1. Field of the Invention
Embodiments disclosed herein generally relate to a magnetic read head for use in a hard disk drive.
2. Description of the Related Art
The heart of a computer is a magnetic disk drive which typically includes a rotating magnetic disk, a slider that has read and write heads, suspension arms above and below the rotating disk and an actuator arm that swings the suspension arm to place the read and/or write heads over selected circular tracks on the rotating disk. The suspension arm biases the slider towards the surface of the disk when the disk is not rotating but, when the disk rotates, air is swirled by the rotating disk adjacent a media facing surface (MFS), such as an air bearing surface (ABS), of the slider causing the slider to ride on an air bearing a slight distance from the surface of the rotating disk. When the slider rides on the air bearing, the write and read heads are employed for writing magnetic transitions corresponding to host data. The read and write heads are connected to a signal processing circuitry that operates according to a computer program to implement the writing and reading functions.
The major limiting factor for achieving the required signal to noise ratio (SNR) for magnetoresistive heads, either tunnel magnetoresistive (TMR) heads or current perpendicular to plane-giant magnetoresistive (CPP-GMR) heads, for applications above 1 Tb/in2 is thermal magnetic noise of the free magnetic layer. The thermal magnetic noise is inversely proportional to the device volume and therefore, the noise becomes a bigger problem as the free magnetic layer volume continues to shrink. The noise is also proportional to the bias current applied through the device and the magnetoresistive ratio of the device, thus, unlike thermal electronic noise (i.e., Johnson noise), thermal magnetic noise cannot be overcome by increasing the bias current or the device magnetoresistive ratio.
Physically, the most effective way to tune the magnetic noise is via a damping parameter of the free magnetic layer because the noise power is directly proportional to the damping parameter of the free magnetic layer and the signal is not affected by changes in damping. Currently, there are no known efficient ways to tune the magnetic noise by exploiting this mechanism.
Therefore, there is a need in the art for a magnetic read head with a tuned damping parameter of the free magnetic layer.
The embodiments disclosed generally relate to a read head in a magnetic recording head. The read head utilizes a spin Hall effect layer disposed over the free magnetic layer. Electrical bias is applied to the top shield, or lead layer, longitudinally so that the current is longitudinally driven through the spin Hall effect layer. The spin Hall effect layer may comprise Pt, Ta, W, or copper doped with either bismuth or iridium, or combinations thereof. The spin Hall effect layer, together with the longitudinally applied bias, reduces the damping in the free magnetic layer and hence, reduces the thermal magnetic noise of the read head.
In one embodiment, a magnetic read head comprises a magnetic sensor having a free magnetic layer; and a spin Hall effect layer disposed over the free magnetic layer, wherein the spin Hall effect layer reduces damping in the free magnetic layer and thermal magnetic noise of the read head.
In another embodiment, a magnetic read head comprises: a bottom shield; a pinned magnetic structure disposed over the bottom shield; a spacer layer disposed on the pinned magnetic structure; a free magnetic layer disposed on the spacer layer; a spin Hall effect layer disposed on the free magnetic layer; a first insulating layer disposed on the bottom shield, sidewalls of the pinned magnetic structure, sidewalls of the spacer layer, sidewalls of the free magnetic layer, and sidewalls of the spin Hall effect layer; a hard bias layer disposed on the first insulating layer, wherein the hard bias layer has a top surface that is collinear with a top surface of thee free magnetic layer; a second insulating layer disposed on the hard bias layer, wherein the second insulating layer has a top surface that is collinear with a top surface of the spin Hall effect layer; and a top shield disposed on the second insulating layer and the spin Hall effect layer, wherein the top shield is electrically coupled to a power source.
In another embodiment, a magnetic read head comprises: a bottom shield; a pinned magnetic structure disposed over the bottom shield; a spacer layer disposed on the pinned magnetic structure; a free magnetic layer disposed on the spacer layer; a spin Hall effect layer disposed on the free magnetic layer; a first insulating layer disposed on the bottom shield, sidewalls of the pinned magnetic structure, sidewalls of the spacer layer, sidewalls of the free magnetic layer, and sidewalls of the spin Hall effect layer; a hard bias layer disposed on the first insulating layer, wherein the hard bias layer has a top surface that is collinear with a top surface of thee free magnetic layer; a second insulating layer disposed on the hard bias layer, wherein the second insulating layer is thinner than the spin Hall effect layer; and a top shield disposed on the second insulating layer and the spin Hall effect layer, wherein the top shield is electrically coupled to a power source.
