Optical device and imaging apparatus using the same

Information

  • Patent Grant
  • 6219483
  • Patent Number
    6,219,483
  • Date Filed
    Friday, January 28, 2000
    24 years ago
  • Date Issued
    Tuesday, April 17, 2001
    23 years ago
Abstract
An optical device 10 comprises an input optical member 11, in which a plurality of optical fibers 14 are arranged parallel to each other and integrally formed, having an entrance surface 11a and an exit surface 11b which intersect an optical axis at respective angles of 90° and 20°; and an output optical member 12, in which a plurality of optical fibers are arranged parallel to each other and integrally formed, having an entrance surface 12a intersecting an optical axis at an angle of 55° and an exit surface 12b parallel to the entrance surface 12a. Here, the exit surface 11b of the input optical member 11 and the entrance surface 12a of the output optical member 12 are in contact with each other, whereas the angle formed between the optical axis of the input optical member 11 and the optical axis of the output optical member 12 is an angle of 35° which is the difference between 55° and 20° mentioned above.
Description




TECHNICAL FIELD




The present invention relates to an optical device and an imaging apparatus using the same.




BACKGROUND ART




Known as an optical member for transmitting an optical image is one in which a plurality of optical fibers are arranged parallel to each other and integrally formed. Also, an optical device in which one of end faces of the above-mentioned optical member is cut perpendicular to the optical axis, whereas the other end face is cut obliquely with respect to the optical axis, is disclosed, for example, in Japanese Patent Application Laid-Open No. SHO 60-194429. Such an optical device can transmit an optical image incident on the above-mentioned one end face while enlarging (or reducing) it to a given magnification in a specific direction.




DISCLOSURE OF THE INVENTION




However, the above-mentioned optical device has been problematic in that, if the angle formed between the above-mentioned other end face and the optical axis is made smaller in order to enhance the magnification, the output image emitted from the other end face becomes unclear. Therefore, it is an object of the present invention to provide an optical device which can yield a vivid output image.




For achieving the above-mentioned object, the optical device of the present invention comprises a first optical member, composed of a plurality of optical fibers arranged parallel to each other and integrally formed, having a first end face and a second end face which intersect an optical axis at respective angles of α


1





1


; and a second optical member, composed of a plurality of optical fibers arranged parallel to each other and integrally formed, having a third end face intersecting an optical axis at an angle of α


2


and a fourth end face parallel to the third end face; wherein the second end face and the third end face are in contact with each other; wherein the above-mentioned β


1


is smaller than the above-mentioned α


2


; and wherein an angle θ


1


formed between the optical axis of the first optical member and the optical axis of the second optical member is an angle of difference between β


1


and α


2


.




Since the second optical member having the configuration mentioned above is disposed in contact with the second end face of the first optical member, the direction of emission of the optical image emitted from the fourth end face of the second optical member approximates the normal direction of the fourth end face. As a consequence, even when the angle formed between the second end face and the optical axis is quite small, a vivid optical image can be obtained from the fourth end face.











BRIEF DESCRIPTION OF THE DRAWINGS





FIG. 1

is a perspective view of an optical device;





FIG. 2

is a schematic sectional view of the optical device;





FIG. 3

is a view for explaining the use of the optical device;





FIG. 4

is an explanatory view showing light propagation within the optical device;





FIG. 5

is an explanatory view showing light propagation within the optical device;





FIG. 6

is an explanatory view showing light propagation within the optical device;





FIG. 7

is an explanatory view showing light propagation within the optical device;





FIG. 8

is an explanatory view showing light propagation within the optical device;





FIG. 9

is an explanatory view showing light propagation within the optical device;





FIG. 10

is an explanatory view showing light propagation within the optical device;





FIG. 11

is a configurational view of an imaging apparatus; and





FIG. 12

is a configurational view of an imaging apparatus.











BEST MODE FOR CARRYING OUT THE INVENTION




(1) Optical Device According to Embodiment of Present Invention




An optical device in accordance with an embodiment of the present invention will be explained with reference to drawings. First, the configuration of the optical device in accordance with this embodiment will be explained. As shown in

FIG. 1

, the optical device


10


comprises an input optical member


11


and an output optical member


12


.




