Enhanced optical absorption of Fe-, Co- and Ni- decorated Ti3C2 MXene: A first-principles investigation
Introduction
As ignited by the fabrication of graphene [1,2], two-dimensional (2D) materials have experienced an increasing attention in recent years and have found wide applications toward electronics, photonics, energy, and environmental devices [[3], [4], [5], [6], [7], [8], [9]]. However, it remains great challenge to apply 2D materials for efficient optical absorption [10,11]. Many efforts through increasing numbers of layers or surface decoration [12,13] have been devoted to further improve optical absorption, but the effect is very limited. New optical absorption materials that can overcome this problem are needed.
MXenes, a large class of 2D carbides, nitrides, and carbonitrides, are recognized as a new family to the 2D world in 2011 [14,15]. The general formula of MXene is Mn+1XnTx (n = 1,2,3), where M represents a transition magnetic metals element, such as Ti, V, Mo, and X represents C, N, or CN, T generally refers to terminal groups distributed on the surface, such as –O, –OH, –F. MXene can be produced by selectively etching the A layer (HF aqueous solution as an etchant) from its corresponding MAX phase at room temperature, where A is a group IIIA to VIA element [16,17]. MXene has high electrical conductivity and extensive chemical properties, in energy storage, electromagnetic interference (EMI) shielding [[18], [19], [20]], transparent conductors [21,22], gas and pressure sensors [[23], [24], [25], [26]], water purification [[27], [28], [29], [30]], photocatalysis [31], Electrocatalysis [32,33], thermoelectrics [34,35] and plasmons have important research value and huge application potential [36].
Lots of theoretical calculations [[37], [38], [39], [40], [41], [42]] have shown that MXenes are mostly conductors, and the conductivity is mainly contributed by the d-orbital electrons of transition magnetic metals. The types of functional groups [41], temperature [43], stress [44], and layer thickness of MXene [45] can all affect the electronic structure and physical properties of MXene to varying degrees. Berdiyorov G R46 studied the effect of surface termination on the dielectric and optical properties of Ti3C2T2 (T = F, O, OH) MXene. It was found that the surface functionalization have a significant impact on the optical properties of MXene [47], where the oxidized samples showed greater absorption compared to the original MXene. Hart J L et al. [48] correlate MXene surface de-functionalization with increased electronic conductivity through in situ vacuum annealing, electrical biasing, and spectroscopic analysis within the transmission electron microscope. These indicate that MXene has the potential to improve electronic conductivity and enable MXene's transition between metals and semiconductors. Anasori B et al. [49] have demonstrated that two-dimensional transition magnetic metals carbides can transform MXene from metal to semiconductor behavior by replacing titanium on the surface of MXene with molybdenum. Calculations of density functional theory (DFT) indicate that Ti3C2Tx is a metal, while OH-terminated Mo–Ti MXene is a semiconductor with a narrow band gap. Bandyopadhyay A et al. [50] use the first-principles simulations to study the structure and magnetoelectronic behavior of point defects that are most likely to occur in the MXene system. The results show that the layered material exhibits outstanding metal-to-semiconductor or semiconductor-to-metal transitions. In addition, unpaired electrons in the spin-splitting d orbitals are predicted, which may lead to novel visible-light response behavior.
The variety of transition magnetic metals and surface functional groups provide MXene with a great deal of flexibility to extend applications, by controlling the combination of transition magnetic metals and X elements to control its surface chemical properties Peyghan A A et al. [51] used first-principles calculations to study the application of graphene decorated with Ni (Pd) as a methylphenol storage material. The results show that, unlike the original graphene, metal-modified flakes can effectively interact with CH3OH molecules and decoration of the Ni and Pd atoms on the surface of graphene induces some changes in the electronic properties of the sheet and its Eg remained unchanged after the adsorption of CH3OH molecules. Sun M et al. [52] also studied the structure, electrons, and magnetic properties of Sn atoms adsorbed on the original graphene through first-principles calculations. The results show that the adsorption of Sn atoms on the original graphene increases the Fermi level, but the unique Dirac point structure remains intact, and the semiconductor graphene with zero band gap also becomes metallic and obtains magnetic moment. It is well demonstrated that surface decoration on low-dimensional nanomaterials is one of effective way to open energy gap, giving rise to promotion optical absorption. Besides, from experience of our previous work [53], magnetic Ni-decoration on graphene which accomplished by enhancing the plasma energy could effectively improve the optical absorption. Comparatively, it is reasonable to assume that transition magnetic metals (Fe-, Co-, Ni-) decoration is favorable to promote optical absorption performance.
