The present invention relates generally to the field of cyclotron design for radiopharmacy and more particularly to a method and apparatus for ion source positioning and adjustment.
Hospitals and other health care providers rely extensively on positron emission tomography (PET) for diagnostic purposes. PET scanners can produce images which illustrate various biological process and functions. In a PET scan, the patient is initially injected with a radioactive substance known as a PET isotope (or radiopharmaceutical). The PET isotope may be 18F-fluoro-2-deoxyglucose (FDG), for example, a type of sugar which includes radioactive fluorine. The PET isotope becomes involved in certain bodily processes and functions, and its radioactive nature enables the PET scanner to produce an image which illuminates those functions and processes. For example, when FDG is injected, it may be metabolized by cancer cells, allowing the PET scanner to create an image illuminating the cancerous region.
PET isotopes are mainly produced with cyclotrons, a type of circular-shaped particle accelerators.
Traditionally, after positioning and adjustment of the slit opening, the only way to determine whether the position is acceptable is by measuring the ion source output. In order to measure the ion source output, the cyclotron chamber has to be pumped down to an acceptable vacuum level. In one cyclotron, for example, it takes about an hour to reach such a vacuum level. If measurement of the ion source output reveals that the slit opening has not been accurately positioned, the cyclotron chamber has to be re-opened to allow re-adjustment. Unfortunately, a simple reading of the ion source output does not offer a clear indication as to which direction or by how much the ion source tube should be adjusted. A service engineer usually has to adjust the position in small increments and repeat the pump-and-measure process for several times until a desired ion source output is measured. One iteration can take 2-3 hours. For an inexperience service engineer, it may take several iterations to achieve an acceptable level of ion source output. Therefore, the traditional approach for ion source positioning and adjustment can be very time-consuming. Even when an acceptable level of ion source output has been achieved, it is seldom clear whether an optimal position of the ion source tube has been reached.
Unfortunately, ion source adjustment is hardly avoidable since an ion source typically has a limited lifetime and requires periodical replacement. During a scheduled service, the cyclotron needs to be opened up to allow access to the ion source. However, since the cyclotron usually becomes radioactive during isotope production, it is necessary to wait for the radiation to decay to a safe level before starting the service. The wait for the radiation decay can sometimes last ten hours, for example. The safe level of radiation usually depends on how long a service engineer will be exposed. That is, a job that takes a short time can be started at a higher radiation level (i.e., after a shorter decay time) than one that takes a long time. Therefore, the shorter it takes to position and adjust a new ion source, the faster a scheduled service may be completed.
In view of the foregoing, it would be desirable to provide a more efficient solution for accurate positioning and adjustment of an ion source tube.
The present invention is directed to a method and apparatus for ion source positioning and adjustment that overcomes drawbacks of known systems and methods.
According to one embodiment, the invention relates to an apparatus for ion source positioning and adjustment. The apparatus comprises a bottom plate, a middle plate and a top plate, wherein the top plate is coupled to the middle plate by at least one adjustment member for causing the top plate to move in a first direction, wherein the at least one adjustment member positions the top plate in a predetermined position with respect to the middle plate; and the middle plate is coupled to the bottom plate by a worm gear assembly for causing the middle plate to move in a second direction with respect to the bottom plate.
According to another embodiment, the invention relates to a method for ion source positioning and adjustment. The method comprises: coupling an ion source tube to a top plate of an adjustment tool, wherein the top plate is coupled to a middle plate by at least one adjustment member for causing the top plate to move in a first direction; installing the adjustment tool by attaching a bottom plate of the adjustment tool to a chamber of a cyclotron; adjusting the at least one adjustment member until the top plate is at a predetermined position with respect to the middle plate; and driving a worm gear that causes the middle plate to move in a second direction with respect to the bottom plate, until a desired output of the ion source tube is measured.
In order to facilitate a fuller understanding of the present invention, reference is now made to the appended drawings. These drawings should not be construed as limiting the present invention, but are intended to be exemplary only.
