The Dynamics of Semigroups of TranscendentalMeromorphic Functions
Semigroup-controlled asymptotic dimension

a rX iv:mat h /68736v1[mat h.MG ]29Aug26SEMIGROUP-CONTROLLED ASYMPTOTIC DIMENSION J.HIGES Abstract.We introduce the idea of semigroup-controlled asymptotic dimension.This notion generalizes the asymptotic dimension and the asymptotic Assouad-Nagata dimension in the large scale.There are also semigroup controlled dimensions for the small scale and the global scale.Many basic properties of the asymptotic dimension theory are satisfied by a semigroup-controlled asymptotic dimension.We study how these new dimensions could help in the understanding of coarse embeddings and uniform embeddings.In particular we have introduced uncountable many invariants under quasi-isometries and uncountable many bi-Lipschitz invariants.Hurewicz type theorems are generalized and some applications to geometric group theory are shown.Contents 1.Introduction and preliminaries 12.Control semigroups 33.Semigroup-controlled dimensions:basic properties rge scale and small scale dimensions 75.Non equivalent semigroup-controlled dimensions 106.Maps between metric spaces and dimension 147.Hurewicz type theorems 17References 191.Introduction and preliminaries The aysmptotic dimension was introduced by Gromov in [8]as one im-portant coarse invariant in the study of geometric group theory.The idea behind its definition is to analyze a metric space as a large scale object.2J.HIGESAn analogous concept to the asymptotic dimension but for small scale ob-jects would be the uniform dimension introduced by Isbell in[10].These two dimensions suggest the idea of seeing a metric space as a global object and then we would get a global definition of dimension.In[4](see also[12]) it was given such definition and it was analyzed some properties of zero dimensional spaces.The following notions associated to a cover U={U s}s∈S of a metric space (X,d)are standard concepts in the theory of metric spaces.They are used in many equivalent definitions of asymptotic dimension.Let U={U s}s∈S be a cover of a metric space(X,d X),not necessarily open.Associated to this cover there is a family a natural family of functions {f s}s∈S with f s:X→R+defined by:f s(x):=d X(x,X\U s).With such functions we can define:-Local Lebesgue number L x(U)of U at x∈X:L x(U):=sup{f s(x)|S∈S}.-Global Lebesgue number L(U):=inf{L x(U)|x∈X}.-Local s-multiplicity s−m U(x)of U at x∈X is defined as the numberof elements of U that intersect B(x,s).-Global s-multiplicity s−m(U):=sup{s−m U(x)|x∈X}.If s=0then the0-multiplicity will be called multiplicity of U and it will benoted by m(U).Given a family of subsets U of a metric space(X,d X)it is said that U is C-bounded with C>0if diam(U)≤C for every U∈U.If U is C-bounded for some C>0it is said that U is uniformly bounded and if d X(U,V)>s for every U,V∈U,it is said also that U is s-disjoint with s>0.A definition of asymptotic dimension could be the following:Definition 1.1.We will say that a metric space(X,d)has asymptotic dimension at most n(notation:asdimX≤n)if there is an s0such that for every s≥s0there exists an uniformly cover(colored cover)U= n+1i=1U i so that each U i is s-disjoint.From this definition we can deduce that there exist a function f:R+→R+with lim x→∞f(x)=∞such that each s-disjoint n+1colored cover is f(s)-bounded.If we restricted the range of functions f allowed to the linear ones(or asymptotically linear ones)we would get the notion of asymptotic Assouad-Nagata dimension,also called linear controlled asymptotic dimen-sion or asymptotic dimension with Higson property.Many results have appeared recently associated to this dimension,see[3],[4],[6],[7]and[9], for example.Here is the definition:Definition 1.2.We will say that a metric space(X,d)has asymptotic Assouad-Nagata dimension at most n(notation:asdimX≤n)if there is a s0>0and a C>0such that for every s≥s0there exist a Cs-bounded cover(colored cover)U= n+1i=1U i so that each U i is s-disjoint.SEMIGROUP-CONTROLLED ASYMPTOTIC DIMENSION3 If we just change the condition of s≥s0by s≤s0we will get the notion of capacity dimension introduced by Buyalo in[5].The asymptotic Assouad-Nagata dimension and the capacity dimension are just the large scale and the small scale versions of the Assouad-Nagata dimension introduced by Assouad in[1].The Assouad-Nagata dimension is a bi-Lipschitz invariant. Lang and Schlichenmaier proved in[11]that the Assouad-Nagata dimension is in fact a quasisymmetry invariant.Many other interesting properties of the Assouad-Nagata dimension appeared in that work.The relations among the capacity dimension,the asymptotic Assouad-Nagata dimension and the Assouad-Nagata dimension were showed in[3]. In this paper we generalize all these notions using the concept of semigroup-controlled asymptotic dimension,semigroup-controlled small scale dimen-sion and semigroup-controlled global dimension.The idea is to modify the range of functions allowed to control the size of the colored covers in def-inition1.2.These functions will have a semigroup structure.In section2 we will study some basic properties of this kind of semigroups.In the next section we will define the notion of semigroup-controlled dimension and we will show that many basic properties of asymptotic dimension(see[2])are satisfied for these new dimensions.Section4is dedicated to relate the large scale,small scale and global dimensions following the same ideas of[3].In section5we will prove that this generalization is not trivial i.e.we have introduced uncountable many different dimensions.The last two sections are dedicated to important topics.In section6we will study the types of maps between metric spaces for which these new dimensions are invariant. In particular we will prove that all these dimensions are quasi-isometric in-variants in the large scale theory or bi-Lipschitz invariants in the global case. Last section generalizes the results of[9]about the Hurewicz type theorem. Some applications to geometric group theory are obtained as corollaries.2.Control semigroupsIn this work we will consider properties P(s)depending on positive real numbers s∈R+.We will say that P(s)is satisfied in a neighborhood of∞(respectively in a neighborhood of0)if there is a s0such that P(s)is true for every s≥s0(resp.s≤s0).Properties that are satisfied in a neighborhood of∞will be called large scale properties or asymptotic properties,properties that are satisfied in a neighborhood of0will be called small scale properties.If a property P(s) is satisfied in a neighborhood of∞and in a neighborhood of0we will say that P(s)is a global property.In this work we will usually give proofs and statements for the large scale case.The small scale case and the global case can be usually done using a dual reasoning and in many cases they will be left to the reader.Next definition describes the type of functions that are going to control the dimension.4J.HIGESDefinition2.1.Let f:R+→R+be an increasing continuous functiona.We will say that it is a large scale(or asymptotic)dim-control func-tion if f(x)≥x in a neighborhood of∞and f(∞)=∞i.e.lim x→∞f(x)=∞.b.If we require that f(x)≥x in a neighborhood of0and f(0)=0wewill say that f is a small scale dim-control function.c.If a function is a small scale dim-control function and a large scaledim-control function then we will say that it is a global dim-controlfunction.If a large scale dim-control function f is equal to some linear function in a neighborhood of∞we will say that it is a large scale(or asymptotically)lin-ear dim-control function.Analogously it can be defined the notion of small scale linear dim-control function and global linear dim-control function. Now we define the notion of large scale(or asymptotic)control semigroup. This notion is the main concept of this paper.Definition2.2.Let S be a set of asymptotic dim-control functions.We will say that S is a large scale(or asymptotic)control semigroup if the following properties are satisfied:(1)Every asymptotically linear dim-control function is in S(linear con-dition).