The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂

The crystal structure and the magnetic and magnetoelastic properties of TbxDy₁₋xFe₂Hy (x = 0.27; 0.41; y ≤ 3) are investigated. The hydrides are obtained by the interaction of TbxDy₁₋xFe₂ samples with hydrogen gas at room temperature. It is established that the hydrides have the same cubic type of s...

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Дата:2001
Автори: Nikitin, S.A., Tereshina, I.S., Touliakov, A.P., Tereshina, E.A., Verbetsky, V.N., Salamova, A.A.
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Опубліковано: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2001
Назва видання:Физика низких температур
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Цитувати:The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂ / S.A. Nikitin, I.S. Tereshina, A.P. Touliakov, E.A. Tereshina, V.N. Verbetsky A. A. Salamova // Физика низких температур. — 2001. — Т. 27, № 4. — С. 403-405. — Бібліогр.: 8 назв. — англ.

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spelling irk-123456789-1300182018-02-05T03:02:46Z The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂ Nikitin, S.A. Tereshina, I.S. Touliakov, A.P. Tereshina, E.A. Verbetsky, V.N. Salamova, A.A. Низкотемпеpатуpная магнитостpикция магнетиков и свеpхпpоводников The crystal structure and the magnetic and magnetoelastic properties of TbxDy₁₋xFe₂Hy (x = 0.27; 0.41; y ≤ 3) are investigated. The hydrides are obtained by the interaction of TbxDy₁₋xFe₂ samples with hydrogen gas at room temperature. It is established that the hydrides have the same cubic type of structure as the parent compounds but the lattice parameter in the hydrides is larger than in the hydrogen-free samples. Both the Curie temperature and the magnetic moment decrease drastically as the hydrogen concentration increases. Measurements of the longitudinal λ|| and transverse magnetostriction λ^ are carried out in magnetic fields up to 12 kOe in the temperature range 78√300 K using strain gauges.The thermal expansion coefficients as a function of temperature are obtained for hydrides with high hydrogen concentration. The magnetostriction of hydrides is strongly different from that of hydride-free samples. The small and negative value of the magnetostriction at low temperatures proves that hydrogen atoms make a strong contribution to the crystal field acting on the rare-earth ions. 2001 Article The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂ / S.A. Nikitin, I.S. Tereshina, A.P. Touliakov, E.A. Tereshina, V.N. Verbetsky A. A. Salamova // Физика низких температур. — 2001. — Т. 27, № 4. — С. 403-405. — Бібліогр.: 8 назв. — англ. 0132-6414 PACS: 74.25.Ha;, 75.30.Gw http://dspace.nbuv.gov.ua/handle/123456789/130018 en Физика низких температур Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic Низкотемпеpатуpная магнитостpикция магнетиков и свеpхпpоводников
Низкотемпеpатуpная магнитостpикция магнетиков и свеpхпpоводников
spellingShingle Низкотемпеpатуpная магнитостpикция магнетиков и свеpхпpоводников
Низкотемпеpатуpная магнитостpикция магнетиков и свеpхпpоводников
Nikitin, S.A.
Tereshina, I.S.
Touliakov, A.P.
Tereshina, E.A.
Verbetsky, V.N.
Salamova, A.A.
The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂
Физика низких температур
description The crystal structure and the magnetic and magnetoelastic properties of TbxDy₁₋xFe₂Hy (x = 0.27; 0.41; y ≤ 3) are investigated. The hydrides are obtained by the interaction of TbxDy₁₋xFe₂ samples with hydrogen gas at room temperature. It is established that the hydrides have the same cubic type of structure as the parent compounds but the lattice parameter in the hydrides is larger than in the hydrogen-free samples. Both the Curie temperature and the magnetic moment decrease drastically as the hydrogen concentration increases. Measurements of the longitudinal λ|| and transverse magnetostriction λ^ are carried out in magnetic fields up to 12 kOe in the temperature range 78√300 K using strain gauges.The thermal expansion coefficients as a function of temperature are obtained for hydrides with high hydrogen concentration. The magnetostriction of hydrides is strongly different from that of hydride-free samples. The small and negative value of the magnetostriction at low temperatures proves that hydrogen atoms make a strong contribution to the crystal field acting on the rare-earth ions.
format Article
author Nikitin, S.A.
