The present disclosure relates generally to medical devices, medical device systems, and medical device methods; and more particularly to medical devices, medical device systems, and medical device methods for use during magnetic resonance imaging.
Magnetic resonance imaging (MRI) can create images of internal aspects of structures by using magnetic fields of various field strengths. When performing MRI, sometimes it is desirable to enhance the visualization of a particular aspect of a structure or an object within a structure, for better signal-to-noise ratios in MRI images. For instance, sometimes it is desirable to enhance the visualization of a medical device when performing an MRI.
One way to enhance visualization when performing MRI is to use a resonator device. An LC circuit can form a basis for a resonator device. An LC circuit with a fixed inductance and a fixed capacitance can resonate at a particular frequency. However, an MRI can use magnetic fields with a range of field strengths to cause material in a structure or an object to resonate over a range of frequencies. Thus, a resonator device with a fixed inductance and a fixed capacitance may not resonate over a range of frequencies.
The illustrations provided in the Figures may not be to scale.
The figures herein follow a numbering convention in which the first digit or digits correspond to the drawing figure number and the remaining digits identify an element or component in the drawing. Similar elements or components between different figures may be identified by the use of similar digits. For example, 110 may reference element “10” in
Embodiments of the present disclosure are directed to resonator devices, resonator systems, and methods of using the resonator devices. Generally, a resonator device can be used in conjunction with a medical device, including a deliverable device, deliverable in a lumen of a body. One embodiment of the present disclosure includes a resonator with an adjustable capacitance for a medical device, which can enhance visualization when performing MRI.
The MRI scanner 110 is a cylindrical tube. The coil 130 is electrically conductive. The coil 130 begins at one terminal 120, winds around the MRI scanner 110 in helical form, and ends at another terminal 120. Each terminal 120 is connected to the coil 130 so that electrical current can flow from the terminal 120 through the coil 130.
When electrical current flows through the coil 130 it can create a static magnetic field, which is represented by the static magnetic field lines 140. Each of the static magnetic field lines 140 has a direction, which is represented by arrows. The direction of the magnetic field lines 140 can depend upon the direction in which electrical current flows through the coil 130.
The static magnetic field also has a magnetic field vector 150. The magnetic field vector 150 coincides with a central axis of the MRI scanner 110. The magnetic field vector 150 also has a direction which can depend upon the direction in which electrical current flows through the coil 130. In MRI, the static magnetic field can cause hydrogen protons within the field to align with the magnetic field vector 150. The magnetic field vector 150 can also serve as a reference direction when performing MRI, as described in
The presence of the static magnetic field causes the hydrogen proton 238 to precess in the spin direction 232. The hydrogen proton 238 precesses in the spin direction 232 around an axis that is parallel to the magnetic field vector 250. The reference arrow 234 indicates that the precessing of the hydrogen proton 238 creates the reference circle 236. The magnetic field vector 250 is perpendicular to the reference circle 236.
The RF pulse 270 can be an oscillating electro-magnetic field, propagating in a direction perpendicular to the magnetic field vector 250. The RF pulse 270 includes the RF pulse magnetic field vector 280 and the RF pulse electrical field vector 290. RF pulse magnetic field vector 280 and the RF pulse electrical field vector 290 can be perpendicular to each other and perpendicular to the direction in which the RF pulse 270 propagates.
An MRI machine can create an RF pulse at a certain frequency called the Larmor frequency. The Larmor frequency is a frequency at which certain protons resonate. The Larmor frequency differs for protons of different elements and for static magnetic fields of different strengths. Many MRI machines create RF pulses for hydrogen protons, and this is assumed throughout this document unless otherwise indicated. For hydrogen protons, the Larmor frequency is 42.9 MHz for each Tesla of static magnetic field strength.
Some MRI machines can create static magnetic fields with flux ranging from 0.3 Teslas to 7.0 Teslas. Many MRI machines create static magnetic fields with flux ranging from 1.5 Teslas to 3.0 Teslas. Thus, MRI machines that create static magnetic fields with flux between 0.3 and 7.0 Teslas operate at Larmor frequencies between 13 and 300 MHz. Similarly, MRI machines that create static magnetic fields with flux between 1.5 and 3.0 Teslas operate at Larmor frequencies between 64 and 129 MHz.
