Criteria of Spectral Gap for Markov Operators

Feng-Yu wang

Introduction

Let (E,F,μ)(E,\mathcal{F},\mu) be a probability space. Let PP be a Markov operator on L2(μ)L^{2}(\mu) (i.e. PP is a linear operator on L2(μ)L^{2}(\mu) such that P1=1P1=1 and f0f\geq 0 implies Pf0Pf\geq 0) such that μP=μ\mu P=\mu (i.e. μ\mu is an invariant probability measure of PP). Let P^=12(P+P)\hat{P}=\frac{1}{2}(P+P^{*}) be the additive symmetrization of PP, where PP^{*} is the adjoint operator of PP on L2(μ)L^{2}(\mu). Assuming that 11 is a simple eigenvalue of PP, we aim to investigate the existence of spectral gap of P^\hat{P} (i.e. 11 is an isolated point in σ(P^)\sigma(\hat{P}), the spectrum of P^\hat{P}).

It is well known by the ergodic theorem that 11 is a simple eigenvalue of PP if and only if PP is ergodic, i.e. for fL2(μ)f\in L^{2}(\mu),

Moreover, the ergodicity (i.e. 11 is a simple eigenvalue) is also equivalent to the μ\mu-essential irreducibility (or resolvent-positive-improving property, see ) of PP:

Indeed, if for some fL2(μ)f\in L^{2}(\mu) with μ(f)=0\mu(f)=0 and μ(f2)=1\mu(f^{2})=1 such that Pf=fPf=f, then by the Jensen inequality we have Pf+(Pf)+=f+Pf^{+}\geq(Pf)^{+}=f^{+}. But μ(Pf+)=μ(f+)\mu(Pf^{+})=\mu(f^{+}), we conclude that Pf+=f+Pf^{+}=f^{+}. Then for any ε>0\varepsilon>0 such that μ(f<ε),μ(f>ε)>0\mu(f<-\varepsilon),\mu(f>\varepsilon)>0, we have

so that (1.1) does not hold. On the other hand, if there exists A,BFA,B\in\mathcal{F} with μ(A),μ(B)>0\mu(A),\mu(B)>0 such that μ(1BPn1A)=0\mu(1_{B}P^{n}1_{A})=0 for all n1n\geq 1, then the class

contains the non-trivial function 1A1_{A}. Since the family is bounded in L2(μ)L^{2}(\mu), we may take a sequence {fn}C\{f_{n}\}\subset\mathcal{C} which converges weakly to some fCf\in\mathcal{C} such that μ(f)=supgCμ(g)\mu(f)=\sup_{g\in\mathcal{C}}\mu(g). As f(Pf)f\lor(Pf) is also in C\mathcal{C}, we have μ((Pf)f)=μ(f)=μ(Pf)\mu((Pf)\lor f)=\mu(f)=\mu(Pf). Thus, Pf=fPf=f. Since μ(f)μ(A)>0\mu(f)\geq\mu(A)>0 and μ(1BPf)=0\mu(1_{B}Pf)=0, we conclude that fμ(f)f-\mu(f) is a non-trivial eigenfunction of PP with respect to 11, so that 11 is not a simple eigenvalue of PP.

When PP is symmetric, the spectrum σ(P)\sigma(P) of PP is contained in .. Then PP has a spectral gap if PP is ergodic and σ(P){1}[1,θ]\sigma(P)\subset\{1\}\cup[-1,\theta] for some θ[1,1);\theta\in[-1,1); or equivalently, the Poincaré inequality

holds. When PP is non-symmetric, (1.2) is equivalent to σ(P^H0)[1,θ]\sigma(\hat{P}|_{\mathcal{H}_{0}})\subset[-1,\theta], where H0:={fL2(μ): μ(f)=0}\mathcal{H}_{0}:=\{f\in L^{2}(\mu):\ \mu(f)=0\}. Thus, (1.2) holds for some θ[1,1)\theta\in[-1,1) if and only if P^\hat{P} has a spectral gap.

