FIELD OF THE INVENTION
[0001] The present invention relates to a target system according to the preamble of claim
1.
BACKGROUND OF THE INVENTION
[0002] There exist today weapon effect simulation systems for use in combat training and/or
shooting practice and which are arranged to simulate the effects of a specific weapon
type. The weapons in one such weapon simulation system are provided with a simulation
unit comprising a laser, a receiver for laser radiation and a hit evaluation unit,
and the targets are provided with retro-reflecting prisms. The laser is arranged to
emit a simulation beam simulating firing of the weapon. The retro-reflecting prism(s)
of the targets is arranged to retro-reflect the simulation beam. The receiver of the
simulation unit is arranged to receive the retro-reflected simulation beam and the
hit evaluation unit is arranged to perform hit evaluation based on the received simulation
beam.
[0003] However, there are some problems associated to use of the above described weapon
effect simulation system. The retro-reflecting prisms tend to give rise to exposing
reflections of incident ambient light and laser radiation of wavelengths other than
the simulation wavelength. This is especially not desired in combat training, as the
training is intended to be as realistic as possible. Further, if a laser range measurement
unit is used by any real or simulated weapon system, there is a risk that the laser
range measurement unit might be damaged if the emitted laser range finder beam intercepts
a target retro-reflector unit, since the laser beam of the range finder is reflected
with very little damping.
[0004] US 6 139 323 relates to an optical weapon effect simulation method for training of
soldiers at least at two weapons, wherein each weapon is equipped as an attacking
system as well as a target system. The attacking system includes a laser pulse transmitter
arranged to transmit laser signals of at least two different wavelengths and a measurement
unit arranged to detect signal reflections. The target system is provided with at
least one retro-reflector with an integrated selective filter, an optical receiver
with a selective filter and evaluation electronics. The selective filter is intended
to ensure that only laser pulses of a defined wavelength are reflected/accepted by
the target system. The attacking system then can identify target type based upon the
wavelength of the laser signal received from the target system. However, the retro-reflectors
as described in US 6 139 323 have the drawback of unwanted specular reflections for
wavelengths other than the used simulation wavelength. Thus, the above described problems
with exposing and damaging reflections is not solved.
SUMMARY OF THE INVENTION
[0005] One object of the present invention is to avoid total internal reflection for a useful
range of incidence angles and inhibit unwanted for wavelengths other than the simulation
wavelength, thus solving the problems described above.
[0006] This has been achieved by means of a target system in accordance with claim 1 comprising
a retro-reflecting prism having at least three back surfaces arranged to an incident
simulation beam and wherein at least one of the back surfaces comprises a first, selectively
reflecting layer arranged to reflect a simulation beam of a predetermined optical
wavelength range and being substantially transparent to optical wavelengths outside
said range, wherein a second layer is mounted on the first layer, said second layer
being arranged to receive beams transmitted through said first layer and said second
layer being of a material having an index of refraction sufficiently high to avoid
total internal reflection between said first and second layer within a predetermined
range of incident angles.
[0007] One advantage of the retro-reflecting prism arrangement is that it does no give rise
to internal reflections within the predetermined range of incidence angles and thus
allow for specular reflections only for the simulation wavelength.
[0008] The basic function of the retro-reflecting prism is known in the art. In brief, a
retro-reflecting prism has three reflecting back surfaces, meeting at right angles
to each other, thus making up a right angle corner. Parallel incident light entering
the prism will be reflected three times against these surfaces (once at each surface)
and return in the opposite direction and parallel to the incidence angle, for a useful
range of incidence angles.
[0009] The first layer is preferably coated on the back surface(s). The first layer ensures
that back surface(s) reflects only light beams having a predetermined wavelength or
a wavelength lying within a predetermined wavelength range. The first layer is therefore
arranged to reflect beams having said predetermined wavelength or lying within said
wavelength range. Other wavelengths are transmitted through the first layer.
