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Claims  |
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What is claimed is:
1. A method for determining a measurement of a physical property of
interest associated with the discrete spatial locations of a three
dimensional object, wherein each spatial location of the three dimensional
object has a unique address, and wherein the three dimensional object is
composed of a plurality of types of matter, each type of matter having at
least two properties, comprising the steps of:
generating a first set of data reflective of at least a first physical
property accessible by a first imaging technique and scanner for each
spatial location of the area of interest;
generating a second set of data reflective of at least a second physical
property accessible by a second, different imaging technique and scanner
for each spatial location of the area of interest;
storing the data generated by the first and second imaging techniques in a
memory storage device along with the address of each spatial location; and
assigning to each unique address a first value, said first value
representing the measurement of said property of interest for each unique
address, said first value based on a correlation between said property of
interest with the measure of the first physical property obtained in the
first imaging scan taken and the correlation between said property of
interest with the measure of the second physical property obtained in the
second imaging scan taken, such that said property of interest is
different from said first and second physical properties.
2. The method of claim 1, further comprising the step of assigning to each
address a pixel display value defining the physical appearance that the
pixel is to have upon its display.
3. The method of claim 2, further comprising the step of
displaying an image based on the pixels so defined.
4. The method of claim 1, wherein the first set of data is generated by a
CT scan.
5. The method of claim 1, wherein the first set of data is generated by a
PET scan.
6. The method of claim 1, wherein the first set of data is generated by a
particular type of MRI scan.
7. The method of claim 1, further comprising the steps of
generating additional sets of data reflective of at least one additional
physical property accessible by additional imaging techniques for each
spatial location of the area of interest, wherein each spatial location
has an address; and
storing the additional sets of data so generated in a computer memory along
with the address of each spatial location.
8. The method of claim 1, wherein the three dimensional object includes a
portion of human anatomy.
9. The method of claim 1, wherein the physical properties being determined
relate to the appearance of the region when exposed to visible light.
10. The method of claim 1, wherein the second set of data is generated by a
CT scan.
11. The method of claim 1, wherein the second set of data is generated by a
PET scan.
12. The method of claim 1, wherein the second set of data is generated by a
particular type of MRI scan.
13. The method of claim 1, wherein the correlation between the property of
interest and a value of at least one of the physical properties measured
in at least one of the generated data sets is determined empirically.
14. The method of claim 1, wherein at least one of the generated sets of
data is reflective of density.
15. The method of claim 1, wherein at least one of the generated sets of
data is reflective of the position of known features in relation to each
other.
16. The method of claim 1, wherein at last one of the generated sets of
data is reflective of the presence of hydrogen.
17. The method of claim 1, wherein at last one of the generated sets of
data is reflective of sound transmissibility.
18. The method of claim 1, wherein at least one of the generated sets of
data is indicative of the manner in which light is absorbed or reflected.
19. The method of claim 1, wherein at last one of the generated sets of
data is reflective of temperature.
20. The method of claim 1, wherein at least one of the generated sets of
data is reflective of electrical activity.
21. The method of claim 1, wherein at least one of the generated sets of
data is reflective of energy usage.
22. A method for determining a measurement of a tissue type property
associated with the discrete spatial locations of a three dimensional
object, wherein each spatial location of the three dimensional object has
a unique address, and wherein the three dimensional object is composed of
a plurality of types of matter, each type of matter having at least two
properties, comprising the steps of:
generating a first set of data reflective of at least a first physical
property accessible by a first imaging technique and scanner for each
spatial location of the area of interest;
generating a second set of data reflective of at least a second physical
property accessible by a second, different imaging technique and scanner
for each spatial location of the area of interest;
storing the data generated by the first and second imaging techniques in a
memory storage device along with the address of each spatial location; and
assigning to each unique address a first value, said first value
representing the measurement of the tissue type property for each unique
address, said first value based on a correlation between the tissue type
property with the measure of the first physical property obtained in the
first imaging scan taken and the correlation between the tissue type
property with the measure of the second physical property obtained in the
second imaging scan taken, such that said first and second physical
properties are different from the tissue type property.
23. The method of claim 22, further comprising the step of assigning to
each unique address a pixel display value defining the physical appearance
that the pixel is to have upon its display.
