<h4>2.1 <span class="Heading">Accessing the tables</span></h4>
<p>All Brauer tables in this package are relative to a <em>generic</em> ordinary character table obtained by one of the following constructions</p>
<dl>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">CharacterTable( "2.Sym(n)" )</code>, the character table of <span class="SimpleMath">2.Sym(n)</span> ,</p>
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">CharacterTable( "2.Alt(n)" )</code>, the character table of <span class="SimpleMath">2.Alt(n)</span> ,</p>
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">CharacterTable( "Sym(n)" )</code>, the character table of <span class="SimpleMath">Sym(n)</span>,</p>
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">CharacterTable( "Alt(n)" )</code>, the character table of <span class="SimpleMath">Alt(n)</span>.</p>
</dd>
</dl>
<p>Note that these are synonymous expressions for</p>
<dl>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">CharacterTable( "DoubleCoverSymmetric", n )</code>,</p>
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">CharacterTable( "DoubleCoverAlternating", n )</code>,</p>
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">CharacterTable( "Symmetric", n )</code>,</p>
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">CharacterTable( "Alternating", n )</code>,</p>
</dd>
</dl>
<p>respectively. More detailed information on these tables is to be found in <a href="chapBib.html#biBNoeske2002">[3]</a>. In this manual, we call such a character table an (ordinary) <em>SpinSym table</em>. If <code class="code">ordtbl</code> is an ordinary SpinSym table, the relative Brauer table in characteristic <code class="code">p</code> can be accessed using the <code class="code">mod</code>-operator (i.e. <code class="code">ordtbl mod p;</code>). Such a Brauer table is called a (<span class="SimpleMath">p</span>-modular) <em>SpinSym table</em> in the following.</p>
<p>An ordinary SpinSym table has character parameters, that is, a list of suitable labels corresponding to the rows of <code class="code">ordtbl</code> and therefore the irreducible ordinary characters of the underlying group. See <code class="code">CharacterParameters()</code> in the GAP Reference Manual.</p>
<h5>2.2-1 <span class="Heading">Parameters of ordinary characters</span></h5>
<p>In the following, `ordinary (spin) character' is used synonymously for `irreducible ordinary (spin) character'. It is well known that there is a bijection between the set of ordinary characters of <span class="SimpleMath">Sym(n)</span> and the set <span class="SimpleMath">P(n)</span> of all partitions of <span class="SimpleMath">n</span>. Recall that a partition of a natural number <span class="SimpleMath">n</span> is a list of non-increasing positive integers (its <em>parts</em>) that sum up to <span class="SimpleMath">n</span>. In this way, every ordinary character <span class="SimpleMath">χ</span> of <span class="SimpleMath">Sym(n)</span> has a label of the form <code class="code">[1,c]</code> where <code class="code">c</code> is a partition of <span class="SimpleMath">n</span>. The labels of the ordinary characters of <span class="SimpleMath">Alt(n)</span> are induced by Clifford theory as follows. Either the restriction <span class="SimpleMath">ψ=χ|_Alt(n)</span> of <span class="SimpleMath">χ</span> to <span class="SimpleMath">Alt(n)</span> is an ordinary character of <span class="SimpleMath">Alt(n)</span>, or <span class="SimpleMath">ψ</span> decomposes as the sum of two distinct ordinary characters <span class="SimpleMath">ψ_1</span> and <span class="SimpleMath">ψ_2</span>.</p>
<p>In the first case there is another ordinary character of <span class="SimpleMath">Sym(n)</span>, say <span class="SimpleMath">ξ</span> labelled by <code class="code">[1,d]</code>, such that the restriction of <span class="SimpleMath">ξ</span> to <span class="SimpleMath">Alt(n)</span> is equal to <span class="SimpleMath">ψ</span>. Moreover, the induced character of <span class="SimpleMath">Sym(n)</span> obtained from <span class="SimpleMath">ψ</span> decomposes as the sum of <span class="SimpleMath">χ</span> and <span class="SimpleMath">ξ</span>. Then <span class="SimpleMath">ψ</span> is labelled by <code class="code">[1,c]</code> or <code class="code">[1,d]</code>.</p>
<p>In the second case, both <span class="SimpleMath">ψ_1</span> and <span class="SimpleMath">ψ_2</span> induce irreducibly up to <span class="SimpleMath">χ</span>. Then <span class="SimpleMath">ψ_1</span> and <span class="SimpleMath">ψ_2</span> are labelled by <code class="code">[1,[c,'+']]</code> and <code class="code">[1,[c,'-']]</code>.</p>
