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CHAPTER 15: MOLECULAR LUMINESCENCE

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Title: CHAPTER 15: MOLECULAR LUMINESCENCE


1
CHAPTER 15 MOLECULAR LUMINESCENCE
2
LUMINESCENCE TECHNIQUES
  • Emission of light is used to determine certain
    properties,e e.g.structure and concentration, of
    the emitting species.
  • Deactivation processes involved in converting a
    substance from excited state to ground state
  • the emission of heat,
  • activation of a chemical reaction or
  • emission of radiation of the same or a modified
    wavelength.
  • Forms of photoluminescence (luminescence after
    absorption) are fluorescence (short lifetime) and
    phosphorescence (long lifetime).
  • Approximately 10x more sensitive than absorption
    techniquesppb detection limit
  • Limited number of systems that photoluminesce.
  • Luminescence observed for simple and complex
    systems and for all three phases.

3
Theory
  • Atoms e.g. dilute Na (g) the
  • 3s ?3p transition occurs by absorption at l
    5895 and 5890 A. with a lifetime ? 10-8 sec,
  • the electron returns to the ground state
    isotropically (isotropically) emitting hn with
    the wavelength of emission being the same as the
    wavelength of excitation. resonance fluorescence.
  • Polyatomic Systems
  • Resonance fluorescence observed
  • Emission of radiation of longer l (called a
    Stoke's shift) more common.. Most fluorescent
    systems are complex organic compounds with 1 or
    more aromatic functional groups so that the
    commonly observed transitions are
  • p p, p n, s s, s s.

4
EXCITED STATES
  • Multiplicity (number of lines observed when the
    molecule is placed in a magnetic field) is
    related number of unpaired spins in the molecule
    (S). M 2S 1.
  • Most molecules have an even number of electrons
    which means that all of their electrons in the
    ground state must be paired
  • Singlet state (M 20 1). all electrons in
    ground state paired.
  • Doublet state (M 2½ 1 2)a free radical
    (substance that has an odd number of electrons).
    electrons can have 2 orientations in the magnetic
    field-opposed to the field and aligned.
  • Triplet state (M 21 1 3), excited state
    in which excited electron spin is flipped so that
    the spins are parallel.
  • Singlet state Triplet state
  • Diamagnetic Paramagnetic
  • Probable Less probable
  • Lifetime 10-8-10-13sec Lifetime up to 1 s

5
ENERGY LEVEL DIAGRAM
  • Let ground , the first excited, second excited
    etc. electronic states be S0, S1, S2 and
    etc..for all of the possible singlet states.
  • Triplet states would then be T1, T2 and so on .
  • All electronic state has several vibrational and
    rotational states.

6
Decay Processes
  • Internal conversion Movement of electron from one
    electronic state to another without emission of a
    photon, e.g. S2 S1) lasts about 10?12 sec.
  • Predissociation internal conversion electron
    relaxes into a state where energy of that state
    is high enough to rupture the bond.
  • Vibrational relaxation (10?10-10?11sec)- Energy
    loss associated with electron movement to lower
    vibrational state without photon emission.
  • Intersystem crossing Conversion from singlet
    state to a triplet state. e.g. S1 to T1
  • External conversion is a non-radiative process in
    which energy of an excited state is given to
    another molecule (e.g. solvent or other solute
    molecules). Related to the collisional frequency
    of excited species with other molecules in the
    solution. Cooling the solution minimizes this
    effect.

7
QUANTUM YIELD
  • Only a fraction of the photon absorbed result in
    fluorescence. Fraction called Quantum yield
    (efficiency), F
  • Excite molecule in say the S1 state can undergo a
    transition back to the ground state S1 S0
    hn. The emitted photon is the useful
    fluorescence line and takes about 10-6-10-10 sec
    to occur.
  • Rate of all processes which involved the
    absorption or emission of a photon can be written
    in terms of a first order rate equation

8
KINETICS OF ADSORPTION
  • The intensity of the light absorbed is
  • .DP Po - PT rate of absorption where
  • Po photon flux to sample, PT photon flux out
    of sample.
  • At steady state rate of absorption equals rate of
    fluorescence or
  • DP (kIC kISC kf kQQ)S1
  • where kQ rate constant for quenching process-a
    second order process since the Q is also
    important in determining the relative rate of
    this process.
  • Let S1 steady state concentration of S1
    molecules. The rate of fluorescence Pf FDP
    F(kIC kISC kf kQQ)S1 and
  • Pf kfS1.
  • Combine and rearrange F
  • large F means a large kf.
  • The lifetime of the fluorescing state is given by
  • The inverse relationship between the rate
    constant and the lifetime tells us that a process
    having a large rate constant has a short lifetime
    and will have the largest fluorescence intensity.

9
FLUORESCENCE INTENSITY VS CONCENTRATION
  • Before fluorescence occurs absorption must
    occur. The absorption process given by Beer's
    Law
  • where e k/2.303 molar absorptivity. We will
    use this in the development of the fundamental
    equation for fluorescence.
  • Earlier we stated that
  • Pf rate of fluorescence F(kIC kISC kf
    kQQ)S1 FDP FPo - PT.
  • Beers law can be written as
  • PT Po10-ebC Poe-2.303ebC.
  • Substituting into the fluorescence equation
    gives
  • Pf FPo - Poe-2.303ebC FPo1 - e-2.303ebC.

