Masteries · Jason GlowneyArithmoí Book 1

Masteries

1.5.7 Smoothing the Minimal Element Basis

Con­tin­u­ous func­tions define there are no gaps be­tween points on the func­tion and that it is dif­fer­en­tiable every­where. This pro­vides the min­i­mum re­quire­ments for a func­tion to be smooth, and the smooth­ness of a func­tion is a prop­er­ty re­lat­ed to the number of con­tin­u­ous de­riv­a­tives it has over a domain. If a func­tion has con­tin­u­ous de­riv­a­tives for all orders in its domain, this func­tion is re­ferred to as a C-in­fin­i­ty func­tion C∞.C^{\infty}.We also note that the min­i­mal el­e­ment basis is the lim­iter in terms of the angle co­ef­fi­cients that can be chosen. Mind­ful of this, we return to

(e2iπ(𝓃𝒹))K𝓂ℯ=e2iπk,\begin{array}{r} \left( e^{2i\pi\left( \frac{\mathcal{n}}{\mathcal{d}} \right)} \right)^{\mathrm{K}_{\mathcal{me}}} = e^{2i\pi k}, \end{array}
(1.5.107)

and state the fol­low­ing the­o­rem.

The­o­rem (1.5.108) – For any so­lu­tions of K𝓂ℯ\mathrm{K}_{\mathcal{me}}, the wind­ing number kk of any re­duced ra­tio­nal number chosen for 𝓃𝒹\frac{\mathcal{n}}{\mathcal{d}}, re­sults in a wind­ing number equal to 𝓃\mathcal{n}. For non-re­duced ra­tio­nals, and 𝓃𝒹\frac{\mathcal{n}}{\mathcal{d}} in ra­di­ans, the wind­ing number kk will be equal to the re­duced number 𝓃\mathcal{n} for that ra­tio­nal.

Proof – Sim­i­lar the pre­vi­ous sec­tion, for K𝓂ℯ\mathrm{K}_{\mathcal{me}}, the number of el­e­ments in the min­i­mal el­e­ment basis, 𝓃\mathcal{n}, the nu­mer­a­tor of the ra­tio­nal ex­pres­sion ∈ℤ\in \mathbb{Z}, 𝒹\mathcal{d}, the de­nom­i­na­tor of the ra­tio­nal ex­pres­sion ∈ℤ\in \mathbb{Z}, and kk, the wind­ing number, we first solve the fol­low­ing for kk

(e2iπ(𝓃𝒹))K𝓂ℯ=e2iπk→ln⁡((e2iπ(𝓃𝒹))K𝓂ℯ)=ln⁡(e2iπk)→\left( e^{2i\pi\left( \frac{\mathcal{n}}{\mathcal{d}} \right)} \right)^{\mathrm{K}_{\mathcal{me}}} = e^{2i\pi k} \rightarrow \ln{\left( \left( e^{2i\pi\left( \frac{\mathcal{n}}{\mathcal{d}} \right)} \right)^{\mathrm{K}_{\mathcal{me}}} \right) = \ln\left( e^{2i\pi k} \right)} \rightarrow
2iπ(𝓃𝒹)K𝓂ℯ=2iπk→k=2iπ𝓃K𝓂ℯi2π𝒹→2i\pi\left( \frac{\mathcal{n}}{\mathcal{d}} \right)\mathrm{K}_{\mathcal{me}} = 2i\pi k \rightarrow k = \frac{2i\pi\mathcal{n}\mathrm{K}_{\mathcal{me}}}{i2\pi\mathcal{d}} \rightarrow
k=𝓃K𝓂ℯ𝒹.\begin{array}{r} k = \frac{\mathcal{n}\mathrm{K}_{\mathcal{me}}}{\mathcal{d}}. \end{array}

We can solve the above to show that K𝓂ℯ=k𝒹𝓃\mathrm{K}_{\mathcal{me}} = \frac{k\mathcal{d}}{\mathcal{n}}, but we can also show that K𝓂ℯ=𝒹,\mathrm{K}_{\mathcal{me}}= \mathcal{d}, based on the fact that the min­i­mal el­e­ment will be 2iπ(1𝒹)2i\pi\left( \frac{1}{\mathcal{d}} \right) for all re­duced ra­tio­nals, and for K𝓂ℯ=k𝒹𝓃,\mathrm{K}_{\mathcal{me}} = \frac{k\mathcal{d}}{\mathcal{n}}, this im­plies that k=𝓃k = \mathcal{n}, and then arrive at K𝓂ℯ=𝒹\mathrm{K}_{\mathcal{me}}= \mathcal{d}, stated ex­plic­it­ly, as

K𝓂ℯ=𝒹k𝓃∴k=𝓃.\begin{array}{r} \mathrm{K}_{\mathcal{me}} = \frac{\mathcal{d}k}{\mathcal{n}}\therefore k = \mathcal{n}. \end{array}

