Optical scanning device with constant speed scan

Claim 2

An optical scanning device comprising: a light source for producing light rays; means for deflecting light rays from the light source toward a predetermined direction; a surface to be scanned by said deflected light rays; single lens means having a distortion coefficient V disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; and said deflecting means having a revolution angle φ 0 sin kt within a definite time, where φ 0 is an amplitude, k is a constant, and t is time, wherein the following equation is satisfied to make the moving velocity of a light beam on said surface constant; ##EQU29## where t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is a distance between said deflecting means and the light source measured from the deflecting means toward the light source.

Claim 3

Scanning device according to claim 1, wherein the beam incident on said deflecting means is a divergent beam.

Claim 4

Scanning device according to claim 1, wherein the beam incident on said deflecting means is a parallel beam.

Claim 5

An optical scanning device comprising: a light source for producing light rays; deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 sin kt within a definite time, where k is constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; and said single lens means having the following distortion coefficient V to make the moving velocity of a light beam on said beam on said surface constant: ##EQU30## where t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is the distance between said deflecting means and the light source measured from said deflecting means toward the light source.

Claim 6

An optical scanning device comprising: a light source for producing light rays; deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 sin kt within a definite time, where k is constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; and said single lens means having the following distortion coefficient V to make the moving velocity of a light beam on said beam on said surface constant: ##EQU30## where t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is the distance between said deflecting means and the light source measured from said deflecting means toward the light source.

Claim 7

Scanning device according to claim 1, wherein the beam incident on said deflecting means is a divergent beam.

Claim 8

Scanning device according to claim 1, wherein the beam incident on said deflecting means is a parallel beam.

Claim 9

An optical scanning device comprising: a light source for producing light rays, deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 sin kt within a definite time, where k is a constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; and said single lens means having the following distortion coefficient V to cause the moving velocity of a light beam on said surface to be substantially constant: ##EQU31## where, V 0 is an ideal distortion; g' is the distance between said single lens means and said surface to be scanned measured from the single lens means toward the surface to be scanned; θ is a deflecting angle; ΔY' is a deviation from the ideal scanning position Y', where ##EQU32## t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is the distance between said deflecting means and light source measured from said deflecting means toward the light source.

Claim 10

An optical scanning device comprising: a light source for producing light rays, deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 sin kt within a definite time, where k is a constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; and said single lens means having the following distortion coefficient V to cause the moving velocity of a light beam on said surface to be substantially constant: ##EQU31## where, V 0 is an ideal distortion; g' is the distance between said single lens means and said surface to be scanned measured from the single lens means toward the surface to be scanned; θ is a deflecting angle; ΔY' is a deviation from the ideal scanning position Y', where ##EQU32## t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is the distance between said deflecting means and light source measured from said deflecting means toward the light source.

Claim 11

The scanning device according to claim 7, wherein the light ray incident on said deflecting means is a divergent beam.

Claim 12

The scanning device according to claim 7, wherein the light ray incident on said deflecting means is a parallel beam.

Claim 13

An optical scanning device comprising: a light source for producing light rays; means for deflecting light rays from the light source toward a predetermined direction for scanning a surface; single lens means having a distortion coefficient V disposed between the deflecting means and the position of the surface for focusing the light rays deflected by the deflecting means; said deflecting means having a revolution angle φ 0 sin kt within a definite time, where φ 0 is an amplitude, k is a constant and this time, wherein the following equation is satisfied to cause the moving velocity of a light beam on said surface to be constant: ##EQU33## where t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is a distance between said deflecting means and the light source measured from the deflecting means toward the light source; and the quantities ΔM of the field curvature of said single lens means in the meridional plane and the quantities ΔS of the field curvature of said single lens means in the sagittal plane satisfy the following equations |ΔM|≦2.44 Fe.sup.2. λ |ΔS|≦2.44 Fe.sup.2. λ where, Fe denotes an effective F number of said single lens means when the diameter of the beam incident on said single lens means is smaller than the focal length of said single lens means, and λ is the wavelength of said light source.

