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CN103323796B - A kind of MTJ magnetic field sensor using Graphene as barrier layer - Google Patents

A kind of MTJ magnetic field sensor using Graphene as barrier layer Download PDF

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CN103323796B
CN103323796B CN201310247035.0A CN201310247035A CN103323796B CN 103323796 B CN103323796 B CN 103323796B CN 201310247035 A CN201310247035 A CN 201310247035A CN 103323796 B CN103323796 B CN 103323796B
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CN103323796A (en
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潘孟春
田武刚
胡靖华
胡佳飞
赵建强
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National University of Defense Technology
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Abstract

The invention discloses a kind of MTJ magnetic field sensor using Graphene as barrier layer, comprise two magnetic line of force collectors, be used for forming four MTJ magnet-sensitive elements of Hui Sitong measuring bridge, four electrodes and substrate, two magnetic line of force collectors symmetrically shape layout, the gap location of two described MTJ magnet-sensitive elements between two magnetic line of force collectors, described in two other, MTJ magnet-sensitive element lays respectively at the bottom of two magnetic line of force collectors, each described MTJ magnet-sensitive element includes the substrate stacking gradually arrangement from the bottom to top, bottom electrode layer, first cushion, free ferromagnetic, Graphene barrier layer, pinned ferromagnetic layer, pinning layer, second cushion and top electrode layer.The present invention have simple and compact for structure, volume is little, with low cost, easy to make, there is the advantages such as high resolution.

Description

一种以石墨烯作为势垒层的MTJ磁场传感器An MTJ magnetic field sensor using graphene as a barrier layer

技术领域 technical field

本发明主要涉及到微弱信号传感技术领域,特指一种以石墨烯作为势垒层的MTJ磁场传感器。 The invention mainly relates to the technical field of weak signal sensing, in particular to an MTJ magnetic field sensor using graphene as a potential barrier layer.

背景技术 Background technique

弱磁场测量广泛应用于目标探测、地磁导航、磁存储器、地质勘探、生物医学等军事和国民经济领域。现有技术中用于微弱磁场测量的传感器类型较多,主要包括磁通门传感器、光泵式磁传感器、质子式磁传感器、光纤磁传感器、巨磁阻抗磁传感器、AMR(Anisotropic Magnetoresistive,各向异性磁阻)磁传感器,GMR(Giant Magnetoresistive,巨磁阻)磁传感器、MTJ(Magnetic Tunnel Junction,磁隧道结)磁传感器等。其中AMR、GMR和MTJ磁传感器是相比其他类型的磁传感器明显具有体积小、功耗低、易批量生产等特点。但是以AMR为敏感元件的磁传感器使用时需要设置set/reset线圈对其进行预设-复位操作,造成其制造工艺的复杂,线圈结构的设置在增加尺寸的同时也增加了功耗。而以多层膜GMR为敏感元件的磁传感器响应曲线呈偶对称,只能测量的磁场大小,不能反映磁场的方向。MTJ元件利用磁性多层膜材料的隧道磁电阻效应(Tunnel Magnetoresistance,TMR)对磁场进行感应,比之前发现并实际应用的AMR元件和GMR元件具有更大的电阻变化率、更高的灵敏度和更好的温度稳定性。 Weak magnetic field measurement is widely used in military and national economic fields such as target detection, geomagnetic navigation, magnetic storage, geological exploration, and biomedicine. In the prior art, there are many types of sensors used for weak magnetic field measurement, mainly including fluxgate sensors, optical pump magnetic sensors, proton magnetic sensors, optical fiber magnetic sensors, giant magnetoresistive magnetic sensors, AMR (Anisotropic Magnetoresistive, anisotropic Anisotropic magnetoresistive) magnetic sensor, GMR (Giant Magnetoresistive, giant magnetoresistance) magnetic sensor, MTJ (Magnetic Tunnel Junction, magnetic tunnel junction) magnetic sensor, etc. Compared with other types of magnetic sensors, AMR, GMR and MTJ magnetic sensors have the characteristics of small size, low power consumption, and easy mass production. However, when a magnetic sensor with AMR as a sensitive element is used, it is necessary to set a set/reset coil to perform a preset-reset operation, resulting in a complicated manufacturing process. The setting of the coil structure increases the size and power consumption. The response curve of the magnetic sensor with multilayer film GMR as the sensitive element is evenly symmetrical, which can only measure the magnitude of the magnetic field, but cannot reflect the direction of the magnetic field. The MTJ element uses the tunnel magnetoresistance effect (Tunnel Magnetoresistance, TMR) of the magnetic multilayer film material to sense the magnetic field, and has a greater resistance change rate, higher sensitivity and more Good temperature stability.