Recall that PP is called hyperbounded if for some p>2p>2

It was conjectured by Simon and Hϕ\phiegh-Krohn that if PP is symmetric, ergodic and hyperbounded, then it has a spectral gap. Although numerous papers aiming to solve this problem or to construct counterexamples have been published, see e.g. where some weaker notions such as the uniform integrability and a tail norm condition have been used to replace the hyperboundedness, the conjecture has been open for more than 40 years until Miclo found a complete proof in his recent paper .

On the other hand, there are a lot of non-hyperbounded Markov operators having spectral gap. So, in the spirit of , we shall prove a stronger statement by using a tail norm condition to replace the hyperboundedness. The tail norm we will use is the following:

According to the Schwartz inequality, Pτ\|P\|_{\tau} is smaller than the following one used in :

where the las step follows by replacing PfPf with ff, since μ(f2)1\mu(f^{2})\leq 1 implies μ(Pf)2)1\mu(Pf)^{2})\leq 1.

According to , PP is called uniformly integrable if Ptail=0\|P\|_{tail}=0. Thus, the uniformly integrability implies Pτ=0.\|P\|_{\tau}=0. In particular, Pτ=0\|P\|_{\tau}=0 holds for hyperbounded PP. We will then strengthen the above conjecture by replacing the hyperboundedness with Pτ<1,\|P\|_{\tau}<1, which is also necessary for the existence of the spectral gap of P^\hat{P} as shown in our following main result. See Theorem 2.1 below for two more equivalent statements on isoperimetric constants for the existence of spectral gap.

Let PP be an ergodic Markov operator on L2(μ)L^{2}(\mu). Then the following statements are equivalent:

The Poincaré inequality \eqrefP0\eqref{P0} holds for some constant θ[1,1)\theta\in[-1,1), i.e. P^\hat{P} has a spectral gap.

(a) Let PP be symmetric. It is easy to see that if P2P^{2} has a spectral gap then Ptail<1\|P\|_{tail}<1. Indeed, letting σ(P2)[0,ε]\sigma(P^{2})\subset[0,\varepsilon] for some ε(0,1)\varepsilon\in(0,1), for R1R\geq 1 and μ(f2)1\mu(f^{2})\leq 1 we have

where f^:=fμ(f).\hat{f}:=f-\mu(f). On the other hand, if Ptail<1\|P\|_{tail}<1 then by Theorem 1.1 P2P^{2} has a spectral gap provided it is ergodic (i.e. 11 is a simple eigenvalue). So, if PP has a spectral gap but 1σess(P)-1\in\sigma_{ess}(P) is not an eigenvalue, then Ptail=1\|P\|_{tail}=1. From this we would believe that in general the existence of spectral gap for PP does not imply Ptail<1.\|P\|_{tail}<1.

The resolvent-uniform-positive-improving condition is weaker than the uniform-positive-improving condition used in , and the condition (E) introduced in . Recall that PP is called uniform-positive-improving if

In the symmetric setting this result is now improved by Theorem 1.1 since the resolvent-uniform-positive-improving property is strictly stronger than the ergodicity, which is equivalent to the resolvent-positivity-improving property (1.1). Examples to ensure this “strictly stronger” property can be constructed from the corresponding ones for Markov semigroups explained in item (c) below. More precisely, it is known that the resolvent-uniform-positive-improving property of PP is equivalent to the validity of the weak Poincaré inequality (see [22, Theorem 2.5]):

for some α:(0,)(0,).\alpha:(0,\infty)\to(0,\infty). Taking P=P1P=P_{1} for a symmetric Markov semigroup PtP_{t} on L2(μ)L^{2}(\mu) and noting that

where (L,D(L))(L,\mathcal{D}(L)) and E\mathcal{E} are the associated generator and Dirichlet form, we see that an example such that E\mathcal{E} is irreducible but the weak Poincaré inequality (1.3) below is not available implies that PP is ergodic but does not possess the resolvent-uniform-positive-improving property.

