One embodiment described herein is directed to a planar collimator has first and second sections each intersecting at a junction between a first axis and a second axis normal to the first axis. Each of the first and second sections have geometries configured to receive light from a source point located on the first axis and collimate the light at respective positive and negative tilting angles relative to the second axis to respective first and second sides of a focusing mirror and away from a gap between the first and second sides of the focusing mirror.
In another embodiment, a method involves orienting a collimator to receive light from a source point located on a first axis and collimate the light at respective positive and negative tilting angles relative to a second axis normal to the first axis. A focusing mirror is oriented along the second axis to receive the collimated light at first and second sides of the focusing mirror. The focusing mirror has a gap between the first and second sides, and the collimated light is not received in the gap. The method further involves launching the light from the source point to the collimator to collimate and reflect the light to the focusing mirror. The focusing mirror directs the collimated light to a near field transducer at a focal region of the focusing mirror.
In another embodiment, an apparatus includes a diagonal mirror configured to receive light from a source point located on a first axis. The diagonal mirror includes non-parallel, first and second mirror portions joined by a split region that is parallel with the first axis. The split region introduces a phase shift between first and second portions of light reflected by the first and second portions. The apparatus includes a parabolic mirror having first and second sections configured to receive the respective first and second portions of light and direct the light to a focal region. The first and second portions are non-symmetrically disposed relative to the focal region to adjust the phase shift introduced by split region of the diagonal mirror.
These and other features and aspects of various embodiments may be understood in view of the following detailed discussion and accompanying drawings.
The discussion below makes reference to the following figures, wherein the same reference number may be used to identify the similar/same component in multiple figures.
In heat-assisted magnetic recording (HAMR), also sometimes referred to as thermal-assisted magnetic recording (TAMR), information bits are recorded in a storage layer at elevated temperatures and the heating area in the storage layer determines the data bit dimension. A HAMR device utilizes a magnetic recording media (e.g., hard drive disk) that is able to overcome superparamagnetic effects that limit the areal data density of typical magnetic media. In order to record on this media, a HAMR device may use integrated optics as described above to heat a magnetic recording media (e.g., hard disk) in order to overcome superparamagnetic effects that limit the areal data density of typical magnetic media. In order to record on this media, a small portion of the media (e.g., a hotspot) is locally heated above the Curie temperature while being written to by a magnetic write head.
In order to achieve desired data density, the HAMR media hotspot may need to be smaller than a half-wavelength of light. However, due to what is known as the diffraction limit, optical components cannot focus the light at this scale. One way to achieve tiny confined hot spots is to use an optical near-field transducer, such as a plasmonic optical antenna or an aperture-integrated in an optical waveguide of high contrast in the index of refractive index between the waveguide core and its claddings. Light propagating in the waveguide is focused by an optical focusing element, such as a planar solid immersion mirror into an optical near-field transducer. This causes surface plasmon excitation at the NFT. Due to the shape of the NFT, this excitation can be used for direct a narrow beam of energy to the media surface.
In such an approach, one of challenges encountered is to launch light into the waveguide in a slider with low cost, insensitivity to variations in wavelength, good alignment tolerance, and good light delivery efficiency. In one arrangement, light can be launched into a slider from free space by a grating coupler fabricated in a slider, called free space light delivery. Another way to launch light into a slider is to place a laser light source, such as a laser diode, into or onto a slider. This may be referred to as laser-in-slider light delivery (or laser-on-slider light delivery). Instead of using a grating, an output facet of the laser may be butted up against an input facet of a waveguide that delivers light to the media surface.
In reference now to
The laser diode 102 provides electromagnetic energy to heat the media surface at a point near to the read/write head 106. Optical coupling components, such as a waveguide 110, are formed integrally within the slider device 100 to deliver light from the laser 102 to the media. For example, a waveguide and near-field transducer (NFT) 112 may be located proximate the read/write head 106 to provide local heating of the media during write operations. While the laser diode 102 in this example is an integral, edge firing device, it will be appreciated that the waveguide/NFT 112 may be applicable to any light source and light delivery mechanisms. For example, surface emitting lasers (SEL) may be used instead of edge firing lasers, and the slider may use any combination of integrated and external lasers. For example, it may be possible to form some or all parts of a laser integrally (e.g., in the layer deposition processes) within the slider 102.
