Noise of Low-Energy Electron Beam
Identifikátory výsledku
Kód výsledku v IS VaVaI
<a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F68081731%3A_____%2F15%3A00464578" target="_blank" >RIV/68081731:_____/15:00464578 - isvavai.cz</a>
Nalezeny alternativní kódy
RIV/00216305:26220/15:PU119935
Výsledek na webu
<a href="http://dx.doi.org/10.1109/ICNF.2015.7288583" target="_blank" >http://dx.doi.org/10.1109/ICNF.2015.7288583</a>
DOI - Digital Object Identifier
<a href="http://dx.doi.org/10.1109/ICNF.2015.7288583" target="_blank" >10.1109/ICNF.2015.7288583</a>
Alternativní jazyky
Jazyk výsledku
angličtina
Název v původním jazyce
Noise of Low-Energy Electron Beam
Popis výsledku v původním jazyce
Noise diagnostics were performed on a tungsten hair-pin cathode operating in a vacuum (3 · 10(-3) Pa). The cathode operates in thermal emission mode at several temperatures based on the level of heating. Several acceleration voltages have been used starting at 5 kV, 10 kV and 20 kV up to 30 kV. There were two modes-with and without electron beam scanning. Both setups were compared from the point of view of the noise spectral density value. Shot noise is about one order below the current noise spectral density of the electron beam. Therefore, in this case the shot noise spectral density can be neglected. Noise spectral density is 1/f type at the frequency band 0.1 to 10 Hz for cathode with thin film of tungsten oxides. For accelerating voltage from 5 to 20 kV noise in the frequency band from 2 to 20 Hz can be described by the g-r noise with noise spectral density proportional to square of a beam current. At accelerating voltage 30 kV a new g-r noise component appears which is related to electric field distribution among anode, condensers, stigmators and objective.
Název v anglickém jazyce
Noise of Low-Energy Electron Beam
Popis výsledku anglicky
Noise diagnostics were performed on a tungsten hair-pin cathode operating in a vacuum (3 · 10(-3) Pa). The cathode operates in thermal emission mode at several temperatures based on the level of heating. Several acceleration voltages have been used starting at 5 kV, 10 kV and 20 kV up to 30 kV. There were two modes-with and without electron beam scanning. Both setups were compared from the point of view of the noise spectral density value. Shot noise is about one order below the current noise spectral density of the electron beam. Therefore, in this case the shot noise spectral density can be neglected. Noise spectral density is 1/f type at the frequency band 0.1 to 10 Hz for cathode with thin film of tungsten oxides. For accelerating voltage from 5 to 20 kV noise in the frequency band from 2 to 20 Hz can be described by the g-r noise with noise spectral density proportional to square of a beam current. At accelerating voltage 30 kV a new g-r noise component appears which is related to electric field distribution among anode, condensers, stigmators and objective.
Klasifikace
Druh
D - Stať ve sborníku
CEP obor
—
OECD FORD obor
20201 - Electrical and electronic engineering
Návaznosti výsledku
Projekt
<a href="/cs/project/TE01020118" target="_blank" >TE01020118: Elektronová mikroskopie</a><br>
Návaznosti
I - Institucionalni podpora na dlouhodoby koncepcni rozvoj vyzkumne organizace
Ostatní
Rok uplatnění
2015
Kód důvěrnosti údajů
S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů
Údaje specifické pro druh výsledku
Název statě ve sborníku
2015 International Conference on Noise and Fluctuations (ICNF) (Proceedings IEEE)
ISBN
978-1-4673-8335-6
ISSN
—
e-ISSN
—
Počet stran výsledku
4
Strana od-do
—
Název nakladatele
IEEE
Místo vydání
Piscataway
Místo konání akce
Xi’an
Datum konání akce
2. 6. 2015
Typ akce podle státní příslušnosti
WRD - Celosvětová akce
Kód UT WoS článku
000380427600048