专利摘要:
A shear wave propagation is used to estimate the speed of sound in a patient. An ultrasound scanner detects a time of occurrence of a shear wave at each of multiple locations. The temporal difference in occurrence, taking into account tissue stiffness or shear rate, is used to estimate the velocity of sound for the patient's specific tissue.
公开号:FR3047405A1
申请号:FR1751086
申请日:2017-02-09
公开日:2017-08-11
发明作者:David Duncan；Fan Liexiang；Seungsoo Kim；Yassin Labyed；Stephen Rosenzweig
申请人:Siemens Medical Solutions USA Inc；
IPC主号:

专利说明:

BACKGROUND
The present embodiments relate to a determination of sound velocity with ultrasound.
In ultrasound imaging, the speed of sound is assumed to be 1450 m / s. Delay or phase profiles for focusing ultrasonic beams rely on the assumed velocity of sound. This assumption may not be precise. The speed of sound in a fabric varies on the basis of the characteristics of the fabric.
Ultrasound tomography can be used to measure the speed of sound. An ultrasound tomography is based on the placement of the patient between a transmitter and a receiver. The travel time for the acoustic energy from the transmitter to completely traverse the patient to the receiver is used to calculate the speed of sound in the patient. Most ultrasonic scanners use a pulse-echo system where the same transducer is used for both transmit and receive operations, so that the speed of sound can not be estimated in the same way with pulse systems -echo. Since the location of the acoustic reflection is not known exactly with respect to the transducer, the pulse-echo back-and-forth delay does not directly indicate the speed of sound.
BRIEF SUMMARY As an introduction, the preferred embodiments described below include methods, computer readable media, and systems for sound velocity imaging. Shear wave propagation is used to estimate the velocity of sound in the patient. An ultrasonic pulse-echo scanner detects a moment of occurrence of a shear wave at each of multiple locations. The difference in time of onset, given the stiffness of the tissue or the shear rate, is used to estimate the speed of sound.
In a first aspect, a method is proposed for imaging the speed of sound. An ultrasound scanner transmits an acoustic radiation force pulse into a tissue of a patient along a first line. The ultrasound scanner detects temporal displacements of tissue generated in response to a shear wave resulting from the acoustic radiation force pulse. Displacements are detected at each of at least two locations spaced from the first line. A change in the time of displacements over time for a first of the locations relative to the displacements over time for a second of the locations is detected. The speed of sound in the patient is calculated from the change in time. An image of the speed of sound is generated.
According to the embodiments, the method may comprise one or more of the following steps or features: the transmission comprises transmitting the acoustic radiation force pulse as focused to a depth along the first line, and wherein the detection comprises the detection with at least one of the locations being at a different depth and with the locations being along a second line different from the first line; the transmission comprises the transmission with the first line being at an angle away from the normal to a transducer, and wherein the detection comprises detecting with the locations along a second line at a different angle from the transducer of the one of the first line; the detection of displacements with time comprises the detection of a displacement profile for each of the locations; displacement detection comprises determining a quantity of shift of tissue relative to a reference; the determination comprises identifying displacement peaks in the displacements with time for each of the locations and determining a difference in time between the displacement peaks; the determination comprises the correlation of the displacements with time of a first one of the locations with the displacements with the time of a second one of the locations; - calculation of the speed of sound includes the calculation of the speed of sound in the patient between locations; and further comprising repeating the detection, determination and calculation for other sets of locations responsive to the shear wave; image generation comprising generating an image of a spatial distribution of sound velocities for the patient for sets of locations; estimating a shear wave velocity in the patient, the calculation of the velocity of the sound comprising calculating from the change in time and the shear wave velocity; - calculation of sound velocity includes calculation from time change, angle, shear wave velocity, default velocity, and distance between given locations with the default speed; - calculation of the speed of sound includes the calculation from a first report of an ultrasound system speed used on the speed of sound and a second report of a distance based on the ultrasound system between the locations and a distance based on the shear wave; the shear wave moves at an angle greater than 20 degrees and less than 70 degrees with respect to a line through the locations, and the calculation includes calculating as a function of the angle; the generation of the image comprises the generation of an image showing a value of the speed of sound; the use of the speed of sound in an ultrasonic scanner beamformer for imaging the patient; the transmission comprises transmitting the acoustic radiation force pulse as such a pulse in a multiple pulse pattern with the detection being performed in response to the pattern, and wherein the determining comprises determining the change over time in from multiple peaks in the moves for each location.
In a second aspect, a system is proposed for imaging the speed of sound. A transmission beamformer is configured to generate an excitation pulse. A receive beamformer is configured to detect tissue responses to a shear wave generated by the excitation pulse. Responses are detected at each of a plurality of locations at each of a plurality of moments. An image processor is configured to estimate the speed of sound in the tissue from the tissue responses to the shear wave. A display can be used to display the speed of sound.
According to the variants, the system may include one or more of the following features: - the image processor is configured to estimate the speed of sound as a function of a measured shear rate in the fabric and a time difference the shear wave passing through the locations; the image processor is configured to estimate the speed of sound at the locations, and wherein the display is configured to display the sound velocities at the plurality of locations as an image; the transmission beamformer, the receiver beamformer, or both of the transmission beamformer and the receiver beamformer are configured to scan with delay profiles based on the estimated speed of sound.
In a third aspect, a computer-readable non-transitory storage medium has, stored therein, data representing instructions executable by a processor programmed to estimate a speed of sound. The storage medium includes instructions for: observing a shear wave propagating in a medium with an ultrasonic scanner, calculating a speed of sound in the medium as a function of (a) shear rate or stiffness, and (b) a time difference so that the shear wave propagates to different locations in the medium, and transmit the speed of sound. Other aspects and advantages of the invention are discussed below in conjunction with the preferred embodiments.
