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Description  |
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BACKGROUND OF THE INVENTION
The invention relates to a device and a method for aligning optical beams.
In particular, this invention relates to a general field of aligning
optical beams for characterizing, testing, evaluating and applying linear
and nonlinear optical materials and devices, electronic materials and
devices, and mechanical materials and devices. Beam alignment is achieved
using a device having either an elliptically curved or a parabolically
curved mirror arranged in a reflected beam path between a rotatable mirror
and the desired target. Combinations of both elliptical and parabolic
mirrors may be used to solve a variety of beam steering and/or beam
alignment problems.
Optical beams are typically steered by reflecting light from one or more
moveable mirrors. Mirrors are moved or rotated with respect to the
longitudinal axis of the optical beam path to produce a reflected or
steered beam. The reflected beam is placed on a target material in
accordance with the angle of rotation of the rotatable mirror. The
rotatable mirror, often called a steering mirror, is typically the sole
means for steering the reflected beam upon the target material. However,
the steering mirror can be combined with a second mirror to direct the
reflected beam onto the target material, wherein the second mirror is
disposed within the reflected beam path and between the steering mirror
and the target material. The second mirror, like the steering mirror, can
be curved and can rotate independently or simultaneously with the steering
mirror to optimally direct the reflected beam.
Merely reflecting optical beams by using a combination of rotatable mirrors
and secondary mirrors does not provide adequate results in specific
applications. Often it is desirable to place the reflected beam at a fixed
position and vary, with a high degree of precision, the angle of incidence
upon the target material. For ultrashort pulse non-linear optics
experiments, for example, one must conserve momentum (phase matching) in
addition to precisely controlling the temporal and spatial overlap of two
or more beams upon the target material. Momentum is conserved by placing
the various beams at the same position upon the target but at varying
angles of incidence. Accordingly, a real need exists for an improved
steering device and method which is also suitable for non-linear
applications which can place an ultrashort optical beam at a precise point
on a target but at varying angles of incidence.
In addition to being able to vary the angle of incidence upon a fixed
target location, it is also highly desirable to direct a reflected beam at
varying locations, but at a fixed angle of incidence. The reflected beam
could be steered to arrive at different positions upon the target material
while maintaining the same angle of incidence at each location. Like the
variable angle, fixed position application, conventional steering
techniques show difficulty in placing beams at variable positions upon a
target while maintaining at fixed angle of incidence. In order to place
reflected ultrashort beams evenly across a target, a real need exists for
an improved steering device and method suitable for material and device
characterization applications which can place an ultrashort optical beam
at various points on a target while maintaining a fixed angle of
incidence.
SUMMARY OF THE INVENTION
Accordingly, the present invention overcomes the prior art by providing an
improved beam steering device and method, wherein a reflected optical beam
can be placed upon a target at either a variable angle, fixed position, or
a variable position, fixed angle. The improved device used for changing
the angle of incidence of the beam upon the target while maintaining a
constant or fixed position upon the target is accomplished using a
rotatable mirror and an elliptical mirror placed within the reflected beam
path and between the rotatable mirror and the target material. Similarly,
the improved device used for changing the position of incidence of the
beam upon the target while maintaining a constant angle of incidence is
accomplished using a rotatable mirror and a parabolic mirror placed within
the reflected beam path and between the rotatable mirror and target
material. Either arrangement will provide selective control over the
direction and placement of the reflected beam. These parameters may be
varied continuously and smoothly with these devices. Furthermore, the two
separate arrangements can be used in a variety of combinations as basic
building blocks for any beam alignment task.
The improved device for aligning optical beams of the present invention
provides not only a high degree of precision in directing the reflected
beam upon the target, but also provides a constant travel time of the
reflected beam from the rotatable mirror to the target material regardless
of the rotatable mirror angle of rotation. Thus, for ultrafast optical
beams having ultrashort pulsewidths, each beam in a plurality of beams
will arrive at the target location at the same time independent of the
rotatable mirror angle of rotation. Provided the mirrors have high quality
smooth surfaces, reflected beams can be placed and can simultaneously
arrive upon the target with a high degree of precision.