1975年Julliere在Fe/Ge/Co隧道结中观察到当两铁磁层磁化方向平行或反平行时,隧道结将具有不同的电阻值(Julliere M. Tunneling Between Ferromagnetic Films. Phys Lett A, 1975, 54(3):225-226)。这种因外磁场改变隧道结铁磁层的磁化状态而导致其电阻变化的现象,称为磁隧道结效应。Fe/Ge/Co隧道结低温下的磁阻变化率高达14%,但在室温下却很小。在随后的30多年中人们对MTJ进行了系列深入研究。1995年Miyazaki小组实现了磁隧道结研究的突破性进展(Miyazki T, Tezuka N. Giant magnetic tunneling effect in Fe/Al2O3/Fe junction. J. Magn. Magn. Mater., 1995, 139:L231),首次在Fe/Al2O3/Fe隧道结中发现在室温和几毫特磁场下的磁阻变化率高达15.6%,低温下更高,约为23%。2008年,S. Ikeda等制备的MgO基MTJ在室温下的磁阻变化率达到了604%,5K低温下则达1144%(S. Ikeda, J. Hayakawa, Y. Ashizawa, Y. M. Lee, K. Miura, H. Hasegawa, M.Tsunoda, F. Matsukura, and H. Ohno, Appl. Phys. Lett.2008, 93: 082508),这一记录性的实验结果已接近MgO基MTJ的理论预测值。 In 1975, Julliere observed in the Fe/Ge/Co tunnel junction that when the magnetization directions of the two ferromagnetic layers are parallel or antiparallel, the tunnel junction will have different resistance values (Julliere M. Tunneling Between Ferromagnetic Films. Phys Lett A, 1975, 54(3):225-226). This phenomenon that the external magnetic field changes the magnetization state of the ferromagnetic layer of the tunnel junction and causes its resistance to change is called the magnetic tunnel junction effect. The magnetoresistance change rate of Fe/Ge/Co tunnel junction is as high as 14% at low temperature, but it is very small at room temperature. In the following 30 years, people conducted a series of in-depth studies on MTJ. In 1995, the Miyazaki group achieved a breakthrough in the study of magnetic tunnel junctions (Miyazki T, Tezuka N. Giant magnetic tunneling effect in Fe/Al 2 O 3 /Fe junction. J. Magn. Magn. Mater., 1995, 139:L231 ), it was first found in the Fe/Al 2 O 3 /Fe tunnel junction that the magnetoresistance change rate is as high as 15.6% at room temperature and a few millitet magnetic field, and is higher at low temperature, about 23%. In 2008, the magnetoresistance change rate of MgO-based MTJ prepared by S. Ikeda et al. reached 604% at room temperature, and 1144% at 5K low temperature (S. Ikeda, J. Hayakawa, Y. Ashizawa, Y. M. Lee, K. Miura, H. Hasegawa, M. Tsunoda, F. Matsukura, and H. Ohno, Appl. Phys. Lett.2008, 93: 082508), this record experimental result is close to the theoretical prediction value of MgO-based MTJ.

中国科学院物理研究所2004年申请了一种以复合铁磁层为铁磁电极的磁隧道结元件国家发明专利(申请号:200410030893.0),通过调节复合铁磁层中的薄铁磁层的厚度可以连续可调复合铁磁层的自旋极化率,从而可以调控该元件的隧道磁电阻值;通过调节作为自由层的复合铁磁层中薄铁磁层的厚度可以连续调整该自由层的矫顽力,从而可以调节该元件的快关场大小。该MTJ元件可应用于磁性随机存储器,但不适合用于对微弱磁场的精确测量。 In 2004, the Institute of Physics of the Chinese Academy of Sciences applied for a national invention patent for a magnetic tunnel junction element with a composite ferromagnetic layer as a ferromagnetic electrode (application number: 200410030893.0). By adjusting the thickness of the thin ferromagnetic layer in the composite ferromagnetic layer, it can The spin polarizability of the composite ferromagnetic layer can be adjusted continuously, so that the tunnel magnetoresistance value of the element can be regulated; the correction of the free layer can be continuously adjusted by adjusting the thickness of the thin ferromagnetic layer in the composite ferromagnetic layer as the free layer. Coercive force, so that the size of the fast-off field of the element can be adjusted. The MTJ element can be applied to magnetic random access memory, but it is not suitable for accurate measurement of weak magnetic fields.

