Hybridization Chain Reaction (HCR) is a method to amplify double-stranded DNA containing many nicks in an enzyme- free manner using microRNA or single-stranded DNA as input. It requires three different templates with a hairpin structure and reacts at 37 ℃. We performed experiments based on existing methods 1.
For more information about the principle of HCR, see Proposed Implementation
For more information about the actual experimental procedure of HCR, see Wet Experiments_HCR
We attempted to observe the amplified product by agarose gel electrophoresis.
Agarose gel electrophoresis showed low resolution and blurred peaks.
Because the peak was blurred in 1., we attempted to observe the amplified product using a more sophisticated capillary electrophoresis system. The concentration of target miRNA or ssDNA corresponding to that was used as the variable.
The elongated peaks were observed only at 1 µM for miRNA and at 1 µM and 100 nM for ssDNA. The paper reported that the dynamic detection range of CRISPR-HCR is 1 fM-100 nM and that of HCR is 10 pM-100 nM, but this could not be reproduced at all.
Because the expected LoD could not be achieved in 2., changes were made to the experimental conditions.
The paper connects the products of HCR to Cas. Therefore, the concentration of target ssDNA/miRNA and the concentration of Cas target in the amplified product are expected to be correlated. It is expected that long amplified products contain more Cas targets and short amplified products contain fewer Cas targets.
Since one Cas target is contained per H2 or H3, one Cas target is contained per 60 bp of amplified product. 1 bp is approximately 330 Da, so this formula can be used to calculate the Cas target concentrations, taking into account all Cas targets contained in the various peaks.
For the results in 2., the peaks obtained by capillary electrophoresis were attributed to the assumed amplification product.
Capillary electrophoresis outputs the “molecular weight" and “concentration" of the peaks.Of these, the “molecular weight" was calculated by applying the molecular weight of the peak to the width of the upper and lower ladder of known molecular weight. If the peak is dsDNA, this calculation method can be used, but the amplified product of HCR is something like dsDNA with many nicks, and a discrepancy between the “molecular weight" calculated by the machine and the actual molecular weight is expected to occur.
Therefore, we avoided this problem by applying an amplified product with a value close to the “molecular weight" of the peak during attribution. Fortunately, the attribution was not difficult because, in principle, there are only a few amplification products with molecular weights close to the molecular weight of the HCR.
The results of the attribution showed that the amplification products are oligomers of n=10 at the longest. This indicates that the amplification efficiency of HCR is inadequate. The MultiNA we used has a lower detection limit of 0.2 ng/µL for DNA and a quantification range of 0.5-50 ng/µL 2. Therefore, the lack of detection when the target was at low concentrations could be due to the fact that it was below the detection limit of MultiNA. However, based on the attribution of this peak, only n=10 oligomers at most were produced, and it would be difficult to amplify a concentration of PAM sufficient to activate Cas from a target of a few fM.
Jia, H.-Y., Zhao, H.-L., Wang, T., Chen, P.-R., Yin, B.-C., & Ye, B.-C. (2022). A programmable and sensitive CRISPR/Cas12a-based MicroRNA detection platform combined with hybridization chain reaction. Biosensors and Bioelectronics, 211, 114382. https://doi.org/https://doi.org/10.1016/j.bios.2022.114382
Shimadzu Corporation. (n.d.). Microchip Electrophoresis System for DNA/RNA Analysis MCE-202 MultiNA Instruction Manual. http://mor.niboch.nsc.ru/public/MBA_Course/References/Electrophoresis/
devices/Shimadzu%20MultiNA%20manual.292-28464D_SWmanualMCE-202(E).pdf
Exponential amplification reaction (EXPAR) is a reaction in which SDA occurs exponentially. After receiving miRNA or ssDNA as input and hybridizing them with template ssDNA, DNA polymerase with strand displacement activity extends to the 5' end of the template to form dsDNA. The restriction enzyme recognition site on the dsDNA is nicked by nickase, and the polymerase recruits to the nicking site to cause strand displacement amplification. If the sequence of ssDNA of the amplified product is the same as the sequence of the input signal, the amplified product plays the same role as the target, and exponential amplification occurs. A 50 ℃ reaction is possible by using Bst 2.0 and Nt.BstNBI. We experimented with existing methods 1.
For more information about the principle of SDA, see Proposed Implementation_Amplification.
For more information about the actual experimental procedure of EXPAR, see Experiments_EXPAR.
We attempted to confirm the amplification in the mechanism of the paper. The paper used dsGreen, but we used SYBR Green Ⅰ. Since SYBR Green Ⅰ is a double-stranded DNA staining reagent with the same performance as dsGreen 2, this change does not affect the experimental results. In addition, OPC-purified oligo DNA was used.
The fluorescence changes were plotted below.
As in the paper, we were able to distinguish between the amplification curves for target 1 pM and 0 M. The amplification curve for target 1 pM started to rise about 7 min after the start of the reaction, which is consistent with the paper.
The reaction temperature of EXPAR is 50 ℃. In designing the ODE model of EXPAR in the Dry Lab, it was necessary to consider thermal inactivation of nickase during the reaction. Therefore, we conducted an experiment to confirm the thermal inactivation of nickase in the Wet Lab. Using the protocol in the ODE model paper 3 as a reference, we performed amplification reactions as usual and measured changes in fluorescence intensity using pre-incubated nickase solution for a certain period of time. The conditions other than pre-incubation of the nickase were the same as in the preliminary experiment.
For more information about the ODE model, see Model.
The fluorescence changes were plotted below. Nickase was not added in NC.
No change in the amplification curve due to the pre-incubation time of the nickase was observed. It can be considered that changes in the enzymatic activity of the nickase due to reaction time are negligible.
We purchased OPC-purified oligo DNA and PAGE-purified oligo DNA. We performed an experiment to see if the difference in amplification efficiency between these two purification methods makes a difference.
The left graph shows the result with OPC-purified oligo DNA and the right graph shows the result with PAGE-purified oligo DNA.
The fluorescence intensity was higher when PAGE-purified oligo DNA was used; since PAGE purification is a method that yields highly purified oligo DNA 4, the higher fluorescence intensity could be attributed to the higher concentration of the oligo DNA of interest in the same volume of solution. As for the amplification speed, there was almost no difference depending on the purification method.
When OPC-purified oligo DNA was used, the experimental procedure was the same as in the 1. Preliminary Experiment, but the amplification speed was about five times faster than in the 1.
The left graph shows the fluorescence change in 1. and the right graph shows the fluorescence change when OPC-purified oligo DNA was used in 3. After rearranging the conditions, it was found that Bst 2.0, a polymerase, was purchased again between section 2. and 3., and that only the lot of Bst 2.0 was different between section 1. and 3. Therefore, we concluded that the difference in amplification speed between the two was due to the difference in Bst 2.0 lot. In subsequent experiments, we used the new Bst 2.0 lot and re-examine the response to template / nickase / polymerace concentration.
An attempt was made to further lower the LoD by tuning the template concentration.
The fluorescence changes were plotted below.
The higher the template concentration, the stronger the fluorescence intensity. The overall amplification speed was so fast that differences in amplification speed due to differences in template concentration were buried, and differences in amplification speed could not be measured. Since lowering the template concentration decreases the amount of amplified product, it is desirable not to lower the template concentration for the purpose of amplifying and quantifying nucleic acids. Therefore, in subsequent experiments, template concentration was set at 25 nM as in the paper.
Attempts were made to further lower the LoD by tuning the nickase concentration.
The largest difference in the time for the amplification curve to rise between the target concentration of 100 pM and 0 M was observed when the nickase concentration was 1/2 times of that in the paper (0.125 U/µL). We considered the possibility of increasing the difference in the time until the amplification curve rises between 100 pM and 0 M by further decreasing the nickase concentration.
We attempted to further lower the LoD by tuning the polymerase concentration. Nickase concentration was set to 1/2 of the published value (0.125 U/µL).
The fluorescence changes were plotted below.
