Optical information reproduction device, optical information reproduction method, and information recording medium

An optical information reproduction device includes a light source (14) configured to emit reproduction light, a plasmon resonance element (9) including a resonance section (22) arranged adjacent to a recording region (4) of a recording layer (2), the resonance section (22) causing plasmon resonance between the recording region (4) and the resonance section (22), a photodetector (17a) configured to detect reflected light or transmitted light from the plasmon resonance element (9) on which the reproduction light is irradiated, and a reproduction unit (24) configured to determine, on the basis of a detection signal from the photodetector (17a), whether the recording region (4) is in a recorded state or an unrecorded state, and reproduce information recorded in the recording region (4).

TECHNICAL FIELD

The present invention relates to an optical information reproduction device and an optical information reproduction method for optically reproducing information recorded on an information recording medium, and also relates to an information recording medium including at least a substrate and a recording layer.

BACKGROUND ART

As an optical information reproduction device, an optical memory system has been put to practical use in which an optical disk such as a CD (compact disc), a DVD, or a BD (Blu-Ray disc), an optical card, or the like is used as an information recording medium.

A reproduction principle of a conventional optical memory system is shown inFIG. 10in a simplified form.FIG. 10is an explanatory diagram showing a part of the configuration of a conventional optical information recording and reproduction device and a state in which information is reproduced from an information recording medium.

In the conventional optical information recording and reproduction device, reproduction light107from a light source (not shown in the figure) is condensed by an objective lens110. The reproduction light107is irradiated, as irradiation light105, on a recording mark104, which is a recording region in which information is recorded, of a recording film102formed on a substrate101of an information recording medium103. Reflected lights106and108from the recording mark104are detected, whereby the information is reproduced from the information recording medium103. For example, if reflectance is set to be low if the recording mark104is in a recorded state and is set to be high if the recording mark104is an unrecorded state, the optical information recording and reproduction device can determine whether the recording mark104is in the recorded state or the unrecorded state and can reproduce optical information of the information recording medium103by detecting light amounts of the reflected lights106and108.

However, in the optical memory system in the past, there is a problem in that the size (recording mark length) of a recording mark that can be reproduced is limited by an optical limit size called diffraction limit determined by an NA (numerical aperture) of the objective lens and the wavelength of reproduction light and a further increase in density is difficult.

In recent years, in order to eliminate the diffraction limit, an optical memory is proposed in which near-field light, a spot diameter of which can be set smaller than the diffraction limit, is used. Patent Literature 1 describes an optical recording and reproduction device in which a near-field light probe made of a microstructure of metal is used.

In the optical recording and reproduction device described in Patent Literature 1, a recording layer of a phase-change recording medium is subjected to phase change from crystal to amorphous by near-field light generated by the near-field light probe, whereby a recording mark is formed and recording is performed. The near-field light is irradiated on the phase-change recording medium on which the recording mark is formed and reproduction is performed by detecting a change in the intensity of scattered light returned from the phase-change recording medium. Since the near-field light is localized light exponentially attenuated as it is further apart from a generation source (light that does not propagate), in general, the near-field light cannot be extracted. However, a small fraction of the near-field light can be extracted as scattered light by bringing an object such as the recording mark close to the near-field light. Specifically, when the near-field light is irradiated on the recording mark of the phase-change recording medium, a rate of scattering of the near-field light changes according to presence or absence of the recording mark. Therefore, in the optical recording and reproduction device described in Patent Literature 1, reproduction is performed by detecting a change in the intensity of the scattered light from the recording mark.

However, as a result of examination, the inventors have found a problem in the optical recording and reproduction device described in Patent Literature 1 in that, although high-density recording can be performed by forming a recording mark having size close to the size of the near-field light (e.g., about several ten nanometers), it is difficult to satisfactorily reproduce a recording mark having the size of the near-field light.

According to the study by the inventors, besides low conversion efficiency from reproduction light (propagated light) into near-field light (in general, only about 1%), when size d of the recording mark is smaller than the diffraction limit and reduced to size of a so-called Rayleigh scattering region (with respect to wavelength λ, d≦˜λ/10, for example, when λ=405 nm, d≦˜40 nm), even if the near-field light can be condensed to size close to the size d of the recording mark and irradiated on the recording mark, a light amount of returning scattered light suddenly decreases as the size d is smaller. For example, the inventors have estimated through optical calculation that, in a recording mark having size of about 20 nm, a light amount of returning scattered light is, for example, about 0.001% with respect to a light amount of the irradiated near-field light and, with respect to a light amount of reproduction light, the light amount of the returning scattered light is only about 1% of the abovementioned value, i.e., about 0.00001% at most.

As a result, there is a problem in that a change in the intensity of scattered light detected according to presence or absence of the recording mark is, for example, smaller than 0.00001% with respect to the reproduction light amount and reproduction of information is difficult because the change in the intensity of the scattered light is too small.

CITATION LIST

Patent Literature

SUMMARY OF THE INVENTION

The present invention has been devised in order to solve the problems and it is an object of the present invention to provide an optical information reproduction device, an optical information reproduction method, and an information recording medium capable of satisfactorily reproducing information even if the size of a recording region in which the information is recorded is smaller than a diffraction limit of light.

An optical information reproduction device according to an aspect of the present invention is an optical information reproduction device that reproduces information recorded on an information recording medium including at least a substrate and a recording layer, the optical information reproduction device including: a light source configured to emit reproduction light; a plasmon resonance element including a resonance section arranged adjacent to a recording region of the recording layer, the resonance section causing plasmon resonance between the recording region and the resonance section; a photodetector configured to detect reflected light or transmitted light from the plasmon resonance element on which the reproduction light is irradiated; and a reproduction unit configured to determine, on the basis of a detection signal from the photodetector, whether the recording region is in a recorded state or an unrecorded state, and reproduce information recorded in the recording region.

With this configuration, the reproduction light emitted from the light source is irradiated on the plasmon resonance element, the reflected light or the transmitted light from the plasmon resonance element is detected, it is determined on the basis of the detection signal whether the recording region is in the recorded state or the unrecorded state, and the information recorded in the recording region is reproduced.

According to the present invention, even if the size of the recording region is smaller than the diffraction limit of light, it is possible to satisfactorily reproduce the information by making use of the fact that a plasmon resonance degree between the recording region and the resonance section of the plasmon resonance element changes according to a state of the recording region, whereby a reflected light amount or a transmitted light amount from the plasmon resonance element changes.

Since the size of the plasmon resonance element is not subjected to a spatial limitation, it is possible to form the plasmon resonance element larger than the recording region. Further, the reflected light or the transmitted light from the plasmon resonance element is detected by directly irradiating the reproduction light on the plasmon resonance element rather than near-field light. Therefore, it is possible to set the reflected light amount, the transmitted light amount, a light amount change of the reflected light amount, or a light amount change of the transmitted light amount sufficiently large. It is possible to improve a modulation degree of a reproduction signal.

Objects, characteristics, and advantages of the present invention are made apparent by the following detailed description and accompanying drawings.

DESCRIPTION OF EMBODIMENTS

Embodiments of the present invention are explained below with reference to the drawings. The embodiments explained below are embodied examples of the present invention and are not meant to limit the technical scope of the present invention.

First Embodiment

First, an optical information reproduction device, an optical information reproduction method, and an information recording medium in a first embodiment of the present invention are explained in detail with reference toFIGS. 1,2,3A, and3B.

