TW448430B - Method for forming magneto-resistance effect film - Google Patents
Method for forming magneto-resistance effect film Download PDFInfo
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- TW448430B TW448430B TW088111363A TW88111363A TW448430B TW 448430 B TW448430 B TW 448430B TW 088111363 A TW088111363 A TW 088111363A TW 88111363 A TW88111363 A TW 88111363A TW 448430 B TW448430 B TW 448430B
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- 238000000034 method Methods 0.000 title claims abstract description 61
- 230000000694 effects Effects 0.000 title claims abstract description 49
- 239000007789 gas Substances 0.000 claims abstract description 85
- 230000005415 magnetization Effects 0.000 claims abstract description 68
- 239000000758 substrate Substances 0.000 claims abstract description 62
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 claims abstract description 59
- 239000001301 oxygen Substances 0.000 claims abstract description 59
- 229910052760 oxygen Inorganic materials 0.000 claims abstract description 59
- 229910052786 argon Inorganic materials 0.000 claims abstract description 34
- 238000004519 manufacturing process Methods 0.000 claims abstract description 24
- 230000005290 antiferromagnetic effect Effects 0.000 claims abstract description 20
- 238000004544 sputter deposition Methods 0.000 claims abstract description 13
- 230000005291 magnetic effect Effects 0.000 claims description 86
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 claims description 66
- 230000002542 deteriorative effect Effects 0.000 abstract description 3
- 239000000203 mixture Substances 0.000 abstract 1
- 239000010410 layer Substances 0.000 description 211
- 230000005294 ferromagnetic effect Effects 0.000 description 49
- 238000012360 testing method Methods 0.000 description 28
- 238000012545 processing Methods 0.000 description 26
- 230000015572 biosynthetic process Effects 0.000 description 11
- 229910003271 Ni-Fe Inorganic materials 0.000 description 10
- 230000000052 comparative effect Effects 0.000 description 9
- 229910052704 radon Inorganic materials 0.000 description 7
- SYUHGPGVQRZVTB-UHFFFAOYSA-N radon atom Chemical compound [Rn] SYUHGPGVQRZVTB-UHFFFAOYSA-N 0.000 description 7
- 238000007781 pre-processing Methods 0.000 description 6
- 239000011241 protective layer Substances 0.000 description 6
- 239000013078 crystal Substances 0.000 description 5
- 238000010168 coupling process Methods 0.000 description 4
- 238000005859 coupling reaction Methods 0.000 description 4
- 239000012535 impurity Substances 0.000 description 4
- 239000012528 membrane Substances 0.000 description 4
- 230000008878 coupling Effects 0.000 description 3
- 230000007423 decrease Effects 0.000 description 3
- 230000001965 increasing effect Effects 0.000 description 3
- 230000003746 surface roughness Effects 0.000 description 3
- 238000012546 transfer Methods 0.000 description 3
- MYMOFIZGZYHOMD-UHFFFAOYSA-N Dioxygen Chemical compound O=O MYMOFIZGZYHOMD-UHFFFAOYSA-N 0.000 description 2
- 238000002441 X-ray diffraction Methods 0.000 description 2
- 238000004140 cleaning Methods 0.000 description 2
- 238000001816 cooling Methods 0.000 description 2
- 230000001419 dependent effect Effects 0.000 description 2
- 230000006866 deterioration Effects 0.000 description 2
- 229910001882 dioxygen Inorganic materials 0.000 description 2
- 229910052735 hafnium Inorganic materials 0.000 description 2
- VBJZVLUMGGDVMO-UHFFFAOYSA-N hafnium atom Chemical compound [Hf] VBJZVLUMGGDVMO-UHFFFAOYSA-N 0.000 description 2
- 229910000889 permalloy Inorganic materials 0.000 description 2
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 2
- 229910017060 Fe Cr Inorganic materials 0.000 description 1
- 229910002544 Fe-Cr Inorganic materials 0.000 description 1
- 229910001030 Iron–nickel alloy Inorganic materials 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 230000005303 antiferromagnetism Effects 0.000 description 1
- 230000000739 chaotic effect Effects 0.000 description 1
- UPHIPHFJVNKLMR-UHFFFAOYSA-N chromium iron Chemical compound [Cr].[Fe] UPHIPHFJVNKLMR-UHFFFAOYSA-N 0.000 description 1
- 239000002772 conduction electron Substances 0.000 description 1
- 230000001808 coupling effect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005108 dry cleaning Methods 0.000 description 1
- 239000000428 dust Substances 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 239000003302 ferromagnetic material Substances 0.000 description 1
- 238000005242 forging Methods 0.000 description 1
- 238000009499 grossing Methods 0.000 description 1
- 230000001771 impaired effect Effects 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- 230000001939 inductive effect Effects 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 229910052741 iridium Inorganic materials 0.000 description 1
- 238000003475 lamination Methods 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 229910052748 manganese Inorganic materials 0.000 description 1
- 125000004430 oxygen atom Chemical group O* 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 238000007747 plating Methods 0.000 description 1
- 229910052702 rhenium Inorganic materials 0.000 description 1
- WUAPFZMCVAUBPE-UHFFFAOYSA-N rhenium atom Chemical compound [Re] WUAPFZMCVAUBPE-UHFFFAOYSA-N 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 238000001179 sorption measurement Methods 0.000 description 1
- 125000006850 spacer group Chemical group 0.000 description 1
- 230000006641 stabilisation Effects 0.000 description 1
- 238000011105 stabilization Methods 0.000 description 1
- 238000003860 storage Methods 0.000 description 1
Classifications
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y25/00—Nanomagnetism, e.g. magnetoimpedance, anisotropic magnetoresistance, giant magnetoresistance or tunneling magnetoresistance
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y40/00—Manufacture or treatment of nanostructures
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F10/00—Thin magnetic films, e.g. of one-domain structure
- H01F10/32—Spin-exchange-coupled multilayers, e.g. nanostructured superlattices
- H01F10/324—Exchange coupling of magnetic film pairs via a very thin non-magnetic spacer, e.g. by exchange with conduction electrons of the spacer
- H01F10/3268—Exchange coupling of magnetic film pairs via a very thin non-magnetic spacer, e.g. by exchange with conduction electrons of the spacer the exchange coupling being asymmetric, e.g. by use of additional pinning, by using antiferromagnetic or ferromagnetic coupling interface, i.e. so-called spin-valve [SV] structure, e.g. NiFe/Cu/NiFe/FeMn
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F41/00—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
- H01F41/14—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for applying magnetic films to substrates
- H01F41/30—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for applying magnetic films to substrates for applying nanostructures, e.g. by molecular beam epitaxy [MBE]
- H01F41/302—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for applying magnetic films to substrates for applying nanostructures, e.g. by molecular beam epitaxy [MBE] for applying spin-exchange-coupled multilayers, e.g. nanostructured superlattices
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N50/00—Galvanomagnetic devices
- H10N50/01—Manufacture or treatment
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- Nanotechnology (AREA)
- Crystallography & Structural Chemistry (AREA)
- Manufacturing & Machinery (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Hall/Mr Elements (AREA)
- Magnetic Heads (AREA)
- Thin Magnetic Films (AREA)
Abstract
Description
4484 3 Ο 五、發明說明(l) — ----- 發明所屬技術領域 本發明係有關於磁阻功效膜之製造方法。更詳而+ 之,係有關於可在不令積層膜之結晶性劣化下改盖積屏 面之平坦性之磁阻功效膜之製造方法。又,用本^明二二 造方法所形成之磁阻功效膜適合用於將寫入硬碟片、磁二 片、磁帶等之磁性信號讀取用磁頭及磁性感測器等。…、 習知技術4484 3 〇 5. Description of the invention (l) — ----- TECHNICAL FIELD OF THE INVENTION The present invention relates to a method for manufacturing a magnetoresistive film. More specifically, + relates to a method for manufacturing a magnetoresistive effect film that can change the flatness of the build-up screen without deteriorating the crystallinity of the build-up film. In addition, the magnetoresistive effect film formed by the method of the present invention is suitable for a magnetic signal reading head and a magnetic sensor for reading magnetic signals written on a hard disk, a magnetic disk, a magnetic tape, and the like. ..., know-how
伴隨磁性記錄密度之提高,媒體所記錄信號磁場之讀 取頭(讀取用磁頭)之形態正自將磁場變化之時間微分讀^ 後輸出之感應型磁頭移向將磁場強度讀取後輸出之磁阻功 效型磁頭。在磁阻功效型磁頭所用之磁阻功效元件上,當 初使用顯示電阻隨元件之通電電流方向和磁化方向之角度 ,變之異向性磁阻功效(AMR)之坡莫合金等之合金獏’但夂 是近年來在Fe-Cr多層膜、Co/Cu多層膜等發現顯示比AMR 大之電阻變化率之巨大磁阻功效(GMR),期待應用於GMR之 磁阻功效元件。 在這種GMR之磁阻功效元件之構造上,除了由在上述 基體之表面上夾著非磁性體層(間隔片)堆積多層強磁性體 層之構造體構成之人工格子型以外,由在基體之表面上夾 著非磁性體層堆積強磁性體層而在最後設置之該強磁性體 層之表面形成了反強磁性體層之構造體構成之自旋閥型係 周知。 在任一種型式’ GMR係電阻隨在構成積層膜之強磁性With the increase of magnetic recording density, the form of the reading head (reading head) of the magnetic field of the signal recorded by the medium is shifted from the time of the magnetic field change to the inductive magnetic head output. Magnetic resistance type magnetic head. On the magnetoresistive element used in the magnetoresistive element type magnetic head, alloys such as permalloy which show the resistance change with the direction of the element's current flow and the direction of magnetization, such as Permalloy, which is anisotropic magnetoresistance effect (AMR). However, in recent years, it has been found in Fe-Cr multilayer films, Co / Cu multilayer films, etc. that it has a large magnetoresistance effect (GMR) showing a larger rate of change in resistance than AMR. In the structure of such a GMR magnetoresistive element, in addition to the artificial lattice type composed of a structure in which a plurality of ferromagnetic layers are stacked on the surface of the above-mentioned substrate, a non-magnetic layer (spacer) is stacked. A spin valve type having a structure in which a ferromagnetic layer is stacked on top of a non-magnetic layer and an anti-ferromagnetic layer is formed on a surface of the ferromagnetic layer provided last is known. In either type, the GMR series resistors follow the strong magnetic properties of the laminated film
第5頁 4484 3 0 五、發明說明(2) 體層之層間之磁化方向之相對角度而變之現象,係在元件 流動之傳導電子在非磁性體層和強磁性體層之界面亂流時 由亂流之方向因電子具有之自旋之方向及強磁性體層之磁 化方向而異之被稱為自旋相依散亂之性質所引起之界面現 象。在利用這種現象之積層膜,在經由非磁性體層相向之 各強磁性體層所發生之磁化方向變成反平行排列之情況顯 示高電阻’而在平行排列之情況顯示低電阻。 在特開平4-3583 1 0號公報公開將顯示GMR之積層膜之 中之自旋閥型磁阻功效元件應用於讀取用磁頭之技術,已 在硬碟用磁性記錄裝置實用化。 如上 成。即, 強磁性體 磁性體層 稱為固定 換磁性異 會引起磁 固定磁化 生之磁化 因此 況,在讀 自媒體之 層之磁化 而變,得 返所示,自旋閥 間隔非磁 層在和與 。在堆積 磁化層或 向性將磁 化轉動。 層及非磁 對於外部 ,在將上 取媒體所 信號磁場 方向構成 到讀取輸 性體層 非磁性 了該反 自旋層 化方向 而,不 性體層 磁場自 述構造 記錄之 ’夬固 之相對 出。 型磁阻功效元件基本上由4層構 设置2層強磁性體層,在一方之 體層之接觸面反側之面設置反強 強磁性體層之強磁性體層(一般 )所發生之磁化因利用感應之交 固定為單方向’對於外部磁場不 堆積反強磁性體層,在至少經由 和反強磁性體層接觸之位置所發 由的磁化轉動。 之磁阻有效應元件用作磁頭之情 信號時,對於成為外部磁場之^ 定磁化層之磁化方向和自由磁化 角度變化,磁阻隨自旋相依散亂Page 5 4484 3 0 V. Description of the invention (2) The relative angle of the magnetization direction between the layers of the body layer changes due to the turbulent flow of the conduction electrons flowing through the element at the interface between the nonmagnetic layer and the ferromagnetic layer. The direction varies depending on the direction of the spin of the electron and the direction of magnetization of the ferromagnetic layer. It is an interface phenomenon caused by the nature of the spin phase scatter. In a laminated film using this phenomenon, a high resistance is shown when the magnetization directions of the ferromagnetic layers facing each other through the non-magnetic layer are aligned in antiparallel, and a low resistance is shown in a parallel arrangement. Japanese Unexamined Patent Publication No. 4-3583 10 discloses a technology in which a spin-valve type magnetoresistive element in a laminated film showing GMR is applied to a magnetic head for reading, and has been put into practical use in a magnetic recording device for a hard disk. As above. That is, the ferromagnetic layer is called the fixed magnetic exchange layer, which will cause the magnetic fixed magnetization to generate magnetization. Therefore, the magnetization of the layer read from the medium changes, as shown in the figure below. The spin valve is spaced between the non-magnetic layer and. The magnetization is turned on the stacked magnetization layer or anisotropy. Layers and non-magnetic For the external, the direction of the signal magnetic field from the pickup medium is read to read the output layer. The anti-spin layering direction is non-magnetic. The magnetic field of the insulative layer is self-explanatory. The magnetoresistive effect element is basically composed of 4 ferromagnetic layers in a 4-layer structure, and a ferromagnetic layer (generally) of an anti-ferromagnetic layer is provided on the opposite side of the contact surface of one body layer. Intersection is fixed in a single direction. No antiferromagnetic layer is deposited on the external magnetic field, and the magnetization rotation is caused at least through a position in contact with the antiferromagnetic layer. When the magnetic resistance effect element is used as a magnetic head signal, the magnetization direction and free magnetization angle of the ^ fixed magnetization layer that becomes an external magnetic field change, and the magnetic resistance is scattered with the spin phase dependence.
