3402 IEEE TRANSACTIONS ON MAGNETICS, VOL. 48, NO. 11, NOVEMBER 2012 Geometrically Planar Ion-Implant Patterned Magnetic Recording Media Using Block Copolymer Aided Gold Nanoisland Masks Chulmin Choi , Kunbae Noh , Duyoung Choi , Jirapon Khamwannah Daehoon Hong , Li-han Chen , and Sungho Jin , Chin-Hung Liu , Center for Magnetic Recording Research, University of California at San Diego, La Jolla, CA 92093 USA Mechanical & Aerospace Engineering, University of California at San Diego, La Jolla, CA 92093 USA Materials Science & Engineering, University of California at San Diego, La Jolla, CA 92093 USA We have developed patterned media via ion implantation using Au nano mask approach for local control of coercivity of magnetically multilayer film. Au nano-islands produced through a di-block copolymer templated technique is used as the mask for hard ion implantation. The sputter deposited multilayer film having vertical magnetic anisotropy is coated with a diblock copolymer layer, two phase decomposed into vertically pored nanostructure, then chemically processed to nucleate gold nanoislands corresponding to the diblock copolymer nanostructures. Subsequent nitrogen (N) ion implantation, using these Au islands as implantation-blocking masks, allows a patterned penetration of implanted ions into unmasked portion of the multilayer film, thus creating invisible but magnetically isolated bit island geometry while maintaining the overall flat configuration of the patterned media. Index Terms—Bit patterned media, nano-island. I. INTRODUCTION A S IS WELL known, bit patterned media (BPM) is one of the promising approaches to overcome the limitation of storage density in magnetic hard disk memory. The major advantages of BPM are firstly, the transition noise is eliminated because the bits are now defined by the physical location of the elements and not by the boundary between two oppositely magnetized (but physically in contact) regions of a thin film media [1]. Secondly, very high data densities can be obtained because the stability criterion now refers to the volume and anisotropy of the entire magnetic element, not to the individual grains comprising the conventional granular media. Each of the magnetic switching elements could therefore become as small as a few nanometers [2], [3], as compared to tens of nanometers. However, the formation of high-density, a few nanometers scale dot arrays is a challenging task for achieving a practical goal of ultrahigh-density data storage [4]–[6]. In particular, methods for producing isolated high-density magnetic nanoscale arrays with a pitch of 20 nm or less have been extensively studied with the aim of fabricating the next generation of patterned magnetic media with a recording and beyond [7]–[9]. Various fabricadensity of 1 tion techniques have been employed, such as those based on e-beam lithography (EBL), nano imprinting lithography (NIL), di-block copolymer (DBCP) and anodized aluminum oxide (AAO) [10]–[15]. One of the essential requirements for bit patterned media is the surface planarization so as to overcome the flying instability of the head-slider on topographically patterned surfaces having valleys and trenches. These extra steps can result in Manuscript received March 02, 2012; revised April 25, 2012 and May 16, 2012; accepted June 07, 2012. Date of current version October 19, 2012. Corresponding author: S. Jin (e-mail: jin@ucsd.edu). Color versions of one or more of the figures in this paper are available online at http://ieeexplore.ieee.org. Digital Object Identifier 10.1109/TMAG.2012.2204867 significantly increased cost and complexity of processing with potential implications on structural reproducibility and reliability issues. In order to produce flat patterned media without topographic features, filling of the recessed trench region , spin-on-glass, with non-magnetic material (e.g., with hydrogen silsesquioxane, etc.) followed by removal of the excess material (chemical mechanical polishing and reactive ion etching) has been the commonly used approach [16], [17]. Alternative methods are sought to produce bit patterned media without topographically protruding island geometry common to many lithography and self-assembly patterning techniques. Utilizing ion implantation damage is a promising technique for creating a topographically flat recording media. Well controlled ion implantation can cause the magnetization to be reduced subatantially depending on the dose and energy utilized to displace atoms by ion irradiation [18]. At suitable ion implantation levels, the lattice parameter and Curie temperature of the magnetic layer can be altered, which can lead to a reduction or disappearance of magnetization and anisotropy [19]. Among the various ions used for trials, nitrogen ion implantation seems to exhibit a