This
is where to find help on various GSAS-II windows and plots. Note that GSAS-II
operates with three windows: the main GSAS-II data tree
window, which provides a hierarchical view of the current project; the GSAS-II data editing window, which shows the contents of
a particular section of the project, where values can be examined and changed;
and the GSAS-II Plots window, which shows graphical
representations of the results.
This
is a hierarchical view of the data items in your GSAS-II project (name.gpx).
Clicking on any item in the tree opens a window where information in that item
can be viewed or edited. For example, the "Sample
Parameters" item under a ‘PWDR’ entry contains information
about how data were collected, such as the sample temperature (see below). The arrow keys (up & down) move
the selection to successive entries in the data tree; both the data window and
the associated plot (if any) will change.
The
menus associated with this window provide access to many features of GSAS-II,
as outlined below:
1. Menu ‘File’ –
a. Open project… - Open a previously saved GSAS-II project file (name.gpx). If you currently have a project file open, you are asked if it is OK to over write it; Cancel will cancel the process. NB: you may open a backup gpx file (e.g. name.bak3.gpx) to recover a previous version of your project. Remember to Save As… to e.g. name.gpx to overwrite the current version. Otherwise you may get backups of your backup file (e.g. name.bak3.bak0.gpx, etc.).
b. Save project – Save the current project. If a file name is shown after ‘Loaded Data:’ in the data tree, it will be saved there. Otherwise, you will be prompted for a new name in a file dialog (you may change directory as well). If the file exists, you will be asked if it OK to overwrite.
c. Save As… - Save the current project to a new file. A file dialog will be shown to enter the name (and change directory if desired). If the file exists, you will be asked if it OK to overwrite.
d. Close project – Close the current project; you will be asked if you want to save it first.
e. Exit – Exit the GSAS-II program; if there is a current project you will be asked if you want to save it first. Pressing the red X in the upper right (Windows) also exits (no save option) GSAS-II; useful for escaping from GSAS-II if needed.
2. Menu ‘Data’ –
a. Read powder data… - Read in powder diffraction patterns (multiple patterns can be selected). GSAS-II can read most of the old GSAS powder format files with the position in centidegrees 2-theta. It can also read “xye” format files used by topas where the position is in degrees 2-theta. As each file is read, an old GSAS style “instrument parameter file” is searched for; if not found a CuKa laboratory data set is assumed.
b. Read image data… - Read in 2-D powder diffraction images (multiple patterns can be selected). GSAS-II can read many different image file formats including MAR345 files, Quantum ADSC files, and tiff files from Perkin-Elmer, Pilatus, and GE. Although many of these formats have data fields that should contain relevant information for the exposure (e.g. wavelength), these are rarely filled in correctly by the data acquisition software. Thus, you should have separately noted this information as it will be needed
c. Read Powder Pattern Peaks… - Read in a list of powder pattern peak positions as either a d-spacing table or a set of 2Q positions; these can be used in GSAS-II powder pattern indexing.
d. Read single crystal data… -
e. Sum powder data -
f. Sum image data -
g. Add phase -
h. Delete phase -
i. Rename data -
j. Delete data -
3. Menu ‘Calculate’ –
a. Make new PDFs – This creates the pair distribution function (PDF) controls for each powder pattern selected in the dialog box. See PDF Controls for further directions.
b. View LS parms – This shows a dialog box with all the parameters for your project; those to be refined are flagged ‘True’, otherwise ‘False’. Blanks indicate parameters that are not refinable. The total number of refined parameters is also shown at the top of the list. The value of each parameter is also given. The parameter names are of the form ‘p:h:name:id’ where ‘p’ is the phase index, ‘h’ is the histogram index and ‘id’ is the item index (if needed). Indexes all begin with ‘0’ (zero). Note that for atom positions the value is not a refinable parameter, but the shift in the value is. Position names are, e.g. ‘0::Ax:0’ for the x-position of the zeroth atom in the zeroth phase while shift names have a ‘d’ in then, e.g. ‘0::dAx:0’.
c. Refine – This performs the refinement (Pawley/Rietveld or single crystal) according to the controls set in the Controls data tree item.
d. Sequential refine -
e. Solve -
4. Menu ‘Import’ –
a. Import Phase (specific) -
1. Import Phase GSAS.EXP…
2. Import Phase PDB…
3. Import Phase CIF…
4. Import Phase GSAS-II gpx…
b. Import Powder Pattern… -
c. Import HKLs… -
5. Menu ‘Export’ –
a. Export Powder Patterns… -
b. Export All Peak Lists… -
c. Export HKLs… -
d. Export PDF… -
e. Export Phase… -
f. Export CIF… -
Different
information is displayed in the Data Editing Window, depending on which section
of the data tree is selected. For example, clicking on
the "Notebook" entry of the tree brings up the Notebook editing
window described below.