4484 3 0 五、發明說明(3) 為了令由上述構造構成自旋閥型磁阻功效元件有效的 作用,在固定磁化層發生之磁化方向之穩定之固定,即交 換磁性異向性之控制及自旋相依散亂之控制變得重要。為 了提高這些控制性,需要提高構成積層膜之各層之結晶粒 子之結晶性,而且實現散亂少之積層界面。 尤其’自旋閥型磁阻功效元件如上述所示,因利用係 界面現象之自旋相依散亂’其特性受到積層膜之積層界面 之狀態強烈影響。因此,在界面之粗糙度大之情況,由於 由其凹凸所引起之局部性強磁性相互作用,本來必須實現 之磁化方向之反平行排列混亂,自旋相依散亂無法有效的 作用,電阻變化量減少,抑制巨大磁阻功效。因而,強烈 要求改善積層界面之平坦性。 ^ 本發明之目的在於提供一種磁阻功效膜之製造方法, 藉著在不令積層膜之結晶性劣化下改善積層界面之平坦 性’可形成可更高靈敏度的讀取磁性信號之具有高㈣比之 磁阻功效元件。 發明之概要 本發明之第一種磁阻元件之製造方法係關於在既定之 基體上順向或逆向堆積自由磁化層、非磁性體層、固定磁 化層以及反強磁性體層而成之磁阻功效膜之製造方法,其 特徵在:於至少具有藉著在成膜室内配置該基體,並將該 成膜室内之到達真空度設為約⑺,^^以下後,在該成膜 室引入至少含有氧氣之氣體a,將該成膜室内之真空度變4484 3 0 V. Description of the invention (3) In order to make the spin-valve-type magnetoresistance effect element composed of the above structure effective, the stabilization of the direction of magnetization occurring in the fixed magnetization layer, that is, the control of exchange magnetic anisotropy and Control of spin-dependent scatter becomes important. In order to improve these controllability, it is necessary to improve the crystallinity of the crystalline particles of each layer constituting the laminated film, and to realize a laminated interface with less scattering. In particular, the 'spin-valve type magnetoresistance effect element is as described above, and its characteristics are strongly affected by the state of the laminated interface of the laminated film due to the spin-dependent scattering of the interfacial phenomenon. Therefore, when the roughness of the interface is large, due to the local strong magnetic interaction caused by its unevenness, the anti-parallel arrangement of the magnetization directions that must be achieved is chaotic, the spin phase scattering is not effective, and the change in resistance is not effective. Reduce and suppress the effect of huge magnetoresistance. Therefore, it is strongly desired to improve the flatness of the laminated interface. ^ The object of the present invention is to provide a method for manufacturing a magnetoresistive film, by improving the flatness of the laminated interface without deteriorating the crystallinity of the laminated film, a high-sensitivity reading magnetic signal can be formed. Compared to magnetoresistive effect elements. SUMMARY OF THE INVENTION The first method for manufacturing a magnetoresistive element of the present invention is a magnetoresistive film formed by stacking a free magnetization layer, a nonmagnetic layer, a fixed magnetization layer, and an antiferromagnetic layer on a predetermined substrate in a forward or reverse direction. The manufacturing method is characterized in that at least the substrate is disposed in the film forming chamber, and the degree of vacuum in the film forming chamber is set to about ⑺, ^^ or less, and then at least oxygen is introduced into the film forming chamber. The gas a changes the degree of vacuum in the film forming chamber.
4484 3 Ο 五、發明說明(4) ' 更成3 XlO_9Torr以上且1 xlO-8Torr以下之固定壓力後 ^ 著引入由氬氣構成之氣體b ’使用該氣體a和氣體b之、. 氣體濺鍍既定之對象,形成位於該非磁性體層之下之"&該"自 由磁化層或該固定磁化層和該非磁性體層之製程a 若依據該第一種製造方法,藉著在將成臈室内之到達 真空度設為1 0-1QTorr以下後,引入既定量之氧氣,使用今 氧氣和氬氣利用濺鍵法形成位於非磁性體層之下+ A丄Α s、卜之自由磁 化層或固定磁化層和該非磁性體層,這3層之良好之結曰 性不會受損,抑制膜之表粗链度。即,改善在自由磁化層 和非磁性體層之界面或在固定磁化層和非磁性體 之平坦性’磁阻功效膜之MR比增大。這作用在將引入含有 氧氣之氣體a後之真空度設為3 X 10_gTorr以上1 X 1〇-8Tq 以下之範圍時發生。此外’在該自由磁化層採用了多声膜 之情況,在該多層膜之全部之界面期待該平坦性效果7 、 本發明之第二種磁阻元件之製造方法係關於在既定之 基體上順向或逆向堆積自由磁化層、非磁性體層、固定磁 化層以及反強磁性體層而成之磁阻功效膜之製造方法,其 特徵在於至少具有:在該自由磁化層上堆積該非磁性體層 之情況在形成該自由磁化層後’或在該固定磁化層上堆積 該非磁性體層之情況在形成該固定磁化層後,在成膜室引 入至少含有氧氣之氣體a,如位於該非磁性體層之下之該 自由磁化層或該固定磁化層之表面之曝露量變為6L以上且 20L 以下(但lL(Langmuir) = l XlCHorrosec)般,在既定壓 力之氧氣環境曝露該自由磁化層或該固定磁化層之表面既4484 3 〇 5. Description of the invention (4) 'After changing to a fixed pressure of 3 XlO_9Torr or more and 1 xlO-8Torr or less ^ Introducing a gas b made of argon b' Using the gas a and gas b. Gas sputtering A predetermined object forms a " & the " free magnetization layer or the fixed magnetization layer and the nonmagnetic layer under the non-magnetic layer. If the first manufacturing method is used, After reaching the vacuum degree below 1 0-1 QTorr, introduce a given amount of oxygen, and use the present oxygen and argon gas to form a free magnetic layer under the non-magnetic layer + A 卜 Α s, or a fixed magnetization using the sputtering method. Layer and the non-magnetic layer, the good bonding of the three layers will not be impaired, and the surface coarse chain degree of the film will be suppressed. That is, the MR ratio of the magnetoresistive film, which improves the flatness at the interface between the free magnetized layer and the non-magnetic layer or the fixed magnetized layer and the non-magnetic body, is increased. This effect occurs when the degree of vacuum after introducing the oxygen-containing gas a is set to a range of 3 X 10_gTorr or more and 1 X 1 0-8 Tq or less. In addition, in the case where a multi-acoustic film is used in the free magnetized layer, the flatness effect is expected at the entire interface of the multilayer film. 7. The manufacturing method of the second magnetoresistive element of the present invention is about smoothing on a predetermined substrate. A method for manufacturing a magnetoresistive film formed by stacking a free magnetization layer, a nonmagnetic layer, a fixed magnetization layer, and an antiferromagnetic layer in a reverse or reverse direction is characterized in that it has at least: the case where the nonmagnetic layer is stacked on the free magnetization layer After the formation of the free magnetization layer or when the non-magnetic layer is stacked on the fixed magnetization layer After the formation of the fixed magnetization layer, a gas a containing at least oxygen gas is introduced into the film forming chamber, such as the free layer located under the non-magnetic layer The exposed amount of the surface of the magnetized layer or the fixed magnetized layer becomes 6L to 20L (but lL (Langmuir) = l XlCHorrosec), and the surface of the free magnetized layer or the fixed magnetized layer is exposed in an oxygen environment with a predetermined pressure.
