07.01.2014 Views

CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...

CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...

CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

luminescence from the 5 D J states of Eu 3+ . The intensity of these transitions depends strongly<br />

on the site symmetry in a host crystal. Magnetic dipole allowed f-f transitions are not affected<br />

much by the site symmetry. The J selection rule in this case is ΔJ = 0, ±1 (except for 0→0).<br />

For electric dipole transition, the difference in the J values (ΔJ) is ±2. Oscillator strengths<br />

are of the order of 10 –5 to 10 –8 for electric dipole transitions, and 10 –8 for magnetic dipole<br />

transitions [31].<br />

1.5.3 Luminescence quenching: Luminescence can be quenched due to the non-radiative<br />

decay of the excited state. This non-radiative decay is brought about by different mechanisms<br />

involving energy transfer from the excited state of the donor to different types of acceptors<br />

like host lattice, organic molecules on the surface, defect levels or nearby ions which may or<br />

may not act as activator. In the following section different types of non-radiative path ways of<br />

the excited state is given.<br />

Multiphonon emission: As discussed in the previous section (equation 5) it is clear that the<br />

extent of quenching due to phonons depends on the energy gap between the emitting states<br />

and value of phonon energy. General observation is that if the energy difference is more than<br />

5 times the phonon energy, then luminescence is the main de-excitation process than the<br />

multi-phonon quenching [42]. This also explains the quenching of lanthanide ions excited<br />

state by organic molecules containing functional groups with high phonon energy. Hence,<br />

efforts for the development of new efficient luminescent materials based on Ln 3+ ions are<br />

directed towards the search for low effective phonon energy host materials. The general order<br />

of phonon energy of hosts are fluorides < sulfides < oxides < phosphates.<br />

Energy transfer: An excited state can also relax to the ground state by non-radiative energy<br />

transfer to a second nearby state/ center. For energy transfer to take place the energy levels of<br />

the donor and acceptor should match. However, when there is a mismatch between the energy<br />

levels/ transitions of the donor and acceptor ions, the energy transfer process needs to be<br />

18

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!