Authors: S.W. D'Souza, R.S. Dhaka, Abhishek Rai, M. Maniraj, J. Nayak, Sanjay Singh, D.L. Schlagel, T.A. Lograsso, Aparna Chakrabarti, S.R. Barman
Abstract: The (100) surface of Ni2MnGa ferromagnetic shape memory alloy exhibits intrinsic surface property dissimilar to the bulk as well as influence of compositional variation at the surface. It is shown that by sputtering at room temperature and annealing at high temperature, it is possible to obtain a clean, ordered and stoichiometric surface. However, for even higher annealing temperatures, the surface becomes Mn rich. The (100) surface of Ni2MnGa is found to have Mn–Ga termination. A surface reconstruction to p4gm symmetry is observed in the austenite phase, while the expected bulk truncated symmetry at surface is p4mm. For the stoichiometric surface, the XPS valence band is compared with our calculations based on first principles density functional theory and good agreement is obtained. The ultraviolet photoelectron spectroscopy (UPS) valence band spectra depend sensitively on composition varying from Ni rich to Mn rich surfaces. A satellite feature observed in both Ni 2p core-level and valence band spectra is related to the narrow 3d valence band in Ni2MnGa.
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Authors: Deepti Jain, Soma Banik, L.S. Sharath Chandra, S.R. Barman, R. Nath, V. Ganesan
Abstract: Evolution of domain structures across the martensitic transition (Tm) in the ferromagnetic shape memory alloy system Ni-Mn-Ga is studied using an optical microscope with a temperature variation. Compositions chosen have Tm < Tc, Tm = Tc and Tm > Tc, (Tc=Curie temperature) so that one can compare the nature of martensitic domains. There are no appreciable domain structures when Tm < Tc as compared to the one with Tm > Tc. However, giant morphological changes in the form of appearance of well-developed domains that are propagating with different directions are seen for the composition in which Tm=Tc. The results are discussed in the light of Magnetic Force Microscopy observations as well as giant entropy changes known to occur on samples with co-occurrence of Tm and Tc.
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Authors: Sanjay Singh, S. Bhardwaj, A.K. Panda, V.K. Ahire, Amitava Mitra, A.M. Awasthi, S.R. Barman
Abstract: The martensitic transition and the ferro- to paramagnetic transition have been studied in a series of Ga excess Ni-Mn-Ga specimens [Ni2-xMnGa1+x (0.4≤ x≤ 0.9)] by differential scanning calorimetry and magnetization measurements. The martensitic transition exhibits a hysteresis whose width is similar to Ni2MnGa, indicating that the transition is thermoelastic. The latent heat of transformation is comparable with other Ni-Mn-Ga alloys. A substantial increase in the martensitic transition temperature is observed due to Ga doping. Interestingly, the x-ray diffraction pattern of all the compositions studied show a modulated martensitic structure in the martensitic phase.
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Authors: Soma Banik, R. Rawat, P.K. Mukhopadhyay, B.L. Ahuja, Aparna Chakrabarti, S.R. Barman
Abstract: We report a detailed investigation of the magneto-transport and magnetic properties of
Mn excess Ni-Mn-Ga using the resistivity and magnetization measurements. Magnetoresistance
(MR) has been measured in the ferromagnetic state for different compositions in the austenitic, premartensitic
and martensitic phases. With Mn doping in Ni2-yMn1+yGa, a decrease in magnetization
and MR has been found, since the doped Mn atoms in Ni position are in the antiferromagnetic
configuration with the Mn atoms in Mn position. MR for the parent stoichiometric composition
Ni2MnGa varies almost linearly with field in the austenitic and pre-martensitic phases, and shows a
cusp-like shape in the martensitic phase. This has been explained by the changes in twin and domain
structures in the martensitic phase. Hysteresis in the heating and cooling cycles is a characteristic of
the first order nature of the martensitic phase transition.
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Authors: V.G. Sathe, Soma Banik, Aditi Dubey, S.R. Barman, A.M. Awasthi, Luca Olivi
Abstract: The XANES studies at Mn, Ni and Ga K-edge of Ni2MnGa compound have been carried
out at room and low temperatures. The Mn K-edge and Ni K-edge spectra shows modulation in the
post edge features when the sample is cooled below martensitic transition temperature. It is strongly
reflected in the XANES of Mn K-edge where the peak after the edge gets totally suppressed when
the sample is in martensitic phase. This peak shows a hysteretic behaviour when thermal cycling
was done across the martensitic transition temperature. This clearly shows that the peak height is a
measure of austenitic phase present at a particular temperature. This demonstrates the strong
correlations of electronic states and crystal structures in these compounds.
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Authors: Aparna Chakrabarti, S.R. Barman
Abstract: The electronic and structural properties of different members of the
Ni-Mn-Ga family calculated by ab initio density functional theory are discussed. From
total energy calculations, we show that the martensitic phase is the stable low
temperature phase. Moreover, occurrence of ferromagnetic and paramagnetic
martensitic phases for Ni2MnGa and Ni2.25Mn0.75Ga, respectively, are explained.
Modifications in the density of states near the Fermi level EF are observed across the
martensitic transition for Ni2MnGa, as well as in Mn2NiGa. While Ni2MnGa is
ferromagnetic, we find Mn2NiGa to be ferrimagnetic. The calculated lattice constants
and the magnetic moments are in good agreement with experiment.
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Authors: Deepti Jain, Soma Banik, L.S. Sharath Chandra, S.R. Barman, R. Nath, V. Ganesan
Abstract: Influence of structural transition in the evolution of the magnetic domains in the
ferromagnetic shape memory alloy system Ni2+xMn1-xGa is reported here using Magnetic Force
Microscopy (MFM) studies. Studies reported are with two samples with their martensite transition
temperature TM less than and greater than the Curie temperature Tc. Present results show an
evolution of MFM across the Tc with a clear twin domains and sub domain structures inside the
twins. The higher spatial resolution of MFM (~50nm) as compared to optical microscope (400nm)
is useful in probing the domain walls. Force derivative of the MFM signal that may be used as an
order parameter seems to scale the onset of magnetic order in the system. One can clearly see the
vanishing of the MFM patterns for T>Tc. Results are discussed in the light of models available for
tip-sample interactions that track the local magnetization.
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Authors: Soma Banik, P.K. Mukhopadhyay, A.M. Awasthi, S.R. Barman
Abstract: We report the structural studies on Mn excess and Ga deficient Ni2Mn1+zGa1-z specimens
with z= 0, 0.05, 0.1, 0.15, 0.2 and 0.25. The crystal structure at room temperature was determined
by the x-ray diffraction (XRD). Rietveld analysis has been performed to obtain the lattice
parameters. For z= 0, 0.05 and 0.1, a cubic austenitic phase is observed. For 0.15≤ z ≤0.25, a
tetragonal martensitic phase is obtained, whose lattice constant c increases and a decreases linearly
with increasing z following Vegard’s law. Phase coexistence is observed for z= 0.15, confirming the
first-order nature of the martensitic transition.
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Authors: A.M. Awasthi, S. Bhardwaj, Soma Banik, S.R. Barman
Abstract: A detailed kinetics study of the first-order structural transition in virgin NiTi, Ni47Fe3Ti50,
and Ni2+xMn1-xGa (x= 0 and 0.26) manifests the varying role of renucleation-driven austenitic
growth with the doping-induced disorder and the magnetization state. The austenite transitions were
investigated using differential scanning calorimeter (DSC) at heating rates spanning over a decade.
They revealed the existence of two Arrhenius processes, with their relative presence, nucleationbarrier
energies, and validity-timescales suggesting that both intra- and inter-domain texturalorderings
undergo de-structuring. In the stoichiometric Ni2MnGa, a single low-energy barrier ( )
fast kinetics observed may be attributed wholly to the short-distance textural order-disorder (a near
absence of bigger, inter-domain interactions). On the other hand, two distinct Arrhenicities are
found in equal strength in NITINOL (NiTi) and Ni47Fe3Ti50, and in unequal proportion in
Ni2.26Mn0.74Ga, over the full range of temperature scanning rates covered (q= 2.5 to 50°C/min). The
relatively fast nucleation-driven growth dominates higher T-scanning rates, with lower barrier
activation (qhi) (albeit > , due to a change in the twins’ character). Another kinetics with higher
barrier energy (qlo) manifests at slow heatings. The crossover in Ni47Fe3Ti50 is interpreted as
increase in the (disorder-induced) A-domain-size dispersion, which also causes a broadening of the
transition. Parameters characterizing the kinetics of various specimens are examined; comparisons
of the relative energy/time scales of inter- and intra-domain processes made, and their
transition/crossover temperature discussed.
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