CN113156350B - Non-invasive light opaque micron-sized living tissue magnetic resonance tomography method and system - Google Patents
Non-invasive light opaque micron-sized living tissue magnetic resonance tomography method and system Download PDFInfo
- Publication number
- CN113156350B CN113156350B CN202110318850.6A CN202110318850A CN113156350B CN 113156350 B CN113156350 B CN 113156350B CN 202110318850 A CN202110318850 A CN 202110318850A CN 113156350 B CN113156350 B CN 113156350B
- Authority
- CN
- China
- Prior art keywords
- imaging
- micron
- resolution
- scale
- magnetic field
- 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
Links
- 238000003325 tomography Methods 0.000 title claims abstract description 60
- 238000000034 method Methods 0.000 title claims abstract description 47
- 238000003384 imaging method Methods 0.000 claims abstract description 241
- 230000003287 optical effect Effects 0.000 claims abstract description 21
- 230000005672 electromagnetic field Effects 0.000 claims abstract description 13
- 230000005284 excitation Effects 0.000 claims abstract description 6
- 238000006243 chemical reaction Methods 0.000 claims description 3
- 210000004895 subcellular structure Anatomy 0.000 abstract description 5
- 210000001519 tissue Anatomy 0.000 description 45
- 210000004027 cell Anatomy 0.000 description 11
- 238000005516 engineering process Methods 0.000 description 9
- CVOFKRWYWCSDMA-UHFFFAOYSA-N 2-chloro-n-(2,6-diethylphenyl)-n-(methoxymethyl)acetamide;2,6-dinitro-n,n-dipropyl-4-(trifluoromethyl)aniline Chemical compound CCC1=CC=CC(CC)=C1N(COC)C(=O)CCl.CCCN(CCC)C1=C([N+]([O-])=O)C=C(C(F)(F)F)C=C1[N+]([O-])=O CVOFKRWYWCSDMA-UHFFFAOYSA-N 0.000 description 7
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 description 4
- 241000699670 Mus sp. Species 0.000 description 4
- 238000013461 design Methods 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 229910052739 hydrogen Inorganic materials 0.000 description 4
- 239000001257 hydrogen Substances 0.000 description 4
- 238000002595 magnetic resonance imaging Methods 0.000 description 4
- 230000003068 static effect Effects 0.000 description 4
- 241000699666 Mus <mouse, genus> Species 0.000 description 3
- 241000700159 Rattus Species 0.000 description 3
- 238000004364 calculation method Methods 0.000 description 3
- 230000007812 deficiency Effects 0.000 description 3
- 238000012634 optical imaging Methods 0.000 description 3
- 238000002604 ultrasonography Methods 0.000 description 3
- 238000012285 ultrasound imaging Methods 0.000 description 3
- 210000004556 brain Anatomy 0.000 description 2
- 238000013170 computed tomography imaging Methods 0.000 description 2
- 235000013601 eggs Nutrition 0.000 description 2
- 238000001727 in vivo Methods 0.000 description 2
- 238000011503 in vivo imaging Methods 0.000 description 2
- 238000009206 nuclear medicine Methods 0.000 description 2
- 230000000149 penetrating effect Effects 0.000 description 2
- 210000004872 soft tissue Anatomy 0.000 description 2
- DGAQECJNVWCQMB-PUAWFVPOSA-M Ilexoside XXIX Chemical compound C[C@@H]1CC[C@@]2(CC[C@@]3(C(=CC[C@H]4[C@]3(CC[C@@H]5[C@@]4(CC[C@@H](C5(C)C)OS(=O)(=O)[O-])C)C)[C@@H]2[C@]1(C)O)C)C(=O)O[C@H]6[C@@H]([C@H]([C@@H]([C@H](O6)CO)O)O)O.[Na+] DGAQECJNVWCQMB-PUAWFVPOSA-M 0.000 description 1
- 241001465754 Metazoa Species 0.000 description 1
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 1
- 241000255588 Tephritidae Species 0.000 description 1
- 238000004458 analytical method Methods 0.000 description 1
- 210000003850 cellular structure Anatomy 0.000 description 1
- 230000003750 conditioning effect Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 210000005061 intracellular organelle Anatomy 0.000 description 1
- 230000005865 ionizing radiation Effects 0.000 description 1
- 210000000056 organ Anatomy 0.000 description 1
- 230000035515 penetration Effects 0.000 description 1
- 229910052698 phosphorus Inorganic materials 0.000 description 1
- 239000011574 phosphorus Substances 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- 239000011734 sodium Substances 0.000 description 1
- 229910052708 sodium Inorganic materials 0.000 description 1
- 210000001082 somatic cell Anatomy 0.000 description 1
- 230000000472 traumatic effect Effects 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
- G01R33/44—Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
- G01R33/48—NMR imaging systems
- G01R33/4808—Multimodal MR, e.g. MR combined with positron emission tomography [PET], MR combined with ultrasound or MR combined with computed tomography [CT]
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B5/00—Measuring for diagnostic purposes; Identification of persons
- A61B5/05—Detecting, measuring or recording for diagnosis by means of electric currents or magnetic fields; Measuring using microwaves or radio waves
- A61B5/055—Detecting, 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
Landscapes
- Health & Medical Sciences (AREA)
- Physics & Mathematics (AREA)
- Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
- Life Sciences & Earth Sciences (AREA)
- High Energy & Nuclear Physics (AREA)
- Engineering & Computer Science (AREA)
- General Health & Medical Sciences (AREA)
- Radiology & Medical Imaging (AREA)
- General Physics & Mathematics (AREA)
- Heart & Thoracic Surgery (AREA)
- Theoretical Computer Science (AREA)
- Pulmonology (AREA)
- Biophysics (AREA)
- Pathology (AREA)
- Biomedical Technology (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Medical Informatics (AREA)
- Molecular Biology (AREA)
- Surgery (AREA)
- Animal Behavior & Ethology (AREA)
- Public Health (AREA)
- Veterinary Medicine (AREA)
- Magnetic Resonance Imaging Apparatus (AREA)
Abstract
一种无创光不透明微米级活体组织磁共振断层成像方法,通过控制如下三项条件实现:A.采用均匀单一方向的超高磁场强度的主磁场,施加于活体生物组织;B.在主磁场基础上,对X、Y、Z三个方向,分别采用强度为10000mT/m以上强度梯度分布的叠加梯度磁场,对具有自旋角动量的元素进行空间编码,使不同空间位置的元素的自旋频率不同;C.采用与主磁场相垂直的射频电磁场,对成像对象进行射频电磁场激励,并拾取激励撤销后,成像对象发射的能级转换射频信号,对射频信号进行重建解码,得到断层成像。能够实现空间分辨率达到1微米尺度的、具备亚细胞结构分辨能力的无创活体组织断层成像。
A non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method is realized by controlling the following three conditions: A. A uniform and single-direction main magnetic field with ultra-high magnetic field strength is applied to the living biological tissue; B. On the basis of the main magnetic field Above, for the three directions of X, Y, and Z, the superimposed gradient magnetic field with the intensity gradient distribution of more than 10000 mT/m is used to spatially encode the elements with spin angular momentum, so that the spin frequencies of elements in different spatial positions are Different; C. The radio frequency electromagnetic field perpendicular to the main magnetic field is used to excite the imaging object with the radio frequency electromagnetic field, and after the excitation is withdrawn, the energy level converted radio frequency signal emitted by the imaging object is picked up, and the radio frequency signal is reconstructed and decoded to obtain a tomographic image. It can realize non-invasive living tissue tomography with a spatial resolution of 1 micron scale and the ability to resolve subcellular structures.
Description
技术领域technical field
本发明涉及生物医学活体成像技术领域,特别是涉及一种无创光不透明微米级活体组织磁共振断层成像方法及其系统。The invention relates to the technical field of biomedical in vivo imaging, in particular to a non-invasive optical opaque micron-scale in vivo magnetic resonance tomography imaging method and a system thereof.
背景技术Background technique
在生物医学成像领域,针对生物组织和/或细胞,主要的成像技术有光学成像、超声成像、X射线成像(包含X射线CT)、核医学成像、光声成像、电磁微波成像、磁共振成像等。In the field of biomedical imaging, for biological tissues and/or cells, the main imaging technologies are optical imaging, ultrasound imaging, X-ray imaging (including X-ray CT), nuclear medicine imaging, photoacoustic imaging, electromagnetic microwave imaging, magnetic resonance imaging Wait.
采用光学成像如激光共聚焦成像等技术,可以观测到亚细胞结构(即细胞内的细胞器),但是其观测对象必须是已经脱离了非透明组织的独立的单个细胞。对于光不透明的活体生物组织,由于光无法穿透成像对象,采用光学成像手段无法实现活体组织内的单个的细胞成像,而绝大部分情况下,生物活体组织都呈现非光透明的特性,比如一般情况下光无法穿透大小鼠的躯体,更无法穿透人体。Using optical imaging techniques such as confocal laser imaging, subcellular structures (ie, intracellular organelles) can be observed, but the observed objects must be independent single cells that have been separated from non-transparent tissues. For optically opaque living biological tissue, since light cannot penetrate the imaging object, it is impossible to use optical imaging methods to image individual cells in the living tissue. Under normal circumstances, light cannot penetrate the bodies of rats and mice, let alone the human body.