(2)For every pair of functions g1,g2∈S we have g1◦g2∈S(semigroupcondition).We define the notion of small scale and global control semigroup for a set of small scale(resp.global)dim-control function analogously.We will note it byξ(resp.¯S)Remark2.3.In this work we will refer to asymptotic control semigroup just as control semigroups unless it were necessary to remark the large scale condition.Here are the main examples of control semigroups.Example2.4.The set of all asymptotic dim-control functions is a control semigroup.It will be called the uniform control semigroup and we will note it by U(u and¯U for the small scale and the global case respectively)The set of all asymptotically linear dim-control functions is a control semigroup.It will be called the Nagata(or the linear)control semigroup and it will be noted by N(n and¯N for the small scale and large scale case respectively).Remark2.5.Let K be a set of asymptotic dim-control functions.From the theory of semigroups we know that such set generates a control semigroup L(K)i.e.the intersection of all control semigroups S so that K⊂S. It will be called the control semigroup generated by K.Note that N= L({x}).We have also obtained many examples of control semigroups using this procedure.SEMIGROUP-CONTROLLED ASYMPTOTIC DIMENSION5 In the set of all control semigroups we can define a partial order.Definition2.6.Given two control semigroups S1and S2,we will say that S2isfiner than S1(notation:S1 S2)if for every asymptotic dim-control function f∈S2there is a dim-control function g∈S1such that f≤g in a neighborhood of∞.If S1 S2and S2 S1we will say that both control semigroups are equivalent and we will note it by S2≈S1.The following result is easy to check and it is left as an exercise. Proposition2.7.Let S be a control semigroup then:(1)U S N.(2)L(K∪S) S with K is any set of asymptotic dim-control functions. Remark 2.8.As a consequence of the second statement in the previous proposition we obtain that L(S2∪S1) S2and L(S2∪S1) S1for every pair of control semigroups.Then the set of all control semigroups with the relation is a directed set.Now we show an example of two different equivalent control semigroups. In the following section we could see how this example allows us to give another definition of asymptotic Assouad-Nagata dimension:Example2.9.Let{C i}n i=1be afinite set of constants with C i≥1.For eachfinite set of those constants we can define an asymptotic dim-controlfunction f{Ci}as a continuous piecewise linear function built with linearfunctions of slope C i such that f{Ci}(∞)=∞.It can be easily checkedthat the set of all functions of the form f{Ci}is a control semigroup.Wewill note it by PL.Clearly we have PL N.Take a f{Ci}∈PL.LetC be the maximum of the C i then the linear function f(x)=Cx satisfiesf(x)≥f{Ci}(x)for all x in a neighborhood of∞.So we have proved thatN L and both semigroups are equivalent.The following is an easy consequence of the semigroup theory and it will be used later.Proposition2.10.Let K be a set of dim-control functions.If g is a dim-control function g of L(K)then there exist afinite sequence of dim-control functions{f i}n i=1such that:g=f1◦f2◦...◦f nwhere each f i belongs to N∪K.3.Semigroup-controlled dimensions:basic properties Now,using the notion of control semigroup we can give the definition of semigroup-controlled asymptotic dimension.It generalizes the notions of Assouad-Nagata asymptotic dimension and asymptotic dimension.Definition3.1.Let S be a control semigroup.We will say that a metric space(X,d)has S-controlled asymptotic dimension at most n(notation:6J.HIGESasdim S X≤n)if there is an f∈S such that for every s in some neighbor-hood of∞there exist a cover(colored cover)U= n+1i=1U i so that each U i is s-disjoint and f(s)-bounded.A metric space is said to have S-controlled asymptotic dimension n if it has S-controlled asymptotic dimension at most n and for every k<n it does not happen that asdim S X≤k.Remark3.2. a.The function f∈S for which asdim S X≤n will be called(n,S)-dimensional control function of X.Such notion willbecome very important in the last section.b.The small scaleξ-controlled dimension will be noted by smdimξX.c.Special remark is needed for the definition of global dimension.Thestrictly analogous definition to the Assouad-Nagata dimension wouldbe the following:(X,d)has¯S-controlled global dimension at most n(notation:dim¯S X≤n)if there is a f∈¯S such that for every s there is a cover(colored cover)U= n+1i=1U i so that each U i is s-disjoint andf(s)-bounded.We will say that two control semigroups S2and S1are dim-equivalent(notation:asdim S2≡asdim S1)if for every metric space(X,d)we haveasdim S2X=asdim S1X.Next proposition and corollaries justify our definition of . Proposition3.3.Let S1and S2be two control semigroups.If S1 S2thenfor every metric space X we have asdim S1X≤asdim S2X.Proof.Given f∈S2take g∈S1such that g(s)≥f(s)in a neighborhood of ∞,then any f(s)-bounded family U of subsets of X is g(s)-bounded with s in a neighborhood of∞. Corollary3.4.Let S be a control semigroup.For every metric space X we have asdim U X≤asdim S X≤asdim N X.Corollary3.5.If two control semigroups are equivalent then they are dim-equivalent,i.e.they define the same asymptotic dimension.Example3.6.Note that dim¯U X and asdim U X are the uniform dimension defined in[4]and the asymptotic dimension of[8]respectively.We have also that asdim N X,smdim n X and dim¯N X are the asymptotic dimension with Higson property(see for example[13]),the capacity dimension(see[5])and the Assouad Nagata dimension(introduced in[1])respectively.Note that applying3.5to the example2.9we get another way of defining the Assouad-Nagata asymptotic dimension.The following proposition covers some basic properties of a semigroup-controlled asymptotic dimension.The proofs are highly similar to that ones for Assouad Nagata dimension and asymptotic Assouad Nagata dimension.SEMIGROUP-CONTROLLED ASYMPTOTIC DIMENSION7 We quote between brackets the works where the analogous proofs can be founded.Proposition3.7.Let(X,d X)and(Y,d Y)be metric spaces and S a control semigroup.Then it is satisfied:(1)asdim S A≤asdim S X for every A⊂X.(This is trivial)(2)asdim S X×Y≤asdim S X+asdim S Y([9]or[11])(3)If X=A∪B then asdim S X=max{asdim S A,asdim S B}([9]or[11]).