<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2018.61005</article-id><article-id pub-id-type="publisher-id">JAMP-81582</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Deep Transfers of p-Class Tower Groups
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Daniel</surname><given-names>C. Mayer</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Naglergasse 53, Graz, Austria</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>05</day><month>01</month><year>2018</year></pub-date><volume>06</volume><issue>01</issue><fpage>36</fpage><lpage>50</lpage><history><date date-type="received"><day>20,</day>	<month>September</month>	<year>2017</year></date><date date-type="rev-recd"><day>2,</day>	<month>January</month>	<year>2018</year>	</date><date date-type="accepted"><day>5,</day>	<month>January</month>	<year>2018</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  
    Let 
   <em>p</em> be a prime. For any finite 
   <em>p</em>-group G, the deep transfers 
   <em>T </em>
   <sub><em>H,G<sup> '</sup> : H / H </em><sup><em> '</em></sup><em> → G</em><sup><em> '</em></sup><em> / G</em><sup> <em> &quot;</em></sup> from the maximal subgroups <em>H</em> of index <em>(G：H) = p</em> in <em>G</em> to the derived subgroup <em>G</em><sup><em> '</em></sup> are introduced as an innovative tool for identifying <em>G</em> uniquely by means of the family of kernels &#249;<sub><em>d</em></sub><em>(G)</em> =(ker(<em>T </em><sub><em>H,G<sup> '</sup>)) <sub><em>(G： H) = p</em></sub>. </em><sup></sup><sub></sub>For all finite 3-groups <em><em>G</em> </em>of coclass cc(G) = 1, the family &#249;<em><sub><em>d</em></sub>(G) i</em><sub></sub>s determined explicitly. The results are applied to the Galois groups G =Gal(<em><em>F</em><sub><em>3</em></sub><sup> (∞)</sup>/ <em>F</em></em><sub></sub><sup></sup>) of the Hilbert 3-class towers of all real quadratic fields F = Q<em>(√<em>d</em>) </em>with fundamental discriminants<em> <em>d</em> &gt; 1, </em>3-class group Cl<sub>3</sub>(F) □ <em><em>C</em><sub><em>3</em></sub><em> &#215; C</em><sub><em>3</em></sub>, </em><sub></sub><sub></sub>and total 3-principalization in each of their four unramified cyclic cubic extensions E/F. A systematic statistical evaluation is given for the complete range<em> 1 &lt; <em>d</em> &lt; 10<sup>7</sup>, </em><sup></sup>and a few exceptional cases are pointed out for 1 &lt;<em> <em>d</em> &lt; 10<sup>8</sup></em><em>.</em></sub></sub> 
  
 
</p></abstract><kwd-group><kwd>Hilbert p-Class Field Towers</kwd><kwd> p-Class Groups</kwd><kwd> p-Principalization</kwd><kwd> Quadratic Fields</kwd><kwd> Dihedral Fields of Degree 2p; Finite p-Groups</kwd><kwd> Two-Step Centralizers</kwd><kwd> Polarization Principle</kwd><kwd> Descendant Trees</kwd><kwd> p-Group Generation Algorithm</kwd><kwd> p-Multiplicator Rank</kwd><kwd> Relation Rank</kwd><kwd> Generator Rank</kwd><kwd> Deep Transfers</kwd><kwd>  Shallow Transfers</kwd><kwd> Partial Order and Monotony Principle of Artin  Patterns</kwd><kwd> Parametrized Polycyclic pc-Presentations</kwd><kwd> Commutator Calculus</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The layout of this paper is the following. Deep transfers of finite p-groups G, with an assigned prime number p, are introduced as an innovative supplement to the (usual) shallow transfers [[<xref ref-type="bibr" rid="scirp.81582-ref1">1</xref>], p. 50], [[<xref ref-type="bibr" rid="scirp.81582-ref2">2</xref>], Equation (4), p. 470] in &#167;2. The family ϰ d ( G ) = ( k e r ( T H , G ′ ) ) ( G : H ) = p of the kernels of all deep transfers of G is called the deep transfer kernel type of G and will play a crucial role in this paper. For all finite 3-groups G of coclass cc ( G ) = 1 , the deep transfer kernel type ϰ d ( G ) = ( k e r ( T H i , G ′ ) ) 1 ≤ i ≤ 4 is determined explicitly with the aid of commutator calculus in &#167;3 using a parametrized polycyclic power-commutator presentation of G [<xref ref-type="bibr" rid="scirp.81582-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref5">5</xref>]. In the concluding &#167;4, the orders of the deep transfer kernels are sufficient for identifying the Galois group G 3 ∞ F : = Gal ( F 3 ( ∞ ) / F ) of the maximal unramified pro-3 extension of real quadratic fields F = ℚ ( d ) with 3-class group Cl 3 ( F ) ≃ C 3 &#215; C 3 , and total 3-principalization in each of their four unramified cyclic cubic extensions E 1 , … , E 4 .</p></sec><sec id="s2"><title>2. Shallow and Deep Transfer of p-Groups</title><p>With an assigned prime number p ≥ 2 , let G be a finite p-group. Since our focus in this paper will be on the simplest possible non-trivial situation, we assume that the abelianization G / G ′ of G is of elementary type ( p , p ) with rank two. For applications in number theory, concerning p-class towers, the Artin pattern has proved to be a decisive collection of information on G.</p><p>Definition 2.1. The Artin pattern AP ( G ) : = ( τ ( G ) , ϰ ( G ) ) of G consists of two families</p><p>τ ( G ) : = ( H i / H ′ i ) 1 ≤ i ≤ p + 1     and     ϰ ( G ) : = ( k e r ( T G , H i ) ) 1 ≤ i ≤ p + 1 (2.1)</p><p>containing the targets and kernels of the Artin transfer homomorphisms T G , H i :   G / G ′ → H i / H ′ i [[<xref ref-type="bibr" rid="scirp.81582-ref5">5</xref>], Lem. 6.4, p. 198], [[<xref ref-type="bibr" rid="scirp.81582-ref2">2</xref>], Equation (4), p. 470] from G to its p + 1 maximal subgroups H i with i ∈ { 1, … , p + 1 } . Since the maximal subgroups form the shallow layer Lyr 1 ( G ) of subgroups of index ( G : H i ) = p of G, we shall call the T G , H i the shallow transfers of G, and ϰ s ( G ) : = ϰ ( G ) the shallow transfer kernel type (sTKT) of G.</p><p>We recall [[<xref ref-type="bibr" rid="scirp.81582-ref2">2</xref>], &#167;2.2, pp. 475-476] that the sTKT is usually simplified by a family of non-negative integers, in the following way. For 1 ≤ i ≤ p + 1 ,</p><p>ϰ s ( G ) i : = ( j if   k e r ( T G , H i ) = H j / G ′     for   some   j ∈ { 1, … , p + 1 } , 0 if   k e r ( T G , H i ) = G / G ′ . (2.2)</p><p>The progressive innovation in this paper, however, is the introduction of the deep Artin transfer.</p><p>Definition 2.2. By the deep transfers we understand the Artin transfer homomorphisms T H i , G ′ : H i / H ′ i → G ′ / G ″ [[<xref ref-type="bibr" rid="scirp.81582-ref5">5</xref>], Lem. 6.1, p. 196], [[<xref ref-type="bibr" rid="scirp.81582-ref6">6</xref>], Dfn. 3.3, p. 69] from the maximal subgroups H 1 , … , H p + 1 to the commutator subgroup G ′ of G, which forms the deep layer Lyr 2 ( G ) of the (unique) subgroup of index ( G : G ′ ) = p 2 of G with abelian quotient G / G ′ . Accordingly, we call the family</p><p>ϰ d ( G ) = ( # k e r ( T H i , G ′ ) ) 1 ≤ i ≤ p + 1 (2.3)</p><p>the deep transfer kernel type (dTKT) of G.</p><p>We point out that, as opposed to the sTKT, the members of the dTKT are only cardinalities, since this will suffice for reaching our intended goals in this paper. This preliminary coarse definition is open to further refinement in subsequent publications (See the proof of Theorem 3.1.).</p></sec><sec id="s3"><title>3. Identification of 3-Groups by Deep Transfers</title><p>The drawback of the sTKT is the fact that occasionally several non-isomorphic p-groups G share a common Artin pattern AP ( G ) : = ( τ ( G ) , ϰ s ( G ) ) [[<xref ref-type="bibr" rid="scirp.81582-ref7">7</xref>], Thm. 7.2, p. 158]. The benefit of the dTKT is its ability to distinguish the members of such batches of p-groups which have been inseparable up to now. After the general introduction of the dTKT for arbitrary p-groups in &#167;2, we are now going to demonstrate its advantages in the particular situation of the prime p = 3 and finite 3-groups G of coclass c c ( G ) = 1 , which are necessarily metabelian with second derived subgroup G ″ = 1 and abelianization G / G ′ ≃ C 3 &#215; C 3 , according to Blackburn [<xref ref-type="bibr" rid="scirp.81582-ref8">8</xref>].</p><p>For the statement of our main theorem, we need a precise ordering of the four maximal subgroups H 1 , … , H 4 of the group G = 〈 x , y 〉 , which can be generated by two elements x , y , according to the Burnside basis theorem. For this purpose, we select the generators x , y such that</p><p>H 1 = 〈 y , G ′ 〉 ,   H 2 = 〈 x , G ′ 〉 ,   H 3 = 〈 x y , G ′ 〉 ,   H 4 = 〈 x y 2 , G ′ 〉 , (3.1)</p><p>and H 1 = χ 2 ( G ) , provided that G is of nilpotency class cl ( G ) ≥ 3 . Here we denote by</p><p>χ 2 ( G ) : = { g ∈ G | ( ∀   h ∈ G ′ )   [ g , h ] ∈ γ 4 ( G ) } (3.2)</p><p>the two-step centralizer of G ′ in G, where we let ( γ i ( G ) ) i ≥ 1 be the lower central series of G = : γ 1 ( G ) with γ i ( G ) = [ γ i − 1 ( G ) , G ] for i ≥ 2 , in particular, γ 2 ( G ) = G ′ .