13990 J. Phys. Chem. B, Vol. 109, No. 29, 2005
Qu and Dai
reagent. The surface morphology and chemical state of Cu foils
play important roles in regulating the structure features, and
hence properties, of the resulting silver clusters. While an
aqueous solution of the silver nanoparticles formed on a glass
plate from the conventional silver mirror reaction shows a broad
surface plasmon absorption peak around 430 nm, the corre-
sponding solution of the silver nanosheets prepared from the
same silver mirror reaction on copper foils gives a light-
scattering band over 350 nm. This work represents a general
approach to the preparation of a large variety of new silver
nanomaterials of potential applications in many areas, as other
metals of a low work function (e.g., Al foil) have also been
demonstrated to undergo similar galvanic displacement reac-
tions.
Note Added in Proof. After the submission of our manu-
script, we note that He et al. recently reported the preparation
of silver nanosheets on an aluminum foil (He, Y.; Wu, X. F.;
Lu, G. W.; Shi, G. Q. Nanotechnology 2005, 16, 791).
Figure 8. UV-vis spectra of (a) silver nanoparticles and (b) nanosheets
dispersed in water by sonication.
Acknowledgment. We are grateful for financial support from
the National Science Foundation (NSF-CCF-0403130), Ameri-
can Chemical Society (ACS-PRF 39060-AC5M), NEDO In-
ternational Joint Research Grant (04IT4), the Materials and
Manufacturing Directorate of the Air Force Research Labora-
tory, The Dayton Development Coaltition, and Wright Brothers
Institute. We also thank Kyung Min Lee and Amanda Schrand
for their help with the X-ray and electron diffraction measure-
ments, respectively. The use of facilities in the NEST Center
at UD is greatly appreciated.
(Figure 1b,c) shows a typical UV-vis spectrum with a strong
surface plasmon absorption band around 430 nm (curve a, Figure
8) characteristic of silver nanoparticles,4,7,8 the corresponding
spectrum for the silver nanosheets prepared in the present study
(curve b, Figure 8) reveals a light-scattering peak over 350 nm
due to the relatively large particle size.9 These observations
clearly indicate that properties (e.g., optical absorption) of silver
clusters are strongly dependent on their size and symmetry.
Therefore, there is considerable room for tailoring the structure-
property relationship of the silver clusters resulting from the
silver mirror reaction by controlling the substrate nature and
its surface features.
References and Notes
(1) See, for example: (a) Handbook of Nanophase Materials; Goldstein,
A. N., Ed.; Marcel Dekker: New York, 1997. (b) Burda, C.; Chen, X.;
Narayanan, R.; El-Sayed, M. A. Chem. ReV. 2005, 105, 1025, and references
cited therein.
(2) See, for example: (a) Swami, A.; Selvakannan, P. R.; Pasricha,
R.; Sastry, M. J. Phys. Chem. B 2004, 108, 19269. (b) Yakutik, I. M.;
Shevchenko, G. P. Surf. Sci. 2004, 566, 414. (c) Ahmadi, T.; Wang, Z.;
Green, T.; Hendlein, A.; El-Sayed, M. Science 1996, 272, 1924. (d) Pileni,
M. Langmuir 1997, 13, 3266. (e) Huang, L.; Ling, G.; Zhang, C.; Li, J.
Plating Surf. Finishing 2004, 91, 46. (f) Ling, G. P.; He, J. H.; Huang, L.
J. Mater. Sci. 2004, 39, 2955.
Conclusions
In summary, we have demonstrated that novel silver clusters
could be reproducibly prepared by simply carrying out the silver
mirror reaction on certain reactive substrates with specific
surface features. While leaflike fractal silver microstructures
were produced from the conventional silver mirror reaction on
a commercially available copper foil with spotlike oxide defects,
perpendicularly aligned silver nanosheets were prepared under
the same reaction conditions on the copper foils after having
been rubbed with sandpapers. Silver nanoclusters with various
morphologies ranging from the leaflike to flowerlike hierarchical
structures have been produced from the silver mirror reaction
by removing the copper oxide layer from commercially available
copper foils through relatively benign acid (e.g., dilute HCl)
treatments under different conditions. Control experiments on
(3) Zhang, S. H.; Xie, Z. X.; Jiang, Z. Y.; Xu, X.; Xiang, J.; Huang,
R. B; Zheng, L. S. Chem. Commun. 2004, 1106.
(4) (a) Kim, K. D.; Han, D. N.; Kim, H. T. Chem. Eng. J. 2004, 104,
55, and references therein. (b) Qu, L. T.; Shi, G. Q.; Wu, X. F.; Fan, B.
AdV. Mater. 2004, 16, 1200.
(5) (a) Aizawa, M.; Cooper, A. M.; Malac, M.; Buriak, J. M. Nano
Lett. 2005, 5, 815. (b) Mandelbrot, B. B. The Fractal Geometry of Nature;
W. H. Freeman and Company: New York, 1983.
(6) Jaenicke, W. In Progress in Photographic Theory; Spencer, D. A.,
Ed.; Focal Press: London, 1958.
(7) Vorobyova, S. A.; Lesnikovich, A. I.; Sobal, N. S. Colloids Surf.,
A 1999, 152, 375.
(8) He, S. T.; Yao, J. N.; Jiang, P.; Shi, D. X.; Zhang, H. X.; Xie, S.
S.; Pang, S. J.; Gao, H. J. Langmuir 2001, 17, 1571.
(9) (a) Kreibig, U.; Vollmer, M. Optical Properties of Metal Clusters;
Springer-Verlag: Berlin, 1995. (b) Eversole, J. D.; Broida, H. P. Phys. ReV.
B 1977, 15, 1644.
+
reactions of AgNO3 or Ag(NH3)2 with copper foils in the
absence of any other reductive reagent indicated that Cu atoms
actively participated in the silver mirror reaction as a reductive