(4)The following conditions are equivalent:([2])a.asdim S X≤n.b.There is a f∈S such that for every s in some neighborhood of∞there exist a cover U with s−m(U)≤n+1and f(s)-bounded.c.There is a g∈S such that for every s in some neighborhoodof∞there exist a cover U with m(U)≤n+1,L(U)≥s andg(s)-boundedd.There is a h∈S such that for everyǫin some neighborhoodof0there is a mapǫ-Lipschitz p:X→K n with K n a n-dimensional simplicial complex such that the family p−1(st v)ish(1/ǫ)-bounded.Remark 3.8.Note that in the proof of the third property it is used the semigroup condition.For the second and fourth properties it is necessary that given g1,g2∈S there exists a g3∈S such that g1+g2≤g3in a neighborhood of∞.Using the semigroup condition and the linear condition define g3=2·g1◦g2if g1(x)>x and g2(x)>x in a neighborhood of∞.rge scale and small scale dimensionsThe aim of this section is to study how the large scale,small scale and the global dimensions are related.Many of these results are based on[3]. Given a global control semigroup we can see it just as a large scale(or small scale)control semigroup.This is the idea behind next definition.Definition4.1.Let¯S be a global control semigroup we will define the large scale(resp.small scale)truncated semigroup of¯S as the semigroup of all functions g for which there exist a dim-control function f∈¯S with g(x)=f(x)in a neighborhood of∞(resp.in a neighborhood of0).We will note it by:T runc∗∗(¯S)(resp.T runc∗∗(¯S)).Now we present some kind of inverse operation of truncation.Given a small scale control semigroupξand a large scale control semigroup S we want to create a global control semigroup¯S associated to those ones.Definition4.2.We define the linked set ofξand S as the set of all contin-uous increasing functions g for which there exist a small scale dim-control function g1with g1∈ξand a large scale dim-control function g2with g2∈S such that g(x)=g1(x)in a neighborhood of0and g(x)=g2(x)in a neigh-borhood of∞.It will be noted by Link(ξ,S).8J.HIGESClearly T runc∗∗(¯S)and T runc∗∗(¯S)are small scale and large scale control semigroups respectively.Next proposition shows we have the same property for linked sets.Proposition4.3.Let Link(ξ,¯S)be a linked set then it is a global control semigroup.Proof.The linear condition is trivial.Now let f,g be two dim-control func-tions of Link(ξ,S)and let(f1,f2),(g1,g2)its small scale and large scale associated functions.we have that f(g(x))=f1(g1(x))in a neighborhood of0and f(g(x))=f2(g2(x))in a neighborhood of∞then as f1◦g1∈ξand f2◦g2∈S the semigroup condition is satisfied. The relationship between truncation and linking is given in the following result:Proposition4.4.Let¯S be a global control semigroup then:Link(T runc∗∗(¯S),T runc∗∗(¯S))≈¯S.Conversely T runc∗∗(Link(ξ,S))≈S and T runc∗∗(Link(ξ,S))≈ξ. Proof.Let P be the global control semigroup Link(T runc∗∗(¯S),T runc∗∗(¯S)). Clearly by¯S⊂P we have P ¯S.Now let g be a dim-control function in P.There exist two dim-control functions g1,g2∈¯S such that g(x)=g1(x)in a neighborhood of0and g(x)=g2(x)in a neighborhood of∞.Let x1≤x2be two positive numbers such that g(x)=g1(x)if x≤x1and g(x)=g2(x)if x≥x2.Let M be the maximum of g in[x1,x2]and let m be the minimum of g1◦g2in the same interval.Suppose m<M then there exist a C>1such that Cm≥M. Define the function g′(x)=C(g1(g2(x))).We have g′(x)≥g(x)for every x and then¯S P.The converse is obvious. Next definition is the key to connect large scale,small scale and global dimensions,see[3].Definition4.5.Let¯S be a global control semigroup and let X be any metric space.We will say that(X,d)has¯S-microscopic controlled dimension at most n and we will note by m−dim¯S X≤n if the metric space(X,d′1= min(d,1))has¯S-controlled dimension at most n.In a similar way we will say that a metric space(X,d)has¯S-macroscopic controlled dimension at most n(M−dim S X≤n)if dim¯S(X,d′′1)≤n with d′′=max(1,d). Lemma 4.6.Let(X,d)be a metric space and let¯S be a global control semigroup.If for every c>0we define the metrics d′c=min(c,d)and d′′c= max(c,d)then m−dim¯S X=dim¯S(X,d′c)and M−dim¯S X=dim¯S(X,d′′c). The proof of this result is given in[3].In such proof the authors used that the Assouad-Nagata dimension is invariant under Lipschitz functions. We give another proof without using this fact.SEMIGROUP-CONTROLLED ASYMPTOTIC DIMENSION9 Proof.We just do the proof for the microscopic case.The macroscopic case is similar.Suppose without loss of generality that c<1.Let s be any positive number.If s≥c then pick the cover U=X.Assume that s<c then there is a cover U with s-Lebesgue number in(X,d′1),multiplicity at most m−dim¯S X+1and f(s)-bounded for some dim-control function f∈¯S. But as d′1(x,y)=d′c(x,y)=d(x,y)if d(x,y)≤c then such cover satisfy L(U)≥s in(X,d′c)and it is f(s)-bounded.We have proved dim¯S(X,d′c)≤m−dim S X.The remaining case is similar. Corollary4.7.Let¯S1be a global control semigroup.If X is a boundedmetric space then m−dim¯S1X=dim¯S1X.If X is a discrete metric spacethen M−dim¯S1X=dim¯S1X.Next lemma shows how the microscopic dimension of a global control semigroup is greater or equal than the semigroup-controlled asymptotic di-mension associated to the large scale truncated semigroup.Lemma4.8.Let X be a metric space and let¯S be a global control semigroup then the following properties are equivalent:(1)M−dim¯S X≤n(2)There is a function f∈¯S such that for all s in a neighborhood of ∞there is a colored cover U= n+1i=1U i with each U i s-disjoint andf(s)-bounded.The proof is almost equal to the proof of Lemma2.7.of[3].It will be left to the reader.Using the same reasoning we can get the analogous Lemma for the mi-croscopic case:Lemma4.9.Let X be a metric space and¯S a global control semigroup then the following properties are equivalent:(1)m−dim¯S X≤n(2)There is a function f∈¯S such that for all s in a neighborhood of 0there is a colored cover U= n+1i=1U i with each U i s-disjoint andf(s)-bounded.Next lemma could be considered some kind of converse of the previous ones.Lemma4.10.Let¯S be a global control semigroup.For every metric space X we have dim¯S X≤n if and only if m−dim¯S X≤n and M−dim¯S X≤n. Proof.The necessary condition is obvious by lemma4.8.Let us prove the sufficient condition.Suppose m−dim¯S X≤n and M−dim¯S X≤n. Without loss of generality we can assume that the f associated to the bounds of the microscopic covers and the macroscopic covers is the same,if not take the composition.Let s be a positive real number.We want tofind a dim-control function g∈¯S and a colored covering U s-disjoint and g(s)-bounded. It is clear that if s>1or f(s)<1the result is obvious.Assume that s≤110J.HIGESand f(s)≥1.Pick s0=f−1(1)and define the function g(x)=f(2f(x)).So if s0≤s≤1take a colored covering U of(X,d′′1)so that it is2f(s)-disjoint and f(2(f(s)))-bounded. Combining all the results of this section we get that the global dimension can be obtained just studying the dimension in a neighborhood of0and in a neighborhood of∞.Theorem4.11.Let¯S be a global control semigroup.For every metric spaceX we have that smdim T runc∗∗(¯S)X=m−dim¯S X and asdim T runc∗∗(¯S)X=M−dim S X.In the other hand givenξa small scale control semigroup and S a largescale control semigroup then:dim Link(ξ,¯S)X=max{smdimξX,asdim S X}.Proof.By the two previous lemmas we get M−dim¯S X≥asdim T runc∗∗(¯S)X. Suppose asdim T runc∗∗(¯S)X≤n.Then for every s≥s0there is a cover U s= n+1i=1U s i that is s-disjoint and f(s)-bounded with f∈T runc∗∗(¯S). That means that there is a f1∈¯S such that f(x)=f1(x)if x≥x1for somex1.Let s′0be the maximum of x1and s0.We have that for every s≥s′0 there is a cover U s= n+1i=1U s i s-disjoint and f1(s)-bounded.Applying4.8 we get the result.The microscopic case is analogous.For the second statement just note:dim