WO2016029402A1 - Shear wave imaging method and system - Google Patents

Shear wave imaging method and system Download PDF

Info

Publication number
WO2016029402A1
WO2016029402A1 PCT/CN2014/085391 CN2014085391W WO2016029402A1 WO 2016029402 A1 WO2016029402 A1 WO 2016029402A1 CN 2014085391 W CN2014085391 W CN 2014085391W WO 2016029402 A1 WO2016029402 A1 WO 2016029402A1
Authority
WO
WIPO (PCT)
Prior art keywords
shear wave
propagation
echo information
shear
module
Prior art date
Application number
PCT/CN2014/085391
Other languages
French (fr)
Chinese (zh)
Inventor
李双双
樊睿
Original Assignee
深圳迈瑞生物医疗电子股份有限公司
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 深圳迈瑞生物医疗电子股份有限公司 filed Critical 深圳迈瑞生物医疗电子股份有限公司
Priority to CN201910848338.5A priority Critical patent/CN110507361B/en
Priority to CN201480081075.5A priority patent/CN106572837B/en
Priority to CN201910847967.6A priority patent/CN110507360B/en
Priority to PCT/CN2014/085391 priority patent/WO2016029402A1/en
Priority to CN201910847961.9A priority patent/CN110507359B/en
Publication of WO2016029402A1 publication Critical patent/WO2016029402A1/en

Links

Classifications

    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B8/00Diagnosis using ultrasonic, sonic or infrasonic waves
    • A61B8/08Detecting organic movements or changes, e.g. tumours, cysts, swellings
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/14Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object using acoustic emission techniques