To prove that K𝓂ℯ=𝒹\mathrm{K}_{\mathcal{me}}= \mathcal{d}, we can use the finite 𝒹×𝒹\mathcal{d} \times \mathcal{d} ma­tri­ces of the cyclic groups of the form Z𝒹Z_{\mathcal{d}}, for 𝒹\mathcal{d}, the in­te­ger value of the ra­tio­nal de­nom­i­na­tor we have been work­ing with. The el­e­ments of the group will have the fol­low­ing matrix tem­plate, where the column number of the first row serves as the nu­mer­a­tor value 𝓃+1\mathcal{n} + 1, and all other matrix en­tries, apart from the en­tries with value e2iπ(𝓃𝒹)e^{2i\pi\left( \frac{\mathcal{n}}{\mathcal{d}} \right)}, will be set to zero

(e2iπ(0𝒹)e2iπ(1𝒹)e2iπ(2𝒹)e2iπ(3𝒹)⋯e2iπ(𝒹 −1𝒹)e2iπ(𝒹 −1𝒹)e2iπ(0𝒹)e2iπ(1𝒹)e2iπ(2𝒹)⋯e2iπ(𝒹−2 𝒹)e2iπ(𝒹−2 𝒹)e2iπ(𝒹 −1𝒹)e2iπ(0𝒹)e2iπ(1𝒹)⋯e2iπ(𝒹−3 𝒹)e2iπ(𝒹−3 𝒹)ei2π(𝒹−2 𝒹)e2iπ(𝒹 −1𝒹)e2iπ(0𝒹)⋯e2iπ(𝒹−4 𝒹)⋮⋮⋮⋮⋱⋮e2iπ(1𝒹)ei2π(2𝒹)e2iπ(3𝒹)e2iπ(4𝒹)⋯e2iπ(0𝒹)).\begin{array}{r} \begin{pmatrix} e^{2i\pi\left( \frac{0}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{2}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{3}{\mathcal{d}} \right)} & \cdots & e^{2i\pi\left( \frac{\mathcal{d}\ - 1}{\mathcal{d}} \right)} \\ e^{2i\pi\left( \frac{\mathcal{d}\ - 1}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{0}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{2}{\mathcal{d}} \right)} & \cdots & e^{2i\pi\left( \frac{\mathcal{d} -2\ }{\mathcal{d}} \right)} \\ e^{2i\pi\left( \frac{\mathcal{d} -2\ }{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{\mathcal{d}\ - 1}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{0}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} & \cdots & e^{2i\pi\left( \frac{\mathcal{d} -3\ }{\mathcal{d}} \right)} \\ e^{2i\pi\left( \frac{\mathcal{d} -3\ }{\mathcal{d}} \right)} & e^{i2\pi\left( \frac{\mathcal{d} -2\ }{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{\mathcal{d}\ - 1}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{0}{\mathcal{d}} \right)} & \cdots & e^{2i\pi\left( \frac{\mathcal{d} -4\ }{\mathcal{d}} \right)} \\ \vdots & \vdots & \vdots & \vdots & \ddots & \vdots \\ e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} & e^{i2\pi\left( \frac{2}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{3}{\mathcal{d}} \right)} & e^{2i\pi\left( \frac{4}{\mathcal{d}} \right)} & \cdots & e^{2i\pi\left( \frac{0}{\mathcal{d}} \right)} \end{pmatrix}. \end{array}

The entry, a1,1=e2iπ(0𝒹)a_{1,1} = e^{2i\pi\left( \frac{0}{\mathcal{d}} \right)}, which con­tin­ues down the main di­ag­o­nal is the iden­ti­ty el­e­ment ϵ.\epsilon. The min­i­mal el­e­ment is the first entry to the right of a1,1a_{1,1}, for a1,2=e2iπ(1𝒹)a_{1,2} = e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)}, and con­tin­ues along its di­ag­o­nal path to form the min­i­mal el­e­ment matrix. These ma­tri­ces are modulo 𝒹\mathcal{d}, which rep­re­sents a ro­ta­tion of 2iπ2i\pi ra­di­ans on the unit circle. In the cyclic groups, the prim­i­tive root is the same thing we have been re­fer­ring to as the min­i­mal el­e­ment, and as such, every el­e­ment in the cyclic group can be thought of as a power of this prim­i­tive root. So, an­oth­er way to con­sid­er every entry in the matrix tem­plate is for the set of en­tries that is sim­i­lar to our orig­i­nal de­f­i­n­i­tion, but with the 𝓃\mathcal{n} vari­able set to 1. This acts on the min­i­mal el­e­ment, or prim­i­tive root, by