In MRI, a resonator device can enhance visualization of images by resonating at the Larmor frequency. In some instances, a resonator device can enhance visualization of images by resonating at a frequency close to a Larmor frequency, depending on the frequency response of the device. A resonator device based on an LC circuit with a fixed inductance and a fixed capacitance may not resonate over a range of frequencies. Additionally, an inductance of an LC circuit may change under certain conditions or may change in certain applications, such as an inductor coil with a radius that changes when used with an expandable stent. As examples, a resonator device can be used with a balloon expandable stent or a self-expandable stent. However, a resonator device with an adjustable capacitance can resonate over a range of frequencies, as described in
The inductor coil 304 is external to the circuit package 308, in the resonator device 301. The circuit package 308 encapsulates electrical components, including sensors 310, an adjustable capacitance 320, and an adjustable capacitance control 330. The inductor coil 304, the connecting conductors 306, at least a portion of the adjustable capacitance 320, and at least a portion of the adjustable capacitance control 330 together form an LC resonator circuit. In the resonator device 301, the circuit package also encapsulates a processor 360, a memory, 370, a power source 380, and a selector 390, which relate to the LC resonator circuit, as described herein.
In the embodiment of
In the resonator device 301 of
In the resonator device 301, the processor 360 is also connected to the memory 370, the power source 380, and the selector 390. The memory 370 can store data which can be used by the processor 360. The processor 360 can communicate with the memory 370 through its connection to the memory 370. The power source 380 can provide the processor 360 with electrical power so the processor 360 can perform its functions, as described in
The power source 380 can have different forms in various embodiments. In one embodiment, the power source 380 can generate electrical power from an electro-magnetic field. As examples, the power source 380 can be the inductor coil 304, another conducting coil, or a secondary resonator circuit. In this embodiment, the powering electro-magnetic field can be an RF pulse from an MRI machine or some other field. In various embodiments, an RF pulse can provide power over longer distances. In one embodiment, the power source 380 can be a battery or a rechargeable capacitor. In various embodiments, the power source 380 can also generate electrical power from an alternating magnetic field, such as a field within a transformer, for powering by induction over shorter distances.
In one embodiment, the processor 360 of
A range of adjustable capacitance for an LC resonator circuit of a resonating device can be estimated, based upon a potential range of MRI Larmor frequencies of and an estimated range of inductor coil inductances. A potential range of MRI Larmor frequencies can be determined as described above. An estimated range of inductor coil inductances can be estimated by mathematically modeling an ideal inductance coil.
An inductance for an ideal inductance coil can be mathematically modeled by using an ideal inductor formula. In that formula, L=(μ*N2*π*r2)/l where L is inductance in Henries, μ is a factor equal to 1.26×10−7 Henries per meter, N is a number of windings in an inductor coil, r is a radius of the inductor coil in meters, and l is a length of the inductor coil in meters. For example, the ideal inductor formula can be used to mathematically model an inductance for an ideal inductor coil sized to match various dimensions of a stent. In this example a stent can range in radius from 0.001 meters to 0.005 meters and in length from 0.008 meters to 0.07 meters. Also in this example, an inductor can have 1 winding for every 0.001 meter of inductor length or 1 winding for every 0.002 meter of inductor length. Using these example numbers for an ideal inductance coil yields an estimated range of inductor coil inductances from 0.79 nanoHenries to 0.69 microHenries.
A range of adjustable capacitance for an LC resonator circuit of a resonating device can be estimated, based upon a potential range of MRI Larmor frequencies, a potential range of inductor coil inductances and an LC circuit resonance formula. In the LC circuit resonance formula, f=1/(2*π*√(L*C)) where f is a resonant frequency of the LC resonator circuit, L is an inductance of the LC resonator circuit at the resonant frequency, and C is the capacitance of the LC resonator circuit at the resonant frequency. Since a potential range of MRI Larmor frequencies can be determined and a range of inductor coil inductances can be estimated, as described herein, the LC circuit resonance formula can be solved for a range of adjustable capacitance. As an example, using a potential range of MRI Larmor frequencies from 13 to 300 MHz and a potential range of inductor coil inductances from 0.79 nanoHenries to 0.69 microHenries in the LC circuit resonance formula yields an estimated range of adjustable capacitance from 0.41 picoFarads to 0.19 microFarads, which can be created as described in
The inductor coil 304 is external to the circuit package 308, in the resonator device 302. The circuit package 308 encapsulates electrical components, including the sensors 310, the adjustable capacitance 320, and the adjustable capacitance control 330. The inductor coil 304, the connecting conductors 306, at least a portion of the adjustable capacitance 320, and at least a portion of the adjustable capacitance control 330 together form an LC resonator circuit. The circuit package also encapsulates a processor 360, a memory, 370, a power source 380, and a selector 390, which relate to the LC resonator circuit, as described herein.