(c) We would like to mention links of the uniform-positive-improving property of a symmetric Markov semigroup PtP_{t} and the weak Poincaré inequality of the associated Dirichlet form (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})). It is well known that PtP_{t} (for some/all t>0t>0) is ergodic if and only if the Dirichlet form is irreducible, i.e. E(f,f)=0\mathcal{E}(f,f)=0 implies ff is constant. Next, according to (see also ), the uniform-positive-improving property of the semigroup (i.e. PtP_{t} is uniform-positive-improving for some, equivalently all, t>0,t>0, see ) implies the weak spectral gap property, which is equivalent to the validity of the weak Poincaré inequality (see ): for some α:(0,)(0,)\alpha:(0,\infty)\to(0,\infty)

Indeed, as explained in (b) that the resolvent-uniform-positive-improving property of PtP_{t} for some t>0t>0 also implies the existence of the weak Poincaré inequality. Moreover, it is shown in [13, §7] that there are conservative irreducible Dirichlet forms which do not satisfy the weak Poincaré inequality. Therefore, the resolvent-uniform-positive-improving property is strictly stronger than the ergodicity.

As applications of Theorem 1.1, we consider functional inequalities conservative symmetric Dirichlet forms. A simple consequence of the equivalence of (1)(1) and (3) is that the defective Poincaré inequality implies the tight one.

Let (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})) be a conservative, irreducible, symmetric Dirichlet form on L2(μ)L^{2}(\mu). Then the Poincaré inequality

holds for some constant C>0C>0 if and only if the defective Poincaré inequality

holds for some constants C1,C2>0.C_{1},C_{2}>0.

This result improves [13, Proposition 1.3] where the weak Poincaré inequality (1.3) is used to replace the irreducibility of the Dirichlet form. Basing on Corollary 1.2, we are able to prove the equivalence of the defective version and the tight version for more general functional inequalities. Here, we consider a family of functional inequalities introduced in , which interpolate the Poincaré inequality (1.4) and the Gross log-Sobolev inequality

for some constant C>0.C>0. Let ϕC()\phi\in C() such that ϕ>0\phi>0 on [1,2)[1,2) and ϕ(2)=0\phi(2)=0 with

When ϕ(p)=2p\phi(p)=2-p the inequality (1.7) is equivalent to the log-Sobolev inequality, and when ϕ\phi reduces to a positive constant it becomes the Poincaré inequality. See for detailed discussions on properties and applications of the inequality (1.7).

Let (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})) be a conservative, irreducible, symmetric Dirichlet form on L2(μ)L^{2}(\mu). Then (\refPH)(\ref{PH}) holds for some constant C>0C>0 if and only if (\refDPH)(\ref{DPH}) holds for some constants C1,C2>0.C_{1},C_{2}>0.

The remainder of the paper is organized as follows. In Section 2, by using an approximation argument introduced in , we extend a known Cheeger type inequality for high order eigenvalues of finite-state Markov chains to the abstract setting, then use this estimate to characterize the existence of spectral gap with high-order isoperimetric constants. This characterization is then used in Section 3 to prove Theorem 1.1. Proofs of Corollaries 1.2 and 1.3 are also addressed in Section 3. Finally, in Section 4 we extend Theorem 1.1 and Corollary 1.2 to the sub-Markov setting.

Essential spectrum and isoperimetric constants

Let PP be a symmetric Markov operator on L2(μ)L^{2}(\mu). We aim to characterize the essential spectrum of PP using high order isoperimetric constants investigated in .

We define the nn-th isoperimetric constant by

Obviously, κ1=0\kappa_{1}=0 and if L2(μ)L^{2}(\mu) is infinite-dimensional then DnD_{n}\neq\emptyset for all n2.n\geq 2. It is also easy to see that κn\kappa_{n} is non-decreasing in nn.

