CN106529126A - Processing method for inheriting monitoring image information after continuous monitoring interruption in brain dynamic electrical impedance imaging - Google Patents
Processing method for inheriting monitoring image information after continuous monitoring interruption in brain dynamic electrical impedance imaging Download PDFInfo
- Publication number
- CN106529126A CN106529126A CN201610916112.0A CN201610916112A CN106529126A CN 106529126 A CN106529126 A CN 106529126A CN 201610916112 A CN201610916112 A CN 201610916112A CN 106529126 A CN106529126 A CN 106529126A
- Authority
- CN
- China
- Prior art keywords
- data
- monitoring
- matrix
- imaging
- interruption
- Prior art date
- Legal status (The legal status 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 status listed.)
- Granted
Links
- 238000012544 monitoring process Methods 0.000 title claims abstract description 87
- 238000003384 imaging method Methods 0.000 title claims abstract description 56
- 238000003672 processing method Methods 0.000 title claims abstract description 12
- 210000004556 brain Anatomy 0.000 title claims description 9
- 239000011159 matrix material Substances 0.000 claims abstract description 42
- 238000005259 measurement Methods 0.000 claims abstract description 40
- 238000000034 method Methods 0.000 claims abstract description 27
- 238000006073 displacement reaction Methods 0.000 claims abstract description 11
- 238000012937 correction Methods 0.000 claims description 15
- 238000004070 electrodeposition Methods 0.000 claims description 14
- 230000003416 augmentation Effects 0.000 claims description 6
- 230000005284 excitation Effects 0.000 claims description 5
- 230000014509 gene expression Effects 0.000 claims description 5
- 238000001514 detection method Methods 0.000 claims description 4
- 230000007423 decrease Effects 0.000 claims description 3
- IAPHXJRHXBQDQJ-ODLOZXJASA-N jacobine Natural products O=C1[C@@]2([C@H](C)O2)C[C@H](C)[C@](O)(C)C(=O)OCC=2[C@H]3N(CC=2)CC[C@H]3O1 IAPHXJRHXBQDQJ-ODLOZXJASA-N 0.000 claims 3
- 230000011218 segmentation Effects 0.000 claims 1
- 230000003190 augmentative effect Effects 0.000 abstract description 11
- 238000012360 testing method Methods 0.000 abstract description 2
- 238000004364 calculation method Methods 0.000 description 6
- 210000003128 head Anatomy 0.000 description 6
- 238000012545 processing Methods 0.000 description 5
- 230000000630 rising effect Effects 0.000 description 4
- 238000002593 electrical impedance tomography Methods 0.000 description 2
- 210000004761 scalp Anatomy 0.000 description 2
- 230000009286 beneficial effect Effects 0.000 description 1
- 238000013480 data collection Methods 0.000 description 1
- 238000003745 diagnosis Methods 0.000 description 1
- 201000010099 disease Diseases 0.000 description 1
- 208000037265 diseases, disorders, signs and symptoms Diseases 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000002847 impedance measurement Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T5/00—Image enhancement or restoration
- G06T5/80—Geometric correction
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T2207/00—Indexing scheme for image analysis or image enhancement
- G06T2207/10—Image acquisition modality
- G06T2207/10072—Tomographic images
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T2207/00—Indexing scheme for image analysis or image enhancement
- G06T2207/30—Subject of image; Context of image processing
- G06T2207/30004—Biomedical image processing
- G06T2207/30016—Brain
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Theoretical Computer Science (AREA)
- Measurement And Recording Of Electrical Phenomena And Electrical Characteristics Of The Living Body (AREA)
Abstract
本发明公开了一种颅脑动态电阻抗成像连续监护中断后监护图像信息继承的处理方法,用于恢复颅脑动态电阻抗成像临床连续监护中断后丢失的监护图像信息。该方法对连续监护中断前后的测量数据进行分析,首先使用样条差分拟合的方法处理测量数据,抑制连续监护中断前后电极接触状态不一致导致的测量数据基线变化引起的图像伪影,然后对图像重构矩阵进行增广处理,将电极位移的先验信息引入重建矩阵,减小监护中断前后电极因安放位置不一致对监护图像的影响。经测试,该方法能有效抑制监护中断前后电极接触状态和安放位置改变导致的图像伪影,恢复正常的监护目标,提高了电阻抗成像监护的临床实用性。
The invention discloses a processing method for inheriting monitoring image information after the continuous monitoring of craniocerebral dynamic electrical impedance imaging is interrupted, which is used for restoring the lost monitoring image information after the clinical continuous monitoring of craniocerebral dynamic electrical impedance imaging is interrupted. This method analyzes the measurement data before and after the interruption of continuous monitoring. First, the method of spline differential fitting is used to process the measurement data to suppress the image artifacts caused by the baseline change of the measurement data caused by the inconsistency of the electrode contact state before and after the interruption of continuous monitoring. The reconstruction matrix is augmented, and the prior information of the electrode displacement is introduced into the reconstruction matrix to reduce the influence of the electrodes on the monitoring image due to the inconsistent placement of the electrodes before and after the interruption of monitoring. After testing, this method can effectively suppress the image artifacts caused by the change of electrode contact state and placement position before and after monitoring interruption, restore the normal monitoring target, and improve the clinical practicability of electrical impedance imaging monitoring.
