Multilayer Structure for Reducing Film Roughness in Magnetic Devices

Abstract

A seed layer stack with a uniform top surface having a peak to peak roughness of 0.5 nm is formed by sputter depositing an amorphous layer on a smoothing layer such as Mg where the latter has a resputtering rate 2 to 30 that of the amorphous layer. The uppermost seed (template) layer is NiW, NiMo, or one or more of NiCr, NiFeCr, and Hf while the bottommost seed layer is one or more of Ta, TaN, Zr, ZrN, Nb, NbN, Mo, MoN, TiN, W, WN, and Ru. Accordingly, perpendicular magnetic anisotropy in an overlying magnetic layer is substantially maintained during high temperature processing up to 400 C. and is advantageous for magnetic tunnel junctions in embedded MRAMs, spintronic devices, or in read head sensors. The amorphous seed layer is SiN, TaN, or CoFeM where M is B or another element with a content that makes CoFeM amorphous as deposited.

Claims

1. A multilayer structure for reducing film roughness in a magnetic device, comprising: (a) a buffer layer that is one or more of Zr, ZrN, Nb, NbN, Mo, MoN, TiN, W, WN, and Ru, or one of more of the aforementioned materials with Ta or TaN that is formed on a substrate; (b) a first smoothing layer (S1) made of a material with a first bond energy, and having a first surface with an as deposited first peak to peak roughness, the S1 layer is formed on the buffer layer; (c) a second smoothing layer (S2) that is non-crystalline or nano-crystalline and is made of a material with a second bond energy that is greater than the first bond energy such that deposition of the S2 layer results in resputtering of the S1 layer to give a S1 layer with a second surface having a second peak to peak roughness substantially less than the as deposited first peak to peak roughness, and the S2 layer formed on the second surface, the upper second layer has a third surface with the second peak to peak roughness; and (d) an uppermost template layer with a top surface having the second peak to peak roughness, the template layer has a (111) crystal orientation to promote PMA in an overlying magnetic layer.

2. The multilayer structure of claim 1, wherein the overlying magnetic layer contacts the top surface of the template layer, and is a reference layer in a magnetic tunnel junction (MTJ) having a bottom spin valve configuration, or is a free layer in a MTJ with a top spin valve configuration.

3. The multilayer structure of claim 1, wherein the overlying magnetic layer is a reference layer, free layer, or dipole layer in a magnetic random access memory (MRAM) device, spin torque oscillator (STO), spintronic device, or a read head sensor.

4. The multilayer structure of claim 2, wherein the MTJ has the bottom spin valve configuration and is further comprised of a tunnel barrier on the reference layer, a free layer on the tunnel barrier layer, and an uppermost capping layer.

5. The multilayer structure of claim 2, wherein the MTJ has the top spin valve configuration and is further comprised of a tunnel barrier on the free layer, a reference layer on the tunnel barrier layer, and an uppermost capping layer.

6. The multilayer structure of claim 4, wherein the reference layer has a synthetic antiparallel (SyAP) configuration with an AP2 layer contacting the top surface of the template layer, a middle anti-ferromagnetic coupling layer, and an uppermost AP1 layer.

7. The multilayer structure of claim 5, wherein the reference layer has a synthetic antiparallel (SyAP) configuration with an AP1 layer contacting a top surface of the tunnel barrier layer, a middle anti-ferromagnetic coupling layer, and an uppermost AP2 layer.

8. The multilayer structure of claim 1 wherein the overlying magnetic layer comprises a laminated stack (D/X).sub.n where D is Co, CoFe, or CoFeR, X is Pt, Pd, Ni, NiCo, Ni/Pt, or NiFe, n is from 2 to 30, and R is one of Mo, Mg, Ta, W, or Cr.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0020] FIG. 1 is a cross-sectional view of a seed layer stack in the prior art where a rough top surface in the bottom buffer layer is reproduced in the upper template layer.

[0021] FIG. 2 is a cross-sectional view of the seed layer stack with four layers formed according to an embodiment of the present disclosure.

[0022] FIG. 3a is a cross-sectional view of the seed layer stack in FIG. 2 wherein the bottommost buffer layer is omitted according to a second embodiment of the present disclosure.

[0023] FIG. 3b is a cross-sectional view of a seed layer stack wherein the high resputtering rate and low resputtering rate (amorphous) layers are repeated according to another embodiment of the present disclosure.