The difference in the time to amplification curve between target concentration 100 pM and 0 M was greatest when the polymerase concentration was 1/4 of the published value (0.02 U/µL). We considered the possibility of increasing the difference in the time to amplification curve rise between the 100 pM and 0 M by further lowering the polymerase concentration.
We attempted to further lower the LoD by simultaneously tuning the polymerase and nickase concentrations.
When the polymerase concentration was 1/16 times of that in the paper (0.005 U/µL) and the nickase concentration was 1/8 times of that in the paper (0.0625 U/µL), the amplification curves at 1 pM and 0 M could be distinguished.
To observe the LoD of this system, the experiment was repeated with a lower target concentration using the conditioning obtained in section 7.
The fluorescence changes were plotted below.
LoD was 1 pM.
The LoD was 1 pM when the new lot of Bst 2.0 was used with a polymerase concentration of 0.005 U/µL and nickase concentration of 0.0625 U/µL. EXPAR is an efficient amplification system and is promising to achieve the required amplification efficiency for POIROT within 30 min. On the other hand, EXPAR was shown to be unstable and highly dependent on the lot of the enzyme. The inclusion of EXPAR in the amplification system would reduce the overall robustness of the system. So we were forced to consider a different amplification system.
Carter, J. G., Orueta Iturbe, L., Duprey, J. H. A., Carter, I. R., Southern, C. D., Rana, M., Whalley, C. M., Bosworth, A., Beggs, A. D., Hicks, M. R., & Tucker, J. H. R. (2021). Ultrarapid detection of SARS-CoV-2 RNA using a reverse transcription-free exponential amplification reaction, RTF-EXPAR. Proceedings of the National Academy of Sciences, 118(35), e2100347118. https://doi.org/10.1073/pnas.2100347118
Funakoshi Co., Ltd. (n.d.). dsGreen: Kakusan geru senshoku shiyaku / riaru taimu PCR-yo SYBR®-kei keikō shikiso. https://www.funakoshi.co.jp/contents/67539
Özay, B., Murphy, S. D., Stopps, E. E., Gedeon, T., & McCalla, S. E. (2022). Positive feedback drives a secondary nonlinear product burst during a biphasic DNA amplification reaction. Analyst, 147(20), 4450-4461. https://doi.org/10.1039/D2AN01067D
FASMAC. (n.d.). DNA/RNA jutaku gosei seisei guredo no sentaku ni tsuite. https://fasmac.co.jp/dna_rna_purify_grade
The Three-Way-Junction SDA (TWJ-SDA) is a mechanism that initiates SDA based on a three-way junction complex formed by a short helper and a long template hybridizing with the target single-stranded nucleic acid. Ying Xu et al. reported achieving high sensitivity by using a hairpin-structured template and employing the ssDNA (trigger) produced from TWJ-SDA as a starting point for amplification in EXPAR 1.
For more information about the principle of TWJ and SDA, see Proposed Implementation_Amplification.
For more information about the actual experimental procedure of TWJ-EXPAR, see Experiments_TWJ-EXPAR.
This experiment aimed to confirm amplification from single-stranded nucleic acids based on the mechanisms described in the paper. Molecular beacon (MB) is used as the template for the latter half of amplification, EXPAR, in the paper. This choice is made for convenience in verifying amplification. In principle, it is equally acceptable to use unmodified ssDNA with the same sequence. Therefore, we conducted experiments using ssDNA with the identical sequence to the MB as the template and measured the fluorescence intensity of SYBR Green Ⅰ.
In the following sections, we denote the ssDNA that forms the three-way complex in the first stage as template1 and helper1, the ssDNA that forms the three-way complex in the second stage as template2 and helper2 and the ssDNA product from the first stage of amplification as trigger.
In the fluorescence measurements using both the MB and SYBR Green Ⅰ, no increase in fluorescence intensity dependent on target concentration was observed at all.
Amplification was not confirmed in either the SYBR Green Ⅰ measurements or the experiments using the MB as described in the paper. In the SYBR Green Ⅰ experiments, the concentration of the DNA used as the template was very high, and it is likely that these templates also possessed hairpin structures. Since SYBR Green Ⅰ primarily labels dsDNA, the background fluorescence intensity may have been high, potentially hindering accurate quantification of the amplification products.
However, the lack of amplification even with the MB as described in the paper suggests a need to segmentalize the mechanism further to identify bottlenecks, as well as to optimize the experimental conditions.
In the preliminary experiments using SYBR Green Ⅰ, the fluorescence intensity was significantly higher compared to the EXPAR conditions. According to reference 2, monitoring amplification reactions using SYBR Green Ⅰ is effective when the concentration of the DNA is extremely high or DNA capable of forming secondary structures do not exist in the system. In our setup, we were using template2 at a very high concentration of 1.3 µM, which was expected to have a hairpin structure that includes regions of dsDNA. Therefore, tracking the reaction via fluorescence intensity measurements with SYBR Green Ⅰ is likely inappropriate.
To address this, we investigated the fluorescence intensity as the concentrations of template2 and helper2 were gradually decreased.
No increase in fluorescence intensity was observed at any concentration. In all conditions, a final target concentration of 1 nM was added.
Regardless of the concentrations of template2 and helper2, the fluorescence intensity did not change. This suggests that a fundamental reconsideration of the amplification system is necessary.
We conducted the experiments in two phases, as illustrated in the diagram below.
To confirm whether amplification in the first phase occurs successfully.
We designed the mechanism as described above, added SYBR Green Ⅰ, and incubated at 37 ℃ to measure the fluorescence intensity.
The changes in fluorescence intensity are shown in the graph below.
When the target concentration was 1 µM, there was an initial high fluorescence intensity that subsequently decreased. The same trend was observed when using miRNA as the target, with very little fluorescence attenuation. Although a slight increase in fluorescence intensity was noted at concentrations below 100 nM, no amplification dependent on target concentration was observed.
In both cases, whether using miRNA or ssDNA as the target, amplification from the first phase could not be confirmed.
To confirm whether amplification in the second half of the reaction occurs successfully. We designed the mechanism as shown below and, in addition to fluorescence measurements using the MB, added SYBR Green Ⅰ with unmodified ssDNA that takes a hairpin structure as the template, incubating at 37 ℃ to measure the fluorescence intensity.
As shown in the graph below, no increase in fluorescence was observed when measuring the fluorescence intensity with SYBR Green Ⅰ.
When observed using the MB, an increase in fluorescence intensity over time was noted. However, this increase was not dependent on the concentration of the trigger.
In all experiments, it is unlikely that amplification of ssDNA occurred as we had expected. Both the first and second phases of the mechanism appear to have underlying problems.
In this mechanism, neither the first nor the second phase is functioning effectively, leading us to conclude that it is difficult to use POIROT as an amplification mechanism. Therefore, we considered alternative approaches.
Ying, X., Yu, W., Su, Liu., Jinghua, Y., Hongzhi, W., Yuna, G., & Jiadong, H. (2016).Ultrasensitive and rapid detection of miRNA with three-way junction structure-based trigger-assisted exponential enzymatic amplification. Biosensors and Bioelectronics, 81, 236-241. https://doi.org/10.1016/j.bios.2016.02.034
Wang, C., & Yang, C. J. (2013). Application of molecular beacons in real-time PCR. In M. D. Teintze (Ed.), Molecular Beacons (pp. 45-59). Springer. https://doi.org/10.1007/978-3-642-39109-5_3
ThisAmp is a modified version of the SDA reaction that incorporates the TWJ structure, and it was reported by Lee et al. 1.
For more information about the principle of TWJ and SDA, see Proposed Implementation_Amplification.
For more information about the actual experimental procedure of ThisAmp, see Experiments_ThisAmp.
This experiment was conducted to determine whether the annealing process of target, template, and helper to form a three-strand complex, which is done in the prior study, is truly necessary. If the annealing step can be omitted, the reaction could begin with a simple mixture of these DNAs and enzymes, making the mechanism more accessible and convenient for use in household settings.
