IP Library Granted Patent US 12,551,732
Granted Patent B2
US 12,551,732 · App. 17/990,454 · Granted Feb 17, 2026

Method and apparatus for removing microvessels

Inventors: Xinmai Yang (Lawrence, KS); Xueding Wang (Ann Arbor, MI); Yannis M. Paulus (Ann Arbor, MI)
Assignees: University of Kansas; The Regents of the University of Michigan
A61N7/022A61B5/1079A61F9/008A61N2007/0095
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Quick Facts
Patent No.
US 12,551,732
App. No.
17/990,454
Granted
Feb 17, 2026
Kind
B2
Abstract

A method of removing microvessels includes applying a burst of acoustic energy at a target location, applying a pulse of optical energy at the target location, and promoting cavitation at the target location by synchronizing an arrival of the burst of acoustic energy and the optical energy at the target location. The burst of acoustic energy has a pressure below 5.0 MPa. The pulse of optical energy at the target location has a fluence less than 100 mJ/cm 2 . At least a portion of the pulse is concurrent with the burst and the optical energy has an optical area that is overlapping with an acoustic area of the acoustic energy at the target location.

Claims (33)

1 . A system, the system comprising:

an acoustic energy source configured to provide an acoustic energy at a target location;

an optical energy source configured to direct optical energy at the target location, the optical energy and the acoustic energy at least partially overlapping at the target location; and

a synchronizer in data communication with the acoustic energy source and the optical energy source and configured to synchronize an arrival of the acoustic energy and the optical energy at the target location during a rarefaction phase of the acoustic energy without the presence of extraneous nanoparticles or contrast agents.

2 . The system of claim 1 , the acoustic energy source being a therapeutic ultrasound transducer.

3 . The system of claim 1 , the optical energy source being a laser.

4 . The system of claim 1 , the final lens providing an initial spot size of greater than 1.0 mm.

5 . The system of claim 1 , the acoustic energy having a maximum pressure less than 5.0 MPa.

6 . The system of claim 1 , the optical energy having a fluence less than 100 mJ/cm2.

7 . The system of claim 1 , wherein the synchronizer is further configured to measure a traveling time of the acoustic energy.

8 . A non-transient computer readable medium containing instructions for causing a computing device to perform a method of:

providing an acoustic energy to a target location, the acoustic energy having a pressure insufficient to cause cavitation in blood alone; and

providing an optical energy to the target location synchronized with the acoustic energy during a rarefaction phase, the optical energy having a fluence insufficient to cause cavitation in blood alone, wherein a combination of the pressure of the acoustic energy during a rarefaction phase and the fluence of the optical energy causes cavitation in blood without the presence of extraneous nanoparticles or contrast agents.

9 . The computer readable medium of claim 8 , the pressure of the acoustic energy being less than 5.0 MPa.

10 . The computer readable medium of claim 8 , the fluence of the optical energy being less than 100 mJ/cm2.

11 . The computer readable medium of claim 8 , the method further including measuring a traveling time of a photoacoustic wave from the target location to a microphone.

12 . The computer readable medium of claim 8 , the computing device being in communication with an optical energy source and an acoustic energy source, the optical energy source being configured to provide the optical energy and the acoustic energy source being configured to provide the acoustic energy.

13 . A system comprising:

an acoustic energy source configured to provide an acoustic energy at a target location, the acoustic energy source having an opening therethrough;

an optical energy source positioned to direct optical energy at the target location through the opening in the acoustic energy source, the optical energy and the acoustic energy at least partially overlapping at the target location;

a synchronizer in communication with the acoustic energy source and the optical energy source configured to synchronize an arrival of the optical energy with a rarefaction phase of the acoustic energy at the target location without the presence of extraneous nanoparticles or contrast agents; and

one or more sensors configured to detect a photoacoustic wave from the target location, the one or more sensors being in communication with the synchronizer.

14 . The system of claim 13 , the acoustic energy and optical energy sharing a focal axis.

15 . The system of claim 13 , the optical energy having an optical area that is concentric with an acoustic area of the acoustic energy at the target location.

16 . The system of claim 15 , the acoustic area having a diameter less than 4.0 mm at the target location.

17 . A method of removing microvessels, the method comprising:

applying a burst of acoustic energy at a target location in a microvessel, the burst of acoustic energy having a pressure below 5.0 MPa;

applying a pulse of optical energy at the target location, the pulse of optical energy having a fluence less than 100 mJ/cm2, at least a portion of the pulse being concurrent with the burst and the optical energy having an optical area that is overlapping with an acoustic area of the acoustic energy at the target location; and

promoting cavitation at the target location in the microvessel by synchronizing an arrival of the burst of acoustic energy and the optical energy during a rarefaction phase of the acoustic energy at the target location without the presence of extraneous nanoparticles or contrast agents.

18 . The method of claim 17 , the pulse having a wavelength between 400 nm and 2400 nm.

19 . The method of claim 17 , further comprising determining a traveling time of the acoustic energy from an acoustic energy source to the target location; and

generating a delay between providing the burst of acoustic energy from the acoustic energy source and providing the pulse of optical energy from an optical energy source based at least partially on the traveling time.

20 . The method of claim 19 , wherein determining the traveling time includes measuring a time period between the pulse of optical energy and receiving a photoacoustic wave at the acoustic energy source.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 24, 2025
From: YANG, XINMAI
To: UNIVERSITY OF KANSAS
Reel/Frame 072362/0422 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 24, 2025
From: WANG, XUEDING; PAULUS, YANNIS M.
To: THE REGENTS OF THE UNIVERSITY OF MICHIGAN
Reel/Frame 072362/0609 →
Continuity (4)
Continuation In Part 15584317 · May 2, 2017
Provisional Application 63281063 · Nov 18, 2021
Provisional Application 62330699 · May 2, 2016
Related Publication 20230083661A1 · Mar 16, 2023
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