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Chapter 6
Photoluminescence Spectroscopy
Sib Krishna Ghoshal (PhD)
Advanced Optical Materials Research Group
Physics Department, Faculty of Science, UTM
Course Code: SSCP 4473
Course Name: Spectroscopy & Materials Analysis
What is Photoluminescence?
Photoluminescence (PL) is a process in which the substance
absorbs photons (EM radiation) and then re-radiates photons.
Presentation Outline
 What is Photoluminescence?
 Basic Physics of luminescence
 Principle of PL
 How PL spectroscopy is performed?
 What information it captures?
 Examples
 Applications
 Conclusion
Very powerful tool for low
dimensional systems,
especially for semiconductors!!
Finding right solar material
and up-converted lasing
material is challenging!!
E0
E1
u
A material that emits light is called luminescent material.
Greek word phosphor (light bearer) is usually used to describe
luminescent nature.
 It emits energy from an excited electronic state as light.
 Some of the incident energy is absorbed and re-emitted as
light of a longer wavelength (Stoke’s law).
 The wavelength of the emitted light is characteristic of the
luminescent substance and not of the incident radiation.
 The emitted light carries the materials signature.
Definition of Luminescence
Characteristics PL
frequencies
Changes in
Frequency of PL
peaks
Polarization of PL
peak
Width of PL peak
Intensity of PL
peak
Composition
Stress/Strain
State
Symmetry/
Orientation
Quality
Amount
Analyses of Samples Fingerprints
Captured by PL Spectra
One broad peak may be
superposition of two or
several peaks: De-
convolution is needed
 Number of peaks
 Peak Intensities
 Peak position
 FWHM
 Peak shape
 It operates from 200 nm to 900 nm wavelength.
 Below 200 nm it needs vaccum because air can absorb much UV light.
 UTM machine does not cover the time and field dependent fluorescence
decay.
Perkin Elmer LS 55
Luminescence Spectrometer
 Photoluminescence implies both Fluorescence and
Phosphorescence.
One broad peak may be superposition of two or several peaks:
De-convolution is needed.
 Main peak may accompanied with kinks, shoulder or satellites.
Basic Physics
Fluorescence – ground state to singlet state and back.
Phosphorescence - ground state to triplet state and back.
Fluorescence: A Type of
Light Emission
• First observed from quinine by Sir J. F. W. Herschel in 1845
Blue glass
Filter
Church Window!
<400nm
Quinine
Solution
Yellow glass of wine
Em filter > 400 nm
1853 G.G. Stoke coined
term “fluorescence”
Forms of photoluminescence (luminescence after absorption)
are fluorescence (short lifetime) and phosphorescence (long
lifetime).
Common Fluorophores
Typically, Aromatic molecules
– Quinine, ex 350/em 450
– Fluorescein, ex 485/520
– Rhodamine B, ex 550/570
– POPOP, ex 360/em 420
– Coumarin, ex 350/em 450
– Acridine Orange, ex 330/em 500
– Many SC & Low dimensional SC
systems
– Some Minerals
– Materials in low dimension
– Glass with Rare Earth Ions
The initial excitation takes place
between states of same multiplicity
and in accord with the Franck-Condon
principle.
What is Fluorescence?
 Fluorescence is a photoluminescence process in which atoms or molecules
are excited by the absorption of electromagnetic radiation. The excited
species then relax to the ground state, giving up their excess energy as
photons.
Attractive features
 One to three orders of magnitude better than absorption spectroscopy,
even single molecules can be detected by fluorescence spectroscopy.
 Larger linear concentration range than absorption spectroscopy.
Shortcomings
 Much less widely applicable than absorption methods.
 More environmental interference effects than absorption methods.
Fluorescence ?
Highly sensitive technique
 1,000 times more sensitive than UV-visible spectroscopy.
 Often used in drug or drug metabolite determinations by HPLC (high
performance liquid chromatography) with fluorimetric detector.
 Non-fluorescing compounds can be made fluorescent – derivitisation.
Selective versatile technique
 Since excitation and emission wavelengths are utilized, gives selectivity
to an assay compared to UV-visible spectroscopy.
 Differing modes of spectroscopy yield wide versatility.
