Brief summary of previous study related to La0.7Pr0.3Fe11.4Si1.6 compound.
Soft ferromagnetic cubic NaZn13-type La0.7Pr0.3Fe11.4Si1.6 has turned out to be a standout amongst the most fascinating compounds for investigating substantial magnetocaloric effect (MCE) on the grounds that the attractive properties of this compound shows large enough spontaneous magnetization for applications, strongly doping dependent, and as well as delicate soft ferromagnetism. These impacts can be attributed to the itinerant electron metamagnetic (IEM) transition especially around the first-order magnetic transition region. However, this compound is difficult to frame by the basic cementing process because of the inherent deficiency of the peritectic response, Υ-Fe + La → La(Fe,Si)13(τ1a), which frequently brings about a blended microstructure of α-Fe + La(Fe,Si)13(τ1a) + LaFeSi(τ4). Additionally, dependability of La(FexSi1−x)13 is no middle-of-the-road stage and common solvency amongst Fe and La in the Fe-La framework as a reality is represented by response dispersion as indicated by magnetic and electronic states’ contribution. From this point of view, the structure, attractive properties and MCE of this compound have been talked about in detail as indicated by various temperatures and times of the annealing treatment. In addition, efficiently contemplating on the doping impact from various concentrations of transition metal elements such as Copper (Cu) and Chromium (Cr) on Iron (Fe) in the La0.7Pr0.3Fe11.4Si1.6 compound is likewise discussed.
- structure properties
- magnetocaloric effect
- magnetic properties
- magnetic application
Attractive refrigeration moves toward becoming more solid to supplant the ordinary refrigeration frame work due to its favourable circumstances utilizing magnetocaloric effect (MCE) application. This innovation has brought huge points of interest as high refrigeration efficiency, environment friendly, practical of volume size, cheapest, nondangerous, and out of sound pollution draw in to additionally look into, contrasted/compared to conventional gas pressure refrigeration system. The MCE was initially found by Warburg  in 1881, and since the discovery of the giant magnetocaloric effect at room temperature in 1997 , attractive materials with expansive MCE have been widely examined tentatively and hypothetically in the previous two decades. Up to the present time, various materials with impressive magnetic entropy change values have been observed, for example, Gd5Si2Ge2 , NdMn2−xTxSi2 (T = transition metal = Cr, Cu, V, Ti) [3, 4, 5], MnAs1−xSbx  and La(Fe,Si)13 [7, 8, 9].
The cubic NaZn13-type La(Fe,Si)13 winds up noticeably as one of the intriguing compounds to investigate large MCE because of their attractive properties, for example, firmly doping reliant, sufficiently extensive unconstrained charge and delicate soft ferromagnetism [10, 11, 12]. These impacts can be attributed to the itinerant electron metamagnetic (IEM) change in the region of the primary request progress temperature. Doping other attractive rare earth elements, for example, Pr, Nd, Ce, Er and Gd, substitute the La position which was utilized to change the temperature and diminish the critical field of 3
The cubic NaZn13 type is difficult to be formed by regular solidification process because of the characteristic inadequacy of a peritectic response, γ-Fe + L → La(Fe,Si)13(τ1a), which frequently results in the blended microstructure of α-Fe + La(Fe,Si)13(τ1a) + LaFeSi(τ4) . Many researchers set up this compound treatment in the range of 1173–1323 K for at least 10 days to produce the NaZn13-type structure [17, 18, 19]. However, the peritectic response temperature in La(Fe,Si)13 is around 1673 K regarding the La-Fe quasi table diagram  and the temperature was found to be more beneficial in the shorting-stage change process  as demonstrated by Liu et al.  and Chen et al. . Both these groups revealed that the readiness in temperature range around 1323–1623 K can create most measures of the NaZn13-type structure. Table 1 indicated the variable case study related to the NaZn13 type which showed different physical properties’ behaviour in substitution or doping effect on the La(FeSi)13 compound, respectively.
