Modifying the Size of Ultrasound-Induced Liquid-Phase Exfoliated Graphene: From Nanosheets to Nanodots

CIESIELSKI, Artur, HAAR, Sébastien, ALIPRANDI, Alessandro, EL GARAH, Mohamed, TREGNAGO, Giulia, COTELLA, Giovanni F., EL GEMAYEL, Mirella, RICHARD, Fanny, SUN, Haiyan, CACIALLI, Franco, BONACCORSO, Francesco et SAMORÌ, Paolo, 2016. Modifying the Size of Ultrasound-Induced Liquid-Phase Exfoliated Graphene: From Nanosheets to Nanodots. ACS Nano. 15 novembre 2016. Vol. 10, n° 12pp. 10768-10777. DOI 10.1021/acsnano.6b03823.
Accès libre Peer reviewed
Version acceptée pour publication (post-print auteur)
Paternité - Pas d'utilisation commerciale [CC] [BY] [NC]
Auteurs Artur Ciesielski
Sébastien Haar
Alessandro Aliprandi
Mohamed El Garah
Giulia Tregnago
Giovanni F. Cotella
Mirella El Gemayel
Fanny Richard
Haiyan Sun
Franco Cacialli
Francesco Bonaccorso
Paolo Samorì
Langue

en
Volume

10
Numéro

12
Page de début

10768
Page de fin

10777
Date de première publication

2016-11-15
ISSN

1936-0851
1936-086X
Titre de la source (revue, livre…)

ACS Nano
Résumé

Ultrasound-induced liquid-phase exfoliation (UILPE) is an established method to produce single- (SLG) and few-layer (FLG) graphene nanosheets starting from graphite as a precursor. In this paper we investigate the effect of the ultrasonication power
Show moreUltrasound-induced liquid-phase exfoliation (UILPE) is an established method to produce single- (SLG) and few-layer (FLG) graphene nanosheets starting from graphite as a precursor. In this paper we investigate the effect of the ultrasonication power in the UILPE process carried out in either N-methyl-2-pyrrolidone (NMP) or ortho-dichlorobenzene (o-DCB). Our experimental results reveal that while the SLGs/FLGs concentration of the NMP dispersions is independent of the power of the ultrasonic bath during the UILPE process, in o-DCB it decreases as the ultrasonication power increases. Moreover, the ultrasonication power has a strong influence on the lateral size of the exfoliated SLGs/FLGs nanosheets in o-DCB. In particular, when UILPE is carried out at ∼600 W, we obtain dispersions composed of graphene nanosheets with a lateral size of 180 nm, whereas at higher power (∼1000 W) we produce graphene nanodots (GNDs) with an average diameter of ∼17 nm. The latter nanostructures exhibit a strong and almost excitation-independent photoluminescence emission in the UV/deep-blue region of the electromagnetic spectrum arising from the GNDs’ intrinsic states and a less intense (and strongly excitation wavelength dependent) emission in the green/red region attributed to defect states. Notably, we also observe visible emission with near-infrared excitation at 850 and 900 nm, a fingerprint of the presence of up-conversion processes. Overall, our results highlight the crucial importance of the solvent choice for the UILPE process, which under controlled experimental conditions allows the fine-tuning of the morphological properties, such as lateral size and thickness, of the graphene nanosheets toward the realization of luminescent GNDs.
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DOI 10.1021/acsnano.6b03823
Titre abrégé de la source

ACS Nano
Type de publication

ACL
Domaine

Chimie/Matériaux
Audience

International