Xia Li等人2009年申请了一种MTJ结构专利(专利号:US20110044096A1),该MTJ由底层电极、固定层、隧道势垒层、自由层和顶层电极组成。Jason Reid等2009年申请了一种包括热障层的MTJ结构的专利(专利号:US20110108937A1),相比传统MTJ结构具有更快的开关速度,与标准半导体制造过程具有更好的兼容性。Xiaohua Lou等2010年申请了一种交错排列MTJ专利(专利号:US20110026320A1,US008203874B2)。但是这些已有的技术方案中MTJ敏感元件用于微弱磁场测量,测量分辨力和精度需要进一步提高。 Xia Li et al. applied for a MTJ structure patent in 2009 (patent number: US20110044096A1). The MTJ consists of a bottom electrode, a fixed layer, a tunnel barrier layer, a free layer and a top electrode. Jason Reid et al. applied for a patent for an MTJ structure including a thermal barrier layer in 2009 (patent number: US20110108937A1), which has faster switching speeds than traditional MTJ structures and better compatibility with standard semiconductor manufacturing processes. Xiaohua Lou et al. applied for a staggered MTJ patent in 2010 (patent number: US20110026320A1, US008203874B2). However, in these existing technical solutions, the MTJ sensitive element is used for weak magnetic field measurement, and the measurement resolution and accuracy need to be further improved.

纵观MTJ的几十年的发展历程,中间势垒层对磁隧道结的发展具有极为重要的推动作用,势垒层从早期的Ge到Al2O3,再到MgO,在铁磁层基本不变的情况下,磁隧道结的磁阻变化率近似呈指数级提高,这一发展规律激发了人们对势垒层的关注和研究。此外,研究人员在分析磁隧道结噪声特性时发现:势垒层在制备过程中存在的不一致性、针孔等缺陷会产生1/f噪声,从而限制了MTJ磁传感器的低频磁场测量能力。 Throughout the decades of development of MTJ, the intermediate barrier layer plays an extremely important role in promoting the development of the magnetic tunnel junction. The barrier layer ranges from early Ge to Al 2 O 3 , and then to MgO. Under the same condition, the magnetoresistance change rate of the magnetic tunnel junction increases approximately exponentially. This development law has inspired people's attention and research on the barrier layer. In addition, when analyzing the noise characteristics of the magnetic tunnel junction, the researchers found that the inconsistency and pinhole defects in the barrier layer during the preparation process will generate 1/f noise, which limits the low-frequency magnetic field measurement capability of the MTJ magnetic sensor.

发明内容 Contents of the invention

本发明要解决的技术问题就在于:针对现有技术存在的技术问题,本发明提供了一种结构简单紧凑、体积小、成本低廉、制作方便、具有高分辨力的采用石墨烯作为势垒层的MTJ磁场传感器。 The technical problem to be solved by the present invention is: aiming at the technical problems existing in the prior art, the present invention provides a simple and compact structure, small volume, low cost, convenient manufacture, and high resolution using graphene as a barrier layer The MTJ magnetic field sensor.

为解决上述技术问题,本发明采用以下技术方案: In order to solve the problems of the technologies described above, the present invention adopts the following technical solutions:

一种以石墨烯作为势垒层的MTJ磁场传感器,包括两个磁力线聚集器、用来构成惠斯通测量电桥的四个MTJ磁敏感元件、四个电极及基底,两个磁力线聚集器呈对称状布置,两个所述MTJ磁敏感元件位于两个磁力线聚集器之间的间隙处,另外两个所述MTJ磁敏感元件分别位于两个磁力线聚集器的底部,每个所述MTJ磁敏感元件均包括由下至上依次堆叠排列的基底、底电极层、第一缓冲层、自由铁磁层、石墨烯势垒层、被钉扎铁磁层、钉扎层、第二缓冲层及顶电极层。 An MTJ magnetic field sensor using graphene as a potential barrier layer, including two magnetic field line concentrators, four MTJ magnetic sensitive elements used to form a Wheatstone measurement bridge, four electrodes and a substrate, the two magnetic field line concentrators are Symmetrically arranged, the two MTJ magnetic sensitive elements are located in the gap between the two magnetic force line concentrators, and the other two MTJ magnetic sensitive elements are respectively located at the bottom of the two magnetic force line concentrators, each of the MTJ magnetic sensitive Each element includes a substrate, a bottom electrode layer, a first buffer layer, a free ferromagnetic layer, a graphene barrier layer, a pinned ferromagnetic layer, a pinned layer, a second buffer layer, and a top electrode stacked in sequence from bottom to top. layer.

