The soft acoustic phonon mode and its relation to the martensitic transformation in In-Tl alloys

Phonon dispersion curves for indium and f.c.t. and f.c.c. indium-thallium alloys have been calculated using the optimised model potential theory. The presence of a soft acoustic mode along [110], polarised [1$\text{1}$0] has been established. The closer the alloy composition is to the phase boundary, the softer this mode becomes: $\text{1}\text{2}\text{(C}{}_{11}\text{–C}{}_{12}\text{)}$ tends towards zero, in agreement with experimental ultrasonic velocity data.     

Elastocaloric effect associated with the martensitic transition in shape-memory alloys

The elastocaloric effect in the vicinity of the martensitic transition of a Cu-Zn-Al single crystal has been studied by inducing the transition by strain or stress measurements. While transition trajectories show significant differences, the entropy change associated with the whole transformation (DeltaS_(t)) is coincident in both kinds of experiments since entropy production is small compared to DeltaS_(t). The values agree with estimations based on the Clausius-Clapeyron equation. The possibility of using these materials for mechanical refrigeration is also discussed.     

Magnetic entropy change involving martensitic transition in NiMn-based Heusler alloys

Our recent progress on magnetic entropy change (ΔS) involving martensitic transition in both conventional and metamagnetic NiMn-based Heusler alloys is reviewed. For the conventional alloys, where both martensite and austenite exhibit ferromagnetic (FM) behavior but show differentmagnetic anisotropies, a positive ΔS as large as 4.1 J·kg^-1·K^-1 under a field change of 0–0.9 T was first observed at martensitic transition temperature T_M ~ 197 K. Through adjusting the Ni:Mn:Ga ratio to affect valence electron concentration e/a, T_M was successfully tuned to room temperature, and a large negative ΔS was observed in a single crystal. The -ΔS attained 18.0 J·kg-1·K-1 under a field change of 0–5 T. We also focused on the metamagnetic alloys that show mechanisms different from the conventional ones. It was found that post-annealing in suitable conditions or introducing interstitial H atoms can shift the T_M across a wide temperature range while retaining the strong metamagnetic behavior, and hence, retaining large magnetocaloric effect (MCE) and magnetoresistance (MR). The melt-spun technique can disorder atoms and make the ribbons display a B2 structure, but the metamagnetic behavior, as well as the MCE, becomes weak due to the enhanced saturated magnetization of martensites. We also studied the effect of Fe/Co co-doping in Ni₄₅(Co_1-xFe_x)5Mn36.6In13.4 metamagnetic alloys. Introduction of Fe atoms can assist the conversion of the Mn–Mn coupling from antiferromagnetic to ferromagnetic, thus maintaining the strong metamagnetic behavior and large MCE and MR. Furthermore, a small thermal hysteresis but significant magnetic hysteresis was observed around T_M in Ni₅₁Mn_49-xIn_x metamagnetic systems, which must be related to different nucleation mechanisms of structural transition under different external perturbations.     

The martensitic transition in A15 compounds— the elastic softening in the low temperature phase

By taking into account the recent electronic band calculations for A15 compounds, the two bands evolving from the Γ₁₂ states are investigated by the k - p perturbation theory in order to clarify the origin of the martensitic transition. The second order martensitic transition and the arrest of the elastic softening in (c₁₁ - c₁₂) are obtained.     

Anomalous elastic behaviour of monoclinic potassium hydrogen carbonate,KHCO3, in the vicinity of the phase transition at 318 K

The elastic constants of monoclinic KHCO₃ have been determined from resonance frequencies of thick plates at ca. 15 MHz in the range between 250 and 370 K. A strong elastic anisotropy is present with a maximum of the longitudinal stiffness near the direction of the hydrogen bonds within the (HCO₃)^2-₂ dimers. The shear stiffness c₆₆ related to transversal waves propagating along the twofold axis [0 1 0]′ and [1 0 0]′ with displacement vectors nearly parallel to [1 0 0]′ and [0 1 0]′, respectively, shows a drastic softening approaching 318 K from below and from above, indicating a ferroelastic transition. All other elastic constants behave normally except in the close vicinity of the transition temperature where in some cases a small discontinuity is visible. The components of the thermal expansion tensor undergo a discontinuous change at the transition. The pressure derivative of the transition temperature is 2.3 K kbar^-1. A comparison with alkali cyanides and KH₂PO₄ reveals that the interactions driving the transition are rather originating from order-disorder processes of protons as in KH₂PO₄ than from an orientational molecular disorder as in alkali cyanides.     

