The present invention relates to a treatment system for percutaneous coronary angioplasty or peripheral angioplasty in which a dilation catheter is used to cross a lesion in order to dilate the lesion and restore normal blood flow in the artery. It is particularly useful when the lesion is a calcified lesion in the wall of the artery. Calcified lesions require high pressures (sometimes as high as 10-15 or even 30 atmospheres) to break the calcified plaque and push it back into the vessel wall. With such pressures comes trauma to the vessel wall which can contribute to vessel rebound, dissection, thrombus formation, and a high level of restenosis. Non-concentric calcified lesions can result in undue stress to the free wall of the vessel when exposed to high pressures. An angioplasty balloon when inflated to high pressures can have a specific maximum diameter to which it will expand but the opening in the vessel under a concentric lesion will typically be much smaller. As the pressure is increased to open the passage way for blood the balloon will be confined to the size of the opening in the calcified lesion (before it is broken open). As the pressure builds a tremendous amount of energy is stored in the balloon until the calcified lesion breaks or cracks. That energy is then released and results in the rapid expansion of the balloon to its maximum dimension and may stress and injure the vessel walls.
Recently, a new system and method has been contemplated for breaking up calcium deposits in, for example, arteries and veins. Such a system is described, for example in U.S. Patent Publication No. 2009/0312768, Published Dec. 17, 2009. Embodiments described therein include a catheter having balloon, such as an angioplasty balloon, at the distal end thereof arranged to be inflated with a fluid. Disposed within the balloon is a shock wave generator that may take the form of, for example, a pair of electrodes, which are coupled to a high voltage source at the proximal end of the catheter through a connector. When the balloon is placed adjacent a calcified region of a vein or artery and a high voltage pulse is applied across the electrodes, a shock wave is formed that propagates through the fluid and impinges upon the wall of the balloon and the calcified region. Repeated pulses break up the calcium without damaging surrounding soft tissue.
Each high voltage pulse causes an arc to form across the electrodes. The arc in turn causes a steam bubble to form. Each steam bubble has the potential of producing two shock waves, a leading edge shock wave as a result of bubble expansion and a trailing edge shock wave as a result of bubble collapse. The trailing edge shock waves exhibit highly variable energy levels and generally, much greater energy levels than the leading edge shock waves. The energy levels of the trailing edge shock waves are substantially dependent on the uniformity of the bubble collapse. The uniform collapse of spherical bubbles to a point appears to create the highest shock wave energies. Unfortunately, spherical bubble configuration requires a substantially larger space than is available in a balloon that must fit into a calcified vein or artery or even a ureter. In fact, the trailing edge shock wave can be substantially eliminated by confining the bubble to an irregular shape. As a result, for angioplasty or other cardiac and non-cardiac applications of shock waves, the trailing edge shock wave cannot be reliably relied upon to produce consistent results.
However, the leading edge shock waves formed by bubble expansion are a different matter. While exhibiting generally lower energies, they are more consistent in energy level. As a result, leading edge shock waves are good candidates for use in medical procedures such, for example, angioplasty or valvuloplasty.
Another consideration is the amount of energy represented by the high voltage applied to the electrodes. Each high voltage pulse removes a portion of the electrode material. Since the size of the electrodes must be small in order to fit into the calcified vein or artery, they are only capable of sustaining a limited numbers of high voltage pulses sufficient to form the shock wave resulting electrical arc.
Also, it has been learned that to sustain a leading edge shock wave, it is not necessary to sustain the high voltage throughout the shock wave. Sustaining the high voltage beyond some point after the initial arc does not lead to shock waves of any greater intensity. Further, since the bubbles are formed of steam, the steam produces heat which can increase the temperature of adjacent soft tissue. Just a two degree Celsius elevation in temperature above body temperature can result in tissue damage.
A still further important aspect of prior art attempts to use shock waves from electrical arcs for therapeutic purposes is that from the time the high voltage is first applied to the electrodes to the time in which the arc occurs there is a dwell time (Td) that is highly variable from one high voltage application to the next. To account for the dwell times that are long, prior art strategies have relied upon high voltage applications where all high voltage pulse durations or pulse widths are of the same length and of a length sufficient to extend through the longest of the anticipated dwell times plus the associated arc and steam bubble. As a result, when the dwell times are shorter than the maximum, the high voltage application durations are longer than necessary and can unnecessarily extend the arc and the steam bubble well beyond a time required to produce a shock wave of maximum intensity. The result is wasted energy, extended electrode erosion, and unnecessary heating of the adjoining tissue.
