2006 IEEE MTT-S International Microwave Symposium Digest 2006
DOI: 10.1109/mwsym.2006.249923
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Temperature Acceleration of Dielectric Charging in RF MEMS Capacitive Switches

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Cited by 33 publications
(27 citation statements)
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“…The switches showed no changes in mechanical stability during or after testing at cryogenic temperatures. The increased pull-in voltage for fixed-fixed capacitive switches at cryogenic reported in [6]- [12] was not observed at 77 K for the cantilever-type switches used for experimentation. In addition, the hysteresis in pull-in voltage reported in [11] after temperature cycling was not present.…”
Section: Discussionmentioning
confidence: 91%
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“…The switches showed no changes in mechanical stability during or after testing at cryogenic temperatures. The increased pull-in voltage for fixed-fixed capacitive switches at cryogenic reported in [6]- [12] was not observed at 77 K for the cantilever-type switches used for experimentation. In addition, the hysteresis in pull-in voltage reported in [11] after temperature cycling was not present.…”
Section: Discussionmentioning
confidence: 91%
“…Cryogenic temperatures have adverse effects on the operational stability and longevity of capacitive MEMS switches. The pull-in voltage substantially increases, and capacitance decreases with decreasing temperature [6]- [12]. An increased mortality rate for switches operating at cryogenic temperatures has also been reported [9].…”
mentioning
confidence: 91%
“…In fact, Q J is of the order of 10 11 q/cm 2 , while the trap density is typically of the order of 10 13 q/cm 2 ; τ CJ and τ DJ are of the order of seconds while trap capture and emission times are typically of the order of milliseconds. A recent study [20] also shows that Q J increases with temperature while τ CJ and τ DJ are independent of temperature, which are not characteristic of a typical trap density and capture/emission times. Similar to the thermionic-emission-diffusion process across a Schottky barrier [22], charge injection into a dielectric is a rather complicated phenomenon.…”
Section: Discussionmentioning
confidence: 87%
“…For extremely long on times (e.g., 500 s), the traps are all charged to their steady-state values before the off time starts so that ∆t OFF = exp(−t ON /τ C ) = 0, and (20) and (21) become the same. In addition, if there is only one set of charging and discharging time constants, (22) and (23) are essentially the same, and so are (20) and (21). However, when a more complicated control waveform is involved in the analysis, the calculation routine using the equation-based model is not as straight forward as the square-wave case.…”
Section: B Square-wave Actuationmentioning
confidence: 99%
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