Sulfate-Mediated End-to-End Assembly of Gold Nanorods - Langmuir

Jan 18, 2017 - Link , S.; El-Sayed , M. A. Shape and size dependence of radiative, non-radiative and photothermal properties of gold nanocrystals Int...
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Sulfate Mediated End-to-End Assembly of Gold Nanorods Seyyed Mohammad Hossein Abtahi, Nathan D. Burrows, Fred A. Idesis, Catherine J. Murphy, Navid B. Saleh, and Peter J. Vikesland Langmuir, Just Accepted Manuscript • DOI: 10.1021/acs.langmuir.6b04114 • Publication Date (Web): 18 Jan 2017 Downloaded from http://pubs.acs.org on January 25, 2017

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Sulfate Mediated End-to-End Assembly

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of Gold Nanorods

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S.M.H. Abtahi,1, 2, 3 Nathan D. Burrows,4 Fred A. Idesis,4 Catherine J. Murphy,4

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Navid B. Saleh,5 and Peter J. Vikesland*1, 2, 3 1.

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Blacksburg, VA, USA

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2.

Virginia Tech, Institute for Critical Technology and Applied Science (ICTAS) Center for Sustainable Nanotechnology (VTSuN), Blacksburg, VA, USA

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3.

Center for the Environmental Implications of Nanotechnology (CEINT), Duke University, Durham, NC, USA

11 4.

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Department of Chemistry, University of Illinois at Urbana-Champaign, 600 S. Matthews Ave., Urbana, IL, 61801, USA

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Virginia Tech, Department of Civil and Environmental Engineering,

5.

The University of Texas at Austin, Department of Civil, Architectural and Environmental Engineering, Austin, TX 78712, USA

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Abstract

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There is interest in the controlled aggregation of gold nanorods (GNRs) for the

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production of extended nanoassemblies. Prior studies have relied upon chemical

21

modification of the GNR surface to achieve a desired final aggregate structure. Herein,

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we illustrate that control of electrolyte composition can facilitate end-to-end assembly of

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cetyltrimethylammonium bromide (CTAB) coated GNRs. By adjusting either the sulfate

24

anion concentration or the exposure time it is possible to connect GNRs in chain-like

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assemblies. In contrast, end-to-end assembly was not observed in control experiments

26

using monovalent chloride salts. We attribute the end-to-end assembly to the localized

27

association of sulfate with exposed quaternary ammonium head groups of CTAB at the

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nanorod tip. To quantify the assembly kinetics, visible-near infrared extinction spectra

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were collected over a pre-determined time period and the colloidal behavior of the GNR

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suspensions was interpreted using plasmon band analysis. Transmission electron

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microscopy and atomic force microscopy results support the conclusions reached via

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plasmon band analysis and the colloidal behavior is consistent with Derjaguin-Landau-

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Verwey-Overbeek (DLVO) theory.

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Introduction

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Gold and silver nanoparticles are of interest because of the unique electro-optical

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properties (e.g., localized surface plasmon resonance [LSPR])1-5 that originate from the

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collective behavior of their surface electrons. In the case of LSPR, visible-infrared light

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interacts with a noble metal nanoparticle smaller than the incident radiation wavelength1,

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6

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conduction band electrons. The LSPR is a function of the local dielectric environment as

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well as the size and shape of the nanoparticle.1,

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extinction spectrum at the wavelength where the frequency of the incident light matches

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the frequency at which the conduction electrons oscillate.1,

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dependent on nanoparticle size and shape and shifts to longer wavelengths with an

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increase in particle size.14-16 Anisotropic nanoparticles, such as gold nanorods (GNRs),

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exhibit two different plasmon oscillations: one along the short axis (the transverse

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oscillation) and the other along the long axis (the longitudinal oscillation).5, 17-21 Each of

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these oscillations exhibits its own specific LSPR band. The transverse LSPR band

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typically occurs at a wavelength between 500-550 nm and shifts to longer wavelengths

50

with an increase in diameter. The longitudinal LSPR band is aspect ratio (AR:

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length/diameter) sensitive, and occurs at longer wavelengths for GNRs with higher

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AR.19, 22, 23 The extinction (absorbance + scattering) of these peaks is linearly related to

and resonant interactions result in the coherent oscillation of the nanoparticle's

