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Journal ArticleDOI

2D metal carbides and nitrides (MXenes) for energy storage

17 Jan 2017-Nature Reviews Materials (Nature Publishing Group)-Vol. 2, Iss: 2, pp 16098
TL;DR: More than twenty 2D carbides, nitrides and carbonitrides of transition metals (MXenes) have been synthesized and studied, and dozens more predicted to exist.
Abstract: The family of 2D transition metal carbides, carbonitrides and nitrides (collectively referred to as MXenes) has expanded rapidly since the discovery of Ti3C2 in 2011. The materials reported so far always have surface terminations, such as hydroxyl, oxygen or fluorine, which impart hydrophilicity to their surfaces. About 20 different MXenes have been synthesized, and the structures and properties of dozens more have been theoretically predicted. The availability of solid solutions, the control of surface terminations and a recent discovery of multi-transition-metal layered MXenes offer the potential for synthesis of many new structures. The versatile chemistry of MXenes allows the tuning of properties for applications including energy storage, electromagnetic interference shielding, reinforcement for composites, water purification, gas- and biosensors, lubrication, and photo-, electro- and chemical catalysis. Attractive electronic, optical, plasmonic and thermoelectric properties have also been shown. In this Review, we present the synthesis, structure and properties of MXenes, as well as their energy storage and related applications, and an outlook for future research. More than twenty 2D carbides, nitrides and carbonitrides of transition metals (MXenes) have been synthesized and studied, and dozens more predicted to exist. Highly electrically conductive MXenes show promise in electrical energy storage, electromagnetic interference shielding, electrocatalysis, plasmonics and other applications.

Summary (3 min read)

Introduction

  • 2D materials have unusual electronic, mechanical and optical properties1-6, which have led them to be extensively studied in the past decade for diverse applications.
  • They can also serve as convenient building blocks for a variety of layered structures, membranes and composites7.
  • Transition metal carbides, carbonitrides and nitrides are among the latest additions to the 2D world15-21.
  • 1) with dozens more predicted to exist and studied in silico (marked with grey in FIG.
  • 1). Density functional theory (DFT) calculations showed that for certain combinations of transition metals, ordered MXenes are energetically more stable than their solidsolution counterparts and more than 25 different ordered MXenes have been predicted20.

Synthesis of MXenes

  • MXenes are made by selective etching of certain atomic layers from their layered precursors, such as MAX phases.
  • Highly selective etching is the key condition for making MXenes.
  • It is also possible to synthesize MXenes from non-MAX phase precursors39-41.
  • This phase, despite its similarity to MAX phases, has two A-element layers (Ga) separating the carbide layers.
  • Zr3C2Tx was synthesized from another non-MAX-phase precursor by selectively etching aluminium carbide (Al3C3) layers from Zr3Al3C5 41, instead of just the Al layers.

Delamination

  • Because multilayered MXenes have two- to sixfold stronger interlayer interactions than that in graphite and bulk MoS260, simple mechanical exfoliation provides a low yield of single layers.
  • There are only two reports of Scotch tape exfoliation of multilayer MXene into single flakes61,62 and the remainder have been delaminated via intercalation (FIG. 2d).
  • MXenes can be intercalated with a variety of polar organic molecules, such as hydrazine, urea and dimethyl sulfoxide (DMSO), isopropylamine or large organic base molecules such as tetrabutylammonium hydroxide , choline hydroxide or n-butylamine63.
  • When etching with a fluoride salt mixed with an acid (for example, HCl and LiF), no additional molecule is needed, because etched MXene is intercalated with metal cations (Supplementary information S2 (table)).
  • In general, the resulting aqueous colloidal MXene suspensions are stable (FIG. 2d) and do not aggregate owing to the negative zeta potential of the MXene flakes69.

Structure of the MXene layer

  • Similar to their MAX precursors, M atoms in MXenes are arranged in a close-packed structure and X atoms fill the octahedral interstitial sites.
  • Here, the capital Roman and Greek letters correspond to the M and X positions, respectively.
  • MXenes overall crystal is a hexagonal close packed structure.
  • In M2X, M atoms follow ABABAB ordering (hexagonal close-packed stacking), whereas in M3C2 and M4C3, M atoms have ABCABC ordering (face-centred cubic stacking).
  • The latter two have been stabilized by inserting another M element (for example, Ti) in the structure to form an ordered double transition metal Mo2TiC2Tx and Mo2Ti2C3Tx (FIG.

Surface terminations

  • MXenes synthesized using acidic fluoride-containing solutions have a mixture of –OH, – O and –F terminations, with the chemical formula Mn+1Xn(OH)xOyFz.
  • Many studies have considered a specific surface termination (for example, pure –OH, –O or –F) and predicted the MXenes’ properties18,24,71-85.
  • In general, milder etching and delamination conditions produce larger MXene flakes with lower defect concentrations (FIG.
  • 3i)67. Ti3C2Tx flakes of 3–6-µm lateral size with minimal defects have been produced via mild delamination (FIG.
  • Different concentrations of HF give different surface termination ratios87.

