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By: Mosa
Charles
MOLECULAR PROBES
FLUORESCENCE
 What is it?
 Detector molecules that investigate, or analyze other molecules,
macromolecules, molecular aggregates or organisms.
 Major driving force of molecular imaging.
 What can be explored?
 Small molecules
 Peptides
 Proteins
 Apatamers
 DNA or RNA with special ability to bind to other molecules.
 Nanoparticles
MOLECULAR “SPECIFIC” PROBES
 What is it?
 They allow the detection of components of complex bimolecular
assemblies such as live cells.
 They are designed to respond to a specific stimulus and localize in
specific region of a biological specimen
 Very sensitive and selective
 Generally poly-aromatic hydrocarbons or heterocyclic molecules.
FLUORESCENT PROBE
Detection of target proteins. Cells stained with multiple fluorescent
probes
 Fluorescence is the result of a three-stage process that occur
within molecules known as fluorophores or fluorescent dyes.
 The Process
1. Excitation
 Energy from an external source
2. Excited-State Lifetime
 This is a very short time.
 Fluorophore undergoes conformational changes
 Two important things happen as result
3. Fluorescence Emission
 The fluorophore returns to ground state.
 The photon is emitted
FLUORESCENCE
MECHANISM OF FLUORESENSCE
Jablonski energy diagram of fluoresence
FLUORESCENCE SPECTRA
• Excitation and emission spectra of a fluorophore and the correlation between
excitation amplitude and emission intensity.
STOKES SHIFT
Fluorophores with greater stokes shift
show clear distinction between excitation
and emission light in a sample.
Fluorophores with smaller Stokes shift
has a smaller difference between
excitation and emission wavelengths.
 Early fluorescence
 Employed fluorophores that only emitted light on the visible range
 390nm to 700nm
 New Technology
 Fluorophores can now detect beyond the visible spectrum
 UV and IR ranges
ELECTROMAGNETIC SPECTRUM
 Molar Extinction Coefficient (ε)
 The quantity of light that can be absorbed by a given
wavelength.
 Measured in M-1cm-1
 Quantum Yield
 Number of photons emitted divided by the number of photons
absorbed.
 Provides the efficiency of the fluor.
FLUOROPHORE BRIGHTNESS
Basic requirements of instrumentation
Excitation light source such lasers, or lamps
A fluorophore
Filters to isolate specific wavelengths
Detector to record output
Instruments
Fluorescent microscopes
Fluorescence scanners
Spectrofluorometers and microplate readers
Flow cytometers
FLUORESENCE DETECTION
 Intensity
 Same parameters as absorbance
 Instrument dependent
 Reference standards essential to calibration
 Applications
 Cell number
 Amount of fluorophore localized to cells
 Or discrete cellular compartments
 Rate if gene expression and protein synthesis
 Rate of cell motility or movement of intracellular components
 Amount of DNA, RNA or protein in a sample
 DNA, RNA or protein sequence
 Enzyme activity
 Viability
QUANTITATIVE USE
 Detection and Analysis of Tumor Fluorescence Using a Two-
Photon Optical Fiber Probe.
 Purpose
 In vivo tumor analysis
 Demonstrate the benefits of TPOFF for in vivo biosensing.
 Demonstrate the benefits of a single-mode fiber
 Detection of tumor antibodies and tumor markers.
 The Project
 Tumors developed in Mice
 Ex vivo detection
 In vivo detection
RESEARCH ARTICLE
TPOFF DIAGRAM
RESULTS
SINGLE AND DOUBLE PHOTON
COMPARISON
Cell targeting comparison
RESULTS
RESULTS
Fluorescence of in vivo targeted tumor cells.
Thomas TP, Myaing MT, Ye JY, Candido K, Kotylar A, Beals J, Cao
P, Keszler B, Patri AK, Norris TB, Baker JR, Jr.: Detection and
Analysis of Tumor Fluorescence Using a Two–Photon Optical iber
Probe. Biophysical Journal, 2004:86(6), 3959–3965.
F
The Molecular Probes® Handbook—A Guide to Fluorescent
Probes and Labeling Technologies
http://www.lifetechnologies.com/us/en/home/references/mole
cular-probes-the-handbook.html
WORKS CITED
Thomas P, Ye JY, Yang C, Myaing M, Majoros IJ, Kotlyar A, Cao Z, Norris TB, Baker
JR, Jr.: Tissue distribution and real–time fluorescence measurement of a tumor–
targeted nanodevice by a two photon optical fiber fluorescence probe. Proc. of
SPIE, 2006:6095, 1–7.

