The present invention relates to magnetoresistive sensors and more particularly to a sensor manufactured by a process that allows the sensor to be formed with a very small magnetic read width.
The heart of a computer is an assembly that is referred to as a magnetic disk drive. The magnetic disk drive includes a rotating magnetic disk, write and read heads that are suspended by a suspension arm adjacent to a surface of the rotating magnetic disk and an actuator that swings the suspension arm to place the read and write heads over selected circular tracks on the rotating disk. The read and write heads are directly located on a slider that has an air bearing surface (ABS). The suspension arm biases the slider into contact with the surface of the disk when the disk is not rotating, but when the disk rotates air is swirled by the rotating disk. When the slider rides on the air bearing, the write and read heads are employed for writing magnetic impressions to and reading magnetic impressions from the rotating disk. The read and write heads are connected to processing circuitry that operates according to a computer program to implement the writing and reading functions.
The write head includes at least a coil, a write pole and one or more return poles. When a current flows through the coil, a resulting magnetic field causes a magnetic flux to flow through the write pole, which results in a magnetic write field emitting from the tip of the write pole. This magnetic field is sufficiently strong that it locally magnetizes a portion of the adjacent magnetic disk, thereby recording a bit of data. The write field, then, travels through a magnetically soft under-layer of the magnetic medium to return to the return pole of the write head.
A magnetoresistive sensor such as a Giant Magnetoresistive (GMR) sensor, or a Tunnel Junction Magnetoresisive (TMR) sensor can be employed to read a magnetic signal from the magnetic media. The sensor includes a nonmagnetic conductive layer (if the sensor is a GMR sensor) or a thin nonmagnetic, electrically insulating barrier layer (if the sensor is a TMR sensor) sandwiched between first and second ferromagnetic layers, hereinafter referred to as a pinned layer and a free layer. Magnetic shields are positioned above and below the sensor stack and can also serve as first and second electrical leads so that the electrical current travels perpendicularly to the plane of the free layer, spacer layer and pinned layer (current perpendicular to the plane (CPP) mode of operation). The magnetization direction of the pinned layer is pinned perpendicular to the air bearing surface (ABS) and the magnetization direction of the free layer is located parallel to the ABS, but free to rotate in response to external magnetic fields. The magnetization of the pinned layer is typically pinned by exchange coupling with an antiferromagnetic layer.
When the magnetizations of the pinned and free layers are parallel with respect to one another, scattering of the conduction electrons is minimized and when the magnetizations of the pinned and free layer are antiparallel, scattering is maximized. In a read mode the resistance of the spin valve sensor changes about linearly with the magnitudes of the magnetic fields from the rotating disk. When a sense current is conducted through the spin valve sensor, resistance changes cause potential changes that are detected and processed as playback signals.
In the push to increase data density sensors have been required to be formed with ever narrower read widths. The read width can be determined by the width of the layers such as the electrically conductive spacer or barrier layer sandwiched between the pinned and free layers. However, certain manufacturing limitations have prevented further narrowing of the read width. Therefore, there remains a need for a method for reducing the read width of a magnetoresistive sensor in order to further increase track density and data density.
The present invention provides a method for manufacturing a magnetic read head having a very narrow track width. The method includes depositing a plurality of sensor layers, depositing a non-Si-containing photoresist, patterning the photoresist and performing an ion milling to define a magnetic read head.
The use of the non-Si-containing photoresist advantageously allows the sensor to be formed with a narrow track width than would be possible with a Si-containing photoresist as was previously used in the construction of magnetic read heads. This is because the non-Si-containing photoresit has better resolution and improved depth of focus as compared with the previously used Si-containing photoresist. The non-Si containing photoresist also provides tolerance of high temperatures such as those needed for atomic layer deposition and chemical vapor deposition.
Certain manufacturing process changes that make possible the use of a non-Si-containing resist include the use of a Si containing Bottom Anti-Reflective Coating beneath the non-Si-containing photoresist to improve RIE selectivity during the image transfer process. In addition, adding a noble gas to the CO, chemistry of the reactive ion etching (during image transfer) helps to avoid early consumption of the non-Si-containing photoresist. A glancing ion milling assisted CMP liftoff process can also be useful in removing the remaining mask layers at very small sensor widths, which may not be possible using CMP alone.
These and other features and advantages of the invention will be apparent upon reading of the following detailed description of preferred embodiments taken in conjunction with the Figures in which like reference numerals indicate like elements throughout.
For a fuller understanding of the nature and advantages of this invention, as well as the preferred mode of use, reference should be made to the following detailed description read in conjunction with the accompanying drawings which are not to scale.
The following description is of the best embodiments presently contemplated for carrying out this invention. This description is made for the purpose of illustrating the general principles of this invention and is not meant to limit the inventive concepts claimed herein.
