- Methodology article
- Open Access
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# Simultaneous fitting of real-time PCR data with efficiency of amplification modeled as Gaussian function of target fluorescence

*BMC Bioinformatics*
**volume 9**, Article number: 95 (2008)

## Abstract

### Background

In real-time PCR, it is necessary to consider the efficiency of amplification (EA) of amplicons in order to determine initial target levels properly. EAs can be deduced from standard curves, but these involve extra effort and cost and may yield invalid EAs. Alternatively, EA can be extracted from individual fluorescence curves. Unfortunately, this is not reliable enough.

### Results

Here we introduce simultaneous non-linear fitting to determine – without standard curves – an optimal common EA for all samples of a group. In order to adjust EA as a function of target fluorescence, and still to describe fluorescence as a function of cycle number, we use an iterative algorithm that increases fluorescence cycle by cycle and thus simulates the PCR process. A Gauss peak function is used to model the decrease of EA with increasing amplicon accumulation. Our approach was validated experimentally with hydrolysis probe or SYBR green detection with dilution series of 5 different targets. It performed distinctly better in terms of accuracy than standard curve, DART-PCR, and LinRegPCR approaches. Based on reliable EAs, it was possible to detect that for some amplicons, extraordinary fluorescence (EA > 2.00) was generated with locked nucleic acid hydrolysis probes, but not with SYBR green.

### Conclusion

In comparison to previously reported approaches that are based on the separate analysis of each curve and on modelling EA as a function of cycle number, our approach yields more accurate and precise estimates of relative initial target levels.

## Background

In real-time PCR, fluorescence is recorded at each cycle to monitor the generation of product [1]. Typically, after several cycles with no or minor changes in background fluorescence, there is a short phase with vigorous exponential increase of fluorescence, which then gradually slows down to a plateau phase. In conventional data analysis, for each fluorescence curve a crossing point (Cp) *alias* threshold cycle (Ct) is determined from the visible exponential amplification phase using either the fit point method or the second-derivative method [2]. It is clear that for proper calculation of initial target levels, differences in efficiency of amplification (EA) must be taken into account [3]. Even small EA differences amplify to large apparent differences in mRNA levels [4]. The above methods require the set-up of standard curves from which EA is deduced. The disadvantages of standard curves are (i) the extra effort and cost to set up additional samples *e.g*. by serial dilution, and (ii) non-matching EAs if inhibitors are present and serially diluted [4].

The alternative to using standard curves is to determine EA directly from the samples [5]. The initial exponential amplification can be described in terms of fluorescence (based on the assumption that accumulation of fluorescence is proportional to accumulation of amplification product) by the following equation:

F_{x} = F_{0}• (EA)^{x}

See Table 1 for definition of parameters. Note that in this report, EA has limits of 1 (= no amplification) and 2 (= ideal amplification, *i.e*. complete doubling of target with each cycle); all references to papers where EA runs between 0 and 1 have been transformed by adding 1. Ideally, one would like to determine the individual EA of each sample to determine accurate F_{0} values; F_{0} is directly proportional to the sample target cDNA amount. However, for each trace of fluorescence there are only very few (around 5 to 7) data points with virtually constant EA which can be used for an analysis according to equation 1. In earlier cycles, there is only background fluorescence (*i.e*. amplification product can not be detected for many cycles), and in later cycles the EA declines due to product accumulation [6]. Thus, very few qualified data points combined with considerable measurement error makes direct exponential extrapolation inaccurate. One strategy to improve parameter estimation is to include later points of the fluorescence curve and to adjust EA as a function of cycle number [7–9]. However, we have observed that these approaches can not properly model target fluorescence in detail.

