This invention concerns radiation therapy, especially brachytherapy, for treating tissues which may have diffuse proliferative disease.
In brachytherapy, a radiation source or a plurality of sources are generally placed within a surgically created or naturally occurring cavity in the body. In particular, this invention relates to delivery of radiation therapy to tissue as might be found in the human breast, or to other tissue, preferably by activation of a miniature, electronic x-ray source. Such therapy often follows surgical treatment of cancer.
Radiation therapy following tumor resection or partial resection is generally administered over a period of time in partial doses, or fractions, the sum of which comprises a total prescribed dose. This fractional application takes advantage of cell recovery differences between normal and cancerous tissue whereby normal tissue tends to recover between fractions, while cancerous tissue tends not to recover.
With conventional brachytherapy, a prescribed dose is selected by the therapist to be administered to a volume of tissue (the target tissue) lying outside the treatment cavity, into which a single radiation source will be placed. Generally the prescribed dose will specify a uniform minimum dose to be delivered at a preferred depth outside the treatment cavity (the prescription depth). Also with conventional brachytherapy, since by the laws of physics radiation intensity falls off, most often exponentially, with increasing distance from the radiation source, it is generally desirable to create and maintain a space between the source of radiation and the first tissue surface to be treated (generally the cavity wall) in order to moderate the absorbed dose at the cavity surface in relation to the prescribed dose delivered at the prescription depth. This is usually accomplished by placing an applicator in the cavity which both fills and shapes the cavity into, most often, a solid figure of revolution (e.g., a sphere or ellipsoid) and positions the radiation source within a source guide situated along a central axis of the cavity so formed and through which the source may be traversed. If the applicator comprises a balloon to shape the cavity, it is preferably inflated using a fluid medium which has radiation attenuation properties similar to those of soft tissue. Water is such a medium. This choice of medium simplifies treatment planning.
Treatment planning is generally automated and is a process whereby system elements are arranged and controlled so as to deliver treatment from a radiation source to target tissue conforming to a dose prescription in an optimal manner. With the apparatus described above, the transverse distance from the source guide on the axis of the cavity to the surface of the cavity varies as the source is traversed through the source guide within the balloon. This creates differences in delivered dose, both from the effects of changing distance as well as from attenuation through varying amounts of inflation medium. These effects do not vary in the same manner as one another, and the combined variation complicates the treatment planning process significantly, particularly when the emissions or isodose patterns of the source are not truly isotropic and their emission characteristics must be accommodated in coordination with the other variations outlined above. Even with automated optimization as part of the planning process, the accuracy of dose delivery may be less than desired.
Furthermore, since the radiation intensity falls off exponentially with increasing distance from the source, when the size of the resection cavity is small, the dose incident on the resection cavity surface may be too great and may risk substantial tissue necrosis if a prescription dose is delivered at the prescription depth. Radiation overdose is to be avoided if at all possible.
One accepted standard in current brachytherapy practice is a prescription depth of one centimeter beyond the treatment cavity surface, thus defining the target tissue, which is used for treatment planning. Assuming the tissue at the prescription depth receives the desired minimum dose, the tissue nearest the source (generally the cavity surface) should not receive more than 2.5 to 3 times the prescription dose (this is the allowable dose ratio). Current standards also require that the skin not receive a dose of more than about 1.5 times the prescription dose. With a one centimeter prescription depth, this usually requires the skin be at least 6-8 mm away from the surface of an applicator engaged against the tissue in the cavity, for a typically sized applicator and cavity. A distance of less than about 6-8 mm may result in doses higher than 1.5 times the prescription dose which are known often to result in undesirable patient cosmesis. Similar complications arise in proximity to bone and other tissues/organs as well. These proximity problems commonly arise and are a contra-indication for conventional isotropic brachytherapy and further complicate the planning process and dose accuracy.
In order to assess distances from cavity surfaces to skin surfaces or to other radiation sensitive structures and to assure cavity shape and contact with the applicator is correct, imaging of the cavity and apparatus is carried out as part of the planning process. Conventional x-ray imaging or CT scanning is often used for this purpose. If, as is often the case, some distances are found to be inadequate, and cannot be overcome, brachytherapy as a treatment modality for the particular patient in question might have to be abandoned.
It is apparent that methods and apparatus are needed that address the complexities described above, simplify the planning process, improve the absorbed dose profile for use with small cavities, and make the therapy more precise, all of which would make brachytherapy an option for a greater proportion of the patient population, and more effective when applied.
In the prior art, Winkler U.S. Pat. No. 6,482,142 describes an applicator to produce an asymmetric radiation pattern in target tissue surrounding a surgical resection cavity. The patent discloses an applicator that holds radioactive isotope “seeds” in an off-axis pattern within the applicator balloon in order to produce asymmetric isodose curves with respect to the balloon volume.