作为本发明的进一步改进: As a further improvement of the present invention:

所述石墨烯势垒层为单层石墨烯或多层石墨烯。 The graphene barrier layer is single-layer graphene or multi-layer graphene.

所述石墨烯势垒层的层数为大于1的奇数。 The number of layers of the graphene barrier layer is an odd number greater than 1.

所述石墨烯通过化学气相沉积法直接制备在自由铁磁层上形成石墨烯势垒层。 The graphene is directly prepared by a chemical vapor deposition method to form a graphene barrier layer on the free ferromagnetic layer.

所述石墨烯通过氧化还原法或有机合成法制备好后转移到自由铁磁层上。 The graphene is prepared by oxidation-reduction method or organic synthesis method and then transferred to the free ferromagnetic layer.

与现有技术相比,本发明的优点在于:本发明以石墨烯作为MTJ的势垒层来制造磁场传感器,由于石墨烯具有极好的自旋输运能力,使得石墨烯基MTJ具有更高的磁阻变化率,从而提高磁场测量灵敏度,此外还同时具有低频噪声低、体积小、功耗低等优点,并且传感器整体结构简单,制造方便,可有效降低磁传感器的制作成本。 Compared with prior art, the advantage of the present invention is: the present invention uses graphene as the potential barrier layer of MTJ to manufacture magnetic field sensor, because graphene has excellent spin transport ability, makes graphene-based MTJ have higher The magnetoresistance change rate is high, thereby improving the sensitivity of magnetic field measurement. In addition, it also has the advantages of low low-frequency noise, small size, and low power consumption. The overall structure of the sensor is simple and easy to manufacture, which can effectively reduce the production cost of the magnetic sensor.

附图说明 Description of drawings

图1是本发明中以石墨烯作为势垒层的MTJ磁敏感元件截面示意图。 Fig. 1 is a cross-sectional schematic diagram of an MTJ magnetic sensitive element using graphene as a barrier layer in the present invention.

图2是本发明中以石墨烯作为势垒层的MTJ磁场传感器结构。 Fig. 2 is the structure of the MTJ magnetic field sensor using graphene as the barrier layer in the present invention.

图3是本发明中以石墨烯作为势垒层的MTJ磁场传感器测量原理示意图。 Fig. 3 is a schematic diagram of the measurement principle of the MTJ magnetic field sensor using graphene as a barrier layer in the present invention.

图例说明: illustration:

1、基底;2、底电极层;3、第一缓冲层;4、自由铁磁层;5、石墨烯势垒层;6、被钉扎铁磁层;7、钉扎层;8、第二缓冲层;9、顶电极层;1201、第一磁力线聚集器;1202、第二磁力线聚集器;1301、第一MTJ磁敏感元件;1302、第二MTJ磁敏感元件;1303、第三MTJ磁敏感元件;1304、第四MTJ磁敏感元件;1401、第一电极;1402、第二电极;1403、第三电极;1404、第四电极。 1. Substrate; 2. Bottom electrode layer; 3. First buffer layer; 4. Free ferromagnetic layer; 5. Graphene barrier layer; 6. Pinned ferromagnetic layer; 7. Pinning layer; 8. The third 2 buffer layer; 9, top electrode layer; 1201, first magnetic force line concentrator; 1202, second magnetic force line concentrator; 1301, first MTJ magnetic sensitive element; 1302, second MTJ magnetic sensitive element; 1303, third MTJ magnetic Sensitive element; 1304, fourth MTJ magnetic sensitive element; 1401, first electrode; 1402, second electrode; 1403, third electrode; 1404, fourth electrode.

具体实施方式 Detailed ways

以下将结合说明书附图和具体实施例对本发明做进一步详细说明。 The present invention will be further described in detail below in conjunction with the accompanying drawings and specific embodiments.

