Loop-mediated isothermal amplification (LAMP) has been widely used in nucleic acid assay because of its high specificity, sensitivity, and isothermal property. However, the complexity of amplification product detection is still a major challenge for its wide applications. Herein, we developed a light scattering technology-assisted, low-cost, and simple detection manner of LAMP products without expensive reagents and complicated instruments. Only needing to add a kind of strong acid to the amplification products, the amplification products can aggregate into large particles in a strongly acidic medium, and large particles can produce strong light scattering, which shows a good proportional relationship with the number of amplification products in a wide range. The proposed method shows excellent sensitivity and high specificity that can quantify RNA as low as 100 aM with a single-base resolution.
Loop-mediated isothermal amplification (LAMP) has been widely used in nucleic acid assay because of its high specificity, sensitivity, and isothermal property. However, the complexity of amplification product detection is still a major challenge for its wide applications. Herein, we developed a light scattering technology-assisted, low-cost, and simple detection manner of LAMP products without expensive reagents and complicated instruments. Only needing to add a kind of strong acid to the amplification products, the amplification products can aggregate into large particles in a strongly acidic medium, and large particles can produce strong light scattering, which shows a good proportional relationship with the number of amplification products in a wide range. The proposed method shows excellent sensitivity and high specificity that can quantify RNA as low as 100 aM with a single-base resolution.
RNAs including microRNAs
(miRNAs) and messenger RNAs (mRNAs) have
always been very important research topics due to their vital roles
in the fundamental process of life.[1,2] As RNA is considered
a hallmark for identifying pathogens,[3] and
its expression profile is relevant to the pathogenesis of the disease,[4] RNA analysis has become an important content
of current biological research. Thus, a simple and sensitive RNA detection
method is particularly important because of its great value in disease
pathophysiology[5] and medical diagnostics.[6]Up to now, many ways for RNA analysis have
been established from
simple to complex and multistep procedures. Among these ways, reverse
transcription-polymerase chain reaction (RT-PCR) is the most popular
amplification technology with a wide dynamic range.[7] However, several main limitations of RT-PCR are its thermal
cycle process, requirement of reverse transcription, and false-positive
signal.[8] Furthermore, since miRNA is quite
short, it is difficult to be amplified by the direct use of PCR, which
makes the PCR construction very complex.[9] As promising alternatives to PCR, isothermal amplification methods
of miRNA,[10] such as digital miRNA detection,[11] loop-mediated isothermal amplification (LAMP),[12−14] rolling circle amplification (RCA),[15,16] exponential
amplification reaction (EXPAR),[17,18] nucleic acid sequence-based
amplification (NASBA),[19] duplex-specific
nuclease signal amplification (DSNSA),[20] catalyzed hairpin assembly (CHA),[21] and
hybridization chain reaction (HCR),[22] are
effective amplification methods under isothermal conditions. Gines
et al. reported an isothermal digital detection method by designing
DNA circuits that inhibits nonspecific amplification common in nucleic
acid amplification methods and provides absolute quantification of
miRNAs.[11] CHA and HCR are enzyme-free methods
that rely on competitive hybridization, which can be used to probe
endogenous miRNAs in living cells.[22] LAMP,
RCA, NASBA, EXPAR, and DSNSA are well-known enzyme-based amplification
strategies that can be used for quantitative analysis of miRNAs through
their exponential or linear amplification mechanism. Among the numerous
enzyme-based isothermal methods, LAMP possesses impressive sensitivity.
Generally, LAMP can amplify a few copies of nucleic acids to detectable
capability at a constant temperature. Therefore, LAMP technology has
been transformed into a popular method for the quantitative assay
of biomarkers[23,24] and pathogen-caused infectious
diseases, such as COVID-19.[25−27] Classic LAMP uses four primers
to target six areas on the target sequence (more than 130 bp), which
results in the requirement of long target sequences and carefully
designed primers.[28] Du et al. used ligation-dependent
LAMP to amplify miRNA target sequences, in which one pair of stem-loop
probes can be specifically linked together to generate double stem-loop
structure DNA to start up LAMP.[12] The strategy
of initiating LAMP based on double stem-loop DNA greatly simplifies
the design of the primer for LAMP.[29] Although
LAMP is quite robust, the detection manner of amplification products
is still a challenge.LAMP reaction is a highly efficient nucleic
acid amplification
reaction, which can produce a mass of stem-loop structure DNAs with
a variety of stem lengths.[28] So far, many
ways have been used for the analysis of amplification products including
gel electrophoresis,[30,31] naked eye monitoring,[32,33] real-time fluorescence,[34] electrochemical
methods,[35] and so on. Magnesium pyrophosphate
can be produced as a by-product during nucleic acid amplification
by DNA polymerase. Based on this characteristic, Notomi and co-workers
put calcein in the reaction solution of LAMP[33] and the amplification reaction can be detected by the naked eye
through the color change of calcein-manganese (orange) turning into
calcein-magnesium (green fluorescence signal) as the reaction proceeds.