Each of the input optical member


11


and the output optical member


12


comprises a plurality of optical fibers which are arranged parallel to each other and integrally formed. Each optical fiber


14


has a diameter on the order of 3 to 10 μm, whereas the refractive index of the core


14




a


, the refractive index of the cladding


14




b


, and the numerical aperture in the optical fiber


14


constituting each optical member are as shown in Table 1.
















TABLE 1











Core




Cladding








Refractive




Refractive




Numerical







Index




Index




Aperture





























Input Optical




1.82




1.495




1.0







Member







Output Optical




1.82




1.495




1.0







Member















Also, gaps among the individual optical fibers


14


constituting the input optical member


11


and output optical member


12


are filled with a light-absorbing material


15


.




The input optical member


11


has an entrance surface


11




a


which is cut with respect to the optical axis (the optical axis of optical fibers constituting the optical member) at an angle of 90° and an exit surface


11




b


which is obliquely cut with respect to the optical axis at an angle of 20°, whereas both of the entrance surface


11




a


and the exit surface


11




b


are optically ground.




The output optical member


12


has an entrance surface


12




a


which is cut with respect to the optical axis at an angle of 55° and an exit surface


12




b


which is parallel to the entrance surface


12




a


, whereas both of the entrance surface


12




a


and the exit surface


12




b


are optically ground. Here, the angle formed between the optical axis of the input optical member


11


and its exit surface


11




b


is smaller than the angle formed between the optical axis of the output optical member


12


and its entrance surface


12




a.






The exit surface


11




b


of the input optical member


11


and the entrance surface


12




a


of the output optical member


12


are in contact with each other. As a consequence, an optical image incident on the entrance surface


11




a


of the input optical member


11


is transmitted to the exit surface


12




b


of the output optical member


12


.




Here, both of the entrance surface


11




a


and exit surface


11




b


of the input optical member


11


and both of the entrance surface


12




a


and exit surface


12




b


of the output optical member


12


are perpendicular to the xz plane of

FIG. 1

, whereas the optical axes of the optical fibers


14


constituting the individual optical members are parallel to the xz plane of FIG.


1


.





FIG. 2

is a schematic sectional view of the optical device taken along a plane parallel to the xz plane. Here,

FIG. 2

is a schematic sectional view showing the relationship between the respective optical axes of the optical members, whereas each optical member is a bundle of several thousands of optical fibers in practice. Here, the angle formed between the optical axis of the input optical member


11


and the optical axis of the output optical member


12


is an angle of 35° which is the difference between the angle of 55° formed between the optical axis of the output optical member


12


and its entrance surface


12




a


and the angle of 20° formed between the optical axis of the input optical member


11


and its exit surface


11




b.






For example, the optical device


10


is arranged as shown in

FIG. 3

when it is used for enlarging and viewing a predetermined image pattern. Namely, a light-shielding plate


4


or the like having a predetermined pattern is irradiated with light from an LED


5


or the like, so that an optical image forming the predetermined input pattern is incident on the entrance surface


11




a


of the input optical member


11


. The optical image is transmitted through the input optical member


11


and the output optical member


12


, and then is emitted from the exit surface


12




b


of the output optical member


12


as being enlarged. Therefore, as shown in

FIG. 3

, an output image enlarging the input pattern can be observed when the exit surface


12




b


of the output optical member


12


is viewed in a direction


6


substantially perpendicular to the exit surface


12




b


of the output optical member


12


.




Operations of the optical device in accordance with this embodiment will now be explained. First, a case where the light incident on the entrance surface


11




a


of the input optical member


11


from the air propagates while being refracted and reflected by the core/cladding interface of the optical fibers


14


constituting the input optical member


11


as shown in

FIG. 4

will be considered. Here, letting n


11


and n


12


be the respective refractive indices of the core


14




a


and cladding


14




b


of the optical fibers


14


constituting the input optical member


11


, and ε


1


be the angle of incidence of light incident on the cladding


14




b


from its core


14




a


, only the light satisfying a total reflection condition at the core/cladding interface






sin ε


1


>n


12


/n


11


  (1)






propagates through the optical fibers


14


constituting the input optical member


11


.




