CN102008308A - Multi-b value diffusion tensor imaging sampling method - Google Patents

Multi-b value diffusion tensor imaging sampling method Download PDF

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CN102008308A
CN102008308A CN 201010612331 CN201010612331A CN102008308A CN 102008308 A CN102008308 A CN 102008308A CN 201010612331 CN201010612331 CN 201010612331 CN 201010612331 A CN201010612331 A CN 201010612331A CN 102008308 A CN102008308 A CN 102008308A
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value
single sweep
under
signal intensity
noise ratio
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CN102008308B (en
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刘伟
吴垠
刘新
郑海荣
邹超
戴睿彬
潘艳丽
张娜
谢国喜
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Shanghai United Imaging Healthcare Co Ltd
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Shenzhen Institute of Advanced Technology of CAS
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Abstract

The invention relates to a multi-b value diffusion tensor imaging sampling method, which comprises the following steps: carrying out single-scanning on the whole visual field under a first b value, sampling to obtain the single-scanning signal-to-noise ratio under the first b value and the single-scanning signal strength under the first b value; obtain the number of multi-scanning under the first b value according to the single-scanning signal-to-noise ratio under the first b value and the designated multi-scanning signal-to-noise ratio under the first b value; calculating to obtain the single-scanning signal-to-noise ratio under a second b value according to the single-scanning signal-to-noise ratio under the first b value and the single-scanning signal strength under the first b value; and calculating to obtain the number of the multi-scanning under the second b value according to the single-scanning signal-to-noise ratio under the second b value and the designated multi-scanning signal-to-noise ratio under the second b value. The multi-b value diffusion tensor imaging sampling method can select the number of repeated scanning which is actually required by various b values in an adaptive manner by implementing the single pre-scanning on the first b value and referring to the relationship followed by the signal-to-noise ratios of the different b values, further reduce the total number of sampling, greatly reduce the sampling time and improve the diffusion tensor imaging speed.

