Hexagonal zero mode TEM coil: A single-channel coil design for imaging multiple small animals

被引:9
作者
Lazovic, J
Stojkovic, DS
Collins, CM
Yang, QX
Vaughan, JT
Smith, MB
机构
[1] Penn State Univ, Coll Med, Ctr Nucl Magnet Resonance Res, Dept Radiol, Hershey, PA 17033 USA
[2] Penn State Univ, Dept Phys, University Pk, PA 16802 USA
[3] Univ Minnesota, Sch Med, Dept Radiol, Ctr MR Res, Minneapolis, MN 55455 USA
关键词
MRI; multi-animal; RF coil; RF homogeneity; signal-to-noise ratio;
D O I
10.1002/mrm.20459
中图分类号
R8 [特种医学]; R445 [影像诊断学];
学科分类号
1002 ; 100207 ; 1009 ;
摘要
A novel hexagonal coil design for simultaneous imaging of multiple small animals is presented. The design is based on a coaxial cavity and utilizes the magnetic field formed between two coaxial conductors with hexagonal cross-sections. An analytical solution describing the B-1 field between conductors of the hexagonal coil was found from the Biot-Savart law. Both experimental results and analytical calculations showed a variation in the B-1 field within the imaging region of less than 10%. Numerical calculations predicted similar to 35% improvement in B-1 field homogeneity with the hexagonal coil design compared to a cylindrical coaxial cavity design. The experimentally-measured signal-to-noise ratio (SNR) of the hexagonal coil loaded with six 50-mM phantoms was only 4-5% lower than that of a single parallel plate resonator loaded with one phantom. In vivo spinecho (SE) images of six 7-day-old rat pups acquired simultaneously demonstrated sufficient SNR for microimaging. The construction scheme of the coil, simple methods for tuning and matching, and an anesthesia device and animal holder designed for the coil are described. The hexagonal coil design utilizes a single receiver and allows for simultaneous imaging of six small animals with no significant compromise in SNR. Magn Reson Med 53:1150-1157, 2005. (c) 2005 WileyLiss, Inc.
引用
收藏
页码:1150 / 1157
页数:8
相关论文
共 14 条
[1]  
[Anonymous], [No title captured], Patent No. 6633161
[2]   Multiple-mouse MRI [J].
Bock, NA ;
Konyer, NB ;
Henkelman, RM .
MAGNETIC RESONANCE IN MEDICINE, 2003, 49 (01) :158-167
[3]  
BOCK NA, 2001, P 9 ANN M ISMRM GLAS, P1108
[4]   THE INTRINSIC SIGNAL-TO-NOISE RATIO IN NMR IMAGING [J].
EDELSTEIN, WA ;
GLOVER, GH ;
HARDY, CJ ;
REDINGTON, RW .
MAGNETIC RESONANCE IN MEDICINE, 1986, 3 (04) :604-618
[5]  
HAACKE ME, 1999, MAGNETICS RESONANCE, P340
[6]   MAPPING OF THE RADIOFREQUENCY FIELD [J].
INSKO, EK ;
BOLINGER, L .
JOURNAL OF MAGNETIC RESONANCE SERIES A, 1993, 103 (01) :82-85
[7]  
JACKSON JD, 1975, CLASSICAL ELECTRODYN, P173
[8]  
Kunz K. S., 1993, FINITE DIFFERENCE TI
[9]   RF COIL OPTIMIZATION - EVALUATION OF B-1 FIELD HOMOGENEITY USING FIELD HISTOGRAMS AND FINITE-ELEMENT CALCULATIONS [J].
LI, SZ ;
YANG, QX ;
SMITH, MB .
MAGNETIC RESONANCE IMAGING, 1994, 12 (07) :1079-1087
[10]  
LIAO ZP, 1984, SCI SIN A-MATH P A T, V27, P1063