In the optical device


10


in accordance with this embodiment, since n


11


=1.82, and n


12


=1.495, light in which ε


1


becomes 55° or greater propagates through the optical fibers


14


constituting the input optical member


11


. Namely, as indicated by the hatched area of

FIG. 4

, only the light forming an angle of 35° or less with the optical axis would propagate through the optical fibers


14


constituting the input optical member


11


.




Also, since the entrance surface


11




a


of the input optical member


11


is perpendicular to the xz plane of FIG.


1


and the optical axis of the input optical member


11


, whereas the exit surface


11




b


of the input optical member


11


is perpendicular to the xz plane and forms an angle of 20° with the optical axis of the input optical member


11


, the input optical member


11


acts to enlarge the optical image incident on the entrance surface


11




a


to about 2.92 times (1/sin20°) in the a-axis direction of FIG.


1


and output thus enlarged optical image.




A case where the light emitted from the exit surface


11




b


of the input optical member


11


propagates while being refracted and reflected by the core/cladding interface of the optical fibers


14


constituting the output optical member


12


will now be considered.




First, for comparison, a case where the output optical member


12


is not provided will be considered. In the case without the output optical member


12


, the light having reached the exit surface


11




b


of the input optical member


11


advances as follows. Namely, letting n


11


be the refractive index of the core


14




a


of the optical fiber


14


constituting the input optical member


11


, and n


0


be the refractive index of the air, the critical angle ζ


max


in the case where the light is emitted from the core


14




a


of the optical fiber


14


into the air satisfies






n


0


sin90°=n


11


sin ζ


max


.  (2)






Here, if n


11


=1.82, and n


0


=1.00, then the critical angle ζ


max


will be about 33.3°. In the input optical member


11


employed in this embodiment, on the other hand, only the light forming an angle of 35° or less with the optical axis propagates through the optical fibers


14


as explained above. Therefore, the light having propagated through the optical fibers


14


, such as that indicated by the hatched area of

FIG. 5

, is totally reflected by the exit surface


11




b


of the input optical member


11


and would not be emitted to the outside. As a result, no output image but a quite dark image would be formed at the exit surface


11




b


of the input optical member


11


.




In the case where the output optical member


12


is provided as in the optical device


10


in accordance with this embodiment, by contrast, the light incident on the entrance surface


12




a


of the output optical member


12


from the exit surface


11




b


of the input optical member


11


behaves in various manners according to its angle of incidence. This will be explained in detail in the following.




While only the light forming an angle of 35° or less with the optical axis propagates through the optical fibers


14


in the input optical member


11


as explained above, the light forming an angle of 35° with the optical axis of the input optical member


11


and having entered the output optical member


12


at an incident angle of 35° advances straight, as shown in

FIG. 6

, without being refracted by the interface between the input optical member


11


and the output optical member


12


since the refractive index n


21


of the core


14




a


of the optical fiber


14


constituting the output optical member


12


is identical to the refractive index n


11


of the core


14




a


of the optical fiber


14


constituting the input optical member


11


. Further, since the critical angle at which light is emitted from the exit surface


12




b


of the output optical member


12


into the air is 33.3° as with the above-mentioned ζ


max


, the light having advanced through the core


14




a


of the optical fiber


14


constituting the output optical member


12


is totally reflected by the exit surface


12




b


of the output optical member


12


and would not be emitted to the outside.




Similarly, the light forming an angle of 33.3° with the optical axis of the input optical member


11


and having entered the output optical member


12


at an incident angle of 36.7° as shown in

FIG. 7

, the light incident on the output optical member


12


in parallel with the optical axis of the input optical member


11


and reflected by the core/cladding interface of the optical fiber


14


constituting the output optical member


12


by an even number of times as shown in

FIG. 8

, and the like are totally reflected by the exit surface


12




b


of the output optical member


12


and would not be emitted to the outside.




Also, the light forming an angle of 10° with the optical axis of the input optical member


11


and having entered the output optical member


12


at an incident angle of 80° as shown in FIG.


