,
Oxford Instruments). Freeze fractured wood substrates with a 1 nm
platinum/palladium coating were used for cell wall imaging. Micrographs
were captured at an accelerating voltage of 15 kV, an amperage of
2 μAm, and a working distance of 5 cm. EDS mapping was performed
on uncoated substrate fractures, using 6 kV, 20 μA, and a working
distance of 15 cm.Raman spectra of the cell wall surfaces of
wood substrates were
measured with a confocal Raman microscope (Jobin Yvon HR800 UV, Horiba)
using a 514 nm laser (Stellar-Pro, Modu-laser). Spectra were accumulatively
acquired 16 times, baselined and normalized to CH2 vibrations
at 1333 cm–1.X-ray diffraction (XRD) measurements
were carried out on wood substrates,
compressed with 15 MPa for 2 min, with a powder X-ray diffractometer
(ARL X’TRA, Thermo Fisher Scientific). Scans over 2θ
of 5–50°, with a 0.04 step size, were performed with Cu
Kα radiation at 40 mA and 45 kV. The peak height method was
used to calculate the crystallinity index (CI) as the quotient of
the crystalline [200] peak and the total peak intensity (I200):[72]Fourier transformed
infrared spectroscopy
(FTIR) was conducted on wood substrates using a Spectrum 100 FTIR
(PerkinElmer) with a MKII Golden Gate ATR system (Specac Ltd.) Spectra
were accumulatively acquired 16 times.
Results and Discussion
Materials
Processing and Mechanical Properties
Structurally
colored transparent wood was prepared by in situ synthesis of plasmonic
nanoparticles (PNPs) in delignified wood substrates, followed by impregnation
and curing of a thiol-ene polymer matrix. Delignification of balsa
veneers was first carried out to remove chromophores,[8] producing bright white wood substrates (Figure b). The substrates were subsequently
washed in deionized water and infiltrated with aqueous solutions of
0.1 mM chloroauric acid or 0.5 mM silver nitrate. Higher metal salt
concentrations were tested but resulted in inferior colors for gold
substrates (Figure S1), likely due to the
formation and agglomeration of larger particles. Silver templates
were seemingly unaffected within the range of concentrations. Silver
NPs are possibly more stable at the reaction temperature than gold
due to higher binding energy to carboxyl groups,[73,74] which are formed during synthesis. Substrates remained white until
subjected to microwave-assisted synthesis of nanoparticles. PNP formation
is apparent from the brilliant colors produced by the substrates;
bright yellow silver and pinkish-purple gold (Figure c,d). Lightly colored and stable nanoparticle
suspensions were also produced in the process. No additional reducing
agent was needed, as wood compounds function as green reducing agents.
Any degradation of the substrate was superficial and structural integrity
was retained. In situ synthesis of PNPs is, thus, a potential method
for preparing wood with structural color.
Figure 1
(a) Schematic sketch
of structurally colored TW processing: delignified
wood is infiltrated with metal salts (silver or gold) which are in
situ reduced to plasmonic nanoparticles by microwave-assisted synthesis.
Nanoparticle-containing substrates are then infiltrated with monomers
and cured to TW composites with structural color. Photographs of (b)
balsa wood, delignified substrate, silver substrate, gold substrate,
(c) Ag-TW, and (d) Au-TW.
(a) Schematic sketch
of structurally colored TW processing: delignified
wood is infiltrated with metal salts (silver or gold) which are in
situ reduced to plasmonic nanoparticles by microwave-assisted synthesis.
Nanoparticle-containing substrates are then infiltrated with monomers
and cured to TW composites with structural color. Photographs of (b)
balsa wood, delignified substrate, silver substrate, gold substrate,
(c) Ag-TW, and (d) Au-TW.To provide optical transmittance and improve mechanical stability,
a polymer matrix with a matching refractive index replaced voids in
the porous substrate.[8,70] A UV-curable thiol-ene thermoset,
previously used for TW preparation,[70] was
used. Impregnation of thiol-ene precursors was mediated by solvent-assisted
impregnation. Substrates were sequentially exchanged from deionized
water to ethanol and acetone prior to precursor impregnation. Acetone
was then evaporated prior to curing. PNPs were well attached to the
substrate, and neither loss in substrate color, nor color acquisition
of the polymer, was observed. Curing of infiltrated precursors resulted
in brilliantly colored transparent wood (TW) biocomposites, i.e.,
bright yellow Ag-TW (silver) and purple Au-TW (gold), as presented
in Figure . The final
composites have a wood content of 6.8 vol % and minuscule amounts
of nanoparticles, 0.02 vol % silver and 0.01 vol % gold. The low nanoparticle
content demonstrates the strong coloration effect from PNPs.TW composites exhibit favorable anisotropic mechanical[67] and optical properties,[25−27] which are linked
to the wood structure. Hardwoods (present class of wood species) consist
primarily of fibers, vessels, and ray cells, all tubular in structure.
