Heat assisted magnetic recording writer having integrated polarization rotation waveguides

Information

  • Patent Grant
  • 9646639
  • Patent Number
    9,646,639
  • Date Filed
    Friday, June 26, 2015
    9 years ago
  • Date Issued
    Tuesday, May 9, 2017
    7 years ago
Abstract
A heat assisted magnetic recording (HAMR) writer is described. The HAMR writer is coupled with a laser that provides energy having a first polarization state. The HAMR writer has an air-bearing surface (ABS) configured to reside in proximity to a media during use, a plurality of waveguides, a main pole and at least one coil. The main pole writes to the media and is energized by the coil(s). The waveguides receive the energy from the laser and direct the energy toward the ABS. The waveguides include an input waveguide and an output waveguide. The input waveguide is configured to carry light having the first polarization state. The output waveguide is configured to carry light having a second polarization state different from the first polarization state. The waveguides are optically coupled and configured to transfer the energy from the first polarization state to the second polarization state.
Description
BACKGROUND

A conventional heat assisted magnetic recording (HAMR) transducer typically includes at least a waveguide, a near-field transducer (NFT), a main pole and a coil for energizing the main pole. The conventional HAMR transducer uses light, or energy, received from a conventional laser in order to write to a magnetic recording media. Light from the laser is incident on and coupled into the waveguide. Light is guided by the conventional waveguide to the NFT near the ABS. The NFT focuses the light to magnetic recording media (not shown), such as a disk. This region is thus heated. The main pole is energized and field from the pole tip is used to write to the heated portion of the recording media.


Although the conventional HAMR transducer functions, improvements in performance are still desired.





BRIEF DESCRIPTION OF SEVERAL VIEWS OF THE DRAWINGS


FIG. 1 is a diagram depicting a side view of an exemplary embodiment of a HAMR disk drive.



FIG. 2 is a diagram depicting an exploded perspective view of an exemplary embodiment of a portion of a HAMR writer.



FIGS. 3 A and 3B are diagrams depicting a cross-sectional and side views of another exemplary embodiment of a portion of a HAMR writer.



FIG. 4 is a diagram depicting a cross-sectional view of another exemplary embodiment of a HAMR writer.



FIG. 5 is a diagram depicting a cross-sectional view of another exemplary embodiment of a HAMR writer.



FIG. 6 is a diagram depicting a cross-sectional view of another exemplary embodiment of a HAMR writer.



FIG. 7 is a diagram depicting a side view of another exemplary embodiment of a HAMR writer.



FIG. 8 is a diagram depicting a side view of another exemplary embodiment of a HAMR writer.



FIG. 9 is a flow chart depicting an exemplary embodiment of a method for fabricating a HAMR write apparatus.



FIG. 10 is a flow chart depicting an exemplary embodiment of a method for fabricating waveguides for a HAMR write apparatus.



FIG. 11 is a flow chart depicting an exemplary embodiment of a method for fabricating waveguides for a HAMR write apparatus.



FIGS. 12-17 depict cross-sectional views of an exemplary embodiment of a wafer during fabrication of waveguides for the HAMR disk drive.





DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS


FIG. 1 depicts a side view of an exemplary embodiment of a portion of a heat-assisted magnetic recording (HAMR) write apparatus, or disk drive 100. For clarity, FIG. 1 is not to scale. For simplicity not all portions of the HAMR disk drive 100 are shown. In addition, although the HAMR disk drive 100 is depicted in the context of particular components other and/or different components may be used. For example, circuitry used to drive and control various portions of the HAMR disk drive 100 is not shown. For simplicity, only single components are shown. However, multiples of each component and their sub-components, might be used.


The HAMR disk drive 100 includes media 102, a slider 110, a HAMR transducer 120 and a laser subassembly 170. Additional and/or different components may be included in the HAMR disk drive 100. Although not shown, the slider 110, and thus the laser assembly 170 and HAMR transducer 120 are generally attached to a suspension. The laser assembly 170 includes a laser 172 and a submount 174. The submount 174 is a substrate to which the laser 172 may be affixed for improved mechanical stability, heat sinking, ease of manufacturing and better robustness. The laser 172 may be a chip such as a laser diode or other laser. The laser 172 outputs energy having a particular polarization state, indicated as Polarization State 1 (first polarization state) in FIG. 1. In some embodiments, this first polarization state is a TE mode. For example, the light may be linearly polarized in the cross-track direction. The laser 172 outputs this light energy through the surface closest to the HAMR transducer 120.


The HAMR transducer 120 is fabricated on the slider 110 and includes an air-bearing surface (ABS) proximate to the media 102 during use. In general, the HAMR write transducer 120 and a read transducer are present in the HAMR write apparatus 100. However, for clarity, only the HAMR write transducer 120 is shown. As can be seen in FIG. 1, HAMR transducer 120 includes a near-field transducer (NFT) 130, waveguides 140, a main pole 150 and coil(s) 155. The waveguides 140 are optically coupled with the laser 172. The waveguides 140 carry light energy from the laser 172 toward the ABS. The NFT 130 couples a portion of this energy from the waveguides 140 to the media 102. In some embodiments, the NFT 130 occupies a portion of the ABS. The NFT 130 transfers energy to the media 102. The write pole 150 is energized by the coils 155 and writes to the media 102. The coil(s) 155 may be solenoidal or spiral (pancake) coils. Other components including but not limited to other poles and/or shields may also be present.


In some embodiments, the NFT 130 may be configured to propagate a surface plasmon polariton. In such embodiments, the NFT 130 may be desired to utilize a transverse magnetic (TM) mode. This electric field of the mode may be oriented in the down track direction. In other embodiments, the NFT 130 may be configured to receive energy polarized in a particular manner for other reason(s). The desired polarization of light received by the NFT 130 is depicted as Polarization State 2 (second polarization) in FIG. 1. The Polarization State 2 is different from the Polarization State 1 emitted by the laser 172.


The waveguides 140 include an input waveguide that receives the light from the laser 172 and an output waveguide that may provide light to the NFT 130. The waveguides 140 are optically coupled. This may be achieved by overlapping the waveguides in regions where the waveguides are in close proximity. This overlap is shown in FIG. 1 by dashed lines. In the embodiment shown in FIG. 1, there are four waveguides 140. However, in another embodiment, another number of waveguides might be used. The waveguides 140 include at least the input waveguide and the output waveguide. The light energy received by the input waveguide closest to the laser 140 is polarized in the first state (Polarization State 1 in FIG. 1). In some embodiments, the first of the waveguide 140 may also be desired to be excited with linearly polarized light in a TE fashion with the electric field in the cross track direction. In other embodiments, the input waveguide may have improved efficiency for light polarized in another manner. However, the first polarization state of the light output by the laser 172 may be different than that which is desired, for example for use by the NFT 130.


Thus, the energy output by the laser 172 in the first polarization state may not match the energy desired to be input to the NFT 130 in the second polarization state. As a result, the waveguides 140 are optically coupled such that the polarization state of light traversing between the waveguides 140 is transferred from the first polarization state to the second polarization state.


For example, the NFT 130 may be configured for light that is linearly polarized in the down track direction (TM polarization), while the laser 172 outputs light polarized in the cross-track direction (TE polarization). Thus, the waveguides 140 are configured such that as energy from the laser 172 is transferred from one waveguide to another waveguide, the polarization state changes. Thus, the waveguides 140 change the polarization of the energy from the laser 172 to match the desired polarization state.


In operation, the laser 172 emits light having the first polarization state. The light then enters the input waveguide in the first polarization state. The input waveguide is optically coupled to the next waveguide, and so on until the output waveguide is reached. The polarization of light at the output of the output waveguide is the second polarization state. For example, the input waveguide may carry the TE polarized energy, while the output waveguide carries TM polarized light. Thus, while traversing the waveguides 140, particularly in the regions the waveguides 140 are optically coupled, the polarization of the light has been rotated from the first polarization state to the second polarization state. The waveguides 140 also direct the light to the NFT 130. Thus, light entering the NFT 130 has the desired second polarization state. The NFT 128 focuses the light to a region of magnetic recording media 102. High density bits can be written on a high coercivity medium with the pole 150 energized by the coils 155 to a modest magnetic field.


The HAMR disk drive 100 may exhibit enhanced performance. Using the waveguides 140, the polarization of the light energy from the laser 172 can be rotated to the desired direction. Thus, energy having the desired polarization can be provided to the NFT 130. For example, an NFT 130 that propagates surface plasmon polariton can be used in the HAMR transducer 100. In addition, a lower cost laser 172 that produces light linearly polarized in the cross-track direction may be used in the HAMR disk drive 100. Thus, performance of the HAMR disk drive may be improved.



FIG. 2 depicts an exploded perspective view of another exemplary embodiment of a portion of the HAMR disk drive 100′. For clarity, FIG. 2 is not to scale. For simplicity not all portions of the HAMR disk drive 100′ are shown. In addition, although the HAMR disk drive 100′ is depicted in the context of particular components other and/or different components may be used. Further, the arrangement of components may vary in different embodiments. The HAMR disk drive 100′ is analogous to the HAMR disk drive 100. Consequently, similar components have analogous labels. The HAMR disk drive 100′ thus includes a laser 172 and a HAMR transducer 120′ that are analogous to the lasers 172 and HAMR transducer 120, respectively. The HAMR transducer 120′ includes waveguides 140′ and NFT 130 that are analogous to the waveguides 140 and NFT 130, respectively. For clarity, components such as the pole and coils have been omitted.