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Molecular Probes Presentation-Final

  • 2.  What is it?  Detector molecules that investigate, or analyze other molecules, macromolecules, molecular aggregates or organisms.  Major driving force of molecular imaging.  What can be explored?  Small molecules  Peptides  Proteins  Apatamers  DNA or RNA with special ability to bind to other molecules.  Nanoparticles MOLECULAR “SPECIFIC” PROBES
  • 3.  What is it?  They allow the detection of components of complex bimolecular assemblies such as live cells.  They are designed to respond to a specific stimulus and localize in specific region of a biological specimen  Very sensitive and selective  Generally poly-aromatic hydrocarbons or heterocyclic molecules. FLUORESCENT PROBE Detection of target proteins. Cells stained with multiple fluorescent probes
  • 4.  Fluorescence is the result of a three-stage process that occur within molecules known as fluorophores or fluorescent dyes.  The Process 1. Excitation  Energy from an external source 2. Excited-State Lifetime  This is a very short time.  Fluorophore undergoes conformational changes  Two important things happen as result 3. Fluorescence Emission  The fluorophore returns to ground state.  The photon is emitted FLUORESCENCE
  • 5. MECHANISM OF FLUORESENSCE Jablonski energy diagram of fluoresence
  • 6. FLUORESCENCE SPECTRA • Excitation and emission spectra of a fluorophore and the correlation between excitation amplitude and emission intensity.
  • 7. STOKES SHIFT Fluorophores with greater stokes shift show clear distinction between excitation and emission light in a sample. Fluorophores with smaller Stokes shift has a smaller difference between excitation and emission wavelengths.
  • 8.  Early fluorescence  Employed fluorophores that only emitted light on the visible range  390nm to 700nm  New Technology  Fluorophores can now detect beyond the visible spectrum  UV and IR ranges ELECTROMAGNETIC SPECTRUM
  • 9.  Molar Extinction Coefficient (ε)  The quantity of light that can be absorbed by a given wavelength.  Measured in M-1cm-1  Quantum Yield  Number of photons emitted divided by the number of photons absorbed.  Provides the efficiency of the fluor. FLUOROPHORE BRIGHTNESS
  • 10. Basic requirements of instrumentation Excitation light source such lasers, or lamps A fluorophore Filters to isolate specific wavelengths Detector to record output Instruments Fluorescent microscopes Fluorescence scanners Spectrofluorometers and microplate readers Flow cytometers FLUORESENCE DETECTION
  • 11.  Intensity  Same parameters as absorbance  Instrument dependent  Reference standards essential to calibration  Applications  Cell number  Amount of fluorophore localized to cells  Or discrete cellular compartments  Rate if gene expression and protein synthesis  Rate of cell motility or movement of intracellular components  Amount of DNA, RNA or protein in a sample  DNA, RNA or protein sequence  Enzyme activity  Viability QUANTITATIVE USE
  • 12.  Detection and Analysis of Tumor Fluorescence Using a Two- Photon Optical Fiber Probe.  Purpose  In vivo tumor analysis  Demonstrate the benefits of TPOFF for in vivo biosensing.  Demonstrate the benefits of a single-mode fiber  Detection of tumor antibodies and tumor markers.  The Project  Tumors developed in Mice  Ex vivo detection  In vivo detection RESEARCH ARTICLE
  • 14. RESULTS SINGLE AND DOUBLE PHOTON COMPARISON Cell targeting comparison
  • 16. RESULTS Fluorescence of in vivo targeted tumor cells.
  • 17. Thomas TP, Myaing MT, Ye JY, Candido K, Kotylar A, Beals J, Cao P, Keszler B, Patri AK, Norris TB, Baker JR, Jr.: Detection and Analysis of Tumor Fluorescence Using a Two–Photon Optical iber Probe. Biophysical Journal, 2004:86(6), 3959–3965. F The Molecular Probes® Handbook—A Guide to Fluorescent Probes and Labeling Technologies http://www.lifetechnologies.com/us/en/home/references/mole cular-probes-the-handbook.html WORKS CITED Thomas P, Ye JY, Yang C, Myaing M, Majoros IJ, Kotlyar A, Cao Z, Norris TB, Baker JR, Jr.: Tissue distribution and real–time fluorescence measurement of a tumor– targeted nanodevice by a two photon optical fiber fluorescence probe. Proc. of SPIE, 2006:6095, 1–7.

