Syntax
data = sw_readspec(datapath)
Description
data = sw_readspec(datapath)
reads experimental spin wave dispersion
data from a text file at the given location. The general format of the
data file is described in sw_readtable with sw_readspec
requires
predefined header names and only specific tag strings are allowed. The
following header line is required:
QH QK QL minE maxE I1 E1 s1 I2 E2 s2 ...
where:
QH
\(h\) index of the \(Q\) point in rlu,QK
\(k\) index of the \(Q\) point in rlu,QL
\(l\) index of the \(Q\) point in rlu,minE
lower boundary of the \(E\) scan,maxE
upper boundary of the \(E\) scan,In
intensity of the \(n\)th spin wave mode,En
center of the \(n\)th spin wave mode, has to be in increasing order,sn
standard deviation of the corresponding energy
The number of modes in a single line of the data file is unlimited, however in every line the number of modes have to be the same. Rows with less modes should contain zero intensities at the position of the missing modes.
sw_readspec
omits modes that have either zero intensity
or zero energy.Before any data line a special tag line can be inserted that gives the
measured correlation in square brackets, for axample: '[Mxx+Myy]'
. For
the formatting of this string, see sw_parstr. If the measured type of
correlation is undefined, unpolarised neutron scattering intensity is
assumed (equivalent to 'Sperp'
). When cross sections measured in the
Blume-Maleev coordinate system, see sw_egrid, the normal to the
scattering plane has to be also defined. This can be given in a second
pair of square brackes in the \(xyz\) coordinate system, for example: '[Myy]
[1 0 0]'
. If \(n\) is undefined, the default value is '[0 0 1]'
.
Examples
Example input data file (polarised scans in the \((0,k,l)\) scattering plane):
QH QK QL ENlim1 ENlim2 I1 EN1 s1 I2 EN2 s2
[Mxx] [1 0 0]
0 1 2.9992 0 15 1 3.7128 1.0 1 8.6778 1.0
0 1 2.8993 0 15 1 7.0000 1.0 1 11.1249 1.0
0 1 2.7993 0 20 1 13.8576 1.0 0 0.0 0.0
0 1 2.6994 0 20 1 17.3861 1.0 0 0.0 0.0
[Myy] [1 0 0]
0 1.0000 2.0000 0 25 1 20.2183 1.0 0 0.0 0.0
0 1.1000 2.0000 15 30 1 22.7032 1.0 0 0.0 0.0
0 1.2000 2.0000 20 35 1 25.1516 1.0 0 0.0 0.0