We will only consider the case that L2(μ)L^{2}(\mu) is infinite-dimensional, since otherwise the spectrum of PP is finite so that the existence of spectral gap becomes trivial. By the Cheeger inequality we know that PP has a spectral gap if and only if κ2>0\kappa_{2}>0, see e.g. by noting that in (1.2) we have

for the symmetric measure JJ on E×EE\times E determined by J(A×B):=μ(1AP1B),A,BFJ(A\times B):=\mu(1_{A}P1_{B}),A,B\in\mathcal{F}.

Consider λess(P):=supσess(P),\lambda_{ess}(P):=\sup\sigma_{ess}(P), where σess(P)\sigma_{ess}(P) is the essential spectrum of PP. Obviously, PP has a spectral gap if and only if it is ergodic and λess(P)<1.\lambda_{ess}(P)<1.

Let PP be a symmetric Markov operator on L2(μ)L^{2}(\mu). Then λess(P)<1\lambda_{ess}(P)<1 if and only if supn1κn>0.\sup_{n\geq 1}\kappa_{n}>0. Consequently, when PP is ergodic then the existence of spectral gap of PP is equivalent to each of the following two statements:

\ \kappa_{2}\big{(}=\inf_{n\geq 2}\kappa_{n}\big{)}>0.

\lim_{n\to\infty}\kappa_{n}\big{(}=\sup_{n\geq 2}\kappa_{n}\big{)}>0.

As mentioned at the end of Introduction, to prove this result we will extend a known estimate on the hight order eigenvalues using κn\kappa_{n} for finite-state Markov chains. So, below we first consider Markov operators on a finite set.

As shown in [10, Theorem 2], we may take c(n)=c0n4c(n)=\frac{c_{0}}{n^{4}} for a universal constant c0>0.c_{0}>0.

Below we aim to extend this estimate to our abstract setting by using an approximation argument introduced in . For any n1n\geq 1, let

To see that this quantity can be regarded as the nn-th eigenvalue of L:=1PL:=1-P, let λess(L)=infσess(L)\lambda_{ess}(L)=\inf\sigma_{ess}(L) be the bottom of the essential spectrum of LL. Then, see e.g. [11, Theorem XIII.2], λn\lambda_{n} is the nn-th eigenvalue of LL if λn<λess(L),\lambda_{n}<\lambda_{ess}(L), and λn=λess(L)\lambda_{n}=\lambda_{ess}(L) otherwise. The following result was stated as Proposition 5 in , we include here a proof for completeness.

Let c(n)c(n) be in (\refB1)(\ref{B1}) for n1n\geq 1. Then κnλnc(n)2κn2.\kappa_{n}\geq\lambda_{n}\geq c(n)^{2}\kappa_{n}^{2}.

Let L=1PL=1-P. Since λ1=κ1=0\lambda_{1}=\kappa_{1}=0, we only prove for n2.n\geq 2.

(a) Upper bound estimate of λn\lambda_{n}. For any f1,,fn1L2(μ)f_{1},\cdots,f_{n-1}\in L^{2}(\mu) and any (A1,,An)Dn(A_{1},\cdots,A_{n})\in D_{n}, there exists a function f:=i=1nai1Aif:=\sum_{i=1}^{n}a_{i}1_{A_{i}} such that i=1nai2=1\sum_{i=1}^{n}a_{i}^{2}=1 and μ(ffi)=0,1in.\mu(ff_{i})=0,1\leq i\leq n. Let

Therefore, by the definition of λn\lambda_{n} and κn\kappa_{n}, we have λnκn\lambda_{n}\leq\kappa_{n}.