[0010] The second layer is tightly mounted to the first layer so that no air gap is present
between the layers. Thereby it is secured that the light beams exiting the first layer
enters the second layer and thus are prevented from being reflected by the air back
into the first layer. If the index of refraction of the second layer is sufficiently
close to the index of refraction of the first layer, preferably substantially the
same as the index of refraction of the first layer, a retro-reflecting prism arrangement
is provided which reflects almost no light beams outside said predetermined wavelength/wavelength
range.
[0011] In accordance with one embodiment of the invention, an intermediate layer is interposed
between the first layer and the second layer. The intermediate layer is for example
an adhesive layer. The three layers are, as described above, tightly mounted to each
other so that no air gap is present between the layers. Further, the index of refraction
of the intermediate layer is preferably substantially equal to the index of refraction
of the first layer.
[0012] If the first and second layers are arranged on all back surfaces of the prism arrangement,
it is ensured that the prism arrangement will not reflect beams other than those of
the predetermined wavelength or wavelength range even when the light beams are incident
from angles outside the predetermined range of incidence angles and only hit one or
some of the back surfaces and thus are not properly retro-reflected. Therefore, the
retro-reflecting prism arrangement causes almost no reflections from ambient light.
[0013] In accordance with one embodiment of the invention, the second layer is arranged
to absorb the transmitted wavelengths.
[0014] In accordance with another embodiment of the invention, the second layer is diffuse
reflecting and therefore has a diffuse reflecting back surface. One advantage of the
diffuse reflecting back surface is that it absorbs little heat, whereby the temperature
gradient of the back surface mirror is small, which results in preserved high accuracy
of the retro-reflecting prism.
BRIEF DESCRIPTION OF THE DRAWINGS
[0015]
Fig 1 shows a known retro-reflecting prism
Fig 2 shows a beam incident on the retro-reflecting prism of fig 1 and specularily
reflected at the back surfaces of the prism so that it is retro-reflected back from
the prism.
Fig 3 shows a schematic side view of a retro-reflected beam
Fig 4 shows a schematic view of a selectively retro-reflected beam according to one
embodiment of the invention
Fig 5 shows a schematic view of a selectively retro-reflected beam according to a
second embodiment of the invention.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0016] In fig 1, a solid retro-reflecting prism 1 is viewed from the front, and consisting
of a corner cube. It has a front surface 9 and three back surfaces 2 and makes up
a solid volume. As shown in figure 2, a beam 3 incident on the retro-reflecting prism
will be specularly reflected in each of the three back surfaces 2 so that the beam
is retro-reflected back 4 from the prism. The direction of the retro-reflected beam
4 is shown schematically in figure 3.
[0017] In the technique according to the prior art, there need not be any coating on the
back surfaces 2 of the prism since the refraction index difference between the material
of the prism and air is sufficient enough to give total internal reflection for a
useful range of incidence angles. The back surfaces could be metal coated to obtain
a wavelength dependent reflection in which case the not reflected part of the beam
would be absorbed in the metal layer. However, all practical metal layers usable at
the simulation wavelength, which is typically about 900 nm, will give a rather high
reflectance also within the visible spectrum, thus giving rise to unwanted reflections
from ambient light. One suggestion could be to apply a wavelength selective reflecting
coating, for example a multi-layer dielectric coating, on at least one and preferably
on all three of the back surfaces 2 of the prism 1. However, this would not work on
its own since, in the same manner as for a non-coated prism, there will be total internal
reflection between the last surface of the reflecting coating and air. The total internal
reflection is not wavelength dependent, but all wavelengths within a very wide spectrum
would be reflected in spite of the wavelength selective coating.
