Sewak, Ram

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  • Sewak, Ram (5)
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Author's Bibliography

Temperature induced phase transformation in Co

Sewak, Ram; Dey, Chandi Charan; Toprek, Dragan

(2022)

TY  - JOUR
AU  - Sewak, Ram
AU  - Dey, Chandi Charan
AU  - Toprek, Dragan
PY  - 2022
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10638
AB  - Temperature dependent phase transformation behavior in cobalt from hexagonal close-packed (hcp) to face centered cubic (fcc) has been found to be contradictory to that reported earlier. It is found that hcp phase stabilizes at both low and high temperature ($$\sim $$873 K) while fcc phase is stabilized at $$\sim $$500 K. At 298 K, hcp Co has been found to be predominant ($$\sim $$70%) where hcp magnetic phase is $$\sim $$60%. At 973 K, hcp phase is again predominant ($$\sim $$73%), but it is mainly the non-magnetic phase ($$\sim $$67%). Contrary to present results, it was found earlier that fcc phase was stabilized at high temperature and hcp to fcc transformation occured at $$\sim $$700 K. Present results from perturbed angular correlation measurements, therefore, requires a new theoretical interpretation for Co phase transformation. From present measurements, hyperfine magnetic fields in Co at room temperature for the hcp and fcc phases have been found to be 18.7(6) and 12.8(3) T, much lower than earlier reported results. The hyperfine magnetic fields at $$^{181}$$Ta impurity atom have been calculated by density functional theory (DFT) employing the full potential (linearized) augmented plane wave method (FP-LAPW). Present calculated results for both hcp and fcc phases corroborate our experimental results.
T2  - Scientific Reports
T1  - Temperature induced phase transformation in Co
VL  - 12
IS  - 1
SP  - 10054
DO  - 10.1038/s41598-022-14302-x
ER  - 
@article{
author = "Sewak, Ram and Dey, Chandi Charan and Toprek, Dragan",
year = "2022",
abstract = "Temperature dependent phase transformation behavior in cobalt from hexagonal close-packed (hcp) to face centered cubic (fcc) has been found to be contradictory to that reported earlier. It is found that hcp phase stabilizes at both low and high temperature ($$\sim $$873 K) while fcc phase is stabilized at $$\sim $$500 K. At 298 K, hcp Co has been found to be predominant ($$\sim $$70%) where hcp magnetic phase is $$\sim $$60%. At 973 K, hcp phase is again predominant ($$\sim $$73%), but it is mainly the non-magnetic phase ($$\sim $$67%). Contrary to present results, it was found earlier that fcc phase was stabilized at high temperature and hcp to fcc transformation occured at $$\sim $$700 K. Present results from perturbed angular correlation measurements, therefore, requires a new theoretical interpretation for Co phase transformation. From present measurements, hyperfine magnetic fields in Co at room temperature for the hcp and fcc phases have been found to be 18.7(6) and 12.8(3) T, much lower than earlier reported results. The hyperfine magnetic fields at $$^{181}$$Ta impurity atom have been calculated by density functional theory (DFT) employing the full potential (linearized) augmented plane wave method (FP-LAPW). Present calculated results for both hcp and fcc phases corroborate our experimental results.",
journal = "Scientific Reports",
title = "Temperature induced phase transformation in Co",
volume = "12",
number = "1",
pages = "10054",
doi = "10.1038/s41598-022-14302-x"
}
Sewak, R., Dey, C. C.,& Toprek, D.. (2022). Temperature induced phase transformation in Co. in Scientific Reports, 12(1), 10054.
https://doi.org/10.1038/s41598-022-14302-x
Sewak R, Dey CC, Toprek D. Temperature induced phase transformation in Co. in Scientific Reports. 2022;12(1):10054.
doi:10.1038/s41598-022-14302-x .
Sewak, Ram, Dey, Chandi Charan, Toprek, Dragan, "Temperature induced phase transformation in Co" in Scientific Reports, 12, no. 1 (2022):10054,
https://doi.org/10.1038/s41598-022-14302-x . .
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1

Ferromagnetism in intermetallic Hf6Co23 alloy

Sewak, Ram; Dey, Chandi Charan; Toprek, Dragan

(2021)

