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1.
The electrical resistivity and average magnetic moment per atom of Ni3(Fe, Ti) and Ni3(Mn, Ti) alloys were measured. X-ray structural analysis revealed the presence of the Ni3Ti phase in Ni3(Fe+7% Ti) and Ni3(Fe + 10.3% Ti), and strong interaction of Ni and Ti is deduced. The introduction of Ti into Ni3Mn reduces the antiferromagnetic Mn-Mn interaction and thus leads to greater ordering.Deceased.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 5, pp. 9–12, May, 1981.  相似文献   

2.
The ordinary Hall constant Ro of quenched Ni3(Fe, Ti) and Ni3(Mn, Ti) alloys was measured. The number of 4s and 3d electrons per atom was calculated on the basis of a four-band model. At low Ti concentrations in Ni3(Fe, Ti) the contribution of 3d holes to Ro is negligible, but at high concentrations it is significant. The contribution of 3d holes to Ro for Ni3(Mn, Ti) is considerable, and for Ni3Mn and Ni3(Mn +9.8% Ti) it is dominant. It is concluded that the changes in band energy of the bond between Ni and Ti in the considered systems are of a different nature.Deceased.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 5, pp. 12–14, May, 1981.  相似文献   

3.
The normal and anomalous Hall constants R0 and Rs, respectively, and the resistivity have been measured for the quasibinary alloys Ni3Mn-Ni3Fe and Ni3Mn-Ni3Co. The results imply that in ternary alloys of Ni3Mn containing slight Fe and Co impurities the hole regions of the Fermi surface make an important contribution to R0 and that the primary scattering mechanism for the carriers corresponding to the anomalous Hall current in the alloys with Fe at room temperature is phonon scattering. It is concluded that the Fermi surface of the Ni3Mn-Ni3Fe alloys is closed.Translated from Izvestiya VUZ. Fizika, No. 3, pp. 21–29, March, 1970.  相似文献   

4.
Some regularities of the fracture of ordered polycrystals of the alloys Ni3Fe, Ni3(FeMn), Ni3FeAl), Ni3(FeCr), Ni3(FeCr) are studied. The alloys Ni3Fe, Ni3(FeMn), and Ni3(FeAl) possess low plasticity in the ordered state at the test temperatures T < 100 °C. In the 100–200 ° C temperature range a brittleness-viscosity transition is detected which is analogous to that observed in body centered cubic (BCC) metals and alloys. The transition from the brittle into the plastic state is not accompanied by a change in the metallographic picture of slip. The distinguishing peculiarity of the strain at elevated temperatures is the significant displacement of the grains along the boundaries. The temperature band of the transition from the brittle into the plastic state of ordered alloys in the tempered state (tempering from a temperature below the temperature of the order-disorder transformation) is observed at tempering temperatures above 450 °C (tests at room temperature). The results obtained permit the assumption that a reduction in the plasticity in ordering alloys based on Ni3Fe is caused by segregation of the impurities along the grain boundaries.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii Fizika, No. 6, pp. 35–41, June, 1971.  相似文献   

5.
Features of the electronic structure of ternary alloys of the quasibinary Ni3Mn-Ni3Fe and Ni3Mn-Ni3Co systems are discussed on the basis of an analysis of the changes in the absolute thermal emf S and in the conductivity . It is concluded that all the ternary Ni3Mn-Ni3Fe alloys have a closed Fermi surface in both the disordered and ordered states. It is confirmed experimentally that a deep minimum appears on the state-density curve Nd(E) during the ordering of Ni3Mn-Ni3Fe alloys, and the alloy composition whose Fermi surface corresponds to this minimum is given.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii Fizika, No. 8, pp. 126–133, August, 1969.  相似文献   

6.
An experimental investigation was made into the influence of the addition of copper and aluminum on the saturation magnetization Js and magnetostriction s of the Ni3Mn alloy. It is shown that the behavior of Js and s depends on the distribution of the atoms of the added element over the sites of the fcc lattice of the Ni3Mn alloy.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 2, pp. 29–33, February, 1981.We should like to thank A. I. Lotkov for the alloys made available for investigation.  相似文献   

