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Articles

A new neutron depth profiling spectrometer at the JCNS for a focused neutron beam

, , , , , , , , , , , & show all
Pages 342-355 | Received 28 Jun 2019, Accepted 14 Oct 2019, Published online: 30 Mar 2020

Figures & data

Figure 1. CAD drawing of the JCNS NDP chamber installed on the sample table of reflectometer MARIA. Cut-view.

Figure 1. CAD drawing of the JCNS NDP chamber installed on the sample table of reflectometer MARIA. Cut-view.

Figure 2. NDP spectrometer installed at the sample position of the reflectometer TREFF.

Figure 2. NDP spectrometer installed at the sample position of the reflectometer TREFF.

Figure 3. The interior of the NDP sample chamber with standard sample holder and single detector. Radiation shielding is removed for visibility.

Figure 3. The interior of the NDP sample chamber with standard sample holder and single detector. Radiation shielding is removed for visibility.

Figure 4. A block diagram of the detector signal readout chain of JCNS NDP spectrometer.

Figure 4. A block diagram of the detector signal readout chain of JCNS NDP spectrometer.

Figure 5. Spectrum collected from a 3 kBq mixed α-particle source (239 Pu, 241 Am,244 Cm) with 30 mm sample to detector distance.

Figure 5. Spectrum collected from a 3 kBq mixed α-particle source (239 Pu, 241 Am,244 Cm) with 30 mm sample to detector distance.

Figure 6. Spectrum collected from SRM–93a borosilicate glass. Highest energies (particles from the sample surface) are marked with dashed lines.

Figure 6. Spectrum collected from SRM–93a borosilicate glass. Highest energies (particles from the sample surface) are marked with dashed lines.

Figure 7. Inverted first derivative of the energy edge 1472 keV. Represents energy resolution of the NDP detectors system.

Figure 7. Inverted first derivative of the energy edge 1472 keV. Represents energy resolution of the NDP detectors system.

Figure 8. Achievable depth resolution for the 100 nm LiCoO2 thin film.

Figure 8. Achievable depth resolution for the 100 nm LiCoO2 thin film.

Figure 9. α-signal collected from 15 nm thick 6LiNbO3 thin film (circles) and a fit (solid line).

Figure 9. α-signal collected from 15 nm thick 6LiNbO3 thin film (circles) and a fit (solid line).

Figure 10. Unfolded NDP spectrum of SRM–2137 collected on MARIA in roughly 14h. Solid line – certified values, dots – as measured.

Figure 10. Unfolded NDP spectrum of SRM–2137 collected on MARIA in roughly 14h. Solid line – certified values, dots – as measured.

Figure 11. α-peak region of the smoothed spectrum collected for multilayer thin-film sample 6LiNbO3/Si/natLiNbO3.

Figure 11. α-peak region of the smoothed spectrum collected for multilayer thin-film sample 6LiNbO3/Si/natLiNbO3.

Figure 12. Smoothed spectra collected on MARIA in 90 minutes for thin films – single film Li4Ti5O12 (LTO) and double layer films Li4Ti5O12/Li3PO4 (LTO–LPO).

Figure 12. Smoothed spectra collected on MARIA in 90 minutes for thin films – single film Li4Ti5O12 (LTO) and double layer films Li4Ti5O12/Li3PO4 (LTO–LPO).

Figure 13. Unfolded Li depth profile (in relative units) of Li4Ti5O12/Li3PO4 film.

Figure 13. Unfolded Li depth profile (in relative units) of Li4Ti5O12/Li3PO4 film.

Figure 14. Smoothed spectra collected on MARIA for Li4Ti5O12(190nm)Li3PO4(180nm) sample (LTO–LPO).

Figure 14. Smoothed spectra collected on MARIA for Li4Ti5O12(190nm)−Li3PO4(180nm) sample (LTO–LPO).