2, 7-12

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A peak is observed in the

6, 8, 13

Peak location is

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the concentration of nanoparticles in suspension. Changes in the number concentration,

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the AR, or the local dielectric environment can be detected by a change in extinction or

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by the shift of these two plasmon peaks.14, 24

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The electro-optical properties of GNRs can be significantly altered by nanoparticle

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assembly. We use the term controlled assembly to refer either to end-to-end, end-to-

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side, or side-by-side assembly.25,

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plasmon preferentially and are of particular interest for sensing technologies that rely on

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large electric fields.26-28 Extended end-to-end GNR assemblies have previously been

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produced by manipulation of GNR surface chemistry,29-32 by alteration of the chemistry

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of the solution in which the GNRs are suspended,13, 30, 33, 34 by applying polystyrene and

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surface enhanced Raman spectroscopy (SERS) markers,35 or by attachment of pH-

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responsive DNA36 to the GNR surface. Side-by-side assemblies of GNRs have been

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prepared by cysteine conjugated GNRs in the presence of lead37 and in adiptic acid

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treated GNR suspensions.38 Interchangeable end-to-end and side-by-side assemblies

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of GNRs have been prepared by addition of tetrahydrofuran,39 dithiol polyethylene

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glycol,40 bifunctional poly(ethylene glycol, PEG),26 or antibodies,25 onto GNR surfaces

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where the final assembled configuration is controlled by the concentration of the organic

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molecule. Each of these approaches requires extensive nanoparticle functionalization.

26

End-to-end assemblies couple the longitudinal

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In this work, we illustrate a simple method in which sulfate ions are used to facilitate

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end-to-end GNR assembly in aqueous suspension. The coordinating activity of sulfate

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anions enables conversion of >80% of well-dispersed GNRs in a suspension into

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extended structures (chains of dimers, trimers, tetramers, etc.). For these experiments

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we used cetyltrimethylammonium bromide capped GNRs (CTAB-GNRs) because CTAB

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is the de facto GNR capping agent in GNR synthesis5, 18, 41-44. Visible-near infrared (Vis-

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NIR) extinction spectra were collected over a pre-determined time period and the

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colloidal behavior of the GNR suspensions was interpreted using plasmon band

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analysis. Transmission electron microscopy (TEM) and atomic force microscopy (AFM)

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were used to further characterize the samples. These results are self-consistent and

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can be explained by Derjaguin-Landau-Verwey-Overbeek (DLVO) theory.

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Materials and Methods

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Preparation of CTAB-coated GNRs

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GNRs were synthesized via the well-established seed-mediated surfactant-directed

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method.45, 46 In brief, 3-4 nm spherical gold nanoparticle seeds were produced through

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the reduction of chloroauric acid (HAuCl4•3H2O, 2.5×10-4 M in aqueous solution) in the

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presence of CTAB ([CH3(CH2)15N(CH3)3]+Br-, 0.10 M) by addition of ice-cooled and

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freshly prepared sodium borohydride (NaBH4, 0.010 M). A rapid color change to light

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brown indicated seed formation. In the next step, GNRs of aspect ratio 4.4 were grown

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from an aqueous growth solution consisting of 0.10 M CTAB, 5.0×10-4 M HAuCl4,

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8.0×10-5 M AgNO3, and 5.5×10-4 M ascorbic acid, which became colorless upon acid

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addition. Once the gold seeds were added to the growth solution, it changed color to

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dark brown over 1-2 h indicating GNR formation. Spheres, cubes, and other shaped

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byproducts

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centrifugation (25 min at 8000 rcf), repeated 5 times with pellet resuspension in 800 µM

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CTAB, yielding CTAB-GNRs. ICP-MS measurements indicated that the GNR stock had

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a 41.0±0.3 mg/L atomic gold concentration. Accordingly, a concentration of 2.1×1014

(minor

component)

and

chemical

byproducts

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removed

by

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GNRs/L was calculated based on the density of gold (19.3 g/cm3)47 and the TEM

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determined average GNR size of 28.8 ± 0.1 nm length and 6.6 ± 0.1 nm diameter.

