Patent Application
20060286337
The present invention relates to digital media and more particularly, this invention relates to digital media manufactured using ion beam technology.
Optical media presently include compact discs (CDs), digital video discs (DVDs), laser discs, and specialty items. Optical media has found great success as a medium for storing music, video and data due to its durability, long life, and low cost.
A CD typically comprises an underlayer of clear polycarbonate plastic. During manufacturing, the polycarbonate is injection molded against a master having protrusions (or pits) in a defined pattern that creates an impression of microscopic bumps arranged as a single, continuous, spiral track of data on the polycarbonate. Then, a thin, reflective aluminum layer is sputtered onto the disc, covering the bumps. Next a thin acrylic layer is sprayed over the aluminum to protect it. A label is then printed onto the acrylic.
During playback, the reader's laser beam passes through the polycarbonate layer, reflects off the aluminum layer and hits an opto-electronic device that detects changes in light. The bumps reflect light differently than the lands, and an opto-electronic sensor detects that change in reflectivity. The electronics in the reader interpret the changes in reflectivity in order to read the bits that make up the data.
The data stored on the CD is retrieved by a CD player that focuses a laser on the track of bumps. The laser beam passes through the polycarbonate layer, reflects off the aluminum layer and hits an opto-electronic device that detects changes in light. The bumps reflect light differently than the lands, and the opto-electronic sensor detects that change in reflectivity. The electronics in the drive interpret the changes in reflectivity in order to read the bits that make up the bytes.
A DVD is very similar to a CD, and is created and read in generally the same way (save for multilayer DVDs, as described below). However, a standard DVD holds about seven times more data than a CD.
Single-sided, single-layer DVDs can store about seven times more data than CDs. A large part of this increase comes from the pits and tracks being smaller on DVDs. Table 1 illustrates a comparison of CD and DVD specifications.
To increase the storage capacity even more, a DVD can have up to four layers, two on each side. The laser that reads the disc can actually focus on the second layer through the first layer. Table 2 lists the capacities of different forms of DVDs.
A DVD is composed of several layers of plastic, totaling about 1.2 millimeters thick.
A DVD player functions similarly to the CD player described above. However, in a DVD player, the laser can focus either on the semi-transparent reflective material behind the closest layer, or, in the case of a double-layer disc, through this layer and onto the reflective material behind the inner layer. The laser beam passes through the polycarbonate layer, bounces off the reflective layer behind it and hits an opto-electronic device, which detects changes in light.
One problem with each of these technologies is that it is very expensive and time consuming to create the master. Another problem is that if the master is not perfectly formed, none of the discs created from it will work properly. Further, as shown in
Another problem is that the ends 306 of the bumps 302 of the master are also rounded, as shown in
CDs and DVDs also come in the form of recordable discs. CD-recordable discs (CD-Rs) and DVD-recordable discs (DVD±Rs), do not have any bumps or flat areas (pits or lands). Instead, as shown on the cross section of a recordable disc 400 in
In place of the CD-R and DVD-R disc's dye-based recording layer, CD-RW and DVD+RW use a crystalline compound made up of a mix of silver, indium, antimony and tellurium. When this combination of materials is heated to one temperature and cooled it becomes an optically transmissive crystalline, but if it is heated to a higher temperature, when it cools down again it becomes amorphous and thus optically opaque. The crystalline areas allow the reflective layer to reflect the laser better while the non-crystalline portion absorbs the laser beam, so it is not reflected.
In order to achieve these effects in the recording layer, the disc recorder use three different laser powers: the highest laser power, which is called “Write Power”, creates a non-crystalline (absorptive) state on the recording layer; the middle power, also known as “Erase Power”, melts the recording layer and converts it to a transmissive crystalline state; and the lowest power, which is “Read Power”, does not alter the state of the recording layer, so it can be used for reading the data.
During writing, a focused “Write Power” laser beam selectively heats areas of the phase-change material above the melting temperature (500-700° C.), so all the atoms in this area can move rapidly in the liquid state. Then, if cooled sufficiently quickly, the random liquid state is “frozen-in” and the so-called amorphous state is obtained. The amorphous version of the material becomes opaque where the laser dot was written, resulting in a recognizable CD or DVD surface. When an “Erase Power” laser beam heats the phase-change layer to below the melting temperature but above the crystallization temperature (200° C.) for a sufficient time (at least longer than the minimum crystallization time), the atoms revert back to an optically tramsmissive ordered state (i.e., the crystalline state). Writing takes place in a single pass of the focused laser beam; this is sometimes referred to as “direct overwriting” and the process can be repeated several thousand times per disc.
