U.S. patent application number 10/763857 was filed with the patent office on 2004-08-05 for methods and apparatus for rendering an optically encoded medium unreadable.
This patent application is currently assigned to FlexPlay Technologies, Inc.. Invention is credited to Lawandy, Nabil M., Norland, Kenneth S., Zepp, Charles M..
Application Number | 20040152015 10/763857 |
Document ID | / |
Family ID | 26782527 |
Filed Date | 2004-08-05 |
United States Patent
Application |
20040152015 |
Kind Code |
A1 |
Lawandy, Nabil M. ; et
al. |
August 5, 2004 |
Methods and apparatus for rendering an optically encoded medium
unreadable
Abstract
Methods and apparatus are provided for making an optically
readable media unreadable. The method includes steps of (a)
providing the media with an optically activated mechanism that
degrades the reflectivity of a surface wherein information is
encoded; (b) exposing the media to optical radiation for reading
out the information; and, during the step of exposing, (c)
initiating the operation of the optically activated mechanism. In
this embodiment the step of initiating includes steps of (d)
generating singlet oxygen in a layer disposed on the media; and (e)
reacting the singlet oxygen with a metal-containing layer for
oxidizing the surface of the metal-containing layer, thereby
degrading the reflectivity of the surface. In a further aspect the
optically activated mechanism causes a defocusing of a readout
beam, thereby degrading reflection of the readout beam from a
surface wherein information is encoded. In another embodiment the
method deforms a surface of the layer resulting in readout beam
aberration or in an inability to correctly stay on track. In
another embodiment a portion of the surface is removed to the
atmosphere, such as by evaporation of sublimation. In this
embodiment a layer of the media is comprised of a volatile
component and at least one other component. Removing at least some
of volatile component by evaporation or sublimation causes an
increase in at least one of photoabsorption or scattering or
surface roughness with the remaining component, thereby rendering
at least a portion of encoded information of the media unreadable,
or affecting the tracking operation.
Inventors: |
Lawandy, Nabil M.; (North
Kingstown, RI) ; Zepp, Charles M.; (Hardwick, MA)
; Norland, Kenneth S.; (Lexington, MA) |
Correspondence
Address: |
WILMER CUTLER PICKERING HALE AND DORR, LLP
60 STATE STREET
BOSTON
MA
02109
US
|
Assignee: |
FlexPlay Technologies, Inc.
|
Family ID: |
26782527 |
Appl. No.: |
10/763857 |
Filed: |
January 23, 2004 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
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10763857 |
Jan 23, 2004 |
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09996058 |
Nov 28, 2001 |
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6709802 |
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09996058 |
Nov 28, 2001 |
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09338959 |
Jun 24, 1999 |
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6338933 |
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60090682 |
Jun 25, 1998 |
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Current U.S.
Class: |
430/270.11 ;
369/284; 428/64.8; 430/945; G9B/7.171 |
Current CPC
Class: |
G11B 7/2542 20130101;
G11B 7/252 20130101; G11B 23/282 20130101; G11B 7/2575 20130101;
G11B 7/2585 20130101; G11B 20/00797 20130101; Y10S 430/146
20130101; G11B 7/2534 20130101; G11B 23/505 20130101; G11B 20/00086
20130101 |
Class at
Publication: |
430/270.11 ;
369/284; 430/945; 428/064.8 |
International
Class: |
G11B 007/24 |
Claims
What is claimed is:
1. A method for making an optically readable media unreadable by a
play process, comprising steps of: providing the media with an
optically activated mechanism that degrades the reflectivity of a
surface wherein information is encoded; exposing the media to
optical radiation for reading out the information; and during the
step of exposing, initiating the operation of the optically
activated mechanism.
2. A method as in claim 1, wherein the step of initiating is
comprised of steps of: generating singlet oxygen in a layer
disposed on the media; and reacting the singlet oxygen with a
metal-containing layer for oxidizing the surface of the
metal-containing layer, thereby degrading the reflectivity of the
surface.
3. A method as in claim 2, wherein the step of generating includes
a step of diffusing the singlet oxygen through a diffusion barrier
that is disposed between the layer and the metal-containing
layer.
4. A method for making an optically readable media unreadable by a
play process, comprising steps of: providing the media with an
optically activated mechanism that causes a defocusing of a readout
beam, thereby degrading reflection of the readout beam from a
surface wherein information is encoded; exposing the media to
optical radiation for reading out the information; and during the
step of exposing, initiating the operation of the optically
activated mechanism.
5. A method as in claim 4, wherein the step of initiating is
comprised of steps of: generating an optical intensity gradient in
a layer disposed on the media; and in response to the generated
gradient, deforming a surface of the layer resulting in at least
one of readout beam aberration or a degradation of a readout
tracking function.
6. A method as in claim 5, wherein the step of providing provides
the layer so as to comprise an azobenzene containing polymer.
7. A method as in claim 4, wherein the step of initiating is
comprised of steps of: irradiating a photocurable polymer region
that comprises the media; and in response to the irradiation,
photopolymerizing the polymer, thereby changing an index of
refraction of the polymer resulting in readout beam aberration.
8. An optically readable media capable of being made unreadable by
a play process, said media comprising an optically activated
mechanism that is responsive to light used to readout information
for degrading the reflectivity of a surface wherein the information
is encoded.
9. A media as in claim 8, wherein said mechanism is comprised of a
photosensitizer compound for reacting with oxygen molecules that
are preloaded within a layer for generating singlet oxygen in the
layer, the singlet oxygen reacting with a metal-containing layer
for oxidizing the surface of the metal-containing layer, thereby
degrading the reflectivity of the surface.
10. A media as in claim 9, and further comprising a diffusion
barrier disposed between said layer and said metal-containing
layer.
11. An optically readable media capable of being made unreadable by
a play process, said media comprising an optically activated
mechanism that is responsive to light used to readout information
for defocusing a readout beam, thereby degrading reflection of the
readout beam from a surface wherein information is encoded.
12. A media as in claim 11, wherein said mechanism is comprised of
a layer of polymer that is responsive to an optical intensity
gradient generated by said readout beam for deforming a surface of
said layer resulting in readout beam aberration.
13. A media as in claim 12, wherein said layer comprises an
azobenzene containing polymer.
14. A media as in claim 11, wherein said mechanism is comprised of
at least one region comprised of photoresponsive polymer that is
responsive to the readout beam for being photopolymerized, thereby
changing an index of refraction of the photocurable polymer
resulting in readout beam aberration.
15. A method for making an optically readable media unreadable,
comprising steps of: providing the media with a layer that is
comprised of a volatile component and at least one other component;
removing at least some of volatile component; and causing an
increase in at least one of photoabsorption or scattering or
surface roughness with the remaining component.
16. A method as in claim 15, wherein the other component is
comprised of a lactone dye.
17. A method as in claim 15, wherein the other component is
comprised of crystal violet lactone.
18. A method as in claim 15, wherein the layer is comprised of
poly-p-(hydroxystyrene), ethanol, crystal violet lactone and
N-methyl pyrrolidinone.
19. A method as in claim 15, wherein the layer is comprised of
poly-p-(hydroxystyrene), ethanol, crystal violet lactone, ammonia,
N-methyl pyrrolidinone, and formaldehyde.
20. A method as in claim 15, wherein the layer is comprised of
cellulose acetate butyrate, ethyl acetate, silica gel, and benzyl
alcohol.
21. A method as in claim 15, wherein the layer is comprised of a
salt of a volatile amine, a non-volatile acid component and a
lactone dye.
22. A method as in claim 15, wherein the layer is comprised of a
salt of a volatile amine, a non-volatile acid component and a pH
indicator dye.
