“…Figure 4 shows the frequency of arcing, f arc , defined as the number of arc occurrence per an hour as a function of the bias voltage for different plasma conditions. When samples were exposed to a pure He plasma without any pre-treatment, f arc was always 0 at the bias voltage range of −150 to −250 V. When Ne was seeded, arcs were not detected at −150 V, but triggered at −200 V and f arc became greater as the bias voltage deepened to −250 V. It is thought that the field emission from the tip of NTBs was enhanced, hence increased chance in transit to breakdown [10]. When Ar was seeded, the arcing occurred at −150 V, likely due to the presence of NTBs on this condition.…”
Section: Frequency Of Arc Occurrence At Various Conditionsmentioning
confidence: 99%
“…Considering that no NTB formation is anticipated on a surface with a pure He plasma exposure, this also suggests that NTBs, which have already grown on the surface, trigger arcing with ease. It is known that the onset of field electron emission on NTBs is on the order of ∼1 kV/mm depending on their shapes [10], which is much lower than that on fuzzy surface (∼7 kV/mm) [13]. It implies that the breakdown could be initiated by the onset of field electron emission from the tip of NTBs and lead to arcing.…”
Section: Frequency Of Arc Occurrence At Various Conditionsmentioning
confidence: 99%
“…This implies that there is a possibility of NTBs formation on the ITER divertor. The field electron emission measurements from NTBs showed that the NTBs can be a trigger of arc ignition with greater possibility compared to fuzz [10], whereas detailed conditions for arc ignition on such NTBs surfaces have not been investigated.…”
Arcing was ignited on deformed tungsten (W) surfaces, where W fuzz and/or nano-tendril bundles (NTBs) were grown, by steady state helium (He) plasma exposures with impurity gas seeding. At the same sample potential of −250 V, the presence of NTBs enhanced the frequency of arc ignition, whereas no arc ignition appeared on typical fuzz surfaces without NTBs. After a series of arc ignitions on a sample surface with NTBs, the aspect ratio of NTBs decreased, indicating that protruded NTBs with larger aspect ratio tend to trigger arcing easily.
“…Figure 4 shows the frequency of arcing, f arc , defined as the number of arc occurrence per an hour as a function of the bias voltage for different plasma conditions. When samples were exposed to a pure He plasma without any pre-treatment, f arc was always 0 at the bias voltage range of −150 to −250 V. When Ne was seeded, arcs were not detected at −150 V, but triggered at −200 V and f arc became greater as the bias voltage deepened to −250 V. It is thought that the field emission from the tip of NTBs was enhanced, hence increased chance in transit to breakdown [10]. When Ar was seeded, the arcing occurred at −150 V, likely due to the presence of NTBs on this condition.…”
Section: Frequency Of Arc Occurrence At Various Conditionsmentioning
confidence: 99%
“…Considering that no NTB formation is anticipated on a surface with a pure He plasma exposure, this also suggests that NTBs, which have already grown on the surface, trigger arcing with ease. It is known that the onset of field electron emission on NTBs is on the order of ∼1 kV/mm depending on their shapes [10], which is much lower than that on fuzzy surface (∼7 kV/mm) [13]. It implies that the breakdown could be initiated by the onset of field electron emission from the tip of NTBs and lead to arcing.…”
Section: Frequency Of Arc Occurrence At Various Conditionsmentioning
confidence: 99%
“…This implies that there is a possibility of NTBs formation on the ITER divertor. The field electron emission measurements from NTBs showed that the NTBs can be a trigger of arc ignition with greater possibility compared to fuzz [10], whereas detailed conditions for arc ignition on such NTBs surfaces have not been investigated.…”
Arcing was ignited on deformed tungsten (W) surfaces, where W fuzz and/or nano-tendril bundles (NTBs) were grown, by steady state helium (He) plasma exposures with impurity gas seeding. At the same sample potential of −250 V, the presence of NTBs enhanced the frequency of arc ignition, whereas no arc ignition appeared on typical fuzz surfaces without NTBs. After a series of arc ignitions on a sample surface with NTBs, the aspect ratio of NTBs decreased, indicating that protruded NTBs with larger aspect ratio tend to trigger arcing easily.
“…The necessary condition for fuzz growth could be satisfied around the strike point in the ITER divertor 7 . There are concerns about fuzz formation in fusion reactors, which leads to the significantly reduced thermal resistance 8 and increased field electron emission [9][10][11] , may lead to the initiation of arcing and the release of large amounts of W 5,[12][13][14] .…”
When tungsten (W) is deposited with helium (He) plasma (He-W co-deposition) on W surface, enhanced growth of fiberform nanostructure (fuzz) occurs, and sometimes it grows into large-scale fuzzy nanostructures (LFNs) thicker than 0.1~mm.In this study, different numbers of mesh openings (apertures) and W plates with nanotendril bundles (NTBs), which are tens of micrometers high nanofiber bundles, were used to investigate the condition for the origin of the LFN growth.It was found that the larger the mesh openings, the larger the area where LFNs are formed and the faster the formation tends to be. On NTB samples, it was found that NTBs grew significantly when exposed to He plasma with W deposition, especially when the size of the NTB reached $\sim$0.1~mm. The concentration of the He flux due to the distortion of the shape of the ion sheath is proposed as one of the reasons to explain the experimental results.
“…The necessary condition for fuzz growth could be satisfied around the strike point in the ITER divertor 7 . There are concerns about fuzz formation in fusion reactors, which leads to the significantly reduced thermal resistance 8 and increased field electron emission [9][10][11] . This may lead to the initiation of arcing and the release of large amounts of W 5,[12][13][14] .…”
When tungsten (W) is deposited with helium (He) plasma (He–W co-deposition) on W surface, enhanced growth of fiberform nanostructure (fuzz) occurs, and sometimes it grows into large-scale fuzzy nanostructures (LFNs) thicker than 0.1 mm. In this study, different numbers of mesh opening (apertures) and W plates with nanotendril bundles (NTBs), which are tens of micrometers high nanofiber bundles, were used to investigate the condition for the origin of the LFN growth. It was found that the larger the mesh opening, the larger the area where LFNs are formed and the faster the formation tends to be. On NTB samples, it was found that NTBs grew significantly when exposed to He plasma with W deposition, especially when the size of the NTB reached $$\sim 0.1$$
∼
0.1
mm. The concentration of the He flux due to the distortion of the shape of the ion sheath is proposed as one of the reasons to explain the experimental results.
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