Heat-assisted rotating disk magnetometer for ultra-high anisotropy magnetic measurements
US-9589588-B2 · Mar 7, 2017 · US
US9916868B1 · US · B1
| Field | Value |
|---|---|
| Publication number | US-9916868-B1 |
| Application number | US-201615229967-A |
| Country | US |
| Kind code | B1 |
| Filing date | Aug 5, 2016 |
| Priority date | May 22, 2015 |
| Publication date | Mar 13, 2018 |
| Grant date | Mar 13, 2018 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
An apparatus comprises a spindle to rotate a magnetic recording medium and a magnetic field generator to expose a track of the medium to a DC magnetic field. The magnetic field generator is configured to saturate the track during an erase mode and reverse the DC magnetic field impinging the track during a writing mode. A laser arrangement heats the track during the erase mode and, during the writing mode, heats the track while the track is exposed to the reversed DC magnetic field so as to write a magnetic pattern thereon. A reader reads the magnetic pattern and generates a read signal. A processor is coupled to the reader and configured to determine an anisotropy parameter using the read signal. The apparatus can further comprise a Kerr sensor that generates a Kerr signal using the magnetic pattern.
Opening claim text (preview).
What is claimed is: 1. An apparatus, comprising: a spindle configured to rotate a magnetic recording medium; a magnetic field generator configured to expose a track of the medium to a DC magnetic field, the generator configured to saturate the track during an erase mode and reverse the DC magnetic field impinging the track during a writing mode; a laser arrangement configured to heat the track during the erase mode and, during the writing mode, heat the track while the track is exposed to the reversed DC magnetic field so as to write a magnetic pattern thereon; a reader configured to read the magnetic pattern and generate a read signal; and a processor coupled to the reader and configured to determine an anisotropy parameter using the read signal. 2. The apparatus of claim 1 , wherein the anisotropy parameter comprises anisotropy field temperature slope data. 3. The apparatus of claim 1 , wherein the processor is configured to determine the anisotropy parameter based on acquired reversal probability versus laser power data. 4. The apparatus of claim 1 , wherein the processor is configured to: compute at least one curve of reversal probability as a function of applied laser arrangement power; derive fitting parameters for the curve; and determine the anisotropy parameter using the fitting parameters. 5. The apparatus of claim 1 , wherein the medium has a coercivity of between about 5 kOe and 100 kOe. 6. A method comprising: rotating a magnetic recording medium proximate a magnetic field generator, a laser arrangement, and an inductive reader; DC erasing a track of the medium by concurrently exposing the track to a first DC magnetic field and heating the track with the laser arrangement; writing a magnetic pattern on the track by concurrently heating the track using the laser arrangement and exposing the track to a second DC magnetic field opposite the first DC magnetic field; reading the magnetic pattern and generating a read signal using the magnetic pattern; measuring reversal probability as a function of power applied to the laser arrangement using the read signal; and determining an anisotropy parameter from the reversal probability. 7. The method of claim 6 , wherein the anisotropy parameter comprises anisotropy field temperature slope data. 8. The method of claim 6 , wherein measuring a reversal probability as a function of power applied to the laser arrangement comprises obtaining a plurality of reversal probability curves where each curve is obtained under a different external field value. 9. The method of claim 6 , further comprising: computing a curve of reversal probability as a function of applied laser arrangement power; deriving fitting parameters for the curve; and determining the anisotropy parameter from the fitting parameters. 10. The method of claim 6 , further comprising: computing a curve of reversal probability as a function of applied laser arrangement power; deriving fitting parameters for the curve; and determining a switching temperature parameter from the fitting parameters. 11. The method of claim 6 , wherein writing the magnetic pattern comprises writing the magnetic pattern to a track. 12. The method of claim 6 , further comprising: rotating the magnetic recording medium proximate a reader; generating a read signal using the magnetic pattern; and measuring the reversal probability as a function of power applied to the laser arrangement using the read signal. 13. The method of claim 6 , wherein writing the magnetic pattern comprises writing the magnetic pattern to a portion of a track, the portion size being determined by a readout laser. 14. The apparatus of claim 1 , wherein the reader comprises an inductive reader. 15. The apparatus of claim 1 , wherein the medium has a coercivity of between about 15 kOe and 50 kOe. 16. The method of claim 8 , wherein the different external field values comprise about 6 to 12 kOe.
using the Kerr effect · CPC title
Erasing · CPC title
Digital recording · CPC title
Power calibration · CPC title
Power control during transducing, e.g. by monitoring · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.