Stability

  • Single MXene flakes are not indefinitely stable in environments with oxygen and water present98.
  • High-temperature stability of MXenes dependens on their composition and the environment.
  • Recently, it was shown that Ti3C2Tx is stable at 500 ºC in an Ar atmosphere, but some TiO2 crystals form, decorating the edges of the particles99.
  • XRD results indicated MXene phase transformation by having strong peaks of cubic TiCx, which is the most stable phase at 1200 ºC in the nonstoichiometric TiC phase diagram52.
  • The better thermal stability of Zr3C2 can be explained by its structure being more energetically favourable than bulk ZrC, in contrast to Ti3C2, which is metastable relative to bulk cubic TiC41.

Mechanical and physical properties

  • The rich transition metal chemistry of MXenes (FIG.
  • This suggests applications of MXene filmsin transparent conductive coating and optoelectronics.
  • Semiconductor-like behaviour of Ti2CO2 was observed after thermal annealing of Ti2CTx at 1100 ºC under Ar/H262.
  • In general, a low concentration of defects and large flake size result in higher conductivity.
  • Of all MXenes, two — Cr2CTx and Cr2NTx — have been predicted to possess a magnetic moment, even with surface terminations18,108; however, their magnetic nature is not clear yet.

MXenes in batteries

  • MXenes have wide chemical and structural variety.
  • The gravimetric capacity of Ti2CTx for Li+ uptake is ~1.5 times higher than that of Ti3C2Tx prepared in the same way63,135, also known as This was confirmed experimentally.
  • Interestingly, further decrease in potential (regions II and III in FIG.
  • Note that the formation of an additional metal layer was predicted for Na+ and other ions, which would result in a doubling of the capacity.
  • MXene-based composite electrodes hold particular promise for high-performance, highrate batteries.

MXene-based electrochemical capacitors

  • MXenes can be spontaneously intercalated by polar organic molecules63-65 and metal ions63,145.
  • When HFproduced Ti3C2Tx was chemically modified using KOH151, N2H4 95, or DMSO136,145 solutions, the gravimetric capacitance values improved by a factor of two to seven, depending on the electrolyte being used, with the most dramatic improvements demonstrated in acidic electrolytes.
  • Mo2CTx40 and Mo2TiC2Tx20 showed high volumetric capacitance with rectangular cyclic voltammetry profiles.
  • Another important fact to keep in mind is that MXenes demonstrate excellent performance when cathodic potentials are applied; yet when the material is subjected to a positive potential in aqueous electrolyte (more than ~0.2–0.4.
  • Also, because organic electrolytes have a lower conductivity and can feature large organic ions like the tetrabutylammonium cation, the introduction of conductive spacers, such as CNTs, is important for improving the accessibility to ions and, therefore, the capacitive and rate performance.

Conclusions

  • 2D carbides, carbonitrides and nitrides were produced in the past 5 years by selective etching and exfoliation of layered ternary precursors forming a large family of 2D materials named MXenes.
  • Hydrophilicity and high surface charge (negative zeta potential exceeding −30 mV) lead to stable water-based colloidal solutions that do not require surfactants for stabilization.
  • High metallic conductivity has been reported for Ti3C2Tx Cations, including multivalent ones, and polar organic molecules intercalate MXenes allowing for control of interlayer spacing, and enabling use of MXenes in energy-storage applications, as well as water desalination and purification.
  • This not only explains how high capacitance can be demonstarted by a material with a moderate surface area, but also opens new avenues for achieving high energy density storage at high charging rates.

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B. Anasori et al. Nature Reviews Materials
1
2D metal carbides and nitrides (MXenes) for energy storage
Babak Anasori, Maria R. Lukatskaya and Yury Gogotsi
A.J. Drexel Nanomaterials Institute and Department of Materials Science & Engineering,
Drexel University, Philadelphia, PA 19104, USA
Correspondence to Y.G.: gogotsi@drexel.edu
((Web summary, 40 words))
More than twenty 2D carbides, nitrides and carbonitrides of transition metals (MXenes)
have been synthesized and studied, and dozens more predicted to exist. Highly
electrically conductive MXenes show promise in electrical energy storage,
electromagnetic interference shielding, electrocatalysis, plasmonics and other
applications.
Abstract
The family of 2D transition-metal carbides, carbonitrides and nitrides (collectively referred
to as MXenes) has expanded rapidly since the discovery of Ti
3
C
2
in 2011. The materials
reported to date always have surface terminations, such as hydroxyl, oxygen or fluorine,
which impart hydrophilicity to their surfaces. About 20 different MXenes have been
synthesized, and the structures and properties of dozens more have been theoretically
predicted. The availability of solid solutions, control of surface terminations, and a recent
discovery of multi-transition-metal layered MXenes offers the potential for synthesis of
many new structures. MXenes versatile chemistry renders their properties tunable for
applications including energy storage, electromagnetic interference shielding, reinforcement
for composites, water purification, bio- and gas-sensors, lubrication, and chemical, photo-
and electro-catalysis. Attractive electronic, optical, plasmonic and thermoelectric properties
have also been shown. In this Review, we present the synthesis, structure and properties of
MXenes, as well as their energy-storage and related applications, and an outlook for future
research.
Cover Article, In Press.