</p><p>The identification of the groups will be achieved with the aid of parametrized polycyclic power-commutator presentations, as given by Blackburn [<xref ref-type="bibr" rid="scirp.81582-ref3">3</xref>], Miech [<xref ref-type="bibr" rid="scirp.81582-ref4">4</xref>], and Nebelung [<xref ref-type="bibr" rid="scirp.81582-ref5">5</xref>]:</p><p>G a n ( z , w ) : = 〈 x , y , s 2 , … , s n − 1 | s 2 = y , x ,   ( ∀ i = 3 n )   s i = [ s i − 1 , x ] ,   s n = 1 ,   [ y , s 2 ] = s n − 1 a , ( ∀ i = 3 n − 1 )   [ y , s i ] = 1 ,   x 3 = s n − 1 w ,   y 3 s 2 3 s 3 = s n − 1 z ,   ( ∀ i = 2 n − 3 )   s i 3 s i + 1 3 s i + 2 = 1 ,   s n − 2 3 = s n − 1 3 = 1   〉 , (3.3)</p><p>where a ∈ { 0,1 } and w , z ∈ { − 1,0,1 } are bounded parameters, and the index of nilpotency n = cl ( G ) + 1 = cl ( G ) + cc ( G ) = l o g 3 ( ord ( G ) ) = : lo ( G ) is an unbounded parameter.</p><p>Lemma 3.1. Let G be an arbitrary group with elements x , y ∈ G . Then the second and third power of the product x y are given by</p><p>1) ( x y ) 2 = x 2 y 2 s 2 t 3 , where s 2 : = [ y , x ] , t 3 : = [ s 2 , y ] ,</p><p>2) ( x y ) 3 = x 3 y 3 ( s 2 t 3 2 t 4 ) 2 s 3 u 4 2 u 5 s 2 t 3 , where s 3 = [ s 2 , x ] , t 4 = [ t 3 , y ] , u 4 = [ s 3 , y ] , u 5 = [ u 4 , y ] .</p><p>If G ≃ G a n ( z , w ) , then ( x y ) 2 = x 2 y 2 s 2 s n − 1 − a and ( x y ) 3 = x 3 y 3 s 2 3 s 3 s n − 1 − 2 a , and the second and third power of x y 2 are given by ( x y 2 ) 2 = x 2 y 4 s 2 2 s n − 1 − 2 a and ( x y 2 ) 3 = x 3 y 6 s 2 6 s 3 2 s n − 1 − 2 a .</p><p>Proof. We prepare the calculation of the powers by proving a few preliminary identities:</p><p>y x = 1 ⋅ y x = x y y − 1 x − 1 ⋅ y x = x y ⋅ y − 1 x − 1 y x = x y ⋅ [ y , x ] = x y s 2 , and similarly s 2 y = y s 2 ⋅ [ s 2 , y ] = y s 2 t 3 and s 2 x = x s 2 ⋅ [ s 2 , x ] = x s 2 s 3 and t 3 y = y t 3 ⋅ [ t 3 , y ] = y t 3 t 4 and s 3 y = y s 3 ⋅ [ s 3 , y ] = y s 3 u 4 and u 4 y = y u 4 ⋅ [ u 4 , y ] = y u 4 u 5 . Furthermore, y x 2 = y x ⋅ x = x y s 2 ⋅ x = x y ⋅ s 2 x = x y ⋅ x s 2 s 3 = x ⋅ y x ⋅ s 2 s 3 = x ⋅ x y s 2 ⋅ s 2 s 3 = x 2 y s 2 2 s 3 , s 2 y 2 = s 2 y ⋅ y = y s 2 t 3 ⋅ y = y s 2 ⋅ t 3 y = y s 2 ⋅ y t 3 t 4 = y ⋅ s 2 y ⋅ t 3 t 4 = y ⋅ y s 2 t 3 ⋅ t 3 t 4 = y 2 s 2 t 3 2 t 4 , s 3 y 2 = s 3 y ⋅ y = y s 3 u 4 ⋅ y = y s 3 ⋅ u 4 y = y s 3 ⋅ y u 4 u 5 = y ⋅ s 3 y ⋅ u 4 u 5 = y ⋅ y s 3 u 4 ⋅ u 4 u 5 = y 2 s 3 u 4 2 u 5 .</p><p>Now the second power of x y is</p><p>( x y ) 2 = x y x y = x ⋅ y x ⋅ y = x ⋅ x y s 2 ⋅ y = x 2 y ⋅ s 2 y = x 2 y ⋅ y s 2 t 3 = x 2 y 2 s 2 t 3</p><p>and the third power of x y is</p><p>( x y ) 3 = x y ⋅ ( x y ) 2 = x y ⋅ x 2 y 2 s 2 t 3 = x ⋅ y x 2 ⋅ y 2 s 2 t 3 = x ⋅ x 2 y s 2 2 s 3 ⋅ y 2 s 2 t 3 = x 3 y s 2 2 ⋅ s 3 y 2 ⋅ s 2 t 3 = x 3 y s 2 2 ⋅ y 2 s 3 u 4 2 u 5 ⋅ s 2 t 3 = x 3 y s 2 ⋅ s 2 y 2 ⋅ s 3 u 4 2 u 5 s 2 t 3 = x 3 y s 2 ⋅ y 2 s 2 t 3 2 t 4 ⋅ s 3 u 4 2 u 5 s 2 t 3 = x 3 y ⋅ s 2 y 2 ⋅ s 2 t 3 2 t 4 s 3 u 4 2 u 5 s 2 t 3 = x 3 y ⋅ y 2 s 2 t 3 2 t 4 ⋅ s 2 t 3 2 t 4 s 3 u 4 2 u 5 s 2 t 3 = x 3 y 3 ( s 2 t 3 2 t 4 ) 2 s 3 u 4 2 u 5 s 2 t 3 .</p><p>If G ≃ G a n ( z , w ) , then t 4 = u 4 = u 5 = 1 , t 3 = s n − 1 − a , t 3 3 = s n − 1 − 3 a = 1 , and G ′ is abelian. □</p><p>Theorem 3.1. (3-groups G of coclass cc(G) = 1.) Let G be a finite 3-group of coclass cc ( G ) = 1 and order ord ( G ) = 3 n with an integer exponent n ≥ 2 . Then the shallow and deep transfer kernel type of G are given in dependence on the relational parameters a , n , w , z of G ≃ G a n ( z , w ) by <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>Proof. The shallow TKT ϰ s ( G ) of all 3-groups G of coclass cc ( G ) = 1 has been determined in [<xref ref-type="bibr" rid="scirp.81582-ref2">2</xref>], where the designations a.n of the types were introduced with n ∈ { 1,2,3 } . Here, we indicate a capable mainline vertex of the tree T 1 ( R ) with root R = C 3 &#215; C 3 [<xref ref-type="bibr" rid="scirp.81582-ref7">7</xref>] by the type a.1* with a trailing asterisk. As usual, type a.3* indicates the unique 3-group G ≃ Syl 3 A 9 with τ ( G ) = ( 3,3,3 ) , ( 3,3 ) 3 . Now we want to determine the deep TKT ϰ d ( G ) , using the presentation of G ≃ G a n ( z , w ) in Formula (3.3). For this purpose, we need expressions for the images of the deep Artin transfers T i : = T H i , G ′ :   H i / H ′ i → G ′ , for each 1 ≤ i ≤ 4 . (Observe that p = 3 implies G ″ = 1 by [<xref ref-type="bibr" rid="scirp.81582-ref8">8</xref>].) Generally, we have to distinguish outer transfers, T i ( g ⋅ H ′ i ) = g 3 if g ∈ H i \ G ′ [[<xref ref-type="bibr" rid="scirp.81582-ref2">2</xref>], Equation (4), p. 470], and inner transfers, T i ( g ⋅ H ′ i ) = g 1 + h + h 2 = g 3 ⋅ [ g , h 3 ] ⋅ [ [ g , h ] , h ] if g ∈ G ′ and h is selected in H i \ G ′ [[<xref ref-type="bibr" rid="scirp.81582-ref2">2</xref>], Equation (6), p. 486].</p><p>First, we consider the distinguished two-step centralizer H 1 = χ 2 ( G ) with i = 1 . Then H 1 = 〈 y , G ′ 〉 and H ′ 1 = 1 if a = 0 ( H 1 abelian), but H ′ 1 = γ n − 1 ( G ) = 〈 s n − 1 〉 if a = 1 ( H 1 non-abelian) [[<xref ref-type="bibr" rid="scirp.81582-ref2">2</xref>], Equation (3), p. 470]. The outer transfer is determined by T 1 ( y ⋅ H ′ 1 ) = y 3 = s 2 − 3 s 3 − 1 s n − 1 z . For the inner transfer, we have T 1 ( s j ⋅ H ′ 1 ) = s j 1 + y + y 2 = s j 3 ⋅ [ s j , y 3 ] ⋅ [ [ s j , y ] , y ] = s j 3 ⋅ 1 3 ⋅ [ 1 , y ] = s j 3 for all j ≥ 3 , but T 1 ( s 2 ⋅ H ′ 1 ) = s 2 3 ⋅ s n − 1 − 3 a ⋅ [ s n − 1 − a , y ] = s 2 3 for j = 2 , since</p><p>s n − 1 − a ∈ 〈 s n − 1 〉 = γ n − 1 ( G ) = ζ 1 ( G ) lies in the centre of G. The first kernel equation s 2 − 3 s 3 − 1 s n − 1 z = 1 is solvable by either n = 3 , where z = 0 , s 3 = 1 , s 2 3 = 1 , or n = 4 , z = 1 , where s 2 3 = 1 , s n − 1 z = s 3 . The second kernel equation s i 3 = 1 is solvable by</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Shallow and deep TKT of 3-groups G with cc ( G ) = 1 </title></caption><table><tbody><thead><tr><th align="center" valign="middle" >G ≃</th><th align="center" valign="middle" >n</th><th align="center" valign="middle" >Type</th><th align="center" valign="middle" >ϰ s ( G )</th><th align="center" valign="middle" >ϰ d ( G )</th></tr></thead><tr><td align="center" valign="middle" >G 0 n ( 0,0 )</td><td align="center" valign="middle" >=2</td><td align="center" valign="middle" >a.1*</td><td align="center" valign="middle" >( 0,0,0,0 )</td><td align="center" valign="middle" >( 3,3,3,3 )</td></tr><tr><td align="center" valign="middle" >G 0 n ( 0,0 )</td><td align="center" valign="middle" >&#179;3</td><td align="center" valign="middle" >a.1*</td><td align="center" valign="middle" >( 0,0,0,0 )</td><td align="center" valign="middle" >( 9,9,9,9 )</td></tr><tr><td align="center" valign="middle" >G 1 n ( 0,0 )</td><td align="center" valign="middle" >&#179;5</td><td align="center" valign="middle" >a.1</td><td align="center" valign="middle" >( 0,0,0,0 )</td><td align="center" valign="middle" >( 3,9,3,3 )</td></tr><tr><td align="center" valign="middle" >G 1 n ( 0, − 1 )</td><td align="center" valign="middle" >&#179;5</td><td align="center" valign="middle" >a.1</td><td align="center" valign="middle" >( 0,0,0,0 )</td><td align="center" valign="middle" >( 3,3,9,9 )</td></tr><tr><td align="center" valign="middle" >G 1 n ( 0,1 )</td><td align="center" valign="middle" >&#179;5</td><td align="center" valign="middle" >a.1</td><td align="center" valign="middle" >( 0,0,0,0 )</td><td align="center" valign="middle" >( 3,3,3,3 )</td></tr><tr><td align="center" valign="middle" >G 0 n ( 0,1 )</td><td align="center" valign="middle" >&#179;4</td><td align="center" valign="middle" >a.2</td><td align="center" valign="middle" >( 1,0,0,0 )</td><td align="center" valign="middle" >( 9,3,3,3 )</td></tr><tr><td align="center" valign="middle" >G 0 n ( − 1,0 )</td><td align="center" valign="middle" >&#179;4 even</td><td align="center" valign="middle" >a.3</td><td align="center" valign="middle" >( 2,0,0,0 )</td><td align="center" valign="middle" >( 9,9,3,3 )</td></tr><tr><td align="center" valign="middle" >G 0 n ( 1,0 )</td><td align="center" valign="middle" >&#179;5</td><td align="center" valign="middle" >a.3</td><td align="center" valign="middle" >( 2,0,0,0 )</td><td align="center" valign="middle" >( 9,9,3,3 )</td></tr><tr><td align="center" valign="middle" >G 0 n ( 1,0 )</td><td align="center" valign="middle" >=4</td><td align="center" valign="middle" >a.3*</td><td