The magnetic spectrometer at Vicksi

Author(s):  
H. G. Bohlen
Author(s):  
A. Kosiara ◽  
J. W. Wiggins ◽  
M. Beer

A magnetic spectrometer to be attached to the Johns Hopkins S. T. E. M. is under construction. Its main purpose will be to investigate electron interactions with biological molecules in the energy range of 40 KeV to 100 KeV. The spectrometer is of the type described by Kerwin and by Crewe Its magnetic pole boundary is given by the equationwhere R is the electron curvature radius. In our case, R = 15 cm. The electron beam will be deflected by an angle of 90°. The distance between the electron source and the pole boundary will be 30 cm. A linear fringe field will be generated by a quadrupole field arrangement. This is accomplished by a grounded mirror plate and a 45° taper of the magnetic pole.


2015 ◽  
Vol 04 (01) ◽  
pp. 28-30
Author(s):  
Yuan-Hann Chang

It is known that the majority (about 80%) of the matter in the universe is not visible, but rather a hypothetical "Dark Matter". The existence of Dark Matter has been postulated to explain the discrepancies between the estimated mass of visible matters in the galaxies, and their gravitational effects. Although it has been postulated for over 70 years, and has been commonly accepted by most scientists, the essence of the Dark Matter has not yet been understood. In particular, we still do not know what constitutes the Dark Matter. Direct detection of the Dark Matter is therefore one of the most important issues in physics.


Author(s):  
J. Alcaraz ◽  
B. Alpat ◽  
G. Ambrosi ◽  
H. Anderhub ◽  
L. Ao ◽  
...  

2007 ◽  
Author(s):  
Marco Molina ◽  
Christian Vettore ◽  
Ivan Corradino ◽  
Gongming Xin ◽  
Zhongchao Zhao ◽  
...  

1973 ◽  
Vol 26 (1) ◽  
pp. 17 ◽  
Author(s):  
CE Moss ◽  
RH Spear ◽  
F Ahmad ◽  
AM Baxter ◽  
LE Carlson ◽  
...  

The reaction 32S(p,p'y)32S has been studied with a 12'7 cm by 10�2 cm NaI(TI) y-ray detector in conjunction with a 61 cm double-focusing magnetic spectrometer to determine the y-ray decay schemes of all known levels in 32S between the excitation energies of 5�40 and 7� 15 MeV.


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