4484 3 Ο 五、發明說明(5) 定之時間之曝露之製程;以及藉著在該曝露後之成膜室 内,替代該氣體a,引入由氬氣構成之氣體乜,使用該氣體 b滅鐘既定之對象’在該曝露後之該自由磁化層或該固定 磁化層之表面上形成該非磁性體層之製程。 若依據該第二種製造方法,因在將自由磁化層或固定 磁化層之表面成膜後’令曝露於氡氣環境,令該表面微量 部分氧化後,在該令微量部分氧化之自由磁化層或固定磁 化層之表面上形成非磁性體層,由於界面之平坦性之劣 化,在由強磁性體構成之2層間,即在自由磁化層和固定 磁化層之間受到局部性強磁性耦合作用,弄亂磁化之反平 行排列,但疋藉著曝露於微量之氡氣環境,在膜表面發生 部分氧氣吸附,結果,物理上之界面之面粗糙度相同,也 因界面之凹ώ而降低強磁性耦合,實現穩定之磁化之反平 行排列,磁阻功效膜之MR比增大。該作用在將位於非磁性 體層下之自由磁化層或固定磁化層之表面之曝露量設為6L 以上2 0L以下之範圍時發生&此外,在該自由磁化層採用 了多層膜之情況,對於該多層膜之中和最上層即非磁性體 層接觸而形成界面之層,若曝露於該氧氣環境,期待該效 圖式簡單說明 圖1係表示本發明之自旋閥型磁阻功效膜之模式上之 圖2係表示自上方所看到用以製作本發明之磁阻功效4484 3 〇 5. Description of the invention (5) The process of exposure at a fixed time; and by replacing the gas a in the film-forming chamber after the exposure, introducing a gas made of argon, and using the gas b to kill the bell The process of forming the non-magnetic layer on the surface of the free magnetized layer or the fixed magnetized layer after the exposure. According to the second manufacturing method, since the surface of the free magnetized layer or the fixed magnetized layer is formed into a film and exposed to a radon environment, a small amount of the surface is oxidized, and then the freely magnetized layer where the minute portion is oxidized. Or a non-magnetic layer is formed on the surface of the fixed magnetization layer. Due to the deterioration of the flatness of the interface, between the two layers composed of ferromagnetic materials, that is, the local strong magnetic coupling between the free magnetization layer and the fixed magnetization layer, The random magnetization is arranged in antiparallel, but by exposure to a small amount of radon gas environment, part of the oxygen adsorption occurs on the film surface. As a result, the physical interface has the same surface roughness, and the strong magnetic coupling is reduced due to the recession of the interface. The anti-parallel arrangement of stable magnetization is achieved, and the MR ratio of the magnetoresistive effect film is increased. This effect occurs when the exposed amount of the surface of the free magnetized layer or the fixed magnetized layer under the non-magnetic layer is set to a range of 6L or more and 20L or less. In addition, in the case where a multilayer film is used for the free magnetized layer, Among the multilayer films, the layer that forms the interface by contacting the uppermost layer, that is, the non-magnetic layer. If exposed to the oxygen environment, the effect diagram is expected to be briefly explained. FIG. 1 shows the mode of the spin-valve type magnetoresistive effect film of the present invention Figure 2 above shows the magnetoresistive effect used to make the invention as seen from above
4484 3 Ο4484 3 Ο
五、發明說明(6) 膜所使用濺鍍成膜裝置之模式上之平面圖。 圖3係表示引入了氧氣時之真空度ρι和所製作磁阻功 效膜之磁阻變化率(MR比)之關係之圖。 圖4係表示引入了氧氣時之真空度ρι和所製作磁阻功 效膜之電阻係數、電阻變化量以及磁阻變化率(mr比)之關 圖5係表示所製作磁阻功效膜之χ射線繞射輪廓^ 圖6係表示氧氣曝露量和所製作磁阻功效 化率(MR比)之關係之圖。 ^ 圖7係表示A氣曝冑量和~製作肖阻功 數、電阻變化量以及磁阻變化率(MR比)之關係之圖電/係 符號說明 1第一載入室 2第二載入室 排氣裝置 2a、3a、4a、4a,' 5a、6a、7a、7a’ 2b、3b、5b、6b、7b、8b 閘閥 3前處理室 4搬運室 5第一成膜室 6第二成膜室 7第三及第四成膜室 8第五成膜室 10、11基板之移動裝置V. Description of the invention (6) A plan view of the mode of the sputtering film-forming device used for the film. Figure 3 is a graph showing the relationship between the degree of vacuum ρm when oxygen is introduced and the rate of change in magnetic resistance (MR ratio) of the produced magnetoresistive power film. Fig. 4 shows the relationship between the degree of vacuum ρm when oxygen is introduced and the resistivity, the resistance change amount, and the rate of change in magnetoresistance (mr ratio) of the produced magnetoresistance effect film. Fig. 5 shows the x-rays of the produced magnetoresistance effect film. Diffraction profile ^ Figure 6 is a graph showing the relationship between the amount of oxygen exposure and the produced magnetoresistance efficiency ratio (MR ratio). ^ Figure 7 is a graph showing the relationship between the amount of A gas exposure and the production resistance, the amount of resistance change, and the rate of change in magnetic resistance (MR ratio). Room exhaust devices 2a, 3a, 4a, 4a, '5a, 6a, 7a, 7a' 2b, 3b, 5b, 6b, 7b, 8b Gate valve 3 Pre-processing chamber 4 Transport chamber 5 First film formation chamber 6 Second condition Film chamber 7 Third and fourth film forming chambers 8 Fifth film forming chambers 10 and 11
------ 第10頁 4484 3 Ο 五 '發明說明(7) 100 基體 101 基板 102底層 1 0 3自由磁化層 104 第一強磁性體層 1 0 5 第二強磁性體層 1 0 6非磁性體層 1 0 7固定磁化層 1 0 8反強磁性體層 1 〇 9保護層 發明之實施例 以下列舉實施例更詳細說明本發明,但是本發明未限 定為這些實施例。 (實施例1) 在本例’在製作由圖1(a)之構造構成之自旋閥型磁阻 功效膜(在固定磁化層上堆積反強磁性體層之情況:稱為 頂自旋閥型)時’只有自由磁化層及非磁性體層,將成膜 室内降壓至約1〇-η Tor r之真空度為止後,引入氧氣(〇2), 將成膜室内之壓力變更為位於1 XI 〇-9T〇rr〜5 X l〇-8Tori·之-固定壓力後,引入氬氣(Ar),使用(Ar + 〇2)混合氣體利用 藏錄法形成。而’構成自旋閥型磁阻功效膜之別層,即固 定磁化層及反強磁性體層只使用氬氣形成。 4484 3 Ο 五、發明說明(8) 由基板101/底層l〇2(Ta膜,膜厚5nm)/第一強磁性體層 104(Ni-Fe膜’膜厚3nm)/第二強磁性體層l〇5(Co膜,膜厚 Inm) /非磁性體層l〇6(Cu膜,膜厚2. 5nm)/固定磁化層 107(C〇膜,膜厚2nm)/反強磁性體層l〇8(Mn- Ir膜,膜厚 5nm) /保遵層l〇9(Ta膜,膜厚5nm)構成之積層構造。 在基板101上使用了在表面設置了熱氧化膜之Si(ioo) 單結晶基板。在本例將在該基板丨〇 1上設置了底層丨02的作 為基體100。又’在該積層構造,第一強磁性體層丨〇4及第 二強磁性體層1 05構成強磁性體層1 〇3。 此外’為了製作上述構造之磁阻功效膜而使用之成膜 裝·置係在特開平10-298*745號公報公開之適應極高真空之 多滅錢裝置(曰立造船製,型式H IMS-005)。圖2係自上方 看到該成膜裝置之模式上之平面圖。在圖2,1係第一載入 室’2係配置於第一載入室之上方之第二載入室,3係前處 理室’ 4係搬運室,5係第一成膜室,6係第二成膜室,7係 第三及第四成膜室,8係第五成膜室,10及11係基板之移 動裝置。又 ’ 2a、3a、4a、4a,、5a、6a、7a、7a,以及8a 係將各室内降壓之排氣裝置。在此,排氣裝置4a和43,配 置於搬運室4之下方(紙面背側)。此外,2b、3b、5b、 6b、7b以及8b係設置於各室間之閘閥β 在表1表示製造本例之磁阻功效膜時之成膜條件。------ Page 10 4484 3 0 5 'Description of the invention (7) 100 Base 101 Substrate 102 Bottom 1 0 3 Free magnetization layer 104 First ferromagnetic layer 1 0 5 Second ferromagnetic layer 1 0 6 Nonmagnetic Bulk layer 10 7 Fixed magnetization layer 108 Antiferromagnetic layer 1 009 Protective layer Examples of the invention The following examples illustrate the invention in more detail, but the invention is not limited to these examples. (Example 1) In this example, when a spin-valve type magnetoresistive film composed of the structure of FIG. 1 (a) is produced (a case where an antiferromagnetic layer is stacked on a fixed magnetization layer: it is called a top-spin valve type ) 'Only has a free magnetization layer and a non-magnetic layer. After the pressure in the film-forming chamber is reduced to a vacuum of about 10-η Tor r, oxygen (〇2) is introduced to change the pressure in the film-forming chamber to 1 XI. 〇-9T〇rr ~ 5 X 〇-8Tori ·--After the pressure is fixed, argon (Ar) is introduced and formed using the (Ar + 〇2) mixed gas by the storage method. The other layers constituting the spin-valve type magnetoresistive film, that is, the fixed magnetization layer and the antiferromagnetic layer are formed using only argon gas. 4484 3 〇 5. Description of the invention (8) Substrate 101 / bottom layer 10 (Ta film, film thickness 5nm) / first ferromagnetic layer 104 (Ni-Fe film 'film thickness 3nm) / second ferromagnetic layer 1 〇5 (Co film, film thickness Inm) / non-magnetic layer 106 (Cu film, film thickness 2.5 nm) / fixed magnetization layer 107 (C0 film, film thickness 2 nm) / antiferromagnetic layer 108 ( A multilayer structure composed of a Mn-Ir film with a film thickness of 5 nm) / guaranteed layer 109 (Ta film with a film thickness of 5 nm). As the substrate 101, a Si (ioo) single crystal substrate having a thermal oxide film provided on the surface was used. In this example, the substrate 100 is provided with a bottom layer 02 on the substrate 101. Furthermore, in this laminated structure, the first ferromagnetic layer 〇04 and the second ferromagnetic layer 105 constitute a ferromagnetic layer 103. In addition, the film-forming device and device used to make the magnetoresistance-effect film with the above structure are disclosed in Japanese Unexamined Patent Application Publication No. 10-298 * 745. -005). Fig. 2 is a plan view of the film forming apparatus as seen from above. In FIG. 2, 1 is a first loading chamber, 2 is a second loading chamber disposed above the first loading chamber, 3 is a pre-processing chamber, 4 is a transfer chamber, 5 is a first film forming chamber, 6 It is the second film forming chamber, 7 is the third and fourth film forming chambers, 8 is the fifth film forming chamber, and 10 and 11 are substrate moving devices. Also, 2a, 3a, 4a, 4a, 5a, 6a, 7a, 7a, and 8a are exhaust devices that reduce the pressure in each room. Here, the exhaust devices 4a and 43 are disposed below the conveyance chamber 4 (back side of the paper surface). In addition, 2b, 3b, 5b, 6b, 7b, and 8b are gate valves β provided between the respective chambers. Table 1 shows the film forming conditions when the magnetoresistive effect film of this example is manufactured.
