chemical communications volume 46 issue 39 2010 [doi 10.1039_c0cc02374d] mei, qingsong; zhang, kui;...
TRANSCRIPT
-
8/13/2019 Chemical Communications Volume 46 Issue 39 2010 [Doi 10.1039_c0cc02374d] Mei, Qingsong; Zhang, Kui; Guan,
1/3
This journal is c The Royal Society of Chemistry 2010 Chem. Commun., 2010, 46, 73197321 7319
Highly efficient photoluminescent graphene oxide with tunable surfacepropertiesw
Qingsong Mei,ab Kui Zhang,ab Guijian Guan,a Bianhua Liu,a Suhua Wang*a and
Zhongping Zhang*ab
Received 5th July 2010, Accepted 18th August 2010DOI: 10.1039/c0cc02374d
A bright blue fluorescent graphene oxide that originates from
passivation of surface reactive sites by amide formation and
ring-opening amination of epoxide has been prepared. The
surface polarity and charges of the fluorescent graphene oxide
can synchronously be tuned by varying the used alkylamines.
Highly efficient and stable luminescent materials are of
fundamental and technological importance in optoelectronic
devices, biological labeling and sensing.14 Intensive efforts
have been made in the exploration of new efficient emitterssuch as semiconductor quantum dots,1 silicon nanoparticles,2
gold nanodots,3 and carbon-based nanomaterials including
carbon nanotubes, nanodiamond, and carbon dots (C-dots).4
Among those materials, the fluorescent carbon-based nano-
materials have been attracting much more attention as they
show more stable emissions, lower cytotoxicity and give rise to
less environmental concern. The origin of photoluminescence
(PL) in these carbon-based nanomaterials is tentatively
proposed to be from isolated polyaromatic structures or
passivated surface defects.4 However, the preparation of these
carbon nanomaterials usually shows a very low yield and is
carried out under extreme conditions,e.g.laser ablation, high
temperature and high pressure.
4
Graphene oxide (GO) nano-sheet, a two-dimensional oxidized derivative of graphene, also
contains isolated polyaromatic clusters and can be easily
exfoliated from graphite with a high yield under simple
oxidizing conditions. While it has been widely studied in
regard to electrical conductivity, drug delivery, self-assembly,
and surface functionalization,5 the PL properties of GO have
rarely been explored due to its low emission efficiency.6
GO possesses a finite electronic bandgap generated by the
disruption of p networks due to the formation of oxygen-
containing groups. It is well documented that GO nanosheet
bears phenol hydroxyl and epoxide groups at the basal plane
and carboxylic groups at the lateral edge.6 Recently, an
extremely weak broad PL from GO was reported, which wasbelieved to originate from the carbon sp2 domains/clusters,6,7
but it was invisible under UV irradiation. Even though the PL
intensity was slightly improved after moderate reduction
using hydrazine, the quantum yield (QY) was too low to be
measured accurately.6 Moreover, the weak PL was quenched
upon further reduction with hydrazine due to the formation of
non-fluorescent graphene that is known as a zero-bandgap
semiconductor.
As we know, the epoxy and carboxylic groups usually
induce non-radiative recombination of localized electronhole
(eh) pairs, which leads to the nonemissive property of GO.6
However, alkylamines are reactive to both the epoxy and
carboxylic groups through nucleophilic reaction. The removal
of non-radiative recombinative sites is expected to transform
GO nanosheet into a highly efficient emitter. Here we report a
bright blue fluorescent GO which was achieved by the surface
amide formation and ring-opening amination of epoxide of an
original GO by using various alkylamines. The functionalized
GO exhibits a maximum QY up toB13% and tunable surface
properties such as hydrophilic, hydrophobic and negative
charges. The highly fluorescent GO nanosheets with diverse
surface properties could facilitate and expand their applications
in optoelectronics, biolabeling, and bioimaging.
GO nanosheet was first prepared by the oxidation of
graphite using a modified Hummers method.8 The fluorescent
GO was obtained through a facile and effective chemical
approach consisting of the acylation reaction to form alkylamides
and the ring-opening aminations of epoxides to yield
1,2-amino alcohols at the lateral edge and basal surface of
GO nanosheets, respectively (see ESI). Typically, the original
GO was activated first using dichlorosulfoxide to transform
carboxylic groups (at the lateral edge) into acyl chloride under
anhydrous conditions. The further treatment with n-butylamine
(C3Me) led to the occurrence of acylation and ring-opening
reactions at the GO nanosheets. The product was separated
from the mixture and was redispersed in appropriate solvents
for further studies. The n-butylamine modified GO is called
GO-C3Me here for easy communication.