The fluorescence changes were plotted below.
In the paper with annealing operation, the amplification curves for target 1 fM and negative control (NC) were distinguishable. However, skipping the annealing step resulted in distinguishable amplification curves only up to target concentrations of 100 nM, which is approximately \(10^8\) orders of magnitude worse than the results presented in the original paper. Based on these results, it was concluded that the annealing process is necessary.
We attempted to verify the amplification mechanism described in the paper. While the paper used NEBuffer 3.1 as the buffer, we opted to use NEBuffer r3.1. The only difference between these buffers is that albumin in the buffers is recombinant in NEBuffer r3.1. Additionally, the paper employed vent (exo-) DNA polymerase, but we used Bst 2.0, which had already demonstrated amplification in EXPAR. To accommodate Bst 2.0, we replaced the ThermoPol Reaction Buffer with Isothermal Amplification Buffer.
The fluorescence changes obtained are shown in the graphs below. The left graph represents the results up to 60 min. While we conducted measurements at 60 min, an increase in fluorescence intensity was observed in less than 2 min. The right graph zooms in on the first 10 min of the reaction.
The amplification curves for 10 nM and NC can be distinguished; however, the difference in the starting time of amplification is less than 2 min. This means that with even a slight extension of the reaction time, it becomes difficult to differentiate between the two. This could lead to an increase in false positive rates when used in a home setting. Therefore, this issue needs to be addressed for more reliable detection.
To suppress the amplification of NC and increase the time gap between the start of amplification for the target and NC, we performed tuning of the template concentration.
The fluorescence changes were plotted below.
When the template concentration was lowered, it was observed that the amplification efficiency decreased, and at concentrations lower than 1/64 of the value used in the reference paper, no amplification could be detected within 60 min in SYBR Green Ⅰ fluorescence measurement. However, lowering the template concentration would not only slow the amplification speed but also reduce the amount of amplified product. Given the goal of amplifying and quantifying nucleic acids, lowering the template concentration was not desirable. Therefore, the template concentration was kept at 50 nM, as specified in the original paper.
Tuning of polymerase concentration was performed to suppress NC amplification by decreasing the rate of amplification while maintaining the amount of amplified product, and to increase the difference between the time when target amplification begins and the time when NC amplification begins.
Fluorescence intensity was as shown in the left figure, and for polymerase concentration, the time until fluorescence intensity reached \(8 \time 10^5\) is shown in the right figure. Error bars represent standard deviation.
The largest difference in the time required for the fluorescence intensity to reach \( 8 \times 10^5 \) between the target concentration of 100 pM and 0 M was observed when the polymerase concentration was 1/4 of the published data, 0.012 U/µL. The difference at this time was about 20 min. Based on this, we thought thatwe could solve the problem described in 2. by reducing the polymerase final concentration to 0.012 U/µL.
To confirm the LoD of this system, the experiment was repeated with the conditions obtained in section 4. and 5.
The fluorescence changes were plotted below.
The LoD was 10 nM in 2. before tuning, but after tuning, the LoD was 100 pM.
ThisAmp had a LoD of 100 pM after optimization. This reaction is characterized by the fact that it proceeds at a constant 55 ℃ and requires no temperature change. ThisAmp is useful in that it can form a TWJ and amplify miRNAs, but it is not suitable for miRNA amplification due to its long target length (59 mer) . In addition, since the target, template, and helper must be annealed before adding the enzyme, it is difficult to connect other amplification mechanisms before this reaction considering a one-pot amplification system. Furthermore, since the main amplification product is dsDNA, it would also be difficult to connect other amplification mechanisms behind this reaction.
Lee, S., Jang, H., Kim, H. Y., & Park, H. G. (2020). Three-way junction-induced isothermal amplification for nucleic acid detection. Biosensors and Bioelectronics, 147, 111762. https://doi.org/10.1016/j.bios.2019.111762
TWJ-Toehold is a variant of the SDA reaction that introduces the TWJ structure and was reported by Chen et al. 1.
For more information about the principle of TWJ and SDA, see Proposed Implementation_Amplification.
For more information about the actual experimental procedure of TWJ-Toehold, see Experiments_ TWJ-Toehold.
We attempted to confirm the amplification by the mechanism in the paper. In the paper, the amplified products (trigger) activate CRISPR-Cas14a for nonspecific collateral cleavage of ss DNA reporter, which turn on for fluorescence. In contrast, we measured fluorescence intensity using SYBR Green Ⅰ. Since TWJ-Toehold is very similar to ThisAmp in the reaction mechanism, we thought that we could perform the same experiment using SYBR Green Ⅰ with TWJ-Toehold as we did with ThisAmp.
The fluorescence changes were plotted below.
LoD was 10 pM. In the paper, the fluorescence intensity is measured by connecting it to the CRISPR-Cas14a system, and the LoD at that time was 50 fM. We thought that we could further lower the LoD even if the reaction was not connected to the CRISPR system, so we decided to conduct tuning.
Tuning of the helper concentration was performed to further lower the LoD.
The fluorescence changes were plotted below.
The difference in the time at which the amplification curve starts rising when the target concentration is 1 pM and 0 M was the largest at the condition with the helper concentration 2.5 nM, as in the paper.
To confirm the LoD of this system, we performed the experiment again.
Fluorescence changes were obtained as shown in the graph below.
The LoD was 10 pM.
TWJ-Toehold had the LoD of 10 pM. This reaction is useful in that it can form a TWJ and amplify without the need for temperature changes at a constant 55 ℃, and has a detection limit \(10^1\) orders lower than ThisAmp, but the target is 51 mer long, making it unsuitable for miRNA amplification. In addition, since the target, template, and helper must be annealed before the enzyme is added, it is difficult to connect other amplification mechanisms before this reaction in a one-pot amplification system. Furthermore, since the main amplification product is dsDNA, it would also be difficult to connect other amplification mechanisms behind this reaction.
Chen, M., Jiang, X., Hu, Q., Long, J., He, J., Wu, Y., Wu, Z., Niu, Y., Jing, C., & Yang, X. (2024). Toehold-Containing Three-Way Junction-Initiated Multiple Exponential Amplification and CRISPR/Cas14a Assistant Magnetic Separation Enhanced Visual Detection of Mycobacterium tuberculosis. ACS Sensors, 9(1), 62-72. https://doi.org/10.1021/acssensors.3c01622
TWJ-2cycle is a variant of the SDA reaction that introduces the TWJ structure and was reported by Zhang et al. 1. This method is expected to have high specificity.
For more information about the principle of TWJ and SDA, see Proposed Implementation_Amplification.
The series of reactions proceed at an isothermal temperature of 37 ℃
First, we attempted to confirm the level of detection limit by conducting experiments based on the paper 1.
In the paper, Klenow (exo-) DNA Polymerase was used as the polymerase, but we used Bst LF, whose amplification at 37 ℃ has been confirmed in previous experiments.
The fluorescence changes were plotted below.
No amplification was observed at all.
The optimal conditions for Nickase and Polymerase are usually different. The optimal condition for Nt.BbvCI, the Nickase used in 1, is rCutSmart buffer, and NEBuffer 2.1 is the optimal condition for Bst LF, also used as Polymerase 2 3.
ThermoPol buffer, which is the optimal condition for Polymerase, was used based on the reference, but experience leading up to this experiment showed that using the buffer optimized for Nickase was a more successful finding.
Buffer was changed to rCutSmart Buffer, the optimal condition for Nt.BbvCI, and the experiment was performed.
The fluorescence changes were plotted below.
Amplification was confirmed by reaction in rCutSmart Buffer.
Even at a target concentration of 10 nM, it took about 100 min for the fluorescence intensity to increase. Amplification efficiency is insufficient for use as an amplification system for POIROT, which aims at detection and quantification at lower concentrations, and tuning or coupling with other methods should be considered.
Polymerase / Nickase was tuned for concentration.
The fluorescence changes were plotted below.