Definitions

  • the present invention relates to the field of ultrasonic imaging, and in particular to a shear wave imaging method and system. Background technique
  • Ultrasound elastography is one of the hotspots of clinical research in recent years. It mainly reflects the elasticity or softness of tissues. It has been applied more and more in the auxiliary detection of cancerous lesions, benign and malignant discrimination, and evaluation of prognosis.
  • ultrasound elastography uses shear waves for imaging, mainly by generating shear wave propagation inside the tissue and detecting its propagation parameters and imaging, thereby reflecting the difference in hardness between tissues.
  • a shear wave imaging method and system are provided to improve the detection signal to noise ratio, reduce the number of redundant detections, and speed up the detection process.
  • a shear wave imaging method comprising the following steps,
  • Estimating the position of the shear wave at different times transmitting a plurality of tracking pulses corresponding to the shear wave at different times and receiving echo information of the tracking pulse;
  • Imaging shows the results of the shear wave parameter calculation.
  • the tracking pulses are transmitted to the respective shear wave estimation positions at the respective times, and the echo information of the respective tracking pulses is received.
  • is any time after the generation of the shear wave
  • is the initial propagation time of the shear wave, which is the average velocity of the shear wave propagating in the target tissue.
  • the moving distance of the shear wave detecting position between two adjacent detecting moments is less than or equal to c h At , and the detecting width of the shear wave is greater than or equal to each of the detected shear waves.
  • the speed varies from to, and At is the time interval between two adjacent detection times.
  • the shear wave parameter when calculating the shear wave parameter based on the echo information of the tracking pulse, performing at least one of a propagation distance of the shear wave, a propagation speed of the shear wave, and a Young's modulus of the target tissue Calculation.
  • the method further includes the following steps:
  • Correlation correlation is performed between the echo information of the tracking pulse at different times in each position in the target area and the reference information corresponding to the position, and the particle displacement data at different times at the position is obtained.
  • the echo information of the tracking pulse at a certain time is selected as the reference information or the reference pulse is transmitted before the shear wave propagation, and the echo information of the reference pulse is used as the reference echo information.
  • the propagation speed of the shear wave satisfies the following formula:
  • C represents the propagation velocity, which can be regarded as longitudinal displacement data, or can be calculated using longitudinal velocity data, where X represents the lateral coordinate and z represents the longitudinal coordinate.
  • a propagation velocity profile is formed, At least one of a Young's modulus parameter map, a shear modulus parameter map, a propagation distance parameter map for a certain period of time, and an average velocity value parameter map within the target region.
  • a shear wave imaging system includes an ultrasound probe, a control module, a signal processing module, a calculation module, and a display system.
  • the ultrasound probe is provided with a transceiver module, a transceiver module, a signal processing module, a calculation module, and a display of the ultrasound probe.
  • the system is connected in sequence, the control module is connected to the transceiver module, and the transceiver module is configured to transmit a tracking pulse according to a shear wave estimation position, and receive echo information of the tracking pulse and the reference pulse;
  • the control module is configured to control the transceiver module to transmit a tracking pulse
  • the signal processing module is configured to perform signal preprocessing on the echo information
  • the calculation module is configured to estimate a shear wave estimation position of the shear wave at different times, and process and calculate a signal output by the signal processing module;
  • the display system is configured to perform image display on a shear wave parameter calculation result generated by the calculation module.
  • calculation module includes
  • an estimating unit configured to estimate a shear wave estimated position of the shear wave at each moment according to an average length of the shear wave propagation time and a shear wave propagation in the target tissue.
  • a data calculation unit for calculating a propagation parameter of the shear wave For calculating a propagation parameter of the shear wave.
  • the shear wave imaging method and system provided by the invention pre-estimate the detection position of the shear wave, so that the detection of the shear wave can be performed in a small range and accurately, so that the detection energy is relatively concentrated, and the detection signal-to-noise ratio is improved. At the same time, it reduces the number of redundant detections, speeds up the detection process, and reduces the data processing burden.
  • FIG. 1 is a schematic flow chart of a shear wave imaging method provided by the present invention.
  • FIG. 2 to FIG. 5 are schematic diagrams showing pulse sequences for emitting different acoustic radiation forces in the shear wave imaging method of the present invention
  • 6 is a schematic diagram showing the change of the shear wave detecting position with time according to the shear wave imaging method of the present invention
  • FIG. 7 to FIG. 8 are schematic diagrams showing the emission deflection angle of the deflection angle of the different tracking pulses in the present invention
  • FIG. 9 is a schematic view showing the configuration of a shear wave imaging system provided by the present invention. detailed description
  • a preferred embodiment of the present invention provides a shear wave imaging method for predicting a detection position of a shear wave in advance, so that the detection of the shear wave can be performed in a small range and accurately, so that the detection energy is relatively concentrated. Improve the detection signal to noise ratio. At the same time, the number of redundant detections is reduced, the detection process is accelerated, and the data processing burden is reduced.
  • the shear wave imaging method of the present invention comprises the following steps:
  • Step S101 generating a shear wave inside the tissue.
  • various methods can be used to generate shear waves inside the tissue, such as external waves vibrating inside the tissue to generate shear waves, and also by transmitting acoustic radiation force pulses to the inside of the tissue (ARFI, acoustic radiation Force impulse ) and the like generate shear waves inside the tissue.
  • ARFI acoustic radiation Force impulse
  • the acoustic radiation force pulse may or may not be in focus.
  • the shear wave itself generated by the acoustic radiation force pulse has a small amplitude, and since the shear wave is rapidly attenuated with the propagation, a series of acoustic radiation force pulses can be emitted to increase the shear wave intensity. , or widening the propagation range of the shear wave, or changing the characteristics of the shear wave waveform has improved the detection sensitivity, etc., thereby avoiding imaging due to the attenuation of the shear wave.
  • multiple focus pulses can be continuously transmitted to the same position to increase the intensity of the generated shear wave.
  • the position of the longitudinal direction of the focus pulse (in the direction of the focus emission) and the direction of the lateral direction (the direction perpendicular to the focus emission) can be changed to widen the propagation range of the shear wave and make the cut The cut wave propagates in a specific direction.
  • pulses can be simultaneously transmitted at different lateral positions to superimpose two shear wave waveforms arriving at different times for convenient detection.
  • Step S102 estimating a position of the shear wave at different times, corresponding to the shear wave being different
  • the position of the moment transmits a plurality of tracking pulses and receives echo information of the tracking pulses.
  • the step S102 further includes the following steps:
  • step S1021 the propagation speed of the shear wave in the target tissue is estimated.
  • the shear wave After the shear wave is generated, it begins to propagate in the tissue, and its propagation speed is different depending on the elastic properties of the tissue. In order to estimate the chasing shear wave, it is necessary to estimate an average speed according to the target organization and estimate the possible speed variation range to c A .
  • the average speed and range can refer to existing academic measurement data, or measurement experience, etc., depending on the situation. Pre-designated. For example, suppose the average propagation velocity of the shear wave in the target tissue is about 2m/s, the possible range of variation is l ⁇ 4m/s, etc., or the average propagation velocity is lm/s, and the possible variation range is 0.5 ⁇ 2m/s and so on.
  • Step S1022 Estimating the position of the shear wave in the target tissue at each time according to the propagation speed of the shear wave in the target tissue, and acquiring the shear wave estimate of the shear wave at each moment. position.
  • the moving distance of the shear wave detecting position between two adjacent detecting moments is less than or equal to ⁇
  • Step S1021 Send a tracking pulse to the corresponding shear wave estimation position at each time, and receive echo information of each tracking pulse.
  • the system transmits the tracking pulse at intervals to continuously detect, and each detection maintains a certain detected lateral beamwidth, that is, simultaneously recovers a certain width of echo information, echo information.
  • the interval of the lateral positions may not be too large to ensure a certain lateral resolution.
  • the beam center remains less than ⁇ between adjacent detections. The moving distance, or if At is small, causes ⁇ to be too small, it is also equivalent to the moving distance at which the beam center distance remains less than every n detection times.
  • the system can start detecting from any time or start from a distance from the shear wave source. It is only necessary to estimate the possible position of the shear wave at the current position or the current time according to the average propagation speed. The shear wave is transmitted to this position and left to change the center position of each test.
  • the system may be required to have ultra-wide beam combining capability, that is, to recover echo information of multiple lateral positions at the same time.
  • the number of beams is, for example, 1 to 1024, and the system adjusts according to requirements, such as 4 beams, 16 beams, 32 beams, 64 beams, 96 beams, 128 beams, and so on. The wider the beam, the weaker the focus of the transmitted sound field, and the more uniform the lateral distribution of the sound field energy, the less concentrated it will also result in a lower signal-to-noise ratio for each detected position in the beam.
  • the same center position can be transmitted multiple times in succession, each time the angle of the beam is different, and then the echo signals of different angles are combined to increase the signal-to-noise ratio.
  • the number of angles and the angle of deflection are adjusted by the system according to actual needs, such as using three angles and deflecting -5. , 0. , 5. Wait.
  • Step S103 performing shear wave parameter calculation according to the echo information of the tracking pulse.
  • various parameters such as propagation distance, propagation speed, Young's modulus, and the like can be calculated.
  • the echo information of the tracking pulse at each moment can be integrated to obtain the echo information of the shear wave at various positions of the target tissue during the propagation process, and the shear wave is just here. Pass the corresponding position for a short period of time.
  • the step S103 further includes the following steps:
  • Step S1031 Obtain reference information; It can be understood that the reference information can be selected according to needs. For example, the echo information of the tracking pulse at a certain moment in the corresponding position is selected as the reference information. It is also possible to transmit a reference pulse before the shear wave propagation and use the echo information of the reference pulse as reference echo information. The reference is required for cross-correlation comparison with tracking pulses that are chasing the shear wave.
  • Step S1032 Correlate the echo information of the tracking pulse at different times in each position in the target area with the reference information corresponding to the position, and obtain the particle displacement data at different times at the position. Further, a displacement-time curve at the position can be formed, during which the shear wave experiences the entire process of approaching, reaching, and leaving the position, and a peak appears in the corresponding curve. As shown in Figure 5, by For the estimated pursuit detection, a corresponding small displacement-time curve can be obtained for each lateral position, but the time corresponding to the curve is different, and the moments corresponding to the adjacent positions may partially overlap. The position of the peak on the displacement-time curve corresponds to the moment when the shear wave reaches the position.
  • the cross-correlation comparison can be performed to obtain the corresponding time difference between the two lateral positions.
  • the shear wave propagation time between these two lateral positions.
  • the ratio of the distance between the lateral positions to the propagation time is the propagation velocity between the two horizontal positions.
  • the displacement data of each lateral position corresponding to the two moments at which the shear wave reaches the position is taken out, and the displacement-transverse position curve of the two moments is formed, and the cross-correlation comparison of the two curves can obtain two
  • the difference in lateral position between the moments which corresponds to the propagation distance of the shear wave between the two moments.
  • the ratio of the propagation distance to the time difference between the two moments is the propagation velocity near the location.
  • the approximate calculation formula can be derived by directly using the wave propagation equation as follows:
  • c is the propagation velocity, which can be regarded as longitudinal displacement data, or can be calculated using longitudinal velocity data, where X represents the lateral coordinate and Z represents the longitudinal coordinate. It is also possible to transform the above formula into the frequency domain for calculation.
  • the propagation velocity of the shear wave has a nearly fixed relationship with the tissue hardness:
  • E 3pc 2
  • P the tissue density and represents the Young's modulus value of the tissue. Under certain conditions, the larger the Young's modulus, the greater the tissue hardness.
  • the shear modulus the propagation distance in a certain fixed period, the average propagation velocity in the target region, and the like can be further calculated.
  • Step S104 imaging displays the result of the shear wave parameter calculation.
  • the final propagation velocity data After obtaining the final propagation velocity data, it can be displayed on the image to form a propagation velocity distribution map.
  • the difference in propagation velocity between each position on the graph directly reflects the difference in hardness.
  • other parameter maps can also be displayed, such as Young's modulus parameter map, shear modulus parameter map, and propagation distance parameters for a certain period of time.
  • Figure the average speed value parameter map in the target area, and so on.
  • the above parameters can be displayed as a movie map, a plane or a spatial distribution map, a parameter value, a graph, etc., or may be grayscale or color coded, or may be superimposed or merged with other pattern diagrams such as an anatomical map. Show together.
  • the present invention further provides a shear wave imaging system, including an ultrasound probe 11 , a control module 12 , a signal processing module 13 , a calculation module 15 , and a display system 17 .
  • the ultrasound probe 11 is provided with a transceiver module 110 .
  • the transceiver module 110, the signal processing module 13, the calculation module 15, and the display system 17 of the ultrasound probe 11 are sequentially connected, and the control module 12 is connected to the transceiver module 110. among them:
  • the transceiver module 110 is configured to transmit a tracking pulse and receive echo data of the tracking pulse and the reference pulse.
  • the control module 12 is configured to control the transceiver module 110 to transmit a tracking pulse.
  • the control module 12 transmits a specific ultrasound sequence formed by the tracking pulses according to a preset time interval, thereby facilitating the pursuit of the shear wave and for the transceiver module 110 of the ultrasound probe 11 to receive the corresponding echo data.
  • the signal processing module 13 is configured to perform signal preprocessing on the echo data, thereby facilitating the calculation module 15 to perform subsequent calculations.
  • the signal preprocessing may include beamforming processing, and may also include, for example, signal amplification, analog to digital conversion, and orthogonality. Decomposition and so on.
  • the calculation module 15 is for estimating the position of the shear wave at different times and for processing and calculating the signal used for the beam synthesis output.
  • the calculating module 15 includes:
  • the estimating unit 151 is configured to estimate the shear wave estimated position of the shear wave at each moment according to the propagation duration of the shear wave and the average speed of the shear wave propagated in the target tissue.
  • the data calculation unit 153 is configured to calculate a propagation parameter of the shear wave.
  • the display system 17 is for performing image display on the shear wave parameter calculation result generated by the calculation module 15.
  • the physical setting positions of the ultrasound probe 11, the control module 12, the signal processing module 13, the calculation module 15, and the display system 17 can be adjusted as needed, such as the ultrasound probe 11, the control module 12, and the signal processing.
  • the module 13, the calculation module 15 and the display system 17 are uniformly arranged in the same casing to realize an integrated setting; the split settings can also be used, and wired or wirelessly connected for data communication.
  • the shear wave imaging method and system provided by the invention generate shear waves inside the tissue, and predict and pursue the propagation process of the shear wave in a period of time, and the pursuit position changes continuously with the propagation, so each moment It is only necessary to obtain the propagation position information in a small and small range, and then integrate the obtained information to calculate the elasticity-related parameters such as the shear wave wavefront movie map, propagation distance, and propagation speed in the target area, and finally image to reflect between different tissues.
  • the difference in elasticity The shear wave imaging method of the present invention predicts the detection position of the shear wave in advance, so that the detection of the shear wave can be performed in a small range and accurately, so that the detection energy is relatively concentrated, and the detection signal-to-noise ratio is improved. At the same time, the number of redundant detections is reduced, the detection process is accelerated, and the data processing load of the system is reduced.

Abstract

The present invention provides a shear wave imaging method. The method comprises the following steps: generating a shear wave in a tissue; pre-estimating the shear wave, sending tracking pulses many times at positions of the shear wave at different time points and receiving echo information of the tracking pulses; performing shear wave parameter calculation according to the echo information of the tracking pulses; and displaying a result of the shear wave parameter calculation in the form of an image. According to the shear wave imaging method and system provided in the present invention, a detection position of a shear wave is pre-estimated, so that shear wave detection can be accurately performed in a small range, and therefore detection energy is relatively concentrated and the signal-to-noise ratio of the detection is improved; the number of redundant detections is reduced, the detection process is accelerated, and the load of data processing is reduced. The present invention also provides a shear wave imaging system.