Driven by the demand of broadening applications in terms of optical absorption and photoelectric devices, the effect of surface adsorption of transition magnetic metals (Fe-, Co-, Ni-) on the electronic structure and optical properties of Ti3C2 MXene is studied comparatively. Based on first-principles density functional theory, depending on the location and type of adsorption, the electronic structure and optical performance of MXene are regulated and enhanced. Improving the electrical conductivity and light absorption properties of MXene through doping modification (adsorption/embedding) will provide theoretical support and technical means for the regulation of the microscopic physical properties of graphene-like two-dimensional materials.
Section snippets
Calculation methods
The CASTEP module of Materials Studio software based on the density functional theory (DFT) [54]. Spin-polarized calculation with plane-wave pseudopotential method was used to optimize the geometric structure and calculate the electronic structure. The exchange-correlation energy is described by the generalized gradient approximation (GGA) using the Perdew-Burke-Ernzerhof (PBE) function [55,56]. The plane wave energy cut-off is 450 eV. In structural optimization, the self-consistent convergence
Results and discussion
In order to find the most suitable interaction site, the structure of the transition metal (Fe-, Co- and Ni-) adsorption on the top, hole and bridge sites of Ti3C2 was optimized. Calculated results have shown that adsorption energy of Fe–Ti3C2 at these three sites are −5.44eV, −5.56eV, −5.26eV, while −4.88eV, −5.17eV, −4.08eV in Co–Ti3C2, and -4.22eV, −4.41eV, −3.25eV in Ni–Ti3C2 (take the absolute value), respectively. From this point of view, atoms Fe, Co and Ni prefer to adsorb on the hole
Conclusion
In summary, the structural and optical properties of transition magnetic metals (Fe-, Co- and Ni-) doped Ti3C2 MXene were studied using density functional theory. Results show that surface adsorption has a significant impact on the performance of the Ti3C2 nanomaterials. Interlamellar spacing between Ti-layer and C-layer is inclined to expand after surface decoration with Fe-, Co-, Ni-terminals. Besides, Ti3C2 MXene remains metallic properties after decoration with Fe-, Co- and Ni-terminals,
Author statement
Xiao Wang and Heng Luo conceived the idea. Xiao Wang and Chen Li performed the simulations, and made substantial contributions to the acquisition, analysis, and interpretation of data for the work. Xiao Wang and Heng Luo wrote the manuscript. Shengxiang Huang, Lianwen Deng, Chen Li, Yan Xu, Yazhe Yan, and Zhexiang Tang revised the manuscript. Heng Luo revised the manuscript and supervises this work.
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
This work is supported by the National Key Research and Development Program of China (Grant No. 2017YFA0204600), and the National Natural Science Foundation of China (Grant No. 51802352). Authors gratefully acknowledge Dr. Yiren Wang (Central South University) for her helpful comments and suggestions.
References (57)
- et al.
Appl. Surf. Sci.
(2017) - et al.
Appl. Surf. Sci.
(2018) - et al.
Adv. Mater.
(2018) - et al.
Carbon
(2016) - et al.
Optik
(2018) - et al.
J. Alloys Compd.
(2015) - et al.
J. Magn. Magn Mater.
(2019) - et al.
Appl. Surf. Sci.
(2019) - et al.
Flatchem
(2018) - et al.
Comput. Mater. Sci.
(2018)
Compos. Appl. Sci. Manuf.
Mater. Des.
Adv. Mater.
Appl. Surf. Sci.
Carbon
Science
Nat. Mater.
Nanoscale
Chem. Rev.
Compos. Appl. Sci. Manuf.
Diamond and Related Materials
J. Appl. Phys.
Adv. Mater.
Chem. Mater.
J. Appl. Phys.
Sci. Rep.
J. Appl. Phys.
Nanoscale
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