ArticlePDF Available

Self-assembly of Au Nanoparticle-containing Peptide Nano-rings on Surfaces

Authors:

Abstract and Figures

The peptide nano-rings containing Au nanoparticles inside their cavities were self-assembled on dithiol SAMs patterned as an array by AFM-based nanolithography. The peptide nano-rings were aligned as a line on these SAMs, and Au formed lines with the spacing between these nanoparticles as the peptide nano-rings functioned as spacers. This type of array fabrication will provide improved tunability in their optical properties of resulting nanoparticle-assembled arrays. In addition, optimization of the inter-particle distance of nanoparticles in the array with various spacers may allow one to design new types of photonic crystals with desired optical properties.
Content may be subject to copyright.
Self-assembly of Au Nanoparticle-containing Peptide Nano-rings
on Surfaces
NURXAT NURAJEa, KAI SUb, JACOPO SAMSONa, AMIT HABOOSHEHa, ROBERT I.
MACCUSPIEa, HIROSHI MATSUIa,*
aDepartment of Chemistry, Hunter College and the Graduate Center, City University of New York,
New York, NY 10021, USA
bDepartment of Chemistry, College of Staten Island, Staten Island, NY 10314, USA
Abstract
The peptide nano-rings containing Au nanoparticles inside their cavities were self-assembled on
dithiol SAMs patterned as an array by AFM-based nanolithography. The peptide nano-rings were
aligned as a line on these SAMs, and Au formed lines with the spacing between these
nanoparticles as the peptide nano-rings functioned as spacers. This type of array fabrication will
provide improved tunability in their optical properties of resulting nanoparticle-assembled arrays.
In addition, optimization of the inter-particle distance of nanoparticles in the array with various
spacers may allow one to design new types of photonic crystals with desired optical properties.
Keywords
Peptide nano-rings; Bionanotechnology; Nanofabrication; Self-assembled monolayers
INTRODUCTION
Recent improved two-dimensional and three-dimensional nanofabrication techniques allow
one to build precisely designed structures in nanoscale for various photonic applications [1–
3]. While the top–down approach has been applied for photonic crystal fabrications, the
bottom– up approach via self-assembly of photonic nano-building blocks is also showing
promising outcomes [4–12]. For the bottom–up approach for the optics fabrications,
synthesis of photonic nanomaterials and their alignments need to be accomplished efficiently
and precisely.
Biomineralization process, where peptides or proteins are utilized to mineralize metals and
semiconductors, has been shown to produce various types of nanocrystals [13–25]. Since the
amino acid sequences are very sensitive to elements for their mineralization, optimized
peptide sequences can produce nanocrystals efficiently [26]. In addition to the effective
crystal growth, the amino acid sequences of mineralizing peptides could also influence the
size, the alignment, and the shape of resulting nanocrystals [27–30]. Further more, in some
*Corresponding author. hmatsui@hunter.cuny.edu.
HHS Public Access
Author manuscript
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Published in final edited form as:
Supramol Chem
. 2006 ; 18(5): 429–434. doi:10.1080/10615800600659196.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
cases, peptides could mineralize nanocrystals in solution at room temperature that do not
grow under the ambient condition [31,32]. Because the size, the alignment, the shape, and
the crystalline structure of photonic nanocrystals control optical properties of those
assembled nanocrystals, the tunabilities of these features and the potential of new material
synthesis by using peptides will provide a significant advantage to apply peptides for
photonic material syntheses.
The one of smart approaches to create photonic materials by using mineralizing peptides is
to pattern these peptides on surfaces based on photonic device designs and grow photonic
crystals on the patterned peptides. For example, a hologram was applied to pattern silica-
mineralizing peptides as an array and resulting silica nanostructures exhibited a nearly fifty-
fold increase in diffraction efficiency over a comparable polymer hologram [14]. Recently,
microfluidics and lithography were also used to pattern silica- and silver-mineralizing
peptides for photonic applications [28,33].
In this report, we assembled ring-shaped peptide nanostructures as an array on surfaces.
Previously, we developed the ring-shaped peptide nanostructures by self-assembling a
peptide monomer, bis(
N
-α-amido-glycylglycine)-1,7-heptane dicarboxylate and an organic
Au precursor, trimethylphosphinegold chloride (AuPMe3Cl) in solution [34]. After reduction
of Au ions trapped inside the cavities of nano-rings, the peptide nano-rings could template
Au nanoparticles. In this report, after Au nanoparticles were grown inside the cavities of the
peptide nano-rings, these nano-rings containing Au nanoparticles were aligned on the
chemically functionalized arrays patterned by nano-lithography (Fig. 1). Since these peptide
nano-rings were self-assembled in a closely packed manner along the array of those
dithiolated self-assembled monolayers (SAMs), these Au nanoparticles were positioned in
the equal spacing on each line without touching each other as the peptide nano-rings
functioned as spacers. This type of alignment of nanomaterials with spacers can be very
useful for improved photonic crystal designs.
