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FALSE ALARM                                                                        FANTASTRON      174



           that vary the detection threshold as a function of the sensed  through a narrowband IF filter, the noise envelope has a Ray-
           environment. See  false-alarm probability;  CONSTANT  leigh distribution, and in this case we can write
           FALSE-ALARM RATE (CFAR). PCH                                                      2
                                                                                           – æ  V T   ö
           Ref.: IEEE (1993), p. 480; DiFranco (1968), p. 270.                    P  fa  =  exp ----------- ÷
                                                                                          ç
                                                                                          è 2y 0 ø
           constant false-alarm rate (see CFAR).
                                                                where y  is the mean square value of the noise voltage in a
                                                                       0
           False-alarm control refers to any technique applied to the  narrowband (compared to midfrequency) IF filter.
           output of a radar detector or detection scheme that attempts to   In Fig. F1, T  is the time between crossing of the thresh-
                                                                              k
           maintain a constant false-alarm rate under varying environ-  old  V  by the noise  envelope, when the slope of crossing
                                                                     T
           mental conditions. (See CFAR). A fixed detection threshold,  noise voltage is positive, and t , t  , t   are the times during
                                                                                        k k+1 k+n
           if set sufficiently high, will result in a uniform false-alarm
           rate, but  at the  cost of reduced sensitivity to true target
           returns. Such use of a fixed threshold is generally unaccept-
           able, and three  different  forms of false-alarm control  have
           been devised in an attempt to solve the problem:
               (1) Adaptive thresholding.
               (2) Nonparametric detectors.
               (3) Clutter maps.
               The  adaptive thresholding and nonparametric detector
                                                                  Figure F1 Envelope of receiver output showing false alarms
           approaches both make the assumption that the samples in the  due to noise (from Skolnik, 1980, Fig. 2.4, p. 25, reprinted by
           reference cells, or the range cells surrounding the test cell, are  permission of McGraw-Hill).
           independent, both in space and time, and have the same statis-
           tical distribution. The detectors then compare the return from  which the noise voltage lies above the threshold. The average
           the  test cell with the statistical average from the  reference  time interval  between  crossings of the threshold  by  noise
           cells and make a detection decision if the test cell return is  alone is the false alarm time T  where
                                                                                        fa
           sufficiently larger.                                                              N
                                                                                          1
               Clutter maps are  most effective in fixed-frequency,             t  =  lim  ----  å  T
           ground-based radars in a stationary land clutter environment.         fa  N ®  ¥  N  k
                                                                                            k =  1
           A clutter map is made by storing an average background clut-
           ter level for each range-azimuth cell, and a target detection is  The false-alarm probability may also be defined as the ratio
           declared in a particular cell if the return exceeds the average  of the duration of time the noise voltage envelope is actually
           for  that  cell by a preestablished amount.  The threshold  is  above the threshold, to the total time it could have been above
           determined based on the average return in that cell over previ-  the threshold. The  average  duration of a noise pulse is
           ous scans (e.g., 5 to 10 scans). An advantage of clutter maps  approximately equal to the reciprocal of the bandwidth B, so
           is that they give the radar a useful interclutter visibility capa-  that
           bility;  they can  see targets that lie between  large  clutter             t áñ    1
                                                                                        k av
                                                                                 P  =  ---------------- =  ---------
           returns. (See CFAR.) PCH                                               fa  á T ñ   t B
                                                                                        k av  fa
           Ref.: Skolnik (1990), pp. 8.12–8.21.
                                                                The false-alarm time can be seen also to equivalent to
           The false-alarm number is the reciprocal of the false-alarm                       2
           probability 1/P  where P  is the probability that the interfer-        t  fa  =  1  æ V T  ö
                                                                                           ç
                                fa
                                                                                       ---exp ---------- ÷
                       fa
           ence voltage envelope will exceed some threshold voltage V .                B   è 2y 0 ø
                                                           T
           (See false-alarm probability.) PCH
                                                                PCH
           Ref.: Skolnik (1980), p. 24.
                                                                Ref.: Skolnik (1980), pp. 23–25.
           False-alarm probability.  If a threshold device is used to
           make a decision as to the presence or absence of a signal in a  false-alarm time (see false-alarm probability).
           background of noise, the performance of this device can be  FANTASTRON.  A fantastron is a single-stage relaxation
           expressed in terms of two probabilities: the probability  of  vacuum-tube oscillator of linearly dropping voltage operating
           detection  P  and the  probability of  false alarm  P . The  in the free-running or delay-line mode. A fantastron processes
                                                       fa
                     d
           threshold can be considered  the value of a receiver output  sawtooth and rectangular voltage pulses, the duration of
           voltage V , that when exceeded, indicates a detection. Due to  which can be regulated within broad limits by changing the
                   T
           the presence of thermal noise in the receiver, there is always a  control voltage.
           nonzero probability that the threshold will be exceeded, even  Fantastrons were used in older types of radars to obtain
           in  the  absence of a target  signal. The probability  that the  precise adjustable pulse delays, to determine the time interval
           threshold value V  is exceeded when no signal is present is  between pulses, and to generate sawtooth voltage. IAM
                          T
           the false-alarm probability. For  Gaussian  noise passed  Ref.: Popov (1980), p. 454.
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