The waveguides 140′ include an input waveguide 142 and an output waveguide 144. The input waveguide 142 is directly coupled with the output waveguide 144. As can be seen in FIG. 2, the laser 172 outputs light having a first polarization state, with the transverse electric (TE) mode in the cross track direction. Light energy polarized with the TE polarization enters the input waveguide 142. The waveguides 142 and 144 are coupled such that the light transmitted from the input waveguide 142 to the output waveguide 144 is the TM mode. Thus, light exiting the output waveguide 144 has the second polarization state, with the electric field oriented in the down track direction. The light is carried from the output waveguide 144 to the NFT 130. Because the polarization of the light is not further changed, the light energy coupled into the NFT 130 has the second polarization state. Stated differently, this light provided to the NFT 130 is polarized in the TM mode. The NFT 130 may then couple the energy from this light to the media (not shown in FIG. 2) and the write pole (not shown in FIG. 2) used to magnetically write to the heated portion of the media.


The HAMR disk drive 100′ shares the benefits of the HAMR transducer 100. Using the input waveguide 142 and output waveguide 144, the polarization of the light energy from the laser 172 can be rotated to be in the desired direction. Thus, energy having the desired polarization can be provided to the NFT 130. Thus, performance of the HAMR disk drive 100′ may be improved.



FIGS. 3A and 3B depict cross-sectional and side views of another exemplary embodiment of a portion of the HAMR write apparatus 200. For clarity, FIGS. 3A-3B are not to scale. For simplicity not all portions of the HAMR disk drive 200 are shown. In addition, although the HAMR write apparatus 200 is depicted in the context of particular components other and/or different components may be used. Further, the arrangement of components may vary in different embodiments. The HAMR write apparatus 200 is analogous to the HAMR disk drives 100 and 100′. The direction of transmission of light is out of the plane of the page in FIG. 3A (e.g. toward the ABS) and in the direction of the arrows labeled TE Mode and TM Mode in FIG. 3B.


The HAMR write apparatus includes a laser (not shown), an NFT (not shown), a write pole (not shown) for writing to the media, a coil and two waveguides 210 and 220. The waveguides 210 and 220 are analogous to the waveguides 140 and 140′. The waveguide 210 is the output waveguide in the embodiment shown, while the waveguide 220 is the input waveguide. The waveguide 210 includes a core 212 and cladding 214. The output waveguide 220 includes an input core 222 and cladding 224. The light carried by the waveguides 210 and 220 is primarily via the cores 212 and 222. The cores 212 and 222 have a different index of refraction than the cladding 214 and 224. For example, the cores 212 and 222 may be formed of tantalum oxide, while the cladding 214 and 224 may be formed of silicon oxide. In the embodiment depicted in FIGS. 3A-3B the waveguides 210 and 220 are separated by a layer 230. This layer 230 may be an etch stop layer used in fabricating the waveguides 210 and 220. For example, the layer 230 may be an aluminum oxide layer. In some embodiments, such a layer is nominally twenty nanometers thick. However, in other embodiments, the layer 230 may simply be a spacer layer.


The waveguides 210 and 220 are optically coupled and transfer the polarization from a TE mode to a TM mode. Thus, the aspect ratios of the cores differ. For example, the input core 222 has a height h1 and a width w1. The width is larger than the height for the input core 222 (w1>hh1). The output core 212 has a height h2 and w width w2. The height is larger than the width for the output core 212 (h2>w2). Thus, the aspect ratios differ. In particular, the long axes of the cores 212 and 222 are perpendicular to each other (w1 is perpendicular to h2). In the embodiment shown in FIGS. 3A-3B, the aspect ratios (height divided by width) for the waveguides 210 and 220 are not reciprocals (h1/w1≠w2/h2). Thus, the widths and heights of the waveguides 210 and 220 differ. However, in other embodiments, the width of one waveguide 210 or 220 may match the height of the other waveguide 220 or 210, respectively. In general, the aspect ratios of the waveguides 210 and 220 may be optimized for the polarization of the light each waveguide 210 and 220, respectively, is desired to support.


In order to couple the waveguides 210 and 220, the waveguides 210 and 220 are directionally coupled along the coupling length, cl, depicted in FIG. 3B. In other embodiments, the waveguides 210 and 220 might be adiabatically coupled or coupled in another manner. In some embodiments, this length is on the order of eleven microns. The waveguides 210 and 220 are parallel along the coupling length such that light transmitted by the waveguides 210 and 220 have the same direction of transmission along the coupling length. In the embodiment shown in FIGS. 3A and 3B, outside of the coupling length, the waveguides 210 and 220 transmit light in other directions. Stated differently, outside of the coupling length, the waveguides 210 and 220 may have different directions of transmission, may not be in close proximity and are not optically coupled.


In addition, the cores 212 and 222 of the waveguides 210 and 220 are offset. As can be seen in FIGS. 3A-3B, the cores 212 and 222 are offset in the height direction by the spacer layer 230. The cores 212 and 222 are also offset in the width direction by the distance o. In the embodiment shown, the cores 212 and 222 overlap by the offset, o. In other embodiments, the cores 212 and 222 may be offset in the width direction such that they do not overlap and/or are spaced apart. Similarly, the cores 212 and 222 are shown as spaced apart in the height direction by the thickness of the layer 230. In other embodiments, the cores 212 and 222 may partially overlap, may not overlap, or may be spaced apart. In general, the cores 212 and 222 are desired to be offset by not more than their length and/or by not more than their width. In some embodiments, the cores 212 and 222 are offset by not more than one-half of their height and/or width.


In operation, the laser provides light having a first polarization state, with the TE mode with its electric field that may be in the cross track direction. The light having the TE mode polarization enters the input waveguide 220. In the coupling region, the light from the input waveguide 220 is transferred to the output waveguide 210 such that the polarization of the light transferred to the output waveguide 220 is changed to the TM mode. The output waveguide 210 may then transfer the light to the NFT or other component. Thus, this light provided to the NFT is polarized as desired (e.g. in the down track direction). The NFT may then couple the energy from this light to the media (not shown in FIGS. 3A-3B) and the write pole (not shown in FIGS. 3A-3B) used to write to the heated portion of the media.


The HAMR write apparatus 200 shares the benefits of the HAMR transducer(s) 100 and/or 100′. Using the input waveguide 220 and output waveguide 210, the polarization of the light energy from the laser can be transferred to be in the desired direction. Thus, energy having the desired polarization can be provided to the NFT (not shown in FIGS. 3A-3B). Thus, performance of the HAMR disk drive 200 may be improved.



FIG. 4 depicts a cross-sectional view of another exemplary embodiment of a portion of the HAMR write apparatus 200′. For clarity, FIG. 4 is not to scale. For simplicity not all portions of the HAMR disk drive 200′ are shown. In addition, although the HAMR write apparatus 200′ is depicted in the context of particular components other and/or different components may be used. Further, the arrangement of components may vary in different embodiments. The HAMR write apparatus 200′ is analogous to the HAMR writers 100, 100′ and/or 200. Thus, similar components have similar labels as in FIGS. 3A-3B. The direction of transmission of light is out of the plane of the page in FIG. 4 (e.g. toward the ABS).


The HAMR write apparatus includes a laser (not shown), an NFT (not shown), a write pole (not shown) for writing to the media, a coil and two waveguides 210′ and 220′. The waveguides 210′ and 220′ are analogous to the waveguides 210 and 220, respectively, as well as the waveguides 140 and 140′. The waveguide 210′ is the output waveguide in the embodiment shown, while the waveguide 220′ is the input waveguide. The waveguide 210′ includes a core 212 and cladding 214. The output waveguide 220′ includes an input core 222 and cladding 224. In the embodiment depicted in FIG. 4 the waveguides 210′ and 220′ are separated by a layer 230, which is analogous to the layer 230 depicted in FIG. 3A.


The waveguides 210′ and 220′ are optically coupled and transfer the polarization from TE to TM. Thus, the aspect ratios of the cores differ in a manner analogous to that described above. The input core 222 has a height h1 and a width w1. The width is larger than the height for the input core 222 (w1>h1). The output core 212 has a height h2 and w width w2. The height is larger than the width for the output core 212 (h2>w2). Thus, the aspect ratios differ. In the embodiment shown, the long axes of the cores 212 and 222 are perpendicular to each other (w1 is perpendicular to h2).


The waveguides 210′ and 220′ may be adiabatically coupled, directionally coupled or coupled in another manner. In addition, the cores 212 and 222 of the waveguides 210′ and 220′ are offset. As can be seen in FIG. 4, the cores 212 and 222 are offset in the width direction such that the right edge of the input waveguide core 222 is aligned with the left edge of the output waveguide core 212. The cores 212 and 222 are offset by the spacer layer 230 in the height direction. In other embodiments, the spacer layer 230 might be omitted. In some such embodiments, the top of the output core 212 may be aligned with the bottom of the input core 222. In such an embodiment, the edges of the cores 212 and 222 (depicted as corners in FIG. 4) may just touch. Different offsets in the height and/or width directions are possible.


The HAMR write apparatus 200′ shares the benefits of the HAMR transducer(s) 100, 100′ and/or 200. Using the input waveguide 220′ and output waveguide 210′, the polarization of the light energy from the laser can be transferred to be in the desired direction. Thus, energy having the desired polarization can be provided to the NFT (not shown in FIG. 4). Thus, performance of the HAMR disk drive 200′ may be improved.



FIG. 5 depicts a cross-sectional view of another exemplary embodiment of a portion of the HAMR write apparatus 200″. For clarity, FIG. 5 is not to scale. For simplicity not all portions of the HAMR disk drive 200″ are shown. In addition, although the HAMR write apparatus 200″ is depicted in the context of particular components other and/or different components may be used. Further, the arrangement of components may vary in different embodiments. The HAMR write apparatus 200″ is analogous to the HAMR writers 100, 100′, 200 and/or 200′. Thus, similar components have similar labels as in FIGS. 3A-4. The direction of transmission of light is out of the plane of the page in FIG. 5 (e.g. toward the ABS).


