Apparatus for slider curvature modification by substrate melting produced with a pulsed laser beam
A method and apparatus for producing very high crown and camber curvature in slider materials using a laser processing system which produces fluence which is variable in a controllable manner, by applying a laser beam to the flex side of the slider material and varying the fluence of the laser beam to optimize the curvature in the slider material. The fluence is variable by finely controlling the power output of the laser or by changing the spot size of the laser beam. The beam spot size can be changed by using a focusing lens to establish a focal plane and then varying the relative positions of the slider relative and the focal plane. An apparatus for producing high crown and camber is also disclosed, as well as a slider produced by the process of applying a laser beam to the flex side of the slider material and varying the fluence of the laser beam to optimize the curvature in the slider material.
Reference is made to U.S. patent application Ser. No. 09/444,793, filed Nov. 22, 1999, entitled PROCESSING OF MULTI-PHASE CERAMIC SLIDER MATERIALS USING HARMONICALLY GENERATED ULTRAVIOLET LASER RADIATION in the names of Paul M. Lundquist, et. al.
BACKGROUND OF THE INVENTION1. Field of the Invention
The present invention relates to an improved method for the manufacture of sliders for disk drives. More particularly, the invention relates to a method for controllably producing very high crown and camber in the air bearing surface of a slider by applying pulsed laser energy in accordance with the method of the present invention to the back side of the slider in order to induce stress, and thus curvature in the slider material.
2. Description of the Background Art
Magnetic storage disk drives typically include a magnetic sensor called a “head” suspended in close proximity to the magnetic disk, which serves as the recording medium. In Winchester-type disk drives, a magnetic thin film head is embedded in a ceramic block, called a slider, which is then attached to a flexible suspension. During operation, the rotation of the magnetic disk relative to the slider provides an air-flow along the surface of the slider, which causes it to lift, so that the slider is supported on a cushion of air. This surface of the slider is referred to as the Air Bearing Surface (ABS) and its separation from the disk the Fly Height (FH). The shape of the slider and of the ABS in particular is crucial to the performance of the head. Contours in the ABS establish the desired pressure gradients for positioning the slider above the disk surface. It is therefore typically necessary to form complex contours in the shape of the slider by micro-machining, etching, or other processes to obtain the desired performance.
As more is learned about the dynamics of flying heads, more subtle changes are being required in the shape of the ABS. To implement these refinements, it is becoming more and more desirable to create contours which are complex in three dimensions. Two parameters pertaining to the curvature or flatness of the ABS that are considered important are “crown” and “camber”. Crown is the maximum separation of the cylindrical contour along the flying direction from an imaginary plane drawn between the two end edges, i.e., the leading and trailing edges, of the ABS. Camber has a similar definition and is the separation from an imaginary plane drawn between the two side edges of the slider. For the modern “pico” sliders, these curvature parameters are typically on the order of several nanometers (nm), while the slider width and length are about 1 mm. The curvatures of the ABS are therefore truly minute, however, the variance of the crown and camber of modern sliders remains to be a key factor for the slider performance. Hence, there is an obvious need to develop and implement a method to finely adjust crown and camber.
A variety of techniques are currently being practiced for controlling the slider curvature beyond the capability of conventional lapping. All these techniques rely on inducing a surface stress change (ΔS) on at least one slider surface. This change of surface stress can be (1) positive (i.e., increase of compressive stress) or (2) negative (i.e., decrease of compressive stress). The change in surface stress produces a curvature change in the slider, as shown in
C=[3(1−ν)/4E](L/a)2(ΔS×b)
where L is the length of the slider, a is its thickness, b is the depth of the surface stress layer, ν is Poisson's ratio, and E is Young's modulus. The camber change is also given by a similar equation for the “bulging” of the slider as viewed from the x-direction.
Several techniques for producing positive or negative stress changes on a slider surface are known. Techniques to induce negative stress changes (i.e., reducing the existing compressive stress, or inducing tensile stress on the surface) are usually practiced on the flex side of the slider, in order to produce an increase in the crown or camber at the ABS side. Stress-reducing techniques that can be used at the flex side include “kiss-lapping” or plasma etching, which can remove part or all of the stressed layer on the surface. However, such processes have characteristics which detract from their use in a commercial environment.