(b) Lower bound estimate of λn.\lambda_{n}. Assume that λn<c(n)2κn2\lambda_{n}<c(n)^{2}\kappa_{n}^{2}. Then there exist f1,,fnL2(μ)f_{1},\cdots,f_{n}\in L^{2}(\mu) such that

where δn:=c(n)2κn2λn>0.\delta_{n}:=c(n)^{2}\kappa_{n}^{2}-\lambda_{n}>0. Indeed, for any ε>0\varepsilon>0 we may find an orthonormal family {f1,,fn}L2(μ)\{f_{1},\cdots,f_{n}\}\subset L^{2}(\mu) such that μ(Lfiλifi2)ε,1in.\mu(|Lf_{i}-\lambda_{i}f_{i}|^{2})\leq\varepsilon,1\leq i\leq n. Since max1inλi=λn=c(n)2κn2δn\max_{1\leq i\leq n}\lambda_{i}=\lambda_{n}=c(n)^{2}\kappa_{n}^{2}-\delta_{n} and μ(fifj)=δij\mu(f_{i}f_{j})=\delta_{ij}, (2.3) holds for small enough ε>0.\varepsilon>0.

Let F=σ(f1,,fn).\mathcal{F}_{\infty}=\sigma(f_{1},\cdots,f_{n}). Since F\mathcal{F}_{\infty} is separable, we may find an increasing sequence of σ\sigma-fields {FN}N1\{\mathcal{F}_{N}\}_{N\geq 1} such that

Then PNP_{N} is a symmetric Markov operator on L2(μN).L^{2}(\mu_{N}).

To identify PNP_{N} with a Markov operator on a finite set, let

holds for DN,n:={(A1,,An)Dn: AkFN,1kn}.D_{N,n}:=\{(A_{1},\cdots,A_{n})\in D_{n}:\ A_{k}\in\mathcal{F}_{N},1\leq k\leq n\}. Since for AkFNA_{k}\in\mathcal{F}_{N} we have μN(Ak)=μ(Ak)\mu_{N}(A_{k})=\mu(A_{k}) and

which contradicts (2.4) for large NN such that εN<δn16n\varepsilon_{N}<\frac{\delta_{n}}{16n}. ∎

If λess(P)<1\lambda_{ess}(P)<1, then σ(L)[0,1λess(P))\sigma(L)\cap[0,1-\lambda_{ess}(P)) is discrete and each eigenvalue in this set is of finite multiplicity. So, in this case λn>0\lambda_{n}>0 for nn lager than the multiplicity of the first eigenvalue λ1=0,\lambda_{1}=0, and hence by Lemma 2.2, κn>0\kappa_{n}>0 for large nn. On the other hand, we aim to prove that if λess(P)=1\lambda_{ess}(P)=1 then κn=0\kappa_{n}=0 for all n1.n\geq 1. Since λess(P)=1\lambda_{ess}(P)=1, i.e. 0σess(L)0\in\sigma_{ess}(L), we have λn=0\lambda_{n}=0 for all nn. Combining this with Lemma 2.2, we prove κn=0\kappa_{n}=0 for all n1n\geq 1. Thus, the proof of the first assertion is finished.

Now, let PP be ergodic. Since (6) follows from (5), it suffices to prove that (1) (i.e. the existence of spectral gap of PP) implies (5) while (6) implies (1). If (1) holds then λ2>0\lambda_{2}>0, so that by Lemma 2.2 we have κ2>0\kappa_{2}>0, i.e. (5) holds. On the other hand, if (6) holds, then by the first assertion of this theorem we have λess(P)<1\lambda_{ess}(P)<1 such that 11 is isolate in σ(P)\sigma(P). Since 11 is a simple eigenvalue of PP, this implies that PP has a spectral gap, i.e. (1) holds. ∎

Proofs of Theorem 1.1 and corollaries

By [3, Theorem 4.1(d)] with π=P^\pi=\hat{P} and rsp(π)=1r_{sp}(\pi)=1, (1) implies (4). Next, it is obvious that (2) implies (3). Moreover, since P^mτP^mtail\|\hat{P}^{m}\|_{\tau}\leq\|\hat{P}^{m}\|_{tail} and by the Jensen inequality the later is decreasing in mm, we see that (4) implies (3) for P^\hat{P} in place of PP. Therefore, it remains to prove that (1) implies (2), and (3) implies (1). Below we prove these two implications respectively.

