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A MXene is a two-dimensional early transition metal carbide or carbonitride, produced by etching the A element from a ]. This family of materials was discovered at ] in 2011.<ref name=Adv2011>M. Naguib, M. Kurtoglu, V. Presser, J. Lu, J. Niu, M. Heon, L. Hultman, Y. Gogotsi, M. W. Barsoum, Adv. Mater. 2011, 23, 4248.</ref> MXenes combine the metallic conductivity of transition metal carbides and hydrophilic nature because of their hydroxyl or oxygen terminated surfaces.<ref name=NaguibNano>M. Naguib, O. Mashtalir, J. Carle, V. Presser, J. Lu, L. Hultman, Y. Gogotsi, M. W. Barsoum, ACS Nano 2012, 6, 1322.</ref><ref>M. Naguib, J. Halim, J. Lu, L. Hultman, Y. Gogotsi, M. W. Barsoum, J. Am. Chem. Soc. 2013,135, 15966.
</ref> The following MXenes have been synthesized: Ti<sub>3</sub>C<sub>2</sub>, Ti<sub>2</sub>C, V<sub>2</sub>C, Nb<sub>2</sub>C, (Ti<sub>0.5</sub>,Nb<sub>0.5</sub>)<sub>2</sub>C, Ta<sub>4</sub>C<sub>3</sub>, (V<sub>0.5</sub>,Cr<sub>0.5</sub>)<sub>3</sub>C<sub>2</sub>, Ti<sub>3</sub>CN, and many more are predicted and analyzed computationally.<ref name=Adv>M. Naguib, V.N. Mochalin, M.W. Barsoum, Y. Gogotsi, 25th Anniversary Article: MXenes: A New Family of Two-Dimensional Materials, Advanced Materials, Volume 26, Issue 7, page 992-1005, 2014.</ref> A MXene is a two-dimensional early transition metal carbide or carbonitride, produced by etching the A element from a ]. This family of materials was discovered at ] in 2011.<ref name=Adv2011>M. Naguib, M. Kurtoglu, V. Presser, J. Lu, J. Niu, M. Heon, L. Hultman, Y. Gogotsi, M. W. Barsoum, Adv. Mater. 2011, 23, 4248.</ref> MXenes combine the metallic conductivity of transition metal carbides and hydrophilic nature because of their hydroxyl or oxygen terminated surfaces.<ref name=NaguibNano>M. Naguib, O. Mashtalir, J. Carle, V. Presser, J. Lu, L. Hultman, Y. Gogotsi, M. W. Barsoum, ACS Nano 2012, 6, 1322.</ref><ref>M. Naguib, J. Halim, J. Lu, L. Hultman, Y. Gogotsi, M. W. Barsoum, J. Am. Chem. Soc. 2013,135, 15966.
</ref> The following MXenes have been synthesized: Ti<sub>3</sub>C<sub>2</sub>, Ti<sub>2</sub>C, V<sub>2</sub>C, Nb<sub>2</sub>C, (Ti<sub>0.5</sub>,Nb<sub>0.5</sub>)<sub>2</sub>C, Ta<sub>4</sub>C<sub>3</sub>, (V<sub>0.5</sub>,Cr<sub>0.5</sub>)<sub>3</sub>C<sub>2</sub>, Ti<sub>3</sub>CN, and many more are predicted and analyzed computationally.<ref name=Adv>M. Naguib, V.N. Mochalin, M.W. Barsoum, Y. Gogotsi, 25th Anniversary Article: MXenes: A New Family of Two-Dimensional Materials, Advanced Materials, Volume 26, Issue 7, page 992-1005, 2014.</ref>


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* http://max.materials.drexel.edu * http://max.materials.drexel.edu
* http://nano.materials.drexel.edu * http://nano.materials.drexel.edu

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A MXene is a two-dimensional early transition metal carbide or carbonitride, produced by etching the A element from a MAX phase. This family of materials was discovered at Drexel University in 2011. MXenes combine the metallic conductivity of transition metal carbides and hydrophilic nature because of their hydroxyl or oxygen terminated surfaces. The following MXenes have been synthesized: Ti3C2, Ti2C, V2C, Nb2C, (Ti0.5,Nb0.5)2C, Ta4C3, (V0.5,Cr0.5)3C2, Ti3CN, and many more are predicted and analyzed computationally.