B. Anasori et al. Nature Reviews Materials
2
2D materials have unusual electronic, mechanical and optical properties
1-6
, which have led them
to be extensively studied in the past decade for diverse applications. They can also serve as
convenient building blocks for a variety of layered structures, membranes and composites
7
.
Although several single-element 2D materials have been prepared, such as graphene, silicene
8
,
germanene
9,10
and phosphorene
11,12
, the majority contain two (for example, dichalcogenides and
oxides)
13,14
or more elements (for example, clays)
1
.
Transition metal carbides, carbonitrides and nitrides (MXenes) are among the latest
additions to the 2D world
15-21
. Their general formula is M
n+1
X
n
T
x
(n = 13), where M represents
an early transition metal (Sc, Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, and so on), X is carbon and/or
nitrogen and T
x
stands for the surface terminations (for example, OH, O or F)
22
. Some examples
include Ti
2
CT
x
16
, Ti
3
C
2
T
x
15
and Nb
4
C
3
T
x
19
. In MXenes, n+1 layers of M cover n layers of X in an
[MX]
n
M arrangement. Structures of M
2
X, M
3
X
2
and M
4
X
3
are shown in FIG. 1. Ti
3
C
2
T
x
was the
first MXene reported in 2011
15
, and 19 different MXene compositions have subsequently been
synthesized (marked with blue in FIG. 1) with dozens more predicted to exist and studied in silico
(marked with grey in FIG. 1)
18,20,23,24
. MXenes with more than one M element also exist in two
forms: solid solutions and ordered phases. In the former, a random arrangement of two different
transition metals is observed in the M layers (marked with green in FIG. 1). By contrast, in the
ordered MXenes, single or double layers of one transition metal (for example, Ti) are sandwiched
between the layers of a second transition metal (for example, Mo) in a 2D carbide structure (third
row in FIG. 1). Density functional theory (DFT) calculations showed that for certain
combinations of transition metals, ordered MXenes are energetically more stable than their solid-
solution counterparts and more than 25 different ordered MXenes have been predicted
20
. These
ordered compositions are marked in purple in FIG. 1. In addition to carbides, 2D transition metal
carbonitrides (that is, Ti
3
CN)
16
and nitrides (that is, Ti
4
N
3
)
25
were also reported, and there have
been numerous predictions of the properties of nitrides, mostly from the M
2
N family
18,26-30
.
Figure 1 | MXenes reported to date. MXenes can have at least three different formulas, M
2
C, M
3
C
2
and M
4
C
3
, where M is
an early transition metal and X is C and/or N. They can be made in three different forms: mono-M elements (for example,
Ti
2
C, Nb
4
C
3
); solid solution of at least two different M elements (for example, (Ti,V)
3
C
2
, (Cr,V)
3
C
2
); or ordered double-M
elements, in which one transition metal occupies the perimeter layers and another fills the central M layers (for example,
Mo
2
TiC
2
, Mo
2
Ti
2
C
3
, in which the outer M layers are Mo and the central M layers are Ti). Solid solutions on the X site
produce carbonitrides.

B. Anasori et al. Nature Reviews Materials
3
Synthesis of MXenes
MXenes are made by selective etching of certain atomic layers from their layered
precursors, such as MAX phases. MAX phases are a very large family of ternary carbides and
nitrides with more than 70 reported to date, in addition to numerous solid solutions and ordered
double transition metal structures
22,31-34
. They are made of layers of transition metal carbides or
nitrides (M
n+1
X
n
) that are interleaved with layers of A-element atoms (mostly group 13 and 14
elements of the periodic table). A list of known MAX phases and their structures are provided in
Supplementary information S1, table and figure. Because the M–A bond is metallic, it has not
been possible to separate the M
n+1
X
n
layers and make MXenes by mechanical shearing of MAX
phases. However, MA bonds are more chemically active than the stronger MX bonds, which
makes selective etching of A layers possible. Highly selective etching is the key condition for
making MXenes.
Aqueous fluoride-containing acidic solutions have been predominantly used to
selectively etch the A layers from MAX phases to synthesize MXenes (FIG. 2), either by using
aqueous hydrofluoric acid (HF)
22
or in situ formation of HF via a reaction of hydrochloric acid
(HCl) and fluoride (for example, lithium fluoride (LiF))
35
. Ammonium hydrogen bifluoride
(NH
4
HF
2
) and ammonium fluoride were also successfully applied for Ti
3
C
2
synthesis from
Ti
3
AlC
2
36-38
. From about 10 different A elements of group 13 and 14 (Supporting information S1,
table), only Al has been successfully etched from MAX phases to form MXenes.
It is also possible to synthesize MXenes from non-MAX phase precursors
39-41
. Mo
2
CT
x
is
the first MXene of this kind that was made by etching Ga layers from Mo
2
Ga
2
C
39,40
. This phase,
despite its similarity to MAX phases, has two A-element layers (Ga) separating the carbide
layers. Zr
3
C
2
T
x
was synthesized from another non-MAX-phase precursor by selectively etching
aluminium carbide (Al
3
C
3
) layers from Zr
3
Al
3
C
5
41
, instead of just the Al layers. Zr
3
Al
3
C
5
belongs
to a family of layered ternary transition metal carbides with general formulas of M
n
Al
3
C
n+2
and
M
n
Al
4
C
n+3
, where M is a transition metal, typically Zr or Hf, and n = 1 3. In these phases, a
carbon layer separates each metal later. Thus, Al-C units, instead of A-element layers, separate
the M
2
C or M
3
C
2
layers
42,43
. It was recently shown that it is energetically more favourable to etch
the Al-C units than just the Al layers in Zr
3
Al
3
C
5
41
. This finding may enable the synthesis of new
MXenes from non-MAX precursors, for example, by etching Al
3
C
3
from U
2
Al
3
C
4
44
to form
U
2
CT
x
and other structures. Ultrathin MoN nanosheets have also been fabricated via liquid
exfoliation of the bulk nitride
45
.
MXenes can also be made by high-temperature etching of MAX phases, as was recently
demonstrated by treating Ti
4
AlN
3
in a molten fluoride salt mixture at 550 ºC under an argon
atmosphere to form Ti
4
N
3
MXene
25
. Before the discovery of MXenes, gaseous etchants (halides)
were used to etch MAX phases at elevated temperatures, but their selectivity was not sufficient
and removed both A and M elements, leading to the formation of carbide-derived carbon
46,47
.
There were also reports of high-temperature (>800 ºC) removal of the A-element layers from
MAX phases using molten salt
48,49
, and evaporating the A layer in a vacuum
50
. However, the
resulting carbides were cubic, not 2D, owing to the specific treatment conditions (for example,
the temperature and gas environment). For example, in 2011, a layered titanium carboxyfluoride
structure with cubic TiC
x
layers was prepared by heating Ti
3
AlC
2
in molten LiF in air at 900 ºC
51
.
This is in agreement with the transition metal carbide nonstoichiometric phase diagrams, in which
ordered nonstoichiometric carbides (for example, Ti
2
C, Ti
3
C
2
, which have similar formulae to
MXenes) are stable below certain temperatures (~800 ºC) depending on the phase
52
. Therefore, it
is reasonable to assume that synthesis and annealing of MXenes must be performed below those
temperatures and in a controlled atmosphere; otherwise, a cubic phase will form preferentially.
Taken together, these results and the recent synthesis of Ti
4
N
3
MXene suggest that the molten-salt
approach is effective for the synthesis of new MXenes.
Bottom-up synthesis methods, such as chemical vapour deposition (CVD), should also be
possible for MXene synthesis
21,53
. In 2015, ultrathin (a few nanometres) α-Mo
2
C orthorhombic