The preferred radiation sources for the system of this invention are electronic x-ray sources, the output of which can be either isotropic or directional (side-firing; emitting throughout a solid angle), which can be modulated with regard to radiation penetration (voltage), intensity (current), and/or which can be switched on and off at will. Such x-ray tubes are well known in the art. One reference describing the principles and construction of such tubes is Atoms, Radiation and Radiation Protection, Second Edition, John E. Turner, Ph.D., CHP, 1995, John Wiley & Sons, Section 2.10. Directional source emissions can also be produced by selective shielding of isotropic x-ray sources following the methods described in application Ser. Nos. 11/471,277 and 11/471,013, incorporated herein in their entirety by reference, and in fact, such shielding methods can even be used to limit isotope seed emissions, thus producing similar patterns to the directional emission patterns of x-ray sources as described above. Isotope sources cannot in principle be modulated, however.
In resecting a tumor, the surgeon customarily creates a cavity which approximates a solid figure of rotation without abrupt changes in cavity surfaces, re-entrant features or tissue structures attached to but dangling from the cavity surfaces. An applicator of a predetermined shape, but similar (when inflated, if a balloon type) to the cavity shape is chosen for radiotherapy. When placed in the cavity (and inflated if of the balloon type), it is intended to fill the cavity. A tubular shaft extends from the cavity-filling portion of the applicator proximally to a hub to be positioned outside the body. Preferred applicators of this invention are of the balloon type such that the applicator can be introduced into the body cavity through a minimal incision with the balloon deflated, then when properly positioned, the balloon can be inflated to fill the cavity.
Within the tubular shaft of such an applicator, and extending into the balloon, is a source guide comprising a resilient member, normally straight, but which can be deflected to a bowed shape, at least along the length which will be positioned within the balloon. The bowed shape may form spontaneously when the guide is extended through the straight applicator shaft and released into the balloon volume, or it may be bowed in response to stress exerted within the balloon by other apparatus members. Spontaneous bowing can result from use of superelastic Nitinol, for example, according to the teachings of U.S. Pat. No. 4,665,906. Using these methods, the guide can comprise a Nitinol tube, or can comprise a polymeric tube carrying a longitudinal Nitinol member capable of forming the polymer tube spontaneously when released from its straight configuration. Alternatively, a source guide which bows in response to stress might result if, for example, a tubular polymer element is placed through the applicator shaft accompanied by a parallel string member running along the outside of the polymer tube from outside the body, through a ring, loop or other restraint (through which the string can slide) fastened near the proximal end of the balloon, and extending further and fastening to the polyester tube proximate its distal end. The distal end of the tube preferably engages a socket in the distal end of the balloon in a manner permitting rotation of the tube relative to the balloon. When fully inserted into the applicator, restraining the string while pushing on the proximal end of the polyester tube will bow the tube within the balloon volume. Yet another source guide embodiment can be fashioned having a variable bow or other shape, similar to a steerable catheter (e.g., see Enpath Medical, Inc., Plymouth, Minn.). Many such catheters are available and are often controlled by longitudinal wires positioned in a dispersed manner around the circumference of the catheter and pulled differentially to alter the catheter shape. A source guide can be fashioned similarly and controlled statically or dynamically (during treatment) to position a source, placed within and/or traversed internally, through substantially any arbitrary solid figure of revolution, e.g., such as a cylindrical or hour-glass shape.
As an alternative to manipulation of a source guide during treatment, a series of satellite guides, with or without a central guide, may be utilized to shape the emission pattern of the radiation. This arrangement and other apparatus utilizing the same bowed or shaped members within the balloon will occur to those of skill in the art and will be within the scope of the invention.
Since the shape of the balloon and cavity is substantially predetermined by the resection and balloon choice, the bowed shape of the source guide or guides can be fashioned to follow the cavity wall, preferably but not necessarily at a constant distance, with either style of bowed member. When a source positioned within such a bowed guide is translated axially, coordinated rotation of the guide tube by an external manipulator will sweep the source throughout the cavity at a uniform distance from the cavity wall. Thus the distance to the wall, and the amount of attenuating medium between the source and the cavity wall, will be constant; therefore the radiation incident on the cavity wall will be uniform, as will the dose at the prescription depth, although lower than at the wall. The translation and rotation of the source in the bowed guide tube can approximate a spherical source emitting from everywhere on its surface, so dose does not fall off in an inverse square relationship to distance but falls off a small amount with distance because of the spherical geometry. The source, if isotropic, can be partly shielded such that backward emissions (opposed to the preferred direction) may be substantially eliminated.
