翻转角度
射频功率放大器
振幅
Echo(通信协议)
脉冲序列
无线电频率
脉搏(音乐)
信号(编程语言)
物理
核磁共振
序列(生物学)
自旋回波
功率(物理)
光学
声学
计算机科学
电信
磁共振成像
化学
光电子学
放大器
医学
放射科
计算机网络
生物化学
CMOS芯片
量子力学
探测器
程序设计语言
作者
William H. Perman,Matt A. Bernstein,John C. Sandstrom
标识
DOI:10.1002/mrm.1910090104
摘要
Abstract Currently the accepted method for setting the correct rf power levels to achieve 90° and 180° rf pulses for MR imaging is to peak the echo amplitude of a rf spin‐echo sequence. The echo amplitude of this α‐2α pulse sequence is proportional to sin 3 (α) and has a relatively broad maximum. Recently another method for setting the rf flip angle by maximizing the ratio of the stimulated echo to the primary echo amplitudes (in a 3α sequence) demonstrated accuracy similar to that of the spin‐echo method using a shorter repetition time. We present a new, more sensitive, and more accurate method for setting the correct rf power levels for 90° and 180° rf pulses. In this method, based upon the stimulated echo pulse sequence, we are able to accurately set the rf power to within ±0.1 dB by minimizing the signal amplitude of the third spin echo. This null method works for both selective and nonselective rf pulses of flip angle 90° or 180°, allowing the user to accurately adjust the relative amplitudes of the four rf pulse types within a single pulse sequence. © 1989 Academic Press, Inc.
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