How can i build electron canyon?

  • Thread starter Thread starter edson jair
  • Start date Start date
  • Tags Tags
    Build Electron
edson jair
Messages
4
Reaction score
0
hi, I'm new in this forum, i was wondering how to build an electron canyon? does somebody knows?
 
Physics news on Phys.org
What do you mean by an "electron canyon"?
 
"Electron cannon"? An accelerator for electrons? I would use existing cathode ray tubes. The basic concept is one hot wire (emitting electrons) and a potential difference (accelerating the electrons) in a vacuum.
 
thanks a lot, sorry about my writting
 
Thread 'Why is there such a difference between the total cross-section data? (simulation vs. experiment)'

Thread 'Why is there such a difference between the total cross-section data? (simulation vs. experiment)'

Well, I'm simulating a neutron-proton scattering phase shift. The equation that I solve numerically is the Phase function method and is $$ \frac{d}{dr}[\delta_{i+1}] = \frac{2\mu}{\hbar^2}\frac{V(r)}{k^2}\sin(kr + \delta_i)$$ ##\delta_i## is the phase shift for triplet and singlet state, ##\mu## is the reduced mass for neutron-proton, ##k=\sqrt{2\mu E_{cm}/\hbar^2}## is the wave number and ##V(r)## is the potential of interaction like Yukawa, Wood-Saxon, Square well potential, etc. I first...
View full post »

Thread 'Toponium Discovered'

Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
View full post »

Thread 'Dirac-Delta from Normalization of Continuous Eigenfunctions'

I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...
View full post »

Similar threads

I Can surface plasmons be used to build GeV gamma-ray lasers?
Replies
2
Views
2K
A Can cooling enhance the monochromaticity of an electron beam?
Replies
13
Views
2K
A Thomson - Rayleigh Scattering: Rotational & Vibrational Energy Levels
Replies
12
Views
3K
A Fast electrons passing a beam of slow electrons at a right angle
Replies
2
Views
2K
A Atmospheric electron neutrinos
Replies
11
Views
2K
B Can a hypothetical atom be made out of positrons and electrons ?
Replies
9
Views
3K
I Electrons from Internal Conversion
Replies
6
Views
2K
I How often would a ϕ meson decay to a electron-positron pair?
Replies
2
Views
2K
I Channel electron multiplier as an electron source
Replies
2
Views
2K
I Experiment finds gluon mass in the proton (?)
Replies
12
Views
3K

Hot Threads

Recent Insights

Back
Top