In reference now to
The waveguide input coupler 204 delivers the light to a first mirror 206 which is configured as a planar parabolic collimator. In this context, the term “planar” refers to the collimator 206 being configured to reflect light within a planar layer of the slider 100. Collimated light from the first mirror 206 is reflected to a second mirror 208. The second mirror 208 is configured as a planar elliptical relay mirror, which directs light to a third mirror 210, which is configured as a second parabolic collimator. The collimated light of the third mirror 210 is directed to a solid immersion focusing mirror 212, which focuses the light on NFT 112.
In
In referenced now to
Light reflected from the collimating mirror 210 into the gap region 302 may be lost, resulting in a reduction in the overall system efficiency. One way of avoiding reflecting light from the mirror 210 into the gap 302 is to form the mirror 210 as first and second parabolic portions 310, 312 coupled via a split 308. The split 308 is oriented in a direction parallel to the x-axis, which in this diagram is the direction along which light is delivered to the mirror 210 from a source location 313 (e.g., elliptical mirror 208 in
The dimension of the split 308 along the x-direction (Δx) is approximately equal to the x-dimension (Wb) of the solid immersion mirror gap 302, and may be selected based on Equation 1 below. In Equation 1, λ0 denotes the light wavelength in free space, neff is the effective waveguide mode index, m is an integer, and Δm0<1 is chosen to accommodate certain requirement for setting the phase shift in the wavefront. For example, it may be desired to shift the phase of the light directed to first side 304 of focusing mirror 212 relative to the second side 306.
In Equation 1, any variation in the light wavelength will be magnified by m times in the phase. For instance, if λ0=830 nm, Wb=6000 nm, neff=1.78, Δx=500 nm for a π phase shift wavefront, this results in m=12. In this case, the performance of the mirror 210 is highly dependent on the wavelength λ0 of the light. While the system is designed to operate at a nominal wavelength, e.g., 830 nm, temperature change can cause the wavelength to shift by some value Δλ. If, for example, Δλ=20 nm then the wavelength of light will be 850 nm and mΔλ=240 nm. This yields an extra phase shift of 0.58 π. This amount of extra phase is not desirable for some NFT designs. In one example, 0.11 π of phase shift is the upper limit for desired NFT performance.
Accordingly, it may be possible to minimize the amount of split, Δx, by setting m=0. If Δx=0, the values of m and Δm0 in Equation 1 are zero such that light delivery via mirror 210 is substantially achromatic. However, in order to achieve desired NFT performance, some phase shifting will be needed between the two mirror sections, such that m=0 and Δm0≠0, However, setting m=0 will result in light being directed into the gap 302, which reduces efficiency. As will be shown below, one way to avoid light being directed into the gap is to cant/tilt parts of the collimator 210 and shape the two sides 310 and 312 such that light will not be directed into the gap 302.
An example configuration of collimating mirror 210A according to an example embodiment is shown in
In the diagram of
Each of the first and second sections 320, 322 have geometries configured to receive light from the source point 313 and collimate the generally in the negative y and y′ directions to respective first and second sides of the solid immersion focusing mirror and away from the gap (e.g., sides 304, 306 and gap 302 of mirror 212 shown in
Referring back to
A ray at angle θ from the x-axis will intersect the collimating mirror 210A at (x, y), which are calculated as shown in Equations 5 and 6 below. Note that for Equations 5 and 6, θ>0 for the upper section 320, and θ<0 for the lower section 322.
Because the sections 320, 322 are sections of parabolas with tilted axes of symmetry, the focusing mirror 212 that receives light from the collimating mirror 210A may also need to have tilted sections relative to their axes of symmetry (y-axis) in order to compensate. For example, focusing mirror 212A of
The diagram in
To better illustrate the relative curvature of the collimating mirror sections 320, 322,
It will be appreciated many variations of collimating and focusing mirrors may be possible in view of the above teachings. For example, the two sections of the collimating mirror (and corresponding sidewalls of the focusing mirror) may be rotated by different angles, e.g., θ21 and −θ22 where θ21≠θ22. This may also involve an asymmetric rotation of the sidewalls of the focusing mirrors by similar angles. Also as noted above, the dimension (Δx) of the split region along the x-axis may be zero, or may be non-zero but less than a wavelength of the light divided by an effective waveguide mode index (λ0/neff).