7.
An experimental study was made of the changes in the normal and anomalous Hall constants R0 and Rs, respectively, the internal saturation induction Bs, and the resistivity ? during the ordering of quasibinary Ni3Mn-Ni3Fe and Ni3Mn-Ni3Co alloys. The concentration dependences of R0, Rs, Bs, and ? were also studied in the ordered state of these alloys. It is concluded from an analysis of the experimental results that the decreases inR0 and ? during the ordering of Ni3Mn and as a result of the alloying of ordered Ni3Mn with slight amounts (~5 at. %) of iron are due primarily to a decrease in the hole contribution to transport and to a decrease in the state density in the 3d band of these alloys near the Fermi level. The experimental data are in satisfactory agreement with the curve calculated by Yamashita et al. [6] for the density of 3d states in ordered Ni3Mn and Ni3Fe alloys.  相似文献   

8.
Investigations of atomic ordering in Ni3Fe, Ni3(Fe, Nb), Ni3(Fe,Cr) and Ni3(Fe, Mn) alloys at room temperature in disordered and ordered states have been carried out by Mössbauer spectroscopy method. The experimental results confirm that in case of Ni3Fe superstructure stabilization is achieved by Nb and Mn atoms, the Cr atoms disturb this structure.  相似文献   

9.
Yield point, hardening factor, and elastic modulus are reported as functions of quenching and test temperatures for the alloys Ni3(Fe + 3 at% Al), Ni3(Fe + 3 at% Mn). A maximum is found in the mechanical properties near the critical temperature Tcr; this does not occur for alloys in the disordered state. The deformation aging under load is examined near this maximum and at 200 ° C. A range of linear hardening occurs up to e of 15–18% in ordered alloys, which is replaced by a range of decreasing hardening coefficient at higher . The results are discussed by reference to earlier ones for Ni3Fe, Ni3(FeCr). Ni3(FeMo).  相似文献   

10.
The anomalous Hall (Rs) and the Nerst-Ettingshausen (QS) constants are measured for hardened Ni3 (Fe, Ti) and Ni3 (Mn, Ti) alloys. Scattering by phonons is detected, con tributing primarily to RS as compared to scattering by magnetic inhomogeneities. Based on the positive signs of Rg and QS, it is concluded that 3d holes wi th antiparallel spin make the main contribution to the conductivity. A model is proposed for the electronic structure of the alloys studied.DeceasedTranslated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 6, pp. 59—63, June, 1981.  相似文献   

11.
Perturbation theory has been applied to the structure of the 4s band of Ni3Mn and Ni3Fe ordered alloys; the Fermi surfaces have been constructed for these alloys in the one-wave approximation, and the electron state densities and electron energy change on ordering have been calculated. It is found that the contribution of the 4s electrons to the ordering energy is much less than that of the 3d electrons.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 7, pp. 102–106, July, 1972.  相似文献   

12.
A study has been made of the change in the Young's modulus, yield point, hardness, hardening coefficient, slip pattern, and duration of the linear stage in the flow curves during the isothermal ordering of the polycrystalline alloys Ni3Fe, Ni3(Fe + 2% Al), Ni3(Fe + 3% Mn), and Ni3(Fe + 2.5% Cr). A definite relationship has been observed between the changes in these properties at the various stages of ordering.  相似文献   

13.
Calculations of the band structure of the ferromagnetic alloys Ni3Mn, Ni3Fe, and Ni3Co are presented. The results are compared with experimental data. Change in the electronic structure as one goes from Ni3Mn to Ni3Co is analyzed. The occurrence of ferromagnetism in the alloys studied and the possibility of their existence in an ordered ferromagnetic state are examined.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 6, pp. 82–88, June, 1988.  相似文献   