promising trend of reducing the magnetization and anisotropy of [Co/Pd]n magnetic multilayers [20]. In this work, we have developed a convenient method for local control of coercivity of flat-surface planar magnetic recording media of [Co/Pd]n multilayer film. Because the available ion implantation dose and energy were such that the nitrogen implanting with Au mask particle alone damaged much of the magnetic material even with the Au nanoparticles, we utilized silica buffer layer to adjust the energy of the incoming ions and them weaker so as to induce more optimal implantation., instead of over-exposure of the magnetic layer to the ions. buffer layer was added on top of the 20–200 nm thick magnetic material multilayer structure and the diblock copolymer was processed to create Au nanoislands. The material was then ion implanted by nitrogen from above the Au nano metal mask and 0018-9464/$31.00 © 2012 IEEE CHOI et al.: GEOMETRICALLY PLANAR ION-IMPLANT PATTERNED MAGNETIC RECORDING MEDIA USING MASKS 3403 Fig. 1. Schematic illustration of the fabrication processes for bit patterned media (BPM) using nanoparticle-masked ion implantation process. buffer layer. Patterned regions intended to be magnetic recording bit islands are blocked from ion implantation due to the presence of Au islands above while the outside regions get preferentially ion implanted. II. EXPERIMENTAL PROCEDURES A. Magnetic Thin Film Deposition Prior to magnetic thin film multilayer deposition, a 4 in. (100) Si substrate was cut into several pieces and cleaned in acetone, isopropyl alcohol, and methanol successively with ultrasonication followed by a de-ionized (DI) water rinse. Then, specimens were immersed in piranha solution comprised of for 20 min at 80 followed by copious DI water rinse. Magnetic recording media with a layer structure having perpendicular magnetic anisotropy were sputter deposited on a flat substrate first. To assist selective-area ion implantation, a buffer layer was used. B. Di-Block Copolymer Thin Film Deposition The patterned structure was made by di-block copolymer self-assembly followed by RIE process. Poly(styrene-b-4vinylpyridine) (S4VP) (number-average molecular weight, , , , where is the average molecular weight) was purchased from Polymer Source (Montreal, Canada) and used without further purification. 0.5 wt.% S4VP copolymer solution dissolved in toluene was spin-coated at 2000 rpm for 60 s on film. This film was then exposed to tetrahydrofuran (THF) vapor in a closed glass vessel for 3 h to induce Fig. 2. SEM micrographs of PS-b-P4VP thin film. (a) As-spun PS-b-P4VP and (b) THF-annealed PS-b-P4VP film (c) after the di-block copolymer process, Au dot arrays are formed on sub. multilayer thin film to serve as mask islands. mobility and allow phase separation to occur. The film was then immersed in pure ethanol for the poly(4-vinylpyridine) (P4VP) phase to swell, thus leading to a porous structure. C. Formation of Au Dot Arrays A 0.05 wt% gold precursor solution in ethanol was spin-coated onto the reconstructed films and then, immediately exposed to toluene vapors for 20 min. The surface reconstructed films were treated with toluene vapor to recover the film with original surface morphology. Subsequent oxygen plasma treatment led to arrays of gold nanoparticles in the same positions as those of the original nanopores, while the polymer was completely degraded. D. Nitrogen Ion Implantation Non-magnetic implantation can lead to magnetic softening and the small ion size would have minimal damages on various materials characteristics [20]. Nitrogen ion implantation was carried out by using the varian implanters system. The machine used in the manufacture of BPM use 10 KeV beam energy and ion dosage irradiation. The overall 3404 IEEE TRANSACTIONS ON MAGNETICS, VOL. 48, NO. 11, NOVEMBER 2012 Fig. 3. Magnetic hysteresis loops for Au dot masked and nitrogen ion implanted [Co/Pd]n multilayer film with as a function of process of nitrogen ion implanted Co/Pd magnetic multilayer were schematically illustrated in Fig. 1. The sample microstructure was characterized by ultrahigh resolution scanning electron microscopy (UHR SEM) and the magnetic properties were evaluated by vibrating sample magnetometers (VSM) before and after non-magnetic ion implantation. III. RESULTS AND DISCUSSION As-spun S4VP type DBCP thin film can be further ordered by THF (tetrahydrofuran) vapor annealing treatment and thus leading to improved close-packed cylindrical P4VP microdomains [21]. However, annealing in THF longer than the optimized time can readily result in a detachment of the DBCP film from the substrate, which deteriorates local ordering of DBCP. In this paper, optimum annealing time was 3 h. When the solventannealed film is immersed in ethanol, the S4VP film reconstruction occurs due