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ZnO Nanoparticles' Interaction with Graphene Oxide: Study on Electron Transfer and Photoca, Notas de estudo de Engenharia Elétrica

This document reports on a study investigating the interaction between excited zno nanoparticles and graphene oxide (go). The researchers observed that go undergoes photocatalytic reduction when in contact with excited zno nanoparticles, as evidenced by the quenching of zno's green emission. The study also discusses the potential role of go in supporting semiconductor catalyst nanoparticles due to its unique 2-d architecture.

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DOI: 10.1021/la900905h 13869Langmuir 2009, 25(24), 13869–13873 Published on Web 05/19/2009
pubs.acs.org/Langmuir
©2009 American Chemical Society
Graphene-Semiconductor Nanocomposites: Excited-State Interactions
between ZnO Nanoparticles and Graphene Oxide
Graeme Williams
and Prashant V. Kamat*
Radiation Laboratory and Department of Chemistry and Biochemistry, University of Notre Dame, Notre Dame,
Indiana 46556.
University of Waterloo cooperative education student
Received March 14, 2009. Revised Manuscript Received April 21, 2009
Graphene oxide sheets suspended in ethanol interact with excited ZnO nanoparticles and undergo photocatalytic
reduction. The luminescence quenching of the green emission of ZnO serves as a probe to monitor the electron transfer
from excited ZnO to graphene oxide. Anchoring of ZnO nanoparticles on 2-D carbon nanostructures provides a new
way to design semiconductor-carbon nanocomposites for catalytic applications.
Introduction
Graphene sheets are analogous to unrolled 2-D carbon nano-
tubes. They are individual sheets separated from the large,
stacked-sheet structure of graphite. The carbon sp
2
network of
single and bilayer graphene exhibits unique 2-D electronic trans-
port that hasbeen shown to produce strongconductivity.
1,2
Given
the economicalcost of graphene, thereis a significantdrive within
the scientific community to gain a greater understanding of its
properties and explore its possible applications. For example, the
potential for conductive graphene-based films and graphene-
sheet transparent conductive films has been explored.
3-6
How-
ever, photochemistry and photovoltaic aspects of 2-D carbon
nanostructures, graphene and graphene oxide (GO) sheets, are
relatively unstudied and provide an exciting new array of ideas
and applications.
Although graphite and graphite oxide have been known to be
in existence since the last century, it is onlyrecently that graphene
and graphene oxide sheets have been prepared and characterized
in a systematic way.
7
The most significant challenge in the
preparation of graphene is overcoming the strong exfoliation
energy of the π-stacked layers in graphite.
8
The recent focus on
graphene sheets involves the simple “micromechanical cleavage”
of graphite, where a piece of Scotch tape is used to remove
individual sheets of graphene. Micrographitic powder, however,
cannot be readily separatedinto individual sheetsor dispersed in a
solvent medium. Several methodsof preparation of graphene and
graphene oxide include the oxidation of graphite combined with
thermal exfoliation, the treatment of graphite fluorides with alkyl
lithium reagents, and theoxidation of graphitefollowed by strong
sonication.
8-10
The factors dictating stable dispersions of gra-
phene in various organic solvents and its interactions with
substituted organic compounds have also been discussed.
11,12
One obvious challenge is to utilize these 2-D carbon nanos-
tructures as conductive carbon mats so that one can anchor
semiconductor or metal nanoparticles and facilitate tailored
catalytic reactions (Scheme 1). Initial efforts to utilize graphene
as a 2-D carbon support to anchor metal nanoparticles have
already been reported.
13,14
ZnO and TiO
2
nanoparticles have
recently been examined in combination with carbon nanotubes,
showing an electron accepting and storing capacity of the
nanotubes.
15-18
