 NAME
 OVERVIEW
 Indexing and threading with PDL
 ndarrays can have children
 Slicing ndarrays
 There are different kinds of assignments in PDL
 Other functions that manipulate dimensions
 Calls to indexing functions can be chained
 Propagated assignments ('.=') and dummy dimensions
 Reasons for the parent/child (or "pointer") concept
 How to make things physical again
 Threading
 PDL::PP
 Appendix A
 Appendix B
 AUTHOR & COPYRIGHT
NAME
PDL::Indexing  Introduction to indexing and slicing ndarrays.
OVERVIEW
This man page should serve as a first tutorial on the indexing and threading features of PDL.
Like all vectorized languages, PDL automates looping over multidimensional data structures ("ndarrays") using a variant of mathematical vector notation. The automatic looping is called "threading", in part because ultimately PDL will implement parallel processing to speed up the loops.
A lot of the flexibility and power of PDL relies on the indexing and threading features of the Perl extension. Indexing allows access to the data of an ndarray in a very flexible way. Threading provides efficient vectorization of simple operations.
The values of an ndarray are stored compactly as typed values in a single block of memory, not (as in a normal Perl listoflists) as individual Perl scalars.
In the sections that follow many "methods" are called out  these are Perl operators that apply to ndarrays. From the perldl (or pdl2) shell, you can find out more about each method by typing "?" followed by the method name.
Dimension lists
A ndarray (PDL variable), in general, is an Ndimensional array where N can be 0 (for a scalar), 1 (e.g. for a sound sample), or higher values for images and more complex structures. Each dimension of the ndarray has a positive integer size. The perl
interpreter treats each ndarray as a special type of Perl scalar (a blessed Perl object, actually  but you don't have to know that to use them) that can be used anywhere you can put a normal scalar.
You can access the dimensions of an ndarray as a Perl list and otherwise determine the size of an ndarray with several methods. The important ones are:
 nelem  the total number of elements in an ndarray
 ndims  returns the number of dimensions in an ndarray
 dims  returns the dimension list of an ndarray as a Perl list
 dim  returns the size of a particular dimension of an ndarray
Indexing and Dataflow
PDL maintains a notion of "dataflow" between an ndarray and indexed subfields of that ndarray. When you produce an indexed subfield or single element of a parent ndarray, the child and parent remain attached until you manually disconnect them. This lets you represent the same data different ways within your code  for example, you can consider an RGB image simultaneously as a collection of (R,G,B) values in a 3 x 1000 x 1000 image, and as three separate 1000 x 1000 color planes stored in different variables. Modifying any of the variables changes the underlying memory, and the changes are reflected in all representations of the data.
There are two important methods that let you control dataflow connections between a child and parent ndarray:
 copy  forces an explicit copy of an ndarray
 sever  breaks the dataflow connection between an ndarray and its parents (if any)
Threading and Dimension Order
Most PDL operations act on the first few dimensions of their ndarray arguments. For example, sumover
sums all elements along the first dimension in the list (dimension 0). If you feed in a threedimensional ndarray, then the first dimension is considered the "active" dimension and the later dimensions are "thread" dimensions because they are simply looped over. There are several ways to transpose or reorder the dimension list of an ndarray. Those techniques are very fast since they don't touch the underlying data, only change the way that PDL accesses the data. The main dimension ordering functions are:
 mv  moves a particular dimension somewhere else in the dimension list
 xchg  exchanges two dimensions in the dimension list, leaving the rest alone
 reorder  allows wholesale mixing of the dimensions
 clump  clumps together two or more small dimensions into one larger one
 squeeze  eliminates any dimensions of size 1
Physical and Dummy Dimensions
document Perl level threading
threadids
update and correct description of slice
new functions in slice.pd (affine, lag, splitdim)
reworking of paragraph on explicit threading
Indexing and threading with PDL
A lot of the flexibility and power of PDL relies on the indexing and looping features of the Perl extension. Indexing allows access to the data of an ndarray in a very flexible way. Threading provides efficient implicit looping functionality (since the loops are implemented as optimized C code).
ndarrays are Perl objects that represent multidimensional arrays and operations on those. In contrast to simple Perl @x
style lists the array data is compactly stored in a single block of memory thus taking up a lot less memory and enabling use of fast C code to implement operations (e.g. addition, etc) on ndarrays.
ndarrays can have children
Central to many of the indexing capabilities of PDL are the relation of "parent" and "child" between ndarrays. Many of the indexing commands create a new ndarray from an existing ndarray. The new ndarray is the "child" and the old one is the "parent". The data of the new ndarray is defined by a transformation that specifies how to generate (compute) its data from the parent's data. The relation between the child ndarray and its parent are often bidirectional, meaning that changes in the child's data are propagated back to the parent. (Note: You see, we are aiming in our terminology already towards the new dataflow features. The kind of dataflow that is used by the indexing commands (about which you will learn in a minute) is always in operation, not only when you have explicitly switched on dataflow in your ndarray by saying $x>doflow
. For further information about data flow check the dataflow man page.)
Another way to interpret the ndarrays created by our indexing commands is to view them as a kind of intelligent pointer that points back to some portion or all of its parent's data. Therefore, it is not surprising that the parent's data (or a portion of it) changes when manipulated through this "pointer". After these introductory remarks that hopefully prepared you for what is coming (rather than confuse you too much) we are going to dive right in and start with a description of the indexing commands and some typical examples how they might be used in PDL programs. We will further illustrate the pointer/dataflow analogies in the context of some of the examples later on.
There are two different implementations of this ``smart pointer'' relationship: the first one, which is a little slower but works for any transformation is simply to do the transformation forwards and backwards as necessary. The other is to consider the child ndarray a ``virtual'' ndarray, which only stores a pointer to the parent and access information so that routines which use the child ndarray actually directly access the data in the parent. If the virtual ndarray is given to a routine which cannot use it, PDL transparently physicalizes the virtual ndarray before letting the routine use it.
Currently (1.94_01) all transformations which are ``affine'', i.e. the indices of the data item in the parent ndarray are determined by a linear transformation (+ constant) from the indices of the child ndarray result in virtual ndarrays. All other indexing routines (e.g. >index(...)
) result in physical ndarrays. All routines compiled by PP can accept affine ndarrays (except those routines that pass pointers to external library functions).
Note that whether something is affine or not does not affect the semantics of what you do in any way: both
$x>index(...) .= 5;
$x>slice(...) .= 5;
change the data in $x
. The affinity does, however, have a significant impact on memory usage and performance.
Slicing ndarrays
Probably the most important application of the concept of parent/child ndarrays is the representation of rectangular slices of a physical ndarray by a virtual ndarray. Having talked long enough about concepts let's get more specific. Suppose we are working with a 2D ndarray representing a 5x5 image (it's unusually small so that we can print it without filling several screens full of digits).
pdl> $im = sequence(5,5)
pdl> p $im
[
[ 0 1 2 3 4]
[ 5 6 7 8 9]
[10 11 12 13 14]
[15 16 17 18 19]
[20 21 22 23 24]
]
pdl> help vars
PDL variables in package main::
Name Type Dimension Flow State Mem