9


and the like fail to satisfy the total reflection condition at the core/cladding interface of the optical fiber


14


constituting the output optical member


12


, and would attenuate and disappear.




By contrast, the light incident on the output optical member


12


in parallel with the optical axis of the input optical member


11


and reflected by the core/cladding interface of the optical fiber


14


constituting the output optical member


12


by an odd number of times as shown in FIG.


10


and the like are emitted in the normal direction of the exit surface


12




b


of the output optical member


12


. More specifically, of the light forming an angle of 35° or less with the optical axis and having propagated through the optical fiber


14


constituting the input optical member


11


, the part incident on the output optical member


12


at an incident angle of 36.7° to 70° and reflected by the core/cladding interface of the optical fiber


14


constituting the output optical member


12


by an odd number of times would be emitted from the exit surface


12




b


of the output optical member


12


at an emission angle within the range of 0° to 90°.




Effects of the optical device in accordance with this embodiment will now be explained. Since the output optical member


12


having the configuration mentioned above is disposed in contact with the exit surface


11




b


of the input optical member


11


, the direction of emission of the optical image emitted from the exit surface


12




b


of the output optical member


12


can approximate the normal direction of the exit surface


12




b


of the output optical member


12


. As a result, even when the angle formed between the exit surface


11




b


of the input optical member


11


and its optical axis is made quite small in order to enhance the magnification of the incident image, a vivid enlarged image can be obtained from the exit surface


12




b


of the output optical member


12


.




In the optical device


10


in accordance with this embodiment, various modifications can be considered concerning the angles formed between the optical axis of the input optical member


11


and its entrance surface


11




a


and exit surface


11




b


, and the angles formed between the optical axis of the output optical member


12


and its entrance surface


12




a


and exit surface


12




b.






A given magnification can be obtained when the angles formed between the optical axis of the input optical member


11


and its entrance surface


11




a


and exit surface


11




b


are adjusted as appropriate.




Table 2 shows the range of incident angle ζ onto the entrance surface


12




a


in which light is emitted from the exit surface


12




b


of the output optical member


12


to the outside, the extent Δζ of the range of incident angle ζ onto the entrance surface


12




a


in which light is emitted from the exit surface


12




b


of the output optical member


12


to the outside, the range of emission angle ζ of light emitted from the exit surface


12




b


of the output optical member


12


to the outside, and the extent Δζ of the range of light emitted from the exit surface


12




b


of the output optical member


12


to the outside in the case where the angle α formed between the optical axis of the output optical member


12


and its entrance surface


12




a


(=the angle formed between the optical axis and the exit surface


12




b


) is varied.
















TABLE 2









α




ζ




Δζ




ξ




Δξ











40°




66.7° ˜ 85.0°




18.3°




28.1° ˜ 90.0°




61.9°






55°




36.7° ˜ 70.0°




33.3°




 0.0° ˜ 90.0°




90.0°






60°




35.0° ˜ 65.0°




30.0°




 0.0° ˜ 50.3°




50.3°














From Table 2, it is seen that, when the angle α formed between the optical axis of the output optical member


12


and its entrance surface


12




a


is smaller or greater than 55°, then Δζ decreases, whereby the transmission efficiency deteriorates. When the angle α formed between the optical axis of the output optical member


12


and its entrance surface


12




a


is enhanced, however, a greater distribution of the emission direction of light emitted from the exit surface


12




b


of the output optical member


12


would lie in the normal direction of the exit surface


12




b


of the output optical member


12


. Also, when the angle α formed between the optical axis of the output optical member


12


and its entrance surface


12




a


is 90°, then all the light incident on the output optical member


12


is totally reflected by the exit surface


12




b


of the output optical member


12


and would not be emitted to the outside.




When an optical image is inputted from the exit surface


12




b


of the output optical member


12


, the optical device in accordance with this embodiment can also be used as an optical device for reducing and outputting the incident image.