align="center" valign="middle" >( 2,0,0,0 )</td><td align="center" valign="middle" >( 27,9,3,3 )</td></tr><tr><td align="center" valign="middle" >G 0 n ( 0,1 )</td><td align="center" valign="middle" >=3</td><td align="center" valign="middle" >A.1</td><td align="center" valign="middle" >( 1,1,1,1 )</td><td align="center" valign="middle" >( 9,3,3,3 )</td></tr></tbody></table></table-wrap><p>either i = n − 1 or i = n − 2 . Thus, the deep transfer kernel is given by</p><p>k e r ( T 1 ) = ( H 1 = 〈 y , s 2 〉 ≃ C 3 &#215; C 3   if   n = 3   ( G   extra   special ) , H 1 = 〈 y , s 2 , s 3 〉 ≃ C 3 &#215; C 3 &#215; C 3   if   n = 4,   z = 1   ( G ≃ Syl 3 A 9 ) , γ n − 2 ( G ) = 〈 s n − 2 , s n − 1 〉 ≃ C 3 &#215; C 3   if   n = 4,   z ≠ 1   or   n ≥ 5,   a = 0, γ n − 2 ( G ) / γ n − 1 ( G ) ≃ 〈 s n − 2 〉 ≃ C 3   if   n ≥ 5,   a = 1   ( H 1   non-abelian ) . (3.4)</p><p>Second, we put i = 2 . Then H 2 = 〈 x , G ′ 〉 and H ′ 2 = γ 3 ( G ) = 〈 s 3 , … , s n − 1 〉 . The outer transfer is determined by T 2 ( x ⋅ H ′ 2 ) = x 3 = s n − 1 w . The inner transfer is given by T 2 ( s j ⋅ H ′ 2 ) = s j 1 + x + x 2 = s j 3 ⋅ [ s j , x 3 ] ⋅ [ [ s j , x ] , x ] = s j 3 s j + 1 3 s j + 2 = 1 , for all j ≥ 2 , independently of a , n , w , z . Consequently, the deep transfer kernel is given by</p><p>k e r ( T 2 ) = ( H 2 / H ′ 2 = 〈 x , s 2 , … , s n − 1 〉 / 〈 s 3 , … , s n − 1 〉 ≃ 〈 x , s 2 〉 ≃ C 3 &#215; C 3   if   w = 0, G ′ / H ′ 2 = 〈 s 2 , … , s n − 1 〉 / 〈 s 3 , … , s n − 1 〉 ≃ 〈 s 2 〉 ≃ C 3   if   w = &#177; 1. (3.5)</p><p>Next, we put i = 3 . Then H 3 = 〈 x y , G ′ 〉 and H ′ 3 = γ 3 ( G ) = 〈 s 3 , … , s n − 1 〉 . The outer transfer is determined by T 3 ( x y ⋅ H ′ 3 ) = ( x y ) 3 = x 3 y 3 s 2 3 s 3 s n − 1 − 2 a = s n − 1 w + z − 2 a . For the inner transfer, we have T 3 ( s j ⋅ H ′ 3 ) = s j 1 + x y + ( x y ) 2 = s j 3 ⋅ [ s j , x y 3 ] ⋅ [ [ s j , x y ] , x y ] = s j 3 s j + 1 3 s j + 2 = 1 , for all j ≥ 3 , independently of a , n , w , z . The first kernel equation s n − 1 w + z − 2 a = 1 ⇔ w + z − 2 a ≡ 0 ( mod 3 ) is solvable by either a = w = z = 0 or a = 1 , w = − 1 .</p><p>Therefore, the deep transfer kernel is given by</p><p>k e r ( T 3 ) = ( H 3 / H ′ 3 ≃ 〈 x y , s 2 〉 ≃ C 3 &#215; C 3   if   either   a = w = z = 0   or   a = 1,   w = − 1, G ′ / H ′ 3 ≃ 〈 s 2 〉 ≃ C 3   otherwise . (3.6)</p><p>Finally, we put i = 4. Then H 4 = 〈 x y 2 , G ′ 〉 and H ′ 4 = γ 3 ( G ) = 〈 s 3 , … , s n − 1 〉 . The outer transfer is determined by T 4 ( x y 2 ⋅ H ′ 4 ) = ( x y 2 ) 3 = x 3 y 6 s 2 6 s 3 2 s n − 1 − 2 a = s n − 1 w + 2 z − 2 a . The inner transfer is given by T 4 ( s j ⋅ H ′ 4 ) = s j 1 + x y 2 + ( x y 2 ) 2 = s j 3 ⋅ [ s j , x y 2 3 ] ⋅ [ [ s j , x y 2 ] , x y 2 ] = s j 3 s j + 1 3 s j + 2 = 1 , for all j ≥ 3 , independently of a , n , w , z . The first kernel equation s n − 1 w + 2 z − 2 a = 1 ⇔ w + 2 z − 2 a ≡ 0 ( m o d 3 ) is solvable by either a = w = z = 0 or a = 1 , w = − 1 .</p><p>Thus, the deep transfer kernel is given by</p><p>k e r ( T 4 ) = ( H 4 / H ′ 4 ≃ 〈 x y 2 , s 2 〉 ≃ C 3 &#215; C 3   if   either   a = w = z = 0   or   a = 1,   w = − 1, G ′ / H ′ 4 ≃ 〈 s 2 〉 ≃ C 3   otherwise .</p><p>(3.7)</p><p>These finer results are summarized in terms of coarser cardinalities in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>□</p></sec><sec id="s4"><title>4. Arithmetical Application to 3-Class Tower Groups</title><sec id="s4_1"><title>4.1. Real Quadratic Fields</title><p>As a final highlight of our progressive innovations, we come to a number theoretic application of Theorem 3.1, more precisely, the unambiguous identification of the pro-3 Galois group G 3 ∞ F = Gal ( F 3 ( ∞ ) / F ) of the maximal unramified pro-3 extension F 3 ( ∞ ) , that is the Hilbert 3-class field tower, of certain real quadratic fields F = ℚ ( d ) with fundamental discriminant d &gt; 1 , 3-class group Cl 3 ( F ) of elementary type ( 3,3 ) , and shallow transfer kernel type a.1, ϰ s ( F ) = ( 0,0,0,0 ) , in its ground state with τ ( F ) ~ ( 9,9 ) , ( 3,3 ) 3 or in a higher excited state with τ ( F ) ~ ( 3 e ,3 e ) , ( 3,3 ) 3 , e ≥ 3 .</p><p>The first field of this kind with d = 62501 was discovered by Heider and Schmithals in 1982 [<xref ref-type="bibr" rid="scirp.81582-ref9">9</xref>]. They computed the sTKT ϰ s ( F ) = ( 0,0,0,0 ) with four total 3-principalizations in the unramified cyclic cubic extensions E i / F , 1 ≤ i ≤ 4 , on a CDC Cyber mainframe. The fact that d = 62501 is a triadic irregular discriminant (in the sense of Gauss) with non-cyclic 3-class group Cl 3 ( F ) ≃ C 3 &#215; C 3 has been pointed out earlier in 1936 by Pall [<xref ref-type="bibr" rid="scirp.81582-ref10">10</xref>] already. The second field of this kind with d = 152949 was discovered by ourselves in 1991 by computing ϰ s ( F ) on an AMDAHL mainframe [<xref ref-type="bibr" rid="scirp.81582-ref11">11</xref>]. In 2006, there followed d = 252977 and d = 358285 , and many other cases in 2009 [<xref ref-type="bibr" rid="scirp.81582-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref13">13</xref>].</p><p>Generally, there are three contestants for the group G = G 3 ∞ F , for any assigned state τ ( F ) ~ ( 3 e ,3 e ) , ( 3,3 ) 3 , e ≥ 2 , and the following Main Theorem admits their identification by means of the deep transfer kernel type (See their statistical distribution at the end of Section 4.1.).</p><p>Theorem 4.1. (3-class tower groups G of coclass cc(G) = 1 and type a.1.) Let F = ℚ ( d ) be a quadratic field with fundamental discriminant d, 3-class group Cl 3 ( F ) ≃ C 3 &#215; C 3 , and shallow transfer kernel type a.1, ϰ s ( F ) = ( 0,0,0,0 ) .</p><p>Then F is real with d &gt; 1 , the 3-class tower group G = G 3 ∞ F of F has coclass cc ( G ) = 1 , and the relational parameters n ≥ 5 and w ∈ { − 1,0,1 } of G ≃ G 1 n ( 0, w ) are given in dependence on the deep transfer kernel type ϰ d ( F ) as follows:</p><p>G ≃ G 1 2 ( e + 1 ) ( 0,0 ) with n = 2 ( e + 1 ) ,   w = 0 ⇔ ϰ d ( F ) ~ ( 3,9,3,3 ) , G ≃ G 1 2 ( e + 1 ) ( 0, − 1 ) with n = 2 ( e + 1 ) ,   w = − 1 ⇔ ϰ d ( F ) ~ ( 3,3,9,9 ) , G ≃ G 1 2 ( e + 1 ) ( 0,1 ) with n = 2 ( e + 1 ) ,   w = 1 ⇔ ϰ d ( F ) ~ ( 3,3,3,3 ) , (4.1)</p><p>where we suppose that the state of type a.1 is determined by the transfer target type τ ( F ) ~ ( 3 e ,3 e ) , ( 3,3 ) 3 with e ≥ 2 .</p><p>Proof. Let F = ℚ ( d ) be a quadratic field with 3-class group Cl 3 ( F ) ≃ C 3 &#215; C 3 , denote by E 1 , … , E 4 its four unramified cyclic cubic extensions and by T E i / F : Cl 3 ( F ) → Cl 3 ( E i ) ( 1 ≤ i ≤ 4 ) the transfer homomorphisms of 3-classes.</p><p>If the 3-principalization is total, that is k e r ( T E i / F ) = Cl 3 ( F ) , for each 1 ≤ i ≤ 4 , then F must be a real quadratic field with positive fundamental discriminant d &gt; 1 , since the order of the principalization kernels k e r ( T E i / F ) of an imaginary quadratic field F is bounded from above by ( U F : N E i / F U E i ) ⋅ E i : F = 1 ⋅ 3 = 3 , according to the Theorem on the Herbrand quotient of the unit groups U E i .</p><p>By the Artin reciprocity law of class field theory [<xref ref-type="bibr" rid="scirp.81582-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref14">14</xref>], the principalization type ϰ ( F ) = ( 0000 ) of the field F corresponds to the shallow transfer kernel type ϰ s ( G ) = ( 0000 ) of the 3-class tower group G = Gal ( F 3 ( ∞ ) / F ) of F, and the abelian type invariants Cl 3 ( F ) ≃ 1 2 of the 3-class group of F correspond to the abelian quotient invariants G / G ′ ≃ 1 2 of G.</p><p>According to [<xref ref-type="bibr" rid="scirp.81582-ref2">2</xref>], a finite 3-group G with G / G ′ ≃ 1 2 and ϰ s ( G ) = ( 0000 ) must be of coclass cc ( G ) = 1 . <xref ref-type="table" rid="table1">Table 1</xref> shows that either G ≃ G 0 n ( 0,0 ) of type a.1<sup>*</sup> with n ≥ 2 or G ≃ G 1 n ( 0, w ) of type a.1 with n ≥ 5 and − 1 ≤ w ≤ 1 .</p><p>For a real quadratic field F, the relation rank d 2 ( G ) = d i m F 3 H 2 ( G , F 3 ) of the 3-class tower group G = G 3 ( ∞ ) F is bounded by d 2 ( G ) ≤ 3 [[<xref ref-type="bibr" rid="scirp.81582-ref15">15</xref>], Thm. 1.3, pp. 75-76]. Consequently, G cannot be a non-abelian mainline vertex G 0 n ( 0,0 ) with n ≥ 3 of the coclass-1 tree T 1 ( R ) with root R = C 3 &#215; C 3 , since all these vertices have the relation rank 4. According to [[<xref ref-type="bibr" rid="scirp.81582-ref12">12</xref>], Thm. 4.1 (1), p. 486], G cannot be the abelian root R = G 0 2 ( 0 , 0 ) either, and we must have G ≃ G 1 n ( 0, w ) with n ≥ 5 and w ∈ { − 1,0,1 } .