Quantized Double-Layer Charging of Highly Monodisperse
Metal Nanoparticles
Jocelyn F. Hicks,
†
Deon T. Miles,
‡
and Royce W. Murray*
Contribution from the Kenan Laboratories of Chemistry, UniVersity of North Carolina CB#3290,
Chapel Hill, North Carolina 27599-3290
Received July 16, 2002
Abstract: We describe unprecedented resolution of electrochemically observed quantized double layer
(QDL) charging, attained with use of reduced solution temperatures and with an annealing procedure that
produces hexanethiolate monolayer protected gold clusters (C6 MPCs) with a high level of monodispersity
in charging capacitance, CCLU. The spacing ΔV ) e/CCLU on the electrochemical potential axis between
one electron changes in the electronic charge of nanoscopic metal particles is determined by their effective
capacitance CCLU. The high monodispersity of the C6 MPCs with Au140 cores facilitates (a) detailed rotated
disk and cyclic voltammetric measurements, (b) simulation of QDL waveshapes based on assumed
reversible, multivalent redox-like behavior, (c) determination of nanoparticle diffusion rates, and (d)
observation of as many as 13 changes in the MPC charge state, from MPC
6-
to MPC
7+
. The single electron
QDL charging peaks are quite evenly spaced (ΔV constant) at potentials near the MPC potential of zero
charge, but are irregularly spaced at more positive and negative potentials. The irregular spacing is difficult
to rationalize with classical double layer capacitance ideas and is proposed to arise from a correspondingly
structured (e.g., not smooth) density of electronic states of the nanoparticle core, resulting from its small
HOMO/LUMO gap and incipiently molecule-like behavior.
Introduction
Monolayer-protected gold clusters (MPCs) are nanoparticles
coated with dense, protecting monolayers of organothiolate,
1
organophosphine,
2
or organoamine ligands.
3
The thiolate mono-
layer inhibits aggregation of the MPC core, even in the absence
of solvent. MPC stability facilitates design and manipulation
1
of its monolayer functionality and detailed analytical charac-
terization. For MPCs having a 1 to 2 nm core dimension, small
variations in the number of core metal atoms may potentially
evoke significant variations in nanoparticle properties. MPC
samples having a mixture of core sizes can accordingly exhibit
a mixture of properties (i.e., dispersity). Dispersity in properties
may additionally arise from the variability of the ligand shells;
there is inadequate analytical information available on mono-
layer variability. Because thiolate-coated MPCs prepared using
the Brust
1c
reaction or its modifications
4
are somewhat poly-
disperse, there have been several studies aimed at reducing their
polydispersity, and analyzing it using solubility fractionation,
5
etching,
6
extraction,
7
chromatography,
8
capillary electrophore-
sis,
9
and mass spectrometry.
10
Of further value are procedures
amenable to producing quantities of monodisperse MPCs
sufficient for subsequent synthetic, as well as physical, inves-
tigations.
The quantized double layer (QDL) charging
1a,7,11,12
of MPC
cores occurs because the effective capacitances (C
CLU
) of
* To whom correspondence should be addressed. E-mail: rwm@
email.unc.edu.
†
Current address: Dupont Experimental Station, Wilmington, DE 09880-
0262.
‡
Current address: University Of The South, 735 University Ave.,
Sewanee, TN 37383.
(1) (a) Templeton, A. C.; Wuelfing, W. P.; Murray, R. W. Acc. Chem. Res.
2000, 33, 27. (b) Whetten, R. L.; Shafigullin, M. N.; Khoury, J. T.; Schaaff,
T. G.; Vezmar, I.; Alvarez, M. M.; Wilkinson, A. Acc. Chem. Res. 1999,
32, 397. (c) Brust, M.; Walker, M.; Bethell, D.; Schiffrin, D. J.; Whyman,
R. J. Chem. Soc. Chem. Commun. 1994, 801. (d) Brown, L. O.; Hutchison,
J. E. J. Am. Chem. Soc. 1997, 119, 12 384.
(2) Schmid, G. Inorg. Synth. 1990, 27, 214.
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(4) Hostetler, M. J.; Wingate, J.; Zhong, C.-J.; Harris, J. E.; Vachet, R. W.;
Clark, M. R.; Londono, J. D.; Green, S. J.; Stokes, J. J.; Wignall, G. D.;
Glish, G. L.; Porter, M. D.; Evans, N. D.; Murray, R. W. Langmuir, 1998,
14, 17.
(5) Whetten, R. L.; Khoury, J. T.; Alvarez, M. M.; Murthy, S.; Vezmar, I.;
Wang, Z. L.; Stephen, P. W.; Cleveland, C. L.; Luedtke, W. D.; Landman,
U. AdV. Mater. 1996, 5, 428.
(6) (a) Schaaff, T. G.; Whetten, R. L. J. Phys. Chem. 1999, 103, 9394. (b)
Wilcoxon, J. P.; Martin, J. E.; Parsapour, F.; Wiedenman, B.; Kelley, D.
F. J. Chem. Phys. 1998, 108, 9137.
(7) Hicks, J. F.; Templeton, A. C.; Chen, S.; Sheran, K. M.; Jasti, R.; Murray,
R. W.; Debord, J.; Schaaff, T. G.; Whetten, R. L. Anal. Chem. 1999, 71,
3703.
(8) (a) Wilcoxon, J. P.; Martin, J. E.; Provencio, P. Langmuir, 2000, 16, 9912.
(b) Wei, G.; Liu, F.; Wang, C. R. C. Anal. Chem. 1999, 71, 2085.
(9) Templeton, A. C.; Chen, S.; Gross, S. M.; Murray, R. W. Langmuir, 1999,
15, 66.
(10) (a) Alvarez, M. M.; Khoury, J. T.; Schaaff, T. G.; Shafigullin, M.; Vezmar,
I.; Whetten, R. L. Chem. Phys. Lett. 1997, 266, 91-98. (b) Schaaff, T. G.;
Shafigullin, M. N.; Khoury, J. T. Vezmar, I.; Whetten, R. I. J. Phys. Chem.
2001, 105, 8785. (b) Au
140, Au143, Au145 are used by different authors
1,12b
to point to the same nanoparticle material. We consider these differences
to be within the uncertainty of the available analytical information and
would not contest the difference in formulation.
(11) (a) Ingram, R. S.; Hostetler, M. J.; Pietron, J. J.; Murray, R. W.; Schaaff,
T. G.; Khoury, J.; Whetten, R. L.; Bigioni, T. P.; Guthrie, D. K.; First, P.
N. J. Am. Chem. Soc. 1997, 119, 9279. (b) Chen, S.; Ingram, R. S.;
Hostetler, M. J.; Pietron, J. J.; Murray, R. W.; Schaaff, T. G.; Khoury, J.;
Alvarez, M. M.; Whetten, R. L. Science 1998, 280, 2098. (c) Chen, S.;
Murray, R. W.; Feldberg, S. W. J. Phys. Chem. B 1998, 102, 9898.
(12) (a) Chen, S. J. Phys. Chem. 2000, 104, 663. (b) Chen, S. J. Am. Chem.
Soc. 2002, 124, 5280. (c) Chen, S.; Murray, R. W. Langmuir, 1999, 3,
682.
Published on Web 10/12/2002
13322 9 J. AM. CHEM. SOC. 2002, 124, 13322-13328 10.1021/ja027724q CCC: $22.00 © 2002 American Chemical Society