The HAMR write apparatus includes a laser (not shown), an NFT (not shown), a write pole (not shown) for writing to the media, a coil and two waveguides 210″ and 220″. The waveguides 210″ and 220″ are analogous to the waveguides 210/210′ and 220/220′, respectively, as well as the waveguides 140 and 140′. The waveguide 210″ is the output waveguide in the embodiment shown, while the waveguide 220″ is the input waveguide. The waveguide 210″ includes a core 212 and cladding 214. The output waveguide 220″ includes an input core 222 and cladding 224. In the embodiment depicted in FIG. 5 the waveguides 210″ and 220″ are separated by a layer 230, which is analogous to the layer 230 depicted in FIG. 3A.


The waveguides 210″ and 220″ are optically coupled and transfer the polarization from TE to TM. Thus, the aspect ratios of the cores differ in a manner analogous to that described above. The input core 222 has a height h1 and a width w1. The width is larger than the height for the input core 222 (w1>hh1). The output core 212 has a height h2 and w width w2. The height is larger than the width for the output core 212 (h2>w2). Thus, the aspect ratios differ. In the embodiment shown, the long axes of the cores 212 and 222 are perpendicular to each other (w1 is perpendicular to h2).


The waveguides 210″ and 220″ may be adiabatically coupled, directionally coupled or coupled in another manner. In addition, the cores 212 and 222 of the waveguides 210″ and 220″ are offset. As can be seen in FIG. 5, the cores 212 and 222 are offset in the width and height directions such that there is space between the waveguides 210″ and 220″ in both directions. Different offsets in the height and/or width directions are possible.


The HAMR write apparatus 200″ shares the benefits of the HAMR transducer(s) 100, 100′, 200 and/or 200′. Using the input waveguide 220″ and output waveguide 210″, the polarization of the light energy from the laser can be transferred to be in the desired direction. Thus, energy having the desired polarization can be provided to the NFT (not shown in FIG. 5). Thus, performance of the HAMR disk drive 200″ may be improved.



FIG. 6 depicts a cross-sectional view of another exemplary embodiment of a portion of the HAMR write apparatus 200′″. For clarity, FIG. 6 is not to scale. For simplicity not all portions of the HAMR disk drive 200′″ are shown. In addition, although the HAMR write apparatus 200′″ is depicted in the context of particular components other and/or different components may be used. Further, the arrangement of components may vary in different embodiments. The HAMR write apparatus 200′″ is analogous to the HAMR writers 100, 100′, 200, 200′ and/or 200″. Thus, similar components have similar labels as in FIGS. 3A-5. The direction of transmission of light is out of the plane of the page in FIG. 6 (e.g. toward the ABS).


The HAMR write apparatus includes a laser (not shown), an NFT (not shown), a write pole (not shown) for writing to the media, a coil and two waveguides 210′″ and 220′″. The waveguides 210′″ and 220′″ are analogous to the waveguides 210/210′/210″ and 220/220′/220″, respectively, as well as the waveguides 140 and 140′. The waveguide 210′″ is the output waveguide in the embodiment shown, while the waveguide 220′″ is the input waveguide. The waveguide 210′″ includes a core 212 and cladding 214. The output waveguide 220″″ includes an input core 222 and cladding 224. In the embodiment depicted in FIG. 6 the layer 230 depicted in FIGS. 3A-5 is omitted.


The waveguides 210′″ and 220′″ are optically coupled and transfer the polarization from TE to TM. Thus, the aspect ratios of the cores differ in a manner analogous to that described above. The input core 222 has a height h1 and a width w1. The width is larger than the height for the input core 222 (w1>hh1). The output core 212 has a height h2 and w width w2. The height is larger than the width for the output core 212 (h2>w2). Thus, the aspect ratios differ. In the embodiment shown, the long axes of the cores 212 and 222 are perpendicular to each other (w1 is perpendicular to h2).


The waveguides 210′″ and 220′″ may be adiabatically coupled, directionally coupled or coupled in another manner. In addition, the cores 212 and 222 of the waveguides 210′″ and 220′″ are offset. As can be seen in FIG. 6, the cores 212 and 222 are offset in the width and height directions such that the cores 212 and 222 overlap by a distance o in the height direction and have their edges aligned in the width direction. In addition, the spacer layer 230 has been omitted. Different offsets in the height and/or width directions are possible.


The HAMR write apparatus 200′″ shares the benefits of the HAMR transducer(s) 100, 100′, 200, 200′ and/or 200″. Using the input waveguide 220″″ and output waveguide 210′″, the polarization of the light energy from the laser can be transferred to be in the desired direction. Thus, energy having the desired polarization can be provided to the NFT (not shown in FIG. 6). Thus, performance of the HAMR disk drive 200′″ may be improved.



FIG. 7 depicts a side view of another exemplary embodiment of a portion of the HAMR write apparatus 200″″. For clarity, FIG. 7 is not to scale. For simplicity not all portions of the HAMR disk drive 200″″ are shown. In addition, although the HAMR write apparatus 200′″″ is depicted in the context of particular components other and/or different components may be used. Further, the arrangement of components may vary in different embodiments. The HAMR write apparatus 200″″ is analogous to the HAMR writers 100, 100′, 200, 200′, 200″ and/or 200′″. Thus, similar components have similar labels as in FIGS. 3A-6. The direction of transmission of light is in the direction of the TE Mode and TM Mode arrows in FIG. 7.


The HAMR write apparatus includes a laser (not shown), an NFT (not shown), a write pole (not shown) for writing to the media, a coil and two waveguides 210″″ and 220″″. The waveguides 210″″ and 220″″ are analogous to the waveguides 210/210′/210″/210′″ and 220/220′/220″/220′″, respectively, as well as the waveguides 140 and 140′. The waveguide 210″″ is the output waveguide in the embodiment shown, while the waveguide 220″″ is the input waveguide. The waveguide 210″″ includes a core 212′ and cladding 214. The output waveguide 220″″ includes an input core 222′ and cladding 224. In the embodiment depicted in FIG. 7 the layer 230 depicted in FIGS. 3A-5 is not shown. The layer 230 might be omitted or might be included.


The waveguides 210″″ and 220″″ are optically coupled and transfer the polarization from TE to TM. Thus, the aspect ratios of the cores differ in a manner analogous to that described above. The waveguides 210′″ and 220′″ are adiabatically coupled in the embodiment shown in FIG. 7. Thus, the core 222′ of the input waveguide 220″″ terminates after the coupling region having length cl′. Similarly, the output waveguide 210″″ starts just before the coupling region. In the embodiment shown, the waveguides 210″″ and 220″″ taper near the ends shown. However, in other embodiments, the waveguides 210″″ and/or 220″″ may terminate in another manner.


The HAMR write apparatus 200″″ shares the benefits of the HAMR transducer(s) 100, 100′, 200, 200′, 200″ and/or 200′″. Using the input waveguide 220″″ and output waveguide 210″″, the polarization of the light energy from the laser can be transferred to be in the desired direction. Further, use of adiabatic coupling allows reduces the need for phase matching between the waveguides 210″″ and 220″″. In addition, the waveguides 210″″ and 220″″ may be easier to fabricate because tolerances for the waveguides 210′″ and 220″″ may be relaxed. Thus, energy having the desired polarization can be provided to the NFT (not shown in FIG. 7). Thus, performance of the HAMR disk drive 200″″ may be improved.



FIG. 8 depicts a side view of another exemplary embodiment of a portion of the HAMR write apparatus 200′″″. For clarity, FIG. 8 is not to scale. For simplicity not all portions of the HAMR disk drive 200′″″ are shown. In addition, although the HAMR write apparatus 200″″″ is depicted in the context of particular components other and/or different components may be used. Further, the arrangement of components may vary in different embodiments. The HAMR write apparatus 200′″″ is analogous to the HAMR writers 100, 100′, 200, 200′, 200″, 200″″ and/or 200″″. Thus, similar components have similar labels as in FIGS. 3A-7. The direction of transmission of light is in the direction of the TE Mode and TM Mode arrows in FIG. 8.


The HAMR write apparatus includes a laser (not shown), an NFT (not shown), a write pole (not shown) for writing to the media, a coil and two waveguides 210″″ and 220′″″. The waveguides 210′″″ and 220′″″ are analogous to the waveguides 210/210′/210″/210′″/210″″ and 220/220′/220″/220′″/220″″, respectively, as well as the waveguides 140 and 140′. The waveguide 210′″″ is the output waveguide in the embodiment shown, while the waveguide 220′″″ is the input waveguide. The waveguide 210′″″ includes a core 212″ and cladding 214. The output waveguide 220′″″ includes an input core 222″ and cladding 224. In the embodiment depicted in FIG. 8 the layer 230 depicted in FIGS. 3A-5 is not shown. The layer 230 might be omitted or might be included.


The waveguides 210′″″ and 220′″″ are optically coupled and transfer the polarization from TE to TM. Thus, the aspect ratios of the cores differ in a manner analogous to that described above. The core 222″ of the input waveguide 220′″″ does not terminates after the coupling region having length cl′. However, the output waveguide 210′″″ starts just before the coupling region. In an alternate embodiment, the input waveguide 220′″″ might terminate after the coupling region while the output waveguide 210″″ does not. Thus, the embodiment shown in FIG. 8 may be considered a combination of the transducer 200 and 200″″. In the embodiment shown, the waveguide 220′″″ tapers near the end shown. However, in other embodiments, the waveguide 220′″″ may terminate in another manner.


The HAMR write apparatus 200′″″ shares the benefits of the HAMR transducer(s) 100, 100′, 200, 200′, 200″, 200′″ and/or 200″″. Using the input waveguide 220′″″ and output waveguide 210′″″, the polarization of the light energy from the laser can be transferred to be in the desired direction. Thus, energy having the desired polarization can be provided to the NFT (not shown in FIG. 8). Thus, performance of the HAMR disk drive 200′″″ may be improved.