3 〇 五、發明說明(9) (表1) 項目 設定值 <清潔處理條件> •加工氣體 Ar -氬氣中之雜質滚度 l(ppb)以下 •加工氣逋壓力 3(mTorr) •基板夾持器之溫度控制 至少將基板失持器水冷 <共同之成膜處理條件> •成膜方法 平行平板型濂鍍法 •基板夾持il之溫度控制 2〇 X:(將基板夾持器水冷) •加工氣趙 Ar、(Ar + 〇2) •氬氣中之雜質濃度 l(ppb>乂下 •各室之到達真空度 l〇-n~l〇-12Torr (成膜室5) 底層102及保護層109 Ta膜(膜厚5nm) •對象 Ta(纯度4N) •加工氣效 Ar •加工氣想壓力 1 (mTorr) (成膜室 第一強磁性逋層104 Ni-Fe 膜(膜厚 3mn) •對象 78-5wt%Ni-Fe(純度 4N) •加工氣韹 (Ar+Oa) •引入〇2後之真空度P1 lxl〇-9~5xlO-8Torr *加工氣想壓力 0.75 (mTorr) (成膜室7) ①第二強磁性體層105 Co膜(膜厚lnm) •對象 Co(纯度3N) •加工氣避 (Αγ+02) •弓1入〇2後之真空度P1 1 xlO·9 〜5 χ10_8Τογγ •加工氣體壓力 0.6 (mTorr) 11Η11 第13頁 4484 3 03 05. Description of the invention (9) (Table 1) Item setting value < Cleaning process conditions > • Process gas Ar-Argon impurity roll below l (ppb) • Process gas pressure 3 (mTorr) • The temperature control of the substrate holder is at least water-cooled by the substrate holder < common film forming processing conditions > • the film formation method is a parallel plate type 濂 plating method • the temperature control of the substrate holder 20x: (clamp the substrate Holder water-cooled) • Process gas Zhao Ar, (Ar + 〇2) • Impurity concentration in argon l (ppb > His Majesty) • Arrival vacuum degree of each chamber l0-n ~ l0-12Torr (film forming chamber 5 ) Bottom layer 102 and protective layer 109 Ta film (film thickness 5nm) • Target Ta (purity 4N) • Processing gas effect Ar • Processing gas pressure 1 (mTorr) (The first ferromagnetic layer 104 Ni-Fe film in the film forming chamber) (Film thickness 3mn) • Target 78-5wt% Ni-Fe (purity 4N) • Processing gas (Ar + Oa) • Vacuum degree after introduction of 02 P1 lxl〇-9 ~ 5xlO-8Torr * Processing gas pressure 0.75 (mTorr) (Film-forming chamber 7) ① The second ferromagnetic layer 105 Co film (film thickness 1 nm) • Target Co (purity 3N) • Processing gas avoidance (Αγ + 02) • After the bow 1 enters 〇2 The degree of vacuum P1 1 xlO · 9 ~5 χ10_8Τογγ • processing gas pressure 0.6 (mTorr) 11Η11 Page 13448430
五、發明說明(ίο) ②非磁性逋層106 Cu膜(膜厚2.5nm) •對象 Cu(純度6N) •加工氣體 (Αγ+〇2) *引入02後之真空度:P1 lxl〇-9~5xl〇-8Torr •加工氣體壓力 0.6(mTorr) ③固定磁化層107 Co膜(膜厚2mn) •對象 Co(純度3N) •加工氣體 Ar •加工氣趙麼力 (成膜室8) 0.6(mTorr) 反強磁性體層108 Μη- It 膜(膜厚 5nm) •對象 17at% Μη (純度 3N) + Ir晶元(純度3N) •加工氣體 Ar •加工氣體壓力 20(mTorr) 以下照步驟說明本例之磁阻功效膜之製造方法。化y 括弧 内之編號表示其步驟。 (A1)基板(圖1之101)引入構成圖2之裝置之第—栽人 室1後,使用排氣裝置(圖上未示)將第一載入室1之内部空 間自大氣壓降壓至約1 0-8Torr為止。 (A2)使用搬運裳置10令配置於第一載入室1之内部之 基板自第一載入室1移至利用排氣裝置2a預先降壓至約 10’Torr之真空度為止之第二載入室2。 (A3)使用搬運裝置11令配置於第二載入室2之内部之 基板移至利用排氣裝置3a預先將内部空間保持在約 10—1〗〜10_12Torr之極高真空之前處理室3。然後利用使用V. Description of the Invention (ίο) ② Non-magnetic rhenium layer 106 Cu film (film thickness 2.5nm) • Object Cu (purity 6N) • Processing gas (Αγ + 〇2) * Vacuum degree after introduction of 02: P1 lxl0-9 ~ 5xl0-8Torr • Process gas pressure 0.6 (mTorr) ③ Fixed magnetized layer 107 Co film (film thickness 2mn) • Object Co (purity 3N) • Process gas Ar • Process gas Zhao Moli (film forming chamber 8) 0.6 ( mTorr) Antiferromagnetic layer 108 Mn-It film (film thickness 5nm) • 17at% Mn (purity 3N) + Ir crystal (purity 3N) • Process gas Ar • Process gas pressure 20 (mTorr) Example of a method for manufacturing a magnetoresistive film. The numbers in parentheses indicate their steps. (A1) After the substrate (101 of Fig. 1) is introduced into the first planting room 1 constituting the device of Fig. 2, the exhaust space (not shown) is used to depress the internal space of the first loading chamber 1 from atmospheric pressure to About 1 0-8Torr. (A2) Use the carrier 10 to move the substrate placed inside the first loading chamber 1 from the first loading chamber 1 to the second that the pressure is reduced to about 10'Torr by the exhaust device 2a in advance. Loading room 2. (A3) Use the conveying device 11 to move the substrate disposed inside the second loading chamber 2 to the pre-processing chamber 3 in which the internal space is maintained at an extremely high vacuum of about 10-1 to 10_12 Torr in advance by the exhaust device 3a. Then use
448430 五、發明說明(11) 超高純度之氬氣在既定之條件產生之感應耦合型電裝乾洗 基板表面。 (A4)自前處理室3往各成膜室5〜8之基板之移動係利用 内藏於搬運室4之搬運裝置(圖上未示)。各成膜室5〜8之内 4空間預先保持在約1 〇-1!〜1 〇-l2T〇rr之極高真空。又,續運 室4之真空度也到達約10-MT〇rr,使用了所内藏之搬運裝 置動作時真空度也不會上升至1. 〇-i〇Torr以上之搬運裝置 (在特願平10-296666號公報公開之適應超高真空之搬運 器人)。 機 (A5)在基板1〇1上形成作為底層1〇2之Ta膜(5nm),作 為本例之基體100。其步驟如以下(人5_4)所 示〇 (A 5 -1)打開閘閥3 b ’利用撤運室4所内藏之搬運裝置 自前處理室3取出基板’關閉3b後,打開5b,令移向成膜 室5。然後,關閉閘閥5b。在設置了基板之狀態,也令成 膜室5之真空度保持約l〇-n〜1〇-丨2T〇rr之極高真空。 (A5-2)其次’將超高純度之氬氣引入成膜室5至變成 成膜條件之加工氣體壓力(表丨)為止。 (A5-3)對陰穩施加既定之電力後,濺鑛Ta對象。首 先,進行固定時間之預濺鍍後,藉著在既定之時間打開覆 蓋基板表面之開閉器在基板上形成了厚度5pm之Ta膜。藉4 著在經過既定之時間後關閉開閉器控制Ta膜之厚度。 (A5-4)其次,降低電力,令放電終了後,停止供給氩 氣’將成膜室5之内部空間排氣至約1〇—n Torr為止。448430 V. Description of the invention (11) Induction-coupling type electric equipment dry-cleaning substrate surface produced by ultra-high purity argon gas under predetermined conditions. (A4) The movement of the substrates from the pre-processing chamber 3 to each of the film-forming chambers 5 to 8 is by using a transporting device (not shown in the figure) built into the transporting chamber 4. Within each of the film forming chambers 5 to 8, 4 spaces are maintained in advance at an extremely high vacuum of about 10-1 to 10-2 Torr. In addition, the vacuum degree of the transfer room 4 also reached about 10-MT〇rr, and the vacuum degree will not rise to 1. 〇-i〇Torr or more when the use of the built-in transfer device operation (in the special wish flat 10-296666 disclosed in the carrier of ultra-high vacuum). A machine (A5) forms a Ta film (5 nm) as a bottom layer 102 on a substrate 101 as a substrate 100 of this example. The steps are as shown in the following (person 5_4). (A 5 -1) Open the gate valve 3 b 'Remove the substrate from the pre-processing chamber 3 using the handling device built in the removal chamber 4' After closing 3b, open 5b to move to膜 室 5。 Membrane chamber 5. Then, the gate valve 5b is closed. In the state where the substrate is set, the vacuum degree of the film forming chamber 5 is also maintained at an extremely high vacuum of about 10-n to 10-2 Torr. (A5-2) Secondly, the ultra-high purity argon gas is introduced into the film forming chamber 5 until the processing gas pressure (Table 丨) becomes the film forming conditions. (A5-3) After a predetermined power is applied to the yin steady, a Ta object is splashed. First, after performing a pre-sputter for a fixed time, a Ta film having a thickness of 5 pm was formed on the substrate by opening a shutter covering the surface of the substrate at a predetermined time. The thickness of the Ta film is controlled by closing the shutter after a predetermined time has elapsed. (A5-4) Secondly, the power is reduced, and after the discharge is completed, the supply of argon gas is stopped to exhaust the internal space of the film forming chamber 5 to about 10-n Torr.
苐15頁 4484 3 Ο 五、發明說明(12) (Α6)其次’在Ta膜(底層)1〇2上形成了 Ni~Fe膜 (3nm) ’作為第一強磁性體層1〇4。其步驟如以下之 〜(A6-5)所示。 1 (A6-1 )形成Ta膜後,打開閘閥5b,利用搬運室4所 藏之搬運裝置自成膜室5取出基板,關閉5b後,打開6b, 令移向成膜室6。然後,關閉閘閥6 b。在設置了基板之狀 態,也令成膜室6之真空度保持極高真 空。 ’、 (A6-2)經由可變洩漏閥(圖上未示)將氧氡弓丨入成膜室 6之内部空間,調整成既定之真空度?1(1><1〇_9〜5><: l〇_8Torr之固定壓力)。 (A6-3)其次,將超高純度之氬氣引入成膜室6之内部 空間至變成成膜條件之加工氣體壓力(表n為止。因此, (Ar+〇2)之真空度成為加工氣體壓力。 (A6-4)對陰極施加既定之電力後,濺鍍(NiFe)對 象。首先,進行固定時間之預濺鍍後,藉著在既定之時間 打開覆蓋基板表面之開閉器在Ta膜上形成了厚度3nm之 N1 -Fe膜。藉著在經過既定之時間後關閉開閉器控制n卜卜 膜之厚度。 片(A6-5)其次’降低電力’令放電終了後,停止供給氬 氣及氧氣,將成膜室6之内部空間排氣至約1〇—„ T〇rr為 止。 (A7)其次’在Ni〜Fe(第一強磁性體層)ι〇4上形成了 Co 膜(Inm),作為第二強磁性體層1〇5,在其上形成Cu膜苐 Page 15 4484 3 〇 5. Description of the invention (12) (Α6) Secondly, a Ni ~ Fe film (3nm) was formed on the Ta film (bottom layer) 102 as the first ferromagnetic layer 104. The steps are shown in the following steps (A6-5). 1 (A6-1) After the Ta film is formed, the gate valve 5b is opened, and the substrate is taken out of the film forming chamber 5 using the conveying device hidden in the conveying chamber 4. After 5b is closed, 6b is opened to move to the film forming chamber 6. Then, close the gate valve 6 b. In the state where the substrate is installed, the vacuum degree of the film forming chamber 6 is kept extremely high. ’, (A6-2) Adjust the oxygen bow into the inner space of the film forming chamber 6 through a variable leakage valve (not shown), and adjust it to a predetermined vacuum degree? 1 (1 > < 1〇-9 ~ 5 > <: fixed pressure of 10-8 Torr). (A6-3) Secondly, ultra-high purity argon gas is introduced into the inner space of the film forming chamber 6 to the pressure of the processing gas that becomes the film forming condition (as shown in Table n. Therefore, the vacuum degree of (Ar + 〇2) becomes the pressure of the processing gas (A6-4) After applying predetermined power to the cathode, sputtering (NiFe) is performed. First, after pre-sputtering for a fixed period of time, a shutter covering the surface of the substrate is opened at the predetermined time to form a Ta film. N1 -Fe film with a thickness of 3nm. The thickness of the n film is controlled by closing the shutter after a predetermined period of time. Sheet (A6-5) Secondly, "reducing the power" to stop the discharge of argon and oxygen , Exhaust the internal space of the film formation chamber 6 to about 10-Torr. (A7) Secondly, a Co film (Inm) is formed on Ni ~ Fe (first ferromagnetic layer) ι04, As the second ferromagnetic layer 105, a Cu film was formed thereon.
第16頁 4484 五、發明說明(13) (2*5nm) ’作為非磁性體層106 ’再在其上形成Co膜 (2nm) ’作為固定磁化層107。其步驟如以下之(A7-I)、 (A 7 - 5 )所示。 (A 7 一㈠形成N i - F e膜1 0 4後,打開閘閥6 b,利用搬運室 4所内藏之搬運裝置自成膜室6取出基板,關閉6b後,打開 7b ’令移向成膜室7。然後’關閉閘閥7b。在設置了基板 之狀態’也令成膜室7之真空度保持約10-Π〜l〇-〗2Torr之極 1¾真空。 (A7-2)經由可變洩漏閥(圖上未示)將氧氣引入成膜室 6之内部空間’調整成既定之真空度Pl(l X 1〇-9〜5 X 10-8Torr之固定壓力)。 (Α7-3)其次’將超高純度之氬氣引入成膜室7至變成 成膜條件之加工氣體壓力(表1)為止。因此,(Ar +02)之 真空度成為加工氣體壓力a (A7-4-1)對2個陰極施加既定之電力後,濺鍍c〇對象 和Cu對象◊首先,進行固定時間之預濺鍍後,藉著在既定 之時間打開覆蓋基板表面之開閉器在Ni_Fe膜丨〇4上形成了 厚度lnm之Co膜(第二強磁性體層)ι〇5。藉著在經過既定之 Ν'間後關閉開閉器控制C 〇膜之厚度。 U7-4-2)利用成膜室7所内藏之搬運裝置令形成了co 膜(第二強磁性體層)1〇5之基板移至cu對象側後,藉著在 既定之時間打開覆蓋基板表面之開閉器在Co膜1 0 5上形成 了厚度2‘5nm之Cu膜(非磁性體層)106。藉著在經過既定之 時間後關閉開閉器控制CU膜Page 16 4484 V. Description of the invention (13) (2 * 5nm) 'as a non-magnetic layer 106' and a Co film (2nm) 'is formed thereon as a fixed magnetization layer 107. The steps are shown in (A7-I) and (A 7-5) below. (As soon as A 7 forms the Ni-Fe film 104, the gate valve 6b is opened, the substrate is taken out of the film forming chamber 6 using the conveying device built in the conveying chamber 4, and after closing 6b, the opening 7b is opened to move to Membrane chamber 7. Then, 'the gate valve 7b is closed. In the state where the substrate is installed', the vacuum degree of the film forming chamber 7 is maintained at about 10-Π ~ l0-〗 2Torr pole 1¾ vacuum. (A7-2) Via variable The leak valve (not shown in the figure) introduces oxygen into the internal space of the film-forming chamber 6 to adjust to a predetermined vacuum degree Pl (fixed pressure of 1 X 10- 9 to 5 X 10-8 Torr). (Α7-3) Second 'Introduce ultra-high purity argon gas into the film-forming chamber 7 until the process gas pressure (Table 1) becomes the film-forming conditions. Therefore, the vacuum degree of (Ar +02) becomes the process gas pressure a (A7-4-1) After applying predetermined power to the two cathodes, sputter the target of C0 and Cu. First, after pre-sputtering for a fixed time, open the shutter covering the surface of the substrate on the Ni_Fe film at a predetermined time. A Co film (second ferromagnetic layer) having a thickness of 1 nm was formed. The thickness of the C film was controlled by closing the shutter after passing through a predetermined N ′ interval. U7-4 -2) After the substrate having formed the co film (second ferromagnetic layer) 105 has been moved to the cu target side by using the transporting device built in the film forming chamber 7, the shutter covering the substrate surface is opened at a predetermined time. A Cu film (non-magnetic layer) 106 having a thickness of 2'5 nm was formed on the Co film 105. Control the CU membrane by closing the shutter after a set time
之厚度。Of thickness.
