The invention is in the field of analytic technology and medical diagnostics, in particular and relates to methods and systems for determining measurements from quantitative nucleic acid amplification reactions, such as PCR. In particular, it describes how to estimate delta-Cq values from measured (raw-)Cq values gained from PCR measurements and how to calculate confidence intervals for them.
Quantitative PCR measurements require normalization to a reference to yield expression values that can be compared across samples and/or patients. One possible method for this task is the so-called delta-Cq method (formerly called delta-Ct method), see [1, 2, 4]. Basically, the difference between the (raw-)Cq value of a gene of interest and the average of the (raw-)Cq values of some reference genes is calculated and called delta-Cq value.
The invention describes how to calculate confidence intervals for delta-Cq values gained from PCR measurements on material from a tissue sample. These confidence intervals can be used to determine how precise and/or reliable a test result is and thus can be used to determine whether the test result should be reported or the measurements should be repeated to improve confidence. Said confidence intervals can also be used to calculate probabilities for a gene expression value, biomarker value or multivariate biomarker score to be above a certain threshold and thus improve the decision process of how to treat the patient if one or more treatment options depend on said threshold.
The invention relates to the method of claim 1 and the System of claim 13. Preferred embodiments are described in the dependent claims.
The Method of claim 1 and the embodiments described in the dependent claims may be implemented with all its features in the system according to the invention.
In particular the invention relates to
Preferentially the variance of the bounded normalized estimation according to step d) for said observable measurement value is not more than four times larger than the median variance of bounded normalized estimations according to step d) in a representative set of samples.
Application of this noise model is realized by the Bayesian formula.
The invention is realized by the following processing steps: A noise model, which might be constructed on some training PCR data, calculates the distribution of the true target material concentration of a single well for an observed measurement results. Said distribution is calculated for all types of measurement results including “Numeric” raw-Cq values as well as Cq being “Undetected”, which denotes that no fluorescence signal was detected during all cycles and thus corresponds to no or very few target molecules. Based on this distribution information from several replicate wells of a gene of interest and several replicate wells of one or more reference genes the distribution of the true delta-Cq value is calculated. In order to come out with a finite variance of the delta-Cq value (which so far would not be the case if all replicates are “Undetected”) a lower bound is defined on the delta-Cq value. This lower bound is chosen so small that no useful information about the clinical implications is lost but so large that even for samples with low total material yield a reliable estimation of the delta-Cq value is possible.
material from a sample: describes any kind of material measurements are performed in or with. The term is not restricted to direct or indirect measurements and it describes the original material as well as extractions of it. Example materials are FFPE breast cancer tissue slides (and eluates from it), fresh-frozen tissue slides, resections gained during surgeries, blood, stool, callus, hairs, spit, leaves, juice, resin and cultured germs.
QPCR: quantitative polymerase chain reaction. The term shall relate to all technical measuring procedures comprising of cycle-based amplification and detection of the amount of amplified substance.
Cq value: quantification cycle of a qPCR as defined by the MIQE guidelines [4]. Examples include the threshold cycle (Ct), the crossing point (Cp) and the adjusted inflexion point (AlP). The Cq value is the measurement result and thus the input into the processing procedure of the present invention.
type of Cq value, type of result, type of measurement result: A measurement (one target, one sample, one replicate) is assumed to result in one of three classes:
(i) “Numeric” denotes a real-valued (raw-)Cq value which relates to the amount of target material in the sample before amplification. The smaller the (raw-)Cq value the higher the amount of material.
(ii) “Undetected” denotes that no amplification was detected. This relates to the situation of no or very few target material in the sample.
(iii) “Invalid” relates to a problem and/or severe doubt associated with this measurement. An “Invalid” Cq value is interpreted as to contain no useful information.
raw-Cq value: Synonym to Cq value; the term raw-Cq value is used to distinguish from delta-Cq values. Raw-Cq values are the input into the procedure describes by the present invention: For each gene of interest and each reference gene there may be several replicate raw-Cq values.
Normalized: Normalization of measurement values shall be understood in a very general meaning. A normalized value is a value calculated from (raw) values that is more related to the chemical behavior or the features of a biological system than the raw values. A raw value may be more related to technical aspects of the sample such as total volume, total RNA or DNA amount, variations in devices and reagents, storage time and conditions, or others.
delta-Cq value: Special instance of normalized measurement value, see [1, 2] for motivation and description. Deviating from this we use a slightly different definition:
delta-Cq(GOI):=20−raw-Cq(GOI)+mean(raw-Cq(reference genes))
The constant 20 was introduced to avoid negative delta-Cq values; the person skilled in the art knows that this constant is arbitrary and does not change the information contained in the calculated results nor its confidence.
The delta-Cq value and its confidence are the output of the procedure describes by the present invention; for one gene of interest and several reference gene one delta-Cq value is calculated.
replicates: one or more measurements of the same gene within the same material of a sample. The present invention can deal with any number of replicates and different numbers of replicates for different genes. Nevertheless two or more replicates for each gene enable the calculation of a delta-Cq even if one replicate results in “Invalid”. Three or more replicates enable the automatic detection and removal of outliers within replicates.
gene of interest (GOI): the substance a delta-Cq value shall be measured and calculated. The term shall not be restricted to genes; it shall be understood as any substance being amplifiable or having a quantitatively equivalent derivative that is amplifiable.
target: synonym to gene of interest.
reference gene: the substance or target the GOI may be referenced to. The term shall not be restricted to genes; it shall be understood as any substance being amplifiable or having a quantitatively equivalent derivative that is amplifiable. Referencing is realized by calculation of delta-Cq values respectively calculating the difference between the raw-Cq value of a GOI and a reference gene.
