CN114646913B - Non-invasive measurement method for microstructure of biological tissue - Google Patents

Non-invasive measurement method for microstructure of biological tissue Download PDF

Info

Publication number
CN114646913B
CN114646913B CN202011515119.4A CN202011515119A CN114646913B CN 114646913 B CN114646913 B CN 114646913B CN 202011515119 A CN202011515119 A CN 202011515119A CN 114646913 B CN114646913 B CN 114646913B
Authority
CN
China
Prior art keywords
chamber
chamber structure
diffusion coefficient
volume ratio
voxel point
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.)
Active
Application number
CN202011515119.4A
Other languages
Chinese (zh)
Other versions
CN114646913A (en
Inventor
韩鸿宾
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Peking University Third Hospital Peking University Third Clinical Medical College
Original Assignee
Peking University Third Hospital Peking University Third Clinical Medical College
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Peking University Third Hospital Peking University Third Clinical Medical College filed Critical Peking University Third Hospital Peking University Third Clinical Medical College
Priority to CN202011515119.4A priority Critical patent/CN114646913B/en
Publication of CN114646913A publication Critical patent/CN114646913A/en
Application granted granted Critical
Publication of CN114646913B publication Critical patent/CN114646913B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/44Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
    • G01R33/48NMR imaging systems
    • G01R33/54Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B5/00Measuring for diagnostic purposes; Identification of persons
    • A61B5/05Detecting, measuring or recording for diagnosis by means of electric currents or magnetic fields; Measuring using microwaves or radio waves 
    • A61B5/055Detecting, measuring or recording for diagnosis by means of electric currents or magnetic fields; Measuring using microwaves or radio waves  involving electronic [EMR] or nuclear [NMR] magnetic resonance, e.g. magnetic resonance imaging
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/44Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
    • G01R33/48NMR imaging systems
    • G01R33/54Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console
    • G01R33/56Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution
    • G01R33/563Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution of moving material, e.g. flow contrast angiography
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/44Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
    • G01R33/48NMR imaging systems
    • G01R33/54Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console
    • G01R33/56Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution
    • G01R33/563Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution of moving material, e.g. flow contrast angiography
    • G01R33/56341Diffusion imaging

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Engineering & Computer Science (AREA)
  • High Energy & Nuclear Physics (AREA)
  • General Health & Medical Sciences (AREA)
  • Radiology & Medical Imaging (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • Signal Processing (AREA)
  • Vascular Medicine (AREA)
  • Heart & Thoracic Surgery (AREA)
  • Surgery (AREA)
  • Animal Behavior & Ethology (AREA)
  • Molecular Biology (AREA)
  • Public Health (AREA)
  • Veterinary Medicine (AREA)
  • Medical Informatics (AREA)
  • Biophysics (AREA)
  • Biomedical Technology (AREA)
  • Pathology (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

A method for non-invasive measurement of biological tissue microstructure comprising: I. performing magnetic resonance diffusion weighted imaging on biological tissues; II. Measuring the actual image signal intensity of each voxel point in each magnetic resonance image; III, substituting the actual image signal intensity of the integral pixel into a formula to solve; IV, judging whether the voxel point is of a single-chamber structure, a double-chamber structure or a three-chamber structure according to the solving result; v, judging the tissue type in the voxel point; and VI, repeating the steps III to V to analyze other voxel points until all voxel points are analyzed. The method is capable of measuring the microstructure of biological tissue.