FIG. 1is a diagram showing the configuration of an optical information reproduction device in a first embodiment of the present invention.FIG. 2is an explanatory diagram showing a plasmon resonance element of the optical information reproduction device in the first embodiment of the present invention and a state in which information is reproduced from an information recording medium.FIG. 3Ais a sectional view taken along line III-III inFIG. 2showing a state of the vicinity of the plasmon resonance element in the case in which, in the first embodiment of the present invention, a recording region of the information recording medium is in a recorded state and a plasmon resonance degree is large.FIG. 3Bis a sectional view taken along line III-III inFIG. 2showing a state of the vicinity of the plasmon resonance element in the case in which, in the first embodiment of the present invention, the recording region of the information recording medium is in an unrecorded state and the plasmon resonance degree is small.

The optical information reproduction device in the first embodiment is an optical information reproduction device that reproduces information recorded on an information recording medium3including at least a substrate1and a recording layer2. The optical information reproduction device includes a light source14configured to emit reproduction light, a plasmon resonance element9including a resonance section22arranged adjacent to a recording region4of the recording layer2, the resonance section22causing plasmon resonance between the recording region4and the resonance section22, a photodetector17aconfigured to detect reflected light6(or transmitted light) from the plasmon resonance element9on which the reproduction light is irradiated, and a reproduction unit24configured to determine, on the basis of a detection signal from the photodetector17a, whether the recording region4is in a recorded state or an unrecorded state, and reproduce information recorded in the recording region4.

An optical information reproduction method in the first embodiment is an optical information reproduction method for reproducing information from an information recording medium3including at least a substrate1and a recording layer2. The optical information reproduction method includes a step of irradiating (irradiation light5) reproduction light emitted from a light source14on a plasmon resonance element9including a resonance section22arranged adjacent to a recording region4of the recording layer2, the resonance section22causing plasmon resonance between the recording region4and the resonance section22, a step of detecting, with a photodetector17a, the reflected light6(or transmitted light) from the plasmon resonance element9on which the reproduction light is irradiated, and a step of determining, on the basis of a detection signal from the photodetector17a, whether the recording region4is in the recorded state or the unrecorded state, and reproducing information recorded in the recording region4.

The optical information reproduction device in the first embodiment is explained in detail. The optical information reproduction device shown inFIG. 1includes a plasmon resonance element9, an objective lens10, a collimator lens11, a light source14, a beam splitter15, a detection lens16, photodetectors17aand17b, an optical element for servo signal detection19, the reproduction unit24, and a driving unit25.

The light source14emits reproduction light. The plasmon resonance element9includes a resonance section22. The resonance section22causes plasmon resonance between a recording region4of a recording layer2and the resonance section22. The resonance section22is arranged adjacent to the recording region4. The photodetector17adetects reflected light from the plasmon resonance element9on which the reproduction light is irradiated. The reproduction unit24determines on the basis of a detection signal from the photodetector17awhether the recording region4is in the recorded state or the unrecorded state, and reproduces information recorded in the recording region4.

As shown inFIG. 1, the optical information reproduction device in the first embodiment includes a semiconductor laser light source as the light source14for reproduction. In an optical path from the light source14to an information recording medium3, the collimator lens11, the beam splitter15, the objective lens10, and the plasmon resonance element9are arranged. In a return optical path from the beam splitter15to the photodetectors17aand17b, the optical element for servo signal detection19and the detection lens16are arranged.

The information recording medium3includes at least a substrate1and the recording layer2. A plurality of recording regions4in which information is recorded are provided on the substrate1as the recording layer2. One recording region4is in the recorded state or the unrecorded state.

The resonance section22in a distal end region of the plasmon resonance element9is arranged adjacent to the recording region4such that a distance between the resonance section22and the recording region4is, for example, within about 100 nm, desirably, about 5 to 30 nm. The plasmon resonance element9only has to be arranged in a position where plasmon resonance with the resonance section22occurs or intensification of the plasmon resonance occurs when the recording region4is in at least one of the recorded state and the unrecorded state.

The reproduction light emitted from the light source14is irradiated on the plasmon resonance element9. In the first embodiment, laser light (emitted light of the reproduction light)12polarized linearly in a Z-axis direction (a polarization direction8c) is emitted from the light source14in a Y-axis direction. It is changed to substantially parallel light13(a polarization direction8b) by the collimator lens11and transmitted through the beam splitter15. The laser light transmitted through the beam splitter15is condensed by the objective lens10on the plasmon resonance element9as the irradiation light5centering on the vicinity of the resonance section22at the distal end and including the recording region4and the like in a region close to the resonance section22. A polarization direction8aindicates a polarization direction on an optical axis of the irradiation light5.

As explained above, the reproduction light is irradiated on the recording region4adjacent to the resonance section of the plasmon resonance element9as well. Therefore, the plasmon resonance is further intensified. Consequently, a difference in a reflected light amount between the recorded state and the unrecorded state increases and detection sensitivity is improved.

The reflected light6reflected by the plasmon resonance element9turns back in the opposite direction and passes through the objective lens10. The reflected light6passed through the objective lens10is made incident on the optical element for servo signal detection19with an optical axis thereof bent in a −Z-axis direction by the beam splitter15. The reflected light6is divided into at least two lights by the optical element for servo signal detection19and divided into two kinds of convergent lights18aand18bby the detection lens16.

The convergent light18ato be reproduction signal light is made incident on the photodetector17a. The photodetector17adetects a signal recorded in the recording region4. The reproduction unit24determines on the basis of a detection signal from the photodetector17awhether the recording region4is in the recorded state or the unrecorded state, and reproduces the information recorded in the recording region4. The convergent light18bis made incident on the other photodetector17b. The photodetector17bdetects a servo signal. The optical information reproduction device in this embodiment includes the driving unit25that integrally moves the plasmon resonance element9and the objective lens10. The driving unit25moves the plasmon resonance element9on the basis of the servo signal from the photodetector17bto thereby perform control of a very small position including, for example, a space between the plasmon resonance element9and the recording layer2.

The objective lens10is a condensing lens of a so-called off-axis type. When the substantially parallel light13, the optical axis of which is parallel to the Y-axis direction, is made incident on the objective lens10, emitted light, the optical axis of which inclines by an angle θ in the Z-axis direction from the Y axis on a YZ plane, is condensed. Since the objective lens10of the of axis type is used, there is an effect of preventing contact of the objective lens10and the information recording medium3and making it easy to condense the reproduction light in the vicinity of the resonance section22of the plasmon resonance element9from an oblique lateral direction.

The plasmon resonance element9is made of metal such as Au and has a triangular prism shape pointed at an end as shown inFIG. 2. The plasmon resonance element9is arranged to be tilted by an angle θ1with respect to a ZX plane in a state in which the resonance section22at the distal end is provided adjacent to the recording region4of the recording layer2.

Besides the triangular shape described above, the plasmon resonance element9only has to have a shape pointed at an end to allow plasmon resonance to easily occur. The overall shape of the plasmon resonance element9may be any shape.

The plasmon resonance element9desirably has a flat section. In this embodiment, θ is set nearly equal to θ1(θ≅θ1) such that the triangular flat section of the plasmon resonance element9is substantially perpendicular to the optical axis of the irradiation light5. Consequently, it is possible to reflect the irradiation light5on the flat section of the plasmon resonance element9as reflected light6in the opposite direction at substantially the same angle. This is desirable because efficiency of light utilization increases. In order to irradiate the irradiation light5, which is the reproduction light, on the flat section of the plasmon resonance element9and satisfactorily extract the reflected light6, the area of the flat section is hundred to about several thousand square nanometer or larger than several thousand square nanometers.

According to the irradiation of the irradiation light5, electrons present in the plasmon resonance element9interact with the irradiation light5, induce (surface) plasmon resonance, and cause near-field light7in the resonance section22in the distal end region according to the induction of the plasmon resonance. The inventors have found that, at this point, when the recording region4and the resonance section22close to each other interact, a condition for causing further intensified plasmon resonance is present, and the plasmon resonance is intensified, a light amount of the reflected light6from the plasmon resonance element9changes.

