Optical: systems and elements – Diffraction – From grating
Reexamination Certificate
2001-06-04
2004-04-20
Robinson, Mark A. (Department: 2872)
Optical: systems and elements
Diffraction
From grating
C359S569000, C359S207110
Reexamination Certificate
active
06724534
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a diffractive optical element and scanning optical apparatus using the same and, more particularly, to an apparatus which records image information by causing a deflection element to deflect a light beam emitted by a light source means formed from a semiconductor laser and optically scanning a surface to be scanned through a scanning optical element (imaging element) having f−&thgr; characteristics, and is suitable for an image forming apparatus such as a laser beam printer (LBP) or digital copying machine having an electrophotography process.
2. Related Background Art
In a conventional scanning optical apparatus used in a laser beam printer, digital copying machine, or the like, a light beam which is optically modulated in accordance with an image signal and is output from a light source means is periodically deflected by an optical deflector such as a rotary polyhedral mirror (polygon mirror), and is focused to form a beam spot on the surface of a photosensitive recording medium (photosensitive drum) by a scanning optical element (imaging element) having f−&thgr; characteristics. Then, the beam spot is scanned on that surface to record an image.
FIG. 1
is a schematic sectional view showing principal part of a conventional scanning optical apparatus of this type.
Referring to
FIG. 1
, a divergent light beam emitted by a light source means
91
is converted into a nearly collimated light beam by a collimator lens
92
, and the light beam (light amount) is limited by a stop
93
. Then, the light beam enters a cylinder lens (cylindrical lens)
94
having a predetermined power in only the sub-scanning direction perpendicular to the drawing surface. Of the nearly collimated light beam that enters the cylinder lens
94
, light components in the main scanning section directly emerge as a nearly collimated light beam. In the sub-scanning section perpendicular to the drawing surface, light components are focused to form a nearly linear image on a deflection surface (reflection surface)
95
a
of an optical deflector
95
that comprises a rotary polyhedral mirror (polygon mirror).
The light beam deflected and reflected by the deflection surface
95
a
of the optical deflector
95
is guided onto a photosensitive drum surface
98
as a surface to be scanned via a scanning optical element (f−&thgr; lens)
96
having f−&thgr; characteristics. By rotating the optical deflector
95
in the direction of an arrow A, the light beam scans the photosensitive drum surface
98
in the direction of an arrow B. In this way, an image is recorded on the photosensitive drum surface
98
as a recording medium.
Conventionally, various scanning optical apparatuses using plastic lenses have been proposed as scanning optical systems because of their capability of highly accurate aberration correction using aspherical surfaces and cost reduction by injection molding.
However, a plastic lens largely changes in its aberration (especially errors in focus or magnification) due to environmental variations. This poses a serious problem in a scanning optical apparatus having a small spot diameter.
Recently, to compensate for aberration variations unique to a plastic lens, some apparatuses use a diffractive optical element as a scanning optical system, as proposed in, e.g., Japanese Patent Application Laid-Open No. 10-68903. In this prior art, for example, when ambient temperature increases, chromatic aberration is generated using a diffractive optical element in advance so as to compensate for a change in aberration due to a decrease in refractive index of a plastic lens with a change in aberration due to wavelength variation of a semiconductor laser as a light source. When a diffractive optical element is used singly, the element has a predetermined thickness. Hence, the element manufactured by injection molding is excellent in molding properties.
A diffractive optical element is very useful as the optical system of a scanning optical apparatus. However, the light utilization efficiency (to be referred to as a diffraction efficiency &eegr; hereinafter) of a diffractive optical element changes depending on conditions, unlike a refractive optical element. This will be described below using a diffraction grating model.
FIG. 2
is an explanatory view of a diffraction grating model. This diffraction grating model comprises a continuous grating having a grating pitch of P &mgr;m and a grating depth of h &mgr;m. The ratio of the grating pitch to the grating depth is called an aspect ratio AR, and it is defined that AR=grating pitch P/grating depth h. A light beam incident on the substrate of the diffraction grating model at an angle of incidence &thgr;i is diffracted and emerges in the direction of designed diffraction order.
FIG. 3
is an explanatory view showing the dependence of the diffraction efficiency on the angle of incidence when the aspect ratio AR is 4 in the above diffraction grating model. As is apparent from
FIG. 3
, the diffraction efficiency greatly changes depending on the angle of incidence, and especially, the diffraction efficiency of a light beam incident at a large angle of incidence lowers.
FIG. 4
is an explanatory view showing the dependence of the diffraction efficiency on the aspect ratio when the angle of incidence on the grating portion is &thgr;i=0 in the above diffraction grating model. In
FIG. 4
, the grating depth h is not changed while the aspect ratio AR is changed by changing the grating pitch P. When the aspect ratio is lower than 4, the diffraction efficiency abruptly decreases.
As is apparent from the above two conditions, when a diffractive optical element is used as the scanning optical system of a scanning optical apparatus, the diffraction efficiency lowers in the off-axis region where the angle of incidence is large and the aspect ratio is low, so the uniformity of an image plane illuminance on a surface to be scanned degrades.
SUMMARY OF THE INVENTION
It is an object of the present invention to provide a diffractive optical element suitable for high-resolution printing, which suppresses a decrease in diffraction efficiency of the diffractive optical element especially in the off-axis region, increases the uniformity of image plane illuminance on a surface to be scanned, and minimizes aberration changes due to various variations, without increasing cost, with a simple arrangement in which a diffraction grating comprises a tilt portion for mainly generating a power and a wall portion connecting one end portion of the tilt portion to a substrate, and the wall portion is tilted with respect to the normal to the substrate, and a scanning optical apparatus using this diffractive optical element.
A diffractive optical element according to the present invention, which has a diffraction grating formed on a substrate surface and diffracts an incident light beam to obtain a predetermined power, is characterized in that
the diffraction grating has a tilt portion for generating a power and a wall portion connecting one end portion of the tilt portion to the substrate, and
the wall portion is tilted with respect to a normal to the substrate surface to increase the diffraction efficiency at that portion.
Especially, the element is characterized in that
the tilt angle &thgr;e of the wall portion of the diffraction grating with respect to the normal to the substrate surface satisfies
tan
−1
(
h/P
)≦&thgr;
e
≦tan
−1
(
h/P
)+10°
where h is the depth of the diffraction grating, and P is the grating pitch,
the tilt angle &thgr;e of the wall portion of the diffraction grating with respect to the normal to the substrate surface continuously changes to increase as a distance away from an optical axis of the diffractive optical element becomes large,
the diffractive optical element is manufactured by forming the diffraction grating on a glass substrate by a replica process, and
the diffractive optical element is manufactured by integrally forming the
Amari Alessandro V.
Robinson Mark A.
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