亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        1.5T下高介電材料幾何結(jié)構(gòu)對(duì)發(fā)射場(chǎng)影響的仿真研究

        2022-06-14 09:52:00唐德港李紅闖劉小玲李海東葉朝輝
        波譜學(xué)雜志 2022年2期
        關(guān)鍵詞:襯墊方形磁共振

        唐德港,李紅闖,劉小玲,石 磊,李海東,葉朝輝,周 欣*

        1.5T下高介電材料幾何結(jié)構(gòu)對(duì)發(fā)射場(chǎng)影響的仿真研究

        唐德港1,2,李紅闖1,2,劉小玲1,2,石 磊1,2,李海東1,2,葉朝輝1,2,周 欣1,2*

        1. 波譜與原子分子物理國(guó)家重點(diǎn)實(shí)驗(yàn)室,武漢磁共振中心(中國(guó)科學(xué)院精密測(cè)量科學(xué)與技術(shù)創(chuàng)新研究院),湖北 武漢 430071;2. 中國(guó)科學(xué)院大學(xué),北京 100049

        引 言

        1 HPMs幾何結(jié)構(gòu)對(duì)發(fā)射場(chǎng)影響的仿真研究

        1.1 HPMs提高射頻線圈發(fā)射效率的原理

        將HPMs放置在成像物體ROI附近,在射頻脈沖激勵(lì)下,根據(jù)麥克斯韋全電流定律:

        1.2 仿真模型及參數(shù)設(shè)置

        圖1 帶有水模負(fù)載的鳥籠線圈仿真模型(對(duì)照組).(a)仿真模型示意圖;(b)水模內(nèi)有限元網(wǎng)格剖分結(jié)果

        在水模附近加入四種文獻(xiàn)報(bào)道過的不同幾何結(jié)構(gòu)的高介電襯墊作為實(shí)驗(yàn)組,包括:(1)四等分圓筒狀襯墊[30];(2)對(duì)稱環(huán)繞水模的四塊方形襯墊[20];(3)同側(cè)三塊方形襯墊[31];(4)120°扇環(huán)柱狀襯墊[32].采用的HPMs厚度均為13 mm、長(zhǎng)度均為71 mm.其中四等分圓筒狀襯墊相鄰單元間隙為3 mm;環(huán)繞四方塊襯墊寬58 mm;同側(cè)三方塊襯墊寬34 mm,相鄰兩單元中心成60°夾角.襯墊材料為摻雜鎬和鈰的鈦酸鋇,首先將鈦酸鋇(Ba/Ti比為0.996)和高純度的ZrO2、CeO2研磨混合,再在1 340°下高溫?zé)Y(jié)為陶瓷襯墊.襯墊相對(duì)介電常數(shù)設(shè)為4 500[20],電導(dǎo)率為0.44 S/m.實(shí)驗(yàn)組水模均采用和對(duì)照組相同的網(wǎng)格剖分,以保證參數(shù)和電磁場(chǎng)的精確度和一致性,實(shí)驗(yàn)組水模仿真模型示意圖如圖2所示.

        圖2 不同幾何結(jié)構(gòu)的高介電襯墊(深灰色)的仿真模型示意圖(隱藏線圈).(a)無襯墊;(b)四等分圓筒狀襯墊;(c)四塊方形襯墊對(duì)稱環(huán)繞水模;(d)同側(cè)三塊方形襯墊;(e) 120°扇環(huán)柱狀襯墊

        2 結(jié)果與討論

        2.1 HPMs幾何結(jié)構(gòu)對(duì)發(fā)射場(chǎng)的影響

        圖3 不同幾何結(jié)構(gòu)的高介電襯墊仿真模型水模中心橫斷面的發(fā)射效率h分布.(a)無襯墊;(b)四等分圓筒狀襯墊;(c)四塊方形襯墊對(duì)稱環(huán)繞水模;(d)同側(cè)三塊方形襯墊;(e) 120°扇環(huán)柱狀襯墊

        表1 不同幾何結(jié)構(gòu)的高介電襯墊仿真模型ROI內(nèi)的發(fā)射效率h均值與不均勻度(CV)

        圖4 不同幾何結(jié)構(gòu)的高介電襯墊仿真模型ROI內(nèi)發(fā)射效率均值和不均勻度分析

        2.2 理論分析

        不同模型水模中心橫斷面沿軸方向中心線的發(fā)射效率分布如圖5所示,可以看出,加入四等分圓筒狀、環(huán)繞四方塊、同側(cè)三方塊襯墊后,發(fā)射效率沿軸方向中心線分布都較為均勻.