Importantly, when a small cavity is to be used for brachytherapy as well as in other circumstances, the radiation emissions can be directed away from the nearest portion of the cavity surface. Since the radiation intensity of an isotropic source decreases exponentially with distance, increasing the distance from the source to the tissue at which the radiation is directed has the effect of reducing the distant cavity-surface incident dose in relation to the prescription dose. In the limit, satellite source guides (or a single guide) can be positioned and fastened at or near the surface of the balloon, maximizing the distance to the opposite balloon surface. Again, and only where the source is isotropic, shielding can be applied to the part of the source guide circumference nearest to or in contact with the cavity surface such that radiation emanating from within the guide would be substantially eliminated on the cavity surfaces nearest or immediately adjacent to the radiation source. Where the source is directed and aimed away from nearby cavity surfaces, however, no shielding is necessary to produce the same effect.
If imaging has revealed radiation-sensitive anatomy unacceptably close to the treatment cavity, the treatment plan can include an over-ride which can interrupt the uniform dose delivery process such that sensitive tissues are spared an overdose and risk of tissue necrosis. Alternatively, radiation sensors placed on or within the body near the at-risk structures can provide monitoring, providing outputs to the system controller signaling the need for a locally reduced dose. Such sensors can be placed using adhesives or needle methods, and power and signal communication can be by conventional wiring or by known wireless methods. Such over-ride might take the form of reduced dwell time of the source when directed toward such structures, or where an x-ray source capable of modulation is used, a reduction in penetration distance or dose intensity can be employed, including shut-off of the source.
The source may be traversed through the cavity in either step-wise or continuous fashion, compensated only for quantity of surface area swept by the solid angle as the source reaches pole of the cavity. The path may be helical or may reciprocate first clockwise, then counterclockwise through 360°, stepping axially after each rotation. Alternatively, the guide may be held at a constant angle while the source translates through the length of the balloon, after which the angular orientation is incremented, and the translation repeated. The speed of source traverse may be used as a dose delivery variable, or the source may be modulated, assuming an x-ray source is being used.
With the methods suggested above, planning is simpler, the ratio of dose incident on the cavity surface to prescription dose at prescription depth can be decreased, and dose accuracy can be improved in many instances. The risk of tissue necrosis is thus minimized, and the proportion of patients for which brachytherapy is indicated is increased.
In
One alternative to a tubular Nitinol guide is a polymer tube guide with provision for a Nitinol member, for example a wire, which is carried by the polymer tube, but preshaped as described above such that the strength of the Nitinol shapes the polymer tube in the absence of other restraint (for example when the polymer and Nitinol wire are contained within the shaft 16). In such a construction, the Nitinol may be confined to a separate lumen within the polymer guide, or it can also be contained within the source lumen.
In yet another alternative construction, some polymers can be conditioned to behave in a manner similar manner to that of Nitinol as described above by methods familiar to those of skill in the art. An example is polyester. A straight tubular element of polyester can be heat set into a curve with the help of curved fixturing, and allowed to cool. It may then be straightened for insertion into the straight lumen of the shaft 16 for insertion into the cavity of the patient, then subsequently advanced into the volume of balloon 12 where it will resume its curved shape. Methods for such shaping are well known to those of skill in the art.
As explained above,
Where the emissions from the radiation source 18 are isotropic and the cavity surface being treated is that nearest the source, the attenuation by the inflation medium opposite the cavity surface being treated (in a sense, behind the emissions of interest) may be inconsequential. If not, the effects of such emissions must be accounted for and included in the treatment planning process. Where the emissions are truly directional, backward emissions can be ignored, but the source catheter 20 and source 18 must be rotated in unison as the source guide is rotated such that the solid angle of emissions continues to address the surface area to be treated, unless the directionality is provided by shielding secured to the guide. One method to assure such directional coordination is to key the catheter rotationally within the source guide, for example by making the lumen of the guide non-circular in cross section, and the outside of the catheter matching in section and size such that, substantially at least, only translation of the catheter within the guide is possible. Alternatively, separate manipulators for catheter and source guide, positioned outside the body and coordinated rotationally by the controller, can achieve the same effect, although differential torsion may require torque resistant construction of catheter and guide in a manner to resist such error. The methods of U.S. Pat. No. 4,425,919 can be employed in this regard. Manipulation of the source may be continuous or intermittent, and rotation can be continuous in one direction, or periodically reversed. Where electronic x-ray sources are employed, periodic reversal of rotation is preferred since that eliminates the need for rotating high-voltage electrical connections. A clockwise 360° rotation followed by counterclockwise reversal followed by a translational step is an example of such preferred manipulation and can be iterated to cover the entire cavity surface. Translation can be simultaneous or sequential, so long as all cavity surfaces are addressed for treatment. Simultaneous movement can be used to generate an essentially helical path of emission. Where the emissions of source 18 are constant, the speed of manipulation can be varied to locally adjust absorbed dose. Where, as with modulated x-ray sources, emissions can be varied, manipulation speed can be constant, or a combination of speed and modulation can be used to accommodate local requirements.