In the resonator device 302 of
The adjustable capacitance 320, as a whole, is electrically in series with the inductor coil 304. One side of the inductor coil 304 is electrically connected to one side of the adjustable capacitance 320 through one of the connecting conductors 306. Another side of the inductor coil 304 is electrically connected to another side of the adjustable capacitance 320 through another of the connecting conductors 306 and through the adjustable capacitance control 330. Thus, while the varactor 321, and the capacitors 322, 324, 326, and 329 are electrically parallel to each other, the adjustable capacitance 320, with its particular capacitance value, is electrically in series with the inductor coil 304. In other words, the inductor coil 304 and the adjustable capacitance 320 respectively form L and C components of the LC resonator circuit, as will be understood by one of ordinary skill in the art. The adjustable capacitance 320 is electrically connected to the adjustable capacitance control 330.
In the resonator device 302, the adjustable capacitance control 330 includes a varactor controller 331, and electrical switches 332, 334, 336, and 339. The varactor controller 331 controls an adjustable capacitance of the varactor 321. Each of the electrical switches 332, 334, 336, and 339 has an open state and a closed state. In the closed state, an electrical switch forms an electrical connection that allows electrical current to flow through that switch. In the open state, an electrical switch forms an electrical break that prevents electrical current from flowing through that switch. Each of the electrical switches of
In the embodiment of
In the resonator device 302 of
In the embodiment of
The processor 360 is also connected to the memory 370, in the resonator device 302. The memory 370 can store data such as logic and/or program instructions and/or values. The processor 360 can transmit such data to the memory 370 and receive such data from the memory 370 through its connection to the memory 370. The processor 360 can use data stored in the memory 370 to perform functions. For example, the memory 370 can store program instructions that the processor 360 can use to direct the adjustable capacitance control 330 to adjust the adjustable capacitance 320 of the LC resonator circuit to a resonant capacitance in a magnetic field, as described herein. The memory 370 can store values that represent signals that the processor 360 receives from one or more of the sensors 310. For example, the memory 370 can store values that represent an electrical voltage differential across the adjustable capacitance 312, as sensed by the voltage sensor 312. The memory 370 can also store known values, such as a known inductance of the LC resonator circuit, including an inductance of the inductor coil 304.
The processor 360 is also connected to the power source 380 and the selector 390. The power source 380 provides the processor 360 with electrical power so the processor 360 can perform its functions, as described in
In one embodiment, the processor 360 of
The processor 360 can direct the adjustment of the adjustable capacitance 320 of the LC resonator circuit to a resonant capacitance by executing logic and/or program instructions in response to known, sensed, and/or calculated values for a flux of a magnetic field and an inductance of the LC resonator circuit. Known values can be provided to the processor 360 from the memory 370, from the selector 390, or from directing the adjustable capacitance 310 to adjust to a known capacitance. The flux sensor 316 can sense a flux of a magnetic field, such as a flux of a static magnetic field from an MRI machine. In various embodiments of the present disclosure, flux values, inductance values, and capacitance values can be calculated as described herein.