Description

Many b value dispersion tensor imaging method of samplings
[technical field]
The present invention relates to the dispersion tensor imaging, relate in particular to a kind of many b value dispersion tensor imaging method of samplings.
[background technology]
Diffusing phenomenon relates to the Brownian movement of molecule in the fluid, and the size of diffusing capacity is represented by dispersion coefficient.In the liquid of homogeneity, dispersion coefficient is identical on all directions, that is to say under 3-D view, and disperse process should be a ball-type; But in bio-tissue, the dispersion coefficient on the different directions is different, and for example moisture is in bigger along the suffered disperse restriction of the direction of aixs cylinder perpendicular to the direction ratio of aixs cylinder at myelinated nerve fiber, and what disperse process presented is spheroid shape.For each voxel in the imaging region, the disperse motor process of hydrone can be considered as a spheroid.The disperse motor process of hydrone can be represented with a dispersion tensor.
The dispersion tensor imaging is the specific form of NMR (Nuclear Magnetic Resonance)-imaging, is to develop new mr imaging technique rapidly in recent years.The dispersion tensor imaging technique is to utilize the disperse anisotropy of hydrone to carry out imaging, can provide disease condition at cell and molecular level from the integrity of the field evaluation of tissue structure of microcosmic, is an important component part of functional mri.Represent the disperse factor with b in the dispersion tensor imaging, the size of b depends on the waveform of the disperse gradient that applies.The size of b value has influence on the process of disperse.The b value is big more, and disperse is big more, and the signal to noise ratio of signal is just more little.The dispersion tensor imaging in actual applications, the common single index Changing Pattern that comes the match disperse process to be followed by a plurality of b values.In order to satisfy signal to noise ratio, traditional way scans to improve signal to noise ratio by all b values being adopted same number of repetition.Thereby cause the overlong time of sampling, influence the speed of dispersion tensor imaging.
[summary of the invention]
Based on this, be necessary to provide a kind of many b value dispersion tensor imaging method of samplings that can improve the dispersion tensor image taking speed.
A kind of many b value dispersion tensor imaging method of samplings may further comprise the steps: single sweep operation whole visual field under a b value, sampling obtain the following single sweep operation noise of a b value following single sweep signal intensity of a b value when; According to a described b value down the when specified b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the b value repeatedly scanning times; Calculate single sweep operation signal to noise ratio under the 2nd b value according to single sweep signal intensity under the when described b value of single sweep operation noise under the described b value; According to described the 2nd b value down when specified the 2nd b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the 2nd b value repeatedly scanning times.
In preferred embodiment, according to a described b value down the when specified b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the b value repeatedly that the formula of scanning times is:
SNR 1 1 = SNR N 1 N 1
Wherein, SNR 1Be single sweep operation signal to noise ratio under the described b value, SNR N1For a described b value repeatedly scans down signal to noise ratio, N1 is a scanning times repeatedly under the described b value.
In preferred embodiment, according to a described b value down the when described b value of single sweep operation noise down single sweep signal intensity calculate that single sweep operation signal to noise ratio step comprises the steps: to descend single sweep signal intensity to calculate single sweep signal intensity under the 2nd b value according to a described b value under the 2nd b value; Relation according to single sweep signal intensity under single sweep signal intensity under the described b value and described the 2nd b value calculates single sweep operation signal to noise ratio under described the 2nd b value.
In preferred embodiment, the formula that calculates single sweep signal intensity under the 2nd b value according to single sweep signal intensity under the described b value is:
ln S 1 - ln S 0 ln S 2 - ln S 0 = - b 1 - b 2
Wherein, b 1Be a described b value, b 2Be described the 2nd b value, S 1Be single sweep signal intensity under the described b value, S 2Be single sweep signal intensity under described the 2nd b value, S 0Signal intensity when not having the disperse gradient.
In preferred embodiment, according to a described b value down the relation of single sweep signal intensity and described the 2nd b value time single sweep signal intensity calculate under the described b value single sweep operation signal to noise ratio and described the 2nd b value and descend the formula of the relation between the single sweep operation signal to noise ratio to be:
S 1 S 2 = SNR 1 SNR 2
Wherein, S 1Be single sweep signal intensity under the described b value, S 2Be single sweep signal intensity under described the 2nd b value, SNR 1Be single sweep operation signal to noise ratio under the described b value, SNR 2Be single sweep operation signal to noise ratio under described the 2nd b value.
In preferred embodiment, according to described the 2nd b value down when specified the 2nd b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the 2nd b value repeatedly that the formula of scanning times is:
SNR 2 1 = SNR N 2 N 2
Wherein, SNR 2Be single sweep operation signal to noise ratio under described the 2nd b value, SNR N2For described the 2nd b value repeatedly scans down signal to noise ratio, N2 is a scanning times repeatedly under described the 2nd b value.
In preferred embodiment, the described b value fitting formula of single sweep signal intensity down is:
S 1 = S 0 e - b 1 D
Wherein, S 1Be single sweep signal intensity under the described b value, S 0Signal intensity when not having the disperse gradient, b 1Be a described b value, D is a dispersion coefficient.