Another variation of collimating and focusing mirrors is shown in the diagram of
In reference now to
A focusing mirror is oriented 704 along the second axis to receive the collimated light at first and second sides of the focusing mirror. The focusing mirror has a gap between the first and second sides, and the collimated light is not received in the gap (in the sense of geometrical optics). The light is launched 706 from the source point to the collimating mirror to collimate the light, such that the focusing mirror directs the collimated light to a near field transducer at a focal region of the focusing mirror.
In reference now to
The first and second portions 802a, 802b of mirror 802 are canted relative to one another by an angle β. Section 802a is canted +β relative to the 45-degree nominal angle 803, and section 802b is canted −β from the nominal angle 803. It will be understood that β may be zero, and the sections 802a, 802b may be canted by different angles, e.g., β1 and β2. The canting angles cause respective portions of light 810a, 810b to be directed to respective sections 812a, 812b of a parabolic mirror 812 without causing light to directly enter a focal region 814 between the sections 812a, 812b.
The first and second sections 812a, 812b are configured to receive the respective first and second portions of light 810a, 810b and direct the light to a focal region 814. The first and second sections 812a, 812b may be tilted by canting angle β in negative and positive directions to compensate for tilting of the diagonal mirror 802. An NFT 818 is disposed at the focal region 814 and reaches surface plasmon resonance in response to incident light reflected by first and second sections 812a, 812b.
The split region 802c causes a beam shadow along the along centerline 822 of the focal region 814 which improves the coherent beam power delivered to the NFT transducer 818. The attenuation of the beam along the centerline 822 (which is not reflected) also reduces the amount of beam interference effects at the NFT 818, thereby reducing beam variation. The net field at the focal region 814 is generally a cross-track-direction field at the focal point, which energizes an NFT plasmonic device. The initial phase shift at the split diagonal mirror 802 gives a zero net field along the centerline 822 which intersects the NFT 818. This may reduce or eliminate interference fields which may cause unpredictable shifts in focus peak field amplitude, position, and profile (FWHM), etc.
The first and second sections 812a, 812b are asymmetrically disposed relative to the focal region 814 so that the phase shift introduced by split region 802c of the diagonal mirror 802 is adjusted. This is indicated by dashed line 820, which indicates a symmetrical projection of first section 812a about the focal region centerline 822. The distance between the dashed line 820 and location of second section 812b is an example of asymmetry about the focal region 814, which is shifted along the x-direction. Other asymmetries may be introduced between sections 812a, 812b, such as a shift along the y-direction or a rotational asymmetry. It should be noted that the asymmetry, as well as other geometric features such as canting angle β, may be significantly exaggerated in
The first and second sections 812a, 812b may be asymmetrically disposed relative to the focal region 814 so that there is no phase shift between the first and second portions of light 810a, 810b at the focal region 818. There may be a desire to have a selectable amount of phase shift, e.g., some NFT designs may perform better with incident light being phase-shifted between the left and right side of the NFT. For example, the illustrated NFT 818 is a disc/peg design, and this may benefit from having a π-angle phase shift on either side. Other NFT designs, such as pins or gap-waveguide NFT may perform best with zero or close to zero phase shift on either side.
The diagonal mirror 802 and the parabolic mirror 812 may both be configured as planar mirrors. At least one of the diagonal mirror 802 and the parabolic mirror 812 may be configured as a solid immersion mirror. The mirror arrangement may introduce phase shifts at both the diagonal mirror 802 and the parabolic reflector 812. This phase shifts may be of same or different amounts.
The foregoing description of the example embodiments has been presented for the purposes of illustration and description. It is not intended to be exhaustive or to limit the embodiments to the precise form disclosed. Many modifications and variations are possible in light of the above teaching. Any or all features of the disclosed embodiments can be applied individually or in any combination are not meant to be limiting, but purely illustrative. It is intended that the scope of the invention be limited not with this detailed description, but rather determined by the claims appended hereto.
This application claims the benefit of Provisional Patent Application Ser. No. 61/637,633 filed on Apr. 24, 2012 and Provisional Patent Application Ser. No. 61/638,472 filed on Apr. 25, 2012, to which priority is claimed pursuant to 35 U.S.C. §119(e) and which are hereby incorporated herein by reference in their entireties.
Number | Date | Country | |
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61637633 | Apr 2012 | US | |
61638472 | Apr 2012 | US |