In heat assisted magnetic recording, information bits are recorded on a data storage medium at elevated temperatures, and the data bit dimension can be determined by the dimensions of the heated area in the storage medium or the dimensions of an area of the storage medium that is subjected to a magnetic field. In one approach, a beam of light is condensed to a small optical spot on the storage medium to heat a portion of the medium and reduce the magnetic coercivity of the heated portion. Data is then written to the reduced coercivity region.
One example of a recording head for use in heat assisted magnetic recording includes a near field transducer (NFT) that is capable of focusing light to a spot size smaller than the diffraction limit. The NFT is designed to reach local surface-plasmon resonance at a designed light wavelength. At resonance, a high electric field surrounding the NFT appears, due to the collective oscillation of electrons in the metal. A portion of the field will tunnel into a storage medium and get absorbed, raising the temperature of the medium locally for recording.
The NFT's temperature significantly increases at plasmonic resonance. In addition, a portion of the NFT may be exposed at the air bearing surface of the recording head and is thus subject to mechanical wearing. NFT performance is greatly influenced by the heat and mechanical stress during HAMR operation. Gold (Au) is currently used as the primary NFT material due to its superior optical properties. However, gold has a relatively low mechanical strength and gold NFTs may experience reflow at elevated temperatures resulting in rounding of the NFT shape. A deformation in shape can reduce coupling efficiency and reduce the amount of light energy transferred to the storage medium. Therefore, there remains a need for NFTs made of materials other than gold.
Disclosed herein is an apparatus that includes a near field transducer, the near field transducer including an electrically conductive nitride.
Also disclosed is an apparatus that includes a light source; a waveguide; and a near field transducer, the near field transducer including an electrically conductive nitride, wherein the light source, waveguide and near field transducer are configured to transmit light from the light source to the waveguide and finally the near field transducer.
Also disclosed is a disc drive that includes at least one actuator arm having a flexure; at least one head, wherein each flexure has a head at the distal end thereof and wherein each head includes: a light source; a near field transducer, the near field transducer including an electrically conductive nitride; a magnetic reader; and a magnetic writer wherein the light source and the near field transducer are configured to transmit light from the light source to the near field transducer in order to assist the magnetic writer with writing.
The above summary of the present disclosure is not intended to describe each disclosed embodiment or every implementation of the present disclosure. The description that follows more particularly exemplifies illustrative embodiments. In several places throughout the application, guidance is provided through lists of examples, which examples can be used in various combinations. In each instance, the recited list serves only as a representative group and should not be interpreted as an exclusive list.
The figures are not necessarily to scale. Like numbers used in the figures refer to like components. However, it will be understood that the use of a number to refer to a component in a given figure is not intended to limit the component in another figure labeled with the same number.
In the following description, reference is made to the accompanying set of drawings that form a part hereof and in which are shown by way of illustration several specific embodiments. It is to be understood that other embodiments are contemplated and may be made without departing from the scope or spirit of the present disclosure. The following detailed description, therefore, is not to be taken in a limiting sense.
Unless otherwise indicated, all numbers expressing feature sizes, amounts, and physical properties used in the specification and claims are to be understood as being modified in all instances by the term “about.” Accordingly, unless indicated to the contrary, the numerical parameters set forth in the foregoing specification and attached claims are approximations that can vary depending upon the properties sought to be obtained by those skilled in the art utilizing the teachings disclosed herein.
The recitation of numerical ranges by endpoints includes all numbers subsumed within that range (e.g. 1 to 5 includes 1, 1.5, 2, 2.75, 3, 3.80, 4, and 5) and any range within that range.
As used in this specification and the appended claims, the singular forms “a”, “an”, and “the” encompass embodiments having plural referents, unless the content clearly dictates otherwise. As used in this specification and the appended claims, the term “or” is generally employed in its sense including “and/or” unless the content clearly dictates otherwise.
“Include,” “including,” or like terms means encompassing but not limited to, that is, including and not exclusive. It should be noted that “top” and “bottom” (or other terms like “upper” and “lower”) are utilized strictly for relative descriptions and do not imply any overall orientation of the article in which the described element is located.
In one aspect, this disclosure provides a near field transducer (NFT) that can be used in a HAMR recording head. Disclosed NFTs include materials that may show advantageous mechanical properties as well as decreased thermal mismatch with adjacent materials, while still possessing acceptable optical properties. In several examples, such materials include nitrides.
