“…Due to the contemporary needs on the studies of nanogaps and short electron bunches, this 1D classical CL law has been extended to various regimes, including multi-dimensions, [3][4][5][6][7] quantum regime, 8,9 short pulse limit, 10,11 single-electron limit, 12 new scaling in other geometries 13 with applications in THz source 14,15 and time dependent current injection. [16][17][18] Electron emission from a sharp tip is important for many applications, such as vacuum microelectronics, 19 compact high current cathodes for high power microwave sources, [20][21][22] ultrafast laser induced electron emission from sharp tip, [23][24][25][26][27] ultrafast electron imaging, [28][29][30] laser-driven dielectric acceleration, 31,32 and high brightness photo-cathode 33,34 for X-ray free electron laser (FEL). For electron emission from a sharp tip, the localized electron density near to the tip is very high, which induces a space charge electric field, strong enough to modify the external applied electric field significantly, and thus to influence the field emission process.…”