TY  - JOUR
AU  - Sewak, Ram
AU  - Dey, Chandi Charan
AU  - Toprek, Dragan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/9704
AB  - Ferromagnetism in Hf6Co23 intermetallic alloy at room temperature has been confirmed from perturbed angular correlation measurements using 181Hf probe. The strength of hyperfine magnetic field at room temperature for this intermetallic compound has been found to be Bhf=2.5(2) T while the earlier report of hyperfine magnetic field in Hf6Co23 has discrepancy. The hyperfine magnetic field at Ta impurity site has also been calculated by density functional theory and the result is found to be Bhf=-4.964 T (at 0 K). This value is closer to the present experimental value measured at 298 K. The compound Hf6Co23 has been found to decompose reversibly to Hf2Co7 at 473 K. Ferromagnetism in this material has been found up to 423 K and its Curie temperature is, therefore, set as TC>423 K. From recent measurements by X-ray diffraction, transmission electron microscopy, scanning electron microscopy, electron probe microanalysis and differential scanning calorimetry, Hf6Co23 was reported to be stable in a wide range of temperature and there was no phase existence of Hf2Co7 while the previous reported phase diagram showed a decomposition of Hf6Co23 to Hf2Co7 at a higher temperature. © 2021 Elsevier B.V.
T2  - Journal of Magnetism and Magnetic Materials
T1  - Ferromagnetism in intermetallic Hf6Co23 alloy
VL  - 534
SP  - 168042
DO  - 10.1016/j.jmmm.2021.168042
ER  - 
@article{
author = "Sewak, Ram and Dey, Chandi Charan and Toprek, Dragan",
year = "2021",
abstract = "Ferromagnetism in Hf6Co23 intermetallic alloy at room temperature has been confirmed from perturbed angular correlation measurements using 181Hf probe. The strength of hyperfine magnetic field at room temperature for this intermetallic compound has been found to be Bhf=2.5(2) T while the earlier report of hyperfine magnetic field in Hf6Co23 has discrepancy. The hyperfine magnetic field at Ta impurity site has also been calculated by density functional theory and the result is found to be Bhf=-4.964 T (at 0 K). This value is closer to the present experimental value measured at 298 K. The compound Hf6Co23 has been found to decompose reversibly to Hf2Co7 at 473 K. Ferromagnetism in this material has been found up to 423 K and its Curie temperature is, therefore, set as TC>423 K. From recent measurements by X-ray diffraction, transmission electron microscopy, scanning electron microscopy, electron probe microanalysis and differential scanning calorimetry, Hf6Co23 was reported to be stable in a wide range of temperature and there was no phase existence of Hf2Co7 while the previous reported phase diagram showed a decomposition of Hf6Co23 to Hf2Co7 at a higher temperature. © 2021 Elsevier B.V.",
journal = "Journal of Magnetism and Magnetic Materials",
title = "Ferromagnetism in intermetallic Hf6Co23 alloy",
volume = "534",
pages = "168042",
doi = "10.1016/j.jmmm.2021.168042"
}
Sewak, R., Dey, C. C.,& Toprek, D.. (2021). Ferromagnetism in intermetallic Hf6Co23 alloy. in Journal of Magnetism and Magnetic Materials, 534, 168042.
https://doi.org/10.1016/j.jmmm.2021.168042
Sewak R, Dey CC, Toprek D. Ferromagnetism in intermetallic Hf6Co23 alloy. in Journal of Magnetism and Magnetic Materials. 2021;534:168042.
doi:10.1016/j.jmmm.2021.168042 .
Sewak, Ram, Dey, Chandi Charan, Toprek, Dragan, "Ferromagnetism in intermetallic Hf6Co23 alloy" in Journal of Magnetism and Magnetic Materials, 534 (2021):168042,
https://doi.org/10.1016/j.jmmm.2021.168042 . .
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Orthorhombic phases in bulk pure HfO2: Experimental observation from perturbed angular correlation spectroscopy

Banerjee, Debashis; Sewak, Ram; Dey, Chandi Charan; Toprek, Dragan; Pujari, Pradeep Kumar

(2021)

