1968
DOI: 10.1016/0020-0891(68)90034-1
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Photoelectrical properties of spherical avalanche diodes in silicon

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Cited by 12 publications
(7 citation statements)
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“…The so-called “spherical avalanche diode” seems to be the first APD intentionally designed using a non-planar approach [ 33 ]. The main idea of the design ( Figure 1 ) was to simultaneously achieve rather contradictory objectives: Uniformity of an avalanche multiplication over the sensitive region at the cone tip in the space angle ; Enhancement of an electric field at the cone tip to lower breakdown voltage; Protection from edge breakdown without guard ring structures; Reduction of an electric field at the surface of the silicon to lower dark current.…”
Section: Non-planar Apd and Sipm Designsmentioning
confidence: 99%
“…The so-called “spherical avalanche diode” seems to be the first APD intentionally designed using a non-planar approach [ 33 ]. The main idea of the design ( Figure 1 ) was to simultaneously achieve rather contradictory objectives: Uniformity of an avalanche multiplication over the sensitive region at the cone tip in the space angle ; Enhancement of an electric field at the cone tip to lower breakdown voltage; Protection from edge breakdown without guard ring structures; Reduction of an electric field at the surface of the silicon to lower dark current.…”
Section: Non-planar Apd and Sipm Designsmentioning
confidence: 99%
“…The ionization rate is approximated by the truncated Taylor series a(e) s a + o^E z (4) E-2 and (2) may then be used to obtain the continuity equations for the RF carrier densities expanded about E with E = E • z , and a. a' = da/de, evaluated at e = E . Equations (1) (6) where only first-order RF terms are retained, c = -a'(J + J )/q, and (5), (6), (10), and (11) constitute a complete set of equations. Equations (5) and (6) may be combined to…”
Section: Model and Basic Equationsmentioning
confidence: 99%
“…The most relevant examples are Geiger-Mode APDs developed as predecessors or alternatives to the planar SiPMs. Spherical avalanche diodes with a radius of the pn-junction of 2 µm and a breakdown voltage of 50 V seems to be the earliest device of this type operated in a photon counting mode [14]. Geiger-Mode APDs with negative feedback, also known as Metal-Resistor-Semiconductor (MRS) APDs, were designed as an array of avalanche micro-channels.…”
Section: Introductionmentioning
confidence: 99%