It is noted that various configurations of waveguides 140, 140′, 210/220, 210′/220′, 210″/220″, 210′″/220′″, 210″″/220″″ and 210′″″/220′″″ are highlighted in FIGS. 3A-8. However, various characteristics of the waveguides 140, 140′, 210/220, 210′/220′, 210″/220″, 210′″/220′″, 210″″/220″″ and/or 210′″″/220′″″ may be combined in a manner not inconsistent with the discussion herein.



FIG. 9 is a flow chart depicting an exemplary embodiment of a method 300 for fabricating a HAMR write apparatus. The method 300 may be used in fabricating disk drives such as the disk drives 100, 100′, 200, 200′, 200″, 200′″, 200″″ and/or 200′″″, though other transducers might be so fabricated. For clarity, the method 300 is described in the context of the writers 100 and 100′ depicted in FIGS. 1 and 2. For simplicity, some steps may be omitted, performed in another order, interleaved and/or combined. The HAMR writers being fabricated may include a writer and a read transducer (not shown) and resides on a slider. For simplicity, however, the reader is not discussed. The method 300 is also described in the context of forming a transducer. However, the method 300 may be used to fabricate multiple transducer(s) at substantially the same time. The method 300 and system are also described in the context of particular layers. However, in some embodiments, such layers may include multiple sub-layers. The method 300 also may commence after formation of other portions of the disk drive.


A main pole 150 is provided. Step 150 may include multiple substeps such as forming a trench for the main pole in a layer, plating the high saturation magnetization material(s) for the main pole and planarizing these materials.


At least one coil 155 for energizing the main pole is provided, via step 304. Step 304 generally includes multiple deposition and removal steps to form the coil. The coil 155 may be a spiral coil, a toroidal coil or have another shape.


The waveguides 140/140′ are also provided, via step 306. The waveguides 140/140′ include an input waveguide such as the waveguide 142 and an output waveguide 144. The waveguides 140/140′ provided in step 306 receive energy from the laser 172 and for direct the energy toward the ABS. The waveguides 140/140′ are optically coupled and configured to transfer the polarization of the energy from the input polarization state to the output polarization state. For example, the waveguides may be configured to transfer the energy from a TE mode to a TM mode.


Using the method 300, the HAMR devices 100, 100′, 200, 200′, 200″, 200′″, 200″″ and/or 200′″″ may be fabricated. The benefit(s) of one or more of the HAMR writer(s) 100, 100′, 200, 200′, 200″, 200′″, 200″″ and/or 200′″″ may thus be achieved.



FIG. 10 is a flow chart depicting an exemplary embodiment of a method 310 for fabricating a portion of a HAMR writer. For example, the method 310 may primarily be used in forming the waveguides 140, 140′, 210/220, 210′/220′, 210″/220″, 210′″/220′″, 210″″/220″″ and/or 210′″″/220′″″. However, other waveguides might be fabricated. For clarity, the method 310 is described in the context of the writer 100′ depicted in FIG. 2. For simplicity, some steps may be omitted, performed in another order, interleaved and/or combined. The HAMR writers being fabricated may include a writer and a read transducer (not shown) and resides on a slider. For simplicity, however, the reader is not discussed. The method 310 is also described in the context of forming a transducer. However, the method 310 may be used to fabricate multiple transducer(s) at substantially the same time. The method 310 and system are also described in the context of particular layers. However, in some embodiments, such layers may include multiple sub-layers. The method 310 also may commence after formation of other portions of the disk drive.


The input waveguide 142 configured for TE light is provided, via step 312. Step 312 typically includes forming a core having the appropriate geometry and substantially surrounding the core with cladding.


The output waveguide 144 is provided, via step 314. The output waveguide configured such that it is optically coupled with the input waveguide 142 and so that the light carried by the output waveguide 144 has a TM polarization.


Using the method 310, the waveguides for the HAMR devices 100, 100′, 200, 200′, 200″, 200′″, 200″″ and/or 200′″″ may be fabricated. The benefit(s) of one or more of the HAMR writer(s) 100, 100′, 200, 200′, 200″, 200′″, 200″″ and/or 200′″″ may thus be achieved.



FIG. 11 is a flow chart depicting an exemplary embodiment of a method 320 for fabricating a portion of a HAMR writer. For example, the method 320 may primarily be used in forming the waveguides 140, 140′, 210/220, 210′/220′, 210″/220″, 210′″/220′″, 210″″/220″″ and/or 210′″″/220′″″. However, other waveguides might be fabricated. FIGS. 12-17 depict a portion of a HAMR write apparatus 350 during fabrication of the waveguides using the method 320. FIGS. 12-17 are not to scale and not all components of the writer 350 are shown. For simplicity, some steps may be omitted, performed in another order, interleaved and/or combined. The HAMR writers being fabricated may include a writer and a read transducer (not shown) and resides on a slider. However, the reader is not discussed. The method 320 is also described in the context of forming a single transducer. However, the method 320 may be used to fabricate multiple transducer(s) at substantially the same time. The method 320 and system are also described in the context of particular layers. However, in some embodiments, such layers may include multiple sub-layers. The method 320 also may commence after formation of other portions of the disk drive.


The core of the lower waveguide (closer to the underlying substrate) is provided, via step 322. Step 322 may include depositing a material having the desired index of refraction, such as tantalum oxide. The regions desired to form the core are then covered in a mask and the exposed regions removed. FIG. 12 depicts a cross-sectional view of the writer 350 after step 322 is performed. Thus, the core 362 of the lower waveguide 360 is formed on the underlying cladding. Note that this lower waveguide 360 could be the input waveguide, the output waveguide or another waveguide (if any) between the input and output waveguides.


A layer of cladding for the lower waveguide is provided, via step 324. Step 324 may include blanket depositing a cladding material, such as silicon oxide, then planarizing the material. FIGS. 13-14 depict the writer 350 during and after step 324. The cladding layer 364 is shown as being deposited in FIG. 13. Thus, the cladding 364 covers the lower core 362. FIG. 14 depicts the transducer 350 after the device has been planarized. Thus, the top surfaces of the core 362 and cladding 364 are substantially flat.


An etch stop layer is optionally deposited, via step 326. The etch stop layer is resistant to removal by an etch that removes the upper core and/or upper cladding. For example, an aluminum oxide layer that is nominally twenty nanometers thick may be provided in step 326. FIG. 15 depicts the writer 350 after step 326 is performed. Thus, the stop layer 370 is shown. In other embodiments, step 326, and thus the etch stop layer 370, may be omitted.


The core of the upper waveguide (further from the underlying substrate) is provided, via step 328. Step 328 may include depositing a material having the desired index of refraction, such as tantalum oxide. The regions desired to form the core are then covered in a mask and the exposed regions removed. The etch stop layer 370 may prevent damage to the underlying core 362 during formation of the core. FIG. 16 depicts a cross-sectional view of the writer 350 after step 326 is performed. Thus, the core 382 of the upper waveguide 380 is formed on the cladding 364 and core 362. Note that this upper waveguide 380 could be the input waveguide, the output waveguide or another waveguide (if any) between the input and output waveguides. In addition, particular offsets between the lower core 362 and upper core 382 are shown in FIGS. 16-17. In other embodiments, different offsets may be used.


A layer of cladding for the upper waveguide 380 is provided, via step 330. Step 330 may include blanket depositing a cladding material, such as silicon oxide, then planarizing the material. FIG. 17 depict the writer 350 after step 330. The cladding layer 384 for the upper waveguide 380 is shown. Thus, the cladding 384 covers the upper core 382 and etch stop layer 370.


Using the method 320, the HAMR writer 350 may be fabricated. The writer 350 is analogous to the writers 100, 100′, 200, 200′, 200″, 200′″, 200′″, and/or 200″″. Performance and/or reliability of the disk drive 350 may thus be improved in a manner analogous to the HAMR disk drives 100, 100′, 200, 200′, 200″, 200′″, 200″″ and/or 200′″″.