Link(ξ,S)X=max{m−dim Link(ξ,S)X,M−dim Link(ξ,S)X}=max{smdim T runc∗∗(Link(ξ,S))X,asdim T runc∗∗(Link(ξ,S))X}So the result follows from the second statement of4.4and3.3.5.Non equivalent semigroup-controlled dimensionsLet SMDIM)be the quotient set of all large scale(resp.small scale)control semigroups with the equivalence relation≡de-fined in section3.In this section we will estimate the cardinality of SMDIM.LetΩbe the set of all the countable ordinals(Ω0)union thefirst uncount-able ordinal.This set is uncountable and it has a natural well order.Wewill prove that there exist two order preserving maps i L:Ω→SMDIM.As usual we will prove the results for the large scalecase.The small scale case will be left to the reader.As afirst step we will estimate the cardinality of the set of all largescale(resp.small scale)control semigroups modulo the equivalence relation≈.They will be noted by ASDIM and SMDIM.The next lemmas are necessary to show that there exist at least countablemany semigroups.SEMIGROUP-CONTROLLED ASYMPTOTIC DIMENSION 11Lemma 5.1.Let g :[a i ,a i +1]→[g (a i ),g (a i +1)]be an increasing continuous function defined in some interval and let f (a i ),f (a i +1)be any pair of points that satisfies f (a i )≥g (a i ),f (a i +1)≥g (a i +1)then there is a continuous increasing function ¯f defined in the same interval such that ¯f ≥g with ¯f(a i )=f (a i )and ¯f (a i +1)=f (a i +1).Proof.Define the function f aux (x )=g (x )+f (a i )−g (a i ).This is an in-creasing continuous function in the interval.If f aux (a i +1)=g (a i +1)then f a ux =¯f.Otherwise let z be the greatest point in [a i ,a i +1]such that the segmenta i +1−z (x −z )+f aux (z )if x ∈(z,a i +1]It is clear that this function satisfies the requirements of the lemma. Lemma 5.2.Let f be a large scale dim-control function such that it is strictly bigger than the identity in a neighborhood of ∞.Then there exist a large scale dim-control function g such that for every n ∈N g (x )>f n (x )in some neighborhood of ∞.Proof.As the function is strictly bigger than the identity we have that there is an increasing sequence x n →∞such that if x ≥x n then f n (x )>f i (x )for all i ≤n −ing 5.1define in each interval [x n ,x n +1]a function g n so that g n (x n )=f n (x n ),g n (x n +1)=f n +1(x n +1)and g n (x )≥f n (x ).Paste all these functions and we get g the required function. Using a similar reasoning we can give the following lemma:Lemma 5.3.Let f be a small scale dim-control function such that it is strictly bigger than the identity in a neighborhood of 0.Then there exist a small scale dim-control function g such that for every n ∈N g (x )>f n (x )in some neighborhood of 0.Next lemma shows that there are at least countable many non equivalent large scale control semigroups.Lemma 5.4.There exist a sequence {S i }i ∈N of large scale control semi-groups with S i ≺S i −1and S i =L ({f i }∪S i −1)where f i is an asymptotic dim-control function such that for every g ∈S i −1f i (x )>g (x )in a neigh-borhood of ∞.Proof.Take S 1=N .Let f :R +→R +be the dim-control function defined by:f (x )= x 2if x ∈[1,∞)x otherwise.It is clear that for every asymptotically linear dim-control function g there is a point x 0∈R +such that f (x )>g (x )if x ≥x 0then we have S 2=L ({f }∪N )≺N =S ∞.12J.HIGESSuppose we have constructed a sequence of control semigroups with S n≺...≺S1so that for each control semigroup S i there is an asymptotic dim-control function f i that S i=L({f i}∪S i−1)and for every dim-control func-tion g of S i−1there exists a x0∈R+such that f i(x)>g(x)if x>x0.Now apply lemma5.2to f n in order to get a dim-control function f n+1so that for every j∈N,f n+1(x)>f j n(x)if x>x0for some x0.We claim that f n+1 satisfies the same property for all g∈S n.Let g be a dim-control function in S ing2.10we have that:g=f1◦f2◦...◦f pFor some functions f i in{f n}∪S n−1.For every f i there exist an x i and a j i such that f j i n(x)>f i(x)if x≥x i.Let x′0be the maximum of all x i then we have that g(x)<f p i=1j i n(x).We have obtained that g(x)<f j n(x)for some j if x≥x0and by the method we have built f n+1we have f n+1(x)>g(x) in a neighborhood of∞.Note that for getting S2we just need an asymptotic dim-control func-tion f that were strictly greater than any asymptotically linear dim-control function in a neighborhood of∞.Doing a dual reasoning we can get:Lemma5.5.There exist a sequence{ξi}i∈N small scale control semigroups withξi≺ξi−1andξi=L({f i}∪ξi−1)where f i is a dim-control function such that for every g∈ξi−1f i(x)>g(x)in a neighborhood of0.We have proved that the sets SMDIM and ASDIM are at least count-able.The lemmas of above suggest the following definition:Definition5.6.We will say that a large scale(small scale)control semigroup S(resp.ξ)is mono-bounded at∞(respectively at0)if there exist an asymptotic dim-control function f such that for every g∈S(resp g∈ξ)we have f(x)>g(x)in a neighborhood of∞(resp.in a neighborhood of0). The function f will be called the bound function of S(ofξ)at∞(resp.at 0).Using the sequence generated in5.4we can build the control semigroup generated by such sequence.Such semigroup will be mono-bounded and then we can begin again a similar process as in5.4.This is the idea of the next two lemmas.Lemma5.7.Let{S i}i∈N be a sequence of large scale control semigroups mono-bounded at∞such that S i≺S i−1and S i=L({f i}∪S i−1)where f i is a bound function of S i−1then the large scale control semigroup given by L( ∞i=1¯S i)is mono-bounded at∞.Proof.The reasoning is similar to the previous ones. Firstly we note that S:=L( ∞i=1S i)= ∞i=1S i.We will prove that S is mono-bounded at∞.We have that there is a sequence of points{a i}i∈N with a i→∞and a i+1>a i such that f i+1(x)>。
高二英语科技发展趋势单选题50题

高二英语科技发展趋势单选题50题1. The development of artificial intelligence has brought great changes to many industries. In this sentence, "artificial intelligence" is a(n) _____.A. verb phraseB. adjective phraseC. noun phraseD. adverb phrase答案:C。
本题考查名词性短语。
“artificial intelligence”是一个名词短语,表示“人工智能”,A 选项“verb phrase”是动词短语,B 选项“adjective phrase”是形容词短语,D 选项“adverb phrase”是副词短语,均不符合题意。
2. With the advancement of 5G technology, the speed of data transmission has significantly increased. The word "advancement" in this sentence can be replaced by _____.A. progressB. movementC. improvementD. development答案:D。
本题考查词汇。
“advancement”有“进步,发展”的意思,A 选项“progress”主要指向前推进的过程,B 选项“movement”侧重于动作或移动,C 选项“improvement”强调改进、改善,D 选项“development”与“advancement”意思相近,都有发展的意思。
3. The application of blockchain technology in finance is becoming more and more widespread. What does "application" mean in this context?A. 使用B. 申请C. 应用D. 适用答案:C。
河北科技大学专业英语考试题精品PPT课件

科技英语的句子特点:
1)逻辑联系语。 一般出现在句子,句群,段落之间,当句子较长时 句子中间也有。 列举:first,second, begin with ,next 增补:and ,and also, in addition, futher more 转折或对比 :but, yet, in fact 原因或结果: hence, for the reason , as a result 解释:that is to say 总结:in all, in conclusion。
工件的温升如果过度的话会降低产品的质量,影 响表面粗糙度和尺寸精度,会引起刀具的过度磨 损,会导致我们不希望的材料金相学的改变
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4)Aluminum develops a thin (a few atomic layers), strong, and adherent hard-oxide film (Al2O3) that better protects the surface from further environmental corrosion. Titanium develops a film of titanium oxide (TiO2). A similar phenomenon occurs in stainless steels, which (because of the chromium present in the alloy) develop a protective film on their surface.