</p><p>Now the claim is a consequence of Theorem 3.1 and <xref ref-type="table" rid="table1">Table 1</xref>. □</p><p><xref ref-type="table" rid="table2">Table 2</xref> shows that the ground state τ ( F ) = ( 9 , 9 ) , ( 3 , 3 ) 3 of the sTKT ϰ s ( F ) = ( 0,0,0,0 ) has the nice property that the smallest three discriminants already realize three different 3-class tower groups G = G 3 ∞ F ≃ 〈 729 , i 〉 with i ∈ { 99,100,101 } , identified by their dTKT ϰ d ( F ) = ϰ d ( G ) .</p><p>In <xref ref-type="table" rid="table3">Table 3</xref>, we see that the first excited state τ ( F ) = ( 27 , 27 ) , ( 3 , 3 ) 3 of the sTKT ϰ s ( F ) = ( 0,0,0,0 ) does not behave so well: although the smallest two discriminants [<xref ref-type="bibr" rid="scirp.81582-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref17">17</xref>] already realize two different 3-class tower groups G = G 3 ∞ F ≃ 〈 6561 , i 〉 with i ∈ { 2225,2227 } , we have to wait for the seventh occurrence until 〈 6561,2226 〉 is realized, as the dTKT ϰ d ( F ) = ϰ d ( G ) shows. The counter 7 is a typical example of a statistic delay.</p><p>The second excited state τ ( F ) = ( 81 , 81 ) , ( 3 , 3 ) 3 of the sTKT</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Deep TKT of 3-class tower groups G with τ ( G ) = ( 9 , 9 ) , ( 3 , 3 ) 3 </title></caption><table><tbody><thead><tr><th align="center" valign="middle" >G</th><th align="center" valign="middle" >ϰ d ( G )</th><th align="center" valign="middle" >MD</th></tr></thead><tr><td align="center" valign="middle" >〈 729,99 〉 ≃ G 1 6 ( 0,0 )</td><td align="center" valign="middle" >( 3,9,3,3 )</td><td align="center" valign="middle" >62,501</td></tr><tr><td align="center" valign="middle" >〈 729,100 〉 ≃ G 1 6 ( 0, − 1 )</td><td align="center" valign="middle" >( 3,3,9,9 )</td><td align="center" valign="middle" >152,949</td></tr><tr><td align="center" valign="middle" >〈 729,101 〉 ≃ G 1 6 ( 0,1 )</td><td align="center" valign="middle" >( 3,3,3,3 )</td><td align="center" valign="middle" >252,977</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Deep TKT of 3-class tower groups G with τ ( G ) = ( 27 , 27 ) , ( 3 , 3 ) 3 </title></caption><table><tbody><thead><tr><th align="center" valign="middle" >G</th><th align="center" valign="middle" >ϰ d ( G )</th><th align="center" valign="middle" >MD</th><th align="center" valign="middle" >further discriminants</th></tr></thead><tr><td align="center" valign="middle" >〈 6561,2225 〉 ≃ G 1 8 ( 0,0 )</td><td align="center" valign="middle" >( 3,9,3,3 )</td><td align="center" valign="middle" >10,399,596</td><td align="center" valign="middle" >16,613,448</td></tr><tr><td align="center" valign="middle" >〈 6561,2226 〉 ≃ G 1 8 ( 0, − 1 )</td><td align="center" valign="middle" >( 3,3,9,9 )</td><td align="center" valign="middle" >27,780,297</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >〈 6561,2227 〉 ≃ G 1 8 ( 0,1 )</td><td align="center" valign="middle" >( 3,3,3,3 )</td><td align="center" valign="middle" >2,905,160</td><td align="center" valign="middle" >14,369,932, 15,019,617, 21,050,241</td></tr></tbody></table></table-wrap><p>ϰ s ( F ) = ( 0,0,0,0 ) , however, is well-behaved again: the smallest three discriminants already realize three different 3-class tower groups G = G 3 ∞ F ≃ G 1 10 ( 0 , w ) with w ∈ { 0, − 1,1 } , identified by their dTKT ϰ d ( F ) = ϰ d ( G ) . (For logarithmic orders ≥ 9 , no SmallGroup identifiers exist.) See <xref ref-type="table" rid="table4">Table 4</xref>.</p><p>In all tables, the shortcut MD means the minimal discriminant [[<xref ref-type="bibr" rid="scirp.81582-ref7">7</xref>], Dfn. 6.2, p. 148].</p><p>The diagram in <xref ref-type="fig" rid="fig1">Figure 1</xref> visualizes the initial eight branches of the coclass tree T 1 ( R ) with abelian root R = 〈 9 , 2 〉 ≃ C 3 &#215; C 3 . Basic definitions, facts, and notation concerning general descendant trees of finite p-groups are summarized briefly in [[<xref ref-type="bibr" rid="scirp.81582-ref18">18</xref>], &#167;2, pp. 410-411] [<xref ref-type="bibr" rid="scirp.81582-ref19">19</xref>]. They are discussed thoroughly in the broadest detail in the initial sections of [<xref ref-type="bibr" rid="scirp.81582-ref20">20</xref>]. Descendant trees are crucial for recent progress in the theory of p-class field towers [<xref ref-type="bibr" rid="scirp.81582-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref22">22</xref>], in particular for describing the mutual location of the second p-class group G p 2 F and the p-class tower group G p ∞ F of a number field G. Generally, the vertices of the coclass tree in the figure represent isomorphism classes of finite 3-groups. Two vertices are connected by a directed edge G → H if H is isomorphic to the last lower central quotient G / γ c ( G ) , where c = cl ( G ) = n − 1 denotes the nilpotency class of G, and | G | = 3 | H | , that is, γ c ( G ) ≃ C 3 is cyclic of order 3. See also [[<xref ref-type="bibr" rid="scirp.81582-ref18">18</xref>], &#167;2.2, p. 410-411] and [[<xref ref-type="bibr" rid="scirp.81582-ref20">20</xref>], &#167;4, p. 163-164].</p><p>The vertices of the tree diagram in <xref ref-type="fig" rid="fig1">Figure 1</xref> are classified by using various symbols:</p><p>1) big contour squares , represent abelian groups,</p><p>2) big full discs ・ represent metabelian groups with at least one abelian maximal subgroup,</p><p>3) small full discs ・ represent metabelian groups without abelian maximal subgroups.</p><p>The groups of particular importance are labelled by a number in angles, which is the identifier in the SmallGroups Library [<xref ref-type="bibr" rid="scirp.81582-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref24">24</xref>] of MAGMA [<xref ref-type="bibr" rid="scirp.81582-ref25">25</xref>]. We omit the orders, which are given on the left hand scale. The sTKT ϰ s [[<xref ref-type="bibr" rid="scirp.81582-ref2">2</xref>] Thm. 2.5, Tbl. 6-7], in the bottom rectangle concerns all vertices located vertically above. The first component τ ( 1 ) of the TTT [[<xref ref-type="bibr" rid="scirp.81582-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref27">27</xref>], Dfn. 3.3, p. 288] in the left rectangle concerns vertices G on the same horizontal level containing an abelian maximal subgroup. It is given in logarithmic notation. The periodicity with length 2 of branches, B ( j ) ≃ B ( j + 2 ) for j ≥ 4 , sets in with branch B ( 4 ) , having a root of order 3<sup>4</sup>.</p><p>3-class tower groups G = G 3 ∞ F with coclass cc ( G ) = 1 of real quadratic</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Deep TKT of 3-class tower groups G with τ ( G ) = ( 81 , 81 ) , ( 3 , 3 ) 3 </title></caption><table><tbody><thead><tr><th align="center" valign="middle" >G</th><th align="center" valign="middle" >ϰ d ( G )</th><th align="center" valign="middle" >MD</th></tr></thead><tr><td align="center" valign="middle" >G 1 10 ( 0,0 )</td><td align="center" valign="middle" >( 3,9,3,3 )</td><td align="center" valign="middle" >63,407,037</td></tr><tr><td align="center" valign="middle" >G 1 10 ( 0, − 1 )</td><td align="center" valign="middle" >( 3,3,9,9 )</td><td align="center" valign="middle" >62,565,429</td></tr><tr><td align="center" valign="middle" >G 1 10 ( 0,1 )</td><td align="center" valign="middle" >( 3,3,3,3 )</td><td align="center" valign="middle" >40,980,808</td></tr></tbody></table></table-wrap><p>fields F = ℚ ( d ) are located as arithmetically realized vertices on the tree diagram in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The minimal fundamental discriminants d, i.e. the MDs, are indicated by underlined boldface integers adjacent to the oval surrounding the realized vertex [<xref ref-type="bibr" rid="scirp.81582-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref25">25</xref>].</p><p>The double contour rectangle surrounds the vertices which became distinguishable by the progressive innovations in the present paper and were inseparable up to now.