Embodiments of the invention relate to designs of, and methods of using, a catheter with merged optical tissue evaluation and laser ablation.
Ablation is a medical technique for producing tissue necrosis. It is used to help treat different pathologies including cancer, Barret's esophagus, or cardiac arrhythmias, among others. In some cases, various types of ablation may be utilized, such as cryogenic cooling for cryoablation, chemicals for chemical ablation, radiofrequency (RF) ablation, laser ablation, and the like. For radiofrequency (RF) ablation, the application of alternating current with an oscillating frequency above several hundreds of kHz avoids the stimulation of excitable tissue while delivering heat by means of the Joule's effect. The increase in tissue temperature produces denaturation of the biological molecules, including proteins such as collagen, myosin, or elastin. Traditionally, RF ablation is done by placing an external electrode on the patient's body, and applying an alternating potential to the tip of a catheter that is placed in contact with the tissue to be treated within the patient's body. The ablation effect depends on a number of factors, including applied electrical power, quality of the electrical contact, local tissue properties, presence of blood flow close to the tissue surface, and the effect of irrigation. Because of the variability of these parameters, it is difficult to obtain consistent results.
Conventional ablation catheters and methods for RF ablation treatments are limited because of the challenges associated with aligning catheter electrodes with target tissues in order for accuracy during RF ablation procedures. In the embodiments presented herein, an ablation catheter for merged optical tissue evaluation and laser ablation is described.
The ablation catheter may provide a cost-effective solution to issues with RF ablation catheters that utilize complex electrical wiring for each electrode in the RF ablation catheter. In some embodiments, the ablation catheter includes a plurality of optical ports for both evaluating and ablating target tissue. By allowing laser ablation energy to be transmitted through the same optical ports that are used to perform tissue evaluation, the ablation catheter may use a single substrate that allows for focused evaluation of the same target tissue that is being ablated. In the embodiments presented herein, devices and methods for performing optical tissue evaluation and laser ablation using catheters with a plurality of optical ports for transmitting exposure radiation beams and laser ablation energy to target tissue are described.
In an embodiment, a catheter system includes a catheter with a distal section, a proximal section, and a sheath coupled between the distal section and the proximal section, and a processing device. The distal section includes a plurality of optical ports and a holder configured to maintain the plurality of optical ports in a fixed spatial relationship. The plurality of optical ports are configured to transmit one or more beams of exposure radiation to a sample, receive one or beams of scattered radiation that have been reflected or scattered from the sample, and transmit laser ablation energy such that at least a portion of the sample is ablated. The processing device or the proximal section of the catheter includes a first optical source configured to generate a source beam of exposure radiation, and a second optical source configured to generate the laser ablation energy. The catheter system also includes a multiplexer configured to direct the one or more beams of exposure radiation from the source beam of radiation to the plurality of optical ports, combine the one or more beams of scattered radiation, and direct the laser ablation energy to at least one optical port of the plurality of optical ports.
An example method for performing merged optical tissue evaluation and laser ablation is described. The method includes providing an ablation catheter, in which the ablation catheter includes a proximal end, a distal end with a plurality of optical ports, and a sheath coupled between the proximal end and the distal end. The method further includes transmitting one or more beams of exposure radiation via the plurality of optical ports to a sample near the distal end of the ablation catheter, receiving one or more beams of scattered or reflected radiation from the sample via the plurality of optical ports, and ablating at least a portion of the sample using laser ablation energy output from at least one optical port of the plurality of optical ports.
In another embodiment, a catheter system for performing merged optical tissue evaluation and laser ablation is described. The catheter system includes a catheter with a distal section, a proximal section, and a sheath coupled between the proximal section and the distal section, and a processing device. The distal section includes a plurality of optical ports configured to transmit one or more beams of exposure radiation to a sample, receive one or beams of scattered radiation that have been reflected or scattered from the sample, and transmit laser ablation energy such at least a portion of the sample is ablated. The processing device or the proximal section of the catheter includes a first optical source configured to generate a source beam of exposure radiation and a second optical source configured to generate the laser ablation energy.
