2019
DOI: 10.1063/1.5084689
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A single crystal CVD diamond x-ray beam diagnostic with embedded graphitic wire electrodes

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Cited by 3 publications
(3 citation statements)
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“…For example, for spectrometric charged particle detectors on alternating current (AC) single‐crystal CVD diamond, an energy resolution of 0.27% has been achieved at the 5.489 MeV Am α‐line . Today, based on CVD diamond, the high‐efficiency thermal and fast neutron detectors are produced based on CVD diamond; microstrip, pixel, and 3D detectors for high‐energy physics and other fields are also being actively developed …”
Section: Introductionmentioning
confidence: 99%
“…For example, for spectrometric charged particle detectors on alternating current (AC) single‐crystal CVD diamond, an energy resolution of 0.27% has been achieved at the 5.489 MeV Am α‐line . Today, based on CVD diamond, the high‐efficiency thermal and fast neutron detectors are produced based on CVD diamond; microstrip, pixel, and 3D detectors for high‐energy physics and other fields are also being actively developed …”
Section: Introductionmentioning
confidence: 99%
“…Highly localised and geometrically confined structural transformations in diamond with intrinsic sp 3 diamond's tetrahedral phase converted into sp 2 -rich graphitic fraction employing a laser light have shown to significantly enhance light absorption in the irradiated areas and, to open a new avenue for the emerging opto-photonic applications, including miniaturised thermionic solar cells 1 , broad-beam light detectors [2][3] and most recently, robust broad-beam polarization filters for infra-red (IR) applications 4 . These applications, however, may only become technologically accomplishable once the thermal stresses associated with laser processing and the formation of sp 2 fraction on the surface or in the bulk of the diamond crystal, are minimised while remaining spatially confined.…”
mentioning
confidence: 99%
“…These applications, however, may only become technologically accomplishable once the thermal stresses associated with laser processing and the formation of sp 2 fraction on the surface or in the bulk of the diamond crystal, are minimised while remaining spatially confined. Additionally, owing to a close lattice match between the diamond's sp 3 tetrahedral fraction and the planar two-dimensional (2D) graphene and graphite structures, direct fabrication of 'graphene-on-diamond' heterostructures by means of an in situ sp 3 -to-sp 2 conversion enables a development of a variety of robust ultra-wide bandgap 'all carbon' opto-electronic devices in a single-step fabrication process, without resorting to processes that normally require high-temperature annealing with a metal catalyst. [5][6] Conventional nano-(ns-) and pico-(ps-) second pulsed lasers transform diamond into graphite by means of a localised phonon-induced graphitization and, owing to their long laser-lattice interactions, primarily an amorphous sp 2 phase is formed in the heat affected zone (HAZ) marked by the appearance of thermally-induced cracks.…”
mentioning
confidence: 99%