23. A method as in claim 15, wherein the layer is comprised of a
water damp polymer film containing a pH indicator dye, wherein
during storage the layer is exposed to an atmosphere of a gas whose
water solution is one of acidic or basic, and wherein upon removal
from storage a volatile gas evaporates from the water damp film,
and the pH changes causing a color change in the pH indicator
dye.
24. A method as in claim 15, and further comprising a preliminary
step of constructing the layer as a separate component layer, and
then a step applying the separate component layer to a surface of
the optically readable media.
25. A method for making an optically readable media unreadable,
comprising steps of: providing the media with a layer that is
comprised of a sensitive inorganic-material; exposing the layer to
an atmosphere containing a substance comprised of at least one of
water vapor or carbon dioxide; and reacting the inorganic material
with the substance to cause an increase in at least one of
photoabsorption or scattering or surface roughness.
26. A method as in claim 25, wherein the layer is comprised of
KBr.
27. A method as in claim 25, wherein the layer is comprised of
CsF.
28. An optically readable media comprising a patterned structure
for encoding information that can be readout by application of
light, said optically readable media further comprising a layer
that is comprised of a volatile component and at least one other
component wherein removing at least some of volatile component
causes an increase in at least one of photoabsorption or scattering
or surface roughness with the remaining component, thereby
rendering at least a portion of the encoded information
unreadable.
29. A media as in claim 28, wherein the other component is
comprised of a lactone dye.
30. A media as in claim 28, wherein the other component is
comprised of crystal violet lactone.
31. A media as in claim 28, wherein the layer is comprised of
poly-p-(hydroxystyrene), ethanol, crystal violet lactone and
N-methyl pyrrolidinone.
32. A media as in claim 28, wherein the layer is comprised of
poly-p-(hydroxystyrene), ethanol, crystal violet lactone, ammonia,
N-methyl pyrrolidinone, and formaldehyde.
33. A media as in claim 28, wherein the layer is comprised of
cellulose acetate butyrate, ethyl acetate, silica gel, and benzyl
alcohol.
34. A media as in claim 28, wherein the layer is comprised of a
salt of a volatile amine, a non-volatile acid component and a
lactone dye.
35. A media as in claim 28, wherein the layer is comprised of a
salt of a volatile amine, a non-volatile acid component and a pH
indicator dye.
36. A media as in claim 28, wherein the layer is comprised of a
water damp polymer film containing a pH indicator dye, wherein
during storage the layer is exposed to an atmosphere of a gas whose
water solution is one of acidic or basic, and wherein upon removal
from storage a volatile gas evaporates from the water damp film,
and the pH changes causing a color change in the pH indicator
dye.
37. A media as in claim 28, wherein said layer is applied by one of
a coating or printing process or as an adhesively affixed separate
component layer.
38. An optically readable media comprising a patterned structure
for encoding information that can be readout by application of
light, said optically readable media further comprising a layer
that is comprised of a sensitive inorganic material wherein
exposure of said layer to an atmosphere containing a substance
causes reaction between the inorganic material and the substance to
cause an increase in at least one of photoabsorption or scattering
or surface roughness, thereby rendering at least a portion of the
encoded information unreadable.
39. A media as in claim 38, wherein the layer is comprised of
KBr.
40. A media as in claim 38, wherein the layer is comprised of
CsF.
41. A method for making an optically readable media unreadable,
comprising steps of: providing the media with a surface layer
having a planar surface topography; and subsequent to or during a
first readout of the optically readable media, modifying at least a
portion of the planar surface topography to a non-planar surface
topography by the use of at least one of a photoresponsive polymer,
a removal of a substance from the surface layer to the atmosphere,
or by interaction with a substance in the atmosphere without
significantly modifying a transparency of the surface layer to a
readout beam, wherein a deviation of the non-planar surface layer
topography from the planar surface layer topography is sufficient
to detrimentally affect at least a tracking operation of a readout
device that generates the readout beam.
Description
CLAIM OF PRIORITY FROM A COPENDING PROVISIONAL PATENT
APPLICATION
[0001] Priority is herewith claimed under 35 U.S.C. .sctn.119(e)
from copending Provisional Patent Application 60/090,682, filed
Jun. 25, 1998. The disclosure of this Provisional Patent
Application is incorporated by reference herein in its
entirety.
FIELD OF THE INVENTION
[0002] This invention relates to optically readable data storage
media and, more particularly, to techniques to render said media
unreadable after being read at least once.
BACKGROUND OF THE INVENTION
[0003] It is often desirable when distributing software or other
information that is recorded on a medium to insure that only one
party is enabled to read the recorded information. For example, a
company that sells computer software will find it advantageous to
enable only the purchaser to read the software from a disk and
transfer or install the software to computer memory, such as a hard
disk, while preventing subsequent access by other parties to the
software. However, this has proven to be a vexing problem that is
not readily solved.
[0004] When the information is distributed on a read/write medium,
such as the ubiquitous floppy disk, it may be possible to cause the
installation software to erase all or part of the information after
it has been successfully installed. Unfortunately, such information
may be distributed on write-protected disks, thereby rendering such
erasure impossible. Also, any protection mechanism that relies on
computer software to implement has the potential to be defeated by
additional computer software.
[0005] U.S. Pat. No. 5,815,484 discloses an optical disk having a
reflective metallic layer with a plurality of data structures (pits
and lands) and a reactive compound superimposed over at least some
of the data structures. The reactive compound is a photochromic
compound which changes from an optically transparent condition to
an optically opaque condition when subjected to readout light
and/or atmospheric oxygen. The darkening of the photochromic
compound prevents a sufficient amount of readout light from being
detected by the readout apparatus, thereby effectively rendering
the optical disk unreadable.
[0006] At least one perceived disadvantage of this approach is that
photochromic darkening is often reversible, which could be used to
defeat the technique.
OBJECTS OF THE INVENTION
[0007] It is a first object and advantage of this invention to
provide an improved system and method to render an optically
readable media, such as, but not limited to, a laser disk, a
compact disk (CD), or a digital video disk (DVD), unreadable.
[0008] It is a second object and advantage of this invention to
provide an improved system and method to render an optically
readable media permanently unreadable, after having been read at
least once.
[0009] It is a third object and advantage of this invention to
provide an optically activated mechanism that destroys or impairs
the reflectivity of a metal-containing layer, thereby rendering an
optically readable media unreadable.
[0010] It is a further object and advantage of this invention to
provide an optically activated mechanism that modifies a
transparent layer so as to cause readout beam aberration, thereby
rendering an optically readable media unreadable.
[0011] It is once further object and advantage of this invention to
provide a mechanism that relies on non-atmospheric oxygen, such as
oxygen preloaded into or generated within a layer of an optically
readable media, for modifying the optical properties of the media
so as to render the media optically unreadable.
[0012] It is still another object and advantage of this invention
to provide a mechanism that relies on an evaporative technique for
modifying the optical properties of an optically readable media so
as to render the media optically unreadable.
[0013] It is another object and advantage of this invention to
provide a mechanism that alters a surface characteristic of an
optically readable media so as to detrimentally affect a readout
apparatus tracking process during an attempted readout of the
media.
[0014] It is a further object and advantage of this invention to
provide a mechanism that causes surface topography changes to an
optically readable media so as to detrimentally affect a readout
apparatus feedback and tracking process, thereby adversely
affecting the fidelity of the readout.
SUMMARY OF THE INVENTION
[0015] The foregoing and other problems are overcome and the
objects and the advantages of the invention are realized by methods
and apparatus in accordance with embodiments of this invention.