Referring now to
At least one slider 113 is positioned near the magnetic disk 112, each slider 113 supporting one or more magnetic head assemblies 121. As the magnetic disk rotates, 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 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 slider 113 against 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 storage system, 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. The air bearing thus counter-balances the slight spring force of suspension 115 and supports slider 113 off and slightly above the disk surface by a small, substantially constant spacing during normal operation.
The various components of the disk storage system 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 121 by way of recording channel 125.
With reference to
The sensor stack 302 can include a non-magnetic layer 308 that is sandwiched between a magnetic pinned layer structure 310 and a magnetic free layer structure 312. The non-magnetic layer 308 can be an electrically conductive material, if the sensor 300 is a Giant Magnetoresistive (GM R) sensor, and can be a thin electrically insulating material layer if the sensor structure 300 is a Tunnel Junction Sensor (TMR).
The pinned layer structure 310 can include first and second magnetic layers 314, 316 with a non-magnetic, antiparallel coupling layer such as Ru 318 sandwiched between the first and second magnetic layer 314, 318. The first magnetic layer 314 has its magnetization pinned in a first direction perpendicular to the ABS. This pinning is a result of exchange coupling with a layer of antiferromagnetic material 320 such as IrMn. The second magnetic layer 316 has its magnetization pinned in a second direction that is antiparallel with the first direction as a result of antiparallel coupling between the first and second magnetic layers 314, 316 across the antiparallel coupling layer 318.
The magnetic free layer 312 has a magnetization that is biased in a direction that is generally parallel with the ABS, but that is free to move in response to a magnetic field. The biasing of the free layer is provided by a magnetostatic coupling with first and second hard magnetic bias layers 322, 324. One or more seed layers 326 may be provided at the bottom of the sensor stack 302 in order to ensure a desired grain growth of the other layers of the sensor stack 302 deposited thereon. In addition a capping layer such as Ta 328 may be provided at the top of the sensor stack to protect the underlying layers during manufacture. In addition, thin insulation layers 330 is provided at either side of the sensor stack 302 and across at least the bottom lead/shield 304 in order to prevent sense current from being shunted through the magnetic bias layers 322, 324. The sensor structure 300 has a read width 322 that is determined by the width of the layers of the sensor stack 302, and especially by the width of the layers at the location of the spacer layer 308. This read width 332 can be advantageously made very small by a novel manufacturing process that will be described herein below. It should be pointed out that the sensor structure 300 is by way of example as various other forms of sensor structure could also be manufactured by the method of the present invention and would fall within the scope of the invention as well.
A basic requirement to achieve higher areal density is to reduce the physical magnetic read width 332 of the sensor 300. One method that has been used to define the read width of sensors is to use reactive ion etching (RIE) to image transfer a photo resist mask into an ion mill hard mask and then use the ion mill to pattern the hard mask image into the sensor. The success of this method requires that the photoresist mask height is sufficient to be image transferred into the ion mill hardmask. At widths of 40 nm or greater, the current lithographic approach is to use a silicon-containing photoresist to serve as an effective imaging layer to pattern a hardmask that consists of a material such as DURIMIDE® and carbon. A major advantage of silicon containing imaging resists is RIE selectivity. In the presence of O2 or CO2 RIE chemistries, the Si component of the imaging photoresist will oxidize to form SiO2. In this form, the imaging photoresist will be resistant to further etching and, therefore, will effectively allow the patterning of the hard mask and subsequently the patterning of the sensor. After patterning of the sensor, ALD alumina deposition is done followed by hard bias.
There is, however, a drawback to the above process for use in defining sensors having very small read widths. At magnetic read widths smaller than 40 nm, major challenges with the silicon-containing resist result in an inability to further reduce the read width. This is mostly due to the photoresist reaching its resolution limit and to poor depth of focus properties of the Si-containing photoresist, which results in more line-edge roughness and not enough imaging photoresist to successfully image transfer the photoresist pattern into the hard mask.
A layer of photoresist 408 is then deposited over the mask 406. This photoresist layer 408 is a non-Si containing photoresist, such as JSR 1891 which is available from JSR MICRO, INC®. Such a non-Si containing photoresists achieves higher resolution than previously used Si containing resists. In addition, such non-Si containing photoresists have a higher heat resistance, which is necessary to withstand chemical vapor deposition (CVD) and/or atomic layer deposition (ALD) processes such as will be used in the construction of the read sensor structure as will be described herein below. Such non-Si containing photoresists also achieve better depth of focus than Si-containing photoresists. Such a non-Si-containing photoresist also has a better dissolution rate than previously used photoresist, has similar reactive ion etching selectivity to optional DLC and BARC materials (described below) and, perhaps most importantly, is soluble in NMP solution, which will further assist in liftoff at smaller read widths.