</p><p>In <xref ref-type="table" rid="table5">Table 5</xref>, we give the isomorphism type of the 3-class tower group G = G 3 ∞ F of all real quadratic fields F = ℚ ( d ) with 3-class group Cl 3 ( F ) ≃ C 3 &#215; C 3 and shallow transfer kernel type a.1, ϰ s = ( 0,0,0,0 ) , in its ground state τ ( F ) = ( 9 , 9 ) , ( 3 , 3 ) 3 , for the complete range 1 &lt; d &lt; 10 7 of 150 fundamental discriminants d. It was determined by means of Theorem 4.1, applied to the results of computing the (restricted) deep transfer kernel type ϰ d ( F ) = ( # k e r ( T F 3 ( 1 ) / E i ) ) 2 ≤ i ≤ 4 , consisting of the orders of the 3-principalization kernels of those unramified cyclic cubic extensions E i , 2 ≤ i ≤ 4 , in the Hilbert 3-class field F 3 ( 1 ) of F whose 3-class group Cl 3 ( E i ) is of type ( 3,3 ) . These trailing three components of the TTT τ ( F ) = ( 9 , 9 ) , ( 3 , 3 ) 3 were called its stable part in [[<xref ref-type="bibr" rid="scirp.81582-ref6">6</xref>], Dfn. 5.5, p. 84]. The computations were done with the aid of the computational algebra system MAGMA [<xref ref-type="bibr" rid="scirp.81582-ref25">25</xref>]. The 3-principalization kernel of the remaining extension E 1 with 3-class group Cl 3 ( E 1 ) of type ( 9,9 ) does not contain essential information and can be omitted. This leading component of the TTT τ ( F ) = ( 9 , 9 ) , ( 3 , 3 ) 3 was called its polarized part in [[<xref ref-type="bibr" rid="scirp.81582-ref6">6</xref>], Dfn. 5.5, p. 84]. For more details on the concepts stabilization and polarization, see [[<xref ref-type="bibr" rid="scirp.81582-ref6">6</xref>], &#167;6, pp. 90-95].</p><p>A systematic statistical evaluation of <xref ref-type="table" rid="table5">Table 5</xref> shows that, with respect to the complete range 1 &lt; d &lt; 10 7 , the group G ≃ 〈 729,99 〉 occurs most often with a clearly elevated relative frequency of 44%, whereas G ≃ 〈 729,100 〉 and G ≃ 〈 729,101 〉 share the common lower percentage of 28%, although the automorphism group Aut ( G ) of all three groups has the same order. However, the proportion 44 : 28 : 28 for the upper bound 10<sup>7</sup> is obviously not settled yet, because there are remarkable fluctuations, as <xref ref-type="table" rid="table6">Table 6</xref> shows. According to Boston, Bush and Hajir [<xref ref-type="bibr" rid="scirp.81582-ref28">28</xref>] [<xref ref-type="bibr" rid="scirp.81582-ref29">29</xref>], we have to expect an asymptotic limit 33 : 33 : 33 of the proportions for d → ∞ .</p></sec><sec id="s4_2"><title>4.2. Totally Real Dihedral Fields</title><p>In fact, we have computed much more information with MAGMA than mentioned at the end of the previous Section 4.1. To understand the actual scope of our numerical results it is necessary to recall that each unramified cyclic cubic relative extension E i / F , 1 ≤ i ≤ 4 , gives rise to a dihedral absolute extension E i / ℚ of degree 6, that is an S 3 -extension [[<xref ref-type="bibr" rid="scirp.81582-ref12">12</xref>], Prp. 4.1, p. 482]. For the trailing three fields E i , 2 ≤ i ≤ 4 , in the stable part of the TTT τ ( F ) = ( 9 , 9 ) , ( 3 , 3 ) 3 , i.e. with Cl 3 ( E i ) of type ( 3,3 ) , we have constructed the unramified cyclic cubic extensions E ˜ i , j / E i , 1 ≤ j ≤ 4 , and determined the Artin pattern AP ( E i ) of</p><table-wrap-group id="5"><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Statistics of 3-class tower groups G with τ ( G ) = ( 9 , 9 ) , ( 3 , 3 ) 3 </title></caption><table-wrap id="5_1"><table><tbody><thead><tr><th align="center" valign="middle" >No.</th><th align="center" valign="middle" >d</th><th align="center" valign="middle" >G</th><th align="center" valign="middle" >No.</th><th align="center" valign="middle" >d</th><th align="center" valign="middle" >G</th><th align="center" valign="middle" >No.</th><th align="center" valign="middle" >d</th><th align="center" valign="middle" >G</th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >62,501</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >51</td><td align="center" valign="middle" >3,995,004</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >101</td><td align="center" valign="middle" >7,313,928</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >152,949</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >52</td><td align="center" valign="middle" >4,045,265</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >102</td><td align="center" valign="middle" >7,391,212</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >252,977</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >53</td><td align="center" valign="middle" >4,183,205</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >103</td><td align="center" valign="middle" >7,406,249</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >358,285</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >54</td><td align="center" valign="middle" >4,196,840</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >104</td><td align="center" valign="middle" >7,415,841</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >531,437</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >4,199,901</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >105</td><td align="center" valign="middle" >7,447,697</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >586,760</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >56</td><td align="center" valign="middle" >4,220,977</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >106</td><td align="center" valign="middle" >7,502,501</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >595,009</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >57</td><td align="center" valign="middle" >4,233,608</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >107</td><td align="center" valign="middle" >7,601,081</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >726,933</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >58</td><td align="center" valign="middle" >4,252,837</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >108</td><td align="center" valign="middle" >7,623,320</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >801,368</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >59</td><td align="center" valign="middle" >4,409,313</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >109</td><td align="center" valign="middle" >7,630,645</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >940,593</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >60</td><td align="center" valign="middle" >4,429,612</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >110</td><td align="center" valign="middle" >7,634,065</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >966,489</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >61</td><td align="center" valign="middle" >4,533,032</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >111</td><td align="center" valign="middle" >7,643,993</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >1,177,036</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >62</td><td align="center" valign="middle" >4,586,797</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >112</td><td align="center" valign="middle" >7,683,308</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >1,192,780</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >63</td><td align="center" valign="middle" >4,662,917</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >113</td><td align="center" valign="middle" >7,704,653</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >1,313,292</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >64</td><td align="center" valign="middle" >4,680,701</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >114</td><td align="center" valign="middle" >7,713,961</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >15</td><td align="center" valign="middle" >1,315,640</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >65</td><td align="center" valign="middle" >4,766,309</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >115</td><td align="center" valign="middle" >7,804,828</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >1,358,556</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >66</td><td align="center" valign="middle" >4,782,664</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >116</td><td align="center" valign="middle" >7,936,316</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >17</td><td align="center" valign="middle" >1,398,829</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >67</td><td align="center" valign="middle" >4,783,697</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >117</td><td align="center" valign="middle" >8,037,645</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >18</td><td align="center" valign="middle" >1,463,729</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >68</td><td align="center" valign="middle" >4,965,009</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >118</td><td align="center" valign="middle" >8,101,277</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >1,580,709</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >69</td><td