例如从齿轮传到轴或者通过啮合的轮齿传到另一个齿轮从三角皮带传到皮带轮或者从凸轮传到从145newtonslawnewtonsthreelaws第一定律如果作用在一个质点上的所有外力平衡那么这个质点保持原来的静止或者匀速直线运动状态不变
小学上册第十四次英语第2单元测验试卷

小学上册英语第2单元测验试卷考试时间:100分钟(总分:110)B卷一、综合题(共计100题共100分)1. 填空题:I want to be a ______ in the future.2. 选择题:What is the currency used in the United States?A. EuroB. YenC. DollarD. Rupee答案: C3. 填空题:The invention of the telephone transformed ________ (沟通).4. 填空题:The _____ (植物组织) is made up of different cells.5. 选择题:What is the capital of Sri Lanka?A. ColomboB. KandyC. GalleD. Jaffna答案:A. Colombo6. 听力题:The weather is very ___. (nice)7. 听力题:A reaction that is reversible can go in ______ directions.8. 听力题:We make _____ (饼干) together.What is the soft drink made from cola?A. TeaB. CoffeeC. ColaD. Juice10. 听力题:The sun is shining ___. (brightly)11. 填空题:The __________ (战争的影响) shaped national identities.12. 选择题:What is the name of the famous mountain in Africa?A. Mount KilimanjaroB. Mount EverestC. Mount ElgonD. Mount Kenya答案: A. Mount Kilimanjaro13. 填空题:I enjoy making crafts with my ________ (手工材料).14. 填空题:The _______ (蜥蜴) loves to bask in the sun.15. 听力题:I want to ______ a superhero. (become)16. 听力题:His favorite book is a ________.17. 听力题:The ________ (glasses) are on the table.18. 填空题:The invention of ________ changed the way we view the world.19. 选择题:What is the capital of Portugal?a. Lisbonb. Portoc. Farod. Braga答案:aThe __________ (植物) in the forest are very diverse.21. 听力题:A catalyst is not consumed in a ______.22. 填空题:Birds can _________ in the sky. (飞)23. 填空题:A ______ (鳄鱼) has tough skin and sharp teeth.24. 听力题:The _____ (鱼) swims in the water.25. 选择题:What is the capital of Palau?A. NgerulmudB. KororC. AiraiD. Melekeok答案: A26. 选择题:Which vegetable is orange and crunchy?A. PotatoB. TomatoC. CarrotD. Cucumber27. 选择题:What do you use to write?A. BrushB. PencilC. HammerD. Spoon28. 听力题:A _______ is a large area of sand or pebbles along the edge of the sea.29. 填空题:The bear catches _________ (鱼) in the river.30. 听力题:Chemical reactions can be classified as ______ or exothermic.A ____ is often seen playing in the grass and chasing after butterflies.32. 填空题:The ________ is a friendly creature that makes everyone smile.33. 听力题:The fish is swimming in the ________.34. 选择题:What is the name of the famous explorer who sailed the ocean blue in 1492?A. Christopher ColumbusB. Ferdinand MagellanC. Vasco da GamaD. Marco Polo答案: A35. 听力题:The process of plants making food is called ______.36. 填空题:The _____ (花期) varies among different plants.37. 填空题:We have a ______ (精彩的) event planned for this weekend.38. 听力题:The teacher is ______ the classroom. (organizing)39. 听力题:The sun is _____ after the rain. (shining)40. 填空题:My favorite toy is a ________ (拼图). I enjoy putting the pieces ________ (在一起).41. 听力题:The _______ of a plant helps it to absorb nutrients.42. 填空题:A ______ (生态友好的方法) can lead to better practices.43. 填空题:The _______ (小狩猎者) stalks its prey quietly.44. 听力题:The ______ is a layer of the Earth that is partially molten and allows for plate movement.45. (Pilgrimage) to Mecca is an important journey for Muslims. 填空题:The ____46. 填空题:I love to ______ (参与) in educational programs.47. 选择题:What do you call a baby lion?A. CubB. KitC. CalfD. Fawn答案: A48. 填空题:My __________ (玩具名) can __________ (动词) if I shake it.49. 填空题:The __________ (历史的不断) progresses with society.50. 填空题:We have a ______ (愉快的) time while traveling.51. 选择题:What is the name of the longest river in the world?A. AmazonB. NileC. MississippiD. Yangtze52. 选择题:What do we call the person who plays a role in a movie?A. DirectorB. ActorC. ProducerD. Writer53. 填空题:The kangaroo uses its powerful legs to ______ (跳跃).54. 选择题:What is the fastest land animal?A. CheetahB. LionC. HorseD. Elephant答案:A55. 填空题:The ________ (生态恢复措施) can revitalize areas.56. 填空题:The _______ (Great Chicago Fire) of 1871 destroyed a large part of the city.57. 选择题:What is the capital city of Japan?A. TokyoB. SeoulC. BeijingD. Bangkok58. 填空题:Butterflies are attracted to ______ (花朵).59. 选择题:What is the name of the largest planet in our Solar System?A. SaturnB. JupiterC. EarthD. Mars60. 听力题:The main gas released during respiration is _______.61. 选择题:Which month comes after March?A. JanuaryB. FebruaryC. AprilD. May答案:C62. 填空题:I want to travel to ________ (不同国家) when I grow up. I want to see ________ (名胜古迹).63. 听力题:A __________ is a sudden release of energy in the Earth's crust.64. 听力题:The soup is very ________.65. 填空题:The _______ (The Civil Rights Act) aimed to eliminate segregation.66. 听力题:The chemical symbol for iron is ______.67. 填空题:The ________ (生态保护区) helps preserve nature.68. 选择题:What do you call the person who helps you learn at school?A. NurseB. TeacherC. PrincipalD. Janitor答案:B69. 听力题:The _____ (商店) has discounts.70. 听力题:The ______ is known for her community service.71. 听力题:Cosmic rays are high-energy particles from _______.72. 选择题:What do we call a baby rabbit?A. KitB. PupC. CalfD. Chick答案: A73. 填空题:The cat has a fluffy _______ that makes it look cute.74. 选择题:What is the opposite of hot?A. WarmB. ColdC. CoolD. Heat答案:B75. n River flows through __________. (巴西) 填空题:The Amaz76. 小象) is gentle and kind. 填空题:The ___77. 听力题:The cookies are _______ (crunchy).78. 选择题:What do you call a sweet, baked treat made from chocolate?A. CakeB. BrownieC. CookieD. All of the above答案:D79. 听力题:The chemical symbol for oxygen is _____.80. 填空题:古代的________ (historians) 通过研究遗留物来了解过去。
高一英语学术研讨会组织单选题40题

高一英语学术研讨会组织单选题40题1. We are going to hold an academic seminar on _____.A.scienceB.historyC.mathD.literature答案:A。
本题考查学术研讨会常见主题名词辨析。
“science”意为“科学”,学术研讨会可以围绕科学领域的新发现、研究方法等展开;“history”意为“历史”,通常侧重于过去事件的研究;“math”意为“数学”,一般是关于数学理论和问题的讨论;“literature”意为“文学”,主要涉及文学作品和文学理论。
在这个语境中,通常学术研讨会会涉及科学领域的前沿研究等,所以选择“science”。
2. The seminar will focus on the topic of _____.A.artB.technologyC.geographyD.philosophy答案:B。
“art”是“艺术”,通常涉及绘画、音乐等艺术形式的讨论;“technology”意为“技术”,学术研讨会可以探讨新技术的发展和应用;“geography”意为“地理”,主要研究地球表面的自然和人文现象;“philosophy”意为“哲学”,侧重于对基本问题的思考和理论探讨。
这里说研讨会聚焦的主题,通常技术的发展变化快,容易成为研讨会的焦点,所以选“technology”。
3. Which of the following is a common theme for an academic seminar?A.musicB.biologyC.sportsD.fashion答案:B。
“music”是“音乐”,一般在音乐领域的活动中讨论;“biology”意为“生物学”,是学术研讨会常见的主题之一,可以探讨生物的结构、功能、进化等;“sports”意为“体育”,更多在体育活动或相关领域讨论;“fashion”意为“时尚”,主要在时尚界或相关领域被关注。
小学上册第十四次英语第6单元测验卷

小学上册英语第6单元测验卷英语试题一、综合题(本题有100小题,每小题1分,共100分.每小题不选、错误,均不给分)1.My uncle is a ______. He travels a lot for work.2.The _______ (小企鹅) waddles on the ice to find food.3.My favorite game is ______ (电子游戏).4.The _______ (蜥蜴) is a quick mover.5.The _____ (tide) is coming in.6.We eat ______ (lunch) in the cafeteria.7.I ride my bike to _____ (学校).8.We enjoy ________ (camping) in the summer.9. A hamster loves to dig and create ______ (隧道).10.What is the opposite of "north"?A. EastB. WestC. SouthD. UpC South11. A ______ has a long life cycle.12.The ______ is a skilled writer and editor.13.What do you call the small, round fruit that is often used in salads?A. CherryB. TomatoC. OliveD. GrapeC14.What do you call the sound a dog makes?A. MeowB. RoarC. BarkD. Tweet15.What is the name of the famous novel by Mark Twain?A. Moby DickB. The Great GatsbyC. Huckleberry FinnD. To Kill a Mockingbird16. A peacock shows off its ______ (羽毛).17. A ____ is often seen lounging in the sun on warm days.18.The __________ is a large area of land that is mostly empty.19.I like to ___ (visit) my grandparents.20.We have a _____ (夏令营) this year.21.Did you hear that _____ (猫咪) purring?22.What is the term for a group of stars forming a pattern?A. GalaxyB. ConstellationC. ClusterD. NebulaB23.The country known for its coral reefs is ________ (以珊瑚礁闻名的国家是________).24.The __________ is soft and white after it snows. (雪)25.The element with the atomic number is ______.26.What is the opposite of 'day'?A. MorningB. NightC. EveningD. AfternoonB27.The chemical symbol for potassium is _______.28.What is the opposite of 'full'?A. EmptyB. PackedC. LoadedD. HeavyA29.The teacher, ______ (老师), makes learning fun and exciting.30.I hope to make a difference in