Embodiments of the present disclosure generally relate to data storage devices, and more specifically, to a magnetic media drive employing a magnetic recording head.
Over the past few years, microwave assisted magnetic recording (MAMR) has been studied as a recording method to improve the areal density of a magnetic read/write device, such as a hard disk drive (HDD). MAMR enabled magnetic recording heads utilize a spin torque oscillator (STO) for generating a microwave (high frequency AC magnetic field). When the magnetic field from the write head is applied and current is conducted to the STO from the main pole, the STO oscillates and may provide an AC magnetic field to the recording medium. The AC magnetic field may reduce the coercive force of the recording medium, thus high quality recording by MAMR may be achieved. Typically the STO includes a spin polarization layer (SPL), a field generation layer (FGL) and an interlayer disposed between the SPL and the FGL. The STO generates high frequency magnetic fields, or microwaves, as a result of the transfer of spin torque from the SPL through the interlayer to the FGL, and the in-plane high speed rotation of the magnetization of the FGL serves as the in-plane free layer.
However, current efficiency from the main pole to the STO is low due to current crowding. Furthermore, hot spots can form at a media facing surface (MFS) when higher current density is driven to the STO, reducing the reliability of the data storage device. Therefore, there is a need in the art for an improved data storage device.
The present disclosure generally relates to data storage devices, and more specifically, to a magnetic media drive employing a magnetic recording head. The head includes a trailing shield, a main pole, an STO disposed between the trailing shield and the main pole, and a non-magnetic conductive structure (or non-magnetic conductive layers) adjacent to the main pole and in contact with the STO. The non-magnetic conductive structure provides additional paths for electrical currents to flow to the STO. The non-magnetic conductive structure enables higher current density to the STO without creating hot spots at the MFS. Maximum current efficiency and uniformity can be achieved with the non-magnetic conductive structure.
In one embodiment, a magnetic recording head includes a main pole, a spin torque oscillator in contact with the main pole, and a non-magnetic conductive structure surrounding at least a portion of the main pole, wherein the non-magnetic conductive structure is in contact with the spin torque oscillator.
In another embodiment, a magnetic recording head includes a main pole, a spin torque oscillator in contact with the main pole, and a non-magnetic conductive structure in contact with the main pole at a media facing surface.
In another embodiment, a magnetic recording head includes a main pole, wherein the main pole includes a first surface at a media facing surface, a second surface adjacent to the first surface, a third surface connected to the second surface, and a fourth surface opposite the third surface, a spin torque oscillator in contact with the second surface of the main pole, a first non-magnetic conductive layer in contact with the spin torque oscillator, and a second non-magnetic conductive layer in contact with the spin torque oscillator.
In another embodiment, a magnetic recording head includes a main pole, a spin torque oscillator in contact with the main pole, and means for providing paths for electrical currents to flow to the spin torque oscillator, wherein the means for providing paths for electrical currents to flow to the spin torque oscillator surrounds a portion of the main pole at a media facing surface.
So that the manner in which the above recited features of the present disclosure can be understood in detail, a more particular description of the disclosure, 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 disclosure and are therefore not to be considered limiting of its scope, for the disclosure 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.
The present disclosure generally relates to data storage devices, and more specifically, to a magnetic media drive employing a magnetic recording head. The head includes a trailing shield, a main pole, an STO disposed between the trailing shield and the main pole, and a non-magnetic conductive structure (or non-magnetic conductive layers) adjacent to the main pole and in contact with the STO. The non-magnetic conductive structure provides additional paths for electrical currents to flow to the STO. The non-magnetic conductive structure enables higher current density to the STO without creating hot spots at the MFS. Maximum current efficiency and uniformity can be achieved with the non-magnetic conductive structure.
