“…Conventional APDs are defined as APDs in which multiplication occurs only within the depletion region of a simple p-i-n bulk semiconductor diode. Additionally, the noise properties of superlattice APDs have been examined by Teich et al [9,14,20], Matsuo et al [21], Kahraman et al [22], Hakim et al [23], Chakrabarti et al [24], Fyath et al [25,26] Van der Ziel et al [27], and Rajamani et al [28]. Superlattice APDs (SAPDs) [29] are comprised of alternating layers of variable bandgap semiconductors.…”
Section: Noise Properties Of Apdsmentioning
confidence: 98%
“…Several authors [22,[47][48][49][50][51][52][53][54][55][56][57][58][59][60][61] have investigated the frequency response of APDs when both carriers contribute to the ionization process. Kahraman et al [22] have developed an analysis, based on the numerical solution of the coupled transport equations, that enables the calculation of the time response of APDs of arbitrary structure. They have found that the speed of an APD is governed by the response time, not the carrier transit time.…”
“…Conventional APDs are defined as APDs in which multiplication occurs only within the depletion region of a simple p-i-n bulk semiconductor diode. Additionally, the noise properties of superlattice APDs have been examined by Teich et al [9,14,20], Matsuo et al [21], Kahraman et al [22], Hakim et al [23], Chakrabarti et al [24], Fyath et al [25,26] Van der Ziel et al [27], and Rajamani et al [28]. Superlattice APDs (SAPDs) [29] are comprised of alternating layers of variable bandgap semiconductors.…”
Section: Noise Properties Of Apdsmentioning
confidence: 98%
“…Several authors [22,[47][48][49][50][51][52][53][54][55][56][57][58][59][60][61] have investigated the frequency response of APDs when both carriers contribute to the ionization process. Kahraman et al [22] have developed an analysis, based on the numerical solution of the coupled transport equations, that enables the calculation of the time response of APDs of arbitrary structure. They have found that the speed of an APD is governed by the response time, not the carrier transit time.…”
“…However, calculation of the second-order statistics of the impulse-response function are generally computationally intensive, with no known closed-form expressions available [15], [28]. As a result, simplifying assumptions that ignore the randomness in the shape of the impulse-response function are often practiced in the calculation of the photocurrent variance.…”
Abstract-This paper reports a novel recurrence theory that enables us to calculate the exact joint probability density function (pdf) of the random gain and the random avalanche buildup time in avalanche photodiodes (
“…Hollenhorst introduced the transfer-matrix model to calculate steady-state gain and the excess noise factor for arbitrary APD structures [19]. Kahraman et al developed a more general matrix approach to analyze the frequency response of an APD with arbitrary structure [20]. In Hollenhorst's model, the device is divided into multiple layers that can each be approximated to have uniform electric fields.…”
Abstract-Previously, it has been demonstrated that resonantcavity-enhanced separate-absorption-and-multiplication (SAM) avalanche photodiodes (APD's) can achieve high bandwidths and high gain-bandwidth products while maintaining good quantum efficiency. In this paper, we describe a GaAs-based resonant-cavity-enhanced SAM APD that utilizes a thin charge layer for improved control of the electric field profile. These devices have shown RC-limited bandwidths above 30 GHz at low gains and gain-bandwidth products as high as 290 GHz. In order to gain insight into the performance of these APD's, homojunction APD's with thin multiplication regions were studied. It was found that the gain and noise have a dependence on the width of the multiplication region that is not predicted by conventional models. Calculations using width-dependent ionization coefficients provide good fits to the measured results. These calculations indicate that the gain-bandwidth product depends strongly on the charge layer doping and on the multiplication layer thickness and, further, that even higher gain-bandwidth products can be achieved with optimized structures.
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