[0024] FIG. 4 is a cross-sectional view of a magnetic tunnel junction (MTJ) with a bottom spin valve configuration, and containing a seed layer stack formed according to an embodiment of the present disclosure.

[0025] FIG. 5 is a cross-sectional view of a MTJ with a top spin valve configuration and a seed layer stack formed according to an embodiment of the present disclosure.

[0026] FIG. 6 is a cross-sectional view of a MTJ with a bottom spin valve configuration and including a dipole layer according to an embodiment of the present disclosure.

[0027] FIG. 7 depicts a process of sputter depositing an amorphous seed layer on a seed layer with a higher resputtering rate according to an embodiment of the present disclosure.

[0028] FIG. 8 is a plot of Kerr signal vs. PMA field for a conventional seed layer/reference layer stack, and for a seed layer stack/reference layer of the present disclosure after a 400 C., 30 minute anneal.

[0029] FIG. 9 is a plot of Kerr signal vs PMA field for the samples in FIG. 7 after an additional anneal of 390 C. for 300 minutes.

DETAILED DESCRIPTION

[0030] The present disclosure is a MTJ wherein at least one of a free layer, reference layer, or dipole layer has perpendicular magnetic anisotropy that is maintained during 400 C. processing in magnetic devices such as embedded MRAM and STT-MRAM, in spintronic devices such as microwave assisted magnetic recording (MAMR) and spin torque oscillators (STO), and in various spin valve designs including those found in read head sensors. PMA is maintained by depositing the magnetic layer on a seed layer stack wherein an uppermost template layer has an unusually smooth top surface made possible by deposition of the template layer on a smoothing layer comprised of a lower seed layer with high resputtering rate and an upper amorphous layer with a low resputtering rate as described herein. The seed layer stack may be used in devices based on bottom spin valve, top spin valve, or dual spin valve designs as appreciated by those skilled in the art.

[0031] Referring to FIG. 1, a cross-sectional view is shown of a seed layer stack formerly fabricated by the inventors. The seed layer is formed on a substrate such as a bottom electrode 10 in a MRAM device, and has a bottom layer called a buffer layer 20 that is used for good adhesion to the substrate. Ta or TaN are commonly selected for the buffer layer, which tends to have considerable roughness at its top surface 20t. In another embodiment, the buffer layer may be one or more of Ta, TaN, Zr, ZrN, Nb, NbN, Mo, MoN, TiN, W, WN, and Ru. An upper template layer 23 made of NiW, NiMo, NiCr, NiFeCr, Hf, Hf/NiCr, Hf/NiFeCr, NiCr/Hf, or NiFeCr/Hf is conformally deposited on the buffer layer, and has a (111) crystal structure in order to promote a fcc (111) crystal orientation in an overlying (Co/X).sub.n multilayer. As a result, the significant roughness in top surface 20t is essentially duplicated in the top surface of the template layer where peaks 23s1 are separated by valleys 23s2 in the film. The substantial peak to peak roughness in the template layer top surface is associated with a loss in PMA in an overlying magnetic layer (not shown) such as a reference layer, free layer, or dipole layer during high temperature processing. Peak to peak roughness is defined as the average difference in the z-axis direction between peaks 23s1 and is about 2 nm over a range r of 100 nm.

[0032] Previously, we described in related U.S. Pat. No. 8,871,365 how thermal stability in a reference layer and free layer may be improved with a RL1/DL1/Ru/DL2/RL2 or FL1/DL1/Ru/DL2/FL2 configuration, respectively, where R1 and R2 (or FL1 and FL2) are two magnetic layers with PMA that are antiferromagnetically coupled through a middle Ru layer. Dusting layers (DL1 and DL2) such as Co or CoFe are responsible for enhancing thermal stability compared with a RL or FL having a R1/Ru/R2, or FL1/Ru/FL2 stack, respectively.

[0033] We also disclosed in related U.S. Pat. No. 8,541,855 how a Hf/NiCr or Hf/NiFeCr seed layer improves PMA in an overlying (Co/Ni) multilayer. Furthermore, in U.S. Pat. No. 9,490,054, we disclosed how a TaN/Mg/NiCr seed layer stack promotes higher PMA in an overlying magnetic layer. Now we have discovered that PMA in a (Co/Ni).sub.n laminate or the like may be maintained during high temperature processing to about 400 C. by a stack of seed layers which promote a more uniform top surface on the uppermost template layer. In this context, the term about 400 C. means the temperature may exceed 400 C. by 10-20 C. for a certain period of time due to temperature fluctuations or excursions in the chamber where an annealing or deposition process is performed.