The present invention allows the usage of more than one reference gene: First, the raw-Cq values of the reference genes are averaged, and then the difference between the raw-Cq value of the GOI and the averaged raw-Cq values of the reference genes is calculated. The person skilled in the art knows that first the averages of the replicates for each reference gene and then the average of the reference genes have to be calculated; averaging all replicates of all reference genes in one step would yield a different result due to potential occurrences of “Invalid” replicates.
measurement noise: describes the fact that repeated measurements do not exactly yield exactly the same results. The term measurement noise relates to a random variable describing this effect in a mathematical model as well as its distribution or its standard deviation. The term measurement noise is not restricted to any specific source or cause of such noise; it may be understood as replicate-to-replicate noise with one PCR plate, deviations between specific devices, operators or lots, statistical deviations between devices, operators or lots, or total noise between PCR-based tests.
noise model: mathematical description of the relation between true and measured raw-Cq values. In particular a noise model describes the distribution of raw-Cq values (including their classes “Numeric”, “Undetected” and “Invalid”) for a fixed (unknown) true raw-Cq value or target amount.
confidence: any information describing the statistically estimated true value of a variable. Variables may be raw-Cq values, delta-Cq values, replicates, averages of replicates, or averages of reference genes. Primarily the term confidence shall be understood as the estimated distribution of the true value of said variable; this is related to the distribution of measured values or estimates for a fixed true value (sec- and interpretation). Confidences may be presented as distributions, approximations to distributions, sets of sampled values, confidence bounds (lower and upper) or standard deviation.
lower bound: Key concept of the present invention. The phrase “lower bound” used in the context of delta-Cq values or their calculation or estimation denotes a fixed number serving as an absolute minimum for delta-Cq values. The rationale for the introduction of a lower bound can be taken from
In the following, the invention is described in conjunction with exemplary embodiments, actual examples and figures, which show:
Genes were analyzed separately: The log-likelihood of predicting metastases is drawn as a function of the lower bound. Genes are known to be predictive within this data set and log-likelihood curves were shifted along the y-axis to have zero maximum value for graphical reasons. The “all” curve is the arithmetic mean of the curves of the genes to fit to the same axes.
As one expects the higher the lower bound the more information about metastases is lost. Nevertheless the plot indicates lower bounds less than about 9 not to destroy information significantly. In fact the lower bound was chosen to be 8.5 here.
Let c be the raw-Cq value for some GOT and r be the reference gene raw-Cq value (one reference gene only). Then the unbounded delta-Cq value is
du=20−(c−r).
Let the lower bound be 8.5, then the (bounded) delta-Cq value is
d=max{du,8.5}.
For the rationale of bounding see
The following table shows some examples of measurement results in each row. Columns “data entry” contain raw measurement results, columns “mathematical interpretation” add estimated noise from some noise model to it. The remaining columns are calculated according to the formulas above.
The PCR machine ran 40 cycles, thus “Undetermined” denotes a raw-Cq value above 40. Sample B is a diluted version of sample A (dilution factor 2̂5=32 if amplification efficiency is perfect), samples D, E and F are diluted versions of sample C (factors 2̂3=8, 2̂5=32 and 2̂10=1024).
As one can see bounding has the following effects. Samples A and B are not affected, neither their estimate nor their confidence. Samples C, D and E have improved confidence. Sample F is a hopeless case; no mathematical method can make a confident delta-Cq value estimate as long as the reference raw-Cq value is such large.
For some measured raw-Cq value (gene of interest or reference gene), the standard deviation of the raw-Cq measurement is calculated as
std.dev.=log 2(2̂0.3+2̂((raw-Cq−35)/2)).
The model then assumes a normal distribution for the true value with this standard deviation and with expected value equal to the measured raw-Cq value. If “Undetected” was measured the true raw-Cq value distribution is modeled as equal distribution within some interval [a, b], where a is the number of PCR cycles measured and b is derived from the definition of the delta-Cq value using the reference gene values and the lower bound for the delta-Cq value.
Same as noise model A1, but for “Undetected” the true value distribution is blurred at the lower interval bound in order to even give raw-Cq values close below a also a positive probability. The degree of blurring should correspond to the estimated standard deviation for “Numeric” Cq values at a.
Same as noise model A1 or noise model A2, but formula
std.dev.=log 2(2̂0.3+2̂((raw-Cq−35)/2))
describes the standard deviation of the measured raw-Cq values for a fixed true raw-Cq value. This can be converted into a distribution of the true raw-Cq value for a fixed measured raw-Cq value using the Bayesian formula, where an appropriate prior distribution for delta-Cq values must be applied. A possible choice for such a prior distribution could be the (improper) equal distribution over all real numbers.
Same as noise model A3, but with a prior distribution that is derived by sampling from some cohort (i.e. training cohort). Among all samples of the cohort those samples are selected that have reference raw-Cq values below a certain threshold. For them delta-Cq values can be calculated directly by definition with good confidence.
It is assumed that the PCR machine runs 40 cycles. Then, for a fixed true raw-Cq value the probability of a measurement to result in “Undetected” is
P(“Undetected”)=exp(−exp(−0.657758*(true raw-Cq−38.5514))).
The probability for a “Numeric” observation is
P(“Numeric”)=1−P(“Undetected”).
Please note that the true raw-Cq value is unknown and may be larger than the number of cycles run.
If a “Numeric” raw-Cq value was observed, then, for a fixed observed raw-Cq value, the true raw-Cq value is normally distributed with mean equal to the observed raw-Cq value and variance given by the following equation:
variance=0.0267907+exp(0.509836*(raw-Cq−37.3691))
Same as noise models A1-A4 or B, but with extension of further measurement noise sources. While the above noise models only consider replicate-to-replicate noise other sources (device, lot, operator, . . . ) may introduce additional noise. Noise model C considers this by folding raw-Cq and/or delta-Cq distributions with an additional normal distributed noise having zero mean and a standard deviation that estimates further measurement noise sources and that is estimated experimentally.
Alternative solutions may differ in alternative noise models and alternative mathematical/numerical calculation methods. Calculation methods depend on the chosen noise model and include the following features:
(i) bounds: lower/upper/both
(ii) dependence of bounds: GOI, reference genes, application, device used, primer/probe design, SOP used, . . .
(iii) Bayesian prior for raw-Cq values: equal distribution/equal distribution between bounds/sampling from training cohort/parametric distribution derived from training cohort/other priors
(iv) approximation: normal distribution for all variables/use samples from training cohort/use equidistant samples/exact with numeric integration
(v) covariance between delta-Cq values of different GOI: ignore/consider
Outlier within replicates may be identified and eliminated as a first processing step. This may be performed for the GOI as well as for each reference gene. Identification of outliers may be realized by application of a noise model to the set of replicates and calculation of a P-value for the null hypothesis “Any real number is the true raw-Cq value” (this P-value is related to the Bayesian evidence). Alternatively, an outher may be identified by estimating a true value with confidence from the other replicates and comparing these to the replicate to test by an appropriate statistic based on some noise model.
Elimination of outliers may be realized by setting them to type “Invalid”.
