2012
DOI: 10.1016/j.nima.2011.12.018
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Design of a new time-of-flight small-angle neutron scattering instrument at CPHS

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Cited by 13 publications
(7 citation statements)
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“…For a large source size and small pinhole size, a distribution of pinholes based on a hexagonal array pattern is most widely used since it maximizes the number of pinholes in a given area (Chaboussant et al, 2012;Brû let et al, 2008;Dé sert et al, 2007). However, for the CPHS-SANS instrument, since the size of the moderator source is 11 Â 11 cm, while Q min is set at approximately 0.007 Å À1 (Huang et al, 2012), the best pinhole distribution is a nine-pinhole structure which forms a square array. Compared with a seven-pinhole structure with a hexagonal array (Glinka et al, 1986), the nine-pinhole structure with a square shape increases the beam intensity by a ratio of 9:7 in the case of uniform source distribution for a larger sample size.…”
Section: Crosstalk Of a Multi-pinhole Collimation Systemmentioning
confidence: 99%
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“…For a large source size and small pinhole size, a distribution of pinholes based on a hexagonal array pattern is most widely used since it maximizes the number of pinholes in a given area (Chaboussant et al, 2012;Brû let et al, 2008;Dé sert et al, 2007). However, for the CPHS-SANS instrument, since the size of the moderator source is 11 Â 11 cm, while Q min is set at approximately 0.007 Å À1 (Huang et al, 2012), the best pinhole distribution is a nine-pinhole structure which forms a square array. Compared with a seven-pinhole structure with a hexagonal array (Glinka et al, 1986), the nine-pinhole structure with a square shape increases the beam intensity by a ratio of 9:7 in the case of uniform source distribution for a larger sample size.…”
Section: Crosstalk Of a Multi-pinhole Collimation Systemmentioning
confidence: 99%
“…Although the Q resolution and Q min are both important parameters that ensure the availability of a suitable Q range for the detailed examination of the structure of a sample, the beam intensity, which is equal to the product of the flux at the sample and the sample size, is crucial since it determines the measurement time required to achieve good statistics during sample analysis. The Compact Pulsed Hadron Source (CPHS) at Tsinghua University is a proton accelerator based neutron source (Wang et al, 2014;Huang et al, 2012). As a compact source, the neutron flux delivered is much lower than that of other large sources.…”
Section: Introductionmentioning
confidence: 99%
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“…We plan to resolve these technical issues step-by-step, beginning with 3-MeV protons on a water-cooled, thin Be target with a room-temperature polyethylene moderator and gradually gain experiences for reliable operation and extend to higher proton energies and cold-neutron production. [4] Two neutron beams are to be built for imaging-the NIRS and small-angle scattering-the SANS. This corresponds to two PhD thesis projects, respectively, for S. F. Su of Sun Yat-Sen University and T.C.…”
Section: Neutron Target Stationmentioning
confidence: 99%
“…Figure 1 shows the setup of the IS, LEBT, and RFQ segments. [Huang et al (2012)] Two neutron beams are to be built for imagingthe NIRS and small-angle scatteringthe SANS. This corresponds to two PhD thesis projects, respectively, for S. F. Su of Sun Yat-Sen University and T.C.…”
Section: Progress In 2010-2012mentioning
confidence: 99%