        圖5 不同仿真模型水模中心橫斷面沿y軸方向中心線的發(fā)射效率分布(以中心為原點(diǎn))

        3 結(jié)論

        [1] UGURBIL K. Imaging at ultrahigh magnetic fields: history, challenges, and solutions[J]. Neuroimage, 2018, 168: 7-32.

        [2] YANG Q X, WANG J, ZHANG X, et al. Analysis of wave behavior in lossy dielectric samples at high field[J]. Magn Reson Med, 2002, 47(5): 982-989.

        [3] SCHICK F. Whole-body MRI at high field: technical limits and clinical potential[J]. Eur Radiol, 2005, 15(5): 946-959.

        [4] DIETRICH O, REISER M F, SCHOENBERG S O. Artifacts in 3-T MRI: Physical background and reduction strategies[J]. Eur J Radiol, 2008, 65(1): 29-35.

        [5] KANGARLU A, BAERTLEIN B A, LEE R, et al. Dielectric resonance phenomena in ultra high field MRI[J]. J Comput Assist Tomogr, 1999, 23(6): 821-831.

        [6] HUANG Q H, GAO Y, XIN X G. Study on the law of B1field homogeneity and SAR inside human body varying with field strength at high and ultra-high field MR[J]. Chin J Biological Eng, 2013, 32(1): 21-27.

        黃綺華, 高勇, 辛學(xué)剛. 高場(chǎng)和超高場(chǎng)MR下人體內(nèi)B1場(chǎng)均勻性及SAR隨場(chǎng)強(qiáng)變化規(guī)律的研究[J]. 中國(guó)生物醫(yī)學(xué)工程學(xué)報(bào), 2013, 32(1): 21-27.

        [7] OSCH M J P V, WEBB A G. Safety of ultra-high field MRI: What are the specific risks?[J]. Curr Radiol Rep, 2014, 2(8): 1-8.

        [8] DOTY F D, ENTZMINGER G, KULKARNI J, et al. Radio frequency coil technology for small-animal MRI[J]. NMR Biomed, 2007, 20(3): 304-325.

        [9] GULSEN G, MUFTULER L T, NALCIOGLU O. A double end-cap birdcage RF coil for small animal whole body imaging[J]. J Magn Reson, 2002, 156(2): 309-312.

        [10] DARDZINSKI B J, LI S H, COLLINS C M, et al. A birdcage coil tuned by RF shielding for application at 9.4 T[J]. J Magn Reson, 1998, 131(1): 32-38.

        [11] LEE K H, CHENG M C, CHAN K C, et al. Performance of large-size superconducting coil in 0.21 T MRI system[J]. IEEE Trans Biomed Eng, 2004, 51(11): 2024-2030.

        [12] LIN I T, YANG H C, HSIEH C W, et al. Human hand imaging using a 20 cm high-temperature superconducting coil in a 3 T magnetic resonance imaging system[J]. J Appl Phys, 2010, 107(12): 124701.

        [13] LIAO Z W, CHEN J F, YANG C S, et al. A design scheme for1H/31P dual-nuclear parallel MRI coil[J]. Chinese J Magn Reson, 2020, 37(3): 273-282.

        廖志文, 陳俊飛, 楊春升, 等.1H/31P雙核并行磁共振成像線圈的研究與設(shè)計(jì)[J]. 波譜學(xué)雜志, 2020, 37(3): 273-282.

        [14] FENG T, CHEN J F, ZHANG Z, et al. A design of short dead-time RF coil and RF switch for low-field NMR[J]. Chinese J Magn Reson, 2021, 38(1): 1-11.

        馮濤, 陳俊飛, 張震, 等. 低場(chǎng)核磁共振短死時(shí)間射頻線圈與射頻開關(guān)的設(shè)計(jì)[J]. 波譜學(xué)雜志, 2021, 38(1): 1-11.

        [15] WEBB A G, VAN DE MOORTELE P F. The technological future of 7 T MRI hardware[J]. NMR Biomed, 2016, 29(9): 1305-1315.