Description

剪切^ A像方法及系统  Cutting ^ A image method and system
技术领域 Technical field
本发明涉及超声波成像领域, 尤其涉及一种剪切波成像方法及系统。 背景技术  The present invention relates to the field of ultrasonic imaging, and in particular to a shear wave imaging method and system. Background technique
超声弹性成像是近年来临床研究关心的热点之一,主要反映组织的弹性或 软硬程度, 在组织癌症病变的辅助检测、 良恶性判别、 预后恢复评价等方面得 到越来越多应用。现有一种超声弹性成像釆用剪切波进行成像, 主要通过在组 织内部产生剪切波的传播并检测其传播参数并成像才,从而反映组织间的硬度 差异。  Ultrasound elastography is one of the hotspots of clinical research in recent years. It mainly reflects the elasticity or softness of tissues. It has been applied more and more in the auxiliary detection of cancerous lesions, benign and malignant discrimination, and evaluation of prognosis. There is a prior art ultrasound elastography that uses shear waves for imaging, mainly by generating shear wave propagation inside the tissue and detecting its propagation parameters and imaging, thereby reflecting the difference in hardness between tissues.
此种方法具有较佳的稳定性和可重复操作性。但由于在应用此方法中,组 织内部产生的剪切波较微弱,且剪切波在组织内的传播是一个瞬态过程, 剪切 波传播一定时间与一定距离后就会衰减消失,因此必须在一段时间内快速且大 面积的提取剪切波信息, 对剪切波的提取要求要求较高, 对进行剪切波提取的 提取系统的数据处理负荷较大, 精度较低。 发明内容  This method has better stability and repeatability. However, in the application of this method, the shear wave generated inside the tissue is weak, and the propagation of the shear wave in the tissue is a transient process. When the shear wave propagates for a certain time and a certain distance, it will attenuate and disappear, so it must be The extraction of shear wave information in a fast and large area over a period of time requires high requirements for the extraction of shear waves, and the data processing load of the extraction system for shear wave extraction is large and the precision is low. Summary of the invention
提供一种剪切波成像方法及系统,提升检测信噪比,减少冗余的检测次数, 加快检测过程。  A shear wave imaging method and system are provided to improve the detection signal to noise ratio, reduce the number of redundant detections, and speed up the detection process.
一种剪切波成像方法, 包括以下步骤,  A shear wave imaging method, comprising the following steps,
于组织内部产生剪切波;  Producing shear waves inside the tissue;
预估所述剪切波在不同时刻的位置,对应所述剪切波在不同时刻的位置发 送多次追踪脉冲并接收所述追踪脉冲的回波信息;  Estimating the position of the shear wave at different times, transmitting a plurality of tracking pulses corresponding to the shear wave at different times and receiving echo information of the tracking pulse;
根据所述追踪脉冲的回波信息进行剪切波参数计算;  Performing shear wave parameter calculation according to echo information of the tracking pulse;
成像显示所述剪切波参数计算的结果。  Imaging shows the results of the shear wave parameter calculation.
进一步的, 当预估剪切波, 对应所述剪切波在不同时刻的位置发送多次追 踪脉冲并接收所述追踪脉冲的回波信息时, 进一步包括以下步骤,  Further, when the shear wave is estimated, corresponding to the shear wave transmitting the tracking pulse at different times and receiving the echo information of the tracking pulse, the following steps are further included,
预估剪切波于目标组织内的传播速度;  Estimating the propagation velocity of the shear wave within the target tissue;
根据所述剪切波于目标组织内的传播速度预估剪切波在各个时刻于所述 目标组织内的剪切波预估位置; Estimating the shear wave at each moment according to the propagation speed of the shear wave in the target tissue The estimated position of the shear wave in the target tissue;
分别于所述各个时刻向相应的剪切波预估位置发送追踪脉冲,并接收各个 追踪脉冲的回波信息。  The tracking pulses are transmitted to the respective shear wave estimation positions at the respective times, and the echo information of the respective tracking pulses is received.
进一步的, 获取所述剪切波在各个时刻的所述剪切波预估位置时, 所述剪 切波距波源的位置距离 满足:  Further, when the shear wave estimation position of the shear wave is obtained at each moment, the distance between the shear wave and the wave source is satisfied:
dk = (tk - t0 ) * d k = (t k - t 0 ) *
其中, 所述 ^为剪切波产生后的任一时刻, 所述 ^为所述剪切波起始传播 时刻, 为剪切波于所述目标组织内传播的平均速度。  Wherein, ^ is any time after the generation of the shear wave, and ^ is the initial propagation time of the shear wave, which is the average velocity of the shear wave propagating in the target tissue.
进一步的,相邻两次检测时刻之间剪切波检测位置的移动距离小于或等于 chAt , 且每次检测时剪切波的检测宽度大于或等于 其中, 所述预估 的剪切波速度的变化范围为 至 , At为相邻两次检测时刻的时间间隔。 Further, the moving distance of the shear wave detecting position between two adjacent detecting moments is less than or equal to c h At , and the detecting width of the shear wave is greater than or equal to each of the detected shear waves. The speed varies from to, and At is the time interval between two adjacent detection times.
进一步的,根据所述追踪脉冲的回波信息进行剪切波参数计算时,对所述 剪切波的传播距离、剪切波的传播速度、 目标组织的杨氏模量中的至少一种进 行计算。  Further, when calculating the shear wave parameter based on the echo information of the tracking pulse, performing at least one of a propagation distance of the shear wave, a propagation speed of the shear wave, and a Young's modulus of the target tissue Calculation.
进一步的,根据所述追踪脉冲的回波信息进行剪切波参数计算时, 进一步 包括以下步骤:  Further, when performing shear wave parameter calculation according to the echo information of the tracking pulse, the method further includes the following steps:
设定参考信息;  Set reference information;
将目标区域内各个位置的不同时刻的追踪脉冲的回波信息与该位置对应 的参考信息做互相关比较, 获取该位置处不同时刻的质点位移数据。  Correlation correlation is performed between the echo information of the tracking pulse at different times in each position in the target area and the reference information corresponding to the position, and the particle displacement data at different times at the position is obtained.
进一步的,设定参考信息时,选用某一时刻的追踪脉冲的回波信息作为参 考信息或在剪切波传播前发送参考脉冲,并将所述参考脉冲的回波信息作为参 考回波信息。  Further, when the reference information is set, the echo information of the tracking pulse at a certain time is selected as the reference information or the reference pulse is transmitted before the shear wave propagation, and the echo information of the reference pulse is used as the reference echo information.
进一步的,根据所述追踪脉冲的回波信息进行剪切波参数计算时, 所述剪 切波的传播速度满足以下公式:
Figure imgf000004_0001
Further, when the shear wave parameter is calculated according to the echo information of the tracking pulse, the propagation speed of the shear wave satisfies the following formula:
Figure imgf000004_0001
式中, C表示传播速度, 可以视为纵向位移数据, 也可釆用纵向速度数 据进行计算, X代表横向坐标, z代表纵向坐标。  Where C represents the propagation velocity, which can be regarded as longitudinal displacement data, or can be calculated using longitudinal velocity data, where X represents the lateral coordinate and z represents the longitudinal coordinate.
进一步的,成像显示所述剪切波参数计算的结杲时,形成传播速度分布图、 杨氏模量参数图、 剪切模量参数图、 某段时间内的传播距离参数图、 目标区域 内的平均速度值参数图中的至少一种。 Further, when the imaging shows the crusting calculated by the shear wave parameter, a propagation velocity profile is formed, At least one of a Young's modulus parameter map, a shear modulus parameter map, a propagation distance parameter map for a certain period of time, and an average velocity value parameter map within the target region.
一种剪切波成像系统, 包括超声探头、 控制模块、 信号处理模块、 计算模 块及显示系统, 所述超声探头设有收发模块, 所述超声探头的收发模块、 信号 处理模块、计算模块、显示系统依次连接,所述控制模块连接于所述收发模块, 所述收发模块用于根据剪切波预估位置发射追踪脉冲,并接收所述追踪脉 冲与所述参考脉冲的回波信息;  A shear wave imaging system includes an ultrasound probe, a control module, a signal processing module, a calculation module, and a display system. The ultrasound probe is provided with a transceiver module, a transceiver module, a signal processing module, a calculation module, and a display of the ultrasound probe. The system is connected in sequence, the control module is connected to the transceiver module, and the transceiver module is configured to transmit a tracking pulse according to a shear wave estimation position, and receive echo information of the tracking pulse and the reference pulse;
所述控制模块用于控制所述收发模块发射追踪脉冲;  The control module is configured to control the transceiver module to transmit a tracking pulse;
所述信号处理模块用于对回波信息进行信号预处理;  The signal processing module is configured to perform signal preprocessing on the echo information;
所述计算模块用于预估剪切波在不同时刻的剪切波预估位置,并对信号处 理模块输出的信号进行处理计算;  The calculation module is configured to estimate a shear wave estimation position of the shear wave at different times, and process and calculate a signal output by the signal processing module;