This
window provides a place for you to enter whatever text commentary you wish.
Each time you enter this window, a date/time entry is provided for you. A
possibly useful technique is to select a portion of the console window after a
refinement completes (it will contain refinement results with residuals, new
values & esds) and paste it into this Notebook
window so it becomes a part of your project file.
This
window provides the main controls for the major calculations in GSAS-II. At
present only Refinement Controls are presented.
Two
of the main refinement tools are the fortran
MINPACK lmdif and lmder
algorithms wrapped in python as provided in the Scipy
package and a third one is a python version utilizing only the numpy package. The purpose is to minimize the sum of
the squares of M
nonlinear functions in N variables by a modification of the Levenberg-Marquardt
algorithm. The lmdif and lmder
routines were written by Burton S. Garbow,
Kenneth E. Hillstrom, Jorge
J. More (Argonne National Laboratory, 1980). The
python/numpy version was developed by us based on the material in Numerical
Recipes (Press, Flannery, Teulosky
& Vetterling) for the Levenberg-Marquardt
algorithm.
1. Select whether the refinement
uses ‘analytic Jacobian’, ‘analytic
Hessian’ or ‘numeric’ derivatives. The last is slower and
perhaps a bit less accurate, but may be needed if the analytic functions are
not fully developed. The Jacobian matrix is shaped N
x M (parameters x observations) and is much larger than the Hessian matrix
which is shaped M x M (parameters x parameters). Generally use ‘analytic
Hessian’ for routine work.
2. Select ‘Min
delta-M/M’ for convergence; the refinement will stop when the change in
the minimization function is less than this value. Set Min delta-M/M = 1.0 to
force just a single cycle to be performed. A value less than 10-4
(the default) generally gives no better result. The allowed range is 10-9
to 1.0.
3. If ‘analytic
Jacobean’ is chosen then select ‘Initial shift factor’ for
the first cycle of refinement. This value is modified by the least squares
routine. The allowed range is 10-5 to 100. Smaller values may be
needed if your initial refinement trials immediately
diverge, however make sure your starting parameter values are
‘reasonable’. The selected default (=1.0) normally gives good
performance.
4. If ‘analytic
Hessian’ is chosen then select ‘Max cycles’, the maximum
number of least squares cycles to be performed. Least squares cycles are
determined by the number of times a new Hessian matrix is computes; the Levenberg-Marquardt algorithm may compute the function
several times between cycles as it finds the optimal value of the Marquardt
coefficient. Choices are given in the pull down selection; the default is 3
cycles.
5. Select data for sequential
refinement; the data sets may be done in ‘reverse order’.
This
window is blank; the GSASII Plots window ‘Covariance’
shows a graphical representation of the variance-covariance matrix
This
window shows the constraints to be used in a refinement. It is organized into
three tabbed pages. ‘Phase constraints’ contain those involving
parameters that describe aspects of the crystalline phases to be used in the
refinement (e.g. atom coordinates, thermal motion and site fraction
parameters). ‘Histogram/Phase constraints’ are those which describe
aspects of the pattern that depend on both the phase and the data set used in
the refinement (e.g. mstrain
and crystallite size parameters). ‘Histogram constraints’ are those
that depend only on the data set (e.g. profile coefficients U,V,W,X
and Y).
1. Select the tab for the
parameter types you wish to constrain. Each will have the same possibilities in
the ‘Edit menu.