|Nominal composition||Condition of case study||Ref|
Different of Si concentration
|Tc found to increase from 195 K for Si=1, 195 K for Si=1.2, 210 K for Si=1.43, 222 K for Si=1.6 and 231 K for Si=1.8|||
Different of Fe concentration
|Tc found to decrease from 208 K for Fe=11.4, 195 K for Fe=11.44, 188 K for Fe=11.57 and 184 K for x=11.7|||
Different of Si concentration
|Tc found to increase from 168 to 218 K for Si=1.5 to Si=2.0|||
|LaFe11.4Si1.6||Large MCE with reversible magnetic phase transition at Tc|||
R=Ce, Pr, Nd
|Tc found to increase up to 11% when 30% of La replaced by R element|||
Doping of Hydrogen
y= 0, 0.5, 1.0 and 1.5
|Tc found to increase from 195 to 330 K for y=0 to 1.5|||
Different of Cu concentration
|Tc found to increase from 197 K for x=0, 210 K for x=0.06, 218 K for x=0.12, 224 K for x=0.23 and 230 K for x=0.34|||
Different of Cr concentration
|Tc found to decrease from 197 K for x=0 to 180 K for x=0.06 and start to increase till 185 K for x=0.12, 190 K for x=0.23 and 195 K for x=0.34|||
According to Shen et al.  findings, substituting La with other rare earth component can prompt surprising improvements of magnetic entropy change. However, these behaviors come with an expansion hysteresis loss as the nature of first-order magnetic transition. In this chapter, we clarify in detail the impact of different temperature-annealing processes on the structure and magnetic properties of La0.7Pr0.3Fe11.4Si1.6. The influence of Cu and Cr doping with the substitute of Fe in the La0.7Pr0.3Fe11.4Si1.6 compound on magnetic properties and magnetocaloric effect was also explained.
2. The phase relation between low temperature with long-time annealing (LTA) and high temperature with short-time annealing (HTA)
2.1. Structural properties
It was all around acknowledged that the stage level of impurity structure in the NaZn13-type compound is dependent on the procedure of preparation process [25, 26]. Starting there, the La0.7Pr0.3Fe11.4Si1.6 compound was chosen to be set up with two different annealing treatments with low-temperature annealing (LTA) at 1323 K for 14 days and high-temperature annealing (HTA) at 1523 K for 4 h to elucidate which method is more advantageous and forms a better NaZn13-type structure. Results from XRD diffraction (as indicated in Figure 1) show that the HTA with less time can form a bigger number of the NaZn13– compound structure phase compared to LTA with long-time annealing process. LTA produces substantially an amount of impurity, LaFeSi and α-Fe phase in the La0.7Pr0.3Fe11.4Si1.6 compound.
It is shown in Table 2 that the LTA procedure brings about less amount of the NaZn13 structure though the peritectic reaction alludes to refined structure. This behaviour happens with respect to non-equilibrium solidification phenomenon regarding the uncompleted peritectic response γ-Fe + L → La(Fe,Si)13(τ1a) . At the point when the annealing temperature is higher, the speed of the dispersion of atom is just large during the high temperature and solid-phase diffusion reaction process. Along these lines, it unmistakably happens that while expanding the annealing temperature to 1523 K for 4 h (HTA), the measure of the NaZn13 structure steadily formed will eliminate nearly all of the LaFeSi structure and decrease the amount of the α-Fe structure. The Retiveld refinement is indicated in Table 2 and it is shown that the weight of NaZn13 structure increases from 69% at LTA to 96% while the weight amount of LaFeSi and the α-Fe stage at HTA is found to decrease. The constitutions of the formed NaZn13 structure in 1523 K for 4 h of annealing treatment are in concurrence with other groups [22, 23]. However, it was hard to shape a single-structure sample by the bulk synthesis technique as a low cooling rate of the solidification procedure which will deliver an inhomogeneous structure to the sample. That is the reason, with a specific method in order to stay away from recrystallization of α-Fe and the LaFeSi structure, the samples were quickly quenched in water.