所述显示系统用于将所述计算模块生成的剪切波参数计算结果进行图像 显示。  The display system is configured to perform image display on a shear wave parameter calculation result generated by the calculation module.
进一步的, 所述计算模块包括,  Further, the calculation module includes
预估单元,用于根据剪切波的传播时长与剪切波于所述目标组织内传播的 平均速度预估所述剪切波在各个时刻的剪切波预估位置。  And an estimating unit configured to estimate a shear wave estimated position of the shear wave at each moment according to an average length of the shear wave propagation time and a shear wave propagation in the target tissue.
数据计算单元, 用于计算剪切波的传播参数。  A data calculation unit for calculating a propagation parameter of the shear wave.
本发明提供的剪切波成像方法及系统,预先估计剪切波的检测位置,使得 剪切波的检测可以小范围准确的进行,从而使得检测能量相对集中,提升检测 信噪比。 同时还减少冗余的检测次数, 加快了检测过程, 减轻数据处理负担。 附图说明  The shear wave imaging method and system provided by the invention pre-estimate the detection position of the shear wave, so that the detection of the shear wave can be performed in a small range and accurately, so that the detection energy is relatively concentrated, and the detection signal-to-noise ratio is improved. At the same time, it reduces the number of redundant detections, speeds up the detection process, and reduces the data processing burden. DRAWINGS
为了更清楚地说明本发明实施例或现有技术中的技术方案,下面将对实施 例或现有技术描述中所需要使用的附图作简单地介绍,显而易见地, 下面描述 中的附图仅仅是本发明的一些实施例, 对于本领域普通技术人员来讲, 在不付 出创造性劳动的前提下, 还可以根据这些附图获得其他的附图。  In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings used in the embodiments or the description of the prior art will be briefly described below. Obviously, the drawings in the following description are only It is a certain embodiment of the present invention, and other drawings can be obtained from those skilled in the art without any creative work.
图 1是本发明提供的一种剪切波成像方法的流程示意图;  1 is a schematic flow chart of a shear wave imaging method provided by the present invention;
图 2至图 5是本发明的剪切波成像方法中的发射不同声辐射力脉冲序列示 意图; 图 6是本发明中剪切波成像方法的剪切波检测位置随时间变化示意图; 图 7至图 8是本发明中釆用不同追踪脉冲发射偏转角度的发射偏转角度示 意图; 2 to FIG. 5 are schematic diagrams showing pulse sequences for emitting different acoustic radiation forces in the shear wave imaging method of the present invention; 6 is a schematic diagram showing the change of the shear wave detecting position with time according to the shear wave imaging method of the present invention; FIG. 7 to FIG. 8 are schematic diagrams showing the emission deflection angle of the deflection angle of the different tracking pulses in the present invention;
图 9是本发明提供的一种剪切波成像系统的构成示意图。 具体实施方式  9 is a schematic view showing the configuration of a shear wave imaging system provided by the present invention. detailed description
下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清 楚、 完整地描述, 显然, 所描述的实施例仅仅是本发明一部分实施例, 而不是 全部的实施例。基于本发明中的实施例, 本领域普通技术人员在没有作出创造 性劳动前提下所获得的所有其他实施例, 都属于本发明保护的范围。  BRIEF DESCRIPTION OF THE DRAWINGS The technical solutions in the embodiments of the present invention will be described in detail below with reference to the accompanying drawings. All other embodiments obtained by a person of ordinary skill in the art based on the embodiments of the present invention without creative work are within the scope of the present invention.
请参阅图 1, 本发明较佳实施方式提供一种剪切波成像方法, 预先预估剪 切波的检测位置,使得剪切波的检测可以小范围准确的进行,从而使得检测能 量相对集中, 提升检测信噪比。 同时还减少了冗余的检测次数, 加快了检测过 程, 减轻数据处理负担。  Referring to FIG. 1 , a preferred embodiment of the present invention provides a shear wave imaging method for predicting a detection position of a shear wave in advance, so that the detection of the shear wave can be performed in a small range and accurately, so that the detection energy is relatively concentrated. Improve the detection signal to noise ratio. At the same time, the number of redundant detections is reduced, the detection process is accelerated, and the data processing burden is reduced.
本发明的剪切波成像方法包括以下步骤:  The shear wave imaging method of the present invention comprises the following steps:
步骤 S101, 于组织内部产生剪切波。 在本步骤中, 可釆用各种方法于组 织内部产生剪切波,如通过组织外部的外力振动于组织内部产生剪切波,还可 通过向组织内部发射声辐射力脉冲( ARFI, acoustic radiation force impulse )等 方式于组织内部产生剪切波。其中,所述声辐射力脉冲可聚焦,也可以无聚焦。  Step S101, generating a shear wave inside the tissue. In this step, various methods can be used to generate shear waves inside the tissue, such as external waves vibrating inside the tissue to generate shear waves, and also by transmitting acoustic radiation force pulses to the inside of the tissue (ARFI, acoustic radiation Force impulse ) and the like generate shear waves inside the tissue. Wherein, the acoustic radiation force pulse may or may not be in focus.
可以理解的是, 由于发射声辐射力脉冲产生的剪切波本身幅度较小, 又由 于剪切波会随着传播迅速衰减,因此可通过发射一系列声辐射力脉冲以提高剪 切波的强度, 或者拓宽剪切波的传播范围, 或者改变剪切波波形特征已提高检 测灵敏度等, 从而避免由于剪切波的衰减影响成像。  It can be understood that the shear wave itself generated by the acoustic radiation force pulse has a small amplitude, and since the shear wave is rapidly attenuated with the propagation, a series of acoustic radiation force pulses can be emitted to increase the shear wave intensity. , or widening the propagation range of the shear wave, or changing the characteristics of the shear wave waveform has improved the detection sensitivity, etc., thereby avoiding imaging due to the attenuation of the shear wave.
如图 2所示, 可向同一个位置连续发射多次聚焦脉冲, 以提高所产生剪切 波的强度。 如图 3、 4所示, 可向改变连续发射的聚焦脉冲的纵向 (指聚焦发 射的方向)及横向(指与聚焦发射垂直的方向)位置, 以拓宽剪切波的传播范 围, 并使得剪切波沿着某特定方向传播。 如图 5所示, 可同时在不同横向位置 发射脉冲, 以使先后不同时间到达的两个剪切波波形叠加起来, 方便检测。  As shown in Fig. 2, multiple focus pulses can be continuously transmitted to the same position to increase the intensity of the generated shear wave. As shown in FIGS. 3 and 4, the position of the longitudinal direction of the focus pulse (in the direction of the focus emission) and the direction of the lateral direction (the direction perpendicular to the focus emission) can be changed to widen the propagation range of the shear wave and make the cut The cut wave propagates in a specific direction. As shown in Fig. 5, pulses can be simultaneously transmitted at different lateral positions to superimpose two shear wave waveforms arriving at different times for convenient detection.
步骤 S102, 预估所述剪切波在不同时刻的位置, 对应所述剪切波在不同 时刻的位置发送多次追踪脉冲并接收所述追踪脉冲的回波信息。 Step S102, estimating a position of the shear wave at different times, corresponding to the shear wave being different The position of the moment transmits a plurality of tracking pulses and receives echo information of the tracking pulses.
所述步骤 S102进一步包括以下步骤:  The step S102 further includes the following steps:
步骤 S1021, 预估剪切波于目标组织内的传播速度。  In step S1021, the propagation speed of the shear wave in the target tissue is estimated.
剪切波产生后, 开始在组织中传播, 随着组织弹性特性的不同, 其传播快 慢是不同的。 为了预估追击剪切波, 需要根据目标组织估计一个平均速度 并估计可能的速度变化范围 至 cA, 这个平均速度及范围可以参考既有的学术 测量数据、 或者测量经验等, 由系统根据情况预先指定。 比如假定目标组织内 剪切波的平均传播速度约为 2m/s, 可能的变化范围为 l~4m/s等, 或者^ ^定其 平均传播速度为 lm/s, 可能的变化范围为 0.5~2m/s等。 After the shear wave is generated, it begins to propagate in the tissue, and its propagation speed is different depending on the elastic properties of the tissue. In order to estimate the chasing shear wave, it is necessary to estimate an average speed according to the target organization and estimate the possible speed variation range to c A . The average speed and range can refer to existing academic measurement data, or measurement experience, etc., depending on the situation. Pre-designated. For example, suppose the average propagation velocity of the shear wave in the target tissue is about 2m/s, the possible range of variation is l~4m/s, etc., or the average propagation velocity is lm/s, and the possible variation range is 0.5~ 2m/s and so on.
步骤 S1022,根据所述剪切波于目标组织内的传播速度预估剪切波在各个 时刻于所述目标组织内的位置,获取所述剪切波在各个时刻的所述剪切波预估 位置。  Step S1022: Estimating the position of the shear wave in the target tissue at each time according to the propagation speed of the shear wave in the target tissue, and acquiring the shear wave estimate of the shear wave at each moment. position.
在剪切波产生后的不同时刻 ^, 假设剪切波起始传播时刻为 t。, 则可以估 测其距波源的位置距离 满足下式关系:  At different times after the shear wave is generated, it is assumed that the shear wave starts to propagate at t. , you can estimate the distance from the source of the wave source to satisfy the following relationship:
dk = (tk - t0 ) * c d k = (t k - t 0 ) * c
假设相邻两次检测时刻的时间间隔为 At, 即满足: At = ^ - tk_x, 则可以估 测两次检测时刻间剪切波的传播范围 Δ 〜 Mh, 满足: MA = chAt 于是,相邻两次检测时刻之间剪切波检测位置的移动距离小于或等于 Δ , 避免剪切波传播太慢时预估定位超前,同时每次检测时剪切波的检测宽度大于 或等于 ΜΛ - Δ = At(ch - ct ) , 以保证每次预估定位能包含该时刻剪切波所有可 能位置。 Assuming that the time interval between two adjacent detection times is At, that is, satisfying: At = ^ - t k _ x , the propagation range Δ 〜 M h of the shear wave between the two detection times can be estimated, which satisfies: M A = c h At Therefore, the moving distance of the shear wave detecting position between two adjacent detecting moments is less than or equal to Δ, and the estimated positioning is advanced when the shear wave propagation is too slow, and the detection width of the shear wave is detected each time. greater than or equal to Μ Λ - Δ = at (c h - c t), in order to ensure that each of the estimated positioning time a shear wave can contain all possible positions.
步骤 S1021, 分别于所述各个时刻向相应的剪切波预估位置发送追踪脉 冲, 并接收各个追踪脉冲的回波信息。  Step S1021: Send a tracking pulse to the corresponding shear wave estimation position at each time, and receive echo information of each tracking pulse.
如图 6所示,从剪切波传播起始开始, 系统以间隔 发送追踪脉冲以持续 检测,每次检测均保持一定的检测横向波束宽度, 即同时收回一定宽度的回波 信息, 回波信息包括上述一定宽度中各个横向位置的信息,横向位置的间隔不 能太大以保证一定的横向分辨力。同时,相邻检测之间波束中心保持小于 Δ 的 移动距离, 或者如果 At较小导致 Δ 太小, 则也等效于每隔 η个检测时刻之间 波束中心距离保持小于 的移动距离。 当然, 系统可以从任意时刻开始检测 或者从距离剪切波波源一定距离开始检测,只需先根据平均传播速度估计下在 当前位置处或当前时刻下剪切波的可能的位置即可,需要等剪切波传到该位置 并离开后才开始改变每次检测的中心位置。 As shown in Fig. 6, starting from the start of the shear wave propagation, the system transmits the tracking pulse at intervals to continuously detect, and each detection maintains a certain detected lateral beamwidth, that is, simultaneously recovers a certain width of echo information, echo information. Including the information of each of the above-mentioned lateral positions of a certain width, the interval of the lateral positions may not be too large to ensure a certain lateral resolution. At the same time, the beam center remains less than Δ between adjacent detections. The moving distance, or if At is small, causes Δ to be too small, it is also equivalent to the moving distance at which the beam center distance remains less than every n detection times. Of course, the system can start detecting from any time or start from a distance from the shear wave source. It is only necessary to estimate the possible position of the shear wave at the current position or the current time according to the average propagation speed. The shear wave is transmitted to this position and left to change the center position of each test.
由于每次检测必须保持一定的横向波束宽度,而横向线间距不能太大以保 证一定的横向分辨力, 则可能要求系统具备超宽波束合成能力, 即同时收回多 个横向位置的回波信息的能力, 如图 7及图 8所示。 波束数目比如 1~1024, 系统才艮据需要调节, 比如 4波束、 16波束、 32波束、 64波束、 96波束、 128 波束等。 波束越宽, 则意味着发射声场的聚焦越弱, 声场能量横向分布越均匀 越不集中, 这也同时会带来波束中每个检测位置的信噪比的降低。 为了改善检 测质量, 对同一个中心位置, 可以连续发射多次, 每次发射波束的角度不同, 然后将不同角度的回波信号进行合成以增加信噪比。角度数目及偏转角度的大 小都由系统根据实际需要来调节, 比如釆用 3个角度, 偏转 -5。 、 0。 、 5。 等。  Since each detection must maintain a certain lateral beamwidth, and the lateral line spacing cannot be too large to ensure a certain lateral resolution, the system may be required to have ultra-wide beam combining capability, that is, to recover echo information of multiple lateral positions at the same time. Ability, as shown in Figure 7 and Figure 8. The number of beams is, for example, 1 to 1024, and the system adjusts according to requirements, such as 4 beams, 16 beams, 32 beams, 64 beams, 96 beams, 128 beams, and so on. The wider the beam, the weaker the focus of the transmitted sound field, and the more uniform the lateral distribution of the sound field energy, the less concentrated it will also result in a lower signal-to-noise ratio for each detected position in the beam. In order to improve the quality of the detection, the same center position can be transmitted multiple times in succession, each time the angle of the beam is different, and then the echo signals of different angles are combined to increase the signal-to-noise ratio. The number of angles and the angle of deflection are adjusted by the system according to actual needs, such as using three angles and deflecting -5. , 0. , 5. Wait.
步骤 S103, 根据所述追踪脉冲的回波信息进行剪切波参数计算。 根据所 述追踪脉冲的回波信息可以计算出多种参数, 比如传播距离、 传播速度、 杨氏 模量等。  Step S103, performing shear wave parameter calculation according to the echo information of the tracking pulse. According to the echo information of the tracking pulse, various parameters such as propagation distance, propagation speed, Young's modulus, and the like can be calculated.
在本步骤中, 可通过对各个时刻的追踪脉冲的回波信息进行整合,从而获 取剪切波在传播过程中目标组织各个位置处一小段时间内的回波信息,且剪切 波刚好在这一小段时间内通过该对应位置。  In this step, the echo information of the tracking pulse at each moment can be integrated to obtain the echo information of the shear wave at various positions of the target tissue during the propagation process, and the shear wave is just here. Pass the corresponding position for a short period of time.
所述步骤 S103进一步包括以下步骤:  The step S103 further includes the following steps:
步骤 S1031 , 获取参考信息; 可以理解的是, 所述参考信息可根据需要自 行选用。如选用相应位置某一时刻的追踪脉冲的回波信息作为参考信息。也可 在剪切波传播前发送参考脉冲,并将所述参考脉冲的回波信息作为参考回波信 息。 所述参考需要用于与对所述剪切波进行追击的追踪脉冲做互相关比较。  Step S1031: Obtain reference information; It can be understood that the reference information can be selected according to needs. For example, the echo information of the tracking pulse at a certain moment in the corresponding position is selected as the reference information. It is also possible to transmit a reference pulse before the shear wave propagation and use the echo information of the reference pulse as reference echo information. The reference is required for cross-correlation comparison with tracking pulses that are chasing the shear wave.
步骤 S 1032, 将目标区域内各个位置的不同时刻的追踪脉冲的回波信息与 该位置对应的参考信息做互相关比较, 获取该位置处不同时刻的质点位移数 据。 进一步的, 可形成该位置处的位移 -时间曲线, 在这段时间内, 剪切波会 经历接近、 到达并离开该位置的全过程, 对应曲线出现波峰。 如图 5所示, 由 于预估追击检测, 每个横向位置都能得到相应的一小段位移 -时间曲线, 只是 曲线对应的时刻不同, 相邻位置对应的时刻可能会有一部分重叠。 位移-时间 曲线上峰值所在位置即对应着剪切波到达该位置的时刻。 Step S1032: Correlate the echo information of the tracking pulse at different times in each position in the target area with the reference information corresponding to the position, and obtain the particle displacement data at different times at the position. Further, a displacement-time curve at the position can be formed, during which the shear wave experiences the entire process of approaching, reaching, and leaving the position, and a peak appears in the corresponding curve. As shown in Figure 5, by For the estimated pursuit detection, a corresponding small displacement-time curve can be obtained for each lateral position, but the time corresponding to the curve is different, and the moments corresponding to the adjacent positions may partially overlap. The position of the peak on the displacement-time curve corresponds to the moment when the shear wave reaches the position.
剪切波的传播速度有多种计算方法可用, 比如,对同一深度上两个不同横 向位置对应的位移 -时间曲线, 进行互相关比较, 可以得到两横向位置之间对 应的时间差异, 该时间差对应着这两个横向位置之间的剪切波传播时间。横向 位置间的距离与传播时间之比即这两个横行位置间的传播速度。  There are various calculation methods for the propagation speed of the shear wave. For example, for the displacement-time curve corresponding to two different lateral positions on the same depth, the cross-correlation comparison can be performed to obtain the corresponding time difference between the two lateral positions. Corresponds to the shear wave propagation time between these two lateral positions. The ratio of the distance between the lateral positions to the propagation time is the propagation velocity between the two horizontal positions.
比如,对某个位置,取出剪切波到达该位置时刻附近两个时刻分别对应的 各个横向位置的位移数据, 形成两个时刻的位移-横向位置曲线, 对两曲线进 行互相关比较可以得到两个时刻之间的横向位置差异,该位置差对应了这两个 时刻之间的剪切波的传播距离。传播距离与两时刻时间差之比即为该位置附近 的传播速度。  For example, for a certain position, the displacement data of each lateral position corresponding to the two moments at which the shear wave reaches the position is taken out, and the displacement-transverse position curve of the two moments is formed, and the cross-correlation comparison of the two curves can obtain two The difference in lateral position between the moments, which corresponds to the propagation distance of the shear wave between the two moments. The ratio of the propagation distance to the time difference between the two moments is the propagation velocity near the location.