Advantages of Fluorescence
Spectroscopy
Various Transitions
Luminescence
 “Inverse” of absorption
 Consequence of radiative
recombination of excited electrons
Compete with non-radiative
recombination processes
 PL: non-equilibrium obtained by
photons
 Important for Laser, LED and
optoelectronics
Radiative: Visible photon
Nonradiative: Thermal photon
Typical Fluorescence Spectra
Fluorescence spectra of 9-
Anthracenecarboxylic Acid
Fluorescence spectra for 1
ppm anthracene in alcohol
Transitions & Time Scales,
Energy Scale…
Jablonski Energy Diagram
Property of Luminescence
Spectrum
Fluorescence vs Phosphorescence
 Phosphorescence is always at longer wavelength compared with
fluorescence
 Phosphorescence is narrower compared with fluorescence
 Phosphorescence is weaker compared with fluorescence
Absorption vs Emission
 absorption is mirrored relative to emission
 Absorption is always on the shorter wavelength compared to emission
 Absorption vibrational progression reflects vibrational level in the
electronic excited states, while the emission vibrational progression
reflects vibrational level in the electronic ground states
 0 transition of absorption is not overlap with the 0 of emission
Why?
Why?
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: A nonradiative 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.
Fluorescent Species
All absorbing molecules have the potential to fluoresce, but most
compounds do not.
Quantum Yield
absorbed
Photons
emitted
Photons
molecules
excited
of
number
Total
fluoresce
that
molecules
of
Number
or


Structure determines the relaxation and fluorescence emission, as well as
quantum yield
Quantum Yield: A Measure
Line shape analyses are important!!
It makes contact with theory, experiment and model!
 In PL-excitation (PLE)
measurements, the PL
intensity is recorded as a
function of excitation
photon energy.
 Under a condition of fast
intra-band relaxation, PLE
is equivalent to linear
absorption spectra.
 Using micro-PL technique,
one can compare the line-
shape of PLE with PL at the
same microscopic region of
1 mm order.
What is Done in Practice?
What is Achieved in Practice?
PL is Used For
 Photoluminescence is an important technique for measuring the purity
and crystalline quality of semiconductors.
 Using Time-resolved photoluminescence (TRPL) one can determine the
minority carrier lifetime of semiconductors like GaAs.
 Can be used to determine the band gap, exciton life time, exciton
energy, bi-exciton, etc. of semiconductor and other functional materials.
 Determine the properties, e.g. structure and concentration, of the
emitting species.
Photoluminescence
 Recombination mechanisms
The return to equilibrium, also known as "recombination," can
involve both radiative and nonradiative processes. The amount
of PL emission and its dependence on the level of photo-
excitation and temperature are directly related to the
dominant recombination process.
 Material quality
Nonradiative processes are associated with localized defect
levels. Material quality can be measured by quantifying the
amount of radiative recombination.
PL recombination is disadvantageous for Solar Cell Material!!
Variables That Affect
Fluorescence and
Phosphorescence
 Both molecular structure and chemical environment
influence whether a substance will or will not luminesce.
These factors also determine the intensity of luminescence
emission.
 Quantum Yield
 Transition Types in Fluorescence
 Quantum Efficiency and Transition Type
 Fluorescence and Structure
Fluorescence Instrumentation
• 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
Major components for fluorescence instrument
Spectrofluorometer - two monochromators for excitation or fluorescence scanning
Instrumentation
Types of Photoluminescence
Spectroscopy
Needs Tunable Laser Source
PL Spectroscopy
 Fixed frequency laser
 Measures spectrum by scanning spectrometer
PL Excitation Spectroscopy (PLE)
 Detect at peak emission by varying
frequency
 Effectively measures absorption
Time-resolved PL Spectroscopy
 Short pulse laser + fast detector
 Measures lifetimes and relaxation processes
PMT
Xenon Source
Excitation
Monochromator Emission
Monochromator
Sample compartment
Fluorescence
Instrumentation
Spectrofluorometer schematic
NPs size dependent
fluorescence
Si NPs
Examples of PL Spectra
500 520 540 560 580 600 620 640
200
300
400
500
Fluoroscence
Intensity
(a.u.)
Wavelength (nm)
1.5 mol% AgCl
1.0 mol% AgCl
0.5 mol% AgCl
No AgCl
4
S3/2
-
4
I15/2
4
F9/2
-
4
I15/2
Up-conversion Spectra of
Phosphate Glass for Excitation
at 797 nm
(59.5-x) P2O5+MgO+xAgCl+0.5Er2O3
0.0 0.5 1.0 1.5
200
250
300
350
400
450
500
550
Intensity
(a.u.)
