| Fluorescence Resonance Energy Transfer |
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| Introduction |
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| Fluorescence
Resonance Energy Transfer (FRET) is a process that shifts energy
from an electronically excited molecule (the donor fluorophore) to a
neighboring molecule (the acceptor or quencher), returning the donor
molecule to its ground state without emission of light (i.e.,
fluorescence emission). |
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| Energy transfer
between different electron states of the donor and acceptor
molecules is outlined in Figure 1 below: |
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| Figure 1. Diagram of the energy levels of the donor and
acceptor molecules |
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| Horizontal lines
represent discreet electron energy levels for each molecule. Energy
levels are labeled as either single states (S) or triplet states (T)
with subscripts numbered 0, 1, or 2, representing the ground state,
first excited electronic state, or second excited electronic state.
Molecules generally reside in its lowest, or ground, electronic
state, S0. A molecule may be excited to one of its higher
energy levels by any of a number of processes, including light
absorption and chemical reaction. Excitation of a molecule is
represented in the figure by the arrows pointing upward from the
ground state. |
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| An excited donor
molecule has several routes available to release its captured energy
and return to a lower energy state or to the ground state. Released
energy can be dissipated to the environment (as light or heat) or
transferred directly to another molecular, which captures that
energy and in turn itself moves to a higher energy state. These
routes are marked by arrows pointing downward from the excited
states; straight lines represent light emissions and wavy lines
represent energy conversion without light emissions. |
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| 1) Internal
energy conversions. Molecules excited into their second or
higher excited states are rapidly de-excited without light to the
first excited state, S1, without interacting with other
molecules. Internal conversion from S1 to S0
can also be rapid but in a luminescent molecule it is slow enough
that de-excitation by light emission is competitive. Intersystem
crossing from S1 to the triplet state, T1,
also occurs. |
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| 2) Light
emissions. Light released by the transition from S1
to S0 is fluorescence emission. Light released from the
triplet state T1, which generates phosphorescence, can
also occur but is less common. |
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| When a second
fluorescence molecule (i.e., a quencher or FRET acceptor) is in
physical proximity to an excited fluorophore, new paths for
de-excitation become available. |
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| 3) Dynamic
quenching. This process only occurs when the product of quencher
concentration and quenching rate constant is high. |
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| 4) Static
quenching. This process results from the formation of a
non-emissive complex between the donor fluorescent molecule and the
quencher. Static quenching reduces the donor fluorescence
intensity. |
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| 5) FRET.
FRET can occur when donor and acceptor molecules are in close
proximity but do not require actual physical contact. In the process
of FRET, de-excitation of the donor molecule is linked to excitation
of the acceptor molecule. In the figure, FRET is represented by the
de-excitation pathway leading from the S1 level of the
donor to the S1 level of the acceptor. Photons of light
are not involved. Once excited, the acceptor can undergo
de-excitation by the same emissive and non-emissive processes
described for the donor. |
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| Primary Conditions for
FRET |
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| 1) The primary
requirement for FRET is that the energy lost by de-excitation of the
donor molecule, S1-S0, be matched by the
energy required for excitation of the acceptor. In other words, the
absorption spectrum of the acceptor molecule must overlap the
emission spectrum of the donor molecule, as shown in Figure
2. |
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| Figure 2. Diagram of the overlapping spectrum of a pair of
FRET donor and acceptor dyes. |
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| 2) Donor and
acceptor molecules must be in close proximity (typically 10-100 Å).
FRET is a distance-dependent energy transfer between the electronic
excited states of two dye molecules. The distance at which energy
transfer is 50% efficient (i.e., 50% of excited donors are
deactivated by FRET) is defined by the Förster radius
(Ro). |
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| The magnitude of
Ro is dependent on the spectral properties of the donor and acceptor
dyes: |
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| Table 1.
