Guided wave ablation and sensing

Patent metadata

Field	Value
Publication number	US-10456198-B2
Application number	US-201514730845-A
Country	US
Kind code	B2
Filing date	Jun 4, 2015
Priority date	Jun 4, 2014
Publication date	Oct 29, 2019
Grant date	Oct 29, 2019

Abstract

Systems and methods for the controlled delivery of laser light to target tissue using an improved waveguide. A waveguide controls transmission of wave energy to a target based on direct contact with the target. The waveguide comprises a propagation medium, a cladding causing the electromagnetic wave to be internally reflected in the medium, and an interface formed in the cladding and configured for direct contact with the target. A portion of the laser light penetrates through the cladding at the interface and propagates into the target while a portion internally reflects within the propagation medium.

First claim

What is claimed is:

1. A system for controlled delivery of an electromagnetic wave to a target comprising:
a housing;
a rectangular waveguide for receiving the electromagnetic wave from an electromagnetic source, the rectangular waveguide configured for sliding engagement in the housing, the rectangular waveguide comprising:
a propagation medium coupled to the source for receiving the electromagnetic wave therefrom and configured to transmit the received electromagnetic wave therethrough; and
a cladding surrounding the propagation medium;
wherein the cladding has a lower refractive index relative to a refractive index of the propagation medium to cause the electromagnetic wave to be internally reflected within the propagating medium and to inhibit energy loss as the electromagnetic wave propagates within the propagation medium;
wherein the cladding comprises an interface at a front surface of the rectangular waveguide, the cladding configured for direct physical contact with the target; and
wherein the cladding is configured to permit a first portion of the electromagnetic wave to penetrate through the cladding at the interface and propagate into the target and to cause a second portion of the electromagnetic wave to be internally reflected such that the second portion of the electromagnetic wave continues to propagate within the propagating medium when the cladding is in direct physical contact with the target at the interface and the refractive index of the target at the interface is approximately the same as or greater than the refractive index of the propagating medium;

a first coupling lens through which the electromagnetic source is coupled to the rectangular waveguide;
an ultrasonic sensor positioned at a back surface of the rectangular waveguide and configured to receive photoacoustic signals incited in the target by the first potion of the electromagnetic wave, the ultrasonic sensor receiving the photoacoustic signals along the same axis as the first portion of the electromagnetic wave propagated into the target;
a beam dump for absorbing energy of the second portion of the electromagnetic wave after the electromagnetic wave propagates through the propagation medium; and
a second coupling lens through which the propagation medium is coupled to the beam dump.

2. The system of claim 1 , wherein the rectangular waveguide is configured to receive the electromagnetic wave when the electromagnetic wave has an intensity level suitable for ablation.

3. The system of claim 2 , further comprising an ultrasonic pulser for increasing the penetration depth of the electromagnetic wave propagated into the target.

4. The system of claim 1 , wherein the rectangular waveguide is configured to receive the electromagnetic wave when the electromagnetic wave has an intensity level suitable for detecting photoacoustic waves incited in the target.

5. The system of claim 1 , wherein the propagation medium comprises a slab.

6. The system of claim 1 , wherein the propagation medium comprises at least one of the following: an optically transparent glass, a polymer, and a crystal.

7. The system of claim 1 , wherein the cladding comprises a material having a low refractive index relative to the propagation medium.

8. The system of claim 1 , wherein the cladding comprises at least one of a metal and a polymer.

9. The system of claim 1 , wherein the cladding comprises an active area scaled to control the energy of the first portion of the electromagnetic wave that propagates into the target through the cladding at the interface.

10. The system of claim 9 , wherein the active area comprises a thin film formed by at least one of: mesoporous silica, zeolites, silver, titanium, and molybdenum.

11. The system of claim 9 , wherein the active area comprises a thin section of the cladding relative to other sections of the cladding on the remainder of the rectangular waveguide, thereby allowing an evanescent field formed by internal reflection of the propagated electromagnetic wave to penetrate into an external medium surrounding the rectangular waveguide; and wherein the relatively thick other sections of cladding on the remainder of the rectangular waveguide inhibits energy loss.

12. A method comprising:
coupling an electromagnetic source to a rectangular waveguide through a first coupling lens;
receiving, by the rectangular waveguide, an electromagnetic wave from the electromagnetic source, the rectangular waveguide configured for sliding engagement in a housing and comprising:
a propagation medium coupled to the source for receiving the electromagnetic wave therefrom and configured to transmit the received electromagnetic wave therethrough; and
a cladding surrounding the propagation medium, the cladding comprising an interface configured for direct physical contact with the target, wherein the cladding has a lower refractive index relative to a refractive index of the propagation medium to cause the electromagnetic wave to be internally reflected within the propagating medium and to inhibit energy loss as the electromagnetic wave propagates within the propagation medium, and wherein the cladding comprises an interface at a front surface of the rectangular waveguide, the cladding configured for direct physical contact with the target;

propagating the electromagnetic wave within the propagation medium when the refractive index at the interface of the cladding is less than that of the propagation medium;
propagating a first portion of the electromagnetic wave into the target by penetrating through the cladding at the interface when the cladding is in direct physical contact with the target at the interface and the refractive index of the target at the interface is approximately the same as or greater than the refractive index of the propagation medium, wherein a second portion of the electromagnetic wave is internally reflected such that the second portion of the electromagnetic wave continues to propagate within the propagating medium when the cladding is in direct physical contact with the target at the interface and the refractive index of the target at the interface is approximately the same as or greater than the refractive index of the propagating medium;
receiving, by an ultrasonic sensor positioned at a back surface of the rectangular waveguide, photoacoustic signals incited in the target by the first portion of the electromagnetic wave, wherein the ultrasonic sensor receives the photoacoustic signals along the same axis as the first portion of the electromagnetic wave propagated into the target;
absorbing, by a beam dump, energy of the second portion of the electromagnetic wave after the electromagnetic wave propagates through the propagation medium; and
coupling the propagation medium to the beam dump through a second coupling lens; and
defining an active area in the cladding scaled to control the energy of the first portion of the electromagnetic wave that propagates into the target through the cladding at the interface.

13. The method of claim 12 , wherein the electromagnetic wave has an intensity level suitable for ablation.

14. The method of claim 13 , further comprising providing ultrasonic pulses to the target for increasing the penetration depth of the electromagnetic wave propagated into the target.

15. The method of claim 12 , wherein the electromagnetic wave has an intensity level suitable for detecting photoacoustic waves incited in the target.

16. The method of claim 12 , further comprising cooling the target.

17. The method of claim 12 , wherein the propagation medium

Assignees

• Whiteside Paul James Douglas
• Goldschmidt Benjamin Samuel
• Viator John A
• Curry Randy D
• Golda Nicholas J
• Univ Missouri

Inventors

• Whiteside Paul James Douglas
• Goldschmidt Benjamin Samuel
• Viator John A
• Curry Randy D
• Golda Nicholas J

Classifications

• A61B2018/00785

  Reflected power · CPC title

• G02B6/4206

  Optical features (G02B6/4207, G02B6/421 take precedence) · CPC title

• A61B2018/00005

  Cooling or heating of the probe or tissue immediately surrounding the probe · CPC title

• A61B18/203 Primary

  applying laser energy to the outside of the body · CPC title

• A61B2018/00577

  Ablation · CPC title