2. Menu ‘Edit’ –
a. Add Hold – select a parameter
that you wish to remain fixed although other parameters of the same type may be
selected as a group for refinement. For example, if the space group for a phase
has a polar axis (e.g. the b-axis in P21), then one atom y-parameter
is arbitrary and should be selected for a Hold to keep the structure from
drifting up or down the y-axis during refinement. If selected, a dialog box
will appear showing the list of available parameters; select one and then OK to
implement it, Cancel will cancel the operation. The held parameter will be
shown in the constraint window with the keyword ‘FIXED’. A Delete
button can be used to remove it.
b. Add
equivalence
– select a list of parameters that should have the same value (possibly
with a non-unitary multiplier for some). Examples are a list of atoms with the
same thermal motion Uiso, sets of profile
coefficients U,V,W across multiple data sets. If
selected, a dialog box will appear with a list of the available parameters.
Select one and press OK; a second dialog box will appear with only those
parameters that can be made equivalent to the first one. Choose those and press
OK. Cancel in either dialog will cancel the operation. The equivalenced
parameters will show as an equation of the form M1*P1+M2*P2=0;
usually M1=1.0 and M2=-1.0, but can be changed via the ‘Edit’
button. The keyword ‘EQUIV’ marks it as an
equivalence. A Delete button can be used to remove it.
c. Add
constraint
– select a list of parameters whose sum (with possible non-unitary
multipliers) is fixed. For example, the sum of site fractions for atoms on the
same site could be fixed to unity. If selected, a dialog box will appear with a
list of the available parameters. Select one and press OK; a second dialog box
will appear with only those parameters that can be used in a constraint with
the first one. Choose those and press OK. Cancel in either dialog will cancel
the operation. The equivalenced parameters will show as an equation of the form
M1*P1+M2*P2+…=C; the
multipliers M1, M2, … and C can be changed via
the ‘Edit’ button. The keyword ‘CONSTR’ marks it as a
constraint. A Delete button can be used to remove it.
d. Add
function
– this is very similar the “Add constraint” type except that
the result of the sum can be varied in the refinement. The keyword
‘FUNCT’ marks it as a function; the ‘Refine?’ box
indicates your choice to refine the result of the sum. A Delete button can be used
to remove it.
This
window is empty
Nothing
just yet
In this window is tabulated the results of your sequential refinement. The columns are the parameter names; the naming convention is ‘p:h:name:n’ where p is the phase number, h is the histogram number, name is the parameter name, and num (if needed) is the item number (e.g. atom number). The rows are the data sets used in the sequential refinement.
These are shown in the data tree with a prefix of ‘PWDR’, ’HKLF’, ‘IMG’, ‘PDF’ or ‘XXXX’ (future – restraints??) and usually a file name. These constitute the data sets (‘Histograms’) to be used by GSAS-II for analysis. Selection of these items does not produce any information in the data window but does display the data in the Plots Window. They are described below.
When
a powder diffraction data set (prefix ‘PWDR’) is selected from the data
tree, a variety
of subcategories in the tree are shown. The items that are shown depend on the
data set type. Selecting a subcategory raises the window listed below.
1.
Menu
‘Analysis’ –
a. Analyze
– this produces a ‘normal probability’ plot for the
refinement result as bounded by the limits. The slope and intercept of the
curve in the central region (-1 < D/s < 1) are shown on the
plot status line. The slope is the square root of GOF for the best fit set of
data points (~68% of the data).
This window shows whatever comment lines (preceded by “#”) found when the powder data file was read by GSAS-II. If you are lucky, there will be useful information here (e.g. sample name, date collected, wavelength used, etc.). If not, this window will be blank. The text is read-only in that anything you try to enter here is not saved.
This
window shows the limits in position to be used in any fitting for this powder
pattern. The ‘original’ values are obtained from the minimum &
maximum values in the powder pattern. You can modify ‘changed’ as
needed.
1. You can change Tmin and Tmax in the
‘changed’ row as needed. Use the mouse to select the value to be
changed (the background on the box will be blue or have a black border or a
vertical bar will appear in the value), then enter the new value and press
Enter or click the mouse elsewhere in the Background window. This will set the
new value.
2. Modify the values of
‘changed’; this can be done on the plot by dragging the limit bars
(left – vertical green dashed line, right – vertical red dashed
line) into position. A left or right mouse click on a data point on the plot
will set the associated limit. In either case the appropriate value on the
‘changed’ row will be updated immediately.
3. Menu ‘File’ –
a. Copy – this copies the
limits shown to other selected powder patterns. If used, a dialog box (Copy
Parameters) will appear showing the list of available powder patterns, you can
copy the limits parameters to any or all of them; select ‘All’ to
copy them to all patterns. Then select ‘OK’ to do the copy;
‘Cancel’ to cancel the operation.
