2010
DOI: 10.1051/sfn/201011004
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Bonnes pratiques de la diffusion de neutrons aux petits angles

Abstract: Résumé. Conceptuellement, une expérience de diffusion de rayonnement donne accès à la densité spectrale de puissance de la densité de longueur de diffusion d'un échantillon (ou section efficace différentielle de diffusion). Cette grandeur s'exprime en cm 2 .Ce cours se veut un guide pratique et explicatif de la réalisation d'une expérience sur un spectromètre de diffusion de neutrons aux petits angles. Dans un premier temps le vocabulaire est précisé. Les notions de cohérence du faisceau en relation avec la ré… Show more

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Cited by 3 publications
(6 citation statements)
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“…The neutrons of different wavelengths are then separated through their speed, the fastest neutrons moving faster than the slower ones. It method enables to work with a good resolution (35) (36). It is obviously suited to pulsed sources (spallation sources) and is lead to develop since all new modern bright sources are spallation sources.…”
Section: Spectrometersmentioning
confidence: 99%
See 1 more Smart Citation
“…The neutrons of different wavelengths are then separated through their speed, the fastest neutrons moving faster than the slower ones. It method enables to work with a good resolution (35) (36). It is obviously suited to pulsed sources (spallation sources) and is lead to develop since all new modern bright sources are spallation sources.…”
Section: Spectrometersmentioning
confidence: 99%
“…It immediately appears that taking away the detector from the sample strongly decreases J because the solid angle is decreased (∝1/ D sample-detector 2 ) and because the collimation must be more accurate. It could be demonstrated that the flux corresponding to the optimized collimation varies like J 0 4 (36). J 0 ( ) has a Maxwellian shape because it corresponds to the thermalization of a perfect gas of neutrons at the temperature of the cold source moderator and follows the Maxwell-Boltzmann statistics P( ) = exp(−( therm / ) 2 ) × −4 ; where therm is the thermal length.…”
Section: Choosing Its Configuration For An Experimentsmentioning
confidence: 99%
“…It immediately appears that taking away the detector from the sample strongly decreases J because the solid angle is decreased (∝1/ D sample-detector 2 ) and because the collimation must be more accurate. It could be demonstrated that the flux corresponding to the optimized collimation varies like J 0 4 (36). J 0 ( ) has a Maxwellian shape because it corresponds to the thermalization of a perfect gas of neutrons at the temperature of the cold source moderator and follows the Maxwell-Boltzmann statistics P( ) = exp(−( therm / )…”
Section: Choosing Its Configuration For An Experimentsmentioning
confidence: 99%
“…The efficiency of the detector increases with the wavelength ( ( ) = 1 − e − / c where c is a critical value that is dependent on the detector used). Altogether, the combination of the effects of J 0 ( ) and ( ) provides an usable flux J use ( ) that an asymmetric shape, a maximum max (around 3-4Å on the SANS machines at LLB) and a raw decay like −4 for large q above max (the decay to the shortest wavelengths below is very sharp, anyway the short wavelength are not useful for SANS) (36). For a given targeted q-range corresponding to one configuration, there is always a set of ( , D sample-detector ) that optimizes the flux.…”
Section: Choosing Its Configuration For An Experimentsmentioning
confidence: 99%
See 1 more Smart Citation