实时间接光泽反射效果有助于提高渲染场景的真实感.为了解决虚拟点光源(virtual point lights,VPLs)在光泽材质处的着色走样问题,提出基于VPLs光照贡献重要性的渲染算法.首先提出基于Tile的光照贡献估算方法,通过分块拟合和分块剔除快...实时间接光泽反射效果有助于提高渲染场景的真实感.为了解决虚拟点光源(virtual point lights,VPLs)在光泽材质处的着色走样问题,提出基于VPLs光照贡献重要性的渲染算法.首先提出基于Tile的光照贡献估算方法,通过分块拟合和分块剔除快速估算VPLs的光照贡献;然后通过自适应权重的时域复用方法,生成重要性驱动的分布图;最后结合Mipmap多级纹理映射技术,快速在场景的不同区域生成不同密度的VPLs.在金属戒指和斯坦福兔子等场景下的实验结果表明,使用相同数量的VPLs进行渲染,所提算法渲染质量优于随机光源裁剪算法,渲染结果的均方根误差不超过2%.展开更多
The neutron Doppler broadening in inertial confinement fusion has been acquired from the time of flight for the neutron, from which the fuel ion temperature can be derived. An ultrafast-quenched plastic scintillation ...The neutron Doppler broadening in inertial confinement fusion has been acquired from the time of flight for the neutron, from which the fuel ion temperature can be derived. An ultrafast-quenched plastic scintillation detector was used to measure the time of flight for the neutron at a low-imploded DT neutron yield (5×107-1×108) in the experiment performed on the Shenguang Ⅱ laser facility. The typical temperatures of ablating targets for indirect drive were around 2.8 keV and the uncertainties were ±30 % - ±40%. The detection efficiency of the detector for DT neutrons was calibrated at a K-400 accelerator. The time response function of the detection system was calibrated by imploded neutrons from a DT-filled capsule, which can be regarded as a S function pulsed neutron source due to its much narrower pulse width than that of the measured neutron time-of-flight spectrum.展开更多
文摘实时间接光泽反射效果有助于提高渲染场景的真实感.为了解决虚拟点光源(virtual point lights,VPLs)在光泽材质处的着色走样问题,提出基于VPLs光照贡献重要性的渲染算法.首先提出基于Tile的光照贡献估算方法,通过分块拟合和分块剔除快速估算VPLs的光照贡献;然后通过自适应权重的时域复用方法,生成重要性驱动的分布图;最后结合Mipmap多级纹理映射技术,快速在场景的不同区域生成不同密度的VPLs.在金属戒指和斯坦福兔子等场景下的实验结果表明,使用相同数量的VPLs进行渲染,所提算法渲染质量优于随机光源裁剪算法,渲染结果的均方根误差不超过2%.
基金The project supported by the National High Technology Development Program of China (No. 863-804-3)
文摘The neutron Doppler broadening in inertial confinement fusion has been acquired from the time of flight for the neutron, from which the fuel ion temperature can be derived. An ultrafast-quenched plastic scintillation detector was used to measure the time of flight for the neutron at a low-imploded DT neutron yield (5×107-1×108) in the experiment performed on the Shenguang Ⅱ laser facility. The typical temperatures of ablating targets for indirect drive were around 2.8 keV and the uncertainties were ±30 % - ±40%. The detection efficiency of the detector for DT neutrons was calibrated at a K-400 accelerator. The time response function of the detection system was calibrated by imploded neutrons from a DT-filled capsule, which can be regarded as a S function pulsed neutron source due to its much narrower pulse width than that of the measured neutron time-of-flight spectrum.