(e2iπ(1𝒹))K𝓂ℯ:K𝓂ℯ={1,2,3,…,𝒹},\begin{array}{r} \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathrm{K}_{\mathcal{me}}}:\mathrm{K}_{\mathcal{me}} = \left\{ 1,2,3,\ldots,\mathcal{d} \right\}, \end{array}

and since the prim­i­tive root ro­tates coun­ter­clock­wise by one el­e­ment at a time on unit circle, this trans­lates as one column shift to the right on the tem­plate matrix. We can ex­press any value of (e2iπ(𝓃𝒹))K𝓂ℯ\left( e^{2i\pi\left( \frac{\mathcal{n}}{\mathcal{d}} \right)} \right)^{\mathrm{K}_{\mathcal{me}}}, as its min­i­mal el­e­ment, or prim­i­tive root, rep­re­sen­ta­tion (e2iπ(1𝒹))𝓃K𝓂ℯ\left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{n}\mathrm{K}_{\mathcal{me}}}, for 𝓃\mathcal{n}, the power to which we raise the min­i­mal el­e­ment, which is also equal to the nu­mer­a­tor in our orig­i­nal form. In this form, it is clear to see that every number in the set of el­e­ments

𝓂ℯ={(e2iπ(1𝒹))1,(e2iπ(1𝒹))2,…,(e2iπ(1𝒹))𝒹},\begin{array}{r} \mathcal{me} =\left\{ \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{1},\left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{2},\ldots,\left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}} \right\}, \end{array}

is a power of the min­i­mal el­e­ment. Since K𝓂ℯ\mathrm{K}_{\mathcal{me}} is the non-zero ex­po­nen­tial power that the min­i­mal el­e­ment is raised to in order to equal ϵ\epsilon, for K𝓂ℯ=𝒹\mathrm{K}_{\mathcal{me}}= \mathcal{d}, we have our first iden­ti­ty ϵ\epsilon, for a non-zero ex­po­nen­tial. As we have stated in the de­f­i­n­i­tion, K𝓂ℯ\mathrm{K}_{\mathcal{me}} is the number of unique el­e­ments in the set of the min­i­mal el­e­ment basis, after pass­ing K𝓂ℯ=𝒹\mathrm{K}_{\mathcal{me}}= \mathcal{d}, for it­er­a­tive powers (e2iπ(1𝒹))K𝓂ℯ\left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathrm{K}_{\mathcal{me}}}, the cyclic nature of the el­e­ment re­peats itself. There­fore, the total number of unique el­e­ments in the set of the min­i­mal el­e­ment basis equals K𝓂ℯ\mathrm{K}_{\mathcal{me}}, which is equal to 𝒹\mathcal{d}. We can now con­sid­er the fol­low­ing equa­tion with subtle changes, and since we are taking powers of the min­i­mal el­e­ment, we know that the wind­ing number will in­crease by one after every factor K𝓂ℯ=𝒹\mathrm{K}_{\mathcal{me}}= \mathcal{d}. Now we can solve again for K𝓂ℯ\mathrm{K}_{\mathcal{me}}, having proved that it is equal to 𝒹\mathcal{d} for the fol­low­ing,

(e(2iπ1𝒹))𝓃K𝓂ℯ=e2iπk→(2iπ𝓃K𝓂ℯ)K𝓂ℯ=2iπk→K𝓂ℯ=k𝓃(K𝓂ℯ),\left( e^{\left( 2i\pi\frac{1}{\mathcal{d}} \right)} \right)^{{\mathcal{n}\mathrm{K}}_{\mathcal{me}}} = e^{2i\pi k} \rightarrow \left( \frac{2i\pi\mathcal{n}}{\mathrm{K}_{\mathcal{me}}} \right)\mathrm{K}_{\mathcal{me}} = 2i\pi k \rightarrow \mathrm{K}_{\mathcal{me}} = \frac{k}{\mathcal{n}}\left( \mathrm{K}_{\mathcal{me}} \right),

there­fore, kk must be equal to the value 𝓃\mathcal{n}.

 □\begin{array}{r} \ \square \end{array}

To clar­i­fy the matrix tem­plate in­tro­duced in the pre­vi­ous the­o­rem, we present an ex­am­ple of a 6×66 \times 6 matrix. We start first by the zero-wind iden­ti­ty per­mu­ta­tion ϵ𝓌𝒾𝓃𝒹(0),\epsilon_{\mathcal{wind}(0)},

ϵ𝓌𝒾𝓃𝒹(0)=(e2iπ(06)000000e2iπ(06)000000e2iπ(06)000000e2iπ(06)000000e2iπ(06)000000e2iπ(06)),\begin{array}{r} \epsilon_{\mathcal{wind}(0)} = \begin{pmatrix} e^{2i\pi\left( \frac{0}{6} \right)} & 0 & 0 & 0 & 0 & 0 \\ 0 & e^{2i\pi\left( \frac{0}{6} \right)} & 0 & 0 & 0 & 0 \\ 0 & 0 & e^{2i\pi\left( \frac{0}{6} \right)} & 0 & 0 & 0 \\ 0 & 0 & 0 & e^{2i\pi\left( \frac{0}{6} \right)} & 0 & 0 \\ 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{0}{6} \right)} & 0 \\ 0 & 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{0}{6} \right)} \end{pmatrix}, \end{array}
(1.5.109)

and the dis­tance trav­elled from ϵ𝓌𝒾𝓃𝒹=0\epsilon_{\mathcal{wind} = 0} to the min­i­mal dis­tance point on the unit circle is e2iπ(16)=eiπ(13)e^{2i\pi\left( \frac{1}{6} \right)} = e^{i\pi\left( \frac{1}{3} \right)}, which is the min­i­mal el­e­ment per­mu­ta­tion 𝓂ℯ𝓌𝒾𝓃𝒹(0)\mathcal{m}\mathcal{e}_{\mathcal{wind}(0)}