Claims
  • 1. A heat assisted magnetic recording (HAMR) write apparatus coupled with a laser for providing energy having a first polarization state, the HAMR write apparatus including an air-bearing surface (ABS) configured to reside in proximity to a media during use and comprising: a main pole;at least one coil for energizing the main pole; anda plurality of waveguides for receiving the energy from the laser and for directing the energy toward the ABS, the plurality of waveguides including an input waveguide and an output waveguide, the input waveguide configured to carry light having the first polarization state, the output waveguide configured to carry light having a second polarization state different from the first polarization state, the plurality of waveguides being optically coupled and configured to transfer the energy from the first polarization state to the second polarization state, the input waveguide having an input long axis and an input short axis in a first plane perpendicular to a first direction of energy propagation in the input waveguide, the output waveguide having an output long axis and an output short axis in a second plane perpendicular to a second direction of energy propagation in the output waveguide, the input long axis being substantially perpendicular to the output long axis.
  • 2. The HAMR write apparatus of claim 1 further comprising: a near-field transducer (NFT) proximate to the ABS for focusing the energy onto a region of the media, the NFT being optically coupled with the output waveguide and receiving the energy having the second polarization state.
  • 3. The HAMR write apparatus of claim 2 wherein the plurality of waveguides consists of the input waveguide and the output waveguide coupled with the input waveguide.
  • 4. The HAMR write apparatus of claim 3 wherein the plurality of waveguides include at least one of a plurality of directionally coupled waveguides and a plurality of adiabatically coupled waveguides.
  • 5. The HAMR write apparatus of claim 1 wherein the input waveguide and the output waveguide are offset in a direction perpendicular to the first direction and the second direction in a coupling region for the input waveguide and the output waveguide.
  • 6. The HAMR write apparatus of claim 5 wherein the input waveguide and the output waveguide are offset by not more than the input long axis.
  • 7. The HAMR write apparatus of claim 5 wherein the input waveguide and the output waveguide are offset by not more than the output short axis.
  • 8. The HAMR write apparatus of claim 5 wherein the coupling region has a coupling length in the direction of transmission and wherein the first direction of propagation and the second direction of propagation are equal in the coupling region.
  • 9. The HAMR write apparatus of claim 8 wherein at least one of the input waveguide and the output waveguide tapers along the coupling length such that the at least one of the input waveguide terminates at a first end of the coupling length and the output waveguide terminates at a second end of the coupling length opposite to the first end.
  • 10. A heat assisted magnetic recording (HAMR) disk drive comprising: a media;a laser for providing energy having a first polarization state;a slider having an air-bearing surface (ABS) and a HAMR write transducer, the HAMR write transducer including a main pole, at least one coil for energizing the main pole and a plurality of waveguides, the plurality of waveguides receiving the energy from the laser and directing the energy toward the ABS, the plurality of waveguides including an input waveguide and an output waveguide, the input waveguide configured to carry light from the laser having the first polarization state, the output waveguide configured to carry light having a second polarization state different from the first polarization state, the plurality of waveguides being optically coupled and configured to transfer the energy from the first polarization state to the second polarization state, the input waveguide having an input long axis and an input short axis in a first plane perpendicular to a first direction of energy propagation in the input waveguide, the output waveguide having an output long axis and an output short axis in a second plane perpendicular to a second direction of energy propagation in the output waveguide, the input long axis being substantially perpendicular to the output long axis.
  • 11. The HAMR disk drive of claim 10 wherein the HAMR write transducer further includes: a near-field transducer (NFT) proximate to the ABS and for focusing the energy onto a region of the media, the NFT being optically coupled with the output waveguide and receiving energy having the second polarization state.
  • 12. The HAMR disk drive of claim 11 wherein the plurality of waveguides consists of the input waveguide and the output waveguide coupled with the input waveguide, wherein the input waveguide and the output waveguide are offset in a direction perpendicular to the first direction and the second direction in a coupling region for the input waveguide and the output waveguide.
  • 13. A method for fabricating a heat assisted magnetic recording (HAMR) write apparatus coupled with a laser for providing energy having a first polarization state, the HAMR write apparatus including an air-bearing surface (ABS) configured to reside in proximity to a media during use, the method comprising: providing a main pole;providing at least one coil for energizing the main pole; andproviding a plurality of waveguides for receiving the energy from the laser and for directing the energy toward the ABS, the plurality of waveguides including an input waveguide and an output waveguide, the input waveguide configured to carry light having the first polarization state, the output waveguide configured to carry light having a second polarization state different from the first polarization state, the plurality of waveguides being optically coupled and configured to transfer the energy from the first polarization state to the second polarization state, the input waveguide having an input long axis and an input short axis in a first plane perpendicular to a first direction of energy propagation in the input waveguide, the output waveguide having an output long axis and an output short axis in a second plane perpendicular to a second direction of energy propagation in the output waveguide, the input long axis being substantially perpendicular to the output long axis.
  • 14. The method of claim 13 further comprising: providing a near-field transducer (NFT) proximate to the ABS and for focusing the energy onto a region of the media, the NFT being optically coupled with the output waveguide and receiving energy having the second polarization state.
  • 15. The method of claim 13 wherein the input waveguide and the output waveguide are offset in a direction perpendicular to the first direction and the second direction in a coupling region for the input waveguide and the output waveguide.
  • 16. The method of claim 15 wherein the step of providing the plurality of waveguides includes at least one of providing a plurality of directionally coupled waveguides and providing a plurality of adiabatically coupled waveguides.
  • 17. A heat assisted magnetic recording (HAMR) write apparatus coupled with a laser for providing energy having a first polarization state, the HAMR write apparatus including an air-bearing surface (ABS) configured to reside in proximity to a media during use and comprising: a main pole;at least one coil for energizing the main pole; anda plurality of waveguides for receiving the energy from the laser and for directing the energy toward the ABS, the plurality of waveguides including an input waveguide and an output waveguide, the input waveguide configured to carry light having the first polarization state, the output waveguide configured to carry light having a second polarization state different from the first polarization state, the plurality of waveguides being optically coupled and configured to transfer the energy from the first polarization state to the second polarization state, the input waveguide having an input long axis and an input short axis in a first plane perpendicular to a first direction of energy propagation in the input waveguide, the output waveguide having an output long axis and an output short axis in a second plane perpendicular to a second direction of energy propagation in the output waveguide, the input long axis being substantially perpendicular to the output long axis, the input waveguide and the output waveguide being offset in a direction perpendicular to the first direction and the second direction in a coupling region for the input waveguide and the output waveguide;wherein the input waveguide and the output waveguide are separated by an etch stop layer.