S/N ratio (ratio of fluorescence intensity to NC at target concentration of 1 nM) is an important factor in determining the quality of an amplification system. We determined the S/N for each condition at each time and its maximum value.
Polymerase 0.063 U/µL and Nickase 0.12 U/µL or Polymerase 0.063 U/µL and Nickase 0.16 U/µL showed good S/N ratios; the latter showed higher values than the former in S/N ratio, but the amplification curve shows no significant difference between them. Since enzymes are expensive and it is desirable to reduce the amount used, we considered 0.063 U/μL for Polymerase and 0.12 U/μL for Nickase to be optimal and decided to use these conditions for future experiments.
In many literatures, TWJ complexes are reported to be superior in terms of specificity. We have confirmed by experiment whether the formation of the TWJ complex has higher sequence specificity than hybridization of a pair of complementary DNAs. The results were fed back to Dry Lab and the reason why the TWJ complex is formed with high sequence specificity was discussed.
Similar sequences are known to exist in hsa-let-7b, the target miRNA of this system, and are named hsa-let-7a, hsa-let-7c, hsa-let-7d,..., hsa-let-7i. In the reference1, specificity has been studied for these series. We evaluated the specificity of the let-7 series plus an originally designed single nucleotide variant of let-7b.
The fluorescence changes were plotted below.
NJ: Sequence recognition using hybridization of complementary pairs of DNA
TWJ: Sequence recognition using the TWJ complex
In NJ-SDA, the amplification reaction occurred faster in some of the let-7 series than in NC, and in the single nucleotide mutant, the mutant was amplified faster than the perfect-match target.
In TWJ-SDA, the amplification curve is similar to that of Negative Control except for target in the let-7 series. This indicates that TWJ-SDA can ensure high specificity compared to NJ, that is, when the three-way complex is not formed.
The fluorescence intensity at 40 min after the start of the reaction, including the error range, is evaluated in the figure below (error bars indicate standard error).
For subsets of the let-7 series, no significant differences in fluorescence intensity were observed in TWJ compared to NC except for let-7b.
In NJ, let-7c was not significantly different from let-7b, and let-7e and let-7i showed significantly higher fluorescence intensity than NC.
Single nucleotide mutants showed no significant difference from the Negative Control except for mutants at 1 mer, 9 mer, and 11 mer from the 5' end.
Mutations from 5' end to 1 mer and 9 mer showed significantly higher fluorescence intensity after 40 min compared to NC, especially the mutation from 5' end to 1 mer, which was not significantly different from the perfect-match let-7b.
Thus, it was confirmed that the specificity changed depending on the position of the mutation.
For a discussion of the reasons for this, click here:
The use of TWJ showed extremely high specificity compared to NJ, indicating that TWJ-SDA is an extremely promising system to ensure the target specificity required for POIROT. However, the amplification efficiency of TWJ-SDA alone is considered insufficient for amplification of extremely low concentrations of miRNA in a few tens of minutes. Therefore, it is necessary to combine the system with other mechanisms to increase amplification efficiency.
Qing, Z., Feng, C.,Feng, X., Yongxi, Z., & Chunhai, F. (2014). Target-Triggered Three-Way Junction Structure and Polymerase/Nicking Enzyme Synergetic Isothermal Quadratic DNA Machine for Highly Specific, One-Step, and Rapid MicroRNA Detection at Attomolar Level. Anal. Chem. 2014, 86, 16, 8098-8105. https://doi.org/10.1021/ac501038r
New England Biolabs. (n.d.). Bst DNA polymerase, large fragment. https://www.neb.com/ja-jp/products/m0275-bst-dna-polymerase-large-fragment
New England Biolabs. (n.d.). Nt.BbvCI (nicking endonuclease). https://www.neb.com/ja-jp/products/r0632-ntbbvci
In SDA using TWJ, amplification can be performed by changing the template and helper sequences to target any miRNA in principle. However, it has been suggested that the stability of the TWJ portion changes the specificity and sensitivity 1.
Designing appropriate template and helper sequences according to the miRNA sequence to establish desired amplification is essential for the versatility of POIROT. Amplification experiments with various sequences were performed to obtain parameters for sequence design by Dry Lab.
We designed a number of templates and helpers to amplify hsa-miR-10b-5p, hsa-miR-375, and hsa-miR-30d-5p (referred to as Biomarker 1, 2, and 3 in this order), which have been reported as biomarkers for glaucoma, and conducted experiments.
More information about biomaker miRNA, click here:
To begin experiments using our own sequence design, we first modified only the miRNA-complementary sequence of the template used in the TWJ-2cycle. The template and helper we used in the TWJ-2cycle recognize let-7b, however, by changing miRNA-complementary sequence, they then recognize other miRNA.
We then changed the hybridization length of the template and helper to 5-7 bp.
We then measured the changes in fluorescence intensity under various target concentrations.
The experiments were performed using SYBR Green Ⅰ under the conditions tuned in TWJ-2cycle for the type and concentration of polymerase and nickase.
In the following, the helper for Biomarker n, which hybridizes with template and m bp, is referred to as helper n-m.
For each biomarker, the following measurements were obtained.
Amplification was confirmed for all helpers. In the case of all biomarker targets, the longer the chain length of hybridization between template and helper, the larger the initial slope of the amplification curve tends to be. To sum it up, the longer the hybridization length of the template and helper was, the greater the amplification rate became.
As for the difference in the fluorescence curve in response to the target concentration, we were able to clearly distinguish between NC and 1 pM or higher for biomarker1 when helper1-7 was used. Furthermore, looking at the slope in the first linear amplification section, it was confirmed that there was a positive correlation with target concentration in the region of 1 pM - 100 pM target concentration. In other words, the amplification rate of TWJ-SDA is considered to be determined by the target concentration.
However, for biomarker 2 and 3, there was no helper that showed a clear target concentration-dependent amplification rate.
The stability of the TWJ complex is related not only to the hybridization region between template and helper, but also to the region where the target and template hybridize. It will be necessary to conduct experiments by changing the hybridization length of the template and target to find the optimal TWJ structure.
As mentioned above, the stability of the TWJ complex is related not only to the hybridization region between template and helper, but also to the region where the target and template hybridize. For this reason, Dry Lab designed three types of templates for each biomarker, and the hybridize lengths of target and template, and helper and template were changed for further experiments independently.
For biomarker 1, 2, and 3, the hybridize lengths of template and target were 10, 11, and 12 bp, and the hybridize lengths of helper and template were 5, 6, 7, and 8 bp, respectively.
The following amplification curves were obtained. For each template/helper pair, the amplification curves are shown with (solid line) and without (dashdot line) the addition of the final 10 nM of target.
In the following, if the hybridize length of template and target is 10 bp, the hybridize length of helper and template is 5 bp, for instance, this experiment condition will be referred to as 10-5.
The ratio of the fluorescence intensity at the 10 nM (target) to that at 0 M after 30, 45, and 60 min was calculated as shown in the table below. Here, the ratio of the fluorescence intensity at each time minus the fluorescence intensity at the first cycle was calculated to exclude what was considered to be background fluorescence.
The larger this ratio, the more clearly the target concentration can be distinguished.For Biomarker 1, when the condition was 12-5, that is, when the hybridize length between template and target was 12 bp, and the hybridize length between template and helper was 5 bp, the ratio was the largest.
Similarly, it was concluded that 10-5 or 12-7 for Biomarker2 and 12-6 for Biomarker3 would be optimal.
For more detailed analysis, click here:
Qing, Z., Feng, C.,Feng, X., Yongxi, Z., & Chunhai, F. (2014). Target-Triggered Three-Way Junction Structure and Polymerase/Nicking Enzyme Synergetic Isothermal Quadratic DNA Machine for Highly Specific, One-Step, and Rapid MicroRNA Detection at Attomolar Level. Anal. Chem. 2014, 86, 16, 8098-8105. https://doi.org/10.1021/ac501038r
Strand Displacement Amplification (SDA) is a method to produce a large amount of ssDNA by using DNA polymerase with strand displacement activity and nickase, which recognizes dsDNA and puts a nick on one of the strands. We focused on the system 1 developed by Dr. Komiya at JAMSTEC. This system is a multi-step combination of SDA reactions to amplify ssDNA. The SDA reaction is originally subject to amplification even in negative control, but in this system, negative control is suppressed by various innovations. We call this system “multistep-SDA" and conducted experiments.