|Nominal composition||Heat treatment (T(K)/t)||Phase||Wt%||Refined composition||Lattice parameter, a (Å)|
|La0.7Pr0.3Fe11.4Si1.6||1323 K/14 days|
|La0.7Pr0.3Fe11.4Si1.6||1523 K/4 hours|
2.2. Magnetic properties
Figure 2 demonstrates the temperature dependent of magnetization measured under the low magnetic field of 0.01 T in temperature range from 100 to 300 K of the La0.7Pr0.3Fe11.4Si1.6 compound for LTA and HTA. The TC values were characterized as a maximum of dM/dT from Figure 2. It found that TC of the La0.7Pr0.3Fe11.4Si1.6 compound from LTA treatment is ~ 200 K which is 13 K higher than HTA treatment as ~197 K. Furthermore, LTA has different magnetic phase transition characteristics because of the different Si concentration in the NaZn13 phase compared to HTA, in which LTA is formed with higher Si concentration and contributes to expand TC and changes the magnetic state from first-order to second-order transition in this case study. Moreover, LTA treatment also interfaced to produce more impurity such as α-Fe and LaFeSi structure and decrease the main NaZn13 structure content with respect to temperature and time during annealing process, which troubles in solution treatment at low temperature directly increasing the Si concentration behaviour. In Table 2, it is shown from XRD refinement that the concentration of Si in the NaZn13 structure for LTA is higher compared to HTA. As far as the impacts of expanding the Si concentration in the NaZn13 structure is concerned, we suggest that this marvel adds to expanding the value of TC and changes the magnetic phase transition. Comparative phenomena likewise have been reported by Bo Liu et al. .
Magnetic hysteresis loss (as shown by the territory encased between ascending and descending branches of the magnetization curves) is additionally normal for first-order magnetic transition. The magnetization curves obtained for La0.7Pr0.3Fe11.4Si1.6 (LTA and HTA) for fields in the range B = 0–5 T around their ferromagnetic ordering temperatures have been studied respectively . This information was obtained for increasing and decreasing fields at 5 K and 2 K intervals at 200 K around TC, consequently giving data about magnetic hysteresis loss effect as discussed using the below Equation .
As exhibited in Figure 3, examination of the magnetic hysteresis loss around the ferromagnetic ordering temperatures for La0.7Pr0.3Fe11.4Si1.6 (LTA and HTA) is up to ~ 12.4 J kg−1 (demonstrated value for B = 0–5 T as appropriate to compare) for La0.7Pr0.3Fe11.4Si1.6 (HTA) at TC ~ 197 K, while almost no magnetic hysteresis loss of ~ 0.1 J kg−1 is found for La0.7Pr0.3Fe11.4Si1.6 (LTA) around TC ~ 210 K. It is exhibited that the field which actuated the first-order magnetic transition from paramagnetic to ferromagnetic was eminently debilitated by the more Si concentration in LTA which demonstrated second-order magnetic transition as a contrast with HTA which showed first-order magnetic transition. The upside of the sample without hysteresis loss expands the proficiency of magnetic refrigerator application  which is of little vitality loss during temperature change in the cycle operation system.