Very recently, Alvarez *et al*. have introduced into real-time PCR data analysis the useful notion to model the decrease of EA not as a function of cycle number, but as a function of fluorescence, the indicator of product accumulation [10]. This insightful concept is more difficult to apply to data analysis though, since it does not allow direct fitting of flourescence as a simple function of cycle number. Alvarez *et al*. calculate, as F_{i+1}/F_{i} ratio, amplification efficiencies for each cycle, then fit 2 parameters of a sigmoidal function to these EA values as a function of fluorescence, and finally estimate, with both parameters fixed, F_{0} by iterative discrete fitting. The downsides of this approach are large errors in the F_{i+1}/F_{i} ratios, non-linear regression with fluorescence as the independent variable (which violates the idea of x having a small or no error), fluorescence data (y axis: F_{i+1}/F_{i} ratio; x axis: F_{i}) on both axes, and fitting twice to the same set of information. Further limitations are indicated in the Discussion.

Based on the innovative concept of modelling EA as a function of amplicon fluorescence, it was our aim here to overcome the defects of the approach of Alvarez *et al*.. As the key improvement, we find that iterative simulation of the PCR process with EA modelled as a Gaussian peak function of amplicon fluorescence yields precise and correct initial EA values, both with hydrolysis probe and SYBR green detection. Our approach includes, for the first time, simultaneous non-linear fitting to determine EA as a common parameter for all samples of a group. Compared to established methods of real-time PCR data analysis, our approach results in more accurate estimates of relative cDNA levels.

## Results

### Modelling EA as a function of target fluorescence

Initially, we tried to fit equation 1 to a limited number (< 6) of data points from the very early visible exponential phase, *i.e*. the first points above background fluorescence. In this phase the EA should still be, as a good approximation, constant and equal to the initial EA. However, this approach was relatively unreliable, even with simultaneous fitting of multiple curves, since there is considerable (random) experimental error (*cf*. background fluorescence differences in Fig. 1B) with every fluorescence reading, yet the last point with the highest fluorescence is always fitted best, even when various weighing options were applied. It is thus necessary to include data points from later cycles in order to mitigate random fluorescence errors. We tested previously reported sigmoid [7, 8], logistic [9], and other (*e.g*. asymmetric sigmoid or reverse asymmetric sigmoid) transition functions in order to model target fluorescence as a function of cycle number. All of these, however, showed systematic deviations between calculated and observed fluorescence particularly in the early exponential phase (not shown).

With the aim of modelling EA as a function of fluorescence [10], we inspected several of our own experimental data sets, plotted as F_{i}/F_{i-1} versus F_{i} (see Fig. 2). This made us consider a Gauss peak function (y = a * exp [-0.5 * {(x - b)/c}^{2}]) and a logistic peak function (y = 4 * a * d/(1 + d)^{2} with d = exp [-(x - b)/c]) for modelling. Since we expected EA (= F_{i}/F_{i-1}) to be maximal at F_{i} = 0, both functions were simplified by setting b to zero. With the Gauss function, it follows that EA = 1 + (EA_{0} - 1)/exp [F_{i}^{2}/k] with k = 2 * c^{2}. With the logistic function, the analogous equation is EA = 1 + 4 * (EA_{0} - 1) * exp [-F_{i}/k]/(1 + exp [-F_{i}/k])^{2} with k = c. Both functions adequately describe F_{i}/F_{i-1} as a function of F_{i} (Fig. 2). As an important difference, the logistic function always yields higher EA_{0} values than the Gauss function (see below). However, it is not possible to determine which function is more appropriate from this plot, since the critical region of low F_{i} is unaccessible, because of very large errors.