In one embodiment of
The processor 360 can also direct the adjustment of the adjustable capacitance 320 of the LC resonator circuit to a resonant capacitance by executing logic and/or program instructions in response to sensed voltages across the adjustable capacitance 320 and/or sensed currents through the resonator circuit, for particular magnetic fields. For example, for a particular magnetic field, the processor 360 can direct the adjustable capacitance 320 to adjust to a particular capacitance, receive a signal from the voltage sensor 312 that represents a sensed voltage across the adjustable capacitance 320, and repeat this adjusting and sensing to determine a resonant capacitance at which a voltage across the adjustable capacitance 320 is a maximum voltage that can be obtained across the adjustable capacitance 320 in that particular magnetic field. In an alternative example, the processor 360 can perform a similar adjusting and sensing using a signal from the current sensor 314 to determine a resonant capacitance at a maximum current that can be obtained through the resonator circuit in a particular magnetic field. For these examples, the processor 360 can store sensed values in the memory 370, as necessary. The processor 360 can also repeat the adjusting of the adjustable capacitance 320 by adjusting through all possible capacitance values, by performing a bracketing approach, or by using some other technique.
In various embodiments of the present disclosure, a resonant capacitance for the LC resonator circuit of the resonator device 302 of
Various embodiments of the inductor coil 304 of the resonator device 302 of
Various embodiments of the adjustable capacitance 320 of the resonator device 302 of
In various embodiments of the resonator device 302, capacitors in the adjustable capacitance 320 can be of increasing size, to provide for a continuous range of possible capacitance. For example, in one embodiment of the present disclosure, the adjustable capacitance 320 can include a varactor with a 1 picoFarad adjustable capacitance, and capacitors with values of 1, 2, 4, 8, 16, 32, 64, 128, 256, 512, 1012, 2048, and 4096 picoFarads. Using combinations of capacitors in this example can provide adjustable capacitance values from zero Farads to 8.2 nanoFarads, which is a sufficient range to provide resonant capacitance in a resonator device for MRI from 1.5 to 3.0 Teslas and inductor coil inductances from 0.79 nanoHenries to 0.69 microHenries, as described herein. In various embodiments, the adjustable capacitance 320 can also include various other combinations of capacitors. Although the embodiment of
As in
As discussed herein, embodiments of a resonator device or system can also be implanted into a body. As will be understood by one of ordinary skill in the art, a variety of procedures can be used to implant an embodiment of a resonator device or system with an implantable medical device. For example, certain embodiments of a resonator device can be implanted adjacent to a stent that has already been implanted in a body. Alternatively, both a stent and certain embodiments of a resonator device can be implanted simultaneously. For example, both a stent and a resonator device could be loaded onto a catheter (e.g., a balloon catheter) for implanting in a body. In various embodiments of the present disclosure a medical device can be a deliverable device, deliverable in a lumen of a body.