The GO-C3Me aqueous suspension exhibits strong blue
fluorescence under UV irradiation which can be easily seen
with the naked eye and recorded with a digital camera, as
shown in Fig. 1a. The PL spectrum of GO-C3Me shows an
emission maximum at 430 nm under the excitation wavelength
of 350 nm (Fig. 1b). Unlike GO-C3Me, the starting GO shows
no visible fluorescence when irradiated under the same UV
lamp (Fig. 1a, bottom) and only a very weak PL maximum at
525 nm (Fig. 1b-B). The PL quantum yield of GO-C3Me was
measured to be B13% (see ESI), which is about six hundred
fold that of the original GO nanosheets (0.02%). The fluorescence
enhancement by n-butylamine treatment could be attributed
to the surface passivation instead of n-butylamine molecules
themselves because they contain no any visible or near-UV
a Institute of Intelligent Machines, Chinese Academy of Sciences,Hefei, Anhui, 230031, China. E-mail: [email protected],[email protected]
b Department of Chemistry, University of Science & Technology ofChina, Hefei, Anhui, 230026, China
w Electronic supplementary information (ESI) available: Preparationand characterization of alkylamine-modified graphene oxide. SeeDOI: 10.1039/c0cc02374d
COMMUNICATION www.rsc.org/chemcomm | ChemComm
View Online / Journal Homepage / Table of Contents for this issue
http://pubs.rsc.org/en/journals/journal/CC?issueid=CC046039http://pubs.rsc.org/en/journals/journal/CChttp://dx.doi.org/10.1039/C0CC02374D -
8/13/2019 Chemical Communications Volume 46 Issue 39 2010 [Doi 10.1039_c0cc02374d] Mei, Qingsong; Zhang, Kui; Guan,
2/3
7320 Chem. Commun., 2010, 46, 73197321 This journal is c The Royal Society of Chemistry 2010
fluorophores. The surface passivation removes reactive sites
such as epoxy and carboxylic groups by nucleophilic reactions
and hence improves the emission efficiency of the sp2 domains
on GO nanosheets. This can be evidenced by the changes of
absorption and excitation spectra of GO before and after
alkylamine treatment (Fig. 1c). Clearly, the absorption peak
around 230 nm of GO is assigned to the pp* transitions of
CQC. After alkylamine treatment, absorption bands at
276 nm and 350 nm become more pronounced and resolved.
Meanwhile, the corresponding excitation spectrum exhibits a
strong exciting band centered at 350 nm. The results suggest
the formation and increase of new luminescent centers at the
surface of GO-C3Me nanosheets.9
Interestingly, the emission maxima of the GO-C3Me
aqueous suspension are dependent on the excitation wavelengths
(Fig. 2). The emission maxima shift from 430 nm to 515 nm
accompanied by the gradual decrease in emission intensity as
the excitation wavelength varies from 350 nm to 470 nm.
Furthermore, the integrated emission intensities are correlated
with the absorbance in a parallel way (Fig. 2b), indicating
similiar PL quantum yield among those emissive sites. The
results further suggest the existence of heterogeneous electronic
structures attributed to the polydistribution of sp2 cluster sizes
within GO-C3Me.
In general, GO shows very weak PL because of the isolated
sp2 domains generated by oxidation.6,7 These sp2 domains
have opened heterogeneous electronic band gaps which are
intrinsically correlated to their sizes, shapes, and fractions. In
principle, large sp2 domains have narrower energy gaps than
those smaller ones and emit longer wavelengths when excited
at appropriate wavelengths. However, the epoxide groups on
the basal plane and carboxylic groups at the edge of GO often
induce non-radiative recombination of localized eh pairs,
leading to a very low quantum yield. After reacting withalkylamines, these groups are removed and this results in a
bright photoluminescence.
Similar photoluminescent characteristics were also observed
when GO was modified with other alkylamines such as
1,6-hexylenediamine (C6NH2), octylamine (C7Me), dodecylamine
(C11Me) and diamine-terminated poly(ethylene glycol)
(PEG1500N). These longer alkylamine-passivated GO also
exhibit bright blue fluorescence under UV light. The emission
maxima show the same dependence on the excitation
wavelengths (see ESI). For example, the emission maximum
of GO-PEG1500N suspension shifts from 430 nm to 570 nm
when the excitation wavelength varies accordingly. The PL
quantum yields of these different surface passivated GO aremeasured using the same procedure and presented in Table 1.
It is clear that the PL quantum yields obviously decrease with
the increase of carbon chain length in the alkylamine
molecules. GO-PEG1500N still exhibits a 4% quantum yield
that is comparable to the PEG1500N capped C-dots (B5%).4
Meanwhile, the alkylamine functionalized GO also become
less hydrophilic as the the length of carbon chain increases,
consistent with their molecular polarity. Furthermore, the
surface charges are dependent not only on pH values but also
on the properties of amines (see ESI). Therefore, the surface
properties of the alkylamine functionalized GO can be easily
tuned by altering the passivation molecular properties.