TY  - JOUR
AU  - Banerjee, Debashis
AU  - Sewak, Ram
AU  - Dey, Chandi Charan
AU  - Toprek, Dragan
AU  - Pujari, Pradeep Kumar
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/9757
AB  - In pure HfO2, only P21/c monoclinic phase was known to exist from previous investigations and there is no report of orthorhombic phase in pure bulk HfO2 at ambient temperature and pressure. Present atomic scale measurements by perturbed angular correlation (PAC) spectroscopy, report two orthorhombic phases in pure bulk HfO2 at room temperature along with the most commonly observed monoclinic phase (similar to 80%). By comparing with the calculated results of density functional theory using full potential (linearized) augmented plane wave method (FP-LAPW), these two orthorhombic phases have been attributed to structures with space group Pbca and Pca2(1). The structures with space group Pca2(1) and Pmn2(1) are non-centrosymmetric and were found to be responsible for ferroelectricity in doped thin film HfO2. At room temperature, the site percentages for the Pca2(1) and Pbca have been found to be similar to 6% and similar to 10%, respectively. At high temperatures of 973 and 1073 K, the Pca2(1) phase was not found but, the Pbca orthorhombic phase was found to be present in the whole temperature range from 298 to 1073 K. The third orthorhombic phase Pmn2(1) was not observed in bulk HfO2. Interestingly, In Gd doped (similar to 5 at%) HfO2, these two orthorhombic phases enhance more than the monoclinic phase. In Gd doped oxide, the P21/c monoclinic phase reduces to similar to 24% while the site percentages for the two orthorhombic phases have been found to be similar to 54% (Pbca) and similar to 17% (Pca2(1)).
T2  - Materials Today Communications
T1  - Orthorhombic phases in bulk pure HfO2: Experimental observation from perturbed angular correlation spectroscopy
VL  - 26
SP  - 101827
DO  - 10.1016/j.mtcomm.2020.101827
ER  - 
@article{
author = "Banerjee, Debashis and Sewak, Ram and Dey, Chandi Charan and Toprek, Dragan and Pujari, Pradeep Kumar",
year = "2021",
abstract = "In pure HfO2, only P21/c monoclinic phase was known to exist from previous investigations and there is no report of orthorhombic phase in pure bulk HfO2 at ambient temperature and pressure. Present atomic scale measurements by perturbed angular correlation (PAC) spectroscopy, report two orthorhombic phases in pure bulk HfO2 at room temperature along with the most commonly observed monoclinic phase (similar to 80%). By comparing with the calculated results of density functional theory using full potential (linearized) augmented plane wave method (FP-LAPW), these two orthorhombic phases have been attributed to structures with space group Pbca and Pca2(1). The structures with space group Pca2(1) and Pmn2(1) are non-centrosymmetric and were found to be responsible for ferroelectricity in doped thin film HfO2. At room temperature, the site percentages for the Pca2(1) and Pbca have been found to be similar to 6% and similar to 10%, respectively. At high temperatures of 973 and 1073 K, the Pca2(1) phase was not found but, the Pbca orthorhombic phase was found to be present in the whole temperature range from 298 to 1073 K. The third orthorhombic phase Pmn2(1) was not observed in bulk HfO2. Interestingly, In Gd doped (similar to 5 at%) HfO2, these two orthorhombic phases enhance more than the monoclinic phase. In Gd doped oxide, the P21/c monoclinic phase reduces to similar to 24% while the site percentages for the two orthorhombic phases have been found to be similar to 54% (Pbca) and similar to 17% (Pca2(1)).",
journal = "Materials Today Communications",
title = "Orthorhombic phases in bulk pure HfO2: Experimental observation from perturbed angular correlation spectroscopy",
volume = "26",
pages = "101827",
doi = "10.1016/j.mtcomm.2020.101827"
}
Banerjee, D., Sewak, R., Dey, C. C., Toprek, D.,& Pujari, P. K.. (2021). Orthorhombic phases in bulk pure HfO2: Experimental observation from perturbed angular correlation spectroscopy. in Materials Today Communications, 26, 101827.
https://doi.org/10.1016/j.mtcomm.2020.101827
Banerjee D, Sewak R, Dey CC, Toprek D, Pujari PK. Orthorhombic phases in bulk pure HfO2: Experimental observation from perturbed angular correlation spectroscopy. in Materials Today Communications. 2021;26:101827.
doi:10.1016/j.mtcomm.2020.101827 .
Banerjee, Debashis, Sewak, Ram, Dey, Chandi Charan, Toprek, Dragan, Pujari, Pradeep Kumar, "Orthorhombic phases in bulk pure HfO2: Experimental observation from perturbed angular correlation spectroscopy" in Materials Today Communications, 26 (2021):101827,
https://doi.org/10.1016/j.mtcomm.2020.101827 . .
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Orthorhombic structure stabilazation in bulk HfO2 by yttrium doping

Banerjee, Debashis; Dey, Chandi Charan; Sewak, Ram; Thakare, Sanjay V.; Toprek, Dragan

(2021)