<p>If <span class="SimpleMath">χ</span> is an ordinary character of <span class="SimpleMath">2.Sym(n)</span> or <span class="SimpleMath">2.Alt(n)</span> , then <span class="SimpleMath">χ(z)=χ(1)</span> or <span class="SimpleMath">χ(z)=-χ(1)</span>. If <span class="SimpleMath">χ(z)=χ(1)</span>, then <span class="SimpleMath">χ</span> is obtained by inflation (along the central subgroup generated by <span class="SimpleMath">z</span>) from an ordinary character of <span class="SimpleMath">Sym(n)</span> or <span class="SimpleMath">Alt(n)</span>, respectively, whose label is given to <spanclass="SimpleMath">χ</span>. Otherwise, if <span class="SimpleMath">χ</span> is a spin character, that is <span class="SimpleMath">χ(z)=-χ(1)</span>, then its label is described next.</p>
<p>The set of ordinary spin characters of <span class="SimpleMath">2.Sym(n)</span> is parameterized by the subset <span class="SimpleMath">D(n)</span> of <span class="SimpleMath">P(n)</span> of all distinct-parts partitions of <span class="SimpleMath">n</span> (also called bar partitions). If <code class="code">c</code> is an even distinct-parts partition of <span class="SimpleMath">n</span>, then there is a unique ordinary spin character of <span class="SimpleMath">2.Sym(n)</span> that is labelled by <code class="code">[2,c]</code>. In contrast, if <code class="code">c</code> is an odd distinct-parts partition of <span class="SimpleMath">n</span>, then there are two distinct ordinary spin characters of <span class="SimpleMath">2.Sym(n)</span> that are labelled by <codeclass="code">[2,[c,'+']]</code> and <code class="code">[2,[c,'-']]</code>. Now the labels of the ordinary spin characters of <span class="SimpleMath">2.Alt(n)</span> follow from the labels of <span class="SimpleMath">2.Sym(n)</span> in the same way as those of <span class="SimpleMath">Alt(n)</span> follow from the labels of <span class="SimpleMath">Sym(n)</span> (see the beginning of this subsection <a href="chap2.html#X87BE0EFA878CA593"><span class="RefLink">2.2-1</span></a>).</p>
<h5>2.2-2 <span class="Heading">Parameters of modular characters</span></h5>
<p>In the following, `<span class="SimpleMath">p</span>-modular (spin) character' is used synonymously for `irreducible p-modular (spin) character'. The set of <span class="SimpleMath">p</span>-modular characters of <span class="SimpleMath">Sym(n)</span> is parameterized by the set of all <span class="SimpleMath">p</span>-regular partitions of <span class="SimpleMath">n</span>. A partition is <span class="SimpleMath">p</span>-regular if no part is repeated more than <span class="SimpleMath">p-1</span> times. Now every <span class="SimpleMath">p</span>-modular character <span class="SimpleMath">χ</span> of <span class="SimpleMath">Sym(n)</span> has a label of the form <code class="code">[1,c]</code> where <code class="code">c</code> is a <span class="SimpleMath">p</span>-regular partition of <span class="SimpleMath">n</span>.</p>
<p>Again, the labels for the <span class="SimpleMath">p</span>-modular spin characters of <span class="SimpleMath">Alt(n)</span> follow from the labels of <span class="SimpleMath">Sym(n)</span>. However, comparing subsection <a href="chap2.html#X87BE0EFA878CA593"><span class="RefLink">2.2-1</span></a>, their format is slightly different.</p>
<p>If <span class="SimpleMath">χ</span> and <span class="SimpleMath">ξ</span> are distinct <span class="SimpleMath">p</span>-modular characters of <span class="SimpleMath">Sym(n)</span> that restrict to the same <span class="SimpleMath">p</span>-modular character <span class="SimpleMath">ψ</span> of <span class="SimpleMath">Alt(n)</span>, then <span class="SimpleMath">ψ</span> is labelled by <code class="code">[1,[c,'0']]</code> where either <span class="SimpleMath">χ</span> or <span class="SimpleMath">ξ</span> is labelled by <code class="code">[1,c]</code>. If <span class="SimpleMath">χ</span> is a <span class="SimpleMath">p</span>-modular character of <span class="SimpleMath">Sym(n)</span> whose restriction to <span class="SimpleMath">Alt(n)</span> decomposes as the sum of two distinct <span class="SimpleMath">p</span>-modular characters, then these are labelled by <code class="code">[1,[c,'+']]</code> and <code class="code">[1,[c,'-']]</code> where <span class="SimpleMath">χ</span> is labelled by <code class="code">[1,c]</code>.</p>