One problem with recordable optical media is that burning takes a long time, making replication of discs by this method very inefficient. For example, it takes over 2 minutes to burn a 640 MB CD-R at 48× normal read speed. It takes 14-16 minutes to burn a single side, single layer DVD±R. These times do not include the other processing time, such as the time it takes to open the drive door, load the disc, close the door, initiate the drive, then after burning open the door, remove the disc, etc.
Another problem with recordable media is that the writing laser inherently produces dye spots with rounded edges. As mentioned above, rounded edges create jitter.
What is therefore needed is a way to improve the write speed for optical media.
What is also needed is a way to create a clean edge between reflective and nonreflective lands and pits so that the reflected laser is better controlled.
What is further needed is a way to write media in a way that the surface features have enhanced edge characteristics.
To overcome the aforementioned drawbacks and provide the desirable advantages, an optical medium includes an underlayer and a reflective layer, where at least one of the underlayer and the surface layer has surface features thereon representing data, the surface features having been formed by directing pulses of a beam of ions from an ion source onto at least one of the underlayer and the reflective layer in a controlled pattern for creating the surface features.
If the optical medium is a disc, the pattern preferably has a generally spiral shape. In one embodiment, the medium comprises a substantially transparent underlayer and a reflective layer, the ion pulses modifying the reflective layer. In another embodiment, the medium comprises an underlayer and a reflective layer, the ion pulses creating pits in the underlayer, the reflective layer preferably being added after the surface features are created. In a further embodiment, the medium comprises a reflective layer, and a dye underlayer being substantially transparent in an unexposed state, the ion pulses creating darkened portions (surface features) on the dye layer. In a still further embodiment, the medium comprises a reflective layer, and a dye underlayer being substantially nontransparent in an unexposed state, the ion pulses creating substantially transparent portions on the dye layer. In yet another embodiment, the surface features are created on at least two layers of the optical medium, as in a double layer DVD.
A system for performing this method, according to one embodiment, includes a medium receiving portion for holding an optical medium, an ion source such as an ion gun for emitting a beam of ions at the optical medium on the medium receiving portion, and a steering mechanism for directing the ion beam onto the optical medium in a controlled manner. The beam of ions strikes the optical medium in intermittent pulses for creating surface features on the optical medium, the surface features representing data.
The system described herein can write data such as audio data, video data, software, etc. to an optical medium very quickly, e.g., in less than one minute, and even in less than one second. The system is able to write data to any type of optical media, including those readable by consumer-grade CD and DVD players. Suitable optical media include any type of commercially available medium, including CD, DVD, laser disc, recordable discs (e.g., CD-R, CD-RW, DVD+R, DVD-R, DVD+RW, DVD-RW), or any type of medium from which data is read optically.
By controlling the power and width of the pulses, the system can create surface features readable by current optical media readers as well as proprietary readers. In any of these methods, the surface features can be made significantly smaller than has heretofore been possible, even using commercially available media. This is due to the fine detail (e.g., ˜5 nanometer) and sharp edges afforded by ion beam technology. For instance, the surface features can have a length along a data track thereof of less than about 500 nanometers, less than about 200 nanometers, less than about 100 nanometers, and less than about 50 nanometers. In this way, the data storable on a single medium can be greatly improved, limited only by the wavelength of the optical system used. For finer surface features, for example, ultraviolet, microwave and x-ray optical systems may be required.
The beam can be directed in the controlled pattern via magnetic fields generated by steering coils. In one embodiment, the pulses are generated by controlling a grid voltage of the ion source. In another embodiment, the pulses are generated by beam blanking.
Other aspects and advantages of the present invention will become apparent from the following detailed description, which, when taken in conjunction with the drawings, illustrate by way of example the principles of the invention.
For a fuller understanding of the nature and advantages of the present invention, as well as the preferred mode of use, reference should be made to the following detailed description read in conjunction with the accompanying drawings.
The following description is the best embodiment presently contemplated for carrying out the present invention. This description is made for the purpose of illustrating the general principles of the present invention and is not meant to limit the inventive concepts claimed herein.