[0016] In one aspect this invention provides a method for making an
optically readable media unreadable during a play process. The
method includes steps of (a) providing the media with an optically
activated mechanism that degrades the reflectivity of a surface
wherein information is encoded; (b) exposing the media to optical
radiation for reading out the information; and, during the step of
exposing, (c) initiating the operation of the optically activated
mechanism. In this embodiment the step of initiating includes steps
of (d) generating singlet oxygen in a layer disposed on the media;
and (e) reacting the singlet oxygen with a metal-containing layer
for oxidizing the surface of the metal-containing layer, thereby
degrading the reflectivity of the surface. The step of generating
may include a step of diffusing the singlet oxygen through a
diffusion barrier that is disposed between the layer and the
metal-containing layer.
[0017] In a further aspect the optically activated mechanism causes
a defocusing of a readout beam, thereby degrading reflection of the
readout beam from a surface wherein information is encoded.
[0018] In one embodiment the method generates an optical intensity
gradient in a layer disposed on the media; and, in response to the
generated gradient, deforms a surface of the layer resulting in
readout beam aberration and/or adversely affecting the tracking
process, resulting in readout degradation and a loss of fidelity.
In this case the step of providing provides the layer so as to
comprise an azobenzene-containing polymer. In an alternate
embodiment a surface layer may react with an atmospheric component,
such as oxygen, so as to degrade the tracking process by inducing a
surface topography change, without inducing any significant change
in the light transmission properties of the surface layer.
[0019] In another embodiment the step of initiating includes steps
of: irradiating a photocurable polymer region that comprises part
of the media; and, in response to the irradiation,
photopolymerizing the polymer, thereby changing an index of
refraction of the polymer resulting in readout beam aberration.
[0020] This invention also encompasses optically encoded media that
operate in accordance with the foregoing methods, and that are
constructed in accordance with the techniques of this
invention.
[0021] In accordance with further embodiments of this invention an
optically readable media has a patterned structure for encoding
information that can be readout by application of light, and
further includes a layer that is comprised of a volatile component
and at least one other component. Removing at least some of
volatile component by evaporation or sublimation causes an increase
in at least one of photoabsorption or scattering with the remaining
component, thereby rendering at least a portion of the encoded
information unreadable. The other component can include a lactone
dye, such as crystal violet lactone, and the volatile component can
be, for example, NMP (N-methyl pyrrolidinone). In a further
embodiment an organic material, such as CsF or KBr, is coated on
the surface of the disk and provides a surface haze when exposed to
water vapor or carbon dioxide, thereby increasing the scattering
and decreasing the signal-to-nose ratio, and degrading the readout
fidelity.
[0022] A method is disclosed for making an optically readable media
unreadable. This method includes steps of (a) providing the media
with a surface layer having a planar surface topography; and (b)
subsequent to or during a first readout of the optically readable
media, modifying at least a portion of the planar surface
topography to a non-planar surface topography. This is accomplished
by the use of at least one of a photoresponsive polymer, a removal
of a substance from the surface layer to the atmosphere, or by
interaction with a substance in the atmosphere. This latter process
may occur without significantly modifying a transparency of the
surface layer to a readout beam. The deviation of the non-planar
surface layer topography from the planar surface layer topography
is sufficient to detrimentally affect at least a tracking operation
of a readout device that generates the readout beam.
BRIEF DESCRIPTION OF THE DRAWINGS
[0023] The above set forth and other features of the invention are
made more apparent in the ensuing Detailed Description of the
Invention when read in conjunction with the attached Drawings,
wherein:
[0024] FIG. 1 is a schematic diagram of a conventional optical
scanning system for reading an optically readable disk that
incorporates one or more features of the present invention;
[0025] FIG. 2 is a schematic side elevation and partial
cross-sectional view of an optical scanning head of the optical
scanning system scanning the optically readable disk of FIG. 1;
[0026] FIGS. 3A and 3B are a first pair of enlarged partial
cross-sectional views showing a portion of the optical disk in FIG.
2 according to a first embodiment of the invention, specifically an
optically deformable photopolymer layer embodiment, wherein the
portion of the disk is shown in FIGS. 3A and 3B both before and
after, respectively, scanning by an optical beam;
[0027] FIGS. 4A and 4B are a first pair of enlarged partial
cross-sectional views showing a portion of the optical disk in FIG.
2 according to a second embodiment of the invention, specifically
an optically induced reflectivity modification embodiment, wherein
the portion of the disk is shown in FIGS. 4A and 4B both before and
after, respectively, scanning by an optical beam;
[0028] FIGS. 5A and 5B are a first pair of enlarged partial
cross-sectional views showing a portion of the optical disk in FIG.
2 according to a third embodiment of the invention, specifically an
optically cured photopolymer embodiment, wherein the portion of the
disk is shown in FIGS. 5A and 5B both before and after,
respectively, scanning by an optical beam;
[0029] FIG. 6 is a flow chart diagrammatically depicting generation
of singlet oxygen in a photosensitizer layer of the optical disk
shown in FIG. 2, according to the reflectivity modifying embodiment
shown in FIGS. 4A and 4B;
[0030] FIG. 7 illustrate a colorless lactone form (crystal violet
lactone) and its cationic (colored) form, and is useful in
explaining an embodiment of this invention that employs an
evaporative method for rendering an optically readable media
unreadable; and
[0031] FIG. 8 is an enlarged cross-sectional view of a portion of
an optically readable media having a surface topography that is
modified from a planar profile, and which can be used to
detrimentally affect the tracking operation of the readout device
in accordance with the teachings of this invention.
DESCRIPTION OF THE INVENTION
[0032] Referring now to FIG. 1, there is shown a schematic diagram
of an optical scanning system 1 for reading an optically readable
disk that incorporates one or more features of the present
invention. Although the present invention will be described with
reference to the embodiments shown in the drawings, it should be
understood that the present invention may be embodied in many forms
of alternative embodiments. In addition, any suitable size, shape
or type of materials or elements could be used.
[0033] It should further be noted at the outset that as employed
herein an "optically encoded" or "optically readable" media or
medium is intended to cover a number of various devices wherein
data, audio and/or video information is stored such that it can be
readout when a lightbeam (either visible light or invisible light)
is applied to the device. Such devices include, but are not limited
to, laser disks, compact disks (CDs), CD-ROMs, and digital video or
versatile disks (DVDs), as well as certain kinds of tape. In
general, the devices of interest to this invention incorporate some
type of structure that is capable of altering the reflectivity of
the device to the readout light such that a logic 1 bit can be
distinguished from a logic 0 bit. By rendering such a device
"unreadable" it should be understood that it is not necessary to
make the entire device unreadable. For example, it may be necessary
to make only a relatively small portion of a boot record or a
directory of contents unreadable such that the entire device
becomes unusable, or such that some predetermined portion of the
device becomes unusable. Making the device unreadable may also
encompass adversely affecting the readout device optical feedback
and tracking process, such as by altering the surface topography.
By example, in this case the readout laser focus adjustments may
not be able to react quickly enough to the surface profile changes,
resulting in an inability to maintain the correct tracking. This
has been found to manifest itself as "skipping" through a music
segment of a compact disk, or to otherwise negatively impact the
fidelity of the output.
[0034] The optical scanning system 1, which may be conventional in
construction, generally comprises a disk drive 10 and an optical
scanning head 30. The disk drive 10 is generally adapted to move an
optically readable disk 20, such as a CD-ROM, relative to the
optical scanning head 30. In the embodiment shown in FIG. 1, the
optical scanning head 30 is located below the optical disk 20 for
scanning a lower surface of the disk, though in other embodiments
the scanning head may located to scan an upper surface of the disk.