In order to describe experimental fluorescence as a function of cycle number, we use an iterative approach that yields all 3 parameters by a single non-linear fitting procedure. Depending on F_{0}, the virtual initial target fluorescence, EA_{0}, the initial efficiency of amplification, and k, the fluorescence is increased cycle by cycle – with EA adjusted as a function of target fluorescence – up to cycle x. Note that *e.g*. function EA = 1 + (EA_{0} - 1)/exp [F_{i}^{2}/k] is valid for the plot of F_{i}/F_{i-1} versus F_{i}. However, in the PCR simulation, it is necessary to calculate – in the other direction – F_{i+1} from F_{i}; since EA is not a linear function of F_{i}, the available ratio F_{i}/F_{i-1} can not be used. Thus, combining EA = F_{i+1}/F_{i} and EA = 1 + (EA_{0} - 1)/exp [F_{i+1}^{2}/k] gives F_{i} * (EA_{0} - 1)/exp [F_{i+1}^{2}/k] + F_{i} - F_{i+1} = 0. We use the algorithm of Newton [11] to solve this equation by iteration. Note that Alvarez *et al*. have used a F_{i+1}/F_{i} plot to avoid the need to calculate F_{i+1} from F_{i} by Newton iteration.

### Selection of data points

Like previously reported approaches, neither Gauss nor logistic function can reliably model the plateau phase of the PCR fluorescence curve (Fig. 2). We therefore exclude all data points beyond the minimum of the second derivative (approximated by a 5 point peak; see Fig. 1 and Methods for details) from analysis. Also with the fluorescence difference (dF) data, we define the background interval that is modeled by a straight line (Fig. 1B).

### Simultaneous fitting

The EA_{0} values that result from fitting to individual fluorescence curves are still uncertain to an extent that precludes direct use (see below). We thus use simultaneous fitting in the final stage of data analysis to determine an optimal common EA_{0}. For this, all associated curves (up to n = 16), with the same points selected as previously for individual fitting, are first pooled into a group by transformation of the cycle numbers (see Methods). Note that the protein of interest and the standard used for normalization, *e.g*. beta-actin, constitute separate groups, since different primers (and probes) are used. Samples with markedly different individual EA_{0}s should be gathered into separate groups. With the iterative algorithm described above, a single common EA_{0} is fitted to all curves of a group; at the same time, individual F_{0} and k parameters are fitted for each curve. Based on the shared EA_{0}, the final F_{0} values, which are proportional to initial target amount, can be directly used to calculate relative expression levels; for this, normalized ratios, calculated from F_{0} values of the protein of interest and of the corresponding standard protein, are compared.

### Validation

Locked nucleic acid (LNA) hydrolysis probe and SYBR green assays with 5 different targets as shown in Table 2 were performed to resolve whether to use the Gauss function or the logistic function and to validate our approach. For each target, 3 identical dilution series of 5 samples each were processed in parallel; all 15 samples were analyzed as a group. Note that these assays are to some extent imperfect, since they were pipetted and operated by 4 different persons with ordinary skills. In these comparisons, goodness of fit, indicated by chi squared, was not always better with the Gauss function; nevertheless, on average goodness of fit was better *i.e*. chi squared was smaller by a factor of 1.23 (geometric mean; data not shown). Decisively, the Gauss function performed better than the logistic function according to 2 criteria: i) the sum of accuracy errors (error = absolute value of accuracy factor – 1; see Table 2) is smaller, *i.e*. 0.26 (Gauss) vs. 0.44 (logistic). ii) With SYBR green detection of the human GAPDH amplicon, the logistic function yielded a concerted EA_{0} of 2.05; this is significantly higher – the standard deviation from fitting of the concerted EA_{0}s was ≤ 0.01 for all 5 targets (data not shown) – than the theoretical upper limit of 2; by contrast, the Gauss function produced an EA of 1.99. Thus, the Gauss function was used for all analyses below.