A more recent approach to slider shaping is the use of laser scribing. Using a laser for creating curvature in sliders is found in U.S. Pat. No. 5,982,583 to Strom. It states in claim 1 the use of a laser to melt and then cool the back surface (here referred to as the flex side) of a slider to add tensile stress which causes tensile stress relief cracks in the back surface, and which causes the air bearing surface to curve thus modifying crown or camber. Strom's tensile stress relief cracks are oriented predominately parallel to the crown curvature axis. The present inventors regard cracks as undesirable, and should be reduced or minimized in number and size so as not to worsen the surface integrity. The presence of such tensile stress cracks as required by the prior art is an indication that excessive laser power is used to melt excessive amounts of material, and such excessive laser power may damage the sensor which is embedded in the ceramic slider material.
Although some presence of micro-cracks are inevitable when the surface is made “tensile”, preferably any cracks made by laser processing should be only very microscopic micro-cracks, visible with a Scanning Electron Microscope. Such micro-cracks tend to orient randomly. An improved approach therefore is to minimize any tensile stress cracks.
Consequently, there is a need for an improved method of laser processing of sliders which does not require the introduction of tensile stress relief cracks in slider material.
It is, therefore, an object of the present invention to provide an improved method for creating controllable crown and camber in sliders by using pulsed laser energy in accordance with the present invention to produce specific, controllable minute curvatures, without the required introduction of tensile stress relief cracks. Other objects and advantages will become apparent from the following disclosure.
SUMMARY OF THE INVENTIONThe present invention relates to a method and apparatus for producing very high crown and camber curvature in slider materials using a laser processing system which produces fluence, which is variable in a controllable manner, by applying a laser beam to the flex side of the slider material and varying the fluence of the laser beam to form the curvature in the slider material.
A more thorough disclosure of the present invention is presented in the detailed description which follows and the accompanying figures.
BRIEF DESCRIPTION OF THE DRAWINGSThe objects and, advantages and features of the present invention will be more clearly understood by reference to the following detailed disclosure and the accompanying drawings in which:
The present invention relates to a method and apparatus for creating very high crown and camber in sliders by creating controlled tensile stress in the flex side of the sliders using variable pulsed laser fluence to melt the slider material without over-heating the sensor in it and without tensile stress relief cracks of controlled or preferred orientation.
The present inventors have found that the production of very precisely controllable crown in slider material is possible by treatment of the flex side of the slider, when a pulsed laser beam is used in accordance with the present invention. The present invention discloses a method of producing very precise and large crown and camber.
It is first preferred for processing of alumina ceramics, that a pulsed laser having a pulse width between 10 nanoseconds (10×10−9 secs.) and 1 microsecond (1×10−6 secs.) and a repetition rate of 200-300 kHz is used. This is preferred because this range of pulse-widths and repetition rates allows very quick and localized heating of the material at the point of application, limiting the spreading of heat to the surrounding material, which can cause thermal damage to the slider sensors. It also allows melting of material without loss of material through ablation. Continuous wave lasers having application times on the order of milliseconds to seconds are more likely to have damaging effects on the sensitive sensor components, and considered unsuitable for this type of operation. It is of course possible that for other substrate materials, other pulse durations and repetition rates may be preferred, and the method disclosed herein contemplates changes in other parameters to accommodate differences in materials and in batches of materials.
A second parameter of the present invention is the laser fluence. The term “fluence” refers to the surface laser energy density produced by a laser, preferably a pulsed laser, onto a surface area. In the present invention, it is measured in units of energy (or energy/pulse) divided by area. The beam spot size is generally so small, that the fluence will generally lie in the region of Joules/cm2.
Fluence can be adjusted for maximal performance and control in two primary ways. First, the spot size can remain constant while the energy per pulse is varied, or second, the energy can remain constant while the spot size is varied.
The energy per pulse of a laser can be varied by several different methods. The current to the excitation mechanism can be adjusted, which has an effect on the power output of the laser. However, it is usually necessary to monitor changes in power output during such changes, since it cannot be relied upon that a 10% change in current input will directly produce a corresponding 10% change in the laser output. The process is complicated by the fact that changes in current input can also produce changes in pulse-width, which can have other effects on the process.
The energy of the laser can also be varied by attenuating the beam by using filters, or using devices such as a Liquid Crystal Variable Retarder (LCVR), which changes polarization in an active manner. When used with a polarizer, the LCVR can be used to reduce the power output in a somewhat controllable manner, although very fine control in the range of a few percent is still difficult to achieve.