Description
技术领域technical field
本发明属于动态电阻抗成像技术领域,具体涉及一种颅脑动态电阻抗成像连续监护中断后监护图像信息继承的处理方法。The invention belongs to the technical field of dynamic electrical impedance imaging, and in particular relates to a processing method for inheriting monitoring image information after the continuous monitoring of cranial dynamic electrical impedance imaging is interrupted.
背景技术Background technique
颅脑动态电阻抗断层成像技术通过均匀分布在头部的周围电极,实时连续地向颅脑施加安全电流激励并测量边界电压,利用两个不同时刻的数据,以其中较早时刻的数据为参考帧,另外一个时刻的数据为前景帧,将两帧数据差分后,结合一定的成像方法,重建出颅脑内部在这两个不同时刻的阻抗变化。因此,连续稳定的采集数据是系统进行正常动态阻抗成像的首要条件。Brain dynamic electrical impedance tomography technology uses electrodes evenly distributed around the head to continuously apply safe current excitation to the brain in real time and measure the boundary voltage, using data at two different times and taking the data at the earlier time as a reference frame, and the data at another moment is the foreground frame. After the difference between the two frames of data, combined with a certain imaging method, the impedance changes inside the brain at these two different moments are reconstructed. Therefore, continuous and stable data acquisition is the primary condition for the system to perform normal dynamic impedance imaging.
在临床实际使用过程中,经常会出现不得不暂时中断监护的情况。比如病人需要进行CT等影像学检查,需要拆除环贴在头部的电极,在检查完毕后继续进行监护的话需要重贴电极。重贴电极后,与最初开始监护的状态相比,电极的位置和接触状态很有可能会发生改变,这种改变会直接影响采集数据。重新开始监护时,如果仍然使用最初开始监护时的参考帧,则由于电极-头皮接触状态和电极位置的改变可能会在重建图像上产生伪影,湮没正常的阻抗变化信息。如果选择重新开始监护时的数据作为参考帧,虽然可以消除电极-头皮接触状态和电极位置改变造成的影响,但重新开始监护前的图像信息无法直接反映在新的监护图像上,造成之前的阻抗变化信息丢失。连续监护的中断严重影响对病情的观察和诊断,不利于动态颅脑电阻抗成像的临床推广和应用。During actual clinical use, it often happens that monitoring has to be temporarily interrupted. For example, if a patient needs to undergo imaging examinations such as CT, the electrodes attached to the head need to be removed, and the electrodes need to be reattached if the monitoring is continued after the examination. After the electrodes are reattached, compared with the initial state of monitoring, the position and contact state of the electrodes are likely to change, and this change will directly affect the collected data. When restarting monitoring, if the reference frame at the beginning of monitoring is still used, the change of electrode-scalp contact status and electrode position may produce artifacts on the reconstructed image, obliterating the normal impedance change information. If the data at the restart of monitoring is selected as the reference frame, although the influence caused by the electrode-scalp contact state and electrode position change can be eliminated, the image information before the restart of monitoring cannot be directly reflected on the new monitoring image, resulting in the previous impedance Change information is lost. The interruption of continuous monitoring seriously affects the observation and diagnosis of the disease, which is not conducive to the clinical promotion and application of dynamic brain electrical impedance imaging.
因此,为了消除电极位置和接触状态改变对图像的影响,并保留前期的图像监护信息,亟需一种能够对连续监护中断后的数据进行处理的方法。Therefore, in order to eliminate the influence of electrode position and contact state changes on the image, and to preserve the previous image monitoring information, there is an urgent need for a method that can process the data after the continuous monitoring is interrupted.
发明内容Contents of the invention
本发明的目的在于提供一种颅脑动态电阻抗成像连续监护中断后监护图像信息继承的处理方法,该方法能够有效抑制电极位置和电极-头皮接触状态变化造成的重建图像伪影,并保留有效的图像监护信息,提高动态电阻抗成像的临床适用性。The purpose of the present invention is to provide a processing method for inheriting monitoring image information after the continuous monitoring of craniocerebral dynamic electrical impedance imaging is interrupted. Improving the clinical applicability of dynamic electrical impedance imaging.
本发明是通过以下技术方案来实现:The present invention is achieved through the following technical solutions:
一种颅脑动态电阻抗成像连续监护中断后监护图像信息继承的处理方法,该处理方法对连续监护中断前后的测量数据进行分析:首先,使用样条差分拟合的方法处理测量数据,抑制连续监护中断前后电极接触状态不一致导致的测量数据基线变化引起的图像伪影;然后,对图像重构算法进行增广处理,将电极位移的先验信息引入重建矩阵,减小监护中断前后电极因安放位置不一致对监护图像的影响。A processing method for inheriting monitoring image information after the continuous monitoring of craniocerebral dynamic electrical impedance imaging is interrupted. The image artifacts caused by the baseline change of the measurement data caused by the inconsistency of the electrode contact state before and after the interruption of monitoring; then, the image reconstruction algorithm is augmented, and the prior information of the electrode displacement is introduced into the reconstruction matrix to reduce the risk of electrode placement before and after the interruption of monitoring. The impact of inconsistencies in position on monitoring images.