        [16] ANDREYCHENKO A, BLUEMINK J J, RAAIJMAKERS A J E, et al. Improved RF performance of travelling wave MR with a high permittivity dielectric lining of the bore[J]. Magn Reson Med, 2013, 70(3): 885-894.

        [17] YANG Q X, MAO W, WANG J, et al. Manipulation of image intensity distribution at 7.0 T: Passive RF shimming and focusing with dielectric materials[J]. J Magn Reson Imaging, 2006, 24(1): 197-202.

        [18] FRANKLIN K M, DALE B M, MERKLE E M. Improvement in B1-inhomogeneity artifacts in the abdomen at 3 T MR imaging using a radiofrequency cushion[J]. J Magn Reson Imaging, 2008, 27(6): 1443-1447.

        [19] DE HEER P, BRINK W M, KOOIJ B J, et al. Increasing signal homogeneity and image quality in abdominal imaging at 3 T with very high permittivity materials[J]. Magn Reson Med, 2012, 68(4): 1317-1324.

        [20] ZIVKOVIC I, TEEUWISSE W, SLOBOZHANYUK A, et al. High permittivity ceramics improve the transmit field and receive efficiency of a commercial extremity coil at 1.5 tesla[J]. J Magn Reson, 2019, 299: 59-65.

        [21] SICA C T, RUPPRECHT S, HOU R J, et al. Toward whole-cortex enhancement with a ultrahigh dielectric constant helmet at 3 T[J]. Magn Reson Med, 2020, 83(3): 1123-1134.

        [22] LEE B Y, ZHU X H, RUPPRECHT S, et al. Large improvement of RF transmission efficiency and reception sensitivity for human in vivo P-31 MRS imaging using ultrahigh dielectric constant materials at 7 T[J]. Magn Reson Imaging, 2017, 42: 158-163.

        [23] RUPPRECHT S, SICA C T, CHEN W, et al. Improvements of transmit efficiency and receive sensitivity with ultrahigh dielectric constant (uHDC) ceramics at 1.5 T and 3 T[J]. Magn Reson Med, 2018, 79(5): 2842-2851.

        [24] VAN GEMERT J, BRINK W, REMIS R, et al. A simulation study on the effect of optimized high permittivity materials on fetal imaging at 3 T[J]. Magn Reson Med, 2019, 82(5): 1822-1831.

        [25] BRINK W M, WEBB A G. High permittivity pads reduce specific absorption rate, improve B-1 homogeneity, and increase contrast-to-noise ratio for functional cardiac MRI at 3 T[J]. Magn Reson Med, 2014, 71(4): 1632-1640.

        [26] SCHMIDT R, WEBB A. A new approach for electrical properties estimation using a global integral equation and improvements using high permittivity materials[J]. J Magn Reson, 2016, 262: 814.

        [27] VAN GEMERT J, BRINK W, WEBB A, et al. High-permittivity pad design tool for 7 T neuroimaging and 3 T body imaging[J]. Magn Reson Med, 2019, 81(5): 3370-3378.

        [28] BRINK W M, REMIS R F, WEBB A G. A theoretical approach based on electromagnetic scattering for analysing dielectric shimming in high-field MRI[J]. Magn Reson Med, 2016, 75(5): 2185-2194.

        [29] LUO M, HU C, ZHUANG Y, et al. Numerical assessment of the reduction of specific absorption rate by adding high dielectric materials for fetus MRI at 3 T[J]. Biomed Eng-Biomed Tech, 2016, 61(4): 455-461.

        [30] SEO J H, HAN S D, KIM K N. Improvements in magnetic field intensity and uniformity for small-animal MRI through a high-permittivity material attachment[J]. Electron Lett, 2016, 52(11): 898-899.

        [31] RUYTENBERG T, O’REILLY T P, WEBB A G. Design and characterization of receive-only surface coil arrays at 3 T with integrated solid high permittivity materials[J]. J Magn Reson, 2020, 311: 106681.

        [32] CHEN W, LEE B Y, ZHU X H, et al. Tunable ultrahigh dielectric constant (TuHDC) ceramic technique to largely improve RF coil efficiency and MR imaging performance[J]. IEEE Trans Med Imaging, 2020, 39(10): 3187-3197.

        [33] 方俊鑫, 殷之文. 電介質(zhì)物理學(xué)[M]. 北京: 科學(xué)出版社, 1989.