Fibers and vessels are oriented parallel to the tree stem (longitudinal
direction), and in Figure c,d this is the horizontal direction of the TW composites.
Fibers dominate the wood structure and provide mechanical support.
Vessels are fewer but larger in size and facilitate transport of liquids
and nutrients. Rays are oriented perpendicular to the longitudinal
direction and results in liquid transport (outward from the center
of the tree) and storage of nutrients. Rays appear as dark streaks
in Figure c,d. Balsa
also contains high fractions of longitudinal parenchyma cells, which
mainly store nutrients. Hardwoods thus show an anisotropic structure
with high strength in the longitudinal direction.[67] In TW biocomposites, the wood substrate thus provides mechanical
reinforcement.[8,9] It is also a scaffold controlling
nanoparticle distribution in the present study and serves as a green
reducing agent during PNP formation.Tensile properties are
summarized in Table and stress–strain curves are in Figure S2. Young’s modulus (4.11 GPa),
tensile strength (50.7 MPa), and strain to failure (1.2%) of reference
TW were not significantly impacted by incorporation of PNPs (3.80
GPa Young’s modulus, 45.7 MPa tensile strength, and 1.3% strain
to failure for Ag-TW). The slight lowering of mechanical properties
is probably from local density variations in wood, rather than a real
effect from structural changes. In situ synthesis of NPs is deemed
to have a low to negligible impact on the mechanical properties of
TW.
Table 1
Tensile Propertiesa
Young’s modulus [GPa]
tensile
strength [MPa]
strain to failure [%]
Ag-TW
3.80 ± 0.62
45.7 ± 2.5
1.3 ± 0.2
TW
4.11 ± 0.50
50.7 ± 2.5
1.2 ± 0.1
Averaged values
from five samples
per composite.
Averaged values
from five samples
per composite.
Optical Properties
Optical properties of structurally
colored TW are interesting in several aspects. Light absorption and
scattering, as well as optical effects associated with material anisotropy
are defined by both the composite components (wood substrate and polymer)
and the added metal nanoparticles. Optical transmittance (Figure a) was characterized
using thin TW samples (1.2 mm) and an integrating sphere set-up, making
scattering losses negligible.[26] A reference
TW (green line in Figure a) demonstrated lower transmittance than neat thiol-ene (blue
line in Figure a),
as expected from wood substrate scattering effects.
Figure 2
Optical properties of
Ag-TW and Au-TW: (a) total transmittance
and (b) ratio of polarization split. (c) Photographs of Ag-TW and
Au-TW with visible text underneath. (d) Specimen set-up for polarized
transmittance measurements of perpendicular and parallel orientation.
Optical properties of
Ag-TW and Au-TW: (a) total transmittance
and (b) ratio of polarization split. (c) Photographs of Ag-TW and
Au-TW with visible text underneath. (d) Specimen set-up for polarized
transmittance measurements of perpendicular and parallel orientation.Addition of metal nanoparticles into the host matrix
significantly
changes the optical transmission. Metal nanoparticles themselves exhibit
band absorption caused by the excitation of surface plasmons with
surface plasmon resonances (SPR) in the visible range. The specific
SPR wavelength is related to the size, geometry, and material of the
nanoparticle.[34,75] The broadening of the SPR extinction
band is defined by the size dispersion of nanoparticles. Transmittance
spectra of structurally colored TW are presented in Figure a. The minimum transmission
for both materials corresponds to the SPR of the respective material,
438 nm (silver) and 538 nm (gold). A stronger absorption of Ag-TW
is related to a higher nanoparticle content in the TW substrate and
higher electrical conductivity of silver.[34]Interestingly, the polarization of transmitted light is also
affected
by the presence of nanoparticles. Pure TW (without nanoparticles)
exhibits variation in light transmission for different polarizations,[27] which was also observed for the reference TW
(green line in Figure S3). The light which
is polarized perpendicular to the direction of fibers demonstrated
a slightly higher transmission, as compared with light polarized along
the wood fibers. This effect can be attributed to the spatial anisotropy
of the wood structure. It resembles a diffraction grating with a uniform
structure parallel to the fiber direction, but poor periodicity perpendicular
to the fiber orientation. Thus, after light propagation through the
material, the light polarization split replicates the polarization
split in conventional diffraction gratings, although with a less noticeable
effect.[76]The light polarization
split between light perpendicular and parallel
to the fibers is more pronounced for Ag-TW compared with Au-TW (Figure S3). For clarity, it is more instructive