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End-to-end linkage of CTAB-GNRs in CaSO4 and MgSO4

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Suspensions of CTAB-GNRs (1.1×1014 GNRs/L) were incubated over a range of

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CaSO4 and MgSO4 concentrations (1-5 mM) for 24 h. To initiate an experiment, CTAB-

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GNRs were washed by centrifugation (20 min at 11000 rcf) and 90% of the supernatant

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was replaced with DI water, followed by bath sonication for 1 min. The resuspended

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GNRs were readily dispersed and were colloidally stable. This step removed excess

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CTAB from the GNR suspension. Following a second centrifugation step (20 min at

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11000 rcf), 90% of the supernatant was replaced with a given CaSO4 or MgSO4 solution

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followed by 1 min of bath sonication. The GNR suspensions were then transferred to

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Vis-NIR cuvettes that were used for colloidal stability monitoring over 24 h. During the

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first hour, 10 min sampling intervals were used. Subsequently, one-hour intervals were

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used for the remaining 23 h. Vis-NIR extinction spectra were collected between 400-

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1200 nm. TEM samples were prepared after 3 and 10 h of exposure to salt solutions. To

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quantitatively capture the temporal changes in the extinction of the GNR suspensions,

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individual peaks within the Vis-NIR spectrum were fit with Lorentzian distributions48,

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using Grams/AI software (Thermo-Fisher, Waltham, MA).

49

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TEM samples were prepared by submerging 200 mesh carbon film coated copper

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grids in a given GNR suspension and then fast dried by putting the grid on top of an

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80 °C hot plate for 10 s. An AFM sample was prepared following 3 h GNR exposure to

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salt solutions. Negatively charged AFM metal specimen discs were submerged

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vertically in a petri dish containing 5 mL GNR suspension sample for half an hour

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followed by DI water rinsing prior to AFM measurement.

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Instrumentation

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An Agilent Cary 5000 spectrometer (Santa Clara, CA) and disposable polystyrene

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cuvettes (10 mm pathlength) were used for Vis-NIR extinction spectroscopy. TEM

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images were taken using a Philips (Thermo-Fisher, Waltham, MA) EM420 conventional

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transmission electron microscope. A Malvern (Worcestershire, UK) Zetasizer Nano-ZS

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was used for electrophoretic mobility measurements. A Bruker (Billerica, MA)

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Nanoscope IIIa AFM and Ted Pella (Redding, CA) 15 mm metal specimen discs were

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used for atomic force microscopy. Sonication was performed using a Fisher Scientific

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FS20H bath sonicator. DI water (18.2 MΩ) was produced by a Thermo Scientific

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Barnstead nanopure system.

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Results and Discussion

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GNR characterization

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The GNRs were characterized via TEM, Vis-NIR spectroscopy, electrophoretic

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mobility, and ICP-MS measurements. The GNRs (inset to Figure 1; Figure S1) have an

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average length of 28.8 ± 0.1 nm and an average diameter of 6.6 ± 0.1 nm (the noted

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errors reflect 95% confidence interval based on n = 2104 measurements obtained using

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ImageJ). These relative dimensions result in an average AR of 4.4 ± 0.1. These GNRs

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exhibit a transverse extinction band at 518 nm and a longitudinal band at 756 nm, which

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are the expected wavelengths for GNRs of these dimensions.45 The electrophoretic

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mobility of the GNRs in DI water was determined to be +3.58 µm•cm/V•s. Applying

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Henry’s equation while considering Smoluchowski equation for Henry’s constant

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resulted in calculated ζ-potential of +45.6 mV. We note that for the GNRs and the

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range of ionic strengths tested in this study,

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the nanoparticle effective diameter in nm) varies from 4.09 to 9.13. Because

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the Smoluchowski equation is an acceptable approximation of ζ-potential (details and

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example calculations are presented in SI; pages 2-3).50,

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consistent with the literature and illustrate that the rods have a positive effective surface

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charge.44, 51

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Figure 1. Vis-NIR extinction spectrum for the synthesized CTAB-GNRs after centrifugal purification and washing. Inset: Transmission electron micrograph of CTABGNRs.