<p>As in the ordinary case, the set of <span class="SimpleMath">p</span>-modular characters of <span class="SimpleMath">2.Sym(n)</span> is the union of the subset consisting of all inflated <span class="SimpleMath">p</span>-modular characters of <span class="SimpleMath">Sym(n)</span> and the subset of spin characters characterized by negative integer values on the central element <span class="SimpleMath">z</span>. The analogue statement holds for <span class="SimpleMath">2.Alt(n)</span>. The set of <span class="SimpleMath">p</span>-modular spin characters of <span class="SimpleMath">2.Sym(n)</span> is parameterized by the set of all restricted <span class="SimpleMath">p</span>-strict partitions of <span class="SimpleMath">n</span>. A partition is called <span class="SimpleMath">p</span>-strict if every repeated part is divisible by <span class="SimpleMath">p</span>, and a <span class="SimpleMath">p</span>-strict partition <span class="SimpleMath">λ</span> is restricted if <span class="SimpleMath">λ_i-λ_i+1<p</span> whenever <span class="SimpleMath">λ_i</span> is divisible <span class="SimpleMath">p</span>, and <span class="SimpleMath">λ_i-λ_i+1≤ p</span> otherwise for all parts <span class="SimpleMath">λ_i</span> of <span class="SimpleMath">λ</span> (where we set <span class="SimpleMath">λ_i+1=0</span> if <span class="SimpleMath">λ_i</span> is the last part). If <code class="code">c</code> is a restricted <span class="SimpleMath">p</span>-strict partition of <span class="SimpleMath">n</span> such that <span class="SimpleMath">n</span> minus the number of parts not divisible by <span class="SimpleMath">p</span> is even, then there is a unique <span class="SimpleMath">p</span>-modular spin character of <span class="SimpleMath">2.Sym(n)</span> that is labelled by <code class="code">[2,[c,'0']]</code>. Its restriction to <span class="SimpleMath">2.Alt(n)</span> decomposes as the sum of two distinct <span class="SimpleMath">p</span>-modular characters which are labelled by <code class="code">[2,[c,'+']]</code> and <code class="code">[2,[c,'-']]</code>. If <span class="SimpleMath">n</span> minus the number of parts of <code class="code">c</code> that are not divisible by <span class="SimpleMath">p</span> is odd, then there are two distinct <span class="SimpleMath">p</span>-modular spin characters of <span class="SimpleMath">2.Sym(n)</span> that are labelled by <code class="code">[2,[c,'+']]</code> and <code class="code">[2,[c,'-']]</code>. Both of these characters restrict to the same irreducible <spanclass="SimpleMath">p</span>-modular spin character of <span class="SimpleMath">2.Alt(n)</span> which is labelled by <code class="code">[2,[c,'0']]</code>.</p>
<p>Let <code class="code">ct</code> be an ordinary SpinSym table. Then <code class="code">ct</code> has a list of class parameters, that is, a list of suitable labels corresponding to the columns of <code class="code">ct</code> and therefore the conjugacy classes of the underlying group. See <codeclass="code">ClassParameters()</code> in the GAP Reference Manual. If <code class="code">bt</code> is a Brauer table in characteristic <span class="SimpleMath">p</span> relative to <code class="code">ct</code>, its class parameters are inherited from <code class="code">ct</code> in correspondence with the <span class="SimpleMath">p</span>-regular conjugacy classes of the underlying group.</p>
<p>Let <span class="SimpleMath">P(n)</span> denote the set of partitions of <span class="SimpleMath">n</span>.</p>
<p>The conjugacy classes of <span class="SimpleMath">Sym(n)</span> are naturally parameterized by the cycle types of their elements, and each cycle type corresponds to a partition of <span class="SimpleMath">n</span>. Therefore a conjugacy class <span class="SimpleMath">C</span> of <span class="SimpleMath">Sym(n)</span> is characterized by its <em>type</em> <span class="SimpleMath">c</span> in <span class="SimpleMath">P(n)</span>. The corresponding entry in the list of class parameters is <code class="code">[1,c]</code>. Assume that <span class="SimpleMath">C</span> is a subset of <span class="SimpleMath">Alt(n)</span>. Then <span class="SimpleMath">C</span> is also a conjugacy class of <span class="SimpleMath">Alt(n)</span> if and only if not all parts of <span class="SimpleMath">c</span> are odd and pairwise distinct. Otherwise, <span class="SimpleMath">C</span> splits as the union of two distinct <span class="SimpleMath">Alt(n)</span>-classes of the same size, <span class="SimpleMath">C^+</span> of type <span class="SimpleMath">c^+</span> and <span class="SimpleMath">C^-</span> of type <span class="SimpleMath">c^-</span>. The corresponding entries in the list of class parameters are <code class="code">[1,[c,'+']]</code> and <code class="code">[1,[c,'-']]</code>, respectively.</p>
<p>Furthermore, the preimage <span class="SimpleMath">C'=C^{π^-1} is either a conjugacy class of 2.Sym(n) of type c with class parameter [1,c], or C'</span> splits as the union of two distinct <span class="SimpleMath">2.Sym(n)</span> -classes <span class="SimpleMath">C'_1 and C'_2=zC'_1 , both of type c with corresponding class parameters [1,c] and [2,c], respectively. An analogous description applies for the conjugacy classes of 2.Alt(n) .