RESULTS AND DISCUSSION
When the peptide monomers were self-assembled in the presence of the water-insoluble
trimethylphosphinegold chloride (AuPMe3Cl) for 5 days in the dark, the ring-shaped peptide
assemblies were observed in solution. The average outer diameter of nano-ring was 50 nm
and the average inner diameter was 15 nm [34]. Our previous spectroscopic investigation
showed that these peptide nano-rings were self-assembled from the peptide monomers and
the organic Au salts by chelating Au with amide groups of the peptide monomers. After UV
light was irradiated to the nano-ring solution for 20 min Au nanoparticles were grown inside
the cavities of nano-rings, however the organic Au salts, trapped inside the cavities, were
reduced to grow Au nanoparticles in the middle of nano-rings [34,35]. In a TEM image of
the nano-ring after reduction of Au ions, the Au nanoparticle appeared darker at the center
of the nano-ring (Fig. 2a). These particles in the cavities were also confirmed as Au
nanoparticles by electron diffraction before their surface assembly on the dithiol SAMs.
When the peptide nano-rings were previously synthesized, they were observed to be stable
in solution [34] however these nano-rings have not been assembled on surfaces. Therefore, it
NURAJE et al. Page 2
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
was necessary to examine their stability via the simple surface-assembly. Before fabricating
the structure shown in Fig. 1, we examined whether the Au nanoparticle-containing peptide
nano-rings are rigid enough to be self-assembled on surfaces by spin-coating them on TEM
grids. A height image of AFM in Fig. 2b confirms that the nano-rings were deposited on a
TEM grid. This figure imaged the assembly of the nano-rings on the surface, but the Au
nanoparticles inside the nano-rings could not be resolved in this AFM height image.
However, when this assembly was imaged by the phase mode of AFM as shown in Fig. 2c,
the Au nanoparticles were observed as a brighter contrast inside the nano-rings because
harder surfaces of Au nanoparticles appeared brighter than softer surfaces of the outer
peptide nano-rings. In the magnified phase image of Fig. 2d, these Au nanoparticles were
not exactly located at the center of the nano-rings, which may be due to the deformation of
the nano-ring shape via spin-coating and the multiple orientations of the nano-rings on TEM
grids.
Since the peptide nano-rings were stable enough to be assembled on TEM grids via spin-
coating, we examined the targeted self-assembly of the peptide nano-rings on the
functionalized surfaces. The functionalized array of dithiol SAMs was patterned by three
steps. First, alkyl SAMs were deposited on a Au substrate and the array was patterned by
removing the alkyl SAMs with the AFM cantilever. Then, mercaptohexadecanoic acid was
assembled on the curved array where Au surfaces were exposed. The carboxylic groups on
the top of these SAMs on trenches were substituted by thiol groups, as shown in Scheme 1.
To align the peptide nano-rings containing Au nanoparticles on the dithiol SAM array
patterned on a Au substrate as shown in Fig. 1, these nano-rings were incubated with this
substrate in solution for 8 h. Because the end groups of the SAMs on the trenches were
functionalized by thiol (Scheme 1), this incubation process allowed the nano-rings to self-
assemble onto these trenches with the thiol-Au interaction, as shown in Fig. 3. Figure 3a is
the AFM image of the patterned substrate in the height mode after the nano-rings were
incubated in the substrate-containing solution. The peptide nano-rings were closely packed
to form the array of continuous lines along the trenches in Fig. 3a. As seen in the height
mode AFM image of the spin-coated samples in Fig. 2b, the individual Au nanoparticle
inside the nano-ring could not be identified in Fig. 3a due to their small height difference
between the peptide nano-ring and the Au nanoparticle. However, when the phase mode of
AFM was applied to image this substrate, the deposited spheres on the trenches looked less
continuous in Fig. 3b since the brighter spheres in this phase image are more likely Au
nanoparticles due to their surface hardness as compared to the one for the peptide nano-
rings. While these AFM images in the phase mode in low resolution do not explicitly show
the discrete positioning of Au nanoparticles inside the nano-rings aligned on the trenches as
shown in Fig. 1, the high-resolution image of the single trench containing the peptide nano-
rings in the phase mode assisted visualizing the peptide nano-ring alignment more clearly.
When the single trench was imaged with the height mode image in high-resolution (Fig. 3c),
still only continuous packing of the nano-rings was observable as a line along the trench and
the discrete Au nanoparticles could not resolve. But when the single trench was imaged in
the phase mode in high-resolution, the discrete alignment of Au nanoparticles was observed,
as shown in Fig. 3d. In this high-resolution image, the harder Au nanoparticles appeared to
be brighter and the spacing between these nanoparticles was visible. The most of Au
NURAJE et al. Page 3
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
nanoparticles in Fig. 3d were self-assembled discretely without touching each other due to
the spacing of the peptide nano-rings (Fig. 1). The darker nano-ring contrast around the Au
nanoparticle, observed in the spin-coated sample in Fig. 2b, was not observed clearly in Fig.
3d, however this phase contrast difference between the spin-coated nano-rings and the self-
assembled nano-rings may be caused by their topological difference. For the spin-coated
sample the nano-rings were forced to pack closely by the external force on very smooth and
flat TEM grids, and the resulting nano-ring monolayer also became relatively flat.
Therefore, the detailed structure of nano-rings and Au nanoparticles was resolved in the
AFM image of the spin-coated nano-ring sample due to the flatness of the coating. However,
for the self-assembled sample, the nano-rings were self-assembled on rough surfaces
consisting of alkyl SAMS and dithiol SAMs in different heights. The trenches were also not
flat because the AFM cantilever could not shave alkyl SAMs smoothly and it further scraped
the Au substrate partially. Shaved SAMs and Au substrate were piled at the edges of
trenches, which also increased the roughness of the substrate. Since all different heights of
SAMs, trenches, and edges contributed unevenness of the surface topology, the AFM
resolution in the phase image on this self-assembled sample was degraded due to its surface
roughness and it prevented to map the locations of the nano-rings and Au nanoparticles in
the phase image. When the neat Au nanoparticles without the peptide nano-rings were
assembled on the same dithiol-functionalized trenches, those Au nanoparticles were aligned
as continuous lines without spacing in their phase AFM image. This observation supports
that the Au nanoparticles observed in Fig. 3d were separated by the peptide nano-rings
otherwise the spacing between Au nanoparticles should not be imaged. It should be noted
that some of these nanoparticles seem to contact each other in Fig. 3d due to the deformation
of the nano-rings during the self-assembly, which was also observed in the spin-coated
sample in Fig. 2.