Claim 14

An optical scanning device comprising: a light source for producing light rays; means for deflecting light rays from the light source toward a predetermined direction for scanning a surface; single lens means having a distortion coefficient V disposed between the deflecting means and the position of the surface for focusing the light rays deflected by the deflecting means; said deflecting means having a revolution angle φ 0 sin kt within a definite time, where φ 0 is an amplitude, k is a constant and this time, wherein the following equation is satisfied to cause the moving velocity of a light beam on said surface to be constant: ##EQU33## where t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is a distance between said deflecting means and the light source measured from the deflecting means toward the light source; and the quantities ΔM of the field curvature of said single lens means in the meridional plane and the quantities ΔS of the field curvature of said single lens means in the sagittal plane satisfy the following equations |ΔM|≦2.44 Fe.sup.2. λ |ΔS|≦2.44 Fe.sup.2. λ where, Fe denotes an effective F number of said single lens means when the diameter of the beam incident on said single lens means is smaller than the focal length of said single lens means, and λ is the wavelength of said light source.

Claim 15

Scanning device according to claim 10, wherein the light ray incident on said deflecting means is a divergent beam.

Claim 16

Scanning device according to claim 10, wherein the light ray incident on said deflecting means is a parallel beam.

Claim 17

An optical scanning device comprising: a light source for producing light rays; means for deflecting divergent light rays from the light source toward a predetermined direction; a surface to be scanned by said deflected light rays; single lens means having a distortion coefficient V disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; said deflecting means having a revolution angle φ 0 sin kt within a definite time, wherein φ 0 is an amplitude, k is a constant, and t is time, wherein the following equation is satisfied to cause the moving velocity of a light beam on said surface to be constant: ##EQU34## wherein t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is a distance between said deflecting means and the light source measured from the deflecting means toward the light source; and said single lens means satisfies the following equation: g=-Nf where, N is the refractive power of said single lens means, and f is the focal length of said single lens means.

Claim 18

An optical scanning device comprising: a light source for producing light rays; means for deflecting divergent light rays from the light source toward a predetermined direction; a surface to be scanned by said deflected light rays; single lens means having a distortion coefficient V disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; said deflecting means having a revolution angle φ 0 sin kt within a definite time, wherein φ 0 is an amplitude, k is a constant, and t is time, wherein the following equation is satisfied to cause the moving velocity of a light beam on said surface to be constant: ##EQU34## wherein t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is a distance between said deflecting means and the light source measured from the deflecting means toward the light source; and said single lens means satisfies the following equation: g=-Nf where, N is the refractive power of said single lens means, and f is the focal length of said single lens means.

Claim 19

An optical scanning device comprising: a light source for producing light rays; deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 sin kt within a definite time, where k is constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; said single lens means having the following distortion coefficient V to cause the moving velocity of a light beam on said surface to be constant: ##EQU35## where t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is the distance between said deflecting means and the light source measured from deflecting means toward the light source; and the quantities ΔM of the field curvature of said single lens means in the meridional plane and the quantities ΔS of the field curvature of said single lens means in the sagittal plane satisfy the following equation |ΔM|≦2.44Fe.sup.2 λ |ΔS|≦2.44Fe.sup.2 λ where, Fe denotes an effective F number of said single lens means when the diameter of the beam incident on said single lens means is smaller than the focal length of said single lens means, and λ is a wavelength of said light source.

Claim 20

An optical scanning device comprising: a light source for producing light rays; deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 sin kt within a definite time, where k is constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; said single lens means having the following distortion coefficient V to cause the moving velocity of a light beam on said surface to be constant: ##EQU35## where t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is the distance between said deflecting means and the light source measured from deflecting means toward the light source; and the quantities ΔM of the field curvature of said single lens means in the meridional plane and the quantities ΔS of the field curvature of said single lens means in the sagittal plane satisfy the following equation |ΔM|≦2.44Fe.sup.2 λ |ΔS|≦2.44Fe.sup.2 λ where, Fe denotes an effective F number of said single lens means when the diameter of the beam incident on said single lens means is smaller than the focal length of said single lens means, and λ is a wavelength of said light source.

Claim 21

Scanning device according to claim 14, wherein the light ray incident on said deflecting means is a divergent beam.

Claim 22

Scanning device according to claim 14, wherein the light ray incident on said deflecting means is a parallel beam.

Claim 23

An optical scanning device comprising: a light source for producing light rays; deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 .sin kt within a definite time, where k is a constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; said single lens means having the following distortion coefficient V to cause the moving velocity of a light beam on said beam on said surface to be constant: ##EQU36## where t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is the distance between said deflecting means and the light source measured from deflecting means toward the light source; and said single lens means satisfies the following equation; g=-Nf where, N is the refractive power of said single lens means, and f is the focal length of said single lens means.