Description

Non-invasive measurement method for microstructure of biological tissue
Technical Field
The invention relates to a method for measuring a biological tissue microstructure, in particular to a noninvasive measuring method for measuring the biological tissue microstructure through magnetic resonance imaging.
Background
Magnetic resonance (magnetic resonance imaging, MRI) has been widely used for imaging biological tissue due to its non-ionizing damage, high soft tissue resolution, and sensitivity to chemical components.
Currently, there is a method for solving the volume ratio of cells, the volume ratio of blood vessels, the volume ratio of extracellular space, the diffusion coefficient of cells, the diffusion coefficient of blood vessels, and the diffusion coefficient of extracellular space at each voxel point of a biological tissue from the actual image signal intensity of each voxel point in a magnetic resonance image. In the solving process, each voxel point is assumed to be composed of cells, blood vessels and extracellular spaces, the actual structure of biological tissues is not met, and the problem that some voxel points cannot be solved exists.
Disclosure of Invention
The invention aims to provide a noninvasive measuring method of microstructure of biological tissue, which can measure microstructure of biological tissue.
The invention provides a noninvasive measurement method of a microstructure of biological tissue, which comprises the following steps:
I. performing magnetic resonance diffusion weighted imaging on biological tissues to obtain weights b respectively corresponding to different weights i Wherein i=1, 2, 3..n, n.gtoreq.6;
II. Measuring the actual image signal intensity S (b) of each voxel point in each magnetic resonance image i );
III, taking any integral pixel point in the magnetic resonance image, and obtaining the actual image signal intensity S (b i ) Substituting the following equations 1 to 3 to solve D, V in the equation 21 、V 22 、D 21 、D 22 、V 31 、V 32 、V 33 、D 31 、D 32 And D 33
Single chamber model:
Figure BDA0002847579090000011
double-chamber model:
Figure BDA0002847579090000012
three-chamber model:
Figure BDA0002847579090000021
wherein: s (b) 0 ) For the signal intensity of the voxel point when no diffusion sensitive gradient pulse is applied, D is the diffusion coefficient of a single-chamber structure, V 21 The volume ratio of the first chamber of the double-chamber structure, V 22 The volume ratio of the second chamber of the double-chamber structure, D 21 Diffusion coefficient of the first chamber of the double-chamber structure, D 22 Diffusion coefficient of the second chamber of the double-chamber structure, V 31 The volume ratio of the first chamber of the three-chamber structure, V 32 The volume ratio of the second chamber of the three-chamber structure, V 33 The volume ratio of the third chamber of the three-chamber structure, D 31 Diffusion coefficient of the first chamber of the three-chamber structure, D 32 Diffusion coefficient of the second chamber of the three-chamber structure, D 33 The diffusion coefficient of the third chamber, which is a three-chamber structure;
IV, judging whether the voxel point is of a single-chamber structure, a double-chamber structure or a three-chamber structure according to the solving result of the step III;
v, if the voxel point is judged to be of a single-chamber structure in the step IV, judging the tissue type of the single-chamber structure according to the step D; the tissue types include cells, blood vessels, and extracellular spaces; the volume ratio and diffusion coefficient of the tissue type not contained in the single-chamber structure are set to 0. If the voxel point is judged to be of a dual-chamber structure in step IV, then the method is performed according to D 21 And D 22 Judging the tissue types of the first chamber and the second chamber of the double-chamber structure; the tissue types include cells, blood vessels, and extracellular spaces; the volume ratio and diffusion coefficient of the tissue type not contained in the dual chamber structure are set to 0. If the voxel point is judged to be of a three-compartment structure in step IV, then the method is performed according to D 31 、D 32 And D 33 Judging the tissue types of the first chamber, the second chamber and the third chamber of the three-chamber structure; the tissue types include cells, blood vessels, and extracellular spaces.
And VI, repeating the step III to the step V to analyze other voxel points until all voxel point analysis is completed.
The non-invasive measurement method of the microstructure of the biological tissue comprises the steps of judging whether each voxel point of the biological tissue belongs to a single-chamber structure, a double-chamber structure or a three-chamber structure, and determining the tissue type of each voxel point based on a judgment result, so that the microstructure of the biological tissue is measured.
In another exemplary embodiment of the non-invasive measurement method for microstructure of biological tissue, in the step IV, the determination of the voxel point as a single-chamber structure, a double-chamber structure or a three-chamber structure according to the result of the solution in the step III is specifically:
if it is
Figure BDA0002847579090000022
And is also provided with
Figure BDA0002847579090000023
Then the voxel point is a single-cell structure.
If it is
Figure BDA0002847579090000024
And is also provided with
Figure BDA0002847579090000025
Figure BDA0002847579090000031
Then the voxel point is a dual-chambered structure. Otherwise, the voxel point is in a three-chamber structure. The judging method is simple.
In yet another exemplary embodiment of the method for non-invasive measurement of a microstructure of a biological tissue, after step VI, further comprises: VII, reconstructing a magnetic resonance image according to any one or more of the volume ratio of cells, the volume ratio of blood vessels, the volume ratio of extracellular space, the diffusion coefficient of cells, the diffusion coefficient of blood vessels and the diffusion coefficient of extracellular space of each voxel point. To facilitate a more visual reflection of the structure of biological tissue.
