Solid immersion lens and production method thereof

Optical: systems and elements – Lens – Including a nonspherical surface

Reexamination Certificate

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C369S044140

Reexamination Certificate

active

06369957

ABSTRACT:

CROSS-REFERENCE TO RELATED APPLICATIONS
This application is based on Patent Application No. 10-261887 filed in Japan, the content of which is hereby incorporated by reference.
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a solid immersion lens and production method thereof, and specifically relates to a solid immersion lens used as a recording/reading head for a high resolution microscope probe or high density optical memory (recording/reading) and production method thereof.
2. Description of the Related Art
In the field of optical memory for optically recording/reading information, the following two methods have been proposed in recent years for increasing the recording density of disks used as a recording media.
(1) Shorten the wavelength of the light used for recording/reading.
(2) Increase the aperture number NA of the object lens converging the light on the disk.
Among these methods, method (1) requires the development of a semiconductor laser or the like for emitting light of a shorter wavelength to reduce the wavelength of the light itself. The development of such a semiconductor laser is not yet a simple matter, however.
Focusing on method (2), there have been various proposals for emitting the light used for recording/reading on a disk using a solid immersion lens. This method is based on the principle of the liquid immersion microscope (i.e., improved resolution microscope via liquid immersion method). That is, this method utilizes the principle of the microscope obtaining a resolution at less than 100 nm in visible light. Prior applications of related art include U.S. Pat. Nos. 5,004,307 and 5,764,613.
Solid immersion lenses heretofore experimentally produced include the hemispherical solid immersion lens
41
shown in
FIG. 14
, and the hyperhemispherical solid immersion lens
42
having a cap piece remaining under the hemisphere as shown in FIG.
15
. In
FIGS. 14 and 15
, reference number
43
refers to a normal objective (condenser) lens, and reference number
44
refers to a recording medium (disk).
In the hemispherical solid immersion lens
41
, the light beam LB enters perpendicular to the concave surface
41
a,
and is converged by the plane surface
41
b
of the center area. When the refractive index of the solid immersion lens
41
is designated n, the wavelength within the lens
41
becomes 1
, and as a result the aperture number NA of the condenser lens
43
becomes a multiple of n. The spot size of the light beam LB is reduced to 1
, and the resolution becomes a multiple of n. That is, when the aperture number NA of the condenser lens
43
is 0.5, the refractive index n of the solid immersion lens
41
is 1.8, and the wavelength &lgr; of the light beam LB is 780 nm, the spot size S is determined by equation (1) below; i.e., the spot size S is 430 nm.
S=&lgr;/
(2
sin &thgr;
)  (1)
In the hyperhemispherical solid immersion lens
42
, the effective optical path is greater than the radius. In this instance, the spot size S of the light beam LB is determined by equation (2) below; i.e., the spot size S is 240 nm.
S=&lgr;/
(2
n sin &thgr;
)  (2)
In this way, a condensed spot having a wavelength less than the used light can be obtained by using the solid immersion lenses
41
and
42
. Using these methods, the spacing (air gap) b between the recording medium
44
and the solid immersion lens
41
and
42
must be sufficiently reduced so as to be maintained at approximately 100 nm or less. In order to control and maintain this air gap, it has been proposed to install the solid immersion lens on a floating slider applying the art of the magnetic hard disk. Prior art citations include U.S. Pat. Nos. 5,125,750, 5,774,281 and 5,786,947, and prior art citations using other than a floating slider include Japanese Laid-Open Application No. 8-212579.
The three issues below must be resolved to practicalize a high density memory using a solid immersion lens.
(1) Lens Holder Mechanism
In the conventional hemispherical and hyperhemispherical solid immersion lenses
41
and
42
, it is difficult to prevent inclination (0 degree) of the plane surface
41
b
relative to the reference surface
49
of the support fixture
47
because there is no fixed reference to the support fixture
47
on the convex surface
41
a,
as shown in FIG.
16
. When the plane surface
41
b
has a standard inclination, the fixed part of the lens disadvantageously protrudes to the object (medium) side of the lens, such that the required air gap cannot be ensured.
(2) Installation on the Slider
When installing a solid immersion lens on a floating slider for use as the recording head of a high density memory, the lens must be compact so as to have a diameter of 2 mm or less to reduce the head weight, and the lens support fixture must be provided with an air-bearing surface for floating. In this case, inclination between the support fixture and the lens plane surface must be prevented to maintain a sufficiently precise position of the solid immersion lens relative to the recording medium.
(3) Manufacturing Cost
Conventionally, hemispherical and hyperhemispherical solid immersion lenses are manufactured by grinding a glass member into a spherical shape to obtain a ball lens, then sectioning or grinding the ball lens. Such a production method, however, entails a complex process which raises the cost and is presently only in the experimental stage which does not result in a usable product.
SUMMARY OF THE INVENTION
An object of the present invention is to provide an improved solid immersion lens and production method thereof.
Another object of the present invention is to provide a solid immersion lens capable of being mounted so as to hold a predetermined position without inclination relative to a support fixture, and further capable of being mounted on a floating slider so as to sufficiently reduce the air gap with an object (medium).
Still another object of the present invention is to provide a production method capable of mass production of a solid immersion lens via a simple process at low cost.
These objects are attained by a first solid immersion lens of the present invention provided with a hemispherical shape or hyperhemispherical shape having a convex surface on the light entering side and an approximately plane surface on the light exiting side, wherein the convex surface comprises a positioning surface and a surface forming an effective optical path part. In this first solid immersion lens, it is desirable that the positioning surface is a curved surface having the opposite sign of the curvature of the surface forming the effective optical path part. Furthermore, includes a radius of curvature of infinity, i.e., a circular conical shape extending the tangent line of the radius at the effective optical path part.
A second solid immersion lens of the present invention provided with a hemispherical shape or hyperhemispherical shape having a convex surface on the light entering side and an approximately plane surface on the light exiting side, wherein a collar part having a positioning surface is provided outside the effective optical path part of the convex surface.
In the first and second solid immersion lenses, the positioning surface formed outside the effective optical path part of the convex surface comprises a fixed reference for the lens support fixture, and allows the solid immersion lens to be supported with excellent positioning (i.e., without inclination). Furthermore, the a sufficiently small air gap is ensured without the fixed part of the lens protruding on the object (medium) side.
Even when the lens is compact, the surface area of the approximate plane surface on the exit side is enlarged by providing the positioning surface, such that when the solid immersion lens is installed on a floating slider, the air-bearing surface is enlarged when floating. In addition to effectively preventing inclination, there is improved positioning accuracy of the solid immersion lens relative to the object (medium).
In the

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