CONCLUSION
The peptide nano-rings containing Au nanoparticles inside their cavities were aligned on
dithiol SAMs patterned as an array by AFM-based nanolithography. The peptide nano-rings
were self-assembled as lines on these SAMs, and Au nanoparticles inside the nano-rings
also formed lines with the spacing between these nanoparticles as the peptide nano-rings
functioned as spacers. This type of fabrication will provide improved tunability in their
optical properties of resulting nanoparticle-assembled arrays. In addition, optimization of the
inter-particle distance of nanoparticles in the array with various spacers may allow one to
design new types of photonics with desired optical properties. However, for those optical
applications, the stability and the rigidity of the nano-rings will be more desirable to be
improved since some of the nano-rings were deformed during the self-assembly and this
deformation caused the uneven spacing of the nanoparticles on the array. For realistic
photonic applications, the nanoparticle assembly needs to be accomplished without
deformation because they require the perfect alignment of nanoparticles with minimum
defects. The additions of hydrogen-bonding functional groups or polymerizing groups to the
monomer may increase the rigidity of the nano-rings, which may help overcome this
problem.
NURAJE et al. Page 4
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
EXPERIMENTAL
Materials
Bis(
N
-α-amido-glycylglycine)-1,7-heptane dicarboxylate was synthesized and recrystallized
in our lab by the published manner [36,37]. 1-Ethyl-3-[3-
(dimethylamino)propyl]carbodiimide hydrochloride (EDAC),
N
-hydroxysuccinimide(NHS),
2-mercaptoethylamine, trimethylphosphinegold chloride, 16-mercaptohexa-decanoic acid
and octadecanothiol from Aldrich. Annealed gold substrates from Molecular Imaging. A
series of trenches (100 nm × 1 µm) were made by shaving the alkylthiol SAM with a Si3N4
tip (Veeco Metrology) of the AFM (Nanoscope IIIa and MultiMode microscope, Digital
Instruments). These trenches were made by customized Nanoscript software
(VeecoMetrology). Formvar Film 200 Mesh Cu TEM grids were obtained from Electron
Microscopy Sciences. UV-Lamp (14 mW/cm2, 254 nm).
Preparation of Peptide Nano-rings
After peptide monomer of bis(
N
-α-amido-glycyl-glycine)-1,7-heptane dicarboxylate, 0.028
g, was dissolved in 10 mL of water and the pH of this solution was adjusted to 5.5 with citric
acid, an excess amount of an organic Au precursor, trimethylphosphinegold chloride
(AuPMe3Cl) was added to this solution. After 5 days in the dark, the peptide nano-rings
were observed in an outer diameter of 50 nm and an inner diameter of 15 nm. The nano-ring
solution was washed with deionized water and centrifuged at 14.5 krpm, and then Au ions
trapped inside the peptide nano-rings were reduced by a UV light (14 mW/cm2, 254 nm) for
20 min. The resulting Au nanoparticles were observed to be about 15 nm in an average
diameter from AFM images.
Nanolithography on Au Substrates
In order to pattern the peptide nano-rings containing Au nanoparticles in their cavities as an
array on Au substrates, an array of dithiolated SAMs was patterned by a cantilever of an
atomic force microscope (AFM) with the following sequence. First, 1-octadecanethiol (0.01
mM) was self-assembled on Au substrates in 99% ethanol at room temperature for 12 h.
Then, an array of trenches (100 nm × 1 µm) was created by removing the alkylthiol SAMs
by the tip of AFM via nanolithography technique [38–40]. On these trenches where Au
surfaces were exposed, 16-mercaptohexa-decanoic acid (0.01 mM) was self-assembled for
overnight. After the resulting substrates were washed by deionized water, the end groups of
the SAMs on trenches were functionalized by thiol via substituting carboxylic acid groups
with thiol groups as shown in Scheme 1. In Scheme 1, 400 µL of ethyl-3-[3-
(dimethylamino)propyl]carbodiimide (EDAC, 75 mM) and 400 µL of
N
-hydroxy
succinimide (NHS, 15 mM) were immersed in aqueous solution containing the
functionalized Au substrates for 30 min. Then, as shown in the step 3 in Scheme 1, 800 µL
of 2-mercaptoethylamine (15 mM,) was incubated in the solution for 24 hrs to modify the
ends groups of the SAMs in trenches to thiol groups [32,41].
NURAJE et al. Page 5
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
Self-assembly of Au Nanoparticle-containing Peptide Nano-rings on Surfaces
When the peptide nano-rings containing Au nanoparticles in their cavities were mixed with
the dithiolated SAM-patterned surfaces in aqueous solution for 8 hrs, the nano-rings were
self-assembled on the trenches with the thiol-Au interaction. After these substrates were
washed with deionized water, the attachment of the peptide nano-rings on the arrayed
trenches was confirmed by AFM. While the height mode of AFM imaging was used to
probe the topology of the nano-ring assembly, the phase mode of AFM imaging was applied
to probe the location of Au nanoparticles since the distinguished hardness of surfaces
between Au nanoparticles and peptide nano-rings allows us to image them respectively in
the trenches.