In the foregoing Detailed Description, various features are grouped together in several embodiments for the purpose of streamlining the disclosure. This method of disclosure is not to be interpreted as reflecting an intention that the embodiments of the disclosure require more features than are expressly recited in each claim. Rather, as the following claims reflect, inventive subject matter lies in less than all features of a single disclosed embodiment. Thus, the following claims are hereby incorporated into the Detailed Description, with each claim standing on its own as a separate embodiment.
Number | Name | Date | Kind |
---|---|---|---|
4890063 | Haragashira | Dec 1989 | A |
5409460 | Krumme | Apr 1995 | A |
5824045 | Alt | Oct 1998 | A |
5843117 | Alt et al. | Dec 1998 | A |
5855600 | Alt | Jan 1999 | A |
5871437 | Alt | Feb 1999 | A |
6027510 | Alt | Feb 2000 | A |
6053873 | Govari et al. | Apr 2000 | A |
6099561 | Alt | Aug 2000 | A |
6106473 | Violante et al. | Aug 2000 | A |
6159142 | Alt | Dec 2000 | A |
6159237 | Alt et al. | Dec 2000 | A |
6231516 | Keilman et al. | May 2001 | B1 |
6245104 | Alt | Jun 2001 | B1 |
6251134 | Alt et al. | Jun 2001 | B1 |
6280385 | Melzer et al. | Aug 2001 | B1 |
6304769 | Arenson et al. | Oct 2001 | B1 |
6385478 | Hajnal | May 2002 | B1 |
6387121 | Alt | May 2002 | B1 |
6398805 | Alt | Jun 2002 | B1 |
6416540 | Mathur | Jul 2002 | B1 |
6463317 | Kucharczyk et al. | Oct 2002 | B1 |
6478815 | Alt | Nov 2002 | B1 |
6511325 | Lalka et al. | Jan 2003 | B1 |
6516213 | Nevo | Feb 2003 | B1 |
6574497 | Pacetti | Jun 2003 | B1 |
6585660 | Dorando et al. | Jul 2003 | B2 |
6585755 | Jackson et al. | Jul 2003 | B2 |
6585763 | Keilman et al. | Jul 2003 | B1 |
6628980 | Atalar et al. | Sep 2003 | B2 |
6652540 | Cole et al. | Nov 2003 | B1 |
6663570 | Mott et al. | Dec 2003 | B2 |
6668197 | Habib et al. | Dec 2003 | B1 |
6673104 | Barry | Jan 2004 | B2 |
6676694 | Weiss | Jan 2004 | B1 |
6702847 | DiCarlo | Mar 2004 | B2 |
6711429 | Gilboa et al. | Mar 2004 | B1 |
6711440 | Deal et al. | Mar 2004 | B2 |
6712844 | Pacetti | Mar 2004 | B2 |
6716237 | Alt | Apr 2004 | B1 |
6718203 | Weiner et al. | Apr 2004 | B2 |
6718207 | Connelly | Apr 2004 | B2 |
6725092 | MacDonald et al. | Apr 2004 | B2 |
6731979 | MacDonald | May 2004 | B2 |
6757566 | Weiner et al. | Jun 2004 | B2 |
6760628 | Weiner et al. | Jul 2004 | B2 |
6763268 | MacDonald et al. | Jul 2004 | B2 |
6765144 | Wang et al. | Jul 2004 | B1 |
6767360 | Alt et al. | Jul 2004 | B1 |
6778856 | Connelly et al. | Aug 2004 | B2 |
6782284 | Subramanyan et al. | Aug 2004 | B1 |
6785572 | Yanof et al. | Aug 2004 | B2 |
6786904 | Döscher et al. | Sep 2004 | B2 |
6787777 | Gagnon et al. | Sep 2004 | B1 |
6788827 | Makram-Ebeid | Sep 2004 | B1 |
6790182 | Eck et al. | Sep 2004 | B2 |
6795730 | Connelly et al. | Sep 2004 | B2 |
6795736 | Connelly et al. | Sep 2004 | B2 |
6799069 | Weiner et al. | Sep 2004 | B2 |
6802811 | Slepian | Oct 2004 | B1 |
6802857 | Walsh et al. | Oct 2004 | B1 |
6808535 | Jordan | Oct 2004 | B1 |
6819954 | Connelly | Nov 2004 | B2 |
6819958 | Weiner et al. | Nov 2004 | B2 |
6829509 | MacDonald et al. | Dec 2004 | B1 |
6844492 | Wang et al. | Jan 2005 | B1 |