哈斯勒合金Ni-Mn-Sn的马氏体相变与反磁热性质

通过结构以及磁性测量,研究了哈斯勒合金Ni₅₀Mn_25+xSn_25-x (x=11,12)的马氏体相变和磁热性质.结果表明,与样品在奥氏体相的磁性不同,由于在马氏体相中反铁磁交换作用的增强,导致铁磁和反铁磁在马氏体状态下共存.此外,通过Maxwell方程,研究了两样品在不同磁场变化下马氏体相变温度附近的反磁热性质,并阐明了该系列合金产生大的正磁熵变(ΔS_M)不仅与其在降温过程中发生马氏体相变所导致的磁跃变(ΔM)有关,而且与发生马氏体相变所经历的温度区间有密切的联系. 关键词： 哈斯勒合金 Ni-Mn-Sn 马氏体相变 正磁熵变     

The martensitic phase transition in NiTi

The technique of perturbed angular correlation of gamma rays (PAC) was applied to study the martensitic phase transition of a shape-memory-effect alloy Ni_49.9Ti_50.1 doped with¹¹¹In/Cd probe atoms. Spectra measured above and below the martensite starting temperature,M _s 340 K, exhibit quadrupole interactions of probes at cubic and noncubic lattice sites, consistent with the respective crystal structures. Unlike spectra measured belowM _s those measured above exhibit a large frequency distribution attributed to lattice displacement waves observed in diffraction studies. Analysis tentatively suggests that the waves are dynamic and not static. BelowM _s, at 290 K, a static quadrupole interaction was observed with coupling frequency ₁=34 Mrad/s and asymmetry parameter =0.18, increasing to ₁=40.5 Mrad/s and =0.34 at 77 K.     

Effect of Al doping on the martensitic transition and magnetic entropy change in Ni-Mn-Sn alloys

Effect of Al doping on the martensitic transition and magnetic entropy change in Mn₅₀Ni₄₀Sn_10−xAl_x was investigated. The experimental results show that the martensitic transition temperatures increase with the increase of Al content due to cell contraction, while the martensitic transition temperature range decreases rapidly. Mn₅₀Ni₄₀Sn₈Al₂ alloy has the largest value of  (3.14 J/kg K) for the magnetic field changing from 0 to 10 kOe, which is nearly twice as large as that of Mn₅₀Ni₄₀Sn₁₀ alloy. It is demonstrated that a larger can be obtained due to the sharper magnetization change around martensitic transition.     

Magneto-optical spectroscopy of the martensitic transition in Fe48Mn24Ga28 Heusler alloys

Magneto-optical spectra of polycrystalline samples of the Fe₄₈Mn₂₄Ga₂₈ Heusler alloy undergoing martensitic transformation from the high-temperature paramagnetic austenitic to ferromagnetic martensitic phase have been studied at 50–320 K in the transversal Kerr effect geometry. A comparison of magnetooptical spectra with data obtained in magnetic measurements has demonstrated that the martensitic transition on the surface of a sample and in its bulk takes place in the same temperature interval. Magnetic anisotropy has been found in the martensitic phase driven by large multidomain inclusions of martensite in austenite. The magneto-optical signal of Fe₄₈Mn₂₄Ga₂₈ differs strongly in spectral shape from that measured in Ni-Mn-Ga.     

Lattice properties in the vicinity of the martensitic transformation in TiNi

A pronounced peak in the thermal expansion coefficient — and thus in the Grüneisen parameter — has been found at the temperature corresponding to the martensitic transformation in TiNi. This finding, together with results of ultrasound wave propagation studies, attests to anomalous lattice-dynamical behaviour in the vicinity of the phase transition. Ultrasonic wave attenuation and velocity data are interpreted on the basis of Akhieser-type, phonon viscosity damping. Results obtained are consistent with the hypothesis that a soft phonon mode plays a dominant role in the lattice properties of TiNi near the transition.     

High pressure phase transition and elastic behaviour of lanthanum monochalcogenides

The Phase transition and elastic properties of La-monochalcogenides have been investigated under pressure by means of a modified charge-transfer potential model which incorporates the Coulomb interaction modified by Coulomb screening due to the delocalization of electron of rare-earth atom leading to many-body interactions, covalency effect and overlap repulsion extended up to second-nearest neighbours. Under high pressure the coordination increases and they transform from rock-salt to CsCl structure. The calculated values of cohesive energy, lattice constant, phase transition pressure, relative volume collapse, harmonic and anharmonic elastic moduli and their first- and second-order pressure derivatives agree well with the available measured data and better than those computed by earlier workers. Present model is capable of explaining the Cauchy’s discrepancy correctly.     

The electrical resistance of some lithium-magnesium alloys near the martensitic transformation

The electrical resistivity of four lithium-magnesium alloys with magnesium concentrations of 1.0, 5.0, 10 and 20 atomic percent has been measured as the specimens were slowly cooled from 300 K to ～3 K and warmed again to 300 K. From a hysteresis in the resistivity in the region of the martensitic transformation the M_s temperatures were found. M_s increases ～5 K per atomic percent of added magnesium and, while in agreement with Dugdale and Gugan the martensite in the dilute alloy is less resistive than the high temperature (bcc) phase, it has a larger resistivity in three less dilute alloys.     