B. Anasori et al. Nature Reviews Materials
4
2D crystals with up to 100-µm lateral size were produced by CVD from methane on a bilayer
substrate of copper foil sitting on a molybdenum foil
53
. Using the same method, other transition
metals, such as W and Ta, were made into ultrathin WC and TaC crystals
53
. This method yields
MXenes with a large lateral size and few defects, facilitating the study of their intrinsic
properties
21,53
. The synthesis of MXene monolayers with this method is still to be demonstrated
and bottom-up synthesis options should be further explored.
We focus on wet etching in this Review, because this is the most widely used method to
fabricate MXenes.
Etching with hydrofluoric acid
Various MXenes can be produced by HF etching, as shown in FIG. 2, from room
temperature to 55 ºC by controlling the reaction time and HF concentration
22,54
. HF is a highly
selective etchant that is even capable of selectively removing different polytypes of SiC
55
.
The etching conditions for Al-containing MAX phases (FIG. 2b) vary from one transition
metal to another, depending on the materials structure, atomic bonding and particle size. Etching
conditions for every MXene synthesized to date are provided in Supplementary information S2
(table). On the basis of experimental findings, increasing the atomic number of M requires a
longer time and stronger etching. This can be related to M–Al bonding
22
knowing that MAl
bonding is metallic, we speculate that a larger number of M valence electrons requires stronger
etching.
Etching is a kinetically controlled process and each MXene needs a different etching time
to achieve complete conversion. Usually MXenes with larger n in M
n+1
C
n
T
x
require stronger
etching and/or a longer duration. For example, Mo
2
Ti
2
AlC
3
(n = 4) requires an etching time twice
as long as its n = 3 counterpart (that is, Mo
2
TiAlC
2
) under the same etching conditions
20,56
(Supplementary information S2, table). In general, every MXene can be made under different
etching conditions, which lead to different quality (concentration of defects and surface
chemistry), as will be discussed in the following sections.
Etching in the presence of a fluoride salt
Instead of HF, a mixture of a strong acid and a fluoride salt can be used to synthesize
MXenes
35,40,57
. HCl and LiF react to form HF in situ, which selectively etches the A atoms.
Recently, using a mixture of HF and LiCl, similar etching results were achieved, suggesting that
the presence of protons and fluoride ions is a necessary condition for etching and MXene clay
formation
58
. Etching in the presence of a metal halide leads to intercalation of cations (for
example, Li
+
) and water, which results in an increased spacing and thus weakened interaction
between MXene layers. This is one of the advantages of this method over pure HF etching,
because MXene can be delaminated with no additional step, simply after washing to a pH value
of about 6 to achieve single- or few-layer flakes (for example, Ti
3
C
2
T
x
59
), as we discuss in the
following section.
Delamination
In general, delamination of any 2D material is a necessary step in exploring its properties
in the 2D state. Because multilayered MXenes have two- to sixfold stronger interlayer
interactions than that in graphite and bulk MoS
2
60
, simple mechanical exfoliation provides a low
yield of single layers. There are only two reports of Scotch tape exfoliation of multilayer MXene
into single flakes
61,62
and the remainder have been delaminated via intercalation (FIG. 2d). A
complete list of MXene intercalants reported to date is presented in Supplementary information
S2. MXenes can be intercalated with a variety of polar organic molecules, such as hydrazine, urea
and dimethyl sulfoxide (DMSO), isopropylamine or large organic base molecules such as
tetrabutylammonium hydroxide (TBAOH), choline hydroxide or n-butylamine
63
. MXene
intercalation with these molecules, followed by mechanical vibration or sonication in water, leads
to a colloidal solution of single- and few-layer MXenes. Filtering then results in freestanding
MXene ‘paper’ (FIG. 2d)
20,63-65
.
MXenes (for example, Ti
3
C
2
T
x
) can be intercalated with different metal cations, using