Hence, there is a need in the art to be able to control the energy applied to the electrodes of an electrical arc shock wave generator. More particularly, there is a need to control the applied energy to assure appropriate bubble and shock wave formation while at the same time conserving electrode material and assuring tissue safety. The present invention addresses these and other issues.
In one embodiment, a system includes a catheter including an elongated carrier and a balloon about the carrier in sealed relation thereto. The balloon is arranged to receive a fluid therein that inflates the balloon. The catheter further includes first and second electrodes within the balloon arranged to receive there-across a high electrical voltage at an initial low current. The high electrical voltage causes an electrical arc to form across the first and second electrodes within the balloon. The electrical arc creates a gas bubble within the liquid, a high current to flow through the first and second electrodes, and a mechanical shock wave within the balloon. The system further includes a power source that provides the first and second electrodes with the high electrical voltage at the initial current and that terminates the high electrical voltage in response to the high current flow through the first and second electrodes.
The power source includes a current sensor that senses current flowing through the first and second electrodes. The current sensor causes the power source to terminate the high electrical voltage when the current flowing through the first and second electrodes reaches a predetermined limit. The predetermined limit may be on the order of fifty amperes.
The system may further include a temperature sensor within the balloon that senses temperature of the fluid within the balloon. The power source may be further responsive to the temperature sensor.
The temperature sensor may cause the power source to decrease energy applied to the first and second electrodes responsive to the temperature of the fluid within the balloon increasing to control the temperature of the fluid. The temperature sensor may cause the power source to decrease energy applied to the first and second electrodes responsive to the temperature of the fluid within the balloon increasing to above two degrees Celsius above ambient temperature.
Each pulse of the serial electrical high voltage pulses has an amplitude. The temperature sensor may cause the power source to decrease the energy applied to the first and second electrodes by decreasing the amplitude of the serial electrical high voltage pulses. Alternatively, the temperature sensor may cause the power source to decrease the energy applied to the first and second electrodes by temporarily terminating the serial electrical high voltage pulses.
The serial electrical high voltage pulses have a pulse rate. The temperature sensor may cause the power source to decrease the energy applied to the first and second electrodes by decreasing the pulse rate of the serial electrical high voltage pulses.
The balloon may be a dilation balloon. The dilation balloon may be an angioplasty balloon. In some applications, such as lithotripsy, a balloon may not be required.
The system may further include a timer that times a delay time in response to the high current flow through the first and second electrodes and the power source may terminate the high electrical voltage after the delay time is timed. The power source may include a current sensor that senses current flowing through the first and second electrodes and the current sensor may cause the timer to time the delay time when the current flowing through the first and second electrodes reaches a predetermined limit. The predetermined limit may be on the order of fifty amperes.
In another embodiment, a system includes a catheter including an elongated carrier having a guide wire lumen and a balloon having an inner surface about the carrier in sealed relation thereto. The balloon forms a channel with the carrier. The channel is arranged to receive a fluid that inflates the balloon. The catheter further includes first and second electrodes within the balloon, between the carrier and the inner surface of the balloon, arranged to receive there-across a high electrical voltage at an initial low current to cause an electrical arc to form across the first and second electrodes within the balloon. The electrical arc creates a gas bubble within the liquid, a high current to flow through the first and second electrodes, and a mechanical shock wave within the balloon. The system further includes a power source that provides the first and second electrodes with the high electrical voltage at the initial current and that terminates the high electrical voltage in response to the high current flow through the first and second electrodes.
In a further embodiment, a system includes a catheter including an elongated carrier and a balloon about the carrier in sealed relation thereto. The balloon is arranged to receive a fluid therein that inflates the balloon. The catheter further includes first and second electrodes within the balloon arranged to receive there-across a high electrical voltage at an initial low current to cause an electrical arc to form across the first and second electrodes within the balloon. The electrical arc creates a steam bubble within the liquid, a high current to flow through the first and second electrodes, and a mechanical shock wave within the balloon. The steam bubble increases the temperature of the fluid. The system further includes a temperature sensor within the balloon that senses temperature of the fluid within the balloon and a power source that provides the first and second electrodes with the high electrical voltage at the initial current and that controls energy provided by the high electrical voltage in response to the sensed temperature of the fluid within the balloon.