第17頁 4484 30 五'發明說明(14) ~ -- —<^A7-4-3)其次,停止供給引入成膜室7之氧氣,變更 成氬氣之真空度成為加工氣體壓力。利用成膜室7所内藏 之搬運裝置令形成了 Cu膜(非磁性體層)1 〇6之基板再移至 對象側後’藉著在既定之時間打開覆蓋基板表面之開閉 器在Cu膜106上形成了厚度2nni之Co膜(固定磁化層)1〇7。 藉著在經過既定之時間後關閉開閉器控制以膜之厚度。 产(A7-5)其次,降低電力,令放電終了後,停止供給氬 氣’將成膜室7之内部空間排氣至約1〇—nT〇rr為止。 (A8)其次,在Co臈(固定磁化層)1〇7上形成了 Mn_ir 膜(5nm),作為反強磁性體1〇8。其步驟如(ah)、(a8 4) 所示。 (Α8-1)打開閑閥7b,利用搬運室4所内藏之搬運裝置 自成膜至7取出基板’關閉7b後’打開8b,令移向成膜室 8。然後’關閉閘閥8b ^在設置了基板之狀態,也令成膜 至8之真空度保持約1〇_11〜1〇-丨2T〇rr之極高真空。 (A8-2)其次’將超高純度之氩氣引入成膜室8至變成 成膜條件(表1)之加工氣體壓力為止。 (A8-3)對陰極施加既定之電力後,濺鍍Mn_Ir對象。 首先’進行固定時間之預濺鍍後’藉著在既定之時間打開 覆蓋基板表面之開閉器在Co膜(固定磁化層)ι〇7上形成了 厚度5nm之Μη- I r膜1 0 8。藉著在經過既定之時間後關閉開 閉器控制Mn-Ir膜之厚度。 (A8-4)其次,降低電力’令放電終了後,停止供給氬 氣,將成膜室8之内部空間排氣至約ι〇-ητου為止。Page 17 4484 30 Fifth invention description (14) ~-<^ A7-4-3) Secondly, the supply of oxygen introduced into the film forming chamber 7 is stopped, and the vacuum degree changed to argon becomes the processing gas pressure. The substrate formed with the Cu film (non-magnetic layer) 1 06 is moved to the target side by using the transporting device built in the film forming chamber 7 'by opening the shutter covering the substrate surface on the Cu film 106 at a predetermined time. A Co film (fixed magnetization layer) 107 having a thickness of 2 nni was formed. The film thickness is controlled by closing the shutter after a predetermined time has elapsed. Production (A7-5) is followed by reducing the power so that after the discharge is completed, the supply of argon is stopped 'and the internal space of the film forming chamber 7 is exhausted to about 10-nTorr. (A8) Next, a Mn_ir film (5 nm) was formed on Co 臈 (fixed magnetization layer) 107 as an antiferromagnetic body 108. The steps are shown in (ah), (a8 4). (Α8-1) Open the idle valve 7b, and take out the substrate from the film formation to 7 by using the transporting device built in the transport chamber 4. 'Close 7b' and open 8b to move to the film formation chamber 8. Then, when the gate valve 8b is closed, the state of the substrate is set, and the vacuum degree of the film formation to 8 is maintained at an extremely high vacuum of about 10-11 to 10-2 Torr. (A8-2) Secondly, ultra-high purity argon gas is introduced into the film forming chamber 8 until the pressure of the process gas becomes the film forming conditions (Table 1). (A8-3) After a predetermined power is applied to the cathode, a Mn_Ir object is sputtered. First, after performing pre-sputtering for a fixed time, a Mn-Ir film 108 having a thickness of 5 nm was formed on a Co film (fixed magnetization layer) 107 by opening a shutter covering the surface of the substrate at a predetermined time. The thickness of the Mn-Ir film is controlled by closing the shutter after a predetermined time has elapsed. (A8-4) Secondly, after the electric power is reduced to stop the discharge, the supply of argon gas is stopped, and the internal space of the film forming chamber 8 is exhausted to about ι0-ητου.
五、發明說明(15) (Α9)其次’在Mn-Ir膜(反強磁性體層)108上形成了 Ta 膜(5nm),作為保護層1〇9。那時之成膜步驟,除了令基板 自成膜室8移向成膜室5以外,和上述(A5) —樣。 (A10)最後,藉著令形成了保護層(Ta膜)1〇9之基板依 次移至成膜室5 —前處理室3 —第二載入室2 —第一載入室 1 ’自製造裝置内取出具備本例之積層構造之磁阻功效 膜。 利用上述製程(A1)〜(A10)形成了本例之磁阻功效 膜。那時’在上述製程(A6)及(A7)藉著變更引入〇2時之真 空度Pl(l Xl0-9~5 Xl〇-8Torr之固定壓力),製作了pi不同 之磁阻功效膜^以下將在本例所製作之磁阻功效膜稱為試 件α 〇 (比較例1 ) 在本例,在實施例1之製程之中之製程(Α6)及(Α7)不 引入氧氣而只使用氬氣,即使用氬氣替代(Ar + 〇2)混合氣 韹’形成第一強磁性體層102/第二強磁性體層103/非磁性 體層104,製作了由和實施例】—樣之積層構造構成之磁阻 功效膜上’和實施例1不同。其他設為和實施例1 一樣。以 下將在本例所製作磁阻功效膜稱為比較試件石1 d (比較例2) 在本例’和比較例1 一樣的在製作磁阻功效膜時,將 構成製造裝置之各成膜室内及搬運室内之到達真空度p2設 為位於10-iDT〇rr〜l〇-7Torr之範圍之固定壓力,製作了由和 實施例1 —樣之積層構造構成之磁阻功效膜。其他設為和5. Description of the invention (15) (A9) Secondly, a Ta film (5 nm) is formed on the Mn-Ir film (antiferromagnetic layer) 108 as a protective layer 109. The film-forming step at that time is the same as that described in (A5) above except that the substrate is moved from the film-forming chamber 8 to the film-forming chamber 5. (A10) Finally, the substrate on which the protective layer (Ta film) 10 is formed is sequentially moved to the film formation chamber 5-pre-processing chamber 3-second loading chamber 2-first loading chamber 1 'self-manufacturing Take out the magnetoresistive film with the laminated structure of this example from the device. The magnetoresistance effect film of this example was formed by the above processes (A1) to (A10). At that time, in the above-mentioned processes (A6) and (A7), by changing the vacuum degree Pl (1 Xl0-9 ~ 5 Xl0-8Torr fixed pressure) when introducing 〇2, a magnetoresistive film with different pi was made ^ Hereinafter, the magnetoresistive efficacy film produced in this example is referred to as test piece α 0 (Comparative Example 1). In this example, the processes (A6) and (Α7) in the process of Example 1 do not introduce oxygen and are used only. The argon gas, that is, the first ferromagnetic layer 102 / the second ferromagnetic layer 103 / non-magnetic layer 104 was formed by replacing the (Ar + 〇2) mixed gas 氩 with argon. The structure of the magnetoresistive film is different from that of the first embodiment. The rest is the same as that of the first embodiment. Hereinafter, the magnetoresistive efficacy film produced in this example will be referred to as a comparative test piece 1 d (Comparative Example 2). In this example, when the magnetoresistive efficacy film is produced in the same manner as in Comparative Example 1, each film constituting the manufacturing device will be formed. The arrival vacuum degree p2 in the room and the conveying room was set to a fixed pressure in the range of 10-iDT0rr to 10-7Torr, and a magnetoresistive effect film composed of the same laminated structure as in Example 1 was produced. Other set to and
第19頁 4484 30 五、發明說明(16) 比較例1 一樣。以下將在本例所製作磁阻功效膜稱為比較 試件/52。 圖3係表示在實施例]之製程(A6)及引入了氧氣時 之真空度P1和所製作磁阻功效膜之磁阻變化率(MR比)之關 係之圖。其結果以_記號表示。又,在圖3,為了比較, 也一併表示比較試件乃1之結果(◦記號)和比較試件^ 2之 結果(◊記號)。此時之橫轴表示各成膜室内及搬運室内之 到達真空度P2。圖4係表示引入了氧氣時之真空度pi和所 製作磁阻功效膜之電阻係數、電阻變化量以及磁阻變化率 (MR比)之關係之圖。但’圖4所示〖丨r比和圖3相同。圖5係 表示所製作磁阻功效膜之X射線繞射輪廓。 由圖3得到以下之實驗結果。 (a)在相當於習知例之比較試件召2(〇記號),隨著成 膜室等之到達真空度P2降低,MR比顯示增加傾向,在將p2 設為約10-1]Torr之比較試件01(〇記號),得到約10%之龍 比0 (b)在本發明之試件’引入氧氣時之真空度ρ丨變高 時’在Ρ1之某特定範圍,MR比提高。 (c )即,在試件α之製造條件之中利闬濺鍍法將自由 磁化層(第一強磁性體層、第二強磁性體層)及非磁性體層 成膜之製程,引入氧氣時之真空度Ρ1位於3 X丨〇-9Torr以 上且lXl〇8T〇rr&下之固定塵力範圍時,可得到具有超過 在習知例之MR比之最大值(比較試件石1之情況)之優異之 MR比之磁阻功效元件。Page 19 4484 30 V. Description of the invention (16) The same as in Comparative Example 1. Hereinafter, the magnetoresistive efficacy film produced in this example is referred to as Comparative Test Piece / 52. Fig. 3 is a graph showing the relationship between the process (A6) in the embodiment] and the degree of vacuum P1 when oxygen is introduced and the magnetoresistance change rate (MR ratio) of the produced magnetoresistance effect film. The result is indicated by _ mark. In Fig. 3, for comparison, the result of the comparison test piece is 1 (◦ symbol) and the result of the comparison test piece ^ 2 (◊ symbol) is also shown. The horizontal axis at this time indicates the reached vacuum degree P2 in each film forming chamber and the conveying chamber. Fig. 4 is a graph showing the relationship between the degree of vacuum pi when oxygen is introduced and the resistivity, resistance change amount, and magnetoresistance change rate (MR ratio) of the produced magnetoresistance effect film. However, the ratio shown in FIG. 4 is the same as that in FIG. 3. Figure 5 shows the X-ray diffraction profile of the fabricated magnetoresistive film. The following experimental results were obtained from FIG. 3. (a) In the comparative test piece 2 (0 mark) equivalent to the conventional example, as the vacuum degree P2 of the film forming chamber and the like decreases, the MR ratio shows an increasing tendency, and p2 is set to about 10-1] Torr Comparing test piece 01 (0 mark), a dragon ratio of about 10% is obtained. (B) In the test piece of the present invention, when the vacuum degree ρ 丨 when oxygen is introduced becomes higher, the MR ratio increases in a certain range of P1. . (c) That is, in the manufacturing conditions of the test piece α, a sputtering process is used to form a free magnetized layer (first ferromagnetic layer, second ferromagnetic layer) and a non-magnetic layer into a film. The vacuum when introducing oxygen is used. When the degree P1 is in a fixed dust force range above 3 X 丨 〇-9 Torr and under 1X108 Torr &, an excellent value having a maximum MR ratio (compared to the test piece 1) exceeding the conventional example can be obtained. The MR ratio is compared to the magnetoresistive effect element.
