Wavelength:  0.96600 A
Run number:    1 consists of batches          2 to        993
Angular range:              105.15 to              253.95
Closest reciprocal axis to spindle: a*   (angle   20.8 degrees)

Using MTZ column labels:      IMEAN  SIGIMEAN  I(+)  SIGI(+)  I(-)  SIGI(-)  N(+)  N(-)
Unit cell and space group:      116.648  121.283  129.500  90.00  90.00  90.00   'P 2 2 2'
Nominal diffraction range:       57.119  3.864
Input reflection count:          16405

Eigenvalues & eigenvectors of redundancy anisotropy tensor:

                              1.379         1.0000   0.0000   0.0000       a*
                              1.347         0.0000   1.0000   0.0000       b*
                              1.683         0.0000   0.0000   1.0000       c*

Diffraction limits & eigenvectors of ellipsoid fitted to diffraction cut-off surface:

                              3.695         1.0000   0.0000   0.0000       a*
                              4.306         0.0000   1.0000   0.0000       b*
                              3.879         0.0000   0.0000   1.0000       c*

GoF to ellipsoid (d*):  0.0457    Fraction of surface points fitted:  100.0%  (     2084 /     2084)

Number of unobserved reflections inside ellipsoid:      628
Number of observed reflections inside ellipsoid:      14916
Number of observed reflections outside ellipsoid:       193

Lowest cut-off diffraction limit:
            4.851 at reflection    0   25    0  in direction   b*

Worst diffraction limit after cut-off:
            5.053 at reflection    0   24    0  in direction   b*

Best diffraction limit after cut-off:
            3.875 at reflection   19   21   13  in direction   0.610 a* + 0.674 b* + 0.417 c*

NOTE that because the cut-off surface is likely to be only very approximately ellipsoidal, in part
due to variations in reflection redundancy arising from the chosen collection strategy, the
directions of the worst and best diffraction limits may not correspond with the reciprocal axes,
even in high-symmetry space groups (the only constraint being that the surface must have point
symmetry at least that of the Laue class).

Fraction of data inside cut-off surface:        91.7%  (   15038 /   16405)

Fraction of cut-off surface above threshold:    64.3%  (     607 /     944)

WARNING: Diffraction of the input data has probably been truncated due to an inappropriate
(an)isotropic diffraction cut-off applied in previous processing, or the diffraction pattern may
have extended beyond the edges of the detector.  In the latter case consider the possibilities of
either moving the detector closer or swinging it out, having carefully checked in the former case
that this will not create a risk of spot overlap.

Scale:                    2.584E+00    [ = factor to place Iobs on same scale as Iprofile/100.]
Beq:                         135.46    [ = equivalent overall isotropic B factor on Fs.]

                                          B11      B22      B33
Delta-B tensor:                        -76.36    74.85     1.51

Note: the delta-B tensor is the overall anisotropy tensor on Fs after subtraction of Beq from its
diagonal elements (so trace = 0).

Eigenvalues (E) & eigenvectors of overall anisotropy (B) tensor on Fs:

                              59.10         1.0000   0.0000   0.0000       a*
                             210.31         0.0000   1.0000   0.0000       b*
                             136.97         0.0000   0.0000   1.0000       c*

The eigenvalues and eigenvectors of the overall B tensor are the squares of the lengths and the
directions of the principal axes of the ellipsoid that represents the tensor.

Delta-B eigenvalues:                   -76.36    74.85     1.51

The delta-B eigenvalues are the eigenvalues of the overall anisotropy tensor after subtraction of
Beq (so sum = 0).

Anisotropy ratio:             1.116    [ = (Emax - Emin) / Beq ]
Fractional anisotropy:        0.508    [ = sqrt(1.5 Sum_i (E_i - Beq)^2 / Sum_i E_i^2) ]

Anisotropic S/N ratio:        18.94    [ = max_h | exp(4 pi^2 s~_h delta(B) s_h) - 1 | <I_h/sd(I_h)> ]

The 'anisotropic S/N ratio', unlike the 'anisotropy ratio' or the 'fractional anisotropy' shown
above, in addition to the anisotropy of the B tensor, takes both the diffraction and the local mean
I/sd(I) into account.