Tereshina, I.S.
Touliakov, A.P.
Tereshina, E.A.
Verbetsky, V.N.
Salamova, A.A.
author_facet Nikitin, S.A.
Tereshina, I.S.
Touliakov, A.P.
Tereshina, E.A.
Verbetsky, V.N.
Salamova, A.A.
author_sort Nikitin, S.A.
title The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂
title_short The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂
title_full The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂
title_fullStr The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂
title_full_unstemmed The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂
title_sort effect of hydrogen on the magnetostriction of rare-earth compounds tbxdy₁₋xfe₂
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
publishDate 2001
topic_facet Низкотемпеpатуpная магнитостpикция магнетиков и свеpхпpоводников
url http://dspace.nbuv.gov.ua/handle/123456789/130018
citation_txt The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy₁₋xFe₂ / S.A. Nikitin, I.S. Tereshina, A.P. Touliakov, E.A. Tereshina, V.N. Verbetsky A. A. Salamova // Физика низких температур. — 2001. — Т. 27, № 4. — С. 403-405. — Бібліогр.: 8 назв. — англ.
series Физика низких температур
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fulltext Fizika Nizkikh Temperatur, 2001, v. 27, No. 4, p. 403–405Nikitin S. A ., Te resh in a I. S., T ouliakov A. P., and T ere shina E. A .Th e effe ct of hyd rog en on t he ma gne tostr iction of r ar e-ear th com pou nds Tb xDy1 –xFe 2Nikit in S. A. , Ter eshina I. S., Tou liako v A . P., a nd Ter eshina E . A. The ef fect o f hydr oge n on the m ag neto strict io n of ra re-ea rth c omp ound s T bxDy1– xFe2 The effect of hydrogen on the magnetostriction of rare-earth compounds TbxDy1–xFe2 S. A. Nikitin, I. S. Tereshina, A. P. Touliakov, and E. A. Tereshina Department of Physics, Moscow State University, Vorobyevy Gory, 119899, Moscow, Russia E-mail: nikitin@rem.phys.msu.su V. N. Verbetsky and A. A. Salamova Department of Chemistry, Moscow State University, Vorobyevy Gory, 119899, Moscow, Russia Received October 26, 2000 The crystal structure and the magnetic and magnetoelastic properties of TbxDy1−xFe2Hy (x = 0.27; 0.41; y ≤ 3) are investigated. The hydrides are obtained by the interaction of TbxDy 1−xFe2 samples with hydrogen gas at room temperature. It is established that the hydrides have the same cubic type of structure as the parent compounds but the lattice parameter in the hydrides is larger than in the hydrogen-free samples. Both the Curie temperature and the magnetic moment decrease drastically as the hydrogen concentration increases. Measurements of the longitudinal λ || and transverse magnetostriction λ⊥ are carried out in magnetic fields up to 12 kOe in the temperature range 78–300 K using strain gauges.The thermal expansion coefficients as a function of temperature are obtained for hydrides with high hydrogen concentration. The magnetostriction of hydrides is strongly different from that of hydride-free samples. The small and negative value of the magnetostriction at low temperatures proves that hydrogen atoms make a strong contribution to the crystal field acting on the rare-earth ions. PACS: 74.25.Ha; 75.30.Gw S. A. N ikitin et al. Introduction Intermetallic compounds of rare earths (R) and 3d-transition metals having MgCu2-type crystal structure are attracting much attention in recent years as giant magnetostrictive materials [1]. These compounds interact actively with hydrogen gas at room temperature and form stable hydrides. Upon hydrogenation these compounds exhibit substantial changes in their magnetic properties [2]. The mag- netoelastic properties of TbxDy1−xFe2 compounds have been investigated insufficiently up to now, because the samples are degraded in the process of hydrogen absorption. We have prepared powder- pressed samples for all of the