According to a degree of the plasmon resonance between the resonance section22of the plasmon resonance element9and the recording region4in the recorded state or the recording region4in the unrecorded state, a reflected light amount from the plasmon resonance element9changes. For example, the change in the reflected light amount from the plasmon resonance element9is larger when a degree of plasmon resonance between the resonance section22of the plasmon resonance element9and a recording region4ain the recorded state or a recording region4bin the unrecorded state is larger.

FIGS. 3A and 3Bare examples in which a degree of plasmon resonance is larger in a recording region4ain the recorded state than in a recording region4bin the unrecorded state.FIG. 3Ashows a case in which the resonance section22of the plasmon resonance element9is present on the recording region4ain the recorded state. InFIG. 3A, near-field light7ais generated between the resonance section22and the recording region4aand the plasmon resonance degree increases. As a result, a light amount of reflected light6achanges (inFIG. 3A, decreases).FIG. 3Bshows a case in which the resonance section22of the plasmon resonance element9is present on the recording region4bin the unrecorded state. InFIG. 3B, near-field light7bis generated only in the vicinity of the resonance section22and the plasmon resonance degree decreases. As a result, the light amount of reflected light6bhardly changes.

It is considered that, when the plasmon resonance between the plasmon resonance element9and the recording region4is intensified, a dielectric loss (absorption) increases in the plasmon resonance element9. As a result, the reflected light amount from the plasmon resonance element9changes. However, depending on the design of the plasmon resonance element9, when the plasmon resonance is intensified, the reflected light amount decreases in some case and increases in other cases.

A polarization state such as a polarization angle of reflected light or transmitted light from the plasmon resonance element9sometimes changes according to the plasmon resonance degree. In this case, it is possible to change the change in the polarization state to a light amount change of the reflected light or the transmitted light by combining an optical element such as an analyzer with the plasmon resonance element9. Therefore, it is possible to reproduce information in the same manner by detecting, with a photodetector, emitted light from the optical element such as the analyzer.

Even if the size of the recording region4is equal to or smaller than a diffraction limit, it is possible to change a degree of plasmon resonance according to whether the recording region4is in the recorded state or the unrecorded state. Therefore, the reflected light6is detected by the photodetector17aand it is determined on the basis of a detection signal from the photodetector17awhether the recording region4is in the recorded state or the unrecorded state, whereby the information recorded in the recording region4can be reproduced. For example, “1” (or “0”) is associated with the recorded state and “0” (or “1”) is associated with the unrecorded state. The recorded information is reproduced according to a combination of “1” and “0”.

It is known that a polarization direction of the irradiation light5is important for plasmon resonance and intensification of the plasmon resonance and the plasmon resonance more often occurs as the longitudinal direction of the plasmon resonance element9in which electrons are present and the polarization direction8aof the irradiation light5are closer to parallel. Therefore, in the arrangement shown inFIG. 1, it is desirable to set θ equal to θ1(θ=θ1). If a polarization component of the irradiation light5with respect to the longitudinal direction of the plasmon resonance element9is present as in the case of, for example, θ1=0 or θ≠θ1, the plasmon resonance occurs.

At this point, for the resonance section22to interact with the recording region4to intensify the plasmon resonance, the light source14is desirably arranged on the optical axis of the irradiation light5irradiated on the plasmon resonance element9to have a characteristic that the amplitude of a polarization component of reproduction light polarizing in the perpendicular direction (the Z-axis direction) with respect to an arrangement surface (an XY plane) of the recording layer2is larger than the amplitude of a polarization component of reproduction light polarizing in another polarization direction (the Y-axis direction). For example, the light source14is arranged such that an angle θ formed by the optical axis of laser light made incident on the objective lens10and the optical axis of laser light made incident on the plasmon resonance element9satisfies 0°≦θ<45° and reproduction light polarized linearly in the Z-axis direction is emitted in the Y-axis direction (FIG. 1).

In the first embodiment, for example, the angle θ is set in a range of 10° to 30° such that the reproduction light has a little oblique component (θ>0°). As a result, the irradiation light5can be irradiated obliquely to include the recording region4and the like in the region close to the resonance section22. This is desirable for intensification of the plasmon resonance.

In an optical path between the light source14and the objective lens10, for example, a polarization control optical element like a wave plate that converts a polarization state of the emitted light12or13emitted from the light source14may be arranged. The polarization control optical element increases the amplitude of the polarization component of the reproduction light polarizing in the perpendicular direction (the Z-axis direction) with respect to the arrangement surface (the XY plane) of the recording layer2to be larger than the amplitude of the polarization component of the reproduction light polarizing in the other polarization direction (the Y-axis direction). For example, when the polarization direction from the light source14to the emitted light12is the X-axis direction, for example, it is advisable to arrange a wave plate such as a half-wave plate in the optical path between the light source14and the objective lens10.

A part or all of the recording region4is made of a recording material. To intensify the plasmon resonance, it is desirable that the recording material of the recording region4has a metallic characteristic. Specifically, it is desirable that a sign of a real part of a dielectric constant of the recording material is negative. Further, when a real part of a relative dielectric constant of the recording material is equal to or smaller than −5, the degree of the plasmon resonance increases. Therefore, it is desirable that the real part of the relative dielectric constant of the recording material is equal to or smaller than −5. For example, taking actual metal as an example, if reproduction light is in a range of visible light, when wavelength is equal to or larger than 0.54 μm in Au, when wavelength is equal to or larger than 0.44 μm in Ag, or when wavelength is equal to or larger than 0.506 μm in Cu, the real part of the relative dielectric constant is equal to or smaller than −5 and the plasmon resonance degree is intensified in the abovementioned range. For other recording materials, a standard of a resonance degree can be determined according to a value of the real part of the relative dielectric constant.

For example, if the recording material of the recording region4shows the metallic characteristic in one of the recorded state and the unrecorded state and shows a nonmetallic characteristic in the other, a change in the reflectance of the recording material showing the metallic characteristic is larger than a change in the reflectance of the recording material showing the nonmetallic characteristic. In other words, a change in a reflected light amount of the recording material having smaller one of a real part of the dielectric constant of the recording material in the recorded state and a real part of the dielectric constant of the recording material in the unrecorded state is larger than a change in a reflected light amount of the recording material having larger one of the real parts. Therefore, a modulation degree of reproduction increases and satisfactory reproduction can be expected.

In other words, it is sufficient that a part or all of the recording region4of the recording layer2is made of the recording material and a sign of the real part of the dielectric constant of the recording material in the recorded state and a sign of the real part of the dielectric constant of the recording material in the unrecorded state are different from each other with respect to the wavelength of the reproduction light. Further, it is sufficient that one of the real part of the relative dielectric constant of the recording material in the recorded state and the real part of the dielectric constant of the recording material in the unrecorded state is equal to or smaller than −5 and the other is larger than −5 with respect to the wavelength of the reproduction light. In this case, the plasmon resonance degree of one of the recording material in the recorded state and the recording material in the unrecorded state is intensified. Therefore, there is an effect that the modulation degree of reproduction is further increases.

As the recording material, a phase-change recording material, an inorganic material such as bismuth oxide or titanium oxide, a photochromic material such as diarylethene, organic dye, or the like is known. Irrespective of which of the materials the recording material is, the modulation degree of reproduction can be increased if the abovementioned condition is satisfied in the wavelength of the reproduction light.

In the first embodiment, as a main component of the recording material, for example, a chalcogenide phase-change recording material of a GeTe—Sb2Te3system such as Ge2Sb2Te5containing GeTe and Sb2Te3at a ratio of 2:1 is used. The recorded state corresponds to crystal and the unrecorded state corresponds to amorphous. However, the recorded state may correspond to amorphous and the unrecorded state may correspond to crystal. The main component indicates a component of a material having a largest volume ratio included in the recording region4. The main component having the volume ratio equal to or higher than 50% is desirable because the modulation degree of reproduction increases.