The system described herein can write data such as audio data, video data, software, etc. to an optical medium very quickly, e.g., in less than one minute, and even in less than one second. The system is able to write data to any type of optical media, including those readable by consumer-grade CD and DVD players. Suitable optical media include any type of commercially available medium, including CD, DVD, laser disc, recordable discs (e.g., CD-R, CD-RW, DVD+R, DVD-R, DVD+RW, DVD-RW), or any type of medium from which data is read optically. Of course, the technology disclosed herein would extend to future types of optical media that are presently under development or have yet to be discovered.
The system of the present invention can incorporate therein a positive ion source or a negative ion source. Illustrative ion species which perform the bombardment are Ar+, O2+, Ga+, Cs+, Li+, Na+, K+, Rb+, etc.
A preferred embodiment implements a Focused Ion Beam (FIB) system. A FIB system takes charged particles from a source, focuses them into a beam through electromagnetic/electrostatic lenses, and then scans across small areas of the target using deflection plates or scan coils. The FIB system produces high resolution imaging by collecting the secondary electron emission produced by the beam's interaction with the target surface. Contrast is formed by raised areas of the sample (hills) producing more secondary electrons than depressed areas (valleys).
In a preferred embodiment, the FIB system uses gallium ions from a field emission liquid metal ion (FE-LMI) source. In operation, a gallium (Ga+) primary ion beam hits the sample surface and sputters a small amount of material, the displaced material leaving the surface as either secondary ions (i+ or i−) or neutral atoms (n0). The primary ion beam also produces secondary electrons (e−). As the primary beam rasters on the sample surface, the signal from the sputtered ions or secondary electrons is collected to form an image.
At low primary beam currents, very little material is sputtered; modern FIB systems can achieve 5 nm imaging resolution. At higher primary currents, a great deal of material can be removed by sputtering, allowing precision milling of the specimen down to a sub-micron scale. One test by the inventors on commercial media resulted in a 40 mm image resolution.
Many variables and material properties affect the sputtering rate of a sample. These include beam current, sample density, sample atomic mass, and incoming ion mass. A preferred ion species is Ga+.
Additionally, gas-assisted etching can be used. When a gas is introduced near the surface of the sample during milling, the sputtering yield can increase depending on the chemistry between the gas and the sample. For instance, by injecting a reactive gas into the mill process, the aspect ratio of the ion beam's cutting depth can be dramatically altered such that it is possible to reach the lower metallization line without disturbing the upper layer metallization. This results in less redeposition and more efficient milling. Two typical gasses are iodine and xenon difluoride.
If the sample is non-conductive, a low energy electron flood gun can be used to provide charge neutralization. In this manner, by imaging with positive secondary ions using the positive primary ion beam, even highly insulating samples may be imaged and milled without a conducting surface coating, as would be required in a SEM. This feature is particularly useful for writing surface features directly to the polymeric layer of an optical medium.
Suitable ion guns include the ILG-2, IGPS-2, E/IMG-16, E/IGPS-16, available from Kimball Physics, 311 Kimball Hill Road, Wilton, N.H. 03086-9742 USA. Another suitable ion gun is the IOG 25 Gallium Liquid Metal Ion Gun, available from Ionoptika Ltd, Epsilon House, Chilworth Science Park, Southampton, Hampshire SO16 7NS, UK. One skilled in the art will recognize that there are several manufacturers of ion guns that are also suitable for use with the system, including those having larger and smaller spot sizes.
The steering mechanism can use rastering technology to aim the ion beam at the optical medium along the data path. One preferred steering mechanism includes steering coils or deflection plates under control of the controller. Steering coils are copper windings that create magnetic fields that affect the direction of the ion beam. One set of coils creates a magnetic field that moves the ion beam in the X direction, while another set moves the beam in the Y direction. The deflection plate assembly consists of two pairs (X and Y) of deflection plates located near the beam-exit end of the gun. Potentials applied to these plates produce a deflecting force in a plane perpendicular to the direction of beam travel. By controlling the voltages in the coils or plates, the ion beam can be positioned at any point on the medium. Because rastering can be performed very quickly, a full data track can be transferred to the optical medium in a fraction of a second.
The raster pattern can be generated by a computer using a standard X-Y grid corresponding to points on the medium. The grid has a density sufficient to allow writing to all necessary points on the medium. The steering mechanism, in turn, directs the ion beam to the points on the medium corresponding to data points on the grid, where a pulse is emitted. A simple raster controller in this type of system can be similar to the controller used in cathode ray tubes (CRTs).