$im Double D [5,5] P 0.20Kb
[ here it might be appropriate to quickly talk about the help vars
command that provides information about ndarrays in the interactive perldl
or pdl2
shell that comes with PDL. ]
Now suppose we want to create a 1D ndarray that just references one line of the image, say line 2; or an ndarray that represents all even lines of the image (imagine we have to deal with even and odd frames of an interlaced image due to some peculiar behaviour of our frame grabber). As another frequent application of slices we might want to create an ndarray that represents a rectangular region of the image with top and bottom reversed. All these effects (and many more) can be easily achieved with the powerful slice function:
pdl> $line = $im>slice(':,(2)')
pdl> $even = $im>slice(':,1:1:2')
pdl> $area = $im>slice('3:4,3:1')
pdl> help vars # or just PDL>vars
PDL variables in package main::
Name Type Dimension Flow State Mem

$even Double D [5,2] C 0.00Kb
$im Double D [5,5] P 0.20Kb
$line Double D [5] C 0.00Kb
$area Double D [2,3] C 0.00Kb
All three "child" ndarrays are children of $im
or in the other (largely equivalent) interpretation pointers to data of $im
. Operations on those virtual ndarrays access only those portions of the data as specified by the argument to slice. So we can just print line 2:
pdl> p $line
[10 11 12 13 14]
Also note the difference in the "Flow State" of $area
above and below:
pdl> p $area
pdl> help $area
This variable is Double D [2,3] VC 0.00Kb
The following demonstrates that $im
and $line
really behave as you would expect from a pointerlike object (or in the dataflow picture: the changes in $line
's data are propagated back to $im
):
pdl> $im++
pdl> p $line
[11 12 13 14 15]
pdl> $line += 2
pdl> p $im
[
[ 1 2 3 4 5]
[ 6 7 8 9 10]
[13 14 15 16 17]
[16 17 18 19 20]
[21 22 23 24 25]
]
Note how assignment operations on the child virtual ndarrays change the parent physical ndarray and vice versa (however, the basic "=" assignment doesn't, use ".=" to obtain that effect. See below for the reasons). The virtual child ndarrays are something like "live links" to the "original" parent ndarray. As previously said, they can be thought of to work similar to a Cpointer. But in contrast to a Cpointer they carry a lot more information. Firstly, they specify the structure of the data they represent (the dimensionality of the new ndarray) and secondly, specify how to create this structure from its parents data (the way this works is buried in the internals of PDL and not important for you to know anyway (unless you want to hack the core in the future or would like to become a PDL guru in general (for a definition of this strange creature see PDL::Internals)).
The previous examples have demonstrated typical usage of the slice function. Since the slicing functionality is so important here is an explanation of the syntax for the string argument to slice:
$vpdl = $x>slice('ind0,ind1...')
where ind0
specifies what to do with index No 0 of the ndarray $x
, etc. Each element of the comma separated list can have one of the following forms:
 ':'

Use the whole dimension
 'n'

Use only index
n
. The dimension of this index in the resulting virtual ndarray is 1. An example involving those first two index formats:pdl> $column = $im>slice('2,:') pdl> $row = $im>slice(':,0') pdl> p $column [ [ 3] [ 8] [15] [18] [23] ] pdl> p $row [ [1 2 3 4 5] ] pdl> help $column This variable is Double D [1,5] VC 0.00Kb pdl> help $row This variable is Double D [5,1] VC 0.00Kb
 '(n)'

Use only index
n
. This dimension is removed from the resulting ndarray (relying on the fact that a dimension of size 1 can always be removed). The distinction between this case and the previous one becomes important in assignments where left and right hand side have to have appropriate dimensions.pdl> $line = $im>slice(':,(0)') pdl> help $line This variable is Double D [5] C 0.00Kb pdl> p $line [1 2 3 4 5]
Spot the difference to the previous example?
 'n1:n2' or 'n1:n2:n3'

Take the range of indices from
n1
ton2
or (second form) take the range of indices fromn1
ton2
with stepn3
. An example for the use of this format is the previous definition of the subimage composed of even lines.pdl> $even = $im>slice(':,1:1:2')
This example also demonstrates that negative indices work like they do for normal Perl style arrays by counting backwards from the end of the dimension. If
n2
is smaller thann1
(in the example 1 is equivalent to index 4) the elements in the virtual ndarray are effectively reverted with respect to its parent.  '*[n]'

Add a dummy dimension. The size of this dimension will be 1 by default or equal to
n
if the optional numerical argument is given.Now, this is really something a bit strange on first sight. What is a dummy dimension? A dummy dimension inserts a dimension where there wasn't one before. How is that done ? Well, in the case of the new dimension having size 1 it can be easily explained by the way in which you can identify a vector (with
m
elements) with an(1,m)
or(m,1)
matrix. The same holds obviously for higher dimensional objects. More interesting is the case of a dummy dimensions of size greater than one (e.g.slice('*5,:')
). This works in the same way as a call to the dummy function creates a new dummy dimension. So read on and check its explanation below.  '([n1:n2[:n3]]=i)'