The temperature sensor causes the power source to decrease energy applied to the first and second electrodes responsive to the temperature of the fluid within the balloon increasing to control the temperature of the fluid. The temperature sensor causes the power source to decrease energy applied to the first and second electrodes responsive to the temperature of the fluid within the balloon increasing to about two degrees Celsius above ambient temperature.
Each pulse of the serial electrical high voltage pulses has an amplitude. The temperature sensor may alternatively cause the power source to decrease the energy applied to the first and second electrodes by decreasing the amplitude of the serial electrical high voltage pulses. The temperature sensor may alternatively cause the power source to decrease the energy applied to the first and second electrodes by temporarily terminating the serial electrical high voltage pulses.
The serial electrical high voltage pulses have a pulse rate. The temperature sensor may alternatively cause the power source to decrease the energy applied to the first and second electrodes by decreasing the pulse rate of the serial electrical high voltage pulses.
The carrier of the catheter may have a guide wire lumen. The balloon has an inner surface that with the carrier, forms a channel arranged to receive the fluid that inflates the balloon. The first and second electrodes may be disposed between the carrier and the inner surface of the balloon.
According to a further embodiment, the invention provides a method that includes the steps of providing a catheter including an elongated carrier, a balloon about the carrier in sealed relation thereto, the balloon being arranged to receive a fluid therein that inflates the balloon, and first and second electrodes within the balloon. The method further includes introducing the fluid into the balloon to inflate the balloon, applying an electrical voltage across the first and second electrodes to form an electrical arc across the first and second electrodes, sensing current flow through the first and second electrodes, and varying the application of the electrical voltage across the first and second electrodes in response to sensed current flow through the first and second electrodes after the electrical arc is formed across the first and second electrodes.
The varying step may include terminating the application of the electrical voltage across the first and second electrodes. The high electrical voltage may be terminated when the current flowing through the first and second electrodes reaches a predetermined limit. The predetermined limit may be on the order of fifty amperes.
The method may include the further step of sensing temperature of the fluid within the balloon and the varying step may include varying the application of the electrical voltage across the first and second electrodes in response to sensed temperature of the fluid.
The varying step may include decreasing energy applied to the first and second electrodes responsive to the temperature of the fluid within the balloon increasing to control the temperature of the fluid. The energy applied to the first and second electrodes may be decreased responsive to the temperature of the fluid within the balloon increasing to above two degrees Celsius above ambient temperature.
The applying step may include applying energy in the form of serial electrical high voltage pulses and the varying step may further include decreasing the energy applied to the first and second electrodes by temporarily terminating the serial electrical high voltage pulses.
The serial electrical high voltage pulses have a pulse rate. Alternatively, the varying step may further include decreasing the energy applied to the first and second electrodes by decreasing the pulse rate of the serial electrical high voltage pulses.
The method may include the further step of timing a delay time in response to sensed current flow through the first and second electrodes and the varying step may include terminating the application of the electrical voltage across the first and second electrodes after timing the delay time. The delay time may be timed when the current flowing through the first and second electrodes reaches a predetermined limit. The predetermined limit may be on the order of fifty amperes.
According to another embodiment, a method includes the steps of providing a catheter including an elongated carrier, a balloon about the carrier in sealed relation thereto, the balloon being arranged to receive a fluid therein that inflates the balloon, and first and second electrodes within the balloon. The method further includes the steps of introducing the fluid into the balloon to inflate the balloon, applying energy in the form of an electrical voltage across the first and second electrodes to form an electrical arc across the first and second electrodes, sensing temperature of the fluid within the balloon, and varying the application of the energy across the first and second electrodes in response to sensed temperature of the fluid within the balloon.
The varying step may include decreasing the energy applied to the first and second electrodes responsive to the temperature of the fluid within the balloon increasing. The varying step may include decreasing the energy applied to the first and second electrodes responsive to the temperature of the fluid within the balloon increasing to about two degrees Celsius above ambient temperature.
Each pulse of the serial electrical high voltage pulses has an amplitude. The varying step may include decreasing the energy applied to the first and second electrodes by decreasing the amplitude of the serial electrical high voltage pulses.
The applying step may include applying energy in the form of serial electrical high voltage pulses and the varying step may further include decreasing the energy applied to the first and second electrodes by temporarily terminating the serial electrical high voltage pulses.
The applying step may include applying energy in the form of serial electrical high voltage pulses, wherein the serial electrical high voltage pulses have a pulse rate. The varying step may further include decreasing the energy applied to the first and second electrodes by decreasing the pulse rate of the serial electrical high voltage pulses.