  • 18. A method for fabricating a heat assisted magnetic recording (HAMR) write apparatus coupled with a laser for providing energy having a first polarization state, the HAMR write apparatus including an air-bearing surface (ABS) configured to reside in proximity to a media during use, the method comprising: providing a main pole;providing at least one coil for energizing the main pole; andproviding a plurality of waveguides for receiving the energy from the laser and for directing the energy toward the ABS, the plurality of waveguides including an input waveguide and an output waveguide, the input waveguide configured to carry light having the first polarization state, the output waveguide configured to carry light having a second polarization state different from the first polarization state, the plurality of waveguides being optically coupled and configured to transfer the energy from the first polarization state to the second polarization state, the input waveguide having an input long axis and an input short axis in a first plane perpendicular to a first direction of energy propagation in the input waveguide, the output waveguide having an output long axis and an output short axis in a second plane perpendicular to a second direction of energy propagation in the output waveguide, the input long axis being substantially perpendicular to the output long axis, the input waveguide and the output waveguide being offset in a direction perpendicular to the first direction and the second direction in a coupling region for the input waveguide and the output waveguide, wherein the step of providing the plurality of waveguides further includes: providing an output waveguide core for the output waveguide;providing cladding surrounding at least a portion of the output waveguide core;depositing an etch stop layer on at least the output waveguide core;depositing an input waveguide core layer for the input waveguide;removing an extraneous portion of the input waveguide core layer, an input waveguide core for the input waveguide including a remaining portion of the input waveguide core layer; anddepositing an additional cladding layer covering at least the input waveguide core.
  • 19. A method for fabricating a heat assisted magnetic recording (HAMR) write apparatus coupled with a laser for providing energy having a first polarization state, the HAMR write apparatus including an air-bearing surface (ABS) configured to reside in proximity to a media during use, the method comprising: providing a main pole;providing at least one coil for energizing the main pole; andproviding a plurality of waveguides for receiving the energy from the laser and for directing the energy toward the ABS, the plurality of waveguides including an input waveguide and an output waveguide, the input waveguide configured to carry light having the first polarization state, the output waveguide configured to carry light having a second polarization state different from the first polarization state, the plurality of waveguides being optically coupled and configured to transfer the energy from the first polarization state to the second polarization state, the input waveguide having an input long axis and an input short axis in a first plane perpendicular to a first direction of energy propagation in the input waveguide, the output waveguide having an output long axis and an output short axis in a second plane perpendicular to a second direction of energy propagation in the output waveguide, the input long axis being substantially perpendicular to the output long axis, the input waveguide and the output waveguide being offset in a direction perpendicular to the first direction and the second direction in a coupling region for the input waveguide and the output waveguide, wherein the step of providing the plurality of waveguides further includes: providing an input waveguide core for the input waveguide;providing cladding surrounding at least a portion of the input waveguide core;depositing an etch stop layer on at least the input waveguide core;depositing an output waveguide core layer for the output waveguide;removing an extraneous portion of the output waveguide core layer, an output waveguide core for the output waveguide including a remaining portion of output waveguide core layer; anddepositing an additional cladding layer covering at least the output waveguide core.
US Referenced Citations (622)
Number Name Date Kind
6011641 Shin et al. Jan 2000 A
6016290 Chen et al. Jan 2000 A
6018441 Wu et al. Jan 2000 A
6025978 Hoshi et al. Feb 2000 A
6025988 Yan Feb 2000 A
6032353 Hiner et al. Mar 2000 A
6033532 Minami Mar 2000 A
6034851 Zarouri et al. Mar 2000 A
6043959 Crue et al. Mar 2000 A
6046885 Aimonetti et al. Apr 2000 A
6049650 Jerman et al. Apr 2000 A
6055138 Shi Apr 2000 A
6058094 Davis et al. May 2000 A
6073338 Liu et al. Jun 2000 A
6078479 Nepela et al. Jun 2000 A
6081499 Berger et al. Jun 2000 A
6094803 Carlson et al. Aug 2000 A
6099362 Viches et al. Aug 2000 A
6103073 Thayamballi Aug 2000 A
6108166 Lederman Aug 2000 A
6118629 Huai et al. Sep 2000 A
6118638 Knapp et al. Sep 2000 A
6125018 Takagishi et al. Sep 2000 A
6130779 Carlson et al. Oct 2000 A
6134089 Barr et al. Oct 2000 A
6136166 Shen et al. Oct 2000 A
6137661 Shi et al. Oct 2000 A
6137662 Huai et al. Oct 2000 A
6160684 Heist et al. Dec 2000 A
6163426 Nepela et al. Dec 2000 A
6166891 Lederman et al. Dec 2000 A
6173486 Hsiao et al. Jan 2001 B1
6175476 Huai et al. Jan 2001 B1
6178066 Barr Jan 2001 B1
6178070 Hong et al. Jan 2001 B1
6178150 Davis Jan 2001 B1
6181485 He Jan 2001 B1
6181525 Carlson Jan 2001 B1
6185051 Chen et al. Feb 2001 B1
6185077 Tong et al. Feb 2001 B1
6185081 Simion et al. Feb 2001 B1
6188549 Wiitala Feb 2001 B1
6190764 Shi et al. Feb 2001 B1
6193584 Rudy et al. Feb 2001 B1
6195229 Shen et al. Feb 2001 B1
6198608 Hong et al. Mar 2001 B1
6198609 Barr et al. Mar 2001 B1
6201673 Rottmayer et al. Mar 2001 B1
6204998 Katz Mar 2001 B1
6204999 Crue et al. Mar 2001 B1
6212153 Chen et al. Apr 2001 B1
6215625 Carlson Apr 2001 B1
6219205 Yuan et al. Apr 2001 B1
6221218 Shi et al. Apr 2001 B1
6222707 Huai et al. Apr 2001 B1
6229782 Wang et al. May 2001 B1
6230959 Heist et al. May 2001 B1
6233116 Chen et al. May 2001 B1
6233125 Knapp et al. May 2001 B1
6237215 Hunsaker et al. May 2001 B1
6252743 Bozorgi Jun 2001 B1
6255721 Roberts Jul 2001 B1
6258468 Mahvan et al. Jul 2001 B1
6266216 Hikami et al. Jul 2001 B1
6271604 Frank, Jr. et al. Aug 2001 B1
6275354 Huai et al. Aug 2001 B1
6277505 Shi et al. Aug 2001 B1
6282056 Feng et al. Aug 2001 B1
6296955 Hossain et al. Oct 2001 B1
6297955 Frank, Jr. et al. Oct 2001 B1
6304414 Crue, Jr. et al. Oct 2001 B1
6307715 Berding et al. Oct 2001 B1
6310746 Hawwa et al. Oct 2001 B1
6310750 Hawwa et al. Oct 2001 B1
6317290 Wang et al. Nov 2001 B1
6317297 Tong et al. Nov 2001 B1
6322911 Fukagawa et al. Nov 2001 B1
6330136 Wang et al. Dec 2001 B1
6330137 Knapp et al. Dec 2001 B1
6333830 Rose et al. Dec 2001 B2
6340533 Ueno et al. Jan 2002 B1
6349014 Crue, Jr. et al. Feb 2002 B1
6351355 Min et al. Feb 2002 B1
6353318 Sin et al. Mar 2002 B1
6353511 Shi et al. Mar 2002 B1
6356412 Levi et al. Mar 2002 B1
6359779 Frank, Jr. et al. Mar 2002 B1
6369983 Hong Apr 2002 B1
6376964 Young et al. Apr 2002 B1
6377535 Chen et al. Apr 2002 B1
6381095 Sin et al. Apr 2002 B1
6381105 Huai et al. Apr 2002 B1
6389499 Frank, Jr. et al. May 2002 B1
6392850 Tong et al. May 2002 B1
6396660 Jensen et al. May 2002 B1
6399179 Hanrahan et al. Jun 2002 B1
6400526 Crue, Jr. et al. Jun 2002 B2
6404600 Hawwa et al. Jun 2002 B1
6404601 Rottmayer et al. Jun 2002 B1
6404706 Stovall et al. Jun 2002 B1
6410170 Chen et al. Jun 2002 B1
6411522 Frank, Jr. et al. Jun 2002 B1
6417998 Crue, Jr. et al. Jul 2002 B1
6417999 Knapp et al. Jul 2002 B1
6418000 Gibbons et al. Jul 2002 B1
6418048 Sin et al. Jul 2002 B1
6421211 Hawwa et al. Jul 2002 B1
6421212 Gibbons et al. Jul 2002 B1
6424505 Lam et al. Jul 2002 B1
6424507 Lederman et al. Jul 2002 B1
6430009 Komaki et al. Aug 2002 B1
6430806 Chen et al. Aug 2002 B1