The terms “over,” “under,” “between,” and “on” as used herein refer to a relative position of one layer with respect to other layers. As such, for example, one layer disposed over or under another layer may be directly in contact with the other layer or may have one or more intervening layers. Moreover, one layer disposed between layers may be directly in contact with the two layers or may have one or more intervening layers. In contrast, a first layer “on” a second layer is in contact with the second layer. Additionally, the relative position of one layer with respect to other layers is provided assuming operations are performed relative to a substrate without consideration of the absolute orientation of the substrate.
At least one slider 113 is positioned near the magnetic disk 112, each slider 113 supporting one or more magnetic head assemblies 121 that may include an STO for applying an AC magnetic field to a disk surface 122 and one or more non-magnetic conductive layers in contact with the STO. As the magnetic disk 112 rotates, the slider 113 moves radially in and out over the disk surface 122 so that the magnetic head assembly 121 may access different tracks of the magnetic disk 112 where desired data are written. Each slider 113 is attached to an actuator arm 119 by way of a suspension 115. The suspension 115 provides a slight spring force which biases the slider 113 toward the disk surface 122. Each actuator arm 119 is attached to an actuator means 127. The actuator means 127 as shown in
During operation of the disk drive 100, the rotation of the magnetic disk 112 generates an air bearing between the slider 113 and the disk surface 122 which exerts an upward force or lift on the slider 113. The air bearing thus counter-balances the slight spring force of suspension 115 and supports slider 113 off and slightly above the disk surface 122 by a small, substantially constant spacing during normal operation.
The various components of the disk drive 100 are controlled in operation by control signals generated by control unit 129, such as access control signals and internal clock signals. Typically, the control unit 129 comprises logic control circuits, storage means and a microprocessor. The control unit 129 generates control signals to control various system operations such as drive motor control signals on line 123 and head position and seek control signals on line 128. The control signals on line 128 provide the desired current profiles to optimally move and position slider 113 to the desired data track on disk 112. Write and read signals are communicated to and from write and read heads on the assembly 121 by way of recording channel 125.
The above description of a typical magnetic media device and the accompanying illustration of
In some embodiments, the magnetic read head 211 is a magnetoresistive (MR) read head that includes an MR sensing element 204 located between MR shields S1 and S2. In other embodiments, the magnetic read head 211 is a magnetic tunnel junction (MTJ) read head that includes a MTJ sensing device 204 located between MR shields S1 and S2. The magnetic fields of the adjacent magnetized regions in the magnetic disk 112 are detectable by the MR (or MTJ) sensing element 204 as the recorded bits.
The write head 210 includes a main pole 220, a leading shield 206, a trailing shield 240, an STO 230 disposed between the main pole 220 and the trailing shield 240, and a coil 218 that excites the main pole 220. The coil 218 may have a “pancake” structure which winds around a back-contact between the main pole 220 and the trailing shield 240, instead of a “helical” structure shown in
The main pole 220, the trailing shield 240 and the STO 230 all extend to the MFS 212, and the STO 230 disposed between the main pole 220 and the trailing shield 240 is electrically coupled to the main pole 220 and the trailing shield 240. During operation, the STO 230 generates an AC magnetic field that travels to the magnetic disk 202 to lower the coercivity of the region of the magnetic disk 202 adjacent to the STO 230. The write head 210 further includes a heater 250 for adjusting the distance between the read/write head 200 and the magnetic disk 202. The location of the heater 250 is not limited to above the leading shield 206, as shown in
The main pole 220 includes a first surface 320 at the MFS 212, a second surface 322 adjacent to the first surface 320, a third surface 324 connected to the second surface 322, and a fourth surface 326 opposite the third surface 324. The second surface 322 is in contact with a surface 321 of the STO 230. The surface 321 is part of the first magnetic layer 302, as shown in
Conventionally, the STO 230 is in contact with a dielectric material that surrounds the main pole 220, so the electrical current flowing to the STO 230 is from the main pole 220 only, which creating a current crowding issue. Furthermore, as higher current density is driven to the STO 230 from the main pole 220, hot spots can form at the MFS 212. In order to spread the electrical current and to increase current uniformity and efficiency, the non-magnetic conductive structure 310 is utilized.