As explained above, a part or all of the recording region4is made of the recording material. The main component of the recording material is the phase-change recording material. Each of the recorded state and the unrecorded state corresponds to one of amorphous and crystal.

In general, the phase-change recording material has a characteristic that, when crystallizing, the phase-change recording material shows the metallic characteristic in a certain wavelength region, the region of wavelength varying depending on the composition.

For example, when the recording material is Ge2Sb2Te5, which is a typical phase-change material, it is desirable that wavelength λ of reproduction light suitable for conversion of the light source14into a semiconductor laser satisfies, for example, 0.35 μm≦λ≦0.45 μm. For example, when the wavelength2of reproduction light of a bluish purple semiconductor laser is 0.41 μm, a real part of the relative dielectric constant of a crystalline recording material is −8.7 and a real part of the relative dielectric constant of an amorphous recording material is 0.57. This is desirable because the condition that the real part of the relative dielectric constant of the crystalline recording material is equal to or smaller than −5 and the real part of the relative dielectric constant of the amorphous recording material is larger than −5 is satisfied.

Similarly, when the wavelength λ of red reproduction light satisfying 0.6 μm≦λ≦0.7 μm suitable for the conversion of the light source14into a semiconductor laser is, for example, 0.65 μm, the real part of the relative dielectric constant of the crystalline recording material is −3.3 and the real part of the relative dielectric constant of the amorphous recording material is 12. Further, when the wavelength λ of infrared reproduction light satisfying 0.73 μm≦λ≦0.83 μm suitable for the conversion of the light source14into a semiconductor laser is, for example, 0.78 μm, the real part of the relative dielectric constant of the crystalline recording material is 5.9 and the real part of the relative dielectric constant of the amorphous recording material is 17.

Therefore, when the recording material is Ge2Sb2Te5, at wavelength of red light to blue light (0.35 μm≦λ≦0.7 μm), signs of the real parts of the dielectric constants are different from each other in the crystalline and amorphous recording materials. Therefore, the wavelength of the red light to the blue light is desirable. In particular, at wavelength of blue light (0.35 μm≦λ≦0.45 μm), the real part of the relative dielectric constant of the crystalline recording material is equal to or smaller than −5 and the real part of the relative dielectric constant of the amorphous recording material is larger than −5. Therefore, the wavelength of the blue light is more desirable. Ge22Sb2Te25in which a component ratio of GeTe and Sb2Te3is changed to 22:1 and recording materials formed at other composition ratios show the same tendency. Therefore, reproduction at the wavelength of the blue light is desirable.

When the recording material is Ge31Bi2Te34of a GeTe—Bi2Te3system, the real part of the relative dielectric constant of the crystalline recording material is −9.3 and the real part of the relative dielectric constant of the amorphous recording material is 3.9 with respect to the wavelength of the blue light. The real part of the relative dielectric constant of the crystalline recording material is −2.9 and the real part of the relative dielectric constant of the amorphous recording material is 14 with respect to wavelength of the red light. The real part of the relative dielectric constant of the crystalline recording material is 15 and the real part of the relative dielectric constant of the amorphous recording material is 15 with respect to the wavelength of infrared light. As in the case of Ge2Sb2Te5, in Ge31Bi2Te34as well, in the wavelength of the red light to the blue light, signs of the real parts of the dielectric constants are different from each other in the crystalline and amorphous recording materials. Therefore, the wavelength of the red light to the blue light is desirable. In particular, at the wavelength of the blue light, the real part of the relative dielectric constant of the crystalline recording material is equal to or smaller than −5 and the real part of the relative dielectric constant of the amorphous recording material is larger than −5. Therefore, it can be said that the wavelength of the blue light is more desirable. A recording material of the GeTe—Bi2Te3system in which a component ratio is changed shows the same tendency.

Other materials, i.e., materials containing any one of Te60Ge4Sn11Au25, Ag4In4Sb76Te16, GeTe, (Ge—Sn)Te, (Ge—Sn)Te—Sb2Te3, (Ge—Sn)Te—Bi2Te3, GeTe—(Sb—Bi)2Te3, (Ge—Sn)Te—(Sb—Bi)2Te3, GeTe—(Bi—In)2Te3, (Ge—Sn)Te—(Bi—In)2Te3, Sb—Ga, (Sb—Te)—Ga, Sb—Ge, (Sb—Te)—Ge, Sb—In, (Sb—Te)—In, Sb—Mn—Ge, Sb—Sn—Ge, Sb—Mn—Sn—Ge, and (Sb—Te)—Ag—In have a characteristic that, when crystallizing, the phase-change recording materials show the metallic characteristic in a certain wavelength region. Therefore, it is possible to effectively use, with attention paid to a value of the real part of the relative dielectric constant, the materials containing any one of the above components in a range of the wavelength that satisfies the desirable condition.

Au is illustrated as the material of the plasmon resonance element9. However, the material of the plasmon resonance element9is not limited to Au. Other materials that can plasmon-resonate with the recording material or can intensify the plasmon resonance may be selected according to the wavelength of reproduction light to be used.

In the wavelength from the red light to the infrared light, in general, irrespective of which metal the plasmon resonance element9is formed, the plasmon resonance is relatively easily caused simply by irradiating reproduction light. Therefore, even if the recording region4changes to one of the recorded state and the unrecorded state, a change in an intensification degree of the plasmon resonance with the recording material relatively less easily occurs. As a result, the modulation degree of reproduction tends to decrease.

However, the inventors have found that, when the wavelength λ of the reproduction light is the wavelength of blue that satisfies 0.35 μm≦λ≦0.45 μm, it is desirable for improving the modulation degree of reproduction that the plasmon resonance element9contains at least one of Au, Cu, Ti, Ni, and Ag as a main component. When the reproduction light having the wavelength of blue is simply irradiated on the materials, since the plasmon resonance degree is small, the generation of the near-field light7is small. However, it has been found that, when the sign of the real part of the dielectric constant of the recording region4is negative or when the rear part of the relative dielectric constant of the recording region4is equal to or smaller than −5, since the plasmon resonance element9and the recording region4interact and the degree of the plasmon resonance substantially increase, it is possible to improve the modulation degree of reproduction.

The substrate1of the information recording medium3desirably has high flatness of a surface on which the recording layer2is formed and high stability when the information recording medium3is rotated. As the material of the substrate1, for example, a glass substrate or a metal plate of aluminum or the like is desirable. Further, resin such as polycarbonate, PMMA (polymethylmethacrylate), norbornene resin (e.g., “ARTON” (manufactured by JSR Corporation)), or cycloolefin resin (e.g., “ZEONEX” (manufactured by Zeon Corporation)) can also be used.

The recording layer2may have a thin film shape. The recording region4may have a form of a recording mark. However, in this embodiment, as shown inFIG. 2, the recording regions4of the recording layer2have thickness h and are arrayed in an island shape. The recording regions4include particles, a part or all of which are made of the recording material. InFIG. 2, the recording region4aindicates the particle in the recorded state and the recording region4bindicates the particle in the unrecorded state. An arraying period of the particles is Λx in the X-axis direction and Λy in the Y-axis direction. One particle corresponds to a conventional recording mark and has recorded information. InFIG. 2, all the particles are regularly arrayed. However, the particles do not always need to be regularly arrayed. An arraying interval or a way of arraying may be changed according to information to be recorded. It is possible to include position information and the like of the particles by variously changing the arraying interval or the way of arraying.

In the case of a thin film shape in which the recording layer2continuously extends, when the recording region4such as a recording mark is formed in the recording material, heat diffuses in the recording material and a large recording mark exceeding a recording spot is recorded. A difference in the size of the recording mark starts to be conspicuous by such heat diffusion when the recording mark is equal to smaller than 30 nm.

