Absorption First Followed by emission of photons in all the direction at lower frequencies
Types of luminescence
Chemiluminescence
Phosphorescence
Fluorescence
Photoluminescence
Collectively Fluorescence and Phosphoresces
Chemiluminescence
Emission of light from an excited species as a result of a chemical rection
Fluorescence
Emission of light by a substance that has absorbed light or other electromagnetic radiation
Fluorescence process
Molecule is excited from ground to excited state due to photon absorption
Excited state is unstable – decays back to ground state, emitting light in the process (fluorescence)
Examples of fluorophores
Ethidium bromide (EtBr)
Phosphor
Fluorescein
Jellyfish Green fluorescent proteins
Green fluorescent protein (GFP)
Small and inert molecule, can be fused to any protein for imaging
Widespread applications in biology., imaging, transgenics
Emission spectrum
Recorded by measuring the intensity of emitted radiation as a function of the emission wavelength
Emission spectrum
Absorption of a photon of energy by a fluorophore, is an all or none phenomenon
Can only occur with incident light within the absorption range (strongest @ excitation maximum = peak in absorbance curve)
Temperature variation induces modification of global and local motions of the fluorophore environment and of the fluorophore itself, modifying its fluorescence emission feature
The intensity, position of the emission wavelength, and lifetime are some of the observables that will characterize a fluorophore
Quantum Efficiency
Fluorescence Quantum efficiency (f) is the ratio of the # photons absorbed versus the # of emitted fluorescent photons. It is measured from 0 to 1 or in % (0to 100%)
It gives the probability of the excited state being deactivated by fluorescence rather than by another, non-radiative mechanism
Fluorescence intensity, F is proportional to the radiant power of the excitation beam absorbed by the species able to undergo fluorescence
F= k f (I0-I) where I0 is the power incident on the sample, I is the power after it traverses a length b of the solution, k is a constant depending on experimental factors, f fluorescence quantum efficiency
Beer's law
I/I0=10-ebc and I=I0 10-ebc
F= k f I0 (1- 10-ebc)
F is not linear with concentration (Unlike Beer's Law)
F= k f I0 ebc, Fluorescence intensity is α to concentration
Jablonski diagrams
Classically presents the various energy levels involved in the absorption and emission of light by a fluorophore
Jablonski diagrams
Straight arrows = absorption or emission of a photon (instantaneous process)
Wavy arrows = molecular internal conversion or non-radiative relaxation process (long timescales)
Thicker lines = electronic energy levels (S0, S1… Sn)
Thinner lines = vibrational energy states (0,1,2,3 etc)
Franck-Condon energy diagrams
In the excited state, the electron is promoted to an anti-bonding orbital
Atoms in the bond are less tightly held (so potential energy curve shift to the right for S1)
Overview of fluorescence process
1. Excitation
2. Non-radiative processes
3. Emission
Absorption of energy takes place on a time scale (10-15 s)
Excitation lifetime
Duration at which the molecule stays at the excited states S1 or S2
Energy diagrams
Graphical representation of energy levels and transitions
In the excited state, the electron is promoted to an anti-bonding orbital
Atoms in the bond are less tightly held (so potential energy curve shift to the right for S1)
Fluorescence process
Excitation
Non-radiative processes
Emission
Excitation
1. Absorption of energy takes place on a time scale (10-15 s)
2. Molecule is excited to higher vibrational energy level of S1 or S2
Non-radiative processes
1. Molecule relaxes to the lowest vibrational energy level of the first excited state S1(0)
2. Internal conversion (loss of energy in the absence of light emission) occurs within 10–12 s or less
As electronic energy increases, the energy levels grow more closely spaced
The energy gap between S1 and S0 is significantly larger compared to other adjacent states, hence S1 lifetime is longer and radiative emission can compete effectively with non-radiative emission
Emission
1. Molecule relaxes to ground state S0
2. Emission of photon (of lower energy than absorbed photon) => fluorescence
3. Fluorescence occurs at a time scale of 10-8 s-tens of nanoseconds regime
Singlet ground state (S0)
Two electrons per orbital; electrons have opposite spin and are paired
Singlet excited state (S1, S2 … Sn)
One electron per orbital; electron in higher energy orbitals has the opposite spin orientation relative to electron in the lower orbital
Triplet excited state (T1, T2…Tn)
One electron per orbital; the excited valence electron may spontaneously reverse its spin (spin flip) so that electrons in both orbitals now have same spin orientation
Intersystem crossing
Non-radiative transition between states of different multiplicity via inversion of the spin of the excited electron
Transitions between states of different multiplicity are in principle forbidden (e.g., S0 → T1,2)
T1 → S0 is also forbidden without emission, instead phosphorescence occurs as molecule returns from T1 to S0 on a long time scale of 10-3-102 s