Synthesis

MXenes are produced by selectively etching out the A element from a MAX phase, which has the general formula Mn+1AXn, where M is an early transition metal, A is an element from group IIIA or IVA of the periodic table, X is C and/or N, and n = 1, 2, or 3. MAX phases have a layered hexagonal structure with P63/mmc symmetry, where M layers are nearly closed packed and X atoms fill octahedral sites. Therefore, Mn+1Xn layers are interleaved with the A element, which is metallically bonded to the M element. MAX phases are etched mainly by using strong etchants such as hydrofluoric acid (HF). Etching of Ti3AlC2 in aqueous HF at room temperature causes the A (Al) atoms to be removed, and the surface of the carbide layers to be terminated by O, OH, and/or F atoms. It has been shown how the higher the value of n in the formula, the more stable the MXene.

One possible method of synthesizing MXenes is etching a MAX phase in aqueous HF for a certain period of time that depends on the HF concentration and temperature at which the procedure is performed. After this, the mixture is centrifuged to separate the solid from the supernatant fluid, followed by washing the solid with deionized water until the pH of the suspension is between 4 and 6. This produces an accordion like structure, which can be referred to as a multilayer MXene (ML-MXene), or a few-layer MXene (FL-MXene) when there are fewer than five layers. Because surface terminations by functional groups in MXenes can occur, the naming convention Mn+1XnTx can be used, where T is a functional group.

Although theoretically possible to produce them, attempts to produce nitride-based MXenes have not yet been successful. The lower cohesion energy of Tin+1Nn compared to Tin+1Cn implies that the nitride structure is less stable, while the higher formation energy of Tin+1Nn from Tin+1AlNn relative to the formation energy of Tin+1Cn from Tin+1AlCn implies that the Al-N bond is stronger than the Al-C bond in their respective MAX phases. It is also possible that less-stable nitride MXenes had been produced but were dissolved in the etchant.

Structure

MXenes that have been produced have three structures inherited from MAX phases: M2C, M3C2, and M4C3. According to DFT (density functional theory) studies, there are two energetically favorable orientations for the terminating group (T) in Ti3C2T2: I and II. In configuration I, T is located above the hollow sites between three neighboring C atoms. In configuration II, T groups are located above C atoms on both sides of the MXene layers. A third stable configuration is possible, III, which occurs when one side of a MXene is terminated in configuration I, and the opposite in II. Relative DFT total energies suggest that the most stable configuration of these three is configuration I, and the least stable is configuration II.

Intercalation

Intercalation in MXenes is possible because of the weak bonds between layers. Different species can intercalate MXenes, whether organic, inorganic, or ionic. Among molecules that have been intercalated into Ti3C2Tx are dimethyl sulfoxide (DMSO), hydrazine, and urea. For example, N2H4 (hydrazine) can be intercalated into Ti3C2(OH)2 with the molecules parallel to the MXene basal planes to form a monolayer. Intercalaction increases the MXene c lattice parameter, which weakens the bonds between MX layers. Ions, including Li, Pb, and Al, can also be intercalaction into MXenes, either spontaneously or when a negative potential is applied to a MXene electrode.

Properties

With a high electron density near the Fermi level, MXene monolayers are predicted to be metallic according to DFT studies. In MAX phases, N(EF) is mostly M 3d orbitals, and the valence states below EF are composed of two sub-bands. One, sub-band A, made of hybridized Ti 3d-Al 3p orbitals, is near EF, and another, sub-band B, -10 to -3 eV below EF which is due to hybridized Ti 3d-C 2p and Ti 3d-Al 3s orbitals. Said differently, sub-band A is the source of Ti-Al bonds, while sub-band B is the source of Ti-C bond. Removing A layers causes the Ti 3d states to be redistributed from missing Ti-Al bonds to delocalized Ti-Ti metallic bond states near the Fermi energy in Ti2, therefore N(EF) is 2.5-4.5 times higher for MXenes than MAX phases.

