The application is directed to an implantable wireless sensor. More particularly, this invention is directed to a wireless, unpowered, micromechanical, flexible sensor that can be delivered using endovascular techniques, to measure a corporeal parameter such as pressure or temperature.
Abdominal aortic aneurysms represent a dilatation and weakening of the abdominal aorta which can lead to aortic rupture and sudden death. Previously, the medical treatment of abdominal aortic aneurysms required complicated surgery with an associated high risk of injury to the patient. More recently, endografts (combining stents and grafts into a single device) have been developed that can be inserted through small incisions in the groin. Once in place, these endografts seal off the weakened section of the aorta. The aneurysms can then heal, eliminating the risk of sudden rupture. This less invasive form of treatment for abdominal aortic aneurysms has rapidly become the standard of care for this disease. An example of an endograft device is disclosed in Kornberg, U.S. Pat. No. 4,617,932.
A significant problem with endografts is that, due to inadequate sealing of the graft with the aorta, leaks can develop that allow blood to continue to fill the aneurysmal sac. Left undiscovered, the sac will continue to expand and potentially rupture. To address this situation, patients who have received endograft treatment for their abdominal aortic aneurysms are subjected to complex procedures that rely on injection of contrast agents to visualize the interior of the aneurysm sac. These procedures are expensive, not sensitive, and painful. In addition, they subject the patient to additional risk of injury. See for example, Baum R A et al., “Aneurysm sac pressure measurements after endovascular repair of abdominal aortic aneurysms”, The Journal of Vascular Surgery, January 2001, and Schurink G W et al., “Endoleakage after stent-graft treatment of abdominal aneurysm: implications on pressure and imaging—an in vitro study”, The Journal of Vascular Surgery, August 1998. These articles provide further confirmation of the problem of endograft leakage and the value of intra-sac pressure measurements for monitoring of this condition.
Thus, there is a need for a method of monitor the pressure within an aneurysm sac that has undergone repair by implantation of an endograft to be able to identify the potential presence of endoleaks. Furthermore, this method should be accurate, reliable, safe, simple to use, inexpensive to manufacture, convenient to implant and comfortable to the patient.
An ideal method of accomplishing all of the above objectives would be to place a device capable of measuring pressure within the aneurysm sac at the time of endograft insertion. By utilizing an external device to display the pressure being measured by the sensor, the physician will obtain an immediate assessment of the success of the endograft at time of the procedure, and outpatient follow-up visits will allow simple monitoring of the success of the endograft implantation.
An example of an implantable pressure sensor designed to monitor pressure increases within an aneurysmal sac is shown in Van Bockel, U.S. Pat. No. 6,159,156. While some of the above objectives are accomplished, this device has multiple problems that would make its use impractical. For example, the sensor disclosed in the Van Bockel patent relies on a mechanical sensing element. Elements of this kind cannot be practically manufactured in dimensions that would allow for endovascular introduction. In addition, this type of pressure sensor would be subject to many problems in use that would limit its accuracy and reliability. One example would be exposure of the mechanical sensing element to body fluids which could disrupt its function. Also, by failing to take advantage of specific approaches to electronic component fabrication, the Van Bockel device requires a complex system for acquiring data from the sensor necessary for the physician to make an accurate determination of intra-aneurysmal pressure. The Van Bockel device would inherently not be as flexible as required for certain endovascular or percutaneous procedures.
It is an object of this invention to provide an implantable wireless sensor.
It is also an object of this invention to provide a wireless, unpowered micromechanical, flexible sensor that can be delivered endovascularly.
It is a further object of this invention to provide an implantable, wireless, unpowered sensor that can be delivered endovascularly to measure pressure and/or temperature.
It is a yet further object of this invention to provide a method of preparing a micromechanical implantable sensor.
These and other objects of the invention will become more apparent from the discussion below.