Outlier identification as described in example 8 can be improved by examining highly correlated genes. These may be different reference genes or different genes from a common motive. By comparing all replicates from all the genes under consideration one may derive P-values of a single replicate or a single gene to be an outlier by methods similar to these described in Example 8: Therefore a noise model as well as a measure of the correlation between genes should be considered.
In this example we describe a mathematical method to calculate delta-Cq values with confidence as part of a test that predicts a patient's recurrence risk from RNA measurements within a primary breast cancer tissue slide.
The number of molecules of a certain gene in a defined volume of eluate depends on a lot of factors. Among them are
The first factor is the one we want to extract because we believe it contains the information about the future tumor development. The other factors can not be standardized effectively; but fortunately they affect—more or less—all genes the same way. This enables us to calculate the expression of a gene relatively: We examine the ratio between the numbers of molecules of a gene of interest (GOI) and some so-called reference genes. The reference gene expressions are treated as internal references inherently contained in each sample.
We distinguish between GOIs on one hand, whose relative expression predicts the risk of recurrence, and reference genes on the other hand which are used to refer to. Not every gene is suitable for reference. Reference genes should be known to have a constant expression level and should be able to be measured precisely. High expressed genes can be measured more precisely than low expressed ones, thus reference genes are chosen among the high expressers. Biologically, probably no gene has an exactly constant expression level. Nevertheless there are some genes that have very similar expression levels between patients (housekeepers) and are thus suitable for usage as reference genes.
Since there is no perfect reference gene and because we need to have a robust reference this example assumes two reference genes to be measured and the average of their raw-Cq values to be used for delta-Cq value calculation. Throughout this text we use two reference genes; nevertheless a generalization to more reference genes is straight forward and can easily be derived by a person skilled in the art. Our software implementation is able to handle arbitrary numbers of reference genes.
Examples of reference genes are RPL37A, GAPDH, CALM2, PPIA, and OAZ1.
Delta-Cq values in this example can be written as
where d is the delta-Cq value, g is the raw-Cq value for some GOI and r(1) and r(2) are the raw-Cq values of our two reference genes. Since Cq values are logarithms of molecule numbers the ratios of molecules mentioned above transform into differences of Cq values, i.e. the difference inside the outer brackets.
The part outside the outer brackets on the right side of equation (1) seems to be arbitrary at first glance. We chose this definition for two reasons: We want higher delta-Cq values to correspond to higher expressions (this explains the minus sign in front of the brackets) and we did not want to deal with negative numbers (this explains the constant 20).
Raw-Cq values is this example are measured in triplicates and we describe our approach in this text using three replicates: Less than three replicates makes outlier elimination impractical. The generalization to more or less than three replicates is straight forward and may easily derived by a person skilled in the art.
Triplicates are three independent measurements for each sample slide and each gene, however on the same plate. Each replicate can have one of three types of result:
In summary, examples of raw-Cq values are 23.5, 37.9, “Undetected”, and “Invalid”. In this example outliers are detected and converted to “Invalid” prior to the calculations described here.
In this example we use delta-Cq values to predict a patient's recurrence risk. Thus for each gene we need a numeric value to put into our risk score formula. Unfortunately “Undetected” gives us incomplete information. Let us discuss this in some example samples:
Sample A describes a typical sample with high yield (raw-Cq of reference genes is small) and low expressed gene (raw-Cq of GOI is much greater than reference genes). From the raw-Cq values of the GOI and the references (both are assumed to have the same value) we can calculate the delta-Cq value from equation (1). Now we dilute sample A by a factor of 25=32 and call it sample B: Compared to sample A both raw-Cq values raise by 5 Cq values, but the delta-Cq value remains unchanged. This is an important feature because sample dilution obviously does not change the recurrence risk of the patient. Samples C and D are again sequential dilutions by a factor 32 each. The raw-Cq value of the reference genes raise up in steps of 5 Cq values, but the GOI does not give a signal any more. Thus, we cannot assign a “Numeric” value to the raw-Cq value, but since we know that 40 cycles were ran we can say that the theoretical raw-Cq value of the GOI must be 40 or above. In other words “Undetected” is interpreted as the interval [40,∞[. We can substitute this into equation (1), which gives us a delta-Cq value which again is an interval. Unfortunately the delta-Cq interval depends on the reference raw-Cq value. The interpretation is very natural:
As discussed above the delta-Cq value may either be a real value or an interval of form ]−∞,dmax]. This is still not suitable for recurrence risk prediction. We demonstrate this by an example. Two of the most important motives for recurrence prediction are proliferation (higher proliferation means higher risk) and immune system (higher immune system activity means lower risk). A simple recurrence risk score might look like
s=0.6d1−0.4d2, (2)
where d1 denotes the delta-Cq value of some proliferation gene and d2 one of an immune gene. Setting the delta-Cq values to intervals of forms as discussed above has different effects on the score form since the coefficients of the genes in equation (2) have different signs. Going back to raw-Cq values we find the form of the score s to depend on the raw-Cq value types of the GOIs:
To report these very different forms of scores makes not much sense, because they cannot be compared to each other; the clinician or patient needs to know whether the risk is low or high.
Fortunately this interval form information is not the end of the rope. For each gene we know the typical range of delta-Cq values and the associated risks. In particular we may not need to distinguish between low expression (e.g. delta-Cq between 8 and 10) and very low expression (e.g. delta-Cq<8) if there is no difference in the recurrence rate between the two patient groups. If so, we could assign the same risk score to samples having delta-Cq values 5, 8, 10, ≦8, or ≦10. The numerical realization of this grouping mechanism is to define a lower bound L on delta-Cq values. One possible way to account for the lower bound is to modify definition (1) to
This definition of delta-Cq values prohibits infinite intervals and so reduces the uncertainty of delta-Cq values to a bounded interval. Let us look on some example samples again (samples A-D are from the table above) using the lower bound L=10:
For samples A-C the delta-Cq value is at the lower bound. Please note that even in case C with an “Undetected” raw-Cq value there is no longer uncertainty in the delta-Cq value. Only sample D with very bad yield shows a large uncertainty in the delta-Cq value estimation. Samples E and F show a different case with high expression in two dilution steps. Even for bad yield the delta-Cq value can be estimated within a +/−0.5 Cq value confidence interval. This might be precise enough to distinguish between high and low recurrence risk. When thinking about quality control the two example samples demonstrate that looking at the yield (i.e. raw-Cq value of reference genes) only one cannot give a good criterion which samples to predict and which to refuse.