Further features and advantages, as well as the structure and operation of various embodiments, are described in detail below with reference to the accompanying drawings. It is noted that the specific embodiments described herein are not intended to be limiting. Such embodiments are presented herein for illustrative purposes only. Additional embodiments will be apparent to persons skilled in the relevant art(s) based on the teachings contained herein.
The accompanying drawings, which are incorporated herein and form a part of the specification, illustrate embodiments of the present invention and, together with the description, further serve to explain the principles of the invention and to enable a person skilled in the pertinent art to make and use the invention.
Embodiments of the present invention will be described with reference to the accompanying drawings.
Although specific configurations and arrangements are discussed, it should be understood that this is done for illustrative purposes only. A person skilled in the pertinent art will recognize that other configurations and arrangements can be used without departing from the spirit and scope of the present invention. It will be apparent to a person skilled in the pertinent art that this invention can also be employed in a variety of other applications.
It is noted that references in the specification to “one embodiment,” “an embodiment,” “an example embodiment,” etc., indicate that the embodiment described may include a particular feature, structure, or characteristic, but every embodiment may not necessarily include the particular feature, structure, or characteristic. Moreover, such phrases do not necessarily refer to the same embodiment. Further, when a particular feature, structure or characteristic is described in connection with an embodiment, it would be within the knowledge of one skilled in the art to effect such feature, structure or characteristic in connection with other embodiments whether or not explicitly described.
As used herein, “laser energy” or “laser ablation energy” refers to light emitted through a process of optical amplification based on stimulated emission of electromagnetic radiation and refers to one or more beams of laser light that is generated by a laser source. It should be noted that although this application may refer specifically to cardiac ablation, the embodiments described herein may target other pathologies as well, along with additional energy sources for ablation. The principles of using laser ablation energy to treat other pathologies are similar, and therefore the techniques used to apply the laser ablation energy are similar.
Disclosed herein are embodiments of an ablation catheter for merged optical tissue evaluation and laser ablation in which the ablation catheter includes a plurality of optical ports for both evaluating and ablating target tissue. In some embodiments, the plurality of optical ports of the catheter may be configured to transmit beams of exposure radiation to a sample, receive one or more beams of scattered radiation that have been reflected or scattered from the sample, and transmit laser energy such that at least a portion of the sample is ablated. By utilizing the same optical ports for transmission of the optical evaluation signals and the laser ablation signals, the ablation catheter may provide focused evaluation of the same target tissue that is being ablated in a single substrate that allows for both modalities.
Herein, the terms “electromagnetic radiation,” “light,” and “beam of radiation” are all used to describe the same electromagnetic signals propagating through the various described elements and systems.
In an embodiment, sheath 106 and distal section 104 are disposable. As such, proximal section 102 may be reused by attaching a new sheath 106 and distal section 104 each time a new procedure is to be performed. In another embodiment, proximal section 102 is also disposable.
In some embodiments, various electrical and optical components such as a power supply, first and second optical sources, and interferometer elements are located in processing device 108. The electrical and optical signals from these components may be sent to proximal section 102 via communication interface 110. By housing these components in processing device 108, the whole of catheter 100 may be disposable.
In other embodiments, proximal section 102 may house various electrical and optical components used in the operation of catheter 100. A first optical source may be included within proximal section 102 to generate a source beam of radiation for optical evaluation. The first optical source may include one or more laser diodes, superluminescent diodes (SLEDs) or light emitting diodes (LEDs). The beam of radiation generated by the optical source may have a wavelength within the infrared range. In one example, the beam of radiation has a central wavelength of 1.3 μm. The optical source may be designed to output a beam of radiation at only a single wavelength, or it may be a swept source and be designed to output a range of different wavelengths. The generated beam of radiation may be guided towards distal section 104 via the optical transmission medium connected between proximal section 102 and distal section 104 within sheath 106. Some examples of optical transmission media include single mode, polarization maintaining, or multimode optical fibers and integrated optical waveguides. In one embodiment, the electrical transmission medium and the optical transmission medium are provided by the same hybrid medium allowing for both electrical and optical signal propagation.