BRIEF DESCRIPTION OF THE DRAWINGS
The components and figures are not necessarily to scale, the emphasis being rather on the illustration of the principles of the invention. In addition, in the figures, like reference numerals denote corresponding parts in the different views.
Figure 1 is a flow chart of an embodiment of a method for imaging a speed of sound; Figure 2 illustrates an example of a shear wave propagation arrangement to displacement detection locations; Figure 3 shows two displacement profiles used to determine a change in time between occurrences of a shear wave; Figures 4A and 4B show examples of B-mode imaging with assumed sound velocity and correct sound velocity, respectively; Figure 5 illustrates an example of radio frequency signals output by a beamformer with the assumed and correct velocities of the sound; Figure 6 is an embodiment of a system for estimating a speed of sound in a fabric.
DETAILED DESCRIPTION OF DRAWINGS AND EMBODIMENTS TODAY PREFERRED
The speed of sound is estimated and imaged using a shear wave. Using an acoustic radiation force pulse, the shear wave is generated. Tissue shifts caused by the shear wave are obtained for multiple locations with an ultrasound scanner and analyzed to estimate the speed of sound. In one embodiment, the speed of sound is estimated by observing a shear wave propagating in a medium. A known or pre-estimated rigidity or shear rate is used with the shear wave propagation information to estimate the velocity of sound.
Since the shear wave displacement rate at different locations is determined, pulse-echo ultrasound can be used to estimate the speed of sound. The speed of sound may be diagnostically useful, such as correlating with a disease state more strongly than other measures (eg correlating more strongly than shear rate or tissue stiffness).
Figure 1 shows an embodiment of a method for sound velocity imagery. An ultrasound scanner observes a shear wave propagation in a medium. The speed of sound in this medium is calculated as a function of the shear rate or stiffness of tissue and a time difference for the shear wave to propagate to different locations in the medium. The locations sampled by an ultrasound scanner use a predicted or previously defined sound velocity, so are at an assumed separation distance. Following the shear wave, the actual distance between two locations is found on the basis of a time difference of occurrence of the shear wave at the locations. The ratio of this actual distance over the assumed distance is the same as the ratio of the actual speed to the assumed speed, so that the actual speed can be calculated.
The method is implemented by the system of Figure 6 or a different system. For example, any ultrasound scanner known today or developed later implements actions of all actions. A processor, controller or image processor of the ultrasonic scanner implements actions 28-32. Alternatively, a processor of a separate computer or workstation or remote from the ultrasonic scanner implements any or all of the actions 28-32. Beam formers, memory, detectors and / or other devices may be used to acquire the data, using actions 24 and 26. The ultrasonic scanner, image processor, display or other device may Action 34. The image processor may control the devices to implement the method of Figure 1.
Additional, different or fewer actions may be planned. For example, the method is implemented without transmitting the velocity to the action 34. As another example, the shear wave is generated without an ARFI transmission of the action 24. In yet another example, a velocity of default or assumed shear or other fabric feature (e.g. rigidity) is used instead of calculating action velocity 30. In other examples, filtering or other data processing is applied to shifts or velocities calculated in time and / or space.
The actions are implemented in the order described or shown (for example from top to bottom), but can be implemented in other orders. For example, action 24 shows the transmission of a single excitation pulse. Action 24 and response actions 26, 28 and 32 may be repeated to measure over a larger region of interest. Actions 26, 28 and 32 may be repeated to measure on a larger region of interest or with more samples in response to the same shear wave. As another example, the action 30 is implemented prior to action 24, such as using ARFI imaging to determine the shear rate in the tissue of interest before using an ARFI to determine the speed of sound in this tissue of interest. At action 24, an ultrasound scanner transmits an ARFI thrust into a patient's tissue. The transmission is a transmission beam focused at a depth or range of depths on a scan line. The focal depth is on the transmission scan line.
Based on a delay profile for the transducer elements, the ARFI transmission beam is transmitted along a transmission scan line. The scan line is at any angle to the transducer, as normal to the transducer. An ARFI pulse is used to generate a shear wave that propagates at an angle Θ relative to the A-lines or detection scan lines to the action 26. In one embodiment, the scan line for the transmission beam ARFI is at any angle within the field of view of the transducer, such as being within ± 30 degrees of normal to the transducer. Figure 2 shows an example with the ARFI transmission scan line 40 at an angle Θ of about 20 degrees from normal. The point of origin on the transducer is the center of the transducer, but may be offset from the center.
An array of elements in an ultrasonic transducer transmits the converted ARFI beam from electric waveforms. The acoustic energy is transmitted to the tissue in a patient. The acoustic waveform is transmitted as a constraint to generate a shear wave to move the tissue. Excitation is an ultrasonic excitation pulse. The acoustic energy is focused to apply sufficient energy to cause the generation of one or more wave (s) which then travels (s) through the tissue from the focal location. The acoustic waveform can itself move the fabric. Other sources of stress may be used, such as an external mechanical force or an internal force.
To generate the wave, high amplitude or power excitations are desired. For example, the excitation has a mechanical index close to but not greater than 1.9 at any of the focal locations and / or in the field of view. To be careful and consider a probe variation, a mechanical index of 1.7 or other level can be used as the upper limit. Higher powers (for example, an IM greater than 1.9) or lower powers can be used. The excitation pulse is transmitted with waveforms having any number of cycles. In one embodiment, one, most, or all of the waveforms for a push pulse transmission event have 100-2000 cycles. The number of cycles is tens, hundreds, thousands, or more for the continuous transmission waveforms applied to the elements of the array for the excitation pulse. Unlike the imaging pulses that are 1-5 cycle (s), the ARFI excitation or thrust pulse has a greater number of cycles to generate sufficient stress to cause the shear wave to move a tissue with sufficient amplitude to be detected. The shear wave is generated at the focal region and propagates laterally from the focal region. The shear wave moves perpendicular to the transmission scan line. In the example of FIG. 2, the shear wave moves at an angle greater than 0 degrees (for example greater than 20) and less than 90 degrees (for example less than 70) with respect to line A or scan lines used to track the shear wave. In the specific example of Figure 2, the angle is about 20 degrees. Tracking locations A, B at action 26 are along a scan line normal to the array. The waves can move in multiple directions. The waves decrease in amplitude as the waves move through the tissue.