The present invention comprises a device that can be implanted into the human body using non-surgical techniques to measure a corporeal parameter such as pressure, temperature, or both. Specific target locations could include the interior of an abdominal aneurysm or a chamber of the heart. This sensor is fabricated using MicroElectroMechanical Systems (MEMS) technology, which allows the creation of a flexible device that is small, accurate, precise, durable, robust, biocompatible, radiopaque and insensitive to changes in body chemistry, biology or external pressure. This device will not require the use of wires to relay pressure information externally nor need an internal power supply to perform its function.
The MEMS approach to sensor design lends itself to the fabrication of small, flat flexible sensors that can be formed using biocompatible polymers as substrate materials. The pressure sensor described above can then be manipulated into a smaller shape and size by rolling, bending, or folding it into a cylindrical form. This smaller object can be introduced into the sac of an abdominal aneurysm at the time an endograft is deployed within the aorta by using standard endovascular catheter techniques. Once inserted in the abdominal aneurysm sac or in a chamber of the heart, the device either on its own or through the addition or inclusion of metallic elements fabricated from stainless steel or super-elastic or shape memory nitinol alloys can unfurl into a preferred flat shape. The metallic components may also include anchors, hooks, harpoons, coils, barbs or other shapes and configurations designed to secure the pressure sensor to the wall on the aneurysm sac or a chamber of the heart. In addition, appropriately biocompatible coatings may be applied to the surface of the sensor to prevent adhesion of biological substances or coagulated blood to the sensor that could interfere with its proper function.
Delivery of the device of the invention to an aneurysm may be accomplished as follows: Using the standard Seldinger technique, the physician gains access to the patient's femoral artery and places a vessel introducer with a hemostatic valve. Under direct fluoroscopic visualization, a flexible guidewire is inserted through the introducer catheter and maneuvered such that its tip is stationed within the sac of the aortic aneurysm. A coaxial delivery catheter consisting of two hollow extruded polymeric catheters, the smaller of the two disposed inside the larger one, is inserted over the guidewire and through the introducer and advanced distally until its tip is within the aneurysmal sac. The smaller catheter has an annular space to hold a folded sensor, which is released when the outer catheter is withdrawn proximally.
In an alternative delivery procedure, a sensor is attached to a small diameter, proximally extending “safety” or tether wire. The sensor and safety wire are also positioned in the annular space between two coaxial catheters, but the safety wire runs the entire length of the smaller delivery catheter and extends proximally past the proximal end of that catheter outside the patient. In this configuration, the sensor remains secured to the tether wire after the coaxial delivery catheter is removed from the patient. Following the insertion and deployment of the stent-graft, the sensor is detached from the tether wire using any of the methods known in the art, and the wire is removed.
In a further alternative delivery procedure the sensor can be loaded into the annular space between the inner and outer catheters by inserting the sensor into a longitudinal slit cut into the outer catheter and attaching a tab on the sensor's surface into a slot cut into the inner coaxial catheter. By rotation of the inner tube, the sensor will be retracted through the slit and positioned in the annular space between the two tubes. To deploy the device, the rotation of the inner tube is reversed and the sensor emerges through the slit of the outer catheter. There are two specific advantages to this deployment mechanism. First, the sensor can be packaged and stored in a flat configuration. This is desirable since long term storage in a pre-loaded curved geometry could make it more difficult for the sensor to re-establish the flat arrangement that is optimal for effective electromagnetic inductive coupling with the external read-out unit. The second advantage is that by cutting the longitudinal slit at angle that is offset from the main axis of the outer tube, the sensor will be biased into a planar configuration as it is forced through the slit during the deployment process.
A safety wire system can also be used with this mechanism, although the wire may be external to the outer coaxial tube. As described above, the wire will remain attached to the sensor during the deployment process and will stay within the aneurysm sac while the delivery catheter is removed. Subsequent to insertion and deployment of the stent-graft, the wire will be detached from the sensor and pulled out of the body.
The detachment of the wire from the sensor can be accomplished in several ways. The wire may be simply glued to the sensor using an adhesive. To separate the sensor from the wire, a thin-walled, metal or polymer tube is passed along the length of the wire and positioned at the adhesive joint. While holding this tube steady, the wire is then retracted into the tube. Sufficient traction can be applied to the segment of the wire that remains outside of the body to cause the adhesive to joint to fail and allow removal of the wire.