超声成像,虽然具备一定的穿透力,能够穿透达几十厘米甚至更大厚度的组织,但是由于受到超声波发射波束、超声探测器等种种限制,无法观测到活体组织中的每个单细胞。现在正在发展的超高频超声成像,虽然能达到低于1毫米的分辨率,但是仍达不到1微米分辨率水平的活体成像;而且其穿透能力,随着频率的增高急剧下降,目前,采用超声成像的技术手段,无法实现大小鼠活体组织的1微米分辨率水平的断层成像。Although ultrasonic imaging has a certain penetrating power and can penetrate tissues with a thickness of tens of centimeters or more, due to various limitations such as ultrasonic emission beams and ultrasonic detectors, it is impossible to observe every single cell in living tissue. . The ultra-high frequency ultrasound imaging currently under development, although it can achieve a resolution of less than 1 mm, still cannot achieve in vivo imaging at the level of 1 micron resolution; and its penetrating ability declines sharply with the increase of frequency. , the use of ultrasonic imaging techniques cannot achieve tomographic imaging at the 1-micron resolution level of living tissue in rats and mice.
X射线成像,包括X射线投照成像以及X射线断层成像(X射线CT)两种,现有X射线CT技术能够达到1毫米左右的分辨率,但是无法达到1微米的分辨率。另外,X射线的软组织分辨能力比较差,也无法实现大小鼠活体组织的1微米分辨率水平的断层成像。X-ray imaging includes two types of X-ray projection imaging and X-ray tomography (X-ray CT). The existing X-ray CT technology can achieve a resolution of about 1 mm, but cannot achieve a resolution of 1 micron. In addition, the soft tissue resolution of X-rays is relatively poor, and it is impossible to achieve tomographic imaging at the 1-micron resolution level of living tissue in rats and mice.
核医学影像,其优点是灵敏度比较高,但是其成像空间分辨率较差,低于CT成像的空间分辨率,与1微米分辨率水平的断层成像要求的空间分辨率,相差甚远。Nuclear medicine imaging has the advantage of relatively high sensitivity, but its imaging spatial resolution is poor, which is lower than the spatial resolution of CT imaging, and is far from the spatial resolution required for tomography at the 1-micron resolution level.
光声成像以光为激励源激发组织产生超声,通过检测超声实现成像,其分辨率本质上不会超过超声成像的分辨率。Photoacoustic imaging uses light as the excitation source to excite tissue to generate ultrasound, and realizes imaging by detecting ultrasound, and its resolution does not essentially exceed that of ultrasound imaging.
电磁微波成像的优点是无电离辐射,但是其分辨率较差,往往在厘米的量级甚至更粗糙,目前还无法形成高分辨率的实用化的系统。The advantage of electromagnetic microwave imaging is that there is no ionizing radiation, but its resolution is poor, often in the order of centimeters or even rougher, and a high-resolution practical system cannot be formed at present.
磁共振成像具有穿透力强、软组织成像分辨率高的优点,但现有的磁共振成像系统分辨率无法实现活体内1微米分辨率水平的断层成像,分辨率最高的小动物磁共振成像系统最多能达到20~40um的空间分辨率,在这个分辨率下会出现多个细胞在图像上呈现为一个像素点的情况。Magnetic resonance imaging has the advantages of strong penetration and high resolution of soft tissue imaging, but the resolution of the existing magnetic resonance imaging system cannot achieve tomography at the level of 1 micron resolution in vivo, and the highest resolution small animal magnetic resonance imaging system The spatial resolution of 20-40um can be achieved at most, and at this resolution, multiple cells will appear as one pixel on the image.
总之,目前为止,当今现有的生物医学成像技术手段都还没有能够在活体层面上无创实现1微米分辨率水平的断层成像,均无法在活体上无创地观察和测量得到单个细胞的形态和功能。In a word, so far, the existing biomedical imaging techniques have not been able to non-invasively achieve tomography at the level of 1 micron resolution on the living body, and none of them can non-invasively observe and measure the morphology and function of individual cells on the living body. .
因此,针对现有技术不足,提供一种无创光不透明微米级活体组织磁共振断层成像方法以克服现有技术不足甚为必要。Therefore, in view of the deficiencies of the prior art, it is necessary to provide a non-invasive optical opaque micron-scale living tissue magnetic resonance tomography imaging method to overcome the deficiencies of the prior art.
发明内容SUMMARY OF THE INVENTION
本发明的目的在于避免现有技术的不足之处而提供一种无创光不透明微米级活体组织磁共振断层成像方法,能够在活体组织层面上无创实现1微米级别分辨率水平的断层成像。The purpose of the present invention is to avoid the deficiencies of the prior art and provide a non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method, which can non-invasively achieve 1-micron-level tomography on the living tissue level.
本发明的目的通过以下技术措施实现。The object of the present invention is achieved by the following technical measures.
提供一种无创光不透明微米级活体组织磁共振断层成像方法,通过控制如下三项条件实现:A non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method is provided, which is realized by controlling the following three conditions:
A.采用均匀单一方向的超高磁场强度的主磁场,施加于作为成像对象的活体生物组织;A. The main magnetic field with a uniform and single-direction ultra-high magnetic field strength is applied to the living biological tissue as the imaging object;
B.在主磁场基础上,在1微米尺度成像区域按照成像空间分辨率为1微米尺度的成像标准施加梯度场,具体是:对X、Y、Z三个方向,分别采用强度为10000mT/m以上强度梯度分布的叠加梯度磁场,对具有自旋角动量的元素进行空间编码,使不同空间位置的元素的自旋频率不同;B. On the basis of the main magnetic field, a gradient field is applied in the 1-micron-scale imaging area according to the imaging standard with an imaging spatial resolution of 1-micron scale, specifically: for the three directions of X, Y, and Z, the intensity is 10000 mT/m respectively. The superimposed gradient magnetic field of the above intensity gradient distribution performs spatial encoding on the elements with spin angular momentum, so that the spin frequencies of elements in different spatial positions are different;
C.采用与主磁场相垂直的射频电磁场,对成像对象进行射频电磁场激励,并拾取激励撤销后,成像对象发射的能级转换射频信号,对射频信号进行重建解码,得到断层成像。C. Use the radio frequency electromagnetic field perpendicular to the main magnetic field to excite the imaging object with the radio frequency electromagnetic field, and pick up the energy level conversion radio frequency signal emitted by the imaging object after the excitation is cancelled, reconstruct and decode the radio frequency signal, and obtain the tomographic imaging.
优选的,上述无创光不透明微米级活体组织磁共振断层成像方法,A中,主磁场的磁场强度不低于9.4特斯拉。Preferably, in the above non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method, in A, the magnetic field strength of the main magnetic field is not lower than 9.4 Tesla.
优选的,上述无创光不透明微米级活体组织磁共振断层成像方法,B中,按照成像空间分辨率为1微米尺度的成像标准施加梯度场,具体为:Preferably, in the above non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method, in B, a gradient field is applied according to an imaging standard with an imaging spatial resolution of 1 micron, specifically:
在Z方向上,收窄选频带宽至20KHz以下,采用强度为10000mT/m至50000mT/m的叠加梯度磁场,实现分辨率为1微米尺度厚度的Z方向选层;In the Z direction, the frequency selection bandwidth is narrowed to below 20KHz, and the superimposed gradient magnetic field with the intensity of 10000mT/m to 50000mT/m is used to realize the layer selection in the Z direction with a resolution of 1 micron thickness;
在X方向上,采用强度为20000mT/m至50000mT/m的叠加梯度磁场,采用频率分辨率为0.8KHz至3.0KHz的接收谱仪,在X方向达到像素为1微米尺度的分辨率;In the X direction, a superimposed gradient magnetic field with an intensity of 20000mT/m to 50000mT/m is used, and a receiving spectrometer with a frequency resolution of 0.8KHz to 3.0KHz is used to achieve a resolution of 1 micron pixel in the X direction;
其中,谱仪的频率分辨率满足式(1):Among them, the frequency resolution of the spectrometer satisfies the formula (1):
Δf=γ*(Gx*Δx)……式(1);Δf=γ*(G x *Δx)... Formula (1);
式(1)中,Δf为谱仪的频率分辨率,γ为旋磁比,Gx为X方向上的叠加梯度磁场的梯度场强,Δx为在X方向达到像素分辨率的尺度;In formula (1), Δf is the frequency resolution of the spectrometer, γ is the gyromagnetic ratio, Gx is the gradient field strength of the superimposed gradient magnetic field in the X direction, and Δx is the scale that reaches the pixel resolution in the X direction;
在Y方向上,采用强度为10000mT/m至50000mT/m的叠加梯度磁场,控制Y方向上梯度打开时间,步长设定为4.7us至4.7*5us,实现分辨率为1微米尺度像素的相位编码;In the Y direction, a superimposed gradient magnetic field with an intensity of 10000mT/m to 50000mT/m is used to control the gradient opening time in the Y direction, and the step size is set to 4.7us to 4.7*5us to achieve a phase resolution of 1 micron-scale pixels. coding;
其中,Y方向上梯度打开时间满足式(2):Among them, the gradient opening time in the Y direction satisfies the formula (2):
式(2)中,Gy为Y方向上的叠加梯度磁场的梯度场强,Δy为在Y方向达到像素分辨率的尺度,Δy不大于1微米,为Y方向上梯度打开时间。In formula (2), G y is the gradient field strength of the superimposed gradient magnetic field in the Y direction, Δy is the scale that reaches the pixel resolution in the Y direction, Δy is not greater than 1 μm, Turns on time for the gradient in the Y direction.