In yet another exemplary embodiment of the non-invasive measurement method of biological tissue microstructure, the solution method in step III employs constrained nonlinear optimization solution; wherein,,
the optimization formula of formula 1 is:
Figure BDA0002847579090000032
s.t.D≥0
the optimization formula of formula 2 is:
Figure BDA0002847579090000033
Figure BDA0002847579090000034
the optimization formula of formula 3 is:
Figure BDA0002847579090000035
Figure BDA0002847579090000036
. Thereby more accurately measuring the microstructure of biological tissue.
In yet another exemplary embodiment of the non-invasive measurement method of biological tissue microstructure, the constrained nonlinear optimization solution employs a Lagrangian multiplier method.
In yet another exemplary embodiment of the method for non-invasive measurement of a microstructure of a biological tissue, after step VI, further comprises: VIII, calculating the cellulose trend distribution of the cells, the blood vessels and the extracellular space according to the diffusion coefficient of the cells, the diffusion coefficient of the blood vessels and the diffusion coefficient of the extracellular space of each voxel point. To facilitate a more visual reflection of the diffuse nature of biological tissue.
In yet another exemplary embodiment of the non-invasive measurement method of the microstructure of the biological tissue, the calculation is performed using a statistical method or a main diffusion direction based tracking method.
Drawings
The following drawings are only illustrative of the invention and do not limit the scope of the invention.
Fig. 1 and 2 are magnetic resonance images of brain tissue.
FIG. 3 is a plot of basal ganglia cell fiber bundle trend.
FIG. 4 is a graph showing the trend of cell fiber bundles on both sides of callus.
FIG. 5 is a plot of tumor and healthy side cell fiber bundle trend profile.
Fig. 6 is a magnetic resonance image of brain tissue.
Fig. 7 is a schematic diagram after reconstitution.
Detailed Description
For a clearer understanding of technical features, objects, and effects of the present invention, a specific embodiment of the present invention will be described with reference to the accompanying drawings.
In this document, "schematic" means "serving as an example, instance, or illustration," and any illustrations, embodiments described herein as "schematic" should not be construed as a more preferred or advantageous solution.
Herein, "first", "second", etc. do not indicate the degree of importance or order thereof, etc., but merely indicate distinction from each other to facilitate description of documents.
Here, the object of each embodiment of the noninvasive measurement method of the microstructure of the biological tissue is brain tissue, but the method is not limited to brain tissue, and may be applied to other biological tissues.
According to the recent studies of the present inventors, it was found that the distribution of the extracellular space in brain tissue is heterogeneous, and in a partial brain region (for example, an inner capsule region), a dense fiber bundle structure makes the volume ratio of the extracellular space in the region 0, and only a cell structure and a blood vessel structure exist in a ventricle region. In the actual structure of biological tissue, for a voxel point, the tissue structure may be one, two or three of cells, blood vessels and extracellular space.
In order to measure the microstructure of biological tissue, the present invention provides a non-invasive measurement method of brain tissue microstructure, which in one exemplary embodiment thereof comprises the following steps.
Step I: using a plurality of different weights b i Performing magnetic resonance diffusion weighted imaging on the measurement interest region of the brain tissue to obtain weights b respectively corresponding to different weights i Wherein i=1, 2, 3..n, n.gtoreq.6. In the illustrative embodiment, the weight b i For vectors with direction, multiple different weights b can be obtained by changing the modulus i That is, this step results in at least six magnetic resonance images of the region of interest of the measurement for the same brain tissue, and the weights b of the respective magnetic resonance images i Is the same and the modulus is different. In the illustrative embodiment, the weight b i The direction of (2) is, for example, laboratory [1,0 ]]Direction or laboratory [0.446,0.895,0 ]]Of course, in the exemplary embodiment, other directions may be provided as desired. In the illustrative embodiment, the weight b can also be changed by i Obtain a plurality of different weights b i I.e. the present step yields at least six magnetic resonance images of the region of interest of the measurement for the same brain tissue, and the weights b of the respective magnetic resonance images i For example, when n=6, the weight b i The directions of (1), (0) and (0)],[0.446,0.895,0],[0.447,0.275,0.851],[0.448,-0.723,-0.525],[0.447,-0.724,0.526],[-0.449,-0.277,0.850]。
Step II: measuring the actual image signal intensity S (b) of each voxel point in each magnetic resonance image obtained in step I i ) And the actual image signal strength S (b i ) The gray scale of the voxel point in the image is reflected in the magnetic resonance image.
Step III: the magnetic resonance image is integratedA pixel point whose actual image signal intensity S (b i ) Substituting the following formulas 1 to 3 and solving D, V in the formulas 21 、V 22 、D 21 、D 22 、V 31 、V 32 、V 33 、D 31 、D 32 And D 33
Single chamber model:
Figure BDA0002847579090000051
double-chamber model:
Figure BDA0002847579090000052
three-chamber model:
Figure BDA0002847579090000053
wherein S (b) 0 ) For the signal intensity of the voxel point when no diffusion sensitive gradient pulse is applied, D is the diffusion coefficient of a single-chamber structure, V 21 The volume ratio of the first chamber of the double-chamber structure, V 22 The volume ratio of the second chamber of the double-chamber structure, D 21 Diffusion coefficient of the first chamber of the double-chamber structure, D 22 Diffusion coefficient of the second chamber of the double-chamber structure, V 31 The volume ratio of the first chamber of the three-chamber structure, V 32 The volume ratio of the second chamber of the three-chamber structure, V 33 The volume ratio of the third chamber of the three-chamber structure, D 31 Diffusion coefficient of the first chamber of the three-chamber structure, D 32 Diffusion coefficient of the second chamber of the three-chamber structure, D 33 Diffusion coefficient of the third chamber, which is a three-chamber structure. The volume ratio refers to the percentage of each chamber to the total volume of the voxel point, and the diffusion coefficient refers to the movement speed of water molecules in each chamber.