An alternative method would rely on a mechanical connection between the wire and sensor such as adding threads to the end of the wire which could then be connected to a matching threaded female receptacle on the sensor. To separate the wire from the sensor, counter-rotation would be applied to the wire until the threads disengage. One could envision many variations of this design that would involve the mechanical locking and un-locking of two mating components.
In a delivery system intended more for cardiac applications, a “daisy shape” sensor is positioned in the distal end of a catheter lumen so that the middle, flat section of the sensor is essentially normal to the longitudinal axis of the catheter. A solid or hollow member fitting within the catheter lumen is used to push the sensor distally. If the sensor has an anchor member, it is meant that the anchor member will pierce or otherwise attach itself and the sensor to the wall of a chamber of the heart.
The invention can perhaps be better understood by referring to the drawings.
One embodiment of a sensor according to the invention is shown in
In
The size of the circular sensors of the invention will vary according to factors such as the intended application, the delivery system, etc. The circular sensors are intended to be from about 0.5 to about 3 cm in diameter, with a thickness of from about 0.05 to about 0.30 in. When a ring 32 is employed, the thickness of the ring, i.e., the width of the outside surface 38, will preferably be from about 1.5 to about 3.5 times the thickness of the sensor.
In the embodiment of the invention shown in
Prior to insertion of the coaxial catheter, as shown in
A better appreciation of certain aspects of the invention, especially of a delivery system, can be obtained from
In another embodiment of the invention, seen in
Actual delivery of a sensor according to the invention is shown in
In
When either delivery system 150 or 182 is retracted, sensor 162 or 194 is left positioned to the side of an aneurysm. Then, as shown in
The pressure sensor of the invention can be manufactured using Micro-machining techniques that were developed for the integrated circuit industry. An example of this type of sensor features an inductive-capacitive (LC) resonant circuit with a variable capacitor, as is described in Allen et al., U.S. Pat. No. 6,111,520, all of which is incorporated herein by reference. The sensor contains two types of passive electrical components, namely, an inductor and a capacitor. The sensor is constructed so that the fluid pressure at the sensor's surface changes the distance between the capacitor's parallel plates and causes a variation of the sensor's capacitance.
In a preferred embodiment the sensor of the invention is constructed by laminating several layers of material together, as shown, for example, in
The sensor exhibits the electrical characteristics associated with a standard LC circuit. An LC circuit is simply a closed loop with only two elements, a capacitor and an inductor. If a current is induced in the LC loop, the energy in the circuit is shared back and forth between the inductor and capacitor. The result is an energy oscillation that will vary at a specific frequency. This is termed the resonant frequency of the circuit and it can be easily calculated as its value is dependent on the circuit's inductance and capacitance. Therefore, a change in capacitance will cause the frequency to shift higher or lower in linear proportion to the change in the value of capacitance.
As noted above, the capacitor in the assembled pressure sensor consists of the two circular conductive segments separated by an air gap. If a pressure force is exerted on these segments it will act to deform the outer polyimide sheet and move the two conductive segments closer together. This will have the effect of reducing the air gap between them which will consequently change the capacitance of the circuit. The result will be a shift in the circuit's resonant frequency that will be in direct proportion to the force applied to the sensor's surface.