to its solvating power difference on PS and P4VP phases; thus leading to a nanoporous film [22]. The representative SEM images before and after solvent annealing treatment are seen in Figs. 2(a) and (b), which show that highly self-ordered S4VP film is developed on substrate multilayer thin film. The diblock copolymer interpore (pore-to-pore) distance, an important parameter that determines the applied voltage for anodization, was 48.3 nm 2.7 nm, based on SEM micrograph analysis. After solvent annealing, Au solution was spin-coated onto the reconstructed films. Subsequent oxygen plasma treatment led to a more or less periodic array of gold nano-particles in the same positions as those of the original nanopores, while the polystyrene (PS) was completely removed. These Au nano dots from spontaneous self-assembly of PS-b-P4VP diblock copolymer are utilized in this study as a metal mask for ion implantation (Fig. 2(c)). After solvent annealing process and oxygen plasma treatment, the sample is covered with Au nano-island array with a good periodicity and high density. A buffer layer thickness. further improvement in Au island periodicity, density and long range ordering would be beneficial for BPM. Fig. 3 shows the magnetic hysteresis loop of nitrogen ion implanted Co/Pd multilayer film prepared using Au island mask. The M-H loop properties for different buffer layer thicknesses (0, 20, 100 nm thickness) are shown in the figure. Because of the particular ion energy and dose utilized for these sets of implantation experiments, the Au nano-island mask alone was not enough to block the impinging ions with dosage at 10 keV. Thus a buffer layer was added to absorb some of the ions and help to create well-defined selective-area ion implantation. With just 20 nm thick buffer layer, the saturation magnetization of the magnetic layer, even in the supposedly masked regions, is significantly reduced and the perpendicular anisotropy is mostly destroyed. The M-H loop with a thicker 100 nm buffer layer, on the other hand, is improved to a higher coercivity value indicating a substantial blocking of implanted ions by buffer layer, the successful isolation of magnetic islands and the excellent exchange decoupling between the magnetic islands enabled by ion implantation to the in-between regions. Those regions outside the magnetic recording bit islands are not masked by Au metal mask dots. using DBCP technique, which was then nitrogen ion implanted to allow penetration into the Co/Pd multilayer film, thus creating magnetically isolated bit island geometry while maintaining the overall flat geometry of the patterned media. However, as can be seen in Fig. 3, the M-H loop of nitrogen ion implanted Co/Pd magnetic multilayer still shows the presence of in-plane magnetized regions in the outer core of the bit patterned area, which indicates that, the processing needs to be improved. At 200 nm thickness buffer layer, there is no difference between the M-H loop of implanted Co/Pd magnetic multilayer and un-implanted sample. In the case of the nitrogen ions with dosage at 10 keV, they are too weak to get through layer having a 200 nm thickness. Various types of non-magnetic ions (e.g., oxygen, argon or fluorine) and different process/materials parameters (e.g., ion beam energy (keV), implantation dose CHOI et al.: GEOMETRICALLY PLANAR ION-IMPLANT PATTERNED MAGNETIC RECORDING MEDIA USING MASKS , beam angle and the thickness of the buffer layer) can be studied for ion implantations for patterned media. IV. SUMMARY AND CONCLUSIONS We have developed a convenient method for local control of coercivity of geometrically planar magnetic recording media of a Co/Pd multilayer magnetically hard film by ion implantation with Au nanoisland metal mask and buffer layer. The Au nano dot arrays fabricated using spontaneous self-assembly of PS-b-P4VP diblock copolymer has been utilized here as an ion-blocking metal mask for selective area patterned ion implantation. buffer layer has been found to be useful in terms of reducing the implanting ion energy to avoid excessive ion damage to the magnetic layer. Optimization of the buffer layer dimension needs to be studied further. It is expected an improved processing specifics will be useful for developing more practical fabrication techniques for bit-patterned magnetic media. ACKNOWLEDGMENT The authors wish to acknowledge the financial support of this work by the NSF-Nanomanufacturing Division under Grant CMMI #0856674, the Center for Magnetic Recording Research at UC San Diego, a National Research Foundation Grant through World Class University Program under Grant R33-2008-000-10025-0, and the Center for Nanostructured Materials Technology under the Grant Frontier R&D Program. REFERENCES [1] C. A. 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