We also assembled the peptide nano-rings containing Au nanoparticles on TEM grids by
spin-coating to examine whether the nano-rings can be packed on surfaces without
distraction. To obtain smooth surfaces of TEM grids, these grids were fixed on the top of
mica substrates, which were also attached on AFM metal pucks. After the Au nanoparticle-
containing peptide rings were spin-coated on the TEM grids, the resulting coatings were
examined by AFM.
Acknowledgement
This work was supported by the US Department of Energy (DE-FG-02–01ER45935) and the National Science
Foundation CARRER Award (ECS-0103430). Hunter College infrastructure is supported by the National Institutes
of Health, the RCMI program (G12-RR-03037).
References
[1]. Murray CB; Kagan CR; Bawendi MG Annu. Rev. Mater 2000, 30, 545.
[2]. Yablonovitch E Phys. Rev. Lett 1987, 58, 2059. [PubMed: 10034639]
[3]. Joannopoulos JD; Villeneuve PR; Fan SH Nature 1997, 387, 830.
[4]. Vlasov YA; Bo XZ; Sturm JC; Norris DJ Nature 2001, 414, 289–293. [PubMed: 11713524]
[5]. Murray CB; Kagan CR; Bawendi MG Science 1995, 270, 1335.
[6]. Colvin VL MRS Bull 2001, 26, 637.
[7]. Blanco A; Chomski E; Grabtchak S; Ibisate M; John S; Leonard SW; Lopez C; Meseguer F;
Miguez H; Mondia JP; Ozin GA; Toader O; van Driel HM Nature 2000, 405, 437. [PubMed:
10839534]
[8]. Lin SY; Fleming JG; Hetherington DL; Smith BK; Biswas R; Ho KM; Sigalas MM; Zubrzycki W;
Kurtz SR; Bur J Nature 1998, 394, 251.
[9]. Liu X; Fu L; Hong S; Dravid VP; Mirkin CA Adv. Mater 2002, 14, 231.
[10]. Redl FX; Cho KS; Murray CB; O’Brien S Nature 2003, 423, 968. [PubMed: 12827196]
[11]. Lee W; Chan A; Bevan MA; Lewis JA; Braun PV Langmuir 2004, 20, 5262. [PubMed:
15986661]
[12]. Huang J; Kim F; Tao AR; Connor S; Yang P Nature Mater 2005, 4, 896. [PubMed: 16284621]
[13]. Kisailus D; Choi JH; Weaver JC; Yang WJ; Morse DE Adv. Mater 2005, 17, 314.
[14]. Brott LL; Naik RR; Pikas DJ; Kirkpatrick SM; Tomlin DW; Whitlock PW; Clarson SJ; Stone
MO Nature 2001, 413, 291. [PubMed: 11565027]
[15]. Whitling JM; Spreitzer G; Wright DW Adv. Mater 2000, 12, 1377.
[16]. Lee SY; Royston E; Culver JN; Harris MT Nanotechnology 2005, 16, S435. [PubMed:
21727464]
[17]. Douglas T; Young M Adv. Mater 1999, 11, 679.
NURAJE et al. Page 6
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
[18]. Chatterji A; Ochoa WF; Ueno T; Lin TW; Johnson JE Nano Lett 2005, 5, 597. [PubMed:
15826093]
[19]. Walsh D; Arcelli L; Ikoma T; Tanaka J; Mann S Nature Mater 2003, 2, 386. [PubMed: 12764358]
[20]. Sano KI; Sasaki H; Shiba K Langmuir 2005, 21, 3090. [PubMed: 15779989]
[21]. Reches M; Gazit E Science 2003, 300, 625. [PubMed: 12714741]
[22]. Lee SW; Mao CB; Flynn CE; Belcher AM Science 2002, 296, 892. [PubMed: 11988570]
[23]. Gao X; Matsui H Adv. Mater 2005, 17, 2037. [PubMed: 31080317]
[24]. Deng ZX; Mao CD Nano Lett 2003, 3, 1545.
[25]. Park SH; Barish R; Li HY; Reif JH; Finkelstein G; Yan H; LaBean TH Nano Lett 2005, 5, 693.
[PubMed: 15826110]
[26]. Djalali R; Chen Y-F; Matsui HJ Am. Chem. Soc 2002, 124, 13660.
[27]. Sarikaya M; Tamerler C; Jen AKY; Schulten K Nature Mater 2003, 2, 577. [PubMed: 12951599]
[28]. Naik RR; Stringer SJ; Agarwal G; Jones SE; Stone MO Nature Mater 2002, 1, 169. [PubMed:
12618805]
[29]. Yu L; Banerjee IA; Matsui HJ Am. Chem. Soc 2003, 125, 14837.
[30]. Banerjee IA; Yu L; Matsui H Proc. Natl. Acad. Sci. USA 2003, 100, 14678. [PubMed: 14645717]
[31]. Sumerel JL; Yang WJ; Kisailus D; Weaver JC; Choi JH; Morse DE Chem. Mater 2003, 15, 4804.
[32]. Banerjee IA; Yu L; Matsui HJ Am. Chem. Soc 2005, 127, 16002.
