Light Rays: Photons, Electrons & Gratings

EIRE2003
Messages
107
Reaction score
0
1. The light rays from the sun and artificial lights, are all light rays made up of 'photons' which travel in the form of waves?

2. During a sunstorm, when the Auroras form in the ionosphere by electrons colliding with atomic o2 and atomic nitrogen, can these electrons be thought of as 'Beta Rays'?

3. When a beam of white light is diffracted in a grating and dispersed into its component colours, do all these photons of light have the same energies yea?
 
Physics news on Phys.org
1. The light rays from the sun and artificial lights, are all light rays made up of 'photons' which travel in the form of waves?
Yes

2. During a sunstorm, when the Auroras form in the ionosphere by electrons colliding with atomic o2 and atomic nitrogen, can these electrons be thought of as 'Beta Rays'?
The term "beta rays" is usually reserved for electrons that are emitted during radioactive decay. However all electrons are the same.

3. When a beam of white light is diffracted in a grating and dispersed into its component colours, do all these photons of light have the same energies yea?
Photon energies are directly proportional to frequency (inverse of wavelength). Therefore energy depends on color.
 
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...
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}...
Back
Top