For more information about the principle of multistep-SDA, see Proposed Implementation_Amplification
For more information about the actual experimental procedure of multistep-SDA, see Experiments_Multistep-SDA
We attempted to confirm the amplification from single stranded nucleic acid by the mechanism described in the paper.
The paper uses NEBuffer 2 as the buffer, but we used NEBuffer 2.1. The only difference between NEBuffer 2 and NEBuffer 2.1 is whether DTT or albumin is used in the buffer, which does not seem to affect the enzyme activity 2. In addition, in the paper, the 3' ends of the template DNA strands are chemically modified with carboxytetramethylrhodamine (TAMRA). We used ssDNA without this modification as the template. Fluorescence intensity was measured using MB as in the paper.
The fluorescence changes were plotted below.
It could be distinguished from NC if the target concentration was at least 100 pM. In the paper, no amplification of NC was observed after 150 min, but in this experiment, amplification started at about 25 min.
We conducted further experiments to elucidate the cause of the apparently faster amplification than in the paper.
We wanted to clarify the cause of the apparent faster amplification than in the paper. To determine which step was responsible, we performed experiments with each step of multistep-SDA, as well as with two or three steps of multistep-SDA connected together. Since the MB used in the paper cannot detect the amplification products of the first and second steps of SDA, we also measured the fluorescence intensity using SYBR Green I or SYBR Green II. Additionally, we performed experiments using the optimized buffer in the paper (we call it LT Buffer) instead of NEBuffer 2.1.
The fluorescence changes were plotted below.
When only step1 and step2 were used, the amplification speed was slow and amplification of NC was not observed, but amplification of target was also almost unobservable. It was confirmed that amplification efficiency increased with the number of steps, but when two or more steps were linked, amplification of NC was observed. Also, when NEBuffer 2.1 and LT Buffer were compared in step123, no significant difference was observed.
In the paper, no amplification of NCs was observed in the 3step-SDA reaction, but in our experiment, amplification of NCs was observed by connecting multiple steps of SDA. We asked Dr. Komiya, the author of the paper and our extra adviser, for tips. He told us that it is important that the 3' ends of template DNA are chemically modified with carboxytetramethylrhodamine (TAMRA) .
Based on the advice, we performed follow-up experiments with template DNA strands whose 3' ends are chemically modified with TAMRA. Fluorescence intensity was measured using MB like in the paper.
Within 200 min of observation, amplification was observed at target concentrations of 10 nM or higher for only step3 and step23, and at target concentrations of 100 pM or higher for step123. In all cases, NC amplification was suppressed.
By using a template with TAMRA modification at the 3' end, amplification was confirmed within 200 min of the observation when the target concentration was 10 nM or higher for only step3 and step23. For step 123, amplification was confirmed when the target concentration was 100 pM or higher. In all cases, amplification of NCs was not confirmed during the observation time.
By using a template with TAMRA modification at the 3' end to link multiple stages of SDA, it was confirmed that target amplification could be efficiently achieved while NC amplification was suppressed. The increase in amplification efficiency by increasing the number of stages was also confirmed. However, amplification was observed within 200 min only when the target concentration was 100 pM or higher, and this mechanism cannot be used in POIROT, which aims for detection in the fM order. Therefore, Multistep-SDA must be combined with other amplification mechanisms.
Multistep-SDA is a system that uses short nucleic acids as input, and in principle, any sequence of nucleic acids can be amplified by changing the template sequence. In addition, this system is characterized by the fact that it proceeds at 37 ºC without the need for temperature changes. Furthermore, it is also possible to amplify dsDNA by changing the template sequence and eliminating the nicking site. Therefore, multistep-SDA is a useful system that can be easily connected to other amplification methods that proceed at 37 °C and to the CRISPR-Cas system that targets dsDNA.
Komiya, K., Noda, C. & Yamamura, M. (2024). Characterization of Cascaded DNA Generation Reaction for Amplifying DNA Signal.New Gener. Comput. 42, 237-252. https://doi.org/10.1007/s00354-024-00249-2
New England Biolabs. (2013). Why did you remove DTT from your restriction enzyme buffers? https://www.neb.com/ja-jp/faqs/2013/02/28/why-did-you-remove-dtt-from-your-restriction-enzyme-buffers
Based on the previous results, it has been confirmed that EXPAR lacks robustness, TWJ-SDA has excellent specificity but insufficient amplification efficiency, and multistep-SDA can achieve high amplification efficiency while minimizing NC compared to conventional linear SDA and TWJ-SDA.
However, for multistep-SDA, amplification has been almost undetectable for low-concentration targets, making it unsuitable as a standalone amplification system for POIROT. Therefore, we pursued the establishment of an amplification system that achieves robustness, specificity, and sufficient amplification efficiency by using the amplification products of TWJ-SDA as the target for multistep-SDA.
To start, we used a TWJ-SDA template that produces the sequence to be the target for multistep-SDA to attempt amplification starting from biomarker1. The sequences used were those modified with a quencher at the 3' end for multistep-SDA and templates suggested to be suitable based on the designed sequence. For the polymerase and nickase, we utilized the conditions tuned in the TWJ_2cycle, specifically 0.063 U/µL Bst LF and 0.12 U/µL Nb.BbvCI.
Additionally, due to the subtle differences in optimal conditions for Cas and nickase, we used a custom-formulated buffer called UTokyo Buffer, which was designed by referencing the compositions of both.
For more Details on the preparation of UTokyo Buffer, see Experiments.
For a discussion of orthogonality with Cas, see CRISPR-Cas.
We refer to the TWJ template as template0, and the templates for the first, second, and third stages of multistep-SDA as template1, template2, and template3, respectively. Experiments were conducted using the TWJ-SDA product as the target under conditions where the first, second, and third stages of SDA were combined. Additionally, for comparison, we also performed experiments with only TWJ, TWJ > 2step-SDA, and 2step-SDA alone.
The fluorescence changes were plotted below.
Even when multiple stages were combined, similar changes in fluorescence intensity were observed as in the case of TWJ-SDA alone. This suggests that the amplification products of TWJ are not effectively connecting to the subsequent stages.
Analysis from the Dry Lab indicated that the amplified ssDNA is more stable when attached to the 5' side of the previous template, suggesting that the process may not advance to the next step until all previous converters are fully occupied on the 5' end.
To address this bottleneck, we redesigned the template to enhance its stability at the 3' end. By conducting experiments with the redesigned template, we expect to resolve the connectivity problems between TWJ-SDA and multistep-SDA. Furthermore, since it is believed that increasing the template concentration in later stages would also be effective, experiments should be conducted to verify this as well.
Using the redesigned sequences, we performed amplification reactions with only TWJ-SDA and with the connection of TWJ-SDA to 3step-SDA. This allowed us to verify whether the problems in the connectivity between TWJ-SDA and multistep-SDA had been resolved.
The fluorescence changes were plotted below.
Note that fluorescence was measured with SYBR Green Ⅰ for TWJ and MB for the 3step-SDA-linked one.
In systems where a large number of templates and primers coexist, as confirmed by multistep-SDA, it is expected that MB can be used to track specific chemical species 1.
In the case of TWJ-SDA, a linear amplification curve was obtained, whereas when TWJ-SDA was connected to 3step-SDA, an increase in amplification speed was observed around the 40-minute mark.
Compared to the 1. preliminary experiment, it was confirmed that the redesign of the template enabled the successful functioning of multistep-SDA using the products of TWJ-SDA as primers.