[Not yet implemented ??????] With an argument like this you make generalised diagonals. The diagonal will be dimension no.
i
of the new output ndarray and (if optional part in brackets specified) will extend along the range of indices specified of the respective parent ndarray's dimension. In general an argument like this only makes sense if there are other arguments like this in the same call to slice. The part in brackets is optional for this type of argument. All arguments of this type that specify the same target dimensioni
have to relate to the same number of indices in their parent dimension. The best way to explain it is probably to give an example, here we make an ndarray that refers to the elements along the space diagonal of its parent ndarray (a cube):$cube = zeroes(5,5,5); $sdiag = $cube>slice('(=0),(=0),(=0)');
The above command creates a virtual ndarray that represents the diagonal along the parents' dimension no. 0, 1 and 2 and makes its dimension 0 (the only dimension) of it. You use the extended syntax if the dimension sizes of the parent dimensions you want to build the diagonal from have different sizes or you want to reverse the sequence of elements in the diagonal, e.g.
$rect = zeroes(12,3,5,6,2); $vpdl = $rect>slice('2:7,(0:1=1),(4),(5:4=1),(=1)');
So the elements of $vpdl will then be related to those of its parent in way we can express as:
vpdl(i,j) = rect(i+2,j,4,5j,j) 0<=i<5, 0<=j<2
[ work in the new index function: $y = $x>index($c);
???? ]
There are different kinds of assignments in PDL
The previous examples have already shown that virtual ndarrays can be used to operate on or access portions of data of a parent ndarray. They can also be used as lvalues in assignments (as the use of ++
in some of the examples above has already demonstrated). For explicit assignments to the data represented by a virtual ndarray you have to use the overloaded .=
operator (which in this context we call propagated assignment). Why can't you use the normal assignment operator =
?
Well, you definitely still can use the '=' operator but it wouldn't do what you want. This is due to the fact that the '=' operator cannot be overloaded in the same way as other assignment operators. If we tried to use '=' to try to assign data to a portion of a physical ndarray through a virtual ndarray we wouldn't achieve the desired effect (instead the variable representing the virtual ndarray (a reference to a blessed thingy) would after the assignment just contain the reference to another blessed thingy which would behave to future assignments as a "physical" copy of the original rvalue [this is actually not yet clear and subject of discussions in the PDL developers mailing list]. In that sense it would break the connection of the ndarray to the parent [ isn't this behaviour in a sense the opposite of what happens in dataflow, where .=
breaks the connection to the parent? ].
E.g.
pdl> $line = $im>slice(':,(2)')
pdl> $line = zeroes(5);
pdl> $line++;
pdl> p $im
[
[ 1 2 3 4 5]
[ 6 7 8 9 10]
[13 14 15 16 17]
[16 17 18 19 20]
[21 22 23 24 25]
]
pdl> p $line
[1 1 1 1 1]
But using .=
pdl> $line = $im>slice(':,(2)')
pdl> $line .= zeroes(5)
pdl> $line++
pdl> p $im
[
[ 1 2 3 4 5]
[ 6 7 8 9 10]
[ 1 1 1 1 1]
[16 17 18 19 20]
[21 22 23 24 25]
]
pdl> print $line
[1 1 1 1 1]
Also, you can substitute
pdl> $line .= 0;
for the assignment above (the zero is converted to a scalar ndarray, with no dimensions so it can be assigned to any ndarray).
A nice feature in recent perl versions is lvalue subroutines (i.e., versions 5.6.x and higher including all perls currently supported by PDL). That allows one to use the slicing syntax on both sides of the assignment:
pdl> $im>slice(':,(2)') .= zeroes(5)>xvals>float
Related to the lvalue sub assignment feature is a little trap for the unwary: recent perls introduced a "feature" which breaks PDL's use of lvalue subs for slice assignments when running under the perl debugger, perl d
. Under the debugger, the above usage gives an error like: Can't return a temporary from lvalue subroutine...
So you must use syntax like this:
pdl> ($pdl = $im>slice(':,(2)')) .= zeroes(5)>xvals>float
which works both with and without the debugger but is arguably clumsy and awkward to read.
Note that there can be a problem with assignments like this when lvalue and rvalue ndarrays refer to overlapping portions of data in the parent ndarray:
# revert the elements of the first line of $x
($tmp = $x>slice(':,(1)')) .= $x>slice('1:0,(1)');
Currently, the parent data on the right side of the assignments is not copied before the (internal) assignment loop proceeds. Therefore, the outcome of this assignment will depend on the sequence in which elements are assigned and almost certainly not do what you wanted. So the semantics are currently undefined for now and liable to change anytime. To obtain the desired behaviour, use
($tmp = $x>slice(':,(1)')) .= $x>slice('1:0,(1)')>copy;
which makes a physical copy of the slice or
($tmp = $x>slice(':,(1)')) .= $x>slice('1:0,(1)')>sever;
which returns the same slice but severs the connection of the slice to its parent.
Other functions that manipulate dimensions
Having talked extensively about the slice function it should be noted that this is not the only PDL indexing function. There are additional indexing functions which are also useful (especially in the context of threading which we will talk about later). Here are a list and some examples how to use them.
dummy

inserts a dummy dimension of the size you specify (default 1) at the chosen location. You can't wait to hear how that is achieved? Well, all elements with index
(X,x,Y)
(0<=x<size_of_dummy_dim
) just map to the element with index(X,Y)
of the parent ndarray (whereX
andY
refer to the group of indices before and after the location where the dummy dimension was inserted.)This example calculates the x coordinate of the centroid of an image (later we will learn that we didn't actually need the dummy dimension thanks to the magic of implicit threading; but using dummy dimensions the code would also work in a threadless world; though once you have worked with PDL threads you wouldn't want to live without them again).
# centroid ($xd,$yd) = $im>dims; $xc = sum($im*xvals(zeroes($xd))>dummy(1,$yd))/sum($im);
Let's explain how that works in a little more detail. First, the product:
$xvs = xvals(zeroes($xd)); print $xvs>dummy(1,$yd); # repeat the line $yd times $prod = $im*xvs>dummy(1,$yd); # form the pixelwise product with # the repeated line of xvalues
The rest is then summing the results of the pixelwise product together and normalizing with the sum of all pixel values in the original image thereby calculating the xcoordinate of the "center of mass" of the image (interpreting pixel values as local mass) which is known as the centroid of an image.
Next is a (from the point of view of memory consumption) very cheap conversion from greyscale to RGB, i.e. every pixel holds now a triple of values instead of a scalar. The three values in the triple are, fortunately, all the same for a grey image, so that our trick works well in that it maps all the three members of the triple to the same source element:
# a cheap greyscale to RGB conversion $rgb = $grey>dummy(0,3)
Unfortunately this trick cannot be used to convert your old B/W photos to color ones in the way you'd like. :(
Note that the memory usage of ndarrays with dummy dimensions is especially sensitive to the internal representation. If the ndarray can be represented as a virtual affine (``vaffine'') ndarray, only the control structures are stored. But if
$y
in$x = zeroes(10000); $y = $x>dummy(1,10000);
is made physical by some routine, you will find that the memory usage of your program has suddenly grown by 100Mb.
diagonal

replaces two dimensions (which have to be of equal size) by one dimension that references all the elements along the "diagonal" along those two dimensions. Here, we have two examples which should appear familiar to anyone who has ever done some linear algebra. Firstly, make a unity matrix:
# unity matrix $e = zeroes(float, 3, 3); # make everything zero ($tmp = $e>diagonal(0,1)) .= 1; # set the elements along the diagonal to 1 print $e;
Or the other diagonal:
($tmp = $e>slice(':1:0')>diagonal(0,1)) .= 2; print $e;
(Did you notice how we used the slice function to revert the sequence of lines before setting the diagonal of the new child, thereby setting the cross diagonal of the parent ?) Or a mapping from the space of diagonal matrices to the field over which the matrices are defined, the trace of a matrix:
# trace of a matrix $trace = sum($mat>diagonal(0,1)); # sum all the diagonal elements
xchg
andmv