The determination of the lower bound is discussed here only briefly. The introduction of a lower bound in general becomes necessary by the observation that “Undetected” raw-Cq values lead to infinite interval estimations in delta-Cq values. What arguments are used to determine the concrete value of L? First, the higher L the more information is lost; in particular this affects genes and samples having “Numeric” values. Since we are interested in information about the recurrence risk this kind of information loss can only be assessed using patient's outcome information (examining non-linearity between delta-Cq and outcome). Second, the lower L the higher the uncertainty in delta-Cq values; this is true for the confidence interval width as well as for the signal-to-noise ratio. Please note, that L must be independent of patients. We addressed these topics in a detailed discussion and found a value for L indicating a compromise. Since the statistical robustness of such a compromise is not very high we chose the same lower bound for all genes.
This example describes the estimation of delta-Cq values and their confidence intervals in mathematical detail. We use a Bayesian methods approach to calculate delta-Cq value distributions.
To estimate a delta-Cq value we need three parts:
Estimation of the true raw-Cq values of the reference genes: r(1),r(2). We assume two reference genes here; the skilled person can easily generalize to a higher or smaller number of reference genes.
Consideration of the lower bound: d≧L.
Estimation of the true raw-Cq values of GOI (gene of interest): g.
In a processing view we perform calculations in this order and also discuss them here in this order.
We denote unknown true values by r(j),g (raw-Cq values), and d (delta-Cq value). We assume measurements in triplicates and denote the measurement values by ri(j) and gi, respectively, where i=1, . . . , 3 runs over replicates. The skilled person can easily generalize to a higher or smaller number of replicates. Let D (“data”) denote all measured values for a particular sample and fixed GOI, thus we have D={g1, . . . , g3, r1(1), . . . , r3(1), r1(2), . . . , r3(2)}.
When examining the covariance of two genes we denote the true values as g(1), g(2), d(1), and d(2), denote measurements by gi(j) for jε{1,2}, and set D={g1(1), . . . , g3(1), g1(2), . . . , g3(2), r1(1), . . . , r3(1), r1(2), . . . , r3(2)}, respectively. Also see the section at the end of this example for a complete list of symbols.
To estimate the true value of a reference gene means to calculate the posterior probability of its true value given the measurement results. This can be done using the Bayesian formula.
The three probabilities on the right hand side can be discussed separately. The prior distribution of the true value is chosen to be equal for all values,
p(r(j))=const. (5)
With “const” we abbreviate factors in equations that are independent of all of the true values g, r, and d. They depend on the data D and may differ between transformation steps. The choice of an equal prior makes is completely non-informative, because each r(j)ε has the same probability and no estimation bias is introduced (see below). The prior is not normalizable, i.e. ∫p(r(j))dr(j)≠1 for all constants, and thus the prior is called an improper prior. The Bayes equation (4) can be written as
and one can now see that the same constant appears in the numerator as well as the denominator. Most non-informative priors are improper and their usage is common practice. The denominator in equation (4) is—as seen—only a normalizing factor. Since it does not depend on the true value we abbreviate it as some constant and rewrite equation (4).
p(r(j)|D)==const·p(D|r(j)) (7)
Obviously only the likelihood factor is left to determine the reference gene true value distribution. Only measurements of reference gene j are affected by the true value,
p(r(j)|D)=const·p(r1(j), . . . ,r1(j)|r(j)), (8)
and these measurements are assumed to be independent.
Since the noise model in this example estimates the distribution of the true value for a fixed measured value (not the other way around), we have to apply the Bayes formula again to each factor on the right hand side.
The denominator is already defined by equation (5), and the prior distribution of the measurement is a constant because it does not depend on the true value. Thus the equation simplifies to
Now we can apply the noise model. If we observe an “Undetected” value for one of the replicates (which was not removed by outlier elimination procedure) we reject the sample. This is because raw-Cq values of reference genes are typically lower than those for GOIs, and if the reference is “Undetected” most GOIs will also be “Undetected” and we will not be able to estimate delta-Cq values properly. If any of the replicates is “Invalid” or an outlier, we just omit the corresponding factor. Thus, for the remaining “Numeric” replicates we apply the noise model, which here consists of the noise function σ(.):
Some transformation steps
show that the data-conditional true value is normally distributed with parameters
Our implementation calculates these values this way. Obviously the estimated mean is a weighted average of the measured values where the weighting factors are σ(ri(j))−2: The higher the measurement noise the lower the weighting factor. Nevertheless, for most samples the raw-Cq value of the references will be below 30, where the noise is nearly constant. Under this approximation the estimated mean simply is the arithmetic average of replicates.
Our delta-Cq value definition uses the average of two reference genes. Before we proceed with the GOIs we summarize our reference genes into one variable. We define
Since the replicates of the different reference genes are independent, variables r(1) and r(2) are independent, too. Using random variable calculus rules we find that r is normally distributed with parameters
Our implementation again calculates these values.
As will be seen below the posterior distribution of the true raw-Cq value of the GOI depends on the reference gene. The main reason for this is the lower bound constraint on the delta-Cq values. Nevertheless, the likelihood (i.e. the probability of observed measurement values) does not depend on the reference gene. This section derives the likelihood of raw-Cq values of a GOI from the noise model.
We measure three replicates and assume they are independent.
Remember that a GOI measurement results in one of three result types: “Numeric” (a real number denoting a cycle), “Undetected” (no signal within all cycles run), or “Invalid” (some failure for this replicate). “Invalid” replicates are assumed to give no information about the true value and we simply omit the corresponding factors on the right hand side of equation (16). Function υ(.) is part of the noise model and estimates the probability of “Undetected” for a given true raw-Cq value.
While “Undetected” determines the likelihood for a single replicate completely by function υ(.), we have to consider the measurement noise in addition for “Numeric” values. Like with the reference values the noise model describes the distribution of the true value for a fixed measured values; thus we first have to apply Bayes formula.
Again, we reduce the normalizing denominator to a constant and choose the data prior in the numerator as constant.
p(gi|g,gi is “Numeric”)=const·p(g|gi,gi is “Numeric”) (19)
The likelihood is taken from the noise model as a normal distribution:
We can summarize equations (16) to (20) to a function of the form
with appropriate constants m,n,μg, and σg. In case there are no “Numeric” measurements we define μg=0 and σg=∞. Our implementation calculates these constants and we define a help function
Later we evaluate the likelihood of all replicates of the GOI by calculating help function values point-wise numerically.