Disclosed herein are NFTs and devices that include such NFTs.
For heat assisted magnetic recording (HAMR), electromagnetic radiation, for example, visible, infrared or ultraviolet light is directed onto a surface of the data storage media to raise the temperature of a localized area of the media to facilitate switching of the magnetization of the area. Recent designs of HAMR recording heads include a thin film waveguide on a slider to guide light toward the storage media and a near field transducer to focus the light to a spot size smaller than the diffraction limit. While
An insulating material 62 separates the coil turns. In one example, the substrate can be AlTiC, the core layer can be Ta2O5, and the cladding layers (and other insulating layers) can be Al2O3. A top layer of insulating material 63 can be formed on the top pole. A heat sink 64 is positioned adjacent to the sloped pole piece 58. The heat sink can be comprised of a non-magnetic material, such as for example Au.
As illustrated in
The storage media 16 is positioned adjacent to or under the recording head 30. The waveguide 42 conducts light from an energy source 78 of electromagnetic radiation, which may be, for example, ultraviolet, infrared, or visible light. The source may be, for example, a laser diode, or other suitable laser light source for directing a light beam 80 toward the waveguide 42. Specific exemplary types of energy sources 78 can include, for example laser diodes, light emitting diodes (LEDs), edge emitting laser diodes (EELs), vertical cavity surface emitting lasers (VCSELs), and surface emitting diodes. In some embodiments, the energy source can produced energy having a wavelength from 300 nm to 2000 nm. In some embodiments, the energy source can produce energy having a wavelength of 830 nm, for example. Various techniques that are known for coupling the light beam 80 into the waveguide 42 may be used. Once the light beam 80 is coupled into the waveguide 42, the light propagates through the waveguide 42 toward a truncated end of the waveguide 42 that is formed adjacent the air bearing surface (ABS) of the recording head 30. Light exits the end of the waveguide and heats a portion of the media, as the media moves relative to the recording head as shown by arrow 82. A near-field transducer (NFT) 84 is positioned in or adjacent to the waveguide and at or near the air bearing surface. The heat sink material may be chosen such that it does not interfere with the resonance of the NFT.
Although the example of
Materials that are to be used in disclosed NFTs generally are plasmonic materials. The plasmonic nature of a material can be estimated based on the refractive index (n) and the extinction coefficient (k). Table I shows optical properties (n and k), thermal conductivity and coefficient of thermal expansion (CTE) for various materials. Table I also provides a figure of merit (FOM) for surface plasmon generation ((n2−k2)/2nk).
As seen from Table 1, the currently measured properties for ZrN and TiN are only lower than those of Ag, Au, and Cu, and are therefore favorable candidates among all alternative plasmonic materials considered. Furthermore, the deposition processes of ZrN and TiN can be affected in order to improve the optical properties. Table II below shows nanoindentation hardness and coefficient of thermal expansion (CTE) of various materials.
As seen from Table II, the nanoindentation hardness of ZrN is 20-40 GPa and that of Tin is 18-21 GPa. These values are an order of magnitude higher than that of Au (around 2 GPa). Furthermore, the CTE of ZrN (9.4×10−6/K) and TiN (9.35×10−6/K) are about 40% lower than that of Au and are closer to the oxide waveguide materials that surround the NFT. This could lead to lesser thermal stresses during HAMR operation.
Disclosed herein are NFTs that include an electrically conductive nitride material. Exemplary electrically conductive nitride materials can include, for example, ZrN, TiN, TaN, HfN, or combinations thereof. In some embodiments NFTs can include ZrN, TiN, or combinations thereof.
In some embodiments, the entire NFT can be made of a nitride material. In some embodiments, the entire NFT can be made of ZrN, TiN, or some combination thereof. In some embodiments, the NFT could be a lollypop type design, a nanorod type design, or any other type of NFT design. In some embodiments, a lollypop type NFT can be made entirely of a nitride material. In some embodiments, a nanorod type NFT can be made entirely of a nitride material.