𝓂ℯ𝓌𝒾𝓃𝒹(0)=(0e2iπ(16)000000e2iπ(16)000000e2iπ(16)000000e2iπ(16)000000e2iπ(16)e2iπ(16)00000).\begin{array}{r} \mathcal{m}\mathcal{e}_{\mathcal{wind}(0)} = \begin{pmatrix} 0 & e^{2i\pi\left( \frac{1}{6} \right)} & 0 & 0 & 0 & 0 \\ 0 & 0 & e^{2i\pi\left( \frac{1}{6} \right)} & 0 & 0 & 0 \\ 0 & 0 & 0 & e^{2i\pi\left( \frac{1}{6} \right)} & 0 & 0 \\ 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{1}{6} \right)} & 0 \\ 0 & 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{1}{6} \right)} \\ e^{2i\pi\left( \frac{1}{6} \right)} & 0 & 0 & 0 & 0 & 0 \end{pmatrix}. \end{array}
(1.5.110)

The next per­mu­ta­tion in the cyclic group Z6Z_{6} is

𝓂ℯ𝓌𝒾𝓃𝒹(0)×𝓂ℯ=(00e2iπ(26)000000e2iπ(26)000000e2iπ(26)000000e2iπ(26)e2iπ(26)000000e2iπ(26)0000),\begin{array}{r} \mathcal{m}\mathcal{e}_{\mathcal{wind}(0)}\times \mathcal{me} =\begin{pmatrix} 0 & 0 & e^{2i\pi\left( \frac{2}{6} \right)} & 0 & 0 & 0 \\ 0 & 0 & 0 & e^{2i\pi\left( \frac{2}{6} \right)} & 0 & 0 \\ 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{2}{6} \right)} & 0 \\ 0 & 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{2}{6} \right)} \\ e^{2i\pi\left( \frac{2}{6} \right)} & 0 & 0 & 0 & 0 & 0 \\ 0 & e^{2i\pi\left( \frac{2}{6} \right)} & 0 & 0 & 0 & 0 \end{pmatrix}, \end{array}
(1.5.111)

and the next

𝓂ℯ𝓌𝒾𝓃𝒹(0)×(𝓂ℯ)2=(000e2iπ(36)000000e2iπ(36)000000e2iπ(36)e2iπ(36)000000e2iπ(36)000000e2iπ(36)000)….\begin{array}{r} \mathcal{m}\mathcal{e}_{\mathcal{wind}(0)} \times \left( \mathcal{me} \right)^{2} = \begin{pmatrix} 0 & 0 & 0 & e^{2i\pi\left( \frac{3}{6} \right)} & 0 & 0 \\ 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{3}{6} \right)} & 0 \\ 0 & 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{3}{6} \right)} \\ e^{2i\pi\left( \frac{3}{6} \right)} & 0 & 0 & 0 & 0 & 0 \\ 0 & e^{2i\pi\left( \frac{3}{6} \right)} & 0 & 0 & 0 & 0 \\ 0 & 0 & e^{2i\pi\left( \frac{3}{6} \right)} & 0 & 0 & 0 \end{pmatrix}\ldots. \end{array}
(1.5.112)

The cyclic per­mu­ta­tion just prior to ar­riv­ing at the iden­ti­ty has the form e2iπ(𝒹−1𝒹)e^{2i\pi\left( \frac{\mathcal{d} - 1}{\mathcal{d}} \right)}, and for Z6Z_{6} is

e2iπ(6−16)=𝓂ℯ𝓌𝒾𝓃𝒹(0)×(𝓂ℯ)6−2=(𝓂ℯ)e𝓌𝒾𝓃𝒹(0)6−1=(𝓂ℯ)1×6−1=(𝓂ℯ)6−1,\begin{array}{r} e^{2i\pi\left( \frac{6 - 1}{6} \right)}= \mathcal{m}\mathcal{e}_{\mathcal{wind}(0)} \times \left( \mathcal{me} \right)^{6 - 2} = \left( \mathcal{me} \right)^{e^{\mathcal{wind}(0)}6 - 1} = \left( \mathcal{me} \right)^{1 \times 6 - 1} = \left( \mathcal{me} \right)^{6 - 1}, \end{array}
(1.5.113)