[33]. Coffman EA; Melechko AV; Allison DP; Simpson ML; Doktycz MJ Langmuir 2004, 20, 8431.
[PubMed: 15379457]
[34]. Djalali R; Jacopo S; Matsui HJ Am. Chem. Soc 2004, 126, 7935.
[35]. Djalali R; Chen Y-F; Matsui HJ Am. Chem. Soc 2003, 125, 5873.
[36]. Kogiso M; Ohnishi S; Yase K; Masuda M; Shimizu T Langmuir 1998, 14, 4978.
[37]. Matsui H; Gologan BJ Phys. Chem. B 2000, 104, 3383.
[38]. Liu GY; Xu S; Qian YL Accounts Chem. Res 2000, 33, 457.
[39]. Nuraje N; Banerjee IA; MacCuspie RI; Yu L; Matsui HJ Am. Chem. Soc 2004, 126, 8088.
[40]. Zhao Z; Banerjee IA; Matsui HJ Am. Chem. Soc 2005, 127, 8930.
[41]. Frey BL; Corn RM Anal. Chem 1996, 68, 3187.
NURAJE et al. Page 7
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
FIGURE 1.
Illustration of Au nanoparticle-containing peptide nano-ring assembly on the patterned Au
substrate.
NURAJE et al. Page 8
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
FIGURE 2.
(a) TEM image of the peptide nano-ring containing a Au nanoparticle inside the cavity, scale
bar = 50 nm. (b) AFM image of spin-coated peptide nano-rings containing Au nanoparticles
in their cavities on TEM grids in height mode, scale bar = 80 nm (c) AFM image of spin-
coated peptide nano-rings containing Au nanoparticles in their cavities on TEM grids in
phase mode, scale bar = 80 nm (d) the phase AFM phase image in high magnification, scale
bar = 40 nm.
NURAJE et al. Page 9
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
FIGURE 3.
AFM images of Au nanoparticle-containing peptide nano-rings assembled on the dithiol
SAM-patterned in (a) height mode, scale bar = 300 nm (b) phase mode, scale bar = 300 nm
(c) height mode in high magnification, scale bar = 50 nm, (d) phase mode in high
magnification, scale bar = 50 nm.
NURAJE et al. Page 10
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
SCHEME 1.
Fabrication of dithiol SAMs on patterned Au substrates.
NURAJE et al. Page 11
Supramol Chem
. Author manuscript; available in PMC 2019 October 07.
Author Manuscript Author Manuscript Author Manuscript Author Manuscript
... Nanorings are nanoscale circular bands, characterized by varying diameters and thicknesses. Nanorings have been synthesized using both physical (Nuraje et al., 2006;Wu et al., 2016) and chemical synthesis routes Jiang et al., 2004;Kelf et al., 2011;Nuraje et al., 2006). In the chemical realm, Hu et al. used the GRR between silver nanoplates and aqueous HAuCl 4 to form Ag-Au nanorings which were used as colorimetric nanosensors . ...
... Nanorings are nanoscale circular bands, characterized by varying diameters and thicknesses. Nanorings have been synthesized using both physical (Nuraje et al., 2006;Wu et al., 2016) and chemical synthesis routes Jiang et al., 2004;Kelf et al., 2011;Nuraje et al., 2006). In the chemical realm, Hu et al. used the GRR between silver nanoplates and aqueous HAuCl 4 to form Ag-Au nanorings which were used as colorimetric nanosensors . ...
Article
Full-text available
Complex metal nanostructures represent an exceptional category of materials characterized by distinct morphologies and physicochemical properties. Nanostructures with shape anisotropies, such as nanorods, nanostars, nanocages, and nanoprisms, are particularly appealing due to their tunable surface plasmon resonances, controllable surface chemistries, and effective targeting capabilities. These complex nanostructures can absorb light in the near‐infrared, enabling noteworthy applications in nanomedicine, molecular imaging, and biology. The engineering of targeting abilities through surface modifications involving ligands, antibodies, peptides, and other agents potentiates their effects. Recent years have witnessed the development of innovative structures with diverse compositions, expanding their applications in biomedicine. These applications encompass targeted imaging, surface‐enhanced Raman spectroscopy, near‐infrared II imaging, catalytic therapy, photothermal therapy, and cancer treatment. This review seeks to provide the nanomedicine community with a thorough and informative overview of the evolving landscape of complex metal nanoparticle research, with a specific emphasis on their roles in imaging, cancer therapy, infectious diseases, and biofilm treatment. This article is categorized under: Diagnostic Tools > In Vivo Nanodiagnostics and Imaging Therapeutic Approaches and Drug Discovery > Nanomedicine for Infectious Disease Diagnostic Tools > Diagnostic Nanodevices
... In an alternative approach [99], Au NPs were precipitated from AuPMe 3 Cl (Me = methyl) in Au-peptide rings which self-assembled on a lithographically patterned substrate. The outer ring diameter was 50 nm and the inner (NP) diameter was 15 nm (r∼7.5 nm, s∼17.5 nm) which are too large, but the principle of defining the structure by the dimensions of an organic ring, e.g. ...