In use, the source guide 22 is advanced into the applicator apparatus 24, advancing the string 30 as well, until the distal end of the guide engages the socket 28 at the distal end of the balloon 26. When so engaged, the string 30 is restrained from further advancement from outside the body, but the guide is forced further into the applicator against the resistance of the string. Such advancement forces the bow to form within the balloon volume as shown in
As an alternative to the use of directional sources, substantially similar effects can be obtained practicing the shielding teachings of copending Ser. Nos. 11/471,277 and 11/471,013, incorporated herein by reference in their entirety. By these methods, isotropic x-ray sources and even isotope sources can be made directional, and to some extent modulated by the imposition of elements which are partially attenuating between the source and cavity surface being treated.
As an example,
Each manipulator depicted comprises a sled 110 riding on and confined to rails 112, with its translation actuated by a servo-motor 111. A rotary spindle and collet 114 for gripping the catheter 20a or the guide 14a is mounted on the sled 110 in bearings (not shown), and connected by a belt or gear drive 116 to a servo-motor 118. The catheter 20a (left manipulator) or source guide 14a (right manipulator) thus rotate with their spindles/collets 114. The servos 111 and 118 are responsive to the system controller (not shown) which manages delivery of the treatment plan.
As pictured, the left and right manipulators are capable of being independently controlled, thereby independently positioning the source catheter 20a and source guide 14a, but must be coordinated by the controller to deliver the desired treatment plan. Depending on system requirements, other manipulators may be devised, and such configurations will be apparent to those of skill in the art.
In contrast to manipulation of single source guides as described above, modeling of absorbed dose profiles obtained with a variety of alternate constructions using multiple curved guides positioned around the axis of the applicator balloon has produced several embodiments having important utility. Some of these configurations additionally include a central source guide.
We have found that when such a satellite configuration as that described in relation to
Note that because the applicator balloon 174 preferably is filled with a liquid having similar attenuation properties as tissue as stated above, the balloon and resection cavity surface do not create a discontinuity in the isodose patterns. In effect, the radiation emitted is attenuated as though passing through a uniform field. Therefore the treatment plan can be fashioned based on distances to deliver the prescribed dose with an acceptable dose ratio to the target tissue as though the balloon and resection cavity surfaces were not present. This illustrates the rationale for using a liquid balloon inflation medium with attenuation properties substantially matched to tissue. If not matched, the problem becomes more complicated, and the position of the balloon/cavity surface becomes important.
Where shielded or directional sources are used, cross-firing (emitting away from the closest tissue and across the balloon volume) can be used to reduce the absorbed dose ratio (surface to prescription depth doses). When used with small balloons and miniature x-ray sources which are easy to shield compared to isotopes, or can be designed to be directional rather than isotropic, this technique is particularly useful, including an embodiment where the source guides are attached to, but are outside the balloon surface. Because of the inherent isotropic nature of isotopic radiation and greater penetration depth of common medical sources, shielding of such sources to create directionality must be more robust and therefore tends to be relatively impractical in such an embodiment.
Such an embodiment with source guides positioned outside the balloon 184 is shown in
With directional sources, control of both translation and rotation are necessary to properly direct emissions, in this case across the volume of the balloon. Such manipulation is, for example, enabled by apparatus as described in the discussion of
Note again that a balloon 184 is shown in
By utilizing the apparatus and methods of this invention, the distance from the source to the cavity surface can be made substantially constant or increased where advantageous. Control of dose distribution and profile is greatly increased. Treatment planning is thereby simplified and delivered dose characteristics are improved. Furthermore, practice of the invention makes brachytherapy an attractive alternative for a greater population of patients than previously possible.
The above described preferred embodiments are intended to illustrate the principles of the invention, but not to limit its scope. Other embodiments and variations to these preferred embodiments will be apparent to those skilled in the art and may be made without departing from the spirit and scope of the invention as defined in the following claims.
This is a continuation-in-part of application Ser. No. 12/012,010, filed Jan. 29, 2008, which is a continuation-in-part of application Ser. No. 10/464,140, filed Jun. 18, 2003, now U.S. Pat. No. 7,322,929, and application Ser. No. 11/925,200, filed Oct. 26, 2007. The disclosures of both are fully incorporated herein by reference.
Number | Date | Country | |
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Parent | 12012010 | Jan 2008 | US |
Child | 12082492 | US | |
Parent | 10464140 | Jun 2003 | US |
Child | 12012010 | US | |
Parent | 11925200 | Oct 2007 | US |
Child | 10464140 | US |