The delta-Cq value definition in equation (1) and the summary reference value definition in equation (14) lead to the simplified delta-Cq value definition
d=20−g+r, (23)
which will be used below. Please keep in mind that g|D and r|D are not independent because of the lower bound constraint on the delta-Cq value. In the following we calculate the posterior delta-Cq value distribution by examining the bivariate p(g,r|D) distribution.
The reference value can be estimated independently from GOIs, thus we give a separate factor to it, which already was determined above.
p(g,r|D)=p(g|D,r)p(r|D) (24)
We now analyze the reference-conditional distribution. First, the GOI distribution only depends on the GOI measurements when the reference value is fixed.
p(g|D,r)=p(g|g1, . . . ,g3,r) (25)
Now we apply Bayes formula.
We discuss the three probabilities on the right hand side separately. The denominator is only a normalizing factor for the left hand probability and thus can be set to some constant.
p(g1, . . . ,g3|r)=const (27)
The prior probability p(g|r) is chosen non-informatively, but reflects the lower bound constraint d≧L, which was already discussed above. Thus we set
where H(.) is the Heaviside step function. This again is an improper prior. The remaining probability in equation (26) is the likelihood. Since the GOI measurements only depend on its true value if known we can rearrange the likelihood to
p(g1, . . . ,g3|g,r)=p(g1, . . . ,g3|g) (29)
Combining equations (26) to (29) we get
p(g|D,r)=const·p(g1, . . . ,g3|g)H(20−g+r−L). (30)
We now combine equations (24) and (30), replace the likelihood of the GOI measurements by our help function (22), and replace the posterior reference distribution by our results from above, (12) to (15).
Here we assigned the constant factor the name c because it will play an important role later. Please note that c depends on constants m,n,μg,σg (as function h(.) does), L, μr and σr, but not on g nor r.
Estimation of delta-Cq values has now been partially separated rated into factors: factor h(g) does not depend on the reference while the last factor does not depend on the GOI true value. Only the Heaviside factor connects them, it just determines an integration limit.
Delta-Cq Value Calculation for normal distributions
In this and the next section we use equation (31) to calculate several features of random variable d. The reason for this is just to speed up processing time of our implementation. The special case we consider first occurs quite often and can be solved analytically; it is:
There is no “Undetected” GOI replicate and g|D and r|D are approximately independent.
These conditions need further discussion. The first condition targets factor h(g) in equation (31), the second aims on the Heaviside factor. Remember that function h(.) as defined by equation (22) is determined through constants m,n,μg, and σg. If there is no “Undetected” GOI replicate then m=n=0 and h(g) describes a normal distribution with mean and variance σg2. We look at the second condition only if the first is fulfilled. In this case we have
g|D∝N(μg,σg2) and r|D∝N(μr,σr2), (32)
and the corresponding delta-Cq distribution (neglecting the Heaviside factor) would be
d|D∝N(20−μg+μr,σg2+σr2. (33)
Random variables g|D and r|D are approximately independent if the corresponding delta-Cq value is far away from the lower bound with high probability. We state condition 2 more precisely as
20−μg+μr−L≧4(σg2+σr2. (34)
With this condition the probability of the Heaviside factor in equation (31) being zero is <3.2·10−5. Our approximation is defined as to set it never zero and with this equation (31) simplifies to
Obviously g|D and r|D become independent. With this, the delta-Cq value distribution is determined by (33) including all of its univariate features.
In addition to this we need to calculate the covariance between two GOIs. For this task we require both conditions to be fulfilled for both GOIs, otherwise we proceed as described in the next section. If all conditions are fulfilled we have
d
(1)=20−g(1)+r and d(2)=20−g(2)+r (36)
with (approximately) independent raw-Cq values. Please note that in the general case g(1)|D and g(2)|D depend on each other only via the reference, because their replicates are independent measurements (see below for a more detailed discussion). We now calculate the covariance straight forward.
In this section we use equation (31) in the general case to calculate features of random variable d. Therefore we use the bivariate distribution of g and r and calculate the expected value and the variance from it. We start with the definitions of the expected value and the variance.
Since we do not know constant c in equation (31) we have to calculate an additional integral to determine it.
1=∫∫p(g,r|D)dgdr (39)
Abbreviating the true reference value distribution function by
we substitute the joint probabilities of the above integrals by the right hand side of equation (31).
1=∫∫c·h(g)H(20−g+r−L)f(r)dgdr
E[d|D]=∫∫(20−g+r)·c·h(g)H(20−g+r−L)f(r)dgdr
E[d
2
|D]=∫∫(20−g+r)2·c·h(g)H(20−g+r−L)f(r)dgdr
We then concentrate the reference-dependents factors into the inner integral and move all other factors out of it.
With respect to r the inner integrals consist of a polynomial of grade 2 at most multiplied with the normal distribution probability density. If we allow the well-known error function
to be called elementary we can calculate these integrals analytically. We start with the monomials.
To have a more compact form we introduce some abbreviating constants.
With them the monomials simplify a lot.
We substitute the inner integrals in equations (42) to (44) by this.
1=c·∫h(g)·α(g)dg (49)
E[d|D]=c·∫h(g)·((20−g+μr)α(g)+β(g))dg (50)
E[d
2
|D]=c·∫h(g)·(((20−g+μr)2+σr2)α(g)+(20−g+L+μr)β(g))dg (51)
Constant c can now be calculated by numerical integration over g using equation (49). The expected value can then be determined by numerical integration using the equation (50) and the variance via (51). Please note that no transformation or substitution of integration variable g has been done and all three integrals have the same limits, thus the implementation can speed up by integrating them “in parallel” (Matlab function quadv), i.e. running one integration on a three-dimensional integrand. Since the integrands represent random variable distributions numerical integration can be interpreted as drawing (special) samples from the distribution and calculating features from the finite set of samples. In this context parallel integration simply means that for all features the same samples are used.