xchg exchanges or "transposes" the two specified dimensions. A straightforward example:
# transpose a matrix (without explicitly reshuffling data and # making a copy) $prod = $x x $x>xchg(0,1);
$prod
should now be pretty close to the unity matrix if$x
is an orthogonal matrix. Oftenxchg
will be used in the context of threading but more about that later.mv works in a similar fashion. It moves a dimension (specified by its number in the parent) to a new position in the new child ndarray:
$y = $x>mv(4,0); # make the 5th dimension of $x the first in the # new child $y
The difference between
xchg
andmv
is thatxchg
only changes the position of two dimensions with each other, whereasmv
inserts the first dimension to the place of second, moving the other dimensions around accordingly. clump

collapses several dimensions into one. Its only argument specifies how many dimensions of the source ndarray should be collapsed (starting from the first). An (admittedly unrealistic) example is a 3D ndarray which holds data from a stack of image files that you have just read in. However, the data from each image really represents a 1D time series and has only been arranged that way because it was digitized with a frame grabber. So to have it again as an array of time sequences you say
pdl> $seqs = $stack>clump(2) pdl> help vars PDL variables in package main:: Name Type Dimension Flow State Mem  $seqs Double D [8000,50] C 0.00Kb $stack Double D [100,80,50] P 3.05Mb
Unrealistic as it may seem, our confocal microscope software writes data (sometimes) this way. But more often you use clump to achieve a certain effect when using implicit or explicit threading.
Calls to indexing functions can be chained
As you might have noticed in some of the examples above calls to the indexing functions can be nicely chained since all of these functions return a newly created child object. However, when doing extensive index manipulations in a chain be sure to keep track of what you are doing, e.g.
$x>xchg(0,1)>mv(0,4)
moves the dimension 1 of $x
to position 4 since when the second command is executed the original dimension 1 has been moved to position 0 of the new child that calls the mv
function. I think you get the idea (in spite of my convoluted explanations).
Propagated assignments ('.=') and dummy dimensions
A subtlety related to indexing is the assignment to ndarrays containing dummy dimensions of size greater than 1. These assignments (using .=
) are forbidden since several elements of the lvalue ndarray point to the same element of the parent. As a consequence the value of those parent elements are potentially ambiguous and would depend on the sequence in which the implementation makes the assignments to elements. Therefore, an assignment like this:
$x = pdl [1,2,3];
$y = $x>dummy(1,4);
$y .= yvals(zeroes(3,4));
can produce unexpected results and the results are explicitly undefined by PDL because when PDL gets parallel computing features, the current result may well change.
From the point of view of dataflow the introduction of greatersizethanone dummy dimensions is regarded as an irreversible transformation (similar to the terminology in thermodynamics) which precludes backward propagation of assignment to a parent (which you had explicitly requested using the .=
assignment). A similar problem to watch out for occurs in the context of threading where sometimes dummy dimensions are created implicitly during the thread loop (see below).
Reasons for the parent/child (or "pointer") concept
[ this will have to wait a bit ]
XXXXX being memory efficient
XXXXX in the context of threading
XXXXX very flexible and powerful way of accessing portions of ndarray data
(in much more general way than sec, etc allow)
XXXXX efficient implementation
XXXXX difference to section/at, etc.
How to make things physical again
[ XXXXX fill in later when everything has settled a bit more ]
** When needed (xsub routine interfacing C lib function)
** How achieved (>physical)
** How to test (isphysical (explain how it works currently))
** >copy and >sever
Threading
In the previous paragraph on indexing we have already mentioned the term occasionally but now its really time to talk explicitly about "threading" with ndarrays. The term threading has many different meanings in different fields of computing. Within the framework of PDL it could probably be loosely defined as an implicit looping facility. It is implicit because you don't specify anything like enclosing forloops but rather the loops are automatically (or 'magically') generated by PDL based on the dimensions of the ndarrays involved. This should give you a first idea why the index/dimension manipulating functions you have met in the previous paragraphs are especially important and useful in the context of threading. The other ingredient for threading (apart from the ndarrays involved) is a function that is threading aware (generally, these are PDL::PP compiled functions) and that the ndarrays are "threaded" over. So much about the terminology and now let's try to shed some light on what it all means.
Implicit threading  a first example
There are two slightly different variants of threading. We start with what we call "implicit threading". Let's pick a practical example that involves looping of a function over many elements of a ndarray. Suppose we have an RGB image that we want to convert to greyscale. The RGB image is represented by a 3dim ndarray im(3,x,y)
where the first dimension contains the three color components of each pixel and x
and y
are width and height of the image, respectively. Next we need to specify how to convert a colortriple at a given pixel into a greyvalue (to be a realistic example it should represent the relative intensity with which our color insensitive eye cells would detect that color to achieve what we would call a natural conversion from color to greyscale). An approximation that works quite well is to compute the grey intensity from each RGB triplet (r,g,b) as a weighted sum
greyvalue = 77/256*r + 150/256*g + 29/256*b =
inner([77,150,29]/256, [r,g,b])
where the last form indicates that we can write this as an inner product of the 3vector comprising the weights for red, green and blue components with the 3vector containing the color components. Traditionally, we might have written a function like the following to process the whole image:
my @dims=$im>dims;
# here normally check that first dim has correct size (3), etc
$grey=zeroes(@dims[1,2]); # make the ndarray for the resulting grey image
$w = pdl [77,150,29] / 256; # the vector of weights
for ($j=0;$j<dims[2];$j++) {
for ($i=0;$i<dims[1];$i++) {
# compute the pixel value
$tmp = inner($w,$im>slice(':,(i),(j)'));
set($grey,$i,$j,$tmp); # and set it in the greyscale image
}
}
Now we write the same using threading (noting that inner
is a threading aware function defined in the PDL::Primitive package)
$grey = inner($im,pdl([77,150,29]/256));
We have ended up with a oneliner that automatically creates the ndarray $grey
with the right number and size of dimensions and performs the loops automatically (these loops are implemented as fast C code in the internals of PDL). Well, we still owe you an explanation how this 'magic' is achieved.
How does the example work ?
The first thing to note is that every function that is threading aware (these are without exception functions compiled from concise descriptions by PDL::PP, later just called PPfunctions) expects a defined (minimum) number of dimensions (we call them core dimensions) from each of its ndarray arguments. The inner function expects two onedimensional (input) parameters from which it calculates a zerodimensional (output) parameter. We write that symbolically as inner((n),(n),[o]())
and call it inner
's signature, where n represents the size of that dimension. n being equal in the first and second parameter means that those dimensions have to be of equal size in any call. As a different example take the outer product which takes two 1D vectors to generate a 2D matrix, symbolically written as outer((n),(m),[o](n,m))
. The [o]
in both examples indicates that this (here third) argument is an output argument. In the latter example the dimensions of first and second argument don't have to agree but you see how they determine the size of the two dimensions of the output ndarray.
Here is the point when threading finally enters the game. If you call PPfunctions with ndarrays that have more than the required core dimensions the first dimensions of the ndarray arguments are used as the core dimensions and the additional extra dimensions are threaded over. Let us demonstrate this first with our example above
$grey = inner($im,$w); # w is the weight vector from above
In this case $w is 1D and so supplied just the core dimension, $im
is 3D, more specifically (3,x,y)
. The first dimension (of size 3) is the required core dimension that matches (as required by inner) the first (and only) dimension of $w
. The second dimension is the first thread dimension (of size x
) and the third is here the second thread dimension (of size y
). The output ndarray is automatically created (as requested by setting $grey
to "null" prior to invocation). The output dimensions are obtained by appending the loop dimensions (here (x,y)
) to the core output dimensions (here 0D) to yield the final dimensions of the autocreated ndarray (here 0D+2D=2D
to yield a 2D output of size (x,y)
).
So the above command calls the core functionality that computes the inner product of two 1D vectors x*y
times with $w
and all 1D slices of the form (':,(i),(j)')
of $im
and sets the respective elements of the output ndarray $grey(i,j)
to the result of each computation. We could write that symbolically as
$grey(0,0) = f($w,$im(:,(0),(0)))
$grey(1,0) = f($w,$im(:,(1),(0)))
.
.
.
$grey(x2,y1) = f($w,$im(:,(x2),(y1)))
$grey(x1,y1) = f($w,$im(:,(x1),(y1)))
But this is done automatically by PDL without writing any explicit Perl loops. We see that the command really creates an output ndarray with the right dimensions and sets the elements indeed to the result of the computation for each pixel of the input image.
When even more ndarrays and extra dimensions are involved things get a bit more complicated. We will first give the general rules how the thread dimensions depend on the dimensions of input ndarrays enabling you to figure out the dimensionality of an autocreated output ndarray (for any given set of input ndarrays and core dimensions of the PPfunction in question). The general rules will most likely appear a bit confusing on first sight so that we'll set out to illustrate the usage with a set of further examples (which will hopefully also demonstrate that there are indeed many practical situations where threading comes in extremely handy).
A call for coding discipline
Before we point out the other technical details of threading, please note this call for programming discipline when using threading:
In order to preserve human readability, PLEASE comment any nontrivial expression in your code involving threading. Most importantly, for any subroutine, include information at the beginning about what you expect the dimensions to represent (or ranges of dimensions).
As a warning, look at this undocumented function and try to guess what might be going on:
sub lookup {
my ($im,$palette) = @_;
my $res;
index($palette>xchg(0,1),
$im>long>dummy(0,($palette>dim)[0]),
($res=null));
return $res;
}
Would you agree that it might be difficult to figure out expected dimensions, purpose of the routine, etc ? (If you want to find out what this piece of code does, see below)
How to figure out the loop dimensions
There are a couple of rules that allow you to figure out number and size of loop dimensions (and if the size of your input ndarrays comply with the threading rules). Dimensions of any ndarray argument are broken down into two groups in the following: Core dimensions (as defined by the PPfunction, see Appendix B for a list of PDL primitives) and extra dimensions which comprises all remaining dimensions of that ndarray. For example calling a function func
with the signature func((n,m),[o](n))
with an ndarray $x(2,4,7,1,3)
as f($x,($o = null))
results in the semantic splitting of x's dimensions into: core dimensions (2,4)
and extra dimensions (7,1,3)
.
 R0

