Ultra-thin corrugated metamaterial film as large-area transmission dynode

被引:2
|
作者
Chan, H. W. [1 ,2 ]
Prodanovic, V [1 ,2 ]
Theulings, A. M. M. G. [3 ]
ten Bruggencate, T. [2 ]
Hagen, C. W. [3 ]
Sarro, P. M. [2 ]
v d Graaf, H. [1 ]
机构
[1] Natl Inst Subat Phys NIKHEF, Sci Pk 105, NL-1098 XG Amsterdam, Netherlands
[2] Delft Univ Technol, Fac Elect Engn Math & Comp Sci, Dept Microelect, ECTM, Feldmannweg 17, NL-2628 CT Delft, Netherlands
[3] Delft Univ Technol, Fac Appl Sci, Dept Imaging Phys, Lorentzweg 1, NL-2628 CJ Delft, Netherlands
关键词
Secondary electron emitters and dynodes and their production; Avalanche-induced secondary effects; Electron multipliers (vacuum);
D O I
10.1088/1748-0221/17/09/P09027
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
Large-area transmission dynodes were fabricated by depositing an ultra-thin continuous film on a silicon wafer with a 3-dimensional pattern. After removing the silicon, a corrugated membrane with enhanced mechanical properties was formed. Mechanical metamaterials, such as this corrugated membrane, are engineered to improve its strength and robustness, which allows it to span a larger surface in comparison to flat membranes while the film thickness remains constant. The ultra-thin film consists of three layers (Al2O3/TiN/Al2O3) and is deposited by atomic layer deposition (ALD). The encapsulated TiN layer provides in-plane conductivity, which is needed to sustain secondary electron emission. Two types of corrugated membranes were fabricated: a hexagonal honeycomb and an octagonal pattern. The latter was designed to match the square pitch of a CMOS pixel chip. The transmission secondary electron yieldwas determined with a collector-based method using a scanning electron microscope. The highest transmission electron yield was measured on a membrane with an octagonal pattern. A yield of 2.15 was achieved for 3.15 keV incident electrons for an Al2O3/TiN/Al2O3 tri-layer film with layer thicknesses of 10/5/15 nm. The variation in yield across the surface of the corrugated membrane was determined by constructing a yield map. The active surface for transmission secondary electron emission is near 100%, i.e. a primary electron generates transmission secondary electrons regardless of the point of impact on the corrugated membrane.
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页数:23
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