会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 3. 发明授权
    • Magneto-resistance effect element and magnetic head
    • 磁阻效应元件和磁头
    • US6052262A
    • 2000-04-18
    • US38848
    • 1998-03-12
    • Yuzo KamiguchiAkiko SaitoHideaki FukuzawaHitoshi IwasakiMasashi Sahashi
    • Yuzo KamiguchiAkiko SaitoHideaki FukuzawaHitoshi IwasakiMasashi Sahashi
    • G11B5/012G11B5/39H01L43/08
    • B82Y25/00B82Y10/00G11B5/3903G11B5/3967H01L43/08G11B2005/3996G11B5/012
    • A magneto-resistance effect element comprising a spin valve film including a first magnetic layer, a second magnetic layer and a non-magnetic layer interposed between the first magnetic layer and the second magnetic layer. Among the first and the second magnetic layers, in at least one of the magnetic layers, close-packed faces of crystal grains which constitute the magnetic layer are isotropically dispersed. Such a magnetic layer, by setting a film thickness of an under layer having an identical crystal structure with the magnetic layer at 2.0 nm or less and by dispersing isotropically close-packed faces of crystal grains constituting the under layer, can be obtained with reproducibility. According to a magneto-resistance effect element comprising such a spin valve film, while maintaining a large MR change rate, for example, magnetostriction constant can satisfy such a low magnetostriction as 1.times.10.sup.-6 or less. Further, excellent soft magnetic property can be provided.
    • 一种磁电阻效应元件,包括自旋阀膜,该自旋阀膜包括介于第一磁性层和第二磁性层之间的第一磁性层,第二磁性层和非磁性层。 在第一和第二磁性层中,在至少一个磁性层中,构成磁性层的晶粒的紧密堆积面各向同性地分散。 通过将具有与磁性层相同的晶体结构的下层的膜厚设定为2.0nm以下,通过使构成下层的晶粒的各向同性紧密堆积面分散,可以得到这样的磁性层。 根据包含这种自旋阀膜的磁阻效应元件,在保持大的MR变化率的同时,例如,磁致伸缩常数可满足1×10 -6以下的低磁致伸缩性。 此外,可以提供优异的软磁性。
    • 7. 发明授权
    • Laminated magnetorestrictive element of an exchange coupling film, an antiferromagnetic film and a ferromagnetic film and a magnetic disk drive using same
    • 交换耦合膜的叠层磁致伸缩元件,反铁磁膜和铁磁膜以及使用它的磁盘驱动器
    • US06313973B1
    • 2001-11-06
    • US09343270
    • 1999-06-30
    • Hiromi FukeKazuhiro SaitoKatsuhiko KouiHideaki FukuzawaAkiko SaitoHitoshi Iwasaki
    • Hiromi FukeKazuhiro SaitoKatsuhiko KouiHideaki FukuzawaAkiko SaitoHitoshi Iwasaki
    • G11B530
    • B82Y25/00B82Y10/00G11B5/012G11B5/3903G11B5/3967G11B2005/3996H01F10/3263H01F10/3268H01F10/3272
    • A magnetoresistive element comprises an exchange coupling film having a under layer, an antiferromagnetic film and a ferromagnetic film, which are laminated in that order, the under layer including a metal having a face centered cubic crystal structure or hexagonal closest packing crystal structure which have a longer nearest neighbor atomic distance than that of the antiferromagnetic film. With this construction, it is possible to improve the exchange coupling field and to satisfy a stable output over a long period of time. A magnetoresistive element having a dual spin valve structure has a magnetization adjusting layer, which is antiferromagnetically connected to a pinned layer via an anti-parallel connection layer, to adjust the value of the product of the saturation magnetization of each of the magnetization adjusting layer and the pinned layer by the thickness thereof. Moreover, a magnetoresistance head use a giant magnetoresistance effect, and has at least one pair of pinned layer and free layer arranged via a non-magnetic spacer layer. The pinned layer has a pair of ferromagnetic layers which have different compositions and different coercive forces and which are antiferromagnetically connected to each other via a connection layer, so that the effective exchange coupling field of the pinned layer is 200 Oe or more.
    • 磁阻元件包括具有下层,反铁磁膜和铁磁膜的交换耦合膜,其按顺序层压,下层包括具有面心立方晶体结构的金属或具有六面体最密堆积晶体结构的金属,其具有 比反铁磁膜的最近邻原子距离更长。 利用这种结构,可以改善交换耦合场并且能够长时间地满足稳定的输出。 具有双自旋阀结构的磁阻元件具有磁化调节层,其通过反并联连接层反铁磁连接到被钉扎层,以调节每个磁化调节层的饱和磁化强度和 被钉扎层的厚度。 此外,磁阻头使用巨磁电阻效应,并且具有通过非磁性间隔层布置的至少一对被钉扎层和自由层。 钉扎层具有一对铁磁层,其具有不同的组成和不同的矫顽力,并且经由连接层彼此反铁磁连接,使得钉扎层的有效交换耦合场为200Oe以上。
    • 8. 发明授权
    • Magnetic material
    • 磁性材料
    • US07076958B2
    • 2006-07-18
    • US10718518
    • 2003-11-24
    • Akiko SaitoTadahiko KobayashiTakao SawaMasashi Sahashi
    • Akiko SaitoTadahiko KobayashiTakao SawaMasashi Sahashi
    • F25B21/00C09K5/00H01F1/04
    • H01F1/015F25B21/00Y02B30/66
    • The magnetic material for magnetic refrigeration of the present invention is characterized by exhibiting, in a certain temperature region, preferably, only in part of a temperature region from 200 K to 350 K, an inflection point at which a second order differential coefficient of a magnetization curve changes from positive to negative with respect to a magnetic field, within the range of this magnetic field formed using a permanent magnet unit. This magnetic material of the present invention can generate a low temperature by using a relatively low magnetic field, by transferring the entropy between the electron spin system and the lattice system near the temperature at which an inflection point appears on the magnetization curve. Examples of the magnetic material meeting this condition are La(Fe,Si)13, (Hf,Ta)Fe2, (Ti,Sc)Fe2, and (Nb,Mo)Fe2, each containing 50 to 60 atomic % of transition metals such as Fe.