In a preferred embodiment, the improved device for aligning optical beams
of the present invention comprises an elliptical mirror having a hole for
receiving the optical beams, a rotatable mirror aligned with the beams for
reflecting the beams upon the elliptical mirror, and a target for
receiving the reflected beams at a fixed position substantially
independent of the angle of rotation of the rotatable mirror. The
rotatable mirror is configured at the first focal point of the ellipse.
The target for receiving the reflected beams is situated at the second
focal point of the ellipse. Moreover, the rotatable mirror can be either
flat or curved depending upon the surface structure of the elliptical
mirror. The rotatable mirror is preferably flat if the elliptical mirror
is an ellipsoid. The rotatable mirror may also be a phase conjugate mirror
in order to correct for phase front distortion. Alternatively, a small,
collimated rotatable light source, such as a semiconductor diode laser,
may replace the rotatable mirror.
In another preferred embodiment, an improved device for aligning optical
beams of the present invention, comprises a parabolic mirror having a hole
for receiving the optical beams, a rotatable mirror aligned with the
optical beams for reflecting the beams upon the parabolic mirror, and a
target for receiving the reflected beams at a fixed angle of incidence
substantially independent of the angle of rotation of the rotatable
mirror. The rotatable mirror is configured at the first focal point of the
parabola. The target for receiving the reflected beams is situated within
the path of travel of the reflected beam. Moreover, the rotatable mirror
can be either curved or flat depending upon the surface characteristics of
the parabolic mirror. A flat rotatable mirror is preferably used if the
parabolic mirror is a paraboloid. The rotatable mirror may also be a phase
conjugate mirror in order to correct for phase front distortion.
Alternatively, a small, collimated rotatable light source, such as a
semiconductor diode laser, may replace the rotatable mirror.
In still another preferred embodiment, an improved method for aligning
optical beams of the present invention comprises combining at least two
geometric mirrors in a cascaded configuration, passing the optical beams
through a hole in a first geometric mirror onto a first rotatable mirror
of the cascaded configuration. The optical beams are then reflected from
the first rotatable mirror onto the first geometric mirror where they are
then reflected through holes in geometric mirrors arranged subsequent to
the first geometric mirror. Upon traveling through the holes of each
subsequent geometric mirror, the reflected beams are then reflected back
upon the respective geometric mirror and eventually onto a target by a
rotatable mirror contained within each geometric mirror. The geometric
mirrors can be elliptical or parabolic mirrors.
In still another preferred embodiment, an improved method for aligning
optical beams of the present invention comprises combining at least two
geometric mirrors, passing the optical beams through a hole in a first
geometric mirror, reflecting the optical beams onto the first geometric
mirror, receiving the reflected beams onto a target and onto a second
geometric mirror, and transmitting the reflected beam through a hole in
the second geometric mirror and upon a fixed detector. The reflected beam
striking the target can either pass through or be reflected by the target
material. Upon further reflection of the reflected beam from the target,
the further reflected beam is received upon the second geometric mirror
and then transmitted through a hole in the second geometric mirror and
upon a fixed detector. However, if the reflected beam passes through the
target material, then it is received upon the second geometric mirror
arranged behind the target. The first and second geometric mirrors of
either the transmissive or reflective target embodiments may be either
elliptical or parabolic mirrors.
The present invention therefore provides an improved device and method for
aligning optical beams which enjoys the advantages of directing beams via
a rotatable mirror, while at the same time targeting the reflected beam at
a fixed location with a variable angle of incidence or at a fixed angle of
incidence with a variable point of incidence. Each application of the
improved alignment device of the present invention can be cascaded or
arranged in tandem as building blocks to provide a high degree of
flexibility for any beam alignment task. These and other advantages of the
present invention will be further appreciated from the drawings and the
detailed description provided below.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a cross-sectional view of a variable angle, fixed position beam
alignment device of the present invention.
