Correlated Power Spectrum of PSCz 0.6 Jy with high-latitude mask
(Hamilton A. J. S., Tegmark M., 2001, MNRAS, in press, astro-ph/0008392).
http://casa.colorado.edu/~ajsh/pscz/

Version of October 2001.
The power spectrum at linear scales (k < .33 h/Mpc) remains unchanged
from the original August 2000 edition.
The power spectrum at nonlinear scales is changed, most notably at small scales.

The definition of power follows the Peebles (1980) convention
P(k) = int e^{i k.r} xi(r) d^3 r
where xi(r) is the correlation function.

k is the median wavenumber (in h/Mpc) of the band-power window.
k- and k+ are the wavenumbers (in h/Mpc) where the band-power window
falls to half its maximum.
At linear scales, k < .33 h/Mpc, the median and half-maximum points
are those of the scaled and discretized band-power windows as defined in
Hamilton A. J. S., Tegmark M., 2000, MNRAS, 312, 285 (astro-ph/9905192).
At nonlinear scales, k > .33 h/Mpc, the band-powers have the power law
times Gaussian form detailed by Hamilton & Tegmark 2000 (astro-ph/0008392).
P(k) is the estimated power (in h^-3 Mpc^3) in the band-power,
and DeltaP(k) (in h^-3 Mpc^3) its 1-sigma uncertainty.

    k     k-     k+  P(k) DeltaP(k)
.0210  .0153  .0269  7200.  15800.
.0239  .0176  .0298 15500.  11400.
.0267  .0203  .0325 19400.   9860.
.0293  .0228  .0355 18900.   8300.
.0329  .0257  .0403 12500.   6510.
.0376  .0292  .0467  9610.   5260.
.0431  .0350  .0518 14400.   4970.
.0490  .0406  .0583 15600.   4300.
.0560  .0467  .0666 10200.   3420.
.0646  .0536  .0776  8060.   2480.
.0748  .0626  .0888  8430.   1920.
.0862  .0728  .101   7180.   1460.
.0998  .0831  .119   5110.    927.
.116   .0973  .137   4590.    703.
.134   .113   .158   3140.    538.
.155   .131   .182   2860.    425.
.179   .151   .210   2440.    321.
.207   .175   .240   1710.    233.
.239   .198   .286    936.    136.
.276   .231   .329    877.    115.
.317   .268   .375    917.    109.
.365   .331   .402    702.    102.
.422   .382   .464    546.     72.
.487   .441   .536    388.     56.
.562   .510   .619    327.     40.
.649   .588   .715    288.     24.
.750   .679   .825    258.     28.
.866   .785   .953    187.     21.
1.00   .906   1.10    149.     18.
1.15   1.05   1.27    124.     12.
1.33   1.21   1.47    98.5     9.5
1.54   1.40   1.69    69.0     8.3
1.78   1.61   1.96    62.0     5.4
2.05   1.86   2.26    46.4     5.6
2.37   2.15   2.61    39.4     5.4
2.74   2.48   3.01    30.9     4.8
3.16   2.87   3.48    25.2     5.2
3.65   3.31   4.02    23.3     4.6
4.22   3.82   4.64    17.4     3.7
4.87   4.41   5.36    11.6     3.4
5.62   5.10   6.19    11.1     3.2
6.49   5.88   7.15    9.74    2.70
7.50   6.79   8.25    7.80    2.12
8.66   7.85   9.53    6.60    2.11
10.0   9.06   11.0    5.13    1.85
11.5   10.5   12.7    4.54    1.28
13.3   12.1   14.7    4.41     .94
15.4   14.0   16.9    3.62     .83
17.8   16.1   19.6    2.52     .96
20.5   18.6   22.6    2.08     .72
23.7   21.5   26.1    1.72     .42
27.4   24.8   30.1    1.50     .36
31.6   28.7   34.8    1.27     .38
36.5   33.1   40.2    .805    .307
42.2   38.2   46.4    .579    .276
48.7   44.1   53.6    .579    .263
56.2   51.0   61.9    .563    .259
64.9   58.8   71.5    .421    .255
75.0   67.9   82.5    .280    .238
86.6   78.5   95.3    .210    .197
100.   90.6   110.    .217    .172
115.   105.   127.    .154    .144
133.   121.   147.    .146    .135
154.   140.   169.    .113    .111
178.   161.   196.    .068    .093
205.   186.   226.    .091    .082
237.   215.   261.    .085    .063
274.   248.   301.    .066    .053
316.   287.   348.    .031    .047