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Lubricant reflow after laser heating in heat assisted magnetic recording
Haoyu Wu, Alejandro Rodriguez Mendez, Shaomin Xiong, and David B. Bogy
Citation: Journal of Applied Physics 117, 17E310 (2015); doi: 10.1063/1.4914073
View online: http://dx.doi.org/10.1063/1.4914073
View Table of Contents: http://scitation.aip.org/content/aip/journal/jap/117/17?ver=pdfcov
Published by the AIP Publishing
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Lubricant reflow after laser heating in heat assisted magnetic recording
Haoyu Wu, Alejandro Rodriguez Mendez, Shaomin Xiong,
a)
and David B. Bogy
Computer Mechanics Lab, University of California at Berkeley, Berkeley, CA 94720, USA
(Presented 6 November 2014; received 11 September 2014; accepted 30 October 2014; published
online 6 March 2015)
In heat assisted magnetic recording (HAMR) technology for hard disk drives, the media will be
heated to about 500
C during the writing process in order to reduce its magnetic coercivity and
thus allow data writing with the magnetic head transducers. The traditional lubricants such as Z-dol
and Z-tetraol may not be able to perform in such harsh heating conditions due to evaporation,
decomposition and thermal depletion. However, some of the lubricant depletion can be recovered
due to reflow after a period of time, which can help to reduce the chance of head disk interface fail-
ure. In this study, experiments of lubricant thermal depletion and reflow were performed using a
HAMR test stage for a Z-tetraol type lubricant. Various lubricant depletion profiles were generated
using different laser heating conditions. The lubricant reflow process after thermal depletion was
monitored by use of an optical surface analyzer. In addition, a continuum based lubrication model
was developed to simulate the lubricant reflow process. Reasonably good agreement between simu-
lations and experiments was achieved.
V
C
2015 AIP Publishing LLC.
[http://dx.doi.org/10.1063/1.4914073]
I. INTRODUCTION
In current hard disk drives (HDDs), nanometer-thick
lubricant layers are applied on the surface of the media to
provide protection for the heads and disks, by reducing the
friction and wear during accidental slider disk contact.
1
The
lubricant films are synthesized from Perfluoropolyether
(PFPE) molecules, e.g., Z-tetraol, which are stable enough to
protect the disk at and around room temperature for at least
five years.
On the other hand, high magnetic anisotropy materials
need to be used to break the limit of superparamagnetism in
order to increase storage areal density beyond 1Tb/in.
2
. The
magnetic state of this kind of media is so stable at room tem-
perature that current magnetic transducers may not be able to
switch its orientation. Therefore, heat assisted magnetic re-
cording (HAMR) technology
2,3
has been proposed to solve
this probl em. In HAMR, the magnetic layer is heated up to
its Curie temperature with a laser such that the magnetic
coercivity of the media is reduced and data writing with the
magnetic transducers is possible.
Since the lubricant layer is on top of the magnetic layer,
it will also be heated locally to a similar temperature. The
harsh heating condition can damage traditional lubricants
and reduce their lifetime due to evaporation, decomposition
and thermal depletion.
4,5
However, some of the lubricant
depletion can be recovered due to reflow after some period
of time. The reflow behavior can help to cure the lubricant
depletion and reduce the chance of hard head disk interface
(HDI) failure. It is therefore important to understand the
mechanisms and characteristics of the lubricant reflow
behavior for HAMR systems.
In this paper, experimental studies of lubricant reflow
were performed in a HAMR test stage for a Z-tetraol type
lubricant. Section II describes the experimental setup. The
observed reflow behavior of the lubricant is discussed in
Sec. III.SectionIV introduces a numerical model for lubri-
cant reflow and compares the numerical simulation w ith our
experimental results.
II. EXPERIMENTAL CONDITIONS AND PROCEDURE
A HAMR test stage was built to provide HAMR-like
heating conditions on the disk and study the lubricant deple-
tion and reflow behavior. The test stage contains the follow-
ing three parts: an illumination module that can generate a
laser beam at different power levels and focus the laser spot
onto the disk with a size of a few microns, a spindle stage
that can spin a disk at a controlled speed, and a servo motor
that can control the radial movement of the laser spot such
that different parts of a disk can be heated by the laser. A
schematic drawing of the test system is shown in Fig. 1.