This
window shows the choice of background functions and coefficients to be used in
fitting this powder pattern. There are three types of contributions available
for the background:
1).
A continuous empirical function (‘chebyschev’,
‘cosine’, ‘lin
interpolate’, ‘inv interpolate’ & ‘log
interpolate’). The latter three select fixed points with spacing that is either equal, inversely equal or equal on a log scale of the
x-coordinate. The set of magnitudes at each point then comprise the background
variables. All are refined when refine is selected.
2). A set of Debye diffuse scattering equation terms of the
form:
where A,R & U are the possible
variables and can be individually selected as desired; Q = 2p/d.
3).
A set of individual Bragg peaks using the pseudo-Voigt profile function as
their shapes. Their parameters are ‘pos’, ’int’, ‘sig’ & ‘gam’; each can be selected for refinement. The
default values for sig & gam (=0.10) are for very
sharp peaks, you may adjust them accordingly to the kind of peak you are trying
to fit before trying to refine them.
1. Menu ‘File’ –
a. Copy – this copies the background
parameters shown to other selected powder patterns. If used, a dialog box (Copy
Parameters) will appear showing the list of available powder patterns, you can
copy the background parameters to any or all of them; select ‘All’
to copy them to all patterns. Then select ‘OK’ to do the copy;
‘Cancel’ to cancel the operation.
2. You can select a different
Background function from the pull down tab.
3. You can choose to refine/not
refine the background coefficients.
4. You can select the number of background
coefficients to be used (1-36).
5. You can change individual
background coefficient values. Enter the value then press Enter or click the
mouse elsewhere in the Background window. This will set the new value.
6. You can introduce one or more
Debye scattering terms into the background. For each one you should enter a
sensible value for ‘R’ – an expected interatomic
distance in an amorphous phase is appropriate. Select parameters to refine;
usually start with the ‘A’ coefficients.
7. You can introduce single
Bragg peaks into the background. For each you should specify at least the
position. Select parameters to refine; usually start with the ‘int’ coefficients.
This
window shows the instrument parameters for the selected powder data set.
1. Menu ‘Operations’ –
a. Reset
profile –
resets the values for the instrument parameters to the default values shown in
parentheses for each entry.
b. Copy – this copies the
instrument parameters shown to other selected powder patterns. If used, a
dialog box (Copy Parameters) will appear showing the list of available powder
patterns, you can copy the instrument parameters to any or all of them; select
‘All’ to copy them to all patterns. Then select ‘OK’ to
do the copy; ‘Cancel’ to cancel the operation.
c. Change
radiation
– this changes the radiation between single wavelength (e.g. for
synchrotron source) and Ka1/Ka2 wavelength pairs (e.g. a
laboratory tube source).
2. You can change any of the
profile coefficients
3. You can choose to refine any
profile coefficients. NB: In certain
circumstances some choices are ignored e.g. Zero is not refined during peak
fitting. Also some choices may lead to unstable refinement, e.g. Lam refinement and lattice parameter refinement. Examine the
‘Covariance’ display for highly
correlated parameters.
This
window...
This
window shows the list of peaks that will be used by the peak fitting
refinement. It is filled by picking peaks in the powder pattern displayed in
the GSASII Plots window as a sequence of ‘+’ marks.
This
window shows the list of peaks that will be used for indexing (see Unit
Cells List).
It must be filled before indexing can proceed. When indexing is completed, this
display will show the resulting hkl values for every
indexed reflection along with the calculated d-spacing (‘d-calc’) for the selected unit cell in Unit
Cells List.
1. Menu ‘Operations’ – Load/Reload – loads the peak
positions & intensities from the Peak List to make them available for
the indexing routine. The d-obs is obtained from
Bragg’s Law after applying the Zero correction shown on the Instrument
Parameters
table to the position shown here.
2. You may deselect individual
peaks from indexing by unchecking the corresponding
‘use’ box.
This
window...
This
window...
This window
This
window...
This
window...
This
window...
When
a phase is selected from the data tree, parameters are
shown for that selected phase in a tabbed window. Clicking on each tab raises
the windows listed below. Each tab is identified by the underlined phrase in
the following:
This
gives overall parameters describing the phase such as the name, space group,
the unit cell parameters and overall parameters for the atom present in the
phase. It also has the controls for computing Fourier maps for this phase.
