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采用 74mT 下极化 3He 和 129Xe 的 Carr-Purcell-Meiboom-Gill 自旋-自旋弛豫时间测量大鼠肺部肺泡氧分压。

Measurement of alveolar oxygen partial pressure in the rat lung using Carr-Purcell-Meiboom-Gill spin-spin relaxation times of hyperpolarized 3He and 129Xe at 74 mT.

机构信息

Imaging Research Laboratories, Robarts Research Institute, London, Canada.

出版信息

Magn Reson Med. 2010 Nov;64(5):1484-90. doi: 10.1002/mrm.22520.

Abstract

Regional measurement of alveolar oxygen partial pressure can be obtained from the relaxation rates of hyperpolarized noble gases, (3) He and (129) Xe, in the lungs. Recently, it has been demonstrated that measurements of alveolar oxygen partial pressure can be obtained using the spin-spin relaxation rate (R(2) ) of (3) He at low magnetic field strengths (<0.1 T) in vivo. R(2) measurements can be achieved efficiently using the Carr-Purcell-Meiboom-Gill pulse sequence. In this work, alveolar oxygen partial pressure measurements based on Carr-Purcell-Meiboom-Gill R(2) values of hyperpolarized (3) He and (129) Xe in vitro and in vivo in the rat lung at low magnetic field strength (74 mT) are presented. In vitro spin-spin relaxivity constants for (3) He and (129) Xe were determined to be (5.2 ± 0.6) × 10(-6) Pa(-1) sec(-1) and (7.3 ± 0.4) × 10(-6) Pa(-1) s(-1) compared with spin-lattice relaxivity constants of (4.0 ± 0.4) × 10(-6) Pa(-1) s(-1) and (4.3 ± 1.3) × 10(-6) Pa(-1) s(-1), respectively. In vivo experimental measurements of alveolar oxygen partial pressure using (3) He in whole rat lung show good agreement (r(2) = 0.973) with predictions based on lung volumes and ventilation parameters. For (129) Xe, multicomponent relaxation was observed with one component exhibiting an increase in R(2) with decreasing alveolar oxygen partial pressure.

摘要

肺部中,超极化惰性气体(3)He 和(129)Xe 的弛豫率可用于测量肺泡氧分压的区域值。最近,已经证明可以在体内使用(3)He 的自旋-自旋弛豫率(R(2))在低磁场强度(<0.1T)下获得肺泡氧分压的测量值。可以使用 Carr-Purcell-Meiboom-Gill 脉冲序列有效地实现 R(2)测量。在这项工作中,介绍了基于 Carr-Purcell-Meiboom-Gill R(2)值的体外和体内(3)He 和(129)Xe 超极化在大鼠肺部在低磁场强度(74mT)下的肺泡氧分压测量值。(3)He 和(129)Xe 的体外自旋-自旋弛豫率常数分别确定为(5.2±0.6)×10(-6) Pa(-1) sec(-1)和(7.3±0.4)×10(-6) Pa(-1) s(-1),与自旋晶格弛豫率常数(4.0±0.4)×10(-6) Pa(-1) s(-1)和(4.3±1.3)×10(-6) Pa(-1) s(-1)相比。使用(3)He 在整个大鼠肺部进行的肺泡氧分压的体内实验测量与基于肺容量和通气参数的预测具有很好的一致性(r(2) = 0.973)。对于(129)Xe,观察到多组分弛豫,其中一个组分的 R(2)随着肺泡氧分压的降低而增加。

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