But this assay found that calcein would reduce the sensitivity of
LAMP compared with reaction results without adding additional reagents.
This is mainly due to the finding that calcein combined with magnesium
can reduce the activity of the enzyme[36] and the interaction between calcein and double-stranded DNA leads
to reduced sensitivity.[37] For example,
by adding SYBR Green I in an amplification reaction,[34] a kind of embedded fluorescent dye, the fluorescence signal
can be collected and the process of LAMP reaction can be detected
in real time. However, this method requires a precise real-time fluorescence
detection system. Recently, a CRISPR/Cas12a-assisted LAMP product
detection method was reported.[38] This method
can improve the specificity of amplification product detection, but
it needs to use a fluorescence probe and CRISPR/Cas12a protease to
generate fluorescence signals, which greatly increases the detection
cost. Therefore, simple and low-cost detection manners are desirable
for popularizing the application of LAMP.In this work, we establish
research on light scattering technology-combined
ligation-dependent LAMP (LL-LAMP) for RNA detection to develop a convenient
and low-cost detection method for the analysis of nucleic acid amplification
products without sophisticated instruments. We just need to add perchloric
acid into the amplification products, and the DNA double-helix structure
of products denatures into single-stranded nucleic acids since hydrogen
bonding between the bases is destroyed in a strongly acidic medium.
Then, single-stranded nucleic acids aggregate into large particles
with a hydrated radius of 200–700 nm.[39] The large particles produce a very strong signal of light scattering,
which shows a good proportional relationship with the number of amplification
products in a wide range.
Experimental Section
Materials and Reagents
SYBR Green I (20 ng/μL)
was supported by Fanbo Biochemicals Co., Ltd. (Beijing, China). T4
RNA ligase 2 and Bst DNA polymerase were obtained from New England
Biolabs (NEB, China). Deoxy-ribonucleotide triphosphate dNTPs, Recombinant
RNase Inhibitor (RRI), and RNase-free water were obtained from Takara
Biotechnology Co., Ltd. (Dalian, China). MCF-7 cells were obtained
from the cell bank of the Chinese Academy of Sciences (Shanghai, China).
TRIzol reagent was purchased from Invitrogen (USA). Stock solutions
for RNA analysis were respectively prepared in RNase-free water. All
oligonucleotides used in this research were obtained from TaKaRa Biotechnology
Co., Ltd. (Dalian, China), and they are listed in Table S2.
Extraction of Total RNA
MCF-7 cells
were kept in 7
mL of DMEM medium (Gibco) containing 100 μg/mL streptomycin,
3 mmol/L l-glutamine, 10% (v/v) fetal calf serum, and 100
U/mL penicillin. The experimental process of extracting total RNA
from MCF-7 cells was based on the protocol of the TRIzol reagent.
The concentration of total RNA was detected using a NanoDrop One (Thermo
Scientific, USA) and then stocked at −80 °C.
Experimental
Process of LL-LAMP-Based RNA Assay
For
the ligation reaction, 1 μL of total RNA sample or 1 μL
of target RNA (microRNA or mRNA) was added to 5.0 μL of the
reaction solution including 2.3 μL of RNase-free water, 1 μL
of 200 nM P1let-7a (or P1mRNA), 1 μL
of 200 nM P2let-7a (or P2mRNA), 0.1 μL
of 40 U/μL RRI, and 0.6 μL of 10× T4 RNA ligase 2
buffer (10 mM DTT, 500 mM Tris–HCl, 4 mM ATP, and 20 mM MgCl2). The reaction solution was put at 65 °C for 2 min and
then at 39 °C for 5 min to accomplish the hybridization reaction
of target RNA and probes. Then, 3.5 μL of RNase-free water,
0.4 μL of 10× ligase 2 buffer, and 0.1 μL of ligase
were put in the reaction solution, and the solution was heated at
37 °C for 30 min for ligation reaction.For the amplification
reaction, a volume of 2 μL reaction product mentioned above
was put into 8 μL of LAMP mixture including 4.3 μL of
RNase-free water, 1.0 μL of 10× ThermalPol buffer (20 mM
MgSO4, 200 mM Tris–HCl, 100 mM KCl, 100 mM (NH4)2SO4, and 1% Triton X-100), 0.5 μL
of 8 U/μL Bst polymerase, 0.2 μL of SYBR Green I, 0.5
μL of 10 μmol/L FIP, 1.0 μL of 2.5 mmol/L dNTPs,
and 0.5 μL of 10 μmol/L BIP with a final system of 10
μL. The reaction mixture was immediately put into a 2720 PCR
system (Applied Biosystems, USA) to carry out the LAMP process at
65 °C. LAMP amplification times were 35 min (the concentration
of RNA ranges from 100 aM to 100 fM) and 15 min (the concentration
of miRNA ranges from 1 pM to 1 nM).Ten microliters of HClO4 (1 M) and 80 μL of water
were added to the above 10 μL of amplified products. One hundred
microliters of the mixture was mixed and added to the cuvette. An
LS55 fluorescence spectrophotometer was used to scan the scattering
spectrum.