上述处理方法具体包括以下步骤:The above processing method specifically includes the following steps:
1)获取测量数据的基线矫正值1) Obtain the baseline correction value of the measurement data
选定连续监护中断前的最后n帧数据和重新开始监护的前n帧数据,将数据连接在一起,为数据x(l),对第i个有效数据通道数据xi(l)使用样条函数拟合,获取拟合序列其中,i∈N,N为测量通道总数;Select the last n frames of data before continuous monitoring is interrupted and the first n frames of data before restarting monitoring, connect the data together, and use splines for the i-th valid data channel data x i (l) for data x(l) function fit, get the fitted sequence Among them, i∈N, N is the total number of measurement channels;
然后,检测在基线跃变处上升侧的极大值和下降侧的极小值计算基线矫正值 Then, detect Maximum value on the rising side at the baseline jump and the minima on the descending side Calculate baseline correction
2)对重新开始监护的数据进行测量基线矫正2) Measure baseline correction for the restarted monitoring data
对重新开始监护后的第i个测量通道数据序列yi(l),使用对yi(l)进行基线矫正,与监护中断前的数据相比,若yi(l)处于基线升高的一侧,则矫正后的若yi(l)处于基线下降的一侧,则矫正后的 For the i-th measurement channel data sequence y i (l) after restarting monitoring, use Baseline correction is performed on y i (l). Compared with the data before the interruption of monitoring, if y i (l) is on the side where the baseline rises, the corrected If y i (l) is on the side of the baseline decline, the corrected
3)对高斯-牛顿图像重建公式进行增广处理3) Augment the Gauss-Newton image reconstruction formula
对Δρ=-[JtJ+λR]-1Jz,Δρ为不同时刻间的电阻抗变化分布向量,z为不同时刻的边界电压差向量;For Δρ=-[J t J+λR] -1 Jz, Δρ is the electrical impedance change distribution vector at different times, and z is the boundary voltage difference vector at different times;
将雅各比矩阵扩展为将约束矩阵扩展为并利用先验信息确定系数λ和约束矩阵Raug的单元项;the Jacobian matrix expands to the constraint matrix expands to And use the prior information to determine the coefficient λ and the unit term of the constraint matrix R aug ;
4)使用矫正后的数据和增广的重建公式重建目标场域的阻抗变化4) Reconstruct the impedance variation of the target field using the rectified data and the augmented reconstruction formula
即其中为t1时刻的测量电压数据,为t2时刻的测量电压数据。which is in is the measured voltage data at time t1, It is the measured voltage data at time t2.
步骤1)中,对第i个有效数据通道数据xi(l)使用样条函数拟合,具体按下式进行:In step 1), the i-th effective data channel data x i (l) is fitted using a spline function, specifically as follows:
其中,S(x)为数据序列xi(l)的样条拟合函数,求S(x)令L的值取到最小;其中,p∈[0,1]反映了拟合函数与实测数据的接近程度;S(x)是分段样条拟合函数,写成一般形式:Among them, S(x) is the spline fitting function of the data sequence x i (l), find S(x) to minimize the value of L; among them, p∈[0,1] reflects the fitting function and the measured The proximity of the data; S(x) is a piecewise spline fitting function, written in a general form:
Sj(l)=aj(l-lj)3+bj(l-lj)2+cj(l-lj)+dj;S j (l)=a j (ll j ) 3 +b j (ll j ) 2 +c j (ll j )+d j ;
加入边界条件利用最小二乘法求解S(l)的各分段拟合函数系数。得到的S(l)具体表达式后,求拟合重构序列检测在基线跃变处上升侧的极大值和下降侧的极小值计算基线矫正值 Add boundary conditions and use the least squares method to solve the coefficients of each segment fitting function of S(l). After obtaining the specific expression of S(l), find the fitting reconstruction sequence detection Maximum value on the rising side at the baseline jump and the minima on the descending side Calculate baseline correction
步骤3)具体操作为:Step 3) The specific operation is:
高斯--牛顿图像重建公式如下式:The Gauss-Newton image reconstruction formula is as follows:
Δρ=-[JtJ+λR]-1Jz;Δρ=-[J t J+λR] -1 Jz;
其中,J为雅各比矩阵,λR为正则化约束项,Δρ为不同时刻间的电阻抗变化分布向量,z为不同时刻的边界电压差向量;Among them, J is the Jacobian matrix, λR is the regularization constraint item, Δρ is the distribution vector of electrical impedance change at different times, and z is the boundary voltage difference vector at different times;
为抑制电极位置变化对成像结果的影响,对重建公式中的矩阵进行增广处理:对于雅各比矩阵扩展为nmeas为一帧数据包含的测量电压数,nelem为成像所用的重构使用的有限元模型单元数,ndim为成像维数,通常进行二维成像,所以取ndim=2,ne为电极数量,雅各比矩阵的扩展部分填充为由于测量电极位置变化的扰动,即:In order to suppress the influence of electrode position changes on imaging results, the matrix in the reconstruction formula is augmented: for the Jacobian matrix expands to n meas is the number of measured voltages contained in one frame of data, n elem is the number of finite element model units used for imaging reconstruction, n dim is the imaging dimension, usually two-dimensional imaging, so take n dim = 2, n e is the number of electrodes, and the expansion part of the Jacobian matrix is filled with the disturbance due to the change of the measurement electrode position, namely:
其中,A为电流激励向量,H为正向计算矩阵,为电极位置在x或y方向上变化后重新计算的正向计算矩阵,该位移量通常统一设置为一个先验常量;Among them, A is the current excitation vector, H is the forward calculation matrix, It is a forward calculation matrix recalculated after the electrode position changes in the x or y direction, and the displacement is usually uniformly set as a priori constant;
然后,对约束矩阵R进行增广处理:Then, augment the constraint matrix R:
将扩展为扩展部分填充为重构数据的噪声先验估计和重构电导率变化的先验估计,即:Will expands to The extension part is populated with prior estimates of the noise of the reconstructed data and a prior estimate of the change in the reconstructed conductivity, namely:
其中,Rextra为一个拉普拉斯滤波器,根据成像场域的先验信息确定正则化参数λ和Rextra的拉普拉斯模板,则有:Among them, R extra is a Laplacian filter, and the regularization parameter λ and the Laplacian template of R extra are determined according to the prior information of the imaging field, then:
其中,avenoise为噪声相对于测量数据的平均先验幅值,aveconduct为电导率变化相对于初始电导率分布的平均先验幅值,avemove为相对于场域半径的电极位移平均先验幅值,为拉普拉斯算子。Among them, ave noise is the average prior amplitude of the noise relative to the measured data, ave conduct is the average prior amplitude of the conductivity change relative to the initial conductivity distribution, and ave move is the average prior amplitude of the electrode displacement relative to the field radius amplitude, is the Laplacian operator.
