The principle of LASER action involves
amplification of particular frequency emitted by the system
population inversion
stimulated emission
All ofthe above
Solar spectrum is an example for
line emission spectrum
continuous emission spectrum
band absorption spectrum
line absorption spectrum
Hydrogen atom does not emit X-rays because
it contains only a single electron
energy levels in it are far apart
its size is very small
energy levels in it are very close to each other
In the Bohr model of hydrogen atom, the electron is pictured to rotate in a circular orbit of radius 5 x 10-11 m at a speed 2.2 × 106 m/s. What is the current associated with electron motion ?
1.12 mA
3 mA
0.75 mA
2.25 mA
If an electron and a proton have the same de-Broglie wavelength, then the kinetic energy of the electron is
zero
less than that of a proton
more than that of a proton
equal to that of a proton
In ruby laser, the stimulated emission is due to transition from
metastable state to any lower state
any higher state to lower state
metastable state to ground state
any higher state to ground state
C.
metastable state to ground state
For a ruby laser, a crystal of ruby is formed into a cylinder. A fully reflecting mirror is placed on one end and a partially reflecting mirror on the other. A high-intensity lamp is spiraled around the ruby cylinder to provide a flash of white light that triggers the laser action. The green and blue wavelengths in the flash excite electrons in the chromium atoms to a higher energy level. Upon returning to their normal state, the electrons emit their characteristic ruby-red light. The mirrors reflect some of this light back and forth inside the ruby crystal, stimulating other excited chromium atoms to produce more red lght, until the light pulse builds up to high power and drains the energy stored in the crystal. In ruby laser stimulated emission is due to transition from metastable state to ground state.
The kinetic energy of an electron gets tripled, then the,de-Broglie wavelength associated with it changes by a factor
3
The spectral series of the hydrogen atom that lies in the visible region of the electromagnetic spectrum
Paschen
Balmer
Lyman
Brackett
According to the quark model, it is possible to build all the hadrons using
2 quarks and 3 antiquarks
3 quarks and 2 antiquarks
3 quarks and 3 antiquarks
2 quarks and 2 antiquarks