Results and Discussion
The Working Principle of
LL-LAMP for RNA Assay
The
method described here applies to any known RNA. Figure gives an illustrated example for the microRNA
(let-7a) assay. According to the sequence of let-7a (arrow represents
the 3′-terminus), we design two stem-loop probes including
P1let-7a and P2let-7a. P1let-7a is composed of the complementary region with
a half sequence of let-7a and the stem-loop structure region from
the 5′-terminus direction to the 3′-terminus direction.
P2let-7a is composed of the stem-loop structure
region and complementary region with a half sequence of let-7a from
the 5′-terminus direction to the 3′-terminus direction.
P2let-7a is modified with two ribonucleotides at
the 3′-end, which effectively improves the connection efficiency.[40] In the presence of let-7a, P1let-7a and P2let-7a respectively hybridize adjacently
with let-7a and are ligated together by the catalysis activity of
ligase to form a special DNA molecule with a double stem-loop structure.
The special DNA with a double stem-loop structure is a starting template
for the subsequent cycle DNA amplification process, which is exactly
a similar process to loop-mediated isothermal amplification (LAMP).[20] Once the starting template is formed, it can
initiate a cycle DNA amplification reaction in the presence of FIP
(forward inner primer) and BIP (backward inner primer) under isothermal
conditions.[29] Cycle DNA amplification reaction
is catalyzed by Bst polymerase with chain replacement activity. First,
double stem-loop DNA will initiate an extension reaction along with
itself as a template to form single stem-loop DNA consisting of a
stem and a loop (structure 1). F2 of FIP hybridizes with a loop of
structure 1 to continue the extension reaction while displacing the
lower strand to form structure 2. Structure 2 continues the extension
reaction to form structure 3 and structure 4. Briefly, DNA strand
displacement occurs in two processes: self-primed extension reaction
and FIP (or BIP)-mediated extension reaction. DNAs released by the
strand displacement process can self-hybridize to continue the self-primed
extension reaction, and then FIP (or BIP) will go on hybridizing with
a loop to start the extension reaction. Finally, such a cycle DNA
amplification reaction can produce a large number of stem-loop DNAs
with different inverted repeats and cauliflower-like structures with
multiple loops. When perchloric acid is added to the LAMP amplification
products, the DNA double-helix structure is first denatured into single
strands and then polymerized into large particles with a radius of
200 to 700 nm,[39] which generates strong
light scattering. Moreover, the intensity of scattered light depends
on the original target RNA dosage, which can realize the highly specific
and sensitive analysis of RNA.
Figure 1
Principle of light scattering technology-combined
ligation-dependent
loop-mediated isothermal amplification for miRNA assay.
Principle of light scattering technology-combined
ligation-dependent
loop-mediated isothermal amplification for miRNA assay.
The Performance of LL-LAMP for RNA Analysis
The influence
of various conditions, including types of acids, the concentration
of HClO4, and the stability of the light scattering signal,
on the performance of LL-LAMP has been optimized (Figures S1–S3). By testing a series of different amounts
of let-7a miRNA as target RNA, the analysis performance of LL-LAMP
was verified under the optimum conditions. As shown in Figure A, the intensity of the light
scattering signal increases gradually with the increase in miRNA concentration
and as low as 1 zmol (100 aM) miRNA can be distinguished from the
blank (without target RNA in LL-LAMP reaction). When the light scattering
intensity at 320 nm was plotted against the negative logarithm concentration
of miRNA (−lg C/M) in the range of 100 aM
to 100 fM, the standard curve showed a good linear relationship (Figure C). The correlation
equation is I320 nm = 1114.2 + 62.8
lg C/M with a linear correlation coefficient R2 = 0.9923, suggesting that the LL-LAMP method
is sensitive enough to quantitatively detect miRNA with the detection
limit of 100 aM. Typically, the miRNA concentration range is about
100 aM to 800 fM in 1 ng of total RNA samples, that is, the dynamic
range of the proposed method is sufficient to detect the vast majority
of miRNAs in unknown actual samples.[37] In
addition, LL-LAMP can expand the testing range by shortening the amplification
time (Figures B,D).
