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EIA JEP 151:2015

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EIA JEP 151:2015

Test Procedure for the Measurement of Terrestrial Cosmic Ray Induced Destructive Effects in Power Semiconductor Devices

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The main reason for accelerated testing is the requirement for power electronic devices for high reliability, according to the respective application, and, therefore, to attain very low failure rates. Without accelerated testing any experimental validation of such low failure rates would be impossible. Power electronic devices that are vulnerable to terrestrial cosmic radiation include power MOSFETs and JFETs, power diodes and IGBTs (Insulated Gate Bipolar Transistors), which are usually employed for power switching and power conversion. They also include GTOs (Gate Turn-Off Thyristors) and Thyristors. Power devices may be with or without control logic and the may be components of integrated circuit. The maximum rated blocking voltage is higher than 300V (see note 2). Power devices may be based on Si, SiC and GaN technologies. This test method defines the requirements and procedures for terrestrial destructive (see note 1) singleevent effects (SEE) for example, single-event breakdown (SEB), single-event latch-up (SEL) and singleevent gate rupture (SEGR) testing. It is valid when using an accelerator, generating a nucleon beam of either -- Mono-energetic protons or mono-energetic neutrons of at least 150 MeV energy, or -- Neutrons from a spallation spectrum with maximum energy of at least 150 MeV This test method does not apply to testing that uses beams with particles heavier than protons. This specific choice of nucleon beam energies is stipulated by the mechanism of power device failure due to terrestrial cosmic radiation. Terrestrial cosmic rays [4] result from extended air showers created by the collision of highly energetic particles of the primary (galactic) cosmic radiation and consist mostly of photons and electrons, muons, pions and nucleons, i.e., protons and neutrons. At sea level about 95% of the strongly interacting particles are neutrons. For SEB to occur in a power device, e.g. a power diode, a nuclear collision between a neutron or proton and a silicon nucleus has to create highly-ionizing spallation fragments which in turn will generate a dense plasma of electron-hole pairs within the semiconductor material. If the local plasma density is high enough this will initiate massive carrier multiplication by impact ionization. Resembling discharge in gases, a 'streamer' will sweep through the device which will be filled with carriers and short-circuited, as a consequence. Thermal destruction of the power device might ensue [5]. This mechanism is in contrast to the failure modes in microelectronic storage devices, SRAMs or DRAMs, where SEU are related to the radiation-induced charging or discharging of storage cells, and which are non-destructive. Accordingly, nucleon beam properties for accelerated testing against Soft Errors [6], which is described in JEDEC Standard JESD89, are different from those that have to be employed for accelerated testing of SEB/SEGR in power devices. Specifically, highly ionizing spallation fragment from the silicon-nucleon collision are required to set off a streamer-like discharge. This process is strongly dependent on the applied voltage but also, the primary nucleon has to have an energy that is significantly higher than that for SEU testing. As borne out by experiment, the cross-section for SEB in power devices is significantly reduced below 150MeV for the range of typical application voltages. If mono-energetic beams are to be employed for the purpose of accelerated testing, therefore, a minimum energy of 150 MeV has to be ensured to assume worst-case conditions for the terrestrial radiation environment. NOTE 1 This test method addresses a separate risk than does JESD89 tests for non-destructive SEE due to cosmic radiation effects on terrestrial applications. NOTE 2 The basic failure mechanism [3] stipulates the electric field-enhanced carrier multiplication from an initial charge deposition by a nucleon-nucleus collision fragment. The initial charge for this process is, in general, much lower as compared to high-LET heavy-ion-induced charge. Massive charge multiplication as a root cause for device failure is therefore limited to power devices of high blocking voltage. Due to thick active substrates layers of these devices of many carrier mean free path lengths along with high internal electric field strengths carrier multiplication is significant also for relatively low induced carrier densities. As borne out by experience, a minimum nominal blocking voltage of 300 V is required for terrestrial cosmic radiation to cause device failure. For devices of lower voltage rating, massive charge generation by avalanche multiplication is less effective, even for high internal electric field strengths, due to limited substrate thickness.

Author EIA
Editor JEDEC
Document type Standard
Format File
ICS 17.240 : Radiation measurements
31.080.01 : Semiconductor devices in general
Number of pages 24
Year 2015
Document history
Country USA
Keyword EIA 151;151;EIA JEP151