如图1所示,本发明的以石墨烯作为势垒层的MTJ磁场传感器,包括由下至上依次堆叠排列的基底1、底电极层2、第一缓冲层3、自由铁磁层4、石墨烯势垒层5、被钉扎铁磁层6、钉扎层7、第二缓冲层8、顶电极层9。在这种结构中,自由铁磁层4为磁性自由层,其磁矩方向A随外磁场的改变而改变;被钉扎铁磁层6是一个固定磁性层,因为其磁矩方向B被钉扎层7固定在一个方向,在一般条件下是不会改变的。MTJ磁敏感元件的电阻值就是底电极层2与顶电极层9之间的电阻值,当自由铁磁层4的磁矩方向A与被钉扎铁磁层6的磁矩方向B顺向平行时,MTJ磁敏感元件为低电阻态;当自由铁磁层4的磁矩方向A与被钉扎铁磁层6的磁矩方向B反向平行时,MTJ磁敏感元件为高电阻态,而MTJ磁敏感元件的电阻随着测量磁场在高阻态和低阻态之间线性变化。 As shown in Figure 1, the MTJ magnetic field sensor using graphene as a barrier layer of the present invention includes a substrate 1, a bottom electrode layer 2, a first buffer layer 3, a free ferromagnetic layer 4, and a graphite layer stacked in sequence from bottom to top. An ene barrier layer 5 , a pinned ferromagnetic layer 6 , a pinning layer 7 , a second buffer layer 8 , and a top electrode layer 9 . In this structure, the free ferromagnetic layer 4 is a magnetic free layer, and its magnetic moment direction A changes with the change of the external magnetic field; the pinned ferromagnetic layer 6 is a fixed magnetic layer, because its magnetic moment direction B is pinned The tie layer 7 is fixed in one direction, which cannot be changed under normal conditions. The resistance value of the MTJ magnetic sensitive element is the resistance value between the bottom electrode layer 2 and the top electrode layer 9, when the magnetic moment direction A of the free ferromagnetic layer 4 is parallel to the magnetic moment direction B of the pinned ferromagnetic layer 6 , the MTJ magnetic sensitive element is in a low resistance state; when the magnetic moment direction A of the free ferromagnetic layer 4 is antiparallel to the magnetic moment direction B of the pinned ferromagnetic layer 6, the MTJ magnetic sensitive element is in a high resistance state, and The resistance of the MTJ magnetic sensitive element changes linearly between the high resistance state and the low resistance state with the measuring magnetic field.

在具体实施例中,基底1通常选用硅、石英、玻璃或者是其他能够晶圆集成的任何材料,硅加工工艺成熟并且由于易于加工,因此为集成电路成为最好的选择。底电极层2和顶电极层9通常采用非磁性导电材料,例如铜、铝、金、银等,可以通过蒸镀、磁控溅射等工艺制备在基底1上。第一缓冲层3和第二缓冲层8的材料一般可以选择钽,并可通过磁控溅射工艺制备。自由铁磁层4和被钉扎铁磁层6均选择铁磁性材料,如铁、镍、钴或它们的合金材料,也可通过磁控溅射工艺制备。石墨烯势垒层5为单层石墨烯或多层(一般为3、5、7等奇数层)石墨烯,石墨烯可以通过化学气相沉积法直接制备在自由铁磁层4上,或通过其它方法氧化还原法、有机合成法制备好后转移到自由铁磁层4上。钉扎层7选用硬磁性材料制备。 In a specific embodiment, the substrate 1 is usually made of silicon, quartz, glass or any other material capable of wafer integration. Silicon processing technology is mature and easy to process, so it is the best choice for integrated circuits. The bottom electrode layer 2 and the top electrode layer 9 are usually made of non-magnetic conductive materials, such as copper, aluminum, gold, silver, etc., and can be prepared on the substrate 1 by evaporation, magnetron sputtering, and other processes. Materials for the first buffer layer 3 and the second buffer layer 8 can generally be selected from tantalum, and can be prepared by magnetron sputtering. Both the free ferromagnetic layer 4 and the pinned ferromagnetic layer 6 are made of ferromagnetic materials, such as iron, nickel, cobalt or their alloy materials, and can also be prepared by magnetron sputtering. The graphene barrier layer 5 is single-layer graphene or multi-layer (generally 3, 5, 7 and other odd-numbered layers) graphene, and graphene can be directly prepared on the free ferromagnetic layer 4 by chemical vapor deposition, or by other Methods The redox method and the organic synthesis method are prepared and then transferred to the free ferromagnetic layer 4 . The pinning layer 7 is made of hard magnetic materials.