In one embodiment, a single excitation pulse is generated. In other embodiments, an excitation pulse pattern may be generated. Any predetermined pattern may be used, such as overlapping pulses in time, but with a frequency, focus, or other different characteristic. An example of a pattern is a sequence of excitations with a short pause between the pulses. The short pause may be less than a duration for a reverberation reduction and / or less than a length of an excitation pulse. The pattern gives different excitations before tracking to action 26. Due to the pattern, a series of shear waves are generated. This results in a corresponding wave pattern and displacements at different locations. This pattern can be used to give additional peaks or other information to estimate a speed. In action 26, the ultrasound scanner measures or detects tissue movements generated in response to the ARFI transmission. The response of the tissue to the shear wave caused by the excitation is detected and used to measure the displacement. The shear wave is generated in response to the ARFI transmission. The response of the tissue is a function of the wave created by the ARFI beam and features of the tissue. The wave is tracked in multiple locations. Figure 2 shows the wave as lines parallel to the transmission scan line 40. For a shear wave, the wave travels perpendicular to the transmission scan line 40, so that the parallel lines are spaced perpendicular to the transmission scan line 40. The tracking locations A, B are along a reception scan line that is not parallel to the transmission scan line. The generated wave is followed. Tracking detects the effects of the wave rather than specifically identifying where the wave is located at a given time. Follow-up is done by ultrasound scanning. To detect the displacement, ultrasonic energy is transmitted to the tissue undergoing movement, and acoustic energy reflections are received. To detect a tissue response to shear waves in a region of interest, transmissions are made to the region, and detection is made in the region. These other transmissions are intended to detect waves or displacement rather than cause wave or displacement. The transmissions for detection may have a lower power and / or short pulses (for example 1-5 carrier cycles).
A B-mode or other scan along one or more receive lines is performed for tracking. Displacement indicates the effects of the wave, such as no displacement indicating absence of the wave and displacement indicating tissue movement caused by the wave. As the wave passes over a given location, the tissue moves in an amount or distance that increases to a peak amount and then decreases as the tissue returns to rest. Similarly, for a given moment, a location may be moved more than other locations since the peak of the wave is located at or near that location. Tracking can detect the effects of the wave at any stage (ie, no wave, increasing displacement, maximum or decreasing displacement).
The tissue is scanned a multiple number of times to determine the displacement, such as scanning a region at least twice. To determine a shift at a time, a sample echo return is compared to a reference. Displacement is given as the difference or offset between the reference scan (first scan) and a later scan (move measurement). The tissue is scanned using any scanning-capable imaging modality for movement during tissue response, such as during or after application of the ARFI excitation pulse.
For ultrasonic scanning, the wave is detected at locations adjacent to and / or spaced from the focal region for the ARFI excitation pulse. Any number of side locations may be used, such as two or more. The locations are along one or more receive scan lines. Non-parallel and / or non-vertical reception lines may be used. The sensing transmissions may have a wider beam profile along at least one dimension, such as laterally, to simultaneously form receive samples along a plurality of scan lines (eg, receive beamforming simultaneously along four or more receiving lines). Any number of simultaneous receive beams may be formed, such as four, eight, sixteen, thirty-two, sixty-four, or more. In one embodiment, a parallel receive beamformer forms beams for sampling the entire region of interest. Parallel beam formation is used to scan the entire region of interest.
Some or all of the sample locations are at different depths. As shown in Figure 2, sample locations A, B are positioned such that the shear wave occurs at different times at different locations. Sample locations at the same depth but on different reception lines or other location distributions resulting in the shear wave passing at different times given the origin of the shear wave can be used.
The tracking transmissions and the corresponding receiving beams are sequentially performed. To sample in time, the tracking transmission and the reception of echoes from the multiple locations simultaneously are repeated. Transmission and reception for detection or tracking are performed a multiple number of times for each receive line to determine a change due to time displacement. Any transmission and reception sequence may be used.
To determine a displacement, a reference scan of all the reception lines in the region of interest is carried out before the ARFI transmission of the action 24. After the ARFI transmission of the action 24, the monitoring makes it possible to measure travel by reception event. Samples or measured tissue responses are used to determine action displacement.
The displacement is calculated from the ultrasound scan data. The fabric moves between two scans. A reference scan is performed prior to the ARFI transmission of action 24 and / or after the generated wave has passed the location. The sample sweep or reference sweep data is translated or shifted in one, two, or three dimension (s) to the data in the other sweep. For each possible relative position, a similarity amount is calculated for the data around the location. The amount of similarity is determined with a correlation, such as cross-correlation. A minimum sum of absolute differences or other function can be used. The spatial offset with the highest or sufficient correlation indicates the amount of displacement for a given location. In other embodiments, a phase shift of received data for different times is calculated. The phase shift indicates the amount of displacement. In still other embodiments, data representing a line (eg axial) at different times is correlated to determine an offset for each of a plurality of depths along the line.
A single ARFI excitation pulse is used to estimate displacements for all locations. By repeating the displacement detection using samples from the repeated tracking, the displacements for all locations are determined for each of the multiple moments (eg sampling every 0.1 ms over 0-7 ms). To monitor a larger region, excitation pulses and tracking may be repeated for other locations.