与现有技术相比,本发明具有以下有益的技术效果:Compared with the prior art, the present invention has the following beneficial technical effects:
本发明公开的颅脑动态电阻抗成像连续监护中断后监护图像信息继承的处理方法,用于恢复颅脑动态电阻抗成像临床连续监护中断后丢失的监护图像信息。该方法对连续监护中断前后的测量数据进行分析,首先使用样条差分拟合的方法处理测量数据,抑制连续监护中断前后电极接触状态不一致导致的测量数据基线变化引起的图像伪影,然后对图像重构矩阵进行增广处理,将电极位移的先验信息引入重建矩阵,减小监护中断前后电极因安放位置不一致对监护图像的影响。经测试,该方法能有效抑制监护中断前后电极接触状态和安放位置改变导致的图像伪影,恢复正常的监护目标,提高了电阻抗成像监护的临床实用性。The invention discloses a processing method for inheriting monitoring image information after the continuous monitoring of craniocerebral dynamic electrical impedance imaging is interrupted, which is used for recovering the lost monitoring image information after the interruption of clinical continuous monitoring of craniocerebral dynamic electrical impedance imaging. This method analyzes the measurement data before and after the interruption of continuous monitoring. First, the method of spline differential fitting is used to process the measurement data to suppress the image artifacts caused by the baseline change of the measurement data caused by the inconsistency of the electrode contact state before and after the interruption of continuous monitoring. The reconstruction matrix is augmented, and the prior information of the electrode displacement is introduced into the reconstruction matrix to reduce the influence of the electrodes on the monitoring image due to the inconsistent placement of the electrodes before and after the interruption of monitoring. After testing, this method can effectively suppress the image artifacts caused by the change of electrode contact state and placement position before and after monitoring interruption, restore the normal monitoring target, and improve the clinical practicability of electrical impedance imaging monitoring.
附图说明Description of drawings
图1是本发明的方法流程示意图;Fig. 1 is a schematic flow chart of the method of the present invention;
图2是连续监护中断前一时刻的重构图像。Figure 2 is the reconstructed image at the moment before the interruption of continuous monitoring.
图3是未使用本发明方法处理,将连续监护中断前一段时间的数据和重新开始监护后一段数据连接起来后的一维数据曲线(a),以及重新选择参考帧(c)和不重新选择参考帧(b)情况下的二维重构图像;Fig. 3 is not processed by the method of the present invention, the one-dimensional data curve (a) after connecting the data of a period of time before the interruption of continuous monitoring and a section of data after restarting the monitoring, and reselecting the reference frame (c) and not reselecting The two-dimensional reconstructed image in the case of the reference frame (b);
图4是使用本方法矫正步骤后的一维数据曲线(a),未使用改进算法(b)和使用了本方法改进成像算法的二维重构图像(c)。Figure 4 is the one-dimensional data curve (a) after the correction step using this method, the two-dimensional reconstructed image (c) without using the improved algorithm (b) and using the improved imaging algorithm of this method.
具体实施方式detailed description
下面结合具体的实施例对本发明做进一步的详细说明,所述是对本发明的解释而不是限定。The present invention will be further described in detail below in conjunction with specific embodiments, which are explanations of the present invention rather than limitations.