ૂa (ૂ is 1/Debye length in 1/nm and “a” is

51, 52

ૂa>>1,

These values are

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End-to-end assembly of CTAB-coated gold nanorods in CaSO4 and MgSO4

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The in situ development of GNR assemblies was probed via Vis-NIR extinction

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spectroscopy. It has been shown previously that during side-to-side and end-to-side

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assemblies, the extinction of the initial transverse LSPR band increases and the band

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slightly red shifts to higher wavelengths; while the extinction of the longitudinal band

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decreases and blue shifts to lower wavelengths, thus resulting in the convergence of the

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two bands.26 The calculated change in extinction intensity versus the incident light

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wavelength and the corresponding transverse and longitudinal bands of these two

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assemblies are presented in Table S3 and Figure S6. These calculations were

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developed based on our experiment parameters, while employing extended Mie theory

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modeling. In end-to-end assembly the bands behave quite differently. For aggregates

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with this configuration, neither the transverse nor the longitudinal band shifts; however,

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the extinction of the longitudinal band significantly decreases as the total average length

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of the GNR chain increases. Under these conditions, a third plasmon band appears at

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wavelengths larger than that of the original longitudinal band (Figure S5). Because of

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extended plasmonic coupling this new plasmon band red shifts to longer and longer

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wavelengths as the GNR chain length increases.22, 26, 53-55

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To evaluate the aggregation behavior of the GNRs, CTAB-GNR suspensions were

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exposed to 1, 2, and 5 mM CaSO4 or MgSO4. We observed salt concentration

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dependent changes in the visual characteristics of the suspensions. In the presence of

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DI water the suspension is brownish in color, while at higher salt concentrations the

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color darkens. At a salt concentration of 5 mM the colloidal stability of the suspension

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was lost within 24 h (Figure S2). As illustrated in representative plots for 2 mM CaSO4

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and 2 mM MgSO4 (Figure 2) there are readily observable declines in the intensities of

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both the transverse and longitudinal bands and additional bands appear at longer

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wavelengths. Such behavior is consistent with the previously described end-to-end

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aggregation process.

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concentrations.

Qualitatively similar results were observed at the other salt

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To quantify the declines in peak intensity we plotted the change in extinction for

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both the transverse and longitudinal bands for each salt concentration. As shown in

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Figure 2C-F, a sharp drop in the longitudinal peak intensity was observed within the first

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hour of exposure of the GNRs to all concentrations of CaSO4 and MgSO4, accompanied

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by a slower decrease in intensity over the next 23 h. In contrast, the transverse band

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intensity did not change as noticeably. To interpret the temporal changes in the

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longitudinal and transverse bands we fitted our collected data using a simple second

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order aggregation model56, 57 (details are presented in the SI; page 4):

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ௗ[௥௢ௗ] ௗ௧

= −݇[‫]݀݋ݎ‬ଶ

(1)

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Where [rod] is the number concentration of individual, fully dispersed rods and k is the

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observed second order rate constant. Other more complex aggregation models may be

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more appropriate for this system due to its complexity; however, our purpose in using

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this model is to capture the differential behavior of the two extinction bands. Number

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concentration-based rate constants and associated 95% confidence intervals for single

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CTAB-GNRs in the presence of CaSO4 and MgSO4 are presented in Table 1. We note

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that for 5 mM CaSO4 the second order model did not fit the collected data as well as it

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did for other experimental conditions. We attribute this behavior to the more rapid

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aggregation observed with CaSO4 and the greater degree of colloidal instability.

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Figure 2. Vis-NIR extinction spectra of 1.1×1014 GNRs/L exposed to A) 2 mM CaSO4 and B) 2 mM MgSO4 from zero hours (red spectra) to 24 hours (blue spectra). Changes in the average normalized transverse band and longitudinal band extinction maxima of CTAB-GNRs (1.1×1014 GNRs/L) in 1-5 mM CaSO4 and MgSO4 solutions as a function of exposure time. (C) Transverse band-CaSO4 (D) Longitudinal band-CaSO4 (E) Transverse band-MgSO4 (F) Longitudinal bandMgSO4.

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Table

1.

Second

order

number

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concentration

rate

constants

L ) for single CTAB-GNRs in the presence of different 1.07 × 10 ( goldnanoro ds ). S concentrations of CaSO4 and MgSO4. Both the changes in the transverse band and the longitudinal band are provided. Errors are reported at the ±95% confidence intervals.

