Total neutron cross section for 181Ta

The neutron time of flight facility nELBE, produces fast neutrons in the energy range from 0.1 MeV to 10 MeV by impinging a pulsed relativistic electron beam on a liquid lead circuit [1]. The short beam pulses (∼10 ps) and a small radiator volume give an energy resolution better than 1% at 1 MeV usi...
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Autor*in:	Schilling K.-D. [verfasserIn] Nolte R. [verfasserIn] Mosconi M. [verfasserIn] Kögler T. [verfasserIn] Massarczyk R. [verfasserIn] Junghans A. [verfasserIn] Hannaske R. [verfasserIn] Grosse E. [verfasserIn] Ferrari A. [verfasserIn] Birgersson E. [verfasserIn] Beyer R. [verfasserIn] Matić A. [verfasserIn] Schwengner R. [verfasserIn] Wagner A. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2010

Übergeordnetes Werk:	In: EPJ Web of Conferences - EDP Sciences, 2010, 8, p 07006(2010)
Übergeordnetes Werk:	volume:8, p 07006 ; year:2010

Links:	Link aufrufen Link aufrufen Link aufrufen Journal toc

DOI / URN:	10.1051/epjconf/20100807006

Katalog-ID:	DOAJ019209215

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allfieldsSound	10.1051/epjconf/20100807006 doi (DE-627)DOAJ019209215 (DE-599)DOAJ6083b7b76a5240329359c347a36606b0 DE-627 ger DE-627 rakwb eng QC1-999 Schilling K.-D. verfasserin aut Total neutron cross section for 181Ta 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The neutron time of flight facility nELBE, produces fast neutrons in the energy range from 0.1 MeV to 10 MeV by impinging a pulsed relativistic electron beam on a liquid lead circuit [1]. The short beam pulses (∼10 ps) and a small radiator volume give an energy resolution better than 1% at 1 MeV using a short flight path of about 6 m, for neutron TOF measurements. The present neutron source provides 2 ⋅ 104 n/cm2s at the target position using an electron charge of 77 pC and 100 kHz pulse repetition rate. This neutron intensity enables to measure neutron total cross section with a 2%–5% statistical uncertainty within a few days. In February 2008, neutron radiator, plastic detector [2] and data acquisition system were tested by measurements of the neutron total cross section for 181Ta and 27Al. Measurement of 181Ta was chosen because lack of high quality data in an anergy region below 700 keV. The total neutron cross – section for 27Al was measured as a control target, since there exists data for 27Al with high resolution and low statistical error [3]. Physics Nolte R. verfasserin aut Mosconi M. verfasserin aut Kögler T. verfasserin aut Massarczyk R. verfasserin aut Junghans A. verfasserin aut Hannaske R. verfasserin aut Grosse E. verfasserin aut Ferrari A. verfasserin aut Birgersson E. verfasserin aut Beyer R. verfasserin aut Matić A. verfasserin aut Schwengner R. verfasserin aut Wagner A. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 8, p 07006(2010) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:8, p 07006 year:2010 https://doi.org/10.1051/epjconf/20100807006 kostenfrei https://doaj.org/article/6083b7b76a5240329359c347a36606b0 kostenfrei http://dx.doi.org/10.1051/epjconf/20100807006 kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 8, p 07006 2010
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callnumber-first	Q - Science
author	Schilling K.-D.
spellingShingle	Schilling K.-D. misc QC1-999 misc Physics Total neutron cross section for 181Ta
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topic_title	QC1-999 Total neutron cross section for 181Ta
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title	Total neutron cross section for 181Ta
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title_full	Total neutron cross section for 181Ta
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author_browse	Schilling K.-D. Nolte R. Mosconi M. Kögler T. Massarczyk R. Junghans A. Hannaske R. Grosse E. Ferrari A. Birgersson E. Beyer R. Matić A. Schwengner R. Wagner A.
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title_sort	total neutron cross section for 181ta
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title_auth	Total neutron cross section for 181Ta
abstract	The neutron time of flight facility nELBE, produces fast neutrons in the energy range from 0.1 MeV to 10 MeV by impinging a pulsed relativistic electron beam on a liquid lead circuit [1]. The short beam pulses (∼10 ps) and a small radiator volume give an energy resolution better than 1% at 1 MeV using a short flight path of about 6 m, for neutron TOF measurements. The present neutron source provides 2 ⋅ 104 n/cm2s at the target position using an electron charge of 77 pC and 100 kHz pulse repetition rate. This neutron intensity enables to measure neutron total cross section with a 2%–5% statistical uncertainty within a few days. In February 2008, neutron radiator, plastic detector [2] and data acquisition system were tested by measurements of the neutron total cross section for 181Ta and 27Al. Measurement of 181Ta was chosen because lack of high quality data in an anergy region below 700 keV. The total neutron cross – section for 27Al was measured as a control target, since there exists data for 27Al with high resolution and low statistical error [3].
abstractGer	The neutron time of flight facility nELBE, produces fast neutrons in the energy range from 0.1 MeV to 10 MeV by impinging a pulsed relativistic electron beam on a liquid lead circuit [1]. The short beam pulses (∼10 ps) and a small radiator volume give an energy resolution better than 1% at 1 MeV using a short flight path of about 6 m, for neutron TOF measurements. The present neutron source provides 2 ⋅ 104 n/cm2s at the target position using an electron charge of 77 pC and 100 kHz pulse repetition rate. This neutron intensity enables to measure neutron total cross section with a 2%–5% statistical uncertainty within a few days. In February 2008, neutron radiator, plastic detector [2] and data acquisition system were tested by measurements of the neutron total cross section for 181Ta and 27Al. Measurement of 181Ta was chosen because lack of high quality data in an anergy region below 700 keV. The total neutron cross – section for 27Al was measured as a control target, since there exists data for 27Al with high resolution and low statistical error [3].
abstract_unstemmed	The neutron time of flight facility nELBE, produces fast neutrons in the energy range from 0.1 MeV to 10 MeV by impinging a pulsed relativistic electron beam on a liquid lead circuit [1]. The short beam pulses (∼10 ps) and a small radiator volume give an energy resolution better than 1% at 1 MeV using a short flight path of about 6 m, for neutron TOF measurements. The present neutron source provides 2 ⋅ 104 n/cm2s at the target position using an electron charge of 77 pC and 100 kHz pulse repetition rate. This neutron intensity enables to measure neutron total cross section with a 2%–5% statistical uncertainty within a few days. In February 2008, neutron radiator, plastic detector [2] and data acquisition system were tested by measurements of the neutron total cross section for 181Ta and 27Al. Measurement of 181Ta was chosen because lack of high quality data in an anergy region below 700 keV. The total neutron cross – section for 27Al was measured as a control target, since there exists data for 27Al with high resolution and low statistical error [3].
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title_short	Total neutron cross section for 181Ta
url	https://doi.org/10.1051/epjconf/20100807006 https://doaj.org/article/6083b7b76a5240329359c347a36606b0 http://dx.doi.org/10.1051/epjconf/20100807006 https://doaj.org/toc/2100-014X
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