Dimensionality plays a special role in nature. From phase transitions to transport phenomena, two-dimensional (2d) systems often exhibit a strikingly different behavior from those with higher or lower dimensionality. Graphene [1] is the prototype 2d material and, as such, has unique mechanical, thermal, electronic, and optical properties, already proven outstanding for both fundamental research and applications [2,3]. Here we demonstrate optical trapping of individual graphene flakes in aqueous dispersion [4]. This enables the investigation of their Raman spectra in the optical trap. The modification of the Raman spectra due to colloidal metallic nanoparticles [7] of different shapes [8] added to the dispersion are investigated both by micro-Raman and Raman tweezers analysis. Graphite is exfoliated by ultrasonication in a water-surfactant solution, followed by ultracentrifugation. (Fig. 1). We do not use any functionalization nor oxidation, in order to retain the electronic structure of pristine graphene in the exfoliated layers [9]. We use dihydroxy sodium deoxycholate (SDC) as surfactant. We then place 75 microlitres of dispersion in a chamber attached to a piezo-stage with 1nm resolution. Optical trapping (Fig. 2a) is obtained by focusing a helium-neon (633 nm) laser through a 100X oil immersion objective (NA=1.3). The latter is coupled to a spectrometer through an edge filter. This allows us to use the same laser light both for optical trapping and for Raman scattering, realizing a Raman optical tweezers to directly probe the structure of the trapped flake. A typical Raman spectrum of trapped flakes measured at 633 nm is plotted in Fig. 2b. Besides the G and 2D peaks, this has significant D and D’ intensities, and the combination mode D+D’2950 cm−1. The large intensity of the D peak in Fig. 2b is assigned to the edges of our submicrometer flakes [10]. We note that the 2D band, although broader than in pristine graphene [5], is well fitted by a single Lorentzian lineshape. Thus, even if the flakes are multilayers, they are electronically almost decoupled.

Raman Optical Trapping of Graphene / Donato, M. G.; Faggio, G.; Bonaccorso, F.; Alfieri, D.; Santangelo, Saveria; Dandrea, C.; Fazio, B.; Gucciardi, P. G.; Ferrari, A. C.; Maragò, O. M.; Messina, Giacomo. - (2011). (Intervento presentato al convegno GraphITA 2011 tenutosi a Assergi-L'Aquila, Italy nel 15-18 May, 2011).

Raman Optical Trapping of Graphene

G. FAGGIO;SANTANGELO, Saveria;MESSINA, Giacomo
2011-01-01

Abstract

Dimensionality plays a special role in nature. From phase transitions to transport phenomena, two-dimensional (2d) systems often exhibit a strikingly different behavior from those with higher or lower dimensionality. Graphene [1] is the prototype 2d material and, as such, has unique mechanical, thermal, electronic, and optical properties, already proven outstanding for both fundamental research and applications [2,3]. Here we demonstrate optical trapping of individual graphene flakes in aqueous dispersion [4]. This enables the investigation of their Raman spectra in the optical trap. The modification of the Raman spectra due to colloidal metallic nanoparticles [7] of different shapes [8] added to the dispersion are investigated both by micro-Raman and Raman tweezers analysis. Graphite is exfoliated by ultrasonication in a water-surfactant solution, followed by ultracentrifugation. (Fig. 1). We do not use any functionalization nor oxidation, in order to retain the electronic structure of pristine graphene in the exfoliated layers [9]. We use dihydroxy sodium deoxycholate (SDC) as surfactant. We then place 75 microlitres of dispersion in a chamber attached to a piezo-stage with 1nm resolution. Optical trapping (Fig. 2a) is obtained by focusing a helium-neon (633 nm) laser through a 100X oil immersion objective (NA=1.3). The latter is coupled to a spectrometer through an edge filter. This allows us to use the same laser light both for optical trapping and for Raman scattering, realizing a Raman optical tweezers to directly probe the structure of the trapped flake. A typical Raman spectrum of trapped flakes measured at 633 nm is plotted in Fig. 2b. Besides the G and 2D peaks, this has significant D and D’ intensities, and the combination mode D+D’2950 cm−1. The large intensity of the D peak in Fig. 2b is assigned to the edges of our submicrometer flakes [10]. We note that the 2D band, although broader than in pristine graphene [5], is well fitted by a single Lorentzian lineshape. Thus, even if the flakes are multilayers, they are electronically almost decoupled.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.12318/12410
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