Current modulation on laser diode for energy assisted magnetic recording transducer

Description

CROSS-REFERENCE TO RELATED APPLICATION

This application claims the benefit of U.S. Provisional Application Ser. No. 61/991,295 filed on May 9, 2014, which is expressly incorporated by reference herein in its entirety.

BACKGROUND

High density storage disks are configured with layers of materials that provide the required data stability for storage. The magnetic properties of the media require a softening when writing to the disk to change the bit state. Energy Assisted Magnetic Recording (EAMR) device or Heat Assisted Magnetic Recording (HAMR) technology provides heat that is focused on a nano-sized bit region when writing onto a magnetic storage disk, which achieves the magnetic softening. A light waveguide directs light from a laser diode to a near field transducer (NFT). The NFT focuses the optical energy to a small spot on the target recording area which heats the magnetic storage disk during a write operation.

EAMR/HAMR uses a controlled magnitude of laser diode power for the magnetic softening at the disk. During operation with temperature and current change, the laser diode gain spectrum shifts causing laser mode hops. Because different longitudinal modes have different spectral positions, the power magnitude changes, which creates recording noise. The delta between longitudinal modes is particularly significant in a case of optical feedback from optical elements located at a distance greater than 100 microns from the laser diode facet. For example, the laser diode may receive reflection from a near field transducer and the magnetic storage disk, which will have different phase shift for different modes, such that laser power will change with mode hopping.

BRIEF DESCRIPTION OF THE DRAWINGS

Various aspects of the present invention will now be presented in the detailed description by way of example, and not by way of limitation, with reference to the accompanying drawings, wherein:

FIG. 1 shows an exemplary implementation of a laser diode in an EAMR enhanced disk-based drive.

FIG. 2 shows an exemplary embodiment of a laser diode having two contact sections for supplying two separate current modulations.

FIG. 3 shows an example graphical illustration of the dual current modulation.

FIG. 4 shows an exemplary variation to the embodiment of a laser diode shown in FIG. 1, in which the two contact sections are asymmetrical.

FIG. 5 shows a block diagram of an exemplary implementation of a current modulated laser diode.

DETAILED DESCRIPTION

The detailed description set forth below in connection with the appended drawings is intended as a description of various exemplary embodiments and is not intended to represent the only embodiments that may be practiced. The detailed description includes specific details for the purpose of providing a thorough understanding of the embodiments. However, it will be apparent to those skilled in the art that the embodiments may be practiced without these specific details. In some instances, well-known structures and components are shown in block diagram form in order to avoid obscuring the concepts of the embodiments. Acronyms and other descriptive terminology may be used merely for convenience and clarity and are not intended to limit the scope of the embodiments.

The various exemplary embodiments illustrated in the drawings may not be drawn to scale. Rather, the dimensions of the various features may be expanded or reduced for clarity. In addition, some of the drawings may be simplified for clarity. Thus, the drawings may not depict all of the components of a given apparatus.

Various embodiments will be described herein with reference to drawings that are schematic illustrations of idealized configurations. As such, variations from the shapes of the illustrations as a result of manufacturing techniques and/or tolerances, for example, are to be expected. Thus, the various embodiments presented throughout this disclosure should not be construed as limited to the particular shapes of elements illustrated and described herein but are to include deviations in shapes that result, for example, from manufacturing. By way of example, an element illustrated or described as having rounded or curved features at its edges may instead have straight edges. Thus, the elements illustrated in the drawings are schematic in nature and their shapes are not intended to illustrate the precise shape of an element and are not intended to limit the scope of the described embodiments.

The word “exemplary” is used herein to mean serving as an example, instance, or illustration. Any embodiment described herein as “exemplary” is not necessarily to be construed as preferred or advantageous over other embodiments. Likewise, the term “embodiment” of an apparatus or method does not require that all embodiments include the described components, structure, features, functionality, processes, advantages, benefits, or modes of operation. As used herein, the term “about” followed by a numeric value means within engineering tolerance of the provided value.

An apparatus includes a laser diode, coupled to the near field transducer. The laser diode has a current modulation source for stabilizing laser power during mode shifts. The laser diode may further include a first contact and a second contact to receive a first current modulation current and a second current modulation current, respectively. The first modulation current may be substantially out of phase with the second modulation current.

In the following detailed description, various aspects of the present invention will be presented in the context of a laser diode control configuration that may be used with a near field transducer for energy assisted magnetic recording on a magnetic storage disk. Various embodiments are well suited to an apparatus and methods for controlling mode shifts of a laser diode. However, those skilled in the art will realize that these aspects may be extended to controlling a laser diode for other purposes and arrangements. For example, various embodiments may be used in the context of devices related to optical media and optical data transmissions. Accordingly, any reference to a specific laser diode apparatus or method is intended only to illustrate the various embodiments, with the understanding that such embodiments may have a wide range of applications.

In one aspect, an apparatus includes a laser diode, a near field transducer configured to direct light emitted from the laser diode to a magnetic storage disk, and a power source configured to provide modulated current to the laser diode.

FIG. 1 shows a diagram of an exemplary implementation of a laser diode in an EAMR enhanced disk-based drive 121, which includes a disk drive base 124, at least one storage disk 123 (such as a magnetic disk, magneto-optical disk, or optical disk), a spindle motor 126 attached to the base 124 for rotating the disk 123. The spindle motor 126 typically includes a rotating hub on which disks are mounted and clamped. Rotation of the spindle motor hub results in rotation of the mounted disks 123. At least one actuator arm 125 supports at least one head gimbal assembly (HGA) 122 that includes a magnetic head assembly with writing and reading heads on a slider. For the EAMR/HAMR enhanced disk-based drive, a near field transducer (NFT) is included on an air bearing surface of the slider as well. During a recording operation of the disk-based drive 121, the actuator arm 125 rotates at the pivot 127 to position the HGA 122 to a desired information track on the disk 123. As the writer head performs the magnetic recording at the desired information track, a laser diode coupled to the NFT supplies a laser for magnetic softening of a nano-sized bit space on the disk.