Since the maximum displacement moment for a given location is unknown, the sampled displacements may or may not be associated with a maximum displacement caused by the wave passing on the tissue. Figure 3 shows a graph of the displacements for each of the two locations A, B as a function of time. Displacement samples as a function of time for a given location are a displacement profile for that location. The profile generally starts with no shear displacement, rises to a peak of displacement representing an occurrence of the shear wave, and then falls back to the steady state of no shifting.
The same shear wave causes a peak of motion to occur at different times for different locations. The temporal difference between locations is a function of the distance between locations, the speed of the shear wave and an angle.
Figure 3 shows a peak for each location. When an excitation pulse pattern is used, multiple waves may be generated. Depending on whether the multiple excitation pulses have a focus location, a transmission scan line angle and / or an identical or different relative time (s) and depending on the sampled moment, more than one peak may occur in displacement as a function of time. Displacements caused by the wave pattern are detected after the excitation pulse pattern has occurred (eg after multiple shear waves have been generated). In action 28, an image processor determines a change in the time of travel over time between any number of locations. The change in time for a location relative to another location is a time difference between shear wave occurrences at locations. Figure 3 shows the change in time as ΔΤ. Coupled with shear rate and angle, this difference in time is used to determine a true distance between the two sample locations A, B.
In one embodiment, the change in time is found from the displacement profiles. The peak is treated as the shear wave. The peak moment indicates the moment of occurrence of the shear wave at the location. Other parts of the profile can be used instead of the peak. The peak is identified as the maximum displacement with time, the measured displacements are compared to find the maximum. As an alternative, a curve is adjusted on the measured displacements, and the maximum of the adjusted curve is used. The displacement peak is identified for each of the displacement profiles (ie for each of the locations).
The difference in time is determined from the displacement peaks. Each peak at a corresponding moment. In the example of Figure 3, the peak for slot A occurs at 5.8 msec and the peak for slot B occurs at 9.6 msec. The difference in time is calculated from the moments of occurrence of the peaks. In Figure 3, ΔΤ is 3.8 ms.
In another embodiment, the displacement profiles for the different locations are correlated. Different time offsets of the profile of a location relative to the profile of the other locations are attempted. The amount of correlation is calculated for each offset. The time shift with the greatest correlation gives the difference in time. Other approaches can be used.
With two locations, the difference in time is between the two peaks. When a pattern of peaks is provided, such as due to the transmission of the ARFI pulse with a definite wavefront shape (ie a pattern), the difference in time has a larger sampling. The differences between respective peaks of multiple peaks in each profile are determined. An average change in time is then found.
When more than two locations are sampled, the difference in time can be found between different combinations of locations. This increases the sampling for a tissue region. At action 30, the shear wave velocity or stiffness of the tissue is obtained. The value is obtained from a memory or calculated from measurements. The speed or rigidity in combination with a change in time and an angle can be used to derive the actual distance between locations A, B. The speed or rigidity is known a priori, obtained after the action 26 (for example obtained in response to a different ARFI transmission), or obtained from the displacements also used to calculate the speed of sound.
Speed or stiffness can be assumed. A default value (for example a population average for the tissue of interest) is used. As an alternative, displacement measurements in the specific patient are used.
In one embodiment, the image processor determines the shear wave velocity by a distance from the shear wave origin at the sample location and a moment of occurrence of the shear wave at the sample location. location. The displacement profile for a location spaced laterally from the ARFI focus is used. Different locations along a line perpendicular to the transmission scan line extending from the ARFI focus may be used.
Different approaches for estimating a shear rate can be used. The speed is calculated from the peak or peaks. When an excitation pattern and resulting waves are used, then more than one peak may be localized for some or all of the moments. This pattern resulting from peaks can be used to estimate the speed of the shear wave.
In one embodiment, the calculation is simply the sample time for the peak and the distance of the peak location from the focal position of ARF1. This calculation can be repeated for other times, giving speeds at different peak locations. As an alternative, the peak moments for different locations are used to estimate a speed for the region of tissue or region of interest. As an alternative, the speed is calculated using phasing. Travel profiles as a function of time for different locations are correlated. The phase shift and the time difference of sampling can be used to determine the speed.
In another embodiment, the adjustment is directly on a two-dimensional map of displacements without peak identification. The adjustment can be weighted by the magnitudes of the displacements. The displacement quantities can be adjusted to take into account a wave attenuation as a function of a distance before the weighted displacement adjustment. Once adjusted, the line gives a slope or angle used to calculate the speed. By using parallel beam formation over the entire region of interest, the resulting adjustment may be less sensitive to errors caused by physiological movement.
When a wave pattern is generated, the adjustment may be different. For each moment, multiple peaks are provided. The peaks can be distinguished from each other so that the different waves are separated. The wave generation pattern (e.g., focal location and / or rhythm) is used to distinguish. Speeds for each wave are calculated separately. The resulting speeds can be combined. Alternatively, patterns of patterns are matched or adjusted on the pattern of peak locations. The best fit pattern is associated with a predetermined speed. Other approaches may be used, such as using a separation of peak locations at a given time to indicate speed.
In one embodiment, the fabric stiffness is used instead of or in addition to the shear wave velocity. Any calculation of rigidity can be used. For example, the stiffness is calculated from the shear wave velocity assuming an elastic and isotropic medium. The stiffness or modulus of Young, E, is calculated as:
where p is the density and Vs is the shear rate.