本发明的一种颅脑动态电阻抗成像连续监护中断后监护图像信息继承的处理方法,包括以下步骤:A processing method for inheriting monitoring image information after continuous monitoring of craniocerebral dynamic electrical impedance imaging is interrupted according to the present invention, comprising the following steps:
(1)获取测量数据的基线矫正值。选定连续监护中断前的最后n帧数据和重新开始监护的前n帧数据,将数据连接在一起为数据x(l),对第i(i∈N,N为测量通道总数)个有效数据通道数据xi(l)使用样条函数拟合:(1) Obtain the baseline correction value of the measurement data. Select the last n frames of data before continuous monitoring is interrupted and the first n frames of data before restarting monitoring, and connect the data together as data x(l), for the ith (i∈N, N is the total number of measurement channels) valid data The channel data x i (l) is fitted using a spline function:
其中S(x)为数据序列xi(l)的样条拟合函数,S(x)令L的值取到最小。其中p∈[0,1]反映了拟合函数与实测数据的接近程度。S(x)是分段样条拟合函数,可以写成一般形式:Among them, S(x) is the spline fitting function of the data sequence x i (l), and S(x) minimizes the value of L. where p∈[0,1] reflects the closeness of the fitting function to the measured data. S(x) is a piecewise spline fitting function, which can be written in general form:
Sj(l)=aj(l-lj)3+bj(l-lj)2+cj(l-lj)+dj S j (l)=a j (ll j ) 3 +b j (ll j ) 2 +c j (ll j )+d j
加入边界条件利用最小二乘法求解S(l)的各分段拟合函数系数。得到的S(l)具体表达式后,求拟合重构序列检测在基线跃变处上升侧的极大值和下降侧的极小值计算基线矫正值 Add boundary conditions and use the least squares method to solve the coefficients of each segment fitting function of S(l). After obtaining the specific expression of S(l), find the fitting reconstruction sequence detection Maximum value on the rising side at the baseline jump and the minima on the descending side Calculate baseline correction
(2)对重新开始监护的数据进行测量基线矫正。对重新开始监护后的第i个测量通道数据序列yi(l),使用对yi(l)进行基线矫正,与监护中断前的数据相比,若yi(l)处于基线升高的一侧,则矫正后的若yi(l)处于基线下降的一侧,则矫正后的 (2) Perform measurement baseline correction on the data of restarting monitoring. For the i-th measurement channel data sequence y i (l) after restarting monitoring, use Baseline correction is performed on y i (l). Compared with the data before the interruption of monitoring, if y i (l) is on the side where the baseline rises, the corrected If y i (l) is on the side of the baseline decline, the corrected
重复步骤(1)(2),对所有的测量通道进行以上处理,。Repeat steps (1) (2) to perform the above processing on all measurement channels.
(3)改进成像算法,对高斯-牛顿图像重建公式进行增广处理。对于高斯-牛顿成像算法公式:(3) Improving the imaging algorithm and augmenting the Gauss-Newton image reconstruction formula. For the Gauss-Newton imaging algorithm formula:
Δρ=-[JtJ+λR]-1JzΔρ=-[J t J+λR] -1 Jz
其中为J重构矩阵,λR为正则化约束项,z为不同时刻的边界电压差向量,Δρ为不同时刻间的电阻抗变化分布向量。where is the J reconstruction matrix, λR is the regularization constraint item, z is the boundary voltage difference vector at different times, and Δρ is the distribution vector of electrical impedance changes at different times.
为了抑制电极位置变化对成像结果的影响,则要对重构公式中的矩阵进行增广处理。对于雅各比矩阵扩展为nmeas为一帧数据包含的测量电压数,nelem为成像所用的重构使用的有限元模型单元数,ndim为成像维数,通常进行二维成像,所以取ndim=2,ne为电极数量,雅各比矩阵的扩展部分填充为由于测量电极位置变化的扰动,即In order to suppress the influence of electrode position changes on imaging results, the matrix in the reconstruction formula should be augmented. For the Jacobian matrix expands to n meas is the number of measured voltages contained in one frame of data, n elem is the number of finite element model units used for imaging reconstruction, n dim is the imaging dimension, usually two-dimensional imaging, so take n dim = 2, n e is the number of electrodes, and the expansion part of the Jacobian matrix is filled with the disturbance due to the change of the measurement electrode position, that is,
其中 in
A为电流激励向量,H为正向计算矩阵,为电极位置在x或y方向上变化后重新计算的正向计算矩阵,该位移量通常统一设置为一个先验常量。A is the current excitation vector, H is the forward calculation matrix, It is a forward calculation matrix that is recalculated after the electrode position changes in the x or y direction, and the displacement is usually uniformly set as a priori constant.
然后对约束矩阵R进行增广处理,将扩展为扩展部分填充为重构数据的噪声先验估计和重构电导率变化的先验估计,即Then the constraint matrix R is augmented, and the expands to The extension part is filled with the noise prior estimate of the reconstructed data and the prior estimate of the reconstructed conductivity change, namely
其中Rextra为一个拉普拉斯滤波器。根据成像场域的先验信息确定正则化参数λ和Rextra的拉普拉斯模板,有Where R extra is a Laplacian filter. Determining the regularization parameter λ and the Laplacian template of R extra according to the prior information of the imaging field, we have
其中avenoise为噪声相对于测量数据的平均先验幅值,aveconduct为电导率变化相对于初始电导率分布的平均先验幅值,avemove为相对于场域半径的电极位移平均先验幅值。where ave noise is the average prior amplitude of the noise relative to the measured data, ave conduct is the average prior amplitude of the conductivity change relative to the initial conductivity distribution, and ave move is the average prior amplitude of the electrode displacement relative to the field radius value.
(4)使用矫正后的数据和增广的重建公式重建目标场域的阻抗变化。即其中为重新开始监护后的参考帧电压数据,为重新开始监护后的前景帧电压数据,又可以简写为Δρ=Saugz。(4) Reconstruct the impedance variation of the target field using the corrected data and the augmented reconstruction formula. which is in For the reference frame voltage data after restarting monitoring, It can be abbreviated as Δρ=S aug z for the foreground frame voltage data after restarting monitoring.