CoNiZ系列合金的结构和马氏体相变性质

利用X射线衍射研究了CoNiZ(Z=Si,Sb,Sn,Ga等)合金在不同热处理条件下的相组成.当Z元素为Sn,Sb时,材料是完全的B2结构;但Z为Si时,材料变成面心立方的γ相.形成B2还是γ相由电子浓度和原子尺寸效应两种因素共同决定.而CoNiGa的研究结果表明,在合金中除了形成B2结构的同时还容易形成γ相,常表现出两相共存的特性.对材料进行不同方式的热处理可以使合金中两相的含量有所消长,γ相含量的多少对CoNiGa合金的马氏体相变有很大的影响.分析指出,两相共存及其所带来的物性变化是CoNiGa铁磁性形状记忆合金非常有利用价值的物理性质.     

Some transport properties in martensitic iron-nickel alloys

Summary Resistivity, Hall effect and magnetoresistivity measurements in Fe−Ni alloy specimens with Ni content ranging from 29 to 32 wt.% and subjected to martensitic transformation have been performed. The results have been interpreted by considering both the mechanisms of the martensitic transformation, different in 29 and 30 wt.% Ni alloys from that in 31 and 32 wt.% Ni ones, and the theories of Smith and Berger on the Hall effect in dilute ferromagnetic alloys, which have been applied to the above-described alloys. The Hall data, analysed by means of Kohler polts, have allowed us to identify the charge carrier scattering mechanisms prevailing in the different alloys,i.e. the skew scattering in 29 and 30 wt.% Ni alloys and the side jump scattering in 31 and 32 wt.% Ni ones. To speed up publication, the authors of this paper have agreed to not receive the proofs for correction.     

First-order phase transition in potassium dysprosium tungstate induced by the field renormalization and softening of the elastic moduli in the vicinity of a structural Jahn-Teller-type transition

The magnetostriction of KDy(WO₄)₂ single crystals is measured in an external magnetic field at temperatures below the temperature of a structural phase transition of the Jahn-Teller type. A steplike irreversible variation in the elastic strain is observed to occur with an increase in the magnetic field applied along the a or b axis of the monoclinic cell of the crystal. The residual change in the strain is retained after changing the sign of the magnetic field. The return to the initial state characterized by field-induced jumps in the strain is possible only after thermal cycling well above the structural phase transition temperature. The theory of this phenomenon is developed using a phenomenologically derived thermodynamic potential of the elastic sub-system that takes into account the crystal symmetry and the field renormalization of the elastic moduli. The jumplike transitions are interpreted as being due to the magnetic softening of the elastic moduli in the vicinity of the structural phase transition temperature.     

TA1[110] phonon dispersion and martensitic phase transition in ordered alloys Fe3Pt

In a previous neutron scattering study, we had observed that the TA phonon softening in L1₂-ordered ferromagnetic Fe₇₂Pt₂₈ Invar is pronounced at the zone boundary M-point and leads to an antiferrodistortive phase transition at low temperatures. Here, we report on similar neutron scattering investigations on two ordered crystals with higher Fe content to investigate the relation between the TA phonon softening and the martensitic transformation, which occurs in Fe-rich ordered Fe-Pt. We find that the TA phonon softening, especially at the M-point zone boundary, does not depend on the composition of the investigated crystals. In Fe_74.5Pt_25.5, however, the antiferrodistortive phase transition temperature is enhanced due to tetragonal strain preceding the martensitic transition. In Fe₇₇Pt₂₃ a precursor driven premartensitic phase transition is not observed. The structure of the martensite is, however, influenced by the soft mode lattice instability of the austenite. This would explain the origin of structural details found previously for Fe₃Pt thermoelastic martensite. Received 18 January 1999 and Received in final form 11 March 1999     

The ultrasonic equation of state in the vicinity of the martensitic transformation in Au-47.5 at.% Cd

The isotropic elastic constants of Au-47.5 at.% Cd, and their hydrostatic pressure derivatives, within the temperature interval (10–95°C) of the thermoelastic martensitic transformation, were determined. From the experimental data, using ultrasonic techniques at hydrostatic pressures (up to 5 kbar), the temperature dependence of the isothermal equation of state of the cubic β-phase was calculated. It was found that the low-temperature orthorhombic β′-phase is elastically softer than the cubic β-phase, consequently affecting the β&larr2;gb′ transformation kinetics upon application of hydrostatic pressure. The high values of the Grüneisen parameter, calculated from the pressure derivatives of the sound velocities, in the orthorhombic β′-phase are indicative of a high anharmonicity of interatomic potential in the vicinity of the β′?β phase transformation.