优选的,上述无创光不透明微米级活体组织磁共振断层成像方法,B中,在X方向上,采用强度为20000mT/m的叠加梯度磁场,采用频率分辨率为852Hz的接收谱仪,在X方向达到像素为1微米的分辨率。Preferably, in the above non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method, in B, in the X direction, a superimposed gradient magnetic field with an intensity of 20,000 mT/m is used, and a receiving spectrometer with a frequency resolution of 852 Hz is used. A resolution of 1 micron pixel is achieved.
优选的,上述无创光不透明微米级活体组织磁共振断层成像方法,B中,在X方向上,采用强度为50000mT/m的叠加梯度磁场,采用频率分辨率为2.5KHz的接收谱仪,在X方向达到像素为1微米尺度的分辨率。Preferably, in the above non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method, in B, in the X direction, a superimposed gradient magnetic field with an intensity of 50,000 mT/m is used, and a receiving spectrometer with a frequency resolution of 2.5 KHz is used. Orientation achieves pixel resolution at 1 micron scale.
优选的,上述无创光不透明微米级活体组织磁共振断层成像方法,B中,Preferably, the above-mentioned non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method, in B,
在Y方向上,采用强度为10000mT/m的叠加梯度磁场,Y方向上梯度打开时间控制在2.35ms,步长设定为4.7us;或者In the Y direction, a superimposed gradient magnetic field with a strength of 10000mT/m is used, the gradient opening time in the Y direction is controlled at 2.35ms, and the step size is set at 4.7us; or
在Y方向上,采用强度为50000mT/m的叠加梯度磁场,Y方向上梯度打开时间控制在2.35ms,步长设定为4.7*5us。In the Y direction, a superimposed gradient magnetic field with an intensity of 50000 mT/m is used, the gradient opening time in the Y direction is controlled at 2.35 ms, and the step size is set at 4.7*5us.
优选的,上述无创光不透明微米级活体组织磁共振断层成像方法,针对整体成像对象,采用成像区域联变断层成像方法,所述成像区域联变断层成像方法是成像区域与成像分辨率联变动态调节进行断层成像;Preferably, the above-mentioned non-invasive optical opaque micron-scale living tissue magnetic resonance tomography imaging method adopts an imaging area co-transformation tomography imaging method for the overall imaging object. Conditioning for tomography;
断层成像范围为10±5cm,当需要的成像范围大时,采用Zoom out(缩小)模式成像;反之,当需要的成像范围小时,采用Zoom in(放大)模式成像;至少所选择的感兴趣区域作为1微米尺度成像区域并以1微米尺度成像区域的标准施加梯度场,感兴趣区域的成像空间分辨率为1微米尺度,且控制单张断层图像的数据大小的上限值在100kB-100MB之间。The tomographic imaging range is 10±5cm. When the required imaging range is large, the Zoom out (zoomed out) mode is used for imaging; on the contrary, when the required imaging range is small, the Zoom in (zoomed in) mode imaging is used; at least the selected area of interest is used for imaging. As a 1-micron-scale imaging area and applying a gradient field with the standard of a 1-micron-scale imaging area, the imaging spatial resolution of the region of interest is 1-micron scale, and the upper limit of the data size of a single tomographic image is controlled between 100kB-100MB between.
优选的,当成像范围大时,采用Zoom out模式成像,还利用Zoom out模式的成像结果获得初始感兴趣区域;Preferably, when the imaging range is large, the Zoom out mode is used for imaging, and the initial region of interest is obtained by using the imaging result of the Zoom out mode;
然后判断初始感兴趣区域是否满足1微米尺度成像条件,如果满足,则对初始感兴趣区域进行1微米尺度分辨率的断层成像;如果不满足,则将初始感兴趣区域划分为多个满足1微米尺度成像条件的子成像区域,对多个子成像区域分别进行1微米尺度分辨率的断层成像;Then judge whether the initial region of interest satisfies the 1-micron-scale imaging conditions, if so, perform tomographic imaging with a resolution of 1-micron scale on the initial region of interest; if not, divide the initial region of interest into multiple 1-micron-scale imaging Sub-imaging areas of scale imaging conditions, tomographic imaging with a resolution of 1 micron scale is performed on multiple sub-imaging areas respectively;
1微米尺度成像条件是:图像空间分辨率为1微米尺度成像得到的单张断层图像的数据大小的上限值在100kB-100MB之间;1-micron-scale imaging conditions are: the upper limit of the data size of a single tomographic image obtained by imaging at 1-micron scale is between 100kB-100MB;
1微米尺度分辨率的断层成像具体是按照成像空间分辨率为1微米尺度的成像标准施加梯度场,并进行成像。Specifically, the tomographic imaging with a resolution of 1 μm is to apply a gradient field and perform imaging according to the imaging standard with an imaging spatial resolution of 1 μm.
优选的,1微米尺度指0.1微米至2微米分辨率范围。Preferably, 1 micron scale refers to a resolution range of 0.1 micron to 2 microns.
优选的,上述无创光不透明微米级活体组织磁共振断层成像方法,条件C中采用的信号增强序列是:在下一个负90度射频脉冲之前添加正90度射频脉冲以缩短TR时间、降低T2信号的衰减、提高信噪比。Preferably, in the above non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method, the signal enhancement sequence used in condition C is: adding a positive 90-degree radio frequency pulse before the next negative 90-degree radio frequency pulse to shorten the TR time and reduce the T2 signal. Attenuate and improve the signal-to-noise ratio.
优选的,上述无创光不透明微米级活体组织磁共振断层成像方法,断层成像的范围为10±2cm。Preferably, in the above non-invasive optically opaque micron-scale living tissue magnetic resonance tomography method, the tomographic imaging range is 10±2 cm.
本发明的无创光不透明微米级活体组织磁共振断层成像方法,通过控制如下三项条件实现:A.采用均匀单一方向的超高磁场强度的主磁场,施加于活体生物组织;B.在主磁场基础上,对X、Y、Z三个方向,分别采用强度为10000mT/m以上强度梯度分布的叠加梯度磁场,对具有自旋角动量的元素进行空间编码,使不同空间位置的元素的自旋频率不同;C.采用与主磁场相垂直的射频电磁场,对成像对象进行射频电磁场激励,并拾取激励撤销后,成像对象发射的能级转换射频信号,对射频信号进行重建解码,得到断层成像。本发明能够在光不透明的活体组织层面上无创实现1微米级别分辨率水平的断层成像,能够实现空间分辨率达到1微米尺度的、具备亚细胞结构分辨能力的无创活体组织断层成像。解决了现有的生物医学成像技术手段无法实现的在活体组织层面无创实现1微米分辨率水平的断层成像的技术难题。The non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method of the present invention is realized by controlling the following three conditions: A. a uniform and single-direction main magnetic field with ultra-high magnetic field strength is applied to the living biological tissue; B. in the main magnetic field On the basis, for the three directions of X, Y and Z, the superimposed gradient magnetic field with the intensity gradient distribution of more than 10000 mT/m is respectively used to spatially encode the elements with spin angular momentum, so that the spins of elements in different spatial positions can be encoded. The frequencies are different; C. The radio frequency electromagnetic field perpendicular to the main magnetic field is used to excite the imaging object with the radio frequency electromagnetic field, and after the excitation is withdrawn, the energy level converted radio frequency signal emitted by the imaging object is picked up, and the radio frequency signal is reconstructed and decoded to obtain the tomographic image. The invention can non-invasively realize tomography at the level of 1 micron resolution on the level of optically opaque living tissue, and can realize non-invasive living tissue tomography with a spatial resolution of 1 micron and the ability to resolve subcellular structures. The technical problem of non-invasively realizing tomographic imaging at the level of 1 micron resolution at the living tissue level, which cannot be achieved by the existing biomedical imaging technology means, is solved.
说明书附图Instruction drawings
利用附图对本发明作进一步的说明,但附图中的内容不构成对本发明的任何限制。The present invention will be further described by using the accompanying drawings, but the content in the accompanying drawings does not constitute any limitation to the present invention.
图1是本发明一种无创光不透明微米级活体组织磁共振断层成像方法的信号增强序列时序图。1 is a sequence diagram of a signal enhancement sequence of a non-invasive optically opaque micron-scale living tissue magnetic resonance tomography method of the present invention.
具体实施方式Detailed ways
结合以下实施例对本发明作进一步说明。The present invention will be further described with reference to the following examples.
实施例1。Example 1.
一种无创光不透明微米级活体组织磁共振断层成像方法,通过控制如下A、B、C三项条件实现。A non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method is realized by controlling the following three conditions: A, B, and C.