(

14

Salt Concentration (mM) 1 2 5

Transverse band CaSO4 MgSO4 0.0006 ± 0.0001 0.0007 ± 0.0001 0.0065 ± 0.0000 0.0032 ± 0.0001 0.22 ± 0.049 0.012 ± 0.0006

Longitudinal band CaSO4 MgSO4 0.025 ± 0.0020 0.019 ± 0.0021 0.05 ± 0.0051 0.028 ± 0.0026 0.49 ± 0.072 0.051 ± 0.0053

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An increase in ionic strength significantly increased the rate at which the GNRs

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assembled. In all cases, the rate of change of the longitudinal band was greater than

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that of the transverse band (Table 1). Over the 24 h period that the GNRs were exposed

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to 1 mM and 2 mM of CaSO4 and MgSO4 there was minimal change in the transverse

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band intensity, while simultaneously there was a 40-60% decline in the longitudinal

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band intensity. If the assemblies were colloidally unstable and were precipitating out of

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suspension and leaving only single GNRs behind then the rate constants for the change

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in the transverse and longitudinal bands of single GNRs should be equal (Table S1 and

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Figure S3). However, the much slower change in the transverse band relative to the

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longitudinal band supports the conclusion that the GNRs are assembling into extended

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structures. In end-to-end nanoparticle assembly the transverse band is not expected to

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shift, while the longitudinal band will decrease in intensity and red-shift.

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Following exposure of the GNRs to CaSO4 or MgSO4 a new shoulder with an

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extinction maximum at a wavelength greater than the longitudinal band appears. The

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intensity of this shoulder increases and red-shifts to longer wavelengths over time and

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at increased salt concentrations.

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assembly of GNRs to produce new structures with elongated AR (i.e., end-to-end

Formation of this shoulder is consistent with the

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assemblies). Past studies have illustrated that chain-like assemblies of GNRs display

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the formation of an extinction band at longer wavelengths compared to individual

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rods.25, 26, 30, 34 The peak wavelength is strongly related to the number of linked rods and

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shifts to longer wavelengths as the chains become increasingly extended over time.

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TEM and AFM images consistent with formation of end-to-end assemblies are

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shown in Figure 3. Both the TEM and AFM images illustrate the formation of end-to-end

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linkages. The AFM images unlike the TEM images were collected in situ without sample

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drying. Observation of an extended end-to-end assembly in the AFM image supports

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the argument that the presence of these assemblies in the TEM images is not

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necessarily a result of drying mediated artifacts. TEM images taken at different times

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and salt concentrations suggest that the end-to-end chains of GNRs grow longer over

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time and with an increase in ionic strength (Figure 3B-C, Figure S4).

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A

B

C

50 nm 244 245 246 247

Figure 3. A) Representative AFM image of CTAB-GNRs after 3 h exposure to 2 mM CaSO4, B) TEM image of CTAB-GNRs after 3 h exposure to 2 mM CaSO4, C) TEM image of CTAB-GNRs after 10 h exposure to 2 mM CaSO4.

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Extinction spectra peak fitting Prior studies have established that there is a linear relationship between the peak

250 251

wavelength location and AR.22,

58

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assemblies of different length can be estimated by application of extended Mie theory

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(see SI for details).22, 58-61 Knowing the physical and chemical properties of the GNRs

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and the solution chemistry employed herein, we were able to calculate the expected

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location of the extinction band for each end-to-end configuration (see SI for details of

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calculations). Our GNRs have an AR of 4.4, therefore the calculated λmax values for

257

dimer (AR=8.8), trimer (AR=13.2), and tetramer (AR=17.6) end-to-end linked AuNRs

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are 860, 965, and 1070 nm, respectively (Figure 4A). These values are qualitatively

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similar to those theoretically calculated for end-to-end assemblies of GNRs of similar

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AR.

Theoretical peak wavelengths for end-to-end GNR

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Figure 4. A) Plasmon band wavelengths of different GNR end-to-end assemblies as calculated by extended Mie theory. B) Exemplary figure illustrating quality of fit for experimental vs. fitted Vis-NIR spectrum for GNRs exposed to 5 mM MgSO4 after 1 hr. The magnitudes of individual extinction bands are illustrated.