FIG. 2 is a cross-sectional view of a variable position, fixed angle beam
alignment device of the present invention.
FIG. 3 is a cross-sectional view of cascaded variable position, fixed angle
beam alignment devices of the present invention.
FIG. 4 is a cross-sectional view of cascaded variable angle, fixed position
beam alignment devices of the present invention.
FIG. 5 is a cross-sectional view of a combination of cascaded variable
angle, fixed position beam alignment devices and variable position, fixed
angle beam alignment devices of the present invention.
FIG. 6 is a cross-sectional view of two variable angle, fixed position beam
alignment devices of the present invention connected in tandem.
FIG. 7 is a cross-sectional view of two variable position, fixed angle beam
alignment devices of the present invention connected in tandem.
FIG. 8 is a cross-sectional view of two variable position, fixed angle
devices of the present invention used in tandem to measure the
transmission through a target as a function of position.
FIG. 9 is a cross-sectional view of two variable angle, fixed position
devices of the present invention used in tandem to measure the
transmission through a target as a function of angle.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
Referring to the drawings, FIG. 1 is a cross-sectional view of a variable
angle, fixed position beam alignment device 10 of the present invention.
Variable angle, fixed position device 10 comprises elliptical mirror 12
having hole 14 through which optical beam 16 is transmitted along the
major axis of the ellipse. Optical beam 16 includes any narrow cross
sectional stream of light particles, or photons, of any wavelength or
wavelengths originated from either a laser or an incoherent source. In
addition, the principles of this invention are suitable to direct charged
and uncharged particle beams. Whatever type of beams are chosen, all that
is required is that the chosen beam be sufficiently focused or
concentrated such that beam radius is sufficiently less than the radius of
hole 14. As beam 16 enters through hole 14, it strikes rotatable mirror 18
located at the first focal point of the ellipse. Depending upon the amount
of rotation, the longitudinal axis of beam 16 forms a variable angle
.alpha. with the longitudinal axis of rotatable mirror 18. Also, depending
upon the amount of rotation of rotatable mirror 18, reflecting beam 20
will strike elliptical mirror 12 at varying locations upon mirror 12.
Thus, a steeper incline of rotatable mirror 18, or larger angle .alpha.,
will cause reflecting beam 20 to strike elliptical mirror 12 nearer hole
14. Conversely, a shallower incline will cause reflecting beam 20 to
strike elliptical mirror 12 at a point further from hole 14.
In keeping with the invention, it is important to note that a sealing
member 21 such as a beam-transmissive window can be substituted for, or
placed in, hole 14. The sealing member 21 functions to allow beam 16 to
enter a vacuum sealed chamber defined by elliptical mirror 12 and another
sealing member 23 at the open end of elliptical mirror 12. A vacuum sealed
chamber is preferred in instances where rotatable mirror 18 and reflecting
beam 20 need be acclimated to a vacuum environment. However, in carrying
out the invention, it is not necessary that reflecting beam 20 operate in
a vacuum environment. In particular, it is not necessary that there even
be a hole or that there is a full elliptical mirror. In other words, all
that is necessary is that a segment of an elliptical mirror be placed so
as to generate first and second focal points at the surface of rotatable
mirror 18 and target 22. This can be achieved by passing beam 16 adjacent
to one end of an elliptical mirror segment, wherein the segment is
suspended at a location necessary to receive and generate reflected beams
at focal points similar to the non-segmented or "full" elliptical mirror
12.
One of the important features of variable angle, fixed position device 10
is where elliptical mirror 12 causes reflecting beam 20 to strike target
22 at a fixed point located at the second focal point of the ellipse
regardless of where reflecting beam 20 strikes elliptical mirror 12.
