In contrast, molecular beacon probes are single-stranded oligonucleotides that

DAPT price form stem-loop structures with the recognition sequence mainly located in the loop region. A 5–7 base pair stem brings the fluorophore at the 5′end and non-fluorescent quencher at the 3′end together [28]. This contact-dependent quenching mechanism is highly efficient and reduces the background fluorescence significantly when the probe is free in solution. The presence of the target sequence leads to the formation of a probe-target hybrid, which is longer and more stable than the stem. This spontaneous conformational reorganization forces dissociation of the fluorophore and the quencher resulting in a significant increase in fluorescence. Because of the specificity of

the interaction between the probe region of the molecular beacon with the complementary target sequence within the PCR amplification product, the presence of the non-specific DNA does not interfere with the quantitative detection of the intended amplification PRIMA-1MET order product. Due to their potential superiority [27], we used molecular beacons for PCR-based quantification of B. burgdorferi in this study and assessed their efficiency, sensitivity and specificity relative to the SYBR Green I based detection system. Furthermore, the molecular beacons were used to detect B. burgdorferi, including the bgp mutant, in infected mouse tissues Thalidomide NVP-BGJ398 cell line effectively. Results Analysis of molecular beacon probes for qPCR detection of recA gene of B. burgdorferi and nidogen gene of mouse The specificity of each

molecular beacon for its respective amplicon was first determined by generating the denaturation profiles for each of three RecA probes with specific or irrelevant target oligonucleotides (Table 1; Figure 1). In the presence of the unrelated Nidogen target or in the absence of any target (buffer control), RecA1, RecA2, and RecA3 molecular beacons remain in a closed state at low temperatures with fluorophore and quencher held in close proximity by the hairpin formation. Molecular beacons remain dark at this state (1A, 1B and 1C). At temperature above the melting temperatures of the stems (71°C, 67°C and 75°C for RecA1, RecA2 and RecA3, respectively), the fluorophore separates from the quencher resulting in increase in fluorescence intensity. In contrast, these molecular beacons bind to their respective targets at low temperature resulting in the dissociation of the stem and an increase in fluorescence. At the melting temperatures of probe-target hybrids (68°C, 73°C and 75°C for RecA1, RecA2 and RecA3, respectively), dissociation of the probe from the target results in the return of the probe to a stem-loop structure, significantly diminishing the fluorescence.