The calculation of the shear wave velocity or tissue stiffness may utilize the shifts measured at action 26. The distance from the origin of the shear wave to the sample location may not be exact, but the shear wave velocity or the resulting rigidity can be sufficiently accurate. The sound velocity assumption may result in inaccuracy of the beamformer-based distance between the ARFI focus and the sample location (eg, location B). As an alternative, displacements measured in response to a different shear wave are used. Displacements can be measured for locations other than the locations used to calculate the speed of sound. At action 32, the image processor calculates the speed of sound. The speed of sound in the specific patient, the specific tissue, and / or a specific tissue location is calculated. The speed of sound between sample locations A, B is calculated.
The speed of sound is calculated from the change in the time since action 28 and the shear rate or the stiffness of the fabric of action 30. Since the shear wave velocity is known and the difference in time of occurrence of the shear wave at different locations is measured, the actual distance between locations can be determined. The ratio of the actual distance over the expected distance or based on the beamformer indicates a weight for the expected sound speed used by the beamformer to provide the actual speed of the sound.
With reference to Figure 2, the speed of sound is a function of the geometry relative to shear wave displacement to locations. The speed of sound, c, is calculated from the change in time ΔΤ, the angle Θ, the shear wave velocity Vs, or the stiffness, the default speed of the sound c 'used by the beamformer, and the default distance between sample locations, given the default speed (ie the expected distance as a function of beamforming or sweep geometry). The actual distance, d, which is the component of the shear wave displacement distance in the direction of the acquired line A (ie along the receiving scan line passing through A and B), is given by :
(1)
The default distance from is based on the ultrasonic scanner beamformer. The default speed is used by the beamformer to assign sample locations. The default distance between points A and B is given by:
(2) where dt is the change in time or ΔΤ and β is a ratio of c 'and c.
(3)
The ratio of the ultrasonic scanner or the default speed c 'to the actual speed c is equal to the ratio of the ultrasonic scanner or the default distance of the actual distance d. the true or real speed is given by:
(4)
Since the distance d is determined from the results of the actions 28 and 30 and the angle of the shear wave propagation with respect to a line passing through the two sample locations is known from the scanning geometry, the actual speed is determined.
When more than two sample locations are used, the detection of the action 26, the determination of the action 28, and the calculation of the action 32 may be repeated. The same shear wave and the same shear wave velocity are used in the repeats. Alternatively, the displacements for all locations are measured using parallel beam formation or beam formation on a single line so that action 26 is not repeated. In other alternatives, the shear rate is different for different pairs of locations, so that the action 30 is also repeated.
By repeating the calculation of the speed of sound for different sets of locations, the increased sampling can be used so that an average speed is more accurate. In another embodiment, the repetition provides values for the speed of sound to each of different locations or regions. A single, two or three dimensional map of sound velocity measurements is provided. The speed of sound is different for a different fabric and / or fabric with different characteristics. At action 34, the image processor transmits the calculated speed or speeds. Transmission is to another component of the ultrasound system or out of the ultrasound system. For example, the speed is transmitted to a memory, a beamformer, a display and / or a network.
An image of the speed of sound can be generated and transferred to the display. The image includes speed as a text, such as an alphanumeric representation. In one embodiment, a single sound velocity is determined. A user positions a pointer on an image. In response, the ultrasound scanner outputs a speed of sound calculated for that point. Graphic, color coding, intensity, or other speed modulation can be used. Alternatively, the image includes a spatial distribution of sound velocities for different locations. A uni, bi or three-dimensional representation of the speed as a function of the location is rendered on the display. The display grid may be different from the scanning grid and / or a grid for which displacements are calculated. A color, brightness, luminance, tone, or other pixel characteristics is modulated as a function of the speed of sound. A variation of speed by region can be visualized.
In another example, the speed is transmitted to a beamformer. The speed is transmitted to the beamformer controller, receiver beamformer and / or transmission beamformer. Alternatively, the speed is used to determine a delay or phase profile, and the profile is transmitted to the beamformer. By using the actual sound speed or sound velocities, the focus and scan format of the beamformer is controlled to increase resolution or for more accurate scanning.
Figures 4A and 4B show examples using the assumed and actual velocity of sound in ultrasound scanner beamforming to image a phantom with various spot or in-line reflectors (light spots). B-mode images are generated, but other types of imaging can be used. In Figure 4A, the speed of sound is assumed to be 1450 m / s. In Figure 4B, the actual sound speed of 1540 m / s is used. Point or line reflectors are more defined or less blurred in Figure 4B. Using the actual sound velocity can improve a sonographer's ability to distinguish anatomy and / or tissue condition, which aids diagnosis. The actual speed of sound also results in a more reliable distance indication. Note that the depth range from the transducer (0 cm) to the farthest depth in Figure 4A is less than that in Figure 4B due to a compression of the distance by the inaccurate speed of sound.
Figure 5 is a graphical representation of beam samples or radio frequency data from about 2.5 cm along the x-axis of both Figures 4A and 4B. The radio frequency data represents an echo response from three reflectors along this vertical line in Figures 4A and 4B. As a result, Figure 5 shows three instances of increased signal intensity for each of the two radio frequency signals. Due to the use of an assumed sound velocity, the three instances of increased intensity for Figure 4A occur closer to the transducer and with less distance between instances. Using the correct speed of sound changes the distance, giving a true distance between points.
Figure 6 shows an embodiment of a system for imaging a speed of sound. By combining scanning data in response to tissue responsive to shear wave displacement, the speed of sound is determined.
The system is an ultrasound imaging system for medical diagnosis. In other embodiments, the system is a personal computer, a workstation, a PACS station, or other arrangement in a single location or distributed over a network for real-time or post-acquisition imaging.
The system implements the method of Figure 1 or other methods. The system includes a transmission beamformer 12, a transducer 14, a receiver beamformer 16, an image processor 18, a display 20, and a memory 22. Additional, different, or fewer components may be provided. . For example, a user input is provided for manual or assisted designation of a region of interest for which information is to be obtained.