1. Menu ‘Compute’ – The compute menu
shows computations that are possible for this phase.
a. Fourier
maps –
compute Fourier maps according to the controls set at bottom of General page.
2. The items in the upper part
of the General page that can be changed are Phase name, Phase type, Space
group, unit cell parameters & refine flag. These are described in turn:
a. Phase
name –
this is the name assigned to this phase. It should only be changed when the
phase is initialized or imported.
b. Phase
type – this
can only be set when there are no atoms in the Atoms page for this phase.
Select it when the phase is initialized.
c. Space
group
– this should be set when the phase is initialized; it can be changed later.
Be careful about the impact on Atom site symmetry and multiplicity if you do.
GSAS-II will recognize any legal space group symbol using the short Hermann-Mauguin forms; put a space between the axial fields (e.g.
‘F d 3 m’ not ‘Fd3m’). For space groups with a choice
of origin (e.g. F d 3 m), GSAS-II always uses the 2nd setting where
the center of inversion is located at the origin. The choice of space group
will set the available unit cell parameters.
d. Refine
unit cell
– set this flag to refine the unit cell parameters in a Rietveld or
Pawley refinement. The actual parameters refined are the symmetry allowed terms
(A0-A5) in the expression
e. a, b, c, alpha, beta, gamma – lattice parameters; only
those permitted by the space group are shown. The volume is computed from the
values entered.
3. If there are entries in the
Atoms page then the Elements table is shown next on the General page; you may
select the isotope (only relevant for neutron diffraction experiments). The
density is computed depending on this choice, the unit cell volume and the atom
fractions/site multiplicities in the entries on the Atoms page.
4. Fourier map controls are
shown at the bottom of the General page. A completed Rietveld or Pawley
refinement is required before a Fourier map can be computed. Select the desired
type of map, the source of the reflection set and the map resolution desired.
This gives a list of the atoms and bonds that are to be rendered as lines, van der Waals radii balls, sticks, balls & sticks, ellipsoids & sticks or polyhedra. There are two menus for this tab; Edit allows modification of the list of atoms to be rendered and Compute gives some options for geometric characterization of selected atoms.
1. Atom Selection from table: select individual atoms by a left click of the mouse when pointed at the left most column (atom numbers) of the atom display; hold down the Ctrl key to add to your selection; a previously selected atom will be deselected. A selected atom will be highlighted (in grey) and the atom will be shown in green on the plot. Selection without the Ctrl key will clear previous selections. A double left click in the (empty) upper left box will select or deselect all atoms.
2. Atom Selection from plot: select an atom by a left click of the mouse while holding down the Shift key and pointed at the center of the displayed atom, it will turn green if successful and the corresponding entry in the table will be highlighted (in grey); any previous selections will be cleared. To add to .your selection use the right mouse button (Shift down); if a previously selection is reselected it is removed from the selection list. NB: beware of atoms that are hiding behind the one you are trying to select, they may be selected inadvertently. You can rotate the structure anytime during the selection process.
3. Double left click a Name, Type and Sym Op column heading: a dialog box is shown that allows you to select all atoms with that characteristic. For example, selecting the Type column will show all the atom types; your choice will then cause all those atoms to be selected.
4. Double left click a Style, Label or Color column: a dialog box is shown that allows you to select a rendering option for all the atoms. For Color a color choice dialog is displayed that covers the entire color spectrum. Choose a color by any of the means available, press the “Add to Custom Colors”, select that color in the Custom colors display and then press OK. NB: selecting Color will make all atoms have the same color and for Style “blank” means the atoms aren’t rendered and thus the plot will not show any atoms or bonds!