14.
The effects of a chromium admixture on certain properties of the electronic structure and on the ordering of Ni3Mn have been studied by neutron diffraction and by measurement of the resistivity , the internal saturation induction BS, and the absolute thermal emf S. Analysis of the experimental data implies a closed Fermi surface for the Ni3(Mn, Cr) alloys with a low chromium concentration c but an open Fermi surface for high c.Translated from Izvestiya VUZ. Fizika, No. 2, pp. 44–51, February, 1970.  相似文献   

15.
The influence of alloying the Ni3Mn alloy with titanium, vanadium, or copper, on the superstructure of the alloy, was studied by the neutron diffraction method. It was shown that Ti, V, and Al stabilize the superstructure of Ni3Mn, and Cu actively destroys it. The distribution of atoms of the alloying elements along the sites of fcc lattice and its connection with the electron structure of the alloy was analyzed. The different influence of alloying with a third element on the superstructure in alloys Ni3Mn and Ni3Fe is explained.  相似文献   

16.
The intermetallic compound Zr2Ni has been found to take up hydrogen on charging at room temperature. Zr2(NiFe) H4.7 and Zr2(NiFe) H4.5 show the same structure (CuAl2 type) as the uncharged compound but with an expanded lattice.Analysis of room temperature spectra in zero and applied fields indicates that the57Fe atoms occupy Ni sites in Zr2(Ni 57Fe). Volume expansion effects account for about one third of the increase in isomer shift ( +0.58 mms–1) observed on hydrogenation. The distribution of hydrogen atoms around the probe37Fe atoms also causes a decrease of 0.23 mms–1 in the mean value for the quadrupole splitting compared Rith uncharged Zr2Ni.  相似文献   

17.
To examine the pressure dependence of magnetic characteristics of Fe and Ni films, the films were prepared in vacuum ranging from 10–5 to 10–2 torr.Saturation magnetizationM s * , perpendicular anisotropyK * and coercive forceH c for Fe and Ni films deposited at around 10–5 torr were in good agreement with the values obtained by others. When the film thickness was less than 500 ,M s * for Fe films increased with pressure, while it decreased monotonically for Ni films. At pressures between 2×10–3 and 10–2 torr,M s * decreased rapidly for Fe but it increased slightly for Ni. This interesting behaviour was most marked with film thickness of about 500 . Corresponding to the change inM s * , bothK * andH c also changed with deposition pressure.The result should be explained in terms of the presence of Fe4N, Fe8N and Ni3N, as well as the macroscopic and microscopic structures of films.  相似文献   

18.
The various factors which can affect ordering in alloys are analyzed. The results of the analysis are applied to the ordering in Ni3(Mn, Me) (Me = Fe, Co, or Cr) alloys. It is concluded that the accelerated ordering in these cases is caused by a change in the ordering mechanism from a homogeneous mechanism in Ni3Mn to a heterogeneous mechanism in the ternary alloys and by an increase in the vacancy concentration due to doping.Translated from Izvestiya Vysshikh Uchebnykh Zavadenii Fizika, No. 1, pp. 73–78, January, 1970.  相似文献   

19.
An experimental study was made of the strain hardening of the Ni3Fe alloy in disordered and ordered states as a function of the grain size. An analysis of the stress-strain diagrams was made using the Hall-Petch equation allowing for the contributions of the density of statistically stored dislocations s and the density of geometrically expected dislocations g to the total dislocation density .Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 2, pp. 33–37, February, 1981.  相似文献   

20.
The kinetics of order-disorder transformation in Ni3(Mn, Al) alloys prequenched from 700°C has been studied by neutron-diffraction analysis. Within the framework of the I. M. Lifshits model, it is shown that in Ni3(Mn, Al) alloys containing 2.0 and 4.3 at.% aluminum, ordering proceeds by the homogeneous mechanism at 400° and by nucleation and growth at 450°. The causes are discussed of the sharp speedup of the order-disorder transformation in its first stage in aluminum-doped Ni3Mn alloy as compared with the binary alloy.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 4, pp. 24–28, April, 1977.  相似文献   

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