Therefore, the recording regions4of the recording layer2are arrayed in an island shape and formed in particle structure having size equal to or smaller than 30 nm. Consequently, since the respective particles are separated, it is possible to satisfactorily manufacture, while avoiding the influence of heat diffusion during recording, an information recording medium including the recording region4(the particle) equal to or smaller than 30 nm.

However, when the recording material is a particle as small as about 3 nm, the number of atoms included the particle decreases and a melting point is too low. As a result, retention of recording in the recording material becomes unstable because of thermal fluctuation. Therefore, it is desirable that the size of the recording region4(the particle) is equal to or larger than 3 nm.

It is desirable in terms of an increase in the density of recording to microminiaturize the particle functioning as the recording region4as much as possible to reduce the size of the particle and provide the particles in an isolated state close to one another as much as possible. However, when the interval of the particles is too small, it is likely that the particles come into contact with one another and independency (the isolated state) of the particles cannot be secured. Therefore, it is desirable to design the interval of the particles taking this point into account.

In this embodiment, the particle functioning as the recording region4indicates a particle processed in a fine convex shape shown inFIG. 2. Besides a columnar shape shown inFIG. 2, the particle may have a shape like a cone, a polygonal pyramid such as a triangular pyramid or a square pyramid, or a polygonal prism such as a triangular prism or a square prism.

In particular, the inventors have found that, as shown inFIG. 4A, a particle having a shape pointed at an end like a cone, or a polygonal pyramid such as a triangular pyramid or a square pyramid is desirable. Moreover, as shown inFIG. 4B, a particle having a shape like a cylinder, or polygonal prism such as a triangular prism or a square prism which has a shape rounded or pointed at an end is also desirable because near-field light tends to be condensed or concentrated in a particle.

FIG. 4Ais a diagram showing an example of an information recording medium including a recording region having a conical shape.FIG. 4Bis a diagram showing an example of an information recording medium including a recording region having a semispherical rounded shape in a distal end portion of a cylinder.

InFIG. 4A, an information recording medium3aincludes the substrate1and the recording layer2. The recording layer2includes a recording region4′ having a conical shape. The recording region4′ includes a recording region4a′ in the recorded state and a recording region4b′ in the unrecorded state. A distal end portion of a particle functioning as the recording region4′ has a pointed cross section. More specifically, the particle has a conical shape.

InFIG. 4B, an information recording medium3bincludes the substrate1and the recording layer2. The recording layer2includes a recording region4″ having a semispherical rounded shape in a distal end portion of a cylinder. The recording region4″ includes a recording region4a″ in the recorded state and a recording region4b″ in the unrecorded state. A distal end portion of a particle functioning as the recording region4″ has an arcuate cross section. More specifically, the particle has a shape having a shape in which a hemisphere is formed in a distal end portion of a cylinder. The particle functioning as the recording region4″ may have a shape in which a cone is formed in a distal end portion of a cylinder or may be a shape in which a pyramid is formed in a distal end portion of a prism.

In the first embodiment, the reproduction light emitted from the light source14is irradiated on the plasmon resonance element9by the objective lens10. However, the reproduction light emitted from the light source14may be irradiated on the plasmon resonance element9by, for example, an optical waveguide or an optical fiber.

An entire portion of the recording region (the particle)4projecting from the substrate1may be formed of the recording material or only a distal end portion of the portion projecting from the substrate1may be formed of the recording material.

The information recording medium3in the first embodiment explained above is an information recording medium characterized in that the information recording medium includes at least the substrate1and the recording layer2, the recording regions4of the recording layer2are arrayed in an island shape, the recording regions4include the particles, a part or all of which are made of the recording material, and the sign of the real part of the dielectric constant of the recording material in the recorded state and the sign of the real part of the dielectric constant of the recording material in the unrecorded state are different with respect to the wavelength of the reproduction light.

The information recording medium3in the first embodiment is an information recording medium characterized in that the information recording medium includes at least the substrate1and the recording layer2, the recording regions4of the recording layer2are arrayed in an island shape, the recording regions4include the particles, a part or all of which are made of the recording material, and one of the real part of the relative dielectric constant of the recording material in the recorded state and the real part of the relative dielectric constant of the recording material in the unrecorded state is equal to or smaller than −5 and the other is larger than −5 with respect to the wavelength of the reproduction light.

In the optical recording and reproduction device in the first embodiment, the plasmon resonance element9is made of, for example, Au. The area of the flat section is 2500 nm2. The reproduction wavelength λ is 0.405 μm. The recording region4is the particle made of Ge2Sb2Te5. The diameter of the particle is 20 nm. The thickness h of the recording layer2is 100 nm. The space between the resonance section22and the recording region4is 15 nm. When the recording region4is crystalline, the reflectance is 1.00%. When the recording region4is amorphous, the reflectance is 1.44%. An amount of a change in the reflectance is 0.44% and a modulation degree of reproduction is 31%. The satisfactory values are respectively obtained. The modulation degree of reproduction can be calculated by dividing the amount of the change in the reflectance by the larger reflectance of the reflectance of the crystalline recording region4and the reflectance of the amorphous recording region4(=0.44/1.44).

Since the size of the plasmon resonance element9is not subjected to a spatial limitation, it is possible to form the plasmon resonance element9larger than the recording region such as the recording mark. The optical recording and reproduction device according to the first embodiment directly irradiates the reproduction light on the plasmon resonance element9rather than near-field light and detects reflected light from the plasmon resonance element9. Therefore, it is possible to set a reflected light amount or a light amount change sufficiently large.

Second Embodiment

An information recording medium in a second embodiment of the present invention is explained next.FIG. 5is a sectional view showing the configuration of an information recording medium3cin the second embodiment of the present invention. The information recording medium3cis different from the information recording medium3in the first embodiment in that a protective layer23, of which dielectric constant has a real part with a positive sign, is formed in an upper layer of the recording region4of the recording layer2formed on the substrate1. In other words, the information recording medium3cfurther includes, in the upper layer of the recording region4, the protective layer23of which dielectric constant has a real part with a positive sign and which is used for protecting the recording region4. Since the protective layer23is provided, it is possible to improve resistance to environment of the particle functioning as the recording region4formed of the recording material. It is possible to reduce damage to the recording region4due to contact of the distal end of the plasmon resonance element9with the resonance section22. Further, since the sign of the real part of the dielectric constant of the protective layer23is positive, it is possible to prevent unnecessary plasmon resonance from occurring between the protective layer23and the resonance section22. As a result, it is possible to prevent deterioration in the modulation degree of reproduction due to an adverse effect from the protective layer23.

As the protective layer23, one or a plurality of nitrides selected out of C—N, Ti—N, Zr—N, Nb—N, Ta—N, Si—N, Ge—N, Cr—N, Al—N, Ge—Si—N, Ge—Cr—N, and the like can also be used. Further, as the protective layer23, a sulfide such as ZnS, a carbonate such as SiC, or a fluoride such as LaF3, CeF3, or MgF2can also be used. The protective layer23may be formed using a mixture of one or a plurality of materials selected out of the abovementioned materials. Further, the protective layer23may be formed of an organic material such as resin. In this case, it is possible to further reduce impact during collision than impact in the case of the inorganic material. The protective layer23may be formed of a mixed material of the organic material and the inorganic material.

The surface of the protective layer23is formed optically flat, whereby unevenness of the surface is eliminated. Therefore, it is possible to reduce contact with the plasmon resonance element9due to the unevenness of the surface.

Third Embodiment

An optical information reproduction device in a third embodiment of the present invention is explained centering on differences from the optical information reproduction device in the first embodiment with reference toFIGS. 6,7,8A, and8B.

