23Na MRI on 0,5T clinical scanner

Author(s):  
N.V. Anisimov ◽  
A.A. Tarasova ◽  
O.S. Pavlova ◽  
D.V. Fomina ◽  
I.A. Usanov ◽  
...  

Object. The purpose of this work is to reveal the possibilities of low-field 23Na MRI. It was supposed to obtain images of various human organs using the 3D-scanning method, and to do this with minimal hardware modifications of a typical clinical 0,5T scanner. Materials and methods. The proprietary receiving coils, originally intended for registering proton signals (21,1 MHz), were transformed to transceiver ones and tuned to the sodium Larmor frequency of 5,6 MHz. The scanning was carried out by the 3D-gradient echo method with the parameters: TR/TE=44,7/12 ms, FA=45° and isotropic resolution of 6 mm. To increase SNR, apodization in k-space was applied during data processing. Results. 23Na MRI (including volumetric reconstructions) of several human organs – head, breast, heart, joints were obtained with SNR up to 15. Discussion. When developing low-field 23Na MRI, it is advisable to focus on recording only the T2long component (>15 ms). In this case, it is possible to narrow the receiver bandwidth as much as possible and thereby minimize noise. In addition, the requirements for the transmission path are reduced. As a result, for debugging MRI methods, the equipment of a typical clinical scanner, which is supplemented by coils tuned to the sodium NMR frequency only, can be used.

2015 ◽  
Vol 188 ◽  
pp. 664-672 ◽  
Author(s):  
María Gudjónsdóttir ◽  
Amidou Traoré ◽  
Ásbjörn Jónsson ◽  
Magnea Gudrún Karlsdóttir ◽  
Sigurjón Arason

2018 ◽  
Vol 7 (1) ◽  
pp. 66-70
Author(s):  
Abhinav Singh Andotra ◽  
Sandeep Sharma

Segmentation plays an important role in separating data from medicinal images and also helps in clinical findings. Segmentation is the way toward apportioning the image into different regions. MRI is utilized to extract images of delicate tissues of human body. It is utilized in analyzing the human organs without the requirement of surgery. For the most part MRI images contain a lot of noise caused by operator performance, equipment and the environment, which prompts genuine errors. MRI is a productive way in giving data in regards to the area of tumors and even the volume. The noise present in the MRI image can be evacuated by utilizing different de-noising procedures whichever is most appropriate method depending on the type of image obtained and afterward can be handled by any of the segmentation techniques. The noise in MRI images might be because of field strength, RF pulses, RF coil, voxel volume, or receiver bandwidth. In our proposed paper a review of different noise handling and filtering mechanism is conducted in order to enhance the quality of image. In this paper we modify the adaptive median filter by applying redundancy handling mechanism and enhance the contrast of image by applying histogram equivalence method.


Diagnostics ◽  
2020 ◽  
Vol 10 (12) ◽  
pp. 1017
Author(s):  
Sheikh Faisal Ahmad ◽  
Young Cheol Kim ◽  
Ick Chang Choi ◽  
Hyun Deok Kim

The radio frequency (RF) coil is one of the key components of the magnetic resonance imaging (MRI) system. It has a significant impact on the performance of the nuclear magnetic resonance (NMR) detection. Among numerous practical designs of RF coils for NMR imaging, the birdcage RF coil is the most popular choice from low field to ultra-high field MRI systems. In the transmission mode, it can establish a strong and homogeneous transverse magnetic field B1 for any element at its Larmor frequency. Similarly, in the reception mode, it exhibits extremely high sensitivity for the detection of even faint NMR signals from the volume of interest. Despite the sophisticated 3D structure of the birdcage coil, the developments in the design, analysis, and implementation technologies during the past decade have rendered the development of the birdcage coils quite reasonable. This article provides a detailed review of the recent progress in the birdcage RF coil technology for the MRI system.


Author(s):  
N.V. Anisimov ◽  
A.A. Tarasova ◽  
I.A. Usanov ◽  
Yu.A. Pirogov

The problems of registration of weak magnetic resonance (MR) signals in conditions of technogenic interference are considered. Their intensity and temporal activity are analyzed by MRI tomography. To reduce their influence on the result of long-term signal accumulation, it is proposed to save its individual realizations during registration. Then, at the end of registration, it is possible analyze them, identify noisy implementations, edit them, and submit edited copies for summing up instead of noisy ones. An approach that is similar in concept is considered for practical application in MRI – instead of increasing the number of accumulations, it is proposed to increase the number of phase encoding steps. Examples of analysis of interference activity during 23Na MRI scanning of various human organs using various coils are given. The possibility of increasing the information content of MRI data by using apodization for kspace data is shown, and this technique is most effective if the effect of noise occurs when only the peripheral part of this space is filled.


Author(s):  
R. Levi-Setti ◽  
J.M. Chabala ◽  
Y.L. Wang

Finely focused beams extracted from liquid metal ion sources (LMIS) provide a wealth of secondary signals which can be exploited to create high resolution images by the scanning method. The images of scanning ion microscopy (SIM) encompass a variety of contrast mechanisms which we classify into two broad categories: a) Emission contrast and b) Analytical contrast.Emission contrast refers to those mechanisms inherent to the emission of secondaries by solids under ion bombardment. The contrast-carrying signals consist of ion-induced secondary electrons (ISE) and secondary ions (ISI). Both signals exhibit i) topographic emission contrast due to the existence of differential geometric emission and collection effects, ii) crystallographic emission contrast, due to primary ion channeling phenomena and differential oxidation of crystalline surfaces, iii) chemical emission or Z-contrast, related to the dependence of the secondary emission yields on the Z and surface chemical state of the target.


1983 ◽  
Vol 44 (C3) ◽  
pp. C3-1033-C3-1036 ◽  
Author(s):  
J. M. Delrieu ◽  
N. S. Sullivan ◽  
Bechgaard
Keyword(s):  

Sign in / Sign up

Export Citation Format

Share Document