Only bare-surface MXenes exhibit magnetic properties; Cr2C, Cr2N, and Ta3C2 are ferromagnetic, Ti3C2 and Ti3N2 are antiferromagnetic. Electronic properties of MXenes are also dependent on surface groups. While Ti3C2 is a metallic conductor, addition of surface groups give rise to small band gaps, 0.05 eV for Ti3C2(OH)2 and 0.1 eV for Ti3C2F2.

Another interesting trait of MXenes is their mechanical properties. Their M-C and M-N bonds are some of the strongest known. High elastic moduli for MXenes have been predicted.

Applications

Because of spontaneous intercalation in aqueous salt solutions of cations between Ti3C2Tx layers, MXenes can be used to produce outstanding supercapictors. MXenes’ chemistries, morphologies, and electrical conductivities make them ideal candidates for applications including sensors, catalysts, conductive reinforcement additives to polymers, and energy storage. Although MXenes' gravimetric capacities may not be as high as that of Si anodes in lithium-ion batteries, their advantage is offering a high cycling rate with good capacity. Because MXenes exhibit high cycling rates, they are good candidates for hybrid cells, which combine high energy densities characteristic of lithium ion batteries and high power densities of electrical double layer capacitors. MXenes have also shown high volumetric capacitance on aqueous electrolytes.

Intercalation of MXenes by Na, Mg, and Al suggests that they can be used in multivalent ion batteries other than lithium ion batteries.

It is expected that MXenes used as additives in polymers can provide excellent mechanical properties and good electrical conductivity.

References

  1. ^ M. Naguib, M. Kurtoglu, V. Presser, J. Lu, J. Niu, M. Heon, L. Hultman, Y. Gogotsi, M. W. Barsoum, Adv. Mater. 2011, 23, 4248.
  2. ^ M. Naguib, O. Mashtalir, J. Carle, V. Presser, J. Lu, L. Hultman, Y. Gogotsi, M. W. Barsoum, ACS Nano 2012, 6, 1322.
  3. M. Naguib, J. Halim, J. Lu, L. Hultman, Y. Gogotsi, M. W. Barsoum, J. Am. Chem. Soc. 2013,135, 15966.

  4. ^ M. Naguib, V.N. Mochalin, M.W. Barsoum, Y. Gogotsi, 25th Anniversary Article: MXenes: A New Family of Two-Dimensional Materials, Advanced Materials, Volume 26, Issue 7, page 992-1005, 2014.
  5. Z. Sun, D. Music, R. Ahuja, S. Li, J. M. Schneider, Phys. Rev. B 2004, 70, 092102.

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  8. C. Eames, M. S. Islam, Ion Intercalation into Two-Dimensional Transition-Metal Carbides: Global Screening for New High-Capacity Battery Materials, Journal of the American Chemical Society Article ASAP, 13 Oct. 2014.
  9. ^ I. R. Shein, A. L. Ivanovskii, Comput. Mater. Sci. 2012, 65, 104.
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M. Estili, Y. Sakka, Y. Kawazoe, Adv. Funct. Mater. 2012, 23, 2185.
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  12. M. R. Lukatskaya, O. Mashtalir, C. E. Ren, Y. Dall’Agnese, P. Rozier, P. L. Taberna, M. Naguib, P. Simon, M. W. Barsoum, Y. Gogotsi, Science 2013, 341, 1502.
  13. J. R. Szczech, S. Jin, Energy Environ. Sci. 2011, 4, 56.

  14. M. Heon, S. Lofland, J. Applegate, R. Nolte, E. Cortes, J. D. Hettinger, P.-L. Taberna, P. Simon, P. Huang, M. Brunet, Y. Gogotsi, Energy Environ. Sci. 2011, 4, 135.

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