如图2所示,为本发明以石墨烯作为势垒层的MTJ磁场传感器,包括磁力线聚集器、用来构成惠斯通测量电桥的四个MTJ磁敏感元件(即第一MTJ磁敏感元件1301、第二MTJ磁敏感元件1302、第三MTJ磁敏感元件1303、第四MTJ磁敏感元件1304)、四个电极(即第一电极1401、第二电极1402、第三电极1403、第四电极1404)及基底1。磁力线聚集器用于放大外部被测磁场,磁力线聚集器包括第一磁力线聚集器1201和第二磁力线聚集器1202,第一磁力线聚集器1201和第二磁力线聚集器1202呈对称状布置,其形状不仅限于图中的矩形,长度方向与传感器磁场敏感方向C一致;第一磁力线聚集器1201和第二磁力线聚集器1202之间留有间隙。磁力线聚集器根据实际需要可以采用软磁性材料制备。四个MTJ磁敏感元件构成了一个惠斯通测量电桥,其中第一MTJ磁敏感元件1301、第二MTJ磁敏感元件1302位于第一磁力线聚集器1201与第二磁力线聚集器1202之间的间隙处,用来感应放大后的磁场,其电阻值随被测磁场而改变,为敏感测量电阻。第三MTJ磁敏感元件1303、第四MTJ磁敏感元件1304分别位于第一磁力线聚集器1201和第二磁力线聚集器1202的底部,它们的电阻值不受被测磁场的影响,为参考电阻。四个电极用于连接四个石墨烯基MTJ磁敏感元件,电极的形状和位置不限于图中所示,电极只要位于基底1边缘即可。该磁场传感器的四个电极可以通过引线连接到封装管壳引线框的封装引脚上或ASIC(Application Specific Integrated Circuit,专用集成电路)。 As shown in Figure 2, it is the MTJ magnetic field sensor with graphene as the potential barrier layer of the present invention, including the magnetic field line concentrator, four MTJ magnetic sensitive elements (i.e. the first MTJ magnetic sensitive element) that are used to form the Wheatstone measurement bridge 1301, second MTJ magnetic sensitive element 1302, third MTJ magnetic sensitive element 1303, fourth MTJ magnetic sensitive element 1304), four electrodes (namely first electrode 1401, second electrode 1402, third electrode 1403, fourth electrode 1404) and base 1. The magnetic force line concentrator is used to amplify the external measured magnetic field. The magnetic force line concentrator includes a first magnetic force line concentrator 1201 and a second magnetic force line concentrator 1202. The first magnetic force line concentrator 1201 and the second magnetic force line concentrator 1202 are symmetrically arranged, and its shape is not limited to The length direction of the rectangle in the figure is consistent with the magnetic field sensitive direction C of the sensor; there is a gap between the first magnetic force line concentrator 1201 and the second magnetic force line concentrator 1202 . The magnetic force line concentrator can be made of soft magnetic materials according to actual needs. Four MTJ magnetic sensitive elements constitute a Wheatstone measurement bridge, wherein the first MTJ magnetic sensitive element 1301 and the second MTJ magnetic sensitive element 1302 are located in the gap between the first magnetic flux concentrator 1201 and the second magnetic flux concentrator 1202 It is used to induce the amplified magnetic field, and its resistance value changes with the measured magnetic field, which is a sensitive measurement resistance. The third MTJ magnetic sensitive element 1303 and the fourth MTJ magnetic sensitive element 1304 are located at the bottom of the first magnetic force line concentrator 1201 and the second magnetic force line concentrator 1202 respectively, and their resistance values are not affected by the measured magnetic field and are reference resistances. The four electrodes are used to connect four graphene-based MTJ magnetic sensitive elements. The shape and position of the electrodes are not limited to those shown in the figure, as long as the electrodes are located on the edge of the substrate 1 . The four electrodes of the magnetic field sensor can be connected to the package pins of the package case lead frame or ASIC (Application Specific Integrated Circuit, application specific integrated circuit) through leads.