which is the per­mu­ta­tion matrix

(𝓂ℯ)6−1=(00000e2iπ(56)e2iπ(56)000000e2iπ(56)000000e2iπ(56)000000e2iπ(56)000000e2iπ(56)0).\begin{array}{r} \left( \mathcal{me} \right)^{6 - 1} = \begin{pmatrix} 0 & 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{5}{6} \right)} \\ e^{2i\pi\left( \frac{5}{6} \right)} & 0 & 0 & 0 & 0 & 0 \\ 0 & e^{2i\pi\left( \frac{5}{6} \right)} & 0 & 0 & 0 & 0 \\ 0 & 0 & e^{2i\pi\left( \frac{5}{6} \right)} & 0 & 0 & 0 \\ 0 & 0 & 0 & e^{2i\pi\left( \frac{5}{6} \right)} & 0 & 0 \\ 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{5}{6} \right)} & 0 \end{pmatrix}. \end{array}
(1.5.114)

Based on the cyclic group nature, the next it­er­a­tion brings us to the iden­ti­ty el­e­ment at the point on the unit circle, e2iπ(66)=e2iπ(1)=e2iπ,e^{2i\pi\left( \frac{6}{6} \right)} = e^{2i\pi(1)} = e^{2i\pi},oc­cur­ring at the cyclic el­e­ment for 𝓀=𝒹\ \mathcal{k} = \mathcal{d}, at e2iπ(𝓀𝒹)e^{2i\pi\left( \frac{\mathcal{k}}{\mathcal{d}} \right)}. For this ex­am­ple, when 𝓀=6\mathcal{k} = 6, the it­er­a­tion is lo­cat­ed at e2iπ(66)=e2iπ(1)=ϵ𝓌𝒾𝓃𝒹(1)e^{2i\pi\left( \frac{6}{6} \right)} = e^{2i\pi(1)} = \epsilon_{\mathcal{wind}(1)},

ϵ𝓌𝒾𝓃𝒹(1)=(e2iπ(66)000000e2iπ(66)000000e2iπ(66)000000e2iπ(66)000000e2iπ(66)000000e2iπ(66)).\begin{array}{r} \epsilon_{\mathcal{wind}(1)} = \begin{pmatrix} e^{2i\pi\left( \frac{6}{6} \right)} & 0 & 0 & 0 & 0 & 0 \\ 0 & e^{2i\pi\left( \frac{6}{6} \right)} & 0 & 0 & 0 & 0 \\ 0 & 0 & e^{2i\pi\left( \frac{6}{6} \right)} & 0 & 0 & 0 \\ 0 & 0 & 0 & e^{2i\pi\left( \frac{6}{6} \right)} & 0 & 0 \\ 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{6}{6} \right)} & 0 \\ 0 & 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{6}{6} \right)} \end{pmatrix}. \end{array}
(1.5.115)

The min­i­mal el­e­ment chosen for e2iπ(𝓃𝒹)e^{2i\pi\left( \frac{\mathcal{n}}{\mathcal{d}} \right)}, was e2iπ(16),e^{2i\pi\left( \frac{1}{6} \right)},which will always have a wind­ing number equal to 𝓃=1\mathcal{n} = 1 on the com­plex unit circle. We saw the re­duced form was equal to eiπ(𝓀𝒹2)=eiπ(13),e^{i\pi\left( \frac{\mathcal{k}}{\frac{\mathcal{d}}{2}} \right)} = e^{i\pi\left( \frac{1}{3} \right)},where the wind­ing number 𝓀\mathcal{k} is also equal to 1.1.Using the non-re­duced eiπ(13)=e2iπ(16){e^{i\pi\left( \frac{1}{3} \right)} = e}^{2i\pi\left( \frac{1}{6} \right)}, we can more read­i­ly see that we are work­ing with the Z6Z_{6} cyclic group. Con­tin­u­ing the ex­am­ple, we know that the next per­mu­ta­tion is going to be the min­i­mal el­e­ment per­mu­ta­tion, or more suc­cinct­ly, e2iπ(ϵ𝓌𝒾𝓃𝒹(1))×e2iπ(1𝒹)=e2iπ(1+1𝒹)=𝓂ℯ𝓌𝒾𝓃𝒹(1)e^{2i\pi\left( \epsilon_{\mathcal{wind}(1)} \right)} \times e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} = e^{2i\pi\left( 1 + \frac{1}{\mathcal{d}} \right)}= \mathcal{m}\mathcal{e}_{\mathcal{wind}(1)}, which is the per­mu­ta­tion

