Parikh Raj A, Alexander Andrew W, Jarrold Martin F
Chemistry Department, Indiana University, 800 E Kirkwood Ave, Bloomington, Indiana 47405.
J Am Soc Mass Spectrom. 2025 Oct 1;36(10):2290-2298. doi: 10.1021/jasms.5c00236. Epub 2025 Sep 9.
In charge detection mass spectrometry (CD-MS) ions are trapped in an electrostatic linear ion trap (ELIT) where they oscillate back and forth through a conducting cylinder. The oscillating ions induce a periodic charge separation that is detected by a charge sensitive amplifier (CSA) connected to the cylinder. The resulting time domain signal is analyzed using short-time Fourier transforms to give the mass-to-charge ratio and charge for each ion, which are then multiplied to give the mass. For ions to be assigned to the correct integer charge states with a low error rate, the charge should be measured with a precision of <0.2 e (elementary charges). Electrical noise reduces the precision of the charge measurement. However, the effect of the noise can be ameliorated by signal averaging, and the measurement time can, in principle, be increased to achieve a precision of <0.2 e. Previously, through optimized ELIT design and improvements to the CSA, the measurement time (with a cryogenically cooled input JFET) required to achieve a charge precision of <0.2 e was reduced by a factor of 2, from 3 s to 1.5 s. In this study, further improvements in JFET selection, capacitance matching, and cryogenic cooling has allowed us to further reduce the electrical noise so that the target precision of <0.2 e can now be achieved for mAb MSQC4 in 600-700 ms with the input JFET cryogenically cooled, and in 900-1000 ms with the input JFET at room temperature. This performance upgrade cuts the overall time for high-resolution charge measurements by more than another factor of 2. For a measurement time of 100 ms, the charge RMSD is 0.51 e with cryogenic cooling. The results presented here further cements CD-MS with an ELIT as the fastest and most accurate approach to single ion MS measurements.
在电荷检测质谱法(CD-MS)中,离子被捕获在一个静电线性离子阱(ELIT)中,在那里它们通过一个导电圆柱体来回振荡。振荡的离子会引起周期性的电荷分离,由连接到圆柱体的电荷敏感放大器(CSA)进行检测。利用短时傅里叶变换对得到的时域信号进行分析,以给出每个离子的质荷比和电荷,然后将它们相乘得到质量。为了以低错误率将离子分配到正确的整数电荷态,电荷测量的精度应<0.2 e(基本电荷)。电噪声会降低电荷测量的精度。然而,通过信号平均可以改善噪声的影响,原则上可以增加测量时间以达到<0.2 e的精度。此前,通过优化ELIT设计和改进CSA,实现<0.2 e电荷精度所需的测量时间(使用低温冷却的输入结型场效应晶体管)减少了一半,从3秒降至1.5秒。在本研究中,通过进一步改进结型场效应晶体管的选择、电容匹配和低温冷却,我们能够进一步降低电噪声,从而在输入结型场效应晶体管低温冷却的情况下,对于mAb MSQC4现在可以在600 - 700毫秒内达到<0.2 e的目标精度,在输入结型场效应晶体管处于室温的情况下,在900 - 1000毫秒内达到该精度。这种性能提升将高分辨率电荷测量的总时间又缩短了一半以上。对于100毫秒的测量时间,低温冷却时电荷均方根偏差为0.51 e。此处呈现的结果进一步巩固了使用ELIT的CD-MS作为单离子质谱测量最快且最准确方法的地位。