<p>To each conjugacy class of <span class="SimpleMath">2.Sym(n)</span> or <span class="SimpleMath">2.Alt(n)</span> a certain standard representative is assigned in the following way. Let <span class="SimpleMath">c=[c_1,c_2,...,c_m]</span> be a partition of <span class="SimpleMath">n</span>. We set <span class="SimpleMath">d_1=0</span>, <span class="SimpleMath">d_i=c_1+... +c_i-1</span> for <span class="SimpleMath">i≥ 2</span>, and</p>
<p>for <span class="SimpleMath">1≤ i≤ m-1</span>, where <span class="SimpleMath">t(c_i,d_i)= 1</span> if <span class="SimpleMath">c_i=1</span>. The <em>standard representative of type</em> <span class="SimpleMath">c</span> is defined as</p>
<p>Furthermore, we define the standard representatives of type <span class="SimpleMath">c^+=</span><code class="code">[c,'+']</code> and <span class="SimpleMath">c^-=</span><code class="code">[c,'-']</code> to be <span class="SimpleMath">t_c^+=t_c</span> and <span class="SimpleMath">t_c^-=t_1^-1t_c t_1</span>, respectively.</p>
<p>For example, the standard representative of type <span class="SimpleMath">c=[7,4,3,1]</span> in <span class="SimpleMath">P(15)</span> is</p>
<p>Now <span class="SimpleMath">C' is a conjugacy class of 2.Sym(n) or 2.Alt(n) with parameter
<dl>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">[1,c]</code> if and only if <span class="SimpleMath">t_c</span> is an element of <span class="SimpleMath">C' ,
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">[2,c]</code> if and only if <span class="SimpleMath">zt_c</span> is an element of <span class="SimpleMath">C' ,
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">[1,[c,'+']]</code> if and only if <span class="SimpleMath">t_c^+</span> is an element of <span class="SimpleMath">C' ,
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">[2,[c,'+']]</code> if and only if <span class="SimpleMath">zt_c^+</span> is an element of <span class="SimpleMath">C' ,
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">[1,[c,'-']]</code> if and only if <span class="SimpleMath">t_c^-</span> is an element of <span class="SimpleMath">C' ,
</dd>
<dt><strong class="Mark"></strong></dt>
<dd><p><code class="code">[2,[c,'-']]</code> if and only if <span class="SimpleMath">zt_c^-</span> is an element of <span class="SimpleMath">C' .
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymStandardRepresentative</code>( <var class="Arg">c</var>, <var class="Arg">rep</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: the image of the standard representative of type <var class="Arg">c</var> under a given <span class="SimpleMath">2.Sym(n)</span>-representation.</p>
<p>Expecting the second entry of a class parameter of <span class="SimpleMath">2.Sym(n)</span> or <span class="SimpleMath">2.Alt(n)</span> , say <var class="Arg">c</var>, the standard representative of type <var class="Arg">c</var> under a given representation of <span class="SimpleMath">2.Sym(n)</span> is computed. The argument <var class="Arg">rep</var> is assumed to be a list <span class="SimpleMath">[t_1^R,t_2^R,...,t_n-1^R]</span> given by the images of the generators <span class="SimpleMath">t_1,...,t_n-1</span> of <span class="SimpleMath">2.Sym(n)</span> under a (not necessarily faithful) representation <span class="SimpleMath">R</span> of <span class="SimpleMath">2.Sym(n)</span> .</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymStandardRepresentativeImage</code>( <var class="Arg">c</var>[, <var class="Arg">j</var>] )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: the image of the standard representative of type <var class="Arg">c</var> under the natural epimorphism <span class="SimpleMath">π:2.Sym({j,...,j+n-1}) -> Sym({j,...,j+n-1})</span>.</p>
<p>Given the second entry <var class="Arg">c</var> of a class parameter of <span class="SimpleMath">2.Sym(n)</span> or <span class="SimpleMath">2.Alt(n)</span> , and optionally a positive integer <var class="Arg">j</var>, the image of the standard representative of type <var class="Arg">c</var> under <span class="SimpleMath">π:2.Sym({j,...,j+n-1}) -> Sym({j,...,j+n-1})</span> with <span class="SimpleMath">t_i^π=(i,i+1)</span> for <span class="SimpleMath">j≤ i≤ j+n-2</span> is computed by calling <code class="keyw">SpinSymStandardRepresentative(c,rep)</code> where <code class="code">rep</code> is the list <code class="code">[(j,j+1),(j+1,j+2),...,(j+n-2,j+n-1)]</code>. By default, <code class="code">j=1</code>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymPreimage</code>( <var class="Arg">c</var>, <var class="Arg">rep</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a (standard) lift of the element <var class="Arg">c</var> of <span class="SimpleMath">Sym(n)</span> in <span class="SimpleMath">2.Sym(n)</span> under a given <span class="SimpleMath">2.Sym(n)</span>-representation.</p>
