Comparison between the imaging properties of two different types of electrostatic quadrupole doublet lenses

Optik ◽  
2017 ◽  
Vol 140 ◽  
pp. 860-865
Author(s):  
Oday A. Hussein
1971 ◽  
Vol 49 (21) ◽  
pp. 2651-2658 ◽  
Author(s):  
E. A. Youssef ◽  
F. E. Vermeulen ◽  
F. S. Chute

A study is made of the imaging properties of an electrostatic quadrupole that has been uniformly twisted about its axis. It is shown that the structure is capable of identically reproducing the injection coordinates and momenta of a system of particles in a coordinate plane which is located some distance along the quadrupole. The imaging takes place with a small amount of aberration. This aberration can be greatly reduced by constructing the lens of two sections which follow each other and which have equal and opposite twists.


1974 ◽  
Vol 52 (5) ◽  
pp. 379-386 ◽  
Author(s):  
F. E. Vermeulen ◽  
F. S. Chute ◽  
E. A. Youssef

A study is made of the imaging properties of an electrostatic quadrupole that has been uniformly twisted about its axis. Such a quadrupole has been built, and it is shown experimentally that the quadrupole identically reproduces the injection coordinates and momenta of a system of particles in a coordinate plane which is located some distance along the quadrupole axis. The experiments have been conducted using a beam of electrically charged micron sized dust particles.


2014 ◽  
Vol 332 ◽  
pp. 301-310 ◽  
Author(s):  
Daniel Weigel ◽  
Holger Babovsky ◽  
Armin Kiessling ◽  
Richard Kowarschik

1991 ◽  
Vol 9 (4) ◽  
pp. 863-867
Author(s):  
B. Heimrich ◽  
H. J. Laue ◽  
H. Wollnik

For first investigations of hot dense matter produced by intense heavy-ion beams we built an electrostatic quadrupole doublet that focused Ar+and Kr+ ions of 45 keV/amu after acceleration through the radio frequency quadrupole (RFQ) accelerator at the GSI onto a small spot of approximate area 1 mm2. This beam then deposited a specific beam power of about 1.5 GW/g to targets.


2018 ◽  
Vol 89 (8) ◽  
pp. 086103
Author(s):  
Jack E. Manuel ◽  
Szabolcs Z. Szilasi ◽  
Todd A. Byers ◽  
Dustin Z. Phillips ◽  
Alexander D. Dymnikov ◽  
...  

1986 ◽  
Vol 23 (04) ◽  
pp. 851-858 ◽  
Author(s):  
P. J. Brockwell

The Laplace transform of the extinction time is determined for a general birth and death process with arbitrary catastrophe rate and catastrophe size distribution. It is assumed only that the birth rates satisfyλ0= 0,λj> 0 for eachj> 0, and. Necessary and sufficient conditions for certain extinction of the population are derived. The results are applied to the linear birth and death process (λj=jλ, µj=jμ) with catastrophes of several different types.


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