Information medium with multi-layered structure, and apparatus and method using this medium

• US 20030002423A1
• Filed: 06/27/2002
• Published: 01/02/2003
• Est. Priority Date: 06/29/2001
• Status: Abandoned Application

• Current Assignee: Kabushiki Kaisha Toshiba (Toshiba Corporation)
• Original Assignee: Kabushiki Kaisha Toshiba (Toshiba Corporation)
• Inventors: Ishibashi, Yoriyuki, Ando, Hideo
• Application Number:
  US10/183,029
• Publication Number:
  US 20030002423A1
• Time in Patent Office: Days
• US Class Current: 369/94
• CPC Class Codes: G11B 7/24 Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the arrangement of information on the carrier G11B7/007

Abstract

An upper recording layer is arranged on a portion having distance h from the disc surface, a lower recording layer is arranged on a portion having distance h+Δh from the disc surface, a space layer having thickness Δh is arranged between the upper and lower recording layers, and a cover layer having thickness h is arranged between the upper recording layer and disc surface. Thickness Δh of the space layer is specified, so that a coherence length (Lc) which is determined by central wavelength λ₀ and its half-width Δλ of the exit light power spectrum of a laser beam is smaller than the optical path difference (ΔL) between light u₀ which is directly reflected by the surface of the cover layer, and light u₂ which is transmitted through the cover layer and space layer, is reflected by the lower recording layer, and leaves the cover layer.

Claims

1. An information medium with a multi-layered structure, which has a lower recording layer, an upper recording layer formed on said lower recording layer via a space layer having a first predetermined thickness, and a cover layer which is formed on said upper recording layer and has a second predetermined thickness,

wherein when λ

₀ represents a central wavelength of a light beam used to read recorded information from said lower or upper recording layer, Δ

λ

represents a broadening or half-width of the wavelength of the light beam, n₂ represents a refractive index of said space layer, and NA represents a numerical aperture of an objective lens used to focus the light beam on said lower or upper recording layer,

the first predetermined thickness of said space layer is determined by a difference between a length determined by λ

₀, Δ

λ

, n₂, and NA, and the second predetermined thickness of said cover layer.

2. A medium according to claim 1, wherein when Δ

h represents the first predetermined thickness, and h represents the second predetermined thickness, Δ

h is determined based on;

Δ

h≧

λ

₀²/(2·

Δ

λ

·

[n₂²−

NA²]^1/2)−

h

3. A medium according to claim 1, wherein Δ

h is determined to have a value approximately ⅕

of the value of h as a lower limit value.

4. A medium according to claim 1, wherein when Δ

h represents the first predetermined thickness, and h represents the second predetermined thickness, Δ

h is determined to have the value of h as an upper limit value.

5. A medium according to claim 1, wherein when λ

₀=400 nm to 405 nm, Δ

λ

=0.1 nm to 1.0 nm, n₂=1.61 to 1.62, NA=0.85±

0.01, h=100 μ

m 1 μ

m, and Δ

h represents the first predetermined thickness, Δ

h is determined to have a value approximately {fraction (1/10)} of h as a lower limit value.

6. A recording method that uses an information medium with a multi-layered structure which has a lower recording layer, an upper recording layer formed on said lower recording layer via a space layer having a first predetermined thickness, and a cover layer which is formed on said upper recording layer and has a second predetermined thickness, and in which when λ

₀ represents a central wavelength of a light beam used to read recorded information from said lower or upper recording layer, Δ

λ

represents a broadening or half-width of the wavelength of the light beam, n₂ represents a refractive index of said space layer, and NA represents a numerical aperture of an objective lens used to focus the light beam on said lower or upper recording layer, the first predetermined thickness of said space layer is determined by a difference between a length determined by λ

₀, Δ

λ

, n₂, and NA, and the second predetermined thickness of said cover layer,

wherein information is recorded on said upper or lower recording layer using a laser beam having central wavelength λ

₀.

7. An optical disc which has an optical disc structure using a substrate having thickness H, and in which a first recording layer formed with signal pits is arranged on a portion having distance h from the surface, a second recording layer formed with signal pits is also arranged on a portion having distance h+Δ

h from the surface, a space layer having thickness Δ

h is arranged between said first and second recording layers, and a cover layer having thickness h is arranged between said first recording layer and the disc surface,

wherein the thickness of said space layer is specified so that a coherence length determined by a central wavelength and its half-width of an exit light power spectrum of a light source of a laser beam with which said first or second recording layer is irradiated is smaller than an optical path difference between light directly reflected by a surface of said cover layer, and light which is transmitted through said cover layer and said space layer, is reflected by said second recording layer, and leaves said cover layer.

8. A disc according to claim 7, wherein when λ

₀ represents a central wavelength of the laser beam, Δ

λ

represents a half-width of the wavelength of the laser beam, n₂ represents a refractive index of said space layer, NA represents a numerical aperture of an objective lens used to focus the light beam on said first or second recording layer, Δ

h represents the thickness of said space layer, and h represents the thickness of said cover layer, Δ

h is determined based on;

Δ

h≧

λ

₀²/(2·

Δ

λ

·

[n₂²−

NA²]^1/2)−

h

9. An optical disc apparatus which irradiates an optical disc of claim 7 with a laser beam which is emitted by the light source via an objective lens, and records or reproduces information on or from said first or second recording layer by the irradiated laser beam, wherein a focus error of the objective lens is detected on the basis of a signal obtained by detecting some light components of the laser beam reflected by said first or second recording layer.

10. An information recording apparatus that uses an information medium with a multi-layered structure which has a lower recording layer, an upper recording layer formed on said lower recording layer via a space layer having a first predetermined thickness, and a cover layer which is formed on said upper recording layer and has a second predetermined thickness, and in which when λ

₀ represents a central wavelength of a light beam used to read recorded information from said lower or upper recording layer, Δ

λ

represents a broadening or half-width of the wavelength of the light beam, n₂ represents a refractive index of said space layer, and NA represents a numerical aperture of an objective lens used to focus the light beam on said lower or upper recording layer, the first predetermined thickness of said space layer is determined by a difference between a length determined by λ

₀, Δ

λ

, n₂, and NA, and the second predetermined thickness of said cover layer,

wherein information is recorded on at least one of said upper and lower recording layers.

11. An information recording method that uses an information medium with a multi-layered structure which has a lower recording layer, an upper recording layer formed on said lower recording layer via a space layer having a first predetermined thickness, and a cover layer which is formed on said upper recording layer and has a second predetermined thickness, and

in which when λ

₀ represents a central wavelength of a light beam used to read recorded information from said lower or upper recording layer, Δ

λ

represents a broadening or half-width of the wavelength of the light beam, n₂ represents a refractive index of said space layer, and NA represents a numerical aperture of an objective lens used to focus the light beam on said lower or upper recording layer,

the first predetermined thickness of said space layer is determined by a difference between a length determined by λ

₀, Δ

λ

, n₂, and NA, and the second predetermined thickness of said cover layer,

wherein information is recorded on at least one of said upper and lower recording layers.