In another embodiment, a magnetic read head comprises: a bottom shield; a pinned magnetic structure disposed over the bottom shield; a spacer layer disposed on the pinned magnetic structure; a free magnetic layer disposed on the spacer layer; a spin Hall effect spacer layer disposed on the free magnetic layer; a spin Hall effect layer disposed on the spin Hall effect spacer layer; a first insulating layer disposed on the bottom shield, sidewalls of the pinned magnetic structure, sidewalls of the spacer layer, sidewalls of the free magnetic layer, and sidewalls of the spin Hall effect layer; a hard bias layer disposed on the first insulating layer, wherein the hard bias layer has a top surface that is collinear with a top surface of thee free magnetic layer; a second insulating layer disposed on the hard bias layer, wherein the second insulating layer is thinner than the spin Hall effect layer; and a top shield disposed on the second insulating layer and the spin Hall effect layer, wherein the top shield is electrically coupled to a power source.
In another embodiment, magnetic read head comprises: a bottom shield; a pinned magnetic structure disposed over the bottom shield; a spacer layer disposed on the pinned magnetic structure; a free magnetic layer disposed on the spacer layer; a spin Hall effect layer disposed on the free magnetic layer; a first insulating layer disposed on the bottom shield, sidewalls of the pinned magnetic structure, sidewalls of the spacer layer, sidewalls of the free magnetic layer, and sidewalls of the spin Hall effect layer; a hard bias layer disposed on the first insulating layer, wherein the hard bias layer has a top surface that is collinear with a top surface of thee free magnetic layer; a second insulating layer disposed on the hard bias layer, wherein the second insulating layer is thinner than the spin Hall effect layer; a laminated shield consisting of a first shield layer disposed on the second insulating layer and the spin Hall effect layer, wherein the first shield layer is electrically coupled to a power source; a third insulating layer that can propagate interlayer exchange coupling disposed on the first shield layer; and a top shield disposed on the third insulating layer.
In another embodiment, a magnetic read head comprises: a bottom shield; a pinned magnetic structure disposed over the bottom shield; a spacer layer disposed on the pinned magnetic structure; a free magnetic layer disposed on the spacer layer; a spin Hall effect layer disposed on the free magnetic layer; a first insulating layer disposed on the bottom shield, sidewalls of the pinned magnetic structure, sidewalls of the spacer layer, sidewalls of the free magnetic layer, and sidewalls of the spin Hall effect layer; a side shield disposed on the first insulating layer and the spin Hall effect layer, wherein the side shield is electrically coupled to a power source; a second insulating layer that can propagate interlayer exchange coupling disposed on the side shield; and a top shield disposed on the second insulating layer.
The magnetic read heads discussed herein may be used in various types of magnetic storage mediums such as hard disk drives, tape magnetic storage and hybrid drives which include a mixture of magnetic disk media and flash memory.
So that the manner in which the above recited features can be understood in detail, a more particular description of the invention, briefly summarized above, may be had by reference to embodiments, some of which are illustrated in the appended drawings. It is to be noted, however, that the appended drawings illustrate only typical embodiments of this invention and are therefore not to be considered limiting of its scope, for the invention may admit to other equally effective embodiments.
To facilitate understanding, identical reference numerals have been used, where possible, to designate identical elements that are common to the figures. It is contemplated that elements disclosed in one embodiment may be beneficially utilized on other embodiments without specific recitation.
In the following, reference is made to embodiments of the invention. However, it should be understood that the invention is not limited to specific described embodiments. Instead, any combination of the following features and elements, whether related to different embodiments or not, is contemplated to implement and practice the invention. Furthermore, although embodiments of the invention may achieve advantages over other possible solutions and/or over the prior art, whether or not a particular advantage is achieved by a given embodiment is not limiting of the invention. Thus, the following aspects, features, embodiments and advantages are merely illustrative and are not considered elements or limitations of the appended claims except where explicitly recited in a claim(s). Likewise, reference to “the invention” shall not be construed as a generalization of any inventive subject matter disclosed herein and shall not be considered to be an element or limitation of the appended claims except where explicitly recited in a claim(s).