Typical Values of Ro |
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| Donor |
Acceptor |
Ro (Å) |
| Fluorescein |
Tetramethylrhodamine |
55 |
| IAEDANS |
Fluorescein |
46 |
| EDANS |
DABCYL |
33 |
| Fluorescein |
Fluorescein |
44 |
| BODIPY FL |
BODIPY FL |
57 |
| Fluorescein |
QSYTM-7 |
61 | |
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| Some typical
values of Ro are listed in the table above. For good donor-acceptor
pairs, Ro values of 30 to 60 Å are common. |
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| 3) Donor and
acceptor transition dipole orientations must be approximately
parallel. |
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| 4) Donor/Acceptor
Pairs: In general, donor and acceptor are different dyes, each
having unique spectral properties. Normally, a fluorophore will
release light at its characteristic emission wavelength following
excitation. When two suitable fluorophores are in proximity within
the distance defined by the Förster radius, FRET will prevent
fluorescent emission from the higher energy group. Instead, energy
is transferred to the lower energy group, exciting the acceptor, and
leading to fluorescence emission at a lower energy wavelength
characteristic for the acceptor. If donor and acceptor are the same
dye, FRET can still occur and can be detected as fluorescence
depolarization. Non-fluorescent acceptors exist which will accept
energy from a donor without any resulting fluorescence emission.
These acceptors as a group are known as "dark quenchers", and
include Dabcyl, QSYTM-7, and
BlackHoleTM dyes. |
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| For more
information on fluorescent dyes, CLICK
HERE! |
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| Applications of
FRET |
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| FRET is highly
efficient within the Förster radius of the donor/acceptor pair
(which is often in the 50 - 60 Å range), making it useful over
distances encountered within many biological macromolecules.
Further, since FRET is dependent on the inverse sixth power of the
intermolecular separation, efficiency dramatically falls as
donor/acceptor distance exceeds the Förster radius, making it an
extremely sensitive indicator of intermolecular distance. Thus, FRET
is an important technique for investigating a variety of biological
phenomena where markers that track physical proximity are necessary
or useful. |
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| For example, in
the TaqManTM 5'-nuclease assay, two
fluorescent dyes (such as Fam and Tamra) are covalently linked by
DNA residues in an oligonucleotide probe. When the higher-energy
fluorophore (Fam) is excited at 488 nm, instead of the expected
fluorescence emission at 520 nm, the captured energy is transferred
to the lower energy fluorophore (Tamra) and is emitted at 580 nm
(FRET has occurred); the Fam signal is quenched. Using the
fluorescein/rhodamine reporter/quencher combination, FRET can occur
even when the groups are separated by 25-30 bases of DNA. During the
course of a TaqManTM assay, the two
fluorophores are physically separated from each other by the
5'-exonuclease action of Taq DNA polymerase - after which 488 nm
stimulation results in visible Fam emission at 520 nm (quenching is
released). |
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| Molecular Beacons
are another variation on the FRET-based nucleic acid probe paradigm.
In this case, a dark quencher (most commonly Dabcyl) is placed at
one end of the DNA probe and a reporter dye is placed at the
opposite end. The probe is designed such that a target-specific
hybridization domain is positioned centrally between short sequences
(unrelated to the target) that lead to hairpin formation. In the
native state, the Molecular Beacon forms a hairpin structure with
the reporter and quencher groups directly adjacent. When hybridized
to the complementary target sequence, the hairpin structure unfolds
and the reporter and quencher separate. Dabcyl has a relatively
short Förster radius and will not quench the reporter dye in the
open configuration. For more information about Molecular Beacons, CLICK
HERE! |
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| A new method to
detect RNase activity was recently developed as a joint project
between IDT and Ambion, called RNaseAlertTM (patent pending). RNaseAlertTM employs a fluorescence-quenching
oligonucleotide probe to detect the presence of RNase activity. A
fluorescein reporter group is connected to a fluorescence-quencher
by several RNA residues. The precise sequence has been optimized for
maximum sensitivity in detecting a wide variety of RNase activities.
Upon cleavage of the RNA, the reporter and quencher separate and a
fluorescent signal is revealed. |
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| To order
Dual-Labeled probes, CLICK
HERE! |
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| To order Molecular
Beacons, CLICK
HERE! |
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| To order
RNaseAlertTM CLICK
HERE! |
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| Other Selected Applications of
FRET |
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- Substrates for enzyme kinetic
studies1
- Structure
and conformation of proteins2
- Spatial
distribution and assembly of protein
complexes3
- Receptor/ligand
interactions4
- Immunoassays5
- Probing
interactions of single molecules6
- Structure
and conformation of nucleic acids7
- Detection
of nucleic acid hybridization8
- Primer-extension assays for detecting
mutations9
- Automated
DNA sequencing10
- Distribution and transport of
lipids11
- Membrane-fusion assays12
- Membrane-potential
sensing13
- Fluorogenic protease
substrates14
- Indicators for cyclic AMP15
|
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| References |
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| 1. Kelemen, B.R.
