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float splitup_freq2(float c0, float c90, float *chirp0, float
*chirp90, float norm, float* twice_inv_noise, int n, int offset, int p,
int* indices, float* stats, float* working,float* htilde)
This routine implements the two-phase
statistic test. It returns
the value of the statistic
as defined
in Eq. (
). It is algorithmically similar to splitup_freq2(), except that it allows for the case where the phase
of the signal is unknown. The arguments are identical to those of splitup_freq2() but the array stats has
elements since the
signals are complex.
Note: The GRASP library includes two additional functions which are
operationally identical to splitup_freq3(), called
splitup_freq4() and splitup_freq5(). The last of
these is currently the most efficient implementation of the two-phase
test. All the arguments of splitup_freq[3-5]() are
identical.
The arguments are:
- c0: Input. Used in the same way as in splitup_freq2().
- c90: Input. Used in the same way as in splitup_freq2(). Note that
if templates have unit norm you can set
.
- chirp0: Input. An array chirp0[0..n-1] containing
the FFT of the 0-phase chirp.
- chirp90: Input. An array chirp90[0..n-1]
containing the FFT of the
-phase chirp.
- norm: Input. The normalization of the 0-phase chirp.
- twice_inv_noise: Input. The array twice_inv_noise[0..n/2] contains
, as described previously.
The array element twice_inv_noise[0] contains the DC value,
and the array element twice_inv_noise[n/2] contains the value
at the Nyquist frequency.
- n: Input. Defines the lengths of the previous arrays.
- offset: Input. The offset of the moment of maximum signal
in the filter output.
- p: Input. The number of frequency bands
for the vetoing test.
- indices: Output. An array indices[0..p-1] used for
internal storage of the frequency subintervals (see splitup().
- stats: Output. An array stats[0..2p-1] containing
the real and imaginary parts of the
for
.
- working: Output. An array working[0..n-1] used for
internal storage.
- htilde: Input. An array htilde[0..n-1] containing
the positive frequency part of
.
- Authors
Bruce Allen, ballen@dirac.phys.uwm.edu,
and Patrick Brady, patrick@tapir.caltech.edu,
and Jolien Creighton jolien@tapir.caltech.edu.
- Comments:
None.
Next: Example: optimal program
Up: GRASP Routines: Gravitational Radiation
Previous: Function: splitup_freq2()
  Contents
Bruce Allen
2000-11-19