2.3. Magnetocaloric effect
Giant MCE value and magnetic entropy changes are generally accompanied with a first-order magnetic transition because of an extensive rate of change in magnetic field. Even these materials have been preferred in terms of the MCE value compared to second-order material; the issues of thermal and magnetic hysteresis loss are impossible to solve. So as to fulfill the reasonableness of various tests and related logical ways to deal with, calculation of the isothermal entropy change, −∆SM, in this study, has been characterized from the decreased field of magnetization measurement by the Maxwell relation [30, 31]:
The −∆SM peak gradually broadens toward higher temperatures with increasing magnetic field (from ΔB = 0–5 T) as shown in Figure 4(a) and (b) for La0.7Pr0.3Fe11.4Si1.6 (LTA and HTA) related to behaviour of a field-induced transition from the paramagnetic to ferromagnetic state, respectively. The changes in magnetic entropy for La0.7Pr0.3Fe11.4Si1.6 (LTA and HTA) around their ferromagnetic ordering temperatures as indicated in Figure 4 are calculated from decreasing applied fields in order to satisfy the isothermal entropy change and suitability of different experiments . The MCE values are −∆SM ~ 16.8 J kg−1 K−1 at TC = 197 for HTA and decrease to −∆SM ~ 7.9 J kg−1 K−1 at TC = 200 K for LTA. The decrease in the value of −∆SM is related to increase in Si and there is less magnetization moment concentration in La0.7Pr0.3Fe11.4Si1.6 (LTA) compared to La0.7Pr0.3Fe11.4Si1.6 (HTA). This phenomenon indicated that La0.7Pr0.3Fe11.4Si1.6 (HTA) is more favorable and advantageous compare to La0.7Pr0.3Fe11.4Si1.6 (LTA) as a refrigerant in the magnetic refrigerator application.
3. The influence of phase and properties in La0.7Pr0.3Fe11.4Si1.6 with partial substitution of Cu for Fe
3.1. Structural properties
La0.7Pr0.3Fe11.4−xCuxSi1.6 (x = 0–0.34) is prepared using the HTA method. As indicated in Table 3, the amount of α-Fe and LaFeSi phases increases with Cu-doping contribution. This behaviour occurs when we substitute Cu for Fe in La0.7Pr0.3Fe11.4Si1.6 and it affected the bulk diffusion rate controlling factor of homogenization in the NaZn13–type structure. Table 3 shows the LaFeSi and α-Fe phase fractions in La0.7Pr0.3Fe11.4−xCuxSi1.6 which increases with the increasing Cu substitution while the NaZn13 phase decreases from 96% at x = 0 to 85% at x = 0.34. In the La-Fe-Si ternary system, the substitution new element directly influences the La-Si and Fe-Si bonding as discussed in detail from the previous study . The substitution of Cu into Fe in La0.7Pr0.3Fe11.4Si1.6 produces the differences in relation between the La-Si and La-Fe pairs, changing the interatomic distances which contribute to affecting the structural stability of the NaZn13 structure. As discussed by Fujita et al. , that diffusion, also sensitive to modification of both the electronic structure and lattice spacing, then agrees well with this study which takes in different atomic radii of Cu (1.28 Å) and Fe (1.24 Å).
|Nominal composition La0.7Pr0.3Fe11.4−xCuxSi1.6||X = 0||x = 0.06||x = 0.12||x = 0.23||x = 0.34|
|Phase (Wt%)||Nazn13 (96.12%)||Nazn13 (91.68%)||Nazn13 (88.20%)||Nazn13 (86.83%)||Nazn13 (85.20%)|
|α-Fe (7.33%)||α-Fe (9.06%)||α-Fe (10.15%)||α-Fe (10.63%)|
|LaFeSi (0.32%)||LaFeSi (0.99%)||LaFeSi (2.74%)||LaFeSi (3.02%)||LaFeSi (4.16%)|
|Lattice parameter, a (Å)||11.45845||11.46035||11.46274||11.46495||11.46621|
|−ΔSM (J/kg K)||17||12||9||7||5|
|MS (μB/ f.u.) at 5 K||22.8||22||21.6||21||21.4|
3.2. Magnetic properties
As indicated in Table 3, increase in Cu doping in La0.7Pr0.3Fe11.4Si1.6 will increase the TC and change the magnetic phase transition from first- to second-order type. This behaviour found that related exchange interactions exist between Fe-Fe in the Fe-rich rare earth intermetallic compounds. It is related to the phenomenon when the separation of the Fe–Fe pair is smaller than 2.45 Å, the exchange interaction will be negative but the interaction is positive at larger Fe–Fe distances as similarly reported by other group . Based on the fact that the atomic radius of Fe is smaller than that of Cu, increase in Cu concentration doping will increase the lattice parameter and the Fe-Fe distance then will enhance the positive interactions with increasing TC.