The scanning head 30 is preferably held by a movable carriage or
arm (not shown) so that the head 30 may be moved relative to a
center of the disk. For example, the scanning head may be able to
translate radially relative to the center of the disk 20 or
circumferentially around the center of the disk. In alternate
embodiments, the optical scanning head may be fixedly held relative
to the center of the optically readable disk. As the disk 20 moves
over the scanning head 30, the head reads optically readable data
structures 23 (see FIG. 2) disposed on the disk 20.
[0035] Referring still to FIG. 1, the disk drive 10 includes a
motor 12, a drive shaft 14 and a disk support or chuck 16. The
drive shaft 14 operably connects the motor 12 to the chuck 16.
Thus, when energized the motor 12 rotates the chuck 16 through the
drive shaft 14. The chuck 16 comprises appropriate holding means
(not shown) to stably hold the disk 20 thereon when the chuck 16 is
rotated by the motor 12. The motor 12 is adapted to rotate the
chuck 16 and the disk 20 held thereon at predetermined speeds. The
motor 12 may operate to rotate the disk 20 at a variable rotational
velocity so that the disk presents a reading surface to the
scanning head 30 which moves at a constant linear velocity. For
example, as the scanning head 30 is radially translated closer to
the center of the disk 20 on the chuck 16, the motor 12 spins the
disk 20 at an increasing rotational velocity. Thus, the portion of
the disk 20 passing over the scanning head 30 is moving at a
constant linear velocity. It is noted that in conventional laser
disks, the data structure is generally disposed in a single track
spiralling from the edge of the disk towards the center which
requires that the disk spin at a variable rate of rotation in order
for the track to move at a constant linear speed relative to the
scanning head. By way of example, the disk drive 10 may rotate a
DVD at an appropriately increasing rate of rotation to provide a
linear velocity of about 3.5 m/sec over the scanning head 30.
[0036] Referring now to FIG. 2, the scanning head 30 generally
includes a light source 32 and a photodetector 34. The light source
32 generates and directs an incident or interrogating beam 100 of
electromagnetic radiation (also referred to herein as optical
radiation) against the optical disk 20. The optical disk 20
includes a reflective layer 22 with data structures 23 formed
thereon or therein. The interrogating beam 100 of electromagnetic
radiation directed against the optical disk 20 is reflected by the
reflecting layer 22 as a reflected beam 102. The reflected beam 102
is then detected by then photodetector 34 of the optical scanning
head 30. When the disk drive 10 rotates the disk 20 relative to the
scanning head 30, the interrogating beam 100 passes over the data
structures 23 on the reflective layer 22 of the disk. As the
interrogating beam 100 moves over the data structures 23, the data
structures modulate the reflected beam 102. The modulation in the
reflected beam 102 is registered at the photodetector 34 of the
scanning head 30 and converted to electrical signals.
[0037] More particularly, and by way of example, the light source
32 may include a laser diode 36 or other such suitable device for
generating the interrogating beam 100 of optical radiation. The
beam 100 generated by the laser diode 36 may be directed through a
quarter wave plate 40 and through polarizing beam splitter 38 as
shown in FIG. 2. Alternatively, the positions of the wave plate and
beam splitter may be reversed so that the beam passes first through
the beam splitter and then through the wave plate. Also, the beam
generated by the laser diode 36 may be collimated by a collimator
(not shown) before encountering the wave plate 40. After the
interrogating beam 100 passes through the beam splitter 38, the
beam encounters an appropriate lens 42 which focuses the
interrogating beam 100 at a predetermined focal point. The
interrogating beam 100 emitted by the light source 30 may have a
wavelength of about 650 nm, although the beam may have other
wavelengths. The interrogating beam 100 may be focused to a spot
size of approximately 0.63 .mu.m. The depth of focus of the beam
100 is about 0.9 .mu.m, though this depth may be adjusted as
required. The interrogating beam 100 is modulated by an appropriate
modulator (such as an acousto-optic or electro-optic modulator, not
shown) to effect a residence time per bit of between about 100-200
nsec. The laser diode 36 is otherwise adapted to deliver
approximately 1 mW of power on the optical disk 20. The energy
deposited per bit by the interrogating beam 100 is about 200 pJ and
the fluence of the beam on the focus spot is about 50 mJ/cm.sup.2.
Therefore, the intensity of the interrogating beam 100 on the focus
spot is about 300 kW/cm.sup.2. In alternate embodiments, the light
source may have any other suitable configuration to generate an
interrogating beam of electromagnetic radiation having appropriate
characteristics for reading data structures from an optical
disk.
[0038] Still referring to FIG. 2, the reflective layer 22 of the
laser disk 20 is disposed between an upper protective layer 24 and
a lower layer 26. The construction of the lower layer 26 will be
described in greater detail below with reference to the three
preferred embodiments of this invention. The reflective layer 22
may be comprised of metal such as aluminum, though other suitable
materials may be used, and which is formed by appropriate means to
provide a reflecting surface 28 to the interrogating beam 100. As
mentioned previously, the reflective surface 28 of layer 22 is
encoded with information stored as data structures 23. The data
structures 23 are adapted to change the reflected beam 102 when the
interrogating beam 100 is incident on features of the data
structures 23. For example, the data structures 23 may comprise a
pattern of lands 25 and pits 27 formed in the reflective surface 28
of the optical disk 20. The lands 25 are raised portions on the
reflective surface 28 of the optical disk. The pits 27 are
depressed portions (relative to the lands 25) in the reflective
surface 28 of the optical disk 20. For example, the individual pits
27 may have a width of about 0.4 .mu.m and a length of between
about 0.41.9 .mu.m, though the pits may have any other suitable
length and width. In alternate embodiments, the data structures
formed in the reflective surface of the optical disk may have any
other suitable features which change a quality of the reflected
beam when the interrogating beam encounters these features. By way
of example such features may be sequences of scarified and
reflective surfaces or through holes in the reflective surface of
the optical disk.
[0039] In the preferred embodiment, as shown in FIG. 2, the
interrogating beam 100 generated by the light source 32 is focused
by the lens 42 such that the focal point is located at the `bottom`
surface of the pits 27 in the reflective surface 28 of the optical
disk 20. When the interrogating beam 100 is incident on the surface
of a pit 27, the interrogating beam 100 is reflected by the pit
surface as a reflected beam 102. The reflected beam 0.102 passes
through the lens 42 (now acting as a collimator for the reflected
beam) and is then deflected by the beam splitter 38 to strike the
photodetector 34 in the scanning head 30. When the interrogating
beam 100 is instead directed at a land 25 of the reflective surface
28, a lesser amount of the beam 100 is reflected back to be
detected by the photodetector 34. This is because the surface of
the land 25 is located at a different depth then the focal depth of
the interrogating beam 100.
[0040] Alternatively, the interrogating beam 100 generated by the
light source may be focused by the lens at the surface of the lands
25 and not the pits 27.
[0041] In either case, it can be appreciated that the change in
reflectivity between two states (corresponding to whether the
interrogating beam 100 is incident on a pit 27 or on a land 25),
provides a mechanism to encode binary data (i.e., ones and zeroes)
into the surface of the disk.
[0042] The preferred embodiments of the present invention will be
described hereafter only with reference to the case where the
interrogating beam 100 is focussed at the surface of the pits 27 in
the reflective surface 28 of the optical disk 20, though the
teachings of this invention are equally applicable to the case
where the interrogating beam is instead focussed at the surface of
the lands 25.
