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The MAX phase is the precursor of MXenes. MAXenes are thermodynamically stable hexagonal carbide and nitride based materials with outstanding metal and ceramic properties. The MAX phase is layered and has a general formula similar to graphite and MoS2: Mn+1AXn(MAX), where n = 1 to 3 and M is an early transition metal, A is a group A element (mostly IIIA and IVA), and X is carbon and/or nitrogen. The layered structure consists of edge-sharing, twisted XM6 octahedra interspersed by a single planar layer of group A elements.
MAX phases, also known as cermets, have a layered structure with metallic and ceramic characteristics as a result of their atomic groupings. Due to their outstanding laminate structure, MAX compounds are also known as nanolaminates.
Combustion synthesis, chemical vapor deposition, physical vapor deposition, arc melting, hot isostatic pressing, reactive sintering, discharge plasma sintering, mechanical alloying, and molten salt reactions are just a few of the techniques used to create ternary MAX-phase compounds and composites. Recently, a technique for obtaining a succession of Mn+1ZnXn and Mn+1CuXn MAX phases in molten salts has also been discovered.
The MAX phases can be divided into 211 (n=1), 312 (n=2) and 413 (n=3) phases, according to the general formula Mn+1AxXn (n=1 to 3) representation of the MAX phase. Examples of MAX phases with these different structures are.
For 211, Ti2AlC, Ti2AlN and V2 Germanium.
For 312, Ti3SiC2, Ti3SnC2, Ta3AlC2, Ti3GeC2, Ti3AlC2;
For 413, Ti4AlN3, V4AlC3, Ti4SiC3, Ta4AlC3, Nb4AlC3, Ti4GeC3, and Ti4G2C3.
Several theoretical and experimental studies also give evidence for higher MAX phases, including 514 (n=4), 615 (n=5), and 716 (n=6).
Fig 1. Crystal phases of 211 (n=1), 312 (n=2), and 413 (n=3) MAX phases. (Deshmukh K, et al. 2022)
Most MAX phases belong to the space group D4 6h-P6 3/mmc, with two formula cells per lattice. These cells have almost tightly packed M6X octahedral layers inserted in the A-element layer, with the X-atoms occupying the octahedral positions between the M-atoms. the M6X octahedra are connected by edge sharing. the A-group elements are located in the center of a trigonal prism larger than the octahedral positions.
The MAX phases are anisotropic, with lattice parameters of a ~ 3 Å and c ~ 13 Å for the 211 phase, c ~ 18 Å for the 312 phase, and c ~ 23-24 Å for the 413 phase. The number of M layers separating the A layers results in structural differences between the 211, 312, and 413 MAX phases. For example, in the 211, 312, and 413 MAX phases, the 2, 3, and 4 M layers are located in the middle of each 2 A-layer.
MAX stationary phases are synthesized in our facilities using large reactor chemical vapor deposition techniques to produce the world's highest purity (99.999% or better guaranteed), electronic and optical grade, and layered MAX stationary phases. If you need a specific type of new MAXene phase, please contact us. Our R&D team will be happy to design, synthesize and deliver new materials on demand.
(Mo2/3Sc1/3)2AlC MAX (1)
(Mo2/3Y1/3)2AlC MAX (1)
(W2/3Sc1/3)2AlC MAX (1)
(W2/3Y1/3)2AlC MAX (1)
Cr2AlC MAX (1)
Cr2TiAlC3 MAX (1)
High Entropy MAX (3)
MAX Target Material (2)
Mo2Ga2C MAX (1)
Mo2Ti2AlC MAX (1)
Mo2Ti2AlC3 MAX (1)
Mo2TiAlC2 MAX (1)
Mo3AlC2 MAX (1)
MoAlB MAX (1)
Nb2AlC MAX (1)
Nb4AlC3 MAX (1)
ScAl3C3 MAX (1)
Ta2AlC MAX (1)
Ta4AlC3 MAX (1)
Ti2AlC MAX (1)
Ti2AlN MAX (1)
Ti2SnC MAX (1)
Ti2VAlC2 MAX (1)
Ti3Al0.5Cu0.5C2 MAX (1)
Ti3AlC2 MAX (11)
Ti3AlCN MAX (1)
Ti3GeC2 MAX (1)
Ti3SiC2 MAX (1)
Ti3SnC2 MAX (1)
Ti4AlN3 MAX (1)
TiNbAlC MAX (1)
TiVAlC MAX (1)
V2AlC MAX (1)
V2AlN MAX (1)
V2GaC MAX (1)
V2GeC MAX (1)
V2PC MAX (1)
V2ZnC MAX (1)
V4AlC3 MAX (1)
VCrAIC MAX (1)
Mn2AlC MAX (1)
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