(1) implies (2). Let θ(0,1)\theta\in(0,1) such that (1.2) holds. For any f0f\geq 0 with μ(f2)1\mu(f^{2})\leq 1, we have

Replacing ff by (fR)+(f-\sqrt{R})^{+} for R>1R>1, and noting that

Since by the Jensen inequality (PfR)+P(fR)+,(Pf-R)^{+}\leq P(f-R)^{+}, combining this with (3.1) we arrive at

(3) implies (1). Let P2m1τ<1\|P^{2m-1}\|_{\tau}<1 for some m1m\geq 1. It suffices to prove for the case that L2(μ)L^{2}(\mu) is infinite-dimensional since in the finite dimensional case the existence of spectral gap is trivial. We first assume that PP is symmetric. In this case, the existence of spectral gap for PP is equivalent to that for P2m1P^{2m-1}. Since P2m1τ<1\|P^{2m-1}\|_{\tau}<1, there exists δ(0,1)\delta\in(0,1) and R>0R>0 such that

On the other hand, if P2m1P^{2m-1} does not have spectral gap, by Theorem 2.1, for any ε(0,1)\varepsilon\in(0,1) and n2n\geq 2, there exists (A1,An)Dn(A_{1},\cdots A_{n})\in D_{n} such that

Letting Bk=Ak{P2m11Ak1ε}B_{k}=A_{k}\cap\{P^{2m-1}1_{A_{k}}\geq 1-\sqrt{\varepsilon}\}, this implies

Since A1,,AnA_{1},\cdots,A_{n} are disjoint with positive μ\mu-mass and μ\mu is a probability measure, there exists 1kn1\leq k\leq n such that μ(Ak)(0,1n).\mu(A_{k})\in(0,\frac{1}{n}). Take

Combining this with (3.2), (3.3) and μ(Ak)(0,1n)\mu(A_{k})\in(0,\frac{1}{n}), we arrive at

Since ε(0,1)\varepsilon\in(0,1) and n2n\geq 2 are arbitrary, by letting ε0\varepsilon\to 0 and nn\to\infty we obtain δ1\delta\geq 1 which contradicts δ(0,1)\delta\in(0,1).

Next, for non-symmetric PP, we consider the symmetrizing operator P^\hat{P}. Obviously, PP satisfies (1.1) implies that P^\hat{P} satisfies (1.1), i.e. P^\hat{P} is ergodic. By (3), there exists m1m\geq 1 such that ε:=P2m1τ<1\varepsilon:=\|P^{2m-1}\|_{\tau}<1. Moreover, as proved above if P^2m1τ<1\|{\hat{P}}^{2m-1}\|_{\tau}<1 then P^\hat{P} has a spectral gap. Therefore, it suffices to show that P^2m1τ<1.\|{\hat{P}}^{2m-1}\|_{\tau}<1. Noting that for any R>0R>0 and f0f\geq 0 with μ(f2)1\mu(f^{2})\leq 1,

we obtain P^2m1τ212mε+1212m<1\|{\hat{P}}^{2m-1}\|_{\tau}\leq 2^{1-2m}\varepsilon+1-2^{1-2m}<1, since ε<1.\varepsilon<1.

It suffices to prove (1.4) from (1.5). Let PtP_{t} be the associated Markov semigroup. Then the irreducibility of the Dirichlet form implies that of PtP_{t} for t>0t>0. Next, by [16, Theorem 3.3] with ϕ1\phi\equiv 1, (1.5) implies that Ptτet/C1<1\|P_{t}\|_{\tau}\leq\text{\rm{e}}^{-t/C_{1}}<1 for t>0t>0. Then due to Theorem 1.1 we conclude that PtP_{t} has a spectral gap, equivalently, the Poincaré inequality (1.4) holds for some constant C>0.C>0.