Furthermore, proximal section 102 may include a second optical source, such as a laser energy source for tissue ablation. In some embodiments, the laser energy source may emit an ablation beam of laser energy at a wavelength of 980 nm or a wavelength of 1060 nm. The laser energy from the source in proximal section 102 may propagate down catheter 100 via an optical transmission medium connected between proximal section 102 and distal section 104 within sheath 106, and the laser energy may be output from the distal section 104 of catheter 100 to target tissue. For example, the laser energy from the source may produce an optical power of 5 W to 12 W that is applied to target tissue for 20-30 seconds to produce transmural lesions in heart tissue. In another example, the laser energy from the source may produce an optical power of 30 W to 50 W that is applied to target tissue for 60-90 seconds. Further details of how the first optical source for optical evaluation and second optical source for laser ablation are coupled together are discussed with reference to
In an embodiment, proximal section 102 includes one or more components of an interferometer in order to perform low coherence interferometry (LCI) using the light generated from the first optical source. Due to the nature of interferometric data analysis, in an embodiment, the optical transmission medium used for guiding the light to and from distal end 104 does not affect the state and degree of light polarization. In another embodiment, the optical transmission medium affects the polarization in a constant and reversible way.
Proximal section 102 may include further interface elements with which a user of catheter 100 can control the operation of catheter 100. For example, proximal section 102 may include a deflection control mechanism that controls a deflection angle of distal section 104. The deflection control mechanism may require a mechanical movement of an element on proximal section 102, or the deflection control mechanism may use electrical connections to control the movement of distal section 104. Proximal section 102 may include various buttons or switches that allow a user to control when laser energy is applied at distal end 104, or when the beams of radiation are transmitted from distal end 104, allowing for the acquisition of optical data. In some examples, these buttons or switches are located at a separate user interface coupled to processing device 108.
Distal section 104 includes a plurality of optical view ports, which will be described further detail below. In an embodiment, one or more of the optical view ports are machined into the outer body of distal section 104. For example, one or more of the optical view ports of the outer body of distal section 104 may be produced by laser drilling, 3D printing, stereolithography (SLA), fused deposition modeling (FDM), selective laser sintering (SLS), and/or other techniques. The optical view ports are distributed over the outside of distal section 104, resulting in a plurality of distinct viewing directions. The optical view ports also allow for a plurality of directions in which laser energy may be directed for tissue ablation through one or more of the optical view ports. In an embodiment, each of the plurality of viewing directions are substantially non-coplanar. The optical view ports may also be designed with irrigation functionality to cool distal section 104 and surrounding tissue during ablation. Further details on the design of distal section 104 are discussed with reference to
Irrigation channel 202 may be a hollow tube used to guide cooling fluid towards distal section 104. Irrigation channel 202 may include heating and/or cooling elements disposed along the channel to affect the temperature of the fluid. In another embodiment, irrigation channel 202 may also be used as an avenue for drawing fluid surrounding distal section 104 back towards proximal section 102.
Deflection mechanism 206 may include electrical or mechanical elements designed to provide a signal to distal section 104 in order to change a deflection angle of distal section 104. The deflection system enables guidance of distal section 104 by actuating a mechanical control placed in proximal section 102, according to an embodiment. This system may be based on a series of aligned and uniformly spaced cutouts in sheath 106 aimed at providing unidirectional deflection of distal section 104, in combination with a wire which connects the deflection mechanism control in proximal section 102 with the catheter tip at distal section 104. In this way, a certain movement of the proximal section may be projected to the distal section. Other embodiments involving the combination of several control wires attached to the catheter tip may enable the deflection of the catheter tip along different directions.
