Optical head

Claim 2

An optical head comprising a beam source for generating a light beam, a base supporting said beam source mounted thereon and having a linear expansion coefficient α, a frame supporting said base secured thereto and having a linear expansion coefficient γ, a lens-barrel disposed in and secured to said frame and having a linear expansion coefficient β, and a collimator lens system disposed in and secured to said lens-barrel for collimating the light beam generated from said beam source, said frame being made of a material having a linear expansion coefficient satisfying either one of the inequalities α≧γ and β≧γ.

Claim 3

The optical head according to claim 1, wherein said base, lens-barrel and frame are made of materials having linear expansion coefficients satisfying either one of inequalities α≧γ≧β and β>γ>α.

Claim 4

The optical head according to claim 1, wherein said base and frame are made of the same material.

Claim 5

The optical head according to claim 1, which further comprises a member for securing said lens-barrel to said frame by point contact securement.

Claim 6

The optical head according to claim 1, wherein said collimator lens system includes at least one collimator lens, an outer periphery portion of said lens-barrel corresponding to the outer periphery of said collimator lens being secured to said frame.

Claim 7

The optical head according to claim 1, wherein the materials of said frame and said lens-barrel are selected such that B×γ-A0×β is substantially zero, where A0 represents the distance from the secured point of said lens-barrel to the front principle point of said collimator lens system, and B represents the distance from said secured point of lens-barrel to said beam source.

Claim 8

The optical head according to claim 1, wherein the materials of said frame and said lens-barrel are selected such that B×γ-A1×β is substantially zero, where A1 represents the distance from the secured point of said lens-barrel to a collimator lens in said collimator lens system, and B represents the distance from said secured point of lens-barrel to said beam source.

Claim 9

An optical head comprising a beam source for generating a light beam, a base supporting said beam source mounted thereon and having a linear expansion coefficient α, a frame secured to said base and having a linear expansion coefficient γ, a lens-barrel disposed in and secured to said frame and having a linear expansion coefficient β, a collimator lens system disposed in and secured to said frame for collimating the light beam generated from said beam source and an objective lens for converging the collimated light beam to form a beam spot on a light-reflecting surface, said beam source and light-reflecting surface being held in an image focusing relation to each other by an optical system provided between said beam source and light-reflecting surface, said frame being made of a material having a linear expansion coefficient satisfying either one of the inequalities α≧γ and β>γ.

Claim 10

An optical head comprising a beam source for generating a light beam, a base supporting said beam source mounted thereon and having a linear expansion coefficient α, a frame secured to said base and having a linear expansion coefficient γ, a lens-barrel disposed in and secured to said frame and having a linear expansion coefficient β, a collimator lens system disposed in and secured to said frame for collimating the light beam generated from said beam source and an objective lens for converging the collimated light beam to form a beam spot on a light-reflecting surface, said beam source and light-reflecting surface being held in an image focusing relation to each other by an optical system provided between said beam source and light-reflecting surface, said frame being made of a material having a linear expansion coefficient satisfying either one of the inequalities α≧γ and β>γ.

Claim 11

The optical head according to claim 8, wherein said base, lens-barrel and frame are made of materials having linear expansion coefficients satisfying either one of the inequalities α≧γ≧β and β>γ>α.

Claim 12

The optical head according to claim 8, wherein said base and frame are made of the same material.

Claim 13

The optical head according to claim 8, which further comprises a member for securing said lens-barrel to said frame by point contact securement.

Claim 14

The optical head according to claim 8, wherein said collimator lens system includes at least one collimator lens, an outer periphery portion of said lens-barrel corresponding to the outer periphery of said collimator lens being secured to said frame.

Claim 15

The optical head according to claim 8, wherein the materials of said frame and lens-barrel are selected such that B×γ-A0×β is substantially zero, where A0 represents the distance from the secured point of said lens-barrel to the front principle point of said collimator lens system, and B represents the distance from said secured point of said lens-barrel to said beam source.

Claim 16

The optical head according to claim 8, wherein the materials of said frame and lens-barrel are selected such that B×γ-A1×β is substantially zero, where A1 represents the distance from the secured point of said lens-barrel to a collimator lens in said collimator lens system, and B represents the distance from said secured point of the lens-barrel to said beam source.

Claim 17

The optical head according to claim 8, wherein said lens-barrel and frame are made of materials satisfying a condition: |(B×γ-A0×β)|≦Mδ/.vertline.Δt| where M represents a longitudinal magnification determined by the optical system provided between said beam source and light-reflecting surface, A0 represents the distance from the secured point of said lens-barrel to the front principle point of said collimator lens system, B represents the distance from said secured point of the lens-barrel to said beam source, δ represents the permissible defocusing value in the objective lens and is 2.0 μm, and |Δt| represents the absolute value of the temperature change from the normal temperature and is 20.

