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<p>Dyadic iota (<apll>L⍳R</apll>) is extended to allow <apll>1&lt;⍴⍴L</apll>, returning a nested array of shape <apll>⍴R</apll> whose items are each integer vectors of length <apll>⍴⍴R</apll>, suitable for use as indices to <apll>L</apll>.</p>
<table border="1" cellpadding="5" cellspacing="0" rules="none" summary="">
<tr>
  <td>
    <table border="0" cellpadding="5" cellspacing="0" summary="">
    <tr>
      <td valign="top"><apll>Z←L⍳R</apll></td>
      <td></td>
      <td></td>
      <td>returns a nested array of indices suitable to indexing <apll>L</apll>.</td>
    </tr>
    </table>
  </td>
</tr>
<tr>
  <td><apll>L</apll> is an array of rank not equal 1.</td>
</tr>
<tr>
  <td><apll>R</apll> is an arbitrary array.</td>
</tr>
<tr>
  <td><apll>Z</apll> is a nested array of shape <apll>⍴R</apll> whose items are each integer vectors of length <apll>⍴⍴L</apll>, suitable for use as indices to <apll>L</apll>, except for where the item in <apll>R</apll> is not found in <apll>L</apll>, in which case the corresponding item in <apll>Z</apll> is <apll>⎕IO+⍴L</apll>.</td>
</tr>
<tr>
  <td>This feature extends dyadic iota to non-vector left arguments.</td>
</tr>
<tr>
  <td>This function is sensitive to <apll>⎕IO</apll> and <apll>⎕CT</apll>.</td>
</tr>
</table>
<br />
<p>For example, in origin-1</p>


<p>For example, in origin-1</p>
<apll><pre>
      M←2 3⍴'abcdef'
      M⍳'afg'
1 1 2 3  3 4
      M[M⍳'af']
af
      L←2 ⋄ ⎕FMT L⍳⍳3
┌3──────────┐
│┌0┐ ┌0┐ ┌0┐│
││0│ │0│ │0││
│└~┘ └~┘ └~┘2
└∊──────────┘</pre></apll>


<apll>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;M←2 3⍴'abcdef'</apll><br />
<p>Note that this extension preserves the identity <apll>R≡L[L⍳R]</apll> for all <apll>R⊆L</apll>.</p>
<apll>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;M⍳'af'</apll><br />
<apll>&nbsp;1 1&nbsp;&nbsp;2 3</apll><br >
<apll>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;M[M⍳'af']</apll><br />
<apll>af</apll>


<p>This extension is implemented via an internal magic function:</p>
<p>This extension is implemented via an internal magic function:</p>


<apll>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;Z←L #DydIota R;⎕IO;O</apll><br />
<apll><pre>
<apll>[1]&nbsp;&nbsp;&nbsp;O←⎕IO ⋄ ⎕IO←0</apll><br />
    ∇ Z←L #DydIota R;⎕IO;O
<apll>[2]&nbsp;&nbsp;&nbsp;Z←⊂[0] O+(1+⍴L)⊤(¯1↓,(1+⍴L)↑L)⍳R</apll><br />
[1]   O←⎕IO ⋄ ⎕IO←0
<apll>&nbsp;&nbsp;&nbsp;&nbsp;∇</apll>
[2]   Z←⊂[0] O+(1+⍴L)⊤(¯1↓,(1+⍴L)↑L)⍳R
    ∇</pre></apll>

Latest revision as of 17:33, 15 April 2018

Z←L⍳R returns a nested array of indices suitable to indexing L.
L is an array of rank not equal 1.
R is an arbitrary array.
Z is a nested array of shape ⍴R whose items are each integer vectors of length ⍴⍴L, suitable for use as indices to L, except for where the item in R is not found in L, in which case the corresponding item in Z is ⎕IO+⍴L.
This feature extends dyadic iota to non-vector left arguments.
This function is sensitive to ⎕IO and ⎕CT.


For example, in origin-1

      M←2 3⍴'abcdef'
      M⍳'afg'
 1 1  2 3  3 4
      M[M⍳'af']
af
      L←2 ⋄ ⎕FMT L⍳⍳3
┌3──────────┐
│┌0┐ ┌0┐ ┌0┐│
││0│ │0│ │0││
│└~┘ └~┘ └~┘2
└∊──────────┘

Note that this extension preserves the identity R≡L[L⍳R] for all R⊆L.

This extension is implemented via an internal magic function:

    ∇ Z←L #DydIota R;⎕IO;O
[1]   O←⎕IO ⋄ ⎕IO←0
[2]   Z←⊂[0] O+(1+⍴L)⊤(¯1↓,(1+⍴L)↑L)⍳R
    ∇