24. The method of claim 23, further comprising the step of displaying an
image based on the pixels so defined.
25. The method of claim 22, wherein the three dimensional object includes a
portion of human anatomy. |
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Claims  |
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Description  |
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BACKGROUND OF THE INVENTION
This invention is directed to the problem of providing images of anatomy
that reflect at least one physical property of interest characteristic of
the anatomy. It is also directed to the problem of inferring information
regarding an unknown property of an interior region of anatomy from known
properties of that and adjacent regions.
Clinicians have long sought ways of visualizing interior portions of the
human body without having to expose those portions to light for direct
visual inspection. The first technology which enabled the clinician to see
an image of an interior portion of anatomy was the X-ray, which was
utilized to form images of bone within months of the discovery of X-rays
by Roentgen in 1895.
These images were essentially 2-dimensional views taken of a three
dimensional volume of space. Of course, anatomy exists in three
dimensional space and, in the 1970's, devices were developed that
permitted the acquisition of information concerning the anatomy on a three
dimensional basis (e.g., the work of Hounsfield in developing scanners
that measured the density of an anatomical volume, which he displayed as
slices).
Subsequent developments have further advanced the state of the art to where
the clinician has at his disposal a variety of tools for obtaining
information regarding each volumetric element within a volume of anatomy.
In each of these techniques, the region of anatomy in question may be
thought of as consisting of a very large number of small elemental units
of volume called voxels. A voxel has length, width, and depth. The size of
a voxel is generally limited by the inherent resolution of the scanner
apparatus and technique utilized, as well as the underlying computational
power with which the technique is practiced. Ideally, a voxel is small
enough to depict an area of generally uniform attributes with respect to a
property of interest.
A number of imaging techniques using a variety of types of imaging
apparatus subdivide a volume of space into voxels. For example, in
Magnetic Resonance Imaging (MRI), a "slice" of a patient's anatomy, or the
like, having a finite thickness is excited with a predetermined pulsing
signal. This pulsing signal causes protons (e.g., Hydrogen protons) in the
slice to resonate giving off a signal, the intensity of which varies
directly with proton density. Different properties can be the focus of the
scan by varying the excitation energy, relaxation time parameters etc.
employed in the scan, as well as by using any or none of a variety of
chemical imaging agents. Whichever technique is employed, it results in
the measurement of a property of the matter contained within each voxel.
Such measurements are converted into electrical signals of varying
intensity across the slice (which is as little as one voxel thick) and
stored in a data base. Each measured intensity actually represents a value
of the property of interest accessed by the scanner technique for a finite
volumetric space in the patient's anatomy, i.e., voxel. A complete
understanding of MRI is beyond the scope of this application. A more
intensive discussion of MRI can be found in "The MRI Manual" by Robert B.
Lufkin, published by Year Book Medical Publishers, 1990, the disclosure of
which is hereby incorporated by reference in its entirety.
Another medical imaging technique is Computed Tomography. In CT, X-rays
impinge upon a slice of a patient's anatomy, for example. Once this
electromagnetic radiation has passed through the anatomy, its intensity is
measure and stored. Generally, the X-ray source is rotated around the
patient's anatomy, and measurements of electromagnetic intensity are taken
for each different position of the X-ray source. The resulting data is
processed in a computer to determine a intensity value for each voxel in
the anatomical slice. This intensity value is proportional to the physical
property CT scanners are constructed to sense--the proton density of
matter located within the voxel. A complete understanding of CT is beyond
the scope of this application. A more intensive discussion of CT imaging
can be found in "Principles of Radiographic Imaging--An Art and a Science"
by Richard R. Carlton and Arlene M. Adler, published by Delmar Publishing
(1992), the disclosure of which is hereby incorporated by reference in its
entirety.
While the concept of a voxel is useful in organizing and processing data,
it is not the form in which information is presented to the clinician, no
matter what the scanning technique employed. Because of limitations in
display technology as well as the manner in which humans desire to view
information, data is presented to clinicians in terms of two-dimensional
renderings, either on a video screen or on a hard copy, such as a
photograph. The elemental units into which a two dimensional image are
presented are known as pixels.