    • 本发明的磁性制冷用磁性材料的特征在于,在一定的温度范围内优选仅显示200K〜350K的温度区域的一部分,其中磁化强度的二阶微分系数 在使用永久磁铁单元形成的该磁场的范围内,曲线相对于磁场从正向变化为负。 本发明的这种磁性材料可以通过在电磁自旋系统和晶格系统之间传递熵在靠近磁化曲线上出现拐点的温度下,通过使用较低的磁场而产生低温。 满足该条件的磁性材料的实例是La(Fe,Si)13,(Hf,Ta)Fe 2 N,(Ti,Sc)Fe 2 /(Nb,Mo)Fe 2 N 2,各自含有50〜60原子%的过渡金属如Fe。
    • 9. 发明授权
    • Magnetic material
    • 磁性材料
    • US06676772B2
    • 2004-01-13
    • US10098568
    • 2002-03-18
    • Akiko SaitoTadahiko KobayashiTakao SawaMasashi Sahashi
    • Akiko SaitoTadahiko KobayashiTakao SawaMasashi Sahashi
    • H01F1055
    • H01F1/015F25B21/00Y02B30/66
    • The magnetic material for magnetic refrigeration of the present invention is characterized by exhibiting, in a certain temperature region, preferably, only in part of a temperature region from 200 K to 350 K, an inflection point at which a second order differential coefficient of a magnetization curve changes from positive to negative with respect to a magnetic field, within the range of this magnetic field formed using a permanent magnet unit. This magnetic material of the present invention can generate a low temperature by using a relatively low magnetic field, by transferring the entropy between the electron spin system and the lattice system near the temperature at which an inflection point appears on the magnetization curve. Examples of the magnetic material meeting this condition are La(Fe,Si)13, (Hf,Ta)Fe2, (Ti,Sc)Fe2, and (Nb,Mo)Fe2, each containing 50 to 60 atomic % of transition metals such as Fe.
    • 本发明的磁性制冷用磁性材料的特征在于,在一定的温度范围内优选仅显示200K〜350K的温度区域的一部分,其中磁化强度的二阶微分系数 在使用永久磁铁单元形成的该磁场的范围内,曲线相对于磁场从正向变化为负。 本发明的这种磁性材料可以通过在电磁自旋系统和晶格系统之间传递熵在靠近磁化曲线上出现拐点的温度下,通过使用较低的磁场而产生低温。 满足该条件的磁性材料的实例是La(Fe,Si)13,(Hf,Ta)Fe 2,(Ti,Sc)Fe 2和(Nb,Mo)Fe 2,每个含有50至60原子%的过渡金属 如Fe。
    • 10. 发明授权
    • Permanent magnet
    • 永久磁铁
    • US06475302B2
    • 2002-11-05
    • US09749803
    • 2000-12-28
    • Wu MeiToshiya SakamotoShinya SakuradaTakao SawaAkihiko TsutaiAkiko SaitoMasashi Sahashi
    • Wu MeiToshiya SakamotoShinya SakuradaTakao SawaAkihiko TsutaiAkiko SaitoMasashi Sahashi
    • H01F1055
    • H01F1/058H01F1/0306H01F1/055H01F1/057
    • Disclosed is a permanent magnet which comprises an alloy containing a hard magnetic phase having a ThMn12 type tetragonal structure and a nonmagnetic phase. The alloy is represented by a general formula given below: [R1-a(M1)a][T1-b-c(M2)b(M3)c]dx&agr; where R is at least one rare earth element (including Y), Ml is at least one element selected from the group consisting of Zr and Hf, T is at least one element selected from the group consisting of Fe, Co and Ni, M2 is at least one element selected from the group consisting of Cu, Bi, Sn, Mg, In and Pb, M3 is at least one element selected from the group consisting of Al, Ga, Ge, Zn, B, P and S, X is at least one element selected from the group consisting of Si, Ti, V, Cr, Mn, Nb, Mo, Ta and W, and the atomic ratios of a, b, c, d and &agr; fall within the ranges of 0≦a≦0.6, 0.01≦b≦0.20, 0≦c≦0.05, 6≦d≦11, and 0.5≦&agr;≦2.0.
    • 公开了一种永磁体,其包含含有ThMn 12型四方晶系的硬磁相和非磁性相的合金。 该合金由以下给出的通式表示:其中R是至少一种稀土元素(包括Y),M1是选自Zr和Hf中的至少一种元素,T是至少一种选自 由Fe,Co和Ni构成的组,M2是选自Cu,Bi,Sn,Mg,In和Pb中的至少一种元素,M3是选自Al,Ga,Ge中的至少一种元素 ,Zn,B,P和S中的至少一种,X是选自由Si,Ti,V,Cr,Mn,Nb,Mo,Ta和W组成的组中的至少一种元素,并且a,b,c, d和α落在0 <= a <= 0.6,0.01 <= b <= 0.20,0 <= c <= 0.05,6 <= d <= 11和0.5 <=α<2.0的范围内。