With reference now to
With reference now to
It can be seen in
The mask layers 408 can be removed by a chemical liftoff process such as by coating with a hot NMP solution (N-Methyl Pyrrolidone) followed by snow cleaning (high pressure CO, spray) to remove resist and fences. However, in order for such a liftoff process to work, the NMP solution must be able to reach the mask 408. This means that a certain amount of the layers 702, 704 must be removed or exposed to allow the NMP solution to access the mask 408.
A wrinkle bake step can be used to form cracks where NMP can reach the mask to remove a greater portion of materials of the mask layers 408 in the field and grid areas. Liftoff is further enhanced by the use of the non-Si-containing resist, which is soluble in NMP. Due to re-deposition that formed during ion milling, in the track area it can be difficult to remove the mask layers at small dimensions. A chemical mechanical polishing process can be used to remove the portion of the layers 704, 702 that extend over the mask 408. This would require either inserting a CMP stop layer such as Ta with Rh, Ru or Ir during the hard magnetic material deposition or separately such as DLC. While CMP assisted lift-off is a preferred method at wider read width dimensions, at very narrow dimensions an ion milling assisted lift-off (UM) can also be used in conjunction with CMP to remove the layers 704, 702 that extend over the mask 408.
In this case an ion milling process in conjunction with CMP can be used to provide access to the mask 408 for the chemical liftoff. If ion milling is used, a bi-layer consisting of a CMP stop layer 706 and an ion milling resistant layer 708 is deposited on the top layer of the hard magnetic material 704. The ion milling resistant layer 708 protects the CMP stop layer 706 on the flat portion of the hard bias layer 704 during ion milling assisted lift-off. The ion milling resistant layer 708 is later removed during CMP. The CMP's slurry will remove the ion milling resistant layer. Materials suitable for use as a CMP stop layer 406 are Rh, Ir, and Ru. Examples of suitable materials for an ion milling resistant layer 708 include Ta, Al2O3, Si3N4, SiO2, Ta2O5 or DLC.
With reference to
A NMP solution 901 may then be applied as shown in
The above description illustrates a method for manufacturing a narrow read-width magnetoresistive sensor using a single layer mask of non-silicon containing resist. A mask with an optional Bottom Anti-Reflective Coating (BARC) formed over a CMP stop layer can also be constructed as will be described herein below.
With reference now to
Then, the photoresist layer is photolithographically patterned to form a read width defining mask as shown in
With reference now to
With reference now to
However, as discussed previously, an optional ion milling assisted lift-off in conjunction with CMP can be used to remove the remaining mask 1304 at very small sensor widths. Again, if such an ion milling assisted lift off process is performed, a second layer of CMP resistant material 1606 is deposited, followed by a layer of ion milling resistant material 1608. The materials for layers 1606, 1608 can be the same materials described above with reference to layers 706, 708 of
A tri-layer mask 2102 is deposited over the sensor layers 404 and CMP stop layer 406. The tri-layer mask includes a release layer 2104 formed at the bottom of the mask structure 2102. The release layer can be a soluble polyimide material such as DURIMIDE® and in addition to functioning as a release layer for assisting in lifting off the mask 2102 also functions as an image transfer layer. A bottom antireflective coating (BARC) 2106 is deposited over the release layer 2104. The BARC layer 2106 can be a Si containing BARC or can be a carbon-only BARC. A non-silicon containing photoresist layer 2108 is deposited over the BARC 2106. A major function of the BARC is to improve resolution of the imaging of the photoresist layer 2106 and may also improve RIE selectivity between the BARC layer 2106 and the release layer 2104. RIE selectivity allows for adjustment of the height of the release/image-transfer layer 2104 to serve as an effective hard mask to pattern the sensor layers 404 and assist in lift-off. A BARC 2106 consisting of carbon only is used to improve photoresist resolution and also reduce faceting during RIE, while silicon containing BARC offers better imaging resolution and also RIE selectivity between the BARC 2106 and the underlying lift off layer 2104.
With reference to
A thin insulation layer such as alumina 2502 is then deposited, preferably by chemical vapor deposition or atomic layer deposition, and a hard magnetic material 2504 is deposited over the insulation layer 2502, leaving a structure as shown in
An ion milling is performed at a glazing angle as indicated by arrows 2602. This glazing angle is nearly perpendicular to normal or nearly parallel with the planes of the deposited layers. For example, the glazing ion milling can be performed at an angle of 0-30 degrees relative to the planes of the as deposited layers as much as possible without damage to the substrate fixture. This removes the magnetic material 2504 from the sides of the sensor 2104 as shown in
While various embodiments have been described above, it should be understood that they have been presented by way of example only and not limitation. Other embodiments falling within the scope of the invention may also become apparent to those skilled in the art. Thus, the breadth and scope of the invention should not be limited by any of the above-described exemplary embodiments, but should be defined only in accordance with the following claims and their equivalents.