具体实施方式如下:The specific implementation is as follows:
在受试者头部贴好全部涂好导电膏的电阻抗测量电极,并用绷带缠绕头部来固定电极,待所有电极接触正常后,开始进行数据采集和图像监护。正常连续监护的图像如图2所示,图像上包含有明显的阻抗变化目标。为了模拟监护中断的情况,将全部测量电极从受试者头部移除,用纱布将受试者头部贴电极的区域擦拭干净后,重贴全部电阻抗测量电极。受操作实际情况的限制,重贴的电极与初始状态相比,在分布位置和与头皮的接触阻抗都会发生变化,影响边界电压,使得重新开始监护前后的测量数据基线不一致,如图3(a)所示。如果不进行任何处理的话,仍然使用监护中断前的参考帧,则会在监护图像上表现出强烈的伪影,湮没原有目标,如图3(b)所示;如果选取重新开始监护后的数据为背景帧,则图像上则没有之前的目标信息,如图3(c)所示。因此需要一定的处理方法,在不重新选择成像参考帧的情况下,抑制图像伪影并恢复图像上原有的目标信息。Put the electrical impedance measurement electrodes coated with conductive paste on the subject's head, and wrap the head with a bandage to fix the electrodes. After all the electrodes are in normal contact, start data collection and image monitoring. The image of normal continuous monitoring is shown in Figure 2, and the image contains obvious impedance change targets. In order to simulate the interruption of monitoring, all the measuring electrodes were removed from the subject's head, and the area where the electrodes were attached to the subject's head was wiped clean with gauze, and then all the electrical impedance measuring electrodes were reattached. Restricted by the actual situation of the operation, compared with the initial state, the re-attached electrodes will change in the distribution position and the contact impedance with the scalp, which will affect the boundary voltage and make the measurement data baseline inconsistent before and after restarting monitoring, as shown in Figure 3(a ) shown. If no processing is performed and the reference frame before the monitoring interruption is still used, strong artifacts will appear on the monitoring image, obliterating the original target, as shown in Figure 3(b); If the data is a background frame, there is no previous target information on the image, as shown in Figure 3(c). Therefore, a certain processing method is needed to suppress image artifacts and restore the original target information on the image without reselecting the imaging reference frame.
根据图1所示流程,在重新开始监护时,按以下步骤对数据和成像算法进行处理:According to the process shown in Figure 1, when monitoring is restarted, the data and imaging algorithms are processed in the following steps:
步骤一:获取电极头皮接触状态不一致导致的测量数据基线变化。读取监护中断前的监护过程的最后n帧数据,以及重新开始的监护的前n帧数据,组合成测量数据序列x(l),数据序列的组成用矩阵表示为:Step 1: Obtain the baseline change of the measurement data caused by the inconsistency of the electrode scalp contact state. Read the last n frames of data of the monitoring process before the monitoring was interrupted, and the first n frames of data of the restarted monitoring, and combine them into a measurement data sequence x(l). The composition of the data sequence is expressed as a matrix:
xmeas(l)表示第l帧数据的第meas个测量通道的测量数据,并且有l=2n。在EIT测量系统中测量通道个数与电极数量和采用的激励-测量模式有关。每次处理选取单个测量通道的数据序列xi(l),利用样条函数按照下式对xi(l)进行拟合,求拟合函数S(l):x meas (l) represents the measured data of the meas-th measurement channel of the l-th frame data, and l=2n. The number of measurement channels in the EIT measurement system is related to the number of electrodes and the excitation-measurement mode used. Select the data sequence x i (l) of a single measurement channel for each processing, use the spline function to fit x i (l) according to the following formula, and find the fitting function S(l):
拟合函数S(l)是一个分段三次多项式,可以写成如下的一般形式:The fitting function S(l) is a piecewise cubic polynomial, which can be written in the following general form:
Sj(l)=aj(l-lj)3+bj(l-lj)2+cj(l-lj)+dj S j (l)=a j (ll j ) 3 +b j (ll j ) 2 +c j (ll j )+d j
加入自然边界条件b0=bl=0,并代入各分段边界条件和导数连续条件,得到矩阵方程:Adding the natural boundary condition b 0 =b l =0, and substituting each segmental boundary condition and derivative continuity condition, the matrix equation is obtained:
hi=xi+1-xi,qi=2(hi-1+hi), h i =x i+1 −x i , q i =2(h i−1 +h i ),
并得到系数aj,cj关于bj,dj的表达式:And get the expression of coefficient a j , c j with respect to b j , d j :
令L'=0,求得对应的三次多项式系数。得到样条拟合函数S(l)的表达式后,计算对应位置的拟合值序列检测在基线跃变处上升侧的极大值和下降侧的极小值计算基线矫正值 Let L'=0, obtain the corresponding cubic polynomial coefficients. After obtaining the expression of the spline fitting function S(l), calculate the fitting value sequence of the corresponding position detection Maximum value on the rising side at the baseline jump and the minima on the descending side Calculate baseline correction
步骤二:矫正变化的测量数据基线。对监护过程2的第i个测量通道数据序列yi(l),使用对yi(l)进行基线矫正。如图3(a)所示,与监护中断前的数据相比,yi(l)处于基线升高的一侧,则矫正后的矫正结果如图4(a)所示。如图4(b)所示,如果直接进行成像,则监护图像上会出现因电极位置变化的导致的监护图像伪影,影响对监护目标的识别判断,需要对图像伪影进行抑制处理。Step 2: Correct the baseline of the measured data for changes. For the ith measurement channel data sequence y i (l) of monitoring process 2, use Baseline correction is performed on y i (l). As shown in Figure 3(a), compared with the data before monitoring interruption, y i (l) is on the side of the baseline increase, and the corrected The rectification result is shown in Fig. 4(a). As shown in Figure 4(b), if imaging is performed directly, monitoring image artifacts caused by electrode position changes will appear on the monitoring images, which will affect the identification and judgment of monitoring targets, and image artifacts need to be suppressed.