𝓂ℯ𝓌𝒾𝓃𝒹(1)=(0e2iπ(76)000000e2iπ(76)000000e2iπ(76)000000e2iπ(76)000000e2iπ(76)e2iπ(76)00000).\begin{array}{r} \mathcal{m}\mathcal{e}_{\mathcal{wind}(1)} = \begin{pmatrix} 0 & e^{2i\pi\left( \frac{7}{6} \right)} & 0 & 0 & 0 & 0 \\ 0 & 0 & e^{2i\pi\left( \frac{7}{6} \right)} & 0 & 0 & 0 \\ 0 & 0 & 0 & e^{2i\pi\left( \frac{7}{6} \right)} & 0 & 0 \\ 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{7}{6} \right)} & 0 \\ 0 & 0 & 0 & 0 & 0 & e^{2i\pi\left( \frac{7}{6} \right)} \\ e^{2i\pi\left( \frac{7}{6} \right)} & 0 & 0 & 0 & 0 & 0 \end{pmatrix}. \end{array}
(1.5.116)

There are easier and less ex­pan­sive ways of prov­ing the pre­vi­ous the­o­rem but by show­ing the con­nec­tion the min­i­mal el­e­ment has with the cyclic groups and prim­i­tive root, we can see that they are the same. By defin­ing the cyclic group tem­plate in terms of powers of the min­i­mal el­e­ment, it proves useful to de­scribe a cyclic matrix group ℤ𝒹(𝓂ℯ)+\mathbb{Z}_{\mathcal{d}\left( \mathcal{me} \right)}^{+}

ℤ𝒹(𝓂ℯ)+=((e2iπ(1𝒹))𝒹s(e2iπ(1𝒹))𝒹s+k(e2iπ(1𝒹))𝒹s+2k(e2iπ(1𝒹))𝒹s+3k⋯(e2iπ(1𝒹))𝒹s+(𝒹−1)k(e2iπ(1𝒹))𝒹s+(𝒹−1)k(e2iπ(1𝒹))ds(e2iπ(1𝒹))𝒹s+k(e2iπ(1𝒹))𝒹s+2k⋯(e2iπ(1𝒹))𝒹s+(𝒹−2)k(e2iπ(1𝒹))𝒹s+(𝒹−2)k(e2iπ(1𝒹))𝒹s+(𝒹−1)k(e2iπ(1𝒹))ds(e2iπ(1𝒹))𝒹s+k⋯(e2iπ(1𝒹))𝒹s+(𝒹−3)k(e2iπ(1𝒹))𝒹s+(𝒹−2)k(e2iπ(1𝒹))𝒹s+(𝒹−2)k(e2iπ(1𝒹))𝒹s+(𝒹−1)k(e2iπ(1𝒹))ds⋯(e2iπ(1𝒹))𝒹s+(𝒹−4)k⋮⋮⋮⋮⋱⋮(e2iπ(1𝒹))𝒹s+k(e2iπ(1𝒹))𝒹s+2k(e2iπ(1𝒹))𝒹s+3k(e2iπ(1𝒹))𝒹s+4k⋯(e2iπ(1𝒹))ds),\begin{array}{r} \mathbb{Z}_{\mathcal{d}\left( \mathcal{me} \right)}^{+} = \begin{pmatrix} \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + 2k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + 3k} & \cdots & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + \left( \mathcal{d} -1 \right)k} \\ \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + \left( \mathcal{d} -1 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{ds} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + 2k} & \cdots & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + \left( \mathcal{d} -2 \right)k} \\ \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + \left( \mathcal{d} -2 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + \left( \mathcal{d} -1 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{ds} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + k} & \cdots & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + \left( \mathcal{d} -3 \right)k} \\ \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + \left( \mathcal{d} -2 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + \left( \mathcal{d} -2 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + \left( \mathcal{d} -1 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{ds} & \cdots & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + \left( \mathcal{d} -4 \right)k} \\ \vdots & \vdots & \vdots & \vdots & \ddots & \vdots \\ \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + 2k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + 3k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s + 4k} & \cdots & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{ds} \end{pmatrix}, \end{array}
(1.5.117)

In ℤ𝒹(𝓂ℯ)+\mathbb{Z}_{\mathcal{d}\left( \mathcal{me} \right)}^{+}, all en­tries are in terms of the min­i­mal el­e­ment, and the ex­po­nen­tial terms are re­lat­ed to the de­nom­i­na­tor value, (or the K𝓂ℯ\mathrm{K}_{\mathcal{me}} value) 𝒹\mathcal{d}, the wind­ing number k={0,1,2,3,…},k = \left\{ 0,1,2,3,\ldots \right\},and the cyclic dis­tance it­er­a­tion s={0,1,2,3,…}s = \left\{ 0,1,2,3,\ldots \right\}, away from the iden­ti­ty el­e­ment ϵ=(e2iπ(1𝒹))𝒹k,\epsilon = \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}k},in the coun­ter­clock­wise ori­en­ta­tion. This kk in the cyclic dis­tance re­lates to our former value of 𝓃\mathcal{n} in the nu­mer­a­tor. We can also define a tem­plate for the clock­wise cyclic group ℤ𝒹(𝓂ℯ)−\mathbb{Z}_{\mathcal{d}\left( \mathcal{me} \right)}^{-}