(2) Imaging Apparatus Using Optical Device According to Embodiment of Present Invention




An imaging apparatus using the optical device in accordance with the above-mentioned embodiment will now be explained with reference to a drawing. First, the configuration of the imaging apparatus using the optical device in accordance with the above-mentioned embodiment will be explained. As shown in

FIG. 11

, the imaging apparatus


100


comprises the above-mentioned optical device


10


(i.e., optical device


10


comprising the input optical member


11


and the output optical member


12


), and a CCD


101


disposed in contact with the exit surface


12




b


of the above-mentioned output optical member


12


. Here, more specifically, the exit surface


12




b


of the output optical member


12


is in contact with the light-receiving surface of the CCD


101


.




Further, all the surfaces (hereinafter referred to as side faces) of the input optical member


11


excluding the entrance surface


11




a


and exit surface


11




b


and the side faces of the output optical member


12


are provided with a light-shielding material.




The side faces of each optical member can be provided with the light-shielding material by a method in which the entrance surface and exit surface of each optical member are masked and then a light-shielding agent (e.g., black paint) is sprayed on the side faces, a method in which the light-shielding agent is applied to the side faces with a brush, a method in which the optical member is immersed into a vessel filled with the light-shielding agent, or the like.




Operations and effects of the imaging unit using the optical device in accordance with the above-mentioned embodiment will now be explained. Since the imaging apparatus


100


comprises the above-mentioned optical device


10


, the optical image incident on the entrance surface


11




a


of the input optical member


11


can efficiently be enlarged and transmitted to the exit surface


12




b


of the output optical member


12


, so as to be outputted from the exit surface


12




b


of the output optical member


12


as a vivid optical image.




Also, since the CCD


101


is disposed in contact with the exit surface


12




b


of the output optical member


12


, the imaging apparatus


100


can capture the optical image transmitted to the exit surface


12




b


of the output optical member


12


.




Further, in the imaging unit


100


, since the light-shielding material is disposed on the side faces of each optical member, light is prevented from entering each optical member from the side faces thereof, whereby the S/N ratio can be enhanced.




As a result, the imaging unit


100


can capture a clear, high-contrast, high-resolution, enlarged image.




Also, the CCD


101


may be disposed in contact with the entrance surface


11




a


of the input optical member


11


constituting the optical device


10


, so as to construct an imaging apparatus


110


as shown in FIG.


12


.




Further, though the CCD


100


is disposed in contact with the optical device


10


in the above-mentioned imaging apparatus


100


or


110


, the output image outputted from the optical device


10


may be made incident on the CCD


101


by way of a lens or the like.




INDUSTRIAL APPLICABILITY




As mentioned above, the optical device of the present invention can be used in imaging apparatus, for example.



Claims
  • 1. An optical device comprising:a first optical member, composed of a plurality of optical fibers arranged parallel to each other and integrally formed, having a first end face and a second end face which intersect an optical axis at respective angles of α1,β1; and a second optical member, composed of a plurality of optical fibers arranged parallel to each other and integrally formed, having a third end face intersecting an optical axis at an angle of α2 and a fourth end face parallel to said third end face; wherein said second end face and said third end face are in contact with each other; wherein said β1 is smaller than said α2; and wherein an angle θ1 formed between the optical axis of said first optical member and the optical axis of said second optical member is an angle of difference between β1 and α2.
  • 2. An optical device according to claim 1, wherein said α1 is 90°.
  • 3. An optical device according to claim 1, wherein said α2 is an acute angle.
  • 4. An imaging apparatus comprising:the optical device according to claim 1; and an imaging device disposed on said fourth end face side.
  • 5. An imaging apparatus comprising:the optical device according to claim 1; and an imaging device disposed on said first end face side.
Priority Claims (1)
Number Date Country Kind
9-204560 Jul 1997 JP
PCT Information
Filing Document Filing Date Country Kind 102e Date 371c Date
PCT/JP98/03395 WO 00 1/28/2000 1/28/2000
Publishing Document Publishing Date Country Kind
WO99/06863 2/11/1999 WO A
US Referenced Citations (3)
Number Name Date Kind
3043910 Hicks, Jr. Jul 1962
5940565 Sugawara Aug 1999
6038360 Sugawara Aug 1999
Foreign Referenced Citations (2)
Number Date Country
60-194429 Oct 1985 JP
8-286048 Nov 1996 JP