As details included in Table 3, the compounds were found to exhibit ferromagnetic behaviour with a saturation magnetization below 24 μB/f.u. . However, it is shown that the replacement Cu for Fe will reduce the saturation magnetization field in La0.7Pr0.3Fe11.4−xCuxSi1.6 according to the characteristics of Cu as a diamagnetic element. As we assume no contribution from the Pr moment with increasing Cu content, the average moment of the Fe can be derived from the total moment. It is indicated that substituting Fe by Cu leads to a decrease in the average moment of the Fe in La0.7Pr0.3Fe11.4Si1.6. This agrees well with x = 0.34; the value of the saturation magnetization is higher than expected. The saturation magnetization is higher because the total moment is included with a large amount of the α-Fe moment in La0.7Pr0.3Fe11.06Cu.34Si1.6.
3.3. Magnetocaloric effect
The values of −∆SM around TC that have been derived from the decrease in magnetic field are shown in Table 3 as a function of temperature with a 0–5 T change in the field for La0.7Pr0.3Fe11.4−xCuxSi1.6 (x = 0–0.34) compounds. It is shown that the −∆SM peak gradually becomes broader at higher temperatures with increasing magnetic field from 1 to 5 T as characteristic of the field-induced IEM transition from the paramagnetic to the ferromagnetic state particularly around temperatures above TC. Furthermore when there is increase in the concentration of Cu in La0.7Pr0.3Fe11.4-Si1.6, the −∆SM decreases from 17 J/kgK for x = 0 to 5 J/kgK for x = 0.34 as it is proved that Cu is dilute and not a magnetic element.
The relative cooling power (RCP) is very important and related to the magnetic refrigerator application performance. Using the full width at half maximum of the peak in the temperature dependence of the magnetic entropy change −∆SM and the maximum of the entropy variation −, the value of RCP has been calculated using the following formula [19, 33]:
A summary of RCP values and other magnetic characterization parameters listed in Table 3 for La0.7Pr0.3Fe11.4−xCuxSi1.6 (x = 0, 0.06, 0.12, 0.23, 0.34) compounds is presented. The RCP value shows the similar behaviour with MCE which starts to decrease from 400 J/kg for x = 0 to 245 J/kg for x = 0.34 on application of a B = 0–5 T, respectively.
4. The influence of phase and properties in La0.7Pr0.3Fe11.4Si1.6 with partial substitution of Cr for Fe
4.1. Structural properties
The x-ray diffraction analysis at room temperature in Table 4 showed that Cr concentration contributes to an increase in the amount of α-Fe and LaFeSi phases from the beginning to x = 0.06. However it was found to increase from x = 0.12 to x = 0.34. We suggest this behaviour to be related to bulk diffusion rate controlling factor of homogenization in the cubic NaZn13–type phase structure (space group
|Nominal composition La0.7Pr0.3Fe11.4−xCrxSi1.6||X = 0||x = 0.06||x = 0.12||x = 0.23||x = 0.34|
|Phase (Wt%)||Nazn13 (96.12%)||Nazn13 (85.90%)||Nazn13 (92.60%)||Nazn13 (94.00%)||Nazn13 (97.60%)|
|α-Fe (3.56%)||α-Fe (10.6%)||α-Fe (6.00%)||α-Fe (4.70%)||α-Fe (2.30%)|
|LaFeSi (0.32%)||LaFeSi (3.55%)||LaFeSi (1.40%)||LaFeSi (1.30%)||LaFeSi (0.20%)|
|Lattice parameter, a (Å)||11.45845||11.45560||11.4540||11.45240||11.45180|
|-ΔSM (J/kg K)||17||12||14.2||15.6||17.5|
4.2. Magnetic properties
The temperature dependence of the magnetization for calculated TC of La0.7Pr0.3Fe11.4−xCrxSi1.6 compound is measured under magnetic field of 0.01 T as shown in Table 4. TC was found to decrease from 197 K at x = 0 to 180 K at x = 0.06 and then increase to 185 K at x = 0.12 until 195 K at Cr concentration where x = 0.34. This variation of temperature occurs related to the more presence of α-Fe and LaFeSi phase (impurity) at lower Cr concentration and starts to decrease that amount by increasing Cr until x = 0.34, respectively. The variation of the TC values with the Cr content in these compounds occurs according to two types of exchange interactions existing between Fe-Fe in the Fe-rich rare earth intermetallic compounds as discussed in detail somewhere else .