第20頁 4484 3 Ο 五、發明說明(17) 以下由圖4明白以下各點。 電阻係數p s只當Ρ1為5 X 1 0—8T〇rr*時增加,在別的P1 區域,幾乎不變化,係和比較試件点1之結果(〇記號)大 致相同之值。而,電阻變化量Ap ,在P1位於3 X 10_9Torr 〜1 X 1 0-8Torr之範圍,比比較試件卢1之結果(〇記號)大, 在5 X 1 (Mor r時顯示極大。即,自圖3得知MR比隨著△ p 增加而提高。又,由利用X射線繞射法調查了令P1變化之 構成試件之膜之結晶構造之結果(圖5),在26=52(deg)附 近所觀測之fcc(iii)之尖峰強度在P1為3 xlO_9Torr以上之 情況有減少之傾向,但是在該值以下之真空度,顯示和比 較試件沒1大致相同之尖峰強度,未發現因添加氡氣而引 起結晶劣化。又,用AFM評價所製作之試件(Pi X 10—9Torr)和比較試件沒1之膜之表面粗度之結果,前者之 Ra係1. 38 ’而後者之“係丨78。由這結果得知,藉著在膜Page 20 4484 3 〇 5. Description of the invention (17) The following points will be understood from FIG. 4 below. The resistivity p s increases only when P1 is 5 X 1 0-8 Torr *, and it hardly changes in other P1 regions, which is about the same value as the result (zero symbol) of the point 1 of the comparison test piece. In addition, the resistance change Ap, which is in the range of 3 X 10_9 Torr to 1 X 1 0-8 Torr, is larger than the result (0 mark) of the comparison sample Lu 1 and shows a maximum value at 5 X 1 (Mor r. That is, It can be seen from Fig. 3 that the MR ratio increases with an increase in Δp. Furthermore, the result of investigating the crystal structure of the film constituting the test piece with P1 changed by the X-ray diffraction method is shown in Fig. 5 at 26 = 52 ( deg) The peak intensity of fcc (iii) observed near P1 tends to decrease when P1 is 3 x 10_9 Torr or more. However, the degree of vacuum below this value shows and compares the peak intensity of the specimen with about 1 and is not found. 38 ° , The deterioration of the crystal caused by the addition of radon. Also, the surface roughness of the test piece (Pi X 10-9Torr) produced by AFM evaluation and the comparison of the film thickness of the test piece was 1. The latter is "78." From this result, we know that
中取入適當量之氧氣降低膜之表面粗糙度。這暗示改善了 積層構造之界面之平坦性Q 因此,至少在將第一強磁性體層、第二 =磁性體層成膜時,藉著制真空度?1變成位於fx層乂 層,Ϊ二上2'?°"以下之量之氧氣和氬氣形成各Take in an appropriate amount of oxygen to reduce the surface roughness of the film. This implies that the flatness of the interface of the laminated structure is improved. Therefore, at least when the first ferromagnetic layer and the second magnetic layer are formed, the degree of vacuum is reduced. 1 becomes located on the fx layer, layer 2 and 2 '? ° " The following amounts of oxygen and argon form each
善積層構造之界面之平坦性,可得SI 圖 此外,在本例,詳述了將本發明 1 (a)之積層構造構成之磁阻^^方法應用方 戏骐(在固定磁化層上The SI plane of the interface of the laminated structure can be obtained. In addition, in this example, the method of applying the magnetic resistance of the laminated structure of 1 (a) of the present invention is described in detail.
4484 3 Ο 五、發明說明(18) 積反強磁性體層之情況:頂自旋閥型)之情況,但是確認 了在層構造相反即圖1(b)所示之積層構造(在反強磁性體 層上堆積固定磁化層之情況:底自旋閥型)也可得到上述 效果。但’在採用圖1(b)之積層構造之情況:在底層1〇2 上例如適合使用在Ta臈上堆積了(Ni-Fe)膜的。 (實施例2) 在本例,變更以下之2點,和實施例1 一樣使用圖2之 成膜裝置製作了由和實施例1 一樣之積層構造(圖丨(a):頂 自旋閥型)構成之磁阻功效膜, ① 在實施例1之製程之中之製程(6)及(7)不引入氧氣 而只使用氬氣,即使用氬氣替代(A r + 〇2)混合氣體,形成 第一強磁性體層(Ni-Fe膜)1〇4/第二強磁性體層(Co 膜)105/非磁性體層(Cu膜)106。 ② 將構成積層構造之非磁性體層(CU膜)1〇6之上下界 面’即構成自由磁化層之第二強磁性體層((;〇膜)1〇5之表 面及非磁性體層(Cu膜)106之表面或某一方之表面曝露於 既定之氧氣環境中。那時,令在1L以上200L以下之範圍改 變曝路量。在此 ’lL = lxlO-6Torr/sec(L 係 Langmuir 單 位)。 其他和實施例1 一樣的製作了磁阻功效膜。 在表2表示製造本例之磁阻功效膜時之成膜條件。4484 3 〇 V. Description of the invention (18) In the case of an antiferromagnetic layer: top spin valve type), it is confirmed that the layer structure is opposite, that is, the layer structure shown in Fig. 1 (b) (in antiferromagnetism) In the case where a fixed magnetization layer is deposited on the body layer: bottom spin valve type), the above-mentioned effect can also be obtained. However, in the case where the laminated structure of FIG. 1 (b) is adopted, for example, a (Ni-Fe) film deposited on Ta 臈 is suitable for the bottom layer 102. (Example 2) In this example, the following two points were changed, and the same lamination structure as in Example 1 was produced using the film-forming apparatus of FIG. 2 in the same manner as in Example 1 (Figure 丨 (a): Top Spin Valve Type) ) Of the magnetoresistive effect film, ① In the process (6) and (7) of the process of Example 1, no oxygen is introduced and only argon is used, that is, argon is used instead of (A r + 〇2) mixed gas, A first ferromagnetic layer (Ni-Fe film) 104 / second ferromagnetic layer (Co film) 105 / nonmagnetic layer (Cu film) 106 is formed. ② The top and bottom interfaces of the non-magnetic layer (CU film) 106 constituting the laminated structure, that is, the surface of the second ferromagnetic layer ((; 〇 film) 105) and the non-magnetic layer (Cu film) constituting the free magnetization layer The surface of 106 or one surface is exposed to a predetermined oxygen environment. At that time, the exposure amount should be changed in the range of 1L to 200L. Here, 'lL = lxlO-6Torr / sec (L is Langmuir unit). Others A magnetoresistive effect film was produced in the same manner as in Example 1. Table 2 shows the film formation conditions when the magnetoresistance effect film of this example was produced.
第22頁 4484 3 (表2) 五、發明說明(19) 項目 設定值 <清潔處理條件> •加工氣體 Ar •氬氣中之雜質濃度 l(ppb)以下 •加工氣體壓力 3(mTorr) •基板夾持器之溫度控制 至少將基板夾持器水冷 <共同之成臈處理條件> •成膜方法 平行平扳型濺鍍法 •基板表面之保持溫度 20°C (將基板夾持器水冷) •加工氣韹 Ar、(Ar + 02) •氩氣中之雜質濃度 l(ppb)以下 •各室之到連真空度 ΙΟ-^-ΙΟ^Τογγ (成膜室5) 底層102及保護層109 Ta膜(膜厚5mn) •對象 Ta(純度4N) •加工氣體 Ar •加工氣體壓力 l(mTorr) (成膜室6) 第一強磁性韹層104 Ni-Fe 膜(膜厚 3nm) •對象 78.5wt°/〇Ni-Fe(純度 4N) •加工氣趙 Ar •加工氣體壓力 0.75(mTorr) (成膜室7) ①第二強磁性體層105 Co膜(膜厚lrnn) •對象 Co(純度3N) •加工氣雜 Ar *加工氣雜壓力 0.6(mTorr)Page 22 4484 3 (Table 2) V. Description of the invention (19) Item setting value < Cleaning process conditions > • Process gas Ar • Impurity concentration of argon gas below l (ppb) • Process gas pressure 3 (mTorr) • The temperature of the substrate holder is controlled by at least water cooling of the substrate holder <common processing conditions> • film formation method parallel flat-type sputtering method • substrate surface holding temperature 20 ° C (holding the substrate (Water cooling of the device) • Ar, (Ar + 02) processing gas • Impurity concentration in argon gas below l (ppb) • The vacuum degree of each chamber is 10-^-ΙΟ ^ Τγγ (film forming chamber 5) Bottom layer 102 and Protective layer 109 Ta film (film thickness 5mn) • Target Ta (purity 4N) • Processing gas Ar • Processing gas pressure l (mTorr) (film forming chamber 6) First ferromagnetic hafnium layer 104 Ni-Fe film (film thickness 3nm ) • Target 78.5wt ° / 〇Ni-Fe (purity 4N) • Processing gas Zhao Ar • Processing gas pressure 0.75 (mTorr) (film forming chamber 7) ①Second ferromagnetic layer 105 Co film (film thickness lrnn) • Target Co (purity 3N) • Processing gas Ar * Processing gas pressure 0.6 (mTorr)
第23頁Page 23
4484 3 C 五、發明說明(20) ① ’氡氣曝蕗(Co膜) *加工氣體 •氡氣曝露時之真空度P3 •氧氣曝露時間 •氡氣曝蕗量 ② 非磁性體層106 •對象 •加工氣趙 *加工氣链壓力 ② ’氡氣曝蕗(CU膜) *加工氣韹 •氡氣曝露時之真空度P3 •氡氣曝蕗時間 *氧氣曝露量 ③ 固定磁化層107 •對象 •加工氣趙 •加工氣體壓力 (成膜室8) 反強磁性體層108 •對象 •加工氣锻 •加工氣體壓力 〇24484 3 C V. Description of the invention (20) ① 'Gas exposure (Co film) * Process gas • Vacuum degree of radon exposure P3 • Oxygen exposure time • Radon exposure ② Non-magnetic layer 106 • Object • Process gas Zhao * Process gas chain pressure ② 'Gas exposure (CU film) * Process gas • Vacuum degree of radon exposure P3 • Radon exposure time * Oxygen exposure amount ③ Fixed magnetization layer 107 • Object • Processing Gas Zhao • Processing gas pressure (film-forming chamber 8) Anti-ferromagnetic layer 108 • Object • Processing gas forging • Processing gas pressure 〇2
2 xl 0_9~3.5 xl 0'7T orr 10分鐘 1L-200L2 xl 0_9 ~ 3.5 xl 0'7T orr 10 minutes 1L-200L
Cu膜(膜厚2.5nm)Cu film (film thickness 2.5nm)
Cu(純度6Ν)Cu (purity 6N)
Ar 0.6(mTorr) 〇2 2xl〇-9~3.5xl〇-7Torr 10分鐘 1L-200L Co膜(膜厚2nm)Ar 0.6 (mTorr) 〇2 2xl〇-9 ~ 3.5xl〇-7Torr 10 minutes 1L-200L Co film (film thickness 2nm)
Co(純度3N)Co (purity 3N)
Ar 0.6(mTorr)Ar 0.6 (mTorr)
Mn- Ir 膜(膜厚 5nm) 17at% Ir· Μη (純度 3N) + Ir晶元(純度3N)Mn- Ir film (film thickness 5nm) 17at% Ir · Μη (purity 3N) + Ir crystal (purity 3N)
Ar 2Q(mTorr)_ 以下照步驟說明本例之磁阻功效膜之製造方法。括弧 内之編號表示其步驟。 (B1)〜(B5)進行和實施例1之製程(A1)~(A5) —樣之製Ar 2Q (mTorr) _ The following describes the manufacturing method of the magnetoresistive effect film in this example. The numbers in parentheses indicate their steps. (B1) ~ (B5) The process (A1) ~ (A5) of Example 1 is carried out-