In preferred embodiment, described the 2nd b value fitting formula of single sweep signal intensity down is:
S 2 = S 0 e - b 2 D
Wherein, S 2Be single sweep signal intensity under described the 2nd b value, S 0Signal intensity when not having the disperse gradient, b 2Be described the 2nd b value, D is a dispersion coefficient.
Above-mentioned many b value dispersion tensor imaging method of samplings, by the relation that the signal to noise ratio of b value enforcement single prescan and different b values is followed, just can be adaptive the multiple scanning number of times of selected each b value actual needs, thereby reduced total sampling number, greatly reduce the time of sampling, improved the speed of dispersion tensor imaging.
[description of drawings]
Fig. 1 is the flow chart of the many b value dispersion tensor imaging method of samplings among the embodiment;
Fig. 2 is for calculating the flow chart of single sweep operation signal to noise ratio under the 2nd b value according to single sweep signal intensity under the when described b value of single sweep operation noise under the described b value in many b value dispersion tensor imaging method of samplings shown in Figure 1.
[specific embodiment]
Describe below in conjunction with accompanying drawing and concrete embodiment.
As shown in Figure 1, a kind of many b value dispersion tensor imaging method of samplings may further comprise the steps:
S100, single sweep operation whole visual field under a b value, sampling obtains the following single sweep operation noise of a b value following single sweep signal intensity of a b value when.The b value is the disperse factor.The visual field is meant with the region-of-interest to be the center, the zone that coil can scan, for example, focus zone, internal organs zone or the like.During sampling, the b value is fixed on the value, coil carries out single sweep operation to whole visual field then, obtains single sweep signal intensity under the b value.
S200, according to a b value down the when specified b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the b value repeatedly scanning times.According to a described b value down the when specified b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the b value repeatedly that the formula of scanning times is:
SNR 1 1 = SNR N 1 N 1
Wherein, SNR 1Be single sweep operation signal to noise ratio under the described b value, SNR N1For a described b value repeatedly scans down signal to noise ratio, N1 is a scanning times repeatedly under the described b value.
S300, according to a b value down the single sweep operation noise when a b value time single sweep signal intensity calculate single sweep operation signal to noise ratio under the 2nd b value.In the present embodiment, a b value b 1Be 500 seconds/every square millimeter, the 2nd b value b 2It is 750 seconds/every square millimeter.As shown in Figure 2, step S300 comprises the steps.
S310 calculates single sweep signal intensity under the 2nd b value according to single sweep signal intensity under the b value.Because the process of disperse is exponential damping, the fitting formula of single sweep signal intensity is under the b value,
S 1 = S 0 e - b 1 D
Wherein, S 1Be single sweep signal intensity under the described b value, S 0Signal intensity when not having the disperse gradient, b 1Be a described b value, D is a dispersion coefficient.In like manner, the fitting formula of single sweep signal intensity is under the 2nd b value:
S 2 = S 0 e - b 2 D
Wherein, S 2Be single sweep signal intensity under the 2nd b value, S 0Signal intensity when not having the disperse gradient, b 2Be the 2nd b value, D is a dispersion coefficient.The formula that calculates single sweep signal intensity under the 2nd b value according to single sweep signal intensity under the b value is:
ln S 1 - ln S 0 ln S 2 - ln S 0 = - b 1 - b 2
Wherein, b 1Be a b value, b 2Be the 2nd b value, S 1Be single sweep signal intensity under the b value, S 2Be single sweep signal intensity under the 2nd b value, S 0Signal intensity when not having the disperse gradient.
S320 descends the relation of single sweep signal intensity to calculate single sweep operation signal to noise ratio under the 2nd b value according to following single sweep signal intensity of a b value and the 2nd b value.The formula that descends the relation of single sweep signal intensity under single sweep signal intensity and the 2nd b value to calculate the relation between the single sweep operation signal to noise ratio under the 2nd b value according to a b value is:
S 1 S 2 = SNR 1 SNR 2
Wherein, S 1Be single sweep signal intensity under the b value, S 2Be single sweep signal intensity under the 2nd b value, SNR 1Be single sweep operation signal to noise ratio under the b value, SNR 2It is single sweep operation signal to noise ratio under the 2nd b value.
S400, according to the 2nd b value down when specified the 2nd b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the 2nd b value repeatedly scanning times.According to the 2nd b value down when specified the 2nd b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the 2nd b value repeatedly that the formula of scanning times is:
SNR 2 1 = SNR N 2 N 2
Wherein, SNR 2Be single sweep operation signal to noise ratio under described the 2nd b value, SNR N2For described the 2nd b value repeatedly scans down signal to noise ratio, N2 is a scanning times repeatedly under described the 2nd b value.
Above-mentioned many b value dispersion tensor imaging method of samplings, by the relation that the signal to noise ratio of b value enforcement single prescan and different b values is followed, just can be adaptive the multiple scanning number of times of selected each b value actual needs, thereby reduced total sampling number, greatly reduce the time of sampling, improved the speed of dispersion tensor imaging.
The above embodiment has only expressed several embodiment of the present invention, and it describes comparatively concrete and detailed, but can not therefore be interpreted as the restriction to claim of the present invention.Should be pointed out that for the person of ordinary skill of the art without departing from the inventive concept of the premise, can also make some distortion and improvement, these all belong to protection scope of the present invention.Therefore, the protection domain of patent of the present invention should be as the criterion with claims.