5. Menu ‘Edit’ - The edit menu shows operations that can be performed on your selected atoms. You must select one or more atoms before using any of the menu items.
a. Atom style – select the rendering style for the selected atoms
b. Atom label – select the item to be shown as a label for each atom in selection. The choices are: none, type, name or number.
c. Atom color – select the color for the atom; a color choice dialog is displayed that covers the entire color spectrum. Choose a color by any of the means available, press the “Add to Custom Colors”, select that color in the Custom colors display and then press OK.
d. Reset atom colors – return the atom color back to their defaults for the selected atoms.
e. View point – position the plot view point to the first atom in the selection.
f. Add atoms – using the selected atoms, new ones are added to the bottom of the list after applying your choice of symmetry operator and unit cell translation selected via a dialog display. Duplicate atom positions are not retained. Any anisotropic thermal displacement parameters (Uij) will be transformed as appropriate.
g. Transform atoms – apply a symmetry operator and unit cell translation to the set of selected atoms; they will be changed in place. Any anisotropic thermal displacement parameters (Uij) will be transformed as appropriate.
h. Fill CN-sphere – using the atoms currently in the draw atom table, find all atoms that belong in the coordination sphere around the selected atoms via unit cell translations. NB: symmetry operations are not used in this search.
i. Fill unit cell - using the atoms currently selected from the draw atom table, find all atoms that fall inside or on the edge/surface/corners of the unit cell. This operation is frequently performed before Fill CN-sphere.
j. Delete atoms – clear the entire draw atom table; it is then refilled from the Atoms table. You should do this operation after any changes in the Atoms table, e.g. by a structure refinement.
6. Menu ‘Compute’ - The compute menu gives a choice of geometric calculations to be performed with the selected atoms. You must select the appropriate number of atoms for these to work and the computation is done for the atoms in selection order.
a. Dist. Ang. Tors. – when 2-4 atoms are selected, a distance, angle or torsion angle will be found for them. The angles are computed for the atoms in their selection order. The torsion angle is a right hand angle about the A2-A3 vector for the sequence of atoms A1-A2-A3-A4. An estimated standard deviation is given for the calculated value if a current variance-covariance matrix is available. The result is shown on the console window; it may be cut & pasted to another application (e.g. Microsoft Word).
b. Best plane – when 4 or more atoms are selected, a best plane is determined for them. The result is shown on the console window; it may be cut & pasted to another application (e.g. Microsoft Word). Shown are the atom coordinates transformed to Cartesian best plane coordinates where the largest range is over the X-axis and the smallest is over the Z-axis with the origin at the unweighted center of the selection. Root mean square displacements along each axis for the best plane are also listed. The Z-axis RMS value indicates the flatness of the proposed plane. NB: if you select (e.g. all) atoms then Best plane will give Cartesian coordinates for these atoms with respect to a coordinate system where the X-axis is along the longest axis of the atom grouping and the Z-axis is along the shortest distance. The origin is at the unweighted center of the selected atoms.
This gives the list of reflections used in a Pawley refinement and can only be seen if the phase type is ‘Pawley’ (see General).
1. Menu ‘Operations’ –
a. Pawley create – this creates a new set of Pawley reflections, over writing any preexisting Pawley set. They are generated with d-spacings larger than the limit set as ‘Pawley dmin’ in the General tab for this phase. By default the refine flags are not set and the Fsq(hkl) = 100.0.
b. Pawley estimate – this attempts an estimate of Fsq(hkl) from the peak heights of the reflection as seen in the 1st powder pattern of those selected in the Data tab.
c. Pawley delete – this clears the set of Pawley reflections.
2. You can change the refine flags either by clicking on the box or by selecting one and then selecting the column (a single click on the column heading). Then type ‘y’ to set the refine flags or ‘n’ to clear the flags. You should deselect those reflections that fall below the lower limit or above the upper limit of the powder pattern otherwise you may have a singular matrix error in your Pawley refinement.
3. You can change the individual Fsq(hkl) values by selecting it, typing in the new value and then pressing enter or selecting somewhere else in the table.
This
window presents all the graphical material as a multipage tabbed set of plots
utilizing the matplotlib python package. Each page
has a tool bar (at bottom in Windows) with the controls
These
are Home, Back, Forward, Pan, Zoom, Save and Help, respectively.
Below
the toolbar may be a status bar that on the left may show either an instruction
for a keyed input or a pull down selection of keyed input; on the right may be
displayed position dependent information that is updated as the mouse is moved
over the plot region.
The
specific types of plots that are pages in the GSASII Plots windows are next.
The
powder patterns that are part of your project are shown on this page. They can
be displayed as a stack of powder patterns, just a single pattern or as a
contour image of the peak intensities. What can be done here will depend on
which is displayed and on which item in the GSAS-II data tree you have
selected.
1. Move the mouse cursor across the
plot, the plot status line will show the cursor position in 2Q, d-spacing and the
intensity. For a q-plot, q is shown instead of 2Q.
