the design of the loopless coil is shown in fig3 . the probe is housed inside a tandem applicator . the probe includes a loopless antenna , decoupling / matching circuits and a balun . in the following subsections , the components of the probe are described . fig2 a is an image obtained with a phantom illustrating the sensitivity of a loop coil in accordance with the present invention by itself . fig2 b shows the sensitivity of a loopless coil or antenna in accordance with the present invention by itself . fig2 c shows the combined sensitivity of a loop coil and a loopless coil in accordance with the present invention . the loopless antenna is a coaxial cable with extended inner conductor and is used for receiving signal during a magnetic resonance imaging examination . since it has a very small profile , it can be used in the body cavities for the purpose of acquiring high signal - to - noise ratio images around the region it is placed . in this work , the loopless antenna is used inside a brachytherapy tandem applicator that can be placed inside the cervix with the aim of high - resolution imaging of cervix . details of the design are shown in section in fig4 . the coaxial portion of the design is constructed by using ptfe tubing with inner diameter of 1 mm , outer diameter of 1 . 3 mm . the length of the wire is adjusted to quarter wavelength . the tubing is covered with a copper braid with a wall thickness of 0 . 25 mm . a 32awg magnet wire is used as inner conductor . the extended inner conductor is coiled with diameter of 2 . 13 mm and length of 3 . 6 cm . the number of the winding of the coil is 186 . a bnc connector is soldered to the proximal end of the loopless antenna . all structure is covered with a polyester heatshrink with wall thickness of 0 . 076 mm . balun ( balanced - unbalanced transformer ) is a frequently used circuit in many applications including microwave circuits and antenna . in this application , it is used to prevent shield currents on the coaxial cables . the unwanted shield currents may affect the signal uniformity and also may cause excessive heating . the design of the balun used in this application is shown in fig3 . the balun is placed in the middle of the coaxial cable and is 33 cm away from the distal end and 48 cm away from the proximal end . the balun is constructed by winding the coaxial cable in 4 loops and placing it inside a cylindrical copper box with 2 . 5 cm diameter and 3 . 5 cm length . at the proximal end of the balun the outer conductor of the probe is shorted to the copper box and then the balun was tuned using a single atc magnetic resonance compatible b type 70 pf capacitor . the aim of the decoupling circuit is to prevent induced currents on the probe during rf transmission by the body coil . decoupling is achieved by simply placing a shunt pin diode at the proximal end of coaxial cable as shown in fig3 . when the diode is on , the quarter wavelength wire transforms the low impedance of the diode to a high impedance value at the distal end of the coaxial cable and hence decreases induced currents . in this design , no tuning is required for matching because the loopless antenna &# 39 ; s impedance is already very close to the characteristic impedance of the coaxial cable . testing of the endocervical mr probe can be separated into three main parts : electrical testing , safety testing , and imaging . antenna impedance : antenna impedance is an important parameter for the performance of the loopless antenna . in an article by ocali et al . “ intravascular magnetic resonance imaging using a loopless catheter antenna ,” magnetic resonance in medicine , vol . 37 ( 1 ), p . 112 - 118 ( 1997 ), it was shown that the square root of the real component of the antenna impedance is inversely proportional with signal - to - noise ratio . in the bare - wire antenna case , the minimum observed impedance was 35 ohms . it was shown that when the antenna is insulated because of some practical requirements , the real part of the impedance goes up and degrades the snr performance of the design . in order to understand the performance of the design , we have measured antenna impedance inside the brachytherapy applicator . salinated water ( 4 % salt ) was used to mimic human cervix . the length of the coiled portion of the loopless antenna was optimized in order to minimize the antenna impedance . 62 ohms was obtained when the coil length was 3 . 6 cm . although this impedance higher than 35 ohms that was obtained by the bare - wire antennas , loss of 33 % reduction in snr reduction ( square root of 62 / 35 ) is acceptable for this application . characteristic impedance : when the characteristic impedance of the coaxial cable matches the antenna impedance , the signal transmission is obtained with minimum loss . in most coils there is a significant difference between coaxial cable impedance and the antenna impedance and therefore a matching circuit is needed . in loopless design as mention above the antenna impedance was found to be 62 ohms . if the characteristic impedance of the coaxial cable that we built matches this value , there will be no need for the matching circuit . in order to measure the characteristic impedance of the manufactured coaxial cable , a 50 ohm load is connected to quarter wavelength coaxial cable and impedance is measured as 59 ohms . therefore the characteristic impedance is calculated ( square root of 50 × 59 ) as 54 ohms . this is in an acceptable range of 62 ohms and therefore there is no need for matching circuit . balun : balun circuit increases the series impedance of the shield of the coaxial cable without affecting its transmission properties . the impedance of the balun was measured by a network analyzer as 3 kohm at 123 . 23 mhz . the adequacy of this value is later tested by heating and imaging tests . decoupling : the performance of the decoupling circuit is measured as the impedance of the antenna during rf transmission . siemens 3t trio scanners provide a dc bias current during this period . the pin diode in the circuit turns on and its rf impedance becomes low . quarter wavelength coaxial cable transforms this low impedance value to a high impedance value . depending on the loss on the coaxial cable this value of this high impedance may vary . however , the effectiveness of the decoupling circuit high depends on this impedance value . for the purpose of understanding the performance of the decoupling circuit we have measured impedance of the shorted quarter wavelength coaxial cable as 2 . 8 k ohm . this value is significantly higher than the antenna impedance of 62 ohms suggesting significant suppression of induced currents . further testing of the decoupling performance was done using imaging experiments . the basic design of the loop coil is shown in fig6 and 7 . the coil has a loop coil , decoupling / matching circuits , coaxial cable and balun ( current trap ). in the following subsections , the components of the probe are described in detail . the loop coil was embedded into the nucletron ct - mr ring applicator which has 60 ° angle and 3 . 