In some embodiments, only a part of a NFT is made of a nitride material. In some embodiments, such a NFT could be a lollypop type design, a nanorod type design, or any other type of NFT design. In some embodiments, only the peg (see peg 96 in
In some embodiments, only one or more portions of a NFT is made of a nitride material. An example of an NFT that could have one or more portions thereof made of a nitride material can include embodiments such as that depicted in
NFTs that include such nitride base layers can enhance mechanical properties of NFTs without significantly sacrificing the coupling efficiency. In some embodiments, such nitride base layers could function to reduce, minimize or eliminate corner rounding issues that have been seen in (for example) gold nanorod type NFTs.
Another example of a NFT that could have one or more portions thereof made of a nitride material can include embodiments such as that depicted in
Another example of a NFT that could have one or more portions thereof made of a nitride material can include embodiments such as that depicted in
In some embodiments, an NFT can include a dispersed material in a base material. For example, a nitride material can be dispersed in a non-nitride material (base material) throughout at least a portion of the NFT. Or, for example, an NFT can include a non-nitride material dispersed in a nitride material (base material) throughout at least a portion of the NFT. In some embodiments, a material can be dispersed in a base material in the entirety of the NFT or only in some portion of the NFT. Such embodiments can be utilized with any type of NFT, including for example nanorod type NFTs and lollypop type NFTs. The material (either nitride or non-nitride) that is dispersed in the base material can be doped into the base material, for example. Similarly, the material that is dispersed in the base material can be in the form of nanoparticles. In some embodiments, the nanoparticles can have average diameters from 1 nm to 100 nm, for example. The dispersed material can be formed separately and then dispersed in the base material, or the dispersed material and the base material can be formed at the same time (for example, co-sputtering). In some embodiments, the non-nitride base materials can include, for example, gold, silver, copper, or alloys thereof.
A nanorod type NFT made entirely of TiN was modeled. The dimensions of the NFT (cross-track width and z height) were chosen with the properties of TiN in mind.
Growth of stoichiometric, crystalline, and low resistivity metallic TiN or ZrN has required high temperature processing in the past, for example up to about 800° C. using physical vapor deposition (PVD) methods such as direct current (DC) or reactive magnetron sputtering. Low resistivity TiN films have been produced at temperatures as low as about 200° C. by highly ionized sputter deposition techniques such as High Power Impulse Magnetron Sputtering (HiPIMS) power sources. TiN films having resistivity as low as 41.9 μΩ-cm have been obtained. Laser ablation deposition techniques have also been used to produce TiN and ZrN films at temperatures ranging from about 100° C. to about 600° C.
Thus, embodiments of near field transducers including nitride materials are disclosed. The implementations described above and other implementations are within the scope of the following claims. One skilled in the art will appreciate that the present disclosure can be practiced with embodiments other than those disclosed. The disclosed embodiments are presented for purposes of illustration and not limitation.