FIG. 6is a diagram showing the configuration of the optical information reproduction device in the third embodiment of the present invention.FIG. 7is an explanatory diagram showing a plasmon resonance element of the optical information reproduction device in the third embodiment of the present invention and a state in which information is reproduced from an information recording medium.FIG. 8Ais a sectional view taken along line VIII-VIII inFIG. 7showing a state of the vicinity of the plasmon resonance element in the case in which, in the third embodiment of the present invention, a recording region of the information recording medium is in a recorded state and a plasmon resonance degree is large.FIG. 8Bis a sectional view taken along line VIII-VIII inFIG. 7showing a state of the vicinity of the plasmon resonance element in the case in which, in the third embodiment of the present invention, the recording region of the information recording medium is in an unrecorded state and the plasmon resonance degree is small.

The optical information reproduction device in the third embodiment is different from the optical information reproduction device in the first embodiment in the shape of a plasmon resonance element9′ and the shape of an objective lens10′. Further, the optical information reproduction device in the third embodiment includes a radially-polarized light generating element20and a mirror21in an optical path between the beam splitter15and the objective lens10′ in an optical path between the light source14and the plasmon resonance element9′.

The plasmon resonance element9′ is a conical prism in which the surface other than the bottom surface is coated with a metal film. The conical prism includes a resonance section22′ in the vicinity of the vertex. The objective lens10′ is a normal inline lens in which the optical axis of incident light and the optical axis of emitted light coincide with each other.

The radially-polarized light generating element20is arranged in the optical path between the light source14and the plasmon resonance element9′. Since the radially-polarized light generating element20is arranged, the radially-polarized light can be included in irradiation light5′ condensed in the plasmon resonance element9′ by the objective lens10′. When the irradiation light5′ including the radially-polarized light is made incident on the bottom surface of the conical prism functioning as the plasmon resonance element9′, propagating surface plasmon propagates to an interface between the metal film coated on the side surface and the conical prism. Near-field light7′, a polarization direction of which is the Z direction, is generated in the resonance section22′ at the distal end.

Therefore, an intensification degree of plasmon resonance between the resonance section22′ and the recording region4changes according to whether the recording region4is in the recorded state or the unrecorded state. Therefore, by detecting reflected light6′ from the plasmon resonance element9′, as in the optical information reproduction device in the first embodiment, it is possible to determine whether the recording region4is in the recorded state or the unrecorded state, and reproduction information recorded in the recording region4.

FIGS. 8A and 8Bare examples in which a degree of plasmon resonance is larger in the recording region4ain the recorded state than in the recording region4bin the unrecorded state.FIG. 8Ashows a case in which the resonance section22′ of the plasmon resonance element9′ is present on the recording region4ain the recorded state. InFIG. 8A, the near-field light7a′ is generated between the resonance section22′ and the recording region4aand the plasmon resonance degree increases. As a result, a light amount of the reflected light6a′ changes (inFIG. 8A, decreases).FIG. 8Bshows a case in which the resonance section22′ of the plasmon resonance element9′ is present on the recording region4bin the unrecorded state. InFIG. 8B, the near-field light7b′ is generated only in the vicinity of the resonance section22′ and the plasmon resonance degree decreases. As a result, the light amount of the reflected light6b′ hardly changes.

Therefore, in the optical information reproduction device in the third embodiment, since the normal inline objective lens10′ is used, it is possible to use an optical system that condenses light perpendicularly to the substrate1of the information recording medium3or the formation surface (the XY plane) of the recording layer2. Therefore, a degree of freedom of design increases and it is easy to arrange the optical system. Further, it is also easy to increase an NA of the objective lens10′. As a result, it is possible to increase the intensity of the near-field light7′ generated from the resonance section22′.

As shown inFIGS. 8A and 8B, a vertical angle of the plasmon resonance element9′ is 2θ2. A metal film of, for example, Au or Al is coated on a conical prism made of, for example, glass or plastic. The shape of the plasmon resonance element9′ is set to so-called Kretschmann arrangement, whereby it is possible to efficiently change the irradiation light5′ of radially-polarized light into surface plasmon. For example, when the reproduction wavelength λ is 0.405 μm, it is desirable that an angle θ2is 43.4° and Al having thickness t of 16.3 nm is coated on a prism. At this point, the irradiation light5′ of nearly 100% can be changed to propagating surface plasmon.

For example, when the vertical angle of 2θ2is as small as to 8°, a mode called super focusing can be present. It is known that, at this point, the wavelength of the propagating surface plasmon decreases as the propagating surface plasmon propagates in the direction of the resonance section22′ at the distal end. It is possible to perform plasmon resonance with the finer recording region4and intensification of the plasmon resonance. Therefore, a modulation degree of reproduction with respect to the finer recording region4is satisfactory. This is desirable in terms of reproduction of a high-density information recording medium.

Fourth Embodiment

An optical information reproduction device in a fourth embodiment of the present invention is explained centering on differences from the optical information reproduction device in the first embodiment with reference toFIG. 9.

FIG. 9is a diagram showing the configuration of the optical information reproduction device in the fourth embodiment of the present invention. In the optical information reproduction device in the first embodiment, reflected light from the plasmon resonance element9is detected. However, in the optical information reproduction device in the fourth embodiment, transmitted light from the plasmon resonance element9is detected.

The optical information reproduction device in the fourth embodiment includes the plasmon resonance element9, the objective lens10, the collimator lens11, the light source14, the beam splitter15, the detection lens16, photodetectors17a′ and17b, the optical element for servo signal detection19, the reproduction unit24, and the driving unit25.

The photodetector17a′ is arranged in contact with a surface opposed to the surface on the light incident side of the plasmon resonance element9. The photodetector17a′ detects transmitted light18a′ from the plasmon resonance element9on which reproduction light is irradiated. The reproduction unit24determines on the basis of a detection signal from the photodetector17a′ whether the recording region4is in the recorded state or the unrecorded state, and reproduces information recorded in the recording region4.

A transmitted light amount changes according to a degree of plasmon resonance between the resonance section22of the plasmon resonance element9and the recording region4in the recorded state or the recording region4in the unrecorded state. For example, the change in the transmitted light amount is larger when the degree of the plasmon resonance between the resonance section22of the plasmon resonance element9and the recording region4ain the recorded state or the recording region4bin the unrecorded state is larger.

It is considered that, when the plasmon resonance between the plasmon resonance element9and the recording region4is intensified, a dielectric loss (absorption) increases in the plasmon resonance element9. In general, the transmitted light amount from the plasmon resonance element9decreases.

As explained above, the transmitted light18a′ is detected by the photodetector17a′ and it is determined on the basis of the detection signal from the photodetector17a′ whether the recording region4is in the recorded state or the unrecorded state. Consequently, it is possible to reproduce the information recorded in the recording region4.

The configuration of the fourth embodiment is the same as the configuration of the first embodiment except that the information recorded in the recording region4is reproduced by detecting the transmitted light18a′. Therefore, detailed explanation of the configuration of the fourth embodiment is omitted.

The optical recording and reproduction device in the fourth embodiment directly irradiate reproduction light on the plasmon resonance element9rather than near-field light and detects transmitted light from the plasmon resonance element9. Therefore, it is possible to set a transmitted light amount or a light amount change sufficiently large.

In the fourth embodiment, the photodetector17a′ is arranged in contact with the surface opposed to the surface on the light incident side of the plasmon resonance element9. However, the present invention is not limited to this arrangement. The photodetector17a′ may be provided in a position away from the plasmon resonance element9. A lens for guiding light transmitted through the plasmon resonance element9to the photodetector17a′ may be provided between the plasmon resonance element9and the photodetector17a′.

The optical information reproduction devices, the optical information reproduction methods, and the information recording media in the first to fourth embodiments are explained above. However, the present invention is not limited to the embodiments. An optical information reproduction device, an optical information reproduction method, and an information recording medium respectively obtained by combining the configurations of the optical information reproduction methods, and the information recording media in the first to fourth embodiments are also included in the present invention. Effects same as the effects in the first to fourth embodiments can be realized.