In
Additionally, laser energy generated from the second optical source (e.g., for laser ablation) within proximal section 102 or processing device 108 may be directed to one or more view ports 302 using the same multiplexing unit 312 or a different multiplexing unit (not shown) to select at least one of the plurality of view ports 302 for targeted ablation. Multiplexing unit 312 receives an input beam of radiation and a laser beam via optical transmission line 316. Optical transmission line 316 may include any number of optical transmission elements (e.g., optical fibers), and may be similar to optical transmission media 210 of
Multiplexing unit 312 may include associated electronics 314 that provide control signals to various modulating elements of multiplexing unit 312. Multiplexing unit 312 may use any multiplexing method that allows for the separation of contributions from the light collected by various view ports 302, as well as separation of the light for optical tissue evaluation and the light for laser ablation. One such multiplexing method is time-domain multiplexing, in which multiplexing unit 312 switches between different output waveguides in a controlled manner, so that at a given time only one of the associated view ports 302 is active. Another suitable multiplexing method is frequency-domain multiplexing, in which light traversing each of view ports 302 is modulated in such a way that the time-frequency behavior of signals corresponding to different view ports 302 can be differentiated by a processing device (e.g., processing device 108). Coherence-domain multiplexing may also be used in multiplexing unit 312, by introducing a different group delay to the light traversing each view port 302, so that the signals corresponding to different view ports 302 appear at different coherence positions and can be therefore differentiated by a processing device (e.g., processing device 108). In an embodiment, these methods are non-exclusive and can be combined in order to find the best design compromise. Some of the multiplexing methods, like coherence-domain multiplexing, do not require any electrical actuation of multiplexing unit 312. Thus, in an embodiment, implementations based on coherence-domain multiplexing do not require electrical transmission media for control signals.
In one embodiment, multiplexing unit 312 is produced on a silicon nitride photonics chip using a network of thermo-electric optical switches. Other suitable materials for use in multiplexing unit 312 include silicon dioxide, oxinitride, lithium niobate, III-V semiconductor materials, silicon on insulator (SOD, gallium arsenide (GaAs), silicon carbide or optical grade polymers, and the like. Other modulation effects to support the optical switching operation include the electro-optic effect, charge carrier density effects, photo-mechanical effects, liquid crystal based refractive index modulation, etc. The multiplexing function may also be obtained through microelectromechanical (MEMS) devices in as far as miniaturization and packaging constraints can be met. The connections between electrical wires 318 and multiplexing unit 312 may be achieved via individual wire-bonding or soldering, or through an intermediate substrate that allows for flip-chip assembly in an individual or batch process. In an embodiment, this intermediate substrate is flexible.
In an embodiment, multiplexing unit 312 is fabricated upon a flexible substrate. A process for forming the optical elements upon a flexible substrate includes a substrate transfer post-processing step applied to Silicon on Insulator (SOI) chips or wafers, as described in more detail in U.S. Pat. No. 9,062,960, the disclosure of which is incorporated by reference herein in its entirety. In an embodiment, the resulting flexible device is thinner (<350 μm) than the starting thickness (500-700 μm). Multiplexing unit 312 may be implemented by an optical integrated chip that is partly flexible. Plurality of waveguides 304 (e.g., optical fibers) are suitably flexible in order to reach the various view ports 302 arranged round distal section 104a, according to an embodiment. As illustrated in
As shown in
Distal section 104a may also include a force sensor 317. In an embodiment, force sensor 317 is designed to measure a force applied to distal section 104a during operation along one or more reference axes. Force sensor 317 may include a rigid element coming from the sheath (e.g. a rigid wire) mechanically connected to a part of the sensor. The general assembly of the catheter and any mechanical fixation element acting between distal section 104a and the sheath must ensure sufficient stress transfer to force sensor 317. In another embodiment, force sensor 317 may be a pressure sensor based on, for example, a strain gauge.
Force sensor 317 may have its readout element defined in the same substrate as multiplexing unit 312, according to an embodiment. The read-out principle may be based on an interferometric analysis of distance change associated to strain, on an spectral analysis of resonant-type devices, on a piezo-electric device, on a capacitance measurement, or based on an electromagnetic measurement. According to an embodiment, the signals generated from force sensor 317 propagate through additional cables and/or optical transmission media running through sheath 106. Alternatively, the signals may propagate through the same electrical and optical paths used for multiplexing unit 312 and its associated electronics 314. In the latter case, the multiplexed optical path and force sensor 317 data path may be separated through a suitable signal multiplexing technique. Additionally, if irrigation channels 310 are perfused at a low and constant flow, the pressure may be measured indirectly by adding a pressure transducer in proximal section 102 of catheter 100.
In an embodiment, a temperature sensor 319 may be included in distal section 104a, measuring the temperature substantially at the tip of the catheter during operation. Although
In some embodiments, distal section 104 may include one or more electrodes for measuring electrocardiograms of tissue and/or one or more magnetic sensors for allowing navigation of the catheter. For example, one or more magnetic sensors of the catheter may be combined with externally-generated magnetic field generators for navigating the catheter with magnetic fields.