[0034] According to a first embodiment depicted in FIG. 2, the seed layer stack 24 of the present disclosure includes a bottom layer 20 and an uppermost template layer 23 as previously described. However, a key feature is a so-called smoothing layer structure having a stack of layers 21/22 where second layer 21 is made of a material with a high resputtering rate that is formed on a top surface 20t of the bottommost layer. Layer 21 preferably is one or more of Mg, Al, Si, C, B, Mn, Rb, Zn, and Ti with a thickness from 3 to 100 Angstroms, and preferably 3 to 20 Angstroms. Non-crystalline or nano-crystalline (grain size <5 nm) layer 22 is made of TaN, SiN, or CoFeM where M is one of B, P, Ta, Zr, Si, Cu, Hf, Mo, W, and Nb with an M content that results in amorphous character for the CoFeM alloy. Preferably, the CoFeM alloy is amorphous as deposited. Layer 22 has a thickness from 1 to 100 Angstroms, and preferably 2 to 15 Angstroms, and has a lower resputtering rate than second layer 21 such that layer 21 has a resputtering rate from 2 to 30 times that of layer 22.

[0035] As defined herein, resputtering rate is related in part to bond energy, which is the energy needed to break apart bonded atoms. Therefore, a material with a low bond energy is easy to resputter and has a higher resputtering rate than a material with a higher bond energy. For example, the bond energy of MgMg is 11.3 kJ/mol while the bond energy of FeFe is 118 kJ/mol and of CoCo is about 127 kJ/mol according to a table of values found in Comprehensive Handbook of Chemical Bond Energies, Y. Luo, CRC Press, Boca Raton, Fla., 2007. It follows that the bond energy ratio between Mg and CoFe (or CoFeB) is about 1:10 to give a resputtering rate for Mg that is about 10 times greater than that for CoFe. Thus, the material in layer 21 has a first bond energy that is less than a second bond energy for the material in layer 22.

[0036] A second important factor in determining resputtering rate is the atomic number (Z) of an element. In particular, materials in layer 21 are more easily displaced during deposition of layer 22 when the material for the non-crystalline or nano-crystalline layer has a higher weight (larger Z value) than the element or alloy selected for layer 21. Accordingly, a greater resputtering rate ratio (layer 21/layer 22) is achieved with a condition where layer 21 is an element or alloy with both of a lower Z value and smaller bond energy than the material in layer 22.

[0037] As a result of the resputtering rate (bond energy) difference, when the non-crystalline or nano-crystalline material is deposited as depicted in the deposition sequence found in FIG. 7, atoms of second layer 21 are displaced from a top surface of the second seed layer and are replaced by a more uniform film of layer 22. In other words, an as deposited top surface 21r of the second layer with a peak to peak roughness v1 becomes a smooth top surface 21t with substantially less roughness as layer 22 is deposited thereon. Peak to peak roughness v2 between peaks 22t has been observed to be only 0.5 nm over a 100 nm range r, and is substantially less than a peak to peak roughness v1 of about 2 nm over a 100 nm range for top surface 21r prior to deposition of layer 22.

[0038] Returning to FIG. 2, top surfaces 21t, 22t of layers 21 and 22, respectively are shown with a relatively smooth profile compared with the uneven (rough) top surface 20t of the bottom seed layer 20. Furthermore, the smooth top surface 22t is essentially reproduced in top surface 23t of the uppermost template layer 23 that typically conforms to the top surface of the underlying layer. As stated previously, the term smooth when referring to a top surface 23t may be described in terms of a peak to peak roughness over a range of 100 nm. In this case, a TEM measurement indicates a peak to peak roughness in top surface 23t of about 0.5 nm, which represents a substantial improvement over the 2 nm value for peak to peak roughness for peaks 23s1 of the template layer in the FIG. 1 reference.

[0039] In a second embodiment illustrated in FIG. 3a, bottom layer 20 may be omitted to provide a seed layer stack 25-1 where the high resputtering rate layer 21 contacts a top surface of the substrate 10. As a result of depositing the non-crystalline or nano-crystalline layer 22, both seed layers in the smoothing layer stack have smooth top surfaces 21t, 22t similar to that found for the template layer as described previously for the first embodiment. Thus, the seed layer stack 25-1 is a trilayer with a 21/22/23 configuration where template layer 23 has a top surface 23t and a peak to peak roughness v2 that is attributed to maintaining PMA in an overlying magnetic layer after processing at temperatures as high as 400 C. as supported by data provided in a later section.