Fig. 1 (a) Photographs of GO-C3Me (above) and GO (below)
aqueous solutions under 350 nm irradiation. (b) Photoluminescence
spectra of (A) GO-C3Me and (B) GO in water (18 mg ml1). (c) The
UV-vis absorption spectra (A) of GO (dashed line, 0.02 mg ml1) and
GO-C3Me (solid line, 0.5 mg ml1) aqueous solution, and the excitation
spectra (B) of GO (dashed line, 18 mg ml1) and GO-C3Me (solid line,
18 mg ml1) aqueous solutions.
Fig. 2 (a) Photoluminescence spectra of GO-C3Me aqueous solution
at the different excitation wavelengths. (b) The correlation between the
integrated PL intensities and the absorbance at the excitation
wavelengths. The excitation beam intensities are calibrated for the
integration of PL intensity.
Table 1 The nitrogen/carbon ratios in the alkylamines and thequantum yields and solubility of various amine functionalizedgraphene oxides
Sample NH2/C F (%)a Solubility
GO 0 0.02 H2O, DMF, ethanolGO-C3Me 1/4 12.8 H2O, DMF, ethanolGO-C6NH2 1/3 11.9 H2O, DMF, ethanolGO-C7Me 1/8 5.0 DMF, ethanol, cyclohexaneGO-C11Me 1/12 5.6 DMF, ethanol, cyclohexaneGO-PEG1500N 1/34 4.0 H2O, DMF, ethanol
a The quantum yields were measured in H2O, H2O, H2O, ethanol,
ethanol and H2O under excitation of 350 nm, respectively.
View Online
http://dx.doi.org/10.1039/C0CC02374D -
8/13/2019 Chemical Communications Volume 46 Issue 39 2010 [Doi 10.1039_c0cc02374d] Mei, Qingsong; Zhang, Kui; Guan,
3/3
This journal is c The Royal Society of Chemistry 2010 Chem. Commun., 2010, 46, 73197321 7321
The surface covalent attachment of n-butylamine is
supported by FT-IR and X-ray spectroscopy (XPS) data, as
shown in Fig. 3. For GO-C3Me, a new vibration band around
1648 cm1 due to the CQO stretching of primary amide
emerges (Fig. 3a),10 but the carboxylic group bands at 1733
and 1225 cm1 of original GO disappear after the chemical
treatment. The results immediately suggest the covalent
attachment of n-butylamine to the GO surface through theformation of an amide bond. It can also be seen that the
epoxide band at 1055 cm1 of the GO completely disappears
in GO-C3Me, accompanied by the appearance of a new band
at 1126 cm1 that is assigned to the CNC asymmetric
stretching of the attached alkylamines. Clearly, n-butylamine
not only successfully removes the epoxy groups but also
covalently attaches on the surface of GO by ring-opening
aminations of epoxides to yield 1,2-amino alcohols. The
double bands around 740 cm1 and 818 cm1 of the NH2vibration in pure n-butylamine disappear in the GO-C3Me
sample, which strongly excludes the physical adsorption of
n-butylamine. The band at 1626 cm1 owing to the CQC
vibration of aromatic rings is observed in both GO-C3Me andGO samples, implying the retention of most of the sp2
characteristic structures in GO-C3Me even after the alkylamine
treatment. XPS results also suggest the covalent attachment of
butylamine through amide formation (Fig. 3b). The result of
deconvolution treatment for the N 1s spectrum revealed two
peaks at 400.6 and 399.5 eV, which are attributed to the N 1s
of the NC bond of the amide linkage and the NC bond of
1,2-amino alcohols of GO nanosheets,10 respectively. Based on
the FT-IR and XPS analysis, a structure of the GO-C3Me is
modeled as presented in Fig. 3c. The GO-C3Me nanosheet
consists of small sp2 conjugated aromatic domains isolated by
sp3 carbon.
In summary, we have prepared a bright blue photo-
luminescent GO by surface alkylamine functionalization
under mild conditions. The fluorescence quantum yields of
the alklyamine-functionalized GO are remarkably enhanced
up to six hundred times compared with the original GO.
Meanwhile, the surface properties of the modified GO can
be easily tuned from hydrophilic to hydrophobic by changing
the molecular structures of the used amines. These will greatly
expand the applications of GO in many fields.
This work was supported by Natural Science Foundation
of China (20925518, 20875090, 20807042, 30901008) and
ChinaSingapore Joint Project (2009DFA51810) and 863
project of China (2007AA10Z434) and Innovation Project of
Chinese Academy of Sciences (KSCX2-YW-G-058).
