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gamma (version 1.1.0)

signal_integrate: Signal Integration

Description

Integration of the spectrum including uncertainty calculation.

Usage

signal_integrate(object, background, ...)

# S4 method for GammaSpectrum,missing signal_integrate(object, range = NULL, energy = FALSE)

# S4 method for GammaSpectrum,GammaSpectrum signal_integrate(object, background, range = NULL, energy = FALSE)

# S4 method for GammaSpectrum,numeric signal_integrate(object, background, range = NULL, energy = FALSE)

# S4 method for GammaSpectra,missing signal_integrate(object, range = NULL, energy = FALSE, simplify = TRUE)

# S4 method for GammaSpectra,GammaSpectrum signal_integrate( object, background, range = NULL, energy = FALSE, simplify = TRUE )

# S4 method for GammaSpectra,numeric signal_integrate( object, background, range = NULL, energy = FALSE, simplify = TRUE )

Value

If simplify is FALSE (the default) returns a list of numeric vectors (the signal value and its error), else returns a matrix.

Arguments

object

A GammaSpectrum or GammaSpectra object.

background

A GammaSpectrum object.

...

Currently not used.

range

A length-two numeric vector giving the energy range to integrate within (in keV).

energy

A logical scalar: use the energy or count threshold for the signal integration

simplify

A logical scalar: should the result be simplified to a matrix? The default value, FALSE, returns a list.

Author

N. Frerebeau

Details

The function supports two integration techniques (see Guérin & Mercier 2011), the (1) count threshold integration and the (2) energy integration method:

The count integration technique (energy = FALSE) integrates all counts in given range:

$$ A = \frac{\Sigma_{i}^{N}S_i}{t_{live}} $$

Contrary, the energy integration techniques is the integrated cross-product of counts and corresponding energy per channel:

$$ A = \frac{\Sigma_{i}^{N}S_i \times E_i}{t_{live}} $$

\(A\) is the area, \(S_i\) is the signal in the \(i^{th}\) channel, \(N\) the number of channels, \(E_i\) the energy of the corresponding channel in keV. \(t_{live}\) is the live time of the measurement in s.

For calculating the uncertainties, Poisson statistics are assumed and hence the errors is calculated as:

$$ \sigma_A = \frac{\sqrt{A}}{t_{live}} $$

References

Guérin, G. & Mercier, M. (2011). Determining Gamma Dose Rates by Field Gamma Spectroscopy in Sedimentary Media: Results of Monte Carlo Simulations. Radiation Measurements, 46(2), p. 190-195. tools:::Rd_expr_doi("10.1016/j.radmeas.2010.10.003").

Mercier, N. & Falguères, C. (2007). Field Gamma Dose-Rate Measurement with a NaI(Tl) Detector: Re-Evaluation of the "Threshold" Technique. Ancient TL, 25(1), p. 1-4.

See Also

Other signal processing: baseline, peaks_find(), peaks_search(), signal_slice(), signal_split(), signal_stabilize(), smooth()