B. Anasori et al. Nature Reviews Materials
5
aqueous solutions of ionic compounds, such as halide salts or metal hydroxides
58,66
. When etching
with a fluoride salt mixed with an acid (for example, HCl and LiF), no additional molecule is
needed, because etched MXene is intercalated with metal cations (Supplementary information S2
(table)). In-situ delamination of MXenes can be achieved by raising the pH to almost neutral and
with very mild mechanical vibration (for example, by hand shaking the solution)
67,68
. In general,
the resulting aqueous colloidal MXene suspensions are stable (FIG. 2d) and do not aggregate
owing to the negative zeta potential of the MXene flakes
69
.
Figure 2 | Synthesis and characterization of MXenes. a | When a layered ternary carbide MAX powders (M
3
AlC
2
here)
is placed into a HF containing acidic aqueous solution (for example, HF or HCl-LiF), Al layer is selectively etched and
replaced with OH, O or F surface terminations (T
x
), forming multilayer M
3
C
2
T
x
MXenes. Intercalation of water, cations,
DMSO, TBAOH and so on into the interlayer spacing, followed by sonication makes it possible to delaminate MXenes to
produce single flake suspensions. b | Images of MAX structures (for example, M
3
AC
2
). From left to right: schematic of the
atomic structure, digital photograph of Ti
3
AlC
2
powder, low magnification and higher magnification SEM images of Ti
3
AlC
2
,
HR STEM image of Mo
2
TiAlC
2
20
. c | Illustrations of multilayered MXene. From left to right: schematic of the atomic
structure, digital photograph of Ti
3
C
2
T
x
powder, low magnification and higher magnification SEM images of Ti
3
C
2
T
x
, HR
STEM of Mo
2
TiC
2
T
x
20
. d | Illustrations of delaminated MXene. From left to right: schematic of the atomic structure, digital
photograph of 400 ml of delaminated Ti
3
C
2
T
x
in water, digital photograph of a Mo
2
TiC
2
T
x
film made by vacuum-assisted
filtration, cross-sectional SEM image
20
of a Mo
2
TiC
2
T
x
film, TEM image of a single-layer Ti
3
C
2
T
x
flake.
SEM, scanning
electron microscope; HR STEM, high-resolution scanning transmission electron microscope; TEM, transmission electron
microscope. HR STEM images in panels b and c and SEM of panel d adapted with permission from Ref.
20
, American
Chemical Society.
Structure and properties
Structure of the MXene layer
Similar to their MAX precursors, M atoms in MXenes are arranged in a close-packed structure
and X atoms fill the octahedral interstitial sites. Three packing arrangements are possible: BγA-
AγB (M
2
X-M
2
X), BγAβC-CγAβB (M
3
X
2
-M
3
X
2
) and BαCβAγB-BγAβCαB (M
4
X
3
-M
4
X
3
). Here,
the capital Roman and Greek letters correspond to the M and X positions, respectively. The
lowercase Greek letters represent the X octahedral interstitial sites corresponding to their Roman
letter counterpart positions (that is, α, β and γ correspond to A, B and C sites, respectively);
Supplementary information S2 (figure). MXenes overall crystal is a hexagonal close packed
structure. However, the ordering of M atoms changes from M
2
X to M
3
X
2
and M
4
X
3
. In M
2
X, M
atoms follow ABABAB ordering (hexagonal close-packed stacking), whereas in M
3
C
2
and M
4
C
3
,
M atoms have ABCABC ordering (face-centred cubic stacking). This atomic ordering (see
Supplementary information S2 (figure)) becomes very important for the synthesis of MXenes

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TL;DR: Two-dimensional transition metal carbides, carbonitrides, and nitrides (MXenes) were discovered in 2011 and more than 20 different compositions have been synthesized by the selective etching of MAX phase and other precursors and many more theoretically predicted as mentioned in this paper.
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1,387 citations

Journal ArticleDOI
TL;DR: The fundamental relationships between electronic structure, adsorption energy, and apparent activity for a wide variety of 2D electrocatalysts are described with the goal of providing a better understanding of these emerging nanomaterials at the atomic level.
Abstract: Over the past few decades, the design and development of advanced electrocatalysts for efficient energy conversion technologies have been subjects of extensive study. With the discovery of graphene, two-dimensional (2D) nanomaterials have emerged as some of the most promising candidates for heterogeneous electrocatalysts due to their unique physical, chemical, and electronic properties. Here, we review 2D-nanomaterial-based electrocatalysts for selected electrocatalytic processes. We first discuss the unique advances in 2D electrocatalysts based on different compositions and functions followed by specific design principles. Following this overview, we discuss various 2D electrocatalysts for electrocatalytic processes involved in the water cycle, carbon cycle, and nitrogen cycle from their fundamental conception to their functional application. We place a significant emphasis on different engineering strategies for 2D nanomaterials and the influence these strategies have on intrinsic material performance, ...