to compare the ratio of the polarization split for different materials
instead of an absolute intensity of the polarized light components. Figure b displays the ratio
of the polarization split, i.e., the ratio between the transmitted
light of perpendicular and parallel polarizations. The transparency
of the composites is demonstrated in Figure c and the set-up for polarization measurements
is shown in Figure d. First, we note that structurally colored TW clearly displays a
stronger polarization split at the SPR band of the added nanoparticles,
compared to the reference TW. The effect of nanoparticles seems akin
to the effect of optical antennas created by surface plasmons.[77] The “base” polarization split
created by pure TW (green lines in Figure b) is enhanced by nanoparticles, as their
distribution depends on the anisotropic structure of wood. In other
words, the wood substrate provides a predesigned anisotropic nanoparticle
distribution. Materials with homogenously distributed PNPs would not
exhibit a polarization effect. The degree of enhancement depends on
the specific nanoparticles, and again, is much more pronounced for
Ag-TW than Au-TW. The silver nanoparticles make a significant contribution
to the observed effect, whereas gold only slightly prevails over the
neat reference TW (Figure b). This is linked to the higher particle content in Ag-TW
and higher electrical conductivity of silver.[34]
Figure 3
(a)
Illustration of wood structure, the green square highlights
the area of interest. Cross-sectional ADF-STEM micrographs of (b–d)
Ag-TW and (e–g) Au-TW sections. The cell wall (CW), cell wall
corner (CC), middle lamella (ML), and lumen (L) are marked. Colored
squares indicate magnified areas. Lumen is the empty space at the
center of a fibrous wood cell.
(a)
Illustration of wood structure, the green square highlights
the area of interest. Cross-sectional ADF-STEM micrographs of (b–d)
Ag-TW and (e–g) Au-TW sections. The cell wall (CW), cell wall
corner (CC), middle lamella (ML), and lumen (L) are marked. Colored
squares indicate magnified areas. Lumen is the empty space at the
center of a fibrous wood cell.
Composite Structure
The structure of Ag-TW and Au-TW
was investigated using ADF-STEM imaging of sample cross-sections.
Micrographs are presented in Figure . The cell wall corners are lignin-rich and degraded
during delignification,[8] but the hierarchical
structure of interconnected wood fibers is still retained as the middle
lamella is only partially degraded. The lumen (empty space in wood
cells), cell wall corners, and voids in the middle lamella were fully
impregnated with the polymer matrix. Visible gaps between the solidified
polymer matrix and cell walls are artifacts from ultra-microtomy sectioning.The nanoparticle distribution and separation at the nanoscale are
of key importance for plasmonic coloration, since SPRs are sensitive
to particle aggregation.[32] Metal nanoparticles
are highly contrasted against organic compounds in ADF-STEM imaging
(Figure b–g).
Spherical nanoparticles of silver and gold, in the size range of 3–12
nm, are observed in the TW biocomposite structures. Silver nanoparticles
are primarily found between wood cells: in the cell wall corner and
in the middle lamella between fiber cells. The particles are visibly
separated and well-dispersed within these regions, and little to no
coloration appears to be lost from particle aggregation. The particle
distribution follows the structure of wood and forms tubular shells
on the “fiber tubes”, effectively producing a “wood
structure” of light-interacting particles. Optical effects
related to the structure are, thus, enhanced by the incorporation
of PNPs. The strong ratio of polarization split exhibited by Ag-TW
(Figure b) is therefore
attributed to the particle distribution, which was predesigned by
the structure of the wood substrate.Gold nanoparticles were
present at a lower concentration, and also
exhibited preferential distribution in the cell wall corners and the
middle lamella, but with fewer particles. Nanoparticle aggregation
is avoided, since the particles are visibly separated. A few gold
nanoparticles were found inside the secondary wood cell wall, and
additional nanostructural details are observable in Figure S4.
Substrate Structure
The particle
distribution and composition
of substrates containing nanoparticles were investigated by EDS mapping
of cross-sectional fracture surfaces. Mapping of gold and silver,
in their respective substrates after microwave-assisted synthesis
(Figure a,d), confirms
a comparably homogeneous distribution of particles in the substrates
on the scale of 100 μm. The respective EDS spectra are available
in the Supporting Information (Figures S5 and S6). The process of mobile metal ion infiltration followed
by in situ reduction facilitates homogeneous particle distribution.
