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SGA-5386 Datasheet(PDF) 1 Page - Stanford Microdevices |
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SGA-5386 Datasheet(HTML) 1 Page - Stanford Microdevices |
1 / 7 page Product Description The information provided herein is believed to be reliable at press time. Stanford Microdevices assumes no responsibility for inaccuracies or omissions. Stanford Microdevices assumes no responsibility for the use of this information, and all such information shall be entirely at the user’s own risk. Prices and specifications are subject to change without notice. No patent rights or licenses to any of the circuits described herein are implied or granted to any third party. Stanford Microdevices does not authorize or warrant any Stanford Microdevices product for use in life-support devices and/or systems. Copyright 1999 Stanford Microdevices, Inc. All worldwide rights reserved. 522 Almanor Ave., Sunnyvale, CA 94086 Phone: (800) SMI-MMIC http://www.stanfordmicro.com Preliminary Doc # EDS-100611 Rev. A SGA-5386 DC-3200 MHz Silicon Germanium HBT Cascadeable Gain Block Product Features • DC-3200 MHz Operation • Single Voltage Supply • High Output Intercept: +31dBm typ. at 850 MHz • Low Current Draw: 60mA at 3.6V typ. • Low Noise Figure: 3.5dB typ. at 850 MHz Applications • Oscillator Amplifiers • PA for Low Power Applications • IF/ RF Buffer Amplifier • Drivers for CATV Amplifiers 0 5 10 15 20 Electrical Specifications at Ta = 25C Frequency MHz dB Small Signal Gain vs. Frequency Stanford Microdevices’ SGA-5386 is a high performance cascadeable 50-ohm amplifier designed for operation at voltages as low as 3.6V. This RFIC uses the latest Silicon Germanium Heterostructure Bipolar Transistor (SiGe HBT) process featuring 1 micron emitters with FT up to 65 GHz. This circuit uses a darlington pair topology with resistive feedback for broadband performance as well as stability over its entire temperature range. Internally matched to 50 ohm impedance, the SGA-5386 requires only DC blocking and bypass capacitors for external components. l o b m y S : s n o i t i d n o C t s e T : s r e t e m a r a P Z 0 z H M 0 0 2 3 - C D = f , s m h O 0 5 = s t i n U . n i M . p y T . x a M P B d 1 n o i s s e r p m o C B d 1 t a r e w o P t u p t u O z H M 0 5 8 = f z H M 0 5 9 1 = f m B d m B d 0 . 7 1 7 . 4 1 S 1 2 n i a G l a n g i S ll a m S z H M 0 0 0 1 - C D = f z H M 0 0 0 2 - 0 0 0 1 = f z H M 0 0 0 5 - 0 0 0 2 = f B d B d B d 0 . 5 12 . 7 1 6 . 6 1 5 . 5 1 S 2 1 n o i t a l o s I e s r e v e R z H M 0 0 0 1 - C D = f z H M 0 0 0 2 - 0 0 0 1 = f z H M 0 0 0 5 - 0 0 0 2 = f B d B d B d 8 . 0 2 2 . 1 2 2 . 1 2 R W S VR W S V t u p n Iz H M 0 0 0 5 - C D = f- 1 : 5 2 . 1 R W S VR W S V t u p t u Oz H M 0 0 0 5 - C D = f- 1 : 5 2 . 1 P I 3 t n i o P t p e c r e t n I r e d r O d r i h T z H M 0 5 8 = f z H M 0 5 9 1 = f m B d m B d 0 . 1 3 0 . 9 2 F Ne r u g i F e s i o N z H M 0 0 0 1 - C D = f z H M 0 0 4 2 - 0 0 0 1 = f B d B d 5 . 3 0 . 4 T D y a l e D p u o r Gz H M 0 0 0 1 = fS p0 . 2 1 1 V D e g a t l o V e c i v e DV 1 . 36 . 31 . 4 I D t n e r r u C e c i v e D A m0 . 0 6 |
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