This application claims priority to U.S. Provisional Application No. 61/637,696 entitled “NEAR FIELD TRANSUCERS (NFTs) INCLUDING NITRIDES” having docket number 430.17123000 filed on Apr. 24, 2012, the disclosure of which is incorporated herein by reference thereto.
Number | Name | Date | Kind |
---|---|---|---|
4492873 | Dmitriev | Jan 1985 | A |
5482611 | Helmer | Jan 1996 | A |
5849093 | Andra | Dec 1998 | A |
5945681 | Tokiguchi | Aug 1999 | A |
6130436 | Renau | Oct 2000 | A |
6144098 | Iyer | Nov 2000 | A |
6589676 | Gui | Jul 2003 | B1 |
6632483 | Callegari | Oct 2003 | B1 |
6641932 | Xu | Nov 2003 | B1 |
6683426 | Kleeven | Jan 2004 | B1 |
6795630 | Challener | Sep 2004 | B2 |
6999384 | Stancil | Feb 2006 | B2 |
7002228 | Deak | Feb 2006 | B2 |
7018729 | Pocker | Mar 2006 | B2 |
7032427 | Niwa | Apr 2006 | B2 |
7262936 | Hamann et al. | Aug 2007 | B2 |
7272079 | Challener | Sep 2007 | B2 |
7330404 | Peng | Feb 2008 | B2 |
7476855 | Huang | Jan 2009 | B2 |
7544958 | Low | Jun 2009 | B2 |
7609003 | Horsky | Oct 2009 | B2 |
7690009 | Miyanishi et al. | Mar 2010 | B2 |
7791839 | Olson | Sep 2010 | B2 |
7961417 | Seigler | Jun 2011 | B2 |
7965464 | Batra | Jun 2011 | B2 |
7986592 | Hirano et al. | Jul 2011 | B2 |
8023225 | Shimazawa | Sep 2011 | B2 |
8031561 | Hellwing | Oct 2011 | B2 |
8040761 | Kawamori | Oct 2011 | B2 |
8077556 | Komura et al. | Dec 2011 | B2 |
8107325 | Komura et al. | Jan 2012 | B2 |
8116034 | Komura | Feb 2012 | B2 |
8116176 | Kato | Feb 2012 | B2 |
8194510 | Sasaki | Jun 2012 | B2 |
8194511 | Sasaki et al. | Jun 2012 | B2 |
8213272 | Takayama | Jul 2012 | B2 |
8223597 | Komura | Jul 2012 | B2 |
8248891 | Lee | Aug 2012 | B2 |
8284521 | Ohtsu | Oct 2012 | B2 |
8284635 | Matsumoto | Oct 2012 | B2 |
8289650 | Seigler et al. | Oct 2012 | B2 |
8320220 | Yuan et al. | Nov 2012 | B1 |
8331205 | Seigler et al. | Dec 2012 | B2 |
8339740 | Zou et al. | Dec 2012 | B2 |
8351151 | Katine | Jan 2013 | B2 |
8385159 | Gao | Feb 2013 | B2 |
8400902 | Huang | Mar 2013 | B2 |
8405056 | Amaldi | Mar 2013 | B2 |
8405932 | Seigler et al. | Mar 2013 | B2 |
8416647 | Zhao | Apr 2013 | B1 |
8427925 | Zhao et al. | Apr 2013 | B2 |
8451555 | Seigler et al. | May 2013 | B2 |
8477454 | Zou | Jul 2013 | B2 |
8514673 | Zhao et al. | Aug 2013 | B1 |
8553505 | Rawat | Oct 2013 | B2 |
8670215 | Zou | Mar 2014 | B2 |
8711662 | Lee | Apr 2014 | B2 |
8733959 | Moriya | May 2014 | B2 |
8830800 | Pitcher | Sep 2014 | B1 |
8842391 | Zou et al. | Sep 2014 | B2 |
8971161 | Cheng et al. | Mar 2015 | B2 |
20050012052 | Platzgummer | Jan 2005 | A1 |
20050190496 | Hamann | Sep 2005 | A1 |
20060238133 | Horsky | Oct 2006 | A1 |
20070069383 | Suzuki | Mar 2007 | A1 |
20080230724 | Low | Sep 2008 | A1 |
20090073858 | Seigler | Mar 2009 | A1 |
20090130365 | Kojima | May 2009 | A1 |
20090225636 | Hirano | Sep 2009 | A1 |
20100103553 | Shimazawa | Apr 2010 | A1 |
20100123965 | Lee | May 2010 | A1 |
20100123967 | Batra | May 2010 | A1 |
20100128579 | Seigler | May 2010 | A1 |
20100149930 | Komura | Jun 2010 | A1 |
20100157746 | Hongo | Jun 2010 | A1 |
20100190036 | Komvopoulos | Jul 2010 | A1 |
20100214685 | Seigler | Aug 2010 | A1 |
20100309581 | Wu | Dec 2010 | A1 |
20100315736 | Takayama | Dec 2010 | A1 |
20100320403 | Amaldi | Dec 2010 | A1 |
20100329085 | Kawamori | Dec 2010 | A1 |
20110006214 | Bonig | Jan 2011 | A1 |
20110026161 | Ikeda | Feb 2011 | A1 |
20110038236 | Mizuno | Feb 2011 | A1 |
20110058272 | Miyauchi | Mar 2011 | A1 |
20110096431 | Hellwig | Apr 2011 | A1 |
