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Sample head for nuclear magnetic resonance whole-body tomography or localized in-vivo nuclear magnetic resonance spectroscopy

机译:核磁共振全身断层扫描或局部体内核磁共振光谱的样品头

摘要

A sample head (50) for nuclear magnetic resonance whole-body tomography or localized in-vivo nuclear magnetic resonance spectroscopy comprises an RF coil (51) having a plurality of inductive sections in the form of metallic strips (53 to 60) and capacitive sections in the form of gaps (61 to 68) arranged alternately one behind the other in the direction of the RF current (I.sub.1), so that the field lines (72) of the magnetic RF field (H.sub.1) generated by the RF coil (51) extend in parallel to an axis (74) defined by the RF coil (51). The RF coil (51) forms a single unit with an outer jacket (52). The number of inductive and capacitive sections is such as to be just below that limit value above which the distribution of the field lines (71) of the electric RF field (E.sub.1) produced by the said RF coil (51) changes from a first distribution (75), where there is a plane (76) between each inductive section (55) and the said axis (74) in which the strength of the electric RF field (E.sub.1) is equal to zero, to a second distribution where the strength of the said electric RF field (E.sub.1) rises in a substantially rotationally symmetrical pattern around the said axis, and linearly from the said axis toward the said RF coil, and this irrespective of the number of inductive sections present.
机译:用于核磁共振全身断层摄影或局部体内核磁共振光谱学的样品头(50)包括RF线圈(51),其具有多个呈金属条(53至60)形式的感应部分和电容性部分以间隙(61至68)的形式在RF电流(I.sub.1)的方向上彼此交替地布置,使得磁场RF(H.sub.1)的场线(72)由RF线圈(51)产生的θ1平行于由RF线圈(51)限定的轴(74)延伸。 RF线圈(51)与外套(52)形成一个单元。电感部分和电容部分的数量恰好在该极限值以下,在该极限值之上,由所述RF线圈(51)产生的RF电场(E1)的场线(71)的分布发生变化从第一分布(75)开始,其中在每个感应部分(55)和所述轴(74)之间存在一个平面(76),其中电场RF(E.sub.1)的强度等于零到第二分布,在该第二分布中,所述R​​F电场的强度(E.sub.1)围绕所述轴以基本旋转对称的方式上升,并且从所述轴朝向所述RF线圈线性地上升,并且这与第二分布无关。存在的感应部分数。

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