Notes and references
1 M. Bruchez, M. Moronne, P. Gin, S. Weiss and A. P. Alivisatos,Science, 1998, 281, 20 13; X. Mich alet , F . F. Pi naud ,
L. A. Bentolila, J. M. Tsay, S. Doose, J. J. Li, G. Sundaresan,A. M. Wu, S. S. Gambhir and S. Weiss, Science, 2005, 30 7, 538;S. H. Wang, M. Y. Han and D. J. Huang, J. Am. Chem. Soc., 2009,131, 11692.
2 J. H. Warner, A. Hoshino, K. Yamaomto and R. D. Tilley,Angew.Chem., Int. Ed., 2005, 44, 4550.
3 C. C. Huang, Z. Yang, K. H. Lee and H. T. Chang,Angew. Chem.,Int. Ed., 2007, 46, 6824; C. C. Huang, H. Y. Liao, Y. C. Shiang,Z. H. Lin, Z. Yang and H. T. Chang, J. Mater. Chem., 2009, 19,755.
4 J. E. Riggs, Z. X. Guo, D. L. Carroll and Y. P. Sun, J. Am. Chem.Soc., 2000, 122, 5879 ; Y. Lin, B. Zh ou, R. B. Marti n,K. B. Henbest, B. A. Harruff, J. E. Riggs, Z. X. Guo,L. F. Allard and Y. P. Sun, J. Phys. Chem. B, 2005, 109, 14779;S. J. Yu, M. W. Kang, H. C. Chang, K. M. Chen and Y. C. Yu,J. Am. Chem. Soc., 2005, 127, 17604; V. N. Mochalin and
Y. Gogotsi, J. Am. Chem. Soc., 2009, 131, 4594; Y. P. Sun,B. Zhou, Y. Lin, W. Wang, K. A. Shiral Fernando, P. Pathak,M. J. Meziani, B. A. Harruff, X. Wang, H. F. Wang, P. G. Luo,M. E. Kose, B. Chen, L. M. Veca and S. Y. Xie,J. Am. Chem. Soc.,2006,128, 7756; H. Liu, T. Ye and C. D. Mao, Angew. Chem., Int.Ed., 2007, 46, 6473; A. B. Bourlinos, A. Stassinopoulos, D. Anglos,R. Zboril, M. Karakassides and E. P. Giannelis, Small, 2008, 4,455.
5 O. C. Compton, D. A. Dikin, K. W. Putz, L. C. Brinson andS. T. Nguyen, Adv. Mater., 2010, 22, 892; L. J. Cote, F. Kim andJ. X. Huang, J. Am. Chem. Soc., 2009, 131, 1043; Z. Liu,J. T. Rovinson, X. M. Sun and H. J. Dai, J. Am. Chem. Soc.,2008, 130, 10876.
6 Z. T. Luo, P. M. Vora, E. J. Mele, A. T. Charlie Johnson andJ. M. Kikkawa, Appl. Phys. Lett., 2009, 94, 111909; G. Eda,Y. Y. Lin, C. Mattevi, H. Yamaguchi, H. A. Chen, I. S. Chen,C. W. Chen and M. Chhowalla, Adv. Mater., 2010, 22, 505.
7 X. M. Sun, Z. Liu, K. Welsher, J. T. Robinson, A. Goodwin,S. Zaric and H. J. Dai, Nano Res., 2008, 1, 203.
8 W. S. Hummers and R. E. Offeman,J. Am. Chem. Soc., 1958, 80,1339; V. C. Tung, M. J. Allen, Y. Yang and R. B. Kaner,Nat.Nanotechnol., 2009, 4, 25.
9 D. Li, M. B. Muller, S. Gilje, R. B. Kaner and G. G. Wallace,Nat.Nanotechnol., 2008, 3, 101; Z. T. Luo, Y. Lu, L. A. Somers andA. T. Charlie Johnson, J. Am. Chem. Soc., 2009, 131, 898.
10 N. B. Colthup, L. Daly and S. E. Weberley, in Introduction toInfrared and Raman Spectroscopy, Academic Press, New York,USA, 1999; O. C. Compton, D. A. Dikin, K. W. Putz,L. C. Brinson and S. T. Nguyen, Adv. Mater., 2009, 21, 1.
Fig. 3 (a) FT-IR spectra of (A) GO-C3Me, (B) n-butylamine and (C)
GO. (b) Nitrogen 1s XPS spectrum obtained from GO-C3Me showing
the oxidation states of nitrogen atoms. (c) The structure of alkylamine
functionalized GO (R represents various hydrocarbon chains).
View Online
http://dx.doi.org/10.1039/C0CC02374D