FIG. 1. Schematic drawing for the HAMR test stage. The Central Controller
is for the spindle, the Laser Generator, and the Servo Motor. The Laser
Generator illuminates the spinning disk with a laser light. The Servo Motor
controls the objective lens such that different parts can be exposed to the
laser.
a)
Author to whom correspondence should be addressed. Electronic mail:
xshaomin@berkeley.edu.
0021-8979/2015/117(17)/17E310/4/$30.00
V
C
2015 AIP Publishing LLC117, 17E310-1
JOURNAL OF APPLIED PHYSICS 117, 17E310 (2015)
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Since HAMR disks were unavailable to us, commercial
Perpendicular Magnetic Recording (PMR) disks were used
instead in this investigation. The disks were 3.5 in. in diame-
ter with aluminum substrates. The lubricant type was Z-
tetraol with A20H additives, 60% bonding ratio and thick-
ness of 9.5 A
˚
.
As shown in Fig. 1, a laser spot generated from the illumi-
nation module was focused on the spinning disk. The laser spot
heats up the disk and provides a HAMR-like condition. This
illumination procedure contains three controllable parameters:
laser power incident on the spinning disk (P
inc
), disk’s spinning
speed (x
disk
) and number of disk revolutions (repetitions) dur-
ing laser illuminat ion (n
illum
). P
inc
was controlled by optical fil-
ters between the laser generator and disk; x
disk
and n
illum
were
controlled by an in-house designed electronic controller based
on a field programmable gate array (FPGA) board. The optical
encoder in the spindle was used to count the number of revolu-
tions of the disk. The laser ill umination repetitions (n
illum
) can
be precisely controlled. The relationship between repetitions
and laser illumination time is shown in Fig. 2.
The disk was exposed to the laser at a constant P
inc
while spinning at a constant x
disk
. However, we used differ-
ent values of n
illum
from 1000 to 1 on different tracks. Soon
after the laser exposure, the disk was measured by a Candela
optical surface analyzer (OSA). The Q-Phase channel was
used to measure the lubricant thickness change.
6
Scans by
the OSA were taken periodically at room temperature at
intervals of about 95-s up to about 22 min in total such that
the lubricant profile could be recorded at different times. A
scan was also taken again after 24 h to see the final state of
the lubricant.
III. LUBRICANT REFLOW PROCESS
Due to spindle run-out, the Q-phase image of the lubri-
cant showed some curvature and background. A script was
developed to post process the images and eliminate the run-
out curvature and non-uniform background. Examples of the
processed OSA images are shown in Fig. 3.
As can be seen in Fig. 3(a), the parallel lines represent
the exposed tracks to the laser for different n
illum
. The
increase of reflectivity in the Q-Phase indicates a lubricant
thickness decrease. This is mainly due to lubricant depletion.
Higher n
illum
causes significantly more lubricant depletion as
shown in Fig. 3 where the tracks on the top have a larger
change of reflectivity. Figures 3(b) and 3(c) show the OSA
Q-phase images after some time has elapsed. The reflectivity
change of the tracks shown in Figs. 3(b) and 3(c) becomes
smaller compared to Fig. 3(a), indicating that the lubricant
flows back to the depleted region. Fig. 3(d) shows the reflec-
tion of the lubricant after 24 h. Fig. 3(d) shows no apparent
reflection when n
illum
100, which means that the lubricant
has recovered back to its initial state. However, when
n
illum
> 100, there still remain some changes of reflectivity
which were not recovered in 24 h of lubricant reflow. This
final state condition may be due to degradation of the carbon
overcoat (COC) or magnetic layers.
4
To eliminate possible
non-lubricant effects, only the n
illum
100 conditions are
discussed below.
Figure 4 shows the maximum lubricant depletion depth
as a function of time for one set of experiments. The
FIG. 2. Modulation of laser by spindle index.
FIG. 3. OSA scanning images of relative reflectivity on a disk after certain
repetitions of illumination by laser at: (a) 0 min, (b) 3 min, (c) 9 min, and
(d) 24 h, respectively. The x-axis is the angular position in units of degrees
and the y-axis is the relative radial position in units of lm. The relative
reflectivity slowly fades as time elapses. The n
illum
from top to bottom for
the seven tracks are 1000, 500, 100, 50, 10, 5, 1, respectively.
FIG. 4. Lubricant relaxation after laser
depletion. (a) The three different lines
show different laser illumination repe-
titions. Less repetitions result in shal-
lower initial lubricant depletion. The
reflow trends are similar for the three
different conditions. (b) Lubricant
depletion normalized with respect to
initial value. The depletion is set to 1
at t ¼ 0. Similar trends are shown.