Notes de l'éditeur

  1. A photon of energy from an external source such a an incandescent lamp or a laser. The fluorophore becomes excited creating ab excited electronic singlet state. Excited State Lifetime Typically 1-10 nanoseconds The conformational changes exposes the molecule to multiple possible interactions with the molecular environment Important events The energy of S1 is only partially dissipated producing a relaxed singlet excited state from which fluorescence emission originates All the molecules initially excited by absorption return to the ground state by fluorescence emission S1 maybe depopulated by other process such as collisional quenching, fluorescence resonance energy transfer and intersystem crossing. Fluorescence Emission Due to energy dissipation during the excited lifetime the emitted photon is a lower energy therefore creating a longer wavelength then the excitation photon The difference in energy is called the stokes shift. This is fundamental to the sensitivity of Fluro techniques because it allows detection of emission photons against a low background This is different from spectrophotometry because it does not require measurement of transmitted light relative to high incident light levels at the same wavelength
  2. As shown a photon of excitation light is absorbed by an electron of the a fluorescent particle This raises the energy level of the electron to an excited state During the short excitation period some of the energy dissipates The remaining energy is emitted as a photon which relaxes the electrons back to ground state The longer wavelength of the this photon distinguishes it from the excitation light The excitation and photon emission is cyclical and will continue until it the fluor is irreversibly damaged
  3. The emission wavelength is independent of of the excitation wavelength again due to the partial loss of energy prior to emission The emission intensity is directly proportional to the amplitude of the excitation wavelength
  4. Early fluorescence had many limitations due to in detecting beyond the visible spectrum New technology offer greater variability, versatility, and multiplexing capabilities for a range of new applications
  5. The flurophore brightness is determined by quantities named molar extinction coefficient and quantum yield Molar extinction coefficient and quantum yield specific to each fluor The brightness of the fluor is the product of the molar extinction coefficient and quantum yield
  6. Basic requirements Xenon lamps or mercury vapor lamps For different fluorophores Instrumentation Microscopes Detect localized fluors in samples in 2 and 3 dimensions Fluorescence scanners Such as microarray readers do the same thing as the microscopes Spectrofluorometers Record the average fluorescence in samples Flow cytometers Analyze the fluorescence of individual cells in a sample population
  7. Quantitatively dependent on the same parameters as absorbance Defined in beer’s law as the product of the molar extinction coefficient, optical path length, solute concentration, Fluorescence also includes the fluorescence quantum yield of the dye, the excitation source intensity and fluorescence collection efficiency of the instrument
  8. Purpose In vivo Tumor analysis This research was based on the need for a non-invasive measurement of cancer signatures, monitoring of drug delivery, and evaluation of drug induced effects in tumors. The identification of mechanisms related to tumor development has impressed the importance in selecting therapeutics. Monitoring of the spatial and temporal distribution of cancer drugs would allow for more effective and precise dosing Benefits of TPOFF Does not require tissue excision and can be inserted through a thin 20- gauge needle or higher Can deliver and retrieve light in vivo Provides a low spatial resolution of only a few microns (extremely localized) Allows a broad range of photochromes to be excited with a single laser and allowing only one to simultaneously measure multiple emitters for example the presence of a tumor marker and drug Employs near IR light which minimizes tissue damage, photobleaching and intrinsic tissue fluorescence Benefits of a single mode fiber Delivers femtosecond laser pulses and collect emitted fluorescence from cell pellets back through the same probe Other systems require 2 separate systems Tumor antibodies and markers Tumor antibodies are drugs used to target antigens produced by cancer cells Can detect the substances that produce cancer cells or from other cells as a response to cancer in that region The Project Tumors in mice Human tumor cells expressing green fluorescent protein were transplanted in 7 week old female mice and allowed to grow to approximately 0.7 to 0.8 cm in diameter Ex vivo The TPOFF probe was used to measure GFP fluorescence from excised tumors containing minuscule amounts of (0.3%) GFP expressing cells In vivo detection They then used the TPOFF to detect GFP expressing cells in live mice.