Similarly, the intensity of light scattering at 320 nm has a linear
relationship with the negative logarithm of the concentration of target
miRNA (−lg C/M) in the range from 1 pM to
1 nM. The linear equation is I320 nm = 785.2 + 56.3 lg C/M (R2 = 0.9921), which indicates that higher concentrations of miRNA can
also be analyzed by reducing the amplification time. It is worth noting
that the timescale of LAMP amplification is different for the different
ranges of miRNA (Figure S4), which has
been discussed in detail in the Supporting Information.
Figure 2
(A, B) Light scattering spectrum of let-7a with different concentrations
by the LL-LAMP protocol. (A) From bottom to top, the concentrations
are 0 (blank, without let-7a in the LL-LAMP system), 100 aM, 1 fM,
10 fM, and 100 fM, respectively. The LL-LAMP reaction time is 35 min.
(B) From bottom to top, the concentrations are 0, 1 pM, 10 pM, 100
pM, and 1 nM, respectively. The LL-LAMP reaction time is 15 min. (C,
D) Linear relationship between the light scattering intensity (at
320 nm) and the logarithm of concentrations. Error bars are the standard
deviation of three replicates in panels (C) and (D).
(A, B) Light scattering spectrum of let-7a with different concentrations
by the LL-LAMP protocol. (A) From bottom to top, the concentrations
are 0 (blank, without let-7a in the LL-LAMP system), 100 aM, 1 fM,
10 fM, and 100 fM, respectively. The LL-LAMP reaction time is 35 min.
(B) From bottom to top, the concentrations are 0, 1 pM, 10 pM, 100
pM, and 1 nM, respectively. The LL-LAMP reaction time is 15 min. (C,
D) Linear relationship between the light scattering intensity (at
320 nm) and the logarithm of concentrations. Error bars are the standard
deviation of three replicates in panels (C) and (D).To further demonstrate the generality of the method, p53
mRNA was
chosen as another model target. According to the sequence of p53 mRNA,
P1mRNA and P2mRNA were designed respectively
by changing complementary regions of the target sequence in P1let-7a and P2let-7a. As displayed
in Figure , LL-LAMP
can sensitively quantify mRNA with the same performance of let-7a.
These results confirm the superior applicability of the proposed method
to the quantitative analysis of other RNA molecules.
Figure 3
(A, B) Light scattering
spectrum of mRNA with different concentrations
by the LL-LAMP protocol. (A) From bottom to top, the concentrations
of mRNA are 0 (blank, without mRNA in the LL-LAMP system), 100 aM,
1 fM, 10 fM, and 100 fM, respectively. The LAMP reaction time is 35
min. (B) From bottom to top, the concentrations of mRNA are 0, 1 pM,
10 pM, 100 pM, and 1 nM, respectively. The LL-LAMP reaction time is
15 min. (C, D) Linear relationship between the light scattering intensity
(at 320 nm) and the −lg of concentrations of mRNA. The linear
correlation equations are I320 nm = 944.2 + 52.4 lg C/M (R2 = 0.9958) with the concentration range from 100 aM to 100 fM and I320 nm = 756.7 + 55.1 lg C/M (R2 = 0.9828) with the concentration
range from 1 pM to 1 nM. Error bars represent the standard deviation
of three replicates in panels (C) and (D).
(A, B) Light scattering
spectrum of mRNA with different concentrations
by the LL-LAMP protocol. (A) From bottom to top, the concentrations
of mRNA are 0 (blank, without mRNA in the LL-LAMP system), 100 aM,
1 fM, 10 fM, and 100 fM, respectively. The LAMP reaction time is 35
min. (B) From bottom to top, the concentrations of mRNA are 0, 1 pM,
10 pM, 100 pM, and 1 nM, respectively. The LL-LAMP reaction time is
15 min. (C, D) Linear relationship between the light scattering intensity
(at 320 nm) and the −lg of concentrations of mRNA. The linear
correlation equations are I320 nm = 944.2 + 52.4 lg C/M (R2 = 0.9958) with the concentration range from 100 aM to 100 fM and I320 nm = 756.7 + 55.1 lg C/M (R2 = 0.9828) with the concentration
range from 1 pM to 1 nM. Error bars represent the standard deviation
of three replicates in panels (C) and (D).