[0040] The present disclosure also anticipates the smoothing layer stack 21/22 may be repeated to give a laminate consisting of alternating layers 21 and 22. A third embodiment is depicted in FIG. 3b where a first high resputtering rate layer 21a is formed on the substrate 10. Above layer 21a is formed sequentially a first low resputtering rate layer 22a, a second high resputtering rate layer 21b, and a second low resputtering rate layer 22b, and a template layer 23 to give a 21a/22a/21b/22b/23 configuration for seed layer stack 25-2. The bond energy for the material in layers 21a, 21b is less than that of the material in layers 22a, 22b. In some embodiments, layers 21a, 21b may be made of the same element or alloy, and layers 22a, 22b are selected from the same material. However, the present disclosure anticipates that layer 21a may have a different composition than layer 21b, and layer 22a may have a different composition than layer 22b.

[0041] It is believed that the third embodiment provides a further improvement in top surface 23t uniformity compared with the previous embodiments. In this seed layer design, each high resputtering rate layer preferably has a thickness from 3 to 20 Angstroms, and each low resputtering rate layer 22a, 22b with amorphous character preferably has a thickness of 2 to 15 Angstroms. It should be understood that the seed layer structure in the first embodiment may be modified accordingly to insert the aforementioned laminated smoothing layer instead of one of each layer 21, 22 between layers 20 and 23 in stack 24. Moreover, there may be more than one repeat of layers 21, 22 in a smoothing layer stack.

[0042] The present disclosure also encompasses a magnetic tunnel junction (MTJ) element comprising a seed layer stack formed according to one of the embodiments described herein. In the exemplary embodiments, a bottom spin valve and top spin valve are depicted. However, the seed layer embodiments described herein may be implemented in other spin valve designs including a dual spin valve structure as appreciated by those skilled in the art.

[0043] Referring to FIG. 4, MTJ 1 is formed between a substrate 10 that may be a bottom electrode, and a top electrode 30. A bottom spin valve configuration is shown wherein the seed layer stack 24, a reference layer 26, tunnel barrier 27, free layer 28, and capping layer 29 are sequentially formed on the substrate. In one preferred embodiment, the reference layer (RL) has a synthetic antiparallel (SyAP) stack with an AP2 layer 26a contacting a top surface of the seed layer, a middle coupling layer 26b such as Ru, and an uppermost AP1 layer 26c. Preferably, both of the AP2 and AP1 layers have PMA such that magnetization 26m1, 26m2, respectively, are aligned in a direction perpendicular to the planes of the MTJ layers. PMA in each of the AP2 and AP1 layers may be intrinsic and derived from a laminated stack (Co/X).sub.n where X is Pt, Pd, Ni, NiCo, Ni/Pt, or NiFe, and n is from 2 to 30. In another aspect, CoFe or CoFeR may replace Co in the laminated stack and R is one of Mo, Mg, Ta, W, or Cr. The smooth template layer formed on the top surface of the non-crystalline or nano-crystalline layer is advantageously used to maintain PMA in the reference layer after high temperature processing up to about 400 C. In alternative embodiments, seed layer stack 25-1 or 25-2 is substituted for stack 24.

[0044] In other embodiments, the reference layer 26 may have a SyAP configuration represented by RL1/DL1/Ru/DL2/RL2 as disclosed in related U.S. Pat. No. 8,871,365. In the present disclosure, R1 corresponds to the AP2 layer and R2 is the AP1 layer described above that are antiferromagnetically coupled through the Ru layer.

[0045] There may be a transition layer (not shown) such as CoFe/Co or CoFeB/Co formed between the uppermost laminated layer in a (Co/X).sub.n stack and the tunnel barrier 27. According to one embodiment, the transition layer is formed between the (111) AP1 layer and a (100) MgO tunnel barrier, and is sufficiently thin to preserve the PMA property of the AP1 layer and yet thick enough to provide a high magnetoresistance (MR ratio). Co is preferably used as the uppermost layer in a transition layer and forms an interface with the tunnel barrier layer since it is more resistant to oxidation than a CoFeB or CoFe layer. The transition layer, when present, is considered part of the reference layer 26 because of the magnetic character in the CoFe/Co and CoFeB/Co layers.

