Quenching (fluorescence)

Last updated
Two samples of quinine dissolved in water with a violet laser (left) illuminating both. Typically quinine fluoresces blue, which is visible in the right sample. The left sample contains chloride ions which quench quinine's fluorescence, so the left sample does not fluoresce visibly (the violet light is just scattered laser light). Quenching of Quinine fluorescence by chloride ions.JPG
Two samples of quinine dissolved in water with a violet laser (left) illuminating both. Typically quinine fluoresces blue, which is visible in the right sample. The left sample contains chloride ions which quench quinine's fluorescence, so the left sample does not fluoresce visibly (the violet light is just scattered laser light).

In chemistry, quenching refers to any process which decreases the fluorescent intensity of a given substance. A variety of processes can result in quenching, such as excited state reactions, energy transfer, complex-formation and collisions. As a consequence, quenching is often heavily dependent on pressure and temperature. Molecular oxygen, iodine ions and acrylamide [1] are common chemical quenchers. The chloride ion is a well known quencher for quinine fluorescence. [2] [3] [4] Quenching poses a problem for non-instant spectroscopic methods, such as laser-induced fluorescence.

Contents

Quenching is made use of in optode sensors; for instance the quenching effect of oxygen on certain ruthenium complexes allows the measurement of oxygen saturation in solution. Quenching is the basis for Förster resonance energy transfer (FRET) assays. [5] [6] [7] Quenching and dequenching upon interaction with a specific molecular biological target is the basis for activatable optical contrast agents for molecular imaging. [8] [9] Many dyes undergo self-quenching, which can decrease the brightness of protein-dye conjugates for fluorescence microscopy, [10] or can be harnessed in sensors of proteolysis. [11]

Mechanisms

Donor emission and quencher absorption spectral overlap Fig1.gif
Donor emission and quencher absorption spectral overlap

Förster resonance energy transfer

There are a few distinct mechanisms by which energy can be transferred non-radiatively (without absorption or emission of photons) between two dyes, a donor and an acceptor. Förster resonance energy transfer (FRET or FET) is a dynamic quenching mechanism because energy transfer occurs while the donor is in the excited state. FRET is based on classical dipole-dipole interactions between the transition dipoles of the donor and acceptor and is extremely dependent on the donor-acceptor distance, R, falling off at a rate of 1/R6. FRET also depends on the donor-acceptor spectral overlap (see figure) and the relative orientation of the donor and acceptor transition dipole moments. FRET can typically occur over distances up to 100 Å.

Dexter electron transfer

Dexter (also known as Dexter exchange or collisional energy transfer, colloquially known as Dexter Energy Transfer) is another dynamic quenching mechanism. [12] Dexter electron transfer is a short-range phenomenon that falls off exponentially with distance (proportional to ekR where k is a constant that depends on the inverse of the van der Waals radius of the atom[ citation needed ]) and depends on spatial overlap of donor and quencher molecular orbitals. In most donor-fluorophore–quencher-acceptor situations, the Förster mechanism is more important than the Dexter mechanism. With both Förster and Dexter energy transfer, the shapes of the absorption and fluorescence spectra of the dyes are unchanged.

Dexter electron transfer can be significant between the dye and the solvent especially when hydrogen bonds are formed between them.

Exciplex

Exciplex (excited state complex) formation is a third dynamic quenching mechanism.

Comparison of static and dynamic quenching mechanisms Dark quenching mechanisms.svg
Comparison of static and dynamic quenching mechanisms

Static quenching

The remaining energy transfer mechanism is static quenching (also referred to as contact quenching). Static quenching can be a dominant mechanism for some reporter-quencher probes. Unlike dynamic quenching, static quenching occurs when the molecules form a complex in the ground state, i.e. before excitation occurs. The complex has its own unique properties, such as being nonfluorescent and having a unique absorption spectrum. Dye aggregation is often due to hydrophobic effects—the dye molecules stack together to minimize contact with water. Planar aromatic dyes that are matched for association through hydrophobic forces can enhance static quenching. High temperatures and addition of surfactants tend to disrupt ground state complex formation.

Collisional quenching

Collisional quenching occurs when the excited fluorophore experiences contact with an atom or molecule that can facilitate non-radiative transitions to the ground state. ... Excited-state molecule collides with quencher molecule and returns to ground state non-radiatively.