Because of the presence of the inductor, it is possible to electromagnetically couple to the sensor and induce a current in the circuit. This allows for wireless communication with the sensor and the ability to operate it without the need for an internal source of energy such as a battery. Thus, if the sensor is located within the sac of aortic aneurysm, it will be possible to determine the pressure within the sac in a simple, non-invasive procedure by remotely interrogating the sensor, recording the resonant frequency and converting this value to a pressure measurement. The readout device generates electromagnetic energy that penetrates through the body's tissues to the sensor's implanted location. The sensor's electrical components absorb a fraction of the electromagnetic energy that is generated by the readout device via inductive coupling. This coupling induces a current in the sensor's circuit oscillates at the same frequency as the applied electromagnetic energy. Due to the nature of the sensor's electro-mechanical system there exists a frequency of alternating current at which the absorption of energy from the readout device is at a minimum. This frequency is a function of the capacitance of the device. Therefore, if the sensor's capacitance changes, so will the frequency at which it minimally absorbs energy from the readout device. Since the sensor's capacitance is mechanically linked to the fluid pressure at the sensor's surface, a measurement of this frequency by the readout device gives a relative measurement of the fluid pressure. If calibration of the device is performed, then an absolute measurement of pressure can be made. See, for example, the extensive discussion in the Allen et al. patent, again incorporated herein by reference, as well as Gershenfeld et al., U.S. Pat. No. 6,025,725, incorporated herein by reference.
The pressure sensor is made of completely passive components having no active circuitry or power sources such as batteries. The pressure sensor is completely self-contained having no leads to connect to an external circuit or power source. Furthermore, these same manufacturing techniques can be used to add additional sensing capabilities, such as the ability to measure temperature by the addition of a resistor to the basic LC circuit.
Several alternative configurations of the LC circuit design can be considered to address specific biological and manufacturing issues. For example, in one embodiment of the sensor the capacitor element consists of two plates that are separated by a suitable dielectric material, such as air, inert gas, fluid or a vacuum. To ensure the long term integrity of the sensor, various coatings could be applied to the surface or between the polymeric layers used to form the sensor. These coating can be used to provide a hermetic seal that will prevent leakage of body fluids into the cavity or permeation of the cavity material (gas, vacuum or fluid) out of the sensor. In an another embodiment of the invention, shown in
It is within the scope of the invention that the frequency response to the sensor will be in the range of from about 1 to about 200 MHz, preferably from about 1 to about 100 MHz, and more preferably from about 2 to about 90 MHz, with a Q factor from about 5 to about 80, preferably from about 10 to about 70, more preferably from about 10 to 60.
In a further embodiment of the invention there is no direct electrical connection between the two sides of the LC circuit. Referring again to the sensor described in the Allen et al. patent, the device is constructed using multiple layers upon lie the necessary circuit elements. Disposed on the top and bottom layer are metal patterns constructed using micro-machining techniques which define a top and bottom conductor and a spiral inductor coil. To provide for an electrical contact between the top and bottom layers small vias or holes are cut through the middle layers. When the layers are assembled, a metal paste is forced into the small vias to create direct electrical connections or conduits. However, experimentation has shown that due to parasitic capacitance that is created between the top and bottom inductor coils, a vialess operational LC circuit can be created. This absence of via holes represents a significant improvement to the sensor in that it simplifies the manufacturing process and, more importantly, significantly increases the durability of the sensor making it more appropriate for use inside the human body.
The design of the sensor is not limited to a specific geometric configuration. In the specific example noted above the inductor component is described as a spiral coil. Other embodiments of the sensor could utilize oval, rectangular or an amorphous shape. Specific electrical, mechanical and biologic advantages could be obtained by employing these various geometric designs. By way of example, a rectangular shaped sensor in which the ratio of length to width was greater than four would greater lend itself to catheter based delivery as is would minimize the radius of curvature required to position the folded device within a small diameter catheter. Alternatively, a more elaborate shape, such as one resembling the petals of a flower, would lend itself to more complex folding patterns that could facilitate delivery to specific areas of an aneurysm sac or an organ such as the heart. For example, in
Another, preferred embodiment of a sensor is shown in
The flexible cut-outs 352 facilitate, among other things, folding of sections of sensor 370 for placement in, or arrangement upon, a delivery catheter. The sections can be folded to create either a “Z” shape or, for example, a “U” shape. It is within the scope of the invention that variously numbered and shaped cut-outs could be used for particular applications.
Sensor 330 could be employed in the delivery catheters shown in
In a delivery system shown in
During delivery to a desired location, such as an abdominal aortic aneurysm, an outer catheter sheath 360 encompasses distal portion 350 to hold sensor 356 in position. As shown in
When the distal end of the delivery catheter is properly positioned, outer catheter sheath 360 is moved proximally to release folded sections 362. Then, outer catheter sheath 360 is moved distally to engage sections 362 and cause sensor 356 to disengage from slot 354.