<p>See <a href="chapBib.html#biBMaas2011">[2, (5.1.12)]</a> for the definition of the lift that is returned by this function. The permutation <var class="Arg">c</var> is written as a product of simple transpositions <span class="SimpleMath">(i,i+1)</span>, then these are replaced by the images of their canonical lifts <span class="SimpleMath">t_i</span> under a given representation <span class="SimpleMath">R</span> of <span class="SimpleMath">2.Sym(n)</span> (recall the beginning of Chapter <a href="chap1.html#X7DFB63A97E67C0A1"><span class="RefLink">1</span></a> for the definition of <span class="SimpleMath">t_i</span>). Here <var class="Arg">rep</var> is assumed to be the list <span class="SimpleMath">[t_1^R,t_2^R,...,t_n-1^R]</span>.</p>
<p>Note that a more efficient computation may be achieved by computing and storing a list of all necessary transpositions once and for all, before lifting (many) elements (under a possibly large representation).</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymBrauerCharacter</code>( <var class="Arg">ccl</var>, <var class="Arg">ords</var>, <var class="Arg">rep</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: the Brauer character afforded by a given representation of <span class="SimpleMath">2.Sym(n)</span> .</p>
<p>This function is based on a simplified computation of the <strong class="pkg">GAP</strong> attribute <code class="code">BrauerCharacterValue(mat)</code> for an invertible matrix <code class="code">mat</code> over a finite field whose characteristic is coprime to the order of <code class="code">mat</code>.</p>
<p>The arguments <var class="Arg">ccl</var> and <var class="Arg">ords</var> are expected to be the values of the attributes <code class="code">ClassParameters(modtbl)</code> and <code class="code">OrdersClassRepresentatives(modtbl)</code> of a (possibly incomplete) <span class="SimpleMath">p</span>-modular SpinSym table <code class="code">modtbl</code> of <span class="SimpleMath">2.Sym(n)</span> .</p>
<p>The argument <var class="Arg">rep</var> is assumed to be a list <span class="SimpleMath">[t_1^R,t_2^R,...,t_n-1^R]</span> given by the images of the generators <span class="SimpleMath">t_1,...,t_n-1</span> of <span class="SimpleMath">2.Sym(n)</span> under a (not necessarily faithful) <span class="SimpleMath">2.Sym(n)</span> -representation <span class="SimpleMath">R</span>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymBasicCharacter</code>( <var class="Arg">modtbl</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a <span class="SimpleMath">p</span>-modular basic spin character of the (possibly incomplete) <span class="SimpleMath">p</span>-modular SpinSym table <var class="Arg">modtbl</var> of <span class="SimpleMath">2.Sym(n)</span> .</p>
<p>This is just a shortcut for constructing a basic spin representation of <span class="SimpleMath">2.Sym(n)</span> in characteristic <span class="SimpleMath">p</span> and computing its Brauer character by calling <code class="func">SpinSymBrauerCharacter</code> (<a href="chap2.html#X8243866286DA609C"><span class="RefLink">2.3-4</span></a>) afterwards.</p>
<p>Let <span class="SimpleMath">k</span> and <span class="SimpleMath">l</span> be integers greater than <span class="SimpleMath">1</span> and set <span class="SimpleMath">n=k+l</span>. The following subgroup of <span class="SimpleMath">2.Sym(n)</span> ,</p>
<p>is called a (maximal) <em>Young subgroup</em> of <span class="SimpleMath">2.Sym(n)</span> . Similarly, the intersection <span class="SimpleMath">2.(Alt(k)×Alt(l))</span> of <span class="SimpleMath">2.(Sym(k)×Sym(l))</span> and <span class="SimpleMath">2.Alt(n)</span> is a (maximal) Young subgroup of <span class="SimpleMath">2.Alt(n)</span> . Note that <span class="SimpleMath">(2.(Sym(k)×Sym(l)))^π</span> is isomorphic to <span class="SimpleMath">Sym(k)×Sym(l)</span> and <span class="SimpleMath">(2.(Alt(k)×Alt(l)))^π</span> is isomorphic to <span class="SimpleMath">Alt(k)×Alt(l)</span> but only <span class="SimpleMath">2.(Alt(k)×Alt(l))</span> which is isomorphic to <span class="SimpleMath">(2.Alt(k)×2.Alt(l))/ <(z,z)></span> is a central product. In between <span class="SimpleMath">2.(Alt(k)×Alt(l))</span> and <span class="SimpleMath">2.(Sym(k)×Sym(l))</span> there are further central products <span class="SimpleMath">2.(Sym(k)×Alt(l))</span> which is isomorphic to <span class="SimpleMath">(2.Sym(k)×2.Alt(l))/<(z,z)></span> and <span class="SimpleMath">2.(Alt(k)×Sym(l))</span> which is isomorphic to <span class="SimpleMath">(2.Alt(k)×2.Sym(l))/<(z,z)></span> which are <span class="SimpleMath">π</span>-preimages of <span class="SimpleMath">Sym(k)×Alt(l)</span> and <span class="SimpleMath">Alt(k)×Sym(l)</span>, respectively. See <a href="chapBib.html#biBMaas2011">[2, Section 5.2]</a>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymCharacterTableOfMaximalYoungSubgroup</code>( <var class="Arg">k</var>, <var class="Arg">l</var>, <var class="Arg">type</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: the ordinary character table of a maximal Young subgroup depending on <var class="Arg">type</var>.</p>