In either embodiment of distal section 104 illustrated in
In an embodiment, one or more of the plurality of view ports 302 includes a scanning element (not shown) that allows for one or more beams exiting through view port 302 (e.g., one or more beams of the exposure radiation and the laser ablation energy) to be scanned in a given direction. The scanning element may include a microelectromechanical system (MEMS) component, or use electro-optical modulators to steer the exit angle of the beam of radiation from an associated view port. Further details and examples regarding the scanning of the beams of radiation may be found in U.S. Pat. No. 9,354,040, the disclosure of which is incorporated by reference herein in its entirety. In some embodiments, the scanning of the exposure radiation allows for the collection of optical coherence tomography (OCT) images of a sample.
Flexible waveguides may extend across the flexible sections to optically connect optical ports to multiplexer 312. The flexible sections may be formed by partial removal of the substrate material to thin the substrate. A layer of polyimide may be added to reinforce the thinned portion. Multiplexer 312 may be formed on a rigid section as shown in
Beam input/output sections 322 may output focused or unfocused beams from optical ports. In addition, the beam may exit in the plane of a beam input/output section 322 (as shown in
Substrate 320 may be any suitable material that allows for surface and/or bulk micromachining patterning steps to be performed. In one example, substrate 320 is a crystalline material such as silicon dioxide, silicon, gallium arsenide, indium phosphide, or the like. In other examples, substrate 320 is amorphous such as glass or polysilicon. Core layer 336 of waveguide 334 may comprise a material having a higher refractive index than cladding layers 338a and 338b in order to confine a beam of radiation propagating through waveguide 334. For example, core layer 336 may comprise silicon nitride (Si3N4). Waveguide 334 may have a crystalline structure or be a polymer. For example, waveguide 334 may be formed from one or more materials that are transparent at the wavelengths utilized for tissue evaluation and laser ablation and capable of implementing phase shifting mechanisms and handling high optical intensities with negligible non-linear effects. In one example, cladding layers 338a and 338b are silicon dioxide, substrate 320 is silicon, and core layer 336 is silicon oxide. Waveguide 334 may be a strip waveguide, ridge waveguide, an optical fiber laid across the surface of substrate 320 or any other type.
Reflector 340 may be formed from etching the layers that form waveguide 334, according to an embodiment. A wet anisotropic etchant (e.g., tetramethyl ammonium hydroxide (TMAH) and/or potassium hydroxide (KOH)) may be used to strip away the material along the crystal planes to form the surface of reflector 340. The surface may be further smoothed via thermal oxidation of silicon and oxide removal process by quickly exposing reflector 340 to another chemical etchant such as hydrofluoric acid (HF). Dry etching techniques may be employed as well for creating the angled surface of reflector 340. For example, reactive ion etching (RIE) using a grey-scale type mask to produce photoresist at varying heights can be used to produce non-planar structures.
Reflector 340 is placed a short distance from an end of waveguide 334, according to an embodiment. This distance cannot be too large, or else the beam of radiation exiting from waveguide 334 will spread too far and undesirable optical losses will occur. In this embodiment, both reflector 340 and waveguide 334 are patterned in-plane on a first surface of substrate 320. Reflector 340 may be designed to have a surface that is angled. For example, reflector 340 may have a surface that is angled at a substantially 45 degree angle with respect to the first surface of substrate 320. This angle causes the beam of radiation to be directed at an angle that is substantially perpendicular to the surface of substrate 320. In another example, reflector 340 has a surface that is angled at a substantially 54.74 degree angle with respect to the first surface of substrate 320. In the embodiment illustrated in
A monolithic holder 350 includes recesses 352 to physically retain and guide rigid beam input/output sections 322. The cross-sectional view in
In addition, the features described above with respect to
In some embodiments, alignment between optical elements 404 and the optical outputs might not be needed for performing merged optical tissue evaluation and laser ablation. That is, cap 410 may include a material that is substantially transparent to a range of wavelengths of light used for optical interrogation and a range of wavelengths of light used for laser ablation. For example, the material of cap 410 may be substantially transparent at 1.3 μm for optical tissue evaluation and at 980 nm or 1060 nm for laser ablation. In some cases, cap 410 may include an anti-reflective coating to avoid undesired back reflections and provide a maximum transmitted energy to the tissue.
