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Probable error
Probable error
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In statistics, probable error defines the half-range of an interval about a central point for the distribution, such that half of the values from the distribution will lie within the interval and half outside.[1] Thus for a symmetric distribution it is equivalent to half the interquartile range, or the median absolute deviation. One such use of the term probable error in this sense is as the name for the scale parameter of the Cauchy distribution, which does not have a standard deviation.

The probable error can also be expressed as a multiple of the standard deviation σ,[1][2] which requires that at least the second statistical moment of the distribution should exist, whereas the other definition does not. For a normal distribution this is (see details).

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from Grokipedia
In statistics, the probable error (PE) of an estimate is defined as the value such that there is a 50% probability the true value lies within that distance from the estimate, representing the half-range of the central 50% interval in the error distribution. For errors following a Gaussian (normal) distribution, the probable error equals approximately 0.6745 times the standard deviation σ, derived from the inverse cumulative distribution function where the probability of the absolute error exceeding PE is 50%. This measure provides a probabilistic assessment of precision in measurements or estimates, particularly useful for quantifying the reliability of repeated observations under the assumption of symmetric random errors. The concept of probable error emerged in the early 19th century as part of the developing of errors in astronomy and , where it served as a median-based indicator of variability before the widespread adoption of the standard deviation. It was formalized in the context of methods and gained significant attention through the work of and others in the late 19th century, who applied it to the analysis of measurement dispersions. A landmark contribution came in 1908 when William Sealy , publishing under the pseudonym "Student," introduced the probable error of the mean in small samples, laying foundational groundwork for the t-distribution and inference in finite datasets. Historically prominent in experimental sciences, the probable error offered an intuitive way to express at the 50% level, contrasting with the more conservative 95% intervals based on roughly 1.96σ. However, by the mid-20th century, it was increasingly supplanted by the standard deviation and , which provide more flexible and theoretically robust frameworks for hypothesis testing and confidence intervals, especially in large-sample asymptotics. Despite this, the probable error retains niche applications in fields like , , and certain physics experiments, where its simplicity aids in communicating median precision without requiring full distributional assumptions.

Definition

Basic Definition

The probable error (PE) is a measure of dispersion in statistics that defines the half-range interval around a central estimate, such as the mean or median of a set of observations, within which the true value is expected to lie with a 50% probability. This interval represents the value by which the estimate might typically deviate, providing a probabilistic bound on the accuracy of the estimate. PE quantifies the "most probable" deviation, such that the likelihood of observing a deviation larger than PE is exactly 50%. For a single measurement, PE specifically denotes the value δ* for which the probability of an magnitude at least as large as δ* is 1/2, capturing the median extent of potential error in that . In the context of repeated measurements, for example, PE indicates the typical magnitude that occurs in half of the cases, offering a practical gauge of reliability without implying . In distributions like , PE aligns with the central 50% of the error spread around the mean.

Mathematical Formulation

The probable error (PE) of a XX following a N(μ,σ2)N(\mu, \sigma^2) is defined as the positive value δ\delta^* satisfying δδ12πσ2exp((xμ)22σ2)dx=0.5.\int_{-\delta^*}^{\delta^*} \frac{1}{\sqrt{2\pi\sigma^2}} \exp\left( -\frac{(x - \mu)^2}{2\sigma^2} \right) \, dx = 0.5.
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