See also

Related Research Articles

<span class="mw-page-title-main">Fluorescence</span> Emission of light by a substance that has absorbed light

Fluorescence is one of two kinds of emission of light by a substance that has absorbed light or other electromagnetic radiation. Fluorescence involves no change in electron spin multiplicity and generally it immediately follows absorption; phosphorescence involves spin change and is delayed. Thus fluorescent materials generally cease to glow nearly immediately when the radiation source stops, while phosphorescent materials, which continue to emit light for some time after.

<span class="mw-page-title-main">Excimer</span> Excited dimeric molecule containing a noble gas

An excimer is a short-lived polyatomic molecule formed from two species that do not form a stable molecule in the ground state. In this case, formation of molecules is possible only if such atom is in an electronic excited state. Heteronuclear molecules and molecules that have more than two species are also called exciplex molecules. Excimers are often diatomic and are composed of two atoms or molecules that would not bond if both were in the ground state. The lifetime of an excimer is very short, on the order of nanoseconds.

<span class="mw-page-title-main">Förster resonance energy transfer</span> Photochemical energy transfer mechanism

Förster resonance energy transfer (FRET), fluorescence resonance energy transfer, resonance energy transfer (RET) or electronic energy transfer (EET) is a mechanism describing energy transfer between two light-sensitive molecules (chromophores). A donor chromophore, initially in its electronic excited state, may transfer energy to an acceptor chromophore through nonradiative dipole–dipole coupling. The efficiency of this energy transfer is inversely proportional to the sixth power of the distance between donor and acceptor, making FRET extremely sensitive to small changes in distance.

<span class="mw-page-title-main">Internal conversion (chemistry)</span>

Internal conversion is a transition from a higher to a lower electronic state in a molecule or atom. It is sometimes called "radiationless de-excitation", because no photons are emitted. It differs from intersystem crossing in that, while both are radiationless methods of de-excitation, the molecular spin state for internal conversion remains the same, whereas it changes for intersystem crossing. The energy of the electronically excited state is given off to vibrational modes of the molecule. The excitation energy is transformed into heat.

In particle physics, the quantum yield of a radiation-induced process is the number of times a specific event occurs per photon absorbed by the system.

Fluorescence anisotropy or fluorescence polarization is the phenomenon where the light emitted by a fluorophore has unequal intensities along different axes of polarization. Early pioneers in the field include Aleksander Jablonski, Gregorio Weber, and Andreas Albrecht. The principles of fluorescence polarization and some applications of the method are presented in Lakowicz's book.

In chemistry, a dark quencher is a substance that absorbs excitation energy from a fluorophore and dissipates the energy as heat; while a typical (fluorescent) quencher re-emits much of this energy as light. Dark quenchers are used in molecular biology in conjunction with fluorophores. When the two are close together, such as in a molecule or protein, the fluorophore's emission is suppressed. This effect can be used to study molecular geometry and motion.

TaqMan probes are hydrolysis probes that are designed to increase the specificity of quantitative PCR. The method was first reported in 1991 by researcher Kary Mullis at Cetus Corporation, and the technology was subsequently developed by Hoffmann-La Roche for diagnostic assays and by Applied Biosystems for research applications.

<span class="mw-page-title-main">Molecular sensor</span>

A molecular sensor or chemosensor is a molecular structure that is used for sensing of an analyte to produce a detectable change or a signal. The action of a chemosensor, relies on an interaction occurring at the molecular level, usually involves the continuous monitoring of the activity of a chemical species in a given matrix such as solution, air, blood, tissue, waste effluents, drinking water, etc. The application of chemosensors is referred to as chemosensing, which is a form of molecular recognition. All chemosensors are designed to contain a signalling moiety and a recognition moiety, that is connected either directly to each other or through a some kind of connector or a spacer. The signalling is often optically based electromagnetic radiation, giving rise to changes in either the ultraviolet and visible absorption or the emission properties of the sensors. Chemosensors may also be electrochemically based. Small molecule sensors are related to chemosensors. These are traditionally, however, considered as being structurally simple molecules and reflect the need to form chelating molecules for complexing ions in analytical chemistry. Chemosensors are synthetic analogues of biosensors, the difference being that biosensors incorporate biological receptors such as antibodies, aptamers or large biopolymers.

<span class="mw-page-title-main">Dexter electron transfer</span>

Dexter electron transfer is a fluorescence quenching mechanism in which an excited electron is transferred from one molecule to a second molecule via a non radiative path. This process requires a wavefunction overlap between the donor and acceptor, which means it can only occur at short distances; typically within 10 Å. The excited state may be exchanged in a single step, or in two separate charge exchange steps.

