A Comparative Study of Field Emission From Pristine, Ion‐Treated and Tungsten Nanoparticle‐Decorated p‐Type Silicon Tips

2019 ◽  
Vol 256 (9) ◽  
pp. 1800646 ◽  
Author(s):  
Victor I. Kleshch ◽  
Pavel Serbun ◽  
Dirk Lützenkirchen‐Hecht ◽  
Anton S. Orekhov ◽  
Victor E. Ivanov ◽  
...  
Author(s):  
Victor Kleshch ◽  
Pavel Serbun ◽  
Anton Orekhov ◽  
Dirk Lutzenkirchen-Hecht ◽  
Alexander Obraztsov ◽  
...  

1997 ◽  
Vol 18 (12) ◽  
pp. 616-618 ◽  
Author(s):  
Qing-An Huang ◽  
Ming Qin ◽  
Bin Zhang ◽  
J.K.O. Sin ◽  
M.C. Poon

2004 ◽  
Vol 85 (15) ◽  
pp. 3277-3279 ◽  
Author(s):  
S. Johnson ◽  
A. Markwitz ◽  
M. Rudolphi ◽  
H. Baumann ◽  
S. P. Oei ◽  
...  

1986 ◽  
Vol 71 ◽  
Author(s):  
H.B. Harrison ◽  
Y.H. Li ◽  
G.A. Sai-Halasz ◽  
S. Iyer

AbstractThis paper presents the results obtained from a comparative study of ion implanted Gallium (Ga) into (100), n type Silicon. A comparison is made between long time (≥ 30 mins) furnace annealed and Rapid Thermally Processed (RTP), 100keV implants of 1 and 3×10l5/cm2 doses of Ga. The results show that for RTP an extremely high substitutional concentration of Gallium, in excess of 3×1020/cm3 can be obtained with approximately 100% electrical activation, resulting in highly conductive very shallow p type layers.


1999 ◽  
Vol 558 ◽  
Author(s):  
T. Matsukawa ◽  
K. Tokunaga ◽  
S. Kanemaru ◽  
J. Itoh

ABSTRACTField emission characteristics from n- and p-type silicon gated emitter tips have been investigated in detail by means of experiments and theoretical estimation of band-bending induced by surface states. Single-tip emitters have been fabricated from n- and p-type silicon and their current-voltage characteristics have been evaluated. The field emission from the p-type emitter has been found to occur at lower extraction voltage than that of the n-type emitter. As the theoretical approach to the origin of the phenomena, potential distribution in the emitter tips has been calculated by using device simulation technique. The surface states of the n-type emitter tip are negatively charged and form a potential barrier against the electrons. On the contrary, there is no potential barrier in the p-type tips. The potential barrier in the n-type tip prevents electrons from reaching the tip apex. This is the reason why the emission current of the n-type emitter was suppressed lower than that of the p-type emitter.


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