Article
Full-text available
The structure and basic experimental electrical properties of vacuum evaporated discontinuous (island) metal thin films of discrete metal nanoparticles on insulating substrates are briefly reviewed. Then the widely accepted Neugebauer and Webb (N&W) electrostatically activated electron tunneling conduction model is covered (with enhancements) before the numerous discrepancies between this model and experimental observations are identified, e.g. minimal substrate bias effect, non-linear field distribution, anomalous AC effects, asymmetrical contact effects, and switching. A modified model, based on contact electron injection and extraction, and computer simulations are introduced which explain these discrepancies at a qualitative level. However, quantitative experimental verification of the model is not possible without stable, reproducible films of known structures. The paper concludes with a review of possible preparation techniques which could yield satisfactory samples, especially self-assembly of organically protected metal nanoparticles. One of these has already demonstrated electrostatically activated conduction.
... It has been reported that noble metal NPs stabilized by only weakly bound ligands, such as citrate, will dynamically sorb and desorb proteins stochastically as the biological matrix they are exposed to changes (Cedervall et al. 2007b; Lundqvist et al. 2008; Lynch Tsai et al. 2010). It is also known that the corona of molecules encapsulating either inorganic (MacCuspie et al. 2010b; Voevodin et al. 2007) or biological (Banerjee et al. 2004; MacCuspie et al. 2008a, b; Nuraje et al. 2004 Nuraje et al. , 2006) NPs will affect their physical and biological properties. Thus, to probe the role of AgNP surface capping agents, three biocompatible capping agents were used on AgNPs surfaces including citrate, bovine serum albumin (BSA), and starch. ...
Article
Full-text available
Understanding the colloidal stability of nanoparticles (NPs) plays a key role in phenomenological interpretation of toxicological experiments, particularly if single NPs or their aggregates or agglomerates determine the dominant experimental result. This report examines a variety of instrumental techniques for surveying the colloidal stability of aqueous suspensions of silver nanoparticles (AgNPs), including atomic force microscopy, dynamic light scattering, and colorimetry. It was found that colorimetry can adequately determine the concentration of single AgNPs that remained in solution if morphological information about agglomerates is not required. The colloidal stability of AgNPs with various surface capping agents and in various solvents ranging from cell culture media to different electrolytes of several concentrations, and in different pH conditions was determined. It was found that biocompatible bulky capping agents, such as bovine serum albumin or starch, that provided steric colloidal stabilization, as opposed to purely electrostatic stabilization such as with citrate AgNPs, provided better retention of single AgNPs in solution over a variety of conditions for up to 64h of observation. KeywordsSilver nanoparticles–BSA-coated nanoparticles–Nanomaterial dispersion protocol–Nanomaterial characterization
Article
Bolaamphiphilic molecules with tyrosyl end groups formed interior-filled spherical self-assemblies, which are distinct from the vesicular or tubular structures of other similar peptidic bolaamphiphile assemblies reported in the literature. In this study, the self-assembly mechanism of these tyrosyl bolaamphiphiles was investigated taking into consideration the solvent effects on the molecular interaction forces using molecular modeling. The dissipative particle dynamics simulation of an aqueous tyrosyl bolaamphiphile solution suggested that the interior-filled assemblies were produced by a solvent-regulated assembly of small aggregates of bolaamphiphiles. These small aggregates were generated by hydrophobic interactions at an early stage, and then further assembled to form large spherical assemblies through intermolecular forces, including hydrogen bonds between the intermediate aggregates. Additional experiments and density functional theory calculations based on solvent variations proved that smaller assembled structures could be obtained by disrupting the hydrogen bonds between the intermediates. The assembly mechanism of these peptidic bolaamphiphiles afforded a facile way to create condensed supramolecular structures with controlled sizes.
Article
In this paper, we use molecular dynamics simulations to study the assembly of DNA-grafted nanoparticles to demonstrate specifically the effect of bidispersity in grafted DNA strand length on the thermodynamics and structure of nanoparticle assembly at varying number of grafted single-stranded DNA (ssDNA) strands and number of guanine/cytosine (G/C) bases per strand. At constant number of grafted ssDNA strands and G/C nucleotides per strand, as bidispersity in strand lengths increases, the number of nanoparticles that assemble as well as the number of neighbours per particle in the assembled cluster increases. When the number of G/C nucleotides per strand in short and long strands is equal, the long strands hybridise with the other long strands with higher frequency than the short strands hybridise with short/long strands. This dominance of the long strands leads to bidisperse systems having similar thermodynamics to that in corresponding systems with monodisperse long strands. Structurally, however, as a result of long-long, long-short and short-short strand hybridisation, bidispersity in DNA strand length leads to a broader inter-particle distance distribution within the assembled cluster than seen in systems with monodisperse short or monodisperse long strands. The effect of increasing the number of G/C bases per strand or increasing the number of grafted DNA strands on the thermodynamics of assembly is similar for bidisperse and monodisperse systems. The effect of increasing the number of grafted ssDNA strands on the structure of the assembled cluster is dependent on the extent of strand bidispersity because the presence of significantly shorter ssDNA strands among long ssDNA strands reduces the crowding among the strands at high grafting density. This relief in crowding leads to larger number of strands hybridised and as a result larger coordination number in the assembled cluster in systems with high bidispersity in strands than in corresponding monodisperse or low bidispersity systems.