<p>For integers <var class="Arg">k</var> and <var class="Arg">l</var> greater than <span class="SimpleMath">1</span> the function returns the ordinary character table of <span class="SimpleMath">2.(Alt(k)×Alt(l))</span>, <span class="SimpleMath">2.(Alt(k)×Sym(l))</span>, <span class="SimpleMath">2.(Sym(k)×Alt(l))</span>, or <span class="SimpleMath">2.(Sym(k)×Sym(l))</span> depending on the string <var class="Arg">type</var> being <code class="code">"Alternating"</code>, <code class="code">"AlternatingSymmetric"</code>, <code class="code">"SymmetricAlternating"</code>, or <code class="code">"Symmetric"</code>, respectively.</p>
<p>If <var class="Arg">type</var> is <code class="code">"Symmetric"</code> then the output is computed by means of Clifford's theory from the character tables of 2.(Sym(k)×Alt(l)), 2.(Alt(k)×Alt(l)), and 2.(Alt(k)×Sym(l)) (see [2, Section 5.2]). These `ingredients' are computed and then stored in the attribute <code class="code">SpinSymIngredients</code> so they can be accessed during the construction (and for the construction of a relative Brauer table too, see <code class="func">SpinSymBrauerTableOfMaximalYoungSubgroup</code> (<a href="chap2.html#X849A37657F53BAE3"><span class="RefLink">2.4-2</span></a>)).</p>
<p>The construction of the character tables of <var class="Arg">type</var> <code class="code">"Alternating"</code>, <code class="code">"AlternatingSymmetric"</code>, or <code class="code">"SymmetricAlternating"</code> is straightforward and may be accomplished by first construcing a direct product, for example, the character table of <span class="SimpleMath">2.Sym(k)×2.Alt(l)</span>, followed by the construction of the character table of the factor group mod <span class="SimpleMath"><(z,z)></span>.</p>
<p>However, we use a faster method that builds up the table from scratch, using the appropriate component tables as ingredients (for example, the generic character tables of <span class="SimpleMath">2.Sym(k)</span> and <span class="SimpleMath">2.Alt(l)</span> ). In this way we can easily build up a suitable list of class parameters that are needed to determine the class fusion in the construction of <var class="Arg">type</var> <code class="code">"Symmetric"</code>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymBrauerTableOfMaximalYoungSubgroup</code>( <var class="Arg">ordtbl</var>, <var class="Arg">p</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: the <var class="Arg">p</var>-modular character table of the ordinary character table <var class="Arg">ordtbl</var> returned by the function <code class="func">SpinSymCharacterTableOfMaximalYoungSubgroup</code> (<a href="chap2.html#X798B9B1482CBDDC0"><span class="RefLink">2.4-1</span></a>).</p>
<p>If the rational prime <var class="Arg">p</var> is odd, then the construction of the irreducible Brauer characters is really the same as in the ordinary case but it depends on the <var class="Arg">p</var>-modular tables of of <var class="Arg">ordtbl</var>'s `ingredients'. If some Brauer table that is necessary for the construction is not available then <code class="code">fail</code> is returned.</p>
<p>Alternatively, the <code class="code">mod</code>-operator may be used.</p>
<p>For <var class="Arg">p</var> <span class="SimpleMath">=2</span> the Brauer table is essentially constructed as a direct product by standard <strong class="pkg">GAP</strong> methods written by Thomas Breuer.</p>
<p>We call a character table returned by <code class="func">SpinSymCharacterTableOfMaximalYoungSubgroup</code> (<a href="chap2.html#X798B9B1482CBDDC0"><span class="RefLink">2.4-1</span></a>) or <code class="func">SpinSymBrauerTableOfMaximalYoungSubgroup</code> a SpinSym table too. It has lists of class and character parameters whose format is explained in <a href="chapBib.html#biBMaas2011">[2, Sections 5.2, 5.3]</a>.</p>
<p>The following functions determine class fusion maps between SpinSym tables by means of their class parameters. Such `default' class fusion maps allow to induce characters from various subgroups of 2.Sym(n) or 2.Alt(n) consistently.