AgCl Concentration (mol%)
540 nm
632 nm
275 300 325 350 375 400 425 450
400
600
800
1000
1200
Intensity
(a.u.)
Wavelenght (nm)
A
B
C
D
2. 63 eV
2.71 eV
2.76 eV
2.86 eV
3.03 eV
3.11 eV
3.23 eV
3.60 eV
3.73 eV
3.98 eV
4.03 eV
2.94 eV
PL Spectra of Ge
Nanoparticles
Schematic diagram of S-K growth mode
of Ge QDs on Si substrate at two
different substrate temperature for
sample A (RT), D (400 °C) responsible for
the origin of PL peaks presented in fig.
320 340 360 380 400 420 440
350
400
450
500
550
600 Gaussian fit
23 nm
Xc: 373.4 nm
(a)
360
420
480
540
600
660
720
31 nm
Intensity
(a.
u.
)
Xc: 383.5 nm
(c)
270
300
330
360
390
420
450
29 nm
Xc: 383.3 nm
(b)
330 360 390 420 450
400
500
600
700
800
900
37 nm
Wavelength (nm)
Xc: 396.3 nm
(d)
PL spectra of sample A
(a), B (b), C (c) and D
(d) with the Gaussian
de-convolution of
intense peak
PL Spectra
Analyses
350 400 450
0
500
3.23 eV
3.21 eV
2.84 eV
340 360 380 400 420
200
In
t
e
n
s
it
y
(
a
.
u
.
)
W avelen g th (n m )
X c: 375.8 nm
FW H M : 61.4 nm
3.29 eV
120 Sec
90 Sec
30 Sec
Pre-Annealed
340 360 380 400 420
250
500
Xc: 383.2 nm
FWHM: 32.5
340 360 380 400 420
200
400
G au ssian fit
X c: 387.5 n m
F W H M : 35.5 n m
340 360 380 400 420
200
Xc: 385.1 nm
FW H M : 34.2 N M
Intensity
(a.
u.
)
Wavelength (nm)
3.19 eV
PL Spectra
Analyses
UC PL Spectra
(a) UC Luminescence spectra of glasses under an excitation of 786 nm i) No
AgCl, ii) 0.1 mol% AgCl, iii) 0.5 mol% AgCl, iv) 1.0 mol% AgCl (b) Ag
concentration dependent emission intensity. Maximum amplification for the
green and red bands occur at 0.5 mol% Ag (Glass C).
Four prominent emission bands located at 520 nm, 550 nm, 650 nm and 835
nm attributed to 2H11/2→4I15/2, 4S3/2→4I15/2, 4F9/2→4I15/2 and 4S3/2→4I13/2
transitions.
(b) All the bands are enhanced significantly by factors of 2.5, 2.3, 2 and 1.7
times, respectively .
786 nm
(a) Down-conversion luminescence spectra of glasses with i) No AgCl, ii) 0.1
mol% AgCl, iii) 0.5 mol% AgCl, iv) 1.0 mol% AgCl (b) plot of emission intensity
vs concentration of Ag (mol%). Maximum amplification for the green and red
bands are found to be occur at 0.5 mol% Ag (Glass C).
DC PL Spectra
 PL spectroscopy is not considered a major structural or qualitative
analysis tool, because molecules with subtle structural differences often
have similar fluorescence spectra
 Used to study chemical equilibrium and kinetics
 Fluorescence tags/markers
 Important for various organic-inorganic complexes
Applications of PL
Spectroscopy
 Sensitivity to local electrical environment polarity, hydrophobicity
 Track (bio-)chemical reactions
 Measure local friction (micro-viscosity)
 Track solvation dynamics
 Measure distances using molecular rulers: fluorescence resonance energy
transfer (FRET)
 Band gap of semiconductors
 Nanomaterials characterization
Conclusions
 Luminescence spectroscopy provides complex information about the defect
structure of solids
- importance of spatially resolved spectroscopy
- information on electronic structures
 There is a close relationship between specific conditions of mineral
formation or alteration, the defect structure and the luminescence properties
(“typomorphism”)
 Useful for determining semiconductor band gap, exciton energy etc.