compounds, including the host alloys, and have measured the magnetos- triction of these compounds. This method was suc- cessfully applied by Clark et al. [3]. The present paper reports on the magnetic and magnetoelastic properties of TbxDy1−xFe2Hy (x = 0.27; 0.41) with different hydrogen concentrations (y ≤ 3). Experimental methods Samples of Tb0.27Dy0.73Fe2 and Tb0.41Dy0.59Fe2 were prepared by melting constituent metals of rare earth and Fe metals with purities of 99.95% and 99.98%, respectively, in an induction furnace, fol- lowed by annealing for 40 h at 1000°C. X-ray diffraction analysis carried out with a powder dif- fractometer using Cr Kα-radiation showed that all of the compounds studied were almost single-phase and had crystalline structures of the MgCu2-type. The amount of extraneous phases in the samples was no more than 2%. The hydrides were obtained by the interaction of the TbxDy1−xFe2 samples with hydrogen gas at room temperature. The concentration of absorbed hydrogen in the samples was calculated using the van der Waals equation and additionally was measured by the full-burning method. Thermomagnetic analysis (TMA) was used to measure the Curie temperature in a field of 1 kOe. The magnetic measurements were made for aligned and free powder samples in the temperature range © S. A. Nikitin, I. S. Tereshina, A. P.Touliakov, E. A. Tereshina, V. N. Verbetsky, and A. A. Salamova, 2001 80–700 K and in magnetic fields up to 12 kOe, using a pendulum magnetometer. The magnetostriction of TbxDy1−xFe2Hy was measured in fields up to 12 kOe in the temperature range 80–300 K by using a conventional strain- gauge bridge. Since the hydrides were available only in the powder form, the measurements were made with powder-pressed samples. The fine pow- der of TbxDy1−xFe2Hy compounds was compacted under pressure near 3 GPa in disks with dimensions of 0.8 mm×1.5 mm×8 mm. The densities of the samples produced in this way were nearly 70% of the powder x-ray densities. We took as the magne- tostriction value for the investigated compounds the values measured on the pressed sample multiplied by the ratio of the powder x-ray density to the pressed sample density [3]. This method was checked on solidified precursor samples. Magnetos- trictive measurements were made as a function of magnetic field strength and temperature. Results and discussion TbxDy1−xFe2 (x = 0.27; 0.41) compounds were found to be crystallized in the cubic MgCu2-type structure (Fig. 1). The lattice constant a and unit cell volume V are listed in Table. It was observed that hydrogenation leads to a lattice expansion of the compounds without change of the cubic struc- ture from the MgCu2 type. The relative cell volume increases ∆V/V show a consistent ∼ 9% (at x = 1) and ∼ 20% (at x = 3) volume expansion over the hydrogen-free unit cell for all the compounds. Table Crystallographic and magnetic data for the Tb x Dy 1−x Fe2 com- pounds and their hydrides. Compound a, A° V, A° 3 ∆V/V, % T C , K Tb 0.27 Dy 0.73 Fe 2 7.325 393.03 — 686 Tb 0.27 Dy 0.73 Fe 2 H 1 7.537 428.15 8.9 596 Tb 0.41 Dy 0.59 Fe 2 7.324 392.87 — 697 Tb 0.41 Dy 0.59 Fe 2 H 3 7.789 472.547 20.2 275 The Curie temperatures TC of TbxDy1−xFe2 com- pounds and their hydrides were determined using TMA, as was mentioned above (Fig. 2). In cases when TC was close to room temperatures, it was obtained from a Belov–Arrott plot (for example, see Fig. 3). The Curie temperatures of TbxDy1−xFe2Hy are summarized in Table in comparison with their original counterparts. Both the Curie temperature and the magnetiza- tion decrease with increasing hydrogen concentra- tion. At y = 3 a compensation temperature appears in the compound. Such behavior has been observed earlier [7] and is typical for all RFe2 compounds (where R is a heavy rare earth). Figure 4,a