2019
DOI: 10.1016/j.aim.2019.05.029
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Small cancellation theory over Burnside groups

Abstract: We develop a version of small cancellation theory in the variety of Burnside groups. More precisely, we show that there exists a critical exponent n0 such that for every odd integer n n0, the well-known classical C ′ (1/6)-small cancellation theory, as well as its graphical generalization and its version for free products, produce examples of infinite n-periodic groups. Our result gives a powerful tool for producing (uncountable collections of) examples of nperiodic groups with prescribed properties. It can be… Show more

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Cited by 11 publications
(10 citation statements)
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“…Moreover, if δ>0 (cf. [12, Lemma 3.12], in their notation, κ0=L, N0=N and we take LS:=200) we have: Afalse(G,Xfalse)10·2002N03false(κ0+5δfalse)Aδ. If X is a simplicial tree A(G,X)=0 by its definition [11, Definition 3.40], which yields the claim.…”
Section: Small Cancellation Theorymentioning
confidence: 88%
“…Moreover, if δ>0 (cf. [12, Lemma 3.12], in their notation, κ0=L, N0=N and we take LS:=200) we have: Afalse(G,Xfalse)10·2002N03false(κ0+5δfalse)Aδ. If X is a simplicial tree A(G,X)=0 by its definition [11, Definition 3.40], which yields the claim.…”
Section: Small Cancellation Theorymentioning
confidence: 88%
“…The key tool for proving Theorem 1.2 is the following result, which is based on [Cou16, Theorem 6.15]. Our statement is a slight simplification of the statement given in [CG17] and will be sufficient for our purposes. It says that a torsion-free group acting non-elementarily and acylindrically and a δ-hyperbolic space admits an infinite n-periodic quotient, so long as n is large enough and odd, where "large enough" only depends on δ and the acylindricity constants of the action.…”
Section: At Densities D mentioning
confidence: 99%
“…If g$g$ is hyperbolic, the quasi‐axis of g$g$, denoted by Afalse(gfalse)$A(g)$, is the union of all geodesics joining g$g^{-}$ and g+$g^{+}$. By [11, Lemma 2.26], the quasi‐axis Afalse(gfalse)$A(g)$ is 11δ$\delta$‐quasi‐convex. If g$g^{\prime }$ is another hyperbolic element of G$G$, one defines the fellow travelling constant normalΔfalse(g,gfalse)$\Delta (g,g^{\prime })$ as follows: normalΔ(g,g)=diam()A(g)+100δA(g)+100δdouble-struckN{},\begin{equation*} \Delta (g,g^{\prime })=\mathrm{diam}{\left(A(g)^{+100\delta }\cap A(g^{\prime })^{+100\delta }\right)}\in \mathbb {N}\cup \lbrace \infty \rbrace , \end{equation*}where Afalse(gfalse)+100δ$A(g)^{+100\delta }$ is the 100δ$100\delta$‐neighbourhood of Afalse(gfalse)$A(g)$…”
Section: Test Sequencesmentioning
confidence: 99%
“…\end{equation*}It follows that diam(A(a)+(100δ+λ+μ)oi,n1oj,nA(a)+(100δ+λ+μ))N.\begin{equation*} \mathrm{diam}(A(a)^{+(100\delta +\lambda +\mu )}\cap o_{i,n}^{-1}o_{j,n}A(a)^{+(100\delta +\lambda +\mu )})\geqslant N^{\prime }. \end{equation*}By [11, Lemma 2.13], we have Δ(a,false(oi,n1oj,nfalse)a(oi,n1oj,n)1)diam(A(a)+(100δ+λ+μ)oi,n1oj,nA(a)+(100δ+λ+μ))false(204δ+2λ+2μfalse)Nfalse(204δ+2λ+2μfalse)=N.\begin{align*} &\Delta (a,{(o_{i,n}^{-1}o_{j,n})}a{(o_{i,n}^{-1}o_{j,n})}^{-1})\\ &\quad \geqslant \mathrm{diam}(A(a)^{+(100\delta +\lambda +\mu )}\cap o_{i,n}^{-1}o_{j,n}A(a)^{+(100\delta +\lambda +\mu )}) - (204\delta +2\lambda +2\mu ) \\ &\quad \geqslant N^{\prime } - (204\delta +2\lambda +2\mu ) =N. \end{align*}It follows from this inequality that the element oi...…”
Section: Proof Of Merzlyakov's Theorem 52 In a Particular Casementioning
confidence: 99%