 For the interpretation of luminescence spectra it is necessary to consider
several analytical and crystallographic factors, which influence the
luminescence signal
Questions ?

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Photoluminescence -chapter-6.pdf

  • 1. Chapter 6 Photoluminescence Spectroscopy Sib Krishna Ghoshal (PhD) Advanced Optical Materials Research Group Physics Department, Faculty of Science, UTM Course Code: SSCP 4473 Course Name: Spectroscopy & Materials Analysis
  • 2. What is Photoluminescence? Photoluminescence (PL) is a process in which the substance absorbs photons (EM radiation) and then re-radiates photons.
  • 3. Presentation Outline  What is Photoluminescence?  Basic Physics of luminescence  Principle of PL  How PL spectroscopy is performed?  What information it captures?  Examples  Applications  Conclusion Very powerful tool for low dimensional systems, especially for semiconductors!! Finding right solar material and up-converted lasing material is challenging!! E0 E1 u
  • 4. A material that emits light is called luminescent material. Greek word phosphor (light bearer) is usually used to describe luminescent nature.  It emits energy from an excited electronic state as light.  Some of the incident energy is absorbed and re-emitted as light of a longer wavelength (Stoke’s law).  The wavelength of the emitted light is characteristic of the luminescent substance and not of the incident radiation.  The emitted light carries the materials signature. Definition of Luminescence
  • 5. Characteristics PL frequencies Changes in Frequency of PL peaks Polarization of PL peak Width of PL peak Intensity of PL peak Composition Stress/Strain State Symmetry/ Orientation Quality Amount Analyses of Samples Fingerprints Captured by PL Spectra One broad peak may be superposition of two or several peaks: De- convolution is needed  Number of peaks  Peak Intensities  Peak position  FWHM  Peak shape
  • 6.  It operates from 200 nm to 900 nm wavelength.  Below 200 nm it needs vaccum because air can absorb much UV light.  UTM machine does not cover the time and field dependent fluorescence decay. Perkin Elmer LS 55 Luminescence Spectrometer
  • 7.  Photoluminescence implies both Fluorescence and Phosphorescence. One broad peak may be superposition of two or several peaks: De-convolution is needed.  Main peak may accompanied with kinks, shoulder or satellites. Basic Physics Fluorescence – ground state to singlet state and back. Phosphorescence - ground state to triplet state and back.
  • 8. Fluorescence: A Type of Light Emission • First observed from quinine by Sir J. F. W. Herschel in 1845 Blue glass Filter Church Window! <400nm Quinine Solution Yellow glass of wine Em filter > 400 nm 1853 G.G. Stoke coined term “fluorescence” Forms of photoluminescence (luminescence after absorption) are fluorescence (short lifetime) and phosphorescence (long lifetime).
  • 9. Common Fluorophores Typically, Aromatic molecules – Quinine, ex 350/em 450 – Fluorescein, ex 485/520 – Rhodamine B, ex 550/570 – POPOP, ex 360/em 420 – Coumarin, ex 350/em 450 – Acridine Orange, ex 330/em 500 – Many SC & Low dimensional SC systems – Some Minerals – Materials in low dimension – Glass with Rare Earth Ions The initial excitation takes place between states of same multiplicity and in accord with the Franck-Condon principle.
  • 10. What is Fluorescence?  Fluorescence is a photoluminescence process in which atoms or molecules are excited by the absorption of electromagnetic radiation. The excited species then relax to the ground state, giving up their excess energy as photons. Attractive features  One to three orders of magnitude better than absorption spectroscopy, even single molecules can be detected by fluorescence spectroscopy.  Larger linear concentration range than absorption spectroscopy. Shortcomings  Much less widely applicable than absorption methods.  More environmental interference effects than absorption methods. Fluorescence ?