6845266 | Weiner et al. | Jan 2005 | B2 |
6847837 | Melzer et al. | Jan 2005 | B1 |
6850804 | Eggers et al. | Feb 2005 | B2 |
6850805 | Connelly et al. | Feb 2005 | B2 |
6875180 | Weiner et al. | Apr 2005 | B2 |
6884234 | Aita et al. | Apr 2005 | B2 |
6892090 | Verard et al. | May 2005 | B2 |
6898454 | Atalar et al. | May 2005 | B2 |
6901290 | Foster et al. | May 2005 | B2 |
6908468 | Daum | Jun 2005 | B2 |
6925322 | Helfer et al. | Aug 2005 | B2 |
6925328 | Foster et al. | Aug 2005 | B2 |
6954674 | Connelly | Oct 2005 | B2 |
6957098 | Hyde et al. | Oct 2005 | B1 |
20010031919 | Strommer et al. | Oct 2001 | A1 |
20010031920 | Kaufman et al. | Oct 2001 | A1 |
20020019660 | Gianotti et al. | Feb 2002 | A1 |
20020026230 | Moll et al. | Feb 2002 | A1 |
20020040815 | Van Vaals | Apr 2002 | A1 |
20020042637 | Stover | Apr 2002 | A1 |
20020045816 | Atalar et al. | Apr 2002 | A1 |
20020049375 | Strommer et al. | Apr 2002 | A1 |
20020082679 | Sirhan et al. | Jun 2002 | A1 |
20020082685 | Sirhan et al. | Jun 2002 | A1 |
20020137014 | Anderson et al. | Sep 2002 | A1 |
20020173724 | Dorando et al. | Nov 2002 | A1 |
20020188345 | Pacetti | Dec 2002 | A1 |
20030004562 | DiCarlo | Jan 2003 | A1 |
20030004563 | Jackson et al. | Jan 2003 | A1 |
20030074049 | Hoganson et al. | Apr 2003 | A1 |
20030083579 | Aita et al. | May 2003 | A1 |
20030087244 | McCarthy | May 2003 | A1 |
20030088178 | Owens et al. | May 2003 | A1 |
20030088308 | Scheuermann et al. | May 2003 | A1 |
20030092013 | McCarthy et al. | May 2003 | A1 |
20030096248 | McCarthy et al. | May 2003 | A1 |
20030099957 | McCarthy | May 2003 | A1 |
20030100830 | Zhong et al. | May 2003 | A1 |
20030105069 | Robinson et al. | Jun 2003 | A1 |
20030139739 | Doscher et al. | Jul 2003 | A1 |
20030143544 | McCarthy | Jul 2003 | A1 |
20030144728 | Scheuermann et al. | Jul 2003 | A1 |
20030163052 | Mott et al. | Aug 2003 | A1 |
20030187335 | McCarthy | Oct 2003 | A1 |
20030199747 | Michlitsch et al. | Oct 2003 | A1 |
20030212448 | Smith | Nov 2003 | A1 |
20040010304 | Weber et al. | Jan 2004 | A1 |
20040019376 | Alt | Jan 2004 | A1 |
20040030379 | Hamm et al. | Feb 2004 | A1 |
20040034300 | Verard et al. | Feb 2004 | A1 |
20040038406 | Unger et al. | Feb 2004 | A1 |
20040039438 | Alt | Feb 2004 | A1 |
20040044397 | Stinson | Mar 2004 | A1 |
20040059280 | Makower et al. | Mar 2004 | A1 |
20040082866 | Mott et al. | Apr 2004 | A1 |
20040091603 | Priewe | May 2004 | A1 |
20040093075 | Kuehne | May 2004 | A1 |
20040097804 | Sobe | May 2004 | A1 |
20040097805 | Verard et al. | May 2004 | A1 |
20040098093 | DiCarlo | May 2004 | A1 |
20040111016 | Casscells, III et al. | Jun 2004 | A1 |
20040116997 | Taylor et al. | Jun 2004 | A1 |
20040117007 | Whitbourne et al. | Jun 2004 | A1 |
20040122494 | Eggers et al. | Jun 2004 | A1 |
20040143180 | Zhong et al. | Jul 2004 | A1 |
20040158310 | Weber et al. | Aug 2004 | A1 |
20040186377 | Zhong et al. | Sep 2004 | A1 |
20040210289 | Wang et al. | Oct 2004 | A1 |
20040230271 | Wang et al. | Nov 2004 | A1 |
20040243220 | Gianotti et al. | Dec 2004 | A1 |
20040249428 | Wang et al. | Dec 2004 | A1 |
20040254419 | Wang et al. | Dec 2004 | A1 |
20040254632 | Alt et al. | Dec 2004 | A1 |
20050004653 | Gerberding et al. | Jan 2005 | A1 |
20050025797 | Wang et al. | Feb 2005 | A1 |