shows the temperature dependence of the magnetization σ(T) measured in an external magnetic field of 12 kOe. It can be seen from Fig. 4 that the σ-curve measured on heating of the sample is characterized by a single minimum at T ≈ 130 K (compensation temperature) and a broad maximum at T ≈ 220 K. Fig. 1. Cubic Laves phase (C15). The large circles represent the rare-earth ions and the small circles represent 3d ions. Fig. 2. The temperature dependence of magnetization σ of the TbxDy1−xFe2 compounds measured at an external magnetic field of 1 kOe: Tb0.41Dy0.59Fe2 (❍); Tb0.27Dy0.73Fe2 (▲); Tb0.27Dy0.73Fe2H1 (∆); Tb0.41Dy0.59Fe2H3 (●). S. A. Nikitin et al. 404 Fizika Nizkikh Temperatur, 2001, v. 27, No. 4 Figure 4,b shows the temperature dependence of longitudinal magnetostriction λ || measured at differ- ent external magnetic fields. The maximum of the longitudinal magnetostriction λ || for all the curves is observed near the TC ≈ 270 K, obtained by the TMA. Near the compensation temperature the λ || longitudinal magnetostriction (Fig. 4,b) changes its sign and becomes negative at low temperatures. Anomalies at these temperatures can be also seen on the thermal expansion curve ∆l/l (see Fig. 4,c). From these results the following comments can be made: (i) hydrogenation leads to a simple vo- lume expansion of the cubic lattice up to 20%; (ii) the Curie temperature, magnetic moment, and magnetostriction decrease drastically with increas- ing hydrogen concentration. As follows from Ref. 8, hydrogen in RFe2 occupies different positions de- pending on concentration. Our measurements are evidence that hydrogen incorporation at high con- centration (y = 3) strongly influences the crystal field acting on the rare-earth atoms. Conclusions Thus a comprehensive study of the structural, magnetic, and magnetoelastic properties of the TbxDy1−xFe2 compounds (x = 0.27; 0.41) and their hydrides has been made. The interstitial atoms oc- cupy sites adjacent to the rare-earth atoms, creating a change of crystal field that reflects the local symmetry and induces a significant change in the magnetic properties (Curie temperature, saturation magnetization, and magnetostriction). Acknowledgments We are very grateful to K.P. Skokov for prepara- tion of the samples. This work has been supported by RFBR Grants No 99-02-17821 and No 99-03- 32824. 1. Supermagnets: Hard magnetic materials, G. J. Long and F. Grandjean (eds. ), vol. 331 of NATO Advanced Study Institute, ser. C, Kluwer Acad. (1991). 2. D. G. R. Jones, P. J. McGuiness, J. S. Abell, and I. R. Harris, J. Less-Comm. Met. 158, 153 (1990). 3. A. E. Clark, J. P. Teter, and O. D. McMasters, J. Appl. Phys. 63, 3910 (1988). 4. L. Ruiz de Angulo, J. S. Abell, and I. R. Harris, J. Appl. Phys. 76, 7157 (1994). 5. S. Annapoorni, G. Markandeyulu, and K. V. S. Rama Rao, J. Appl. Phys. 65, 4955 (1989). 6. A. E. Clark, S. F. Cheng, J. P. Teter, M. Wung-Fogle, M. Q. Huang, and Y. Zheng, J. Magn. Magn. Mater. 104, 1433 (1992). 7. A. Ye. Yermakov, N. V. Mushnikov, N. K. Zajkov, V. S. Gaviko, and V. A. Barinov, Philos. Mag. B68, 883 (1993). 8. N. K. Zajkov, N. V. Mushnikov, A. Ye. Yermakov, Fiz. Met. Metalloved. 79, 50 (1995) (in Russian). Fig. 4. The temperature dependence of magnetization σ of crystalline Tb0.41Dy0.59Fe2H3 samples measured at an external magnetic field of 12 kOe (a). The temperature dependence of the longitudinal magnetostriction λ || measured at different values of external magnetic fields H, kOe: 2 (1), 10 (2), 12 (3) (b); Temperature dependence of the thermal expansion λt = ∆l/l (c). Fig. 3. The dependence of H/σ versus σ2 for Tb0.41Dy0.53Fe2H2.8 at different T, K: 280 (❏); 290 (∆), and 302 (●). The effect of hydrogen on the magnetostriction of rare-earth compounds Tb x Dy1–x Fe2 Fizika Nizkikh Temperatur, 2001, v. 27, No. 4 405