At least one of sections 362 has a tether wire 370 attached at an adhesive point 372, as can be seen in
Further, the invention is not limited to the implantation of a single sensor. Since the biological environment within an aortic aneurysm is not necessarily homogeneous, multiple pressure sensors may be introduced into the aneurysm space, each being positioned at different locations. In this situation, each sensor may be designed with a unique signature (obtained by changing the resonant frequency of the sensor), so that the pressure measurement derived from one sensor can be localized to its specific position within the aneurysm.
Clearly, if multiple sensors are used the same type of wire delivery system described above can also be employed to position the sensors within the aneurysm sac. For example, as shown in
When introduced into the sac of an abdominal aorta, the pressure sensor can provide pressure related data by use of an external measuring device. As disclosed in the Allen et al. patent, several different excitation systems can be used. The readout device generates electromagnetic energy that can penetrate through the body's tissues to the sensor's implanted location. The sensor's electrical components can absorb a fraction of the electromagnetic energy that is generated by the readout device via inductive coupling. This coupling will induce a current in the sensor's circuit that will oscillate at the same frequency as the applied electromagnetic energy. Due to the nature of the sensor's electro-mechanical system there will exist a frequency of alternating current at which the absorption of energy from the readout device is at a minimum. This frequency is a function of the capacitance of the device. Therefore, if the sensor's capacitance changes so will the frequency at which it minimally absorbs energy from the readout device. Since the sensor's capacitance is mechanically linked to the fluid pressure at the sensor's surface, a measurement of this frequency by the readout device can give a relative measurement of the fluid pressure. If calibration of the device is performed then an absolute measurement of pressure can be made
The circuitry used to measure and display pressure is contained within a simple to operate, battery powered, hand-held electronic unit 400, as shown in
Accordingly, the present invention provides for an impedance system and method of determining the resonant frequency and bandwidth of a resonant circuit within a particular sensor. The system includes a transmitting antenna, which is coupled to an impedance analyzer. The impedance analyzer applies a constant voltage signal to the transmitting antenna scanning the frequency across a predetermined spectrum. The current passing through the transmitting antenna experiences a peak at the resonant frequency of the sensor. The resonant frequency and bandwidth are thus determined from this peak in the current.
The method of determining the resonant frequency and bandwidth using an impedance approach may include the steps of transmitting an excitation signal using a transmitting antenna and electromagnetically coupling a sensor having a resonant circuit to the transmitting antenna thereby modifying the impedance of the transmitting antenna. Next, the step of measuring the change in impedance of the transmitting antenna is performed, and finally, the resonant frequency and bandwidth of the sensor circuit are determined.
In addition, the present invention provides for a transmit and receive system and method for determining the resonant frequency and bandwidth of a resonant circuit within a particular sensor. According to this method, an excitation signal of white noise or predetermined multiple frequencies is transmitted from a transmitting antenna, the sensor being electromagnetically coupled to the transmitting antenna. A current is induced in the resonant circuit of the sensor as it absorbs energy from the transmitted excitation signal, the current oscillating at the resonant frequency of the resonant circuit. A receiving antenna, also electromagnetically coupled to the transmitting antenna, receives the excitation signal minus the energy which was absorbed by the sensor. Thus, the power of the received signal experiences a dip or notch at the resonant frequency of the sensor. The resonant frequency and bandwidth are determined from this notch in the power.
The transmit and receive method of determining the resonant frequency and bandwidth of a sensor circuit includes the steps of transmitting a multiple frequency signal from transmitting antenna, and, electromagnetically coupling a resonant circuit on a sensor to the transmitting antenna thereby inducing a current in the sensor circuit. Next, the step of receiving a modified transmitted signal due to the induction of current in the sensor circuit is performed. Finally, the step of determining the resonant frequency and bandwidth from the received signal is executed.
