a) Schematic diagrams for the comparison of Na nucleation, deposition in Ti3C2 and CT‐Sn(II)@Ti3C2 matrixes. Binary phase diagrams of b) Na with Sn,59 c) Na with Cu.63

a) Schematic diagrams for the comparison of Na nucleation, deposition in Ti3C2 and CT‐Sn(II)@Ti3C2 matrixes. Binary phase diagrams of b) Na with Sn,59 c) Na with Cu.63

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Sodium (Na) metal is a promising alternative to lithium metal as an anode material for the next‐generation energy storage systems due to its high theoretical capacity, low cost, and natural abundance. However, dendritic/mossy Na growth caused by uncontrollable plating/stripping results in serious safe concerns and rapid electrode degradation. This...

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... Among the electrochemical ESDs (EESDs) family, rechargeable batteries (especially lithium-ion batteries (LIBs)), supercapacitors (SCs), and their hybrid forms are the most beneficial EESDs-based technology. Still, the same new storage techniques are underway for commercial use in the near future [43]. Batteries are used broadly nowadays, mostly in hybrid electric vehicles (EVs) and portable wearable electronic devices. ...
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... Additionally, we conducted a comparative analysis of the electrochemical performance of the representative MXene electrodes for Na metal anodes ( Figure S17 and Table S2, Supporting Information). [23][24][25][43][44][45][46][47][48][49][50] The findings indicate that our designed 3DP Nb 2 CT x /rGO electrodes demonstrate exceptional performance, particularly in terms of outstanding long-term cycling stability. ...
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... In terms of interfacial engineering, "zincophilic" coatings such as Ti 3 C 2 T x MXene (MX) were recently demonstrated to be particularly effective as an interfacial layer to achieve smooth deposition on metal anodes such as Li, Na, K, and Zn [24][25][26][27]. Ti 3 C 2 T x MXene can unlock fast electrochemical kinetics in the plating/stripping process due to its high electronic conductivity and rapid Zn-ion diffusion. ...
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... [35][36][37] Large interlayer spacing is more compatible with Na + (larger than Li + ) and boosts the kinetics of sodium ion. [38] The S-doping can enlarge the interlayer spacing of the materials, conducive to pseudocapacitive capacity. [39] Besides, C-S-S-C bonds situated at the carbon skeleton edge can enlarge the interlayer distance of the carbonaceous materials. ...
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... The most direct strategy is to increase the interlayer distance of MXene (Fig. 3d). By introducing large ions like Sn 2+ and cetyltrimethylammonium cation (CTA + ) as the pillars between the adjacent MXene layers, the electrode can fulfil the ion transport requirement for large-size ions like Na + or K + [55][56][57]. Additionally, changing the 2D layer-like structure in MXenes can offer high electrochemical performance in the beyond-lithium batteries. ...
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... Two-dimensional (2D) MXene materials have aroused the interest of scientists in numerous disciplines [35][36][37][38][39] Ti 3 C 2 T x MXene has the potential to be employed as an anode host for the deposition of metals in energy storage devices on account of its high metallic electrical conductivity (~10 4 S cm − 1 ) and ion-friendly hydrophilic property provided by the surface functional groups (OH, O, and F) [15,29,38,[40][41][42][43][44]. Nonetheless, 2D Ti 3 C 2 T x film is mostly restacked during structure formation and thus has a compact, dense structure with inaccessible sites and inhomogeneous nucleation sites on the surface, which provide hotspots for the development of mossy dendrites during plating and stripping in cycling and, eventually, cell death [15,29,40]. ...
... Two-dimensional (2D) MXene materials have aroused the interest of scientists in numerous disciplines [35][36][37][38][39] Ti 3 C 2 T x MXene has the potential to be employed as an anode host for the deposition of metals in energy storage devices on account of its high metallic electrical conductivity (~10 4 S cm − 1 ) and ion-friendly hydrophilic property provided by the surface functional groups (OH, O, and F) [15,29,38,[40][41][42][43][44]. Nonetheless, 2D Ti 3 C 2 T x film is mostly restacked during structure formation and thus has a compact, dense structure with inaccessible sites and inhomogeneous nucleation sites on the surface, which provide hotspots for the development of mossy dendrites during plating and stripping in cycling and, eventually, cell death [15,29,40]. It is inevitable to tailor the interspace of a nanostructured anode host and exert control over the initial nucleation site to maximize the performance of AFSMBs with excellent sodiophilicity and electrophilicity. ...
