2021
DOI: 10.1016/j.jallcom.2021.161118
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Critical behavior and magnetocaloric effect of the ferromagnetic Weyl semimetal candidate Co2−ZrSn single crystals

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Cited by 9 publications
(4 citation statements)
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“…The plots exhibit broad peaks centered around PM-FM transition T C = 101 K and the peak values monotonically increases with increasing field, reaches maximums 2.1 (1.8) J kg –1 K –1 under a field of 5 T applied in ab plane ( c -axis). Furthermore, there exists a tiny shift of the – Δ S M max peak from 101 K to near 102 K with an increasing of magnetic field from 0.5 to 5 T, excluding the mean-field model, , consistent with the above critical behavior analysis. Remarkably, below T = 55 K negative values of MCE are observed under H // ab , which is opposite to that of ordinary ferromagnetic systems with a positive MCE.…”
Section: Resultssupporting
confidence: 83%
“…The plots exhibit broad peaks centered around PM-FM transition T C = 101 K and the peak values monotonically increases with increasing field, reaches maximums 2.1 (1.8) J kg –1 K –1 under a field of 5 T applied in ab plane ( c -axis). Furthermore, there exists a tiny shift of the – Δ S M max peak from 101 K to near 102 K with an increasing of magnetic field from 0.5 to 5 T, excluding the mean-field model, , consistent with the above critical behavior analysis. Remarkably, below T = 55 K negative values of MCE are observed under H // ab , which is opposite to that of ordinary ferromagnetic systems with a positive MCE.…”
Section: Resultssupporting
confidence: 83%
“…In addition, the position of the peaks gradually transfer to higher temperatures with an increasing of applied magnetic fields, which eliminates the mean-field model [79][80][81], consistent with the above analyses on critical behavior. −ΔS M (T, H) reaches to a maximal value of 1.18 J kg −1 K −1 at μ 0 H = 5 T, the value is comparable with that of typical systems with a second-order FM transition [51,82,83]. Except for −ΔS M , another crucial parameter to characterize the potential importance of the magnetocaloric effect of systems is the RCP [84], which equals −ΔS max represents the maximal value of the −ΔS M , δ FWHM is the full width at half maximal value of −ΔS M (T).…”
Section: Magnetic Entropy Changesupporting
confidence: 59%
“…Since the Arrott plots can not appropriately describe the magnetization in Co 7 Zn 8 Mn 5 , the modified Arrott plots (MAP) are utilized to characterize the M(H) curves. For systems with a second-order FM transition, the spontaneous magnetization (M s ) below T C , the M(H) curve at T C , and the initial magnetic susceptibility (χ −1 0 ) above T C are depicted by various critical exponents β, δ, and γ, respectively [47,48], To achieve proper critical exponents, an iterative way is utilized to determine the MAP [49][50][51][52], which successfully generates a series of parallel lines in the high-field region (figure 6(b)). Linearly extrapolated M s and χ −1 0 as a function of temperature are displayed in figure 7(a).…”
Section: Critical Behaviormentioning
confidence: 99%
“…The value of both m and n indicates the second-order magnetic phase transition in the sample. [94][95][96][97] The heat capacity (ΔC p ) has been calculated using the following relation:…”
mentioning
confidence: 99%