If pre-made, liquid-dispersed nanoparticles are used to impregnate
wood substrates, uneven or incomplete infiltration may become a problem
simply because of their larger size compared with ions. In Figure , the wood structure
is clearly visible from the EDS signals, since particles are deposited
on the cell wall, demonstrating the predesigning function of the wood
substrate.
Figure 4
Cross-sectional EDS maps of (a) silver and (d) gold in respective
substrates. SEM micrographs of the radial surface (white arrows indicate
the fiber direction) of (b, c) silver and (e, f) gold-containing substrates,
with higher magnifications show the inside of the fiber cell wall
facing the “empty” lumen space.
Cross-sectional EDS maps of (a) silver and (d) gold in respective
substrates. SEM micrographs of the radial surface (white arrows indicate
the fiber direction) of (b, c) silver and (e, f) gold-containing substrates,
with higher magnifications show the inside of the fiber cell wall
facing the “empty” lumen space.The elemental compositions of the substrates are presented in Table . The substrates attained
nanoparticle contents of 2.1 wt % silver and gold, separately. This
value matches the reported content in a silver-decorated wood filter.[46] Assuming similar densities between nanoparticles
and bulk materials, the respective substrates contain 0.30 vol % silver
and 0.16 vol % gold, resulting in 0.02 vol % silver and 0.01 vol %
gold in the final composites, Ag-TW and Au-TW. The lower SPR extinction
and lower ratio of polarization split of Au-TW (Figure b) in comparison with Ag-TW, stem from the
lower particle content, coupled with the lower electrical conductivity
of gold.[34] The chlorine content in both
substrates is mainly caused by the delignification process.
Table 2
Elemental Composition of Substrates
Containing Nanoparticlesa
element
gold substrate [%]
silver
substrate [%]
gold/silver
2.1
2.1
carbon
69.8
66.4
oxygen
25.9
28.2
chlorine
2.0
3.0
Data presented in weight percentages,
measured with EDS mapping.
Data presented in weight percentages,
measured with EDS mapping.Nanoparticle and substrate structures were investigated by SEM-imaging
of cut surfaces. Micrographs of radial surfaces are presented in Figure . The hierarchical
wood structure, on micro- and nanoscale, was retained for the substrates
after in situ synthesis of PNPs.The microstructure of interconnected
fibers is visible at lower
magnification. Higher magnification micrographs of the cell wall facing
the empty lumen in wood revealed fibrils with retained structure and
orientation.Nanoparticles were observed on the lumen facing
the cell wall of
respective substrates (Figure c,f) and were larger in comparison with particles observed
in the middle lamella and cell wall corners of TW composites (Figure ). The difference
may be caused by the larger void cavity of the lumen, resulting in
a larger reservoir of the metal salt and continued growth during nanoparticle
synthesis. Larger particles are fewer and have lower probability to
be located in thin sections used for ADF-STEM imaging. The strategy
to precipitate PNPs inside the wood structure is successful, and infiltration-related
challenges of preformed PNPs are avoided.[78]
Reduction Mechanism for Nanoparticle Synthesis
The
wood tissue serves as a reducing agent, which makes the present process
environmentally benign compared with those using common reduction
agents, e.g., sodium boron hydride. The mechanism for the reduction
of metal salts to PNPs in delignified wood substrates was therefore
investigated with vibrational spectroscopy. Superficial confocal Raman
measurements could detect differences in the vibrational spectra,
which were not observed in FTIR bulk measurements (Figure S7). The reason is that the reactions were primarily
active on cell wall surfaces. The Raman spectra (normalized to CH2 vibrations at 1333 cm–1) of substrates
before and after nanoparticle synthesis are presented in Figure a.
Figure 5
(a) Raman (normalized
to CH2 vibrations at 1333 cm–1) and (b)
XRD spectra of substrates before and after
nanoparticle synthesis. (c) Schematic of xylan (common hemicellulose)
with highlights of the glycosidic and ether linkages with their respective
Raman active wavenumber. (d) Schematic of the proposed mechanism:
redox reaction involving oxidizing the polysaccharide C1 carbon and
reducing metal ions, followed by cleavage of the glycosidic linkage
and hydration to a carboxylate group.