Consequently, the fixed point of incidence upon target 22 is not effected
by the rotation of rotatable mirror 18. Also, another important feature of
variable angle, fixed position device 10 is that the travel path length of
reflected beam 20 from rotatable mirror 18 to target 22 is constant
regardless of the changes in angle .alpha. of rotatable mirror 18. Since
the path length of reflecting beam 20 is constant, the travel time, T, of
reflected beam 20 is also constant and can be expressed in the following
formula:
##EQU1##
where a and b are respectively, the major and minor axes of the ellipse
and c is the speed of light. Although both travel time and point of
incidence upon target 22 are constant regardless of changes in .alpha.,
angle of incidence (.phi.) will change in accordance with changes in
.alpha.. Variable angle, fixed position device 10 requires that angle of
incidence, .phi., be variable in accordance with the variability in angle
.alpha.. In general, the angle of incidence, .phi. at target 22 is given
in terms of the rotatable mirror angle, .alpha., by the following formula:
##EQU2##
It is important to note that, depending upon the magnitude of a and b,
approximately a 2:1 gearing ratio between .alpha. and .phi. exists. This
is a desirable outcome since it provides controllability with a high
degree of precision in changes of .phi. relative to larger changes in
.alpha..
There are numerous changes that can be made to variable angle, fixed
position device 10 without substantially changing the function of the
device. For example, rotatable mirror 18 can be either curved or flat
depending upon the characteristics of elliptical mirror 12. If elliptical
mirror 12 is a true ellipsoid (three dimensional elliptical pattern formed
by rotatable an ellipse around either axis), then the reflecting surface
of rotatable mirror 18 can be flat. If, however, elliptical mirror 12 is
not an ellipsoid but is an elliptically curved mirror which extends
directly upward in the Z direction in accordance with the XY ellipse
pattern, then the reflecting surface of rotatable mirror 18 can be curved,
wherein the curvature is used to compensate for partial astigmatic
corrections that must be made. Further, curvature of the rotatable mirror
can provide additional focussing or defocussing depending on the specific
application. The rotatable mirror may also be a phase conjugate mirror in
order to correct for phase front distortion. Alternatively, a small,
collimated rotatable light source, such as a semiconductor diode laser,
may replace the rotatable mirror. In addition to rotatable mirror 18 being
either flat or curved, mirror 18 can be easily controlled by mechanical or
electrical actuators which function to rotate mirror 18 in a controllable,
pre-defined pattern. Pursuant to movement of mirror 18, it is noted that
mirror 18 can be rotated either continuously or in discrete movements
whereby beam 16 impinges upon mirror 18 either during the continuous
rotatable movement or between discrete movements. Although continuous
rotatable movement will carry out the invention, it is sometimes
preferable that mirror 18 be rotatable in discrete movements with beam 16
striking the surface of mirror 18 between each movement.
FIG. 2 illustrates another embodiment of the present invention showing the
variable position, fixed angle beam alignment device 24 having a parabolic
mirror 26. Parabolic mirror 26 functions to receive optical beam 16,
aligned along the axis of the parabola, through a hole 14 within parabolic
mirror 26. Upon striking rotatable mirror 18, located at the focus of the
parabola, optical beam 16 is reflected as reflecting beam 28. Reflecting
beam 28 then strikes parabolic mirror 26 to be reflected back at an angle
parallel to the X-axis of parabolic mirror 26.
An important feature of variable position, fixed angle device 24 is that
reflecting beam 28 strikes a target 30 at various locations depending upon
the amount of rotation or changes in .alpha. of rotatable mirror 18.
Although the point of incidence upon target 30 is variable, reflecting
beam 28 will strike target 30 at a fixed angle of incidence, .phi.,
regardless of the changes in angle .alpha.. Reflecting beam 28 will
maintain a path parallel to the optical beam 16 path and will be displaced
a distance Y away from the path of beam 16 according to the following
formula:
##EQU3##
where x=dy.sup.2, defines the parabola.
In accordance with variable position, fixed angle device 24, the travel
distance of reflecting beam 28 remains constant regardless of the changes
in .alpha., as long as .phi.=90 degrees. Since the travel distance is
constant, so must be the travel time of reflecting beam 28 as it travels
between rotatable mirror 18 and target 30. Like the elliptical embodiment,
the parabolic embodiment of variable position, fixed angle device 24
provides synchronized arrival of optical beams upon target 30. The time of
flight through variable position, fixed angle device 24 can be described
by the following formula:
##EQU4##
where target 30 is situated upon the plane x=X.sub.s.