Non-photochemical quenching (NPQ) is a mechanism employed by plants and algae to protect themselves from the adverse effects of high light intensity. It involves the quenching of singlet excited state chlorophylls (Chl) via enhanced internal conversion to the ground state, thus harmlessly dissipating excess excitation energy as heat through molecular vibrations. NPQ occurs in almost all photosynthetic eukaryotes, and helps to regulate and protect photosynthesis in environments where light energy absorption exceeds the capacity for light utilization in photosynthesis.

<span class="mw-page-title-main">Lipid bilayer fusion</span>

In membrane biology, fusion is the process by which two initially distinct lipid bilayers merge their hydrophobic cores, resulting in one interconnected structure. If this fusion proceeds completely through both leaflets of both bilayers, an aqueous bridge is formed and the internal contents of the two structures can mix. Alternatively, if only one leaflet from each bilayer is involved in the fusion process, the bilayers are said to be hemifused. In hemifusion, the lipid constituents of the outer leaflet of the two bilayers can mix, but the inner leaflets remain distinct. The aqueous contents enclosed by each bilayer also remain separated.

<span class="mw-page-title-main">Förster coupling</span> Resonant energy transfer between excitons within adjacent QDs (quantum dots)

Förster coupling is the resonant energy transfer between excitons within adjacent QD's. The first studies of Forster were performed in the context of the sensitized luminescence of solids. Here, an excited sensitizer atom can transfer its excitation to a neighbouring acceptor atom, via an intermediate virtual photon. This same mechanism has also been shown to be responsible for exciton transfer between QD's and within molecular systems and biosystems, all of which may be treated in a similar formulation.

<span class="mw-page-title-main">Fluorescence in the life sciences</span> Scientific investigative technique

Fluorescence is used in the life sciences generally as a non-destructive way of tracking or analysing biological molecules. Some proteins or small molecules in cells are naturally fluorescent, which is called intrinsic fluorescence or autofluorescence. Alternatively, specific or general proteins, nucleic acids, lipids or small molecules can be "labelled" with an extrinsic fluorophore, a fluorescent dye which can be a small molecule, protein or quantum dot. Several techniques exist to exploit additional properties of fluorophores, such as fluorescence resonance energy transfer, where the energy is passed non-radiatively to a particular neighbouring dye, allowing proximity or protein activation to be detected; another is the change in properties, such as intensity, of certain dyes depending on their environment allowing their use in structural studies.

Single-molecule fluorescence resonance energy transfer is a biophysical technique used to measure distances at the 1-10 nanometer scale in single molecules, typically biomolecules. It is an application of FRET wherein a pair of donor and acceptor fluorophores are excited and detected at a single molecule level. In contrast to "ensemble FRET" which provides the FRET signal of a high number of molecules, single-molecule FRET is able to resolve the FRET signal of each individual molecule. The variation of the smFRET signal is useful to reveal kinetic information that an ensemble measurement cannot provide, especially when the system is under equilibrium with no ensemble/bulk signal change. Heterogeneity among different molecules can also be observed. This method has been applied in many measurements of intramolecular dynamics such as DNA/RNA/protein folding/unfolding and other conformational changes, and intermolecular dynamics such as reaction, binding, adsorption, and desorption that are particularly useful in chemical sensing, bioassays, and biosensing.

Fluorescent glucose biosensors are devices that measure the concentration of glucose in diabetic patients by means of sensitive protein that relays the concentration by means of fluorescence, an alternative to amperometric sension of glucose. Due to the prevalence of diabetes, it is the prime drive in the construction of fluorescent biosensors. A recent development has been approved by the FDA allowing a new continuous glucose monitoring system called EverSense, which is a 90-day glucose monitor using fluorescent biosensors.

Fluorescent chloride sensors are used for chemical analysis. The discoveries of chloride (Cl) participations in physiological processes stimulates the measurements of intracellular Cl in live cells and the development of fluorescent tools referred below.

<span class="mw-page-title-main">Surface energy transfer</span>

Surface energy transfer (SET) is a dipole-surface energy transfer process involving a metallic surface and a molecular dipole.

Lanthanide probes are a non-invasive analytical tool commonly used for biological and chemical applications. Lanthanides are metal ions which have their 4f energy level filled and generally refer to elements cerium to lutetium in the periodic table. The fluorescence of lanthanide salts is weak because the energy absorption of the metallic ion is low; hence chelated complexes of lanthanides are most commonly used. The term chelate derives from the Greek word for “claw,” and is applied to name ligands, which attach to a metal ion with two or more donor atoms through dative bonds. The fluorescence is most intense when the metal ion has the oxidation state of 3+. Not all lanthanide metals can be used and the most common are: Sm(III), Eu(III), Tb(III), and Dy(III).

