The present invention relates to a method, device and storage medium for optical data storage.
There exist a number of optical storage techniques. One example of a technique is based on changing reflectivity of a storage layer when “writing” thereto. Systems based on this technique have an advantageous property in respect of that the collection efficiency of the objective lens, for a single-layer, always is 100% due to the fact that an outgoing light as a reflection of a coherent incoming light, also is coherent, which means that the light path for the incoming and outgoing light is reversible. However, this storage technique is typically not suitable for multi-layer recording in a stacked storage device because of ghost images, coherent cross talk as a result of coherent light, and poor transmission for each layer for both incident laser light and signal light. Yet another drawback is that a difference in index of refraction of written and non-written memory cells causes an optical beam to scatter as it transverses the different layers, resulting in a decreased beam quality.
Other techniques may involve the usage of fluorescent materials such as dyes etc. One is to use a fluorescent dye that is dissolved in a polymer matrix. In this case the index of refraction can be tuned to that of the substrates to avoid problems with scattering of the optical beams. Furthermore, the multi-layer storage mediums can be chosen such that they are transparent at the fluorescent signals wavelengths, effectively eliminating half the losses and disturbances associated with standard reflective technologies. By means of using fluorescent dyes, there are several possibilities to obtain a storage device. Irreversible storage of data such as Write Once Read Many (WORM) data storage is possible by photo bleaching of fluorescent material in a polymer matrix. The material is heated directly upon irradiation with a writing laser beam. Alternatively, quencher molecules are initially deposited in a layer above a layer containing the fluorescent material, comprising so-called “fluorophores”. When the material is heated by the laser beam the quencher molecules decompose and form radicals, which can diffuse to the fluorophores when the temperature exceeds a prior adjusted transition temperature of the polymer matrix, such as a glass transition temperature, and the melting and/or decomposition temperature of the quencher molecules. The chemical structure of the fluorophores, and hence the fluorescence spectrum and fluorescence efficiency is changed after the radicals have reacted with the fluorophores. The fluorescent signal emitted by reacted fluorophores is significantly different from the signal emitted by unreacted fluorophores upon irradiation with a “reading beam”. This feature is then used for reading stored data. However, this concept suffers from the disadvantage of a low data rate during writing due to slow diffusion of the radicals. Furthermore, the contrast obtained is poor because only a part of the illuminated dyes will be photo bleached resulting in a low data rate.
Another technique based on fluorescence is to co-dissolve the quencher molecules with the fluorophores in the polymer matrix. In this way, the radicals, which are formed upon heating, do not have to diffuse into the layer containing the fluorophores, but can directly react with them. This results in an increased contrast and thus an increased data rate; however, a drawback is that the stability of the non-written memory cells is significantly decreased.
As far as storage techniques that utilize fluorescence goes, the light path of the emitted light is not the reverse of the incident laser light path, hence the reversibility of the incident and emitted light path is not true. The optical characteristics of the emitted photons, such as their energy and phase, using such a technique are not the same as the optical characteristics of the incident photons. While this in fact has many advantages (see below) one disadvantage is that the light being emitted is emitted under a larger solid angle than that defined by the NA (numeric aperture) used by the incident light. Therefore a significant amount of signal intensity is lost during signal collection of emitted light. By simple geometrical considerations it can be shown that the collection efficiency for isotropic light emission ≈(NA/2n)2, where NA is the numerical aperture for the incident light and n the refractive index of the substrate being used. For a NA of 0.6 and a refractive index of 1.62 of a polycarbonate substrate at a certain wavelength, this results in a collection efficiency of only 3.6%.
Moreover, from the patent application WO 02/47090, A1, is known a data storage method and device including materials that have three-dimensional optical storage capabilities, where said materials comprise a polymer matrix and nematic liquid crystal droplets as well as photosensitive material dispersed through the matrix. Storage of data is performed by illuminating zones of data storage material by coherent polarized infra-red light, whereby directors of illuminated material are aligned, causing alignment of photosensitive material. Reading of stored optical data comprises illumination of data storage material which has optical data stored therein, causing photosensitive material of zones of aligned directors of nematic liquid crystal droplets to emit fluorescence at a greater intensity compared to zones of non-aligned directors, and detecting fluorescence within the zones of aligned detectors.
This device and method of writing and reading has the property of being relatively complex and is therefore likely to become expensive for data storage applications. Another property of such a device and such a method is a relatively long switching time, of the order of 100 ms, which thus disables high data rates.