In producing an MRI image, the measured signal intensities for each voxel
are converted into a value related to a display device. For example, if
the measured intensities are to be displayed on an 8-bit/pixel gray-scale
monitor, each measured intensity for each voxel in the displayed slice
would be converted into a value between 0 and 255 (i.e., 0 to {2.sup.8
-1}). Depending on the measured intensities, an image, which is the
display of the constituent pixels, is generated, with one pixel being
defined for each voxel in the slice. In the aggregate, these pixels
visually portray the structure contained within the slice in terms of the
properties detected by the imager in a manner which results in an image
that can be interpreted by trained personnel.
Similarly, in formulating a CT image for display, the intensity values
corresponding to a measured property--proton density--for each voxel in
the slice must be scaled to a monochromatic grey scale for defining the
pixels that actually form the image on the display device. In a CT image,
one observes a higher level of definition of bone matter as compared to an
MRI image. This is due to higher density of the bone matter which
corresponds to a higher value in the grey scale for the CT image (i.e.,
pure white represents the highest value on the grey scale). Once again,
these pixels visually portray the structure contained within the slice in
terms of the properties detected by the imager in a manner which results
in an image that can be interpreted by trained personnel.
Within the individual scanning techniques that have been developed, efforts
have been made to enhance the information presented to the clinician. For
example, a number of methods have been utilized for differentiating
between different types of matter in a medical image. For instance, in
U.S. Pat. No. 4,835,712 to Drebin et al., each voxel is classified as to
percentages of different materials (i.e., air, fat, bone, and soft
tissue). A color is assigned to each material (e.g., white for bone, green
for fat, etc.) which is used to generate the appearance of each voxel.
In U.S. Pat. No. 5,185,809 to Kennedy et al. an apparatus is described for
outlining different portions of the medical image depending on tissue
type. Such outlining allows the user to discern between different matter
types in the image.
In U.S. Pat. No. 4,991,092 to Greensite, an image processor is described
for enhancing contrast between subregions of a region of interest.
Biological tissue of different types are each assigned a different color
depending on their NMR characteristics for better contrast.
U.S. Pat. No. 4,945,478 to Merickel et al. pertains to an imaging system
for displaying an image of the aorta. MRI derived data (e.g., T.sub.1 -
weighted, T.sub.2 - weighted) of the patient are used to discern different
tissue types (esp. plaque constituent tissue) in the aorta. Once the
tissue type is discerned, those pixels representing each tissue type are
given a uniform color.
U.S. Pat. No. 5,187,658 to Cline et al. describes a system for segmenting
internal structures contained within the interior region of a solid
object.
U.S. Pat. No. 5,224,175 to Gouge et al. describes a method for analyzing
ultrasound images. Values from the ultrasound image are compared to values
for known tissues in order to identify tissue type.
U.S. Pat. No. 3,903,414 to Herbstein et al. simply describes a system that
combines X-ray diffraction, fluorescence, and absorption.
The disclosure of the foregoing references are hereby incorporated by
reference in their entirety. In general, the techniques taught therein
calls for manipulating the data provided by a single type of scanner. The
resulting image may be more pleasing to the eye or even have some
additional functionality, but it still inevitably incorporates whichever
uncertainties characterize the underlying scanning modality in question.
Each individual scanning technique is limited to providing a visual
representation of a physical property of the material that the imager
measures. Unfortunately, that physical property may not correspond to what
the clinician really wants to directly measure, or it may contain inherent
levels of uncertainty that the clinician may wish to reduce. This problem
is more clearly understood when considering the special case of the
property that clinicians most clearly want to access: the visual
appearance of tissue in light.
The clinician is most interested in viewing a hidden, interior region of
anatomy without having to expose it by surgery, or, if he is to operate
anyway, he wishes to see what surgery will reveal before the patient is
cut open, so that he may better plan his surgical approach. In addition,
he would like to see adjacent regions beyond what surgery will expose.