A.采用均匀单一方向的超高磁场强度的主磁场,施加于活体生物组织。需要说明的是,本发明提到的超高磁场强度的主磁场,是指磁场强度不低于9.4特斯拉的主磁场,如可选9.4T、10.5T、16T等。超高磁场强度主磁场的实现,可以通过相关磁共振设备实现,该技术属于本领域公知技术,在此不再赘述。A. The main magnetic field with ultra-high magnetic field strength in a uniform single direction is applied to the living biological tissue. It should be noted that the main magnetic field with ultra-high magnetic field strength mentioned in the present invention refers to the main magnetic field with a magnetic field strength not lower than 9.4 Tesla, such as 9.4T, 10.5T, 16T and so on. The realization of the main magnetic field with the ultra-high magnetic field strength can be realized by the relevant magnetic resonance equipment, which belongs to the well-known technology in the art, and will not be repeated here.
本发明的微米级尺度是指成像的分辨率在1微米左右的分辨率,具体指指0.1微米至2微米分辨率范围,如1微米分辨率或者略小于1微米分辨率。活体生物组织内的含有的自旋角动量的元素,包括质子、磷元素、钠元素等。采用均匀单一方向的超高磁场强度的主磁场,可对活体生物组织内的含有的自旋角动量的元素进行自旋方向一致化处理。当生物组织处于强的外加磁场的作用下,具有自旋角动量的元素,其自旋角动量的矢量方向,将与外加磁场方向保持一致(或者180度反向)。A项条件的设计,是确保实现微米尺度分辨率断层成像的一个关键。The micron-scale scale of the present invention refers to the resolution of imaging at about 1 micron, and specifically refers to the resolution range of 0.1 micron to 2 microns, such as 1 micron resolution or slightly less than 1 micron resolution. Elements containing spin angular momentum in living biological tissues, including protons, phosphorus elements, sodium elements, etc. Using a main magnetic field with a uniform and single-direction ultra-high magnetic field strength, the spin direction alignment process can be performed on elements with spin angular momentum contained in living biological tissues. When biological tissue is under the action of a strong external magnetic field, the vector direction of the spin angular momentum of elements with spin angular momentum will be consistent with the direction of the external magnetic field (or 180 degrees opposite). The design of the condition of item A is a key to ensure the realization of micron-scale resolution tomography.
B.在主磁场基础上,当所要成像的目标区域需要实现1微米尺度断层成像时(此目标区域即为1微米尺度成像区域),按照成像空间分辨率为1微米尺度的成像标准施加梯度场,具体是:对X、Y、Z三个方向,分别采用强度为10000mT/m以上强度梯度分布的叠加梯度磁场,对具有自旋角动量的元素进行空间编码,使不同空间位置的元素的自旋频率不同。B. On the basis of the main magnetic field, when the target area to be imaged needs to achieve 1-micron-scale tomography (the target area is the 1-micron-scale imaging area), apply a gradient field according to the imaging standard with an imaging spatial resolution of 1-micron scale , specifically: for the three directions of X, Y, and Z, respectively use superimposed gradient magnetic fields with an intensity gradient distribution of more than 10000 mT/m to spatially encode elements with spin angular momentum, so that the elements in different spatial positions are The rotation frequency is different.
具体为:在Z方向上,收窄选频带宽至20KHz以下,采用强度为10000mT/m至50000mT/m的叠加梯度磁场,实现分辨率为1微米尺度厚度的Z方向选层。Specifically, in the Z direction, the frequency selection bandwidth is narrowed to below 20KHz, and a superimposed gradient magnetic field with an intensity of 10000mT/m to 50000mT/m is used to achieve Z direction layer selection with a resolution of 1 micron thickness.
在X方向上,按照式(1)的关系,采用强度为20000mT/m至50000mT/m的叠加梯度磁场,采用频率分辨率为0.8KHz至3.0KHz的接收谱仪,在X方向达到像素为1微米尺度的分辨率;In the X direction, according to the relationship of formula (1), a superimposed gradient magnetic field with an intensity of 20000mT/m to 50000mT/m is used, and a receiving spectrometer with a frequency resolution of 0.8KHz to 3.0KHz is used to achieve a pixel of 1 in the X direction. micron-scale resolution;
其中,谱仪的频率分辨率满足式(1):Among them, the frequency resolution of the spectrometer satisfies the formula (1):
Δf=γ*(Gx*Δx)……式(1);Δf=γ*(G x *Δx)... Formula (1);
式(1)中,Δf为谱仪的频率分辨率,γ为旋磁比,Gx为X方向上的叠加梯度磁场的梯度场强,Δx为在X方向达到像素分辨率的尺度。In formula (1), Δf is the frequency resolution of the spectrometer, γ is the gyromagnetic ratio, Gx is the gradient field strength of the superimposed gradient magnetic field in the X direction, and Δx is the scale that reaches the pixel resolution in the X direction.
例如,在X方向上,对于氢核,旋磁比为γ=42.6MHzT-1,要在X方向达到像素为1微米的分辨率,对于频率编码而言,按照梯度场强Gx大于20000mT/m计算,采用梯度频率编码规则计算得到,像素为1微米时,对应的谱仪的频率分辨率为:For example, in the X direction, for hydrogen nuclei, the gyromagnetic ratio is γ=42.6MHzT -1 , to achieve a resolution of 1 micron pixel in the X direction, for frequency encoding, according to the gradient field strength G x is greater than 20000mT/ m is calculated by using the gradient frequency coding rule. When the pixel is 1 micron, the corresponding frequency resolution of the spectrometer is:
Δf=γ*(Gx*Δx)=42.6×106HzT-1×20Tm-1×10-6m=852Hz,上述结果意味着,如果接收谱仪的频率分辨率能达到852Hz(约1KHz),就能实现像素为1微米(X方向成像)的频率编码,目前的谱仪完全可以达到这个频率分辨率水平;如果继续增大梯度场强Gx至50000mT/m,则接收谱仪的频率分辨率要求更低,约2.5KHz。Δf=γ*(G x *Δx)=42.6×10 6 HzT -1 ×20Tm -1 ×10 -6 m=852Hz, the above result means that if the frequency resolution of the receiving spectrometer can reach 852Hz (about 1KHz) , the frequency encoding with a pixel of 1 micron (imaging in the X direction) can be achieved, and the current spectrometer can fully achieve this level of frequency resolution; if the gradient field strength G x continues to increase to 50000mT/m, the frequency of the receiving spectrometer will be The resolution requirement is lower, about 2.5KHz.
需要说明的是,按照式(1)的关系,调控X方向上的叠加梯度磁场的梯度场强、谱仪的频率分辨率,可以实现1微米尺度空间分辨率成像。本发明的方法,不仅适合氢核,也适用于其它符合作为磁共振的具有自旋特性的元素。It should be noted that, according to the relationship of formula (1), by adjusting the gradient field strength of the superimposed gradient magnetic field in the X direction and the frequency resolution of the spectrometer, 1-micron-scale spatial resolution imaging can be achieved. The method of the present invention is suitable not only for hydrogen nuclei, but also for other elements having spin properties that are compatible with magnetic resonance.
在Y方向上,按照式(2)的关系,采用强度为10000mT/m至50000mT/m的叠加梯度磁场,控制Y方向上梯度打开时间,步长设定为4.7us至4.7*5us,实现分辨率为1微米尺度像素的相位编码;In the Y direction, according to the relationship of formula (2), a superimposed gradient magnetic field with an intensity of 10000mT/m to 50000mT/m is used to control the gradient opening time in the Y direction, and the step size is set to 4.7us to 4.7*5us to achieve resolution. Rate of phase encoding of 1-micron-scale pixels;
其中,Y方向上梯度打开时间满足式(2):Among them, the gradient opening time in the Y direction satisfies the formula (2):
式(2)中,Gy为Y方向上的叠加梯度磁场的梯度场强,Δy为在Y方向达到像素分辨率的尺度,Δy不大于1微米,为Y方向上梯度打开时间。In formula (2), G y is the gradient field strength of the superimposed gradient magnetic field in the Y direction, Δy is the scale that reaches the pixel resolution in the Y direction, Δy is not greater than 1 μm, Turns on time for the gradient in the Y direction.
例如,在Y方向上,同样对于氢核,旋磁比γ=42.6MHzT-1,Y方向上梯度场强度Gy按照10000mT/m计算,在成像区域Y方向线度长度为r=1mm的范围内,是y方向上梯度打开持续时间,同样要求成像的分辨率为1um,则需要满足:For example, in the Y direction, also for hydrogen nuclei, the gyromagnetic ratio γ=42.6MHzT -1 , the gradient field intensity Gy in the Y direction is calculated as 10000mT/m, and the linear length in the Y direction of the imaging area is within the range of r=1mm , is the gradient opening duration in the y direction, and the resolution of the imaging is also required to be 1um, then it needs to meet:
即:意味着只需要将梯度打开时间控制在2.35ms,步长可设定为4.7us,就可以实现分辨率为1um的像素的相位编码需要。y方向上梯度强度一般在10000mT/m至50000mT/m之间。如果增加Gy至50000mT/m,则可相应放宽步长的要求,使得步长为4.7us*5。which is: It means that only the gradient opening time can be controlled to 2.35ms, and the step size can be set to 4.7us, and the phase encoding needs of pixels with a resolution of 1um can be achieved. The gradient strength in the y direction is generally between 10000 mT/m and 50000 mT/m. If G y is increased to 50000mT/m, the step size requirement can be relaxed accordingly, so that the step size is 4.7us*5.