Claim 18

The optical head according to claim 8, wherein said lens-barrel and frame are made of materials satisfying a condition: |(B×γ-A1×β)≦Mδ/|.DELTA.t| where M represents a longitudinal magnification determined by the optical system provided between said beam source and light-reflecting surface, A1 represents the distance from the secured point of said lens-barrel to a collimator lens in said collimator lens system, B represents the distance from said secured point of the lens-barrel to said beam source, δ represents the permissible defocusing value in the objective lens and is 2.0 μm, and |Δt| represents the absolute value of the temperature change from the normal temperature and is 20.

Claim 19

The optical head according to claim 8, wherein said collimator lens system includes at least one collimator lens, an outer periphery portion of said lens-barrel corresponding to the outer periphery of said collimator lens being secured to said frame, the materials of said frame and lens-barrel being made of materials satisfying a condition: |C×γ|≦Mδ/|Δt.vertline. where M represents a longitudinal magnification determined by the optical system provided between said beam source and light-reflecting surface, C the distance from the secured point of said lens-barrel to said beam source, δ represents the permissible defocusing value in the objective lens and is 2.0 μm, and |Δt| represents the absolute value of the temperature change from the normal temperature and is 20.

Claim 20

An optical head comprising a beam source for generating a light beam, a first base supporting said beam source mounted thereon and having a linear expansion coefficient α, a frame supporting said first base secured thereto and having a linear expansion coefficient γ, a first lens-barrel disposed in and secured to said frame and having a linear expansion coefficient β, a collimator lens system secured to said first lens-barrel and having a focal distance f1 for collimating the light beam generated from said beam source, an objective lens having a focal distance f0 for converging the collimated light beam to form a beam spot on a light-reflecting surface, a projecting lens having a focal distance f2 for transferring the light beam reflected from the light reflecting surface, a light detector for detecting a defocusing by detecting the light beam from said projecting lens, and a second base supporting said light detector mounted thereon, a second lens barrel secured to said second base and accommodating said light detector and projecting lens mutually faced to each other and having a fixed linear expansion coefficient X, said second lens-barrel being made of a material permitting cancellation of the defocusing caused by thermal deformation of said frame and first lens-barrel of the defocusing caused by thermal deformation of said second lens-barrel.

Claim 21

An optical head comprising a beam source for generating a light beam, a first base supporting said beam source mounted thereon and having a linear expansion coefficient α, a frame supporting said first base secured thereto and having a linear expansion coefficient γ, a first lens-barrel disposed in and secured to said frame and having a linear expansion coefficient β, a collimator lens system secured to said first lens-barrel and having a focal distance f1 for collimating the light beam generated from said beam source, an objective lens having a focal distance f0 for converging the collimated light beam to form a beam spot on a light-reflecting surface, a projecting lens having a focal distance f2 for transferring the light beam reflected from the light reflecting surface, a light detector for detecting a defocusing by detecting the light beam from said projecting lens, and a second base supporting said light detector mounted thereon, a second lens barrel secured to said second base and accommodating said light detector and projecting lens mutually faced to each other and having a fixed linear expansion coefficient X, said second lens-barrel being made of a material permitting cancellation of the defocusing caused by thermal deformation of said frame and first lens-barrel of the defocusing caused by thermal deformation of said second lens-barrel.

Claim 22

The optical head according to claim 18, wherein the materials and shapes of said first base, frame and first and second lens-barrels are selected to meet a condition: (B×γ-A0×β)×χL>0 where A0 represents the distance from the secured point of the lens-barrel to the front principle point of said collimator lens system, B represents the distance from said secured point of the lens-barrel to said beam source, and L represents the distance between said projecting lens and light detector.

Claim 23

The optical head according to claim 18, wherein the materials and shapes of said first base, frame and first and second lens-barrels are selected to meet a condition: |{(f0/f1).sup.2 (B×γ-A0×β)-(f0/f2).sup.2 χL}|≦d/Δt where A0 represents the distance from the secured point of the lens-barrel to the front principle point of said collimator lens system, B represents the distance from said secured point of the lens-barrel to said beam source, L is the distance between said projecting lens and light detector, d represents the permissible defocusing value in said objective lens and is 2.0 μm, and |Δt| is the absolute value of the temperature change from the normal temperature and is 20.

Claim 24

The optical head according to claim 18, wherein the materials and shapes of said first base, frame and first and second lens-barrels are selected to meet a condition: (f0/f1).sup.2 (B×γ-A0×β)=(f0/f2)χL

Claim 25

The optical head according to claim 18, wherein the materials and shapes of said first base, frame and first and second lens-barrels are selected to meet a condition: |(f0/f1).sup.2 (B×γ-A0×β)|+|(f0/f2).sup.2 χL|≦d/Δt where A0 is the distance from the secured point of the lens-barrel to the front principle point of said collimator lens system, B represents the distance from said secured point of lens-barrel to said beam source, L is the distance between said projecting lens and light detector, d represents the permissible defocusing value in said objective lens and is 2.0 μm, and |Δt| is the absolute value of the temperature change form the normal temperature and is 20.