Dang Van Thanha,
Chien-Chung Pana,
Chih-Wei Chub and
Kung-Hwa Wei*a
aDepartment of Material Science and Engineering, National Chiao Tung University, Hsinchu 300, Taiwan. E-mail: khwei@mail.nctu.edu.tw; Fax: +886-35-724-727
bResearch Center for Applied Sciences, Academia Sinica, Taipei, 11529, Taiwan
First published on 18th March 2014
We demonstrate an efficient method for the production of few-layer MoS2 nanosheets through exfoliation of bulk MoS2 compounds that were subject to quenching in liquid N2 and subsequent ultrasonication. This solution-based method, which involves a “quenching cracks” phenomenon, was performed open to the atmosphere. Subsequent ultrasonication of the exfoliated MoS2 in solution provided us with MoS2 nanosheets comprising two to four layers.
Quenching is one of the most fundamental yet complex processes in the heat treatment of metals; it involves the surface of a sample being suddenly cooled in a solution medium, such as oil or liquid N2.29 The instant cooling on the surface induces quenching cracks because of different quenching stresses between the surface and the interior of the sample. In MoS2, each layer of Mo atoms is sandwiched between two layers of hexagonally close-packed S atoms, with the adjacent layers, bound by weak van der Waals interactions, readily exfoliating into individual MoS2 nanosheets upon quenching with liquid N2 and ultrasonication; as a result, we suspected that the quenching cracks phenomenon might be involved in breaking van der Waals force bonded MoS2 layers in the bulk state to produce MoS2 nanosheets. Recently, high-quality single and few-layer graphene sheets have been synthesized through rapid quenching of hot bulk highly ordered pyrolytic graphite (HOPG) and expandable graphite (EG) in aqueous solutions of 1.0 wt% NH4HCO3 and hydrazine hydrate, respectively.30,31 These processes involve rapid expansion of HOPG/EG at high temperature to weaken van der Waals forces and then rapid quenching of the heated samples in appropriate quenching media to form graphenes. To the best of our knowledge, the quenching approach has not been adopted previously for the production of MoS2 nanosheets.
In the present study, we stirred a mixture of MoS2 and KOH at 80 °C for 24 h and then quenched the sample in a matter of a few seconds to low temperature in liquid N2. The stresses generated from the sudden, large temperature gradient between the surface and the interior of the sample during this quenching process disrupted the van der Waals forces binding these MoS2 layers and resulted in MoS2 nanosheets. The resulting liquid N2–quenched MoS2 served as a precursor for the production of MoS2 nanosheets through solution-based exfoliation [see detailed experimental conditions in the ESI†]. Unlike previously employed quenching-based methods,30,31 this approach does not require either a rapid heating process or a special quenching medium. Thus, the major advantages when using this quenching approach for the production of MoS2 nanosheets from MoS2 powder are (i) MoS2 nanosheets can be derived from commercially available MoS2 powder without the need for Li+ intercalation prior to ultrasonication (ii) environmental friendliness, and (iii) facile operation open to the atmosphere.
Fig. 1 compares the Raman spectra of the exfoliated MoS2 with that of bulk MoS2. The spectrum of the bulk MoS2 displays bands at 376 and 403.2 cm−1 representing the A1g and E2g modes, respectively, while that of the exfoliated MoS2 features these bands at 383.8 and 405.2 cm−1, respectively; the frequency difference for of the latter (21.4 cm−1) is smaller than that for the former (27.2 cm−1), consistent with the Raman signature of MoS2 nanosheets comprising two to four layers.11,23
![]() | ||
Fig. 1 Raman spectra of bulk MoS2 and exfoliated MoS2 nanosheets processed using the liquid N2-exfoliation process. |
Fig. 2 presents an AFM image of a sample prepared by spin-coating a diluted solution (0.05 wt%) of exfoliated MoS2 onto the surfaces of a Si/SiO2 substrate and then drying in air. The lateral dimension of this exfoliated nanosheet was approximately 3.0 μm; its thickness was approximately 1.5 nm, corresponding to approximately two layers, based on the thickness of a single MoS2 layer being 0.7 nm—again, consistent with our production of few-layer MoS2 nanosheets. AFM images of other individual nanosheets (see ESI†) revealed that the thickness varied from 1.5 to 3.5 nm and the lateral dimensions from 0.5 to 3.5 μm. For further examination of an individual sheet-like nanostructure, Fig. 3 presents a TEM image of an exfoliated MoS2 product. It indicates that the sheets were flat, folded, and slightly transparent to the electron beam. A selected-area electron diffraction pattern (SAED) of the flat area of the nanosheet (inset to Fig. 3) reveals the typical six-fold symmetry of MoS2, indicating that the MoS2 sheets obtained using this method had good crystallinity; furthermore, point energy dispersive X-ray spectroscopy (EDS) from the same area revealed the presence of Mo and S atoms in a 1:
2 ratio, further confirming the formation of MoS2 nanosheets. We consider a possible two-step mechanism for the exfoliation of the liquid N2–quenched MoS2 powder. The first step of the quenching process involved gradual heating of the bulk MoS2 powder at a moderate temperature (80 °C, 24 h), resulting in a uniform dispersion of MoS2 flakes. The hot flake-like MoS2 particles were then cooled rapidly to low temperature in liquid N2. Because the surfaces of the hot flake-like MoS2 particles cooled faster than their interiors, quenching stresses occurred instantly upon contact with the liquid N2, leading to cracking of bonds between the layers of weakly bonded MoS2 layers, instantly freezing the cracks within the liquid N2 medium. The interaction between the hot flake-like MoS2 particles and the liquid N2 quenching medium resulted in quenching-cracked layers that allow further ultrasonic-facilitated exfoliation. Then, the detachment of MoS2 layers preferentially occurs at these quenching-cracked layers via ultrasonication and subsequent re-dispersion in chloroform. To further identify the mechanism behind this quenching approach, we exfoliated MoS2 solutions in both DI water and in aqueous KOH with and without the quenching process. The MoS2 nanosheets prepared from exfoliation of bulk MoS2 in DI water with and without quenching are termed MoS2-DIQ and MoS2-DI, respectively, and the MoS2 nanosheets prepared from exfoliation of bulk MoS2 in aqueous KOH with and without quenching are termed MoS2-KOHQ and MoS2-KOH, respectively. Table 1, Fig. S1 and S2† provide details of the experimental methods and the obtained results. We observed that exfoliation of MoS2 in aqueous KOH was greater than that in DI water. We suspect that aqueous KOH created better conditions for uniform dispersion of the flake-like MoS2 particles than did DI water, leading to more-uniform quenching on the surfaces of the hot flake-like MoS2 particles. One possible reason for the more uniform dispersion of flake-like MoS2 in the presence of KOH is that KOH can dissociate into K+ and OH− ions, and K+ ion might intercalate into the layered MoS2 in bulk, which facilitates exfoliation.
![]() | ||
Fig. 3 TEM image of a MoS2 sample processed from a dispersion of exfoliated MoS2; inset: SAED pattern and EDS spectrum of the in situ-recorded area. The Cu signal arose from the TEM support grid. |
Exfoliation | Results | |
---|---|---|
With quenching | Without quenching | |
Solution of MoS2 in DI water | Large amounts of exfoliated sheets having a thickness of 3 nm; difference in frequency between the A1g and E2g signals of ca. 22.2 cm−1, but not uniform among sheets | Small amounts of exfoliated sheets having a thickness of 5 nm; difference in frequency between the A1g and E2g signals of ca. 25.4 cm−1. Flake-like MoS2 particles did not fully exfoliate and remained on the surfaces of the sheets. Obtained sheets were relatively thick, with a lack of uniformity among them |
KOH-based MoS2 solution | Large amounts of uniformly exfoliated sheets having a thickness of 2 nm; difference in frequency between the A1g and E2g signals was ca. 21.4 cm−1 | Small amounts of exfoliated sheets having a thickness of 5 nm; difference in frequency between the A1g and E2g signals was ca. 25.8 cm−1. Obtained sheets were relatively thick, with a lack of uniformity among them |
In conclusion, we have synthesized MoS2 nanosheets from commercially available bulk MoS2 through a two-step process involving quenching in liquid N2 and subsequent exfoliation through sonication. To the best of our knowledge, this paper provides the first example of the use of quenching technology for the preparation of MoS2 nanosheets at low temperature and under atmospheric pressure. This method is quite promising because of its highly efficient, green, and facile operation.
Footnote |
† Electronic supplementary information (ESI) available: Details on experimental procedures. See DOI: 10.1039/c4ra00297k |
This journal is © The Royal Society of Chemistry 2014 |