  • 11. Highly sensitive technique  1,000 times more sensitive than UV-visible spectroscopy.  Often used in drug or drug metabolite determinations by HPLC (high performance liquid chromatography) with fluorimetric detector.  Non-fluorescing compounds can be made fluorescent – derivitisation. Selective versatile technique  Since excitation and emission wavelengths are utilized, gives selectivity to an assay compared to UV-visible spectroscopy.  Differing modes of spectroscopy yield wide versatility. Advantages of Fluorescence Spectroscopy
  • 13. Luminescence  “Inverse” of absorption  Consequence of radiative recombination of excited electrons Compete with non-radiative recombination processes  PL: non-equilibrium obtained by photons  Important for Laser, LED and optoelectronics Radiative: Visible photon Nonradiative: Thermal photon
  • 14. Typical Fluorescence Spectra Fluorescence spectra of 9- Anthracenecarboxylic Acid Fluorescence spectra for 1 ppm anthracene in alcohol
  • 15. Transitions & Time Scales, Energy Scale… Jablonski Energy Diagram
  • 16. Property of Luminescence Spectrum Fluorescence vs Phosphorescence  Phosphorescence is always at longer wavelength compared with fluorescence  Phosphorescence is narrower compared with fluorescence  Phosphorescence is weaker compared with fluorescence Absorption vs Emission  absorption is mirrored relative to emission  Absorption is always on the shorter wavelength compared to emission  Absorption vibrational progression reflects vibrational level in the electronic excited states, while the emission vibrational progression reflects vibrational level in the electronic ground states  0 transition of absorption is not overlap with the 0 of emission Why? Why?
  • 17. 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: A nonradiative 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.
  • 18. Fluorescent Species All absorbing molecules have the potential to fluoresce, but most compounds do not. Quantum Yield absorbed Photons emitted Photons molecules excited of number Total fluoresce that molecules of Number or   Structure determines the relaxation and fluorescence emission, as well as quantum yield Quantum Yield: A Measure Line shape analyses are important!! It makes contact with theory, experiment and model!
  • 19.  In PL-excitation (PLE) measurements, the PL intensity is recorded as a function of excitation photon energy.  Under a condition of fast intra-band relaxation, PLE is equivalent to linear absorption spectra.  Using micro-PL technique, one can compare the line- shape of PLE with PL at the same microscopic region of 1 mm order. What is Done in Practice?
  • 20. What is Achieved in Practice?
  • 21. PL is Used For  Photoluminescence is an important technique for measuring the purity and crystalline quality of semiconductors.  Using Time-resolved photoluminescence (TRPL) one can determine the minority carrier lifetime of semiconductors like GaAs.  Can be used to determine the band gap, exciton life time, exciton energy, bi-exciton, etc. of semiconductor and other functional materials.  Determine the properties, e.g. structure and concentration, of the emitting species.
  • 22. Photoluminescence  Recombination mechanisms The return to equilibrium, also known as "recombination," can involve both radiative and nonradiative processes. The amount of PL emission and its dependence on the level of photo- excitation and temperature are directly related to the dominant recombination process.  Material quality Nonradiative processes are associated with localized defect levels. Material quality can be measured by quantifying the amount of radiative recombination. PL recombination is disadvantageous for Solar Cell Material!!
  • 23. Variables That Affect Fluorescence and Phosphorescence  Both molecular structure and chemical environment influence whether a substance will or will not luminesce. These factors also determine the intensity of luminescence emission.  Quantum Yield  Transition Types in Fluorescence  Quantum Efficiency and Transition Type  Fluorescence and Structure
  • 24. Fluorescence Instrumentation • 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 Major components for fluorescence instrument
  • 25. Spectrofluorometer - two monochromators for excitation or fluorescence scanning Instrumentation
  • 26. Types of Photoluminescence Spectroscopy Needs Tunable Laser Source PL Spectroscopy  Fixed frequency laser  Measures spectrum by scanning spectrometer PL Excitation Spectroscopy (PLE)  Detect at peak emission by varying frequency  Effectively measures absorption Time-resolved PL Spectroscopy  Short pulse laser + fast detector  Measures lifetimes and relaxation processes
  • 27. PMT Xenon Source Excitation Monochromator Emission Monochromator Sample compartment Fluorescence Instrumentation Spectrofluorometer schematic
  • 28. NPs size dependent fluorescence Si NPs Examples of PL Spectra
  • 29. 500 520 540 560 580 600 620 640 200 300 400 500 Fluoroscence Intensity (a.u.) Wavelength (nm) 1.5 mol% AgCl 1.0 mol% AgCl 0.5 mol% AgCl No AgCl 4 S3/2 - 4 I15/2 4 F9/2 - 4 I15/2 Up-conversion Spectra of Phosphate Glass for Excitation at 797 nm (59.5-x) P2O5+MgO+xAgCl+0.5Er2O3 0.0 0.5 1.0 1.5 200 250 300 350 400 450 500 550 Intensity (a.u.) AgCl Concentration (mol%) 540 nm 632 nm
  • 30. 275 300 325 350 375 400 425 450 400 600 800 1000 1200 Intensity (a.u.) Wavelenght (nm) A B C D 2. 63 eV 2.71 eV 2.76 eV 2.86 eV 3.03 eV 3.11 eV 3.23 eV 3.60 eV 3.73 eV 3.98 eV 4.03 eV 2.94 eV PL Spectra of Ge Nanoparticles Schematic diagram of S-K growth mode of Ge QDs on Si substrate at two different substrate temperature for sample A (RT), D (400 °C) responsible for the origin of PL peaks presented in fig.
