Ferromagnetic materials

Information

  • Patent Grant
  • 5382304
  • Patent Number
    5,382,304
  • Date Filed
    Monday, October 19, 1992
    32 years ago
  • Date Issued
    Tuesday, January 17, 1995
    30 years ago
Abstract
This invention provides a ferromagnetic material Fe.sub.60 M.sub.x N.sub.y where M is at least one element selected from Al, Ga, In and Tl, N is at least one element selected from P, As, Sb and Bi, x has a range of 1.ltoreq..times..ltoreq.39 and x+y=40 and excluding Fe.sub.60 Ga.sub.X AS.sub.y. A preferred ferromagnetic material is Fe.sub.60 Ga.sub.x As.sub.y , preferably when x has a range of 3.ltoreq..times..ltoreq.37, more preferably when x has a range of 20.ltoreq..times..ltoreq.37, and even more preferably when x has a range of 30.ltoreq..times..ltoreq.37. Typically, ferromagnetic materials of this type can be homogenised by annealing or melt spinning. Melt spun Fe.sub.60 Ga.sub.x As.sub.y can show Curie Temperatures (T.sub.c) of about 470.degree. C. and saturation magnestions of about 89 emu/g. Typically a ferromagentic material of the Fe.sub.60 M.sub.x N.sub.y has a B8.sub.2 type structure.
Description

SUMMARY OF THE INVENTION
This invention relates to ferromagnetic materials.
Ferromagnetic materials display a marked increase in magnetisation in an independently established magnetic field. The temperature at which ferromagnetism changes to paramagnetism is defined as one Curie Temperature, T.sub.c.
Ferromagnetic materials may be used for a wide variety of applications such as motors, electromechanical transducers. Most of these applications use ferromagnets made from SmCo.sub.5, (K Strnat et. al. J App Phys 38 p1OO1 1967), Sm.sub.2 Co.sub.17, (W Ervens Goldschmidt Inform 2:17 NR, 48 P3 1979), Nd.sub.2 Fe.sub.14 B (M Sagawa et. al. J App Phys 55 p2083 1984) and AlNiCo or ferrites (B D Cullity, Introduction to Magnetic Materials, Addison Wesley Publishing).
Nd.sub.2 Fe.sub.14 B has one of the highest reported Curie Temperatures of rare earth-iron based alloys at 315.degree. C. The inclusion of iron within an alloy is a well-established method of producing a ferromagnetic material. Iron has been used to dope GaAs in order to produce a material with ferromagnetic properties. I R Harris et. al. (J Crystal Growth 82 p450 1987) reported the growth of Fe.sub.3 GaAs with a T.sub.c of about 100.degree. C. More recently (International Patent Application Number PCT/GB 89/00381) it has been shown to be possible to obtain Curie Temperatures higher than those of Nd.sub.2 Fe.sub.14 B with M.sub.3 Ga.sub.2-x As.sub.x where 0.15.ltoreq..times..ltoreq.0.99 and M may represent Fe is partially substituted by either manganese or cobalt. Where M=Fe, and x=0.15 then the material is characterised by Curie Temperature of about 310.degree. C. Other ferromagnetic materials include that of GB 932,678, where the material has a tetragonal crystal structure and a transition metal composition component range of 61 to 75 %, and an amorphous alloy ferromagnetic filter of the general formula M.sub.x N.sub.y T.sub.z where M is selected as at least one element from iron, nickel and cobalt, N is at least one metalloid element selected from phosphorous, boron. Carbon and silicon and T is at least one additional metal selected from molybdenum, chromium, tungsten, tantalum, niobium, vanadium, copper, manganese. zinc, antimony, tin, germanium, indium, zirconium and aluminum and x has a range of between 60 and 95%.
According to this invention a ferromagnetic material having a B8.sub.2 type crystal structure comprises Fe.sub.60 M.sub.x N.sub.y where M is at least one element from the group of Al, Ga, In and Tl, N is at least one element from the group of P, As, Sb and Bi, where 1.ltoreq..times..ltoreq.39 and where x+y =40 and excluding Fe.sub.60 Ga.sub.x As.sub.y. .
Preferably the ferromagnetic has a composition where M is gallium and N is antimony. This preferred material preferably has a preferred range of x of 3.ltoreq..times..ltoreq.37, and even more preferred range of 20.ltoreq..times..ltoreq.37 and most preferably a range of 30.ltoreq..times..ltoreq.37.
The ferromagnetic material can be produced by methods including casting, which may be carried out in a Czochralski growth furnace. Where constituents of the ferromagnetic material are volatile at the high temperatures required for production, such as eg P and As, then an encapsulation layer is used to stop loss of the volatile constituents. A typical encapsulant is B.sub.2 0.sub.3.
Where homogenisation of the phases within the material is required, then techniques such as annealing or melt spinning may be employed. A typical annealing program is one carried out at a temperature between 600.degree. C. and 900.degree. C. for a time length of between 7 and 21 days.





BRIEF DESCRIPTION OF THE DRAWINGS
This invention will now be described by way of example only, with reference to the accompanying diagram: FIG. 1 is a schematic representation of a casting furnace.