需要说明的是,按照式(2)的关系,调控Y方向上的叠加梯度磁场的梯度场强、梯度打开时间、步长,可以实现1微米尺度空间分辨率成像。本发明的方法,不仅适合氢核,也适用于其它符合作为磁共振的具有自旋特性的元素。It should be noted that, according to the relationship of formula (2), by adjusting the gradient field strength, gradient opening time, and step size of the superimposed gradient magnetic field in the Y direction, 1-micron-scale spatial resolution imaging can be achieved. The method of the present invention is suitable not only for hydrogen nuclei, but also for other elements having spin properties that are compatible with magnetic resonance.
C.采用与主磁场相垂直的射频电磁场,对成像对象进行射频电磁场激励,并拾取激励撤销后,成像对象发射的能级转换射频信号,对射频信号进行重建解码,得到断层成像;断层成像的范围为10±5cm,优选范围为10±2cm,感兴趣区域的成像空间分辨率为1微米尺度。C. Use the radio frequency electromagnetic field perpendicular to the main magnetic field to excite the imaging object with the radio frequency electromagnetic field, and pick up the energy level conversion radio frequency signal emitted by the imaging object after the excitation is cancelled, reconstruct and decode the radio frequency signal, and obtain the tomographic imaging; The range is 10±5 cm, the preferred range is 10±2 cm, and the imaging spatial resolution of the region of interest is 1 micron scale.
射频电磁场采用收发一体的设计方式,具体绕线可以采用8通道或者16通道笼式结构、柱状线圈部分重叠四周覆盖结构等方式,覆盖整个成像物体。The RF electromagnetic field adopts the design method of integrated transceiver, and the specific winding can adopt the 8-channel or 16-channel cage structure, the cylindrical coil partially overlaps the surrounding structure, etc., covering the entire imaging object.
针对整体成像对象,采用成像区域联变断层成像方法。成像区域联变断层成像方法是成像区域与成像分辨率联变动态调节进行断层成像。即对成像区域和成像分辨率进行动态调节,控制单张断层图像的数据大小的上限值在100kB-100MB之间。For the whole imaging object, the imaging area CT imaging method is adopted. The imaging area co-transformation tomography method is to perform tomography imaging by dynamic adjustment of imaging area and imaging resolution. That is, the imaging area and imaging resolution are dynamically adjusted, and the upper limit of the data size of a single tomographic image is controlled between 100kB-100MB.
当需要的成像范围大时,采用Zoom out(缩小)模式成像;反之,当需要的成像范围小时,采用Zoom in(放大)模式成像;至少所选择的感兴趣区域作为1微米尺度成像区域并以1微米尺度成像区域的标准施加梯度场,感兴趣区域的成像空间分辨率为1微米尺度,且控制单张断层图像的数据大小的上限值在100kB-100MB之间。When the required imaging range is large, use the Zoom out (zoom out) mode for imaging; on the contrary, when the required imaging range is small, use the Zoom in (zoom in) mode for imaging; at least the selected area of interest is used as a 1-micron-scale imaging area and is The standard applied gradient field of the 1-micron-scale imaging area, the imaging spatial resolution of the region of interest is 1-micron scale, and the upper limit of the data size of a single tomographic image is controlled between 100kB-100MB.
这个方法是申请人首次提出,其最本质的特征是:成像区域与成像分辨率联变,形成的断层成像,其图像数据大小,控制在需要的范围内。具体讲,当需要的成像范围较大时,采用Zoom out模式(缩小模式)对应的梯度线圈及电流控制和驱动模式;反之,当需要的成像范围较小时,采用Zoom in模式(放大模式)对应的梯度线圈及电流控制和驱动模式。Zoomout模式可为Zoom in模式提供定位帮助,且Zoom out模式中梯度场强要小于Zoom in模式对应的梯度场强。在此创新断层成像模式中,对应不同的成像区域(FOV)和成像分辨率要求,设置不同的参数组合配套,设置的规则是:控制每张断层图像的数据,在设定的图像数据大小范围内;一般将单张断层图像的数据大小,设定在100kB-100MB之间。比如,如果成像FOV设置为5cm*5cm*5cm,这个时候如果直接对整个FOV范围进行水平分辨率为1um*1um的成像重建,则每幅断层图像像素大小将达到2500MB,显然不合适。为此,我们通过控制梯度变化,分割大的FOV为小的FOV,类似“成像区域联变断层”的过程,实现合理的重建图像像素大小与分辨率要求的搭配。This method is proposed by the applicant for the first time, and its most essential feature is that the imaging area is linked with the imaging resolution, and the image data size of the formed tomographic imaging is controlled within the required range. Specifically, when the required imaging range is large, the gradient coils and current control and driving modes corresponding to the Zoom out mode (zoom out mode) are used; on the contrary, when the required imaging range is small, the Zoom in mode (zoom in mode) corresponding to gradient coils and current control and drive modes. The Zoomout mode can provide positioning assistance for the Zoom in mode, and the gradient field strength in the Zoom out mode is smaller than the gradient field strength corresponding to the Zoom in mode. In this innovative tomographic imaging mode, corresponding to different imaging area (FOV) and imaging resolution requirements, different parameter combinations are set. The setting rule is: control the data of each tomographic image, within the set image data size range In general, the data size of a single tomographic image is set between 100kB-100MB. For example, if the imaging FOV is set to 5cm*5cm*5cm, if the entire FOV range is directly reconstructed with a horizontal resolution of 1um*1um, the pixel size of each tomographic image will reach 2500MB, which is obviously inappropriate. To this end, by controlling the gradient change, we segment large FOVs into small FOVs, similar to the process of "imaging area connected tomography", to achieve a reasonable matching of reconstructed image pixel size and resolution requirements.
本发明的成像方法,兼顾了计算量问题。针对具体的成像目标,如果单张断层图像的数据太大,则计算机进行的图像运算处理量会几何级增加,使得本方案的方法无法有效实现。本发明设计“成像区域联变”断层成像方法,根据成像范围的实际情况,动态调整成像区域以及对应的分辨率,以降低图片的运算量。对于成像范围较小的,采用放大模式成像,此时可以设置相关梯度场、一实现1微米尺度分辨率的断层成像。当成像范围大时,避免对全部范围进行整体1微米尺度分辨率的断层成像,而是选择感兴趣区域,只对感兴趣区域进行1微米尺度分辨率的断层成像,对非感兴趣区域可以进行较大尺度分辨率的断层成像。而感兴趣区域的选择,可以利用Zoom out模式成像提供感兴趣区域定位参考功能。The imaging method of the present invention takes into account the problem of calculation amount. For a specific imaging target, if the data of a single tomographic image is too large, the processing amount of the image operation performed by the computer will increase geometrically, so that the method of this scheme cannot be effectively implemented. The invention designs a tomographic imaging method of "interchangeable imaging area", which dynamically adjusts the imaging area and the corresponding resolution according to the actual situation of the imaging range, so as to reduce the calculation amount of the picture. For those with a small imaging range, the magnification mode is used for imaging, and the relevant gradient fields can be set at this time to achieve tomographic imaging with a resolution of 1 μm. When the imaging range is large, avoid performing tomographic imaging with a resolution of 1 micron in the whole range, but select the region of interest, and perform tomography imaging with a resolution of 1 micron only for the region of interest, and can perform tomography for the non-interested region. Larger-scale resolution tomography. For the selection of the region of interest, the Zoom out mode imaging can be used to provide a reference function for positioning the region of interest.
下面列举一种成像范围大时,感兴趣区域及成像设置过程:当成像范围大时,采用Zoom out模式成像,还利用Zoom out模式的成像结果获得初始感兴趣区域;The following is an example of a region of interest and the imaging setting process when the imaging range is large: when the imaging range is large, the Zoom out mode is used for imaging, and the initial region of interest is obtained by using the imaging results of the Zoom out mode;
然后判断初始感兴趣区域是否满足1微米尺度成像条件,如果满足,则对初始感兴趣区域进行1微米尺度分辨率的断层成像;如果不满足,则将初始感兴趣区域划分为多个满足1微米尺度成像条件的子成像区域,对多个子成像区域分别进行1微米尺度分辨率的断层成像;Then judge whether the initial region of interest satisfies the 1-micron-scale imaging conditions, if so, perform tomographic imaging with a resolution of 1-micron scale on the initial region of interest; if not, divide the initial region of interest into multiple 1-micron-scale imaging Sub-imaging areas of scale imaging conditions, tomographic imaging with a resolution of 1 micron scale is performed on multiple sub-imaging areas respectively;
其中,1微米尺度成像条件是:图像空间分辨率为1微米尺度成像得到的单张断层图像的数据大小的上限值在100kB-100MB之间;Among them, the 1-micron-scale imaging conditions are: the upper limit of the data size of a single tomographic image obtained by the image spatial resolution of 1-micron-scale imaging is between 100kB-100MB;
1微米尺度分辨率的断层成像具体是按照成像空间分辨率为1微米尺度的成像标准施加梯度场,并进行成像。Specifically, the tomographic imaging with a resolution of 1 μm is to apply a gradient field and perform imaging according to the imaging standard with an imaging spatial resolution of 1 μm.