Alternatively, a preferred manner of controlling the fluence of the laser is by controlling the spot size, an operation which can be easily and inexpensively controlled by use of a lens which can be adjusted to move the focal plane relative to the slider material, or by moving the slider piece relative to the focal plane. This method of increasing the spot size is preferred because of its simplicity over the traditional method of using an adjustable beam collimating device to decrease the diameter of the laser beam before the focusing lens, which has the effect of increasing the spot size.
The slider 28 will be assumed to be placed at the focal plane 34 in
In general terms, the lens 20 and lens stage 22, as well as the movable slider stage 30, can be thought of as fluence varying devices, since the spot size, and thus the fluence can be varied through their adjustment. Another way of varying the fluence is by adjusting the power output of the laser, which is typically done by reducing the current to the excitation mechanism (not shown) of the laser. Examples would include decreasing the current to diodes or flashlamps in diode-pumped or flashlamp-pumped lasers, or controlling the voltage to an excimer laser's excitation mechanism.
The typical appearance of the melt after laser irradiation of the slider material is shown in
As defined above, crown is the maximum separation of the cylindrical contour along the flying direction from an imaginary plane drawn between the two end edges, i.e., the leading and trailing edges, of the ABS. Camber is the separation from an imaginary plane drawn between the two side edges of the slider. As shown in
In a similar way,
In addition to the use of a fundamental laser wavelength from a Nd-doped solid-state laser, it is possible that the laser beam is produced through a process of harmonic generation to yield a wavelength which is absorbed well by the substrate material, as disclosed in pending U.S. patent application Ser. No. 09/444,793, filed Nov. 22, 1999, entitled PROCESSING OF MULTI-PHASE CERAMIC SLIDER MATERIALS USING HARMONICALLY GENERATED ULTRAVIOLET LASER RADIATION.
Although this invention has been described with respect to specific embodiments, the details thereof are not to be construed as limitations, for it will be apparent that various embodiments, changes and modifications may be resorted to without departing from the spirit and scope thereof; and it is understood that such equivalent embodiments are intended to be included within the scope of this invention.
While various embodiments have been described above, it should be understood that they have been presented by way of example only, and not limitation. Thus, the breadth and scope of a preferred embodiment should not be limited by any of the above described exemplary embodiments, but should be defined only in accordance with the following claims and their equivalents.
Claims
1. A method for producing very high crown and camber curvature in slider materials having a flex side and an air-bearing side using a laser processing system which produces a pulsed laser beam, comprising the steps of:
- (A) establishing a focal plane for the laser beam, the laser beam having a pulse width in the range of 1×10−9 seconds to 1×10−3 seconds, with an energy per pulse in the range of 1 to 1,000,000 microjoules, and a repetition rate between 1 Hz and 400 kHz;
- (B) applying the pulsed laser beam to the flex side of the slider material; and
- (C) varying the relative positions of the slider material and the focal plane of the laser beam to optimize the curvature.
2. The method of claim 1, wherein the laser processing system further comprises a focusing device, whereby the focal plane of the laser beam is established.
3. The method of claim 2, wherein said focusing device is at least one lens mounted on a moveable stage, whereby the position of the focal plane relative to the slider material can be varied.
4. The method of claim 1, wherein the laser processing system further comprises a movable stage to which the slider material is attached, the position of the slider material relative to the focal plane can be varied.
5. The method of claim 1, wherein the laser is Q-switched.
6. The method of claim 1, wherein the laser beam is conditioned with a beam expander with adjustable beam expansion.
7. The method of claim 1, wherein the laser beam is produced through harmonic generation.
8. The method of claim 1, wherein the laser beam is moved by at least one directing optic.
9. The method of claim 8, wherein at least one directing optic includes at least one reflecting mirror.
10. The method of claim 1, wherein the slider material is one or more rows of sliders.
11. A method for producing very high crown and camber curvature in slider materials having a flex side, using a laser processing system which produces a laser beam which produces fluence which is variable in a controllable manner, comprising the steps of:
- (A) applying the laser beam to the flex side of the slider material, the laser beam having a pulse width in the range of 1×10−9 seconds to 1×10−3 seconds, with an energy per pulse in the range of 1 to 1,000,000 microjoules, and a repetition rate between 1 Hz and 400 kHz; and
- (B) varying the fluence of the laser to optimize the curvature in the slider material.