7 cm diameter . the ring applicator was cut into two parts with the help of the cnc and then a new 3 . 3 cm groove was opened for the loop coil ( fig6 ). the loop coil was created by a capper magnet wire with 1 mm diameter . the wire was shaped such that it could be embedded into the previously opened groove ( fig7 ). the coil was tuned with two parallel 20 and 3 . 9 pf atc nonmagnetic capacitor matched with a single 270 pf capacitor ( fig7 ). the measured impedance of the loaded coil was 52 ohm at 123 . 23 mhz . the aim of the decoupling circuit is to prevent induced currents on the probe during rf transmission by the body coil . decoupling is achieved by placing a shunt pin diode at the proximal end of micro strip . the micro strip is formed by two parallel conductors affixed to an insulating carrier . the conductors may be approximately 2 mm wide and spaced from each other by approximately 3 mm . when the diode is on , the circuit transforms the low impedance of the diode to a high impedance value at the loop coil and hence decreases induced currents . in order to create the decoupling circuit the matching capacitor was removed from the coil and soldered to the distal end of the micro strip . then the proximal end of the micro strip was shorted and the impedance on the capacitor was measured . the distance of the short circuit to the capacitor is adjusted such that the measured impedance would be real . a 240 ohm real impedance was observed when the distance between capacitor and short circuit was adjusted to 12 mm . then the short circuit is replaced with a macom ma4p1461f - 1072 pin diode and the decoupling circuit is soldered to the loop coil ( fig1 ). the size of the decoupling circuit can be minimized and embedded into the applicator . the loop coil is connected to the mr scanner using a 40 cm 50 ohm rg58 coaxial cable with a nonmagnetic connector at the distal end . an illustration of a complete version of the modified ring applicator is given in fig5 . the diameter of the loop antenna is adjusted such that it could be easily inserted into the applicator during the imaging and taken out during the radiation brachytherapy procedure . both channels of the coils were connected for the aforementioned testing to the mr scanner with nonmagnetic sma connector . however , in order to satisfy clinical requirements , a medical connector that will be sterilizable and therefore reusable will be used instead . testing of the coil can be separated into two main parts : phantom imaging experiments and animal experiments . imaging experiments are crucial in order to test the coil performance . with this motivation , we designed a cylindrical ( water with 4 gr / lt copper sulfate and 1 gr / lt salt ) phantom with 22 cm diameter and 35 cm length . kiwi was used in order to simulate human cervix . the phantom is placed in the center of the siemens trio 3t mr scanner and the endocervical magnetic resonance coil is placed at the center of the phantom . imaging parameters are t1 - weighted turbo spin echo , tr / te = 800 / 12 , slice thickness 2 . 6 mm , fov read 150 mm , fov phase 100 mm , averages 2 concatenation 2 , distance factor 30 %, number of slices 15 , bw = 260 hz / pixel . in order to evaluate the performance of the coil , a kiwi phantom was also imaged with the body matrix coil using same parameters . the snr of the image obtained using the endocervix coil is measured as approximately 5 times higher than the snr of the image obtained using a body matrix coil . an in - vivo canine experiment was made using a siemens 3t trio scanner . a turbo spin echo sequence was used with the following imaging parameters : a slice thickness = 4 mm , tr = 6 seconds , te = 114 milliseconds , pixel bandwidth 250 hz / pixel , flip angle = 120 degrees , the field - of - view = 20 by 20 centimeters . the resulting t2 - weighted coronal images of the female canine are given in fig8 . fig8 a , 8 b and 8 c was obtained solely with the loopless coil . all of the pelvic space is highly visible . in fig8 b , the image obtained with the loop coil is given . the region between the cervical canal and the uterine cavity can be seen easily . in the loop coil image ( fig8 b ), endometrium and internal os can be observed much better than the conventional mr imaging strategies ( fig8 a ). in fig8 c , the combined image is shown . the cervix , uterus and all pelvic viscera can be clearly seen in the combined image . as shown in fig9 , the tandem applicator can be provided with one or more mri - visible markers , such as metal rings that proceed around the exterior of the applicator housing . these markers are visible in a magnetic resonance image obtained with the coil assembly in place at a patient in an mri apparatus . the markers allow the position and orientation of the applicator to be identified from the magnetic resonance image . a further embodiment employing mri - visible markers is shown in fig1 wherein , in addition to mri - visible markers located on the tandem applicator housing , or the conductor therefor , a control panel is attached to the assembly . the control panel has three indicators thereon that are visible in a magnetic resonance image , which designate the axes of a cartesian coordinate system , in order to further assist determination of the position and orientation of the overall assembly in a magnetic resonance image of a patient with the applicator applied thereto . the invention a simple two - channel coil designed that can easily be mounted on a ring hdrb applicator . the coils produce high signal intensity in the target region and the cervix , the uterus and all the pelvic viscera can be clearly seen from the obtained in - vivo images . it should be noted that these coils are designed for human anatomy , hence their structure is not very suitable for animal anatomy . as a result , the performances of the coils drop , but the inventive structure introduces improvements over the current techniques . although modifications and changes may be suggested by those skilled in the art , it is the intention of the inventors to embody within the patent warranted hereon all changes and modifications as reasonably and properly come within the scope of their contribution to the art .
a radio - frequency coil for obtaining magnetic resonance data for imaging the cervical region of a patient has a loop coil contained in a housing of an applicator assembly that is adapted for placement against the cervix of the patient , and a loopless antenna contained in a tandem applicator of the assembly , that is adapted for intracorporeal placement in the cervix of the patient .