                                                                                     Compl. Spher.   Multiplicity                                   Compl. Ellip. 
                                                                                     --------------  ------------                                  --------------- 
            Resolution      #uniq     #Rfac  Rmerge   Rmeas    Rpim   #Isig  I/sigI     all     ano    all    ano CC(1/2)  #CCAno CC(ano)  SigAno    all     ano
 -----------------------------------------------------------------------------------------------------------------------------------------------------------------
         57.119 -  11.496     752      3476   0.024   0.027   0.013     752  45.288  0.9843  0.9921   4.66   2.77  0.9995     419 -0.0417   0.720   0.9843  0.9921
         11.496 -   9.045     752      4014   0.028   0.031   0.013     752  42.422  1.0000  0.9949   5.35   2.98  0.9994     534 -0.1433   0.728   1.0000  0.9949
          9.045 -   7.850     751      3627   0.041   0.046   0.020     751  29.113  0.9987  0.9837   4.85   2.69  0.9984     490 -0.1245   0.731   0.9987  0.9837
          7.850 -   7.110     753      3988   0.069   0.077   0.033     753  18.736  1.0000  0.9968   5.31   2.89  0.9976     552 -0.0903   0.748   1.0000  0.9968
          7.110 -   6.586     751      4161   0.111   0.123   0.051     751  13.269  0.9987  1.0000   5.54   2.98  0.9933     581 -0.0605   0.716   0.9987  1.0000
          6.586 -   6.183     751      4236   0.140   0.154   0.064     751  10.868  0.9973  0.9969   5.64   3.02  0.9908     594  0.1108   0.800   0.9973  0.9969
          6.183 -   5.857     753      4151   0.162   0.179   0.075     753   9.654  0.9960  0.9939   5.52   2.95  0.9850     593 -0.0310   0.798   0.9960  0.9939
          5.857 -   5.596     752      3730   0.171   0.191   0.084     752   8.402  0.9987  0.9755   4.98   2.70  0.9805     514 -0.0428   0.768   0.9987  0.9755
          5.596 -   5.375     751      3972   0.171   0.190   0.081     751   8.885  0.9987  0.9924   5.30   2.84  0.9882     577  0.1022   0.822   0.9987  0.9924
          5.375 -   5.186     752      4140   0.178   0.198   0.083     752   8.795  0.9987  0.9924   5.51   2.93  0.9917     593  0.0089   0.813   0.9987  0.9924
          5.186 -   5.020     753      4148   0.180   0.199   0.083     753   8.704  0.9947  0.9821   5.52   2.94  0.9917     592 -0.0153   0.788   0.9947  0.9821
          5.020 -   4.873     751      4123   0.178   0.198   0.084     751   9.074  1.0000  0.9851   5.50   2.93  0.9926     584  0.0340   0.833   1.0000  0.9851
          4.873 -   4.738     753      4065   0.191   0.211   0.088     753   8.278  0.9767  0.9721   5.42   2.89  0.9929     561  0.0381   0.826   0.9767  0.9721
          4.738 -   4.610     752      4078   0.212   0.235   0.099     752   7.806  0.9353  0.9287   5.44   2.89  0.9894     559 -0.0371   0.817   0.9353  0.9287
          4.610 -   4.492     751      3954   0.236   0.262   0.110     751   7.047  0.8962  0.8602   5.30   2.86  0.9894     528 -0.0522   0.798   0.8962  0.8602
          4.492 -   4.374     752      3523   0.268   0.302   0.135     752   5.816  0.8026  0.7794   4.72   2.56  0.9772     497  0.0080   0.829   0.8026  0.7794
          4.374 -   4.259     751      2878   0.269   0.310   0.149     751   4.951  0.7421  0.6927   3.91   2.17  0.9681     347  0.0210   0.806   0.7540  0.7020
          4.259 -   4.140     752      2574   0.318   0.369   0.182     752   3.733  0.6533  0.5780   3.55   2.03  0.9488     288 -0.0940   0.776   0.7416  0.6494
          4.140 -   4.015     752      2236   0.445   0.524   0.268     752   2.561  0.5529  0.4585   3.15   1.87  0.8538     236 -0.1279   0.765   0.7356  0.6085
          4.015 -   3.875     753      2057   0.623   0.750   0.406     753   1.729  0.4325  0.3666   2.90   1.69  0.6834     200 -0.0125   0.783   0.6596  0.5881
 -----------------------------------------------------------------------------------------------------------------------------------------------------------------
 Total:  57.119 -   3.875   15038     73131   0.082   0.092   0.041   15038  12.756  0.8514  0.8160   4.90   2.69  0.9994    9839 -0.0335   0.785   0.9115  0.8787

• Mouse:

  Left-down & drag:	Rotate view.
  Middle-down & drag:	Translate.
  Right-down & drag:	Zoom.
  Wheel:	Adjust z-clipping depth.
  Left-down & wheel:	Adjust z-clipping position.
  Most of the mouse actions should also work on a touchscreen (e.g. tablet or smartphone), though a gesture to emulate the mousewheel may not be available on all devices!

• Keyboard:

  - =	Adjust point size.
  0 .. 8	Toggle points in sets 0 (grey) to 9 (pink).
  c	Reset only translation and z-clipping so that the objects are re-centred.
  d	Toggle depth-cueing.
  h	Toggle on-screen help text (all text can be resized by clicking in the caption text immediately above the graphics canvas or in the text in the bottom frame, then using Ctrl/Wheel over either text).
  i	Reset to initial orientation, translation, zoom and z-clipping.
  p	Make screenshot (PNG): requires pop-ups from server to be allowed.
  s	Toggle d-spacing labels.
  x	Reset orientation, translation and z-clipping to view down world x axis (initially to right).
  y	Ditto for y axis (initially up).
  z	Ditto for z axis (initially towards viewer).
  Shift-x/y/z	View from negative axis direction.
  Down/up arrow	Decrease/increase rocking amplitude.
  Left/right arrow	Decrease/increase rock/roll speed.

If you don't see in the local mean I/σ(I) plot at least a thin layer of red points (i.e. representing rejected data) that covers most of an outer orange spherical or ellipsoidal surface (representing the diffraction limit of observed significant data, (i.e. ignore any dark blue points representing unmeasured data), it means either that there were good data beyond the edges of the detector, or (more likely) that the advice concerning the application of a diffraction cut-off to the data prior to running STARANISO was not heeded.  This should also have shown up as a warning in the summary of the anisotropy information extracted from the STARANISO log file above.