Results of Table 2 indicate good precision (median of relative errors: 5%) and accuracy. In order to compare our approach with the standard curve approach [3], each dilution series was analyzed as a separate subgroup as shown in Table 3. With our approach, precision was better by a factor of 1.5 (median of relative errors: 8% vs. 12%); more importantly, accuracy was better by a factor of 2.1 (median of relative errors: 13% vs. 27.5%). Note that our method yields EA_{0}s both higher and lower than the corresponding EAs of the standard curve approach. We suppose that this is caused by the LightCycler software for Cp estimation, which can not properly correct a drifting baseline, since the best available baseline adjustment ("arithmetic") simply subtracts a constant offset from all data points. Table 4 shows results from analysis of our data sets with 2 of the tools that are available for data analysis without standard curves. Estimates from LinRegPCR analysis [4] were much less precise (38.5%) and accurate (58.5%). In comparison to the DART-PCR approach [12], which uses the average of individual EAs to calculate F_{0} values, precision was virtually identical (8% vs. 7%); however, accuracy was in favour of our approach by a factor of 1.5 (13% vs. 19.5%). Table 5 suggests that our approach is better than DART-PCR because individual EAs are determined more precisely; SEMs on average (geometric mean) were smaller by a factor of 2.0.

Surprisingly, with some hydrolysis probe assays we obtained EA_{0}s definitely higher than 2.00; concurrently, the measured dilution factors of corresponding dilution series were strikingly wrong. With the same primers, but SYBR green instead of hydrolysis probe detection, EA_{0}s ≤ 2.00 were determined, and measured matched intended dilution factors. Thus, with LNA hydrolysis probes (Roche Universal Probe Library), efficiency of fluorescence generation can be higher than efficiency of amplification. Extra fluorescence is not caused by the probe alone, since for one amplicon probe #89 gave a higher EA_{0} than the SYBR green assay (2.11 *vs*. 1.86; ≥ 3 samples per group), but for another amplicon detection with same probe matched SYBR green (1.84 *vs*. 1.84). Based on sequence analysis and dedicated experiments we have devised a hypothesis, depicted in Figure 3, to explain additional exponential probe hydrolysis. We suppose that, given matching partial binding sites as indicated, the tightly-binding LNA probe may guide the polymerase to switch to a second antisense strand during synthesis of sense strand. This low-efficiency template-switching [13, 14] generates an extended amplicon with two perfect probe binding sites instead of one. The extended amplicon can be extended further by the same mechanism. In support of the model, when CCCA (antisense strand, close to the 5' end; read from right to left) was replaced by GGTG, EA_{0} dropped from 2.27 to 2.08 (3 samples per group). Residual fluorescence growth may be caused analogously by the sequence TGAG (marked by half dashes in the figure) in reverse strand synthesis.

## Discussion

In real-time PCR, without a doubt, it would be optimal to determine an individual EA for each sample. However, it does not seem possible with present experimental technology to determine individual EAs according to equation 1 reliably: very few qualified data points (*i.e*. only the first 5–7 points that rise above background fluorescence with virtually constant EA) combined with considerable measurement error makes direct exponential extrapolation inaccurate. One strategy to improve parameter estimation is to include later points of the fluorescence curve. However, we find that sigmoid [7, 8], logistic [9], or other functions can not properly model target fluorescence in detail. Very recently, Alvarez *et al*. have introduced a fundamentally different approach [10]. It appreciates that the decrease of EA is caused by product accumulation [6, 15]. This concept allows to embrace even more points for analysis (*i.e*. up to the minimum of the second derivative of fluorescence) than other methods, which use the maximum of the second derivative as an upper limit [9] or the center of selection [12]. Unfortunately, the particular algorithm of Alvarez *et al*., which is based on a sigmoidal function, suffers from a number of disadvantages (see Introduction and below). In the present report we use iterative non-linear fitting with a Gauss function to describe EA as a function of fluorescence. Both approaches use the same number of parameters for fitting, *i.e*. 2 parameters plus the actual result, F_{0}. However, our approach has the following advantages over the approach of Alvarez *et al*.: i) Parameters EA_{0}, F_{0}, and k are fitted directly to the fluorescence *vs*. cycle number data without any data transformation except for inevitable subtraction of background; this avoids additional errors (as in the F_{i+1}/F_{i} ratios) and preserves error composition. ii) All final parameters are estimated in a single round of fitting. Alvarez *et al*. have rejected direct iterative fitting of F_{0} alongside with their 2 model parameters because of large uncertainty in the estimation of F_{0}. Instead, they use an unfavourable algorithm that involves data transformation and fitting twice to the same data set. By contrast, data from Tables 2 and 3 suggests that our Gauss function model allows accurate fitting of the same number of parameters concurrently. iii) EA_{0} can freely surpass 2; this was very instrumental to uncover overestimation of DNA amplification with certain LNA hydrolysis probe assays. By contrast, with the sigmoid function of Alvarez *et al*., EA_{0} is forced to values < 2; to recognize this flaw of formula design, insert a very large T_{m}/b ratio in equation 3 of the cited work. iv) Our model is compatible with simultaneous fitting to determine a common EA. Note that simultaneous fitting of EA_{0} is not directly possible with the function of Alvarez *et al*., since there EA_{0} is not a single parameter, but a function of 2 parameters.