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion</code>( <var class="Arg">ctSource</var>, <var class="Arg">ctDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map from the SpinSym table <var class="Arg">ctSource</var> to the SpinSym table <var class="Arg">ctDest</var>. This map is stored if there is no other fusion map from <var class="Arg">ctSource</var> to <var class="Arg">ctDest</var> stored yet.</p>
<p>The possible input tables are expected to be either ordinary or <span class="SimpleMath">p</span>-modular SpinSym tables of the following pairs of groups</p>
<p>The appropriate function (see the descriptions below) is called to determine the fusion map <code class="code">fus</code>. If <code class="code">GetFusionMap(ctSource, ctDest)</code> fails, then <code class="code">fus</code> is stored by calling <code class="code">StoreFusion(ctSource, fus, ctDest)</code>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion2Ain2S</code>( <var class="Arg">cclSource</var>, <var class="Arg">cclDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map between the SpinSym tables of <span class="SimpleMath">2.Alt(n)</span> and <span class="SimpleMath">2.Sym(n)</span>.</p>
<p>Given lists of class parameters <var class="Arg">cclSource</var> and <var class="Arg">cclDest</var> of (ordinary or <span class="SimpleMath">p</span>-modular) SpinSym tables of <span class="SimpleMath">2.Alt(n)</span> and <span class="SimpleMath">2.Sym(n)</span>, respectively, a corresponding class fusion map is determined. See <a href="chapBib.html#biBMaas2011">[2, (5.4.1)]</a>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion2Sin2S</code>( <var class="Arg">cclSource</var>, <var class="Arg">cclDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map between the SpinSym tables of <span class="SimpleMath">2.Sym(k)</span> and <span class="SimpleMath">2.Sym(n)</span> for <span class="SimpleMath">k≤ n</span>.</p>
<p>Given lists of class parameters <var class="Arg">cclSource</var> and <var class="Arg">cclDest</var> of (ordinary or <span class="SimpleMath">p</span>-modular) SpinSym tables of <span class="SimpleMath">2.Sym(k)</span> and <span class="SimpleMath">2.Sym(n)</span> for <span class="SimpleMath">k≤ n</span>, respectively, a corresponding class fusion map is determined. See <a href="chapBib.html#biBMaas2011">[2, (5.4.2)]</a>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion2Ain2A</code>( <var class="Arg">cclSource</var>, <var class="Arg">cclDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map between the SpinSym tables of <span class="SimpleMath">2.Alt(k)</span> and <span class="SimpleMath">2.Alt(n)</span> for <span class="SimpleMath">k≤ n</span>.</p>
<p>Given lists of class parameters <var class="Arg">cclSource</var> and <var class="Arg">cclDest</var> of (ordinary or <span class="SimpleMath">p</span>-modular) SpinSym tables of <span class="SimpleMath">2.Alt(k)</span> and <span class="SimpleMath">2.Alt(n)</span> for <span class="SimpleMath">k≤ n</span>, respectively, a corresponding class fusion map is determined. See <a href="chapBib.html#biBMaas2011">[2, (5.4.3)]</a>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion2Sin2A</code>( <var class="Arg">cclSource</var>, <var class="Arg">cclDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map between the SpinSym tables of <span class="SimpleMath">2.Sym(n-2)</span> and <span class="SimpleMath">2.Alt(n)</span>.</p>
<p>Given lists of class parameters <var class="Arg">cclSource</var> and <var class="Arg">cclDest</var> of (ordinary or <span class="SimpleMath">p</span>-modular) SpinSym tables of <span class="SimpleMath">2.Sym(n-2)</span> and <span class="SimpleMath">2.Alt(n)</span>, respectively, a corresponding class fusion map with respect to the embedding of <span class="SimpleMath">< t_1t_n-2,...,t_n-3t_n-1 ></span> isomorphic to <span class="SimpleMath">2.Sym(n-2)</span> in <span class="SimpleMath">2.Alt(n)</span> is determined. See <a href="chapBib.html#biBMaas2011">[2, (5.4.4)]</a>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion2SSin2S</code>( <var class="Arg">cclSource</var>, <var class="Arg">cclDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map between the SpinSym tables of <span class="SimpleMath">2.(Sym(k)×Sym(l))</span> and <span class="SimpleMath">2.Sym(k+l)</span>.</p>