第24頁 4484 3 五、發明說明(21) 程,在既定之基板101上形成底層102和Ta膜(5 ηπι),作為 基體100。 (Β6)其次,在Ta膜(底層)102上形成了Ni〜Fe膜 (3nm),作為第一強磁性體層1〇4。其步驟如以下之(B6-1) ~ (B6-4)所示。 (B6-1 )形成Ta膜102後,打開閘閥5b,利用搬運室4所 内藏之搬運裝置自成膜室5取出基板,關閉5b後,打開 6b ’令移向成膜室6。然後,關閉閘閥6b。在設置了基板 之狀態,也令成膜室6之真空度保持約1 〜1 〇_]2Torr之極 高真空。 (B6-2)將超高純度之氬氣引入成膜室6至變成成膜條 件之加工氣體壓力(表2)為止。 (B6-3)對陰極施加既定之電力後,濺鍍(Ni_Fe)對 象。首先’進行固定時間之預濺鍍後,藉著在既定之時間 打開覆蓋基板表面之開閉器在Ta膜上形成了厚度3ηιη之 N1 -Fe膜。藉著在經過既定之時間後關閉開閉器控制N丨 膜之厚度。 卜(^6:4)其次’降低電力’令放電終了後,停止供給氬 氣及氧氣’將成膜室6之内部空間排氣至約1〇_u T〇rrPage 24 4484 3 V. Description of the invention (21) Process, a bottom layer 102 and a Ta film (5 ηπ) are formed on a predetermined substrate 101 as a substrate 100. (B6) Next, a Ni-Fe film (3 nm) was formed on the Ta film (underlayer) 102 as the first ferromagnetic layer 104. The steps are shown in (B6-1) to (B6-4) below. (B6-1) After the Ta film 102 is formed, the gate valve 5b is opened, and the substrate is taken out of the film forming chamber 5 using the conveying device built in the conveying chamber 4. After closing 5b, 6b 'is opened to move to the film forming chamber 6. Then, the gate valve 6b is closed. In the state where the substrate is installed, the vacuum degree of the film forming chamber 6 is maintained at an extremely high vacuum of about 1 to 1 〇_] 2Torr. (B6-2) The ultra-high purity argon gas is introduced into the film forming chamber 6 until the pressure of the processing gas (Table 2) becomes a film forming condition. (B6-3) After applying a predetermined power to the cathode, a (Ni_Fe) object is sputtered. First, after pre-sputtering for a fixed period of time, by opening a shutter covering the surface of the substrate at a predetermined time, a N1 -Fe film having a thickness of 3 nm was formed on the Ta film. The thickness of the N 丨 film is controlled by closing the shutter after a predetermined time has elapsed. Bu (^ 6: 4) Secondly, “reducing the power” to stop the supply of argon and oxygen after the discharge is completed, and exhaust the internal space of the film forming chamber 6 to about 10_u T〇rr
止。 W (ΒΉ其次,在Ni_Fe(第一強磁性體層)1〇4上形成了 膜(Ιηπι),作為第二強磁性體層1〇5,在其上形成⑸膜 (2_5nn〇,作為非磁性體層1〇6 ’再在其上形成〇〇膜 (2nm) ’作為固定磁化層1〇7。其步驟如以下之(Β7_ι)〜stop. W (ΒΉ) Secondly, a film (1ηπ) was formed on Ni_Fe (first ferromagnetic layer) 104, and a second ferromagnetic layer 105 was formed thereon, and a hafnium film (2_5nn0) was formed thereon as a nonmagnetic layer 1 〇6 'A film (2nm) is formed thereon as the fixed magnetization layer 107. The procedure is as follows (B7_ι) ~
第25頁 4484 五、發明說明(22^ — 一' (B7-5)所示。 1 )形成N i -Fe膜1 04後’打開閘閥6b,利用搬運室 4所内&藏之搬運装置自成膜室6取出基板,關閉6b後,打開 7b ’,移向成獏室7 =然後,關閉閘閥7b。在設置了基板 之狀態’也令成膜室7之真空度保持約l〇-n〜i〇]2Torr之極 高真空。 (B7-2)將超高純度之氬氣引入成膜室7至變成成膜條 件之加工氣體壓力(表2)為止。 )對陰極施加既定之電力後,濺鍍以對象。首 先’進行固定時間之預濺鍍後,藉著在既定之時間打開覆 蓋基板表面之開閉器在Ni_Fe膜104上形成了厚度1ηιη之〇〇 膜(第二強磁性體層)1 〇 5。藉著在經過既定之時間後關閉 開閉器控制Co膜之厚度。 (A7-4-2)將Co膜(第二強磁性體層)ι〇5成膜後,停止 放電’切斷氬氣。然後’經由可變洩漏閥(圖上未示)將氧 氣引入成膜室7之内部空間,調整成既定之真空度p3(2x l〇-9~3. 5 X 10_7Torr之固定壓力)。然後,原封不動保持固 定時間(10分鐘),將Co膜105之表面曝露於氧氣環境。利 用此操作,在1L~200L之範圍改變Co膜105之曝露量。 (B7-4-3)在經過固定時間後切斷氧氣,利闬成膜室7 所内藏之搬運裝置令形成了 Co膜105之基板移至Cu對象 侧。然後’在成膜室7之内部空間再引入氬氣,對陰極施 加既定之電力’將Cu對象濺鍍。藉著在既定之時間打開覆 蓋基板表面之開閉器在Co膜105上形成了厚度2.5nm之Cu膜P.25 4484 5. Description of the invention (22 ^-1 '(B7-5). 1) After forming the Ni-Fe film 104, the gate valve 6b is opened, and the transportation device in the 4th transportation room & The film-forming chamber 6 takes out the substrate, and after closing 6b, it opens 7b 'and moves to the film-forming chamber 7 = Then, the gate valve 7b is closed. In the state where the substrate is provided, the vacuum degree of the film forming chamber 7 is maintained at an extremely high vacuum of about 10-n to 10] 2 Torr. (B7-2) The ultra-high-purity argon gas is introduced into the film forming chamber 7 until the pressure of the processing gas (Table 2) becomes a film forming condition. ) After applying a predetermined power to the cathode, the target is sputtered. First, after pre-sputtering for a fixed time, a shutter having a thickness of 1 nm (a second ferromagnetic layer) 105 is formed on the Ni_Fe film 104 by opening a shutter covering the surface of the substrate at a predetermined time. The thickness of the Co film is controlled by closing the shutter after a predetermined time has elapsed. (A7-4-2) After the Co film (second ferromagnetic layer) ι was formed, the discharge was stopped and the argon gas was cut off. Then, the oxygen gas is introduced into the inner space of the film forming chamber 7 through a variable leak valve (not shown in the figure), and adjusted to a predetermined vacuum degree p3 (a fixed pressure of 2 x 10-9 to 3.5 X 10_7 Torr). Then, the surface of the Co film 105 was exposed to an oxygen environment for a fixed time (10 minutes) as it is. With this operation, the exposure amount of the Co film 105 is changed in a range of 1L to 200L. (B7-4-3) After a fixed time has elapsed, the oxygen is cut off, and the transporting device built in the Li film forming chamber 7 moves the substrate on which the Co film 105 is formed to the Cu target side. Then, argon gas is further introduced into the inner space of the film forming chamber 7, and a predetermined power is applied to the cathode to sputter the Cu target. A 2.5 nm-thick Cu film was formed on the Co film 105 by opening the shutter covering the surface of the substrate at a predetermined time.
第26頁 4484 30 五、發明說明(23) (非磁性體層)1 0 6。藉著在經過既定之時間後關閉開閉器 控制Cu膜之厚度。 (B7-4-4)將Cu膜(非磁性體層)106成膜後,停止放 電,切斷氬氣。然後,經由可變洩漏閥(圖上未示)將氧氣 引入成膜室7之内部空間,調整成既定之真空度P3(2 X 10-9〜3.5父10-7丁〇]:1'之固定壓力)。然後,原封不動保持固 定時間(1 0分鐘),將Cu膜1 0 6之表面曝露於氧氣環境。利 用此操作,在1L〜200L之範圍改變Cu膜106之曝露量。 (B7-4-5)在經過固定時間後切斷氧氣,利用成膜室7 所内藏之搬運裝置令形成了 Cu膜(非磁性體層)1 06之基板 再移至Co對象侧然後,在成膜室7之内部空間再弓丨入氬 氣’對陰極施加既定之電力,濺鍍Co對象。藉著在既定之 時間打開覆蓋基板表面之開閉器在Cu膜106上形成了厚度 2ηπι之Co膜(固定磁化層)1〇7。藉著在經過既定之時間後關 閉開閉器控制Co膜之厚度。 (B7-5)其次,降低電力,令放電終了後,停止供給氬 氣,將成膜室7之内部空間排氣至約lO-UTorr為止。 (B8)〜(B9)進行和實施例1之製程(A8MA9) —樣之製 程’在Co膜(固定磁化層)1〇7上依次形成作為反強磁性體 層108之Mn-Ir膜(5nm)、作為保護層109之Ta膜(5nm)。 (B10)進行和實施例1之製程(A10) —樣之製程,自製 造裝置内取出具備本例之積層構造之磁阻功效膜。 利用上述製程(B1)〜(B10)形成了本例之磁阻功效 膜。那時,在上述製程(B7)藉著變更將Cu膜(非磁性體層)Page 26 4484 30 V. Description of the invention (23) (non-magnetic layer) 106. The thickness of the Cu film is controlled by closing the shutter after a predetermined time has elapsed. (B7-4-4) After the Cu film (non-magnetic layer) 106 is formed, the discharge is stopped and the argon gas is cut off. Then, a variable leak valve (not shown in the figure) is used to introduce oxygen into the internal space of the film forming chamber 7 and adjust it to a predetermined vacuum degree P3 (2 X 10-9 to 3.5 parent 10-7 but 0): 1 ' Fixed pressure). Then, the surface of the Cu film 106 was exposed to an oxygen environment for a fixed time (10 minutes) as it is. With this operation, the exposure amount of the Cu film 106 is changed in a range of 1L to 200L. (B7-4-5) After a fixed period of time, cut off the oxygen, and use the transporting device built in the film-forming chamber 7 to make the substrate on which the Cu film (non-magnetic layer) 106 is formed, and then move it to the Co object side. The internal space of the membrane chamber 7 is further filled with argon gas, and a predetermined power is applied to the cathode to sputter the Co object. By opening the shutter covering the surface of the substrate at a predetermined time, a Co film (fixed magnetization layer) 107 having a thickness of 2 nm was formed on the Cu film 106. The thickness of the Co film is controlled by closing the shutter after a predetermined time has elapsed. (B7-5) Secondly, the power is reduced, and after the discharge is completed, the supply of argon gas is stopped, and the internal space of the film forming chamber 7 is exhausted to about 10-UTorr. (B8) ~ (B9) The same process as in Example 1 (A8MA9) was performed-the same process was performed on the Co film (fixed magnetization layer) 107 in order to form an Mn-Ir film (5 nm) as the antiferromagnetic layer 108. A Ta film (5 nm) as the protective layer 109. (B10) The same process as in Example 1 (A10) is performed. The same process is performed, and the magnetoresistive film having the laminated structure of this example is taken out of the self-made device. The magnetoresistive effect film of this example was formed by the above processes (B1) to (B10). At that time, the Cu film (non-magnetic layer) was changed by the above-mentioned process (B7).