DESCRIPTION OF THE PREFERRED EMBODIMENTS
Production of the ferromagnetic material by casting techniques may be seen in FIG. 1. A pyrolitic boron nitride (PBN) crucible 1 is placed within a furnace 2. The PBN crucible contains melt constituents 3 in appropriate ratios and typical purity values of 99.999%. With the PBN crucible in the furnace, valves 4 and 5 are closed, valves 6 and 7 are opened, And vacuum pump 8 pumps the furnace down to a vacuum of about 10.sup.-3 Torr. When a vacuum of this level is achieved, valves 6 and 7 are closed, the vacuum pump is stopped and valves 4 and 5 are opened. With valves 4 and 5 open, a continuous flow of high purity nitrogen gas is flushed through the furnace 2. The furnace is then heated up as quickly as possible until the melt constituents are molten. Boric oxide 9 forms an upper encapsulating layer on melting and prevents loss of volatile melt constituents.
The furnace is maintained at the elevated temperature for about 2 hours in order to facilitate substantially a fully homogeneous mixture of melt constituents. The furnace 2 is then switched off, with the PBN comacible 1 and its contents brought down to ambient temperature by .Furnace cooling in a flowing nitrogen atmosphere.
Where homogenisation of the ferromagnetic material is required the production may include an annealing process. A typical annealing program is to elevate, and maintain, the as cast material to temperature of about 800.degree. C. for about 14 days in a vacuum of about 10.sup.6 Torr. followed by furnace cooling.
Table 1 gives, by way of example only, specific compositions where M is gallium and N is antimony with typical saturation magnetization and T.sub.c values. It can be seen that for some compositions these values are provided for annealed samples, whilst all samples have typical melt spun values. Table 2 gives typical X-Ray diffraction data concerning lattice constants of ferromagnetic material where M is gallium and N is antimony
TABLE 1______________________________________ T.sub.c (.degree.C.) M.sub.s (emu/g)Ga/Sb Annealed M Spun Annealed M Spun______________________________________10/30 83 128 36 4120/20 309 308 72 6822.5/17.5 377 362 79 7625/15 382 81 78.527.5/12.5 431 384 83 81.529/11 389 8430/10 431 88 8232/8 461 360 94 8233/7 470 8534/6 472 463 8936/4 45838/2 458 89______________________________________
TABLE 2______________________________________Atomic % Annealed Melt Spun at vol at volFe Ga Sb a (.ANG.) c (.ANG.) (.ANG..sup.3) a (.ANG.) c (.ANG.) (.ANG..sup.3)______________________________________60 10 30 4.111 5.141 15.05 4.127 5.147 15.1960 20 20 4.108 5.110 14.94 4.110 5.116 14.9760 25 15 4.108 5.085 14.86 4.107 5.108 14.8860 30 10 4.105 5.066 14.79 4.106 5.074 14.8260 32 8 4.104 5.067 14.78 4.108 5.063 14.8060 34 6 4.103 5.051 14.7360 36 4 4.106 5.043 14.7360 38 2 4.114 5.030 14.75______________________________________
Claims
  • 1. A ferromagnetic material having a B8.sub.2 crystal structure consisting essentially of Fe.sub.60 M.sub.x N.sub.y where M is at least one element selected from the group consisting of Al, Ga, In and Tl; N is at least one element selected from the group consisting of As, Sb and Bi; where x has a range of 1.ltoreq..times..ltoreq.39; and where x+y=40 and wherein when M is Ga, N is not As.
  • 2. The ferromagnetic material according to claim 2 where M is Ga and N is Sb.
  • 3. The ferromagnetic material according to claim 2 where x has a range of 3.ltoreq..times..ltoreq.37.
  • 4. The ferromagnetic material according to claim 3 where x has a range of 20.ltoreq..times..ltoreq.37.
  • 5. The ferromagnetic material according to claim 3 where x has a range of 20.ltoreq..times..ltoreq.37 .
  • 6. The ferromagnetic material according to claim 4 where the material has been homogenized.
  • 7. The ferromagnetic material according to claim 6 where homogenization has been achieved by annealing.
  • 8. The ferromagnetic material according to claim 7 where annealing has been carried at a temperature of between 600.degree. C. and 900.degree. C.
  • 9. The ferromagnetic material according to claim 6 where homogenization has been achieved by melt spinning.
  • 10. A ferromagnetic material having a B8.sub.2 crystal structure consisting essentially of Fe.sub.60 M.sub.x N.sub.y where M is at least one element selected from the group consisting of Al, Ga, In and Tl; N is at least one element selected from the group consisting of As, Sb and Bi; where x has a range of 30.ltoreq..times..ltoreq.39; and where x+y=40 and wherein when M is Ga, N is not As.
Priority Claims (2)
Number Date Country Kind
9006055 Mar 1990 GBX
9006056 Mar 1990 GBX
PCT Information
Filing Document Filing Date Country Kind 102e Date 371c Date
PCT/GB91/00346 3/5/1991 10/19/1992 10/19/1992
Publishing Document Publishing Date Country Kind
WO91/14271 9/19/1991
US Referenced Citations (3)
Number Name Date Kind
3126346 Bither Mar 1964
5178689 Okamura et al. Jan 1993
5198040 Sawa et al. Mar 1993
Foreign Referenced Citations (4)
Number Date Country
0167118 Jan 1986 EPX
0258609 Mar 1988 EPX
0342921 Nov 1989 EPX
61-10209 Jan 1986 JPX
Non-Patent Literature Citations (4)
Entry
Moffatt, W. G., et al., "The Structure and Properties of Materials," vol. 1, pp. 46-47, 1964.
Journal of Applied Physics, vol. 55, No. 5, Mar. 1, 1984, M. Sagawa et al, "New Material for Permanent Magnets on a Base of Nd & Fe" pp. 2083-2089.
Journal of Applied Physics, vol. 38, No. 5, Mar. 1967, K. Strnat et al, "A Family of New Cobalt--Base Permanent Magnet Materials", pp. 1001--1002.
Journal of Crystal Growth, vol. 82, No. 3, Mar. 1987, Harris et al, "Phase Identification in Fe-Doped GaAs Single Crystals" pp. 450-458.