步骤三:改成成像算法,抑制电极位置变化造成的图像伪影。对动态成像所使用的高斯-牛顿图像重建公式进行增广处理。有高斯-牛顿成像算法公式:Step 3: Change to an imaging algorithm to suppress image artifacts caused by electrode position changes. The Gauss-Newton image reconstruction formula used in dynamic imaging is augmented. There is a Gauss-Newton imaging algorithm formula:
Δρ=-[JtJ+λR]-1JzΔρ=-[J t J+λR] -1 Jz
其中为J重构矩阵,λR为正则化约束项,z为不同时刻的边界电压差向量,Δρ为不同时刻间的电阻抗变化分布向量。where is the J reconstruction matrix, λR is the regularization constraint item, z is the boundary voltage difference vector at different times, and Δρ is the distribution vector of electrical impedance changes at different times.
对于雅各比矩阵扩展为nmeas为一帧数据包含的测量电压数,nelem为成像所用的重构使用的有限元模型单元数,ne为测量电极数量,雅各比矩阵的扩展部分填充为测量电极位置变化的先验扰动补偿值,即:For the Jacobian matrix expands to n meas is the number of measured voltages contained in one frame of data, n elem is the number of finite element model units used for reconstruction for imaging, n e is the number of measurement electrodes, and the expansion part of the Jacobian matrix is filled with the precedence of the position change of the measurement electrodes. Check the disturbance compensation value, namely:
为了求得其中的填充元素,要利用电阻抗成像的正向计算公式 In order to obtain the filling elements, the forward calculation formula of electrical impedance imaging is used
z=HAz=HA
其中A为电流激励向量,H为正向计算矩阵,与用于成像的有限元模型坐标有关,z为边界电压向量。要计算先设置一个先验量θ,修改1号电极的x轴方向坐标ux为ux=ux+θ,重新计算正向重建矩阵,得到新的边界电压向量:Among them, A is the current excitation vector, H is the forward calculation matrix, which is related to the coordinates of the finite element model used for imaging, and z is the boundary voltage vector. to calculate First set a priori quantity θ, modify the x-axis coordinate u x of electrode 1 to u x = u x + θ, and recalculate the forward reconstruction matrix to obtain a new boundary voltage vector:
zmove=HmoveAz move = H move A
则有then there is
同理计算其它电极和y轴坐标发生位移的情况下的J矩阵增广元素,先验量都使用θ。In the same way, calculate the J matrix augmentation elements when other electrodes and y-axis coordinates are displaced, and use θ for the prior quantities.
然后对约束矩阵R进行增广处理,将扩展为扩展部分填充为重构数据的噪声先验估计和重构电导率变化的先验估计,即Then the constraint matrix R is augmented, and the expands to The extension part is filled with the noise prior estimate of the reconstructed data and the prior estimate of the reconstructed conductivity change, namely
其中Rextra为离散拉普拉斯滤波器形式,可写成:where R extra is in the form of a discrete Laplacian filter, which can be written as:
具体元素为:Ri,j|(extra)=2.1·δ2,Ri,j|(extra)=-1·δ2(i单元和j单元相邻),其它元素为0。其中aveconduct为目标电导率变化相对于初始电导率分布的比例系数,avemove为电极平均位移相对于场域半径的的比例系数。The specific elements are: R i,j|(extra) =2.1·δ 2 , R i,j|(extra) =-1·δ 2 (unit i and unit j are adjacent), and other elements are 0. in ave conduct is the proportional coefficient of the target conductivity change relative to the initial conductivity distribution, and ave move is the proportional coefficient of the average electrode displacement relative to the radius of the field.
约束系数λ为:The constraint coefficient λ is:
其中,avenoise为噪声信号相对于测量数据的比例系数。Among them, ave noise is the proportional coefficient of the noise signal relative to the measured data.
矫正后的成像结果如图4(c)所示。与未经算法处理,重新选择成像参考帧的成像结果相比,处理后的成像结果能有效反映出监护中断前的成像目标。与未经算法处理,未重新选择成像参考帧的成像结果相比,处理后的成像结果可以有效抑制数据测量的基线变化导致的图像伪影。经过对电极位置变化的算法补偿,和测量数据的基线矫正,与图2相比,经本文算法处理后的成像结果有效还原了原图像信息,参考图像右侧的色阶条,可以保证还原的图像结果在数值分布与原图像一致。因此,该监护图像信息继承处理的处理方法可以有效应对颅脑动态电阻抗成像连续监护中断后重新开始监护后原有监护信息丢失的情况。The corrected imaging result is shown in Fig. 4(c). Compared with the imaging results without algorithm processing and reselecting the imaging reference frame, the processed imaging results can effectively reflect the imaging target before the interruption of monitoring. Compared with the imaging results without algorithm processing and without reselecting the imaging reference frame, the processed imaging results can effectively suppress the image artifacts caused by the baseline change of the data measurement. After the algorithm compensation for the electrode position change and the baseline correction of the measurement data, compared with Figure 2, the imaging result processed by the algorithm in this paper effectively restores the original image information. Refer to the color scale bar on the right side of the image to ensure the restoration The image result is consistent with the original image in the value distribution. Therefore, the monitoring image information inheritance processing method can effectively deal with the loss of the original monitoring information after the continuous monitoring of the craniocerebral dynamic electrical impedance imaging is interrupted and the monitoring is restarted.