比如可以直接利用波的传播方程推导出近似计算公式如下:
Figure imgf000009_0001
For example, the approximate calculation formula can be derived by directly using the wave propagation equation as follows:
Figure imgf000009_0001
式中, c表示传播速度, 可以视为纵向位移数据, 也可釆用纵向速度数 据进行计算, X代表横向坐标, Z代表纵向坐标。 还可以将上述公式变换到频 域进行计算。  Where c is the propagation velocity, which can be regarded as longitudinal displacement data, or can be calculated using longitudinal velocity data, where X represents the lateral coordinate and Z represents the longitudinal coordinate. It is also possible to transform the above formula into the frequency domain for calculation.
在一定条件下, 剪切波的传播速度与组织硬度有近似固定的关系:  Under certain conditions, the propagation velocity of the shear wave has a nearly fixed relationship with the tissue hardness:
E = 3pc2 式中, P表示组织密度, 表示组织的杨氏模量值。 一定条件下, 杨氏模 量越大, 意味着组织硬度越大。 E = 3pc 2 where P is the tissue density and represents the Young's modulus value of the tissue. Under certain conditions, the larger the Young's modulus, the greater the tissue hardness.
此外,从各位置的剪切波的传播速度值,还可以进一步计算得到剪切模量、 某段固定时间内的传播距离、 目标区域内的平均传播速度等。  Further, from the value of the propagation velocity of the shear wave at each position, the shear modulus, the propagation distance in a certain fixed period, the average propagation velocity in the target region, and the like can be further calculated.
步骤 S 104, 成像显示所述剪切波参数计算的结果。  Step S104, imaging displays the result of the shear wave parameter calculation.
得到最终传播速度数据后,将其显示在图像上可形成传播速度分布图, 图 上各个位置之间的传播速度差异直接反映其硬度差异。 当然,也可以显示其他 参数图, 比如杨氏模量参数图、 剪切模量参数图、 某段时间内的传播距离参数 图、 目标区域内的平均速度值参数图等。 对上述参数, 可经过一定处理显示成 为电影图、平面或空间分布图、参数值、 曲线图等,也可釆用灰阶或彩色编码, 也可与其他模式图比如解剖图进行叠加或融合后一起显示。 After obtaining the final propagation velocity data, it can be displayed on the image to form a propagation velocity distribution map. The difference in propagation velocity between each position on the graph directly reflects the difference in hardness. Of course, other parameter maps can also be displayed, such as Young's modulus parameter map, shear modulus parameter map, and propagation distance parameters for a certain period of time. Figure, the average speed value parameter map in the target area, and so on. The above parameters can be displayed as a movie map, a plane or a spatial distribution map, a parameter value, a graph, etc., or may be grayscale or color coded, or may be superimposed or merged with other pattern diagrams such as an anatomical map. Show together.
如图 9所示, 本发明还提供一种剪切波成像系统, 包括超声探头 11、 控 制模块 12、 信号处理模块 13、 计算模块 15及显示系统 17, 所述超声探头 11 设有收发模块 110, 所述超声探头 11的收发模块 110、 信号处理模块 13、 计 算模块 15、显示系统 17依次连接,所述控制模块 12连接于所述收发模块 110。 其中:  As shown in FIG. 9 , the present invention further provides a shear wave imaging system, including an ultrasound probe 11 , a control module 12 , a signal processing module 13 , a calculation module 15 , and a display system 17 . The ultrasound probe 11 is provided with a transceiver module 110 . The transceiver module 110, the signal processing module 13, the calculation module 15, and the display system 17 of the ultrasound probe 11 are sequentially connected, and the control module 12 is connected to the transceiver module 110. among them:
所述收发模块 110用于发射追踪脉冲,并接收所述追踪脉冲与所述参考脉 冲的回波数据。  The transceiver module 110 is configured to transmit a tracking pulse and receive echo data of the tracking pulse and the reference pulse.
所述控制模块 12用于控制所述收发模块 110发射追踪脉冲。实际使用中, 所述控制模块 12按照预设时间间隔发射追踪脉冲构成的特定的超声序列, 从 而便于追击剪切波并供所述超声探头 11的收发模块 110接收相应的回波数据。  The control module 12 is configured to control the transceiver module 110 to transmit a tracking pulse. In actual use, the control module 12 transmits a specific ultrasound sequence formed by the tracking pulses according to a preset time interval, thereby facilitating the pursuit of the shear wave and for the transceiver module 110 of the ultrasound probe 11 to receive the corresponding echo data.
所述信号处理模块 13用于对回波数据进行信号预处理, 从而便于计算模 块 15进行后续计算, 所述信号预处理可包括波束合成处理, 还可包括如信号 放大、 模数转换、 正交分解等。  The signal processing module 13 is configured to perform signal preprocessing on the echo data, thereby facilitating the calculation module 15 to perform subsequent calculations. The signal preprocessing may include beamforming processing, and may also include, for example, signal amplification, analog to digital conversion, and orthogonality. Decomposition and so on.
计算模块 15用于预估剪切波在不同时刻的位置, 并用于对用于对波束合 成输出的信号进行处理计算。  The calculation module 15 is for estimating the position of the shear wave at different times and for processing and calculating the signal used for the beam synthesis output.
在本实施例中, 所述计算模块 15包括:  In this embodiment, the calculating module 15 includes:
预估单元 151, 用于根据剪切波的传播时长与剪切波于所述目标组织内传 播的平均速度预估所述剪切波在各个时刻的所述剪切波预估位置。  The estimating unit 151 is configured to estimate the shear wave estimated position of the shear wave at each moment according to the propagation duration of the shear wave and the average speed of the shear wave propagated in the target tissue.
数据计算单元 153, 用于计算剪切波的传播参数。  The data calculation unit 153 is configured to calculate a propagation parameter of the shear wave.
显示系统 17用于将所述计算模块 15生成的剪切波参数计算结果进行图像 显示。  The display system 17 is for performing image display on the shear wave parameter calculation result generated by the calculation module 15.
可以理解的是, 所述超声探头 11、 控制模块 12、 信号处理模块 13、 计算 模块 15及显示系统 17的物理设置位置可根据需要自行调整,如可将超声探头 11、 控制模块 12、 信号处理模块 13、 计算模块 15及显示系统 17统一设置于 同一壳体中, 从而实现一体化设置; 也可釆用分体设置, 并通过有线或无线的 方式相连接以进行数据通信。 本发明提供的剪切波成像方法及系统, 于组织内部产生剪切波, 并在一段 时间内预估并追击剪切波的传播过程, 追击位置随着传播的进行不断改变, 因 此每个时刻只需快速小范围获取其传播位置信息, 然后将所得信息进行整合, 计算出目标区域内剪切波波前电影图、传播距离、传播速度等与弹性有关的参 数, 最终成像以反映不同组织间的弹性差异。本发明的剪切波成像方法由于预 先预估了剪切波的检测位置,使得剪切波的检测可以小范围准确的进行,从而 使得检测能量相对集中, 提升检测信噪比。 同时还减少了冗余的检测次数, 加 快了检测过程, 减轻了系统的数据处理负担。 It can be understood that the physical setting positions of the ultrasound probe 11, the control module 12, the signal processing module 13, the calculation module 15, and the display system 17 can be adjusted as needed, such as the ultrasound probe 11, the control module 12, and the signal processing. The module 13, the calculation module 15 and the display system 17 are uniformly arranged in the same casing to realize an integrated setting; the split settings can also be used, and wired or wirelessly connected for data communication. The shear wave imaging method and system provided by the invention generate shear waves inside the tissue, and predict and pursue the propagation process of the shear wave in a period of time, and the pursuit position changes continuously with the propagation, so each moment It is only necessary to obtain the propagation position information in a small and small range, and then integrate the obtained information to calculate the elasticity-related parameters such as the shear wave wavefront movie map, propagation distance, and propagation speed in the target area, and finally image to reflect between different tissues. The difference in elasticity. The shear wave imaging method of the present invention predicts the detection position of the shear wave in advance, so that the detection of the shear wave can be performed in a small range and accurately, so that the detection energy is relatively concentrated, and the detection signal-to-noise ratio is improved. At the same time, the number of redundant detections is reduced, the detection process is accelerated, and the data processing load of the system is reduced.
以上所揭露的仅为本发明一种较佳实施例而已,当然不能以此来限定本发 明之权利范围,本领域普通技术人员可以理解实现上述实施例的全部或部分流 程, 并依本发明权利要求所作的等同变化, 仍属于发明所涵盖的范围。  The above is only a preferred embodiment of the present invention, and of course, the scope of the present invention is not limited thereto, and those skilled in the art can understand all or part of the process of implementing the above embodiments, and according to the present invention. The equivalent changes required are still within the scope of the invention.