Merged Optical Evaluation and Laser Ablation Embodiments
In some embodiments, coupling element 506 may couple first and second optical sources 502 and 504 together in a single fiber, for propagation of one or more exposure radiation beams and laser ablation energy beams in the same fiber down sheath 106 of catheter 100. Optical splitter 508 may separate or split the one or more exposure radiation beams from the one or more laser energy beams at the distal section 104 of catheter 100. In some embodiments, optical splitter 508 and/or coupling element 506 may be located in processing device 108 or proximal section 102 of catheter 100. After the beams are isolated, first multiplexer 510 may direct the one or more beams of exposure radiation to the plurality of optical ports 326 of distal section 104 of catheter 100. In some embodiments, first multiplexer 510 may include a passive multiplexer (e.g., distribution tree) or an active multiplexer (e.g., switch) in which the one or more beams of exposure may be directed to one or more optical ports 326. Second multiplexer 512 may direct the laser energy to at least one optical port of the plurality of optical ports 326 of distal section 104 of catheter 100. The one or more beams of exposure radiation and laser energy from first and second multiplexers 510 and 512 may be coupled by coupling element 513, which may be a fiber optic coupling element. The one or more beams of exposure radiation and laser ablation energy may then be transmitted to sample 514 from the plurality of optical ports 326. In some embodiments, first and second multiplexers 510 and 512 may be located in distal section 102 or proximal section 104 of catheter 100. In additional embodiments, a single multiplexer may be utilized to multiplex both the laser ablation energy and the one or more beams of exposure radiation to at least one optical port of the plurality of optical ports 326. Although
The merged optical evaluation and laser ablation catheter as described herein may be further configured to perform temperature measurements. For example, a detector (e.g., located in processing device 108 or in proximal section 102 or distal section 104 of catheter 100) may determine one or more temperatures of target tissue by measuring a blackbody spectrum emitted by the tissue before, during, or after laser ablation.
In some embodiments, the merged optical evaluation and laser ablation catheter may be implemented using silicon nitride as the material of the waveguide in order for low loss and broad bandwidth. Silicon nitride may allow optical waveguide loss as low as 0.7 dB/m, and the material may be transparent from 400 nm (silicon nitride bandgap) to 4000 nm (SiO2 absorption) approximately. In some embodiments, silicon nitride materials may also have a higher refractive index than silicon dioxide materials as the wavelengths of interest (e.g., 980 nm for laser ablation, 1300 nm for optical tissue evaluation, 2000 nm for temperature measurements). Table 1 provides values of measured refractive index values of both Si3N4 and SiO2 materials grown via Plasma-Enhanced Chemical Vapor Deposition (PECVD) as a function of the wavelength.
In some embodiments, the tissue evaluation functionality may be prioritized during design of the focusing optical elements of the substrate for the merged optical evaluation and laser ablation catheter. For example, a design wavelength of about 1300 nm, and reaching a depth of focus (DOF) of 1.5 mm in tissue, may be desired to accurately evaluate lesion transmurality. In order to get the desired DOF in tissue, a waist beam diameter of about 30.54 μm may be used at the focal point, which is placed at a distance equal to half DOF from the cap outer wall, e.g., 0.75 mm, according to an embodiment.
In an embodiment, reflector 810 is formed from a facet at the end of waveguide 804. In this way, a beam of radiation 812 is reflected downwards towards substrate 802 before it has exited from waveguide 804. An antireflective (AR) coating 816 may be included at an interface between waveguide 804 and substrate 802, according to an embodiment. AR coating 816 may be patterned such that it only exists beneath reflector 810. In another example, AR coating 816 covers a larger area on the surface of substrate 802. AR coating 816 may exist across the entire surface of substrate 802.
In some embodiments, in order to avoid undesired back-reflections coming from the lens interface, an AR layer 820 is provided on the lenses, as shown in
In additional embodiments, AR layer 820 comprises silicon nitride. In some embodiments, a layer thickness of about 174 nm for AR layer 820 results in negligible reflectivity if used in air, while a reflectivity value of about 2% is reached when saline is in contact with the lenses. Similarly, AR layers 823 and 824 may similarly be designed to avoid undesired reflectivity in both the cap's 821 inner and outer surfaces.