The non-magnetic conductive structure 310 is fabricated from a non-magnetic electrically conductive metal, such as NiTa, Cr, Cu, Ag, Au, or Rh. In some embodiments, the non-magnetic conductive structure 310 is fabricated from a multi-layer stack, such as NiTa/Ru, Cr/Cu, or Cr/Rh. The non-magnetic conductive structure 310 surrounds a portion of the main pole 220 at the MFS 212. For example, the non-magnetic conductive structure 310 surrounds the third surface 324 and the fourth surface 326 of the main pole 220. In one embodiment, the non-magnetic conductive structure 310 includes a first portion 314 and a second portion 316, and the first portion 314 and the second portion 316 are fabricated from the same non-magnetic conductive material. The first portion 314 of the non-magnetic conductive structure 310 faces the fourth surface 326 of the main pole 220. The definition of the term “face” is extended to include a material located between a first element that is facing a second element and the second element. For example, the dielectric material 254 is located between the first portion 314 of the non-magnetic conductive structure 310 and the fourth surface 326 of the main pole 220. The second portion 316 faces the third surface 324 of the main pole 220. The first portion 314 includes a first surface 334 in contact with the surface 321 of the STO 230, a second surface 336 opposite the first surface 330, and a third surface 313 at the MFS 212 connecting the first surface 334 and the second surface 336. The second portion 316 includes a first surface 330 in contact with the surface 321 of the STO 230, a second surface 332 opposite the first surface 330, and a third surface 315 at the MFS 212 connecting the first surface 330 and the second surface 332. The first surface 334 of the first portion 314, the first surface 330 of the second portion 316, and the second surface 322 of the main pole 220 are co-planar. The second surface 336 of the first portion 314 and the second surface 332 of the second portion 316 are co-planar. The first surface 334 of the first portion 314 has a width W4 at the MFS 212, and the first surface 330 of the second portion 316 has a width W3 at the MFS 212. In one embodiment, the width W3 is substantially the same as the width W4. In one embodiment, the width W3 is substantially different from the width W4. The widths W3, W4 may be substantially greater than the width W2 of the surface 322 of the main pole 220. The widths W1, W2, W3, W4 are in the cross-track direction, as indicated by the X-axis. In one embodiment, the non-magnetic conductive structure 310 is separated from the main pole 220 by the dielectric material 254. In one embodiment, the dielectric material 254 between the non-magnetic conductive structure 310 and the main pole is replaced with a non-magnetic electrically resistive material. The non-magnetic conductive structure 310 is separated from the side shield 312 by the dielectric material 254.
One or multiple current sources may be used to provide a current flowing to the STO 230 from the main pole 220 and a current flowing to the STO 230 from the non-magnetic conductive structure 310. When multiple current sources are used, the current uniformity can be further controlled by controlling the multiple current sources. The non-magnetic conductive structure 310 provides additional paths for electrical currents to flow to the STO 230. The non-magnetic conductive structure 310 enables higher current density to the STO 230 without creating hot spots at the MFS 212. Maximum current efficiency and uniformity can be achieved with the non-magnetic conductive structure 310. In one embodiment, two current sources are utilized. The first current source is connected to the