In a still further embodiment, a system treats obstructions within bodily fluid and includes a catheter including first and second electrodes arranged to receive there-across a high electrical voltage at an initial low current. The high electrical voltage causes an electrical arc to form across the first and second electrodes. The electrical arc creates a gas bubble within the bodily fluid, a high current to flow through the first and second electrodes, and a mechanical shock wave within the bodily fluid. The system further includes a power source that provides the first and second electrodes with the high electrical voltage at the initial current and that terminates the high electrical voltage in response to the high current flow through the first and second electrodes.
The energy applied by the power source may be in the form of serial electrical high voltage pulses. Each pulse of the serial electrical high voltage pulses has an amplitude. The power source may control the energy applied to the first and second electrodes by varying the amplitude of the serial electrical high voltage pulses.
The serial electrical high voltage pulses have a pulse rate. Alternatively, the power source may vary the energy applied to the first and second electrodes by varying the pulse rate of the serial electrical high voltage pulses.
The system may further include a timer that times a delay time in response to the high current flow through the first and second electrodes and the power source may terminate the high electrical voltage after the delay time is timed. The power source may include a current sensor that senses current flowing through the first and second electrodes and the current sensor may cause the timer to time the delay time when the current flowing through the first and second electrodes reaches a predetermined limit. The predetermined limit may be on the order of fifty amperes.
In still a further embodiment, a method includes the steps of providing a catheter including first and second electrodes, applying an electrical voltage across the first and second electrodes to form an electrical arc across the first and second electrodes, sensing current flow through the first and second electrodes, and varying the application of the electrical voltage across the first and second electrodes in response to sensed current flow through the first and second electrodes after the electrical arc is formed across the first and second electrodes.
The applying step may includes applying energy in the form of serial electrical high voltage pulses, the serial electrical high voltage pulses having a pulse rate, and wherein the varying step further includes controlling the energy applied to the first and second electrodes by varying the pulse rate of the serial electrical high voltage pulses.
The serial high voltage pulses have amplitudes. The varying step may alternatively or in addition include controlling the energy applied to the first and second electrodes by varying the amplitude of the serial electrical high voltage pulses.
The method may include the further step of timing a delay time in response to sensed current flow through the first and second electrodes and the varying step may include terminating the application of the electrical voltage across the first and second electrodes after timing the delay time. The delay time may be timed when the current flowing through the first and second electrodes reaches a predetermined limit. The predetermined limit may be on the order of fifty amperes.
The features of the present invention which are believed to be novel are set forth with particularity in the appended claims. The invention, together with further features and advantages thereof, may best be understood by making reference to the following description taken in conjunction with the accompanying drawings, in the several figures of which like reference numerals identify identical elements, and wherein:
The sheath 21 forms with the guide wire member 28 a channel 27 through which fluid, such as saline, may be admitted into the balloon to inflate the balloon. The channel 27 further permits the balloon 26 to be provided with an electrode pair 25 including electrodes 22 and 24 within the fluid filled balloon 26.
As may be seen in
The electrical arcs between electrodes 22 and 24 in the fluid are used to generate shock waves in the fluid. Each pulse of high voltage applied to the electrodes 22 and 24 forms an arc across the electrodes. The voltage pulses may have amplitudes as low as 500 volts, but preferably, the voltage amplitudes are in the range of 1000 volts to 10,000 volts. The balloon 26 may be filled with water or saline in order to gently fix the balloon in the walls of the artery or vein, for example, in direct proximity with the calcified lesion. The fluid may also contain an x-ray contrast to permit fluoroscopic viewing of the catheter during use. Once the catheter 20 is positioned with the guide wire (not shown), the physician or operator can start applying the high voltage pulses to the electrodes to form the shock waves that crack the calcified plaque. Such shockwaves will be conducted through the fluid, through the balloon, through the blood and vessel wall to the calcified lesion where the energy will break the hardened plaque without the application of excessive pressure by the balloon on the walls of the artery.
It has been found that effective shock wave intensity may be accomplished without holding the high voltage pulses on during the entire extent of their corresponding steam bubbles. Moreover, terminating the application of the high voltage before steam bubble collapse can serve to preserve electrode material, permitting a pair of electrodes to last for an increased number of applied high voltage pulses. Still further, as will be seen subsequently, early termination of the high voltage can also be used to advantage in controlling the temperature within the balloon fluid.