There is still a problem how to achieve a higher collection efficiency for light emission, leading to increased detected signal strength and data rate, in combination with a high writing speed, a good sensitivity during writing and a high stability of written and non-written storage areas.
Furthermore, problems including scattering, concerning stacking of storage layers to obtain large capacity have to be solved.
It is an object of the invention to provide a significant amount of anisotropic emission when reading data stored in a storage medium.
The invention also provides optical storage of data with a good sensitivity during writing and reading of said data.
According to an aspect of the invention, it has now been found that an especially beneficial form of optical data storage is provided by (re)orientation of aligned anisotropic molecules initiated by a very short light pulse, which aligned anisotropic molecules thereafter self-develop during a time period which is typically longer than the time period for the light pulse. Typically, this light is laser light. Preferably, the variation of orientation (or molecular order) is achieved by means of irradiation of light, especially by means of a laser beam. Generally, the method is performed in such a manner that the optical information is stored by means of a laser beam through a local reorientation or disorientation of molecular segments.
According to another aspect of the invention, there is provided a device for optical data storage using polymer material as storage medium, whereby the device comprises a film at least partly made of a polymer material in order to store data by means of local variation of the molecular order, or orientation, of a polymer comprising photo-orientable groups.
According to a preferred embodiment of the invention, there is provided a method for writing data in a storage medium comprising polymer material by modifying its optical properties, said method comprising the steps of:
heating up the material above the glass-transition temperature (Tg),
performing alignment of the material, and
initiating the writing by reorientation of photo-orientable-groups in the polymer material by means of illuminating with light at a wavelength and for a time period, or by other means, that initiates the reorientation, enabling anisotropic emission during reading of stored data.
According to another embodiment of the invention, there is provided a device for optical data storage, comprising:
polymer material as storage medium,
means for heating up the material above the glass-transition temperature (Tg),
means for performing alignment of said material, and
means for initiating the writing by orientation of photo-orientable units of the polymer by illuminating with light at a wavelength and for a time period, or by other means, that initiates the reorientation, whereby data can be stored in the device comprising polymer material by modifying its optical properties, enabling anisotropic emission during reading of stored data.
According to yet another embodiment of the invention, there is provided a storage medium comprising polymer material, adapted to store data by modifying its optical properties, said polymer material comprising photo-orientable groups, which can be reoriented upon illumination with light at a wave-length and for a time period that initiates the reorientation, which can self-develop at a suitable temperature, typically above the glass transition temperature (Tg).
According to still yet another embodiment of the present invention, there is provided a method to read data stored in an optical data storage device, that comprises polymer material as storage medium, means for heating up the material above the glass-transition temperature (Tg), means for performing alignment of the material, means for initiating the writing by reorientation of photo-orientable units of the polymer and dipole emitters that can be aligned, said method comprising the steps of:
illuminating with light at a wavelength, that causes the anisotropic fluorescent dipole emitters to emit light and,
collecting the anisotropic emission from said dipole emitters.
Besides the invention provides optical storing of data at high speed and provides high stability of stored information. Herein, the term “high speed” means not significantly slower than within nano-seconds, such as within 10-50 ns. Initiating writing is performed during a time period that is significantly shorter than a time scale on which the polymer, such as an LC polymer, reorients.
These and other aspects of the invention will be apparent from the embodiments(s) described hereinafter.
The present invention will also be more clearly understood from the following description of the preferred embodiments of the invention read in conjunction with the attached drawings, in which:
The invention will now be described starting with reference to
The different properties that are required to store information are combined in the multi-functional polymer as illustrated in
It is also possible to use a polymer with less than three functional groups if different functionalities are combined in one group, e.g. a fluorescent moiety and a mesogenic group can be combined in a fluorescent liquid crystalline group. Other combinations are also possible. For instance, the function of the third group R3 incorporated in the photo-orientable group, R2.
Preferably, the polymer is provided with groups that provide the high stability of anisotropic polymers for data storage, but at the same time avoid problems with slow switching. The storage is based on a photo-induced change in suitable molecular groups, which can be provided into the main chain of the polymer or in side-groups.
The polymer described in
The first group R1 inducing liquid crystallinity can be provided in an essentially known manner, as for instance described in “Handbook of Liquid Crystal Research”, Peter J. Collings, Jay S. Patel (Eds.), Oxford University Press, New York, 1997, which will therefore not be described in more detail. As an example, the first group R1 comprises repetitive units, including spacer units, and groups providing liquid crystal character such as mesogenic groups. The liquid crystalline units are typically provided in side-groups, but may also be present in the backbone of the polymer 10, or in both.
