Fast laser scanning optical CT apparatus
View Patent ↗Disclosed are scanning devices which measure and quantify optical properties within an object such as the absorption of light, refractive index, light scattering, fluorescence, and phosphorescence. Through the use of two rotating plane mirrors and two paraboloid mirrors, a laser light beam is made to traverse the object to be scanned wherein the beam is always parallel to the optical axis. The invention provides an improvement over previously reported scanning devices by virtue of increased speed and resolution. Two-dimensional projections gleaned by each scan of the object are reconstructed into a three-dimensional image through the use of various computer techniques.
1. A scanner for imaging optical properties of a three-dimensional object ranging in size from a volume of about 1 cm 3 to a cylinder having a radius of about 25 cm and a height of about 25 cm, said scanner comprised of:
a highly collimated light source emitting a light beam transmitted through said object;
a first photoreceiver, for measuring the attenuation of said light beam by said object;
a first and second rotating mirror;
a first converging lens;
a tank containing refractive index matching liquid in which the object is immersed;
a means to rotate said object about an axis substantially perpendicular to the optical axis;
a computer for controlling the movement of said rotating mirrors, for controlling the orientation of the object with respect to the scanning beam, and for calculating said optical properties;
wherein said imaging comprises forming a series of two-dimensional projections by scanning said object in a two-dimensional raster pattern, changing the orientation of the object with respect to the scanning beam, repeating the scanning and the orientation a plurality of times, employing computerized algorithms to filter the series of projections, and reconstructing a three-dimensional image using computerized tomographic techniques.
2. The scanner according to claim 1 further comprising relay optics.
3. The scanner according to claim 2 wherein the rotating mirrors are galvanometric mirrors.
4. The scanner according to claim 3 wherein said relay optics is selected from the group consisting of paraboloidal mirrors and spherical mirrors.
5. The scanner according to claim 3 wherein said relay optics is comprised of a first paraboloidal mirror and a second paraboloidal mirror.
6. The scanner according to claim 5 further comprising a beamsplitter, a second photoreceiver, and a second converging lens, wherein said light beam is split by said beamsplitter so that a first portion of the beam falls on said second photoreceiver allowing a reference intensity to be measured, and a second portion of the beam encounters the surface of said first rotating mirror, is deflected onto the surface of said first paraboloidal mirror, is subsequently deflected onto the surface of said second paraboloidal mirror, is subsequently deflected onto the surface of said second rotating mirror, is subsequently deflected through said first converging lens, is subsequently transmitted through said object, is subsequently passed through said second converging lens, and subsequently enters said first photoreceiver.
7. The scanner according to claim 6 , wherein said light beam is split by said beamsplitter so that a first portion of the beam encounters the surface of said first rotating mirror, is deflected onto the surface of said first paraboloidal mirror, is subsequently deflected onto the surface of said second paraboloidal mirror, is subsequently deflected onto the surface of said second rotating mirror, is subsequently deflected through said first converging lens, is subsequently transmitted through said object, is subsequently passed through said second converging lens, and subsequently enters said first photoreceiver; and so that a second portion of the beam falls on said second photoreceiver allowing a reference intensity to be measured, such measurement is made to be stored in a computer memory, said object is rotated on an axis substantially perpendicular to the optical axis, the measurement and rotation are repeated a plurality of times, and a three-dimensional image is generated using computed tomographic means.
8. The scanner of claim 1 wherein said attenuation is absorption.
9. The scanner according to claim 1 in which said collimated light source is a laser.
10. The scanner according to claim 1 wherein the means to rotate causes an increment of 0.5 to 1.5 degrees.
11. The scanner of claim 10 wherein the means to rotate causes an increment of about one degree, and said image is 60×60×60 cubic voxels.
12. The scanner of claim 11 wherein the image is acquired in less than two minutes.
13. The scanner of claim 1 wherein the three-dimensional object is a dosimeter used in assessing radiotherapeutic parameters.