需要说明的是,成像范围大小可以根据实际需要灵活设置。本发明的方法,一般适合成像范围10±5cm。成像范围大与成像范围小的界限,可以根据实际需要灵活设置。如在一些情况下,可以设定成像范围小于等于5cm的为成像范围小的情形,将成像范围大于5cm的认定为成像范围大的情形。It should be noted that the size of the imaging range can be flexibly set according to actual needs. The method of the present invention is generally suitable for an imaging range of 10±5cm. The boundary between the large imaging range and the small imaging range can be flexibly set according to actual needs. For example, in some cases, it may be set that the imaging range is less than or equal to 5 cm as the case where the imaging range is small, and the imaging range is larger than 5 cm as the case where the imaging range is large.
在成像技术实现方法方面,除了常规的方式外,本发明还通过采用高的信噪比的采集序列,来提高成像的信噪比。在满足分辨率要求的前提下,再考虑序列的扫描时间。条件C中采用的信号增强序列是:在下一个负90度射频脉冲之前添加正90度射频脉冲以缩短TR时间、降低T2信号的衰减、提高信噪比。本发明的信号增强序列时序图如图1所示,Slice指的是层厚,phase指的是相位编码,read是读出梯度,RF射频脉冲,TE回波时间,TR是重复时间。该序列,可以通过在下一个90度射频(RF)脉冲之前添加90度RF脉冲(组合:负90度+正90度)的办法,来极大缩短TR时间,降低T2信号的衰减,提高信噪比,既保证了信噪比,也提高了成像速度。In terms of the method for realizing the imaging technology, in addition to the conventional manner, the present invention also improves the signal-to-noise ratio of imaging by adopting an acquisition sequence with a high signal-to-noise ratio. On the premise of meeting the resolution requirements, consider the scan time of the sequence. The signal enhancement sequence used in Condition C is: adding a positive 90 degree radio frequency pulse before the next negative 90 degree radio frequency pulse to shorten the TR time, reduce the attenuation of the T2 signal, and improve the signal-to-noise ratio. The timing diagram of the signal enhancement sequence of the present invention is shown in Fig. 1, where slice refers to layer thickness, phase refers to phase encoding, read is readout gradient, RF radio frequency pulse, TE echo time, and TR is repetition time. In this sequence, the TR time can be greatly shortened, the attenuation of the T2 signal can be reduced, and the signal-to-noise can be improved by adding a 90-degree RF pulse (combination: minus 90 degrees + plus 90 degrees) before the next 90-degree radio frequency (RF) pulse. ratio, which not only ensures the signal-to-noise ratio, but also improves the imaging speed.
针对光不透明的生物活体组织或者器官,当今现有的生物医学成像技术手段都无法在活体组织层面上无创实现1微米分辨率水平的断层成像。导致上述缺点的具体原因:若想能够在活体层面上,实现无创的1微米分辨率水平的断层成像,必须在技术上,同时达到以下三个方面的要求:(1)成像的关键媒介(例如:光、X射线、超声、电磁波等),需要无创的、穿透光不透明的活体组织;(2)空间分辨率达到1微米或小于1微米的尺度;(3)同时获得成像区域内,1微米或小于1微米的尺度的分辨率水平的,所有成像单个单元的对应信息。综观目前所有的技术手段,均无法同时满足上述三个方面的技术要求,因此,当今现有的生物医学成像技术手段都无法在活体组织层面上无创实现1微米分辨率水平的断层成像。For optically opaque living tissue or organs, none of today's existing biomedical imaging techniques can non-invasively achieve 1-micron resolution tomography at the living tissue level. The specific reasons for the above shortcomings: If you want to achieve non-invasive tomography at the level of 1 micron resolution at the living level, you must technically meet the following three requirements: (1) The key media for imaging (such as : light, X-ray, ultrasound, electromagnetic waves, etc.), which requires non-invasive, light-opaque living tissue; (2) the spatial resolution reaches 1 micron or less than 1 micron; (3) simultaneously obtains the imaging area, 1 At a resolution level of micrometers or less than 1 micrometer, all imaged individual cells correspond to information. Looking at all the current technical means, none of them can meet the technical requirements of the above three aspects at the same time. Therefore, today's existing biomedical imaging technology means cannot non-invasively achieve tomography at the level of 1 micron resolution at the level of living tissue.
本发明的无创光不透明微米级活体组织磁共振断层成像方法,通过A、B、C三项条件的设计。能够在光不透明的活体组织层面上无创实现1微米级别分辨率水平的断层成像,能够实现空间分辨率达到1微米尺度的、具备亚细胞结构分辨能力的无创活体组织断层成像。解决了现有的生物医学成像技术手段无法实现的在活体组织层面无创实现1微米分辨率水平的断层成像的技术难题。The non-invasive optical opaque micron-scale living tissue magnetic resonance tomography method of the present invention is designed through the three conditions of A, B and C. It can non-invasively achieve tomography at the level of 1 micron resolution on the level of optically opaque living tissue, and can achieve non-invasive living tissue tomography with a spatial resolution of 1 micron and the ability to resolve subcellular structures. The technical problem of non-invasively realizing tomographic imaging at the level of 1 micron resolution at the living tissue level, which cannot be achieved by the existing biomedical imaging technology means, is solved.
实施例2。Example 2.
以本发明的无创光不透明微米级活体组织磁共振断层成像方法,对光不透明的活体生物体——卵生生物受精卵,进行1微米或小于1微米尺度超高分辨率的、包含成像区域内所有单个细胞的结构和功能的断层成像。Using the non-invasive optically opaque micron-scale living tissue magnetic resonance tomography method of the present invention, the optically opaque living organism, the oviparous fertilized egg, is subjected to ultra-high resolution of 1 micron or less than 1 micron, including all imaging areas. Tomographic imaging of the structure and function of single cells.
按照上述的设计技术方法,选用高的磁场强度比如16T静磁场,在此静磁场基础上,施加X,Y,Z三个方向上的强梯度磁场,梯度场强在Z方向上,采用强度为10000mT/m以上的叠加梯度磁场,通过收窄选频带宽至20KHz或者以下,就可以达到分辨率为1微米的厚度的Z方向选层;According to the above-mentioned design techniques, a high magnetic field strength, such as a 16T static magnetic field, is selected. On the basis of this static magnetic field, a strong gradient magnetic field in the three directions of X, Y, and Z is applied. The gradient field strength is in the Z direction, and the strength is For superimposed gradient magnetic fields above 10000mT/m, by narrowing the frequency selection bandwidth to 20KHz or below, the Z-direction layer selection with a thickness of 1 micron can be achieved;
梯度场强在X方向上,采用强度为20000mT/m以上的叠加梯度磁场,接收谱仪的频率分辨率能达到852Hz(约1KHz),就可以达到分辨率为1微米的X方向上的分辨率;The gradient field strength is in the X direction, using a superimposed gradient magnetic field with a strength of more than 20000mT/m, the frequency resolution of the receiving spectrometer can reach 852Hz (about 1KHz), and the resolution in the X direction with a resolution of 1 micron can be achieved. ;
梯度场强在Y方向上,采用强度为10000mT/m以上的叠加梯度磁场,要将梯度打开时间控制在2.35ms,步长设定为4.7us,就可以实现分辨率为1um的像素的相位编码。The gradient field strength is in the Y direction, and a superimposed gradient magnetic field with a strength of more than 10000mT/m is used. To control the gradient opening time to 2.35ms and the step size to 4.7us, the phase encoding of pixels with a resolution of 1um can be realized. .
采用“成像区域联变断层”成像方法,采用高的信噪比的采集序列,来提高成像的信噪比,成像区域与成像分辨率联变,形成的断层成像,其图像数据大小,控制在需要的范围内,一般为100MB以内。The imaging method of "imaging area co-transformation tomography" is adopted, and a high signal-to-noise ratio acquisition sequence is used to improve the imaging signal-to-noise ratio. The imaging area and imaging resolution are co-transformed, and the image data size of the tomographic imaging formed is controlled within The required range is generally within 100MB.
本发明通过一系列的创新技术手段及组合,实现无创地在光不透明的活体生物体卵生生物受精卵、1微米或小于1微米尺度超高分辨率的、包含成像区域内所有单个细胞的结构和功能的,断层成像技术。Through a series of innovative technical means and combinations, the present invention non-invasively realizes the structure and the Functional, tomographic techniques.
需要说明的是,本发明的方法能够对光不透明的活体如小鼠、果蝇、卵生生物受精卵等无创实现1微米尺度的高分辨率成像。It should be noted that, the method of the present invention can non-invasively achieve high-resolution imaging at a scale of 1 micrometer on living organisms that are opaque to light, such as mice, fruit flies, and oviparous fertilized eggs.
实施例3。Example 3.
需要观察小白鼠脑部细胞情况,对一小白鼠的脑部进行1微米尺度断层成像。小白鼠的头部尺寸大致为3cm*3cm*3cm。It is necessary to observe the cells in the mouse brain, and perform 1-micron-scale tomography on the brain of the mouse. The head size of a mouse is roughly 3cm*3cm*3cm.
