The electronic structure and optical properties of Mn and B, C, N co-doped MoS2 monolayers
© Xu et al.; licensee Springer. 2014
Received: 15 July 2014
Accepted: 9 September 2014
Published: 6 October 2014
The electronic structure and optical properties of Mn and B, C, N co-doped molybdenum disulfide (MoS2) monolayers have been investigated through first-principles calculations. It is shown that the MoS2 monolayer reflects magnetism with a magnetic moment of 0.87 μB when co-doped with Mn-C. However, the systems co-doped with Mn-B and Mn-N atoms exhibit semiconducting behavior and their energy bandgaps are 1.03 and 0.81 eV, respectively. The bandgaps of the co-doped systems are smaller than those of the corresponding pristine forms, due to effective charge compensation between Mn and B (N) atoms. The optical properties of Mn-B (C, N) co-doped systems all reflect the redshift phenomenon. The absorption edge of the pure molybdenum disulfide monolayer is 0.8 eV, while the absorption edges of the Mn-B, Mn-C, and Mn-N co-doped systems become 0.45, 0.5, and 0 eV, respectively. As a potential material, MoS2 is widely used in many fields such as the production of optoelectronic devices, military devices, and civil devices.
Layered transition metal dichalcogenides (TMD) belong to a well-defined chemical and structural family characterized by strong covalent intralayer bonding and weak van der Waals interactions between adjacent layers[1, 2]. Transition metal oxides and sulfides have always been an interesting subject in experimental and theoretical works[3–9] due to their important role in lithium-ion batteries (LIB), flexible electronic devices, photoluminescence, valleytronics[13, 14], and field-effect transistors. Molybdenum disulfide (MoS2) monolayer contains hexagonal planes of Mo atoms lying between two hexagonal planes of S atoms, forming a sheet of S-Mo-S. Each Mo atom bonds with six neighboring S atoms through covalent bonds.
Cheng et al. have found that the formation energy of substitutional doping is formidably large in graphene, rendering doping in this 2D material a challenging issue. It has been proved that a very thin MoS2 owns a good property of lubrication. It is mainly because the binding energy between S atoms and metal materials is so strong that MoS2 has a great adsorbability on the metal surface. MoS2 can also be used as a kind of desulfurization catalyst[16, 17] for crude oil in the industry, indeed preventing the phenomenon of sulfur poisoning. Due to its good chemical stability, thermal stability, specific surface area, and high surface activity, MoS2 can be a utility material. Though its optical and electronic properties[18–24] have been discussed, MoS2 still has limitations in improving the optical property for the production of photodetectors in the industry. Doping in MoS2[25–27], as a typical 2D material, attracts more attention. Through a series of calculations, Mn doping and B (C, N) doping can improve the characters of MoS2[24, 25]. In order to get more ideal characters of MoS2, we calculated three structures including Mn-B, Mn-C, and Mn-N co-doped MoS2 monolayers in this paper. The MoS2 monolayer co-doped with Mn-C reflects magnetism. However, the systems co-doped with Mn and B (N) atoms exhibit semiconducting behavior with bandgaps smaller than those of the corresponding primitive state. Mn-B (C, N) co-doping all make the optical absorption edges generate the redshift phenomenon for the MoS2 monolayer, which results in the enhancement of absorption for infrared light in the MoS2 monolayer. The redshift degree of the Mn-N co-doped system is the largest. This result may open a new route to MoS2 in optical device applications.
Results and discussion
Formation energy and crystal structure
Etot[MoS2] and Etot[X] represent the total energy of the primitive MoS2 monolayer and the total energy doped with impurities, respectively. ni >0 means the number of atoms which are doped into the system, while ni <0 means the number of atoms which are replaced from the MoS2 monolayer. Ei represents the energy of the single atom. The smaller the value of the formation energy, the greater the stability of the structure. The formation energy under the circumstances of Mn and B, C, N co-doped MoS2 monolayers is 7.42, 7.03, and 7.56 eV, respectively. Obviously, the case of the Mn-C co-doped system obtains the most stable state.
The crystal structure of the co-doped MoS 2 monolayers
Density of states
However, both Mo15MnBS31 and Mo15MnNS31 are still semiconductors, which spin up and spin down symmetrically. In Mo15MnCS31, the role of Mn upon the conduction band is stronger than that in Mo15MnS32. This phenomenon is due to the Mn and C atoms sharing pairs of electrons. Meanwhile, the interaction between electric charges is reinforced and the polarization phenomenon generated. Consequently, the role of Mn-3d upon the conduction band around the Fermi level is reinforced.