By [19, Proposition 2.1], for any fL2(μ)f\in L^{2}(\mu) and f^:=fμ(f)\hat{f}:=f-\mu(f), we have

Next, since ϕ(2)=0\phi(2)=0, from the proof of [19, Theorem 1.1(2)] we see that the FF-Sobolev inequality (1.7) in holds for some nonnegative function FF with F(r)F(r)\uparrow\infty as rr\uparrow\infty. According to (see also ), this inequality is equivalent to the super Poincaré inequality

for some function β:(0,)(0,)\beta:(0,\infty)\to(0,\infty). In particular, the defective Poincaré inequality holds. Thus, by Corollary 1.2, we have the Poincaré inequality

Extensions to the sub-Markov setting

In this section we let (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})) be a non-conservative Dirichlet form on L2(μ)L^{2}(\mu), for which either 1D(E)1\notin\mathcal{D}(\mathcal{E}) or 1D(E)1\in\mathcal{D}(\mathcal{E}) but E(1,1)>0.\mathcal{E}(1,1)>0. In this case the Dirichlet form is irreducible if and only if for any fD(E)f\in\mathcal{D}(\mathcal{E}) with E(f,f)=0\mathcal{E}(f,f)=0 one has f=0.f=0. Let Pp\|P\|_{p} be the norm in Lp(μ)L^{p}(\mu) for p1.p\geq 1. Below is an extension of Corollary 1.2 to the present situation.

Let (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})) be a non-conservative irreducible Dirichlet form on L2(μ)L^{2}(\mu). Then the Poincaré inequality

holds for some C>0C>0 if and only if the defective Poincaré inequality

Assume that (4.2) holds. We aim to prove (4.1) for some constant C>0C>0. According to [17, Proposition 3.2] we need only to prove the weak Poincaré inequality

for some function α:(0,)(0,).\alpha:(0,\infty)\to(0,\infty). This is ensured by Lemma 4.3 below. ∎

Before introducing Lemma 4.3, we present an application of Theorem 4.1 to sub-Markov operators.

Let PP be a sub-Markov operator on L2(μ)L^{2}(\mu); i.e. PP is a contraction linear operator on L2(μ)L^{2}(\mu) with P11P1\leq 1 such that f0f\geq 0 implies Pf0.Pf\geq 0. Let PP^{*} be the adjoint operator of PP. Assume that Ker(1PP)={0}{\rm Ker}(1-P^{*}P)=\{0\}. Then

It suffices to prove P2<1\|P\|_{2}<1 from Ptail<1\|P\|_{tail}<1. To apply Theorem 4.1, let

Then (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})) is a symmetric Dirichlet form. Since Ker(1PP)=0\,(1-P^{*}P)=0 and noting that the contraction of PP^{*} in L2(μ)L^{2}(\mu) implies

this Dirichlet form is non-conservative and irreducible. By Ptail<1\|P\|_{tail}<1, there exist R>0R>0 and ε(0,1)\varepsilon\in(0,1) such that

Thus, (4.2) holds for C1=21ε,C2=R2(1ε)2.C_{1}=\frac{2}{1-\varepsilon},C_{2}=\frac{R^{2}}{(1-\varepsilon)^{2}}. By Theorem 4.1, there exists C>0C>0 such that

This implies that P22C1C<1.\|P\|_{2}^{2}\leq\frac{C-1}{C}<1.

Correspondingly to Remark 1.1(a) in the ergodic setting, we would believe that in the present situation Pτ<1\|P\|_{\tau}<1 is not enough to imply P2<1\|P\|_{2}<1. But it seems hard to give a proof or a counterexample.