Claims (4)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201610916112.0A CN106529126B (en) | 2016-10-20 | 2016-10-20 | A kind of on-line monitor guards the processing method that image information is inherited after interrupting |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201610916112.0A CN106529126B (en) | 2016-10-20 | 2016-10-20 | A kind of on-line monitor guards the processing method that image information is inherited after interrupting |
Publications (2)
Publication Number | Publication Date |
---|---|
CN106529126A true CN106529126A (en) | 2017-03-22 |
CN106529126B CN106529126B (en) | 2018-05-04 |
Family
ID=58332479
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201610916112.0A Active CN106529126B (en) | 2016-10-20 | 2016-10-20 | A kind of on-line monitor guards the processing method that image information is inherited after interrupting |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN106529126B (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108714027A (en) * | 2018-03-26 | 2018-10-30 | 中国人民解放军第四军医大学 | A kind of device and measurement method for measuring multi-electrode/scalp contact impedance in real time |
CN112150572A (en) * | 2020-09-30 | 2020-12-29 | 河南省人民医院 | A method and device for suppressing image contact impedance artifacts for dynamic electrical impedance imaging |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102370480A (en) * | 2011-09-30 | 2012-03-14 | 中国人民解放军第四军医大学 | Impedance detection device and detection method for craniocerebral radiation therapy treatment |
CN102599908A (en) * | 2012-04-09 | 2012-07-25 | 成都晨德科技有限公司 | Electrical impedance tomography method based on gridding displacement model with balance factor |
-
2016
- 2016-10-20 CN CN201610916112.0A patent/CN106529126B/en active Active
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102370480A (en) * | 2011-09-30 | 2012-03-14 | 中国人民解放军第四军医大学 | Impedance detection device and detection method for craniocerebral radiation therapy treatment |
CN102599908A (en) * | 2012-04-09 | 2012-07-25 | 成都晨德科技有限公司 | Electrical impedance tomography method based on gridding displacement model with balance factor |
Non-Patent Citations (2)
Title |
---|
张戈: "颅脑电阻抗成像数据采集中电极干扰的预处理方法研究", 《中国优秀硕士学位论文全文数据库》 * |
陈晓艳等: "电阻抗与 EIT 测量微系统设计", 《中国生物医学工程学报》 * |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108714027A (en) * | 2018-03-26 | 2018-10-30 | 中国人民解放军第四军医大学 | A kind of device and measurement method for measuring multi-electrode/scalp contact impedance in real time |
CN112150572A (en) * | 2020-09-30 | 2020-12-29 | 河南省人民医院 | A method and device for suppressing image contact impedance artifacts for dynamic electrical impedance imaging |
CN112150572B (en) * | 2020-09-30 | 2021-08-17 | 河南省人民医院 | A method and device for suppressing image contact impedance artifacts for dynamic electrical impedance imaging |
Also Published As
Publication number | Publication date |
---|---|
CN106529126B (en) | 2018-05-04 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US12059260B2 (en) | Channel integrity detection and reconstruction of electrophysiological signals | |
Trigo et al. | Electrical impedance tomography using the extended Kalman filter | |
US9977060B2 (en) | Channel integrity detection | |
Erem et al. | Using transmural regularization and dynamic modeling for noninvasive cardiac potential imaging of endocardial pacing with imprecise thoracic geometry | |
EP2867861B1 (en) | Motion parameter estimation | |
EP2690598A2 (en) | Method and apparatus for determining blood flow required, method and apparatus for producing blood flow image, and method and apparatus for processing myocardial perfusion image | |
EP2693401A1 (en) | Vessel segmentation method and apparatus using multiple thresholds values | |
KR20120024842A (en) | Image processing apparatus, control method thereof, and computer program | |
US10357178B2 (en) | System and method for enhanced electrical impedance tomography | |
CN108830875B (en) | Electrical impedance tomography image segmentation method based on minimum residual error | |
CN106529126B (en) | A kind of on-line monitor guards the processing method that image information is inherited after interrupting | |
Amelon et al. | A measure for characterizing sliding on lung boundaries | |
CN111588353A (en) | Body temperature measuring method | |
Agnelli et al. | Simultaneous reconstruction of conductivity, boundary shape, and contact impedances in electrical impedance tomography | |
CN116869504A (en) | Data compensation method for cerebral ischemia conductivity distribution reconstruction | |
CN103065286A (en) | Image reconstruction method in quasi-static electrical impedance imaging | |
CN116824048B (en) | A sensor, Jacobian matrix solution method, three-dimensional imaging system and method | |
CN112043271A (en) | Electrical impedance measurement data correction method and device | |
CN112150572B (en) | A method and device for suppressing image contact impedance artifacts for dynamic electrical impedance imaging | |
Liew et al. | Spatial cardiac dysfunction assessment via personalized modelling from MRI | |
Moghaddam et al. | Analytical method to measure three-dimensional strain patterns in the left ventricle from single slice displacement data | |
CN113413149B (en) | A design method for EIT sensor with optimized edge sensitivity | |
CN110988043B (en) | Multi-media separation imaging method based on multi-frequency weighted frequency difference | |
Kirchberg et al. | Modeling the human aorta for MR-driven real-time virtual endoscopy | |
CN117338278A (en) | Multi-frequency electrical impedance tomography method and system |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |