Nonlinear effects induced in the normalized ion density in a linear trap system for a large ion cloud

2018 ◽  
Vol 53 (10) ◽  
pp. 927-933
Author(s):  
Laura Pedrosa-Rodriguez ◽  
D.A. Outerelo ◽  
Francisco J. Diaz-Otero
2021 ◽  
pp. 146906672110201
Author(s):  
NV Konenkov

The process of nonlinear resonant excitation of ion oscillations in a linear trap is studied. There is still no detailed simulation of the resonance peak in the literature. We propose to use the excitation contour to describe the collective ion resonance. The excitation contour is a resonant mass peak obtained by the trajectory method with the Gaussian distribution of the initial coordinates and velocities. The following factors are considered: excitation time, low order hexapole and octopole harmonics with amplitudes A3 and A4, the depth of the initial ion cloud position. These multipoles are used for selective ion ejection from linear ion trap. All these factors affect the ion yield and the shape of the contours. Obtained data can be useful for control of such processes as ion fragmentation, ion isolation, ion activation, and ion ejection. Simulated resonance peaks are important for the theoretical description of the ion collective nonlinear resonances.


2021 ◽  
Vol 31 (4) ◽  
pp. 41-54
Author(s):  
I. V. Kurnin ◽  

The paper presents an analytical model describing the dynamics of ion cloud, taking into account the action of space charge during a motion in ion mobility spectrometer — starting from the reaction region, where the shutter forms an ion pulse, and the further drift of the formed ion pulse towards the collector. The presented model lets to estimate the degree of influence of the space charge on possible ion losses and the resolution of ion mobility spectrometer. The effect of the space charge becomes noticeable, starting with the ion density of 106 cm–3. Comparison of the results obtained using the analytical model with the results of numerical solution of the initial equations shows that they practically coincide.


2008 ◽  
Vol 86 (1) ◽  
pp. 321-325 ◽  
Author(s):  
W Hu ◽  
Y Fu ◽  
P Gong ◽  
K Yao ◽  
D Lu ◽  
...  

In this report, a brief description of the current progress at the Shanghai EBIT project is presented. This is followed by a short discussion of the measurement of various parameters (electron beam diameter and ion density) under a number of operational conditions. A brief introduction to di-electronic recombination measurements for highly ionized xenon is given. Next, we present a preliminary measurement of the time dependence of xenon X-ray emission lines. Finally, a comparison of calculated and experimental charge-state distributions is given. This shows the influence of multi-electron capture and different distributions of the ion cloud on the charge state distribution.PACS Nos.: 41.85.–p; 34.80.Kw; 34.80Lx


2004 ◽  
Author(s):  
Riki Takeuchi ◽  
David P. Lepak ◽  
Sophia Marinova ◽  
Seokhwa Yun

1966 ◽  
Vol 90 (11) ◽  
pp. 435-489 ◽  
Author(s):  
Vadim N. Tsytovich
Keyword(s):  

1980 ◽  
Vol 130 (2) ◽  
pp. 357 ◽  
Author(s):  
T.S. Velichkina ◽  
O.I. Vasil'eva ◽  
A.N. Izrailenko ◽  
I.A. Yakovlev

2019 ◽  
pp. 77-88
Author(s):  
V.I. Dyrda ◽  
◽  
S.M. Grebenyuk ◽  
S.P. Sokol ◽  
S.B. Slobodian ◽  
...  
Keyword(s):  

2018 ◽  
Vol 1 (3) ◽  
pp. 2
Author(s):  
José Stênio De Negreiros Júnior ◽  
Daniel Do Nascimento e Sá Cavalcante ◽  
Jermana Lopes de Moraes ◽  
Lucas Rodrigues Marcelino ◽  
Francisco Tadeu De Carvalho Belchior Magalhães ◽  
...  

Simulating the propagation of optical pulses in a single mode optical fiber is of fundamental importance for studying the several effects that may occur within such medium when it is under some linear and nonlinear effects. In this work, we simulate it by implementing the nonlinear Schrödinger equation using the Split-Step Fourier method in some of its approaches. Then, we compare their running time, algorithm complexity and accuracy regarding energy conservation of the optical pulse. We note that the method is simple to implement and presents good results of energy conservation, besides low temporal cost. We observe a greater precision for the symmetrized approach, although its running time can be up to 126% higher than the other approaches, depending on the parameters set. We conclude that the time window must be adjusted for each length of propagation in the fiber, so that the error regarding energy conservation during propagation can be reduced.


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