In order to realize the effect of the Mn-3d orbit deeply, the GGA + U method is used. The results show us that the orbital coupling between C-2 s, C-2p and Mn-3d becomes stronger as U increases. And the electronic transition between B-2p, C-2 s, C-2p, N-2 s and Mn-3d becomes more active. Above all, the role of Mn-3d enhanced. Considering the Coulomb repulsion between the electrons, the results become convincing.
The optical properties of Mo15MnBS31, Mo15MnCS31, and Mo15MnNS31 all reflect the redshift phenomenon which leads to the MoS2 monolayer absorbing more infrared light. The optical property of the primitive state well agrees with studies before[37, 38].
In Figure 5b, the absorption edge of the pure molybdenum disulfide monolayer is 0.8 eV, corresponding to the electrons which transfer from the conduction band to the valence band partially, which is in very good agreement with the experimental value. The co-doped structures all reflect the redshift phenomenon, and the absorption edges of the Mn-B, Mn-C, and Mn-N systems become 0.45, 0.5, and 0 eV, respectively. And the value of absorption peaks decreased simultaneously. The redshift phenomenon shows us that the co-doped systems have better optical gas sensing property. Although the number of absorption peaks decreased, the energy range increased, which indicates that the wavelength range for the absorption became wider. In the high-energy region, the absorption of Mo15MnBS31, Mo15MnCS31, and Mo15MnNS31 is so little such that the MoS2 monolayer has high transmittance in the visible light region under these circumstances. These findings indicate that the pure MoS2 is more suitable to make a near-ultraviolet (6.0 ~ 6.5, 6.8 ~ 7.0, and 8.5 ~ 9.5 eV) photodetector than the MoS2 monolayer co-doped with Mo-B (C, N). But Mo15MnCS31 is the most suitable to make a near-ultraviolet (3.3 ~ 5.8 eV) photodetector. The Mn-B co-doped MoS2 monolayer is more suitable to make an infrared photodetector.
Figure 5c,d shows us the reflectivity and refractivity of the MoS2 monolayer. Mo15MnBS31, Mo15MnCS31, and Mo15MnNS31 all produce a series of peaks in the low-energy area and reflect the redshift phenomenon. These peaks are mainly due to the electronic transition of B-2p and Mn-4 s; C-2 s and Mn-3d, Mn-4 s; and N-2 s and Mn-4 s, respectively. Due to the active electronic transition between B-2p and Mn-4 s as well as the symmetry breaking induced by the Mn-B dopant, Mo15MnBS31 owns a maximum peak. On the contrary, in the infrared light region, Mo16S32 gets the minimum reflectivity. Hence, Mo16S32 obtains high transmittance in the infrared light region. The variation tendency of the primitive MoS2 monolayer in reflectivity is consistent with what Newaz has done.
According to our calculation, the electronic structure and optical properties of Mn and B, C, N co-doped MoS2 monolayers have been investigated through first-principles. As is shown, the MoS2 monolayer co-doped with Mn-C reflects magnetism and the magnetic moment is 0.87 μB. It is due to the Mn providing one more electron than the Mo atom; when C substitutes for the S atom, it needs more electrons to make the 2p orbit saturated. However, the co-doped systems with Mn and B (N) atoms exhibit semiconducting behavior with bandgaps smaller than those of the corresponding pristine state because of the effective charge compensation between Mn and B (N) atoms. And the energy bandgaps are 1.03 and 0.81 eV, respectively. Mn-B (C, N) co-doping all make the optical absorption edges generate the redshift phenomenon for the MoS2 monolayer, which results in the enhancement of the MoS2 monolayer absorbing infrared light. The absorption edge of the pure molybdenum disulfide monolayer is 0.8 eV, where the absorption edges of Mn-B, Mn-C, and Mn-N co-doped systems become 0.45, 0.5, and 0 eV, respectively. Mo15MnCS31 is easier to achieve in the experiments than other structures. As a potential material, it is necessary to realize the tunable bandgap in the MoS2 monolayer by surface adsorption. Furthermore, our research will progress towards quantum transport simulation and tunneling transistors like silicene[39, 40].
This work was supported by the National Natural Science Foundation of China (Grant Nos. 61172028, 11274143, and 11304121) and the Natural Science Foundation of Shandong Province (Grant No. ZR2010EL017).