Claims

权 利 要 求 Rights request
1、 一种剪切波成像方法, 其特征在于, 包括以下步骤, A shear wave imaging method, comprising: the following steps,
于组织内部产生剪切波;  Producing shear waves inside the tissue;
预估所述剪切波在不同时刻的位置,对应所述剪切波在不同时刻的位置发 送多次追踪脉冲并接收所述追踪脉冲的回波信息;  Estimating the position of the shear wave at different times, transmitting a plurality of tracking pulses corresponding to the shear wave at different times and receiving echo information of the tracking pulse;
根据所述追踪脉冲的回波信息进行剪切波参数计算;  Performing shear wave parameter calculation according to echo information of the tracking pulse;
成像显示所述剪切波参数计算的结果。  Imaging shows the results of the shear wave parameter calculation.
2、 如权利要求 1所述的剪切波成像方法, 其特征在于,  2. The shear wave imaging method according to claim 1, wherein
当预估剪切波,对应所述剪切波在不同时刻的位置发送多次追踪脉冲并接 收所述追踪脉冲的回波信息时, 进一步包括以下步骤,  When the shear wave is estimated, corresponding to the shear wave transmitting the tracking pulse at different times and receiving the echo information of the tracking pulse, the following steps are further included,
预估剪切波于目标组织内的传播速度;  Estimating the propagation velocity of the shear wave within the target tissue;
根据所述剪切波于目标组织内的传播速度预估剪切波在各个时刻于所述 目标组织内的剪切波预估位置;  Estimating a shear wave estimated position of the shear wave in the target tissue at each time according to the propagation speed of the shear wave in the target tissue;
分别于所述各个时刻向相应的剪切波预估位置发送追踪脉冲,并接收各个 追踪脉冲的回波信息。  The tracking pulses are transmitted to the respective shear wave estimation positions at the respective times, and the echo information of the respective tracking pulses is received.
3、 如权利要求 2所述的剪切波成像方法, 其特征在于, 获取所述剪切波 在各个时刻的所述剪切波预估位置时, 所述剪切波距波源的位置距离 满足: dk = (tk - t0 ) * c The shear wave imaging method according to claim 2, wherein when the shear wave estimated position of the shear wave is obtained at each moment, the position distance of the shear wave source is satisfied : d k = (t k - t 0 ) * c
其中, 所述 为剪切波产生后的任一时刻, 所述 ^为所述剪切波起始传播 时刻, 为剪切波于所述目标组织内传播的平均速度。  Wherein, at any time after the generation of the shear wave, the ^ is the initial propagation time of the shear wave, and is the average velocity of the shear wave propagating in the target tissue.
4、 如权利要求 2所述的剪切波成像方法, 其特征在于, 相邻两次检测时 刻之间剪切波检测位置的移动距离小于或等于 At, 且每次检测时剪切波的检 测宽度大于或等于 At(cA - ), 其中, 所述预估的剪切波速度的变化范围为 至 c" , At为相邻两次检测时刻的时间间隔。 4. The shear wave imaging method according to claim 2, wherein a moving distance of the shear wave detecting position between two adjacent detecting times is less than or equal to c3⁄4 At, and the shear wave is detected each time. The detection width is greater than or equal to At(c A - ), wherein the estimated shear wave velocity varies from c " , At is the time interval between two adjacent detection times.
5、 如权利要求 1所述的剪切波成像方法, 其特征在于, 根据所述追踪脉 冲的回波信息进行剪切波参数计算时, 对所述剪切波的传播距离、剪切波的传 播速度、 目标组织的杨氏模量中的至少一种进行计算。  The shear wave imaging method according to claim 1, wherein when the shear wave parameter is calculated based on the echo information of the tracking pulse, the propagation distance of the shear wave and the shear wave are At least one of the propagation speed and the Young's modulus of the target tissue is calculated.
6、 如权利要求 1所述的剪切波成像方法, 其特征在于, 根据所述追踪脉 冲的回波信息进行剪切波参数计算时, 进一步包括以下步骤: 6. The shear wave imaging method according to claim 1, wherein: according to said tracking pulse When the echo information of the punch is calculated by the shear wave parameter, the following steps are further included:
设定参考信息;  Set reference information;
将目标区域内各个位置的不同时刻的追踪脉冲的回波信息与该位置对应 的参考信息做互相关比较, 获取该位置处不同时刻的质点位移数据。  Correlation correlation is performed between the echo information of the tracking pulse at different times in each position in the target area and the reference information corresponding to the position, and the particle displacement data at different times at the position is obtained.
7、 如权利要求 6所述的剪切波成像方法, 其特征在于, 设定参考信息时, 选用某一时刻的追踪脉冲的回波信息作为参考信息或在剪切波传播前发送参 考脉冲, 并将所述参考脉冲的回波信息作为参考回波信息。  7. The shear wave imaging method according to claim 6, wherein when the reference information is set, the echo information of the tracking pulse at a certain time is selected as the reference information or the reference pulse is transmitted before the shear wave propagates. The echo information of the reference pulse is used as reference echo information.
8、 如权利要求 1所述的剪切波成像方法, 其特征在于, 根据所述追踪脉 冲的回波信息进行剪切波参数计算时, 所述剪切波的传播速度满足以下公式:
Figure imgf000013_0001
The shear wave imaging method according to claim 1, wherein when the shear wave parameter is calculated based on the echo information of the tracking pulse, the propagation speed of the shear wave satisfies the following formula:
Figure imgf000013_0001
式中, c表示传播速度, 可以视为纵向位移数据, 也可釆用纵向速度数 据进行计算, X代表横向坐标, Z代表纵向坐标。  Where c is the propagation velocity, which can be regarded as longitudinal displacement data, or can be calculated using longitudinal velocity data, where X represents the lateral coordinate and Z represents the longitudinal coordinate.
9、 如权利要求 1所述的剪切波成像方法, 其特征在于, 成像显示所述剪 切波参数计算的结果时, 形成传播速度分布图、 杨氏模量参数图、 剪切模量参 数图、 某段时间内的传播距离参数图、 目标区域内的平均速度值参数图中的至 少一种。  9. The shear wave imaging method according to claim 1, wherein when the imaging results of the shear wave parameter calculation are performed, a propagation velocity profile, a Young's modulus parameter map, and a shear modulus parameter are formed. The graph, the propagation distance parameter map in a certain period of time, and at least one of the average speed value parameter maps in the target area.
10、 一种剪切波成像系统, 其特征在于, 包括超声探头、 控制模块、 信号 处理模块、 计算模块及显示系统, 所述超声探头设有收发模块, 所述超声探头 的收发模块、 信号处理模块、 计算模块、 显示系统依次连接, 所述控制模块连 接于所述收发模块,  A shear wave imaging system, comprising: an ultrasonic probe, a control module, a signal processing module, a calculation module, and a display system, wherein the ultrasonic probe is provided with a transceiver module, the transceiver module of the ultrasonic probe, and signal processing The module, the computing module, and the display system are sequentially connected, and the control module is connected to the transceiver module.
所述收发模块用于根据剪切波预估位置发射追踪脉冲,并接收所述追踪脉 冲与所述参考脉冲的回波信息;  The transceiver module is configured to transmit a tracking pulse according to a shear wave estimated position, and receive echo information of the tracking pulse and the reference pulse;
所述控制模块用于控制所述收发模块发射追踪脉冲;  The control module is configured to control the transceiver module to transmit a tracking pulse;
所述信号处理模块用于对回波信息进行信号预处理;  The signal processing module is configured to perform signal preprocessing on the echo information;
所述计算模块用于预估剪切波在不同时刻的剪切波预估位置,并对信号处 理模块输出的信号进行处理计算;  The calculation module is configured to estimate a shear wave estimation position of the shear wave at different times, and process and calculate a signal output by the signal processing module;
所述显示系统用于将所述计算模块生成的剪切波参数计算结果进行图像 显示。 The display system is configured to perform image display on the shear wave parameter calculation result generated by the calculation module.
11、 如权利要求 10所述的剪切波成像系统, 其特征在于, 所述计算模块 包括, 11. The shear wave imaging system of claim 10, wherein the calculation module comprises
预估单元,用于根据剪切波的传播时长与剪切波于所述目标组织内传播的 数据计算单元, 用于计算剪切波的传播参数。  The estimating unit is configured to calculate a propagation parameter of the shear wave according to a data calculation unit that is based on a propagation time of the shear wave and a shear wave propagated in the target tissue.
PCT/CN2014/085391 2014-08-28 2014-08-28 Shear wave imaging method and system WO2016029402A1 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
CN201910848338.5A CN110507361B (en) 2014-08-28 2014-08-28 Shear wave imaging method and system
CN201480081075.5A CN106572837B (en) 2014-08-28 2014-08-28 Shearing wave imaging method and system
CN201910847967.6A CN110507360B (en) 2014-08-28 2014-08-28 Shear wave imaging method and system
PCT/CN2014/085391 WO2016029402A1 (en) 2014-08-28 2014-08-28 Shear wave imaging method and system
CN201910847961.9A CN110507359B (en) 2014-08-28 2014-08-28 Shear wave imaging method and system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
PCT/CN2014/085391 WO2016029402A1 (en) 2014-08-28 2014-08-28 Shear wave imaging method and system