In the above solving process, when the number of unknowns is less than the number of effective equations, an overdetermined equation is used to solve the optimal solution. For exampleIf the integral pixel point is larger than one corresponding weight b i Actual image signal intensity S (b) i ) Substituting equation 1 can result in a number of equations greater than one effective; if a voxel point is greater than four corresponding weights b i Actual image signal intensity S (b) i ) Substituting equation 2 can result in a number of equations greater than four valid; if the integral pixel point is greater than six corresponding weights b i Actual image signal intensity S (b) i ) Substituting equation 3 may yield a number of equations greater than six. In this case, an overdetermined equation is used to find the optimal solution. It will be appreciated that the greater the number of equations available, the greater the accuracy of the solution.
In the present exemplary embodiment, the above solution employs a constrained nonlinear optimization solution, wherein,
the optimization formula of formula 1 is:
Figure BDA0002847579090000061
s.t.D 0
The optimization formula of formula 2 is:
Figure BDA0002847579090000062
Figure BDA0002847579090000063
the optimization formula of formula 3 is:
Figure BDA0002847579090000064
Figure BDA0002847579090000065
in this step, the voxel point is calculated assuming a single-chamber structure (i.e., including one of a cell, a blood vessel, and an extracellular space), a double-chamber structure (i.e., including two of a cell, a blood vessel, and an extracellular space), and a triple-chamber structure (i.e., including a cell, a blood vessel, and an extracellular space), respectively. In the present exemplary embodiment, the constrained nonlinear optimization solution employs a Lagrangian multiplier method. But is not limited thereto, in other exemplary embodiments, other constrained nonlinear optimization solving methods may be employed, such as conjugate gradient method, steepest descent method, multidimensional newton method, and the like.
Step IV: and D, judging whether the voxel point is of a single-chamber structure, a double-chamber structure or a three-chamber structure according to the solving result of the step III. In the present exemplary embodiment, specifically:
if it is
Figure BDA0002847579090000066
And is also provided with
Figure BDA0002847579090000067
Then the voxel point is a single-cell structure.
If it is
Figure BDA0002847579090000068
/>
And is also provided with
Figure BDA0002847579090000069
Figure BDA0002847579090000071
Then the voxel point is a dual-chambered structure. Otherwise, the voxel point is in a three-chamber structure. Where e is an empirical parameter that varies depending on the nuclear magnetic device and the tissue being scanned, for example, scanning brain tissue based on a GE nmr machine, e may be 0.1. The determination of e is based on anatomical results. The actual distribution of cells, blood vessels and extracellular spaces in the biological tissue is determined according to anatomy, the steps I to IV are carried out on the same biological tissue, and the appropriate epsilon is selected so that the judgment result is consistent with the anatomy result, thereby determining the experience value epsilon. In other illustrative embodiments, the e may also be obtained using a machine learning method from a large amount of annotation data. But is not limited thereto. In the exemplary embodiment, the above determination may be instead performed based on a method such as machine learning.
Step V: if the voxel point is judged to be a single-chamber structure in the step IV, judging the tissue type of the single-chamber structure according to the D; the volume ratio and diffusion coefficient of the tissue type not contained in the single-chamber structure are set to 0. If the voxel point is judged to be of a dual-chamber structure in step IV, then the method is performed according to D 21 And D 22 Judging the tissue types of the first chamber and the second chamber of the double-chamber structure; the volume ratio and diffusion coefficient of the tissue type not contained in the dual chamber structure are set to 0. If the voxel point is judged to be of a three-compartment structure in step IV, then the method is performed according to D 31 、D 32 And D 33 The tissue type of the first, second and third chambers of the three-chamber structure is determined. The tissue types described above include cells, blood vessels, and extracellular spaces. In the present exemplary embodiment, for example, based on anatomical results, by D, D 21 、D 22 、D g1 、D 32 And D 33 Is used to determine the tissue type. Specifically, the actual distribution situation of cells, blood vessels and extracellular spaces in biological tissues is determined according to anatomy, the steps I to IV are carried out on the same biological tissues, and D values of voxel points of the single-chamber structure of the cells, the single-chamber structure of the blood vessels and the single-chamber structure of the extracellular spaces determined in the anatomy result are used as the basis for judging the corresponding tissue types respectively.
Step VI: and (3) repeating the steps III to V to analyze other voxel points until all voxel point analysis is completed.
Step VII: reconstructing a magnetic resonance image from any one or more of the volume ratio of cells, the volume ratio of blood vessels, the volume ratio of extracellular space, the diffusion coefficient of cells, the diffusion coefficient of blood vessels, and the diffusion coefficient of extracellular space at each voxel point. By displaying the reconstructed image, the structure of the biological tissue is more intuitively reflected.