A non-conservative Dirichlet form (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})) on L2(μ)L^{2}(\mu) is irreducible if and only if there exists α:(0,)(0,)\alpha:(0,\infty)\to(0,\infty) such that

Consequently, for any symmetric ((sub-)) Markov semigroup PtP_{t} on L2(μ)L^{2}(\mu), limtPtf2=0\lim_{t\to\infty}\|P_{t}f\|_{2}=0 for any fL2(μ)f\in L^{2}(\mu) if and only if

(a) Let PtP_{t} be the associated semigroup of (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})). Then (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})) is irreducible if and only if μ((Ptf)2)0\mu((P_{t}f)^{2})\to 0 as tt\to\infty for any fL2(μ).f\in L^{2}(\mu). Indeed, the sufficiency is obvious since E(f,f)=0\mathcal{E}(f,f)=0 implies

so that μ(Ptf2)=μ(f2)\mu(|P_{t}f|^{2})=\mu(f^{2}) for all t0t\geq 0, while the necessity holds since the irreducibility of the Dirichlet form implies that

where {Eλ}λ0\{E_{\lambda}\}_{\lambda\leq 0} is the spectral family of the generator such that dEλ(f)2\text{\rm{d}}\|E_{\lambda}(f)\|^{2} is a finite measure on (,0)(-\infty,0) for fL2(μ)f\in L^{2}(\mu) (by the irreducibility {0}\{0\} is a null-set of the measure).

On the other hand, by [13, Theorem 2.1] with Φ(f)=f2\Phi(f)=\|f\|_{\infty}^{2}, (4.3) holds for some α\alpha if and only if (4.4) holds. So, the second assertion follows from the first one.

(c) Now, let (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})) be irreducible. We claim that (4.3) holds for some function α:(0,)(0,).\alpha:(0,\infty)\to(0,\infty). Otherwise, there exist some r>0r>0 and a sequence {fn}D(E)\{f_{n}\}\subset\mathcal{D}(\mathcal{E}) such that

Since E(fn,fn)E(fn,fn)\mathcal{E}(|f_{n}|,|f_{n}|)\leq\mathcal{E}(f_{n},f_{n}), we may and do assume that fn0f_{n}\geq 0 for all n1.n\geq 1. Since {fn}\{f_{n}\} is bounded in L2(μ)L^{2}(\mu), there exist fL2(μ)f\in L^{2}(\mu) and a subsequence {fnk}\{f_{n_{k}}\} such that fnkf_{n_{k}} converges weakly to ff in L2(μ)L^{2}(\mu).

Let PtP_{t} be the (sub-) Markov semigroup and (L,D(L))(L,\mathcal{D}(L)) the generator associated to (E,D(E))(\mathcal{E},\mathcal{D}(\mathcal{E})). Then PtfD(L)P_{t}f\in\mathcal{D}(L) for any t>0.t>0. By the symmetry of PtP_{t} and the weak convergence of {fnk}\{f_{n_{k}}\} to ff in L2(μ)L^{2}(\mu), we have

Moreover, due to (4.5) and the symmetry of E\mathcal{E},

Combining this with (4.6) we conclude that E(Ptf,Ptf)=0\mathcal{E}(P_{t}f,P_{t}f)=0 for all t>0t>0. Thus, by the irreducibility, Ptf=0P_{t}f=0 holds for all t>0.t>0. This implies f=0f=0 by the strong continuity of PtP_{t} in L2(μ)L^{2}(\mu). Since (4.5) implies fnr1/2,f_{n}\leq r^{-1/2}, by the weak convergence of {fnk}\{f_{n_{k}}\} to f=0f=0 in L2(μ)L^{2}(\mu) and 1L2(μ)1\in L^{2}(\mu), we obtain

This contradicts the assumption that μ(fn2)=1\mu(f_{n}^{2})=1 for all n1.n\geq 1. Therefore, (4.3) holds for some function α:(0,)(0,).\alpha:(0,\infty)\to(0,\infty).

I would like to thank professor Laurent Miclo for sending me his exciting paper and useful discussions, as well as the referee, Professor L. Gross and Dr. Shaoqin Zhang for helpful comments and corrections.

References