The Specificity of LL-LAMP for miRNA Detection
Accurate
single-base identification of target RNAs for genetic biomarker analysis
is an important aspect, especially those miRNA sequences that are
extremely similar. To evaluate the specificity of the LL-LAMP protocol
for RNA assay, the same amount (1 fM) of let-7a family (let-7a, let-7d,
and let-7e) and a random miRNA (miR-143) were simultaneously detected
by using let-7a-specific probes (P1let-7a and P2let-7a). As shown in Figure , P1let-7a and P2let-7a can perfectly hybridize with let-7a. Let-7a can be used as a template
to effectively ligate the let-7a-specific stem-loop probes, start
the subsequent amplification reaction, and generate a clear light
scattering signal. On the contrary, the mismatched nucleotide from
the other miRNA can form the overhang with several nucleotides, which
can avoid effective ligation reactions. As displayed in Figure A, the light scattering signal
of let-7a can be distinguished from the other kinds of miRNA. It is
worth noting that let-7a, let-7d, and let-7e are different from one
to two nucleotides. One can see from Figure B that let-7e and let-7d produce 2.29 and
2.0% nonspecific signals, respectively. For miR-143, the light scattering
signal is the same as the blank, indicating that there is no interference
from miR-143. Overall, these results demonstrate that the LL-LAMP
protocol has high specificity and the ability to identify highly similar
RNAs with only single-base differences.
Figure 4
(A) Light scattering
spectrum of the LL-LAMP-based assay of different
miRNAs. (B) Relative light scattering responses (at 320 nm) of other
miRNAs compared to let-7a. The relative response of let-7a is defined
as 100% and calculates the relative responses of other miRNAs based
on the linear equation in Figure . Error bars are the standard deviation of three replicates.
(A) Light scattering
spectrum of the LL-LAMP-based assay of different
miRNAs. (B) Relative light scattering responses (at 320 nm) of other
miRNAs compared to let-7a. The relative response of let-7a is defined
as 100% and calculates the relative responses of other miRNAs based
on the linear equation in Figure . Error bars are the standard deviation of three replicates.
Quantification of miRNA in the Total RNA
Sample
Furthermore,
to investigate the practicability of the LL-LAMP system for miRNA
assay in complex biological samples, let-7a in total RNA extracted
from MCF-7 cells was detected. As shown in Figure , 50 pg of the total RNA sample produced
a well-defined light scattering curve. With the calibration curve
in Figure C, the amount
of let-7a in 50 pg of total RNA is estimated to be 1.68 zmol. Upon
adding 5 zmol of synthetic let-7a to 50 pg of the total RNA sample,
after five repeated determinations, the average let-7a content was
6.51 zmol, and the average recovery rate was 96.6%. These results
indicate that LL-LAMP is a reliable and practical method for the quantitation
of miRNA in biological samples.
Figure 5
Quantification of let-7a in 50 pg of total
RNA samples by using
LL-LAMP. (A) Light scattering spectra for the assay of let-7a in total
RNA samples. (B) Let-7a content in total RNA. Error bars indicate
the standard deviation of five replicates.
Quantification of let-7a in 50 pg of total
RNA samples by using
LL-LAMP. (A) Light scattering spectra for the assay of let-7a in total
RNA samples. (B) Let-7a content in total RNA. Error bars indicate
the standard deviation of five replicates.
Conclusions
In summary, we developed a convenient and low-cost
method (LL-LAMP)
for RNA analysis based on light scattering technology and ligation-dependent
loop-mediated isothermal amplification. In the proposed method, the
efficient mechanism of LAMP ensures the sensitivity of RNA assay.
The target RNA-templated ligation reaction of two stem-loop probes
enables LL-LAMP with single-base resolution. More importantly, the
amplification products can aggregate into large particles after adding
perchloric acid and produce strong light scattering. Thus, the target
RNA can be quantitatively detected by using light scattering technology
without expensive reagents. By using miRNA and mRNA as proof-of-concept
RNA targets, we have demonstrated that LL-LAMP is a practical and
reliable method for RNA analysis. These features highlight that the
LL-LAMP protocol has great potential in the field of nucleic acid
assay.
Authors: Kevin W Soli; Monalisa Kas; Tobias Maure; Masahiro Umezaki; Ayako Morita; Peter M Siba; Andrew R Greenhill; Paul F Horwood Journal: Diagn Microbiol Infect Dis Date: 2013-09-28 Impact factor: 2.803