The second group R2 comprises photosensitive units, that are capable to isomerize. The photosensitive units are typically provided in side-groups, but may also be present in the backbone of the polymer 10, or in both. Usually these photosensitive groups are based on one or more of the general formula
R—PH
where PH is a photosensitive group, preferably selected from the group comprising azobenzene, biazobenzene, triazobenzene and azoxybenzene, as well as alkyl substituted derivatives of the same, stilbene or spiropyran groups, and where R stands for a group which enables the chemical bonding of the photochemical unit into the polymer 10, typically a group that is capable of polymerization or polycondensation. For instance azo-benzene groups are rewritable. Upon irradiation with light of an appropriate wavelength, azo-benzene units will undergo a reversible cis-trans isomerization around the nitrogen-nitrogen double bond. In this process, there is a driving force for the azo-benzene units to decrease the absorption cross section and orient their absorption dipole moment along the propagation direction of the light.
It is also possible to use other groups than those that can form cis-trans isomers, which reversibly can change molecular order by irradiation with light, of which particular examples will not be discussed herein, since they are obvious for a person skilled in the art. It is also possible to provide irreversible writing by means of for instance cinnamate groups. Such a group undergoes upon irradiation with light of suitable wavelength a photo-addition reaction, which results in an orientation perpendicular to an E-vector of the light. Since this reaction is not reversible, the writing can be considered as an example of WORM-type of writing.
Presently, there is a great demand for WORM optical data storage disks, so-called “CD-R” and this demand is expected to increase which the increase of the storage capacity of the optical data disks. When using a WORM medium for content distribution, the writing process could be serial (data bits are written one after the other); however, it is economically not interesting to incorporate serial writing processes in the manufacturing process of cheap optical data storage media. Data replication during manufacturing is typically only worth-while when it can be done in a parallel writing process, e.g. via a stamper or a mould. This is one of the essential advantages of optical storage over other storage options such as hard disk and solid state memories. Therefore, in a ROM medium, it is preferred to use some type of parallel writing, even if this is not disclosed herein.
In
The change of absorption cross section is also valid for the second group R2 and in some cases, depending on the group, also for the first group R1. The variation of molecular geometry and the induced local non-equilibrium states causes variations in the optical properties such as refractive index, double refraction or absorption properties, of which the latter will be described herein when a device for storing data and the storing principle thereof are further described below.
The order of the functional groups of
In
The polymer layer 42 is covered with a separation layer 43, optionally coated on the interface between 42 and 43 with an alignment layer as described above, whereby this combination, i.e. the polymer layer 42, the separation layer 43, optionally including said alignment layer can be stacked several times, in this particular embodiment illustrating three polymer layers. However, multiple polymer layers 42, typically more than ten can be provided. Alternatively, the polymer can be provided as laminate with other suitable materials, or as a coating on a matrix layer, even if these examples are not illustrated in this figure.
When writing into one polymer layer, a first laser beam from a light source (illustrated by an arrow labeled “light”) is focused on a certain area in the data storage medium, whereby the polymer in this area reorients due to the photo-orientable groups, which will be further disclosed below. The first laser beam, for instance having blue light, initiates the reorientation, whereby a second beam (from the same source) of an intensity high enough to heat the polymer above its glass-transition temperature Tg, completes the reorientation. The resulting written area can then be read as optical data.
The optical data storage device 40 can for instance be in the form of an optical disk, whereby data, typically in the form of bits, are read into circular tracks by means of a probing laser beam when this disk rotates in an optical record player or an optical card. Another possibility could be to provide holographic storage, whereby a hologram of an image is recorded as an interference pattern. These, and other applications will not be described in more detail, since such technologies are well known within this technical field. Now,
In short, it is this reorientation of the aligned area 52 that enables en increased collection efficiency of emitted light, during the reading process, as will become more clear in the following paragraphs down below.
The initial orientation of the multi-functional polymers in
It is also possible to combine an alignment inducing layer and an alignment field. The alignment inducing layer could for instance force a homeotropic alignment of the functional groups in the polymer. The aligning force of the alignment inducing layer can be overruled by the force of an alignment field during deposition of the data layer. In this way a planar alignment is obtained. Now, during the writing process, the force exerted by the photo-orientable units and the force of the alignment inducing layer will co-operate to cause a reorientation of all functional groups. In this way, the writing speed can be enhanced. In the normal case where the alignment inducing layer causes planar alignment, the forces exerted by the alignment inducing layer and the photo-orientable units oppose each other during the writing process, limiting the writing speed.