In an extensive comparison, the approach of Alvarez *et al*. displayed the lowest quantification error of all methods of individual curve analysis (Fig. 3B and Table 2 in the cited work); similar results were only obtained with EAs estimated from standard curves based on dilution series [3]. We have not applied the approach of Alvarez *et al*. to our data, since, as explained above, the approach is based in parts on unfavorable design. However, our comparison with the widely-used standard curve approach suggests that our approach gives markedly better results (Table 3). Also, we find that our approach is much better in terms of precision and accuracy than the LinRegPCR approach (Table 4). With the DART-PCR approach, which uses the average of individual EAs to calculate F_{0} values, precision was virtually identical; however, accuracy was distinctly better with our approach. We suppose that this is caused predominantly by much more (factor 2.0) precise individual EAs (Table 5). Moreover, with DART-PCR, the mean EAs of 2 amplicons were markedly smaller than the corresponding EA_{0}s from our approach; the other 3 were not significantly larger. This is not surprising, since DART-PCR assumes a constant EA which is determined around the second derivative maximum and thereby may underestimate the initial EA.

In spite of these improvements, the F_{0} values that result from fitting to individual fluorescence curves are still uncertain to an extent that precludes direct use (see Table 5, column EA_{0} individual). The individual EAs are useful to identify erratic samples and to judge the quality of primers and probes, but, as was observed previously, they introduce additional error and thus increase data variance [12]. Indeed, in the afore-mentioned comparison of available individual curve analysis methods, accuracy and precision in quantification of experimental dilution series was poor [10]; similarly, with our data sets, the LinRegPCR software yielded the least accurate results (Table 4). Given that determination of F_{0} values from individual EAs is futile because of experimental limitations, then the next best thing is to analyze related samples as a group with a concerted EA. Towards this end, Peirson *et al*. have simply calculated the arithmetic mean of individual EAs [12]. In the present report we introduce simultaneous non-linear regression to determine an optimal EA for all samples of a group. Note that with our large data sets, EA_{0} determined by simultaneous fitting was not dramatically different from the arithmetic mean (compare Arithmetic mean values, Table 5, with EA_{0} group values, Table 2). However, with few samples per group, for example with 6 GAPDH amplicon samples (individual EA_{0}s LNA probe: 2.17, 2.25, 2.25; SYBR green: 1.89, 1.96, 1.96), simultaneous fitting (EA_{0} group = 2.01) and arithmetic mean (2.08) may yield markedly disparate results. We suggest that simultaneous fitting provides the best possible EA_{0} that optimally unifies all related fluorescence curves; simultaneous fitting thus contributes to the better performance of our approach. Empirically, for a reliable EA_{0} we would recommend to employ at least 3 samples per group.

Making good use of accurate EA_{0}s, our study has revealed that fluorescence generation with some LNA hydrolysis probe assays may overestimate DNA amplification and hence cause incorrect results. To explain this, we assume low-efficiency polymerase template switching that leads to progressive amplicon elongation including additional probe binding sites (Fig. 3). It would thus seem advisable to verify each new LNA hydrolysis probe amplicon with SYBR green detection to avoid spurious fluorescence generation.

