The improvement of the detector susceptibility for carrying out the neutrino investigations on the electron magnetic spectrometer

2011 ◽  
Vol 221 ◽  
pp. 391-393
Author(s):  
G.V. Sapozhnikov ◽  
A.V. Kholzakov ◽  
I.N. Shabanova ◽  
A.E. Kazanzev
2004 ◽  
Vol 137-140 ◽  
pp. 383-385 ◽  
Author(s):  
V.A Trapeznikov ◽  
I.N Shabanova ◽  
A.V Kholzakov ◽  
A.G Ponomaryov

2012 ◽  
Vol 83 (10) ◽  
pp. 10D311 ◽  
Author(s):  
Y. Kim ◽  
H. W. Herrmann ◽  
T. J. Hilsabeck ◽  
K. Moy ◽  
W. Stoeffl ◽  
...  

2008 ◽  
Vol 136 (4) ◽  
pp. 042057
Author(s):  
G V Sapozhnikov ◽  
A V Kholzakov ◽  
I N Shabanova ◽  
A E Kazantzev

2017 ◽  
Vol 60 (5) ◽  
pp. 690-694 ◽  
Author(s):  
A. V. Rusakov ◽  
K. A. Ivanov ◽  
N. A. Borisov ◽  
I. N. Tsymbalov ◽  
D. A. Gorlova ◽  
...  

2014 ◽  
Vol 85 (11) ◽  
pp. 11E122 ◽  
Author(s):  
Y. Kim ◽  
H. W. Herrmann ◽  
H. J. Jorgenson ◽  
D. B. Barlow ◽  
C. S. Young ◽  
...  

2003 ◽  
Vol 32 (3) ◽  
pp. 389-394
Author(s):  
G.C. Ho ◽  
D.G. Mitchell ◽  
S. Livi ◽  
D.K. Haggerty ◽  
B.H. Mauk

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.


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