IP Library › Granted Patent US 9,239,373
Granted Patent B2
US 9,239,373 · App. 13/298,182 · Granted Jan 19, 2016

Adaptive image optimization in induced wave ultrasound imaging

Inventors: Paul Donald Freiburger (Seattle, WA); Liexiang Fan (Sammamish, WA)
Assignee: Siemens Medical Solutions USA, Inc.
G01S7/52042A61B8/485A61B8/5269A61B8/5292G01S7/52046A61B8/469G01S7/52085
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Quick Facts
Patent No.
US 9,239,373
App. No.
13/298,182
Granted
Jan 19, 2016
Kind
B2
Abstract

Adaptive image optimization is provided in induced wave ultrasound imaging. The values for various transmit and receive parameters may be set adaptively. Based on feedback from use with a given patient, the values are set to better optimize signal-to-noise ratio, off-time, tracking accuracy or other consideration. Transmit frequency, F-number, line spacing, tracking pulse repetition frequency, line sampling count, and/or push pulse amplitude values may adapt.

Claims (43)

1. A method for adaptive image optimization in induced wave ultrasound imaging, the method comprising:

transmitting, from a transducer of an ultrasound system, acoustic energy into a patient;

generating a wave in response to the transmitting;

scanning, with a beamformer of the ultrasound system, a region of the patient with ultrasound;

detecting, from the scanning, displacement of tissue caused by the wave; and

changing a transmit setting of the ultrasound system for transmit operation subsequent to the transmitting, the transmit setting being for a transmit frequency, line spacing, F-number, pulse repetition frequency, line sampling count, acoustic energy amplitude, acoustic energy pulse length, or combinations thereof and the transmit setting changing to a value that is a function of the displacement.

2. The method of claim 1 wherein the wave comprises a longitudinal wave, and the acts of transmitting, generating, scanning and detecting being performed as acoustic radiation force imaging.

3. The method of claim 1 wherein the wave comprises a shear wave, and the acts of transmitting, generating, scanning and detecting being performed as shear wave imaging.

4. The method of claim 1 wherein changing to the value that is the function of the displacement comprises:

calculating a signal-to-noise ratio of the displacement; and

adapting the transmit setting as a function of the signal-to-noise ratio.

5. The method of claim 4 wherein calculating the signal-to-noise ratio comprises calculating a magnitude of the displacement and dividing the magnitude by a value of one for the noise.

6. The method of claim 1 wherein changing to the value that is the function of the displacement comprises:

calculating a wave distance or wave velocity from the displacement; and

adapting the transmit setting as a function of the wave distance or wave velocity.

7. The method of claim 1 wherein changing further comprises adapting the transmit setting as a function of off time of the transmitting, the off time being a limitation due to transducer or tissue temperature.

8. The method of claim 1 wherein changing comprises:

performing the transmitting, generating, scanning, and detecting with a first value of the transmit setting;

repeating the transmitting, generating, scanning, and detecting with different values of the setting; and

selecting the value as one of the values for the setting.

9. The method of claim 1 wherein changing comprises:

performing the transmitting, generating, scanning, and detecting with a first value of the transmit frequency;

repeating the transmitting at different values of the transmit frequency;

setting the value of the transmit frequency of the acoustic energy as a function of a highest of the displacements caused by the performance and repetition at the different values of the transmit frequency.

10. The method of claim 1 wherein changing comprises:

performing the scanning with a first value of a scanning frequency;

repeating the scanning at different values of the scanning frequency;

calculating signal-to-noise ratios from the displacements detected from the performing and repeating of the scanning; and

setting the transmit frequency of the scanning as a function of the signal-to-noise ratios.

11. The method of claim 1 wherein changing comprises:

calculating a shear wave velocity as a function of the displacement;

setting a line spacing as a line density for the scanning, the line spacing being a function of the shear wave velocity.

12. The method of claim 1 wherein changing comprises setting the line spacing for a lateral distance, the lateral distance being a function of the displacement.

13. The method of claim 1 wherein changing comprises setting the F-number as a function of the displacement such that greater focus is provided for lesser displacement and lesser focus is provided for greater displacement.

14. The method of claim 1 wherein changing comprises:

calculating a maximum wave velocity; and

setting the pulse repetition frequency of the scanning as a function of the maximum velocity.

15. The method of claim 14 wherein setting comprises setting the pulse repetition frequency and the line sampling count as a function of the maximum velocity, the line sampling count being a number of repetitions of the transmitting, generating, scanning and detecting for each scan line.

16. The method of claim 1 wherein changing comprises:

performing the transmitting, generating, scanning, and detecting with a first value of the acoustic energy amplitude;

repeating the transmitting, generating, scanning and detecting with different values of the acoustic energy amplitude for the acoustic energy; and

setting the acoustic energy amplitude as a function of the displacements caused by the different values.

17. The method of claim 1 wherein changing further comprises interpolating or extrapolating a setting.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 4, 2012
From: FREIBURGER, PAUL DONALD; FAN, LIEXIANG
To: SIEMENS MEDICAL SOLUTIONS USA, INC.
Reel/Frame 029401/0396 →
Continuity (1)
Related Publication 20130123630A1 · May 16, 2013