Core dimensions are identified with the first N dimensions of the respective ndarray argument (and are required). Any further dimensions are extra dimensions and used to determine the loop dimensions.
 R1

The number of (implicit) loop dimensions is equal to the maximal number of extra dimensions taken over the set of ndarray arguments.
 R2

The size of each of the loop dimensions is derived from the size of the respective dimensions of the ndarray arguments. The size of a loop dimension is given by the maximal size found in any of the ndarrays having this extra dimension.
 R3

For all ndarrays that have a given extra dimension the size must be equal to the size of the loop dimension (as determined by the previous rule) or 1; otherwise you raise a runtime exception. If the size of the extra dimension in an ndarray is one it is implicitly treated as a dummy dimension of size equal to that loop dim size when performing the thread loop.
 R4

If an ndarray doesn't have a loop dimension, in the thread loop this ndarray is treated as if having a dummy dimension of size equal to the size of that loop dimension.
 R5

If output autocreation is used (by setting the relevant ndarray to
PDL>null
before invocation) the number of dimensions of the created ndarray is equal to the sum of the number of core output dimensions + number of loop dimensions. The size of the core output dimensions is derived from the relevant dimension of input ndarrays (as specified in the function definition) and the sizes of the other dimensions are equal to the size of the loop dimension it is derived from. The automatically created ndarray will be physical (unless dataflow is in operation).
In this context, note that you can run into the problem with assignment to ndarrays containing greaterthanone dummy dimensions (see above). Although your output ndarray(s) didn't contain any dummy dimensions in the first place they may end up with implicitly created dummy dimensions according to R4.
As an example, suppose we have a (here unspecified) PPfunction with the signature:
func((m,n),(m,n,o),(m),[o](m,o))
and you call it with 3 ndarrays $x(5,3,10,11)
, $y(5,3,2,10,1,12)
, and $z(5,1,11,12)
as
func($x,$y,$z,($d=null))
then the number of loop dimensions is 3 (by R0+R1
from $y
and $z
) with sizes (10,11,12)
(by R2); the two output core dimensions are (5,2)
(from the signature of func) resulting in a 5dimensional output ndarray $c
of size (5,2,10,11,12)
(see R5) and (the automatically created) $d
is derived from ($x,$y,$z)
in a way that can be expressed in pdl pseudocode as
$d(:,:,i,j,k) .= func($x(:,:,i,j),$y(:,:,:,i,0,k),$z(:,0,j,k))
with 0<=i<10, 0<=j<=11, 0<=k<12
If we analyze the color to greyscale conversion again with these rules in mind we note another great advantage of implicit threading. We can call the conversion with an ndarray representing a pixel (im(3)
), a line of rgb pixels (im(3,x)
), a proper color image (im(3,x,y)
) or a whole stack of RGB images (im(3,x,y,z)
). As long as $im
is of the form (3,...)
the automatically created output ndarray will contain the right number of dimensions and contain the intensity data as we expect it since the loops have been implicitly performed thanks to implicit threading. You can easily convince yourself that calling with a color pixel $grey
is 0D, with a line it turns out 1D grey(x)
, with an image we get grey(x,y)
and finally we get a converted image stack grey(x,y,z)
.
Let's fill these general rules with some more life by going through a couple of further examples. The reader may try to figure out equivalent formulations with explicit forlooping and compare the flexibility of those routines using implicit threading to the explicit formulation. Furthermore, especially when using several thread dimensions it is a useful exercise to check the relative speed by doing some benchmark tests (which we still have to do).
First in the row is a slightly reworked centroid example, now coded with threading in mind.
# threaded mult to calculate centroid coords, works for stacks as well
$xc = sumover(($im*xvals(($im>dims)[0]))>clump(2)) /
sumover($im>clump(2));
Let's analyze what's going on step by step. First the product:
$prod = $im*xvals(zeroes(($im>dims)[0]))
This will actually work for $im
being one, two, three, and higher dimensional. If $im
is onedimensional it's just an ordinary product (in the sense that every element of $im
is multiplied with the respective element of xvals(...)
), if $im
has more dimensions further threading is done by adding appropriate dummy dimensions to xvals(...)
according to R4. More importantly, the two sumover operations show a first example of how to make use of the dimension manipulating commands. A quick look at sumover's signature will remind you that it will only "gobble up" the first dimension of a given input ndarray. But what if we want to really compute the sum over all elements of the first two dimensions? Well, nothing keeps us from passing a virtual ndarray into sumover which in this case is formed by clumping the first two dimensions of the "parent ndarray" into one. From the point of view of the parent ndarray the sum is now computed over the first two dimensions, just as we wanted, though sumover has just done the job as specified by its signature. Got it ?
Another little finesse of writing the code like that: we intentionally used sumover($pdl>clump(2))
instead of sum($pdl)
so that we can either pass just an image (x,y)
or a stack of images (x,y,t)
into this routine and get either just one xcoordiante or a vector of xcoordinates (of size t) in return.
Another set of common operations are what one could call "projection operations". These operations take a ND ndarray as input and return a (N1)D "projected" ndarray. These operations are often performed with functions like sumover, prodover, minimum and maximum. Using again images as examples we might want to calculate the maximum pixel value for each line of an image or image stack. We know how to do that
# maxima of lines (as function of line number and time)
maximum($stack,($ret=null));
But what if you want to calculate maxima per column when implicit threading always applies the core functionality to the first dimension and threads over all others? How can we achieve that instead the core functionality is applied to the second dimension and threading is done over the others. Can you guess it? Yes, we make a virtual ndarray that has the second dimension of the "parent ndarray" as its first dimension using the mv
command.
# maxima of columns (as function of column number and time)
maximum($stack>mv(1,0),($ret=null));
and calculating all the sums of subslices over the third dimension is now almost too easy
# sums of pixels in time (assuming time is the third dim)
sumover($stack>mv(2,0),($ret=null));
Finally, if you want to apply the operation to all elements (like max over all elements or sum over all elements) regardless of the dimensions of the ndarray in question clump
comes in handy. As an example look at the definition of sum
(as defined in Ufunc.pm
):
sub sum {
PDL::Ufunc::sumover($name>clump(1),($tmp=null));
return $tmp>at(); # return a Perl number, not a 0D ndarray
}
We have already mentioned that all basic operations support threading and assignment is no exception. So here are a couple of threaded assignments
pdl> $im = zeroes(byte, 10,20)
pdl> $line = exp(rvals(10)**2/9)
# threaded assignment
pdl> $im .= $line # set every line of $im to $line
pdl> $im2 .= 5 # set every element of $im2 to 5
By now you probably see how it works and what it does, don't you?