Previously, template concentrations had been template1: 10 nM, template2: 50 nM and template3: 100 nM, according to the multistep-SDA reference paper 2. However, due to the changes in the buffer and the connection from TWJ-SDA, it is necessary to retune the template concentration. This system, being a combination of multiple stages of SDA, makes the ratio of template concentrations a critical factor for success, as mentioned previously.
2step-SDA was linked after TWJ-SDA. template0 (template of TWJ-SDA) concentrations were 1, 5 and 10 nM, with template2/template1 and template1/template0 concentration ratios of 2, 3, 4 and 5 fold, respectively. Experiments were performed at 10 pM Biomarker1 and 0 M and fluorescence intensity was measured using SYBR Green Ⅰ.
The fluorescence changes were plotted below.
Here, the \(r\) in the caption indicates the ratio of concentrations between templates.
As the concentration of template0 increases and the ratio of template concentrations becomes larger, the slope of the amplification curve increases for both the presence and absence of the target. In other words, the amplification speed is greater.
When the total template concentration is high, the background fluorescence intensity also increases.
When the concentration of template0 is relatively high at 10 nM, the differences between the presence and absence of the target become unclear, or it is observed that the fluorescence intensity and amplification speed are greater in the absence of the target. This indicates that non-specific amplification for the target is dominating.
We decided to adopt conditions where the concentration of template0 is set at 5 nM and the ratio between the templates is 2, as these conditions facilitate faster amplification in the presence of a biomarker at 10 pM compared to the absence of a biomarker, without overly increasing the template concentration. That is, 5 nM template0, 5 nM helper, 10 nM template1, 20 nM template2, 40 nM template3.
The multistep-SDA we are using allows for flexibility in the number of stages that can be added. While increasing the number of stages is expected to improve amplification efficiency, it is essential to avoid overly complex mechanisms.
Based on the experimental results above, it is expected that connecting TWJ-SDA with 3step-SDA yields the desired amplification efficiency within approximately 30 to 60 minutes. Under the tuning conditions, experiments were conducted using a mechanism that connects the TWJ-SDA with 2step and 3step-SDA, adding microRNA of fM order.
Additionally, a new MB was designed to detect the products of the 2step-SDA, and in this experiment, fluorescence was measured using the MB for both the 2step and 3step processes.
The fluorescence changes were plotted below.
As expected, the 3step-SDA showed superior amplification efficiency. Although the 2step mechanism is simpler and more desirable, its amplification was slow and diminishes the difference in target concentration. Therefore, we decided to connect the TWJ-SDA and the 3step-SDA as the amplification system for POIROT.
Furthermore, to ultimately produce dsDNA that activates Cas3 or Cas12a, it is necessary to perform an elongation reaction using the final products of the multistep-SDA to produce dsDNA.
To activate Cas3 or Cas12a in the final step, it is necessary to produce dsDNA. We designed the following mechanism to produce the desired dsDNA through an elongation reaction using the final products of the multistep-SDA as primers.
In this mechanism, similar to the elongation reactions using previous templates, the primer hybridizes to the 3' end of the template, and then the DNA polymerase elongates the 3' end of the primer. The key difference is that the product does not contain a nicking site, allowing for the production of dsDNA without introducing nicks.
The ssDNA that serves as the template for this mechanism is referred to as ds-template.
Cas3 or Cas12a recognizes a double-stranded PAM sequence and a single-stranded spacer sequence for activation. It has been reported by Yoshimi et al. that even partial PAM sequences combined with a complete spacer sequence can still elicit some level of activity 3. Therefore, a sequence complementary to the spacer sequence was incorporated into the ds-template.
In other words, the ds-template sequentially contains a complementary sequence to the primer, a PAM sequence, and one strand of the complementary spacer sequence, starting from the 3' end. The final product is dsDNA, and tracking it using the fluorescence intensity of MB is not feasible in principle. Therefore, we conducted the experiments using SYBR Green Ⅰ. In the final stage, we performed two types of experiments: elongation only after 1step-SDA and elongation using the ds-template.
The fluorescence changes were plotted below.
In both experimental conditions, the background fluorescence intensity was high, and subsequent fluorescence changes were not monotonic. Particularly in experiments using only the ds-template, only elongation reactions occurred. Fluorescence measurements using SYBR Green, which emits fluorescence through non-specific nucleic acid recognition, suggested that changes in fluorescence intensity were buried in background noise, making accurate quantification difficult. There are no known simple methods for sequence-specific recognition using fluorescent dyes or aptamers. By connecting to the Cas system, we expect to be able to quantify dsDNA in a sequence-specific manner for the first time. Therefore, we decided to perform the tuning for the part that produces dsDNA in section CRISPR-Cas. Please refer to the details here.
In previous experiments, nucleic acids diluted with TE were used as targets. POIROT targets miRNA in tear fluid, and in order to further increase the reliability of POIROT as an amplification system, we conducted amplification using miRNA diluted in artificial tear fluid as a target, taking into account the effects of differences in solution types on amplification. The conditions were those that had been tuned so far. In addition, comparative experiments were conducted using nucleic acids diluted with TE.
The fluorescence changes were plotted below.
When miRNA diluted with artificial tear fluid or TE was used as a target, the following amplification curve was obtained.
Under the tuned conditions, we were able to detect target miRNAs down to about 1 fM.
In particular, it was confirmed that amplification whose speed was depending on the target concentration occurred in the range of 1 fM to 100 fM.
When comparing artificial tear and TE, amplification occurs faster in artificial tear at all target concentrations. This is presumed to be due to changes in enzyme activity due to differences in salt concentration. The composition of the artificial tear is 13 nM KCl, 68 nM NaCl (pH 7.0 - 8.0) 4. However, it was confirmed that the relative relationship did not change and that the amplification reaction occurred without any problem in the artificial tear.
Through the experiments conducted thus far, the overall structure of the amplification system for POIROT has been determined. Specifically, we initiate with the product of TWJ-SDA, followed by 3step-SDA, and use the final product as a primer for the elongation reaction, which produces dsDNA that activates either Cas3 or Cas12a.
At this stage, by using a sequence complementary to the spacer in the ds-template, we ensure that dsDNA is produced only when the elongation reaction occurs, which in turn activates Cas. Additionally, we expect that using the Cas-based method allows for accurate quantification of the final product, dsDNA.
Wang, C., & Yang, C. J. (2013). Application of molecular beacons in real-time PCR. In M. D. Teintze (Ed.), Molecular Beacons (pp. 45-59). Springer. https://doi.org/10.1007/978-3-642-39109-5_3
Komiya, K., Noda, C. & Yamamura, M. (2024). Characterization of Cascaded DNA Generation Reaction for Amplifying DNA Signal.New Gener. Comput. 42, 237-252. https://doi.org/10.1007/s00354-024-00249-2
Yoshimi, K., Takeshita, K., Kodera, N., Shibumura, S., Yamauchi, Y., Omatsu, M., ... & Mashimo, T. (2022). Dynamic mechanisms of CRISPR interference by Escherichia coli CRISPR-Cas3. Nature Communications, 13 (4917), 1-11. https://doi.org/10.1038/s41467-022-32618-0
Santen Ct,.Ltd. (n.d.). Soft Santear. https://www.santen.com/content/dam/santen/japan/pdf/
healthcare/eye/products/otc/soft_santear.pdf
To determine the type of Cas to be used as the detection system in POIROT, we compare the collateral activity of Cas3 and Cas12a. For reasons why these Cas proteins were selected as candidates, see Proposed Implementation_Amplification. Both cas3 and cas12a proteins are activated by dsDNA and exhibit collateral activity, indiscriminately cleaving ssDNA present in the vicinity.
Based on the study by Yoshimi et al. 1, we evaluated the collateral activity using the FQ Probe employed in their research. The FQ Probe is an ssDNA with a fluorescent molecule attached to the 5' end and a quencher attached near the center and at the 3' end. Normally, fluorescence is not observed due to the quenching effect. However, when the ssDNA is cleaved by collateral activity, fluorescence is emitted.