In operation, the microprocessor 90 through the optical driver 92, causes the switch 86 to apply the high voltage to the electrodes 22 and 24. The current sensed through resister 96 is monitored by the microprocessor 90 through the optical isolator 98. When the current flowing through the electrodes reaches a predetermined limit, as for example 50 amperes, the microprocessor 90 causes the application of the high voltage to be terminated. The forgoing occurs for each high voltage pulse applied to the electrodes 22 and 24. Each pulse creates a shock wave of consistent and useful intensity. Further, because the application of the high voltage is terminated early, the electrode material is preserved to lengthen the useful life of the electrodes.
The catheter 133 of system 134 is shown in a ureter 130. The ureter has a kidney stone 131 requiring treatment. According to this embodiment, voltage pulses are applied to the electrode pair 132 to produce leading edge shock waves as previously described. The shock waves propagate through the fluid within the ureter and impinge directly on the kidney stone 131. In a manner as previously described, the power source may be operated to maintain the energy applied to the electrode pair within limits to assure that the steam bubbles produced by the generated arcs do not harm the ureter. To that end, the amplitude or pulse rate of the applied voltages may be controlled. Hence, by controlling the energy of the current during the produced arc, such as by controlling the on time of the current, barotrauma to the ureter may be minimized even though a balloon is not employed as in previous embodiments. Of course, the system of
Referring now to the flow diagram 200 of
As a result of the foregoing, a maximum intensity shock wave is formed without wasting energy, without unduly eroding the electrodes, and without generating unnecessary heat. As may be appreciated, the delay timing may be employed to advantage in each of the embodiments disclosed herein including the embodiment of
While particular embodiments of the present invention have been shown and described, modifications may be made. It is therefore intended in the appended claims to cover all such changes and modifications which fall within the true spirit and scope of the invention as defined by those claims.
This application is a continuation application of U.S. application Ser. No. 13/615,107, entitled SHOCKWAVE CATHETER SYSTEM WITH ENERGY CONTROL, filed Sep. 13, 2012, which is hereby incorporated by reference in its entirety and for all purposes.
Number | Name | Date | Kind |
---|---|---|---|
3785382 | Schmidt et al. | Jan 1974 | A |
3902499 | Shene | Sep 1975 | A |
4027674 | Tessler et al. | Jun 1977 | A |
4662126 | Malcolm | May 1987 | A |
4685458 | Leckrone | Aug 1987 | A |
4809682 | Forssmann et al. | Mar 1989 | A |
4900303 | Lemelson | Feb 1990 | A |
5009232 | Hassler et al. | Apr 1991 | A |
5057103 | Davis | Oct 1991 | A |
5078717 | Parins et al. | Jan 1992 | A |
5103804 | Abele et al. | Apr 1992 | A |
5152767 | Sypal et al. | Oct 1992 | A |
5152768 | Bhatta | Oct 1992 | A |
5176675 | Watson et al. | Jan 1993 | A |
5246447 | Rosen et al. | Sep 1993 | A |
5281231 | Rosen et al. | Jan 1994 | A |
5324255 | Passafaro et al. | Jun 1994 | A |
5336234 | Vigil et al. | Aug 1994 | A |
5368591 | Lennox et al. | Nov 1994 | A |
5395335 | Jang | Mar 1995 | A |
5417208 | Winkler | May 1995 | A |
5425735 | Rosen et al. | Jun 1995 | A |
5472406 | de la Torre et al. | Dec 1995 | A |
5582578 | Zhong et al. | Dec 1996 | A |
5603731 | Whitney | Feb 1997 | A |