12. The method of claim 11, wherein fluence is controllably varied by changing the power output of the laser.
13. The method of claim 11, wherein fluence is controllably varied by changing the spot size of the laser beam.
14. The method of claim 13, wherein the spot size of the laser beam is varied by changing the relative positions of the slider material and the focal plane of the laser beam.
15. The method of claim 14, wherein the spot size is controllably varied by moving the focal plane of the laser beam relative to the slider material.
16. The method of claim 15, wherein the focal plane of the laser is moved relative to the slider material by using at least one focusing lens which is attached to a movable mount.
17. The method of claim 14, wherein the slider material is moved relative to the focal plane of the laser by using a movable mount to which the slider material is attached.
18. The method of claim 11, wherein fluence is controllably varied by adjusting the beam expansion of the laser beam.
19. The method of claim 11, wherein the slider material is one or more rows of sliders.
20. An apparatus for creating high crown and camber curvature in slider materials having an air bearing surface and a flex side, comprising:
- a laser which produces a pulsed laser beam for machining the slider material, the laser beam having a pulse width in the range of 1×10−9 seconds to 1×10−3 seconds, with an energy per pulse in the range of 1 to 1,000,000 microjoules, and a repetition rate between 1 Hz and 400 kHz;
- at least one beam directing device, which directs the laser beam onto the flex side of the slider material; and
- a fluence varying device so that optimal fluence is achieved to produce optimal curvature.
21. The apparatus of claim 20, wherein:
- the fluence varying device is at least one focusing lens which directs the laser beam to focus within a focal plane and a movable fixture which varies the position of the slider material with respect to the focal plane.
22. The apparatus of claim 21, wherein:
- the movable fixture is a movable stage upon which the slider material is attached, and by which the slider material is moved relative to the focal plane.
23. The apparatus of claim 21, wherein:
- the movable fixture is a movable stage upon which the lens is attached, and by which the focal plane is moved relative to the slider material.
24. The apparatus of claim 20, wherein the laser is Q-switched.
25. The apparatus of claim 20, wherein the laser beam is produced through harmonic generation.
26. The apparatus of claim 20, wherein the laser beam is moved by at least one directing device.
27. The apparatus of claim 26, wherein at least one directing optic includes at least one reflecting mirror.
28. The apparatus of claim 20, wherein the laser beam is conditioned with a beam expander that has adjustable beam expansion.
29. The apparatus of claim 20, wherein the slider material is one or more rows of sliders.
30. A slider having optimized crown or camber curvature prepared from substrate material having an air-bearing side and a flex side, prepared by a process using a laser which produces a pulsed laser beam, the laser beam having a pulse width in the range of 1×10−9 seconds to 1×10−3 seconds, with an energy per pulse in the range of 1 to 1,000,000 microjoules, and a repetition rate between 1 Hz and 400 kHz, the process comprising the steps of:
- (A) applying the laser beam to the flex side of the substrate material; and
- (B) varying the fluence of the laser beam to optimize the curvature in the substrate material.
31. A slider prepared by the process of claim 30, wherein fluence is controllably varied by changing the power output of the laser.
32. A slider prepared by the process of claim 30, wherein fluence is controllably varied by changing the spot size of the laser beam.
33. A slider prepared by the process of claim 32, wherein the spot size of the laser beam is varied by changing the position of the substrate material relative to the focal plane of the laser beam.
34. A slider prepared by the process of claim 32, wherein the spot size is controllably varied by changing the position of the focal plane of the laser beam relative to the substrate material.
35. A slider prepared by the process of claim 34, wherein the focal plane of the laser is moved relative to the substrate material by using at least one focusing lens which is attached to a movable mount.
36. A slider prepared by the process of claim 30, wherein the laser beam is conditioned with a beam expander that has adjustable beam expansion.
37. A slider prepared by the process of claim 30, wherein the substrate material is one or more rows of sliders, which are then separated to produce individual sliders.
Type: Application
Filed: Aug 29, 2003
Publication Date: Aug 11, 2005
Inventors: Andrew Tam (Saratoga, CA), Chie Poon (San Jose, CA), Ping-Wei Chang (San Jose, CA)
Application Number: 10/652,346