To finish the examples in this paragraph here is a function to create an RGB image from what is called a palette image. The palette image consists of two parts: an image of indices into a color lookup table and the color lookup table itself. [ describe how it works ] We are going to use a PPfunction we haven't encoutered yet in the previous examples. It is the aptly named index function, signature ((n),(),[o]())
(see Appendix B) with the core functionality that index(pdl (0,2,4,5),2,($ret=null))
will return the element with index 2 of the first input ndarray. In this case, $ret
will contain the value 4. So here is the example:
# a threaded index lookup to generate an RGB, or RGBA or YMCK image
# from a palette image (represented by a lookup table $palette and
# an colorindex image $im)
# you can say just dummy(0) since the rules of threading make it fit
pdl> index($palette>xchg(0,1),
$im>long>dummy(0,($palette>dim)[0]),
($res=null));
Let's go through it and explain the steps involved. Assuming we are dealing with an RGB lookuptable $palette is of size (3,x)
. First we exchange the dimensions of the palette so that looping is done over the first dimension of $palette
(of size 3 that represent r, g, and b components). Now looking at $im
, we add a dummy dimension of size equal to the length of the number of components (in the case we are discussing here we could have just used the number 3 since we have 3 color components). We can use a dummy dimension since for red, green and blue color components we use the same index from the original image, e.g. assuming a certain pixel of $im
had the value 4 then the lookup should produce the triple
[palette(0,4),palette(1,4),palette(2,4)]
for the new red, green and blue components of the output image. Hopefully by now you have some sort of idea what the above piece of code is supposed to do (it is often actually quite complicated to describe in detail how a piece of threading code works; just go ahead and experiment a bit to get a better feeling for it).
If you have read the threading rules carefully, then you might have noticed that we didn't have to explicitly state the size of the dummy dimension that we created for $im
; when we create it with size 1 (the default) the rules of threading make it automatically fit to the desired size (by rule R3, in our example the size would be 3 assuming a palette of size (3,x)
). Since situations like this do occur often in practice this is actually why rule R3 has been introduced (the part that makes dimensions of size 1 fit to the thread loop dim size). So we can just say
pdl> index($palette>xchg(0,1),$im>long>dummy(0),($res=null));
Again, you can convince yourself that this routine will create the right output if called with a pixel ($im
is 0D), a line ($im
is 1D), an image ($im
is 2D), ..., an RGB lookup table (palette is (3,x)
) and RGBA lookup table (palette is (4,x)
, see e.g. OpenGL). This flexibility is achieved by the rules of threading which are made to do the right thing in most situations.
To wrap it all up once again, the general idea is as follows. If you want to achieve looping over certain dimensions and have the core functionality applied to another specified set of dimensions you use the dimension manipulating commands to create a (or several) virtual ndarray(s) so that from the point of view of the parent ndarray(s) you get what you want (always having the signature of the function in question and R1R5 in mind!). Easy, isn't it ?
Output autocreation and PPfunction calling conventions
At this point we have to divert to some technical detail that has to do with the general calling conventions of PPfunctions and the automatic creation of output arguments. Basically, there are two ways of invoking PDL routines, namely
$result = func($x,$y);
and
func($x,$y,$result);
If you are only using implicit threading then the output variable can be automatically created by PDL. You flag that to the PPfunction by setting the output argument to a special kind of ndarray that is returned from a call to the function PDL>null
that returns an essentially "empty" ndarray (for those interested in details there is a flag in the C pdl structure for this). The dimensions of the created ndarray are determined by the rules of implicit threading: the first dimensions are the core output dimensions to which the threading dimensions are appended (which are in turn determined by the dimensions of the input ndarrays as described above). So you can say
func($x,$y,($result=PDL>null));
or
$result = func($x,$y)
which are exactly equivalent.
Be warned that you can not use output autocreation when using explicit threading (for reasons explained in the following section on explicit threading, the second variant of threading).
In "tight" loops you probably want to avoid the implicit creation of a temporary ndarray in each step of the loop that comes along with the "functional" style but rather say
# create output ndarray of appropriate size only at first invocation
$result = null;
for (0...$n) {
func($x,$y,$result); # in all but the first invocation $result
func2($y); # is defined and has the right size to
# take the output provided $y's dims don't change
twiddle($result,$x); # do something from $result to $x for iteration
}
The takehome message of this section once more: be aware of the limitation on output creation when using explicit threading.
Explicit threading
Having so far only talked about the first flavour of threading it is now about time to introduce the second variant. Instead of shuffling around dimensions all the time and relying on the rules of implicit threading to get it all right you sometimes might want to specify in a more explicit way how to perform the thread loop. It is probably not too surprising that this variant of the game is called explicit threading. Now, before we create the wrong impression: it is not either implicit or explicit; the two flavours do mix. But more about that later.
The two most used functions with explicit threading are thread and unthread. We start with an example that illustrates typical usage of the former:
[ # ** this is the worst possible example to start with ]
# but can be used to show that $mat += $line is different from
# $mat>thread(0) += $line
# explicit threading to add a vector to each column of a matrix
pdl> $mat = zeroes(4,3)
pdl> $line = pdl (3.1416,2,2)
pdl> ($tmp = $mat>thread(0)) += $line
In this example, $mat>thread(0)
tells PDL that you want the second dimension of this ndarray to be threaded over first leading to a thread loop that can be expressed as
for (j=0; j<3; j++) {
for (i=0; i<4; i++) {
mat(i,j) += src(j);
}
}
thread
takes a list of numbers as arguments which explicitly specify which dimensions to thread over first. With the introduction of explicit threading the dimensions of an ndarray are conceptually split into three different groups the latter two of which we have already encountered: thread dimensions, core dimensions and extra dimensions.
Conceptually, it is best to think of those dimensions of an ndarray that have been specified in a call to thread
as being taken away from the set of normal dimensions and put on a separate stack. So assuming we have an ndarray x(4,7,2,8)
saying
$y = $x>thread(2,1)
creates a new virtual ndarray of dimension y(4,8)
(which we call the remaining dims) that also has 2 thread dimensions of size (2,7)
. For the purposes of this document we write that symbolically as y(4,8){2,7}
. An important difference to the previous examples where only implicit threading was used is the fact that the core dimensions are matched against the remaining dimensions which are not necessarily the first dimensions of the ndarray. We will now specify how the presence of thread dimensions changes the rules R1R5 for thread loops (which apply to the special case where none of the ndarray arguments has any thread dimensions).
 T0

