Thermal transport properties, magnetic susceptibility and neutron diffraction studies of the (Cr100-xAlx)95Mo5 alloy system

dc.contributor.authorMuchono, B.
dc.contributor.authorSheppard, C.J
dc.contributor.authorVenter, A.M.
dc.contributor.authorPrinsloo, A.R.E.
dc.date.accessioned2018-04-10T12:55:23Z
dc.date.accessioned2023-06-26T13:01:50Z
dc.date.available2018-04-10T12:55:23Z
dc.date.available2023-06-26T13:01:50Z
dc.date.issued2018
dc.descriptionJournal Articleen_US
dc.description.abstractPrevious electrical resistivity ðρÞ and specific heat ðCP Þ studies on the ternary (Cr100-xAlx)95Mo5 alloy system suggested that it harbours two quantum critical points (QCPs). This study reports comprehensive investigations of this alloy system through Seebeck coefficient ðSÞ, thermal conductivity ðκÞ, magnetic susceptibility ðχ Þ and neutron diffraction ðNDÞ measurements in the concentration range 0 x 8.6. The results of S and χ show that spin-density-wave (SDW) antiferromagnetism is suppressed to temperatures below 2 K for concentrations in the range 1.4 x 4.4. Plots of dS=dT in the limit as T→ 2 K depict two minima, i.e. just above x 1⁄4 1.4 and 4.4. This parameter has been used as a key indicator of quantum critical behaviour (QCB) in Cr alloys. Analyses against the Nordheim-Gorter relationship demonstrates a positive slope for the incommensurate (I) SDW alloys and a negative slope for the commensurate (C) SDW alloys. Extrapolations of these two slopes intercept at a concen- tration of 3.2 at.% Al indicating the occurrence of band structure modifications when Al is added into the Cr95Mo5 base alloy. The Lorenz number ðLÞ for the alloys with x 1⁄4 0 and 0.5 shows interesting anomalous behaviour associated with band structure effects and SDW magnetic ordering. ND measurements as a function of temper- ature confirm that alloys with x < 1.4 order in the incommensurate (I) SDW phase whilst alloys with x > 4.4 show commensurate (C) SDW order. Power law fits of the form TN ∝ð1:40 À xÞ0:35 Æ 0:05 for the ISDW to P phase transition and TN ∝ðx À 4:40Þ0:63 Æ 0:03 for the P to CSDW phase transition rendered the critical exponents 0:35 Æ 0:05 and 0:63 Æ 0:03 respectively. Overall the results of S, κ, χ and ND corroborate the existence of two QCPs at x % 1.4 and 4.4.en_US
dc.identifier.citationMuchono, B. et al. 2018. Thermal transport properties, magnetic susceptibility and neutron diffraction studies of the (Cr100-xAlx)95Mo5 alloy system.en_US
dc.identifier.urihttp://196.220.97.103:4000/handle/123456789/887
dc.language.isoenen_US
dc.publisherElsevieren_US
dc.subjectChromium alloysen_US
dc.subjectSpin density waveen_US
dc.subjectQuantum criticalityen_US
dc.subjectResistivityen_US
dc.subjectSusceptibilityen_US
dc.subjectNeutron diffractionen_US
dc.titleThermal transport properties, magnetic susceptibility and neutron diffraction studies of the (Cr100-xAlx)95Mo5 alloy systemen_US
dc.typeArticleen_US
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