Transmission beamformer 12 is an ultrasonic transmitter, memory, blower, analog circuit, digital circuit, or combinations thereof. The transmission beamformer 12 is configured to generate waveforms for a plurality of channels with different or relative amplitudes, delays, and / or phasing. Waveforms are generated and applied to transducer elements 14 at any rate or frequency of pulse repetition. For example, the transmission beamformer 12 generates an excitation pulse to generate a shear wave in a region of interest and generates corresponding transmissions for tracking resulting displacements with ultrasound. The transmission beamformer 12 may be configured to generate a sequence or other combination of excitation pulses to generate multiple waves to be tracked.
The transmission beamformer 12 connects with the transducer 14, such as through a transmit / receive switch. When transmitting acoustic waves from the transducer 14, one or more beams (x) are formed during a given transmission event. The beams are excitation pulses and / or tracking beams. To scan a tissue shift, a transmission beam sequence is generated to scan a region into one, two, or three dimension (s). Vector, vector®, linear or other sector scan formats can be used. The scanning by the transmission beamformer 12 is done after transmission of the excitation pulse (ie ARFI thrust pulse), but may include a scan for reference frames used in the tracking before transmission of the pulse excitation. The same elements of the transducer 14 are used for both scanning and tissue displacement, but different elements, transducers, and / or beamformers can be used.
The transducer 14 is a 1, 1.25, 1.5, 1.75 or 2 dimension array of piezoelectric or capacitive membrane elements. The transducer 14 includes a plurality of elements for transduction between acoustic and electrical energies. For example, the transducer 14 is a one-dimensional PZT matrix with about 64-256 elements.
The transducer 14 connects with the transmission beamformer 12 to convert electrical waveforms into acoustic waveforms, and connects with the receiver beamformer 16 to convert acoustic echoes to electrical signals. The transducer 14 transmits the excitation pulse and tracking beams. The waveforms are focused at a tissue region or location of interest in the patient. The transmission beams describe an angle to the transducer at any of various angles within a field of view of the transducer 14. The acoustic waveforms are generated in response to the application of the waveforms to the transducer elements. To scan with ultrasound to detect a displacement, the transducer 14 transmits acoustic energy and receives echoes. Receiving signals are generated in response to ultrasound energy (echoes) impinging on the transducer elements 14.
The receiver beamformer 16 includes a plurality of channels with amplifiers, delays, and / or phase rotators, and one or more summers. Each channel connects with one or more transducer elements. The receive beamformer 16 applies relative delays, phases, and / or apodization to form one or more receive beams (x) in response to each transmission for the detection of the tissue response or tracking. A dynamic focus on reception can be provided. When only one depth or depth range is of interest, dynamic focus may or may not be provided. The receiver beamformer 16 outputs data representing spatial locations using the acoustic signals received. Relative delays and / or phasing and summation of signals from different elements results in beam formation. In other embodiments, the receive beamformer 16 is a processor for generating samples using a Fourier transform or the like.
For parallel receive beam formation, the receive beamformer 16 is a parallel receive beamformer configured to include additional sets of channels and corresponding adders. Each channel applies relative delays and / or phasing to form a beam with the adder. The receiver beamformer 16 may have any number N of sets of channels and adders. N is an integer of 1 or more, to form a corresponding number of beams simultaneously or in response to the same tracking transmission beam. Receiving beams can be formed as a regular sampling of space in a region of interest. The locations are sampled simultaneously by respective receiving beams formed by the receiver beamformer 16.
The receiver beamformer 16 may include a filter, such as a filter, for isolating information at a second harmonic or other frequency band with respect to the transmission frequency band. Such information may more likely include a desired tissue, a contrast agent, and / or flow information.
The receiver beamformer 16 outputs beam summed data representing spatial locations. Data for a single location, locations along a line, locations for a zone, or locations for a volume are outputted. The data can have different purposes. For example, different scans are performed for mode B or tissue detection data and for shear wave or longitudinal wave detection. Alternatively, Mode B data is also used to determine displacement caused by a shear or longitudinal wave.
The receive beamformer 16 is configured to detect tissue responses to the wave generated by the excitation pulse. The fabric is swept. The receive signals generated by the receive beamformer 16 represent a response of the tissue at the time of sampling. Different locations are sampled simultaneously.
Since the tissue is subjected to any displacement caused by the wave, the tissue response is captured by sampling. The acoustic responses are detected at each of a plurality of locations at each of a plurality of moments. Tissue responses to more than one wave can be detected. The receive beamformer 16 detects a tissue response to a shear wave at each of a plurality of locations at each of a plurality of moments.
The image processor 18 or a separate beamformer controller configures the beamformers 12,16. By loading values into registers or a table used for an operation, the acquisition parameter values used by the beamformers 12, 16 for ARFI imaging or the like are set. Values include delay or phase profiles that rely on the speed of sound. For a given scan, the transmit beamformer 12 and / or the receive beamformer 16 use (s) a given or default sound velocity. Any structure or command format can be used to set up the imagery. The beamformers 12, 16 are acquired for imaging at frame rate and / or resolution. Different values of one or more acquisition parameter (s) may result in a different frame rate and / or resolution.
The image processor 18 is a mode B detector, a Doppler detector, a pulsed wave Doppler detector, a correlation processor, a Fourier transform processor, a specific integrated circuit, a general processor, a control processor, a user programmable gate array, a digital signal processor, an analog circuit, a digital circuit, combinations thereof, or other device known today or later developed to calculate displacements from outputted responses by the receiver beamformer 16, calculating a shear rate, calculating differences in time and / or calculating a speed of sound.