17E310-2 Wu et al. J. Appl. Phys. 117, 17E310 (2015)
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lubricant depletion and reflow profiles were obtained from
the OSA Q-phase images, some of which were shown in Fig.
3. The experimental parameters used in Fig. 4 are x
disk
¼600
RPM and P
inc
¼165 mW. The illumination repetitions were
100, 50, and 5, respectively. The depletion curve with
n
illum
¼ 1 was too small for a reliable analysis, therefore
these result is not presented.
As shown in Fig. 4, the lubricant depletion is more
severe when the disk is illuminated for mo re repetitions. To
exclude the effect of different initial lubricant depletion on
the reflow, we normalized the lubricant depletion curves by
its initial value as shown in Fig. 4(b). It is observed that the
lubricant depletion decreases as time elapses, which indi-
cates that the lubricant flows back into the depleted area. The
reflow rate is initially fast and decreases with time. Almost
80% of the lubricant recovers within 20-min of relaxation at
room temperature.
7
IV. COMPARISON BETWEEN SIMULATION AND
EXPERIMENTS
Simulations of lubricant reflow were carried out to com-
pare them with the experimental results. The lubricant reflow
was described using continuum theory with a modified
(effective) viscosity.
8
Within the continuum approach, the
dimensions of the thin film on the disk surface make it possi-
ble to use lubrication theory and thus we obtain the govern-
ing equations described below
@h
@t
þ
1
3l
@
@x
h
3
dP h
ðÞ
dh
@h
@x
¼ 0 ; (1)
where h ¼ hðx; tÞ is the film thickness, l is the effective
lubricant viscosity, PðhÞ is the disjoining pre ssure arising
from van der Waals interaction s between the lubricant and
the solid substrate.
9
This disjoining pressure is of the form
PðhÞ¼Ah
3
, where A is the Hamaker constant. The initial
condition, as seen in Fig. 5(a), was given by the lubricant
depletion profile obtained in the experiments at time t ¼ 0s.
As boundary conditions, we considered zero volume flow at
the right and left boundaries. This condition is equivalent to
setting dh=dx ¼ 0 at the boundaries. It can be observed that
Eq. (1) depends only on the ratio of the Hamaker constant to
lubricant visco sity. This ratio was adjusted to give the best
match to the experimental results. The simulation results of
lubricant reflow are shown in Fig. 5.
It can be seen from Fig. 5(b) that the simulation results
fit adequately the experimental data. However, there exist
regions of some discrepancy. In the first 400 s of reflow, the
simulation results show a faster recovery rate than the experi-
ments. After this time, the reflow in the simulation slows
down relative to the experiments. This discrepancy may be
explained by noting that the lubricant viscosity of thin films
can be thickness dependent as discussed in Ref. 10. This phe-
nomenon was not included in the present simulation model.
V. CONCLUSION
In this paper, the thermal depletion behavior of Z-tetraol
due to a free laser beam heating condition as well as the re-
covery behavior after heating was studied. The initial lubri-
cant depletion was different for different laser heating
conditions, i.e., a longer heating duration causes more lubri-
cant depletion. However, a similar trend was found regard-
less of initial lubricant depletion. Almost 80% of lubricant
reflows back within 20 min at room temperature. Simulation
results show a reasonably good agreement with experiments.
Real HAMR laser conditions use a near field transducer
(NFT) as a heating method to achieve heated spots of tens of
nanometers rather than a few microns. So the NFT heating
has a spot size a few orders of magnitude smaller and its du-
ration is a few orders of magnitude shorter than our free laser
beam heating. Further study will be made with the NFT heat-
ing and HAMR disks as soon as the needed components
become available.
ACKNOWLEDGMENTS
This research was supported by the Computer
Mechanics Laboratory (CML) of the University of
California at Berkeley.
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FIG. 5. (a) Film thickness profile at
selected times obtained from simula-
tions. (b) Depth of the maximum
depletion point in the film as obtained
from experiments and results. The
experiment parameters are x
disk
¼ 600
RPM, P
inc
¼ 165 mW and n
illum
¼ 100.
The simulation parameters are l
¼ 1:5Pa s and A ¼ 1 10
21
J.
17E310-3 Wu et al. J. Appl. Phys. 117, 17E310 (2015)
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