Step VIII: the cellulose trend distribution of the cells, the blood vessels and the extracellular space is calculated by the diffusion coefficient of the cells, the diffusion coefficient of the blood vessels and the diffusion coefficient of the extracellular space of each voxel point. The calculation is performed using a statistical method or a main diffusion direction-based tracking method, and in the present exemplary embodiment, a recursive method described in chinese patent application No. CN201510082396.3 is used, for example. However, the present invention is not limited to this, and in other exemplary embodiments, other methods may be used for estimation.
The following are experimental results obtained by the non-invasive measurement method of the microstructure of biological tissue according to the present exemplary embodiment. Wherein the values of N are all 6, and the values of E are all 0.1. Magnetic resonance apparatus produced by GE company, weight b i The directions of (1), (0) and (0)],[0.446,0.895,0],[0.447,0.275,0.851],[0.448,-0.723,-0.525],[0.447,-0.724,0.526],[-0.449,-0.277,0.850]。
Fig. 1 is a magnetic resonance image of brain tissue, wherein the rectangular region is the center of a semicircle to be analyzed. Table 1 shows the volume ratios and diffusion coefficients of the cells, blood vessels and extracellular spaces in the center of the semicircle obtained by the non-invasive measurement method of the microstructure of the biological tissue. Wherein V is vas V is the volume ratio of the blood vessels ecs V as the volume ratio of the extracellular space cell Is the volume ratio of cells, D vas Is the diffusion coefficient of blood vessel, D ecs Is the diffusion coefficient of extracellular space, D cell Is the diffusion coefficient of the cell.
TABLE 1 volume ratios and diffusion coefficients of cells, vessels and extracellular spaces in the semi-oval center of brain tissue
Type(s) Maximum value Minimum value Median of Standard deviation of Number of pixels
V vas (%) 18 0.67 7.3 0.091 56
V ecs (%) 40 0.75 12 0.74 56
V cell (%) 94 56 79 0.73 56
D vas (*10 -6 mm 2 /s) 2.2 0.28 0.49 0.23 56
D ecs (*10 -6 mm 2 /s) 0.71 0.32 0.52 0.0084 56
D cell (*10 -6 mm 2 /s) 0.004 0.0016 0.0023 0.00000026 56
Fig. 2 is a magnetic resonance image of brain tissue, wherein the rectangular region is the callus area to be analyzed. Table 1 shows the volume ratios and diffusion coefficients of cells, blood vessels and extracellular spaces of the callus area obtained by the non-invasive measurement method of the microstructure of biological tissue described above.
TABLE 2 volume ratio and diffusion coefficient of cells, vessels and extracellular spaces of callus areas of brain tissue
Type(s) Maximum value Minimum value Median of Standard deviation of Number of pixels
V vas (%) 20 3.5 11 0.2 39
V ecs (%) 38 3.7 16 0.68 39
V cell (%) 89 53 70 0.87 39
D vas (*10 -6 mm 2 /s) 2.6 0.25 0.37 0.55 39
D ecs (*10 -6 mm 2 /s) 1.3 0.21 0.43 0.035 39
D cell (*10 -6 mm 2 /s) 0.0041 0.0012 0.0019 0.00000047 39
Fig. 3 to 5 are fiber bundle trend profiles obtained by the non-invasive measurement method of the microstructure of biological tissue described above. Wherein FIG. 3 shows the cellular fiber bundle trend distribution of basal ganglia, including transverse, coronal, sagittal, and magnified views. FIG. 4 shows the distribution of cell fiber bundles on both sides of the corpus callosum, including transection, coronal, sagittal, and magnified views. FIG. 5 shows the distribution of tumor and healthy side cell fiber bundles including transection, coronal, sagittal, and magnified views.
The non-invasive measurement method of the microstructure of the biological tissue according to the present exemplary embodiment obtains the volume ratios of cells, blood vessels and extracellular spaces of brain tissue of a normal population as follows:
frontal cortex: the volume ratio of cells is about 90%;
semi-oval center: the volume ratio of cells is about 80-85%, and the volume ratio of extracellular space to blood vessel is about 1:1;
base section: the volume ratio of the extracellular space is about 15%, which is consistent with the 15-20% ratio reported in the prior literature.
Fig. 6 shows a magnetic resonance image of brain tissue of a patient. As can be seen in fig. 6, the patient has malignant edema in the right hemisphere (i.e., left side of the drawing). Fig. 7 is a schematic representation of a reconstruction of fig. 6 by a non-invasive measurement method of the microstructure of biological tissue as described above. In the upper three images in fig. 7, the diffusion coefficient of cells, the diffusion coefficient of blood vessels, and the diffusion coefficient of extracellular space are shown from left to right, respectively; in the lower three images, the volume ratio of cells, the volume ratio of blood vessels, and the volume ratio of extracellular space are shown from left to right, respectively.
The noninvasive measuring method of the microstructure of the biological tissue is characterized in that each voxel point of the biological tissue is judged to belong to a single-chamber structure, a double-chamber structure or a three-chamber structure, and the tissue type of each voxel point is determined based on the judging result, so that the method is more in line with the actual structural characteristics of the biological tissue, and the microstructure of the biological tissue is measured.
It should be understood that although the present disclosure has been described in terms of various embodiments, not every embodiment is provided with a separate technical solution, and this description is for clarity only, and those skilled in the art should consider the disclosure as a whole, and the technical solutions in the various embodiments may be combined appropriately to form other embodiments that will be understood by those skilled in the art.
The above list of detailed descriptions is only specific to practical examples of the present invention, and they are not intended to limit the scope of the present invention, and all equivalent embodiments or modifications, such as combinations, divisions or repetitions of features, without departing from the technical spirit of the present invention are included in the scope of the present invention.

