2018
DOI: 10.1063/1.5004054
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Unusual strain glassy phase in Fe doped Ni2Mn1.5In0.5

Abstract: Fe doped Ni2Mn1.5In0.5, particularly, Ni2Mn1.4Fe0.1In0.5, despite having an incommensurate, modulated 7M martensitic structure at room temperature exhibits frequency dependent behavior of storage modulus and loss that obeys Vogel-Fulcher law as well as shows ergodicity breaking between zero field cooled and field cooled strain measurements just above the transition temperature. Both, frequency dependence and ergodicity breaking are characteristics of a strain glassy phase and occur due to presence of strain do… Show more

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Cited by 12 publications
(17 citation statements)
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“…2. This observation is consistent with earlier results of Fe doping in Ni-Mn based Heusler alloys [16,17,11]. The cubic composition Ni 1.8 Mn 1.5 Fe 0.2 In 0.5 does not seem to show any transition over the temperature range of 450K-150K as can be seen from Fig.…”
Section: Resultssupporting
confidence: 93%
See 1 more Smart Citation
“…2. This observation is consistent with earlier results of Fe doping in Ni-Mn based Heusler alloys [16,17,11]. The cubic composition Ni 1.8 Mn 1.5 Fe 0.2 In 0.5 does not seem to show any transition over the temperature range of 450K-150K as can be seen from Fig.…”
Section: Resultssupporting
confidence: 93%
“…Therefore, it would be interesting to explore the effect of site occupancy on the occurrence of strain glassy phase in Heusler alloys. Presence of strain glassy phase in Ni 2 Mn 1.5−x Fe x In 0.5 , wherein Fe is doped for Mn at the Y/Z site is already documented [11]. Here, we explore the effect of Fe doping at Ni (X) site in the same martensitic composition of Ni 2 Mn 1.5 In 0.5 to realize Ni 2−x Fe x Mn 1.5 In 0.5 (x = 0, 0.1, 0.15, 0.2).…”
Section: Introductionmentioning
confidence: 83%
“…Competing ferromagnetic and antiferromagnetic interactions are responsible for the superparamagneticlike ground state [25,26] in these alloys. Impuritylike Fe doping in Ni-Mn-In alloys induces a transition from the ferroelastic ground state to a strain glass [27]. The ferroelastic/martensitic to strain glass transition usually occurs due to the formation of point defects when the dopant concentration exceeds a critical value [28].…”
Section: Introductionmentioning
confidence: 99%
“…Recent years have witnessed a lot of interest in understanding the precursor state of premartensite phase in the off-stoichiometric SMAs and MSMAs in relation to the occurrence of a fascinating strain glass state [48,55,56,[66][67][68][69][70][71][72] which bears close analogy with spin glasses [73], dipole glasses [74], and relaxors [75]. In this context, one of the most investigated systems is Ti 50 Ni 50−x Fe x , which for low concentrations of Fe shows austenite B2 phase to incommensurate premartensite-I phase (3R) to LRO commensurate R-phase (premartensite-II) to LRO martensite B19 phase (monoclinic) transitions with decreasing temperature [33,55,68,70].…”
Section: Introductionmentioning
confidence: 99%