1,363 citations

Journal ArticleDOI
TL;DR: In this article, a strategy to prepare flexible and conductive MXene/graphene (reduced graphene oxide, rGO) supercapacitor electrodes by using electrostatic self-assembly between positively charged rGO modified with poly(diallyldimethylammonium chloride) and negatively charged titanium carbide MXene nanosheets is presented.
Abstract: A strategy to prepare flexible and conductive MXene/graphene (reduced graphene oxide, rGO) supercapacitor electrodes by using electrostatic self-assembly between positively charged rGO modified with poly(diallyldimethylammonium chloride) and negatively charged titanium carbide MXene nanosheets is presented. After electrostatic assembly, rGO nanosheets are inserted in-between MXene layers. As a result, the self-restacking of MXene nanosheets is effectively prevented, leading to a considerably increased interlayer spacing. Accelerated diffusion of electrolyte ions enables more electroactive sites to become accessible. The freestanding MXene/rGO-5 wt% electrode displays a volumetric capacitance of 1040 F cm−3 at a scan rate of 2 mV s−1 , an impressive rate capability with 61% capacitance retention at 1 V s−1 and long cycle life. Moreover, the fabricated binder-free symmetric supercapacitor shows an ultrahigh volumetric energy density of 32.6 Wh L−1, which is among the highest values reported for carbon and MXene based materials in aqueous electrolytes. This work provides fundamental insight into the effect of interlayer spacing on the electrochemical performance of 2D hybrid materials and sheds light on the design of next-generation flexible, portable and highly integrated supercapacitors with high volumetric and rate performances.

1,260 citations

Journal ArticleDOI
TL;DR: For the first time, an efficient and facile approach is reported to fabricate freestanding, flexible, and hydrophobic MXene foam with reasonable strength by assembling MXene sheets into films followed by a hydrazine-induced foaming process.
Abstract: Ultrathin, lightweight, and flexible electromagnetic-interference (EMI) shielding materials are urgently required to manage increasingly serious radiation pollution. 2D transition-metal carbides (MXenes) are considered promising alternatives to graphene for providing excellent EMI-shielding performance due to their outstanding metallic electrical conductivity. However, the hydrophilicity of MXene films may affect their stability and reliability when applied in moist or wet environments. Herein, for the first time, an efficient and facile approach is reported to fabricate freestanding, flexible, and hydrophobic MXene foam with reasonable strength by assembling MXene sheets into films followed by a hydrazine-induced foaming process. In striking contrast to well-known hydrophilic MXene materials, the MXene foams surprisingly exhibit hydrophobic surfaces and outstanding water resistance and durability. More interestingly, a much enhanced EMI-shielding effectiveness of ≈70 dB is achieved for the lightweight MXene foam as compared to its unfoamed film counterpart (53 dB) due to the highly efficient wave attenuation in the favorable porous structure. Therefore, the hydrophobic, flexible, and lightweight MXene foam with an excellent EMI-shielding performance is highly promising for applications in aerospace and portable and wearable smart electronics.

1,241 citations

References
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Journal ArticleDOI
25 Jul 2013-Nature
TL;DR: With steady improvement in fabrication techniques and using graphene’s springboard, van der Waals heterostructures should develop into a large field of their own.
Abstract: Fabrication techniques developed for graphene research allow the disassembly of many layered crystals (so-called van der Waals materials) into individual atomic planes and their reassembly into designer heterostructures, which reveal new properties and phenomena. Andre Geim and Irina Grigorieva offer a forward-looking review of the potential of layering two-dimensional materials into novel heterostructures held together by weak van der Waals interactions. Dozens of these one-atom- or one-molecule-thick crystals are known. Graphene has already been well studied but others, such as monolayers of hexagonal boron nitride, MoS2, WSe2, graphane, fluorographene, mica and silicene are attracting increasing interest. There are many other monolayers yet to be examined of course, and the possibility of combining graphene with other crystals adds even further options, offering exciting new opportunities for scientific exploration and technological innovation. Research on graphene and other two-dimensional atomic crystals is intense and is likely to remain one of the leading topics in condensed matter physics and materials science for many years. Looking beyond this field, isolated atomic planes can also be reassembled into designer heterostructures made layer by layer in a precisely chosen sequence. The first, already remarkably complex, such heterostructures (often referred to as ‘van der Waals’) have recently been fabricated and investigated, revealing unusual properties and new phenomena. Here we review this emerging research area and identify possible future directions. With steady improvement in fabrication techniques and using graphene’s springboard, van der Waals heterostructures should develop into a large field of their own.