20110122735 | Kato | May 2011 | A1 |
20110205863 | Zhao et al. | Aug 2011 | A1 |
20120045662 | Zou | Feb 2012 | A1 |
20120105996 | Katine | May 2012 | A1 |
20120127839 | Rawat | May 2012 | A1 |
20120213042 | Aoki | Aug 2012 | A1 |
20130107679 | Huang | May 2013 | A1 |
20130161505 | Pitcher | Jun 2013 | A1 |
20130164453 | Pitcher | Jun 2013 | A1 |
20130164454 | Pitcher | Jun 2013 | A1 |
20130235707 | Zhao et al. | Sep 2013 | A1 |
20130279315 | Zhao | Oct 2013 | A1 |
20130286799 | Zhu et al. | Oct 2013 | A1 |
20130286804 | Zhao et al. | Oct 2013 | A1 |
20130288077 | Dhawan | Oct 2013 | A1 |
20140004384 | Zhao | Jan 2014 | A1 |
20140043948 | Hirata | Feb 2014 | A1 |
20140050057 | Zou | Feb 2014 | A1 |
20140113160 | Pitcher | Apr 2014 | A1 |
20150132503 | Kautzky | May 2015 | A1 |
Number | Date | Country |
---|---|---|
024088 | Oct 1987 | EP |
0 580 368 | Jan 1994 | EP |
0942072 | Sep 1999 | EP |
1328027 | Jul 2003 | EP |
2106678 | Oct 2009 | EP |
2011198450 | Oct 2011 | JP |
20111248991 | Dec 2011 | JP |
200929183 | Jul 2009 | TW |
WO 9745834 | Dec 1997 | WO |
WO 2013163195 | Oct 2013 | WO |
WO 2013163470 | Oct 2013 | WO |
Entry |
---|
Al-Bayati et al., Junction Profiles of Sub keV Ion Implantation for Deep Sub-Quarter Micron Devices, IEEE, 2000, pp. 87-90. |
Angel et al., “Enhanced Low Energy Drift-Mode Beam Currents in a High Current Ion Implanter,” IEEE, 1999, pp. 219-222. |
U.S. Appl. No. 13/923,925, Jun. 21 2013, Pitcher. |
U.S. Appl. No. 14/062,651, Oct. 24, 2013, Zou. |
Bannuru et al., “The Electrical and Mechanical Properties of Au-V and Au-V205 Thin Films for Wear-Resistant RF MEMS Switches”, Journal of Applied Physics, 103, (2008), pp. 083522-1-083522-6. |
Druz et al., “Diamond-Like Carbon Films Deposited Using a Broad, Uniform Ion Beam from an RF Inductively Coupled CH4-Plasma Source”, Diamond and Related Materials, vol. 7, No. 7, Jul. 1998, pp. 965-972. |
Liu et al., “Influence of the Incident Angle of Energetic Carbon Ions on the Properties of Tetrahedral Amorphous Carbon (ta-C) films”, Journal of Vacuum Science and Technology, vol. 21, No. 5, Jul. 25, 2003, pp. 1665-1670. |
Metallization: “Metallization”; chapter 5, In: Kris v. Srikrishnan and Geraldine C. Schwartz: “Handbook of Semiconductor Interconnection Technology, Second Edition”, 2006, CRC Press, Boca Raton, FL, USA, XP002711255, ISBN:978-1-4200-1765-6, pp. 311-382, Section 5.4.1.2 Adhesion; p. 320. |
Piazza et al., “Large Area Deposition of Hydrogenated Amorphous Carbon Films for Optical Storage Disks”, Diamond and Related Materials, vol. 13, No. 4-8, Apr. 2004, pp. 1505-1510. |
Robertson, J., “Diamond-Like Amorphous Carbon,” Materials Science and Engineering R 37, 2002, pp. 129-281. |
Satoh et al., “Evaluation of Adhesion Materials for Gold Line-and-Space Surface Plasmon Antenna on SOI-MOS Photodiode”, Silicon Nanoelectronics Workshop (SNW), 2010, IEEE, Piscataway, NJ, USA, Jun. 13, 2010, pp. 1-2. |
Vogt, K.W. et al., “Characterization of Thin Titanium Oxide Adhesion Layers on Gold Resistivity, Morphology, and Composition”, Surface Science, North-Holland, Amsterdam, NL, vol. 301, No. 1-3, Jan. 10, 1994, pp. 203-213. |
Williams, et al., “Strengthening Gold Films with Zirconia Nanoparticles for MEMS Electrical Contacts”, ScienceDirect, Acta Materialia 56, (2008), pp. 1813-1819. |
PCT/US2013/038120 Search Report and Written Opinion dated Jul. 19, 2013 (8 pages). |
Number | Date | Country | |
---|---|---|---|
20130279315 A1 | Oct 2013 | US |
Number | Date | Country | |
---|---|---|---|
61637696 | Apr 2012 | US |