We added various concentrations of dsDNA that activate Cas to the FQ Probe and Cas3 or Cas12a, and observed the fluorescence intensity for each.
The fluorescence changes were plotted below.
For both Cas proteins, it was confirmed that without dsDNA, there was no change in fluorescence intensity. On the other hand, with dsDNA, the fluorescence intensity increased over time. The fluorescence intensity was found to increase roughly in proportion to time until it reached saturation. Therefore, by analyzing the slope of the fluorescence curve between 1 min and 3 min after the start of the reaction, the results were as shown below.
The slope of the fluorescence curve corresponds to the cleavage rate of Cas's collateral activity. It was confirmed that for Cas3, the cleavage rate fully depended on the target dsDNA concentration across the entire range of 0-30 nM. For Cas12a, it was dependent on the range of 0-10 nM. Within the 0-10 nM range of dsDNA, Cas12a's cleavage rate was approximately five times higher than that of Cas3. Given that Cas3 exhibits a broader concentration-dependent range and that suppressing false positives is crucial in POIROT, we decided to use Cas3 in the detection system. Further experiments will be conducted to link Cas3 with amplification in order to incorporate it into POIROT.
In the paper, Cas3 reaction is performed in CONAN Buffer, and we also used it in the above experiments. However, in POIROT, which plans to perform amplification and Cas reactions in the same solution, it is necessary to find a buffer that will work well for both reactions. From our experimental results, we knew that the TWJ reaction works in rCutSmart Buffer, the multistep-SDA reaction works in NEBuffer 2.1, and the Cas reaction works in CONAN Buffer. Therefore, we independently prepared UTokyo Buffer, which mimics the composition of CONAN Buffer but has a pH of 7.7, which is between rCutSmart Buffer (pH 7.9) 2, NEBuffer 2.1 (pH 7.9) 3, and CONAN Buffer (pH 7.5) 1. Then, we connected TWJ-SDA and 3step-SDA and attempted amplification starting from biomarker 1 using four types of buffers (rCutSmart Buffer, NEBuffer 2.1, CONAN Buffer, UTokyo Buffer).
For more information about the components of UTokyo Buffer, see Experiments Basic Operations
The fluorescence changes were plotted below.
When rCutSmart Buffer, NEBuffer 2.1, and CONAN Buffer were used, NC amplification was fast and could not be distinguished from the case with target contained. On the other hand, when UTokyo Buffer was used, the amplification rate of NC was suppressed, and it was possible to distinguish between target concentration 100 pM and NC. From this, it is thought that the amplification system will work if TWJ-SDA and multistep-SDA are connected using UTokyo Buffer.
In experiment 2., we confirmed that our amplification system works in UTokyo Buffer. In order to perform amplification and Cas reactions in the same solution at POIROT, we conducted an experiment to confirm whether Cas3 works in UTokyo Buffer.
When a low concentration of dsDNA was used, the fluorescence change shown in the lower left graph was obtained. The lower right shows the fluorescence change when the collateral activity of Cas3 was investigated in CONAN Buffer.
It was shown that Cas3 works without problems even in UTokyo Buffer. Therefore, if UTokyo Buffer is used, it is thought that both the amplification and Cas reactions will work, and the presence or absence of target can be distinguished using Cas3.
A comparison of the collateral activities of Cas3 and Cas12a showed that Cas3 has a wider region in which the cleavage rate is completely dependent on the target concentration. Since it is important to suppress false positives in POIROT, we decided to incorporate Cas3 into POIROT.
In addition, it was shown that amplification occurred without problems even when TWJ Amplification and multistep-SDA were connected in a uniquely adjusted UTokyo Buffer, and that it was possible to suppress the amplification speed of NC. Furthermore, Cas3 was shown to work in UTokyo Buffer. Since POIROT is intended to perform the amplification and Cas reactions in the same solution, we decided to use UTokyo Buffer, which is thought to work well for both reactions.
Yoshimi, K., Takeshita, K., Yamayoshi, S., Shibumura, S., Yamauchi, Y., Yamamoto, M., Yotsuyanagi, H., Kawaoka, Y., & Mashimo, T. (2022). CRISPR-Cas3-based diagnostics for SARS-CoV-2 and influenza virus.iScience 25, 103830, 1-13. https://doi.org/10.1016/j.isci.2022.103830
New England Biolabs. (n.d.). rCutSmart™ Buffer. https://www.neb.com/ja-jp/products/b6004-rcutsmart-buffer
New England Biolabs. (n.d.). NEBuffer™ 2.1. "https://www.neb.com/ja-jp/products/b7202-nebuffer-2-1
The experiments conducted so far aimed to establish the amplification system, allowing for the amplification of DNA in a manner dependent on the initial concentration of fM order biomarker miRNA by the selection of methods and tuning the concentrations of reagents. To visually represent the concentration of nucleic acids as an input signal, we aimed to use dsDNA as the final product and employ the collateral activity of Cas3 to quantify the biomarker miRNA.
To start, we performed a series of amplification reactions using biomarker 1, and then designed an elongation reaction for dsDNA using the final products of the multistep-SDA as primers. Similar to the Wet Results_CRISPR-Cas, we measured the collateral activity of Cas using an FQ probe.
For comparison, we designed an elongation reaction for dsDNA using the products of the 2-step multistep-SDA as the starting point, and conducted experiments on this as well, utilizing an FQ probe in the same manner.
The fluorescence changes were plotted below.
In both cases, an increase in fluorescence intensity was observed at all target concentrations, including the NC. However, no differences based on target concentration were noted, making it impossible to distinguish between the NC and other samples. From the experimental results conducted by varying dsDNA concentrations, it was evident that the collateral activity of Cas3 is completely dependent on the concentration of the activated dsDNA. This suggests that the final product dsDNA is produced in a independent manner relative to the target in the amplification system.
The experiment of 1. was conducted in a one-pot manner, meaning that amplification and the cleavage of ssDNA by Cas3's collateral activity occurred simultaneously. This could lead to different behavior, as the template may also be cleaved, compared to previous experiments that focused solely on amplification.
To address this, we performed the amplification for a fixed incubation time (in this case, 40 minutes) before adding Cas3 protein, cascade protein, and the FQ probe, followed by measuring changes in fluorescence intensity. This approach allows the amplification reaction to proceed without the influence of Cas3's collateral activity, leading to collateral activity dependent on the concentration of the dsDNA product generated from amplification.
Therefore, we expect to observe rapid changes corresponding to the initial concentration.
The fluorescence changes were plotted below.
Even in the two-pot reaction, amplification of the NC was observed. During the initial few minutes of fluorescence measurement, the slope for the NC was nearly indistinguishable from that of the target concentrations ranging from 1 fM to 10 pM. From the results of CRISPR-Cas, the slope of the graph in this section, that is, the cleavage rate due to collateral activity, should depend on the concentration of the produced dsDNA. Therefore, it suggests that there may be some problem in the amplification stage, leading to the final product dsDNA being produced in a target-independent manner.
To address this problem, we first conducted experiments by segmenting the mechanism to investigate which part of the amplification system was acting as a bottleneck.
To identify the bottleneck, we designed a system that connects the ds-template after the 0, 1, 2, and 3 steps of SDA and measured the collateral activity of Cas3. In each experiment, the target concentration was varied around the expected amount of intermediate products when starting with 1 fM of miRNA.
The fluorescence changes were plotted below.
In the case of the dsDNA extension reaction alone, no increase in NC fluorescence intensity was observed, and the graph showed a slope dependent on target concentration. When connecting the 1step-SDA with the dsDNA extension reaction, the final concentration displayed a slope dependent on the target concentration in the range of 0 - 10 nM. However, an increase in NC fluorescence intensity was observed.
When the 2step-SDA was connected with the dsDNA extension reaction, the target final concentration could be clearly distinguished between 0 M and above 1 nM, but differences above 1 nM were not distinguishable. In the case of connecting the 3step-SDA with the dsDNA extension reaction, the fluorescence intensity in NC increased at a rate similar to other conditions, making it impossible to differentiate between conditions.