In one embodiment, the image processor 18 includes one or more detector (s) and a separate processor. The separate processor is a control processor, a general processor, a digital signal processor, a graphics processing unit, a specific integrated circuit, a field programmable gate array, a network, a server, a group of processors, a data path, combinations thereof or other device known today or later developed to determine a displacement and / or calculate a speed of sound from displacements. The processor 18 is configured by software and / or hardware to implement the actions.
In one embodiment for sound velocity imaging, the processor 18 estimates tissue displacement for each of a plurality of side locations over time. Movements occurring at different times are estimated for each location. For example, displacement estimates for the various locations are formed for each of the multiple sampling moments. Data output from the receive beamformer 16 is used to determine the movements at each location for each of the different times. Displacements can be obtained by correlating or otherwise determining a level of similarity between reference data and data obtained to represent the tissue at a time.
The image processor 18 may be configured to estimate the shear wave velocity or other tissue characteristic from the displacements used to calculate a velocity of sound or displacements measured in response to a different shear wave. One or more peak (s) in a displacement profile as a function of time is / are found. Based on the distance from the excitation pulse focus to the sample location and the moment of occurrence of the shear wave at the sample location, the image processor 18 calculates the wave speed shearing. In another example, processor 18 calculates fabric stiffness, viscosity, and / or a modulus. The processor 18 can calculate other properties, such as stress or elasticity. In other embodiments, an assumed or default value of the shear wave velocity is used in place of a measured value.
The image processor 18 is configured to estimate the speed of sound in the tissue from the tissue responses to the shear wave. The speed of sound is estimated from the movements. The time displacements for each location are compared to find a difference in the timing of the shear wave at the locations. When the transmission line for the shear wave is not parallel to a line passing through the sample locations, the shear wave arrives at or passes through each of the locations at a different time. The angle for the transmission scan line for the ARFI relative to the line passing through the sample locations, the difference in time, and the shear wave velocity are used to calculate the actual distance between the sample locations . Beamformer-based sound velocity and distance between locations are used along with the actual distance to calculate the speed of sound. The ratio of the actual distance to the beamformer distance is equal to the ratio of the actual sound velocity to the beamformer sound velocity, allowing the image processor 18 to calculate the velocity of the sound.
The speed of sound is estimated for a location, such as a location designated by a user. As an alternative, the speed of sound is estimated for each of a plurality of locations. The image processor 18 determines a spatial distribution of sound velocities in the patient.
The processor 18 generates and outputs an image or display values represented from the speed of sound on the display 20. A text or digital indication of the speed of sound is displayed to the user . In one embodiment, the speed of sound is displayed as a function of a location. Values, graphs and / or tissue representations can be displayed using the speed at different locations. For a representation of the fabric, the sound speed modulates the color, tone, brightness and / or other display characteristic for different pixels representing a tissue region. The image processor 18 determines a pixel value (for example, RGB) or a scalar value converted into a pixel value. The image is generated as scalar or pixel values. The image may be outputted to a video processor, a lookup table, a color table, or directly to the display 20. The display 20 is a CRT display, an LCD display, a plasma display , a projector, a printer or other device for displaying an image or a sequence of images. Any display known today or developed later may be used. The display 20 can be used to display an image or a sequence of images. The display 20 displays two-dimensional images or three-dimensional representations. The display 20 displays one or more images representing the speed of sound derived from shear wave displacement. A table, a patient report or a tissue representation is displayed with the included speed. As another example, a speed of sound associated with a location indicated on a two-dimensional image or a three-dimensional representation in B mode is displayed. As an alternative or in addition, the image is a graphic. In still other embodiments, a B-mode image with a color modulation overlay for the speed of sound is displayed.
The image processor 18 may transmit the speed of sound to the transmission beamformer 12, the receiver beamformer 16 or both. The transmission to the beamformers 12/14 may be to a beamformer controller. The speed value of the sound itself or the speed of sound as incorporated into delay / phase profiles based on the speed of sound are transmitted, the beam formers 12, 14 are configured to scan using delay and / or phase profiles based on the speed of sound. Using the measured or actual sound velocity for the patient tissue to configure the beamformers 12, 14 may result in a more accurate spatial representation. The estimated speed of sound is used to operate the beamformers 12, 14 in any subsequent scan of any type (eg B-mode imaging). The speed is estimated once for a given imaging session. In other embodiments, the rate is periodically estimated over an entire imaging session for a patient.
The processor 18, the receive beamformer 16 and the transmission beamformer 12 operate in accordance with instructions stored in the memory 22 or other memory. The instructions configure the system for carrying out the actions of Fig. 1. The instructions configure the image processor 18, the receive beamformer 16 and / or the transmission beamformer 12 for operation while being loaded. in a controller, causing the loading of a table of values and / or being executed. The transmission beamformer 12 is configured by the instructions to cause the generation of an excitation beam, tracking beams, and / or other imaging beams. The receive beamformer 16 is configured by the instructions to acquire data for tracking and / or imaging. The image processor 18 is configured to estimate displacements and velocities of the sound from the displacements.
The memory 22 is a non-transitory storage medium readable by computer. The instructions for implementing the processes, methods, and / or techniques discussed herein are provided on the computer-readable storage medium or memories, such as a cache, a buffer, a RAM, a removable medium, a disk hard or other computer readable storage medium. Computer readable storage media include various types of volatile and nonvolatile storage media. The functions, actions, or tasks illustrated in the figures or described herein are performed in response to one or more instruction sets stored in or on a computer readable storage medium. Functions, actions, or tasks are independent of the particular type of instruction set, storage medium, processor, or processing strategy, and can be implemented by software, hardware, integrated circuits, firmware, a microcode and the like, operating alone or in combination. Similarly, treatment strategies may include multiprocessing, multitasking or parallel processing, and the like.
