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Measuring temperature effects on nano-bubble growth in tungsten with grazing incidence small angle X-ray scattering

机译:用掠入射小角X射线散射测量温度对钨纳米气泡生长的影响

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Highlights ? W samples were exposed to He plasma in the MAGPIE, NAGDIS-II and PISCES-A across a range of sample temperatures between 473–1123K. ? GISAXS was used to quantify the effect of plasma fluence and W surface temperature on He nano-bubble size distributions. ? In NAGDIS-II at 873K and Pisces-A at 643–673K, nano-bubbles are exponentially distributed with mean diameters μ ≈ 0.5 nm. ? Above ~900K nano-bubbles followed an approximately exponential distribution with μ > 0.65 nm demonstrating a significant increase in nano-bubble sizes at higher temperatures. Abstract W samples were exposed to He plasma in the MAGPIE, NAGDIS-II and PISCES-A across a range of sample temperatures between 473–1123K. GISAXS was used to quantify the effect of plasma fluence and W surface temperature on He nano-bubble size distributions. In NAGDIS-II at 873K nano-bubbles are exponentially distributed with mean diameters μ = 0.64 ± 0.01 nm , similar to the value of μ = 0.62 ± 0.01 nm found for the MAGPIE plasma device at the much lower temperature of 473K. Above ~900K nano-bubbles followed an approximately exponential distribution with μ > 0.72?nm?demonstrating a significant increase in nano-bubble sizes at higher temperatures.
机译:强调 ?在473-1123K的样品温度范围内,W样品在MAGPIE,NAGDIS-II和PISCES-A中暴露于He等离子体。 ? GISAXS用于量化等离子通量和W表面温度对He纳米气泡尺寸分布的影响。 ?在873K的NAGDIS-II和643-673K的双鱼座-A中,纳米气泡以平均直径μ≈0.5 nm呈指数分布。 ?在〜900K以上,纳米气泡呈指数分布,μ> 0.65 nm,表明在较高温度下纳米气泡尺寸显着增加。摘要在473-1123K的样品温度范围内,在MAGPIE,NAGDIS-II和PISCES-A中将W样品暴露于He等离子体。 GISAXS用于量化等离子通量和W表面温度对He纳米气泡尺寸分布的影响。在NAGDIS-II中,在873K处,纳米气泡呈指数分布,平均直径μ= 0.64±0.01 nm,与在低得多的473K温度下MAGPIE等离子设备发现的μ= 0.62±0.01 nm的值相似。在〜900K以上,纳米气泡呈指数分布,μ> 0.72?nm ?,表明在较高温度下纳米气泡尺寸显着增加。

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