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Damages induced by heavy ions in titanium silicon carbide: effects of nuclear and electronic interactions at room temperature

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TLDR
In this article, the Ti3SiC2 ternary compound can be distinguished for its noteworthy mechanical properties: the nanolamellar structure imparts to this material some softness as well as better toughness than other classical carbides such as SiC or TiC.
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This article is published in Journal of Nuclear Materials.The article was published on 2009-03-31 and is currently open access. It has received 99 citations till now. The article focuses on the topics: Carbide & Silicon carbide.

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The Mn+1AXn phases: Materials science and thin-film processing

TL;DR: A critical review of the M(n + 1)AX(n) phases from a materials science perspective is given in this article, where the authors discuss the potential for low-temperature synthesis, which is essential for deposition of MAX phases onto technologically important substrates.
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Effect of neutron irradiation on select MAX phases

TL;DR: In this paper, the effect of neutron irradiation on polycrystalline samples of Ti3AlC2, Ti2AlC, Ti3SiC2 and Ti2N was investigated.
Journal ArticleDOI

Radiation tolerance of Mn+1AXn phases, Ti3AlC2 and Ti3SiC2

TL;DR: In this paper, ternary carbides with compositions Ti{sub 3}AlC{sub 2} and SiC{Sub 2} have been irradiated with high Xe fluences, 6.25 x 10{sup 15} ions cm{sup -2} ({approx}25-30 dpa), using the IVEM-TANDEM facility at Argonne National Laboratory.
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Synthesis and DFT investigation of new bismuth-containing MAX phases.

TL;DR: It is shown that Zr2(Al1−xBix)C, and particularly with x ≈ 0.58, can be formed from powders even though the end members Zr 2BiC and Zr1AlC seemingly cannot.
References
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Synthesis and Characterization of a Remarkable Ceramic: Ti3SiC2

TL;DR: In this paper, a polycrystalline bulk sample of Ti sub 3, SiC sub 2 was fabricated by reactively hot-pressing Ti, graphite, and SiC powders at 40 MPa and 1,600 C for 4 h.
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Frequently Asked Questions (18)
Q1. What are the effects of electronic interactions on Ti3SiC2?

Elastic collisions lead to the amorphisation of all the phases of the specimens, sputtering of the Ti3SiC2 grain boundaries, and preferential sputtering as a function of the crystallite orientation. 

Among those studied, the Ti3SiC2 ternary compound can be distinguished for its noteworthy mechanical properties: the nanolamellar structure imparts to this material some softness as well as better toughness than other classical carbides such as SiC or TiC. 

Irradiation induced microstrains seem to be an appropriate explanation since an expansion of the unit cell was also noted for Ti3SiC2. 

It brings out both a decrease of the peak intensity of the three phases as a function of the Au fluence from 1014 cm-2, and an increase of the baseline. 

When Se is higher than Seth (threshold electronic stopping power), melting of the cylindrical zone followed by cooling and resolidification lead to the formation of amorphous tracks inside the material. 

In fact, orientation of the basal planes of the Ti3SiC2 hexagonal close-packed structure perpendicularly to the ion beam would lower the ion channeling effects inside the lattice, and so would increase the sputtering yield; therefore, as a function of the crystallite orientation, the sputtering yield would vary and so lead to this kind of microstructure. 

In order to understand the effects of both nuclear and electronic interactions on Ti3SiC2, two runs of irradiation were performed. 

Estimating the parameters of the unit cell as a function of the fluence (Fig. 6), an expansion of the unit cell along the c axis without significant variation of the unit volume may be underlined. 

This phenomenon, which is more important at the near surface (where Se is maximum), leads to high stresses and strains that would result in a flow of matter to form one hill by each ion. 

On the other hand, electronic interactions induce the amorphisation of only Ti3SiC2, expansion of the Ti3SiC2 unit cell along the c axis, and the formation of “hills”, the latter of which remains misunderstood yet. 

At the beginning of the '90s, Pampuch et al. [3,4] and Lis et al. [5-7] led works on the pure bulk Ti3SiC2 synthesis; their best results were compounds with 80-90 % purity, impurities being TiCx and TiSi2. 

These systems are characterised by an increased security level, better economic competitiveness, and an ability to recycle all the fuel in order to upgrade to a fissionable material and minimize longlived waste production by transmutation. 

the authors can notice a modification of the unit cell of this compound; the peak initially located at 40.9°, relative to the (00l) diffraction planes, is shifted to lower 2θ as a function of the fluence. 

The XRD analysis was realised under a 3° incidence angle (Fig. 5), which corresponds to an X-ray penetration depth of 720 nm in Ti3SiC2. 

the aim of this study is a better knowledge of the behaviour under irradiation of Ti3SiC2, whose otherwise outstanding properties allow its consideration it as a cladding material for future fuels. 

Nevertheless these explanations are not valid in their case: first, the density of hills is about 105 lower than the fluence, so thermal spikes cannot account for the bumps; second, this type of relief are only noted from 1015 cm-2 (not at lower fluences), so bumps are not due to agglomeration. 

like Goto et al. [8] some years before, they noted that the hardness of this carbide decreases as the applied load increases; this property led them to qualify Ti3SiC2 as a “ductile ceramic”. 

Amorphisation can be explained by several processes such as the formation of amorphous tracks by thermal spikes, irradiation induced microstrains in the unit cell, or a drop-off of the crystallite size.