        [34] WEBB A G. Dielectric materials in magnetic resonance[J]. Concepts Magn Reson Part A, 2011, 38A(4): 148-184.

        [35] HOULT D I. The principle of reciprocity in signal strength calculations—A mathematical guide[J]. Concepts Magn Reson, 2000, 12(4): 173-187.

        [36] 羅超. 基于超材料的3 T磁共振射頻接收線圈性能研究[D]. 重慶: 重慶理工大學(xué), 2016.

        [37] 張巍巍. 基于1.5 T磁共振系統(tǒng)體線圈電磁參數(shù)分析及共振頻率算法實(shí)現(xiàn)[D]. 成都: 西南交通大學(xué), 2016.

        [38] XIN S X, HUANG Q, GAO Y, et al. Fetus MRI at 7 T: B1shimming strategy and SAR safety implications[J]. IEEE Trans Microw Theory Tech, 2013, 61(5): 2146-2152.

        1,2,1,2,1,2,1,2,1,2,1,2,1,2*

        1. State Key Laboratory of Magnetic Resonance and Atomic and Molecular Physics, National Center for Magnetic Resonance in Wuhan, Innovation Academy for Precision Measurement Science and Technology, Chinese Academy of Sciences, Wuhan 430071, China; 2. University of Chinese Academy of Sciences, Beijing 100049, China

        O482.53

        A

        10.11938/cjmr20212904

        2021-04-01;

        2021-05-15

        國(guó)家重點(diǎn)研發(fā)計(jì)劃(2016YFC1304702);國(guó)家自然科學(xué)基金資助項(xiàng)目(82127802,81227902);中國(guó)科學(xué)院戰(zhàn)略性先導(dǎo)科技專項(xiàng)(XDB25000000);廣東省重點(diǎn)領(lǐng)域研發(fā)計(jì)劃(2018B030333001);湖北省科技重大專項(xiàng)(2021ACA013);中國(guó)科學(xué)院磁共振技術(shù)聯(lián)盟資助項(xiàng)目(2020GZL002).

        * Tel: 027-87198802, E-mail: xinzhou@wipm.ac.cn.

        猜你喜歡
        襯墊方形磁共振
        膝關(guān)節(jié)活動(dòng)平臺(tái)單髁置換術(shù)后襯墊脫位研究 進(jìn)展
        超聲及磁共振診斷骶尾部藏毛竇1例
        方形料倉(cāng)堵料解決方法
        捕捉方形泡泡
        方形夾具在線切割切槽的應(yīng)用
        哈爾濱軸承(2021年4期)2021-03-08 01:00:48
        磁共振有核輻射嗎
        不同減振襯墊 對(duì)模擬運(yùn)輸獼猴桃生理和品質(zhì)影響
        磁共振有核輻射嗎
        變方形
        防滲襯墊自身的穩(wěn)定計(jì)算分析
        久久久久无码精品国产app| 国产肥熟女视频一区二区三区| 国产91精品清纯白嫩| 九九久久精品国产免费av| 久久人妻无码一区二区| 国产va在线观看免费| 天天做天天爱天天综合网| 亚洲国产精品午夜电影| 蜜臀一区二区av天堂| 亚洲精品成人无百码中文毛片| 亚洲无线码一区二区三区| 亚洲欧洲日产国码高潮αv| 久久亚洲午夜牛牛影视| 日本免费三片在线视频| 日本免费视频| 国产一区二区在线视频| 欧美在线不卡视频| 国产亚洲精品成人av在线| 日韩精品视频高清在线| 亚洲av无码精品国产成人| 国产亚洲av片在线观看18女人| 中日韩欧美高清在线播放| 亚洲国产女同在线观看| 97久久婷婷五月综合色d啪蜜芽 | 日本区一区二区三视频| 色婷婷亚洲精品综合影院| 成年视频国产免费观看| 蜜桃av多人一区二区三区| 国产不卡在线观看视频| 欧美黑寡妇特a级做爰| 女人与牲口性恔配视频免费| 视频女同久久久一区二区三区| 精品久久综合日本久久综合网| 亚洲av日韩精品久久久久久久| 免费jjzz在线播放国产| 女同另类一区二区三区| 草色噜噜噜av在线观看香蕉| 大胆欧美熟妇xxbbwwbw高潮了| 丝袜美腿爆炒国产在线观看 | 日日碰日日摸日日澡视频播放 | 国产最新女主播福利在线观看|