Article
Given the diverse scientific and technological applications of gold nanoparticles (Au NPs), understanding the impact of macromolecular additives on the distribution of size, shape, and composition is crucial to ensure reproducibility and lower production cost. In situ measurement of the evolution of these distributions challenges current techniques; however, it is critical for in-line manufacturing controls. Using mild Au(I) reduction by tert-butylamine-borane in toluene, the utility and limitations of SAXS, UV/Vis spectroscopy, and TEM are considered by comparing the mean nanoparticle size, size distribution, and relative number density. Individually, these techniques are insufficient to follow these parameters through the initial process of nucleation and growth; either providing insufficient information on the number of particles (UV/Vis), introducing artifacts (TEM), or not providing a unique solution for the shape of the distribution (SAXS). However, when used in conjunction, especially SAXS calibrated with TEM of reaction aliquots, the time evolution of these parameters can be quantified. For the single-phase Au NP synthesis with Au(I) and mild reductants, four distinct experimental regions are revealed that entail two growth mechanisms, which complement previous discussions of single-mode growth kinetics. The kinetics of Au(I):borane reactions are dependent on the Au precursor/reductant ratio and the thiol capping agent length, when reductant concentration is low. The final reaction products exhibit an LSW size distribution.
Article
In this review, the main concept of ferroelectricity of perovskite oxides and related materials at nanometer scale and existing difficulties in the synthesis of those nanocrystals are discussed. Important effects, such as depolarization field and size effect, on the existence of ferroelectricity in perovskite nanocrystals are deliberated. In the discussion of modeling works, different theoretical calculations are pinpointed focusing on their studies of lattice dynamics, phase transitions, new origin of ferroelectricity in nanostructures, etc. As the major part of this review, recent research progress in the facile synthesis, characterization and various applications of perovskite ferroelectric nanomaterials, such as BaTiO3, PbTiO3, PbZrO3, and BiFeO3, are also scrutinized. Perspectives concerning the future direction of ferroelectric nanomaterials research and its potential applications in renewable energy, etc., are presented. This review provides an overview in this area and guidance for further studies in perovskite ferroelectric nanomaterials and their applications.
Article
Macroscopic assemblies of nanoparticles with fluid like characteristics, i.e. nanoparticle liquids (NPLs), are a new class of materials that exhibit unique properties compared with dispersions of nanoparticles in a molecularly distinct matrix phase. By focusing on reaction ratios, techniques to maximize concentration of reactants and quantification of chemical content during washing steps, a high degree of control over the purity of NPLs was maintained while allowing for easy scalability in batch sizes and synthesis throughput. A range of tertiary amines and quaternary ammoniums were used to successfully synthesize Au NPLs from a range of Au nanoparticles with nominal diameters from 6 to 20 nm and initially stabilized with either citrate or dodecanethiol. Stable Au NPLs after purification exhibited a sub-equivalence ratio of canopy to ligand molecules within the corona. This small canopy density most likely arose from the incommensurate areal density of anionic charge within the ligand shell relative to the larger size of the cationic canopy molecule, resulting in a population of cation–anion pairs too weakly bound to be retained in the initial assembly of the canopy post-purification. Finally, increasing either the volume fraction or molecular weight of the canopy was found to increase exponentially the electrical resistance of the bulk NPLs. Removal of excess canopy molecules created a conductive Au NPL that improved hot-current switching durability by at least two orders of magnitude beyond prior reports. Published in 2010 by John Wiley & Sons, Ltd.
Article
Full-text available
Solution phase syntheses and size-selective separation methods to prepare semiconductor and metal nanocrystals, tunable in size from similar to 1 to 20 nn acid monodisperse to less than or equal to 5% are presented. Preparation of monodisperse samples enables systematic characterization of the structural, electronic, and optical properties of materials as they evolve from molecular to bulk in the nanometer size range. Sample uniformity makes it possible to manipulate nanocrystals into close-packed, glassy, and ordered nanocrystal assemblies (superlattices, colloidal crystals, supercrystals). Rigorous structural characterization is critical to understanding the electronic and optical properties of both nanocrystals and their assemblies. At inter-particle separations 5-100 Angstrom, dipole-dipole interactions lead to energy transfer between neighboring nanocrystals, and electronic tunneling between proximal nanocrystals gives rise to dark and photoconductivity. At separations <5 Angstrom, exchange interactions cause otherwise insulating assemblies to become semiconducting, metallic, or superconducting depending on nanocrystal composition. Tailoring the size and composition of the nanocrystals and the length and electronic structure of the matrix may tune the properties of nanocrystal solid-state materials.
Article
Full-text available
The ability to confine and control light in three dimensions would have important implications for quantum optics and quantum-optical devices: the modification of black-body radiation, the localization of light to a fraction of a cubic wavelength, and thus the realization of single-mode light-emitting diodes, are but a few examples. Photonic crystals - the optical analogues of electronic crystal - provide a means for achieving these goals. Combinations of metallic and dielectric materials can be used to obtain the required three-dimensional periodic variations in dielectric constant, but dissipation due to free carrier absorption will limit application of such structures at the technologically useful infrared wavelengths. On the other hand, three-dimensional photonic crystals fabricated in low-loss gallium arsenide show only a weak `stop band' (that is, range of frequencies at which propagation of light is forbidden) at the wavelengths of interest. Here we report the construction of a three-dimensional infrared photonic crystal on a silicon wafer using relatively standard microelectronics fabrication technology. Our crystal shows a large stop band (10-14.5μm), strong attenuation of light within this band (~12dB per unit cell) and a spectral response uniform to better than 1 per cent over the area of the 6-inch wafer.
Article
Full-text available
The self-organization of CdSe nanocrystallites into three-dimensional semiconductor quantum dot superlattices (colloidal crystals) is demonstrated. The size and spacing of the dots within the superlattice are controlled with near atomic precision. This control is a result of synthetic advances that provide CdSe nanocrystallites that are monodisperse within the limit of atomic roughness. The methodology is not limited to semiconductor quantum dots but provides general procedures for the preparation and characterization of ordered structures of nanocrystallites from a variety of materials.