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... The XRD pattern in Figure 2a shows that the (104) peak of Ti 3 AlC 2 disappeared and the (002) peak of Ti 3 C 2 T x shifted toward a lower range, indicating the formation of a uniform, ordered layer structure in the Ti 3 C 2 T x . 27,28 The 2θ of the (002) peak was shifted from 6.2°for Ti 3 C 2 T x to 5.5°for h-Ti 3 C 2 T x (24 h), indicating the expansion of the d-spacing from 1.42 to 1.60 nm based on Bragg's law. The increase in d-spacing was favorable for the rapid diffusion of phosphate anions along the nanoscale channels between the nanosheets. ...
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Due to ultralow defect formation energy, borophene differs significantly from other 2D (two-dimensional) materials in that it is difficult to distinguish between its crystal and boron (B) vacancy defect. In contrast to other 2D materials like graphene, borophene does not form layers when it is in its bulk state. In addition, borophene NM’s atomic structure is different from graphene’s in that it consists of connected triangles rather than hexagons. This atomic configuration has gaps where atoms are missing, resulting in a flaw called a "hollow hexagon" (HH). In borophene phases, these HHs can be found in a variety of ratios. The phase intermixing of borophene is a brandnew example of an ’ordered’ defect discovered in 2D materials. The majority of 2D materials have flaws or disruptions to the atom arrangement at the boundaries between various domains or phases. Defects play a major influence in determining the properties of materials in a 2D system, because all atoms are virtually on the surface. For instance, the line defects along phase boundaries in borophene have no effect on the material’s electrical characteristics at ambient temperature, in contrast to insulating flaws in metallic graphene. The atoms at the borders of borophene easily fit along line faults and adopt the configuration of their neighbors, causing no disruption. Additionally, the line flaws do not disrupt the seamless structure of borophene and maintain its stability and metallic properties. Experimentally, all four borophene phases have been synthesized, and they are all metallic. A list of borophene NM’s special characteristics, including its negative Poisson’s ratio and extremely anisotropic Young’s modulus, is discussed. Here we also emphasized on B’s conductive and superconductive qualities. An overview of borophene NM’s uses in the energy sectors, including metal ion batteries, and supercapacitors (SCs), is covered in great length at the very end.
... MXene is an emerging two-dimensional (2D) transition metal carbide/nitride with high conductivity, abundant functional groups, good hydrophilicity, and high mechanical modulus [143]. The sodiophilic function groups (e.g., -O and -F) on the surface of MXene play important roles in reducing nucleation overpotential and inducing uniform Na nucleation [144]. Moreover, MXene has high electron and ion transport dynamics due to its high electronic conductivity and open cross-linked network. ...
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Sodium metal is one of the ideal anodes for high-performance rechargeable batteries because of its high specific capacity (~ 1166 mAh·g ⁻¹ ), low reduction potential (−2.71 V compared to standard hydrogen electrodes), and low cost. However, the unstable solid electrolyte interphase, uncontrolled dendrite growth, and inevitable volume expansion hinder the practical application of sodium metal anodes. At present, many strategies have been developed to achieve stable sodium metal anodes. Here, we systematically summarize the latest strategies adopted in interface engineering, current collector design, and the emerging methods to improve the reaction kinetics of sodium deposition processes. First, the strategies of constructing protective layers are reviewed, including inorganic, organic, and mixed protective layers through electrolyte additives or pretreatments. Then, the classification of metal-based, carbon-based, and composite porous frames is discussed, including their function in reducing local deposition current density and the effect of introducing sodiophilic sites. Third, the recent progress of alloys, nanoparticles, and single atoms in improving Na deposition kinetics is systematically reviewed. Finally, the future research direction and the prospect of high-performance sodium metal batteries are proposed.