Core dimensions are matched against the first n remaining dimensions of the ndarray argument (note the difference to R1). Any further remaining dimensions are extra dimensions and are used to determine the implicit loop dimensions.
 T1a

The number of implicit loop dimensions is equal to the maximal number of extra dimensions taken over the set of ndarray arguments.
 T1b

The number of explicit loop dimensions is equal to the maximal number of thread dimensions taken over the set of ndarray arguments.
 T1c

The total number of loop dimensions is equal to the sum of explicit loop dimensions and implicit loop dimensions. In the thread loop, explicit loop dimensions are threaded over first followed by implicit loop dimensions.
 T2

The size of each of the loop dimensions is derived from the size of the respective dimensions of the ndarray arguments. It is given by the maximal size found in any ndarrays having this thread dimension (for explicit loop dimensions) or extra dimension (for implicit loop dimensions).
 T3

This rule applies to any explicit loop dimension as well as any implicit loop dimension. For all ndarrays that have a given thread/extra dimension the size must be equal to the size of the respective explicit/implicit loop dimension or 1; otherwise you raise a runtime exception. If the size of a thread/extra dimension of an ndarray is one it is implicitly treated as a dummy dimension of size equal to the explicit/implicit loop dimension.
 T4

If an ndarray doesn't have a thread/extra dimension that corresponds to an explicit/implicit loop dimension, in the thread loop this ndarray is treated as if having a dummy dimension of size equal to the size of that loop dimension.
 T4a

All ndarrays that do have thread dimensions must have the same number of thread dimensions.
 T5

