遇见数据集

Long-term Increase in Equatorial Rayleigh-Taylor Instability: Synergistic Effects of Greenhouse Gas Cooling and Geomagnetic Field Secular Variation

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Mendeley Data2026-07-02 收录
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1. Five JPEG image files These are the figures in the paper. 2. Five IDL programs that plot the figures. 3. IDL sav data: These data are in IDL sav format. RTI_1965_2014_combined_case1.sav: equatorial fieldline integrated Rayleigh–Taylor Instability (RTI); ratio of F-region Pedersen conductivity to the total; plasma-drift in the magnetic meridian plane and perpendicular to the magnetic field (positive upward/outward), field (positive upward/outward); corresponding neutral-wind component (positive upward/outward); the effective gravity–collision term (scalar magnitude); the normalized plasma density gradient; the effective recombination rate, simulated by WACCM-X, driven by greenhouse gas forcing alone; RTI_1965_2014_combined_case2.sav: equatorial fieldline integrated Rayleigh–Taylor Instability (RTI); ratio of F-region Pedersen conductivity to the total; plasma-drift in the magnetic meridian plane and perpendicular to the magnetic field (positive upward/outward), field (positive upward/outward); corresponding neutral-wind component (positive upward/outward); the effective gravity–collision term (scalar magnitude); the normalized plasma density gradient; the effective recombination rate, simulated by WACCM-X, driven by greenhouse gas forcing and secular change of the earth's magnetic field.

1. 五份JPEG图像文件(JPEG):对应论文中的附图。 2. 五份用于绘制上述附图的IDL程序(IDL)。 3. IDL sav格式数据集: 所有数据均采用IDL sav格式存储,具体包含以下两个数据文件: RTI_1965_2014_combined_case1.sav:包含赤道磁力线积分瑞利-泰勒不稳定性(Rayleigh–Taylor Instability,RTI);F区佩德森电导率与总电导率的比值;磁子午面内且垂直于磁场的等离子体漂移(正向向上/向外)、磁场(正向向上/向外);对应的中性风分量(正向向上/向外);有效重力碰撞项(标量幅值);归一化等离子体密度梯度;由仅受温室气体强迫驱动的WACCM-X模拟得到的有效复合率。 RTI_1965_2014_combined_case2.sav:包含赤道磁力线积分瑞利-泰勒不稳定性(Rayleigh–Taylor Instability,RTI);F区佩德森电导率与总电导率的比值;磁子午面内且垂直于磁场的等离子体漂移(正向向上/向外)、磁场(正向向上/向外);对应的中性风分量(正向向上/向外);有效重力碰撞项(标量幅值);归一化等离子体密度梯度;由WACCM-X模拟得到的有效复合率,该模拟同时受温室气体强迫与地球磁场长期变化共同驱动。

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2026-06-18
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