[0018] Figure 4 shows a first embodiment of this invention, where the back surfaces of the
retro-reflecting prism are coated with a wavelength selective reflecting coating 6
and a material 7 of sufficiently high refractive index is glued to the back surfaces
on top of the coating. Thus, total internal reflection at the last surface of the
reflection coating is avoided for a range of incidence angles and the wavelengths
not reflected will be transmitted into the glued on material. This is shown in figure
4 where a part of the incident light within a selective wavelength range is retro-reflected
4 and the other part, outside the selected wavelenght range, is transmitted 5. In
figure 4 the function is only shown schematically for just one back surface. At least
one and preferably all three back surfaces of the retro-reflecting prism should be
configured in this way. The glued on material is made absorbing for the wavelengths
transmitted into said material. The absorbing material could for example be a colour
filter, an IR high-pass filter or an IR band-pass filter. In this embodiment the retro-reflecting
prism would look black.
[0019] In fig 5, the glued on material is made to diffusely reflect the light transmitted
into said material. (As light we include wavelengths from UV to IR.) Figure 5 shows
a schematic view of the function of this embodiment, where a part of the incident
light within a selected wavelength range is retro-reflected 4 and the other part,
outside the selected wavelenght range, is diffusely reflected 8. Said diffusely reflecting
material could for example be an opal glass or plastic, or a glass or plastic plate
having its back surface frosted (either by etching or grounding or some other process),
the material having an appropriate index of refraction according to this invention.
In this embodiment the retro-reflecting prism would look matt white.
[0020] In an extended example, the glued on material is made to diffusely reflect the light
transmitted into said material, as is described in relation to fig 5. Further, a wavelength
selective reflecting layer is put on top of the diffusing material. This could for
example be some kind of paint. In this embodiment the retro-reflecting prism would
look matt and have the same colour as the reflecting layer. This embodiment could
be used to camouflage the retro-reflecting prism.
[0021] It is assumed that an appropriate anti-reflection coating is used for the front surface
9 of the prism.
1. A target system for a weapon effect simulation system, said target system comprising
a retro-reflecting prism having at least three back surfaces arranged to retro-reflect
an incident simulation beam and wherein at least one of the back surfaces comprises
a first, selectively reflecting layer arranged to reflect a simulation beam of a predetermined
optical wavelength range and being substantially transparent to optical wavelengths
outside said range,
characterized in that a second layer is mounted on the first layer, said second layer being arranged to
receive beams transmitted through said first layer and said second layer being of
a material having an index of refraction sufficiently high to avoid total internal
reflection between said first and second layer within a predetermined range of incident
angles.
2. A target system according to claim 1,characterized in that the second layer is arranged to absorb at least parts of the transmitted beam.
3. A target system according to claim 1, characterized in that the second layer is arranged to diffuse reflect at least parts of the transmitted
beam.
4. A target system according to claim 1,characterized in that the second layer comprises an IR high-pass filter.
5. A target system according to claim 1, characterized in that the second layer comprises an IR band-pass filter.
6. A target system according to claim 1, characterized in that the index of refraction of the second layer is substantially equal to the index of
refraction of the first layer.
7. A target system according to claim 1, characterized in that the first layer comprises a multi-layer dielectric coating.
8. A target system according to claim 1, characterized in that an adhesive layer is interposed between the first and second layer.
9. A target system according to claim 8, characterized in that the index of refraction of the adhesive layer is substantially equal to the index
of refraction of the first layer.
10. A target system according to claim 1, characterized in that a third, wavelength selective reflective layer is mounted on top of the second layer.
11. A retro-reflecting prism having at least three back surfaces arranged so as to retro-reflect
an incident optical beam and wherein at least one of the back surfaces comprises a
first, selectively reflecting layer arranged to reflect an optical beam of a predetermined
optical wavelength range and being substantially transparent to optical wavelengths
outside said range,
characterized in that a second layer is mounted on the first layer, said second layer being arranged to
receive optical beams transmitted through said first layer and said second layer being
of a material having an index of refraction sufficiently high to avoid total internal
reflection between said first and second layer within a predetermined range of incident
angles.