Therefore, what is ideally required is a scan that shows the surgeon what
his eyes would see, including the proper choice of color for each type of
matter (i.e., tissue) viewed. In brain surgery, the number of visually
distinct types of anatomy, i.e, differentiable by color and appearance,
that the surgeon sees is small in number (although, were one to take the
non-visible ways in which one could characterize tissue into account, such
as by function or electrical activity, there would be potentially many
more "types" of anatomy). There are perhaps ten or so such types of tissue
that are visible and distinguishable to the unaided eye of the surgeon
(e,g., bone, white matter, grey matter, venous tissue, etc.) and which are
visibly characterized by a unique appearance and color (i.e., the
appearance of each type of tissue is its "property"). Unfortunately, none
of the existing scanning techniques can present an image that corresponds
to what the clinician would actually see, because of the aforementioned
limitations in each scanner type with regard to the information they can
acquire. For example, a CAT scan simply does not do a very good job of
detecting and differentiating among the various types of soft tissue
present, but does do an excellent job of showing bone. Similarly, an MRI
scan (which can be varied through the selection of various parameters and
contrast agents) is better at differentiating among the various types of
soft tissue present, but does not accurately scan bone. Other forms of
scanning or imaging a portion of anatomy also are deficient in the range
of physical properties that they can access. Because of the limitations
inherent in the known types of scans and the tissue-specificity of their
optimal uses, even colorization of pixels derived from these scans cannot
show a true image of a section of anatomy, because the individual scans
are simply unable to differentiate among all the various types of tissue
that the clinician sees.
There remains a need for an imaging technique that can take advantage of
the comparative advantages possessed by the various imaging techniques in
imaging particular types of tissue so as to form a composite image based
on the information most accurately perceived by each of the imaging
techniques.
There remains a need for an imaging technique that can more accurately form
inferences regarding a property not readily accessible from any one
scanning technique (such as visible appearance) by utilizing information
provided by several scanning techniques concerning properties that are
more readily accessible.
SUMMARY OF THE INVENTION
This invention presents a new manner of integrating voxelly-assigned
information derived from a number of sources into an accurate
representation of the region of interest. The method creates a data set
that can be used to generate visual depictions of. the region of interest.
Typically, the clinician will prefer that this visual representation
depict what he would see were he to directly look at the corresponding two
dimensional surface of anatomy with his eyes in ordinary light. This
representation may take the form of a two dimensional pixel-based display,
or a three dimensional view (as via a holographic display). More broadly,
the method enables one to draw inferences regarding a property of a hidden
region of matter that is not directly accessible by utilizing information
concerning other properties that are more readily accessible.
Considering the voxel as a volume of anatomy, one can attribute a number of
properties to each voxels. These properties include, and of course are not
limited to, density (as via a CT scan), sound transmission
characteristics, electrical activity, temperature, true appearance under
visible light, energy usage, manner of incorporating a radioactive isotope
(via PET), various MRI-based parameters (such as t1 and t2 among others),
as well as any other parameter detectable by a scanner or other device
that provides location specific information. Some of the aforementioned
properties (such as density) are directly ascertainable for at least some
types of tissue using known scanning techniques (e.g., CT). But others,
such as the true visual appearance for each of the approximately ten types
of tissue of interest to a neurosurgeon, may not be directly accessible
with any one scan, or may require several scans to ascertain.
According to one aspect of this invention, one first empirically determines
the relationship between each one of the ten or so visually distinct types
of matter and each of the directly accessible scannable properties by
applying standard statistical methods to the image data collected in a
controlled, well defined series of observations. This information can then
be used to determine which combination of measures of properties, chiefly
derived from various scan modalities, sufficiently define with the
requisite degree of specificity each of the ten known types of tissue by
appearance (the properties in question here).
More broadly, information concerning known, measurable properties can be
used to form an inference regarding the value of another, perhaps
inaccessible, physical property of a voxel. The true-color appearance of a
section of anatomy is but one example of a property that is not directly
accessible to the clinician surgically exposing the area in question. This
information is then stored in a series of look-up tables contained within
a computers memory.
Once the necessary correlations between scannable properties and the true
visual image (i.e., property) of a tissue type (or other discernable
surface or volumetric element of a region of interest) is obtained, it
becomes possible to generate pixels to provide two dimensional views of a
portion of anatomy that can be color coded to provide true color fidelity
of the area in question. The clinician would get an image showing just
what he would see upon surgically exposing the area in question to his
eyes and to the light.
