Ion collision cross section analyses in quadrupole ion traps using the filter diagonalization method: a theoretical study

2016 ◽  
Vol 18 (17) ◽  
pp. 12058-12064 ◽  
Author(s):  
Ting Jiang ◽  
Miyi He ◽  
Dan Guo ◽  
Yanbing Zhai ◽  
Wei Xu

Theoretical results show that an up to 200 resolving power could be achieved for ion collision cross section measurements in quadrupole ion traps.

2016 ◽  
Vol 18 (42) ◽  
pp. 29642-29642 ◽  
Author(s):  
Ting Jiang ◽  
Muyi He ◽  
Dan Guo ◽  
Yanbing Zhai ◽  
Wei Xu

Correction for ‘Ion collision cross section analyses in quadrupole ion traps using the filter diagonalization method: a theoretical study’ by Ting Jiang et al., Phys. Chem. Chem. Phys., 2016, 18, 12058–12064.


2013 ◽  
Vol 48 (8) ◽  
pp. 937-944 ◽  
Author(s):  
Yuzhuo Wang ◽  
Zejian Huang ◽  
You Jiang ◽  
Xingchuang Xiong ◽  
Yulin Deng ◽  
...  

2019 ◽  
Vol 18 ◽  
pp. 13
Author(s):  
A. Tsinganis ◽  
M. Diakaki ◽  
M. Kokkoris ◽  
A. Lagoyannis ◽  
C. T. Papadopoulos ◽  
...  

In the present work, the 197Au(n,2n) reaction cross section is studied within the framework of the Gen- eralized Superfluid Model (GSM). The cross sections for the population of the second isomeric state (12−) of 196Au and the sum of the ground (2−) and first isomeric state (5−) population cross sections were independently studied in the 8 to 25 MeV region with the use of the STAPRE-F, EMPIRE and TALYS codes, which were also compared in their implementation of the GSM. The theoretical results are compared with previous work in the same mass region and the strong dependence on the level scheme of the nuclei involved was revealed.


The Analyst ◽  
2014 ◽  
Vol 139 (23) ◽  
pp. 6144-6153 ◽  
Author(s):  
Muyi He ◽  
Dan Guo ◽  
Yu Chen ◽  
Xingchuang Xiong ◽  
Xiang Fang ◽  
...  

In this study, a method for measuring ion collision crosssections (CCSs) was proposed through time–frequency analysis of ion trajectories in quadrupole ion traps.


An important parameter in the quantum theory of molecular scattering as developed by Massey and Mohr is a quantity Q which corresponds roughly to a collision cross-section in classical theory. Of the quantities related to Q, that which is most directly accessible to observation is the decay constant of the intensity of a molecular beam traversing a scattering medium; the reciprocal of this constant corresponds to the mean free path of classical theory. Thus if I is the intensity of a beam which has passed through a distance d of a scattering medium, and I 0 is the original intensity, measured at the same distance from the source as is I, then I = I 0 e - d /λ , (1) where 1/λ is the decay constant; and we define Q by the relation λ = 1/Q v 2 √1 + m 1 / m 2 where m 1 , m 2 are the masses of the scattered and scattering molecules respectively, and v 2 is the molecular concentration of the scattering medium. The intensity I in equation (1) refers to those molecules which have suffered no deviation whatsoever in traversing the scattering medium. It is justifiable to assign this meaning to I, since quantum theory shows that if the interaction energy vanishes at infinity faster than 1/(distance) 2 , the ratio I/I 0 , and hence Q, is finite. Direct observation of the value of I/I 0 is, however, impossible, since it presumes an apparatus of infinite resolving power. Nevertheless, by using long narrow slits to define the beam, it is quite feasible to obtain angular apertures of only some 10 -4 radians without serious loss of intensity; and it is therefore pertinent to enquire how far the theory allows the deduction of the desired value of I/I 0 at zero angle from measurements made with beams of ribbon cross-section possessing small but finite apertures.


2009 ◽  
Vol 64 (1-2) ◽  
pp. 44-48
Author(s):  
Hwa-Min Kima ◽  
Young-Dae Jung

The nonthermal and plasmon effects on elastic electron-ion collisions are investigated in hot quantum Lorentzian plasmas. The modified interaction model taking into account the nonthermal screening and plasmon effects is employed to represent the electron-ion interaction potential in hot quantum Lorentzian plasmas. The eikonal phase and differential collision cross-section are obtained as functions of the impact parameter, collision energy, spectral index, and plasma parameters by using the second-order eikonal analysis. It is shown that the plasmon effect suppresses the eikonal phase and collision cross-section for 0 < β (ћω0/kBT < 0.6) and, however, enhances it for 0.6 < β < 1, where ω0 is the plasma frequency and T is the plasma temperature. It is also shown that the nonthermal character of the quantum Lorentzian plasma suppresses the elastic electron-ion collision cross-section.


The Analyst ◽  
2016 ◽  
Vol 141 (12) ◽  
pp. 3554-3561 ◽  
Author(s):  
Dayu Li ◽  
Yang Tang ◽  
Wei Xu

High-vacuum ion collision cross section (CCS) measurements in Fourier transform mass analyzers.


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