5609606 | O'Boyle | Mar 1997 | A |
5662590 | de la Torre et al. | Sep 1997 | A |
5931805 | Brisken | Aug 1999 | A |
6007530 | Dornhofer et al. | Dec 1999 | A |
6033371 | Torre et al. | Mar 2000 | A |
6083232 | Cox | Jul 2000 | A |
6210408 | Chandrasekaran et al. | Apr 2001 | B1 |
6217531 | Reitmajer | Apr 2001 | B1 |
6277138 | Levinson et al. | Aug 2001 | B1 |
6287272 | Brisken et al. | Sep 2001 | B1 |
6352535 | Lewis et al. | Mar 2002 | B1 |
6367203 | Graham et al. | Apr 2002 | B1 |
6371971 | Tsugita et al. | Apr 2002 | B1 |
6398792 | O'Connor | Jun 2002 | B1 |
6406486 | de la Torre et al. | Jun 2002 | B1 |
6514203 | Bukshpan | Feb 2003 | B2 |
6524251 | Rabiner et al. | Feb 2003 | B2 |
6589253 | Cornish et al. | Jul 2003 | B1 |
6607003 | Wilson | Aug 2003 | B1 |
6638246 | Naimark et al. | Oct 2003 | B1 |
6652547 | Rabiner et al. | Nov 2003 | B2 |
6736784 | Menne et al. | May 2004 | B1 |
6740081 | Hilal | May 2004 | B2 |
6755821 | Fry | Jun 2004 | B1 |
6989009 | Lafontaine | Jan 2006 | B2 |
7241295 | Maguire | Jul 2007 | B2 |
7569032 | Naimark et al. | Aug 2009 | B2 |
8556813 | Cioanta et al. | Oct 2013 | B2 |
8728091 | Hakala et al. | May 2014 | B2 |
20010044596 | Jaafar | Nov 2001 | A1 |
20020177889 | Brisken et al. | Nov 2002 | A1 |
20030004434 | Greco et al. | Jan 2003 | A1 |
20030176873 | Chernenko et al. | Sep 2003 | A1 |
20030229370 | Miller | Dec 2003 | A1 |
20040044308 | Naimark et al. | Mar 2004 | A1 |
20040097996 | Rabiner et al. | May 2004 | A1 |
20040254570 | Hadjicostis et al. | Dec 2004 | A1 |
20050015953 | Keidar | Jan 2005 | A1 |
20050021013 | Visuri et al. | Jan 2005 | A1 |
20050251131 | Lesh | Nov 2005 | A1 |
20060004286 | Chang et al. | Jan 2006 | A1 |
20060184076 | Gill et al. | Aug 2006 | A1 |
20060190022 | Beyar et al. | Aug 2006 | A1 |
20070088380 | Hirszowicz et al. | Apr 2007 | A1 |
20070239082 | Schultheiss et al. | Oct 2007 | A1 |
20070239253 | Jagger et al. | Oct 2007 | A1 |
20070244423 | Zumeris et al. | Oct 2007 | A1 |
20080097251 | Babaev | Apr 2008 | A1 |
20080188913 | Stone et al. | Aug 2008 | A1 |
20090041833 | Bettinger et al. | Feb 2009 | A1 |
20090247945 | Levit et al. | Oct 2009 | A1 |
20090254114 | Hirszowicz et al. | Oct 2009 | A1 |
20090312768 | Hawkins et al. | Dec 2009 | A1 |
20100016862 | Hawkins et al. | Jan 2010 | A1 |
20100036294 | Mantell et al. | Feb 2010 | A1 |
20100114020 | Hawkins et al. | May 2010 | A1 |
20100114065 | Hawkins et al. | May 2010 | A1 |
20100121322 | Swanson | May 2010 | A1 |
20100305565 | Truckai et al. | Dec 2010 | A1 |
20110034832 | Cioanta et al. | Feb 2011 | A1 |
20110118634 | Golan | May 2011 | A1 |
20110166570 | Hawkins et al. | Jul 2011 | A1 |
20110257523 | Hastings et al. | Oct 2011 | A1 |
20110295227 | Hawkins et al. | Dec 2011 | A1 |
20120071889 | Mantell et al. | Mar 2012 | A1 |
20120095461 | Herscher et al. | Apr 2012 | A1 |
20120203255 | Hawkins et al. | Aug 2012 | A1 |
20120221013 | Hawkins et al. | Aug 2012 | A1 |
20130030431 | Adams | Jan 2013 | A1 |
20130030447 | Adams | Jan 2013 | A1 |
20130150874 | Kassab | Jun 2013 | A1 |
20140046229 | Hawkins et al. | Feb 2014 | A1 |
20140052147 | Hakala et al. | Feb 2014 | A1 |
20140074111 | Hakala et al. | Mar 2014 | A1 |
20140074113 | Hakala et al. | Mar 2014 | A1 |
20140243820 | Adams et al. | Aug 2014 | A1 |
Number | Date | Country |
---|---|---|
3038445 | May 1982 | DE |
0442199 | Aug 1991 | EP |
0571306 | Nov 1993 | EP |
62-275446 | Nov 1987 | JP |
6-125915 | May 1994 | JP |
7-47135 | Feb 1995 | JP |
10-99444 | Apr 1998 | JP |
10-513379 | Dec 1998 | JP |
2002-538932 | Nov 2002 | JP |
2004-81374 | Mar 2004 | JP |
2005-95410 | Apr 2005 | JP |