The objective lens, the collimator lens, and the detection lens used in the first to fourth embodiments are named only for convenience and are the same as a general lens.

In the first to fourth embodiments, an optical disk is explained as an example of the information recording medium. However, application to a card-like, drum-like, or tape-like product designed to be capable of reproducing, with the optical information reproduction devices in the first to fourth embodiment, a plurality of media with different specifications such as thickness and recording density is also included in the scope of the present invention.

Inventions having configurations explained below are mainly included in the specific embodiments explained above.

An optical information reproduction device according to an aspect of the present invention is an optical information reproduction device that reproduces information recorded on an information recording medium including at least a substrate and a recording layer, the optical information reproduction device including: a light source configured to emit reproduction light; a plasmon resonance element including a resonance section arranged adjacent to a recording region of the recording layer, the resonance section causing plasmon resonance between the recording region and the resonance section; a photodetector configured to detect reflected light or transmitted light from the plasmon resonance element on which the reproduction light is irradiated; and a reproduction unit configured to determine, on the basis of a detection signal from the photodetector, whether the recording region is in a recorded state or an unrecorded state, and reproduction information recorded in the recording region.

With this configuration, the reproduction light emitted from the light source is irradiated on the plasmon resonance element, the reflected light or the transmitted light from the plasmon resonance element is detected, it is determined on the basis of the detection signal whether the recording region is in the recorded state or the unrecorded state, and the information recorded in the recording region is reproduced.

Therefore, even if the size of the recording region is smaller than a diffraction limit of light, it is possible to satisfactorily reproduce the information by making use of the fact that a plasmon resonance degree between the recording region and the resonance section of the plasmon resonance element changes according to a state of the recording region, whereby a reflected light amount or a transmitted light amount from the plasmon resonance element changes.

Since the size of the plasmon resonance element is not subjected to a spatial limitation, it is possible to form the plasmon resonance element larger than the recording region. Further, the reflected light or the transmitted light from the plasmon resonance element is detected by directly irradiating the reproduction light on the plasmon resonance element rather than near-field light. Therefore, it is possible to set the reflected light amount, the transmitted light amount, a light amount change of the reflected light amount, or a light amount change of the transmitted light amount sufficiently large. It is possible to improve a modulation degree of a reproduction signal.

In the optical information reproduction device, it is desirable that the reproduction light is irradiated also on the recording region adjacent to the resonance section.

With this configuration, the reproduction light is irradiated on the recording region4adjacent to the resonance section of the plasmon resonance element as well. Therefore, the plasmon resonance is further intensified, a difference between the reflected light amount or the transmitted light amount between the recorded state and the unrecorded state increases, and detection sensitivity is improved.

In the optical information reproduction device, it is desirable that a reflected light amount or a transmitted light amount from the plasmon resonance element changes according to the degree of the plasmon resonance between the resonance section of the plasmon resonance element and the recording region in the recorded state or the recording region in the unrecorded state.

With this configuration, the reflected light amount or the transmitted light amount from the plasmon resonance element changes according to a degree of the plasmon resonance between the resonance section of the plasmon resonance element and the recording region in the recorded state or the recording region in the unrecorded state. Therefore, by detecting the reflected light or the transmitted light from the plasmon resonance element, it is possible to determine whether the recording region is in the recorded state or the unrecorded state.

In the optical information reproduction device, it is desirable that a part or all of the recording region is made of a recording material, and a sign of a real part of the dielectric constant of the recording material in the recorded state and a sign of a real part of the dielectric constant of the recording material in the unrecorded state are different from each other with respect to the wavelength of the reproduction light.

With this configuration, the sign of the real part of the dielectric constant of the recording material in the recorded state and the sign of the real part of the dielectric constant of the recording material in the unrecorded state are different from each other with respect to the wavelength of the reproduction light. Therefore, a plasmon resonance degree of one of the recording material in the recorded state and the recording material in the unrecorded state is intensified. It is possible to further improve the modulation degree of reproduction.

In the optical information reproduction device, it is desirable that a part or all of the recording region is made of a recording material, and one of a real part of the relative dielectric constant of the recording material in the recorded state and a real part of the relative dielectric constant of the recording material in the unrecorded state is equal to or smaller than −5 and the other is larger than −5 with respect to the wavelength of the reproduction light.

With this configuration, one of the real part of the relative dielectric constant of the recording material in the recorded state and the real part of the relative dielectric constant of the recording material in the unrecorded state is equal to or smaller than −5 and the other is larger than −5 with respect to the wavelength of the reproduction light. Therefore, the plasmon resonance degree of one of the recording material in the recorded state and the recording material in the unrecorded state is further intensified. It is possible to further improve the modulation degree of reproduction.

In the optical information reproduction device, it is desirable that a change in a reflected light amount or a transmitted light amount of the recording material with a smaller real part of the dielectric constant among the real part of the dielectric constant of the recording material in the recorded state and the real part of the dielectric constant of the recorded material in the unrecorded state, is larger than a change in a reflected light amount or a transmitted light amount of the recording material with the larger real part of the dielectric constant.

With this configuration, the change in the reflected light amount or the transmitted light amount of the recording material with a smaller real part of the dielectric constant among the real part of the dielectric constant of the recording material in the recorded state and the real part of the dielectric constant of the recorded material in the unrecorded state, is larger than the change in the reflected light amount or the transmitted light amount of the recording material with the larger real part of the dielectric constant. Therefore, the modulation degree of reproduction increases and it is possible to satisfactorily reproduce the information.

In the optical information reproduction device, it is desirable that a part or all of the recording region is made of a recording material, a main component of the recording material is a phase-change recording material, and the recorded state and the unrecorded state respectively correspond to one of amorphous and crystal.

With this configuration, dielectric constants of the crystalline recording material and the amorphous recording material are different from each other. Therefore, the plasmon resonance degree of one of the recording material in the recorded state and the recording material in the unrecorded state is intensified. It is possible to improve the modulation degree of reproduction.

In the optical information reproduction device, it is desirable that wavelength λ of the reproduction light satisfies 0.35 μm≦λ≦0.45 μm.

With this configuration, it is possible to apply the optical information reproduction device to the reproduction light, the wavelength λ of which satisfies 0.35 μm≦λ≦0.45 μm.

In the optical information reproduction device, it is desirable that the plasmon resonance element includes a flat section arranged substantially perpendicularly to an optical axis of the reproduction light, and the reproduction light is irradiated on the flat section.

With this configuration, it is possible to reflect the reproduction light, which is irradiated on the flat section of the plasmon resonance element, as reflected light at substantially the same angle and in the opposite direction. It is possible to increase efficiency of light utilization.

In the optical information reproduction device, it is desirable that the light source has a characteristic that, on an optical axis of the reproduction light irradiated on the plasmon resonance element, the amplitude of a polarization component of the reproduction light polarizing in a perpendicular direction with respect to an arrangement surface of the recording layer is larger than the amplitude of a polarization component of the reproduction light polarizing in other polarization directions.

With this configuration, on the optical axis of the reproduction light irradiated on the plasmon resonance element, the amplitude of the polarization component of the reproduction light polarizing in the perpendicular direction with respect to the arrangement surface of the recording layer is set larger than the amplitude of the polarization component of the reproduction light polarizing in other polarization directions. Therefore, it is possible to cause the resonance section of the plasmon resonance element to interact with the recording region and cause plasmon resonance of the resonance section of the plasmon resonance element.

In the optical information reproduction device, it is desirable that the optical information reproduction device further includes a polarization control optical element configured to convert a polarization state of the reproduction light emitted from the light source, and the polarization control optical element sets the amplitude of a polarization component of the reproduction light polarizing in a perpendicular direction with respect to an arrangement surface of the recording layer larger than the amplitude of a polarization component of the reproduction light polarizing in other polarization directions.