Output autocreation cannot be used if any of the ndarray arguments has any thread dimensions. Otherwise R5 applies.
The same restrictions apply with regard to implicit dummy dimensions (created by application of T4) as already mentioned in the section on implicit threading: if any of the output ndarrays has an (explicit or implicitly created) greaterthanone dummy dimension a runtime exception will be raised.
Let us demonstrate these rules at work in a generic case. Suppose we have a (here unspecified) PPfunction with the signature:
func((m,n),(m),(),[o](m))
and you call it with 3 ndarrays a(5,3,10,11)
, b(3,5,10,1,12)
, c(10)
and an output ndarray d(3,11,5,10,12)
(which can here not be automatically created) as
func($x>thread(1,3),$y>thread(0,3),$c,$d>thread(0,1))
From the signature of func and the above call the ndarrays split into the following groups of core, extra and thread dimensions (written in the form pdl(core dims){thread dims}[extra dims]
):
a(5,10){3,11}[] b(5){3,1}[10,12] c(){}[10] d(5){3,11}[10,12]
With this to help us along (it is in general helpful to write the arguments down like this when you start playing with threading and want to keep track of what is going on) we further deduce that the number of explicit loop dimensions is 2 (by T1b from $a
and $b
) with sizes (3,11)
(by T2); 2 implicit loop dimensions (by T1a from $b
and $d
) of size (10,12)
(by T2) and the elements of are computed from the input ndarrays in a way that can be expressed in pdl pseudocode as
for (l=0;l<12;l++)
for (k=0;k<10;k++)
for (j=0;j<11;j++) effect of treating it as dummy dim (index j)
for (i=0;i<3;i++) 
d(i,j,:,k,l) = func(a(:,i,:,j),b(i,:,k,0,l),c(k))
Ugh, this example was really not easy in terms of bookkeeping. It serves mostly as an example how to figure out what's going on when you encounter a complicated looking expression. But now it is really time to show that threading is useful by giving some more of our so called "practical" examples.
[ The following examples will need some additional explanations in the future. For the moment please try to live with the comments in the code fragments. ]
Example 1:
*** inverse of matrix represented by eigvecs and eigvals
** given a symmetrical matrix M = A^T x diag(lambda_i) x A
** => inverse M^1 = A^T x diag(1/lambda_i) x A
** first $tmp = diag(1/lambda_i)*A
** then A^T * $tmp by threaded inner product
# index handling so that matrices print correct under pdl
$inv .= $evecs*0; # just copy to get appropriately sized output
$tmp .= $evecs; # initialise, no backpropagation
($tmp2 = $tmp>thread(0)) /= $evals; # threaded division
# and now a matrix multiplication in disguise
PDL::Primitive::inner($evecs>xchg(0,1)>thread(1,1),
$tmp>thread(0,1),
$inv>thread(0,1));
# alternative for matrix mult using implicit threading,
# first xchg only for transpose
PDL::Primitive::inner($evecs>xchg(0,1)>dummy(1),
$tmp>xchg(0,1)>dummy(2),
($inv=null));
Example 2:
# outer product by threaded multiplication
# stress that we need to do it with explicit call to my_biop1
# when using explicit threading
$res=zeroes(($x>dims)[0],($y>dims)[0]);
my_biop1($x>thread(0,1),$y>thread(1,0),$res>(0,1),"*");
# similar thing by implicit threading with autocreated ndarray
$res = $x>dummy(1) * $y>dummy(0);
Example 3:
# different use of thread and unthread to shuffle a number of
# dimensions in one go without lots of calls to >xchg and >mv
# use thread/unthread to shuffle dimensions around
# just try it out and compare the child ndarray with its parent
$trans = $x>thread(4,1,0,3,2)>unthread;
Example 4:
# calculate a couple of bounding boxes
# $bb will hold BB as [xmin,xmax],[ymin,ymax],[zmin,zmax]
# we use again thread and unthread to shuffle dimensions around
pdl> $bb = zeroes(double, 2,3 );
pdl> minimum($vertices>thread(0)>clump>unthread(1), $bb>slice('(0),:'));
pdl> maximum($vertices>thread(0)>clump>unthread(1), $bb>slice('(1),:'));
Example 5:
# calculate a selfrationed (i.e. self normalized) sequence of images
# uses explicit threading and an implicitly threaded division
$stack = read_image_stack();
# calculate the average (per pixel average) of the first $n+1 images
$aver = zeroes([stack>dims]>[0,1]); # make the output ndarray
sumover($stack>slice(":,:,0:$n")>thread(0,1),$aver);
$aver /= ($n+1);
$stack /= $aver; # normalize the stack by doing a threaded division
# implicit versus explicit
# alternatively calculate $aver with implicit threading and autocreation
sumover($stack>slice(":,:,0:$n")>mv(2,0),($aver=null));
$aver /= ($n+1);
#
Implicit versus explicit threading
In this paragraph we are going to illustrate when explicit threading is preferable over implicit threading and vice versa. But then again, this is probably not the best way of putting the case since you already know: the two flavours do mix. So, it's more about how to get the best of both worlds and, anyway, in the best of Perl traditions: TIMTOWTDI !
[ Sorry, this still has to be filled in in a later release; either refer to above examples or choose some new ones ]
Finally, this may be a good place to justify all the technical detail we have been going on about for a couple of pages: why threading ?
Well, code that uses threading should be (considerably) faster than code that uses explicit forloops (or similar Perl constructs) to achieve the same functionality. Especially on supercomputers (with vector computing facilities/parallel processing) PDL threading will be implemented in a way that takes advantage of the additional facilities of these machines. Furthermore, it is a conceptually simply construct (though technical details might get involved at times) and can greatly reduce the syntactical complexity of PDL code (but keep the admonition for documentation in mind). Once you are comfortable with the threading way of thinking (and coding) it shouldn't be too difficult to understand code that somebody else has written than (provided he gave you an idea what expected input dimensions are, etc.). As a general tip to increase the performance of your code: if you have to introduce a loop into your code try to reformulate the problem so that you can use threading to perform the loop (as with anything there are exceptions to this rule of thumb; but the authors of this document tend to think that these are rare cases ;).
PDL::PP
An easy way to define functions that are aware of indexing and threading (and the universe and everything)
PDL:PP is part of the PDL distribution. It is used to generate functions that are aware of indexing and threading rules from very concise descriptions. It can be useful for you if you want to write your own functions or if you want to interface functions from an external library so that they support indexing and threading (and maybe dataflow as well, see PDL::Dataflow). For further details check PDL::PP.
Appendix A
Affine transformations  a special class of simple and powerful transformations
[ This is also something to be added in future releases. Do we already have the general make_affine routine in PDL ? It is possible that we will reference another appropriate man page from here ]
Appendix B
signatures of standard PDL::PP compiled functions
A selection of signatures of PDL primitives to show how many dimensions PP compiled functions gobble up (and therefore you can figure out what will be threaded over). Most of those functions are the basic ones defined in primitive.pd
# functions in primitive.pd
#
sumover ((n),[o]())
prodover ((n),[o]())
axisvalues ((n)) inplace
inner ((n),(n),[o]())
outer ((n),(m),[o](n,m))
innerwt ((n),(n),(n),[o]())
inner2 ((m),(m,n),(n),[o]())
inner2t ((j,n),(n,m),(m,k),[o]())
index (1D,0D,[o])
minimum (1D,[o])
maximum (1D,[o])
wstat ((n),(n),(),[o],())
assgn ((),())
# basic operations
binary operations ((),(),[o]())
unary operations ((),[o]())
AUTHOR & COPYRIGHT
Copyright (C) 1997 Christian Soeller (c.soeller@auckland.ac.nz) & Tuomas J. Lukka (lukka@fas.harvard.edu). All rights reserved. Although destined for release as a man page with the standard PDL distribution, it is not public domain. Permission is granted to freely distribute verbatim copies of this document provided that no modifications outside of formatting be made, and that this notice remain intact. You are permitted and encouraged to use its code and derivatives thereof in your own source code for fun or for profit as you see fit.