main pole 220, and the second current source is connected to the non-magnetic conductive structure 310 to provide independent flow control to the main pole 220 and the non-magnetic conductive structure 310. In one embodiment, one current source is connected to the main pole 220 and the non-magnetic conductive structure 310, and the non-magnetic electrically resistive material is disposed between the main pole 220 and the non-magnetic conductive structure 310 instead of the dielectric material 254. With the non-magnetic electrically resistive material separating the main pole 220 and the non-magnetic conductive structure 310, a differential current can flow through each of the main pole 220 and the non-magnetic conductive structure 310 with one current source to achieve maximum current uniformity and efficiency. Various current flow patterns using the one or more current sources are illustrated in
In one embodiment, the non-magnetic conductive structure 310 includes a single piece of material, as shown in
The first non-magnetic conductive layer 340 is separated from the main pole 220, the side shield 312, and the second non-magnetic conductive layer 342 by the dielectric material 254. The second non-magnetic conductive layer 342 is separated from the main pole 220, the side shield 312, and the first non-magnetic conductive layer 340 by the dielectric material 254. The first non-magnetic conductive layer 340 includes a first surface 344 in contact with the surface 321 of the STO 230, a second surface 346 opposite the first surface 344, and a third surface 348 at the MFS 212 connecting the first surface 344 and the second surface 346. The second non-magnetic conductive layer 342 includes a first surface 350 in contact with the surface 321 of the STO 230, a second surface 352 opposite the first surface 350, and a third surface 354 at the MFS 212 connecting the first surface 350 and the second surface 352. The first surface 344 of the first non-magnetic conductive layer 340, the first surface 350 of the second non-magnetic conductive layer 342, and the second surface 322 of the main pole 220 are co-planar. The second surface 346 of the first non-magnetic conductive layer 340 and the second surface 352 of the second non-magnetic conductive layer 342 are co-planar. The first surface 344 of the first non-magnetic conductive layer 340 has a width W5 at the MFS 212, and the first surface 350 of the second non-magnetic conductive layer 342 has a width W6 at the MFS 212. In one embodiment, the width W5 is substantially the same as the width W6. In one embodiment, the width W5 is substantially different from the width W6. The widths W5, W6 may be substantially greater than the width W2 of the surface 322 of the main pole 220. The widths W5, W6 are in the cross-track direction, as indicated by the X-axis. In some embodiments, one or both non-magnetic conductive layers 340, 342 are connected to a resistor 370 (
In one embodiment, the one or more resistors 370 are recessed from the MFS 212, as shown in
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The data storage device including the MAMR write head having a non-magnetic conductive structure provides additional paths for electrical currents to flow to the STO. The non-magnetic conductive structure enables higher current density to the STO without creating hot spots at the MFS. Maximum current efficiency and uniformity can be achieved with the non-magnetic conductive structure.
While the foregoing is directed to embodiments of the present disclosure, other and further embodiments of the disclosure may be devised without departing from the basic scope thereof, and the scope thereof is determined by the claims that follow.