Hence, it is reasonable to expect that GO sheets
may play a similar role of providing unique 2-D architecture to
support semiconductor catalyst nanoparticles. The ability of
semiconductor nanoparticles to partially reduce GO samples
when excited with UV light was demonstrated recently with
TiO
2
.
19
In our quest to further explore the interaction between
graphene oxide and semiconductor nanoparticles, we have now
probedthe ZnO emission to monitor theelectron transfer between
the semiconductor nanoparticles and GO sheets (Scheme 1). The
photochemical processes that illustrate the partial reduction of
GO in a ZnO nanoparticle suspension are presented here.
Experimental Section
Materials.
Graphene oxide was prepared by the Hummers’
method, where micrographitic powder was mixed with strong
oxidizing agents, filtered, and dried.
7
The oxidation process
functionalizes the graphene sheets with various hydroxyl and
epoxy groups, in addition to carbonyl and carboxyl groups along
Part of the Langmuir 25th Year:Nanoparticles synthesis, properties, and
assembliesspecial issue.
*Address Correspondence to this author. E-mail: [email protected].
(1) Gomez-Navarro, C.; Weitz, R. T.; Bittner, A. M.; Scolari, M.; Mews, A.;
Burghard, M.; Kern, K. Nano Lett. 2007,7, 3499 –3503.
(2) Castro, E. V.; Novoselov, K. S.; Morozov, S. V.; Peres, N. M. R.; Dos
Santos, J.; Nilsson, J.; Guinea, F.; Geim, A. K.; Neto, A. H. C. Phys. Rev. Lett.
2007, 99.
(3) Dikin, D. A.; Stankovich, S.; Zimney, E. J.; Piner, R. D.; Dommett, G. H. B.;
Evmenenko, G.; Nguyen, S. T.; Ruoff, R. S. Nature 2007,448, 457–460.
(4) Wang, X.; Zhi, L. J.; Mullen, K. Nano Lett. 2008,8, 323–327.
(5) Watcharotone, S. Nano Lett. 2007,7, 1888–1892.
(6) Kim, K.; Park, H. J.; Woo, B. C.; Kim, K. J.; Kim, G. T.; Yun ,W. S. Nano
Lett. 2008,8, 3092–3096.
(7) Hummers, W. S.; Offeman, R. E. J. Am. Chem. Soc. 1958,80, 1339–1339.
(8) Schniepp, H. C.; Li, J. L.; McAllister, M. J.; Sai, H.; Herrera-Alonso, M.;
Adamson, D. H.; Prud’homme, R. K.; Car, R.; Saville, D. A.; Aksay, I. A. J. Phys.
Chem. B 2006,110, 8535–8539.
(9) Worsley, K. A.; Ramesh, P.; Mandal, S. K.; Niyogi, S.; Itkis, M. E.; Haddon,
R. C. Chem. Phys. Lett. 2007,445, 51–56.
(10) Niyogi, S.; Bekyarova, E.; Itkis, M. E.; McWilliams, J. L.; Hamon, M. A.;
Haddon, R. C. J. Am. Chem. Soc. 2006,128, 7720–7721.
(11) Paredes, J. I.; Villar-Rodil, S.; Martinez-Alonso, A.; Tascon, J. M. D.
Langmuir 2008,24, 10560–10564.
(12) Rochefort, A.; Wuest, J. D. Langmuir 2009,25, 210–215.
(13) Muszynski, R.; Seger, B.; Kamat, P. J. Phys. Chem. C 2008 ,112, 5263–
5266. (b) Seger, B.; Kamat, P. V.; J. Phys. Chem. C 2009,113, 7990–7995.
(14) Xu, C.; Wang, X.; Zhu, J. W. J. Phys. Chem. C 2008,112, 19841–19845.
(15) Vietmeyer, F.; Seger, B.; Kamat, P. V. Adv. Mater. 2007,19, 2935–2940.
(16) Kongkanand, A.; Kamat, P. V. J. Phys. Chem. C 2007,111, 9012–9015.
(17) Kongkanand, A.; Kamat, P. V. ACS Nano 2007,1, 13–21.
(18) Kongkanand, A.; Domı
´nguez, R. M.; Kamat, P. V. Nano Lett. 2007,7,
676–680.
(19) Williams, G.; Seger, B.; Kamat, P. V. ACS Nano 2008,2, 1487–1491.
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Langmuir 2009, 25(24), 13869–13873 Published on Web 05/19/2009 DOI: 10.1021/la900905h 13869

pubs.acs.org/Langmuir © 2009 American Chemical Society

Graphene-Semiconductor Nanocomposites: Excited-State Interactions

between ZnO Nanoparticles and Graphene Oxide

Graeme Williams ‡^ and Prashant V. Kamat*

Radiation Laboratory and Department of Chemistry and Biochemistry, University of Notre Dame, Notre Dame, Indiana 46556. ‡^ University of Waterloo cooperative education student

Received March 14, 2009. Revised Manuscript Received April 21, 2009

Graphene oxide sheets suspended in ethanol interact with excited ZnO nanoparticles and undergo photocatalytic reduction. The luminescence quenching of the green emission of ZnO serves as a probe to monitor the electron transfer from excited ZnO to graphene oxide. Anchoring of ZnO nanoparticles on 2-D carbon nanostructures provides a new way to design semiconductor-carbon nanocomposites for catalytic applications.