Claims (8)

1. the dispersion tensor of b value more than kind imaging method of sampling may further comprise the steps:
Single sweep operation whole visual field under a b value, sampling obtain the following single sweep operation noise of a b value following single sweep signal intensity of a b value when;
According to a described b value down the when specified b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the b value repeatedly scanning times;
Calculate single sweep operation signal to noise ratio under the 2nd b value according to single sweep signal intensity under the when described b value of single sweep operation noise under the described b value;
According to described the 2nd b value down when specified the 2nd b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the 2nd b value repeatedly scanning times.
2. many b value dispersion tensor imaging method of samplings according to claim 1 is characterized in that, according to a described b value down the when specified b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the b value repeatedly that the formula of scanning times is:
SNR 1 1 = SNR N 1 N 1
Wherein, SNR 1Be single sweep operation signal to noise ratio under the described b value, SNR N1For a described b value repeatedly scans down signal to noise ratio, N1 is a scanning times repeatedly under the described b value.
3. many b value dispersion tensor imaging method of samplings according to claim 1, it is characterized in that, according to a described b value down the when described b value of single sweep operation noise time single sweep signal intensity calculate that single sweep operation signal to noise ratio step comprises the steps: under the 2nd b value
Calculate single sweep signal intensity under the 2nd b value according to single sweep signal intensity under the described b value;
Relation according to single sweep signal intensity under single sweep signal intensity under the described b value and described the 2nd b value calculates single sweep operation signal to noise ratio under described the 2nd b value.
4. many b value dispersion tensor imaging method of samplings according to claim 3 is characterized in that, the formula that calculates single sweep signal intensity under the 2nd b value according to single sweep signal intensity under the described b value is:
ln S 1 - ln S 0 ln S 2 - ln S 0 = - b 1 - b 2
Wherein, b 1Be a described b value, b 2Be described the 2nd b value, S 1Be single sweep signal intensity under the described b value, S 2Be single sweep signal intensity under described the 2nd b value, S 0Signal intensity when not having the disperse gradient.
5. many b value dispersion tensor imaging method of samplings according to claim 3, it is characterized in that the formula that descends the relation of single sweep signal intensity under single sweep signal intensity and described the 2nd b value to calculate the relation between the single sweep operation signal to noise ratio under described the 2nd b value according to a described b value is:
S 1 S 2 = SNR 1 SNR 2
Wherein, S 1Be single sweep signal intensity under the described b value, S 2Be single sweep signal intensity under described the 2nd b value, SNR 1Be single sweep operation signal to noise ratio under the described b value, SNR 2Be single sweep operation signal to noise ratio under described the 2nd b value.
6. many b value dispersion tensor imaging method of samplings according to claim 1 is characterized in that, according to described the 2nd b value down when specified the 2nd b value of single sweep operation noise time repeatedly scan signal-to-noise ratio computation and obtain under the 2nd b value repeatedly that the formula of scanning times is:
SNR 2 1 = SNR N 2 N 2
Wherein, SNR 2Be single sweep operation signal to noise ratio under described the 2nd b value, SNR N2For described the 2nd b value repeatedly scans down signal to noise ratio, N2 is a scanning times repeatedly under described the 2nd b value.
7. many b value dispersion tensor imaging method of samplings according to claim 1 is characterized in that, the described b value fitting formula of single sweep signal intensity down is:
S 1 = S 0 e - b 1 D
Wherein, S 1Be single sweep signal intensity under the described b value, S 0Signal intensity when not having the disperse gradient, b 1Be a described b value, D is a dispersion coefficient.
8. many b value dispersion tensor imaging method of samplings according to claim 1 is characterized in that, described the 2nd b value fitting formula of single sweep signal intensity down is:
S 2 = S 0 e - b 2 D
Wherein, S 2Be single sweep signal intensity under described the 2nd b value, S 0Signal intensity when not having the disperse gradient, b 2Be described the 2nd b value, D is a dispersion coefficient.
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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103892831A (en) * 2012-12-26 2014-07-02 上海联影医疗科技有限公司 Magnetic resonance imaging method and magnetic resonance system
CN103919552A (en) * 2013-01-14 2014-07-16 张剑戈 Water dispersion movement visualizing method
CN104042216A (en) * 2014-07-01 2014-09-17 中国科学院武汉物理与数学研究所 Fast thin layer magnetic resonance imaging method based on pre-scanning and non-uniform sampling
CN105807244A (en) * 2014-12-30 2016-07-27 西门子(中国)有限公司 Data acquisition method for dispersion models of magnetic resonance imaging system and magnetic resonance imaging method thereof