[0043] Referring now to FIGS. 3A and 3B, there is shown an enlarged
cross-sectional view of a portion A of the optical disk 20 in
accordance with a first embodiment of this invention. The optical
disk 20 is constructed so as to include a surface relief
photopolymer layer 200. The surface relief photopolymer layer 200
is comprised of one or more polymers, such as, by example, an
azobenzene containing polymer. It is known that an azobenzene
containing polymer is capable of exhibiting a surface deformations
in response to a presence of an optical intensity gradient.
[0044] Reference in this regard may be had to an article entitled
"Gradient force: The mechanism for surface relief grating formation
in azobenzene functionalized polymers", Applied Physics Letters,
Vol. 72, No. 17, pps. 2096-2098, 27 April 1998, J. Kumar et al. The
authors report on the derivation of a model for the formation of
holographic surface relief gratings in azobenzene functionalized
polymers. Forces leading to migration of polymer chains upon
exposure to light in the absorption band of an azo chromophore are
attributed to dipoles interacting with the gradient of the electric
field present in the polymer material. The authors further report
that an efficient trans-cis cycling in the azobenzenes allows
cooperative movement of the chromophores under the influence of
gradient forces.
[0045] In accordance with the teachings of this invention the
surface relief photopolymer layer 200 is disposed on the optical
disk 20 such that the interrogating beam 100 passes through the
layer 200 when the beam 100 interrogates the data structures 23 on
the reflective layer 22 of the optical disk 20. The surface relief
photopolymer layer 200 in this case forms the lower layer of the
optical disk 20.
[0046] One surface 201 of the photopolymer layer 200 interfaces on
an adjoining layer of the optical disk 20 and the opposite surface
202 of the photopolymer layer is a free or unconstrained surface
(see FIG. 3A). In this preferred embodiment, the surface relief
photopolymer layer 200 is deposited by appropriate methods (e.g.
spraying or spin distribution) directly against the reflective
surface 28 of the reflective layer 22 in the optical disk 20. In
alternate embodiments, the surface relief photopolymer layer may be
deposited on an % intermediate substrate between the reflective
layer of the optical disk and the photopolymer layer, such that
again the photopolymer layer has an unconstrained surface.
[0047] FIGS. 3A and 3B respectively show the surface relief
photopolymer layer 200 in an initial or undeformed condition,
before exposure to the interrogating beam 100, and then in a
deformed condition after exposure to the interrogating beam 100
(FIG. 3B may not be drawn to scale). The surface relief
photopolymer layer 200 is exposed to the interrogating beam 100
when the optical disk 20 is scanned by the optical scanning head 30
(see also FIG. 2).
[0048] As shown in FIG. 3A, when the optical disk is first scanned
and the surface relief layer 200 is in an undeformed condition, the
interrogating beam 100 is focussed to penetrate through the surface
relief layer 200 and be reflected as a reflected beam 102 from the
surface of the pits 27. Thus, the disk may be read in the normal
manner as previously described. However, exposure of the
surface-relief photopolymer layer 200 to the interrogating beam 100
also causes a deformation 210 in the unrestrained surface 202' of
the photopolymer layer 200, as shown in FIG. 3B. The outwardly
protruding deformation 210 in the photopolymer layer 200 changes an
amount of polymer material through which the beam must travel and,
due at least to the fact that this additional material has an index
of refraction that differs from air, the interrogating beam 100
experiences beam aberration, resulting in a defocusing of the
interrogating beam. This defocusing is sufficient to cause a change
in the amount of reflected light that is received by the
photodetector 34, and to thus cause at least a portion of the disk
to be read incorrectly, which is the desired result. As such,
errors are generated in subsequent attempts to read the optical
disk.
[0049] It has been observed that surface relief deformations,
created optically or by the evaporative mechanism of this
invention, of but a few hundred nanometers can be sufficient to
cause an optical disk to become unreadable, or to significantly
diminish readout fidelity due to induced readout beam tracking
problems. More particularly, the interrogating beam 100 generated
by the light source 32 of the scanning head 30 (see FIG. 2) is
focussed to penetrate through the undeformed surface relief
photopolymer layer 200 and form a spot size of less than, for
example, 1 .mu.m at the surface of the pits 27. The highly focussed
interrogating beam 100 creates a large optical intensity gradient
of approximately 10.sup.9 mW/cm.sup.3. The unconstrained surface
202 of the surface relief photopolymer layer 200 undergoes surface
relief modulation in response to optical intensity variations in
the Mw/cm.sup.2 range over micron scale lengths (i.e. an optical
intensity gradient of around 10 Mw/cm.sup.3). Thus, when-subjected
to the high intensity gradient generated by the interrogating beam
100 focussed at the surface of the pits 27, the unconstrained
surface of the surface relief photopolymer layer 200 undergoes
large surface deformations 210 (see FIG. 3B). When the surface
relief deformation 210 in the surface 202' grows to some threshold
size, it causes an aberration of the interrogating beam 100 which
is thus no longer focused at the surface of the pits 27 with
sufficient acuity to be reflected as a reflected beam 102
detectable by the photodetector 34 (see FIG. 2). This results in
readout failure. The exposure time for the unrestrained surface 202
to form a surface deformation of the desired size to cause
aberration of the interrogating beam is dependent on the polymer
blend and viscosity of the of the surface relief layer 200. The
polymer blend and viscosity of the photopolymer in the layer 200
may be selected such that surface relief deformations 210 of the
desired size are formed immediately after but not during
application of the interrogating beam 100 when reading the disk 20
for the first time. This in effect results in the disk being
rendered unreadable after the disk is read one time. Alternatively,
the polymer blend and viscosity of the surface relief layer 200 may
be selected to form the surface relief deformation of desired size
after a predetermined number of applications of the interrogating
beam, which consequently renders the disk unreadable after the disk
has been read the predetermined number of times. In this regard the
readout procedure can be modified so as to repetitively scan the
interrogating beam over the same portion(s) of the disk surface,
thereby insuring that the surface relief polymer will be
affected.
[0050] In accordance with this embodiment of the invention, a
method for rendering the optical disk 20 unreadable by a play
process includes the steps of: a) providing the optical disk 20
with a surface relief photopolymer layer 200 which undergoes
surface deformation at an unconstrained surface in the presence of
an optical intensity gradient, as can be generated by the
interrogating beam 100; and b) irradiating the surface relief
photopolymer layer with the interrogating beam 100 for inducing at
least one surface relief deformation in the unconstrained surface
of the photopolymer layer. The surface relief deformation thus
induced during the play process causes an aberration in the
interrogating beam, which prevents focussing of the interrogating
beam at desired locations on the features of the data structures 23
during subsequent readout processes. This results in a failure to
readout the data on the disk during a subsequent readout
process.
[0051] FIG. 8 is an enlarged cross-sectional view of a portion of
an optically readable media 20 having a surface topography that is
modified from a planar profile, and which can be used to
detrimentally affect the tracking operation of the readout device
in accordance with the teachings of this invention. In this
embodiment the planar surface topography is modified to the
non-planar surface topography (not shown to scale in FIG. 8) by the
use of a photoresponsive polymer as described above, or through one
of the evaporative techniques described below, or by providing a
surface layer that interacts with a substance in the atmosphere,
such as oxygen, water vapor, or carbon dioxide. In these cases it
is not necessary to modify the transparency of the surface layer to
the readout beam, such as by increasing its radiation absorbing
properties through a color change. Instead, the varying surface
topography, and its deviation from the expected planar surface
layer topography, is sufficient to detrimentally affect the
tracking operation of the readout device.