Yet another system and method for determining the resonant frequency and bandwidth of a resonant circuit within a particular sensor includes a chirp interrogation system. This system provides for a transmitting antenna which is electromagnetically coupled to the resonant circuit of the sensor. An excitation signal of white noise or predetermined multiple frequencies is applied to the transmitting antenna for a predetermined period of time, thereby inducing a current in the resonant circuit of the sensor at the resonant frequency. The system then listens for a return signal which radiates from the sensor. The resonant frequency and bandwidth of the resonant circuit are determined from the return signal.
The chirp interrogation method for determining the resonant frequency and bandwidth of a resonant circuit within a particular sensor includes the steps of transmitting a multi-frequency signal pulse from a transmitting antenna, electromagnetically coupling a resonant circuit on a sensor to the transmitting antenna thereby inducing a current in the sensor circuit, listening for and receiving a return signal radiated from the sensor circuit, and determining the resonant frequency and bandwidth from the return signal.
A representative block diagram of an electrical circuit that can be used to interrogate the sensor and determine the resonant frequency is shown in
The present invention also provides an analog system and method for determining the resonant frequency of a resonant circuit within a particular sensor. The analog system comprises a transmitting antenna coupled as part of a tank circuit which in turn is coupled to an oscillator. A signal is generated which oscillates at a frequency determined by the electrical characteristics of the tank circuit. The frequency of this signal is further modified by the electromagnetic coupling of the resonant circuit of a sensor. This signal is applied to a frequency discriminator which in turn provides a signal from which the resonant frequency of the sensor circuit is determined.
The analog method for determining the resonant frequency and bandwidth of a resonant circuit within a particular sensor includes the steps of generating a transmission signal using a tank circuit which includes a transmitting antenna, modifying the frequency of the transmission signal by electromagnetically coupling the resonant circuit of a sensor to the transmitting antenna, and converting the modified transmission signal into a standard signal for further application.
The invention further includes an alternative method of measuring pressure in which a non-linear element such as a diode or polyvinylidenedifloride piezo-electric polymer is added to the LC circuit. A diode with a low turn-on voltage such as a Schottky diode can be fabricated using micro-machining techniques. The presence of this non-linear element in various configurations within the LC circuit can be used to modulate the incoming signal from the receiving device and produce different harmonics of the original signal. The read-out circuitry can be tuned to receive the particular harmonic frequency that is produced and use this signal to reconstruct the fundamental frequency of the sensor. The advantage of this approach is two-fold; the incoming signal can be transmitted continuously and since the return signal will be at different signals, the return signal can also be received continuously.
The above methods lend themselves to the creation of small and simple to manufacture hand-held electronic devices that can be used without complication.
One additional concern regarding devices designated for long term implantation in the human body is maintenance of electrical stability over time as the environment the sensor has been placed in changes. Under this scenario the sensor's accuracy may drift from its original baseline. It would thus be desirable to have available to the user of the device, a method for determining if the sensor is functioning properly and also to be able to recalibrate the device anytime after it has been implanted. This invention therefore also includes a method of using acoustic energy to challenge the sensor and determining to what degree (if any) sensor performance has been degraded. In this method, energy in the ultrasound range is directed towards the sensor and a measurement is made of the mechanical resonance of the sensor membrane. This same measurement can be made at point after the sensor has been implanted. By comparing the values of these two measurements a determination of the degree of change in mechanical resonance frequency can be established. This value can then be used to create a calibration factor that can be applied to the pressure reading taken post-implantation in order to adjust the measured value to reflect the actual pressure within the aneurysm.
The preceding specific embodiments are illustrative of the practice of the invention. It is to be understood, however, that other expedients known to those skilled in the art or disclosed herein, may be employed without departing from the spirit of the invention of the scope of the appended claims.