[0046] A tunnel barrier 27 is formed on the reference layer 26. The tunnel barrier is preferably an oxide, nitride, or oxynitride of one or more of Mg, MgZn, Ta, Ti, Zn, Al, or AlTi. The thickness and extent of oxidation in the metal oxide layer may be adjusted to tune the resistance x area (RA) value for the tunnel barrier. It is believed that the smoothness of the template layer top surface 23t is substantially duplicated in the overlying layers in MTJ 1 including the tunnel barrier.

[0047] A free layer/capping layer stack is formed on the tunnel barrier. The free layer 28 may be selected from one of the laminated compositions described with respect to the reference layer. In an alternative embodiment, the free layer may be one or more of Co, Fe, CoFe, and alloys thereof with one or both of Ni and B. In another aspect, a moment diluting layer (L) such as Ta or Mg is inserted in one of the aforementioned metals or alloys to give a CoFeB/L/CoFeB configuration, for example. Furthermore, the free layer (FL) may have a FL1/DL1/Ru/DL2/FL2 configuration where FL1 and FL2 are two magnetic layers or a laminate with PMA as previously described that are antiferromagnetically coupled through a middle Ru layer. DL1 and DL2 are dusting layers as explained earlier.

[0048] In some embodiments, the capping layer 29 is a metal oxide such as MgO or MgTaOx to enhance PMA in the free layer by inducing interfacial perpendicular anisotropy along an interface with the free layer. In other embodiments, the capping layer has an uppermost layer that is one or more of Ru and Ta to give a capping layer stack that is Ru/Ta/Ru or MgO/Ru/Ta, for example.

[0049] Referring to FIG. 5, a top spin valve embodiment shown as MTJ 2 is formed according to the present disclosure. Seed layer 24 (or 25-1 or 25-2) is formed on the substrate 10 and then free layer 28, tunnel barrier 27, reference layer 26, and capping layer 29 are sequentially laid down on the free layer. When the reference layer has a SyAP configuration, the AP1 layer 26c contacts the tunnel barrier and AP2 layer 26a is the uppermost layer in the reference layer stack. The free layer contacts the top surface 23t of the template layer in the seed layer stack and has a smooth top surface wherein the peak to peak thickness variation value associated with top surface 23t is believed to be substantially reproduced in the top surface 28t of the free layer. The free layer may comprise two magnetic layers FL1 28a and FL2 28c that are anti-ferromagnetically coupled through layer 28b that is preferably Ru. As a result, magnetization 28m1 and 28m2 in the FL1 and FL2 layers, respectively, are perpendicular to the plane of the layers and aligned in opposite directions. Each of FL1 and FL2 may be a (Co/X).sub.n laminate as described earlier with respect to the reference layer, or one or both of FL1, FL2 may be one or more of Co, Fe, CoFe, and alloys thereof with one or both of Ni and B. Furthermore, the free layer may have a FL1/DL1/Ru/DL2/FL2 configuration.

[0050] In another bottom spin valve embodiment illustrated in FIG. 6, MTJ 1 is modified to give MTJ 3 by inserting a second seed layer stack 25-1 and a PMA layer that serves as a dipole layer 32 between the free layer 28 and capping layer 29. Thus, the MTJ has a first seed layer (SL1) stack 24 (or 25-1 or 25-2) contacting a top surface of the substrate 10, and the second seed layer (SL2) stack contacting a top surface of a spacer 31 in a SL1/RL/tunnel barrier/FL/spacer/SL2/dipole layer/capping layer configuration. The spacer is a material including but not limited to one of Ta and Mg that getters oxygen from the free layer. The second seed layer stack that optionally is layer 24 or 25-2 is employed as an underlayer for the PMA layer to maintain the PMA therein after high temperature processing. The dipole layer is preferably a (Co/X).sub.n laminate with a composition that is one of the multilayers previously described with respect to layer 26 in MTJ 1.

[0051] The present disclosure also encompasses a method of forming the seed layer stack in the embodiments disclosed herein. All layers in the MTJ stack including the seed layers may be deposited in a DC sputtering chamber of a sputtering system such as an Anelva C-7100 sputter deposition system or the like that includes ultra high vacuum DC magnetron sputter chambers with multiple targets and at least one oxidation chamber. Typically, the sputter deposition process for the seed layer stack including the high resputtering rate layer 21 and low resputtering rate layer 22 involves an inert gas such as Ar and a base pressure between 510.sup.8 and 510.sup.9 torr. A lower pressure enables more uniform films to be deposited. The temperature in the sputter deposition chamber during deposition processes may vary from 100 K to 400 C., and the forward power applied to one or more targets to form each seed layer is usually in the range of 20 W to 5000 W.