纵向断层的厚度为1微米,XY平面成像范围为3cm*3cm,也进行1微米空间分辨率成像,此时满足单张断层图像的数据大小的上限值在100kB-100MB范围内。The thickness of the longitudinal tomography is 1 micron, the imaging range of the XY plane is 3cm*3cm, and imaging with a spatial resolution of 1 micron is also performed. At this time, the upper limit of the data size of a single tomographic image is in the range of 100kB-100MB.
选用高的磁场强度10.5T静磁场,在此静磁场基础上,施加X,Y,Z三个方向上的强梯度磁场,梯度场强在Z方向上,采用强度为10000mT/m以上的叠加梯度磁场,收窄选频带宽至20KHz,达到分辨率为1微米的厚度的Z方向选层。Select a static magnetic field with a high magnetic field strength of 10.5T. On the basis of this static magnetic field, apply a strong gradient magnetic field in the three directions of X, Y, and Z. The gradient field strength is in the Z direction, and a superimposed gradient with a strength of more than 10000 mT/m is used. Magnetic field, narrow the frequency selection bandwidth to 20KHz, and achieve the Z-direction layer selection with a thickness of 1 micron.
梯度场强在X方向上,采用强度为20000mT/m以上的叠加梯度磁场,接收谱仪的频率分辨率为1KHz,达到分辨率为1微米的X方向上的分辨率。The gradient field strength is in the X direction, using a superimposed gradient magnetic field with a strength of more than 20000mT/m, the frequency resolution of the receiving spectrometer is 1KHz, and the resolution in the X direction with a resolution of 1 micron is achieved.
梯度场强在Y方向上,采用强度为30000mT/m以上的叠加梯度磁场,要将梯度打开时间控制在2.35ms,步长设定为4.7*3us,就可以实现分辨率为1um的像素的相位编码。The gradient field strength is in the Y direction, and a superimposed gradient magnetic field with a strength of more than 30000mT/m is used. To control the gradient opening time to 2.35ms and the step size to 4.7*3us, the phase of the pixel with a resolution of 1um can be achieved. coding.
采用与主磁场相垂直的射频电磁场,对成像对象进行射频电磁场激励,并拾取激励撤销后,成像对象发射的能级转换射频信号,对射频信号进行重建解码,得到断层成像。由于满足单张断层图像的数据大小的上限值在100kB-100MB范围内,因此计算量较小,能够实现微米级成像。The radio frequency electromagnetic field perpendicular to the main magnetic field is used to excite the imaging object with radio frequency electromagnetic field. Since the upper limit of the data size of a single tomographic image is in the range of 100kB-100MB, the calculation amount is small, and micron-level imaging can be realized.
在成像技术实现方法方面,除了常规的做法外,本发明还通过采用高的信噪比的采集序列,来提高成像的信噪比。在满足分辨率要求的前提下,再考虑序列的扫描时间。条件C中采用的信号增强序列是:在下一个负90度射频脉冲之前添加正90度射频脉冲以缩短TR时间、降低T2信号的衰减、提高信噪比。本发明的信号增强序列时序图如图1所示。该序列,可以通过在下一个90度射频(RF)脉冲之前添加90度RF脉冲(组合:负90度+正90度)的办法,来极大缩短TR时间,降低T2信号的衰减,提高信噪比,既保证了信噪比,也提高了成像速度。In terms of the imaging technology implementation method, in addition to the conventional practice, the present invention also improves the imaging signal-to-noise ratio by adopting a high signal-to-noise ratio acquisition sequence. On the premise of meeting the resolution requirements, consider the scan time of the sequence. The signal enhancement sequence used in Condition C is: adding a positive 90 degree radio frequency pulse before the next negative 90 degree radio frequency pulse to shorten the TR time, reduce the attenuation of the T2 signal, and improve the signal-to-noise ratio. The timing diagram of the signal enhancement sequence of the present invention is shown in FIG. 1 . In this sequence, the TR time can be greatly shortened, the attenuation of the T2 signal can be reduced, and the signal-to-noise can be improved by adding a 90-degree RF pulse (combination: minus 90 degrees + plus 90 degrees) before the next 90-degree radio frequency (RF) pulse. ratio, which not only ensures the signal-to-noise ratio, but also improves the imaging speed.
本发明的方法,能够对活体对象非创伤状态下,进行微米级成像。能够在细胞级的基础上观察分析活体组织的细胞结构,为细胞研究提供了先进的分析手段。The method of the present invention can perform micron-level imaging on a living object in a non-traumatic state. It can observe and analyze the cellular structure of living tissue on the basis of cell level, which provides an advanced analysis method for cell research.
实施例4。Example 4.
需要对一较大对象的体细胞情况进行观察研究,待测对象的部分位置如手部尺寸较小、某些部位尺寸较大如胸部。It is necessary to observe and study the somatic cell condition of a larger object. Some positions of the object to be measured, such as the size of the hand, are smaller, and some parts of the object are larger in size, such as the chest.
待观察的其中一个尺寸较小部位尺寸大致为2cm*2cm*1cm,带观察的其中一个较大部位的尺寸大致为20cm*20cm*20cm。The size of one of the smaller parts to be observed is approximately 2cm*2cm*1cm, and the size of one of the larger parts to be observed is approximately 20cm*20cm*20cm.
对尺寸较小部位成像,纵向断层的厚度可以控制到1微米尺度,XY平面成像范围为2cm*2cm,也进行1微米空间分辨率成像,此时满足单张断层图像的数据大小的上限值在100kB-100MB范围内。For imaging small-sized parts, the thickness of the longitudinal tomography can be controlled to 1 micron scale, the imaging range of the XY plane is 2cm*2cm, and imaging with a spatial resolution of 1 micron is also performed, which meets the upper limit of the data size of a single tomographic image. In the 100kB-100MB range.
对于较大部位,纵向断层的厚度可以控制到1微米尺度,XY平面成像范围为20cm*20cm,则单张断层图像的数据大小将达到40000MB,这样断层图像的数据量将非常庞大,成像结果无法有效获得。故,较大部位,通过本发明的成像区域联变断层成像方法,寻找感兴趣区域作为1微米尺度成像区域并以1微米尺度成像区域的标准施加梯度场,感兴趣区域的成像空间分辨率为1微米尺度,且控制单张断层图像的数据大小的上限值在100kB-100MB之间。For larger parts, the thickness of the longitudinal tomography can be controlled to 1 micron scale, and the imaging range of the XY plane is 20cm*20cm, the data size of a single tomographic image will reach 40,000MB, so the data volume of the tomographic image will be very large, and the imaging results cannot be effectively obtained. Therefore, for a larger part, through the imaging area combined tomography imaging method of the present invention, the region of interest is found as a 1-micron-scale imaging region and a gradient field is applied based on the standard of a 1-micron-scale imaging region, and the imaging spatial resolution of the region of interest is: 1 micron scale, and the upper limit of the data size of a single tomographic image is controlled between 100kB-100MB.
寻找感兴趣区域的过程,利用Zoom out模式成像提供感兴趣区域定位参考功能。先对成像范围以Zoom out模式成像,利用Zoom out模式的成像结果获得初始感兴趣区域;In the process of finding a region of interest, the Zoom out mode imaging is used to provide a reference function for positioning the region of interest. First, image the imaging range in Zoom out mode, and use the imaging results in Zoom out mode to obtain the initial region of interest;
然后判断初始感兴趣区域是否满足1微米尺度成像条件,如果满足,则对初始感兴趣区域进行1微米尺度分辨率的断层成像;如果不满足,则将初始感兴趣区域划分为多个满足1微米尺度成像条件的子成像区域,对多个子成像区域分别进行1微米尺度分辨率的断层成像。Then judge whether the initial region of interest satisfies the 1-micron-scale imaging conditions, if so, perform tomographic imaging with a resolution of 1-micron scale on the initial region of interest; if not, divide the initial region of interest into multiple 1-micron-scale imaging In the sub-imaging area of the scale imaging condition, tomographic imaging with a resolution of 1 μm is performed on the multiple sub-imaging areas respectively.
需要说明的是,此处是以两个不通过成像范围为例进行说明的,针对实际的成像对象不同位置,根据本发明的成像区域联变断层成像方法,将成像区域与空间分辨率动态联变,调整对应施加的梯度场,实现至少对感兴趣区域进行1微米尺度成像;非感兴趣区域可以选择1微米尺度成像,也可以采用较大分辨率的成像方式。It should be noted that two non-passing imaging ranges are used as examples for description here. For different positions of the actual imaging objects, according to the imaging region linked tomographic imaging method of the present invention, the imaging region and the spatial resolution are dynamically linked. Change, adjust the corresponding applied gradient field to achieve at least 1-micron-scale imaging of the region of interest; 1-micron-scale imaging can be selected for non-interested regions, or a higher-resolution imaging method can be used.