2. On the plot status line ‘key press’ – you can either press the key on the key board or select from the pull down menu. For line plots:
a. l: offset left – for a waterfall plot of multiple powder profiles, increase the offset to the left. Does not apply if only one pattern.
b. r: offset right - for a waterfall plot of multiple powder profiles, increase the offset to the left. Does not apply if only one pattern.
c. d: offset down - for a waterfall plot of multiple powder profiles, increase the offset down. Does not apply if only one pattern.
d. u: offset up - for a waterfall plot of multiple powder profiles, increase the offset up. Does not apply if only one pattern.
e. o: reset offset - for a waterfall plot of multiple powder profiles, reset to no offset. Does not apply if only one pattern.
f. n: log(I) on/off – changes the y-axis to be the log10 of the intensity; difference curve is not shown for log(I) on.
g. c: contour on/off – if multiple powder profiles, then a contour plot is shown of the observed intensities. All data sets must be the same length as the first one to be included in the contour plot.
h. q: toggle q plot – changes the x-axis from 2Q to q=2p/d. This will put multiple powder patterns taken at different energies on the same x-axis scale.
i. s: toggle single plot – for multiple powder profiles, this will show only the one selected from the data tree. The offset options are not active.
j. w: toggle divide by sig – for the pattern selected from the data tree, this will divide the observed, calculated and difference curves by the esd for the data points. Other data sets are not shown.
k. +: no selection - for multiple powder profiles, only the observed curve is shown.
3. For contour plots the status
line ‘key press’ options are different:
a. d: lower contour max – this lowers the
level chosen for the highest contour color.
b. u:
raise contour max
– this raises the level chosen for the highest contour color
c. i:
interpolation method
– this changes the method used to represent the contours. If selected a
dialog box appears with all the possible choices. Default is
‘nearest’; the other useful choice is ‘bilinear’, this
will smooth out the contours.
d. s: color scheme – this changes the
color scheme for the contouring. Default is ‘Paired’,
black/ white options are ‘Greys’ and
‘binary’ (for black on white) or ‘gray’ (for white on
black). Others can be very colorful (but not useful)!
e. c: contour off/on – this turns off contouring
and returns to a waterfall plot with any offsets applied.
4. Depending on the item chosen
for the selected powder pattern in the data tree, the mouse buttons have
different actions:
a. Limits - Modify the values of
‘changed’; this can be done on the plot by dragging the limit bars
(left – vertical green dashed line, right – vertical red dashed
line) into position. A left or right mouse click on a data point on the plot
will set the associated limit. In either case the appropriate value on the
‘changed’ row will be updated immediately.
b.
The
variance-covariance matrix as a color coded array is shown on this page. The
color bar to the right shows the range of covariances
(-1 to 1) and corresponding colors. The parameter names are to the right and
the parameter numbers are below the plot.
1. Move the mouse cursor across the plot. If on a diagonal cell, the parameter name, value and esd is shown both as a tool tip and in the right hand portion of the status bar. If the cursor is off the diagonal, the two parameter names and their covariance are shown in the tool tip and the status bar.
2. Use the Zoom and Pan buttons to focus on some section of the variance-covariance matrix.
3. Type ‘s’ – A color scheme selection dialog is shown. Select a color scheme and press OK, the new color scheme will be plotted. The default is ‘RdYlGn’.
This
plot shows...
This
plot shows the line positions for the peak list
This plot shows….
This
plot shows the contributions to the powder pattern peak widths as Dd/d (= Dq/q) vs
q(=2p/d)
from the Gaussian and Lorentzian parts of the profile
function. The computed curves are based on the values of U, V, W, X and Y shown
in the Instrument Parameters window in parentheses. These are the values for
the instrument contribution that were set when the powder pattern was first
read in to GSAS-II. If individual peak fitting has been performed, the values
of ‘sig’ & ‘gam’ for the
peaks are plotted as ‘+’; these are computed from the fitted values
of U, V, W, X and Y as well as any sig or gam
individually refined.
This
plot shows...
This
plot shows the variation of the selected parameters with respect to the data
sequence number.
This
plot shows...
This
plot shows...
This
plot shows...
This
plot shows...
This
plot shows...
This
plot shows...
Last
modified: Tue Nov 22 13:19:47 CST 2011