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. 2003 Feb 15;31(4):1319-30.
doi: 10.1093/nar/gkg212.

Hybridization kinetics and thermodynamics of molecular beacons

Affiliations

Hybridization kinetics and thermodynamics of molecular beacons

Andrew Tsourkas et al. Nucleic Acids Res. .

Abstract

Molecular beacons are increasingly being used in many applications involving nucleic acid detection and quantification. The stem-loop structure of molecular beacons provides a competing reaction for probe-target hybridization that serves to increase probe specificity, which is particularly useful when single-base discrimination is desired. To fully realize the potential of molecular beacons, it is necessary to optimize their structure. Here we report a systematic study of the thermodynamic and kinetic parameters that describe the molecular beacon structure-function relationship. Both probe and stem lengths are shown to have a significant impact on the binding specificity and hybridization kinetic rates of molecular beacons. Specifically, molecular beacons with longer stem lengths have an improved ability to discriminate between targets over a broader range of temperatures. However, this is accompanied by a decrease in the rate of molecular beacon-target hybridization. Molecular beacons with longer probe lengths tend to have lower dissociation constants, increased kinetic rate constants, and decreased specificity. Molecular beacons with very short stems have a lower signal-to-background ratio than molecular beacons with longer stems. These features have significant implications for the design of molecular beacons for various applications.

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Figures

Figure 1
Figure 1
(A) The design and structural parameters of molecular beacons considered in the study. (B) Molecular beacons in solution can have three phases: bound to target, closed and random coil.
Figure 2
Figure 2
Determination of the changes in enthalpy (slope of the fitted line) and entropy (y-intercept) describing the transition between molecular beacons bound to wild-type target and free in the stem–loop conformation for molecular beacons with stem lengths of five bases and probe lengths of 17, 18 and 19 bases.
Figure 3
Figure 3
Determination of the changes in enthalpy (slope of the fitted line) and entropy (y-intercept) describing the transition between molecular beacons bound to wild-type target and free in the stem–loop conformation for molecular beacons with probe lengths of 17 bases and stem lengths of 4, 5 and 6 bases.
Figure 4
Figure 4
Determination of the changes in enthalpy (slope of the fitted line) and entropy (y-intercept) describing the transition between molecular beacons bound to target and free in the stem–loop conformation for molecular beacons with a stem length of five bases and a probe length 18 bases in the presence of wild-type (WT) and mutant targets (target A – D).
Figure 5
Figure 5
Melting temperatures for molecular beacons with various structures in the presence of wild-type target. The melting temperature was determined for samples containing 200 nM of molecular beacons and 400 nM of targets.
Figure 6
Figure 6
(A) Melting curves for molecular beacons hybridizing to wild-type target (solid line) and target B (dashed line) and (B) the difference in the fraction of molecular beacons bound to wild-type target and that to mutant target B. The molecular beacons have a probe length of 17 bases and stem lengths of 4, 5 and 6 bases.
Figure 6
Figure 6
(A) Melting curves for molecular beacons hybridizing to wild-type target (solid line) and target B (dashed line) and (B) the difference in the fraction of molecular beacons bound to wild-type target and that to mutant target B. The molecular beacons have a probe length of 17 bases and stem lengths of 4, 5 and 6 bases.
Figure 7
Figure 7
The difference in the fraction of molecular beacons bound to wild-type target and that to mutant target B for molecular beacons with a stem length of four bases and probe lengths of 17, 18 and 19 bases.
Figure 8
Figure 8
A comparison between the difference in the fraction of molecular beacons and that of linear probes bound to wild-type target and mutant target B.
Figure 9
Figure 9
Hybridization kinetics of molecular beacons in the presence of wild-type targets. (A) The normalized restoration in fluorescence that accompanies target hybridization for molecular beacons with probe lengths of 17 bases and stem lengths of 4, 5 and 6 bases. (B) The rate of hybridization k1 (on-rate) for molecular beacons with various probe and stem lengths hybridized to their complementary targets.
Figure 9
Figure 9
Hybridization kinetics of molecular beacons in the presence of wild-type targets. (A) The normalized restoration in fluorescence that accompanies target hybridization for molecular beacons with probe lengths of 17 bases and stem lengths of 4, 5 and 6 bases. (B) The rate of hybridization k1 (on-rate) for molecular beacons with various probe and stem lengths hybridized to their complementary targets.
Figure 10
Figure 10
Normalized background fluorescence as a function of temperature for molecular beacons with a probe length of 17 bases and stem lengths of 4, 5 and 6 bases. Similar results were obtained for molecular beacons with probe lengths of 18 and 19 bases (data not shown).

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