[0052] Referring now to FIGS. 4A and 4B, there is shown an enlarged
cross-sectional view of Section A' of the optical disk 20' in
accordance with a second embodiment of the present invention. The
optical disk 20' in the second embodiment of the invention is
substantially similar to the optical disk 20 described previously
with reference to FIG. 2, except as otherwise noted below. As seen
in FIGS. 4A and 4B, in this second embodiment the optical disk 20'
includes an oxygen (O.sub.2) loaded photosensitizer layer 300. The
photosensitizer layer 300 is disposed on the optical disk 20' such
that the interrogating beam 100 passes through the photosensitizer
layer 300 when the optical disk 20' is being scanned by the optical
scanning head 30 (see FIG. 2). The photosensitizer layer 300 may be
separated from the reflective layer 22' of the optical disk 20' by
a diffusion barrier 302. The lower surface 304 of the
photosensitizer layer 300 may be sealed from the environment by
some means, such an impervious polymer layer.
[0053] When the optical disk. 20' is scanned with the optical
scanning head 30, the interrogating beam 100 generated by the light
source 32 passes through both the photosensitizer layer 300 and the
diffusion barrier 302 and is focussed at the surface of the pits
27' in the reflective layer 22' of the optical disk.
Correspondingly, the focussed interrogating beam 100 is then
reflected from the reflective aluminum surface of the pits 27' as a
reflected beam 102 detectable by the photodetector 34 in the
scanning head 30 as mentioned previously (see FIG. 2). Irradiation
of the photosensitizer layer 300 with the interrogating beam 100
generates singlet oxygen (.sup.1O.sub.2) in the oxygen (O.sub.2)
loaded photosensitizer layer 300. The highly reactive singlet
oxygen (.sup.1O.sub.2) generated in the photosensitizer layer 300
diffuses through the diffusion barrier to the reflective surface of
the optical disk and reacts with the metal in the reflective
surface so as to oxidize the reflective surface. Oxidation of the
reflective surface, at least in the pits 27' of the optical disk,
degrades its reflectivity such that when the interrogating beam 100
strikes the oxidized surface the reflection of the interrogating
beam is diminished. The decrease in reflectivity may be interpreted
as the presence of a land 25, and not a pit 27, thereby resulting
in a readout failure, which is the desired result.
[0054] More specifically, and by way of example, the
photosensitizer layer 300 contains one or more photosensitizer
compounds in combination with one or more solvents, such as for
example methanol, acetone, a 10% freon/ethanol mixture, or a 1%
freon/ethanol mixture. The solvent provides a source of molecular
oxygen (O.sub.2) internal to the photosensitizer layer 300.
[0055] Referring to FIG. 6, and in accordance with the present
invention, a combination of the photosensitizer compound (PS) plus
electromagnetic radiation (i.e. light) having a wavelength of about
650 nm activates the photosensitizer, wherein the activated
photosensitizer may be indicated as PS.sub.*. The activated
photosensitizer then combines with non-atmospheric molecular oxygen
(O.sub.2) to produce singlet oxygen (.sup.1O.sub.2). In this
embodiment of the invention, this reaction occurs within the
photosensitizer layer 300 upon application of the interrogating
laser beam 100, as when scanning the optical disk 20'. Hence, in
the region of the photosensitizer layer 300 through which the
interrogating beam passes, the photosensitizer compound becomes
activated and combines with molecular oxygen (O.sub.2) provided
from the solvent which is internal to the layer 300 to produce the
singlet oxygen (.sup.1O.sub.2). After generation in the
photosensitizer layer 300, the singlet oxygen (.sup.1O.sub.2)
proceeds to diffuse through the diffusion barrier 302 towards the
reflective surface of one or more of the pits 27'. The singlet
oxygen (.sup.1O.sub.2) reaches the reflective surface and begins to
chemically attack the metal after a delay time T.sub.D. The delay
time T.sub.D is sufficient to allow the interrogating beam 100 to
be reflected as reflected beam 102 by the surface of the pit 27',
and hence allow readout of the data encoded therein before the
singlet oxygen (.sup.1O.sub.2) attacks the pit surface. Thus, the
diffusion barrier 302 can be employed to delay oxidation of the
reflective surface 28' of the optical disk until readout of the
disk has been completed at least once.
[0056] The delay time T.sub.D for the singlet oxygen
(.sup.1O.sub.2) to diffuse through the diffusion barrier 302
depends on the thickness h of the diffusion barrier 302 and the
diffusivity D of the diffusion barrier to singlet oxygen
(.sup.1O.sub.2). The relation between the diffusion delay time
T.sub.D the thickness h and diffusivity of the barrier 302 is
generally described by the equation: 1 T D = h 2 D ( 1 )
[0057] The diffusion barrier 302 comprises an appropriate medium
which does not quench singlet oxygen (.sup.1O.sub.2) and has a
controlled diffusivity D. For example, the diffusivity D of the
diffusion barrier 302 may vary in a range from about 10.sub.-5 to
10.sub.-9 cm.sub.2/sec depending on the material selected for the
barrier 302. Therefore, the delay time T.sub.D may be controlled to
be greater than the time required to read the data encoded on the
reflective layer 22' of the disk 20' by selecting a material with
the appropriate diffusivity D and selecting an appropriate
thickness h for the diffusion barrier 302. However, the delay time
T.sub.D is constrained by the lifetime (T.sub.1) of singlet oxygen
(.sup.1O.sub.2). The lifetime T.sub.D of singlet oxygen
(.sup.1O.sub.2) is a function of the hydrophobic and paramagnetic
properties of the host. Examples of general lifetimes T.sub.1 for
singlet oxygen (.sup.1O.sub.2) for different solvents are given
below:
1 T.sub.1 (.mu.sec) Solvent 7 methanol 45 acetone 150 freon/ethanol
(10%) 1400 freon/ethanol (1%)
[0058] Thus the diffusion barrier 302 separating the
photosensitizer layer 300 from the reflective layer 22 of the
optical disk is suitably sized to provide a delay time T.sub.D for
singlet oxygen diffusion which is both greater than the readout
time (T.sub.read) and less than the lifetime T.sub.1 of singlet
oxygen (.sup.1O.sub.2) (i.e. T.sub.1>T.sub.D>T.s-
ub.read)
[0059] Two suitable materials for the diffusion barrier 302 are
polyurethane or Teflon.TM., while suitable materials for the
photosensitizer layer 300 include a pthalocyanine doped polymer,
such as polycarbonate or PMMA, or a polymer doped with a porphyrin
derivative, or other high triplet yield dye. Other suitable
materials could be used as well, and these specifically listed
materials should not be read in a limiting sense upon the practice
of this invention.
[0060] Referring now to FIGS. 5A and 5B, there is shown an enlarged
cross-sectional view of Section A" of the optical disk 20" in
accordance with a third embodiment of this invention. The optical
disk 20" in this embodiment of the invention is substantially
similar to the optical disk 20 described previously with reference
to FIG. 2, except as otherwise noted below. As seen in FIGS. 5A and
5B, the optical disk 20" in accordance with this embodiment
includes a substrate 400 which may be formed from a polycarbonate
material disposed generally against the reflective surface 28" of
the reflective layer 22" in the optical disk. Included between the
substrate 400 and the reflective surface 28" of the disk 20" are
regions or pockets 402A, 402B of an uncured photopolymer 402. As
shown in FIG. 5A, the photopolymer 402 is disposed within the pits
27" formed in the reflective layer 22" of the optical disk 20". In
an uncured state, the index of refraction of the photopolymer 402
is such that the interrogating beam 100 generated by the light
source 32 (see FIG. 2) passes through both the substrate 400 and
the uncured photopolymer 402, and the interrogating beam 100 is
focussed at the surface of the pits 27". The uncured photopolymer
402 is adapted to cure after illumination by light having a
suitable wavelength, for example about 650 nm, though the
photopolymer may be adapted to cure when irradiated with light
having other wavelengths. Thus, illumination by the interrogating
beam 100 from the optical scanning head 30 (e.g., laser light
having a wavelength of about 650 nm) cures the photopolymer 402
after a given time period (i.e., causes cross-linking between the
molecules of the photopolymer, resulting in a change of viscosity
and a general solidification of the photopolymer).
