Tsybin Youri O, Witt Matthias, Baykut Gökhan, Håkansson Per
Division of Ion Physics, The Angström Laboratory, Uppsala University, Box 534, SE-751 21, Uppsala, Sweden.
Rapid Commun Mass Spectrom. 2004;18(14):1607-13. doi: 10.1002/rcm.1525.
Electron capture dissociation (ECD) of polypeptide cations was obtained with pencil and hollow electron beams for both sidekick and gas-assisted dynamic ion trapping (GADT) using Fourier transform ion cyclotron resonance mass spectrometry (FTICR-MS) with an electrostatic ion transfer line. Increasing the number of trapped ions by multiple ICR trap loads using GADT improved the ECD sensitivity in comparison with sidekick ion trapping and ECD efficiency in comparison with single ion trap load by GADT. Furthermore, enhanced sensitivity made it possible to observe ECD in a wide range of electron energies (0-50 eV). The degree, rate and fragmentation characteristics of ECD FTICR-MS were investigated as functions of electron energy, electron irradiation time, electron flux and ion trapping parameters for this broad energy range. The results obtained show that the rate of ECD is higher for more energetic (>1 eV) electrons. Long electron irradiation time with energetic electrons reduces average fragment ion mass and decreases efficiency of formation of c- and z-type ions. The obtained dependencies suggest that the average fragment ion mass and the ECD efficiency are functions of the total fluence of the electron beam (electron energy multiplied by irradiation time). The measured electron energy distributions in low-energy ECD and hot ECD regimes are about 1 eV at full width half maximum in employed experimental configurations.
使用带有静电离子传输线的傅里叶变换离子回旋共振质谱仪(FTICR-MS),通过铅笔束和空心电子束对多肽阳离子进行电子捕获解离(ECD),用于侧踢和气体辅助动态离子阱(GADT)。与侧踢离子阱相比,使用GADT通过多次ICR阱加载增加捕获离子的数量提高了ECD灵敏度;与GADT单次离子阱加载相比,提高了ECD效率。此外,灵敏度的提高使得在很宽的电子能量范围(0 - 50 eV)内观察ECD成为可能。针对这个宽能量范围,研究了ECD FTICR-MS的程度、速率和碎裂特征与电子能量、电子辐照时间、电子通量和离子阱参数的关系。所得结果表明,能量更高(>1 eV)的电子的ECD速率更高。高能电子的长时间辐照会降低平均碎片离子质量,并降低c型和z型离子的形成效率。所得的相关性表明,平均碎片离子质量和ECD效率是电子束总注量(电子能量乘以辐照时间)的函数。在所采用的实验配置中,低能ECD和热ECD模式下测得的电子能量分布在半高宽处约为1 eV。