- Friend H, Yoffe A: Layer compounds. Ann Rev Mater Sci 1973, 3: 147–170. 10.1146/annurev.ms.03.080173.001051View ArticleGoogle Scholar
- Levy F: Intercalated layered materials. Physics and Chem Mater with A 1979, 6: 99–100.Google Scholar
- Han SW, Kwon H, Kim SK: Band-gap transition induced by interlayer van der Waals interaction in MoS2. Phys Rev B 2011, 84: 045409.View ArticleGoogle Scholar
- Lebegue S, Eriksson O: Electronic structure of two-dimensional crystals from ab initio theory. Phys Rev B 2009, 79(11):115409.View ArticleGoogle Scholar
- Li T, Galli G: Electronic properties of MoS2 nanoparticles. J Phys Chem C 2007, 111(44):16195–16196.Google Scholar
- Ataca C, Sahin H, Akturk E: Mechanical and electronic properties of MoS2 nanoribbons and their defects. J Phys Chem C 2011, 115(10):3934–3941. 10.1021/jp1115146View ArticleGoogle Scholar
- Mak KF, Lee C, Shan J, Heinx TF: Atomically thin MoS2: a new direct-gap semiconductor. Phys Rev Lett 2010, 105: 136805.View ArticleGoogle Scholar
- Splendiani A, Sun L, Zhang Y: Emerging photoluminescence in monolayer MoS2. Nano Lett 2010, 10(4):1271–1275. 10.1021/nl903868wView ArticleGoogle Scholar
- Newaz AKM, Prasai D, Ziegler JI: Electrical control of optical properties of monolayer MoS2. Solid State Commun 2013, 155: 49–52.View ArticleGoogle Scholar
- Hwang H, Kim H, Cho J: MoS2 nanoplates consisting of disordered graphene-like layers for high rate lithium battery anode materials. Nano Lett 2011, 11: 4826–4830. 10.1021/nl202675fView ArticleGoogle Scholar
- Bertolazzi S, Brivio J, Kis A: Stretching and breaking of ultrathin MoS2. ACS Nano 2011, 5: 9703–9709. 10.1021/nn203879fView ArticleGoogle Scholar
- Eda G, Yamaguchi H, Voiry D, Fujita T, Chen M, Chhowalla M: Photoluminescence from chemically exfoliated MoS2. Nano Lett 2012, 11: 5111–5116.View ArticleGoogle Scholar
- Cao T, Wang G, Han W: Valley-selective circular dichroism of monolayer molybdenum disulphide. Nat Commun 2012, 3: 887–892.View ArticleGoogle Scholar
- Mak K, He K, Shan J, Heinz TF: Control of valley polarization in monolayer MoS2 by optical helicity. Nat Nanotechnol 2012, 7: 494–498. 10.1038/nnano.2012.96View ArticleGoogle Scholar
- Cheng YC, Zhu ZY, Mi WB: Prediction of two-dimensional diluted magnetic semiconductors: doped monolayer MoS2 systems. Phys Rev B 2013, 87: 100401.View ArticleGoogle Scholar
- Fan XB, Liu F, Yao SY: Preparation of MoS2 nanocatalyst and its application in hydrodesulfurization. J Cata 2012, 33: 1027–1031.Google Scholar
- Pollack SS, Makovsky LE, Brown FR: Identification by X-ray diffraction of MoS2 in used CoMoAl2O3 desulfurization catalysts. J Cata 1979, 59(3):452–459. 10.1016/S0021-9517(79)80015-9View ArticleGoogle Scholar
- Kam KK, Parkinson B: Detailed photocurrent spectroscopy of the semiconducting group VIB transition metal dichalcogenides. J Chem Phys 1982, 86(4):463–467. 10.1021/j100393a010View ArticleGoogle Scholar
- Young PA: Lattice parameter measurements on molybdenum disulphide. J Phys D Appl Phys 1968, 1(7):936. 10.1088/0022-3727/1/7/416View ArticleGoogle Scholar
- Böker T, Severin R, Müller A: Band structures of MoS2, MoSe2 and a-MoTe2: angle-resolved photoelectron spectroscopy in the constant-final-state mode and ab initio calculations. Phys Rev B 2001, 64: 235–305.View ArticleGoogle Scholar
- Kim C, Kelty S: Near-edge electronic structure in NbS2. J Chem Phys 2005, 123: 244705. 10.1063/1.2140708View ArticleGoogle Scholar