## Conclusion

In the present report we introduce a new approach to analyze real-time PCR fluorescence curves without standard curves. Our strategy is based on the useful concept of Alvarez *et al*. to model EA as a function of amplicon fluorescence. As the key improvement, we find that a Gaussian model overcomes the defects of the original sigmoidal model. Iterative simulation of the PCR process up to the minimum of the second derivative of fluorescence yields precise and meaningful initial amplification efficiency values. In the final stage of analysis, a common EA_{0} is fitted simultaneously to all curves of a group of related samples. In comparison to previously reported approaches that are based on the separate analysis of each curve and on modelling EA as a function of cycle number, our approach yields more accurate and precise estimates of relative initial target levels.

## Methods

### Isolation of total RNA and reverse transcription

Total RNA was isolated by the method of Chomczynski and Sacchi [16] from frozen (-80°C) tissues. Reverse transcription was performed as detailed previously [17] with the following modifications: i) RQ1-DNase (Promega, Mannheim, Germany) was used at 1 U/μg total RNA; ii) Random nonamers were used for priming; iii) cDNA synthesis was performed at 42°C.

### PCR

A LightCycler 1.0 apparatus with system 2.0 software (Roche, Mannheim, Germany) was used for real-time PCR. Product accumulation was detected with SYBR green I or with locked nucleic acid hydrolysis probes (TaqMan principle [18]) from the Universal ProbeLibrary (Roche). Primers and probes (see Table 6 for sequences) were selected online with the ProbeFinder (Roche) version 2.35 [19]. A single reaction (total volume 10 μl) contained 1 μl master mix (5 × concentration; LightCycler TaqMan Master; Roche 04735536001), 1 μmol/l each of forward and reverse primer, SYBR Green I at 1 : 30.000 dilution (Invitrogen S7563) or 50 nmol/l probe, and various amounts of cDNA or plasmid DNA. Contamination controls contained water instead of DNA. After enzyme activation (10 min, 95°C), thermocycling consisted of 45 cycles of 10 s at 95°C, 30 s at 55°C, and 1 s at 72°C; velocity of temperature change was 1.1°C/s.

### Analysis of real-time PCR data

Data were analyzed with pro Fit 6.0.6 Software (Quantum Soft, Switzerland) running on a Mac OS X system (Apple, California, U.S.A). Fitting was achieved by non-linear regression with self-written program (SimFitEAv) and function (EAv, EAvPeak, M16EAv) plug-ins. Complete listings (text files) are available online [see Additional file 1] [see Additional file 2] [see Additional file 3] [see Additional file 4]. Functions calculate a single y value from the input; input consists of a single x value and multiple model parameters. Program SimFitEAv analyzes 1 to 16 fluorescence curves simultaneously; it works as follows:

#### Selection of points

First, each fluorescence curve is analyzed separately. The change of fluorescence (dF) as a function of cycle number is used to define an upper limit of useful points and to select points for linear background definition. With the dF data (calculated as fluorescence at cycle i minus fluorescence at cycle i-1), a 5 point peak is identified as the highest sum of dF values of a 5 point sliding window (Fig. 1A). The background fluorescence is modeled individually for each curve by a straight line; this line is defined by a 9 point interval as explained in the legend to Figure 1B. Slope and offset of the background line are determined by linear regression of the corresponding raw fluorescence data. Points preceding the 9 point interval and following the 5 point peak are excluded from further analysis (Fig. 1C). The parameters of a peak function (EAvPeak) are fitted to all remaining points to estimate starting parameters for function EAv. The EAvPeak function basically works like the EAv function described below, but it yields the fluorescence difference between the last and the second-to-last cylce as y output. Note that the number of points used for definition of peak and background were chosen empirically; higher numbers might work as well.