(a) Raman (normalized
to CH2 vibrations at 1333 cm–1) and (b)
XRD spectra of substrates before and after
nanoparticle synthesis. (c) Schematic of xylan (common hemicellulose)
with highlights of the glycosidic and ether linkages with their respective
Raman active wavenumber. (d) Schematic of the proposed mechanism:
redox reaction involving oxidizing the polysaccharide C1 carbon and
reducing metal ions, followed by cleavage of the glycosidic linkage
and hydration to a carboxylate group.The reduction of both metal nanoparticles follows similar oxidative
paths: glycosidic (1095 cm–1) and ether linkages
(1420 cm–1) of the substrate are cleaved as carboxylate
groups form (1600 cm–1).[79−81] The generation
of carboxylate groups is observed as the growth and broadening of
the overlapping peak of aryl stretching (1602 cm–1)[80] from residual lignin in the wood template.
The width of the carboxylate peak is related to various structures
coordinating with metal nanoparticles.[81] The coordinating structures attract the nanoparticles to the cell
wall, so that particle aggregation is limited. The strong particle
connection to the substrate makes it possible to wash, carry out solvent
exchange, and infiltrate polymer precursors without loss of nanoparticles.
Schematics of common hemicellulose (xylan) and the proposed mechanism
is shown in Figure c,d.Glycosidic and ether linkages are found both in cellulose
and in
hemicelluloses, which are the amorphous polysaccharide compounds surrounding
the nanoscale cellulose fibrils.[82] The
crystallinity indices (CI) of cellulose in substrates before and after
nanoparticle synthesis were calculated from XRD measurements (Figure b), using the peak
height method.[72] Cellulose was largely
unaffected by nanoparticle synthesis as the CI remained the same after
the reactions, at 0.73. The oxidation, therefore, occurs primarily
on superficial hemicelluloses, and possibly on amorphous cellulose.
Some degradation of cellulose was observed for gold since the Raman
active peak related to cellulose crystallinity decreased (900 cm–1,[79]Figure a). The same peak was unaffected for silver.
This mechanism differs from studies where primary hydroxyls in cellulose
nanocrystals[55] or phenols in lignin[54,57] are reducing metal salts.
Conclusions
Plasmonic
silver and gold nanoparticles were in situ synthesized
in wood substrates by a low-temperature process to produce structurally
colored transparent wood (TW), with load-bearing functions. The reinforcing
wood substrate in TW brings additional functions during the processing
of structurally colored TW. It serves as a green reducing agent and
a predesigning scaffold, which ensures allocation of well-dispersed
nanoparticles by substrate attachment. The nanoscale particle distribution
was controlled by the substrate morphology, since the nanoparticles
were formed on and inside the wood cell walls, effectively forming
an anisotropic wood structure of nanoparticles. The light-interacting
PNPs, are able to enhance structure-related optical properties, e.g.,
the polarization effect of TW. The thiol-ene polymer matrix not only
provides optical transmittance and improves mechanical properties
but also contributes to specific thiol-ene-related chemical stability
of the PNPs. Our investigation demonstrates how structurally colored
TW can be produced by facile means and shows the potential to fabricate
anisotropic plasmonic nanocomposites based on wood, useful in load-bearing
optical elements.
Authors: Stefan A Maier; Pieter G Kik; Harry A Atwater; Sheffer Meltzer; Elad Harel; Bruce E Koel; Ari A G Requicha Journal: Nat Mater Date: 2003-04 Impact factor: 43.841
Authors: Hui Chen; Adil Baitenov; Yuanyuan Li; Elena Vasileva; Sergei Popov; Ilya Sychugov; Max Yan; Lars Berglund Journal: ACS Appl Mater Interfaces Date: 2019-09-13 Impact factor: 9.229
Authors: P W Barnes; T M Robson; P J Neale; C E Williamson; R G Zepp; S Madronich; S R Wilson; A L Andrady; A M Heikkilä; G H Bernhard; A F Bais; R E Neale; J F Bornman; M A K Jansen; A R Klekociuk; J Martinez-Abaigar; S A Robinson; Q-W Wang; A T Banaszak; D-P Häder; S Hylander; K C Rose; S-Å Wängberg; B Foereid; W-C Hou; R Ossola; N D Paul; J E Ukpebor; M P S Andersen; J Longstreth; T Schikowski; K R Solomon; B Sulzberger; L S Bruckman; K K Pandey; C C White; L Zhu; M Zhu; P J Aucamp; J B Liley; R L McKenzie; M Berwick; S N Byrne; L M Hollestein; R M Lucas; C M Olsen; L E Rhodes; S Yazar; A R Young Journal: Photochem Photobiol Sci Date: 2022-02-21 Impact factor: 4.328