This application is a divisional of co-pending U.S. patent application Ser. No. 16/015,163, filed Jun. 21, 2018, which application claims priority to U.S. Provisional Patent Application Ser. No. 62/606,128, filed on Jun. 23, 2017, each of which herein is incorporated by reference.
Number | Name | Date | Kind |
---|---|---|---|
8472135 | Kusukawa et al. | Jun 2013 | B1 |
8582240 | Chen et al. | Nov 2013 | B1 |
8879295 | Barth, Jr. et al. | Nov 2014 | B1 |
9001444 | Contreras et al. | Apr 2015 | B1 |
9064508 | Shiimoto et al. | Jun 2015 | B1 |
9196271 | Shirotori et al. | Nov 2015 | B1 |
9230571 | Chen et al. | Jan 2016 | B1 |
9230573 | Etoh et al. | Jan 2016 | B1 |
9275672 | Shiroishi et al. | Mar 2016 | B2 |
9311934 | Shiimoto et al. | Apr 2016 | B1 |
9368135 | Gao | Jun 2016 | B2 |
9378759 | Nagasaka | Jun 2016 | B2 |
9747932 | Taguchi | Aug 2017 | B1 |
9881637 | Wilson et al. | Jan 2018 | B1 |
9899042 | Venugopal et al. | Feb 2018 | B1 |
10032470 | Degawa | Jul 2018 | B1 |
10121497 | Takahashi et al. | Nov 2018 | B1 |
10186284 | Narita et al. | Jan 2019 | B2 |
10236021 | Narita et al. | Mar 2019 | B2 |
10276193 | Narita et al. | Apr 2019 | B2 |
10325618 | Wu et al. | Jun 2019 | B1 |
10366714 | Olson et al. | Jul 2019 | B1 |
10446178 | Tang et al. | Oct 2019 | B1 |
10546600 | Koizumi | Jan 2020 | B1 |
10580441 | Chen | Mar 2020 | B1 |
10714126 | Matsumoto | Jul 2020 | B2 |
10762917 | Le et al. | Sep 2020 | B1 |
10839829 | Sasaki | Nov 2020 | B1 |
10997988 | Le | May 2021 | B1 |
11011193 | Wu | May 2021 | B1 |
11049513 | Le | Jun 2021 | B1 |
20080268291 | Akiyama et al. | Oct 2008 | A1 |
20080304176 | Takagishi et al. | Dec 2008 | A1 |
20090059423 | Yamada et al. | Mar 2009 | A1 |
20090310244 | Shimazawa et al. | Dec 2009 | A1 |
20110038080 | Alex et al. | Feb 2011 | A1 |
20110096443 | Zhang | Apr 2011 | A1 |
20110279921 | Zhang | Nov 2011 | A1 |
20110293967 | Zhang | Dec 2011 | A1 |
20120126905 | Zhang | May 2012 | A1 |
20130027803 | Tanabe et al. | Jan 2013 | A1 |
20130057983 | Tanabe et al. | Mar 2013 | A1 |
20130250456 | Yamada et al. | Sep 2013 | A1 |
20140139952 | Takeo et al. | May 2014 | A1 |
20140177100 | Sugiyama et al. | Jun 2014 | A1 |
20140313616 | Kusukawa et al. | Oct 2014 | A1 |
20150015992 | Funayama | Jan 2015 | A1 |
20150310881 | Koui | Oct 2015 | A1 |
20160027455 | Kudo et al. | Jan 2016 | A1 |
20170047084 | Funayama et al. | Feb 2017 | A1 |
20170061995 | Taguchi et al. | Mar 2017 | A1 |
20170148471 | Tabata et al. | May 2017 | A1 |
20170236537 | Murakami et al. | Aug 2017 | A1 |
20180268848 | Narita et al. | Sep 2018 | A1 |
20190088274 | Narita et al. | Mar 2019 | A1 |
20190088275 | Narita et al. | Mar 2019 | A1 |
20190251991 | Le et al. | Aug 2019 | A1 |
20190251992 | Ho | Aug 2019 | A1 |
20190279663 | Song | Sep 2019 | A1 |
20200082845 | Suto et al. | Mar 2020 | A1 |
20200090685 | Takagishi et al. | Mar 2020 | A1 |
20210012794 | Tang | Jan 2021 | A1 |
Number | Date | Country |
---|---|---|
104835510 | Nov 2017 | CN |
2013251042 | Dec 2013 | JP |
2018156709 | Oct 2018 | JP |
2019057338 | Apr 2019 | JP |
2015126326 | Aug 2015 | WO |
Entry |
---|
Mallary et al. “Head and Media Challenges for 3 Tb/in2 Microwave-Assisted Magnetic Recording,” IEEE Transactions on Magnetics, vol. 50, No. 7, Jul. 2014, 8 pages. |
Zhang et al. “State Diagram of Spin-Torque Oscillator with Perpendicular Reference Layer and Planar Field Seneration Layer,” Science Direct, Progress in Natural Science: Materials International 25, 2015, pp. 258-262. |
Number | Date | Country | |
---|---|---|---|
20210233559 A1 | Jul 2021 | US |
Number | Date | Country | |
---|---|---|---|
62606128 | Jun 2017 | US |
Number | Date | Country | |
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Parent | 16015163 | Jun 2018 | US |
Child | 17229560 | US |