Claims (7)

1. A method for non-invasive measurement of a microstructure of biological tissue, comprising:
i, performing magnetic resonance diffusion weighted imaging on biological tissues to obtain weights respectively corresponding to the biological tissues
Figure QLYQS_1
Is defined, wherein +.>
Figure QLYQS_2
II, measuring the actual image signal intensity of each voxel point in each magnetic resonance image
Figure QLYQS_3
III, taking any integral pixel point from the magnetic resonance image, and obtaining the actual image signal intensity of the pixel point
Figure QLYQS_5
Substituting the following formulas 1 to 3 to solve +.>
Figure QLYQS_9
、/>
Figure QLYQS_12
、/>
Figure QLYQS_6
、/>
Figure QLYQS_8
、/>
Figure QLYQS_11
、/>
Figure QLYQS_14
、/>
Figure QLYQS_4
、/>
Figure QLYQS_10
、/>
Figure QLYQS_13
Figure QLYQS_15
And->
Figure QLYQS_7
Single chamber model:
Figure QLYQS_16
double-chamber model:
Figure QLYQS_17
three-chamber model:
Figure QLYQS_18
wherein:
Figure QLYQS_19
for the signal intensity of the voxel point when no diffusion sensitive gradient pulse is applied,
Figure QLYQS_20
the diffusion coefficient of the single-chamber structure,
Figure QLYQS_21
the ratio of the volumes of the first chambers in a dual chamber structure,
Figure QLYQS_22
the volume ratio of the second chamber which is a dual chamber structure,
Figure QLYQS_23
first chamber of double-chamber structureIs used for the diffusion coefficient of (a),
Figure QLYQS_24
diffusion coefficient of the second chamber which is a dual chamber structure,
Figure QLYQS_25
the ratio of the volumes of the first chambers in a three-chamber structure,
Figure QLYQS_26
the volume ratio of the second chamber which is a three-chamber structure,
Figure QLYQS_27
the volume ratio of the third chamber which is a three-chamber structure,
Figure QLYQS_28
the diffusion coefficient of the first chamber being a three-chamber structure,
Figure QLYQS_29
the diffusion coefficient of the second chamber which is a three-chamber structure,
Figure QLYQS_30
the diffusion coefficient of the third chamber, which is a three-chamber structure;
IV, judging whether the voxel point is of a single-chamber structure, a double-chamber structure or a three-chamber structure according to the solving result of the step III;
v, if the voxel point is judged to be of a single-chamber structure in the step IV, the method is based on
Figure QLYQS_31
Judging the tissue type of the single-chamber structure; the tissue types include cells, blood vessels, and extracellular spaces; the single-chamber structure not comprising groupsThe volume ratio and diffusion coefficient of the weave type are set to 0,
if the voxel point is judged to be of a double-chamber structure in the step IV, the method is based on the following steps
Figure QLYQS_32
And->
Figure QLYQS_33
Judging the tissue types of the first chamber and the second chamber of the double-chamber structure; the tissue types include cells, blood vessels, and extracellular spaces; the volume ratio and diffusion coefficient of the tissue type not contained in the dual chamber structure are set to 0,
if the voxel point is judged to be of a three-chamber structure in the step IV, the method is based on
Figure QLYQS_34
、/>
Figure QLYQS_35
And->
Figure QLYQS_36
Judging the tissue types of the first chamber, the second chamber and the third chamber of the three-chamber structure; the tissue types include cells, blood vessels, and extracellular spaces;
and VI, repeating the steps III to V to analyze other voxel points until all voxel points are analyzed.
2. The non-invasive measurement method of microstructure of biological tissue according to claim 1, wherein in the step iv, the voxel point is determined to be a single-chamber structure, a double-chamber structure or a three-chamber structure according to the result of the solving in the step iii, specifically:
if it is
Figure QLYQS_37
And is also provided with
Figure QLYQS_38
Then the voxel point is a single-chamber structure;
if it is
Figure QLYQS_39
And is also provided with
Figure QLYQS_40
Figure QLYQS_41
Then the voxel point is a dual-chamber structure;
otherwise, the voxel point is in a three-chamber structure;
wherein the method comprises the steps of
Figure QLYQS_42
Is an empirical parameter.
3. The method for non-invasive measurement of biological tissue microstructure according to claim 1, wherein after step vi further comprises:
and reconstructing the magnetic resonance image according to any one or more of volume ratio of cells, volume ratio of blood vessels, volume ratio of extracellular space, diffusion coefficient of cells, diffusion coefficient of blood vessels and diffusion coefficient of extracellular space of each voxel point.
4. The non-invasive measurement method of biological tissue microstructure according to claim 1, wherein the solving method in step iii adopts constrained nonlinear optimization solution; wherein,,
the optimization formula of formula 1 is:
Figure QLYQS_43
Figure QLYQS_44
the optimization formula of formula 2 is:
Figure QLYQS_45
/>
Figure QLYQS_46
the optimization formula of formula 3 is:
Figure QLYQS_47
Figure QLYQS_48
5. the non-invasive measurement method of biological tissue microstructure according to claim 4, wherein the constrained nonlinear optimization solution employs lagrangian multiplier method.
6. The method for non-invasive measurement of biological tissue microstructure according to claim 1, wherein after step vi further comprises:
and VIII, calculating the cellulose trend distribution of the cells, the blood vessels and the extracellular space according to the diffusion coefficient of the cells, the diffusion coefficient of the blood vessels and the diffusion coefficient of the extracellular space of each voxel point.
7. The non-invasive measurement method of biological tissue microstructure according to claim 6, wherein the estimation uses a statistical method or a main diffusion direction-based tracking method.
CN202011515119.4A 2020-12-21 2020-12-21 Non-invasive measurement method for microstructure of biological tissue Active CN114646913B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202011515119.4A CN114646913B (en) 2020-12-21 2020-12-21 Non-invasive measurement method for microstructure of biological tissue