Similar to variable angle, fixed position device 10, variable position,
fixed angle device 24 can include either a flat or a curved reflecting
surface of rotatable mirror 18 depending upon whether or not parabolic
mirror 26 is a paraboloid. If mirror 26 is not a paraboloid but is merely
a parabola extending directly upward into the Z-axis, then a curved
surface on rotatable mirror may be desired to correct for the astigmatic
surface of the Z-extending parabola. Conversely, if mirror 26 is a
paraboloid, then the surface of rotatable mirror 18 may be flat. The
curvature of the rotatable mirror can also provide additional focussing or
defocussing, depending on the given application. The rotatable mirror may
also be a phase conjugate mirror in order to correct for phase front
distortion. Alternatively, a small, collimated rotatable light source,
such as a semiconductor diode laser, may replace the rotatable mirror.
In keeping with the invention, it is important to note that, like the
elliptical mirror embodiment, parabolic mirror 26 can utilize a sealing
member or window 21 placed in hole 14. The sealing member 21 can provide a
vacuum sealed chamber through which reflected beam 28 travels. Also, a
partial parabolic mirror or segment absent hole 14 can be used instead of
a full parabolic mirror having hole 14 through which beam 16 travels.
It is important to note that variable angle, fixed position device 10 and
variable position, fixed angle device 24 can be used as building blocks
and can be cascaded together in any combination sufficient to provide
flexible steering for any beam alignment task. As illustrated in FIG. 3, a
plurality of fixed angle devices 24 are shown cascaded together. The
cascaded arrangement of fixed angle devices 24 provides a reflecting beam
28 which strikes target 30 at a fixed angle .phi. regardless of the amount
of rotation of each mirror 18. The rotatable mirrors 18 can be
simultaneously rotated or rotated independently of one another depending
upon where the designer wants to steer the reflecting beam upon target 30.
Also, the amount of rotation can be adjusted so as to align beams 16 and
28 of each fixed angle device 24 with beams 16 and 28 of proceeding and
subsequent fixed angle devices 24. It is important to note that design
advantages are gained even if only one mirror is rotatable. If necessary,
the downstream devices may be translated perpendicular to the direction of
propagation for improved alignment.
FIG. 4 illustrates a cascaded arrangement of variable angle, fixed position
devices 10, wherein reflecting beam 20 is placed at a fixed point upon
target 30 in response to movement of rotatable mirrors 18. Again,
rotatable mirrors 18 can be moved simultaneously or independently of each
other depending upon alignment constraints between each fixed position
device and the desired position upon target 30. If necessary the
downstream devices may be rotated about the axis of propagation for
improved alignment. As illustrated, the cascaded ellipses must share
common focal points.
FIG. 5 illustrates a combination of variable angle, fixed position devices
10 and variable position, fixed angle devices 24 that can be arranged in
any cascaded format depending upon the desired beam alignment task. FIG. 5
shows variable position, fixed angle device 24 receiving optical beam 16
and a subsequent variable position, fixed angle device 24 delivering
reflecting beam 28 upon target 30. If necessary, the downstream devices
may be translated or rotated for improved alignment. It is important to
note, however, that variable angle, fixed position devices 10 can be
substituted for variable position, fixed angle devices 24 without
deviating from the scope of the invention. The arrangement of the devices
10 and 24 as building blocks in the beam alignment scheme can be varied
for any outcome desired by the optical designer.
