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The Background in Flow Measurement using Pulsed Neutron Activation

In flow measurement with Pulsed Neutron Activation (PNA), water flowing in a pipe is activated with 14 MeV neutrons, producing the radioactive nuclide sup 1 sup 6 N. The gamma radiation emitted from this radionuclide will produce a characteristic peak in a time spectrum from a detector downstream. E...

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Detalles Bibliográficos
Autores principales: Mattsson, H, Dahl, B, Nordlund, A
Lenguaje:eng
Publicado: 2003
Materias:
Acceso en línea:http://cds.cern.ch/record/747276
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author Mattsson, H
Dahl, B
Nordlund, A
author_facet Mattsson, H
Dahl, B
Nordlund, A
author_sort Mattsson, H
collection CERN
description In flow measurement with Pulsed Neutron Activation (PNA), water flowing in a pipe is activated with 14 MeV neutrons, producing the radioactive nuclide sup 1 sup 6 N. The gamma radiation emitted from this radionuclide will produce a characteristic peak in a time spectrum from a detector downstream. Experiments have shown that the peak is superimposed on a background distribution, which can affect the measurement. As it is necessary to correct for the background, different subtraction methods have been used in the past, although the origin of the background has not been known. In this work the source of the background has been investigated. It has been found that there are two components of the background: one time dependent and one time independent. The time-dependent component is shown to be caused by stationary sup 1 sup 6 N in the surroundings. A method for subtracting the background in a reproducible way has been developed. This was done by fitting the peak with an empirical function consisting of several Taylor distributions
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2003
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spelling cern-7472762019-09-30T06:29:59Zhttp://cds.cern.ch/record/747276engMattsson, HDahl, BNordlund, AThe Background in Flow Measurement using Pulsed Neutron ActivationDetectors and Experimental TechniquesIn flow measurement with Pulsed Neutron Activation (PNA), water flowing in a pipe is activated with 14 MeV neutrons, producing the radioactive nuclide sup 1 sup 6 N. The gamma radiation emitted from this radionuclide will produce a characteristic peak in a time spectrum from a detector downstream. Experiments have shown that the peak is superimposed on a background distribution, which can affect the measurement. As it is necessary to correct for the background, different subtraction methods have been used in the past, although the origin of the background has not been known. In this work the source of the background has been investigated. It has been found that there are two components of the background: one time dependent and one time independent. The time-dependent component is shown to be caused by stationary sup 1 sup 6 N in the surroundings. A method for subtracting the background in a reproducible way has been developed. This was done by fitting the peak with an empirical function consisting of several Taylor distributionsCTH-RF-170oai:cds.cern.ch:7472762003
spellingShingle Detectors and Experimental Techniques
Mattsson, H
Dahl, B
Nordlund, A
The Background in Flow Measurement using Pulsed Neutron Activation
title The Background in Flow Measurement using Pulsed Neutron Activation
title_full The Background in Flow Measurement using Pulsed Neutron Activation
title_fullStr The Background in Flow Measurement using Pulsed Neutron Activation
title_full_unstemmed The Background in Flow Measurement using Pulsed Neutron Activation
title_short The Background in Flow Measurement using Pulsed Neutron Activation
title_sort background in flow measurement using pulsed neutron activation
topic Detectors and Experimental Techniques
url http://cds.cern.ch/record/747276
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