align="center" valign="middle" >5,039,692</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >119</td><td align="center" valign="middle" >8,235,965</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >1,595,669</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >70</td><td align="center" valign="middle" >5,048,988</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >120</td><td align="center" valign="middle" >8,248,953</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >21</td><td align="center" valign="middle" >1,722,344</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >71</td><td align="center" valign="middle" >5,111,669</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >121</td><td align="center" valign="middle" >8,263,020</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >1,751,909</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >72</td><td align="center" valign="middle" >5,119,637</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >122</td><td align="center" valign="middle" >8,320,764</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >23</td><td align="center" valign="middle" >1,831,097</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >73</td><td align="center" valign="middle" >5,154,385</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >123</td><td align="center" valign="middle" >8,375,228</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >24</td><td align="center" valign="middle" >1,942,385</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >74</td><td align="center" valign="middle" >5,226,941</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >124</td><td align="center" valign="middle" >8,501,541</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >2,021,608</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >75</td><td align="center" valign="middle" >5,226,941</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >125</td><td align="center" valign="middle" >8,523,385</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >26</td><td align="center" valign="middle" >2,042,149</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >76</td><td align="center" valign="middle" >5,350,569</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >126</td><td align="center" valign="middle" >8,578,617</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >27</td><td align="center" valign="middle" >2,076,485</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >77</td><td align="center" valign="middle" >5,353,240</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >127</td><td align="center" valign="middle" >8,623,704</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >28</td><td align="center" valign="middle" >2,185,465</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >78</td><td align="center" valign="middle" >5,362,136</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >128</td><td align="center" valign="middle" >8,637,717</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >29</td><td align="center" valign="middle" >2,197,669</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >79</td><td align="center" valign="middle" >5,400,712</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >129</td><td align="center" valign="middle" >8,674,397</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >2,314,789</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >5,478,321</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >130</td><td align="center" valign="middle" >8,723,237</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >31</td><td align="center" valign="middle" >2,409,853</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >81</td><td align="center" valign="middle" >5,827,564</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >131</td><td align="center" valign="middle" >8,737,913</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >32</td><td align="center" valign="middle" >2,433,221</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >82</td><td align="center" valign="middle" >5,891,701</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >132</td><td align="center" valign="middle" >8,748,764</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >33</td><td align="center" valign="middle" >2,539,129</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >83</td><td align="center" valign="middle" >5,909,217</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >133</td><td align="center" valign="middle" >8,816,389</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >34</td><td align="center" valign="middle" >2,555,249</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >84</td><td align="center" valign="middle" >5,982,269</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >134</td><td align="center" valign="middle" >8,957,485</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >35</td><td align="center" valign="middle" >2,710,072</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >85</td><td align="center" valign="middle" >6,105,693</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >135</td><td align="center" valign="middle" >8,993,409</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >36</td><td align="center" valign="middle" >2,851,877</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >86</td><td align="center" valign="middle" >6,155,861</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >136</td><td align="center" valign="middle" >9,006,397</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >37</td><td align="center" valign="middle" >2,954,929</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >87</td><td align="center" valign="middle" >6,337,340</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >137</td><td align="center" valign="middle" >9,051,665</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >38</td><td align="center" valign="middle" >3,005,369</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >88</td><td align="center" valign="middle" >6,429,997</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >138</td><td align="center" valign="middle" >9,058,892</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >39</td><td align="center" valign="middle" >3,197,864</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >89</td><td align="center" valign="middle" >6,618,085</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >139</td><td align="center" valign="middle" >9,130,973</td><td align="center" valign="middle" >〈 729,99 〉</td></tr></tbody></table></table-wrap><table-wrap id="5_2"><table><tbody><thead><tr><th align="center" valign="middle" >40</th><th align="center" valign="middle" >3,197,944</th><th align="center" valign="middle" >〈 729,101 〉</th><th align="center" valign="middle" >90</th><th align="center" valign="middle" >6,658,973</th><th align="center" valign="middle" >〈 729,100 〉</th><th align="center" valign="middle" >140</th><th align="center" valign="middle" >9,185,153</th><th align="center" valign="middle" >〈 729,101 〉</th></tr></thead><tr><td align="center" valign="middle" >41</td><td align="center" valign="middle" >3,258,120</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >91</td><td align="center" valign="middle" >6,792,365</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >141</td><td align="center" valign="middle" >9,195,769</td><td align="center" valign="middle" >〈 729,101 〉</td></tr><tr><td align="center" valign="middle" >42</td><td align="center" valign="middle" >3,323,065</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >92</td><td align="center" valign="middle" >6,806,152</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >142</td><td align="center" valign="middle" >9,328,597</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >43</td><td align="center" valign="middle" >3,342,785</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >93</td><td align="center" valign="middle" >6,882,737</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >143</td><td align="center" valign="middle" >9,379,849</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >44</td><td align="center" valign="middle" >3,644,357</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >94</td><td align="center" valign="middle" >6,927,452</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >144</td><td align="center" valign="middle" >9,380,744</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >45</td><td align="center" valign="middle" >3,658,421</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >95</td><td