Reference will now be made in detail to exemplary embodiments of the invention, examples of which are illustrated in the accompanying drawings.
In an ion source similar to the one shown in
The exemplary ion source adjustment tool may comprise three plates: a top plate 13, a middle plate 12, and a bottom plate 11. The top plate 13 may be coupled to the middle plate 12 by a knurled screw 19. The knurled screw 19 may go through the top plate 13 and into the middle plate 12, such that, when the knurled screw 19 is turned, the top plate 13 may slide back or forth with respect to the middle plate 12. Movement of the top plate 13 may be a linear movement along the ±X directions. A stop screw 18 placed next to the knurled screw 19 may control a relative position of the top plate 13 with respect to the middle plate 12. This relative position may vary for different cyclotrons. The stop screw 18 may go through the top plate 13 and may act as a stop when it touches a back part of the middle plate 12. The stop screw 18 may be adjusted to control how far it extends to touch the middle plate 12. Apart from the combination of a knurled screw and a stop screw, other mechanisms known in the art may also be used to control the relative position of the top plate 13 with respect to the middle plate 12. For example, a single knurled screw may be used, together with markings along the edges of top plate 13 and/or the middle plate 12, to adjust the relative position.
The middle plate 12 may be coupled to the bottom plate 11 by a worm gear assembly 304. The worm gear assembly 304 may cause the middle plate 12 to rotate slightly around a pivot 302. The rotation is typically so small that the tip of the middle plate 12 can be viewed as moving along the ±Y directions. Details of the worm gear assembly 304 and its operation will be described in connection with
To replace the ion source, the top plate 13, with the old ion source tube attached, may be removed from the chamber. Then, the old ion source tube may be replaced by a new one. An angle tool may be used to facet the slit opening on the new ion source tube in an appropriate angle. Next, the top plate 13, with the new ion source tube attached, may be re-installed in the magnet pole valley 402. Since the stop screw 18 “remembers” the relative position between the top plate 13 and the middle plate 12, such position may be easily restored by tightening the knurled screw 19 until the stop screw 18 touches the middle plate 12. A feeler gauge (not shown) may used to quickly ascertain that the original distance (approximately 1.5 mm, for example) between the puller and the ion source tube has been restored. Once the cyclotron chamber has been closed and pumped down to an acceptable vacuum level, an output of the new ion source may be measured, for example, with an ion probe. Based on the measured output (i.e., the ion probe current), the worm gear assembly may be continuously adjusted from outside the cyclotron chamber to move the middle plate 12 (and thus the top plate 13 and the ion source tube attached thereto) in the ±Y directions, until a desired ion source output is measured. For example, the ion source tube may be initially moved in one direction (e.g., +Y direction). If the ion probe current increases, the ion source tube may be kept moving in the same direction. If the ion probe current starts to drop, that is, it passes a maximum value, the ion source tube may have passed an optimal position. The ion source adjustment tool may control the ion source tube to move in an opposite direction until a maximum value is measured for the ion probe current. Apart from the adjustment upon installation of a new ion source, the optimization may also be performed during operation of the cyclotron.
Since the ion source tube's longitudinal position has been restored upon installation, and the lateral position is remotely and continuously adjustable while the cyclotron chamber is under high vacuum, service time required for the ion source may be significantly shorter than with the traditional approach. As a result, the service engineer(s) may have much less radiation exposure. Due to the faster and easier installation, highly skilled service engineers are no longer necessary for consistent results.
Referring now to
The flexible shaft may be coupled to a driving unit located outside the cyclotron chamber.
While the foregoing description includes many details and specificities, it is to be understood that these have been included for purposes of explanation only, and are not to be interpreted as limitations of the present invention. It will be apparent to those skilled in the art that other modifications to the embodiments described above can be made without departing from the spirit and scope of the invention. Accordingly, such modifications are considered within the scope of the invention as intended to be encompassed by the following claims and their legal equivalents.