Now we calculate the covariance between two GOIs. Therefore we first specify the joint raw-Cq value distribution and then extend equation (31) to two GOIs appropriately. The joint distribution of all three raw-Cq values can be written as
p(g(1),g(2),r|D)=p(g(1),g(2)|D,r)p(r|D). (52)
As stated above the raw-Cq value distribution of a GOI depends on the reference value through the lower bound constraint, but the reference value distribution itself is independent. We now assume in addition, that the raw-Cq values of the GOIs are independent for a fixed reference value.
p(g(1),g(2),r|D)=p(g(1)|D,r)p(g(2)|D,r)p(r|D) (53)
We apply some basic transformations to end up in a form using the right hand side of equation (31). Please note that the true reference value is normally distributed and thus has a positive probability density for every value.
We can now substitute the numerator using equation (31) and denominator using the results from above to derive a concrete form for the joint raw-Cq value distribution.
Please note that by construction any feature of a GOIs delta-Cq value distribution is consistent to what was calculated in the previous section: E[d(1)|D] and VAR[d(1)|D] do not depend on whether they are calculated from p(g(1),r|D) by double integration or from p(g(1), g(2), r|D) by triple integration. With the joint distribution defined in equation (55) we can now calculate the covariance.
We can focus on the calculation of the expected value of the product of the delta-Cq values. Therefore we use the same strategy as in the previous section: We integrate over the reference analytically.
Using equations (48) and substituting g:=max{g(1),g(2)} we can solve the inner integral.
This equation can be evaluated numerically, the results leads to an estimation of the covariance of two GOIs.
Summary of symbols and abbreviations in this example
c special constant for the joint probability of g and r, see equation (31).
c(j) special constant for the joint probability of g(j) and r, see equation (31).
const some constant with respect to all true values d, g, and r(j); may depend on D.
D “data”; abbreviation of all measured values g1, . . . , g3, r1(1), . . . , r3(1), r1(2), . . . , r3(2), . . .
d true delta-Cq value of the GOI
d(j) true delta-Cq value of j-th GOI
E[.] expected value
Erf(.) error function. See equation (45) for definition.
g true raw-Cq value of the GOI
g(j) true raw-Cq value of j-th GOI
gi measured raw-Cq value of GOI, i-th replicate
gi(j) measured raw-Cq value of j-th GOI, i-th replicate GOI gene of interest (in contrast to reference gene)
H(.) Heaviside step function: H(x)=0 for x<0, H(x)=1 for x≧0
h(g) help function: proportional to likelihood of all replicates of GOI
i index denoting the replicate
j index denoting the reference gene
L lower bound
μr mean of the posterior distribution of true raw-Cq value
N(μ,σ2) normal distribution with mean μ and variance σ2
p(.) probability
P(.) probability density
r true mean raw-Cq value of reference genes, r=(r(1)+r(2))/2
r(j) true raw-Cq value of reference gene j
ri(j) measured raw-Cq value of reference gene j, i-th replicate
σ(.) noise model estimating the standard deviation of replicate-to-replicate noise
σr2 variance of the posterior distribution of true raw-Cq value
VAR[.] variance
υ(.) noise model estimating the probability of “Undetected” End of Example 11
We use the same symbols as in example 11, see above.
Delta-Cq values in this example are defined as
d=max{20−(g−r),L} (59)
where d is the delta-Cq value, g is the raw-Cq value of the GOI, r is the mean raw-Cq value of the reference genes, and L is the lower bound. Several reference genes are averaged,
where r(j) is the raw-Cq value of the j-th reference gene and J is the number of reference genes.
The distribution of the true delta-Cq value is estimated from the measurement results using a Bayesian approach: The likelihood is calculated based on a noise model and the prior distribution is sampled from a training set. Technically, the prior distribution is a delta-Cq value distribution which is transformed to a raw-Cq value distribution conditional on the raw-Cq values of the reference genes according to equation (59). The sampling character of the prior is used for an efficient and fast numeric calculation algorithm.
Said prior distribution is a distribution of delta-Cq values sampled from some training set. The training set used here is a set of about 300 samples; the same training set was used for other calculations involving additional variables as well.
The prior distribution was constructed by selecting samples from the set of available samples. The selected samples should represent the basic population, thus selection criteria were chosen in a way that did not introduce a bias. On the other hand selection was necessary because not all calculated delta-Cq values have sufficient confidence. This seems like a chicken-and-egg problem: Without a prior distribution we cannot calculate the confidence, without confidence we cannot calculate the prior. We overcame this by evaluating confidence only qualitatively (not quantitatively) using some conservative heuristics. These heuristics may also be applied to other data than the prior distribution training set.
The first selection criterion was that all reference gene replicates had type “Numeric”. This excludes samples with no or extremely few total material (“Undetected”) as well as “Invalid” measurements.
As discussed in example 1 the confidence of a delta-Cq value is bad only if both, the reference genes and the GOI raw-Cq values are high. We describe this as a heuristic inequality by requiring the uncertainty caused by the lack of information caused by an “Undetected” type measurement result to be completely repaired by the lower bound. This means: We ran 40 PCR cycles, thus the highest possible “Numeric” measurement value is 40. If such a value yields a delta-Cq value equal to the lower bound, then all “Undetected” raw-Cq values with the same reference gene values will also yield a delta-Cq value equal to the lower bound, and thus will be assumed to be sufficiently confident. Mathematically we require
20−(g−r)≦L for g=40. (61)
Substitution and rearrangement yields
r≦L+20. (62)
This is a simple condition on the reference genes value which can easily be tested based on the reference genes replicates. We refined this criterion by inclusion of a safety zone, because the noise model predicts quite high noise (bad confideuce) for raw-Cq values of about 40:
r≦L+20−z, (63)
where we chose the safety zone size z between 1 and 5, mainly depending on the size of the training cohort. Please note that the noise model predicts that the noise increases monotonically as a function of the raw-Cq value.
Equation (63) is the second and last inclusion criterion for samples of the prior distribution. Approximately half of the available samples from the training cohort were selected for the prior.
We first estimate the distribution of the true mean of the reference genes values r according to equation (60) from the measured reference genes values {ri(j)} where i denotes the replicate index and j denotes the reference gene index. All measured reference genes values are required to be either “Numeric” or “Invalid” (we assume outliers within replicates to be eliminated before this processing step).
For a fixed true value r(j) the noise model σ(.) we use in this example predicts a measurement value ri(j) to be normally distributed with standard deviation from the noise model function:
r
i
(j)
|r
(j)
∝N(r(j),σ2(r(j)). (64)
Note that σ(.) has a different meaning here compared with example 11. In addition, while example 11 uses a Bayesian estimation to determine the true values at this point, we here apply some approximations to avoid too complicated formulas. First, we average the replicates of reference gene j:
where I(j) is the number of “Numeric” (non-“Invalid”) replicates for reference gene j. We can easily derive a distribution for this average.