ℤ𝒹(𝓂ℯ)−=((e2iπ(1𝒹))𝒹s(e2iπ(1𝒹))𝒹s−k(e2iπ(1𝒹))𝒹s−2k(e2iπ(1𝒹))𝒹s−3k⋯(e2iπ(1𝒹))𝒹s−(𝒹−1)k(e2iπ(1𝒹))𝒹s−(𝒹−1)k(e2iπ(1𝒹))ds(e2iπ(1𝒹))𝒹s−k(e2iπ(1𝒹))𝒹s−2k⋯(e2iπ(1𝒹))𝒹s−(𝒹−2)k(e2iπ(1𝒹))𝒹s−(𝒹−2)k(e2iπ(1𝒹))𝒹s−(𝒹−1)k(e2iπ(1𝒹))ds(e2iπ(1𝒹))𝒹s−k⋯(e2iπ(1𝒹))𝒹s−(𝒹−3)k(e2iπ(1𝒹))𝒹s−(𝒹−2)k(e2iπ(1𝒹))𝒹s−(𝒹−2)k(e2iπ(1𝒹))𝒹s−(𝒹−1)k(e2iπ(1𝒹))ds⋯(e2iπ(1𝒹))𝒹s−(𝒹−4)k⋮⋮⋮⋮⋱⋮(e2iπ(1𝒹))𝒹s−k(e2iπ(1𝒹))𝒹s−2k(e2iπ(1𝒹))𝒹s−3k(e2iπ(1𝒹))𝒹s−4k⋯(e2iπ(1𝒹))ds),\begin{array}{r} \mathbb{Z}_{\mathcal{d}\left( \mathcal{me} \right)}^{-} = \begin{pmatrix} \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - 2k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - 3k} & \cdots & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - \left( \mathcal{d} -1 \right)k} \\ \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - \left( \mathcal{d} -1 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{ds} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - 2k} & \cdots & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - \left( \mathcal{d} -2 \right)k} \\ \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - \left( \mathcal{d} -2 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - \left( \mathcal{d} -1 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{ds} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - k} & \cdots & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - \left( \mathcal{d} -3 \right)k} \\ \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - \left( \mathcal{d} -2 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - \left( \mathcal{d} -2 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - \left( \mathcal{d} -1 \right)k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{ds} & \cdots & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - \left( \mathcal{d} -4 \right)k} \\ \vdots & \vdots & \vdots & \vdots & \ddots & \vdots \\ \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - 2k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - 3k} & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}s - 4k} & \cdots & \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{ds} \end{pmatrix}, \end{array}
(1.5.118)

with a de­nom­i­na­tor 𝒹∈ℤ+\mathcal{d} \in\mathbb{Z}^{+}, wind­ing number k={0,−1,−2,−3,…},k = \left\{ 0, - 1, - 2, - 3,\ldots \right\},and a cyclic dis­tance set {0,−1,−2,−3,…,−(𝒹−1)}\left\{ 0, - 1, - 2, - 3,\ldots, - (\mathcal{d} -1) \right\}, away from the iden­ti­ty el­e­ment ϵ=(e2iπ(1𝒹))𝒹k,\epsilon = \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}k},in the clock­wise ori­en­ta­tion. The util­i­ty of these forms for the ℤ𝒹(𝓂ℯ)±\mathbb{Z}_{\mathcal{d}\left( \mathcal{me} \right)}^{\pm} groups is having a con­sis­tent one-column right­ward march of the el­e­ments for each ex­po­nent it­er­a­tion, mean­ing that for any wind­ing number kk, and frac­tion of 2iπ2i\pi as it re­lates to 1𝒹,\frac{1}{\mathcal{d}},the group dy­nam­ics are con­sis­tent with the prim­i­tive root el­e­ment. It should be read­i­ly ap­par­ent any el­e­ment choice will it­er­ate 𝒹=K𝓂ℯ\mathcal{d} =\mathrm{K}_{\mathcal{me}} times before re­turn­ing to the iden­ti­ty, ϵ=ϵ=(e2iπ(1𝒹))𝒹k.\epsilon = \epsilon = \left( e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)} \right)^{\mathcal{d}k}.Using our ini­tial ex­am­ple (e2iπ(514))(14)s+k\left( e^{2i\pi\left( \frac{5}{14} \right)} \right)^{(14)s + k}, as ex­pect­ed, the fol­low­ing pro­gres­sion holds

{(e2iπ(514))0,(e2iπ(114))5,(e2iπ(114))10,(e2iπ(114))15,…,(e2iπ(114))65}.\begin{array}{r} \left\{ \left( e^{2i\pi\left( \frac{5}{14} \right)} \right)^{0},\left( e^{2i\pi\left( \frac{1}{14} \right)} \right)^{5},\left( e^{2i\pi\left( \frac{1}{14} \right)} \right)^{10},\left( e^{2i\pi\left( \frac{1}{14} \right)} \right)^{15},\ldots,\left( e^{2i\pi\left( \frac{1}{14} \right)} \right)^{65} \right\}. \end{array}
(1.5.119)

