The invention relates to the medical field and in particular to the treatment of cancer and prostate problems.
In many diseases it is desired to destroy or affect a non-desired tissue without harming the adjacent normal tissue. A non surgical approach has many advantages, such as shorter recovery time and shorter treatment time. Common non surgical approaches are:
Examples of the need for such non-surgical procedure are the destruction of tumors, shrinking of an enlarged prostate and collapsing of diseased parts of a lung affected by emphysema. The use of high intensity focused ultrasound (HIFU) is well known. Ultrasound destroys the undesirable tissue be creating heat and also mechanical damage to the cells. In this disclosure the terms “heating” and “ablation” are used interchangeably and the word “heating” should be broadly interpreted as any mechanism of coupling energy into a tissue, whether the main reaction is heating or not. One advantage of ultrasound is that it can be finely focused into a small spot, as the wavelength of the commonly used ultrasound in such applications is on the order of one mm. A common problem is the need to focus a high energy beam on the non-desired, or diseased, tissue without causing damage to healthy tissue. Since healthy tissue should not be subjected to temperatures much above 40° C. and the undesired tissue should ideally be heated to over 60° C., the increase of temperature in the undesired tissue has to be many times higher than the surrounding tissue (23 degrees vs. 3 degrees in this example when body temperature is 37° C.). Sometimes it is required to heat up the undesired tissue to as high as 90° C. In such a case the temperature increase of the undesired tissue, 53°, is almost 20 times higher as the healthy tissue. Prior art attempts to overcome the problem were local cooling and the superposition of two or more sources of ultrasound. Local cooling can only protect a thin layer of tissue, because of the poor heat conductivity of tissue. The superposition of two or more sources is disclosed in US patent 2005/0038339. When two sources are focused on the same spot the heating of the healthy tissue is reduced by a factor of 2, as the malignant or otherwise undesired tissue is exposed to both beams while the adjacent tissue is exposed only to one beam, assuming beams overlap only over the target area. In the previous example it was shown that the undesired tissue will require from seven to twenty times the temperature increase of the desired tissue (23-53 degrees vs. 3 degrees). Even after allowing for the fact that the beam is more concentrated over the target area, a large number of beams will be required to achieve the desired ratio. This is particularly true for treating enlarged prostates and prostate cancer, where the transition from heated to non-heated area has to be very sharp. Such an array of many transducers is bulky and expensive. The invention allows achieving the equivalent of a very large number of beams using the simplicity and low cost of a single beam. Also, because of the fixed mechanical constraints of US patent 2005/0038339, a system configured for breast cancer (as in the patent) will not be suitable for prostate cancer. A system according to the present invention can be used to treat any part of the body simply by setting up a different scan pattern.
The invention can selectively heat a diseased area, such as a tumor, in the body while minimizing heating of healthy surrounding tissue. This is done by exposing the undesired tissue to a scanning focused ultrasound beam arriving from different angular directions at different times, all directions passing through the undesired tissue. The system can scan the target area with low power ultrasound, and then activate the higher power over the selected target areas.
One aspect of the invention is maximizing the heating of the diseased (or otherwise undesirable) tissue while minimizing heating of the surrounding tissue. This can be achieved by moving around the energy source in order for the heat creating beam to arrive from different directions at different times, all directions having a common point of intersection that is located within the diseased tissue. If all these directions pass through the diseased tissue, the diseased tissue will be heated continuously while the surrounding tissue will be heated intermittently. A similar method is employed today in radiation therapy for cancer; however using heat energy has a significant advantage: the effect or radiation, such as X-ray or radioactivity, is cumulative while the effect of heating is non-cumulative. Heating a tissue by 30 degrees will permanently change it, while heating it 10 times by 3 degrees will have no effect. In the case of radiation the effect will be cumulative. The non-cumulative nature of heating allows the re-use of the same direction after the heat dissipated, a process taking from seconds to minutes.
Another aspect of the invention is the need to match the area and depth of the heated area inside the body, which corresponds to the focused spot size and depth of focus, to the treated organ. In case of small organs such as a prostate the heated area can be a few cubic centimeters and it has to be defined with a accuracy of a few millimeters, with the temperature falling off from, by the way of example, from 60° C.-90° C. degrees to 40° C. over a few millimeters. This is difficult to achieve with RF, microwave or other energy forms but relatively easy to achieve with high intensity focused ultrasound. The focused spot size is related to wavelength, transducer size and tissue properties. It is easiest to express the relationship as a function of the f/# of the transducer, f/# being the ratio of the focal length to the diameter of the transducer. The size of the focused spot is approximately 1.2f/#×wavelength and the depth of the focused zone is approximately 3(f/#)2×wavelength. The common frequencies used for high intensity ultrasound are from 0.5 MHz to 5 MHz, with corresponding wavelengths of about 1.3 mm-0.13 mm. Using these numbers and an f/1 transducer a focused spot of 0.2 mm-2 mm can be achieved. A low f/# is desired not only for achieving a small focused spot but also to ensure that the power density becomes large only in the vicinity of the focused spot. The “depth of focus” in this example, defining the depth of the heated tissue, will be about 0.6 to 6 mm, depending on the frequency used. By selecting the f/#, a large degree of control is possible. More advanced beam shaping techniques can be used to improve these figures. For example, apodizing can greatly increase the focal depth. Clearly the focused spot can be created from a planar transducer by using an acoustic focusing lens of a phased array transducer. The alternative is to use a spherical or parabolic transducer. Such a transducer usually comprises a plurality of smaller transducers operating in parallel.
A third aspect of the invention is the ability to use the high intensity transducer at a lower intensity in order to scan the treatment area and create a 3D map of the area. This can be done by using the same transducer or by a second, co-located transducer. Such an arrangement eliminates any position offset errors between the diagnostic scanning system and the treatment system. Any position offset error between such systems will cause a shift between the desired treatment volume and the actual one.
The method of taking advantage of the non-cumulative heating effect is shown in
Since the robot can be programmed for any scanning pattern the same system can be used to treat different cancers and medical conditions such as breast, liver, colon, bone and other cancers as well as heating non-malignant tissue. An example of treating non-malignant tissue is destroying or liquefying fat cells for cosmetic reasons.