Article
Full-text available
Photonic technology, using light instead of electrons as the information carrier, is increasingly replacing electronics in communication and information management systems. Microscopic light manipulation, for this purpose, is achievable through photonic bandgap materials, a special class of photonic crystals in which three-dimensional, periodic dielectric constant variations controllably prohibit electromagnetic propagation throughout a specified frequency band. This can result in the localization of photons, thus providing a mechanism for controlling and inhibiting spontaneous light emission that can be exploited for photonic device fabrication. In fact, carefully engineered line defects could act as waveguides connecting photonic devices in all-optical microchips, and infiltration of the photonic material with suitable liquid crystals might produce photonic bandgap structures (and hence light-flow patterns) fully tunable by an externally applied voltage. However, the realization of this technology requires a strategy for the efficient synthesis of high-quality, large-scale photonic crystals with photonic bandgaps at micrometre and sub-micrometre wavelengths, and with rationally designed line and point defects for optical circuitry. Here we describe single crystals of silicon inverse opal with a complete three-dimensional photonic bandgap centred on 1.46 microm, produced by growing silicon inside the voids of an opal template of dose-packed silica spheres that are connected by small 'necks' formed during sintering, followed by removal of the silica template. The synthesis method is simple and inexpensive, yielding photonic crystals of pure silicon that are easily integrated with existing silicon-based microelectronics.
Article
Virus protein cages, capsids, which display a wide range of sizes and shapes, can be used for constrained materials synthesis. The authors briefly review recent work involving capsids, including the use of spherical viruses for inorganic mineralization and organic polymer encapsulation and the mineralization of anisotropic structures such as the tobacco mosaic virus, which can lead to mineralized fibers of iron oxide or silica with very high aspect ratios. The topic of gating—which enables the selective entrapment and release of materials from within the central cavity—is briefly touched upon.
Article
Technical Feature From Opals to Optics: Colloidal Photonic Crystals • Article author query • colvin vl [Google Scholar] Vicki L. Colvin Over a decade ago, theorists predicted that photonic crystals active at visible and near-infrared wavelengths would possess a variety of exciting optical properties. Only in the last several years, however, have experimentalists begun to build materials that realize this potential in the laboratory. This lag between experiment and theory is primarily due to the to the challenges associated with fabricating these unique materials. As the term “crystal” suggests, these samples must consist of highly perfect ordered arrays of solids. However, unlike conventional crystals, which exhibit order on the angstrom length scale, photonic crystals must have order on the submicrometer length scale. In addition, many of the most valuable properties of photonic crystals are only realized when samples possess a “full” photonic bandgap. For such systems, large dielectric contrasts and particular crystal symmetries create a range of frequencies over which light cannot propagate. Realizing the nanoscopic architectures required to form such systems is a challenge for experimentalists. As a result, fabrication schemes that rely on lithographic techniques or spontaneous assembly have been a focus in the development of the field.
Article
The stabilization of size-specific monodisperse CdS nanoclusters has received much attention. However, the development of matrices, e.g., polymers, micelles, zeolites, for this purpose has remained largely empirical. Here a combinatorial and informatics approach to the discovery of ligands for CdS nanocluster stabilization is introduced. It is shown that combinatorially derived peptide and peptidomimetic ligands based on phytochelatins can stabilize CdS nanoclusters and that an informatics analysis of the library used yields design parameters critical for obtaining second-generation ligands.
Article
Research News: Virus protein rages, capsids, which display a wide range of sizes and shapes, can be used for constrained materials synthesis. The authors briefly review recent work involving capsids, including the use of spherical viruses for inorganic mineralization and organic polymer encapsulation and the mineralization of anisotropic structures such as the tobacco mosaic virus, which can lead to mineralized fibers of iron oxide or silica with very high aspect ratios. The topic of gating-which enables the selective entrapment and release of materials from within the central cavity-is briefly touched upon.
Article
The assembled structure of the heptane bolaamphiphile, bis(N-alpha-amido-glycylglycine)-1,7-heptane dicarboxylate, displays a sensitivity to the acidity of a solution. At pH 4, the heptane bolaamlihiphile grows to a crystalline tubule in two weeks. At pH 8, a helical ribbon structure is formed in one week. The degree of carboxylic acid protonation was used to control the final assembled structures since the structures are determined by the strengths of the amide-amide and carboxylic acid dimer hydrogen bonds. Direct structural transformation between tubules and helical ribbons was also confirmed as a function of pH using optical microscopy and Raman microscopy. Conversion from the helical ribbons to the tubules occurs within one day, while the reverse conversion, from the tubules to the helical ribbons, is ten times slower.
Article
This Account focuses on our recent and systematic effort in the development of generic scanning probe lithography (SPL)-based methodologies to produce nanopatterns of self-assembled mono- layers (SAMs). The key to achieving high spatial precision is to keep the tip-surface interactions strong and local. The approaches used include two AFM-based methods, nanoshaving and nanografting, which rely on the local force, and two STM-based techniques, electron-induced diffusion and desorption, which use tunneling electrons for fabrication. In this Account we discuss the principle of these procedures and the critical steps in controlling local tip- surface interactions. The advantages of SPL will be illustrated through various examples of production and modification of SAM nanopatterns and their potential applications.