- Fang CM, Ettema ARHF, Haas C: Electronic structure of the misfit-layer compound (SnS)1.17NbS2 deduced from band-structure calculations and photoelectron spectra. Phys Rev B 1995, 52: 2336. 10.1103/PhysRevB.52.2336View ArticleGoogle Scholar
- Novoselov KS, Jiang D, Schedin F, Booth TJ: Two-dimensional atomic crystals. Proc Nat Acad Sci USA 2005, 102: 10451–10453. 10.1073/pnas.0502848102View ArticleGoogle Scholar
- Ayari A, Cobas E, Ogundadegbe O: Realization and electrical characterization of ultrathin crystals of layered transition-metal dichalcogenides. J Appl Phys 2007, 101: 014507. 10.1063/1.2407388View ArticleGoogle Scholar
- Yue Q, Chang S, Qin S: Functionalization of monolayer MoS2 by substitutional doping: a first-principles study. Phys Lett A 2013, 377(19):1362–1367.View ArticleGoogle Scholar
- Ramasubramaniam A, Naveh D: Mn-doped monolayer MoS2: an atomically thin dilute magnetic semiconductor. Phys Rev B 2013, 87(19):195201.View ArticleGoogle Scholar
- Sun QC, Mazumdar D, Yadgarov L: Spectroscopic determination of phonon lifetimes in rhenium-doped MoS2 nanoparticles. Nano Letter 2013, 13(6):2803–2808. 10.1021/nl401066eView ArticleGoogle Scholar
- Blaha P, Schwarz K, Madsen GKH, Kvasnicka D: WIEN2k, an augmented plane wave +local orbitals program for calculating crystal properties. 2001, 165–168.Google Scholar
- Perdew JP, Burke K, Ernzerhof M: Generalized gradient approximation made simple. Phys Rev Lett 1996, 77(18):3865. 10.1103/PhysRevLett.77.3865View ArticleGoogle Scholar
- Coehoorn R, Haas C, Dijkstra J: Electronic structure of MoSe2, MoS2, and WSe2. I. Band-structure calculations and photoelectron spectroscopy. Phys Rev B 1987, 35: 61–95.Google Scholar
- Kobayashi K, Yamauchi J: Electronic structure and scanning-tunneling-microscopy image of molybdenum dichalcogenide surfaces. Phys Rev B 1995, 51(23):17085. 10.1103/PhysRevB.51.17085View ArticleGoogle Scholar
- Ye LH, Freeman AJ, Delley B: Half-metallic ferromagnetism in Cu-doped ZnO: density functional calculations. Phys Rev B 2006, 73: 033203.View ArticleGoogle Scholar
- Xiao WZ, Wang LL, Xu L: First-principles study of magnetic properties in Ag-doped SnO2. Phys Status Solidi B 2011, 248(8):1961–1966. 10.1002/pssb.201046567View ArticleGoogle Scholar
- Pan H, Zhang YW: Edge-dependent structural, electronic and magnetic properties of MoS2 nanoribbons. J Mate Chem 2012, 22(15):7280–7290. 10.1039/c2jm15906fView ArticleGoogle Scholar
- Rahman G, Morbec JM: Intrinsic magnetism in nanosheets of SnO2: a first-principles study. J Magnetism Magn Mater 2013, 328: 104–108.View ArticleGoogle Scholar
- Ivanovskaya VV, Zobelli A, Gloter A: Ab initio study of bilateral doping within the MoS2-NbS2 system. Phys Rev B 2008, 78: 134104–134117.View ArticleGoogle Scholar
- Singh N, Jabbour G: Optical and photocatalytic properties of two-dimensional MoS2. J Euro Phys B 2012, 85(11):1–4.View ArticleGoogle Scholar
- Shi HL, Pan H: Quasiparticle band structures and optical properties of strained monolayer MoS2 and WS2. Phys Rev B 2013, 87(15):155304.View ArticleGoogle Scholar
- Quhe R, Fei R, Liu Q: Tunable and sizable band gap in silicene by surface adsorption. Sci Rep 2012, 2: 853–858.View ArticleGoogle Scholar
- Ni Z, Zhong H, Jiang X: Tunable band gap and doping type in silicene by surface adsorption: towards tunneling transistors. Nanoscale 2014, 6(13):7609–7618. 10.1039/c4nr00028eView ArticleGoogle Scholar
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