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6670812B1 (en) * 2002-09-13 2003-12-30 Ge Medical Systems Global Technology, Llc B-value calculation and correction using a linear segment gradient waveform model
US20050237057A1 (en) * 2004-04-13 2005-10-27 Porter David A Movement-corrected multi-shot method for diffusion-weighted imaging in magnetic resonance tomography
CN101627910A (en) * 2008-07-17 2010-01-20 株式会社东芝 Magnetic resonance imaging apparatus and magnetic resonance imaging method

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6670812B1 (en) * 2002-09-13 2003-12-30 Ge Medical Systems Global Technology, Llc B-value calculation and correction using a linear segment gradient waveform model
US20050237057A1 (en) * 2004-04-13 2005-10-27 Porter David A Movement-corrected multi-shot method for diffusion-weighted imaging in magnetic resonance tomography
CN101627910A (en) * 2008-07-17 2010-01-20 株式会社东芝 Magnetic resonance imaging apparatus and magnetic resonance imaging method

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
《生物医学工程与临床》 20091130 张翼等 《PM滤波方法对提高不同b值弥散张量成像图像质量的应用研究》 506-509 第13卷, 第6期 2 *

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103892831A (en) * 2012-12-26 2014-07-02 上海联影医疗科技有限公司 Magnetic resonance imaging method and magnetic resonance system
CN103919552A (en) * 2013-01-14 2014-07-16 张剑戈 Water dispersion movement visualizing method
CN104042216A (en) * 2014-07-01 2014-09-17 中国科学院武汉物理与数学研究所 Fast thin layer magnetic resonance imaging method based on pre-scanning and non-uniform sampling
CN104042216B (en) * 2014-07-01 2015-12-30 中国科学院武汉物理与数学研究所 A kind of thin layer rapid magnetic resonance imaging method based on prescan and nonuniform sampling
CN105807244A (en) * 2014-12-30 2016-07-27 西门子(中国)有限公司 Data acquisition method for dispersion models of magnetic resonance imaging system and magnetic resonance imaging method thereof
US10132901B2 (en) 2014-12-30 2018-11-20 Siemens Healthcare Gmbh Diffusion model data acquisition method for magnetic resonance imaging system, and magnetic resonance imaging method
CN105807244B (en) * 2014-12-30 2019-03-22 西门子(中国)有限公司 The collecting method and MR imaging method of the dispersion model of magnetic resonance imaging system

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