FIG. 6 illustrates that fixed position devices 10 can be arranged in tandem
to realign optical beam 16 into reflecting beam 20. Instead of reflecting
beam 20 being transmitted away from hole 14 and towards a target, it can
be transmitted back towards and through hole 14 and away from target 22 as
shown. The tandem arrangement of FIG. 6 can be used in multi-spectral
angular scanning applications. Multi-spectral angular scanning is useful
in ellipsometry, thin film characterization and industrial vision system
applications. In the tandem configuration, target 22 is placed at the
common focus of two ellipses as shown. Optical beam 16 is projected
through hole 14 of one variable angle, fixed position device 10 and then
imaged onto target 22. The beam reflected off target 22 is then collected
and directed onto a detector 32 by the second variable angle, fixed
position device 10. The two rotatable mirrors 18 can move in concert
either through an appropriate mechanical linkage or through computer
controlled actuators, in order to provide variable and differential angle
scanning. In this manner, optical beam 16, target 22 and detector 32 may
be fixed in place during the scan. This is useful for two reasons.
Typically, the optical source which provides optical beam 16 and the
detector 32 may be large and bulky assemblies, and precise relative
movement of these assemblies are not needed if mirrors 18 are moved
instead. Thus, mirror movement compensates for lack in movement of the
assemblies. Also, there is an additional degree of freedom associated with
target 22, and thus, it may be irradiated by an extremely aligned pump
laser or particle beam, or mounted on a traditional conveyor belt.
FIG. 7 illustrates that variable position, fixed angle devices 24 can also
be arranged in tandem similar to the variable angle, fixed position
devices 10 of FIG. 6. Tandem arrangement will provide the same advantages
previously described. However, using variable position, fixed angle
devices 24 will provide an additional degree of freedom in aligning
reflecting beam 28 upon detector 32. Depending upon the relative location
of incoming optical beam 16 and outgoing reflecting beam 28, tandemly
arranged variable position, fixed angle devices 24 might be preferred to
tandemly arranged variable angle, fixed position devices 10.
FIG. 8 illustrates that two variable position, fixed angle devices 24 can
also be arranged in tandem to measure the transmission through target 30
as a function of position, or, more generally, to vary the optical
properties of reflecting beam 28 by a target 30 whose transmission
properties may purposefully vary as a function of position. The first
variable position, fixed angle device 24 adjusts the position of incidence
upon target 30. The second variable position, fixed angle device 24 can,
for example, redirect the beam back along the original path of propagation
and into a fixed detector 32. FIG. 9 illustrates that two variable angle,
fixed position devices 10 that can also be arranged in tandem to measure
the transmission through target 22 as a function of angle, or, more
generally, to vary the optical properties of the beam by target 22 whose
transmission properties purposefully vary as a function of angle of
incidence. The first variable angle, fixed position device 10 adjusts the
angle of incidence upon target 22. The second variable angle, fixed
position device 10, can, for example, redirect the beam back along the
original path of propagation, into a fixed detector. The second focal
point of each ellipse is common and defines the location of target 22.
The foregoing description of the invention has been directed to multiple
preferred embodiments of the present invention. It will be apparent,
however, to those skilled in the art that modifications and changes in
both apparatus and method may be made without departing from the scope and
spirit of the invention. For example, instead of using elliptical and
parabolic mirrors, ellipsoid and paraboloid mirrors can be used. Also,
either flat or curved surfaces can be used upon rotatable mirror 18. Also,
the physical size of these devices are scalable from the micron size for
photonic applications to the meter size for astronomical and industrial
applications. Also, as shown in FIGS. 3-8, variable angle, fixed position
devices 10 and variable position, fixed angle devices 24 can be arranged
in cascaded or tandem fashion to achieve any desired beam alignment
outcome. Also, it is appreciated by one skilled in the art that the
precision by which reflected beams are placed upon target is dependent
upon smoothness or surface quality of mirrors 12, 18 and/or 26. If the
mirrors are of high optical quality, then placement of reflected beam 20
or angle of incidence of reflected beam 28 will not deviate substantially
during the rotation of mirror 18. High quality mirrors presently exist
which can fix the amount of deviation to be less than 10%, and in some
instances, less than 1%. Therefore, it is the applicants' intention in the
following claims to cover all such equivalent modifications and variations
which fall within the true spirit and scope of the invention.
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Description  |
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