Magnetic hysteresis is one characteristic of the first-order magnetic transition as discuss in the previous section. It can be seen that the M-B curves exhibit almost no magnetic hysteresis for x = 0.34 which is found to be similar of the characteristic at x = 0 but did not change the first-order magnetic transition behaviour . The phenomenon will provide the advantage of the sample with higher IEM transition and will contribute to enhance the value of magnetic entropy change [11, 23, 35].
4.3. Magnetocaloric effect
The values of −∆SM around TC have been derived from the magnetic data and are indicated in Table 4 for La0.7Pr0.3Fe11.4−xCrxSi1.6 compounds. −∆SM was found to decrease from 17 J kg−1 K−1 at x = 0 to 12 J kg−1 K−1 at x = 0.06 and then increase to 14.2 J kg−1 K−1 at x = 0.12 until it reaches 17.5 J kg−1 K−1 at x = 0.34 which is larger than Gd (10.2 J kg−1 K−1). The relative cooling power (RCP) is defined by Eq. (3). It can clearly list at Table 4 that the RCP values increase from 365 J kg−1 at x = 0.06 to 420 J kg−1 at x = 0.34 under 0–5 T field applied. The RCP value at x = 0.34 is slightly higher than the parent compound as indicated by the promising material of the La0.7Pr0.3Fe11.06Cr0.34Si1.6 compound.
A systematic investigation of the structural and magnetic characterization of La0.7Pr0.3Fe11.4Si1.6 for HTA and LTA samples has been carried out. The results show that the HTA offers more advantages in solving the problem of non-equilibrium solidification behaviour due to the incomplete peritectic reaction γ-Fe + L → La(Fe,Si)13(τ1a) that occurs in the LTA process. The HTA sample shows promising values of −∆SM with very small hysteresis loss. This indicates that the elevated temperature in HTA plays an important role to form the NaZn13-type structure in the La0.7Pr0.3Fe11.4Si1.6 compound.
Furthermore, the substitution of Cu for Fe in La0.7Pr0.3Fe11.4−xCuxSi1.6 leads to a decrease the magnetic entropy change but eliminates hysteresis loss. Increasing the Cu concentration also changes the magnetic-phase transition type from first to second order which in effect reduces the characteristics of IEM transition. The Curie temperature, TC, increases with increasing Cu concentration. This phenomenon is related with the increase in the lattice parameter and the modification of the composition. The compound with a small amount of Cu substitution shows a promising magnetic performance for magnetic refrigerator application, with no hysteresis loss and reasonable RCP.
In conclusion, substitution of Cr for Fe La0.7Pr0.3Fe11.4−xCrxSi1.6 compound leads to decreases in lattice parameter but variation behaviour on TC. The variation of TC with increasing Cr concentration can be understood in terms of sensitive changes of Fe1-Fe2 and Fe2-Fe2 distances. Analysis of the magnetisation data demonstrates that the order of magnetic phase transition around TC is consistent on the first-order type even when x = 0.34 for La0.7Pr0.3Fe11.4−xCrxSi1.6 compounds. Replacement of Fe by Cr leads to a reduction of the magnetic entropy change from x = 0 to x = 0.06; however, it starts to enhance again when one increases Cr concentration until x = 0.34.
The authors thank the National Defense University of Malaysia for financial support of this research. M. F, Md Din acknowledges the Ministry of Higher Education Malaysia for an FRGS Grant (FRGS/1/2015/SG06/UPNM/03/3).