Number | Name | Date | Kind |
---|---|---|---|
2796863 | von Wittern | Jun 1957 | A |
3867950 | Fischell | Feb 1975 | A |
3942382 | Hok | Mar 1976 | A |
3958558 | Dunphy et al. | May 1976 | A |
4026276 | Chubbuck | May 1977 | A |
4127110 | Bullara | Nov 1978 | A |
4206762 | Cosman | Jun 1980 | A |
4207903 | O'Neill | Jun 1980 | A |
RE30366 | Rasor et al. | Aug 1980 | E |
4237900 | Schulman et al. | Dec 1980 | A |
4354506 | Sakaguchi et al. | Oct 1982 | A |
4378809 | Cosman | Apr 1983 | A |
4485813 | Anderson et al. | Dec 1984 | A |
4494950 | Fischell | Jan 1985 | A |
4521684 | Gilby et al. | Jun 1985 | A |
4593703 | Cosman | Jun 1986 | A |
4596563 | Pande | Jun 1986 | A |
4713540 | Gibly et al. | Dec 1987 | A |
4718425 | Tanaka et al. | Jan 1988 | A |
4796641 | Mills et al. | Jan 1989 | A |
4815472 | Wise et al. | Mar 1989 | A |
4846191 | Brockway et al. | Jul 1989 | A |
4890623 | Cook et al. | Jan 1990 | A |
4899752 | Cohen | Feb 1990 | A |
4913147 | Fahlstrom et al. | Apr 1990 | A |
4934369 | Maxwell | Jun 1990 | A |
4987897 | Funke | Jan 1991 | A |
5113868 | Wise et al. | May 1992 | A |
5115128 | Cook | May 1992 | A |
5129394 | Mehra | Jul 1992 | A |
5131399 | Sciarra | Jul 1992 | A |
5165289 | Tilmans | Nov 1992 | A |
5181423 | Philipps et al. | Jan 1993 | A |
5192314 | Daskalakis | Mar 1993 | A |
5207103 | Wise et al. | May 1993 | A |
5265606 | Kujawski | Nov 1993 | A |
5353800 | Pohndorf et al. | Oct 1994 | A |
5367376 | Lagakas et al. | Nov 1994 | A |
5373852 | Harrison et al. | Dec 1994 | A |
5411551 | Winston et al. | May 1995 | A |
5431171 | Harrison et al. | Jul 1995 | A |
5440300 | Spillman, Jr. | Aug 1995 | A |
5487760 | Villafana | Jan 1996 | A |
5497099 | Walton | Mar 1996 | A |
5515041 | Spillman, Jr. | May 1996 | A |
5535752 | Halperin et al. | Jul 1996 | A |
5538005 | Harrison et al. | Jul 1996 | A |
5551427 | Altman | Sep 1996 | A |
5566676 | Rosenfeldt et al. | Oct 1996 | A |
5583474 | Mizoguchi et al. | Dec 1996 | A |
5593430 | Renger | Jan 1997 | A |
5600245 | Yamamoto et al. | Feb 1997 | A |
5626630 | Markowitz et al. | May 1997 | A |
5686841 | Stolarczyk et al. | Nov 1997 | A |
5695155 | Macdonald et al. | Dec 1997 | A |
5702427 | Ecker et al. | Dec 1997 | A |
5703576 | Spillman, Jr. et al. | Dec 1997 | A |
5713917 | Leonhardt et al. | Feb 1998 | A |
5722414 | Archibald et al. | Mar 1998 | A |
5723791 | Koch et al. | Mar 1998 | A |
5743267 | Nikolic et al. | Apr 1998 | A |
5796827 | Coppersmith et al. | Aug 1998 | A |
5807265 | Itoigawa et al. | Sep 1998 | A |
5836886 | Itoigawa et al. | Nov 1998 | A |
5860938 | Lafontaine et al. | Jan 1999 | A |
5899927 | Ecker et al. | May 1999 | A |
5935084 | Southworth | Aug 1999 | A |
5942991 | Gaudreau et al. | Aug 1999 | A |