Klink, T.A., Behlke, M.A., Eubanks, S.R., Leland, P.A. and Raines
R.T. (1999) "Hypersensitive
substrate for ribonucleases" Nucleic Acids Res.,
27:3696-3701 |
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| 2. Luo Y., Wu
J.L., Gergely J., and Tao T. (1998) "Localization of
Cys133 of Rabbit Skeletal Troponin-l with Respect to
Troponin-C by Resonance Energy Transfer." Biophys. J.
74:3111-3119. |
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| 3. Watson B.S.,
Hazlett T.L., Eccleston J.F., Davis C., Jameson D.M. and Johnson
A.E.(1995) "Macromolecular Arrangement in the
Aminoacyl-tRNA-Elongation Factor TuGTP Ternary Complex. A
Fluorescence Energy Transfer Study." Biochemistry
34:7904-7912. |
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| 4. Berger W.,
Prinz H., Striessnig J., Kang H.C., Haugland R. and Glossmann H.
(1994) "Complex Molecular Mechanism for Dihydropyridine Binding to
L-Type Ca2+-Channels as Revealed by Fluorescence
Resonance Energy Transfer." Biochemistry
33:11875-11883. |
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| 5. Morrison, L.E.
(1988) "Time-Resolved Detection of Energy Transfer: Theory and
Application to Immunoassays." Anal. Biochem.
174:101-120. |
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| 6. Ha T., Enderle
T., Ogletree D.F., Chemla D.S., Selvin P.R. and Weiss S.(1996)
"Probing the Interaction between Two Single Molecules: Fluorescence
Resonance Energy Transfer between a Single Donor and a Singer
Acceptor." Proc. Natl. Acad. Sci. USA
93:6264-6268. |
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| 7. Tòth, K.,
Sauermann, V. and Langowski, J. (1998) "DNA Curvature in Solution
Measured by Fluorscence Resonance Energy Transfer."
Biochemistry 37:8173-8179. |
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| 8. Tyagi, S.,
Bratu, D.P. and Kramer, F.R. (1998) "Multicolor Molecular Beacons
for Allele Discrimination." Nature Biotech.
16:49-53. |
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| 9. Chen X.,
Zehnbauer B., Gnirke A., and Kwok P.Y.(1997) "Fluorescence Energy
Transfer Detection as a Homogeneous DNA Diagnostic Method." Proc
Natl Acad Sci USA 94:10756-10761. |
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| 10. Hung, S.-C.,
Mathies, R.A. and Glazer A.N. (1998) "Comparison of Fluorescence
Energy Transfer Primers with Different Donor-Acceptor Dye
Combinations." Anal. Biochem.
255:32-38. |
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| 11.
Gutierrez-Merino C., Bonini de Romanelli I.C., Pietrasanta L.I. and
Barrantes F.J. (1995) "Preferential Distribution of the Fluorescent
Phospholipid Probes NBD-Phosphatidylcholine and
Rhodamine-Phosphatidylethanolamine in the Exofacial Leaflet of
Acetylcholine Receptor-Rich Membranes from Torpedo
marmorata." Biochemistry
34:4846-4855. |
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| 12. Pecheur E.I.,
Martin I., Ruysschaert J.M., Bienvenue A. and Hoekstra D. (1998)
"Membrane Fusion Induced by 11-mer Anionic and Cationic Peptides: A
Structure-Function Study." Biochemistry
37:2361-2371. |
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| 13. Gonzalez J.E.
and Tsien R.Y.(1995) "Voltage Sensing by Fluorescence Resonance
Energy Transfer in Single Cells." Biophys. J.
69:1272-1280. |
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| 14. Kurth T.,
Grahn S., Thormann M., Ullmann D., Hofmann H.J., Jakubke H.D., and
Hedstrom L.(1998) "Engineering the S1' Subsite of Trypsin: Design of
a Protease Which Cleaves between Dibasic Residues."
Biochemistry 37:11434-11440. |
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| 15. S.R. Adams,
et al. (1993) "Optical Probes for Cyclic AMP." Fluorescent
and Luminescent Probes for Biological Activity, W.T. Mason, Ed. ,
pp. 133-149. |
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| Wei Tao, Ph.D. |
| Research
Scientist, Molecular Genetics and Bioinformatics |
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| Mark Behlke, M.D., Ph.D. |
| Vice President,
Molecular Genetics and Bioinformatics |
| Integrated DNA
Technologies |
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| December 2000 |
| Printer
Friendly Version |