Neutrons are not easily detected with high resolution and good efficiency. Consequently high-quality neutron detectors remain a challenge to manufacture. A few nuclides such as He-3, Boron-10, and Li-6 are commonly used to convert impinging neutrons into an electrical pulse that post-processing electronics can cope with. The two most commonly used neutron position-sensitive detectors are a 3He proportional counter and a ZnS/6LiF scintillator. The first has, perhaps, the highest detection efficiency, but is costly to make, and the resolution is relatively poor. The latter has better spatial resolution, but suffers as an optimal solution as the afterglow in a scintillator can last for up to 10 microseconds, making it unsuitable for any high count-event application. The neutron-active surface of a straw detector is sputter coated with enriched boron carbide (10B 4C). In operation, two highly energetic charged particles are generated by neutron capture. One of those two particles must escape the deposit and ionize gas within the hollow straw. A pulse signal is read out via the suspended wire running through the center of the straw. Many straws are close packed into a 2D array that forms the large-area neutron position-sensitive detector. (Figure 1)
The balloon illustrates the boron-10 reaction. The atomic thickness of the 10B4C coating applied to the straw strongly influences detector efficiency and overall performance. The 10B4C must be sufficiently thin to permit the efficient escape of one or the other reaction product emitted upon each neutron reaction with a 10B atom. Otherwise, the event is lost in self absorption. Furthermore, if the film was too thick, remaining neutrons could not continue along their trajectory to the next straw, leading to another inefficient loss. Obviously, the accurate determination of boron depth distribution (stoichiometry) and total mass – not linear thickness - of this thin (≈ 1μm) lining is critical in the manufacture of straw elements. The required metrology is readily achieved using NDP. Sample coupons were selected representing material along the length and width of the 10B4C deposition chamber. NDP spectra were then determined from each sample; three spectra are overlaid and presented in Figure 2 illustrating the variations in the atomic thickness of boron found. NDP results revealed that the masks used in applying the film yielded a smoothly varying thickness in coating across the chamber (see Figure 3). Using the metrology provided by NDP, a practical and reliable approach to compensate the deposition mask was provided as determined in subsequent production runs.