5967986 | Cimochowski et al. | Oct 1999 | A |
6015386 | Kensey et al. | Jan 2000 | A |
6015387 | Schwartz et al. | Jan 2000 | A |
6019729 | Itoigawa et al. | Feb 2000 | A |
6024704 | Meador et al. | Feb 2000 | A |
6025725 | Gershenfeld et al. | Feb 2000 | A |
6030413 | Lazarus | Feb 2000 | A |
6033366 | Brockway et al. | Mar 2000 | A |
6053873 | Govari et al. | Apr 2000 | A |
6076016 | Feierbach | Jun 2000 | A |
6111520 | Allen et al. | Aug 2000 | A |
6113553 | Chubbuck | Sep 2000 | A |
6134461 | Say et al. | Oct 2000 | A |
6140740 | Porat et al. | Oct 2000 | A |
6159156 | Van Bockel | Dec 2000 | A |
6198965 | Penner et al. | Mar 2001 | B1 |
6201980 | Darrow et al. | Mar 2001 | B1 |
6206835 | Spillman et al. | Mar 2001 | B1 |
6229190 | Bryzek et al. | May 2001 | B1 |
6237398 | Porat et al. | May 2001 | B1 |
6239724 | Doron et al. | May 2001 | B1 |
6277078 | Porat et al. | Aug 2001 | B1 |
6278379 | Allen et al. | Aug 2001 | B1 |
6287253 | Ortega et al. | Sep 2001 | B1 |
6373264 | Matsumoto et al. | Apr 2002 | B1 |
6400974 | Lesho | Jun 2002 | B1 |
6409674 | Brockway et al. | Jun 2002 | B1 |
6442413 | Silver | Aug 2002 | B1 |
6454720 | Clerc et al. | Sep 2002 | B1 |
6645143 | Van Tassell et al. | Nov 2003 | B2 |
6667725 | Simons et al. | Dec 2003 | B1 |
6682490 | Roy et al. | Jan 2004 | B2 |
6765493 | Lonsdale et al. | Jul 2004 | B2 |
6855115 | Fonseca et al. | Feb 2005 | B2 |
6923769 | Nishii et al. | Aug 2005 | B2 |
6926670 | Rich et al. | Aug 2005 | B2 |
6939299 | Petersen et al. | Sep 2005 | B1 |
20020077556 | Schwartz et al. | Jun 2002 | A1 |
20020151816 | Rich et al. | Oct 2002 | A1 |
20020188207 | Richter | Dec 2002 | A1 |
20030031587 | Hu et al. | Feb 2003 | A1 |
20030136417 | Fonseca et al. | Jul 2003 | A1 |
20030139677 | Fonseca et al. | Jul 2003 | A1 |
20040122494 | Eggers et al. | Jun 2004 | A1 |
20050075697 | Olson et al. | Apr 2005 | A1 |
20050085703 | Behm | Apr 2005 | A1 |
20050154321 | Wolinsky et al. | Jul 2005 | A1 |
Number | Date | Country |
---|---|---|
1 158 061 | Jun 1983 | CA |
196 44 858.5 | Oct 1996 | DE |
0257801 | Mar 1988 | EP |
0 337 035 | Nov 1993 | EP |
0 646 365 | Apr 1995 | EP |
WO 8303348 | Oct 1983 | WO |
WO 9006723 | Jun 1990 | WO |
WO 9533517 | Dec 1995 | WO |
WO 9709926 | Mar 1997 | WO |
WO 9732518 | Sep 1997 | WO |
WO 9732519 | Sep 1997 | WO |
WO 9733513 | Sep 1997 | WO |
WO 9934731 | Jul 1999 | WO |
WO 9942176 | Aug 1999 | WO |
WO 9962587 | Dec 1999 | WO |
WO 0016686 | Mar 2000 | WO |
WO 0100089 | Jan 2001 | WO |
WO 0187137 | Nov 2001 | WO |
WO 0197908 | Dec 2001 | WO |
WO 02058551 | Aug 2002 | WO |
WO 03061467 | Jul 2003 | WO |
WO 03061504 | Jul 2003 | WO |
WO 03096889 | Nov 2003 | WO |
Number | Date | Country | |
---|---|---|---|
20030136417 A1 | Jul 2003 | US |