In some embodiments, the waveguide of
High Power Considerations of Catheter Embodiments
In some embodiments, there may be high power considerations for the merged optical evaluation and laser ablation system of the catheter. For example, the power of the laser ablation energy that is utilized to ablate tissue is in the order of few tens of Watts.
The light-matter interaction may become non-linear for high optical intensities. In one embodiment, laser ablation energy emitted at a wavelength of 980 nm with powers up to 12 W may be delivered to the target tissue. For example, in an embodiment of an embedded silicon nitride waveguide of 1 μm2 cross-section area, the power density reaches about 1.2 GW/cm2. In this embodiment, several non-linear effects may become relevant due to the relatively large optical intensities propagating through the waveguide, such as Two-Photon Absorption (TPA), nonlinear loss and refractive index, Four-Wave Mixing (FWM), Self-Phase Modulation (SPM) and Cross-Phase Modulation (XPM). In the presence of non-linear loss, the total loss coefficient may be described in Equation 1 as:
α=αL+αNL(|E|2) (1)
where αL, αNL and |E|2 accounts for the linear loss contributions, non-linear loss contributions, and the optical intensity, respectively.
During the TPA process, the band gap energy of a certain material may be bridged by the energy absorption of two photons, thus exciting electrons from the valence to the conduction bands. This process may induce non-linear loss αNL,TPA, which is dependent on the optical intensity according to Equation 2:
αNL,TPA=α2(|E|2) (2)
where α2 is the TPA coefficient. The energy band gap of silicon nitride may be calculated as follows in Equation 3:
where h, c, n and λ0 are the Planck constant (h=4.136·10−15 eV·s), the speed of light in the vacuum, the refraction index of silicon nitride (n0=1.9378) and the onset wavelength, which is about 400 nm, respectively. On the other hand, the energy band gap at the laser ablation wavelength (e.g., at 980 nm), is calculated by Equation 4:
Equations 3 and 4 show that TPA should not occur in silicon nitride at 980 nm because photon energies at this wavelength are less than Eg(SiN)/2. In addition, an optical intensity of 1.2 GW/cm2 assures a linear regime in the waveguide because non-linear loss is induced by power densities typically at least one order of magnitude higher.
In some embodiments, high optical intensities may also lead to non-linear refractive index, in which the dependence can be written as shown in Equation 5:
n(ω,|E|2)=n0(ω)+n2|E|2 (5)
where E is the electric field amplitude and n2 is the non-linear Kerr coefficient that is related to the third-order material susceptibility χ(3) by Equation 6
In an example, the non-linear Kerr coefficient was experimentally measured in silicon nitride waveguides to be n2=2.4.10−15 cm2/W. This measurement indicates refractive index changes in the order of 2.88.10−6 at 980 nm, which is more than one order of magnitude lower compared with the thermo-optical effect efficiency in silicon nitride.
In χ(3)-materials, the third-order polarization term may involve the nonlinear interaction of four waves and leads to the phenomenon of FWM. In an embodiment, the FWM may result from the radiation-induced modulation of the refractive index as shown by Equation 5, where E(t)=E1 cos(2πf1t)+E2 cos(2πf2t)+E3 cos(2πf3t) with f1=0.15·1015 Hz, f2=0.231·1015 Hz, and f3=0.306·1015 Hz. The frequencies f1, f2, and f3 correspond to the frequencies of the temperature monitoring, the tissue evaluation, and the ablation systems respectively. As a result, the generation of light at the new frequencies are detailed in the following Table 2:
In some embodiments, the new frequencies that are below 400 nm and greater than 4000 nm in Table 2 may not be propagated due to the silicon nitride bandgap and SiO2 absorption, respectively. Moreover, the generated frequencies that involve the temperature signal (f1) are expected to be negligible because of its very low optical intensity (e.g., according to the black body spectrum shown in
In some embodiments, another consequence of the Kerr effect may be Self-Phase Modulation (SPM). As derived by Equation 5, relatively large optical intensities may result in a varying refractive index of the medium enabled by light-matter interaction. This variation in the refractive index produces a phase shift of the optical signal, which translates into a broadening of the frequency spectrum. In some embodiments, this change may be irrelevant for both the tissue evaluation and the temperature monitoring systems because the change in the spectrum characteristics of the laser ablation signal may not have any impact on them. However, apart from SPM, Cross-Phase Modulation (XPM) may also occur. XPM is similar to SPM, but the phase shift induced by the intensity of light affects other frequencies instead of the laser ablation frequency. The strength of the XPM effect decreases with the wavelength detuning between the pump (laser ablation) and the probe (tissue evaluation) signals. Taking into account that the wavelength detuning may be greater than 300 nm, this effect might not provide any significant impact on the tissue evaluation wavelengths.