align="center" valign="middle" >6,953,513</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >145</td><td align="center" valign="middle" >9,419,704</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >46</td><td align="center" valign="middle" >3,692,717</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >96</td><td align="center" valign="middle" >6,974,609</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >146</td><td align="center" valign="middle" >9,511,580</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >47</td><td align="center" valign="middle" >3,721,565</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >97</td><td align="center" valign="middle" >7,010,133</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >147</td><td align="center" valign="middle" >9,615,813</td><td align="center" valign="middle" >〈 729,100 〉</td></tr><tr><td align="center" valign="middle" >48</td><td align="center" valign="middle" >3,799,597</td><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" >98</td><td align="center" valign="middle" >7,019,717</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >148</td><td align="center" valign="middle" >9,645,393</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >49</td><td align="center" valign="middle" >3,821,244</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >99</td><td align="center" valign="middle" >7,075,740</td><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" >149</td><td align="center" valign="middle" >9,801,773</td><td align="center" valign="middle" >〈 729,99 〉</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >3,869,909</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7,263,365</td><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" >150</td><td align="center" valign="middle" >9,834,557</td><td align="center" valign="middle" >〈 729,99 〉</td></tr></tbody></table></table-wrap></table-wrap-group><table-wrap id="table6" ><label><xref ref-type="table" rid="table6">Table 6</xref></label><caption><title> Proportions of 3-class tower groups G ≃ 〈 729, i 〉 with i ∈ { 99,100,101 } </title></caption><table><tbody><thead><tr><th align="center" valign="middle" >G</th><th align="center" valign="middle" >for d &lt; 10 6 &#215;</th><th align="center" valign="middle" >1</th><th align="center" valign="middle" >2</th><th align="center" valign="middle" >3</th><th align="center" valign="middle" >4</th><th align="center" valign="middle" >5</th><th align="center" valign="middle" >6</th><th align="center" valign="middle" >7</th><th align="center" valign="middle" >8</th><th align="center" valign="middle" >9</th><th align="center" valign="middle" >10</th></tr></thead><tr><td align="center" valign="middle" >〈 729,99 〉</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >36%</td><td align="center" valign="middle" >38%</td><td align="center" valign="middle" >41%</td><td align="center" valign="middle" >43%</td><td align="center" valign="middle" >40%</td><td align="center" valign="middle" >42%</td><td align="center" valign="middle" >45%</td><td align="center" valign="middle" >41%</td><td align="center" valign="middle" >43%</td><td align="center" valign="middle" >44%</td></tr><tr><td align="center" valign="middle" >〈 729,100 〉</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >36%</td><td align="center" valign="middle" >29%</td><td align="center" valign="middle" >24%</td><td align="center" valign="middle" >24%</td><td align="center" valign="middle" >31%</td><td align="center" valign="middle" >31%</td><td align="center" valign="middle" >30%</td><td align="center" valign="middle" >32%</td><td align="center" valign="middle" >29%</td><td align="center" valign="middle" >28%</td></tr><tr><td align="center" valign="middle" >〈 729,101 〉</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >27%</td><td align="center" valign="middle" >33%</td><td align="center" valign="middle" >35%</td><td align="center" valign="middle" >33%</td><td align="center" valign="middle" >29%</td><td align="center" valign="middle" >27%</td><td align="center" valign="middle" >25%</td><td align="center" valign="middle" >27%</td><td align="center" valign="middle" >28%</td><td align="center" valign="middle" >28%</td></tr></tbody></table></table-wrap><p>E i , in particular, the 3-principalization type of E i in the fields E ˜ i , j . The dihedral fields E i of degree 6 share a common polarization E ˜ i , 1 = F 3 ( 1 ) , the Hilbert 3-class field of F, which is contained in the relative 3-genus field ( E i / F ) ∗ , whereas the other extensions E ˜ i , j with 2 ≤ j ≤ 4 are non-abelian over F, for each 2 ≤ i ≤ 4 . Our computational results suggest the following conjecture concerning the infinite family of totally real dihedral fields E i for varying real quadratic fields F.</p><p>Conjecture 4.1. (3-class tower groups G of totally real dihedral fields.) Let F = ℚ ( d ) be a real quadratic field with fundamental discriminant d &gt; 1 , 3-class group Cl 3 ( F ) ≃ C 3 &#215; C 3 , and shallow transfer kernel type a.1, ϰ s ( F ) = ( 0,0,0,0 ) , in the ground state with transfer target type τ ( F ) ~ ( 9,9 ) , ( 3,3 ) 3 . Let E 2 , E 3 , E 4 be the three unramified cyclic cubic relative extensions of F with 3-class group Cl 3 ( E i ) of type ( 3,3 ) .</p><p>Then E i / ℚ is a totally real dihedral extension of degree 6, for each 2 ≤ i ≤ 4 , and the connection between the component ϰ d ( F ) i = # k e r ( T F 3 ( 1 ) / E i ) of the deep transfer kernel type ϰ d ( F ) of F and the 3-class tower group G i = G 3 ∞ E i = Gal ( ( E i ) 3 ( ∞ ) / E i ) of E i is given in the following way:</p><p>ϰ d ( F ) i = 3 ⇔ G i ≃ 〈 243,27 〉 with   ϰ s ( G i ) = ( 1,0,0,0 ) , ϰ d ( F ) i = 9 ⇔ G i ≃ 〈 243,26 〉 with   ϰ s ( G i ) = ( 0,0,0,0 ) . (4.2)</p><p>Remark 4.1. The conjecture is supported by all 3 ⋅ 150 = 450 totally real dihedral fields E i which were involved in the computation of <xref ref-type="table" rid="table5">Table 5</xref>. A provable argument for the truth of the conjecture is the fact that ϰ d ( F ) i = # k e r ( T F 3 ( 1 ) / E i ) = # ϰ s ( E i ) 1 = # ϰ s ( G i ) 1 , for 2 ≤ i ≤ 4 , but it does not explain why the sTKT ϰ s ( G i ) is a.2 with a fixed point if ϰ d ( F ) i = 3 . It is interesting that a dihedral field E i of degree 6 is satisfied with a non-s group, such as 〈 243,27 〉 , as its 3-class tower group. On the other hand, it is not surprising that a mainline group, such as 〈 243,26 〉 with sTKT a.1* and relation rank d 2 = 4 , is possible as G i = G 3 ∞ E i , since the upper Shafarevich bound for the relation rank of the 3-class tower group of a totally real dihedral field E i of degree 6 with Cl 3 ( E i ) ≃ C 3 &#215; C 3 is given by ρ + r 1 + r 2 − 1 = 2 + 6 + 0 − 1 = 7 &gt; 4 [[<xref ref-type="bibr" rid="scirp.81582-ref15">15</xref>], Thm. 1.3, p. 75].</p><p>Assuming an asymptotic limit 33 : 33 : 33 of the proportion of the real quadratic 3-class tower groups G ∈ { 〈 729,99 〉 , 〈 729,100 〉 , 〈 729,101 〉 } for the ground state of sTKT a.1, we can also conjecture an asymptotic limit 33 : 66 of the corresponding totally real dihedral 3-class tower groups G i ∈ { 〈 243,26 〉 , { 〈 243,27 〉 } , since the restricted dTKTs ( 9,3,3 ) , ( 3,9,9 ) , ( 3,3,3 ) together contain three times the 9 and six times the 3 in Equation (4.2).</p></sec></sec><sec id="s5"><title>Acknowledgements</title><p>The author gratefully acknowledges that his research was supported by the Austrian Science Fund (FWF): P 26008-N25. Note added in proof: While this paper was under review, we succeeded in proving Conjecture 4.1with the aid of Theorems 5.1, 6.1, 6.5,on pages 676, 678, 682 in [<xref ref-type="bibr" rid="scirp.81582-ref30">30</xref>].</p></sec><sec id="s6"><title>Cite this paper</title><p>Mayer, D.C. (2018) Deep Transfers of p-Class Tower Groups. Journal of Applied Mathematics and Physics, 6, 36-50. https://doi.org/10.4236/jamp.2018.61005</p></sec></body><back><ref-list><title>References</title><ref id="scirp.81582-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Artin, E. (1929) Idealklassen in Oberk&amp;#246rpern und allgemeines Reziprozit&amp;#228tsgesetz. Abh. Math. Sem. Univ. Hamburg, 7, 46-51. https://doi.org/10.1007/BF02941159</mixed-citation></ref><ref id="scirp.81582-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2012) Transfers of Metabelian p-Groups. Monatsh. Math., 166, 467-495. https://doi.org/10.1007/s00605-010-0277-x</mixed-citation></ref><ref id="scirp.81582-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Blackburn, N. (1958) On a Special Class of p-Groups. Acta Math., 100, 45-92.  