  • 31. 320 340 360 380 400 420 440 350 400 450 500 550 600 Gaussian fit 23 nm Xc: 373.4 nm (a) 360 420 480 540 600 660 720 31 nm Intensity (a. u. ) Xc: 383.5 nm (c) 270 300 330 360 390 420 450 29 nm Xc: 383.3 nm (b) 330 360 390 420 450 400 500 600 700 800 900 37 nm Wavelength (nm) Xc: 396.3 nm (d) PL spectra of sample A (a), B (b), C (c) and D (d) with the Gaussian de-convolution of intense peak PL Spectra Analyses
  • 32. 350 400 450 0 500 3.23 eV 3.21 eV 2.84 eV 340 360 380 400 420 200 In t e n s it y ( a . u . ) W avelen g th (n m ) X c: 375.8 nm FW H M : 61.4 nm 3.29 eV 120 Sec 90 Sec 30 Sec Pre-Annealed 340 360 380 400 420 250 500 Xc: 383.2 nm FWHM: 32.5 340 360 380 400 420 200 400 G au ssian fit X c: 387.5 n m F W H M : 35.5 n m 340 360 380 400 420 200 Xc: 385.1 nm FW H M : 34.2 N M Intensity (a. u. ) Wavelength (nm) 3.19 eV PL Spectra Analyses
  • 33. UC PL Spectra (a) UC Luminescence spectra of glasses under an excitation of 786 nm i) No AgCl, ii) 0.1 mol% AgCl, iii) 0.5 mol% AgCl, iv) 1.0 mol% AgCl (b) Ag concentration dependent emission intensity. Maximum amplification for the green and red bands occur at 0.5 mol% Ag (Glass C). Four prominent emission bands located at 520 nm, 550 nm, 650 nm and 835 nm attributed to 2H11/2→4I15/2, 4S3/2→4I15/2, 4F9/2→4I15/2 and 4S3/2→4I13/2 transitions. (b) All the bands are enhanced significantly by factors of 2.5, 2.3, 2 and 1.7 times, respectively . 786 nm
  • 34. (a) Down-conversion luminescence spectra of glasses with i) No AgCl, ii) 0.1 mol% AgCl, iii) 0.5 mol% AgCl, iv) 1.0 mol% AgCl (b) plot of emission intensity vs concentration of Ag (mol%). Maximum amplification for the green and red bands are found to be occur at 0.5 mol% Ag (Glass C). DC PL Spectra
  • 35.  PL spectroscopy is not considered a major structural or qualitative analysis tool, because molecules with subtle structural differences often have similar fluorescence spectra  Used to study chemical equilibrium and kinetics  Fluorescence tags/markers  Important for various organic-inorganic complexes Applications of PL Spectroscopy  Sensitivity to local electrical environment polarity, hydrophobicity  Track (bio-)chemical reactions  Measure local friction (micro-viscosity)  Track solvation dynamics  Measure distances using molecular rulers: fluorescence resonance energy transfer (FRET)  Band gap of semiconductors  Nanomaterials characterization
  • 36. Conclusions  Luminescence spectroscopy provides complex information about the defect structure of solids - importance of spatially resolved spectroscopy - information on electronic structures  There is a close relationship between specific conditions of mineral formation or alteration, the defect structure and the luminescence properties (“typomorphism”)  Useful for determining semiconductor band gap, exciton energy etc.  For the interpretation of luminescence spectra it is necessary to consider several analytical and crystallographic factors, which influence the luminescence signal