(j)
|r
(j)
∝N(r(j),σ2(r(j))/I(j)) (66)
Obviously our average is an unbiased estimator for the true value. Unfortunately its confidence in terms of the variance, σ2(r(j))/I(j), depends on the true value, which is unknown. Since our average
s
(j)=σ(r(j))/√{square root over (I(j))} and STD[r(j)|
Under this approximation we estimate the noise by averaging the noise function in the range of the estimated true value.
s
(j)
=E[σ(N(
This circular equation is solved in s(j) by fix-point iteration. The expected value in equation (68) is calculated based on sample nodes z1, . . . , zM generated from percentiles of the standard normal distribution such that z1, . . . , zM have zero mean and variance equal to 1. Using these sample nodes equation (68) transforms to the fix-point iteration update rule
which can be calculated numerically. The starting value is s0(j)=σ(
In summary, the true reference gene value (conditional on the measurements) is estimated as
r
(j)
∝N(
and the estimate of the mean of the reference genes values then becomes
Since we use these calculation results below we assign variable names to them. Define
thus we have the r∝N(μr,σr2).
In opposite to the reference genes measurements the GOI measurements are allowed to result in “Undetected”. “Undetected” in this example means that the true raw-Cq value is above 40 (the number of PCR cycles run here) with high probability. Since in this case the true value cannot be well described by a normal distribution we use a Bayesian approach for the estimation.
The true delta-Cq value is estimated from the GOI replicate measurement values g1, . . . , gI and the true mean value of the reference genes r. Similar to the reference genes measurements “Invalid” measurements contain no information and are removed first; thus, g1, . . . , gI are of type “Numeric” or “Undetected” only. We use the Bayesian equation conditional on the reference to calculate the posterior distribution of the true delta-Cq value.
We discuss the terms on the right hand side separately. The prior distribution is modeled to be independent of the reference, p(d|r)=p(d), and then the prior distribution samples from the training set as discussed above are used. Please note that by using this prior delta-Cq values below the lower bound L have zero probability in the prior, and thus also have zero probability in the posterior.
The likelihood in equation (73) can be divided into factors for the separate measurements since they are independent observations. Moreover the conditions d and r can be summarized into one variable only, g, based on the definition of delta-Cq values: g=20−d+r. Please note that due to the prior we do not have to consider delta-Cq values below the lower bound here.
The denominator in equation (73) does not depend on the delta-Cq value and thus is abbreviated as a constant that is determined later by normalizing the posterior distribution. So far we have
The replicate likelihood factors have different forms according to the type of measurement. As already discussed with the application for references, for “Numeric” replicates the measured raw-Cq value is modeled by a normal distribution using the noise model.
“Undetected” replicates represent a raw-Cq value above 40, therefore we use the cumulated normal distribution function Φ(.) for the likelihood.
Please note that variable g within the right sides of equations (75) and (76) is directly connected to the delta-Cq value d via its definition since the reference r is fixed.
Substituting equations (75) and (76) into (74) enables us to calculate a posterior distribution for the delta-Cq value. Since the prior is based on sample nodes the posterior is a distribution over these finite-numbered sample nodes. Let d1, . . . , dK be the prior sample nodes. The prior distribution assigns equal probability to each of them. The posterior is calculated by
Please note that on the right hand side of this equation variable gk is calculated by gk=20−dk+r. The constant term is different from that of equation (74), is independent of the sample node index k and is determined by normalization, i.e. solution of
The posterior distribution of the delta-Cq values now is described in terms of the prior sample nodes and their probability. In the next step of processing this description of a distribution is changed to an alternative one: The distribution is now described by a set of sample nodes {tilde over (d)}1, . . . , {tilde over (d)}M having equal probability but describing (approximately) the same distribution. The mapping is done by linear interpolation of the cumulated probability. There are two advantages of the new distribution description: First, the number of sample nodes M can be chosen much smaller since we do not need to describe many sample nodes with negligible probability; this saves memory storage as well as computation time in the next processing steps. Second, the number of sample nodes M can be chosen independently of the GOI while the number of prior sample nodes K depends on the gene. This enables us to store the results for several genes in a matrix instead of vectors of different length for each gene.
So far we have calculated the posterior distribution conditional on the true reference value r. Since we do not know r exactly we have to include the estimated variance of it into our delta-Cq value distribution. Therefore, as the next processing step, we apply an approximate adjustment to our distribution sample nodes. The m-th adjusted sample node dm′ will be
d
m
′={tilde over (d)}
m
+αz
m, (79)
where α is the adjustment size factor and zm is a percentile of the standard normal distribution as introduced above with application to the reference gene value estimation. Please note that {tilde over (d)}1, . . . , {tilde over (d)}M as well as z1, . . . , zM are in ascending order. The adjustment size factor α is determined by requiring the adjusted variance to include the reference estimation variance, i.e.
VAR[d1′, . . . ,dM′]=VAR[{tilde over (d)}1, . . . ,{tilde over (d)}M]+σr2. (80)
Remember that σr is the standard deviation of the estimated mean of the reference genes values, and that the GOI estimations {tilde over (d)}1, . . . , {tilde over (d)}M are independent of the reference measurements. Calculating the variance on both sides of equation (79) yields
VAR[d1′, . . . , dM′]=VAR[{tilde over (d)}1, . . . , {tilde over (d)}M]+α2+2αCOV[{tilde over (d)}1, . . . ,{tilde over (d)}M;z1, . . . , zM]. (81)
This can be combined with equation (80) and solved in α.
α=−COV[{tilde over (d)}1, . . . ,{tilde over (d)}M;z1, . . . ,zM]+√{square root over (COV[{tilde over (d)}1, . . . ,{tilde over (d)}M;z1, . . . ,zM]+σr2)} (82)
Now we can calculate the adjusted delta-Cq values.
The last processing step is to apply the lower bound again.
d
m″:=max{dm′,L} (83)
Sample nodes d1″, . . . , dM″ are the final estimated distribution for the delta-Cq values. In an application one may calculate the mean and standard deviation from them to use as estimate with confidence.