From these results, it can be concluded that while the dsDNA extension reaction alone allows for quantitative detection while suppressing NC, the increase in fluorescence intensity in NC when connected with SDA indicates that tuning the template concentration is necessary.
When connecting the 1step-SDA with the dsDNA extension reaction, we need to find the appropriate ds-template concentration.
In condition Establishment of Amplification, the concentration of template 3 is 40 nM, and the concentration ratio between templates is tuned to 2, resulting in a ds-template concentration of 80 nM. However, to suppress NC while allowing for rapid amplification in the presence of the target, experiments were conducted by varying the concentration.
The fluorescence changes were plotted below.
As the concentration of the ds-template increased, a trend was observed where the amplification of the NC occurred more rapidly. It was determined that a final concentration of either 8 nM or 16 nM of ds-template would be promising, as it allows for clear differentiation between low target concentrations and the NC while effectively suppressing the NC.
Therefore, we tuned the ds-template concentration to 12 nM and conducted experiments connected through a 3step-SDA.
We tuned the ds-template concentration to 12 nM and conducted experiments connected through a 3step-SDA. For comparison, we also performed experiments at the original concentration of 80 nM.
The fluorescence changes were plotted below.
The increase in fluorescence intensity at 12 nM of ds-template was also observed at NCs, but 1 fM and NCs were clearly distinguishable.
In the control experiment, when the ds-template concentration was 80 nM, the fluorescence intensities at all concentrations showed similar changes and could not be used as a detection mechanism.
Tuning made it possible to link 3step-SDA and cas3 to detect nucleic acids at low concentrations.
We succeeded in detecting 1 fM nucleic acids by our mechanism of linking 3step-SDA and ds-Amplification by tuning the template concentration. The mechanism linking miRNA to Cas3 via TWJ has not been realized due to time constraints; however, it has been demonstrated that our mechanism can be used to detect nucleic acids at low concentrations using Cas3.
We were able to establish the mechanism of POIROT from Amplification to Detection by our previous experiments.
All previous experiments have measured fluorescence intensity by using a special machine. Finally, we aim at visual detection and quantification by using LFA.
The principles of LFA differ depending on the reagents used. We assembled the LFA with reference to CONAN developed by Yoshimi et al. 1.
The strip used was pre-installed with AuNPs with rb anti FITC antibody on the conjugate pad, streptavidin on the control line (C-line), and anti rb antibody on the test line (T-line). FITC-ssDNA-biotin was used as a reporter 2. When CRISPR-Cas3 is activated, the ssDNA within the reporter molecule is cleaved, producing FITC-labeled reporter fragments and biotin-labeled reporter fragments. Using this, both the T-line and C-line turn red if the test is positive, and only the C-line turns red if the test is negative.
For more information about the principle of LFA, see Proposed Implementation_Selection of Amplification and Quantitative Detection Module.
For more information about the actual experimental procedure of LFA, see Experiments.
We conducted an experiment to confirm the performance of the strip used. The purpose of this experiment was to confirm that only the C-line turns red when a reaction solution containing only FITC-ssDNA-biotin is used.
According to the product guide 2, if the concentration of FITC-ssDNA-biotin is not appropriate or the viscosity of the buffer is low, the T-line may turn red even if ssDNA is not cleaved. Therefore, we referred to the product guide and adjusted the concentration of FITC-ssDNA-biotin to 1.00 pM/LFA. A comparison was made between using the assay buffer that comes with the product as is and adding 5% polyethylenglycol (PEG) to the assay buffer.
The product used this time is designed to be used by standing the strip vertically, immersing the bottom part in the developing solution, and using the developing solution to flow the reaction solution. However, we are convinced that POIROT would be easier to use by placing the strip horizontally so that the user did not have to hold the strip vertically during the reaction. So we conducted an experiment with the strip horizontal. We kept the strip horizontal without touching it by folding a piece of paper to create a stand like the one pictured below.
After 5 min of development, the following bands were obtained. The upper strip had no PEG added to the buffer, and the lower strip had PEG added to the buffer.
When PEG was not added to the assay buffer, not only the C-line but also the T-line became colored. On the other hand, when 5% PEG 6000 was added to the buffer, the T-line did not turn red and only the C-line turned red. When performing quantitative determination using this product, it was shown that it is necessary to increase the viscosity of the assay buffer by adding PEG, etc.
We conducted an experiment to determine whether LFA functions when connected from the amplification system. First, we thought about connecting from a simple 1step-SDA.
A case where primer2 of multistep-SDA was added to the reaction solution at a final concentration of 5 nM was compared with a case where primer2 was not added (NC).
After 10 min of development, the following bands were obtained. The upper strip is NC and the lower strip is when primer2 was added.
Even when primer2 was added, no T-line coloration was observed.
The graph below shows the fluorescence change measured using an FQ probe up to 20 minutes later when 1step-SDA was connected to Cas3. Regardless of whether the final concentration of ds-template is 8 nM or 16 nM, an increase in fluorescence intensity can be confirmed when the final concentration of primer2 is 4 nM.
The conditions for this experiment were an incubation time of 20 min, ds-template (12 nM), and primer2 (5 nM) or NC (primer2: 0 M). From the above graphs, it is expected that a sufficient amount of ssDNA would be cleaved when the primer is added, and no cleavage would occur when the primer2 is not added. That is, if primer2 was present, both the C-line and T-line would be colored, and if primer2 was not present, only the C-line would be colored. However, in reality, even when primer2 was added, the T-line did not turn red.
Furthermore, the color of the C-lines were extremely pale compared to when PEG 6000 was not added to the assay buffer in experiment 1. AuNPs with rb anti FITC antibody flowing on the conjugate pad are captured by either C-line or T-line. Therefore, if the T-line is not colored, it is expected that the C-line will be strongly colored. However, in this experiment, the coloring of the C-line was weak even though the T-line was not colored. From this, it is thought that the binding between FITC-ssDNA-biotin or FITC-labeled reporter fragment and AuNPs with rb anti FITC antibody did not occur sufficiently on the conjugate pad, and the AuNPs with rb anti FITC antibody remained on the conjugate pad.
In the product used this time, it was suggested that the negative control only works by increasing the viscosity of the assay buffer. However, if the viscosity of the assay buffer is made too high, the reporter and AuNPs with rb anti-FITC antibody will not be able to bind in sufficient quantities on the conjugate pad, and the T-line may not be colored even under conditions that should be positive. When incorporating this product into POIROT, it is necessary to optimize the viscosity of the buffer.
Yoshimi, K., Takeshita, K., Yamayoshi, S., Shibumura, S., Yamauchi, Y., Yamamoto, M., Yotsuyanagi, H., Kawaoka, Y., & Mashimo, T. (2022). CRISPR-Cas3-based diagnostics for SARS-CoV-2 and influenza virus.iScience 25, 103830, 1-13. https://doi.org/10.1016/j.isci.2022.103830
Milenia Biotec GmbH. (n.d.). CRISPR/Cas-based Detection Methods and HybriDetect: Universal Test Strips - Individual Readout. https://www.milenia-biotec.com/uploads/2019/07/improved-CRISPR-readout_final-1.pdf
The system construction of POIROT can be broadly divided into four parts: biomarker, amplification, detection, and visualization (Lateral Flow Assay, LFA). In particular, since there are various methods for amplification, we conducted many experiments.
To our knowledge, there have been no previous examples of connecting TWJ-SDA with multistep-SDA or multistep-SDA with Cas3. Therefore, we can confidently say that we have independently developed a detection system that has both high selectivity and sensitivity.
Through repeated experiments, we have independently developed a detection system that has both high selectivity and sensitivity. However, further experiments, as outlined below, are necessary to complete POIROT.
To complete POIROT, which enables the amplification and quantification of miRNAs with any sequence, we will continue our experiments.