Alternatively, the raster pattern can be set to follow a data track, such as a spiral. The steering coils are energized in such a way that the ion beam moves along the data track, the ion beam pulsing at selected points along the data track. In this type of system, for example, the field emitted by the steering coils in the X and Y directions can follow generally sinusoidal curves where the amplitudes of the curves gradually increase as the beam moves from the inner diameter of the media to its periphery along a spiral data track.
As mentioned above, the surface features are created by ion beam pulses. In most ion guns, including those available from Kimball Physics, the ion beam may be turned off and on while the gun is running. The way this is accomplished depends on the particular gun design. Often several beam pulsing methods are available for a particular gun.
Pulsing includes stopping and starting the flow of ions in a fast cycle. This pulsing is usually accomplished by rapidly switching the grid voltage to its cut off potential to stop the beam. The grid provides the first control over the beam and usually can be used to shut off the beam. In an ion gun, if the grid voltage is sufficiently negative with respect to the cathode, it will suppress the emission of the ions, first from the edge of the cathode and at higher (more negative) voltages from the entire cathode surface. The minimum voltage required to completely shut off the flow of ions to the target is called the grid cut off. The grid voltage can be controlled by the controller manipulating the power supply; thus, in most guns, the beam can be turned off while the gun is running by setting the grid to the cut off voltage.
The grid voltage can be controlled by several different methods, one being capacitive. Many guns can be equipped with a capacitor-containing device (either a separate pulse junction box or cylinder, or a cable with a box) that receives a signal from an external pulse generator (available from the gun manufacturer). The grid power supply and pulse generator outputs are superimposed to produce the voltage at the grid aperture. The general pattern of the beam pulsing is a square wave with a variable width (time off and time on) and a variable repetition rate. Capacitive pulsing can provide the fastest rise/fall time and shortest pulse length of the various methods. However, the capacitor does not permit long pulses or DC operation. If there is a separate grid lead on the gun, this capacitive pulsing option can be added to most existing gun systems without modification.
A typical pulse length is ˜20-100 nanoseconds, defined as the time the beam is on, measured as the width at 50% of full beam and may include some ringing. The rise/fall time is typically 10 nanoseconds measured between 10% and 90% of full beam. Shortening the rise/fall will typically increase ringing. Pulsing performance may also depend on the performance of the user-supplied pulse generator.
Not all guns are designed to be pulsed. For example, a few ion guns have a positive grid in order to extract more ions, and so these guns do not usually have grid cut off, unless a dual grid supply is ordered. In some high-current ion guns, the optical design, the position of the cathode, does not allow for cut-off with the grid, and so a different option, called blanking, must be used to interrupt the beam instead of pulsing.
Beam blanking deflects the ion beam to one side of the ion gun tube to interrupt the flow of ions to the target without actually turning off the beam. The voltage applied to the blanker plate in the gun is controlled by a potentiometer on the power supply. Blanking can be used to pulse the final beam current repeatedly on and off in response to a TTL signal input. The blanker voltage required for beam cutoff depends on the gun configuration and on the beam energy, and can be readily determined from the reference materials accompanying the ion gun from the manufacturer.
As mentioned above, the system 500 can write data to commercially available media, recordable media, and specialty media. How the system 500 writes data to commercially available media such as CDs and DVDs will be discussed first.
As mentioned above, a CD and DVD typically comprises a clear polycarbonate plastic underlayer, a thin, reflective aluminum layer sputtered onto the polycarbonate, and a thin protective layer, e.g., acrylic, lacquer, etc. sprayed over the aluminum to protect it. In this method 600, the target disc as loaded into the system comprises polycarbonate, a reflective layer, and acrylic backing. The acrylic backing faces the ion gun. In operation 604, data is selected for addition to the disc and loaded into the controller. In operation 606, under control of the controller, a beam of ions from the ion gun is directed onto the disc for creating surface features on the disc. The ion beam is caused to pulse intermittently in a controlled manner to create the surface features along the data track, the surface features representing data in a data track. The resulting data track is a spiral pattern starting from the inner diameter of the disc. The power of the ion beam is set such that it will pierce the backing layer and create optically discernable features on the reflective layer so that the reader will only detect reflections from the nonexposed parts of the reflective layer, thereby creating surface features along the data track. For a CD, the data points are about 0.5 microns (500 nanometers) wide, and a minimum of 0.83 (830 nanometers) microns long. The track spacing is about 6 microns (6000 nanometers). In a DVD, the damaged sections of the reflective layer that make up the data track are each about 320 nanometers wide and a minimum of 400 nanometers long. The track spacing is about 740 nanometers.