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202011515119.4A CN114646913B (en) 2020-12-21 2020-12-21 Non-invasive measurement method for microstructure of biological tissue

Publications (2)

Publication Number Publication Date
CN114646913A CN114646913A (en) 2022-06-21
CN114646913B true CN114646913B (en) 2023-06-02

Family

ID=81991413

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202011515119.4A Active CN114646913B (en) 2020-12-21 2020-12-21 Non-invasive measurement method for microstructure of biological tissue

Country Status (1)

Country Link
CN (1) CN114646913B (en)

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104274176A (en) * 2013-07-11 2015-01-14 韩鸿宾 Noninvasive measuring method for microstructure of brain tissue
CN105078456A (en) * 2015-02-15 2015-11-25 北京大学第三医院 Noninvasive measuring method of microstructure of biological tissue
CN105559829A (en) * 2016-01-29 2016-05-11 任冰冰 Ultrasonic diagnosis and imaging method thereof
CN105825508A (en) * 2016-03-17 2016-08-03 电子科技大学 Hydrocephalus auxiliary diagnosis method based on brain medical image segmentation
CN108020796A (en) * 2016-10-31 2018-05-11 西门子(深圳)磁共振有限公司 A kind of MR diffusion-weighted imaging method and apparatus
CN109730677A (en) * 2019-01-09 2019-05-10 王毅翔 Signal processing method, device and the storage medium of irrelevant movement imaging in voxel
CN109923426A (en) * 2016-11-09 2019-06-21 Cr发展公司 The method that diffusion-weighted magnetic resonance measurement is executed to sample
CN110811622A (en) * 2019-11-12 2020-02-21 北京大学 Individual structure connection brain atlas drawing method based on diffusion magnetic resonance imaging fiber bundle tracking technology
CN111932513A (en) * 2020-08-07 2020-11-13 深圳市妇幼保健院 Method and system for imaging three-dimensional image of fetal sulcus gyrus in ultrasonic image

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8593142B2 (en) * 2008-01-03 2013-11-26 The Johns Hopkins University Automated fiber tracking of human brain white matter using diffusion tensor imaging
US9404986B2 (en) * 2011-05-06 2016-08-02 The Regents Of The University Of California Measuring biological tissue parameters using diffusion magnetic resonance imaging
KR101754291B1 (en) * 2017-04-04 2017-07-06 이현섭 Medical image processing system and method for personalized brain disease diagnosis and status determination
WO2019232532A1 (en) * 2018-06-01 2019-12-05 New York University Characterizing prostate microstructure using water diffusion and nuclear magnetic resonance relaxation