10
Concentration Dependence 2
  • From the mathematics handbook
  • ex 1 x
  • We substitute this for the exponential terms to
    get the following
  • For dilute solutions A ebC is small which will
    make the squared and higher powered terms quite
    small.
  • e.g. if A 0.05, then the second term is while
    the first term is 2.3030.05 0.115.
  • The fluorescence equation then reduces to
  • Pf PoF2.303ebC or Pf KC or a linear
    response in the fluorescence intensity with
    concentration will be observed as long as the A lt
    0.05

11
Fluorescence Intensity vs Conc.
  • When performing a fluorometric analysis, Pf is
    measured independently of Po so that it is not
    necessary to determine P0 i.e. only one
    measurement of intensity is made.
  • Remember that Beers law for absorption requires
    measurement of both P and P0
  • In the fluorescence experiment, one can increase
    Po and should expect an increase in Pf. Thus,
    one can increase the sensitivity to the analyte
    by increasing the power of the exciting light.
  • In the absorption experiment, one needs the ratio
    of the input and output power. Increasing the
    input power also increases the output power but
    does little to the ratio.
  • This makes fluorescent techniques inherently more
    sensitive than absorption techniques. The
    detection limits are 10-8M in fluorimetry they
    are 10-12M.

12
F AND TRANSITION TYPE
  • In absorption spectrum of organics we can observe
    the following transitions to excited states s
    s n s p p n p.
  • Fluorescence p. p .Same orbitals possible.
  • .s s, and s n transitions are seldom
    observed however when the l of the transition is
    240 nm(UV) since the energy of the transition
    is often high enough to dissociate the molecule.
  • Less energetic transitions p p p n
    transitions observed.
  • .F, for the p p transition is usually greatest
    since process has shortest average lifetime and
    greatest molar absorptivity.
  • Other affects on the quantum yield In our
    equation describing quantum yield
  • .F
  • All terms except kf must be minimized to obtain a
    large fluorescent signal. Chemical structures
    that minimize one or more of the these rate
    constants increase the quantum yield.
  • Structural rigidity Decreases the chances of
    vibrational and rotational de-excitation (which
    we have called IC (internal conversion)..
    Prevents the loss of energy by the internal
    conversion process so that the fluorescent yield
    is higher in rigid molecules.
  • Ring structures with alternating single and
    double bonds (conjugation) that are aromatic
    usually best fluorescing compounds, although
    highly conjugated aliphatic compounds may also
    fluoresce.
  • Temperature Raising the temperature of a system
    increases the collisional frequency between
    excited molecules and the solvent which increases
    the amount of external conversion.
  • Solvent Decrease in solvent viscosity also leads
    to increase in external conversion and a decrease
    in fluorescence intensity.

13
PHOTOLUMINESCENT ANALYSIS
  • Since many compounds fluoresce at the same l,
    fluorescence cannot be used for qualitative
    analysis.
  • Quantitative analysis of a large number of
    organic compounds in particular polycyclic
    molecules with extensive conjugation possible.
  • E.g. Vitamin A which has a blue-green
    fluorescence with lmax 500 nm in ETOH.
  • Often molecules will be polynuclear aromatics
    such as phenol.
  • Inorganic species
  • Direct form a fluorescent complex with organic
    species and measure the fluorescent intensity.
    Fluorometric agents usually polyfunctional group
    aromatic compounds.
  • Indirect diminution of fluorescence measured
    when the ion is added to a fluorescent solution.
    Reaction stoichiometry between the ion and the
    fluorescent reagent must be known.

14
Fluorescence Problem
  • 5.00 mL of an unknown zinc solution was placed in
    each of two separatory funnels and 4.00 mL of
    1.10 ppm Zn2 was added to the second solution.
    Each was extracted with three 5 mL aliquots of
    CCl4 containing an excess of 8-hydroxyquinoline.
    The extracts were then diluted and their
    fluorescence measured with a fluorometer. The
    fluorescent intensities were 6.12 for the
    solution containing no added zinc and 11.16 for
    the other solution. Determine the concentration
    of the original zinc solution.
  • Strategy
  • Determine concentration of final solution
    containing the unknown (Standard Addition
    Method).
  • Determine concentration of the original solution.

15
INSTRUMENTATION
  • Source Hg or Xe arc lamp is used. (continuous
    radiation in the 250-600 nm range is produced).
  • Monochromators or filters needed to select both
    wavelength of excitation emission.
  • Monochromators are used when dealing with narrow
    absorption or emission peaks while filters may be
    used when peaks are not as narrow.
  • When filters are used, one is limited to
    wavelength range that passes through the
    particular filter used.
  • Instruments using filters are called fluorometers
    while instrument using monochromators are called
    spectrofluorimeter.
  • Cells and Cell compartments cylindrical or
    rectangular (less scattering rectangular cell)
    quartz or glass depending upon the wavelength
    range needed Outlet of the sample cell usually
    90 from the inlet.(minimizes source light at
    detector.
  • Detector Phototube or photomultiplier (small
    signals)

16
A Fluorometer or Spectrofluorometer
17
A Sectrofluorometer
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