6433965 Gopinathan et al. Aug 2002 B1
6433968 Shi et al. Aug 2002 B1
6433970 Knapp et al. Aug 2002 B1
6437945 Hawwa et al. Aug 2002 B1
6445536 Rudy et al. Sep 2002 B1
6445542 Levi et al. Sep 2002 B1
6445553 Barr et al. Sep 2002 B2
6445554 Dong et al. Sep 2002 B1
6447935 Zhang et al. Sep 2002 B1
6448765 Chen et al. Sep 2002 B1
6451514 Iitsuka Sep 2002 B1
6452742 Crue et al. Sep 2002 B1
6452765 Mahvan et al. Sep 2002 B1
6456465 Louis et al. Sep 2002 B1
6459552 Liu et al. Oct 2002 B1
6462920 Karimi Oct 2002 B1
6466401 Hong et al. Oct 2002 B1
6466402 Crue, Jr. et al. Oct 2002 B1
6466404 Crue, Jr. et al. Oct 2002 B1
6468436 Shi et al. Oct 2002 B1
6469877 Knapp et al. Oct 2002 B1
6477019 Matono et al. Nov 2002 B2
6479096 Shi et al. Nov 2002 B1
6483662 Thomas et al. Nov 2002 B1
6487040 Hsiao et al. Nov 2002 B1
6487056 Gibbons et al. Nov 2002 B1
6490125 Barr Dec 2002 B1
6496330 Crue, Jr. et al. Dec 2002 B1
6496334 Pang et al. Dec 2002 B1
6504676 Hiner et al. Jan 2003 B1
6512657 Heist et al. Jan 2003 B2
6512659 Hawwa et al. Jan 2003 B1
6512661 Louis Jan 2003 B1
6512690 Qi et al. Jan 2003 B1
6515573 Dong et al. Feb 2003 B1
6515791 Hawwa et al. Feb 2003 B1
6532823 Knapp et al. Mar 2003 B1
6535363 Hosomi et al. Mar 2003 B1
6552874 Chen et al. Apr 2003 B1
6552928 Qi et al. Apr 2003 B1
6577470 Rumpler Jun 2003 B1
6583961 Levi et al. Jun 2003 B2
6583968 Scura et al. Jun 2003 B1
6597548 Yamanaka et al. Jul 2003 B1
6611398 Rumpler et al. Aug 2003 B1
6618223 Chen et al. Sep 2003 B1
6629357 Akoh Oct 2003 B1
6633464 Lai et al. Oct 2003 B2
6636394 Fukagawa et al. Oct 2003 B1
6639291 Sin et al. Oct 2003 B1
6650503 Chen et al. Nov 2003 B1
6650506 Risse Nov 2003 B1
6654195 Frank, Jr. et al. Nov 2003 B1
6657816 Barr et al. Dec 2003 B1
6661621 Iitsuka Dec 2003 B1
6661625 Sin et al. Dec 2003 B1
6674610 Thomas et al. Jan 2004 B1
6680863 Shi et al. Jan 2004 B1
6683763 Hiner et al. Jan 2004 B1
6687098 Huai Feb 2004 B1
6687178 Qi et al. Feb 2004 B1
6687977 Knapp et al. Feb 2004 B2
6691226 Frank, Jr. et al. Feb 2004 B1
6697294 Qi et al. Feb 2004 B1
6700738 Sin et al. Mar 2004 B1
6700759 Knapp et al. Mar 2004 B1
6704158 Hawwa et al. Mar 2004 B2
6707083 Hiner et al. Mar 2004 B1
6713801 Sin et al. Mar 2004 B1
6721138 Chen et al. Apr 2004 B1
6721149 Shi et al. Apr 2004 B1
6721203 Qi et al. Apr 2004 B1
6724569 Chen et al. Apr 2004 B1
6724572 Stoev et al. Apr 2004 B1
6729015 Matono et al. May 2004 B2
6735850 Gibbons et al. May 2004 B1
6737281 Dang et al. May 2004 B1
6744608 Chen et al. Jun 2004 B1
6747301 Hiner et al. Jun 2004 B1
6751055 Alfoqaha et al. Jun 2004 B1
6754049 Seagle et al. Jun 2004 B1
6756071 Shi et al. Jun 2004 B1
6757140 Hawwa Jun 2004 B1
6760196 Niu et al. Jul 2004 B1
6762910 Knapp et al. Jul 2004 B1
6765756 Hong et al. Jul 2004 B1
6775902 Huai et al. Aug 2004 B1
6778358 Jiang et al. Aug 2004 B1
6781927 Heanuc et al. Aug 2004 B1
6785955 Chen et al. Sep 2004 B1
6791793 Chen et al. Sep 2004 B1
6791807 Hikami et al. Sep 2004 B1
6798616 Seagle et al. Sep 2004 B1
6798625 Ueno et al. Sep 2004 B1
6801408 Chen et al. Oct 2004 B1
6801411 Lederman et al. Oct 2004 B1
6803615 Sin et al. Oct 2004 B1
6806035 Atireklapvarodom et al. Oct 2004 B1
6807030 Hawwa et al. Oct 2004 B1
6807332 Hawwa Oct 2004 B1
6809899 Chen et al. Oct 2004 B1
6816345 Knapp et al. Nov 2004 B1
6828897 Nepela Dec 2004 B1
6829160 Qi et al. Dec 2004 B1
6829819 Crue, Jr. et al. Dec 2004 B1
6833979 Spallas et al. Dec 2004 B1
6834010 Qi et al. Dec 2004 B1
6853758 Ridgway et al. Feb 2005 B2
6859343 Alfoqaha et al. Feb 2005 B1
6859997 Tong et al. Mar 2005 B1
6861937 Feng et al. Mar 2005 B1
6870712 Chen et al. Mar 2005 B2
6873494 Chen et al. Mar 2005 B2
6873547 Shi et al. Mar 2005 B1
6879464 Sun et al. Apr 2005 B2
6888184 Shi et al. May 2005 B1
6888704 Diao et al. May 2005 B1
6891702 Tang May 2005 B1
6894871 Alfoqaha et al. May 2005 B2
6894877 Crue, Jr. et al. May 2005 B1
6906894 Chen et al. Jun 2005 B2
6909578 Missell et al. Jun 2005 B1
6912106 Chen et al. Jun 2005 B1
6934113 Chen Aug 2005 B1
6934129 Zhang et al. Aug 2005 B1
6940688 Jiang et al. Sep 2005 B2
6942824 Li Sep 2005 B1
6943993 Chang et al. Sep 2005 B2
6944938 Crue, Jr. et al. Sep 2005 B1
6947258 Li Sep 2005 B1
6950266 McCaslin et al. Sep 2005 B1
6954332 Hong et al. Oct 2005 B1
6958885 Chen et al. Oct 2005 B1
6961221 Niu et al. Nov 2005 B1
6969989 Mei Nov 2005 B1
6975486 Chen et al. Dec 2005 B2
6987643 Seagle Jan 2006 B1
6989962 Dong et al. Jan 2006 B1
6989972 Stoev et al. Jan 2006 B1
7006327 Krounbi et al. Feb 2006 B2
7007372 Chen et al. Mar 2006 B1
7012832 Sin et al. Mar 2006 B1
7023658 Knapp et al. Apr 2006 B1
7026063 Ueno et al. Apr 2006 B2
7027268 Zhu et al. Apr 2006 B1
7027274 Sin et al. Apr 2006 B1
7035046 Young et al. Apr 2006 B1
7041985 Wang et al. May 2006 B1
7046490 Ueno et al. May 2006 B1
7054113 Seagle et al. May 2006 B1
7057857 Niu et al. Jun 2006 B1
7059868 Yan Jun 2006 B1
7092195 Liu et al. Aug 2006 B1
7110289 Sin et al. Sep 2006 B1
7111382 Knapp et al. Sep 2006 B1
7113366 Wang et al. Sep 2006 B1
7114241 Kubota et al. Oct 2006 B2
7116517 He et al. Oct 2006 B1
7124654 Davies et al. Oct 2006 B1
7126788 Liu et al. Oct 2006 B1
7126790 Liu et al. Oct 2006 B1
7131346 Buttar et al. Nov 2006 B1
7133253 Seagle et al. Nov 2006 B1
7134185 Knapp et al. Nov 2006 B1
7151789 Jette et al. Dec 2006 B2
7154715 Yamanaka et al. Dec 2006 B2
7170725 Zhou et al. Jan 2007 B1
7177117 Jiang et al. Feb 2007 B1
7190850 Mimura et al. Mar 2007 B2
7193815 Stoev et al. Mar 2007 B1
7196880 Anderson et al. Mar 2007 B1
7199974 Alfoqaha Apr 2007 B1
7199975 Pan Apr 2007 B1
7211339 Seagle et al. May 2007 B1
7212384 Stoev et al. May 2007 B1
7238292 He et al. Jul 2007 B1
7239478 Sin et al. Jul 2007 B1
7248431 Liu et al. Jul 2007 B1
7248433 Stoev et al. Jul 2007 B1
7248449 Seagle Jul 2007 B1
7280325 Pan Oct 2007 B1
7283327 Liu et al. Oct 2007 B1
7284316 Huai et al. Oct 2007 B1
7286329 Chen et al. Oct 2007 B1
7289303 Sin et al. Oct 2007 B1
7292409 Stoev et al. Nov 2007 B1
7296339 Yang et al. Nov 2007 B1
7307814 Seagle et al. Dec 2007 B1
7307818 Park et al. Dec 2007 B1
7310204 Stoev et al. Dec 2007 B1
7318947 Park et al. Jan 2008 B1
7333295 Medina et al. Feb 2008 B1
7337530 Stoev et al. Mar 2008 B1
7342752 Zhang et al. Mar 2008 B1
7349170 Rudman et al. Mar 2008 B1
7349179 He et al. Mar 2008 B1
7354664 Jiang et al. Apr 2008 B1
7363697 Dunn et al. Apr 2008 B1
7371152 Newman May 2008 B1
7372665 Stoev et al. May 2008 B1
7375926 Stoev et al. May 2008 B1
7379269 Krounbi et al. May 2008 B1
7386933 Krounbi et al. Jun 2008 B1
7389577 Shang et al. Jun 2008 B1
7417832 Erickson et al. Aug 2008 B1
7419891 Chen et al. Sep 2008 B1
7428124 Song et al. Sep 2008 B1
7430098 Song et al. Sep 2008 B1
7436620 Kang et al. Oct 2008 B1
7436638 Pan Oct 2008 B1
7440220 Kang et al. Oct 2008 B1
7443632 Stoev et al. Oct 2008 B1
7444740 Chung et al. Nov 2008 B1
7493688 Wang et al. Feb 2009 B1
7508627 Zhang et al. Mar 2009 B1
7519254 Ramachandran Apr 2009 B2
7522377 Jiang et al. Apr 2009 B1
7522379 Krounbi et al. Apr 2009 B1
7522382 Pan Apr 2009 B1
7542246 Song et al. Jun 2009 B1
7551406 Thomas et al. Jun 2009 B1
7552523 He et al. Jun 2009 B1
7554767 Hu et al. Jun 2009 B1
7583466 Kermiche et al. Sep 2009 B2
7595967 Moon et al. Sep 2009 B1
7639457 Chen et al. Dec 2009 B1
7660080 Liu et al. Feb 2010 B1
7672080 Tang et al. Mar 2010 B1
7672086 Jiang Mar 2010 B1
7684160 Erickson et al. Mar 2010 B1
7688546 Bai et al. Mar 2010 B1
7691434 Zhang et al. Apr 2010 B1
7695761 Shen et al. Apr 2010 B1
7719795 Hu et al. May 2010 B2
7726009 Liu et al. Jun 2010 B1
7729086 Song et al. Jun 2010 B1
7729087 Stoev et al. Jun 2010 B1
7736823 Wang et al. Jun 2010 B1
7785666 Sun et al. Aug 2010 B1
7796356 Fowler et al. Sep 2010 B1
7800858 Bajikar et al. Sep 2010 B1
7819979 Chen et al. Oct 2010 B1
7829264 Wang et al. Nov 2010 B1
7846643 Sun et al. Dec 2010 B1
7855854 Hu et al. Dec 2010 B2
7869160 Pan et al. Jan 2011 B1
7872824 Macchioni et al. Jan 2011 B1
7872833 Hu et al. Jan 2011 B2
7910267 Zeng et al. Mar 2011 B1
7911735 Sin et al. Mar 2011 B1
7911737 Jiang et al. Mar 2011 B1
7916426 Hu et al. Mar 2011 B2
7918013 Dunn et al. Apr 2011 B1
7968219 Jiang et al. Jun 2011 B1
7982989 Shi et al. Jul 2011 B1
8008912 Shang Aug 2011 B1
8012804 Wang et al. Sep 2011 B1
8015692 Zhang et al. Sep 2011 B1
8018677 Chung et al. Sep 2011 B1
8018678 Zhang et al. Sep 2011 B1
8024748 Moravec et al. Sep 2011 B1
8072705 Wang et al. Dec 2011 B1
8074345 Anguelouch et al. Dec 2011 B1
8077418 Hu et al. Dec 2011 B1
8077434 Shen et al. Dec 2011 B1
8077435 Liu et al. Dec 2011 B1