[0052] The tunnel barrier and metal oxide (when included) for the capping layer are prepared by first depositing a first metal layer, oxidizing the first metal layer with a natural oxidation (NOX) or radical oxidation (ROX) process, and then depositing a second metal layer on the oxidized first metal layer. During a subsequent annealing step, oxygen migrates into the second metal layer to oxidize the second metal. In some embodiments, one or more additional metal layers are deposited in the tunnel barrier stack and each oxidized by a NOX or ROX process before an uppermost metal layer is deposited and then oxidized by way of annealing to generate tunnel barrier 27.

[0053] Once all of the layers in the MTJ are formed, an annealing process is performed that is comprised of a temperature between 330 C. and 400 C. for a period of 1 minute to 10 hours. Thereafter, the spin valve stack may be patterned to form a plurality of MTJ elements on the substrate 10 by a well known photolithography and etch sequence. In an embodiment where the substrate is a bottom electrode, the bottom electrode in some cases is patterned simultaneously with the overlying spin valve stack to enable a higher density of patterned structures for advanced technology designs.

Example 1

[0054] To demonstrate the advantages of the present disclosure, a (Co/Ni).sub.n multilayer stack with PMA where n=3 was fabricated on two different seed layers. The seed layer in the reference sample, which represents the FIG. 1 structure, has a TaN20/NiCr50 stack formed on a first wafer where the TaN thickness is 20 Angstroms and the NiCr thickness is 50 Angstroms. A second seed layer taken from the FIG. 2 embodiment has a TaN20/Mg7/CoFeB10/NiCr50 stack formed on a second wafer where Mg (7 Angstroms thick) is the high resputtering rate layer 21 and CoFeB (10 Angstroms thick) is the amorphous layer 22. Each wafer was annealed at 400 C. for 30 minutes and a Kerr microscope was used to measure a Kerr signal vs perpendicular field as illustrated in FIG. 8 where curve 50 is the signal from the reference wafer, and curve 51 is obtained from the wafer with the seed layer stack formed according to the first embodiment depicted in FIG. 2. The curves show PMA intensities that are essentially the same.

[0055] Thereafter, the wafers were annealed at 390 C. for 300 minutes and a second plot of Kerr signal vs. perpendicular field was obtained as shown in FIG. 9. There is only a slight degradation in PMA compared with the first Kerr measurement for the FIG. 2 embodiment according to curve 51a. However, the reference sample exhibits significant PMA degradation as a result of the second anneal step as indicated by curve 50a. Thus, the seed layer stack of the present disclosure is beneficial in substantially maintaining PMA in an overlying magnetic layer during prolonged heating at about 400 C. while the reference sample fails to maintain a substantial PMA during the same annealing period.

Example 2

[0056] In a second experiment that demonstrates the benefit of reduced peak to peak roughness in a template layer top surface provided by a seed layer stack of the present disclosure, a seed layer stack with a TaN20/Mg7/NiCr50 configuration previously fabricated by the inventors, and where the number following each layer is the thickness in Angstroms, was formed on a substrate. For comparison, a laminated smoothing layer having a 21a/22a/21b/22b stack according to the third embodiment was deposited and the TaN/Mg/NiCr seed layer stack deposited thereon to give a Mg25/CoFeB20/Mg50/CoFeB20/TaN20/Mg7/NiCr50 configuration. Each seed layer stack was evaluated by using a TEM to determine a peak to peak roughness of the uppermost NiCr layer top surface. We found the peak to peak roughness of 2 nm for the TaN/Mg/NiCr stack was significantly decreased to only 0.5 nm for the seed layer stack with the laminated smoothing layer. Therefore, a smoother template layer top surface is achieved by inserting a smoothing layer in the seed layer stack and is believed to be responsible for the advantage of substantially maintaining PMA in an overlying magnetic layer after high temperature processing such as annealing to about 400 C. for an extended period of time, typically 1 minute to 10 hours.

[0057] The seed layer stack of the embodiments described herein is formed by employing conventional processes and materials without any significant added cost and can readily be implemented in a manufacturing environment.

[0058] While this disclosure has been particularly shown and described with reference to, the preferred embodiment thereof, it will be understood by those skilled in the art that various changes in form and details may be made without departing from the spirit and scope of this disclosure.