Publications (1)

Publication Number Publication Date
WO2016029402A1 true WO2016029402A1 (en) 2016-03-03

Family

ID=55398616

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/CN2014/085391 WO2016029402A1 (en) 2014-08-28 2014-08-28 Shear wave imaging method and system

Country Status (2)

Country Link
CN (4) CN110507361B (en)
WO (1) WO2016029402A1 (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110710989B (en) * 2019-09-27 2021-12-24 深圳迈瑞生物医疗电子股份有限公司 Elasticity imaging method, system and computer readable storage medium
CN111521136B (en) * 2020-05-09 2021-03-26 大连理工大学 Reinforced concrete structure crack depth detection method and detection device based on horizontal shear wave
CN112244889A (en) * 2020-10-15 2021-01-22 中国科学院苏州生物医学工程技术研究所 Method for determining vibration element array, puncture needle imaging method and ultrasonic equipment
CN114403921A (en) * 2022-01-24 2022-04-29 陕西师范大学 Shear wave velocity estimation method and system based on real-time curve tracking technology

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5810731A (en) * 1995-11-13 1998-09-22 Artann Laboratories Method and apparatus for elasticity imaging using remotely induced shear wave
CN101869485A (en) * 2010-06-23 2010-10-27 深圳大学 Ultrasonic imaging method and device
CN102667522A (en) * 2009-11-25 2012-09-12 皇家飞利浦电子股份有限公司 Ultrasonic shear wave imaging with focused scanline beamforming
CN103462643A (en) * 2013-09-29 2013-12-25 深圳市开立科技有限公司 Shear wave speed measurement method, device and system

Family Cites Families (14)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4177281B2 (en) * 2004-03-29 2008-11-05 関西電力株式会社 Measuring apparatus and measuring method
US7675820B2 (en) * 2007-04-17 2010-03-09 Delphi Technologies, Inc. Method of characterizing a vehicle crash event based on shear waves in the vehicle frame
CN101569543B (en) * 2008-04-29 2011-05-11 香港理工大学 Two-dimension displacement estimation method of elasticity imaging
RU2559910C2 (en) * 2009-06-30 2015-08-20 Конинклейке Филипс Электроникс Н.В. Propagation/tracking sequences for vibrometry of dispersion transverse waves
US8500639B2 (en) * 2009-09-11 2013-08-06 Mr Holdings (Hk) Limited Systems and methods for shear wave field formation
US8715185B2 (en) * 2010-04-05 2014-05-06 Hitachi Aloka Medical, Ltd. Methods and apparatus for ultrasound imaging
DE102010014211A1 (en) * 2010-04-08 2011-10-13 Siemens Aktiengesellschaft Evaluation method for a sequence of image data sets with twice the elastic distortion of the image data records
EP2612600B1 (en) * 2010-08-31 2018-02-21 Hitachi, Ltd. Three-dimensional elastic image generation method and ultrasonic diagnosis device
WO2012077579A1 (en) * 2010-12-08 2012-06-14 株式会社日立メディコ Ultrasound diagnosis apparatus
CN103269639B (en) * 2010-12-22 2015-11-25 皇家飞利浦电子股份有限公司 Utilize centroid estimation shear wave velocity
CN102727255B (en) * 2012-07-13 2014-04-30 深圳市理邦精密仪器股份有限公司 Method and device for ultrasonic image space compound imaging
US20140187904A1 (en) * 2012-12-28 2014-07-03 Marjan RAZANI Method and system for determining whether arterial tissue comprises atherosclerotic plaque
CN103431874B (en) * 2013-09-06 2015-06-03 中国科学院深圳先进技术研究院 Method and system for estimating acoustic radiation force pulse imaging
CN103519848A (en) * 2013-10-25 2014-01-22 中国科学院深圳先进技术研究院 Tissue displacement estimation method and system based on ultrasonic echo radio frequency signals

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5810731A (en) * 1995-11-13 1998-09-22 Artann Laboratories Method and apparatus for elasticity imaging using remotely induced shear wave
CN102667522A (en) * 2009-11-25 2012-09-12 皇家飞利浦电子股份有限公司 Ultrasonic shear wave imaging with focused scanline beamforming
CN101869485A (en) * 2010-06-23 2010-10-27 深圳大学 Ultrasonic imaging method and device
CN103462643A (en) * 2013-09-29 2013-12-25 深圳市开立科技有限公司 Shear wave speed measurement method, device and system

Also Published As

Publication number Publication date
CN110507360B (en) 2022-06-03
CN110507360A (en) 2019-11-29
CN110507359B (en) 2022-06-07
CN110507361B (en) 2022-11-29
CN110507361A (en) 2019-11-29
CN106572837A (en) 2017-04-19
CN110507359A (en) 2019-11-29
CN106572837B (en) 2019-10-08

Similar Documents

Publication Publication Date Title
US9895137B2 (en) Ultrasonic diagnosis device and transmission/reception method
JP2015154949A (en) Method and system for obtaining shear wave information in ultrasonic imaging for medical treatment
JP2014004375A5 (en)
JP2012081269A5 (en)
JP2013544615A5 (en)
CN105816205A (en) Sparse tracking in acoustic radiation force impulse imaging
CN104510499A (en) Shear wave detection in medical ultrasound imaging
WO2016033752A1 (en) Elasticity measurement and detection method and system
JP6179940B2 (en) Doppler imaging signal transmitter, Doppler imaging signal receiver, Doppler imaging system and method
JP2010008295A (en) Target searching device, target searching program and target searching method
WO2016029402A1 (en) Shear wave imaging method and system
JP2016512130A (en) System and method for detecting and presenting interventional devices via ultrasound imaging
JP2017535327A (en) Ultrasound system and method for measurements using shear waves
CN105167802A (en) Doppler imaging method and device
JP6724593B2 (en) Active sonar and control method of active sonar
WO2020113397A1 (en) Ultrasonic imaging method and ultrasonic imaging system
JP4815840B2 (en) Sound wave propagation distance estimation method and sound wave propagation distance estimation apparatus
WO2014157510A1 (en) Ultrasonic diagnostic device and ultrasonic diagnostic method
JP2010071920A (en) Ultrasonic flaw detection method, program used for same, and recording medium in which program is recorded
JP5704695B2 (en) Doppler radar system, Doppler radar transmitter and transmission wave optimization method
KR101551469B1 (en) Ultrasonics wave transmission receive focusing method and system using plane wave
Shkuratnik et al. Characteristics of instrumental support of structural heterogeneity control around mining using noise probing signals
JP6610224B2 (en) Bistatic active sonar device and its receiver
CN110495903A (en) The shearing wave based on ultrasound with increased pulse recurrence interval is imaged
WO2019218141A1 (en) Shear wave elasticity measurement method and shear wave elastography system

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 14900929

Country of ref document: EP

Kind code of ref document: A1

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 14900929

Country of ref document: EP

Kind code of ref document: A1

32PN Ep: public notification in the ep bulletin as address of the adressee cannot be established

Free format text: NOTING OF LOSS OF RIGHTS PURSUANT TO RULE 112(1) EPC