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Based upon these wavelengths we used a non-linear least squares iterative62

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procedure (within GRAMS/AI) to fit the collected Vis-NIR spectra for each experiment as

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the summation of five separate Lorentzian bands that correspond to the transverse

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band and the longitudinal band for single, dimer, trimer, and tetramer GNRs. The

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Lorentzian distribution can be explained as a Fourier-transform of exponentially

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decaying oscillations63. We used extended Mie theory modeling to calculate the change

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in extinction intensity versus the incident light wavelength and to locate the plasmon

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bands of different end-to-end assemblies as has been done previously22 (refer to SI

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page 7 for calculation details). As a result, Lorentzian distributions were used for curve

277

fitting. In this exercise, the center of each peak is fixed while the amplitude (height) and

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width are unknown parameters. Using this constrained fitting approach, we are able to

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fit and reproduce the collected Vis-NIR spectra quite readily (Figure 4B). By fitting each

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of the spectra collected over the course of an experiment we can probe the relative

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numbers of single, dimer, trimer, and tetramer assemblies present at any time. Figure 5

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illustrates the temporal changes in each Lorentzian distribution band for the CaSO4

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experiments, while the results for the MgSO4 experiments are shown in Figure S7.

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Figure 5: Extinction intensities of different Lorentzian distribution band end-to-end assemblies of GNRs exposed to three different CaSO4 concentrations A) Transverse bands of single rod B) Longitudinal bands of single rod C) Longitudinal bands of dimer D) Longitudinal bands of trimer E) Longitudinal bands of tetramer

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With an increase in salt concentration increasing numbers of GNRs participate in

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end-to-end assembly and there is a concomitant decrease in the extinction of the

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longitudinal band that represents single GNRs (Figure 5B). At 1 and 2 mM CaSO4, the

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extinction of the dimer band at 860 nm increases rapidly and then plateaus, while at 5

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mM it increases and then decreases with time (Figure 5C). At 5 mM CaSO4, the dimer,

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trimer, and tetramer extinction intensities rapidly increase but then decrease over

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extended time. These results collectively show that at high salt concentrations the end-

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to-end GNRs assemblies that are formed initially, grow further to be colloidally unstable,

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and finally undergo precipitation. This precipitation trend is consistent with visual

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observation of large dark pellets at the bottom of the sample cuvette (Figure S2).

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The validity of our curve fitting technique was studied by analyzing 36 TEM images

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taken from one sample (GNRs exposed to 2 mM CaSO4) at three different time periods

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(3, 10, and 24 h). A total of 270 GNRs were counted via TEM image analysis. Figure 6

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shows the change in percentage of these assemblies as a function of time. As

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expected, the length of the end-to-end assemblies generally increase over time. As an

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example, after 3 h almost 50% of GNRs are in the dimer form and no tetramers were

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found; but after 24 h 50% of GNRs are in the tetramer form while only 12% single GNRs

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were observed. Because of the potential for drying mediated artifacts and the potential

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effects of the TEM substrate on aggregate formation the results presented in Figure 6

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cannot be directly compared to the plasmon band analyses; however, the general trend

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is the same with longer and longer assemblies forming with extended time.

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Figure 6. Percentage of GNRs forming different end-to-end assemblies. Analysis of 36 TEM images taken from GNRs exposed to 2 mM CaSO4 at three different time periods. Representative TEM images are shown Figure S4.

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Anion identity and valence dictate assembly

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Past studies have suggested that CTAB forms a dense 3.5 nm thick vesicle-like

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bilayer on the GNR side facets, while it may not fully coat the ends.44, 64, 65 The presence

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of the positively charged vesicle-like bilayer around the side facets protects the GNRs

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from undergoing side-by-side aggregation. To investigate the chemistry underlying the

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observed end-to-end assembly we exposed CTAB-GNRs to CaCl2, MgCl2, NaCl, and

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Na2SO4 salts at the same ionic strength used in the CaSO4 and MgSO4 experiments.

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The collected Vis-NIR extinction spectra over a period of 24 h are shown in Figures S8

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and S9. The decline in the transverse and longitudinal absorption bands is shown in

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Figures S10 and S11.

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No change in the extinction of the transverse band, a