With this configuration, the amplitude of the polarization component of the reproduction light polarizing in the perpendicular direction with respect to the arrangement surface of the recording layer is set larger than the amplitude of the polarization component of the reproduction light polarizing in other polarization directions. Therefore, it is possible to cause the resonance section of the plasmon resonance element to interact with the recording region and cause plasmon resonance of the resonance section of the plasmon resonance element.

In the optical information reproduction device, it is desirable that the polarization control optical element includes a wave plate. With this configuration, it is possible to easily change a polarization direction with the wave plate.

In the optical information reproduction device, it is desirable that the optical information reproduction device further includes an off-axis condensing lens configured to irradiate the reproduction light on the plasmon resonance element.

With this configuration, the off-axis condensing lens is used. Therefore, it is possible to prevent contact of the condensing lens and the information recording medium and condense the reproduction light in the vicinity of the resonance section of the plasmon resonance element from an oblique lateral direction.

In the optical information reproduction device, it is desirable that the optical information reproduction device further includes a radially-polarized light generating element arranged in an optical path between the light source and the plasmon resonance element and configured to include radially-polarized light in the reproduction light condensed in the plasmon resonance element. With this configuration, it is possible to irradiate the reproduction light including the radially-polarized light on the plasmon resonance element.

In the optical information reproduction device, it is desirable that the plasmon resonance element is a conical prism in which a surface other than a bottom surface is coated with a metal film, and the conical prism includes the resonance section in the vicinity of the vertex.

With this configuration, when the reproduction light including the radially-polarized light is made incident on the bottom surface of the conical prism functioning as the plasmon resonance element, propagating surface plasmon propagates to an interface between the metal film coated on the surface other than the bottom surface and the conical prism and near-field light is generated in the resonance section in the vicinity of the vertex of the conical prism.

Therefore, an intensity degree of plasmon resonance between the resonance section and the recording region changes according to whether the recording region is in the recorded state or the unrecorded state. Therefore, it is possible to determine, by detecting reflected light from the plasmon resonance element, whether the recording region is in the recorded state or the unrecorded state and satisfactorily reproduce the information recorded in the recording region.

In the optical information reproduction device, it is desirable that wavelength λ of the reproduction light satisfies 0.35 μm≦λ≦0.45 μm, and a main component of the plasmon resonance element is at least one of Au, Cu, Ti, Ni, and Ag.

With this configuration, when at least one of Au, Cu, Ti, Ni, and Ag is used as the main component of the plasmon resonance element and the sign of the real part of the dielectric constant of the recording region is negative or the real part of the relative dielectric constant of the recording region is equal to or smaller than −5, the degree of the plasmon resonance substantially increases. Therefore, it is possible to improve the modulation degree of reproduction.

An optical information reproduction method according to another aspect of the present invention is an optical information reproduction method for reproducing information from an information recording medium including at least a substrate and a recording layer, the optical information reproduction method including: a step of irradiating reproduction light emitted from a light source on a plasmon resonance element including a resonance section arranged adjacent to a recording region of the recording layer, the resonance section causing plasmon resonance between the recording region and the resonance section; a step of detecting, with a photodetector, reflected light or transmitted light from the plasmon resonance element on which the reproduction light is irradiated; and a step of determining, on the basis of a detection signal from the photodetector, whether the recording region is in a recorded state or an unrecorded state, and reproducing information recorded in the recording region.

With this configuration, the reproduction light emitted from the light source is irradiated on the plasmon resonance element, the reflected light or the transmitted light from the plasmon resonance element is detected, it is determined on the basis of the detection signal whether the recording region is in the recorded state or the unrecorded state, and the information recorded in the recording region is reproduced.

Therefore, even if the size of the recording region is smaller than a diffraction limit of light, it is possible to satisfactorily reproduce the information by making use of the fact that a plasmon resonance degree between the recording region and the resonance section of the plasmon resonance element changes according to a state of the recording region, whereby a reflected light amount or a transmitted light amount from the plasmon resonance element changes.

Since the size of the plasmon resonance element is not subjected to a spatial limitation, it is possible to form the plasmon resonance element larger than the recording region. Further, the reflected light or the transmitted light from the plasmon resonance element is detected by directly irradiating the reproduction light on the plasmon resonance element rather than near-field light. Therefore, it is possible to set the reflected light amount, the transmitted light amount, a light amount change of the reflected light amount, or a light amount change of the transmitted light amount sufficiently large. It is possible to improve a modulation degree of a reproduction signal.

An information recording medium according to still another aspect of the present invention includes at least a substrate and a recording layer. A recording region of the recording layer is arrayed in an island shape, the recording region includes a particle, a part or all of which is made of a recording material, and a sign of a real part of the dielectric constant of the recording material in a recorded state and a sign of a real part of the dielectric constant of the recording material in an unrecorded state are different from each other with respect to the wavelength of the reproduction light.

With this configuration, the sign of the real part of the dielectric constant of the recording material in the recorded state and the sign of the real part of the dielectric constant of the recording material in the unrecorded state are different from each other with respect to the wavelength of the reproduction light. Therefore, a plasmon resonance degree of one of the recording material in the recorded state and the recording material in the unrecorded state is intensified. It is possible to further improve the modulation degree of reproduction and satisfactorily reproduce the information.

An information recording medium according to still another aspect of the present invention includes at least a substrate and a recording layer. A recording region of the recording layer is arrayed in an island shape, the recording region includes a particle, a part or all of which is made of a recording material, and one of a real part of the relative dielectric constant of the recording material in a recorded state and a real part of the relative dielectric constant of the recording material in an unrecorded state is equal to or smaller than −5 and the other is larger than −5 with respect to the wavelength of the reproduction light.

With this configuration, one of the real part of the relative dielectric constant of the recording material in the recorded state and the real part of the relative dielectric constant of the recording material in the unrecorded state is equal to or smaller than −5 and the other is larger than −5 with respect to the wavelength of the reproduction light. Therefore, the plasmon resonance degree of one of the recording material in the recorded state and the recording material in the unrecorded state is further intensified. It is possible to further improve the modulation degree of reproduction and satisfactorily reproduce the information.

In the information recording medium, it is desirable that a distal end portion of the particle includes a pointed cross section or an arcuate cross section.

With this configuration, the distal end portion of the particle includes the pointed cross section or the arcuate cross section. Therefore, near-field light is condensed or concentrated on the particle. It is possible to intensify the plasmon resonance degree.

In the information recording medium, it is desirable that the information recording medium further includes, in an upper layer of the recording region, a protective layer of which dielectric constant has a real part with a positive sign.

With this configuration, the protective layer, of which dielectric constant has a real part with a positive sign, is arranged in the upper layer of the recording region. Therefore, it is possible to improve resistance to environment of the particle functioning as the recording region formed of the recording material and reduce damage to the recording region due to contact of the distal end of the plasmon resonance element with the resonance section.

The specific embodiments and the examples described in the section of Description of Embodiments are solely clarifying the technical contents of the present invention. The present invention should not be limited to such specific examples and interpreted narrowly. The present invention can be variously modified and carried out within the scope of the spirit of the present invention and claimed elements.

INDUSTRIAL APPLICABILITY

With an optical information reproduction device, an optical information reproduction method, and an information recording medium according to the present invention, it is possible to satisfactorily reproduce information even if the size of a recording region such as a recording mark in which the information is recorded is smaller than a diffraction limit of light. The optical information reproduction device, the optical information reproduction method, and the information recording medium according to the present invention are useful for an optical information reproduction device and an optical information reproduction method for optically reproducing information recorded in an information recording medium and useful for an information recording medium including at least a substrate and a recording layer.