<p>Given lists of class parameters <var class="Arg">cclSource</var> and <var class="Arg">cclDest</var> of (ordinary or <span class="SimpleMath">p</span>-modular) SpinSym tables of <span class="SimpleMath">2.(Sym(k)×Sym(l))</span> and <span class="SimpleMath">2.Sym(k+l)</span>, respectively, a corresponding class fusion map is determined by means of <a href="chapBib.html#biBMaas2011">[2, (5.1.6)]</a>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion2SAin2SS</code>( <var class="Arg">cclSource</var>, <var class="Arg">cclDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map between the SpinSym tables of <span class="SimpleMath">2.(Sym(k)×Alt(l))</span> and <span class="SimpleMath">2.(Sym(k)×Sym(l))</span>.</p>
<p>Given lists of class parameters <var class="Arg">cclSource</var> and <var class="Arg">cclDest</var> of (ordinary or <span class="SimpleMath">p</span>-modular) SpinSym tables of <span class="SimpleMath">2.(Sym(k)×Alt(l))</span> and <span class="SimpleMath">2.(Sym(k)×Sym(l))</span>, respectively, a corresponding class fusion map is determined. See <a href="chapBib.html#biBMaas2011">[2, (5.4.6)]</a>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion2ASin2SS</code>( <var class="Arg">cclSource</var>, <var class="Arg">cclDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map between the SpinSym tables of <span class="SimpleMath">2.(Alt(k)×Sym(l))</span> and <span class="SimpleMath">2.(Sym(k)×Sym(l))</span>.</p>
<p>Given lists of class parameters <var class="Arg">cclSource</var> and <var class="Arg">cclDest</var> of (ordinary or <span class="SimpleMath">p</span>-modular) SpinSym tables of <span class="SimpleMath">2.(Alt(k)×Sym(l))</span> and <span class="SimpleMath">2.(Sym(k)×Sym(l))</span>, respectively, a corresponding class fusion map is determined analogously to <a href="chapBib.html#biBMaas2011">[2, (5.4.6)]</a>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion2AAin2SA</code>( <var class="Arg">cclSource</var>, <var class="Arg">cclDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map between the SpinSym tables of <span class="SimpleMath">2.(Alt(k)×Alt(l))</span> and <span class="SimpleMath">2.(Sym(k)×Alt(l))</span>.</p>
<p>Given lists of class parameters <var class="Arg">cclSource</var> and <var class="Arg">cclDest</var> of (ordinary or <span class="SimpleMath">p</span>-modular) SpinSym tables of <span class="SimpleMath">2.(Alt(k)×Alt(l))</span> and <span class="SimpleMath">2.(Sym(k)×Alt(l))</span>, respectively, a corresponding class fusion map is determined. See <a href="chapBib.html#biBMaas2011">[2, (5.4.7)]</a>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion2AAin2AS</code>( <var class="Arg">cclSource</var>, <var class="Arg">cclDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map between the SpinSym tables of <span class="SimpleMath">2.(Alt(k)×Alt(l))</span> and <span class="SimpleMath">2.(Alt(k)×Sym(l))</span>.</p>
<p>Given lists of class parameters <var class="Arg">cclSource</var> and <var class="Arg">cclDest</var> of (ordinary or <span class="SimpleMath">p</span>-modular) SpinSym tables of <span class="SimpleMath">2.(Alt(k)×Alt(l))</span> and <span class="SimpleMath">2.(Alt(k)×Sym(l))</span>, respectively, a corresponding class fusion map is determined analogously to <a href="chapBib.html#biBMaas2011">[2, (5.4.7)]</a>.</p>
<div class="func"><table class="func" width="100%"><tr><td class="tdleft"><code class="func">‣ SpinSymClassFusion2AAin2A</code>( <var class="Arg">cclSource</var>, <var class="Arg">cclDest</var> )</td><td class="tdright">( function )</td></tr></table></div>
<p>Returns: a fusion map between the SpinSym tables of <span class="SimpleMath">2.(Alt(k)×Alt(l))</span> and <span class="SimpleMath">2.Alt(k+l)</span>.</p>
<p>Given lists of class parameters <var class="Arg">cclSource</var> and <var class="Arg">cclDest</var> of (ordinary or <span class="SimpleMath">p</span>-modular) SpinSym tables of <span class="SimpleMath">2.(Alt(k)×Alt(l))</span> and <span class="SimpleMath">2.Alt(k+l)</span>, respectively, a corresponding class fusion map is determined. See <a href="chapBib.html#biBMaas2011">[2, (5.4.8)]</a>.</p>
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