This is done as follows. The clinician determines which area of the anatomy
(e.g., the brain) he wishes to obtain a color-true view of. If it is the
brain, he and the computer know that there are only ten or so types of
visually distinctive types of matter present. The computer then searches
its memory, and tells the clinician which types of scans are necessary in
order to provide the data necessary to provide the color-true image. The
scans required must provide registration of image space to physical space
within each scan, as well as of image space onto image space across scans.
One way of accomplishing this is through the use of image markers, the use
of which is described in U.S. Pat. No. 4,991,579 (the contents of which
are incorporated herein by reference); another, less preferred method is
through the use of a stereotactic frame. If the necessary scans have
already been taken, then the information generated by these scans are
loaded into memory. The computer, armed with the empirically derived
relationships previously established between the various parameters the
clinician can remotely access via the scans and the various tissue types
by their true visual appearance, selectively culls the addresses of those
voxels in the plane in question corresponding to each of the ten tissue
types by appearance, one after the other. (Of course, if a lesser degree
of color fidelity is desired by the clinician, fewer tissue types may be
needed or fewer scans may be required.) By considering the voxels in
planes, The address of each voxel of interest can define a pixel address
on the forming image. For example, the addresses of voxels lying along a
plane can be used to define a group of pixels that will form a plane
image. Then, the computer assigns a color to each pixel on the basis of
the tissue type, as a second table within the computer defines the true
color corresponding to each of the specific tissue types that have been
assigned to each voxel. Once this has been done, the computer generates an
image on a screen or on paper in which each pixel is defined within the
computer to depict one of the ten known tissue types, and which has been
assigned a color for display that matches the actual color of the known
corresponding tissue type.
The invention is not limited to providing views that correspond to what a
surgeon sees, but could be extended to providing graphical representations
of any anatomical or physiological feature by relying on empirically
established relationships between the feature or property one wishes to
depict and the data that one can obtain via various imaging techniques.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a flow chart of the method of the present invention; and
FIG. 2 is a block diagram of a system for implementing the method of the
present invention.
DETAILED DESCRIPTION
The method of the invention shall be further explained by reference to the
task of providing a true color image of the human head.
The clinician first determines which areas of the head he wishes to image,
and which particular types of tissue present he wishes to see. Typically,
the physician would be interested in obtaining an image that showed only
those portions of the head of the greatest interest for a particular
diagnosis. In this example, to evaluate the brain for certain symptoms,
the physician may decide that he requires a view of the following tissues
for forming a diagnosis: skull, veins, arteries, brain tissue including
grey matter and white matter, a tumor, ventricles and optic nerves. This
information is entered via a user interface 50 to a computer 55, where it
is stored in a table 52 called the Designated Property Table. This table
contains a sub-table 53 that correlates the type or types of scans which
should be performed to best provide information for forming an image of
each type of tissue the clinician has designated. A list of these scans,
along with scan-specific parameters required (e.g., the use of Gadolinium
for an MRI scan) is then displayed to the clinician via the interface 50.
The patient is then subjected to the computer specified scans.
The computer then determines the particular scans that are most appropriate
for characterizing each designated type of tissue. This is determined
chiefly through prior empirical study. With respect to the example
presented above, it is known that bone or skull can best be seen with a CT
scan un-enhanced; the veins and arteries can be seen best with a Venous
MRI Angiogram and Arterial MRI Angiogram, respectively; the white matter
of the brain can be seen more clearly with a T-1 MRI Scan; the grey matter
can be seen best with a T-2 MRI Scan; if there is interest in the optic
nerves, these can be seen with a T-1 MRI Scan. If there is interest in
locating a specific tumor, such as a meningioma, this can best be seen
with a T-2 MRI scan with Gadolinium; and for ventricles, this can best be
seen again with a T-1 MRI Scan. Furthermore, it can be empirically
determined with respect to each physical property measured by the
aforementioned scan which range of values of that property correlate with
any particular feature. For example, a correlation can be drawn between
the magnitude of the Hounsfield numbers generated in a CT scan with the
probability that the voxel associated with that particular Hounsfield
number contains bone. Similarly, statistical correlations can be
empirically determined with respect to any other property and a measured
value by empirical study. These relationships are stored in the Empirical
Relationship Table 70.
In each scan, the patient is provided wit | | |