The first laser beam that initiates the reorientation as illustrated in
The laser beams can for instance originate from a diode laser, typically with a wavelength of approximately 400 nm. However, there is a great flexibility in the choice of wavelengths, both for writing and reading. For instance dyes can be added to provide sensitivity at a suitable wavelength. Both the writing beam and the heating beam can according to a preferred embodiment of the invention, be combined into one beam (as illustrated in
The method for writing data according to a general preferred embodiment of the invention can be illustrated with a flow-chart as presented in
Erasing the stored information can be obtained by increasing the temperature above the glass-transition temperature Tg and cooling in an electrical or magnetic field. It can also be obtained by re-alignment to the alignment layer when above the Tg or by a reversed photo-orientation process.
The glass-transition temperature Tg typically is above ambient temperature. However, it is preferred to have control over the glass transition temperature in order to be sure that the stored data will not be degraded during storage at desired temperatures. Such methods, for instance to use vinyl based polymers, are well known and will therefore not be further described herein. The time scale on which the laser pulse has to be applied is much shorter than the time-scale on which the anisotropic molecules reorient. Thereby, high recording data rates can be combined with a high recording stability.
If the groups are aligned by means of an electrical field, transparent electrodes can be provided surrounding the polymer layers from two sides. However, the electrodes do not have to be incorporated in the device. During manufacturing it is possible to apply an electric field even when the electrodes are not incorporated in the medium. For a WORM application, typically electrodes neither are required nor desired. For a (limited) RW application it is also possible to envision only two general electrodes that sandwich all storage layers to provide a general re-orientation capability for the whole device. If electrodes sandwich every layer, a more local erasure and initial material orientation per layer is possible. In principle, even a user-drive could be made to provide the external global alignment field so that an RW medium without internal electrodes is achieved. Because of the high voltages required in this case (the voltages increase linearly with the separation of the electrodes), this might not be the most practical solution, even if it is possible.
Reading of information can be performed by, by for instance, irradiating the polymer layer or layers with monochromatic coherent light. Typically laser light is used to read data by means of using the change in orientation of anisotropic fluorescent chromophores comprised in the third group R3. These fluorescent chromophores can be constituted of any fluorescent organic or inorganic molecules with a dipole moment, preferably selected from the group of: liquid crystal systems, organic dyes, nanotubes, nanowires and polymers with substitutents containing any molecules selected from the above mentioned group. Also other groups than those mentioned may however be used, instead or in combination.
The different orientation of the transition dipole moments of the fluorescent chromophores in “written” and “non-written” areas causes a contrast in absorption and thus in fluorescence. The contrast can typically be about 1:7. Of course, also other anisotropic groups that change orientation can be employed, for instance the photo-orientable group. Also other types of groups than anisotropic, which change optical properties when illuminated with light from an intense writing beam, and which properties can be read by a reading beam, having an intensity lower than that of the writing beam, may be possible, provided that the initiation is fast enough. It is also possible to provide the optical properties in a blend, rather than in the polymer itself, or to use additives.
In addition, the third group R3 comprising the anisotropic fluorescent chromophores are typically aligned as explained above. With reference to
The inventive concept of this invention titled optimized medium with anisotropic dipole emission for fluorescent single or multi layer storage, has several advantageous over prior art.
These advantages are the following: increased fluorescent signal intensity through anisotropic emission (realistically a factor two in photons), increased absorption cross section (enabling thinner layers for a given, optimal absorption), increased stability of stored information, fast writing speed made possible, and independent optimization of material properties made possible.
Since also the invention provides a small difference in the index of refraction of written and non-written bits, this will result in reduction of beam quality as the light transverses the different layers, even if it is small compared to conventional techniques. In a stacked device having many polymer layers, say above ten, the differences between written and non-written bits can be further reduced by careful choice of materials, i.e. typically by selecting a fourth compensating group. Alternatively, this difference could instead be increased to be used by sensing this as an optical parameter, for instance by means of a differential phase contrast microscope set-up in transmission.
Even if only reading by means of using fluorescence is described in the examples, any other method capable of sensing optical parameters dependent on molecular orientation can be employed.
The device for optical data storage can also be used e.g. for optical signal processing, Fourier transform, and other recording purposes than described.
As used in the following claims, the word “comprise” means including, but not necessarily limited to.
Number | Date | Country | Kind |
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02077425.3 | Jun 2002 | EP | regional |
03100621.6 | Mar 2003 | EP | regional |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/IB03/02870 | 6/13/2003 | WO | 12/14/2004 |