8,162 citations

Journal ArticleDOI
TL;DR: In this article, a few-layer black phosphorus crystals with thickness down to a few nanometres are used to construct field effect transistors for nanoelectronic devices. But the performance of these materials is limited.
Abstract: Two-dimensional crystals have emerged as a class of materials that may impact future electronic technologies. Experimentally identifying and characterizing new functional two-dimensional materials is challenging, but also potentially rewarding. Here, we fabricate field-effect transistors based on few-layer black phosphorus crystals with thickness down to a few nanometres. Reliable transistor performance is achieved at room temperature in samples thinner than 7.5 nm, with drain current modulation on the order of 10(5) and well-developed current saturation in the I-V characteristics. The charge-carrier mobility is found to be thickness-dependent, with the highest values up to ∼ 1,000 cm(2) V(-1) s(-1) obtained for a thickness of ∼ 10 nm. Our results demonstrate the potential of black phosphorus thin crystals as a new two-dimensional material for applications in nanoelectronic devices.

6,924 citations

Journal ArticleDOI
TL;DR: 2D nanosheets, composed of a few Ti 3 C 2 layers and conical scrolls, produced by the room temperature exfoliation of Ti 3 AlC 2 in hydrofl uoric acid are reported, which opens a door to the synthesis of a large number of other 2D crystals.
Abstract: Currently, however, there are relatively few such atomically layered solids. [ 2–5 ] Here, we report on 2D nanosheets, composed of a few Ti 3 C 2 layers and conical scrolls, produced by the room temperature exfoliation of Ti 3 AlC 2 in hydrofl uoric acid. The large elastic moduli predicted by ab initio simulation, and the possibility of varying their surface chemistries (herein they are terminated by hydroxyl and/or fl uorine groups) render these nanosheets attractive as polymer composite fi llers. Theory also predicts that their bandgap can be tuned by varying their surface terminations. The good conductivity and ductility of the treated powders suggest uses in Li-ion batteries, pseudocapacitors, and other electronic applications. Since Ti 3 AlC 2 is a member of a 60 + group of layered ternary carbides and nitrides known as the MAX phases, this discovery opens a door to the synthesis of a large number of other 2D crystals. Arguably the most studied freestanding 2D material is graphene, which was produced by mechanical exfoliation into single-layers in 2004. [ 1 ] Some other layered materials, such as hexagonal BN, [ 2 ] transition metal oxides, and hydroxides, [ 4 ] as well as clays, [ 3 ] have also been exfoliated into 2D sheets. Interestingly, exfoliated MoS 2 single layers were reported as early as in 1986. [ 5 ] Graphene is fi nding its way to applications ranging from supercapacitor electrodes [ 6 ] to reinforcement in composites. [ 7 ] Although graphene has attracted more attention than all other 2D materials combined, its simple chemistry and the weak van der Waals bonding between layers in multilayer structures limit its use. Complex, layered structures that contain more than one element may offer new properties because they

6,846 citations

Journal ArticleDOI
21 Mar 2014-ACS Nano
TL;DR: In this paper, the 2D counterpart of layered black phosphorus, which is called phosphorene, is introduced as an unexplored p-type semiconducting material and the authors find that the band gap is direct, depends on the number of layers and the in-layer strain, and significantly larger than the bulk value of 0.31-0.36 eV.
Abstract: We introduce the 2D counterpart of layered black phosphorus, which we call phosphorene, as an unexplored p-type semiconducting material. Same as graphene and MoS2, single-layer phosphorene is flexible and can be mechanically exfoliated. We find phosphorene to be stable and, unlike graphene, to have an inherent, direct, and appreciable band gap. Our ab initio calculations indicate that the band gap is direct, depends on the number of layers and the in-layer strain, and is significantly larger than the bulk value of 0.31–0.36 eV. The observed photoluminescence peak of single-layer phosphorene in the visible optical range confirms that the band gap is larger than that of the bulk system. Our transport studies indicate a hole mobility that reflects the structural anisotropy of phosphorene and complements n-type MoS2. At room temperature, our few-layer phosphorene field-effect transistors with 1.0 μm channel length display a high on-current of 194 mA/mm, a high hole field-effect mobility of 286 cm2/V·s, and an...

5,233 citations

Journal ArticleDOI
TL;DR: In this article, a new family of two-dimensional early transition metal carbides and carbonitrides, called MXenes, was discovered and a detailed outlook for future research on MXenes is also presented.
Abstract: Recently a new, large family of two-dimensional (2D) early transition metal carbides and carbonitrides, called MXenes, was discovered. MXenes are produced by selective etching of the A element from the MAX phases, which are metallically conductive, layered solids connected by strong metallic, ionic, and covalent bonds, such as Ti2AlC, Ti3AlC2, and Ta4AlC3. MXenes ­combine the metallic conductivity of transition metal carbides with the hydrophilic nature of their hydroxyl or oxygen terminated surfaces. In essence, they behave as “conductive clays”. This article reviews progress—both ­experimental and theoretical—on their synthesis, structure, properties, intercalation, delamination, and potential applications. MXenes are expected to be good candidates for a host of applications. They have already shown promising performance in electrochemical energy storage systems. A detailed outlook for future research on MXenes is also presented.

3,973 citations

Frequently Asked Questions (14)
Q1. What are the contributions in this paper?