8077557 Hu et al. Dec 2011 B1
8079135 Shen et al. Dec 2011 B1
8081403 Chen et al. Dec 2011 B1
8091210 Sasaki et al. Jan 2012 B1
8094978 Tokushima Jan 2012 B2
8097846 Anguelouch et al. Jan 2012 B1
8104166 Zhang et al. Jan 2012 B1
8116043 Leng et al. Feb 2012 B2
8116171 Lee Feb 2012 B1
8125856 Li et al. Feb 2012 B1
8134794 Wang Mar 2012 B1
8136224 Sun et al. Mar 2012 B1
8136225 Zhang et al. Mar 2012 B1
8136805 Lee Mar 2012 B1
8141235 Zhang Mar 2012 B1
8146236 Luo et al. Apr 2012 B1
8149536 Yang et al. Apr 2012 B1
8151441 Rudy et al. Apr 2012 B1
8163185 Sun et al. Apr 2012 B1
8164760 Willis Apr 2012 B2
8164855 Gibbons et al. Apr 2012 B1
8164864 Kaiser et al. Apr 2012 B2
8165709 Rudy Apr 2012 B1
8166631 Tran et al. May 2012 B1
8166632 Zhang et al. May 2012 B1
8169473 Yu et al. May 2012 B1
8171618 Wang et al. May 2012 B1
8179636 Bai et al. May 2012 B1
8191237 Luo et al. Jun 2012 B1
8194365 Leng et al. Jun 2012 B1
8194366 Li et al. Jun 2012 B1
8196285 Zhang et al. Jun 2012 B1
8200054 Li et al. Jun 2012 B1
8203800 Li et al. Jun 2012 B2
8208350 Hu et al. Jun 2012 B1
8220140 Wang et al. Jul 2012 B1
8222599 Chien Jul 2012 B1
8225488 Zhang et al. Jul 2012 B1
8227023 Liu et al. Jul 2012 B1
8228633 Tran et al. Jul 2012 B1
8231796 Li et al. Jul 2012 B1
8233248 Li et al. Jul 2012 B1
8248896 Yuan et al. Aug 2012 B1
8254060 Shi et al. Aug 2012 B1
8257597 Guan et al. Sep 2012 B1
8259410 Bai et al. Sep 2012 B1
8259539 Hu et al. Sep 2012 B1
8262918 Li et al. Sep 2012 B1
8262919 Luo et al. Sep 2012 B1
8264797 Emley Sep 2012 B2
8264798 Guan et al. Sep 2012 B1
8270126 Roy et al. Sep 2012 B1
8276258 Tran et al. Oct 2012 B1
8277669 Chen et al. Oct 2012 B1
8279719 Hu et al. Oct 2012 B1
8284517 Sun et al. Oct 2012 B1
8288204 Wang et al. Oct 2012 B1
8289821 Huber Oct 2012 B1
8291743 Shi et al. Oct 2012 B1
8307539 Rudy et al. Nov 2012 B1
8307540 Tran et al. Nov 2012 B1
8308921 Hiner et al. Nov 2012 B1
8310785 Zhang et al. Nov 2012 B1
8310901 Batra et al. Nov 2012 B1
8315019 Mao et al. Nov 2012 B1
8316527 Hong et al. Nov 2012 B2
8320076 Shen et al. Nov 2012 B1
8320077 Tang et al. Nov 2012 B1
8320219 Wolf et al. Nov 2012 B1
8320220 Yuan et al. Nov 2012 B1
8320722 Yuan et al. Nov 2012 B1
8322022 Yi et al. Dec 2012 B1
8322023 Zeng et al. Dec 2012 B1
8325569 Shi et al. Dec 2012 B1
8333008 Sin et al. Dec 2012 B1
8334093 Zhang et al. Dec 2012 B2
8336194 Yuan et al. Dec 2012 B2
8339738 Tran et al. Dec 2012 B1
8341826 Jiang et al. Jan 2013 B1
8343319 Li et al. Jan 2013 B1
8343364 Gao et al. Jan 2013 B1
8349195 Si et al. Jan 2013 B1
8351307 Wolf et al. Jan 2013 B1
8357244 Zhao et al. Jan 2013 B1
8373945 Luo et al. Feb 2013 B1
8375564 Luo et al. Feb 2013 B1
8375565 Hu et al. Feb 2013 B2
8381391 Park et al. Feb 2013 B2
8385157 Champion et al. Feb 2013 B1
8385158 Hu et al. Feb 2013 B1
8394280 Wan et al. Mar 2013 B1
8400731 Li et al. Mar 2013 B1
8404128 Zhang et al. Mar 2013 B1
8404129 Luo et al. Mar 2013 B1
8405930 Li et al. Mar 2013 B1
8409453 Jiang et al. Apr 2013 B1
8413317 Wan et al. Apr 2013 B1
8416540 Li et al. Apr 2013 B1
8419953 Su et al. Apr 2013 B1
8419954 Chen et al. Apr 2013 B1
8422176 Leng et al. Apr 2013 B1
8422342 Lee Apr 2013 B1
8422841 Shi et al. Apr 2013 B1
8424192 Yang et al. Apr 2013 B1
8441756 Sun et al. May 2013 B1
8443510 Shi et al. May 2013 B1
8444866 Guan et al. May 2013 B1
8449948 Medina et al. May 2013 B2
8451556 Wang et al. May 2013 B1
8451563 Zhang et al. May 2013 B1
8454846 Zhou et al. Jun 2013 B1
8455119 Jiang et al. Jun 2013 B1
8456961 Wang et al. Jun 2013 B1
8456963 Hu et al. Jun 2013 B1
8456964 Yuan et al. Jun 2013 B1
8456966 Shi et al. Jun 2013 B1
8456967 Mallary Jun 2013 B1
8458892 Si et al. Jun 2013 B2
8462592 Wolf et al. Jun 2013 B1
8468682 Zhang Jun 2013 B1
8472288 Wolf et al. Jun 2013 B1
8480911 Osugi et al. Jul 2013 B1
8486285 Zhou et al. Jul 2013 B2
8486286 Gao et al. Jul 2013 B1
8488272 Tran et al. Jul 2013 B1
8491801 Tanner et al. Jul 2013 B1
8491802 Gao et al. Jul 2013 B1
8493693 Zheng et al. Jul 2013 B1
8493695 Kaiser et al. Jul 2013 B1
8495813 Hu et al. Jul 2013 B1
8498084 Leng et al. Jul 2013 B1
8506828 Osugi et al. Aug 2013 B1
8514517 Batra et al. Aug 2013 B1
8518279 Wang et al. Aug 2013 B1
8518832 Yang et al. Aug 2013 B1
8520336 Liu et al. Aug 2013 B1
8520337 Liu et al. Aug 2013 B1
8524068 Medina et al. Sep 2013 B2
8526275 Yuan et al. Sep 2013 B1
8531801 Xiao et al. Sep 2013 B1
8532450 Wang et al. Sep 2013 B1
8533937 Wang et al. Sep 2013 B1
8537494 Pan et al. Sep 2013 B1
8537495 Luo et al. Sep 2013 B1
8537502 Park et al. Sep 2013 B1
8545999 Leng et al. Oct 2013 B1
8547659 Bai et al. Oct 2013 B1
8547667 Roy et al. Oct 2013 B1
8547730 Shen et al. Oct 2013 B1
8555486 Medina et al. Oct 2013 B1
8559141 Pakala et al. Oct 2013 B1
8563146 Zhang et al. Oct 2013 B1
8565049 Tanner et al. Oct 2013 B1
8576517 Tran et al. Nov 2013 B1
8578594 Jiang et al. Nov 2013 B2
8582238 Liu et al. Nov 2013 B1
8582241 Yu et al. Nov 2013 B1
8582253 Zheng et al. Nov 2013 B1
8588039 Shi et al. Nov 2013 B1
8593914 Wang et al. Nov 2013 B2
8597528 Roy et al. Dec 2013 B1
8599520 Liu et al. Dec 2013 B1
8599657 Lee Dec 2013 B1
8603593 Roy et al. Dec 2013 B1
8607438 Gao et al. Dec 2013 B1
8607439 Wang et al. Dec 2013 B1
8611035 Bajikar et al. Dec 2013 B1
8611054 Shang et al. Dec 2013 B1
8611055 Pakala et al. Dec 2013 B1
8614864 Hong et al. Dec 2013 B1
8619512 Yuan et al. Dec 2013 B1
8625233 Ji et al. Jan 2014 B1
8625941 Shi et al. Jan 2014 B1
8628672 Si et al. Jan 2014 B1
8630068 Mauri et al. Jan 2014 B1
8634280 Wang et al. Jan 2014 B1
8638529 Leng et al. Jan 2014 B1
8643980 Fowler et al. Feb 2014 B1
8649123 Zhang et al. Feb 2014 B1
8665561 Knutson et al. Mar 2014 B1
8670211 Sun et al. Mar 2014 B1
8670213 Zeng et al. Mar 2014 B1
8670214 Knutson et al. Mar 2014 B1
8670294 Shi et al. Mar 2014 B1
8670295 Hu et al. Mar 2014 B1
8675318 Ho et al. Mar 2014 B1
8675455 Krichevsky et al. Mar 2014 B1
8681594 Shi et al. Mar 2014 B1
8689430 Chen et al. Apr 2014 B1
8693141 Elliott et al. Apr 2014 B1
8703397 Zeng et al. Apr 2014 B1
8705205 Li et al. Apr 2014 B1
8711518 Zeng et al. Apr 2014 B1
8711528 Xiao et al. Apr 2014 B1
8717709 Shi et al. May 2014 B1
8720044 Tran et al. May 2014 B1
8721902 Wang et al. May 2014 B1
8724259 Liu et al. May 2014 B1
8749790 Tanner et al. Jun 2014 B1
8749920 Knutson et al. Jun 2014 B1
8753903 Tanner et al. Jun 2014 B1
8760807 Zhang et al. Jun 2014 B1
8760818 Diao et al. Jun 2014 B1
8760819 Liu et al. Jun 2014 B1
8760822 Li et al. Jun 2014 B1
8760823 Chen et al. Jun 2014 B1
8763235 Wang et al. Jul 2014 B1
8780498 Jiang et al. Jul 2014 B1
8780505 Xiao Jul 2014 B1
8786983 Liu et al. Jul 2014 B1
8790524 Luo et al. Jul 2014 B1
8790527 Luo et al. Jul 2014 B1
8792208 Liu et al. Jul 2014 B1
8792312 Wang et al. Jul 2014 B1
8793866 Zhang et al. Aug 2014 B1
8797680 Luo et al. Aug 2014 B1
8797684 Tran et al. Aug 2014 B1
8797686 Bai et al. Aug 2014 B1
8797692 Guo et al. Aug 2014 B1
8813324 Emley et al. Aug 2014 B2
8855449 Roth Oct 2014 B1
9123374 Tohmon et al. Sep 2015 B1
20030002127 George Jan 2003 A1
20070165494 Cho Jul 2007 A1
20100290157 Zhang et al. Nov 2010 A1
20110086240 Xiang et al. Apr 2011 A1
20120093454 Filgas Apr 2012 A1
20120111826 Chen et al. May 2012 A1
20120216378 Emley et al. Aug 2012 A1
20120237878 Zeng et al. Sep 2012 A1
20120298621 Gao Nov 2012 A1
20130142474 Dallesasse et al. Jun 2013 A1
20130142475 Dallesasse et al. Jun 2013 A1
20130216702 Kaiser et al. Aug 2013 A1
20130216863 Li et al. Aug 2013 A1
20130235890 Creazzo et al. Sep 2013 A1
20130243362 Van Orden et al. Sep 2013 A1
20130257421 Shang et al. Oct 2013 A1
20140037286 Krasulick et al. Feb 2014 A1
20140112669 Mizrahi et al. Apr 2014 A1
20140154529 Yang et al. Jun 2014 A1
20140175050 Zhang et al. Jun 2014 A1
20140321797 Van der Tol Oct 2014 A1
20150279394 Peng Oct 2015 A1
Non-Patent Literature Citations (4)
Entry
J. Yamauchi, N. Shibuya, and H. Nakano. “Polarization Coupling Between Strongly Guiding Waveguides Stacked Laterally,” Journal of Lightwave Technology, vol. 27, No. 11, 2009.
M. Watts and H. Haus. “Integrated mode-evolution-based polarization rotators, Optics Letters,” vol. 30, No. 2, 2005.
D. Dai and J. Bowers. “Novel concept for ultracompact polarization splitter-rotator based on silicon nanowires,” Optics Express, vol. 19, No. 11, 2011.
Y. Ding, L. Liu, C. Peucheret, and H. Ou, “Fabrication tolerant polarization splitter and rotator based on a tapered directional coupler,” Optics Express, vol. 20, No. 18, 2012.
Related Publications (1)
Number Date Country
20160379677 A1 Dec 2016 US