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• Quantum yield of fluorescence, Ff, is defined as
In practice, is measured by comparative measurements with reference
compound for which has been determined with high degree of accuracy.
Fluorescein
• Ideally, reference compound should have
– the same absorbance as the compound of interest at given excitation wavelength
– similar excitation-emission characteristics to compound of interest
– Same solvent, because intensity of emitted light is dependent on refractive index
(otherwise, apply correction
absorbedphotonsofnumber
emittedphotonsofnumber
F f
)(
)(
2
2
sn
un
I
I
s
f
u
f
s
f
u
f

F
F
1a. Quantum yield of fluorescence
Another definition for Ff is
where kr is the radiative rate constant and Sk is the sum of the rate
constants for all processes that depopulate the S1 state.
 In the absence of competing pathways Ff=1
 The observed fluorescence lifetime, is the average time the
molecule spends in the excited state, and it is

F
k
kr
f


k
f
1

Fluorescence lifetime
 Illumination source
 Broadband (Xe lamp)
 Monochromatic (LED, laser)
 Light delivery to sample
 Lenses/mirrors
 Optical fibers
 Wavelength separation (potentially for both excitation and
emission)
 Monochromator
 Spectrograph
 Detector
 PMT
 CCD camera
PMT
Xenon Source
Excitation
Monochromator Emission
Monochromator
Sample compartment
Fluorescence Instrumentation
Spectrofluorometer schematic
Phosphorescence:
T1  S1  S0 + hn
Intersystem crossing
Because intersystem crossing is a “forbidden” process which occurs
with low intensity with low probability phosphorescence is a slow
process where photons may be emitted over a period of fractions of
seconds to hours
•Phosphoresence – return from a triplet excited state
to a ground state; electron requires change in spin
orientation
The sequence leading
to phosphorescence:
The intersystem crossing
is the key step, where
T1  S1.
The triplet state acts
as a slowly leaking
reservoir, in that this
transition is normally
spin-forbidden
T1
S1
S0
T1  S1
Phosphorescence:
* Phosphorence spectra occure at longer wave length
Long life time, (10-6 to 102 Sec
Phosphoresence is not routinly obsereved at room temp.
(quenching of triplet excited state by oxygen)
Degasing is required
Several methods have been used to enable the observation of
phosphorescence,
One of the most commontechniques is to supercool solutions to a
rigid glass state usually at the temperature of liquid nitrogen (77 K).
At these low temperatures, molecular
collisions are greatly reduced and strong phosphorescence signals
are observed.
Due to long life-times, the molecule has a very high probability
of losing its excess energy by radiativeless routes such as internal
conversion, bimolecular collision, and photodecompositions
Inorganic salts and oxides of rare earths, europium, and Uranium
show phosphoresence
Compounds exhibit phosphorescence when adsorbed onto
certain substrates such as paper, cellulose, silica, etc.
*Phosphoroscope
*Two types of Phosphoroscopes
1) Rotating disc
2) Rotating can Phosphoroscope
*Measurement of Phosphoresence
*Samples are prepared in rigid media (polymer matrix)
*Temperature (liquid nitrogen)
• good solubility of the analyte
• formation of a clear rigid glass at 77 K
• low phosphorescence background (high
purity)
Polar compounds, ethanol is an excellent solvent and small
quantities of base or acid may be added to produce a clear solid.
For non-polar compounds, the most popular solvent is a
mixture of diethyl ether, isopentane and ethanol in the ratioof 5 :
5 : 2 respectively, called EPA

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Quantum yeild

  • 1. • Quantum yield of fluorescence, Ff, is defined as In practice, is measured by comparative measurements with reference compound for which has been determined with high degree of accuracy. Fluorescein • Ideally, reference compound should have – the same absorbance as the compound of interest at given excitation wavelength – similar excitation-emission characteristics to compound of interest – Same solvent, because intensity of emitted light is dependent on refractive index (otherwise, apply correction absorbedphotonsofnumber emittedphotonsofnumber F f )( )( 2 2 sn un I I s f u f s f u f  F F 1a. Quantum yield of fluorescence
  • 2. Another definition for Ff is where kr is the radiative rate constant and Sk is the sum of the rate constants for all processes that depopulate the S1 state.  In the absence of competing pathways Ff=1  The observed fluorescence lifetime, is the average time the molecule spends in the excited state, and it is  F k kr f   k f 1  Fluorescence lifetime
  • 3.  Illumination source  Broadband (Xe lamp)  Monochromatic (LED, laser)  Light delivery to sample  Lenses/mirrors  Optical fibers  Wavelength separation (potentially for both excitation and emission)  Monochromator  Spectrograph  Detector  PMT  CCD camera
  • 4. PMT Xenon Source Excitation Monochromator Emission Monochromator Sample compartment Fluorescence Instrumentation Spectrofluorometer schematic
  • 5. Phosphorescence: T1  S1  S0 + hn Intersystem crossing Because intersystem crossing is a “forbidden” process which occurs with low intensity with low probability phosphorescence is a slow process where photons may be emitted over a period of fractions of seconds to hours •Phosphoresence – return from a triplet excited state to a ground state; electron requires change in spin orientation
  • 6. The sequence leading to phosphorescence: The intersystem crossing is the key step, where T1  S1. The triplet state acts as a slowly leaking reservoir, in that this transition is normally spin-forbidden T1 S1 S0 T1  S1 Phosphorescence:
  • 7. * Phosphorence spectra occure at longer wave length Long life time, (10-6 to 102 Sec Phosphoresence is not routinly obsereved at room temp. (quenching of triplet excited state by oxygen) Degasing is required Several methods have been used to enable the observation of phosphorescence, One of the most commontechniques is to supercool solutions to a rigid glass state usually at the temperature of liquid nitrogen (77 K). At these low temperatures, molecular collisions are greatly reduced and strong phosphorescence signals are observed. Due to long life-times, the molecule has a very high probability of losing its excess energy by radiativeless routes such as internal conversion, bimolecular collision, and photodecompositions
  • 8. Inorganic salts and oxides of rare earths, europium, and Uranium show phosphoresence Compounds exhibit phosphorescence when adsorbed onto certain substrates such as paper, cellulose, silica, etc. *Phosphoroscope *Two types of Phosphoroscopes 1) Rotating disc 2) Rotating can Phosphoroscope
  • 9. *Measurement of Phosphoresence *Samples are prepared in rigid media (polymer matrix) *Temperature (liquid nitrogen) • good solubility of the analyte • formation of a clear rigid glass at 77 K • low phosphorescence background (high purity) Polar compounds, ethanol is an excellent solvent and small quantities of base or acid may be added to produce a clear solid. For non-polar compounds, the most popular solvent is a mixture of diethyl ether, isopentane and ethanol in the ratioof 5 : 5 : 2 respectively, called EPA