https://doi.org/10.1007/BF02559602</mixed-citation></ref><ref id="scirp.81582-ref4"><label>4</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Miech</surname><given-names> R.J. </given-names></name>,<etal>et al</etal>. (<year>1970</year>)<article-title>Metabelian p-Groups of Maximal Class. Trans. Amer. Math. Soc</article-title><source></source><volume> 152</volume>,<fpage> 331</fpage>-<lpage>373</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.81582-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Nebelung, B. (1989) Klassifikation metabelscher 3-Gruppen mit Faktorkommutatorgruppe vom Typ   und Anwendung auf das Kapitulationsproblem. Inauguraldissertation, Universit&amp;#228t zu K&amp;#246ln (W. Jehne).</mixed-citation></ref><ref id="scirp.81582-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2016) Artin Transfer Patterns on Descendant Trees of Finite p-Groups. Adv. Pure Math., 6, 66-104. Special Issue on Group Theory Research.  
https://doi.org/10.4236/apm.2016.62008</mixed-citation></ref><ref id="scirp.81582-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2017) Criteria for Three-Stage Towers of p-Class Fields. Adv. Pure Math., 7, 135-179. Special Issue on Number Theory.  
https://doi.org/10.4236/apm.2017.72008</mixed-citation></ref><ref id="scirp.81582-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Blackburn, N. (1957) On Prime-Power Groups in Which the Derived Group Has Two Generators. Proc. Camb. Phil. Soc., 53, 19-27.  
https://doi.org/10.1017/S0305004100031959</mixed-citation></ref><ref id="scirp.81582-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Heider, F.-P. and Schmithals, B. (1982) Zur Kapitulation der Idealklassen in unverzweigten primzyklischen Erweiterungen. J. Reine Angew. Math., 336, 1-25.</mixed-citation></ref><ref id="scirp.81582-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Pall, G. (1936) Note on Irregular Determinants. J. London Math. Soc., 11, 34-35.  
https://doi.org/10.1112/jlms/s1-11.1.34</mixed-citation></ref><ref id="scirp.81582-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (1991) List of Discriminants   of Totally Real Cubic Fields L, Arranged According to Their Multiplicities m and Conductors f. Computer Centre, Department of Computer Science, University of Manitoba, Winnipeg, Canada, Austrian Science Fund, Project Nr. J0497-PHY.</mixed-citation></ref><ref id="scirp.81582-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2012) The Second p-Class Group of a Number Field. Int. J. Number Theory, 8, 471-505. https://doi.org/10.1142/S179304211250025X</mixed-citation></ref><ref id="scirp.81582-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2014) Principalization Algorithm via Class Group Structure. J. Théor. Nombres Bordeaux, 26, 415-464. https://doi.org/10.5802/jtnb.874</mixed-citation></ref><ref id="scirp.81582-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Artin, E. (1927) Beweis des allgemeinen Reziprozit&amp;#228tsgesetzes. Abh. Math. Sem. Univ. Hamburg, 5, 353-363. https://doi.org/10.1007/BF02952531</mixed-citation></ref><ref id="scirp.81582-ref15"><label>15</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Mayer</surname><given-names> D.C. </given-names></name>,<etal>et al</etal>. (<year>2016</year>)<article-title>Recent Progress in Determining p-Class Field Towers. Gulf J. Math</article-title><source></source><volume> 4</volume>,<fpage> 74</fpage>-<lpage>102</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.81582-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2016) p-Capitulation over Number Fields with p-Class Rank Two. J. Appl. Math. Phys., 4, 1280-1293. https://doi.org/10.4236/jamp.2016.47135</mixed-citation></ref><ref id="scirp.81582-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2016) p-Capitulation over Number Fields with p-Class Rank Two. 2nd International Conference on Groups and Algebras (ICGA) 2016, Suzhou, Presentation delivered on July 26, 2016. https://doi.org/10.4236/jamp.2016.47135</mixed-citation></ref><ref id="scirp.81582-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2013) The Distribution of Second p-Class Groups on Coclass Graphs. J. Théor. Nombres Bordeaux, 25, 401-456. https://doi.org/10.5802/jtnb.842</mixed-citation></ref><ref id="scirp.81582-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2011) The Distribution of Second p-Class Groups on Coclass Graphs. 27ièmes Journées Arithmétiques, Faculty of Math. and Informatics, Univ. of Vilnius, Lithuania, Presentation Delivered on 1 July 2011.</mixed-citation></ref><ref id="scirp.81582-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2015) Periodic Bifurcations in Descendant Trees of Finite p-Groups. Adv. Pure Math., 5, 162-195. Special Issue on Group Theory.  
https://doi.org/10.4236/apm.2015.54020</mixed-citation></ref><ref id="scirp.81582-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2016) Three-Stage Towers of 5-Class Fields. arXiv: 1604.06930v1 [math.NT] 23 Apr 2016.</mixed-citation></ref><ref id="scirp.81582-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2016) Recent Progress in Determining p-Class Field Towers. 1st International Colloquium of Algebra, Number Theory, Cryptography and Information Security (ANCI) 2016, Faculté Polydisciplinaire de Taza, Université Sidi Mohamed Ben Abdellah, Fès, Morocco, Invited Keynote Delivered on 12 November 2016.  
http://www.algebra.at/ANCI2016DCM.pdf</mixed-citation></ref><ref id="scirp.81582-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Besche, H.U., Eick, B. and O'Brien, E.A. (2002) A Millennium Project: Constructing Small Groups. Int. J. Algebra Comput., 12, 623-644.  
https://doi.org/10.1142/S0218196702001115</mixed-citation></ref><ref id="scirp.81582-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Besche, H.U., Eick, B. and O'Brien, E.A. (2005) The Small Groups Library—A Library of Groups of Small Order. An Accepted and Refereed GAP Package, Available Also in MAGMA.</mixed-citation></ref><ref id="scirp.81582-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">The MAGMA Group, MAGMA (2017) Computational Algebra System. Version 2.23-3, Sydney. http://magma.maths.usyd.edu.au</mixed-citation></ref><ref id="scirp.81582-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2015) Index-p Abelianization Data of p-Class Tower Groups. Adv. Pure Math., 5, 286-313. Special Issue on Number Theory and Cryptography.  
https://doi.org/10.4236/apm.2015.55029</mixed-citation></ref><ref id="scirp.81582-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2015) Index-p Abelianization Data of p-Class Tower Groups. 29ièmes Journées Arithmétiques, Univ. of Debrecen, Hungary, Presentation Delivered on 9 July 2015.</mixed-citation></ref><ref id="scirp.81582-ref28"><label>28</label><mixed-citation publication-type="other" xlink:type="simple">Boston, N., Bush, M.R. and Hajir, F. (2017) Heuristics for p-Class Towers of Imaginary Quadratic Fields. Math. Ann., 368, 633-669.  
https://doi.org/10.1007/s00208-016-1449-3</mixed-citation></ref><ref id="scirp.81582-ref29"><label>29</label><mixed-citation publication-type="other" xlink:type="simple">Boston, N., Bush, M.R. and Hajir, F. Heuristics for p-Class Towers of Real Quadratic Fields, to Appear.</mixed-citation></ref><ref id="scirp.81582-ref30"><label>30</label><mixed-citation publication-type="other" xlink:type="simple">Mayer, D.C. (2017) Successive Approximation of p-Class Towers. Adv. Pure Math., 7, 660-685. Special Issue on Abstract Algebra. 
https://doi.org/10.4236/apm.2017.712041</mixed-citation></ref></ref-list></back></article>