TY  - JOUR
AU  - Banerjee, Debashis
AU  - Dey, Chandi Charan
AU  - Sewak, Ram
AU  - Thakare, Sanjay V.
AU  - Toprek, Dragan
PY  - 2021
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/10034
AB  - The recently observed ferroelectricity in thin films of pure and doped Hafnium oxide (HfO2) has initiated a sustaining effort to stabilize its ferroelectric phase which is the polar orthorhombic (o) phase with space group Pca21. This polar o-phase of the oxide does not appear in its phase transition sequence and is also not thought to be stabilized in bulk oxide. Here, we report the stabilization of three o-phases of this oxide in bulk with space groups Pbca, Pca21 and Pbcm in presence of Yttrium (Y) dopant. For inducing o-phase, 10 at% of Y-dopant has been used and temperature mediated phase transformation from monoclinic (m) to o-phase has been observed. The third o-phase with space group Pbcm could be stabilized for the first time in bulk oxide by Y-dopant. All the o-phases in presence of m-phase could be identified by Time Differential Perturbed γ-γ Angular Correlation (TDPAC) Spectroscopy. The TDPAC parameters assigned to Pbcm phase confirm the theoretical modelization for the phase performed by Wien2K calculation based on Density Functional Theory (DFT). The present work reports the possibility of stabilizing different o-phases including polar one and shows the widening of scope of this oxide for future ferroelectric applications.
T2  - Hyperfine Interactions
T1  - Orthorhombic structure stabilazation in bulk HfO2 by yttrium doping
VL  - 242
IS  - 1
SP  - 31
DO  - 10.1007/s10751-021-01765-z
ER  - 
@article{
author = "Banerjee, Debashis and Dey, Chandi Charan and Sewak, Ram and Thakare, Sanjay V. and Toprek, Dragan",
year = "2021",
abstract = "The recently observed ferroelectricity in thin films of pure and doped Hafnium oxide (HfO2) has initiated a sustaining effort to stabilize its ferroelectric phase which is the polar orthorhombic (o) phase with space group Pca21. This polar o-phase of the oxide does not appear in its phase transition sequence and is also not thought to be stabilized in bulk oxide. Here, we report the stabilization of three o-phases of this oxide in bulk with space groups Pbca, Pca21 and Pbcm in presence of Yttrium (Y) dopant. For inducing o-phase, 10 at% of Y-dopant has been used and temperature mediated phase transformation from monoclinic (m) to o-phase has been observed. The third o-phase with space group Pbcm could be stabilized for the first time in bulk oxide by Y-dopant. All the o-phases in presence of m-phase could be identified by Time Differential Perturbed γ-γ Angular Correlation (TDPAC) Spectroscopy. The TDPAC parameters assigned to Pbcm phase confirm the theoretical modelization for the phase performed by Wien2K calculation based on Density Functional Theory (DFT). The present work reports the possibility of stabilizing different o-phases including polar one and shows the widening of scope of this oxide for future ferroelectric applications.",
journal = "Hyperfine Interactions",
title = "Orthorhombic structure stabilazation in bulk HfO2 by yttrium doping",
volume = "242",
number = "1",
pages = "31",
doi = "10.1007/s10751-021-01765-z"
}
Banerjee, D., Dey, C. C., Sewak, R., Thakare, S. V.,& Toprek, D.. (2021). Orthorhombic structure stabilazation in bulk HfO2 by yttrium doping. in Hyperfine Interactions, 242(1), 31.
https://doi.org/10.1007/s10751-021-01765-z
Banerjee D, Dey CC, Sewak R, Thakare SV, Toprek D. Orthorhombic structure stabilazation in bulk HfO2 by yttrium doping. in Hyperfine Interactions. 2021;242(1):31.
doi:10.1007/s10751-021-01765-z .
Banerjee, Debashis, Dey, Chandi Charan, Sewak, Ram, Thakare, Sanjay V., Toprek, Dragan, "Orthorhombic structure stabilazation in bulk HfO2 by yttrium doping" in Hyperfine Interactions, 242, no. 1 (2021):31,
https://doi.org/10.1007/s10751-021-01765-z . .
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Local structure study of Hf dopants in Zr2Pd and ZrPd2 intermetallics

Sewak, Ram; Dey, Chandi Charan; Dey, Sandhya K.; Belošević-Čavor, Jelena; Kapidžić, Ana

(2019)