在成像技术实现方法方面,除了常规的做法外,本发明还通过采用高的信噪比的采集序列,来提高成像的信噪比。在满足分辨率要求的前提下,再考虑序列的扫描时间。条件C中采用的信号增强序列是:在下一个负90度射频脉冲之前添加正90度射频脉冲以缩短TR时间、降低T2信号的衰减、提高信噪比。本发明的信号增强序列时序图如图1所示。该序列,可以通过在下一个90度射频(RF)脉冲之前添加90度RF脉冲(组合:负90度+正90度)的办法,来极大缩短TR时间,降低T2信号的衰减,提高信噪比,既保证了信噪比,也提高了成像速度。In terms of the imaging technology implementation method, in addition to the conventional practice, the present invention also improves the imaging signal-to-noise ratio by adopting a high signal-to-noise ratio acquisition sequence. On the premise of meeting the resolution requirements, consider the scan time of the sequence. The signal enhancement sequence used in Condition C is: adding a positive 90 degree radio frequency pulse before the next negative 90 degree radio frequency pulse to shorten the TR time, reduce the attenuation of the T2 signal, and improve the signal-to-noise ratio. The timing diagram of the signal enhancement sequence of the present invention is shown in FIG. 1 . In this sequence, the TR time can be greatly shortened, the attenuation of the T2 signal can be reduced, and the signal-to-noise can be improved by adding a 90-degree RF pulse (combination: minus 90 degrees + plus 90 degrees) before the next 90-degree radio frequency (RF) pulse. ratio, which not only ensures the signal-to-noise ratio, but also improves the imaging speed.
本实施例能够在光不透明的活体组织层面上无创实现1微米级别分辨率水平的断层成像,能够实现空间分辨率达到1微米尺度的、具备亚细胞结构分辨能力的无创活体组织断层成像。This embodiment can non-invasively achieve 1-micron-level resolution tomography on the level of optically opaque living tissue, and can achieve non-invasive living tissue tomography with 1-micron spatial resolution and subcellular structure resolution capability.
最后应当说明的是,以上实施例仅用以说明本发明的技术方案而非对本发明保护范围的限制,尽管参照较佳实施例对本发明作了详细说明,本领域的普通技术人员应当理解,可以对本发明的技术方案进行修改或者等同替换,而不脱离本发明技术方案的实质和范围。Finally, it should be noted that the above embodiments are only used to illustrate the technical solutions of the present invention and not to limit the protection scope of the present invention. Although the present invention has been described in detail with reference to the preferred embodiments, those of ordinary skill in the art should The technical solutions of the present invention may be modified or equivalently replaced without departing from the spirit and scope of the technical solutions of the present invention.
Claims (7)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202110318850.6A CN113156350B (en) | 2021-03-25 | 2021-03-25 | Non-invasive light opaque micron-sized living tissue magnetic resonance tomography method and system |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202110318850.6A CN113156350B (en) | 2021-03-25 | 2021-03-25 | Non-invasive light opaque micron-sized living tissue magnetic resonance tomography method and system |
Publications (2)
Publication Number | Publication Date |
---|---|
CN113156350A CN113156350A (en) | 2021-07-23 |
CN113156350B true CN113156350B (en) | 2022-07-19 |
Family
ID=76884675
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN202110318850.6A Active CN113156350B (en) | 2021-03-25 | 2021-03-25 | Non-invasive light opaque micron-sized living tissue magnetic resonance tomography method and system |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN113156350B (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN117860226B (en) * | 2024-01-12 | 2024-07-09 | 安徽硕金医疗设备有限公司 | Large-caliber short-cavity interventional therapy type magnetic resonance equipment and design method thereof |
Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6326787B1 (en) * | 1999-06-10 | 2001-12-04 | Sandia National Laboratories | NMR of thin layers using a meanderline surface coil |
WO2014149064A1 (en) * | 2013-03-21 | 2014-09-25 | Weinberg Medical Physics Llc | Method and apparatus for high resolution physiological imaging of neurons |
CN106164736A (en) * | 2014-05-30 | 2016-11-23 | 斯坦福大学托管董事会 | For big intact tissue sample being carried out the method and device of imaging |
CN106716167A (en) * | 2014-09-01 | 2017-05-24 | 生物质子有限责任公司 | Selective sampling magnetic resonance-based method for assessing structural spatial frequencies |
CN107250828A (en) * | 2015-01-16 | 2017-10-13 | 因格瑞恩股份有限公司 | The chip analysis described for improved shaft bottom NMR characteristics |
CN108366753A (en) * | 2015-10-07 | 2018-08-03 | 生物质子有限责任公司 | Selective sampling for assessing the structure space frequency with specified contrast mechanisms |
CN109975727A (en) * | 2019-03-04 | 2019-07-05 | 中国科学技术大学 | Nanoscale magnetic resonance imaging imaging device and method |
CN110833413A (en) * | 2019-11-21 | 2020-02-25 | 中国科学院化学研究所 | Ultralow field magnetic imaging device for small living animals |
CN110958854A (en) * | 2017-05-24 | 2020-04-03 | 生物质子股份有限公司 | Selective sampling for evaluating spatial frequency of a structure with a specified contrast mechanism |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US8765099B2 (en) * | 1996-04-08 | 2014-07-01 | Koninklijke Philips N.V. | Magnetic resonance imaging hyperpolarization of liquids or solids by light with orbital angular momentum |
-
2021
- 2021-03-25 CN CN202110318850.6A patent/CN113156350B/en active Active
Patent Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6326787B1 (en) * | 1999-06-10 | 2001-12-04 | Sandia National Laboratories | NMR of thin layers using a meanderline surface coil |
WO2014149064A1 (en) * | 2013-03-21 | 2014-09-25 | Weinberg Medical Physics Llc | Method and apparatus for high resolution physiological imaging of neurons |
CN106164736A (en) * | 2014-05-30 | 2016-11-23 | 斯坦福大学托管董事会 | For big intact tissue sample being carried out the method and device of imaging |
CN106716167A (en) * | 2014-09-01 | 2017-05-24 | 生物质子有限责任公司 | Selective sampling magnetic resonance-based method for assessing structural spatial frequencies |
CN107250828A (en) * | 2015-01-16 | 2017-10-13 | 因格瑞恩股份有限公司 | The chip analysis described for improved shaft bottom NMR characteristics |
CN108366753A (en) * | 2015-10-07 | 2018-08-03 | 生物质子有限责任公司 | Selective sampling for assessing the structure space frequency with specified contrast mechanisms |
CN110958854A (en) * | 2017-05-24 | 2020-04-03 | 生物质子股份有限公司 | Selective sampling for evaluating spatial frequency of a structure with a specified contrast mechanism |
CN109975727A (en) * | 2019-03-04 | 2019-07-05 | 中国科学技术大学 | Nanoscale magnetic resonance imaging imaging device and method |
CN110833413A (en) * | 2019-11-21 | 2020-02-25 | 中国科学院化学研究所 | Ultralow field magnetic imaging device for small living animals |
Non-Patent Citations (1)
Title |
---|
人体组织电特性磁共振断层成像(MR+EPT)技术进展;辛学刚;《中国生物医学工程学报》;20150228;第34卷(第1期);第83-90页 * |
Also Published As
Publication number | Publication date |
---|---|
CN113156350A (en) | 2021-07-23 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US11768257B2 (en) | Magnetic resonance imaging | |
US6925319B2 (en) | Integrated multi-modality imaging system | |
KR100972709B1 (en) | MRI-induced ultrasound therapy device | |
JP3176221U (en) | Imaging device and method for three-dimensional anatomical and functional imaging | |
EP2383586A1 (en) | Compact, hybrid and integrated gamma/rf system used to form simultaneous pet or spect and mr images | |
US10310036B2 (en) | Magnetic resonance imaging apparatus and method for detecting error of magnetic resonance imaging apparatus | |
JP2024037819A (en) | Unilateral magnetic resonance imaging system with an interventional aperture and method for operating the system | |
US20130274590A1 (en) | Method and apparatus for generating a signal indicative of motion of a subject in a magnetic resonance apparatus | |
CN104619249B (en) | Device for producing the Distribution of Magnetic Field for meeting MPI and MRI requirements | |
CN106821500A (en) | One kind is used for minimally invasive operation navigating system and method | |
Qian et al. | Wireless amplified nuclear MR detector (WAND) for high-spatial-resolution MR imaging of internal organs: preclinical demonstration in a rodent model | |
US11536786B2 (en) | Systems and methods for data transmission in imaging system | |
JPWO2002022012A1 (en) | Magnetic resonance imaging system | |
CN114209300B (en) | Pulse magnetic particle imaging method and system | |
CN113156350B (en) | Non-invasive light opaque micron-sized living tissue magnetic resonance tomography method and system | |
US20180113185A1 (en) | System and method for imaging nanodiamonds as dynamic nuclear polarization agent | |
Ladd et al. | Germany’s journey toward 14 Tesla human magnetic resonance | |
WO2018156543A1 (en) | Systems and methods for intervention guidance using pre-operative planning with ultrasound | |
CN103293497B (en) | Local screen and method for the screening out of magnetic resonance signals | |
CN113640723A (en) | A system and method for improving the signal-to-noise ratio of immediate monitoring type magnetic resonance imaging | |
KR102082855B1 (en) | Dielectric pad and magnetic resonance imaging device including the same | |
US20110270073A1 (en) | Electron spin resonance imaging scanner | |
CN115552271A (en) | Permittivity enhanced Magnetic Resonance Imaging (MRI) and Magnetic Resonance Spectroscopy (MRS) | |
CN109143133B (en) | Method and magnetic resonance apparatus for improving the contrast of low signal shadows around hepatobiliary-specific hepatocellular carcinoma with disodium gadoxetate | |
Park et al. | Improvement of 19 F MR image uniformity in a mouse model of cellular therapy using inductive coupling |
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 |