第27頁 4484 3 Ο 五 '發明說明(24) 106之上下界面’即Co膜(第二強磁性體層)1〇5及Cu膜(非 磁性體層)106之各表面曝露於氧氣環境時之真空度p3(2 X 1〇—9〜3. 5 X 10 7Torr之固定壓力),製作了曝露量不同之磁 阻功效膜。以下將Cu膜(非磁性體層)1 06之上下界面都曝 露於氧氣環境所製作之磁阻功效膜稱為試件了1。 (實施例3) 在本例,在實施例2之製程(Β7 ),不將非磁性體層(cu 膜)106之上下界面’即第二強磁性體層(c〇膜)1〇5及非磁 性體層(Cu膜)106之各表面曝露於氧氣環境,而只有第二 強磁性體層(Co膜)1〇5之表面曝露於氧氣環境下製作了磁 阻功效膜上和實施例2不同。其他和實施例2 一樣。以下, 將只有第二強磁性體層(c〇膜)1〇5之表面曝露於氧氣環境 下所製作磁阻功效膜稱為試件了2。 (實施例4) 在本例,在實施例2之製程(B7) ’不將非磁性體層(Cu 膜)106之上下界面,即第二強磁性體層((:〇膜)1〇5及非磁 性體層(Cu膜)106之各表面曝露於氧氣環境,而只有非磁 性體層(Cu膜)106之表面曝露於氧氣環境下製作了磁阻功 效膜上和實施例2不同。其他和實施例2 一樣。以下,將只 有非磁性體層(Cu膜)1〇6之表面曝露於氧氣環境下所製作 磁阻功效膜稱為試件r 3。 圖6係表示在上述製程(B7)第二強磁性體層((:〇膜)1〇5 及^或非磁性體層(〇11膜)1〇6之表面曝露於氧氣環境時之曝 露量和所製作磁阻功效膜之MR比之關係之圖。在圖6,_Page 27 4484 3 〇 5 Description of the invention (24) 106 Upper and lower interfaces, namely Co film (second ferromagnetic layer) 105 and Cu film (non-magnetic layer) Each surface of the vacuum when exposed to an oxygen environment Degree p3 (fixed pressure of 2 X 10- 9 to 3.5 X 10 7 Torr), made of magnetoresistive films with different exposure. Hereinafter, a magnetoresistance effect film made by exposing the upper and lower interfaces of a Cu film (non-magnetic layer) 106 to an oxygen environment is referred to as a test piece 1. (Example 3) In this example, in the process (B7) of Example 2, the non-magnetic layer (cu film) 106 is not placed above and below the interface, that is, the second ferromagnetic layer (co film) 105 and non-magnetic Each surface of the bulk layer (Cu film) 106 was exposed to an oxygen environment, and only the surface of the second ferromagnetic layer (Co film) 105 was exposed to an oxygen environment to make a magnetoresistive effect film different from that in Example 2. The rest is the same as that of the second embodiment. Hereinafter, the magnetoresistive efficacy film produced by exposing only the surface of the second ferromagnetic layer (co film) 105 to an oxygen environment is referred to as a test piece 2. (Example 4) In this example, in the process (B7) of Example 2, 'the non-magnetic layer (Cu film) 106 is not provided above and below the interface, that is, the second ferromagnetic layer ((: 0 film) 105 and non- Each surface of the magnetic layer (Cu film) 106 was exposed to an oxygen environment, and only the surface of the non-magnetic layer (Cu film) 106 was exposed to an oxygen environment. A magnetoresistive effect film was produced differently from Example 2. Others and Example 2 Same. Hereinafter, the magnetoresistive film made by exposing only the surface of the non-magnetic layer (Cu film) 106 to an oxygen environment is called test piece r 3. Figure 6 shows the second strong magnetism in the above process (B7). The relationship between the exposure amount of the surface of the bulk layer ((: 0 film) 105 and non-magnetic layer (0 11 film) 10 when exposed to an oxygen environment and the MR ratio of the magnetoresistive film produced. Figure 6,_
4484 3〇 五、發明說明(25) 記號表示第二強磁性體層(Co膜)之上下界面都曝露於氧氣 之試件7 1 (記為Co&Cu)之情況,△記號表示只有第二強磁 性體層(Co層)之表面曝露於氧氣試件γ2(記為Co)之情 凡 口1己喊表示只有非磁性體層(Cu層)之表面曝露於氧氣 试件r 3 (記為Cu)之情況。此外’在圖6中也表示在比較例 1所製作之比較試件卢1 (〇記號)之結果(Μί?比=約1〇%)。圖 7係表示氧氣曝露量和所製作磁阻功效膜之電阻係數、電 阻變化量以及磁阻變化率(MR比)之關係之圖。但,圖7所 示MR比和圖6的相同。 由圖6得到以下之實驗結果。 (1) 試件Tl和試件T2在氧氣曝露量位於6L以上20L以 下之範圍時,可製作具有超過在習知例之服比之最大值 (試件/51之情況)之優異之mr比之磁阻功效膜D尤其,氧 氣曝露量超過20L時,MR比顯著減少。 (2) 而’試件73幾乎不受氧氣曝露量之增加影響,在 任何氧氣曝露量都顯示和MR比之最大值大致同位準之|^ 比。 自上述結果(1)及(2)’得知藉著將至少第二強磁性體 層(Co膜)1〇3之表面曝露於氧氣環境並將其曝露量限制在 既定之範圍可得到MR比之增大效果。 而’自圖7明白如下事項。 電阻係數p s在只有Co膜曝露之情況及兩面(c〇膜和Cu 膜兩面)都曝露之情況,曝露量超過2〇L時急劇增加。在只 有Cu膜曝露之情況,ps和曝露量無關而幾乎變成定值^4484 30.5. Description of the invention (25) The symbol indicates that the upper and lower interfaces of the second ferromagnetic layer (Co film) are exposed to oxygen sample 7 1 (denoted as Co & Cu), and the △ symbol indicates that it is only the second strongest. The surface of the magnetic layer (Co layer) is exposed to the oxygen test piece γ2 (denoted as Co). Where mouth 1 has shouted that only the surface of the non-magnetic layer (Cu layer) is exposed to the oxygen test piece r 3 (denoted as Cu). Happening. In addition, FIG. 6 also shows the results of the comparative test piece Lu 1 (zero mark) produced in Comparative Example 1 (Mil? Ratio = about 10%). Fig. 7 is a graph showing the relationship between the amount of oxygen exposure and the resistivity, resistance change, and magnetoresistance change rate (MR ratio) of the fabricated magnetoresistance effect film. However, the MR ratio shown in Fig. 7 is the same as that of Fig. 6. The following experimental results are obtained from FIG. 6. (1) When the test specimen T1 and test specimen T2 are in the range of 6L or more and 20L or less, it is possible to produce an excellent mr ratio that exceeds the maximum value of the service ratio in the conventional example (in the case of the test piece / 51). Especially for the magnetoresistive film D, when the oxygen exposure exceeds 20L, the MR ratio decreases significantly. (2) The 'test piece 73 is hardly affected by the increase in the amount of oxygen exposure, and at any oxygen exposure amount, it is approximately equal to the maximum value of the MR ratio | ^ ratio. From the results (1) and (2) above, it is known that the MR ratio can be obtained by exposing at least the surface of the second ferromagnetic layer (Co film) 103 to an oxygen environment and limiting the exposure amount to a predetermined range. Increase effect. On the other hand, the following matters are understood from FIG. 7. The resistivity p s increases sharply when only the Co film is exposed and when both sides (both the c0 film and the Cu film) are exposed. In the case of only Cu film exposure, ps is almost constant regardless of the amount of exposure ^
4484 3ϋ 五'發明說明(26)4484 3ϋ Five 'invention description (26)
而,電阻變化 (Co膜和Cu膜兩面) 增加。在只有Cu膜 變成定值。 量△!〇在只有C〇膜曝露之情況及兩面 都曝露之情況,曝露量超過2 〇 l時急劇 曝露之情況’ Λρ和曝露量無關而幾乎 因此,試件γ 7 ,丨、尨a π a 和试件7 2在曝露量超過2〇L時急劇減 ^ 又到氧氣曝露之影響比Cu膜大。又,推測試 7 : 7 2在氧氣曝露量位於6L以上20L以下之範圍 時可得到超過習知例(試件Μ之情況)之MR比之理由如 下。 +在由強磁性體構成之2層之間’即在自由磁化層和固 定磁化層之間局部性強磁性耦合作用係由於在界面之凹凸 f 5局部性磁極。藉著將界面曝露於氧氣,該凹凸部吸收 氧氣原子,雖無物理上之界面平坦化效果,卻抑制局部性 磁極之感應,有減少局部性強磁性耦合之效果。 此外,在本例,詳述了將本發明之製造方法應用於由 圖1(a)之積層構造構成之磁阻功效臈(在固定磁化層上堆 積反強磁性體層之情況:頂自旋閥型)之情況,但是確認 了在層構造相反即圖1(b)所示之積層構造(在反強磁性體 層上堆積固足磁化層之情況:底自旋閥型)也可得到上述 效果。即’在底自旋閥型’至少應曝露於氧氣之界面係固 疋磁化層107和非磁性體層之界面,即固定磁化層1〇7 之表面。但’在採用圖1 (b)之積層構造之情況,在底層 102上例如適合使用在Ta膜上堆積了(Ni-Fe)膜的。However, changes in resistance (both sides of the Co film and the Cu film) increase. Only the Cu film becomes constant. Amount △! 〇 In the case where only the C0 film is exposed and the case where both sides are exposed, the case where the exposure amount is sharply exceeded when the exposure amount exceeds 20 l 'Λρ has almost nothing to do with the exposure amount, so the test piece γ 7, 丨, 尨 a π a and test piece 72 were sharply reduced when the exposure amount exceeded 20L, and the effect of oxygen exposure was greater than that of the Cu film. The reason why push test 7: 7 2 can obtain the MR ratio exceeding the conventional example (in the case of test piece M) when the oxygen exposure amount is in the range of 6L to 20L is as follows. + Between two layers made of a ferromagnetic body ', that is, the local strong magnetic coupling effect between the free magnetization layer and the fixed magnetization layer is due to the unevenness at the interface f 5 local magnetic poles. By exposing the interface to oxygen, the uneven portion absorbs oxygen atoms, and although there is no physical interface flattening effect, it suppresses local magnetic pole induction and has the effect of reducing local strong magnetic coupling. In addition, in this example, the application of the manufacturing method of the present invention to the magnetoresistance effect composed of the laminated structure of FIG. 1 (a) is described in detail (a case where an antiferromagnetic layer is stacked on a fixed magnetization layer: top spin valve Type), but it was confirmed that the above-mentioned effect can also be obtained in the layered structure shown in FIG. 1 (b) where the layer structure is reversed (the case where a solid magnetized layer is deposited on the antiferromagnetic layer: bottom spin valve type). That is, at the bottom spin valve type, at least the interface between the fixed magnetized layer 107 and the non-magnetic layer should be exposed to oxygen, that is, the surface of the fixed magnetized layer 107. However, in the case where the laminated structure of Fig. 1 (b) is adopted, for example, a (Ni-Fe) film deposited on a Ta film is suitably used for the bottom layer 102.
第30頁 ^434 3 c 五、發明說明(27) 產業上之可利用性 如上述所示,若利用本發明之第一種製造方法,至少 在將第一強磁性體層、第二強磁性體層以及非磁性體層成 膜時,藉著使用真空度P1變成3 xlO_9Torr以上1 XlO^Torr 以下之量之氧氣和氬氣形成各層,因在保持膜之良好之結 晶性下,改善積層構造之界面之平坦性,可得到具有比習 知高之MR比之磁阻功效膜。 又,若利用本發明之第二種製造方法,至少將構成自 由磁化層之第二強磁性體層之表面曝露於氧氣環境,藉著 將其曝露量設在6L以上20L以下之範圍,可製作比習知高 之MR比之磁阻功效膜。 藉著本發明之磁阻功效膜之製造方法,可穩定的製造 可適應更高記錄密度化之MR磁頭。Page 30 ^ 434 3 c V. Description of the invention (27) Industrial applicability As shown above, if the first manufacturing method of the present invention is used, at least the first ferromagnetic layer and the second ferromagnetic layer When forming a non-magnetic layer, each layer is formed by using oxygen and argon in an amount of 3 xlO_9Torr or more and 1 XlO ^ Torr or less in vacuum degree P1. The interface of the laminated structure is improved while maintaining the good crystallinity of the film. Flatness, a magnetoresistance effect film having a higher MR ratio than conventional can be obtained. In addition, if the second manufacturing method of the present invention is used, at least the surface of the second ferromagnetic layer constituting the free magnetization layer is exposed to an oxygen environment, and the exposure amount is set to a range of 6L or more and 20L or less. Knowing the high MR ratio of the magnetoresistive effect film. By the method of manufacturing the magnetoresistive effect film of the present invention, it is possible to stably manufacture an MR head capable of adapting to a higher recording density.
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