• DocumentCode
    679902
  • Title

    Active electronically scanned array (AESA) system noise temperature

  • Author

    Brookner, Eli

  • Author_Institution
    Raytheon Co., Sudbury, MA, USA
  • fYear
    2013
  • fDate
    15-18 Oct. 2013
  • Firstpage
    760
  • Lastpage
    767
  • Abstract
    In calculating the antenna system noise temperature the question always arises as to how to account for the antenna mismatch. In this paper it is shown that the antenna mismatch introduces another term into the antenna system temperature equation. This term increases the system temperature. It is due to the reflection of the noise coming out of the receiver in the direction of the antenna that is reflected back into the receiver towards its signal output port. For a single port reflector antenna system this term is equal to the temperature Tr of the noise coming out of the receiver towards the antenna times the antenna power reflection coefficient |Γ|2. This is usually included in the radiometer field but not by those in the radar and communication fields. For an active phased array the question that arises is: What reflection coefficient to use? It is shown that for an active electronically scanned array (AESA) the reflection coefficient to use for this incoherent noise is the same one used for a coherent signal transmitted in the direction of the main beam. This result is new for those in the radiometer, radar and communication fields. Sometimes system engineers argue that because antenna mismatch is nonohmic it has no effect in calculating the system temperature of an AESA. Doing this can yield a large underestimate of the system temperature at large scan angles, 1.2 to 2.4 dB for the examples cases considered here. It is shown that if the mismatch loss is treated as fully ohmic the correct system noise temperature results are obtained. However to determine the temperature of the ohmic mismatch requires understanding that this noise originates from the noise coming out of the receiver in the direction of the antenna. The temperature of the ohmic mismatch loss will be equal to the temperature of this receiver noise at the point of the mismatch. We will first analyze single port dish and lens antennas which use a single Low Noise Amplifier (LNA)- for the sum channel and then cover active electronically scanned arrays (transmit/receive or receive only).
  • Keywords
    antenna phased arrays; lens antennas; losses; low noise amplifiers; noise; active electronically scanned array; active phased array; antenna mismatch; antenna power reflection coefficient; coherent signal transmission; lens antennas; low noise amplifier; mismatch loss; noise temperature; ohmic mismatch; radiometer field; single port dish; single port reflector antenna system; Arrays; Noise; Receiving antennas; Reflection; Reflector antennas; AESA noise temperature; Array system noise temperature; active array noise temperature; array noise temperature; communication noise temperature. passive array noise temperature; noise temperature; radar noise temperature;
  • fLanguage
    English
  • Publisher
    ieee
  • Conference_Titel
    Phased Array Systems & Technology, 2013 IEEE International Symposium on
  • Conference_Location
    Waltham, MA
  • Type

    conf

  • DOI
    10.1109/ARRAY.2013.6731925
  • Filename
    6731925