The materials reported to date always have surface terminations, such as hydroxyl, oxygen or fluorine, which impart hydrophilicity to their surfaces. In this Review, the authors present the synthesis, structure and properties of MXenes, as well as their energy-storage and related applications, and an outlook for future research. Nature Reviews Materials 2 2D materials have unusual electronic, mechanical and optical properties, which have led them to be extensively studied in the past decade for diverse applications. 1. Ti3C2Tx was the first MXene reported in 2011, and 19 different MXene compositions have subsequently been synthesized ( marked with blue in FIG. 1 ) with dozens more predicted to exist and studied in silico ( marked with grey in FIG. This method yields MXenes with a large lateral size and few defects, facilitating the study of their intrinsic properties. The authors focus on wet etching in this Review, because this is the most widely used method to fabricate MXenes. The etching conditions for Al-containing MAX phases ( FIG. 2b ) vary from one transition metal to another, depending on the material ’ s structure, atomic bonding and particle size. In general, every MXene can be made under different etching conditions, which lead to different quality ( concentration of defects and surface chemistry ), as will be discussed in the following sections. This is one of the advantages of this method over pure HF etching, because MXene can be delaminated with no additional step, simply after washing to a pH value of about 6 to achieve singleor few-layer flakes ( for example, Ti3C2Tx ), as the authors discuss in the following section. A complete list of MXene intercalants reported to date is presented in Supplementary information S2. Intercalation of water, cations, DMSO, TBAOH and so on into the interlayer spacing, followed by sonication makes it possible to delaminate MXenes to produce single flake suspensions. The surface terminations and flake stacking of Ti3C2Tx and V2CTx, among all MXenes, were recently studied by electron energy-loss spectroscopy in transmission electron microscopy, neutron scattering, and nuclear magnetic resonance ( NMR ) spectroscopy. However, it is important to note that this is a result of the particles ’ morphology and does not imply that 50 % HF-etched MXene atomic layers are more separated. The availability of solid solutions, control of surface terminations, and a recent discovery of multi-transition-metal layered MXenes offers the potential for synthesis of many new structures. Taken together, these results and the recent synthesis of Ti4N3 MXene suggest that the molten-salt approach is effective for the synthesis of new MXenes. The synthesis of MXene monolayers with this method is still to be demonstrated and bottom-up synthesis options should be further explored. Recently, using a mixture of HF and LiCl, similar etching results were achieved, suggesting that the presence of protons and fluoride ions is a necessary condition for etching and MXene ‘ clay ’ formation. In general, the resulting aqueous colloidal MXene suspensions are stable ( FIG. 2d ) and do not aggregate owing to the negative zeta potential of the MXene flakes. Based on neutron scattering measurements on Ti3C2Tx, it was suggested that interactions between the layers can be described by ( i ) hydrogen bonding between O or F atoms of one surface with the OH surface groups of the opposing Ti3C2Tx sheet, and ( ii ) van der Waals bonding of O and/or F atoms between the sheets. 

A combination of high electronic conductivity, oxide/hydroxide-like surface with redox-active transition metal atoms exposed make MXenes very attractive for fabrication of electrodes. 

Ferromagnetic and antiferromagnetic properties have been predicted for some termination-free MXenes, although magnetism disappears in presence of surface terminations18,27,108,131. 

MXenes can be intercalated with a variety of polar organic molecules, such as hydrazine, urea and dimethyl sulfoxide (DMSO), isopropylamine or large organic base molecules such as tetrabutylammonium hydroxide (TBAOH), choline hydroxide or n-butylamine63. 

In general, oxidation of MXene flakes starts from the edges, leading to the formation of metal oxide nanocrystals (for example, TiO2) decorating the flake edges, and then develops via nucleation and growth throughout the entire surface99-101. 

The extent of interlayer hydrogen bonding depends not only on the orientation of the OH groups relative to the layers, but also on the amount and distribution of –OH relative to the –O and –F moieties positioned on the opposing surface87. 

Because the bonds between M and X are too strong to be broken easily, it is reasonable to assume that ions penetrate only between the MXene sheets. 

Because multilayered MXenes have two- to sixfold stronger interlayer interactions than that in graphite and bulk MoS260, simple mechanical exfoliation provides a low yield of single layers. 

The better thermal stability of Zr3C2 can be explained by its structure being more energetically favourable than bulk ZrC, in contrast to Ti3C2, which is metastable relative to bulk cubic TiC41. 

Before the discovery of MXenes, gaseous etchants (halides) were used to etch MAX phases at elevated temperatures, but their selectivity was not sufficient and removed both A and M elements, leading to the formation of carbide-derived carbon46,47. 

This potentially provides a route to creating energy-storage devices with 0D change upon charging and discharging, which is a key criteria for achieving a long lifetime and minimizing energy dissipation. 

Further increase in capacity was achieved by optimization of the electrode architecture, hybridizing porous MXene flakes with carbon nanotubes, resulting in a Li-ion capacity in excess of 750 mAh g−1 138. 

Etching and delamination conditions affect the quality, overall crystallinity, defects and surface functionalization in MXene flakes, as well as their delamination efficiency. 

The stability of MXene flakes depends on the manufacturing procedure: higher-quality single flakes of MXene have higher stability59.