The cyclic per­mu­ta­tion will have en­tries

e2iπ(kd+sd )=e2iπ(k+sd),\begin{array}{r} e^{2i\pi\left( \frac{kd + s}{d}\ \right)} = e^{2i\pi\left( k + \frac{s}{d} \right)}, \end{array}
(1.5.120)

where kk, is the wind­ing number, ss is the cyclic dis­tance in the coun­ter­clock­wise ori­en­ta­tion from the iden­ti­ty ϵ\epsilon, and e2iπ(1𝒹)e^{2i\pi\left( \frac{1}{\mathcal{d}} \right)}, as the min­i­mal el­e­ment. As dd gets larger, the min­i­mal el­e­ment gets small­er in ar­clength and closer to the origin at e2iπke^{2i\pi k}. Taking the limit of the matrix en­tries in the ℤ𝒹(𝓂ℯ)+\mathbb{Z}_{\mathcal{d}\left( \mathcal{me} \right)}^{+} group

lim𝒹→∞⁡(e2iπ(k+s𝒹))=e2iπk,\begin{array}{r} \lim_{\mathcal{d \rightarrow \infty}}\left( e^{2i\pi\left( k + \frac{s}{\mathcal{d}} \right)} \right) = e^{2i\pi k}, \end{array}
(1.5.121)

brings us to the origin for k∈ℤ,k\in \mathbb{Z},and we arrive at the iden­ti­ty based on the wind­ing number kk.

As a next step, we want to ensure that the func­tion we have been work­ing with can be sim­pli­fied to a single vari­able that rep­re­sents any an­gu­lar ro­ta­tion in ra­di­ans, where the goal is to derive a func­tion f(θ)f(\theta), such that

f(θ)=(e(2iπk𝒹)).\begin{array}{r} f(\theta) = \left( e^{\left( \frac{2i\pi k}{\mathcal{d}} \right)} \right). \end{array}
(1.5.122)

Taking the limit as Δ(2πk𝒹\Delta(\frac{2\pi k}{\mathcal{d}}) ap­proach­es zero shows that we can make the sub­sti­tu­tion for θ=2πk𝒹\theta = \frac{2\pi k}{\mathcal{d}}

limΔ(2πk𝒹)→0⁡(e(2iπk𝒹+Δ(2πk𝒹))−e(2iπk𝒹)Δ(2πk𝒹))=ie(2iπk𝒹),\begin{array}{r} \lim_{\Delta\left( \frac{2\pi k}{\mathcal{d}} \right) \rightarrow 0}\left( \frac{e^{\left( \frac{2i\pi k}{\mathcal{d}} + \Delta\left( \frac{2\pi k}{\mathcal{d}} \right) \right)} - e^{\left( \frac{2i\pi k}{\mathcal{d}} \right)}}{\Delta\left( \frac{2\pi k}{\mathcal{d}} \right)} \right) = ie^{\left( \frac{2i\pi k}{\mathcal{d}} \right)}, \end{array}
(1.5.123)

where this rep­re­sents an in­fin­i­tes­i­mal change in ei(2πk𝒹)e^{i\left( \frac{2\pi k}{\mathcal{d}} \right)}, which is the de­riv­a­tive, and it will take the same form ddθ(eiθ)=ieiθ\frac{d}{d\theta}\left( e^{i\theta} \right) = ie^{i\theta}, since the imag­i­nary co­ef­fi­cient ii on the left side de­fines the or­thog­o­nal tan­gent of eiθe^{i\theta}. So, it can also be said that we have the same or­thog­o­nal­i­ty for iei(2πk𝒹)ie^{i\left( \frac{2\pi k}{\mathcal{d}} \right)}, there­fore, the sub­sti­tu­tion is con­sis­tent for θ=(2πk𝒹)\theta = \left( \frac{2\pi k}{\mathcal{d}} \right), and

f(θ)=(e(2iπk𝒹))=eiθ.\begin{array}{r} f(\theta) = \left( e^{\left( \frac{2i\pi k}{\mathcal{d}} \right)} \right) = e^{i\theta}. \end{array}
(1.5.124)

We start­ed this sec­tion by talk­ing about smooth­ness and con­tin­u­ous func­tions. Sub­se­quent­ly, we have seen that by taking the limit as Δ(2πk𝒹)\Delta\left( \frac{2\pi k}{\mathcal{d}} \right) ap­proach­es zero, we obtain an in­fin­i­tes­i­mal min­i­mal el­e­ment basis con­sis­tent with a C∞C^{\infty} func­tion since f(θ)f(\theta) is smooth and in­fi­nite­ly dif­fer­en­tiable.