TY  - JOUR
AU  - Sewak, Ram
AU  - Dey, Chandi Charan
AU  - Dey, Sandhya K.
AU  - Belošević-Čavor, Jelena
AU  - Kapidžić, Ana
PY  - 2019
UR  - https://linkinghub.elsevier.com/retrieve/pii/S0966979518307696
UR  - https://vinar.vin.bg.ac.rs/handle/123456789/8042
AB  - The intermetallic compounds Zr2Pd and ZrPd2 have been investigated by perturbed angular correlation (PAC) spectroscopy considering anomalies in their hydrogen absorption properties. It is known that both these compounds have same crystal structure, but Zr2Pd forms an excellent hydride while ZrPd2 does not, even at high pressure. From PAC measurement at room temperature in annealed ZrPd2 sample, this phase is found as a minor component (∼27%) while the dominating phase is identified to be the ZrPd3 (∼73%). In Zr2Pd, this phase has been found to be predominant (∼86%) along with a minor phase (∼14%) due to ZrPd. In ZrPd2, unlike Zr2Pd, a weak temperature dependence of electric field gradient (EFG) has been found from present PAC measurements. Also, site occupancies for both Zr and Pd atoms by the Ta-probe atoms have been found in ZrPd2 and ZrPd3 (formed in ZrPd2). In ZrPd3, Pd site occupancy by the probe is found to be maximum while a small fraction for Zr site occupancy has been found. But, in case of Zr2Pd and ZrPd, no Pd site occupancy of the probe is observed. Calculation of electric field gradients at 181Ta impurity atom for different phases have been performed by density functional theory based on the all electron full potential linearized augmented plane wave plus local orbitals (FP-(L)APW + lo) method to assign the different components observed from PAC measurements. Measurements by XRD have also been carried out to confirm the presence of component phases in the samples. © 2019
T2  - Intermetallics
T1  - Local structure study of Hf dopants in Zr2Pd and ZrPd2 intermetallics
VL  - 107
SP  - 93
EP  - 102
DO  - 10.1016/j.intermet.2019.01.014
ER  - 
@article{
author = "Sewak, Ram and Dey, Chandi Charan and Dey, Sandhya K. and Belošević-Čavor, Jelena and Kapidžić, Ana",
year = "2019",
abstract = "The intermetallic compounds Zr2Pd and ZrPd2 have been investigated by perturbed angular correlation (PAC) spectroscopy considering anomalies in their hydrogen absorption properties. It is known that both these compounds have same crystal structure, but Zr2Pd forms an excellent hydride while ZrPd2 does not, even at high pressure. From PAC measurement at room temperature in annealed ZrPd2 sample, this phase is found as a minor component (∼27%) while the dominating phase is identified to be the ZrPd3 (∼73%). In Zr2Pd, this phase has been found to be predominant (∼86%) along with a minor phase (∼14%) due to ZrPd. In ZrPd2, unlike Zr2Pd, a weak temperature dependence of electric field gradient (EFG) has been found from present PAC measurements. Also, site occupancies for both Zr and Pd atoms by the Ta-probe atoms have been found in ZrPd2 and ZrPd3 (formed in ZrPd2). In ZrPd3, Pd site occupancy by the probe is found to be maximum while a small fraction for Zr site occupancy has been found. But, in case of Zr2Pd and ZrPd, no Pd site occupancy of the probe is observed. Calculation of electric field gradients at 181Ta impurity atom for different phases have been performed by density functional theory based on the all electron full potential linearized augmented plane wave plus local orbitals (FP-(L)APW + lo) method to assign the different components observed from PAC measurements. Measurements by XRD have also been carried out to confirm the presence of component phases in the samples. © 2019",
journal = "Intermetallics",
title = "Local structure study of Hf dopants in Zr2Pd and ZrPd2 intermetallics",
volume = "107",
pages = "93-102",
doi = "10.1016/j.intermet.2019.01.014"
}
Sewak, R., Dey, C. C., Dey, S. K., Belošević-Čavor, J.,& Kapidžić, A.. (2019). Local structure study of Hf dopants in Zr2Pd and ZrPd2 intermetallics. in Intermetallics, 107, 93-102.
https://doi.org/10.1016/j.intermet.2019.01.014
Sewak R, Dey CC, Dey SK, Belošević-Čavor J, Kapidžić A. Local structure study of Hf dopants in Zr2Pd and ZrPd2 intermetallics. in Intermetallics. 2019;107:93-102.
doi:10.1016/j.intermet.2019.01.014 .
Sewak, Ram, Dey, Chandi Charan, Dey, Sandhya K., Belošević-Čavor, Jelena, Kapidžić, Ana, "Local structure study of Hf dopants in Zr2Pd and ZrPd2 intermetallics" in Intermetallics, 107 (2019):93-102,
https://doi.org/10.1016/j.intermet.2019.01.014 . .
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