the world using my ________ (玩具名) creativity.31.The Civil Rights Act was signed in the year ________.32.Earth is the ______ planet from the sun.33.The cat can see well in the _______.34. A suspension is a mixture where particles are ______ in a liquid.35. (African) kingdoms were rich in resources and trade. The ____36.The ________ (framework) supports the project.37.I think it’s important to be curious. Asking questions helps us learn and grow. I love discovering new facts about __________ and sharing them with my friends.38.What do you call a baby hedgehog?A. HogletB. KidC. PupD. Kit39.The _____ (狮子) is a social animal that lives in groups.40.The _______ (The French Revolution) inspired movements for change worldwide.41.What is the capital of Kenya?A. NairobiB. MombasaC. KisumuD. Eldoret42.The ancient Greeks held festivals in honor of their ________.43.ts can produce ______ (种子) without flowers. Some pla44.Acids can turn blue litmus paper ______.45.In the garden, I see many colorful _______.46.My favorite activity is ________ (骑自行车).47.I enjoy _______ with my family.48.The chemical symbol for barium is ______.49.What do you call a story that is told using pictures?A. NovelB. ComicC. BiographyD. PoemB50.cultural identity) shapes community values. The ____51. A __________ is a geological feature that can shape human activities.52.s are popular for their ______ (耐旱) qualities. Sugar di53.The chemical name for HO is _______.54.The chemical formula for sulfuric acid is ______.55.My sister is _____ a song. (singing)56.The chemical formula for sodium sulfate is __________.57.My dad shows me how to ____.58.The __________ (气候带) affects the types of crops grown.59.What is the process of plants making food called?A. RespirationB. PhotosynthesisC. GerminationD. DigestionB60.The capital of Mexico is _____.61.The _______ (狐狸) is very sly.62. A _____ (78) is an area with many trees and animals.63.Which of these is a mode of transportation?A. AppleB. TrainC. ChairD. House64.The flowers are ________ in the vase.65.Which animal is known for its black and white stripes?A. TigerB. ZebraC. LeopardD. PandaB66.What is the capital of Fiji?A. SuvaB. LautokaC. NadiD. LabasaA67.My _____ (花盆) is full of soil.68.The country known for its volcanoes is ________ (冰岛).69.What do you call a place where you can buy books?A. LibraryB. StoreC. SchoolD. ParkB70.__________ (分子动力学) studies how molecules move and interact.71.What is the first letter of the alphabet?A. AB. BC. CD. DA72.What is the capital of Lesotho?A. MaseruB. MaputoC. MbabaneD. GaboroneA73.What is the capital of Mexico?A. CancunB. GuadalajaraC. Mexico CityD. MonterreyC74. A _______ can help to demonstrate the principles of buoyancy in action.75.The park is _______ for playing games.76.What do we call a series of events that happen in a story?A. PlotB. ThemeC. SettingD. CharacterA77. A ________ (植物观察小组) shares knowledge.78.I love to draw pictures of _____ in my sketchbook.79.I want to _______ a new friend.80.My brother is a __________ (数据分析师).81.The __________ (地貌) shapes the landscape.82.What do we call the process of changing from a tadpole to a frog?A. MetamorphosisB. TransformationC. EvolutionD. GrowthA83.Minerals can be identified by their hardness, color, and ______.84.We are ___ in the pool. (playing)85.I want to _____ (understand) how plants grow.86.The force that pulls objects toward each other is called ______ (gravity).87.What is the opposite of 'happy'?A. SadB. AngryC. ExcitedD. TiredA88.The _____ (香草) is used in cooking.89.What is the name of the famous waterfall in North America?A. Victoria FallsB. Angel FallsC. Niagara FallsD. Iguazu FallsC90.I enjoy ________ with my friends.91.I have a pet ________ (狗). His name is ________ (小白). He loves to ________ (玩耍) in the park.92.Finally, I would spend some time relaxing on the ______. I can imagine reading a book or just listening to the sound of the ______. It would be the perfect way to unwind.93.The __________ (历史的教育价值观) shape future leaders.94.Antarctica is located at the __________ of the Earth.95.What is the name of the fairy tale character who lost her shoe?A. Snow WhiteB. CinderellaC. RapunzelD. Sleeping BeautyB96.Which food is made from milk?A. BreadB. CheeseC. RiceD. Meat97.The country famous for its tango is ________ (阿根廷).98.I enjoy _____ (弹奏) the piano.99.What is the capital city of Slovakia?A. BratislavaB. KošiceC. PrešovD. Nitra100.__________ (燃烧) is a rapid reaction that produces heat and light.。
稀土掺杂氧化物激光玻璃英文综述
Rare-earth ion doped TeO 2and GeO 2glassesas laser materialsAnimesh Jha a ,⇑,Billy Richards a ,Gin Jose a ,Toney Teddy-Fernandez a ,Purushottam Joshi b ,Xin Jiang c ,Joris Lousteau da Institute for Materials Research,School of Process,Environmental and Materials Engineering,University of Leeds,Leeds LS29JT,UKb Corporate Research Laboratory,Laird Technologies India Pvt.Ltd.,Unit-3,Fourth Floor,Navigator Building,ITPL,Whitefield Road,Bangalore 560066,Indiac Max-Planck-Institute for the Science of Light,Günther-Scharowsky-Straße 1/Bau 24,91058Erlangen,Germanyd Department of Materials Science and Chemical Engineering,Politecnico di Torino,Corso Duca degli Abruzzi 24,10129Turin,Italy a r t i c l e i nf o Article history:Received 16May 2011Received in revised form 17January 2012Accepted 10March 2012Available online 3May 2012a b s t r a c tGermanium oxide (GeO 2)and tellurium oxide (TeO 2)based glassesare classed as the heavy metal oxide glasses,with phonon energiesranging between 740cm À1and 880cm À1.These two types ofglasses exhibit unique combinations of optical and spectroscopicproperties,together with their attractive environmental resistanceand mechanical properties.Engineering such a combination ofstructural,optical and spectroscopic properties is only feasible asa result of structural variability in these two types of glasses,sincemore than one structural units (TeO 4bi-pyramid,TeO 3trigonalpyramid,and TeO 3+d polyhedra)in tellurite and (GeO 4tetrahedron,GeO 3octahedron)in GeO 2based glasses may exist,depending oncomposition.The presence of multiple structural moities createsa range of dipole environments which is ideal for engineeringbroad spectral bandwidth rare-earth ion doped photonic devicematerials,suitable for laser and amplifier devices.Tellurite glasseswere discovered in 1952,but remained virtually unknown to mate-rials and device engineers until 1994when unusual spectroscopic,nonlinear and dispersion properties of alkali and alkaline earthmodified tellurite glasses and fibres were reported.Detailed spec-troscopic analysis of Pr 3+,Nd 3+,Er 3+,and Tm 3+doped telluriteglasses revealed its potential for laser and amplifier devices foroptical communication wavelengths.This review summarises thethermal and viscosity properties of tellurite and germanate glasses 0079-6425/$-see front matter Ó2012Elsevier Ltd.All rights reserved./10.1016/j.pmatsci.2012.04.003⇑Corresponding author.Tel.:+441133432342;fax:+441133432384.E-mail address:a.jha@ (A.Jha).A.Jha et al./Progress in Materials Science57(2012)1426–14911427forfibre fabrication and compares the linear loss for near and mid-IR device engineering.The aspects of glass preform fabrication forfibre engineering is discussed by emphasising the raw materialsprocessing with casting of preforms andfibre fabrication.The spec-troscopic properties of tellurite and germanate glasses have beenanalysed with special emphasis on oscillator strength and radiativerate characteristics for visible,near IR and mid-IR emission.Thereview also compares the latest results in the engineering of lasersand amplifiers,based onfibres for optical communication and mid-IR.The achievements in the areas of near-IR waveguide and mid-IRbulk glass,fibre,and waveguide lasers are discussed.The latestlandmark results in mode-locked2l m bulk glass lasers sets theprecedence for engineering nonlinear and other laser devices foraccessing the inaccessible parts of the mid-IR spectrum and discov-ering new applications for the future.