Example Method of Operation
Catheter 100 may be used to perform merged optical evaluation, laser ablation, and temperature monitoring of target tissue according to embodiments described herein. At least a portion of tissue volume surrounding one or more optical ports of the plurality of optical ports in the distal section 104 of catheter 100 may be ablated. By adjusting the laser power and ablation time, the total laser energy delivered to target tissue may be accurately controlled. In additional embodiments, the catheter may also provide temperature monitoring and additional cooling to surrounding blood flow around the target tissue.
Various ablation methods and other embodiments of ablation catheters with substrates described thus far can be implemented, for example, using catheter 100 shown in
At block 1202, an ablation catheter is provided. For example, an ablation catheter with a proximal end, a distal end with a plurality of optical ports, and a sheath coupled between the proximal end and the distal end is provided. For example, the ablation catheter may include a holder configured to maintain the plurality of optical ports in a fixed spatial relationship and a cap that is substantially transparent at wavelengths of the exposure radiation, the temperature monitoring system and laser energy, in which the cap is secured to the holder and configured to cover the holder and the plurality of optical ports.
At block 1204, one or more beams of exposure radiation may be transmitted to a sample via the plurality of optical ports. For example, the one or more beams of exposure radiation may be provided from a first optical source configured to generate a source beam of exposure radiation. The one or more beams of exposure radiation from the source beam may be directed to the plurality of optical ports by a multiplexer located in the proximal end or distal end of the catheter.
At block 1206, one or more beams of scattered or reflected radiation from the sample may be received from the sample via the plurality of optical ports. For example, the one or more beams of scattered or reflected radiation may be guided by optical transmission media in the sheath of the catheter
At block 1208, at least a portion of the sample may be ablated with laser energy output from at least a portion of the optical ports. For example, the laser energy may be provided from a second optical source configured to generate the laser energy. The laser energy from the second optical source may be directed to at least one optical port by a multiplexer located in the proximal end or distal end of the catheter.
It is to be appreciated that the Detailed Description section, and not the Summary and Abstract sections, is intended to be used to interpret the claims. The Summary and Abstract sections may set forth one or more but not all exemplary embodiments of the present invention as contemplated by the inventor(s), and thus, are not intended to limit the present invention and the appended claims in any way.
Embodiments of the present invention have been described above with the aid of functional building blocks illustrating the implementation of specified functions and relationships thereof. The boundaries of these functional building blocks have been arbitrarily defined herein for the convenience of the description. Alternate boundaries can be defined so long as the specified functions and relationships thereof are appropriately performed.
The foregoing description of the specific embodiments will so fully reveal the general nature of the invention that others can, by applying knowledge within the skill of the art, readily modify and/or adapt for various applications such specific embodiments, without undue experimentation, without departing from the general concept of the present invention. Therefore, such adaptations and modifications are intended to be within the meaning and range of equivalents of the disclosed embodiments, based on the teaching and guidance presented herein. It is to be understood that the phraseology or terminology herein is for the purpose of description and not of limitation, such that the terminology or phraseology of the present specification is to be interpreted by the skilled artisan in light of the teachings and guidance.
The breadth and scope of the present invention should not be limited by any of the above-described exemplary embodiments, but should be defined only in accordance with the following claims and their equivalents.
This application claims the benefit under 35 U.S.C. § 119(e) of U.S. provisional patent application Ser. No. 62/686,159, filed Jun. 18, 2018, which is incorporated by reference herein in its entirety.
Number | Date | Country | |
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62686159 | Jun 2018 | US |