In one embodiment, the instructions are stored on a removable media device for playback by local or remote systems. In other embodiments, the instructions are stored at a remote location for transfer over a computer network or over telephone lines. In still other embodiments, the instructions are stored in a given computer, CPU, graphics unit, or system.
If the invention has been described above with reference to various embodiments, it should be understood that many changes and modifications can be made without departing from the scope of the invention. It is therefore intended that the foregoing detailed description be considered illustrative rather than limiting.

权利要求:
Claims (20)
[1" id="c-fr-0001]
claims
A method of sound velocity imaging, the method comprising: transmitting, with an ultrasonic scanner, an acoustic radiation force pulse into tissue of a patient along a first line; detecting, with the ultrasonic scanner, tissue time displacements generated in response to a shear wave resulting from the acoustic radiation force pulse, the displacements being detected at each of at least two locations spaced from the First line ; determining a change in the time of displacements over time for a first of the locations relative to the displacements over time of a second one of the locations; calculating a speed of sound in the patient from the change in time; and generating an image of the speed of sound.
[2" id="c-fr-0002]
The method of claim 1 wherein the transmission comprises transmitting the acoustic radiation force pulse as focused at a depth along the first line, and wherein the sensing comprises sensing with at least one of the locations being at a different depth and with the locations being along a second line different from the first line.
[3" id="c-fr-0003]
The method of claim 1 wherein the transmission comprises the transmission with the first line being at an angle away from the normal to a transducer, and wherein the detection comprises detecting with locations along a second line at a different angle from the transducer than the one in the first line.
[4" id="c-fr-0004]
The method of claim 1 wherein detecting displacements with time comprises detecting a motion profile for each of the locations.
[5" id="c-fr-0005]
The method of claim 1 wherein the motion detection comprises determining a tissue offset amount with respect to a reference.
[6" id="c-fr-0006]
The method of claim 1 wherein the determining comprises identifying displacement peaks in displacements over time for each of the locations and determining a difference in time between the displacement peaks.
[7" id="c-fr-0007]
The method of claim 1 wherein the determining comprises correlating displacements with time of a first of the locations with time displacements of a second one of the locations.
[8" id="c-fr-0008]
The method of claim 1 wherein calculating the speed of sound comprises calculating the velocity of sound in the patient between locations; and further comprising repeating the detection, determination and calculation for other sets of locations responsive to the shear wave; wherein the image generation comprises generating an image of a spatial distribution of sound velocities for the patient for the sets of locations.
[9" id="c-fr-0009]
The method of claim 1 further comprising estimating a shear wave velocity in the patient; wherein calculating the speed of sound comprises calculating from the change in time and shear wave velocity.
[10" id="c-fr-0010]
The method of claim 1 wherein calculating the speed of sound comprises calculating from time change, angle, shear wave speed, default speed, and a distance between the given locations with the default speed.
[11" id="c-fr-0011]
The method of claim 1 wherein calculating the speed of sound comprises calculating from a first report an ultrasonic system speed used on the speed of sound and a second ratio of a distance. based on the ultrasound system between locations and a distance based on the shear wave.
[12" id="c-fr-0012]
The method of claim 1 wherein the shear wave travels at an angle greater than 20 degrees and less than 70 degrees from a line across the locations, and the calculation includes computing as a function of the angle.
[13" id="c-fr-0013]
The method of claim 1 wherein the generation of the image comprises generating an image showing a value of the speed of sound.
[14" id="c-fr-0014]
The method of claim 1 further comprising using the speed of sound in an ultrasonic scanner beamformer to image the patient.
[15" id="c-fr-0015]
The method of claim 1 wherein the transmission comprises transmitting the acoustic radiation force pulse as such a pulse in a multiple pulse pattern with the detection being performed in response to the pattern, and wherein the determining comprises Determining the change over time from multiple peaks in the moves for each location.
[16" id="c-fr-0016]
A system for imaging a speed of sound, the system comprising: a transmission beamformer configured to generate an excitation pulse; a receive beam former configured to detect tissue responses to a shear wave generated by the excitation pulse, the responses being detected at each of a plurality of locations at each of a plurality of moments; an image processor configured to estimate the speed of sound in the tissue from the tissue responses to the shear wave; and a display that can be used to display the speed of sound.
[17" id="c-fr-0017]
The system of claim 16 wherein the image processor is configured to estimate the speed of sound as a function of a measured shear rate in the tissue and a time difference of the shear wave passing through. by the locations.
[18" id="c-fr-0018]
The system of claim 16 wherein the image processor is configured to estimate the speed of sound at the locations, and wherein the display is configured to display the sound velocities at the plurality of locations as an image.
[19" id="c-fr-0019]
The system of claim 16 wherein the transmission beamformer, the receive beamformer or both of the transmission beamformer and the receiver beamformer are configured to scan with delay profiles based on the transmission beamformer and the receiver beamformer. estimated speed of sound.
[20" id="c-fr-0020]
20. A computer-readable non-transitory storage medium having stored therein data representing executable instructions by a processor programmed to estimate a speed of sound, the storage medium including instructions for: observing a shear wave propagating in a medium with an ultrasound scanner; calculate a sound velocity in the medium as a function of (a) a shear rate or rigidity and (b) a time difference for the shear wave to propagate to different positions in the medium; and transmit the speed of sound.

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同族专利:

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法律状态:
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2020-02-11| PLFP| Fee payment|Year of fee payment: 4 |

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2021-02-15| PLFP| Fee payment|Year of fee payment: 5 |

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2021-02-19| PLSC| Publication of the preliminary search report|Effective date: 20210219 |

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2022-02-23| PLFP| Fee payment|Year of fee payment: 6 |

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