[0061] After the photopolymer cures, the index of refraction of the
photopolymer 402 changes such that the interrogating beam 100
directed at the pits 27" and passing through the cured photopolymer
402' (as shown in FIG. 5B) is no longer focussed at the surface of
the pits 27". That is, the curing of the photopolymer material
results in beam aberration, and a loss of focus within the pit 27".
Therefore, in accordance with this embodiment of the invention,
illuminating the uncured photopolymer 402 in the pits 27" of the
optical disk 20", as when reading the disk for the first time or
during multiple passes after the initial reading, cures the
photopolymer. After being cured the photopolymer 402', such as that
disposed in the pits 27", defocuses the interrogating beam 100 such
that it is no longer reflected as reflected beam 102 detectable by
the photodetector 34. This in turn causes a readout failure, which
is the desired result.
[0062] The uncured photopolymer 402 preferably has a curing time
which allows unencumbered first-time readout (i.e. the
interrogating beam 100 is reflected by a pit 27" as the reflected
beam 102 that is detectable by the photodetector 34 before the
photopolymer cures) but prevents subsequent readout of the pit
27".
[0063] Suitable photocurable polymers, such as acrylic resins,
include wavelength sensitized resins, such as those used generally
in photolithography or in some rapid prototyping applications with,
for example, argon or krypton excitation lasers. General reference
with regard to photopolymers may be had to the inventor's U.S. Pat.
No.: 5,028,109, issued Jul. 2, 1991, entitled "Methods for
Fabricating Frequency Doubling Polymeric Waveguides Having
Optimally Efficient Periodic Modulation Zone and Polymeric
Waveguides Fabricated Thereby".
[0064] Reference may also be had in the literature to other
suitable photoresponsive polymers, such as those mentioned in U.S.
Pat. No. 4,865,942, "Photohardenable Compositions Containing a
Dye-Borate Complex and Photosensitive Materials Employing the
Same", by Gottschalk et al.
[0065] The foregoing three embodiments of this invention render an
optical disk 20, 20', 20" unreadable, or limit its viability to
perhaps no more than four hours after first reading (i.e. playing)
the optical disk with the optical scanning system 1. Furthermore
the three embodiments of the present invention accomplish this
without rendering the optical disk 20, 20', 20" susceptible to
becoming unreadable prematurely from competing optical conditions
such as, for example, sunlight or indoor lighting.
[0066] Typical indoor lighting will generally not adversely affect
the viability of the optical disk 20, 20', 20" in the three
preferred embodiments of the present invention. However, should the
possible exposure to sunlight be of concern, then a narrow band
filter material (not shown) may be deposited on the lower surface
26 of the disk to prevent sunlight activation of the polymeric
medium(s) of choice.
[0067] It should be understood that the above description is merely
illustrative of the invention. For example, the step of directing
the interrogating beam may be performed by directing the beam at
the optical disk for a continuous period of time sufficient to
cause the reaction in the photopolymer layer 200, 402 or
photosensitizer layer 300. Alternatively, the interrogating beam
may be directed at the disk in discrete time periods which
cumulatively trigger the reaction. Furthermore, the interrogating
beam may be directed in discrete time periods during a single scan
of the disk or over a multiple number of scans of the disk.
[0068] A fourth embodiment of this invention will now be described.
This fourth embodiment has the object of providing a method for
disrupting an optical signal such as that used in the reading of a
DVD or CD by evaporation of a substance. This embodiment is thus
also useful in the construction of optical disks that become
unreadable after a period of time.
[0069] This method provides a means of generating color, which is
capable of absorbing an interrogating light beam, by evaporation of
a substance.
[0070] By way of introduction, it is known that certain substances
become colored or change color upon changes in solvent or
environment. An example is the class of lactone dyes that are used
in carbonless copy papers. The colorless lactone form of the dye
can be caused to "open" to the colored cationic form of the dye by
absorption onto an acidic clay or other acidic substrate, by
lowering of the pH of the lactone in solution, or by changing the
polarity of the solvent in which the lactone is dissolved. The
colorless lactone form and the colored cationic form of an
exemplary lactone dye, crystal violet lactone, is shown in FIG.
7.
[0071] Polymers derived from phenol and formaldehyde have been
shown to be effective in causing the opening of a lactone dye (see
U.S. Pat. No. 4,578,690), presumably due to the acidic nature of
the phenolic component. A test was performed using
poly-p-(hydroxystyrene) obtained from Hoechst-Celenese (Mw=6300) to
determine if this polymer would also cause crystal violet lactone
to open and become colored. A solution of the polymer in THF was
mixed with a small amount of crystal violet lactone and this
solution was spotted on a glass plate and air dried. Upon drying a
dark blue spot formed. It was observed that the polymer-lactone
solution remained colorless until the mixture was dried, whereupon
the intense color of the cationic form of the dye formed.
[0072] This mechanism forms the basis of this embodiment of the
invention, that is, of using a mixture of solvents, one relatively
volatile and a second one which is relatively non-volatile, to
prepare the polymer-lactone solution. Upon drying of the solution,
the less volatile solvent remains upon evaporation of the more
volatile solvent, and the mixture remains colorless until the less
volatile solvent evaporates over a period of time. Mixtures of
poly-p-(hydroxystyrene) (PHS), ethanol (as the more volatile
solvent), crystal violet lactone (CVL) and several less volatile
solvents (LVS) were prepared. Drops of the mixtures were allowed to
air dry at room temperature and the color of the remaining films
were noted to see what effect the less volatile solvent had upon
color generation.
[0073] Preparation of the solutions:
2 PHS ethanol CVL LVS color Solution #1 500 mg 2.0 mL 20 mg 300
.mu.L NMP -- Solution #2 500 mg 2.0 mL 20 mg 300 .mu.L TEGDME +
Solution #3 500 mg 2.0 mL 20 mg 300 .mu.L BA ++ Solution #4 500 mg
2.0 mL 20 mg 300 .mu.L THN +++ * denotes no color, +++ denotes
intense color formation
[0074]
3 Solvent Name BP .degree. C. Z value NMP N-methyl pyrrolidinone
202 65 TEGDME triethyleneglycol dimethyl ether 216 60 BA benzyl
alcohol 205 75 THN tetrahydronaphthalene 207 55 * The Z value is a
measure of relative polarity. The values listed above are
estimations.
[0075] From the above experiment, NMP was chosen as the best of the
less volatile solvents tested since the polymer film remained
colorless upon evaporation of the ethanol.
EXAMPLE #1
[0076] A solution of poly-p-(hydroxystyrene) (5 gm), ethanol (10
mL), crystal violet lactone (200 mg) and NMP (3.0 mL) was prepared.
A few drops were applied to a glass slide and the mixture was
allowed to air dry at room temperature. The film which formed was
soft and tacky to the touch but it was colorless. Color formation
was followed over the course of several days through the use of a
spectrophotometer.
4 Time (hours) Optical Density (607 nm) 0 0 18 0.181 85 0.242
[0077] Since the film formed in example #1 was soft and tacky
formaldehyde was added to cross link the phenolic polymer.