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104274176A (en) * 2013-07-11 2015-01-14 韩鸿宾 Noninvasive measuring method for microstructure of brain tissue
CN105078456A (en) * 2015-02-15 2015-11-25 北京大学第三医院 Noninvasive measuring method of microstructure of biological tissue
CN105559829A (en) * 2016-01-29 2016-05-11 任冰冰 Ultrasonic diagnosis and imaging method thereof
CN105825508A (en) * 2016-03-17 2016-08-03 电子科技大学 Hydrocephalus auxiliary diagnosis method based on brain medical image segmentation
CN108020796A (en) * 2016-10-31 2018-05-11 西门子(深圳)磁共振有限公司 A kind of MR diffusion-weighted imaging method and apparatus
CN109923426A (en) * 2016-11-09 2019-06-21 Cr发展公司 The method that diffusion-weighted magnetic resonance measurement is executed to sample
CN109730677A (en) * 2019-01-09 2019-05-10 王毅翔 Signal processing method, device and the storage medium of irrelevant movement imaging in voxel
CN110811622A (en) * 2019-11-12 2020-02-21 北京大学 Individual structure connection brain atlas drawing method based on diffusion magnetic resonance imaging fiber bundle tracking technology
CN111932513A (en) * 2020-08-07 2020-11-13 深圳市妇幼保健院 Method and system for imaging three-dimensional image of fetal sulcus gyrus in ultrasonic image

Non-Patent Citations (5)

* Cited by examiner, † Cited by third party
Title
Tracking developmental changes in subcortical structures of the preterm brain using multi-modal MRI;A. Serag,et al.;《2011 IEEE International Symposium on Biomedical Imaging: From Nano to Macro, Chicago, IL, USA》;349-352 *
光、磁成像法探测脑胶质瘤微环境脑组织间隙结构及脑组织间液引流的变化;王彤 等;《中国微创外科杂志》;第20卷(第1期);46-51 *
应用磁共振成像技术定量测量活体大鼠脑细胞外间隙的扩散参数;韩鸿宾;《北京大学学报(医学版)》;第44卷(第05期);770-775 *
细胞微环境成像新方法与脑分区稳态的发现;韩鸿宾;《武警医学》;第27卷(第04期);325-328 *
脑微环境及其成像与检测技术;王伟 等;《中华老年心脑血管病杂志》;第18卷(第02期);211-214 *

Also Published As

Publication number Publication date
CN114646913A (en) 2022-06-21

Similar Documents

Publication Publication Date Title
Winter et al. Comparison of three multichannel transmit/receive radiofrequency coil configurations for anatomic and functional cardiac MRI at 7.0 T: implications for clinical imaging
CN106023194B (en) Amygdaloid nucleus spectral clustering dividing method based on tranquillization state function connects
CN105848578B (en) MR imaging apparatus and method
Chang et al. Assessment of left ventricular mass in hypertrophic cardiomyopathy by real-time three-dimensional echocardiography using single-beat capture image
US20070053554A1 (en) Display and analysis of multicotrast- weighted magnetic resonance images
WO2010116124A1 (en) Diffusion-weighted nuclear magnetic resonance imaging
Oshio et al. Interpretation of diffusion MR imaging data using a gamma distribution model
Matsuda et al. Imaging of a large collection of human embryo using a super-parallel MR microscope
Reiter et al. On the way to routine cardiac MRI at 7 Tesla-a pilot study on consecutive 84 examinations
CN109242866B (en) Automatic auxiliary breast tumor detection system based on diffusion magnetic resonance image
Ma et al. Experimental implementation of a new method of imaging anisotropic electric conductivities
Gorczewski et al. Reproducibility and consistency of evaluation techniques for HARDI data
CN114646913B (en) Non-invasive measurement method for microstructure of biological tissue
EP3497460B1 (en) Multi-dimensional spectroscopic nmr and mri using marginal distributions
Knight et al. A novel anthropomorphic flow phantom for the quantitative evaluation of prostate DCE-MRI acquisition techniques
Giovannetti et al. Sodium radiofrequency coils for magnetic resonance: From design to applications
KR102170977B1 (en) Brain metabolite network generation method using time varying function based on MRS
CN104274176A (en) Noninvasive measuring method for microstructure of brain tissue
CN102759723A (en) Method for generating magnetic resonance T2* image
Shusharina et al. Consistency of muscle fibers directionality in human thigh derived from diffusion-weighted MRI
Farzi et al. Assessing myocardial microstructure with biophysical models of diffusion MRI
CN114098696A (en) Magnetic resonance imaging apparatus, image processing apparatus, and image processing method
CN111598898A (en) Superpixel-based cardiac MRI image segmentation method applied to medical treatment and MRI equipment
Marshall et al. Application of kt-BLAST acceleration to reduce cardiac MR imaging time in healthy and infarcted mice
CN109498016A (en) A kind of magnetic resonance electrical characteristics tomograph imaging method

Legal Events

Date Code Title Description
PB01 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