Introduction

Graphene sheets are analogous to unrolled 2-D carbon nano- tubes. They are individual sheets separated from the large, stacked-sheet structure of graphite. The carbon sp^2 network of single and bilayer graphene exhibits unique 2-D electronic trans- port that has been shown to produce strong conductivity.1,2^ Given the economical cost of graphene, there is a significant drive within the scientific community to gain a greater understanding of its properties and explore its possible applications. For example, the potential for conductive graphene-based films and graphene- sheet transparent conductive films has been explored.^3 -^6 How- ever, photochemistry and photovoltaic aspects of 2-D carbon nanostructures, graphene and graphene oxide (GO) sheets, are relatively unstudied and provide an exciting new array of ideas and applications. Although graphite and graphite oxide have been known to be in existence since the last century, it is only recently that graphene and graphene oxide sheets have been prepared and characterized in a systematic way.^7 The most significant challenge in the preparation of graphene is overcoming the strong exfoliation energy of the π-stacked layers in graphite.^8 The recent focus on graphene sheets involves the simple “micromechanical cleavage” of graphite, where a piece of Scotch tape is used to remove individual sheets of graphene. Micrographitic powder, however, cannot be readily separated into individual sheets or dispersed in a solvent medium. Several methods of preparation of graphene and graphene oxide include the oxidation of graphite combined with thermal exfoliation, the treatment of graphite fluorides with alkyl

lithium reagents, and the oxidation of graphite followed by strong sonication.^8 -^10 The factors dictating stable dispersions of gra- phene in various organic solvents and its interactions with substituted organic compounds have also been discussed.11, One obvious challenge is to utilize these 2-D carbon nanos- tructures as conductive carbon mats so that one can anchor semiconductor or metal nanoparticles and facilitate tailored catalytic reactions (Scheme 1). Initial efforts to utilize graphene as a 2-D carbon support to anchor metal nanoparticles have already been reported.13,14^ ZnO and TiO 2 nanoparticles have recently been examined in combination with carbon nanotubes, showing an electron accepting and storing capacity of the nanotubes.^15 -^18 Hence, it is reasonable to expect that GO sheets may play a similar role of providing unique 2-D architecture to support semiconductor catalyst nanoparticles. The ability of semiconductor nanoparticles to partially reduce GO samples when excited with UV light was demonstrated recently with TiO 2.^19 In our quest to further explore the interaction between graphene oxide and semiconductor nanoparticles, we have now probed the ZnO emission to monitor the electron transfer between the semiconductor nanoparticles and GO sheets (Scheme 1). The photochemical processes that illustrate the partial reduction of GO in a ZnO nanoparticle suspension are presented here.

Experimental Section

Materials. Graphene oxide was prepared by the Hummers’ method, where micrographitic powder was mixed with strong oxidizing agents, filtered, and dried.^7 The oxidation process functionalizes the graphene sheets with various hydroxyl and † epoxy groups, in addition to carbonyl and carboxyl groups along Part of the “Langmuir 25th Year: Nanoparticles synthesis, properties, and assemblies” special issue. *Address Correspondence to this author. E-mail: [email protected]. (1) Gomez-Navarro, C.; Weitz, R. T.; Bittner, A. M.; Scolari, M.; Mews, A.; Burghard, M.; Kern, K. Nano Lett. 2007 , 7 , 3499 –3503. (2) Castro, E. V.; Novoselov, K. S.; Morozov, S. V.; Peres, N. M. R.; Dos Santos, J.; Nilsson, J.; Guinea, F.; Geim, A. K.; Neto, A. H. C. Phys. Rev. Lett. 2007 , 99. (3) Dikin, D. A.; Stankovich, S.; Zimney, E. J.; Piner, R. D.; Dommett, G. H. B.; Evmenenko, G.; Nguyen, S. T.; Ruoff, R. S. Nature 2007 , 448 , 457–460. (4) Wang, X.; Zhi, L. J.; Mullen, K. Nano Lett. 2008 , 8 , 323–327. (5) Watcharotone, S. Nano Lett. 2007 , 7 , 1888–1892. (6) Kim, K.; Park, H. J.; Woo, B. C.; Kim, K. J.; Kim, G. T.; Yun, W. S. Nano Lett. 2008 , 8 , 3092–3096. (7) Hummers, W. S.; Offeman, R. E. J. Am. Chem. Soc. 1958 , 80 , 1339–1339. (8) Schniepp, H. C.; Li, J. L.; McAllister, M. J.; Sai, H.; Herrera-Alonso, M.; Adamson, D. H.; Prud’homme, R. K.; Car, R.; Saville, D. A.; Aksay, I. A. J. Phys. Chem. B 2006 , 110 , 8535–8539.

(9) Worsley, K. A.; Ramesh, P.; Mandal, S. K.; Niyogi, S.; Itkis, M. E.; Haddon, R. C. Chem. Phys. Lett. 2007 , 445 , 51–56. (10) Niyogi, S.; Bekyarova, E.; Itkis, M. E.; McWilliams, J. L.; Hamon, M. A.; Haddon, R. C. J. Am. Chem. Soc. 2006 , 128 , 7720–7721. (11) Paredes, J. I.; Villar-Rodil, S.; Martinez-Alonso, A.; Tascon, J. M. D. Langmuir 2008 , 24 , 10560–10564. (12) Rochefort, A.; Wuest, J. D. Langmuir 2009 , 25 , 210–215. (13) Muszynski, R.; Seger, B.; Kamat, P. J. Phys. Chem. C 2008 , 112 , 5263–

  1. (b) Seger, B.; Kamat, P. V.; J. Phys. Chem. C 2009 , 113 , 7990–7995. (14) Xu, C.; Wang, X.; Zhu, J. W. J. Phys. Chem. C 2008 , 112 , 19841–19845. (15) Vietmeyer, F.; Seger, B.; Kamat, P. V. Adv. Mater. 2007 , 19 , 2935–2940. (16) Kongkanand, A.; Kamat, P. V. J. Phys. Chem. C 2007 , 111 , 9012–9015. (17) Kongkanand, A.; Kamat, P. V. ACS Nano 2007 , 1 , 13–21. (18) Kongkanand, A.; Domı´nguez, R. M.; Kamat, P. V. Nano Lett. 2007 , 7 , 676–680. (19) Williams, G.; Seger, B.; Kamat, P. V. ACS Nano 2008 , 2 , 1487–1491.

13870 DOI: 10.1021/la900905h Langmuir 2009, 25(24), 13869–

Article Williams and Kamat

the edges of the sheets. The dried product was suspended in ethanol and sonicated in order to disperse GO sheets. The details of the procedure are described elsewhere.^13 The method of synthesis for zinc oxide nanoparticles, adopted from the literature,20,21^ involves the addition of zinc acetate to an ethanol solution, followed by sonication in an ice bath.^15 A base, lithium hydroxide, was then added to the solution, and the reaction vessel was further sonicated at room temperature, allow- ing the particles to complete the growth process. AFM samples were prepared by drop casting dilute mixtures of the semiconductor nanoparticles and GO sheets in ethanol onto heated, freshly cleaved mica substrates. Atomic force microscopy (AFM) was conducted using a Digital Nanoscope III in tapping mode. An etched silicon tip was used as a probe to image the samples. Optical and Emission Measurements. Absorption spectra were recorded using a Shimadzu UV-3101 PC spectrophotometer. Emission spectra were recorded using an SLM-S 8000 spectro- fluorometer. Emission lifetimes were measured using a Horiba Jobin Yvon single-photon counting system with a diode (277 nm, 1 MHz repetition, 1.1 ns pulse width) excitation source. Filtered light (λ > 300 nm) from an Oriel 150 W xenon arc lamp was used to carry out steady-state photolysis. All experiments were conducted under ambient conditions.

Results and Discussion

Fluorescence Studies. ZnO nanoparticles, with a bulk band- gap of 3.37 eV, are photocatalytically active under UV irradia- tion. In ethanol, they can be prepared in the size-quantized regime (2-5 nm) by controlling the hydrolysis temperature.^22 These particles exhibit green emission under bandgap excitation.^23 This green emission (λmax ≈ 530 nm), arising from oxygen vacancies, serves as a probe to monitor the interfacial electron-transfer processes. The ability of ZnO nanoparticles to transfer photo- generated electrons to carbon nanotubes has been demonstrated from the quenching of ZnO emission.^15 Figure 1 shows the fluorescence of a 1 mM solution of ZnO nanoparticles with varying amounts of graphene oxide added to the solution. The decrease in fluorescence yield suggests that an additional pathway for the disappearance of the charge carriers dominates because of the interactions between the excited ZnO particles and the GO sheets. As demonstrated earlier, such emission quenching represents interfacial charge-transfer processes.^22 -^24 In the pre- sent experiments, the emission quenching represents electron

transfer from the excited ZnO nanoparticles to the GO to produce reduced GO (RGO).

ZnO þ hν f ZnOðh þ eÞ f

C 2 H 5 OH ZnOðeÞ þ•C 2 H 4 OH ð 1 Þ

ZnOðeÞ þ GO f ZnO þ RGO ð 2 Þ

The ethoxy radicals produced during the hole oxidation step are also reductive in nature and thus contribute to the reduction process. No such reductive radicals are produced in the absence of ZnO. The absorption spectra of ZnO suspensions containing differ- ent amounts of GO are shown in Figure 2. Upon close examina- tion of these absorption spectra, it is evident that GO absorbs strongly in the UV region and may interfere with the excitation at 315 nm of ZnO nanoparticles in emission studies. The absorbance difference between ZnO-GO and ZnO at 315 nm can be used to estimate the fraction of excited light absorbed by GO. For all of the samples examined in Figure 1, the decreased absorption at 315 nm due to GO is significantly lower than the fluorescence quenching observed for the same sample. For example, at the highest GO concentration (0.24 mg/mL) the contribution of GO absorption at 315 nm amounts to 25%, but the extent of ZnO quenching was more than 95% of the pristine ZnO emission yield. Thus, we consider the contribution of GO

Scheme 1. Excited-State Interaction between ZnO and Graphene Oxide

Figure 1. Emission spectra of a 1 mM ZnO suspension at different GO concentrations: (a) 0, (b) 0.035, (c) 0.09, (d) 0.14, (e) 0.20, and (f ) 0.24 mg/mL

Figure 2. Absorption of a 1 mM ZnO nanoparticle suspension in ethanol containing different amounts of GO.

(20) Spanhel, L.; Anderson, M. A. J. Am. Chem. Soc. 1991 , 113 , 2826–2833. (21) Kamat, P. V.; Patrick, B. Photochemistry and Photophysics of ZnO Colloids. In Symp. Electron. Ionic Prop. Silver Halides; The Society for Imaging Science and Technology: Springfield, Va, 1991. (22) Kamat, P. V.; Patrick, B. J. Phys. Chem. 1992 , 96 , 6829–34. (23) Subramanian, V.; Wolf, E. E.; Kamat, P. V. J. Phys. Chem. B 2003 , 107 , 7479–7485. (24) Kamat, P. V.; Huehn, R.; Nicolaescu, R. J. Phys. Chem. B 2002 , 106 , 788–

13872 DOI: 10.1021/la900905h Langmuir 2009, 25(24), 13869–

Article Williams and Kamat

and more typical values of 1-1.3 nm for a hydrated sample examined by AFM. 8,27^ The composite system studied in this and shown in Figure 5 therefore exhibits mono- and bilayers of graphene, as indicated by 1 to 2 nm sheet heights. Although we were initially interested in individual graphene sheets, it should be noted that the presence of bilayer and few-layer graphene is not necessarily indicative of a bad sample. Studies have shown that bilayer graphene can exhibit conductivities significantly greater than those for single-layer graphene. 1 The ZnO-GO system consists of nanoparticles on the order of 2-7 nm, and the nanoparticles appear to be completely covering the graphene sheets. Film Resistance. Upon photocatalytic reduction, it is ex- pected that the reduced GO (RGO) sheets exhibit an improve- ment in conductivity. Solid-film resistivity tests were performed to evaluate the effectiveness of the photocatalytic reduction of GO in improving the conductivity. Borosilicate glass slides were sput- tered with a 40 nm layer of gold except for a 2 mm gap in the center. Large resistances between the gold terminations were confirmed before further manipulations to the slides were made. The GO and RGO solutions were then drop cast on the gap between the gold terminations at slightly elevated temperatures

(50- 60 °C) in order to ensure immediate evaporation of the ethanol solvent. This was done to ensure a fairly uniform coverage of the GO film. However, a variation in the film thickness is evident from the large standard deviations witnessed for these samples. The gold terminations were then connected to a digital multimeter where resistance measurements of the GO and RGO samples were made. Sheet resistance values were calculated by dividing measured lateral resistances by the square of the sample (equal to the ratio of the length to the width of the gap). A comparison was also made between the photocatalytic reduc- tion using ZnO and TiO 2 nanoparticles. A summary of the results of the resistance measurements averaged for five different samples is given in Table 2. A similar method of determining resistivity changes was previously used for measurements of chemically reduced gra- phene oxide.^28 The lateral resistance of a reduced graphite oxide sample across a 2-mm-long, 3-mm-wide gap reported in this study was 12 kΩ. Lateral resistance values of 16 and 31 kΩ found for the ZnO-RGO and TiO 2 - RGO samples observed in the present experiments are of the same order as those in previous reports. The unreduced lateral resistance of 32 MΩ^28 is lower than the several hundred MΩ resistance seen for GO films. The presence of semiconductor particles (ZnO or TiO 2 ) in the GO film is expected

Figure 4. (Left) Suspensions of ZnO, ZnO-GO, and ZnO-RGO. The color changes from brown (middle vial) to dark brown (right vial) as we irradiate the ZnO-GO sample with UV light. (Right) Absorption spectra of 0.5 mg/mL GO and 1 mM ZnO in deaerated ethanol at different UV irradiation times of (a) 0, (b) 60, (c) 180, and (d) 420 s. The inset shows the growth of absorption with UV irradiation time.

Figure 5. AFM analysis of ZnO nanoparticles deposited onto graphene oxide sheets.

Table 2. Resistances of Unreduced and Photocatalytically Reduced GO ZnO-GO ZnO-RGO TiO 2 - GOa^ TiO 2 - RGOa

lateral resistance (kΩ) 583 ( 107 16.3 ( 5.16 233 ( 105 30.5 ( 8. sheet resistance (kΩ/sq) 2920 ( 535 81.7 ( 25.8 1170 ( 525 152 ( 41. a (^) From ref 19.

(27) Stankovich, S.; Piner, R. D.; Nguyen, S. T.; Ruoff, R. S. Carbon 2006 , 44 , 3342–3347. (28) Kotov, N. A.; Dekany, I.; Fendler, J. H. Adv. Mater. 1996 , 8 , 637–641.

Langmuir 2009, 25(24), 13869–13873 DOI: 10.1021/la900905h 13873

Williams and Kamat Article

to contribute to this enhanced photoconductivity of the unre- duced GO film. Nevertheless, the lower resistance observed with photocatalytically reduced GO films confirms the effectiveness of semiconductor nanoparticles in facilitating reduction under band- gap excitation.

Conclusions

The electron transfer from excited ZnO nanoparticles to GO is effective in carrying out reduction and decreasing the resistivity of chemically functionalized graphene films. On the basis of the luminescence decay measurements, we estimate the appa- rent electron-transfer rate constant to be 1.2  109 s-^1. The

on-demand reduction of GO using UV irradiation is potentially useful in fine tuning conductivity over a single graphene sheet. In addition, graphene-semiconductor nanoparticle composites can also provide new ways to tailor catalytic and photocatalytic reactions.

Acknowledgment. The research described herein was supported by the Office of Basic Energy Sciences of the Depart- ment of Energy. We also thank Brian Seger for his help in synthesizing GO and helpful discussions. This is contribu- tion number NDRL 4798 from the Notre Dame Radiation Laboratory.