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Finite Noncommutative Geometries Related to Fp[x]$\mathbb {F}_{p}[x]$
Algebras and Representation Theory ( IF 0.6 ) Pub Date : 2019-01-31 , DOI: 10.1007/s10468-018-09846-4
M. E. Bassett , S. Majid

It is known that irreducible noncommutative differential structures over \(\mathbb {F}_{p}[x]\) are classified by irreducible monics m. We show that the cohomology \(H_{\text {dR}}^{0}(\mathbb {F}_{p}[x]; m)=\mathbb {F}_{p}[g_{d}]\) if and only if Trace(m)≠ 0, where \(g_{d}=x^{p^{d}}-x\) and d is the degree of m. This implies that there are \({\frac {p-1}{pd}}{\sum }_{k|d, p\nmid k}\mu _{M}(k)p^{\frac {d}{k}}\) such noncommutative differential structures (μM the Möbius function). Motivated by killing this zero’th cohomology, we consider the directed system of finite-dimensional Hopf algebras \(A_{d}=\mathbb {F}_{p}[x]/(g_{d})\) as well as their inherited bicovariant differential calculi Ω(Ad;m). We show that Ad = CdχA1 is a cocycle extension where \(C_{d}=A_{d}^{\psi }\) is the subalgebra of elements fixed under ψ(x) = x + 1. We also have a Frobenius-fixed subalgebra Bd of dimension \(\frac {1}{d} {\sum }_{k | d} \phi (k) p^{\frac {d}{k}}\) (ϕ the Euler totient function), generalising Boolean algebras when p = 2. As special cases, \(A_{1}\cong \mathbb {F}_{p}(\mathbb {Z}/p\mathbb {Z})\), the algebra of functions on the finite group \(\mathbb {Z}/p\mathbb {Z}\), and we show dually that \(\mathbb {F}_{p}\mathbb {Z}/p\mathbb {Z}\cong \mathbb {F}_{p}[L]/(L^{p})\) for a ‘Lie algebra’ generator L with eL group-like, using a truncated exponential. By contrast, A2 over \(\mathbb {F}_{2}\) is a cocycle modification of \(\mathbb {F}_{2}((\mathbb {Z}/2\mathbb {Z})^{2})\) and is a 1-dimensional extension of the Boolean algebra on 3 elements. In both cases we compute the Fourier theory, the invariant metrics and the Levi-Civita connections within bimodule noncommutative geometry.

中文翻译:

与Fp [x] $ \ mathbb {F} _ {p} [x] $相关的有限非交换几何

已知\(\ mathbb {F} _ {p} [x] \)上的不可约非交换微分结构是由不可约一元m进行分类的。我们证明了同调\(H _ {\ text {dR}} ^ {0}(\ mathbb {F} _ {p} [x]; m)= \ mathbb {F} _ {p} [g_ {d} ] \)并且仅当Trace(m)≠0时,其中\(g_ {d} = x ^ {p ^ {d}}-x \)dm的次数。这意味着存在\({\ frac {p-1} {pd}} {\ sum __ {k | d,p \ nmid k} \ mu _ {M}(k)p ^ {\ frac {d } {K}} \) ,例如非对易微分结构(μ中号莫比乌斯功能)。出于消除零同调的动机,我们考虑了有限维霍夫代数的有向系统\(A_ {d} = \ mathbb {F} _ {p} [x] /(g_ {d})\)以及它们继承的双协变微分计算Ω(A d ; m)。我们表明,d = C ^ d⊗ χ1是一个闭链延伸,其中\(C_ {d} = A_ {d} ^ {\ PSI} \)是下固定元件的子代数ψX =)X + 1 。我们还有一个维\(\ frac {1} {d} {\ sum} _ {k | d} \ phi(k)p ^ {\ frac {d} {k}}的Frobenius固定子代数B d \)ϕ Euler totient函数),当p时推广布尔代数=2。作为特殊情况,\(A_ {1} \ cong \ mathbb {F} _ {p}(\ mathbb {Z} / p \ mathbb {Z})\),有限群上函数的代数\ (\ mathbb {Z} / p \ mathbb {Z} \),并且我们双重显示\(\ mathbb {F} _ {p} \ mathbb {Z} / p \ mathbb {Z} \ cong \ mathbb {F } _ {p} [L] /(L ^ {p})\)用于'李代数'发生器大号Ë大号团状,使用截断指数。与此相反,2以上\(\ mathbb {F} _ {2} \)是一个闭链修饰\(\ mathbb {F} _ {2}((\ mathbb {Z} / 2 \ mathbb {Z}) ^ {2})\)是布尔代数在3个元素上的一维扩展。在这两种情况下,我们都将计算傅立叶理论,双模非交换几何中的不变度量和Levi-Civita连接。
更新日期:2019-01-31
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