1995
DOI: 10.1016/0921-4526(95)00180-h
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Systematics of lattice parameters and bonding distances of the omega phase in ZrNb alloys

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Cited by 31 publications
(34 citation statements)
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“…revealed remarkable regularities in the composition dependence of the IDs in the ⍀ phase, [3][4][5][6] which motivated a THE relation between structure, phase stability, and systematic study of the properties of this phase and its relachemical bonding is a key ingredient of the physico-chemical tions to other metastable structures in alloys formed by the approach to material systems. For stable phases, it is often elements of the Ti-group (Ti, Zr, Hf) with other TMs.…”
Section: Introductionmentioning
confidence: 99%
“…revealed remarkable regularities in the composition dependence of the IDs in the ⍀ phase, [3][4][5][6] which motivated a THE relation between structure, phase stability, and systematic study of the properties of this phase and its relachemical bonding is a key ingredient of the physico-chemical tions to other metastable structures in alloys formed by the approach to material systems. For stable phases, it is often elements of the Ti-group (Ti, Zr, Hf) with other TMs.…”
Section: Introductionmentioning
confidence: 99%
“…However, by quenching hightemperature bcc alloys to room temperature, it is possible to obtain retained metastable bcc phases. Grad et al (1995) performed neutron scattering study of the quenched Zr-Nb bcc alloys and found a linear relation between the lattice parameter and the alloy composition at room temperature. Combining with previous data, they extrapolated to pure bcc Zr and obtained a value of the lattice parameter at room temperature.…”
Section: Bcc Ti and Bcc Zrmentioning
confidence: 99%
“…The zero-pressure volume determined for the b phase from EOS is 22.06 Å 3 /atom, which is line with the 22.19 Å 3 /atom determined from the neutron diffraction measurements conducted on various compositions of the Zr-Nb alloy. [28] Figure 4 also shows that the energy of the b phase is always lower than that of the x phase under all the hydrostatic compressions, and the energy difference increases with increasing compression up to V/V 0 = 0.86 with a corresponding pressure of 17.5 GPa (the compression up to which calculations have been performed), suggesting no b fi x transformation under hydrostatic compression up to 17.5 GPa. Our experimental finding is in agreement with the theoretical calculations.…”
Section: Resultsmentioning
confidence: 86%
“…The d substates (d z 2 ,d x 2 Ày 2 , d xy , d yz and d xz ) in the hexagonal symmetry decompose into three irreducible representations, d z 2 , d x 2 Ày 2 þ d xy and d xz + d yz . [28] We observe that in the x stability region, the dominant contributions are from the d xz + d yz character at the Al site and d z 2 and d x 2 Ày 2 þ d xy character at the B site (in fact, at the B site the average charge per state of both the characters is almost equal). On increasing pressure (decreasing volume) the populations of all the partial d states increase, but the increase is largest for the d z 2 state.…”
Section: B Ti Zr and Hfmentioning
confidence: 95%