2005-515825 | Jun 2005 | JP |
2006-516465 | Jul 2006 | JP |
9624297 | Aug 1996 | WO |
2004069072 | Aug 2004 | WO |
2006127158 | Nov 2006 | WO |
2007149905 | Dec 2007 | WO |
2009121017 | Oct 2009 | WO |
2009152352 | Dec 2009 | WO |
2010014515 | Feb 2010 | WO |
2011143468 | Nov 2011 | WO |
2013059735 | Apr 2013 | WO |
Entry |
---|
International Search Report received for PCT Patent Application No. PCT/US2009/047070, mailed on Jan. 19, 2010, 4 pages. |
International Preliminary Report on Patentability received for PCT Patent Application No. PCT/US2011/047070, mailed on Feb. 21, 2013, 7 pages. |
International Written Opinion received for PCT Patent Application No. PCT/US2011/047070, mailed on May 1, 2012, 5 pages. |
International Search Report received for PCT Patent Application No. PCT/US2012/023172, mailed on Sep. 28, 2012, 3 pages. |
International Search Report and Written Opinion received for PCT Patent Application No. PCT/US2013/031805 mailed on May 20, 2013, 13 pages. |
Adams et al., U.S. Appl. No. 13/534,658, filed Jun. 27, 2012, titled “Shock Wave Balloon Catheter with Multiple Shock Wave Sources”, 35. |
Adams et al., U.S. Appl. No. 13/777,807, filed Feb. 26, 2013, titled “Shock Wave Catheter System with ARC Preconditioning”, 15 pages. |
Hakala et al., U.S. Appl. No. 13/831,543, filed Mar. 14, 2013, titled “Low Profile Electrodes for an Angioplasty Shock Wave Catheter”, 52 pages. |
Non Final Office Action received for U.S. Appl. No. 12/482,995, mailed on Jul. 12, 2013, 11 pages. |
Hakala et al., U.S. Appl. No. 13/615,107, filed Sep. 13, 2012, titled “Shockwave Catheter System with Energy Control”, 38 pages. |
Office Action received for Australian Patent Application No. 2009257368, issued on Jul. 31, 2013, 4 pages. |
Extended European Search Report (includes Supplementary European Search Report and Search Opinion) received for European Patent Application No. 097636401, mailed on Oct. 10, 2013, 5 pages. |
International Preliminary Report on Patentability received for PCT Patent Application No. PCT/US2012/023172, mailed on Aug. 15, 2013, 6 pages. |
International Search Report and Written Opinion received for PCT Patent Application No. PCT/US2013/039987, mailed on Sep. 23, 2013, 15 pages. |
International Search Report and Written Opinion received for PCT Patent Application No. PCT/US2013/048277, mailed on Oct. 2, 2013, 14 pages. |
International Search Report and Written Opinion received for PCT Patent Application No. PCT/US2013/059533, mailed on Nov. 7, 2013, 14 pages. |
Office Action received for Japanese Patent Application No. 2011-513694, mailed on Aug. 27, 2013, 6 pages. |
Final Office Action received for U.S. Appl. No. 13/267,383, mailed on Oct. 25, 2013, 8 pages. |
Final Office Action received for U.S. Appl. No. 12/482,995, mailed on Feb. 20, 2014, 11 pages. |
Rosenschein et al., “Shock-Wave Thrombus Ablation, a New Method for Noninvasive Mechanical Thrombolysis”, The American Journal of Cardiology, vol. 70, Nov. 15, 1992, pp. 1358-1361. |
Zhong et al., “Transient Oscillation of Cavitation Bubbles Near Stone Surface During Electohydraulic Lithotripsy”, Journal of Endourology, vol. 11, No. 1, Feb. 1997, pp. 55-61. |
Non Final Office Action received for U.S. Appl. No. 14/079,463, mailed on Mar. 4, 2014, 9 pages. |
Notice of Allowance received for U.S. Appl. No. 14/079,463, mailed on Apr. 1, 2014, 5 pages. |
International Search Report and Written Opinion received for PCT Patent Application No. PCT/US2013/055431, mailed on Nov. 12, 2013, 9 pages. |
Advisory Action received for U.S. Appl. No. 13/267,383, mailed on Jan. 6, 2014, 4 pages. |