#### Fitting to a single fluorescence curve with variable efficiency of amplification

For all remaining points, linear fluorescence background is subtracted from raw fluorescence. Then, the parameters of function EAv are determined by non-linear regression. In essence, our Gauss model is based on the following equation (exp indicates e raised to the power of its argument in square brackets):

F_{i} = F_{i-1}• (1 + (EA_{0} - 1)/exp [F_{i-1}^{2}/k])

See Table 7 for definition of parameters. Note, however, that F_{i+1} is calculated from F_{i} by means of Newton iteration [11]. For details, see the function listings provided online as additional files (see above). Amplification is repeated until the cycle number reaches the x input; the final fluorescence is yielded as y output. In other words, each call of function EAv simulates a PCR reaction up to cycle x, starting with F_{i} = F_{0} at cycle 1. Apart from linear background, which is added for visual display of final results, this generates a step-wise increase in fluorescence. Individual fitted EA_{0} values are displayed to the user for comparison.

#### Simultaneous fitting

In the final stage, a simultaneous fit is made with all curves of a group, with the same points selected as previously for function EAv. Function M16EAv uses a single global EA_{0} parameter for all fluorescence curves; for each curve, parameters F_{0} and k are fitted individually. The same algorithm as in function EAv is used; however, data sets are first joined by transformation of the cycle numbers: curve 1 uses cycle numbers 1 to 50, curve 2 uses 51 to 100 and so forth. Function M16EAv recognizes the input cycle number x and picks the F_{0} and k parameters accordingly. Individual F_{0} values and the common EA_{0} are displayed to the user as the final result.

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## Acknowledgements

We thank Beatrix Steinrücken for skillful technical assistance. This work was funded by Deutsche Forschungsgemeinschaft (GR 1681/2-1 to D. G.) and Koeln Fortune Program, Faculty of Medicine, University of Cologne (21/2006 to D. G.).

## Author information

### Authors and Affiliations

### Corresponding author

## Additional information

### Authors' contributions

AB, AN, CF, AU, DL, TL, and JP performed experiments. AL and ES helped to draft the manuscript. DG developed the software, designed experiments, analyzed data, and drafted the manuscript. All authors read and approved the final manuscript.

## Electronic supplementary material

### 12859_2007_2080_MOESM1_ESM.txt

Additional file 1: Program SimFitEAv. The main program for PCR data analysis to be used as pro Fit (Quantum Soft, Switzerland) plug-in. (TXT 14 KB)

### 12859_2007_2080_MOESM2_ESM.txt

Additional file 2: Function EAv. Function called from SimFitEAv to be used as pro Fit (Quantum Soft, Switzerland) plug-in. (TXT 747 bytes)

### 12859_2007_2080_MOESM3_ESM.txt

Additional file 3: Function EAvPeak. Function called from SimFitEAv to be used as pro Fit (Quantum Soft, Switzerland) plug-in. (TXT 577 bytes)

### 12859_2007_2080_MOESM4_ESM.txt

Additional file 4: Function M16EAv. Function called from SimFitEAv to be used as pro Fit (Quantum Soft, Switzerland) plug-in. (TXT 2 KB)

### 12859_2007_2080_MOESM5_ESM.xls

Additional file 5: Original raw data. Excel file with raw fluorescence and cycle data exported from LightCycler. (XLS 126 KB)

## Authors’ original submitted files for images

Below are the links to the authors’ original submitted files for images.

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### Cite this article

Batsch, A., Noetel, A., Fork, C. *et al.* Simultaneous fitting of real-time PCR data with efficiency of amplification modeled as Gaussian function of target fluorescence.
*BMC Bioinformatics* **9**, 95 (2008). https://doi.org/10.1186/1471-2105-9-95

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DOI: https://doi.org/10.1186/1471-2105-9-95

### Keywords

- Cycle Number
- Lock Nucleic Acid
- Hydrolysis Probe
- Fluorescence Curve
- SYBR Green Detection