Ó2012Elsevier Ltd.All rights reserved. Contents1.Introduction (1428)1.1.Background of lasers and broadband sources,applications and market (1428)1.2.A brief description of laser principles in the context of materials engineering (1430)2.Optical transitions in rare-earth ion doped glasses (1431)2.1.Absorption and photoluminescence properties including the competition between radiativeand non-radiative rates (1431)2.2.Radiative and non-radiative rate processes (1433)2.2.1.An introductory summary of radiative and non-radiative decay processes (1434)2.2.2.Energy transfer and related non-radiative processes (1436)3.Background on the development of rare-earth ion doped optical fibre lasers and amplifiers (1437)4.A summary of the optical,phonon vibrational,and thermal properties of tellurite and germanateglasses for laser and amplifier applications (1438)4.1.A brief description of the structures of tellurite and germanate glasses (1438)4.2.Structure and glass formation in tellurium and germanium oxide multicomponentcompositions (1440)4.3.A comparative summary of the thermal and viscosity properties of tellurite and germanateglasses for glass preform and fibre fabrication (1444)4.3.1.Thermal stability of heavy metal glasses (1444)4.4.Fabrication of low OHÀgermanate and tellurite glasses under reactive atmosphere.....processing (1446)4.5.Design and characterisation of single-mode,multi-mode,and multi core fibres (1448)5.Spectroscopic analysis of bulk glasses and glass ceramics (1450)5.1.Sm3+-doped tellurite and germanate glasses for optical transition in the visible range (1451)5.2.Spectroscopic properties of Eu3+ions in tellurite and germanate glass hosts (1454)5.3.Spectroscopic properties of Tb3+ions in tellurite and germanate glass hosts (1456)5.4.Spectroscopy of Nd3+,Yb3+and Pr3+doped tellurite and germanate glasses and devices (1459)5.5.Spectroscopic analysis of Er3+-ions in germanate and tellurite based glasses and devices..14615.5.1.Er3+ion spectroscopy (1461)5.5.2.Co-doped glasses and fibres and energy transfer analysis (1462)5.5.3.Quenching of metastable states (1464)5.5.4.Multiphonon assisted population inversion at4I13/2from4I11/2 (1464)5.5.5.The influence of controlled crystallisation of glass-hosts on Er3+-doped spectroscopy1465sing and amplification in fibres,waveguides,and micro-cavities (1467)6.1.Amplification and gain characterisations of Er3+and co-doped waveguide and fibre hosts..14676.1.1.Amplification methodologies in Er3+-and co-doped fibres (1467)6.1.2.The Er3+waveguide amplifiers and lasers in tellurite and germanate glasses (1469)6.1.3.The Er3+-ion doped micro-cavities (1471)1428 A.Jha et al./Progress in Materials Science57(2012)1426–14916.2.Near-IR and mid-IR optical transitions in Tm3+and Ho3+doped tellurite and germanateglass hosts (1472)6.2.1.Introduction (1472)6.2.2.The optical transitions in Tm3+and Ho3+and spectroscopic parameters (1473)6.2.3.Visible and near-IR transitions in Tm3+and Ho3+activated by Yb3+and amplificationof signals in1460–1510nm (1475)6.2.4.A summary of mid-IR transitions and CW,Q-switched,and mode-locking results inTm3+and Ho3+doped bulk glass,waveguide,and fibre lasers (1481)7.Future trends and conclusions (1483)Acknowledgements (1484)References (1485)1.Introduction1.1.Background of lasers and broadband sources,applications and marketLasers are classified on the basis of defects or colour generating centres present in a gain medium for the multiplication of coherent photon states.The defect states for light amplification may be gas molecules(e.g.in He–Ne lasers),chemical and dyes including metal-vapours,ions dissolved in an opti-cally transparent matrix known as solid-state lasers(SSLs),andfinally the carriers(electrons or holes) in semiconductor laser diodes(SLDs).Although the overall laser types,market and market share,as shown in Fig.1a,and b are dominated by semiconductor lasers,there has been a record level of improvement in the performance of diode pumped solid-state lasers(DPSSLs)[1],especiallyfibre lasers,from a few tens of watts at the end of the1990s to several kilowatts using Yb3+doped silica fibres.In the past decade,wherefibre lasers have reached kilowatt levels of output power[2,3],bulk ceramic and glass lasers for the nuclear fusion programme in US have already exceeded peta watts (1015)of output power and are targeted to achieve exa watts(1018)in the future.Besides cavity engi-neering,the thermal and structural stabilities of materials at such ultra high powers are an essential aspect of the overall system requirement.Einstein wasfirst to report[4]the theory of spontaneous and stimulated emission,following which in the early1950s,Nobel laureates Townes[5]reported their respective discoveries of gas masers. However,thefirst solid state ruby laser,pumped with aflash lamp,was reported by Maiman in 1960[6].Snitzer[7]in1961reported both thefirstfibre and rare-earth ion(Nd3+)doped solid-state flash-lamp pumped laser,operating at1061nm and1062nm.Thermal management of a gain medium is also important in small-scale devices,e.g.in semicon-ductor and optical communication lasers for maintaining wavelength stability.For such applications the device dimensions are critical,the gain per unit length with minimum thermal management is necessary for achieving low costs.One of the main challenges in engineering small foot-print solid state devices,comparable with the traditional semiconductor devices,is the spectroscopic limitations within the materials structure in traditional glass and ceramic materials,which fundamentally limits the gain per unit length.The materials related factors are limited by the solubility of rare-earth ions in standard silicate glasses used for optical communication.By comparison in borate glasses,the low melting point and high-energy phonon structure adversely affect the gain per unit length,whereas phosphate hosts exhibit1000times higher solubility for the majority of the rare-earth oxides compared to silicate and borate glasses.However,the intrinsic hygroscopic nature of phosphates has proven to be a major challenge for complex device fabrication.This review compares the materials and spectroscopic properties of rare-earth doped germanium oxide(GeO2)and tellurium oxide(TeO2)based glasses and devices,in comparison to the spectroscopic performance of traditional silicate,borate and phosphate materials by presenting data on the solubil-ity of rare-earth ions,oscillator strength,lifetimes,branching ratio,and radiative transition probabil-ities of competing transitions.We have also taken examples of novel devices which have beenSymbols and notations usedSection1R1,R2reflectivities of laser cavity mirrorsg gain coefficient per unit length‘length of the cavity(cm or m)G round trip signal gain(dB m,dB,mW,W)a absorption(cmÀ1)s lifetime of the states on an energy levelc velocity of light(2.99Â108m sÀ1)m number of modes in a waveguide volume Vm frequency(cmÀ1)t thickness of a medium(cm)Section2r ab(m),r em(m)absorption cross-section,emission cross-section(pm2)N number of ions per unit volume(no.cmÀ3)k wavelength(nm or cm or m)P peak wavelength(nm)/i,f oscillator or dipole strength,electric dipole(ed)and magnetic dipole(md)s r,s nr radiative,non-radiative lifetimes(sÀ1)4pe o permittivity in electrostatic uniti,j energy multiplet representing the ground and upper statese electronic charge(Coulomb)W R,W NR,W MP,W x radiative,non-radiative,multiphonon decay,and energy transfer rates(sÀ1) n refractive index of the mediumv:linear susceptibility of a mediumh Planck’s constant(6.67Â10À34J s),h h/2pb ij branching ratioT temperature in absolute scale(K)or celcius(°C)D E energy gap(in cmÀ1or eV)a coupling constant parameter(cm)j B Boltzmann constant(1.38Â10À23J KÀ1)p number of phonons required for bridging the energy gap(D E)h x phonon energy(cmÀ1)equals to¼D E pSections4and5NA numerical aperture¼n2core Àn2cladÀÁ0:5D k dispersionD M materials dispersionm Abbe Abbe numbern2nonlinear