20050033407 | Weber et al. | Feb 2005 | A1 |
20050049480 | Gray | Mar 2005 | A1 |
20050049481 | Gray et al. | Mar 2005 | A1 |
20050049482 | Gray et al. | Mar 2005 | A1 |
20050049683 | Gray et al. | Mar 2005 | A1 |
20050049684 | Gray et al. | Mar 2005 | A1 |
20050049685 | Gray et al. | Mar 2005 | A1 |
20050049686 | Gray et al. | Mar 2005 | A1 |
20050049688 | Gray et al. | Mar 2005 | A1 |
20050049689 | Gray et al. | Mar 2005 | A1 |
20050065430 | Wiethoff et al. | Mar 2005 | A1 |
20050065437 | Weber et al. | Mar 2005 | A1 |
20050079132 | Wang et al. | Apr 2005 | A1 |
20050080459 | Jacobson et al. | Apr 2005 | A1 |
20050085895 | Brown et al. | Apr 2005 | A1 |
20050090886 | MacDonald et al. | Apr 2005 | A1 |
20050107870 | Wang et al. | May 2005 | A1 |
20050113669 | Helfer et al. | May 2005 | A1 |
20050113676 | Weiner et al. | May 2005 | A1 |
20050113873 | Weiner et al. | May 2005 | A1 |
20050113874 | Connelly et al. | May 2005 | A1 |
20050113876 | Weiner et al. | May 2005 | A1 |
20050131522 | Stinson et al. | Jun 2005 | A1 |
20050143651 | Verard et al. | Jun 2005 | A1 |
20050149002 | Wang et al. | Jul 2005 | A1 |
20050149157 | Hunter et al. | Jul 2005 | A1 |
20050149169 | Wang et al. | Jul 2005 | A1 |
20050152946 | Hunter et al. | Jul 2005 | A1 |
20050154374 | Hunter et al. | Jul 2005 | A1 |
20050155779 | Wang et al. | Jul 2005 | A1 |
20050158356 | Hunter et al. | Jul 2005 | A1 |
20050159661 | Connelly et al. | Jul 2005 | A1 |
20050165470 | Weber | Jul 2005 | A1 |
20050165471 | Wang et al. | Jul 2005 | A1 |
20050169960 | Hunter et al. | Aug 2005 | A1 |
20050169961 | Hunter et al. | Aug 2005 | A1 |
20050175664 | Hunter et al. | Aug 2005 | A1 |
20050175665 | Hunter et al. | Aug 2005 | A1 |
20050175703 | Hunter et al. | Aug 2005 | A1 |
20050178395 | Hunter et al. | Aug 2005 | A1 |
20050178396 | Hunter et al. | Aug 2005 | A1 |
20050178584 | Wang et al. | Aug 2005 | A1 |
20050181005 | Hunter et al. | Aug 2005 | A1 |
20050181009 | Hunter et al. | Aug 2005 | A1 |
20050181010 | Hunter et al. | Aug 2005 | A1 |
20050182450 | Hunter et al. | Aug 2005 | A1 |
20050182463 | Hunter et al. | Aug 2005 | A1 |
20050182467 | Hunter et al. | Aug 2005 | A1 |
20050182468 | Hunter et al. | Aug 2005 | A1 |
20050182469 | Hunter et al. | Aug 2005 | A1 |
20050183731 | Hunter et al. | Aug 2005 | A1 |
20050186239 | Hunter et al. | Aug 2005 | A1 |
20050186244 | Hunter et al. | Aug 2005 | A1 |
20050186245 | Hunter et al. | Aug 2005 | A1 |
20050187140 | Hunter et al. | Aug 2005 | A1 |
20050187582 | Weiner | Aug 2005 | A1 |
20050187600 | Hunter et al. | Aug 2005 | A1 |
20050192647 | Hunter et al. | Sep 2005 | A1 |
20050196421 | Hunter et al. | Sep 2005 | A1 |
20050208095 | Hunter et al. | Sep 2005 | A1 |
20050209664 | Hunter et al. | Sep 2005 | A1 |
20050209665 | Hunter et al. | Sep 2005 | A1 |
20050209666 | Hunter et al. | Sep 2005 | A1 |
20050215764 | Tuszynski et al. | Sep 2005 | A1 |
20050216075 | Wang et al. | Sep 2005 | A1 |
20050277844 | Strother et al. | Dec 2005 | A1 |
Number | Date | Country |
---|---|---|
10127850 | Feb 2003 | DE |
0144405 | Aug 1984 | EP |
05209948 | Aug 1993 | JP |
WO 9919739 | Apr 1999 | WO |
WO 9942039 | Aug 1999 | WO |
WO 9942176 | Aug 1999 | WO |
WO 0174241 | Oct 2001 | WO |
WO 02094339 | Nov 2002 | WO |
Number | Date | Country | |
---|---|---|---|
20070106151 A1 | May 2007 | US |