FIG. 2 shows a diagram of an exemplary embodiment of an apparatus 100 that includes a laser diode 120 having two separate contacts 101 and 102 connected to current modulation sources 111 and 112, respectively. The laser diode 120 is grounded by a ground contact 109. The laser diode 120 includes a p-type semiconductor 103 and an n-type semiconductor 104, with laser output 105 transmitted longitudinally from the p-n junction. Current modulation source 111 drives a current I₁ through contact 101, across p-n junction 110 and to ground contact 109. The size and position of contact 101 controls the length of p-n junction 110 energized by current I₁, which may be defined as a first section of the diode 100. Current modulation source 112 drives a current I₂ through contact 102, which acts on the p-n junction 110 of a second section of the diode 100. The second section of diode 100 may be defined by a length of p-n junction 110 effected by current I₂, which depends on the size and position of contact 102. While shown as two separate current sources 111 and 112, the power source to contacts 101 and 102 may be a single power supply with filters that separately control the phase difference of current at contacts 101 and 102.

FIG. 3 shows a graphical illustration of the currents I₁ and I₂ that are generated by current sources 111 and 112. As shown, currents I₁ and I₂ are triangular waves in antiphase (i.e., having a phase difference=π). Alternatively, the phase difference between current I₁ and current I₂ may be about π. By providing current I₁ and I₂ modulated with such a phase offset, the total laser current I_TOTAL may be maintained at constant level as shown in FIG. 3.

The localized change of current density (i.e., the two current waves for I₁ and I₂ shown in FIG. 3) may lead to a corresponding local p-n junction temperature changes T₁ and T₂ in diode 100 in the first and second sections of diode 120, as shown in FIG. 3. In response to the localized temperature changes, a corresponding shifting in wavelength of peak gain G₁ and G₂ for the first and second sections of the laser diode 120 may result. The shifting positions of G₁ and G₂ provide additional opportunities for the laser mode to shift. If modulation frequency for currents I₁ and I₂ is high enough, the laser diode 100 may experience multiple mode-hops during a single recording pulse, and effects of separate hops can be averaged over time, which results in reduced laser noise. Hence, as a result of the modulated currents I₁ and I₂, the average laser output power P_ave is substantially constant over a duration of multiple laser mode hops as shown in FIG. 3. While triangular current modulation I₁ and I₂ is depicted in FIG. 3, it should be noted that other current modulation wave shapes may be generated within the scope of the described embodiments.

Because total power may be maintained at a constant level, the modulation rate of currents I₁ and I₂ may be approximately equal to the recording rate of the write head on the EAMR device. However, it is not necessary for the current modulation currents I₁ and I₂ to be synchronized with the write (i.e., recording) pulses. Alternatively, the modulation rate for currents I₁ and I₂ may be lower than the rate of the recording pulses.

FIG. 4 shows a diagram of an exemplary laser diode apparatus 200, which is a variation of the laser diode apparatus 100 shown in FIG. 2. In FIG. 4, contact 201 is smaller than contact 202, which alters the p-n junction temperature effect across diode 220. Contact 201 is disposed along a surface of a first section of diode 220 having less surface area than a second section of diode 220, on which contact 202 is disposed. Current modulation source 111 drives a current I₁ through contact 201, which acts on the p-n junction of the first section of the diode 220. Current modulation source 112 drives a current I₂ through contact 202, which acts on the p-n junction of the second section of the diode 220. The laser diode 220 includes a p-type semiconductor 103 and an n-type semiconductor 104, with laser output 105 transmitted longitudinally from the p-n junction. For the embodiment shown in FIG. 4, with diode 220 having contact sections 201 and 202 with different sizes, the lasing mode position may be defined by the local temperature as controlled by the larger contact 202 on the longer second section of diode 220.

FIG. 5 shows a diagram of an exemplary embodiment for a laser diode apparatus 300 which may implement the current modulated laser diode apparatus 100, 200. As shown, the laser diode apparatus 100, 200 may be coupled to a waveguide 302 for directing the laser 305 to a near field transducer (NFT) 304 mounted at an air bearing surface 306 of a magnetic recording device, e.g., an EAMR device. As the writer head of the EAMR device performs the magnetic recording at the desired information track of the storage disk 310, the laser diode apparatus coupled to the NFT 304 supplies the laser 305 for magnetic softening of a nano-sized bit space on the storage disk 310. The various aspects of this disclosure are provided to enable one of ordinary skill in the art to practice the present invention.

Various modifications to exemplary embodiments presented throughout this disclosure will be readily apparent to those skilled in the art, and the concepts disclosed herein may be extended to other devices. Thus, the claims are not intended to be limited to the various aspects of this disclosure, but are to be accorded the full scope consistent with the language of the claims. All structural and functional equivalents to the various components of the exemplary embodiments described throughout this disclosure that are known or later come to be known to those of ordinary skill in the art are expressly incorporated herein by reference and are intended to be encompassed by the claims. Moreover, nothing disclosed herein is intended to be dedicated to the public regardless of whether such disclosure is explicitly recited in the claims. No claim element is to be construed under the provisions of 35 U.S.C. §112(f) unless the element is expressly recited using the phrase “means for” or, in the case of a method claim, the element is recited using the phrase “step for.”