Non-Final Office Action received for U.S. Appl. No. 12/501,619, mailed on Jan. 28, 2014, 10 pages. |
Non-Final Office Action received for U.S. Appl. No. 13/049,199, mailed on Feb. 4, 2014, 8 pages. |
Non-Final Office Action received for U.S. Appl. No. 12/581,295, mailed on Mar. 10, 2014, 11 pages. |
Non-Final Office Action received for U.S. Appl. No. 14/061,554, mailed on Mar. 12, 2014, 14 pages. |
Notice of Allowance received for U.S. Appl. No. 14/061,554, mailed on Apr. 25, 2014 8 pages. |
Adams et al., Unpublished U.S. Appl. No. 14/271,342, filed May 6, 2014, titled “Shock Wave Balloon Catheter with Multiple Shock Wave Sources”, 21 pages. |
Adams, John M., U.S. Appl. No. 14/218,858, filed Mar. 18, 2014, titled “Shockwave Catheter System with Energy Control”, 24 pages. |
Non-Final Office Action received for U.S. Appl. No. 13/646,583, mailed on Oct. 31, 2014, 8 pages. |
Written Opinon received for PCT Patent Application No. PCT/US2009/047070, mailed on Jan. 19, 2010, 5 pages. |
International Preliminary Report on Patentability received for PCT Patent Application No. PCT/US2009/047070, mailed on Dec. 23, 2010, 7 pages. |
Non Final Office Action received for U.S. Appl. No. 12/482,995, mailed on Aug. 13, 2014, 10 pages. |
Advisory Action Received for U.S. Appl. No. 12/581,295, mailed on Jul. 3, 2014, 3 pages. |
Final Office Action received for U.S. Appl. No. 13/049,199 mailed on Aug. 11, 2014, 8 pages. |
Notice of Allowance received for U.S. Appl. No. 13/831,543, mailed on Oct. 8, 2014, 14 pages. |
Non-Final Office Action received for U.S. Appl. No. 14/271,342, mailed on Sep. 2, 2014, 6 pages. |
Notice of Acceptance Received for Australian Patent Application No. 2009257368, mailed on Aug. 28, 2014, 2 pages. |
Final Office Action received for U.S. Appl. No. 12/581,295, mailed on Jun. 5, 2014, 14 pages. |
Office Action received for Australian Patent Application No. 2009257368, issued on Apr. 28, 2014, 4 pages. |
Office Action Received for Japanese Patent Application No. 2011-513694, mailed on Jun. 10, 2014, (See Communication under 37 CFR § 1.98(a) (3)). |
Cleveland et al., “The Physics of Shock Wave Lithotripsy”, Extracorporeal Shock Wave Lithotripsy Part IV, Chapter 38, 2012, pp. 317-332. |
Connors et al., “Renal Nerves Mediate Changes in Contralateral Renal Blood Flow after Extracorporeal Shockwave Lithotripsy”, Nephron Physiol, vol. 95, 2003, pp. 67-75. |
Gambihler et al., “Permeabilization of the Plasma Membrane of LI210 Mouse Leukemia Cells Using Lithotripter Shock Waves”, The Journal of Membrane Biology, vol. 141, 1994, pp. 267-275. |
Grassi et al., “Novel Antihypertensive Therapies: Renal Sympathetic Nerve Ablation and Carotid Baroreceptor Stimulation”, Curr. Hypertens Rep., vol. 14, 2012, pp. 567-572. |
Kodama et al., “Shock Wave-Mediated Molecular Delivery Into Cells”, Biochimica et Biophysica Acta vol. 1542, 2002, pp. 186-194. |
Lauer et al., “Shock Wave Permeabilization as a New Gene Transfer Method”, Gene Therapy, vol. 4, 1997, pp. 710-715. |
Non Final Office Action received for U.S. Appl. No. 13/465,264, mailed on Oct. 29, 2014, 13 pages. |
Non Final Office Action received for U.S. Appl. No. 13/646,570, mailed on Oct. 29, 2014, 10 pages. |
Doug Hakala, “Unpublished U.S. Appl. No. 14/515,130, filed Oct. 15, 2014, titled “Low Profile Electrodes for an Angioplasty Shock Wave Catheter””. |
Number | Date | Country | |
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20140243847 A1 | Aug 2014 | US |
Number | Date | Country | |
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Parent | 13615107 | Sep 2012 | US |
Child | 14271276 | US |