The embodiments disclosed generally relate to a read head in a magnetic recording head. The read head utilizes a spin Hall effect layer disposed on the free magnetic layer. Electrical bias is applied to the top shield, or lead layer, longitudinally so that the current is longitudinally driven through the spin Hall effect layer. The spin Hall effect layer may comprise Pt, Ta, W, or copper doped with either bismuth or iridium, or combinations thereof. The spin Hall effect layer, together with the longitudinally applied bias, reduces the damping in the free magnetic layer and hence, reduces the thermal magnetic noise of the read head.
Magnetic disks 110 may include circular tracks of data on both the top and bottom surfaces of the disk. A magnetic head 180 mounted on a slider may be positioned on a track. As each disk spins, data may be written on and/or read from the data track. Magnetic head 180 may be coupled to an actuator arm 130 as illustrated in
A pinned magnetic layer 308 is deposited on the antiferromagnetic layer 306. The pinned magnetic layer 308 may comprise one or more magnetic materials such as, for example, NiFe, CoFe, CoFeB, or diluted magnetic alloys. A nonmagnetic coupling layer 310 is deposited on the pinned magnetic layer 308. The coupling layer 310 may comprise Ru, Ta or combinations thereof. A reference magnetic layer 312 is deposited on the nonmagnetic coupling layer 310. The reference magnetic layer 312 may comprise one or more magnetic materials such as, for example NiFe, CoFe, CoFeB, or diluted magnetic alloys. A spacer layer 314 is deposited on the reference magnetic layer 312. In the case of a TMR sensor, the spacer layer 314 comprises an insulating material such as MgO, TiO2 or alumina. For a GMR sensor, the spacer layer 314 may comprise a conductive material such as Cu, Ag, or their alloys with other metals. Each of the layers of the sensor structure 302 may be deposited by well known deposition methods such as sputtering.
A free magnetic layer 316 is deposited on the spacer layer 314. The free magnetic layer 316 may comprise Co, Fe, B, Co, CoFe, CoFeB, NiFe, CoHf or combinations thereof. The free magnetic layer 316 may comprise a single layer of magnetic material or, in other embodiments, multiple layers. The free magnetic layer 316 has a thickness of between about 15 Angstroms to about 75 Angstroms. While not shown, a capping layer may be disposed on the free magnetic layer 316. The capping layer would have a thickness of between about 15 Angstroms and about 75 Angstroms. In some embodiments, the capping layer may comprise multiple layers.
Bordering the sensor structure 302 is a first insulating layer 318 that is disposed on the first shield layer S1 as well as the sidewalls of the sensor structure 302, such as the pinned magnetic structure 304, the spacer layer 314 and the free magnetic layer 316. The first insulating layer 318 may comprise an insulating material such as aluminum oxide or silicon nitride. The first insulating layer 318 may be deposited by well known deposition methods such as atomic layer deposition (ALD), chemical vapor deposition (CVD), and ion beam sputtering (IBD). On the first insulating layer 318, a magnetic bias layer 320 is then deposited. The bias layer 320 may comprise a single material or laminated magnetic materials such as CoPt, FePt, high moment CoFe or NiFe. Once the bias layer 320 is deposited, a bias capping structure, not shown, may be deposited over the bias layer 320. In one embodiment, the bias capping structure may comprise a multiple layered structure comprising one or combination of a tantalum layer, an iridium layer, a chromium layer, a titanium layer and a ruthenium layer.
As shown in
The spin Hall effect arises from spin orbit interaction of conduction electrons in normal metals. When the electric current density jC is applied in an x direction through a conducting layer of thickness t along the z-direction, the spin current jS of y-polarized spins flows in the z direction, i.e., across the layer thickness. If there is a ferromagnetic layer on the conducting layer, the spin current can affect the ferromagnetic layer's static and dynamic magnetic properties via spin transfer torque and/or spin pumping effects. Hence, in the embodiment shown in
In the embodiment shown in
A second insulating layer 326 is disposed over the bias layer 320 and the first insulating layer 318. The second insulating layer 326 may be deposited by well known deposition methods such as ALD, CVD, and IBD. In the embodiment shown in
In the embodiment shown in
In the embodiment shown in
In the embodiment shown in
As shown in
By applying a bias to a shield layer that is in contact with a spin Hall effect layer, the damping of the free magnetic layer is reduced as is the magnetic noise. As such, the magnetic read head has an increased signal to noise ratio due to the reduced magnetic noise.
While the foregoing is directed to exemplary embodiments, other and further embodiments of the invention may be devised without departing from the basic scope thereof, and the scope thereof is determined by the claims that follow.