<span class="mw-page-title-main">Small molecule sensors</span>

Small molecule sensors are an effective way to detect the presence of metal ions in solution. Although many types exist, most small molecule sensors comprise a subunit that selectively binds to a metal that in turn induces a change in a fluorescent subunit. This change can be observed in the small molecule sensor's spectrum, which can be monitored using a detection system such as a microscope or a photodiode. Different probes exist for a variety of applications, each with different dissociation constants with respect to a particular metal, different fluorescent properties, and sensitivities. They show great promise as a way to probe biological processes by monitoring metal ions at low concentrations in biological systems. Since they are by definition small and often capable of entering biological systems, they are conducive to many applications for which other more traditional bio-sensing are less effective or not suitable.

References

  1. Phillips SR, Wilson LJ, Borkman RF (August 1986). "Acrylamide and iodide fluorescence quenching as a structural probe of tryptophan microenvironment in bovine lens crystallins". Current Eye Research. 5 (8): 611–9. doi:10.3109/02713688609015126. PMID   3757547.
  2. O'Reilly JE (September 1975). "Fluorescence experiments with quinine". Journal of Chemical Education. 52 (9): 610–2. Bibcode:1975JChEd..52..610O. doi:10.1021/ed052p610. PMID   1165255.
  3. Sacksteder L, Ballew RM, Brown EA, Demas JN, Nesselrodt D, DeGraff BA (1990). "Photophysics in a disco: Luminescence quenching of quinine". Journal of Chemical Education. 67 (12): 1065. Bibcode:1990JChEd..67.1065S. doi:10.1021/ed067p1065.
  4. Gutow JH (2005). "Halide (Cl-) Quenching of Quinine Sulfate Fluorescence: A Time-Resolved Fluorescence Experiment for Physical Chemistry". Journal of Chemical Education. 82 (2): 302. Bibcode:2005JChEd..82..302G. doi:10.1021/ed082p302.
  5. Peng X, Draney DR, Volcheck WM (2006). "Quenched near-infrared fluorescent peptide substrate for HIV-1 protease assay". In Achilefu S, Bornhop DJ, Raghavachari R (eds.). Optical Molecular Probes for Biomedical Applications. Vol. 6097. pp. 60970F. doi:10.1117/12.669174. S2CID   98507102.
  6. Peng X, Chen H, Draney DR, Volcheck W, Schutz-Geschwender A, Olive DM (May 2009). "A nonfluorescent, broad-range quencher dye for Förster resonance energy transfer assays". Analytical Biochemistry. 388 (2): 220–8. doi:10.1016/j.ab.2009.02.024. PMID   19248753.
  7. Osterman H (2009). "The Next Step in Near Infrared Fluorescence: IRDye QC-1 Dark Quencher". Review Article. 388: 1–8. Archived from the original on 20 March 2020.
  8. Blum G, Weimer RM, Edgington LE, Adams W, Bogyo M (July 2009). "Comparative assessment of substrates and activity based probes as tools for non-invasive optical imaging of cysteine protease activity". PLOS ONE. 4 (7): e6374. Bibcode:2009PLoSO...4.6374B. doi: 10.1371/journal.pone.0006374 . PMC   2712068 . PMID   19636372.
  9. Weissleder R, Tung CH, Mahmood U, Bogdanov A (April 1999). "In vivo imaging of tumors with protease-activated near-infrared fluorescent probes". Nature Biotechnology. 17 (4): 375–8. doi:10.1038/7933. PMID   10207887. S2CID   12362848.
  10. Jacobsen MT, Fairhead M, Fogelstrand P, Howarth M (August 2017). "Amine Landscaping to Maximize Protein-Dye Fluorescence and Ultrastable Protein-Ligand Interaction". Cell Chem Biol. 24 (8): 1040–1047. doi: 10.1016/j.chembiol.2017.06.015 . PMC   5563079 . PMID   28757182.
  11. Voss EW Jr, Workman CJ, Mummert ME (February 1996). "Detection of protease activity using a fluorescence-enhancement globular substrate". BioTechniques. 20 (2): 286–291. doi: 10.2144/96202rr06 . PMID   8825159.
  12. IUPAC , Compendium of Chemical Terminology , 2nd ed. (the "Gold Book") (1997). Online corrected version: (2006) " Dexter excitation transfer (electron exchange excitation transfer) ". doi : 10.1351/goldbook.D01654