如图3所示,为本发明在具体应用实例中的测量原理示意图。四个MTJ磁敏感元件(即第一MTJ磁敏感元件1301、第二MTJ磁敏感元件1302、第三MTJ磁敏感元件1303、第四MTJ磁敏感元件1304)构成了一个惠斯通全桥,其中第一MTJ磁敏感元件1301和第二MTJ磁敏感元件1302的敏感方向相同,并且其电阻值随着被测磁场变化,第三MTJ磁敏感元件1303和第四MTJ磁敏感元件1304为参考电阻。在理想情况下,当外磁场为零时,这四个敏感元件的电阻值相等,这时电桥输出电压为零。第三电极1403和第一电极1401之间的电压差(Vout1-Vout2)为输出电压Vout,它与外部测量磁场呈线性关系。 As shown in FIG. 3 , it is a schematic diagram of the measurement principle of the present invention in a specific application example. Four MTJ magnetic sensitive elements (ie, the first MTJ magnetic sensitive element 1301, the second MTJ magnetic sensitive element 1302, the third MTJ magnetic sensitive element 1303, and the fourth MTJ magnetic sensitive element 1304) constitute a Wheatstone full bridge, wherein The first MTJ magnetic sensitive element 1301 and the second MTJ magnetic sensitive element 1302 have the same sensitive direction, and their resistance value changes with the measured magnetic field. The third MTJ magnetic sensitive element 1303 and the fourth MTJ magnetic sensitive element 1304 are reference resistors. Ideally, when the external magnetic field is zero, the resistance values of these four sensitive elements are equal, and the output voltage of the bridge is zero at this time. The voltage difference ( V out1 - V out2 ) between the third electrode 1403 and the first electrode 1401 is the output voltage V out, which has a linear relationship with the external measurement magnetic field.

上述的电桥型磁传感器可以在同一基底1上采用相同的工艺制备,作为单一芯片磁传感器使用,其电极可以连接到ASIC或封装管壳引线框的封装引脚上。 The bridge-type magnetic sensor mentioned above can be prepared on the same substrate 1 by the same process, and used as a single-chip magnetic sensor, and its electrodes can be connected to the packaging pins of the ASIC or the packaging package lead frame.

以上仅是本发明的优选实施方式,本发明的保护范围并不仅局限于上述实施例,凡属于本发明思路下的技术方案均属于本发明的保护范围。应当指出,对于本技术领域的普通技术人员来说,在不脱离本发明原理前提下的若干改进和润饰,应视为本发明的保护范围。 The above are only preferred implementations of the present invention, and the protection scope of the present invention is not limited to the above-mentioned embodiments, and all technical solutions under the idea of the present invention belong to the protection scope of the present invention. It should be pointed out that for those skilled in the art, some improvements and modifications without departing from the principle of the present invention should be regarded as the protection scope of the present invention.

Claims (5)

1. the MTJ magnetic field sensor using Graphene as barrier layer, it is characterized in that, comprise two magnetic line of force collectors, be used for forming four MTJ magnet-sensitive elements of Hui Sitong measuring bridge, four electrodes and substrate, two magnetic line of force collectors symmetrically shape layout, the gap location of two described MTJ magnet-sensitive elements between two magnetic line of force collectors, described in two other, MTJ magnet-sensitive element lays respectively at the bottom of two magnetic line of force collectors, each described MTJ magnet-sensitive element includes the substrate stacking gradually arrangement from the bottom to top, bottom electrode layer, first cushion, free ferromagnetic, Graphene barrier layer, pinned ferromagnetic layer, pinning layer, second cushion and top electrode layer.
2. the MTJ magnetic field sensor using Graphene as barrier layer according to claim 1, is characterized in that, described Graphene barrier layer is single-layer graphene or multi-layer graphene.
3. the MTJ magnetic field sensor using Graphene as barrier layer according to claim 2, is characterized in that, when described Graphene barrier layer is multi-layer graphene, the number of plies of described Graphene barrier layer be greater than 1 odd number.
4. the MTJ magnetic field sensor using Graphene as barrier layer according to claim 2, is characterized in that, described Graphene is directly prepared on free ferromagnetic by chemical vapour deposition technique and forms Graphene barrier layer.
5. the MTJ magnetic field sensor using Graphene as barrier layer according to claim 2, is characterized in that, described Graphene is transferred on free ferromagnetic after being prepared by oxidation-reduction method or organic synthesis method.
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