The general case using a Bayesian estimation as described above is quite time-consuming and its results (mean of final distribution) slightly deviate from a direct calculation, i.e. averaging “Numeric” replicates and then calculating the delta-Cq value by its definition d=20−(g−r). Therefore we describe an alternative calculation scheme here which can be used if no “Undetected” replicate is present. Most parts of this calculation have already been discussed above. First, we apply the procedure used for the reference genes value estimation to our GOI: let the results be called μg (instead of μr) for the mean and σg (instead of σr) for the standard deviation. The true raw-Cq value of the GOI is then estimated as g∝N(μg,σ22). The delta-Cq value then is estimated as
g∝N(20−μg+μr,σg2+σr2). (84)
To produce a compatible data format we describe this distribution by sample nodes d1′, . . . , dM′ with equal weight; thus we define
d
m′:=20−μg+μr+zm(σg2+σr2. (85)
The last step of calculation is the application of the lower bound according to equation (83).
We complete this example by showing some Matlab® (The Math-Works, Inc., Version 2009b) script code that calculates a delta-Cq value distribution from GOI and reference genes replicates. In addition to the text above it contains some ideas to improve numerical behavior and to speed-up the implementation.
Calculation of delta-delta-Cq value distributions Livak and Schmittgen, [1], and Pfaffl, [2], describe a method for comparing or compensating delta-Cq values with a reference sample, the so-called delta-delta-Cq method. Let d1 be the delta-Cq value for the sample of interest and d2 be the delta-Cq value for the reference sample, the delta-delta-Cq value δ is defined as
δ=d1−d2. (86)
Delta-Cq values d1 and d2 may be calculated according to any of the above examples. With these estimates an estimate for the delta-delta-Cq value can easily be derived, because d1 and d2 are independent. If the estimation of the true value of d1 and d2 is calculated as a general distribution, the corresponding delta-delta-Cq value distribution can be calcufated by convolution according to equation (86). If the true values of d1 and d2 are described by an expected value and a variation only, these features can be calculated for the delta-delta-Cq value, too:
E[δ]=E[d
1
]−E[d
2]
VAR[δ]=VAR[d1]+VAR[d2]. (87)
The delta-Cq method assumes GOI and reference genes to have equal efficiency: Diluting the sample will raise both Cq values by the same amount and leaves the delta-Cq value unchanged.
Removing this assumption introduces constant factors for the raw-Cq values:
d=20−(cg·g−cr·r), (88)
where d is the efficiency-compensated delta-Cq value, g is the raw-Cq value of the GOI, r is the raw-Cq value of the reference gene and cg and cr are constants compensating for non-ideal efficiencies. Constants cg and cr do not depend on the sample nor measured values associated with it; they may depend on the reagent lots or other technical parameters of the measuring process. The noise model may or may not consider the efficiency compensation. Nevertheless, for a chosen noise model and fixed constants cg and cr the skilled person can easily derive the delta-Cq value estimate including confidence information similar to any of the above examples.
From a breast cancer tumor removed during surgery tissue slides are cut, RNA is extracted and the expression levels of several genes are measured by quantitative PCR. The resulting raw-Cq values are processed by a calculation method that is claimed by this patent application and that calculates delta-Cq value estimates in term of a mean and a variance for each GOI. More precise, let K be the number of GOIs (K=1 for a normalized, single gene assay; K≧2 for multi-index assays), let m1, . . . , mK be the estimated delta-Cq values, and let s1, . . . , sK contain the corresponding confidence information in terms of the standard deviations. The method assumes an approximate normal distribution of the true delta-Cq values d1, . . . , dK:
d
k
∝N(mk,sk2). (89)
Furthermore, let
where q is a score that predicts the probability of the patient to develop a metastasis, and c1, . . . , cK are some constant coefficients. An estimation of the score can be calculated from the estimations of the delta-Cq values:
Based on these results one can define confidence intervals for the score, i.e. [μ−1.96σ,μ+1.96σ]. In addition, if only the estimated score μ shall be reported to the patient or physician, one may define a quality rule: If σ≦σmax for some constant σmax the score is reported, otherwise the measurements have to be repeated.
Another application comes into play when a threshold θ is applied to the score. The physician may select a different or more intense treatment if q>θ. To decide whether the score is above or below the threshold the corresponding probability can be calculated from the cumulative normal distribution function.
The application of a threshold to a fixed score may in particular apply to some special, single genes (K=1): ESR1, PGR, ERBB2, KI67 and other proliferation-related genes.
Comparison to state of the art:
Bengtsson et al, [3], present a detailed noise model considering different sources of measurement noise during concerning the RT-PCR: pure PCR noise, dilution noise, RT-step noise and biological noise. These sources with the exception of the pure PCR noise can be seen as possible extensions to the present invention. [3] does not consider delta-Cq values.
Livak and Schmittgen, [1], describe the so-called delta-delta-Ct method: It extends the delta-Ct method described in this patent application by comparing the sample to measure with a reference sample. The reference sample may be tissue from a different organ or tissue from a differently treated animal. In addition the described method considers different amplification efficiencies of the GOI as well as the reference gene.
The authors do not discuss confidences for delta-Ct nor delta-delta-Ct values. No noise model is discussed. The skilled person can easily combine the definition of delta-delta-Ct values with this patent application: E.g. similar to the derivation of equations describing the distribution of delta-Cq values as shown in examples 10, 11 and 12, the skilled person can derive corresponding equations for delta-delta-Ct values.
Pfaffl, [2], describes a similar mathematical approach as [1], but uses a calibrator sample as reference. Again, confideuces for raw measurement values nor calculated results are discussed, no noise model is applied. The skilled person can easily combine the approach with this patent application.
We think that confidences for individual test results are not calculated up to now. Instead of this the total RNA amount or the reference material amount is controlled which means that samples with small of said amount are rejected. The disadvantage of this method is that more samples than necessary are rejected, in particular in cohorts with small tissue samples and/or long storage time (i.e. training and validation cohorts). The disadvantages are (i) increased costs and processing time for the unnecessarily rejected samples, and (ii) worse confidence and potential biases due to reduced sample sizes in training and validation cohorts.
Controlling test results individually by confidence calculations is superior to controlling them only statistically in general.
Number | Date | Country | Kind |
---|---|---|---|
10166256.7 | Jun 2010 | EP | regional |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/EP2011/057863 | 5/16/2011 | WO | 00 | 12/17/2012 |