In operation 608, the disc is ejected from the system. In operation 610, a label is then printed onto the acrylic using a printing device known in the art, or affixed as an adhesive layer. In this way, the damaged area of the disc is covered and is nonapparent to the end user. The side of the label adjacent the disc is preferably nonreflective so as not to reflect the reader's laser during playback. Also note that a protective layer can optionally be added prior to affixing the label.
Again, the ion beam is pulsed in a controlled manner to create the surface features along the data track. For a CD, the pits are about 0.5 microns (500 nanometers) wide, and a minimum of 0.83 (830 nanometers) microns long. The track spacing is about 6 microns (6000 nanometers). In a DVD, the pits are each about 320 nanometers wide, a minimum of 400 nanometers long. The track spacing is about 740 nanometers.
In operation 708, a reflective layer is sputtered onto the disc. In operation 710, the disc is ejected from the system. In operation 712, a label is then printed onto the acrylic using a printing device known in the art, or affixed as an adhesive layer.
In operation 810, data is selected for addition to the inner readable layer of the disc and loaded into the controller. In operation 812, under control of the controller, intermittent pulses of a beam of ions from the ion gun are directed onto the reflective layer for creating surface features on the disc, the surface features representing data in a data track that is readable as the inner data track. Then additional steps, such as adding an acrylic backing and label can be performed.
This method 800 has the advantage that the disc does not move, and the ion gun does not move. Thus, the inner and outer readable layers are inherently aligned perfectly every time.
The process can be repeated to create two additional data layers which can be coupled to the first and second polycarbonate discs, thereby creating a dual side, double layer DVD. The process can even be used to make media having more than two readable layers on each side, e.g., 3, 4, 5, 6 layers per side.
Likewise, the method of 700, where the transparent layers are modified by the ion beam, can be adapted to create multi-level optical media, as will be apparent to one skilled in the art. In this situation, the transparent layer of the outer readable layer is first written to, and a semi-transparent layer is sputtered onto it. A second transparent layer (inner readable layer) is coupled to the semi-transparent layer and data written thereto. A reflective layer is then sputtered onto the second transparent layer followed by labeling or addition of other layers.
This method can also be used to write to rewritable discs, e.g., CD-RW and DVD±RW. In that case, the power of the ion beam is set to heat areas of the phase-change material above the melting temperature (500-700° C.), so all the atoms in this area can move rapidly in the liquid state. Then, if cooled sufficiently quickly, the random liquid state is “frozen-in” and the so-called amorphous state is obtained. The amorphous version of the material is opaque, creating an equivalent to a “pit” where the data point was written by the ion beam, resulting in a recognizable CD or DVD surface.
One skilled in the art will appreciate that the various operations of the methods described above can be combined to create additional methods for writing data to optical media, such additional method being considered within the scope of the present invention. One skilled in the art will also appreciate that the methods can be adapted with software instructions to write to types of media other than disc shaped media.
In any of these methods, the surface features can be made significantly smaller than has heretofore been possible, even using commercially available media. This is due to the fine detail (e.g., ˜5 nanometer) and sharp edges afforded by ion beam technology. For instance, the surface features can have a length along a data track thereof of less than about 500 nanometers, less than about 200 nanometers, less than about 100 nanometers, and less than about 50 nanometers. In this way, the data storable on a single medium can be greatly improved, limited only by the wavelength of the optical system used. For discs having surface features finer than a DVD, a reader capable of reading finer-than-DVD features is used. For even finer surface features, for example, ultraviolet, microwave and x-ray optical systems may be required.
Also note that the surface features created can have almost perfectly straight edges.
In another variation, the electron beam can be used to create “pits and lands” of varying reflectivity on a surface having nanofeatures that affect the reflectivity of light. The shapes and number of the nanofeatures determine the amount of reflectivity (if any) of the surface. Thus, a separate reflective layer is not needed. Those skilled in the art will appreciate that the shape and size of the nanofeatures can vary, and will be able to select a shape and size without undue experimentation.
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.
This application is a continuation-in-part of copending U.S. patent application Ser. No. 10/934,234 filed Sep. 3, 2004 under the title “Fabrication of Digital Media using Ion Beam Technology” to the same inventors as the present application.
| Number | Date | Country | |
|---|---|---|---|
| Parent | 10934234 | Sep 2004 | US |
| Child | 10955025 | Sep 2004 | US |