Claim 24

An optical scanning device comprising: a light source for producing light rays; deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 .sin kt within a definite time, where k is a constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; said single lens means having the following distortion coefficient V to cause the moving velocity of a light beam on said beam on said surface to be constant: ##EQU36## where t 1 is the distance between said single lens means and said deflecting means measured from said single lens means toward said deflecting means; g is the distance between said deflecting means and the light source measured from deflecting means toward the light source; and said single lens means satisfies the following equation; g=-Nf where, N is the refractive power of said single lens means, and f is the focal length of said single lens means.

Claim 25

An optical scanning device comprising: a light source for producing light rays; deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 sin kt within a definite time, where k is constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; said single lens means having the following distortion V to cause the moving velocity of a light beam on said surface to be constant: ##EQU37## where, V 0 is an ideal distortion, g' is the distance between said single lens means and said the surface to be scanned, θ is a deflecting angle; ΔY' is a deviation from the ideal scanning position Y', where ##EQU38## t 1 is the distance between said single lens means and the deflecting means measured from said single lens means toward the deflecting means; g is the distance between the deflecting means and the light source measured from deflecting means toward the light source; and the quantities ΔM of the field curvature of said single lens means in the meridional plane and the quantities ΔS of the field curvature of said single lens means in the sagittal plane satisfy the following equation: |ΔM|≦2.44Fe.sup.2 λ |ΔS|≦2.44Fe.sup.2 λ where, Fe denotes an effective F number of said single lens means when the diameter of the beam incident on said single lens means is smaller than the focal length of said single lens means, and λ is a wavelength of said light source.

Claim 26

An optical scanning device comprising: a light source for producing light rays; deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 sin kt within a definite time, where k is constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; said single lens means having the following distortion V to cause the moving velocity of a light beam on said surface to be constant: ##EQU37## where, V 0 is an ideal distortion, g' is the distance between said single lens means and said the surface to be scanned, θ is a deflecting angle; ΔY' is a deviation from the ideal scanning position Y', where ##EQU38## t 1 is the distance between said single lens means and the deflecting means measured from said single lens means toward the deflecting means; g is the distance between the deflecting means and the light source measured from deflecting means toward the light source; and the quantities ΔM of the field curvature of said single lens means in the meridional plane and the quantities ΔS of the field curvature of said single lens means in the sagittal plane satisfy the following equation: |ΔM|≦2.44Fe.sup.2 λ |ΔS|≦2.44Fe.sup.2 λ where, Fe denotes an effective F number of said single lens means when the diameter of the beam incident on said single lens means is smaller than the focal length of said single lens means, and λ is a wavelength of said light source.

Claim 27

The scanning device according to claim 18, wherein the light ray incident on said deflecting means is a divergent beam.

Claim 28

The scanning device according to claim 18, wherein the light ray incident on said deflecting means is a parallel beam.

Claim 29

A scanning device comprising: a light source for producing divergent light rays; deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 sin kt within a definite time, where k is a constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; said single lens means having the following distortion V to cause the moving velocity of a light beam on said surface to be constant: ##EQU39## where, V 0 is an ideal distortion; g' is the distance between said single lens means and said the surface to be scanned, θ is a deflecting angle; ΔY' is a deviation from the ideal scanning position Y', where ##EQU40## t 1 is the distance between said single lens means and the deflecting means measured from said single lens means toward the deflecting means; g is the distance between said deflecting means and light source measured from deflecting means toward the light source; and said single lens means satisfies the following equation: g=-Nf where, N is the refractive power of said single lens means, and f is the focal length of said single lens.

Claim 30

A scanning device comprising: a light source for producing divergent light rays; deflecting means with an amplitude φ 0 (0<φ 0 ≦∞) having a revolution angle φ 0 sin kt within a definite time, where k is a constant and t is time; a surface to be scanned by said deflected light rays; single lens means disposed between the deflecting means and the surface for focusing the light rays deflected by the deflecting means; said single lens means having the following distortion V to cause the moving velocity of a light beam on said surface to be constant: ##EQU39## where, V 0 is an ideal distortion; g' is the distance between said single lens means and said the surface to be scanned, θ is a deflecting angle; ΔY' is a deviation from the ideal scanning position Y', where ##EQU40## t 1 is the distance between said single lens means and the deflecting means measured from said single lens means toward the deflecting means; g is the distance between said deflecting means and light source measured from deflecting means toward the light source; and said single lens means satisfies the following equation: g=-Nf where, N is the refractive power of said single lens means, and f is the focal length of said single lens.