EXAMPLE #2
[0078] A solution of poly-p-(hydroxystyrene) (5 gm), ethanol (10
mL), crystal violet lactone (220 mg), 28% ammonia (0.5 mL as a
cross linking catalyst) and NMP (3.0 mL) was prepared. To this
solution was added 37% aqueous formaldehyde (3.0 mL). A few drops
were applied to a glass slide and the mixture was cured at about
65.degree. C. on a hot plate until the film was hard. This took
about 5 minutes. The film which formed was hard to the touch and it
was colorless after curing. Color formation was followed over the
course of several days through the use of a spectrophotometer.
5 Time (hours) Optical Density (607 nm) 1 0 24 0.270 50 0.315
EXAMPLE #3
[0079] To test the color stability of the system on storage, a film
was prepared as described in example #1. The air dried glass slide
was sealed in a polyethylene zip-lock bag along with one drop of
NMP to form a NMP saturated environment in the bag. The slide
stored in this manner showed no color formation after one week at
room temperature. Upon removal from the bag, color began to form as
in examples 1 and 2. The slide was dark blue with an optical
density of 0.875 at 605 nm after five days in the air at room
temperature.
[0080] The scattering of light rather than absorbance can also be
used to attenuate an optical signal. An evaporative method to cause
increased scattering can be achieved by mixing a polymer with a
solid where there is a mismatch between the refractive indexes of
the two materials, and then adding a solvent for the polymer which
adjusts the refractive index of the polymer-solvent mixture to
match that of the solid. Under these conditions the mixture is
non-scattering or poorly scattering since there is a refractive
index match between the polymer-solvent pair and the solid.
However, slow evaporation of the solvent causes a mismatch between
the remaining polymer and solid and, therefore, the scattering
increases.
EXAMPLE #4
[0081] A solution of 1.0 gm of cellulose acetate butyrate (CAB,
Mw=70,000, 13.5% acetyl, 37.5% butyryl, n=1.46) in 20 mL of ethyl
acetate was prepared and to this solution, was added 1.0 gm of
silica gel (70-230 mesh, n about 1.50) and 600 .mu.L of benzyl
alcohol (n about 1.54). A drop of this mixture was placed on a
glass slide and the ethyl acetate was allowed to evaporate to
provide a clear, transparent film through which news print could
easily be read. Upon standing in the air for two days the film
became quite cloudy and news print could be read through the film
only with difficulty.
[0082] In accordance with the teachings of this invention, one or
both of the foregoing evaporative-based methods can be used to
render an optically readable media, such as a DVD or CD, unreadable
after a period of time. Referring by example to FIG. 2, the upper
protective layer 24 could be comprised of one of the mixtures
described in examples 1 and 2 above, which is initially colorless
and transparent, but which becomes colored and absorbing after
sufficient solvent evaporation has occurred. The upper protective
layer 24 could also be comprised of the CAB-ethyl acetate solution
referred to in example 4, which is initially colorless and
transparent, but which becomes milky and scattering after
sufficient solvent evaporation has occurred. While it may be
preferred to have this layer exposed as a top-most layer, it is
also within the scope of the invention to apply an overlayer, so
long as the overlayer is sufficiently permeable to enable the
evaporative process to occur.
[0083] It can be appreciated that this embodiment of the invention
also does not require the presence of atmospheric oxygen, as the
evaporation could take place as well in a vacuum, and neither does
it require the presence of a lightbeam to catalyze or initiate the
process, as the color change or increase in opacity and scattering
can occur as well in a dark enclosure, so long as the evaporative
process is not significantly impeded.
[0084] Other methods for attenuation of an optical signal can also
be employed to practice this invention.
[0085] For example, it is well known that salts of a weak acid and
a weak base in which either the acid or base or both are volatile
will revert to the free acid and free base upon standing in the
open due to the volatilization of one of the components. An example
of this is the solid ammonium carbonate, which slowly sublimes in
the open due to the formation of the volatile components of the
salt, ammonia and carbon dioxide. This property may be used to
generate color and thus optical absorption in several ways. For
example, the salt of a volatile amine and a non-volatile acid
component (carboxylic acid, phenol, etc.) may be mixed with a
lactone dye, such as crystal violet lactone, or with an pH
indicator dye. Volatilization of the basic (amine) component will
leave the acidic component behind. The acidic component may be used
to catalyze the opening of the lactone dye, or cause the color
change in a pH indicator.
[0086] The volatilization of a gas can also be used to generate a
color. For example, a water damp polymer film containing a pH
indicator dye may be stored in an atmosphere of a gas whose water
solution is acidic. (e.g. carbon dioxide, sulfur dioxide) or basic
(ammonia, trimethylamine etc.) Upon removal of the film from the
atmosphere the volatile gas will evaporate from the water damp
film, and the pH will change causing a color change in the pH
indicator dye. This type of mechanism has been used to detect
carbon dioxide and amines (see Mills, et al. Anal. Chem 1992, 64,
1383, Lakowicz et al., Biotechnol. Prog. 1998, 14, 326, and U.S.
Pat. Nos. 5,183,763 and 5,846,836.)
[0087] The increase in absorbance or light scatter (or both) can be
accomplished by coating a chemically reactive layer, exemplified by
the various examples given above, on the surface of a disk, using
methods such as a spin coating, spraying, slot coating, or vacuum
deposition. Patterned deposition can be done by a printing process,
such as silk screen or inkjet, or with masks using spray or vacuum
coating. Alternately, the reactive layer may be prepared separately
as an adherent plastic film, cut to size, and applied to the
surface of the disk.
[0088] Furthermore, the timed readout disablement can occur by
increasing scattering from the interrogating laser beam, thereby
degrading the overall signal-to-noise ratio (SNR) level to an
unacceptable level. This approach is less sensitive to changes in
laser power, error correction codes, or improved detector
design.
[0089] Further by example, the vacuum deposition of thin layers of
sensitive inorganic materials, such as KBr or CsF, on the surface
of the disk can provide a surface haze when exposed to an
atmospheric substance, such as water vapor and/or carbon dioxide,
thereby increasing at least one of the photoabsorption, the
scattering, or the surface roughness, and thereby also decreasing
the SNR.
[0090] Further by example, the evaporation of a volatile solvent
from a polymer coating may lead to the precipitation of small
scattering crystals, or the evaporation could lead to a phase
change of a polymer or polymer mixture with concomitant light
scattering.
[0091] Also, and as was discussed previously, the timed readout
disablement can also occur by lowering the reflectivity of the
reflective metal coated surface(s) of the disk. This method is
sensitive to the same factors noted above for the absorbance
increase. It should be noted that the corrosion of the buried
reflective layer is essentially irreversible.
[0092] The adhesive layer in both CDs and DVDs can be modified to
exploit the corrosive effects of air on metals. Since a goal of the
instant invention is to provide short-lived disks, the use of
different materials is an option, compatible with
manufacturability. The composition of adhesive and plastic can be
tailored to promote a corrosive reaction, once the disk packaging
is removed. Also, the reflective layer itself can be made using
metals more reactive than aluminum, such as potassium or
calcium.
[0093] This invention can be practiced by providing an optically
encoded medium with two or more of the foregoing embodiments. For
example, an optical disk can be constructed so as provide the
surface deformation feature as well as the aluminum layer oxidation
feature, or the evaporatively-driven absorption and/or scattering
change in combination with the reflective metal oxidation, thereby
further ensuring the effective destruction of the disk after being
initially read.
[0094] Thus, various alternatives and modifications may be devised
by those skilled in the art without departing from this invention.
Accordingly, the present invention is intended to embrace all such
alternatives, modifications and variances which fall within the
appended claims.
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