refractive index(m2WÀ1)a t total absorption(cmÀ1or dB kmÀ1)A0Rayleigh coefficient(dB l mÀ4)B0,C0constants(dB kmÀ1)B1,C1constants(l m)À1D dB l mÀ2kmÀ1E dB kmÀ1T g glass transition temperature(°C or K)T x onset of crystallisation temperature(°C or K)T p peak of crystallisation temperature(°C or K)T m onset of melting temperature(°C or K)t R Raman peaks(cmÀ1)A.Jha et al./Progress in Materials Science57(2012)1426–14911429demonstrated using these two types of oxide materials.TeO 2and GeO 2based glass lasers also offer much larger wavelength tuning in combination with Q-switching and mode locking for power density at lower pump powers than in comparable crystal based devices.1.2.A brief description of laser principles in the context of materials engineeringIn Fig.2,a schematic diagram of a laser gain medium is shown with ‘as the path length of the light oscillating between two mirrors with R 1and R 2reflectivities,with one of the mirrors acting as an out-put coupler by having a reflectivity of less than 100%at the laser wavelength.For a gain coefficient per unit length of the medium,g ,for each trip along the length ‘,the intensity of photons increases by a factor,exp(g ‘).However the end mirrors with reflectivities,R 1and R 2will lead to loss of intensity by fractions (1ÀR 1)times (1ÀR 2).At the threshold condition the intensity of reflected photons from mirrors R 1and R 2must be equal to the initial photon density,which must be maintained then onwards by compensating for any loss within the laser cavity.At the threshold the condition can be expressed by [8]:R 1R 2Áexp ð2g ‘Þ¼1ð1ÞFig.1.(a)Various types of lasers with market share and (b)application of lasers [1].D T temperature differential between T x and T gD T p temperature differential between T p and T xSstability parameter (K)g viscosity (Pa s)X t Omega parameter (cm 2)/i ,felectric or magnetic dipole strengths,oscillator strength C j and C 0thermal occupation factorsP d and P a standard energy transfer probabilityg d and (g 0d )intensities of donor in the presence and absence of an acceptorD g a increase in fluorescence of the acceptor in the presence of the donor,g B c the quantum efficiency of the acceptors the exponent which is to equal to 6,8,and 10for dipole–dipole (d–d),dipole–quadrapole(d–q),and 10for qudrapole–qudrapole (q–q)interaction,respectivelym T energy transfer rate at a temperature Tq i distribution function1/s i transfer rate,rR 0critical distance R inter-ionic distance 1430 A.Jha et al./Progress in Materials Science 57(2012)1426–1491For round trip signal gain G ,beyond threshold,the left hand side in Eq.(1)must be larger than 1,which means that the population at the lasing level will build until it becomes unstable causing stim-ulated emission favouring the energetically most probable photon states within the amplified sponta-neous spectrum of the lasing medium.When the stimulated emission occurs,the value of g decreases instantaneously before the population can build up again.However,each laser cavity suffers from overall loss,a which will reduce the gain,leading to the following equation:R 1R 2Áexp ½ð2‘ðg Àa Þ ¼1ð2ÞFor laser materials engineering,it is important that the value of g be large.The values of g and a depend upon the emission and absorption cross-sections,respectively,of a dopant.a also depends upon the cavity loss,governed by scattering,extrinsic absorption (for example by OH Àions),and the extrinsic defects at the pump and signal wavelengths which may selectively absorb photons non-radiatively.In addition with the loss term,it should also be remembered that the gain,g is equal to a product of inverted population,N times the stimulated emission cross-section (r st ).To maximise the gain it is essential that the lifetime (s met )of the level from which the stimulated emission (or optical transition)occurs is long enough for energy to be stored in the form of occupied states,so that one of the signal photons may be able to trigger the stimulated emission.The stimulated photon decay time (s st ),governed by the spectral width of the transition,depends upon the cavity length and the loss term,as shown in the following equation:s st ¼2‘c :a Total ð3ÞThe value of s st therefore determines the bandwidth of the laser line through frequency or the uncer-tainty relationship.Another important feature for laser oscillation,e.g.,in a three-level system is the total number of resonant modes,m allowable inside a laser cavity having a volume V ,which is expressed in terms of the frequency of oscillation and spontaneous emission bandwidth in the following equation [8]:m ¼8p m 2D m ÁVc 3ð4ÞFrom Eq.(4),the number of oscillating modes,m will increase with the frequency bandwidth of an optical transition.In the examples discussed below we explain the spectroscopic properties of rare-earth ion doped germanium oxide and tellurium oxide glasses in terms of engineering laser and amplifier hosts.2.Optical transitions in rare-earth ion doped glasses2.1.Absorption and photoluminescence properties including the competition between radiative and non-radiative ratesThe most important parameter for amplification is the gain per unit length which depends on the concentrations of dispersed rare-earth ions in a sub-lattice structural site.These ions act as the defect centres in the medium for light amplification.The gain per unit length is proportional to the product of the cross section for stimulated emission,r em and the metastable lifetime (s met ).For example,theλlasingℓλpumpR 1Pump photonsFig.2.A Schematic representation of lasing in a given medium.A.Jha et al./Progress in Materials Science 57(2012)1426–149114311432 A.Jha et al./Progress in Materials Science57(2012)1426–1491typical values for r em are in the10À21–10À20cm2range and10ms of lifetime yield1dB gain in a cen-timetre long device.Such a large value of emission cross-section necessitates a large absorption coef-ficient and/or cross-section(r(m)),which for a transition is determined by the oscillator strength U ab, and can be calculated using the following equation:rðmÞð5ÞaðmÞ¼2:3026twhere2.3026is the conversion factor from log e to log10for determining the intensity ratio:log(I/I0)of light going through the sample of thickness t,in a UV–visible–NIR spectrometer r(m)=a(m)/N,N is the ion concentration in terms of the number density per unit volume.Wyatt[9]compared the absorption cross-sections of a range of opticalfibres,which are listed below in Table1.In this table,wefind that the absorption cross-section is strongly dependent on the Al:Ge ratio.In Table2,the absorption cross-sections and intensity ratios for four different types of glasses are com-pared for1mol%doping of Er2O3.The corresponding values at1530nm for a phosphate glass are in the range of(0.48–0.55)Â10À20pm2[10].The main conclusion from the comparison of data in Tables1and2is that a host material must depict high rare-earth ion solubility and absorption cross-section.Based on the structural and compo-sitional properties of tellurite glasses,described by Vogel[11],these glasses are quite versatile in terms of compositions by incorporating the mono-,di-,tri-,tetra-,penta-,and hexa-valence oxides. The structural properties of tellurite glasses were subsequently analysed in detail by Sekiya and co-workers[12–16],and on this basis it has been established that some tellurite glasses may dissolve up to25mol%of rare-earth oxides.By contrast,little research has been carried out on the spectro-scopic properties of rare-earth doped germanium oxide glasses,one of which is reported in Table2.As an example,the absorption cross-sections of an Er3+-doped tellurium oxide and ZBLAN(50ZrF4–20BaF2–20NaF–5AlF3–4LaF3–1ErF3)glass are compared in Figs.3a and3b.Tellurium oxide glass exhibits much larger absorption cross-section at1480nm(4I15/2?4I13/2)compared to ZBLAN due to the higher refractive index which determines the dipole strength of the transition.In Fig.3b,the absorption cross-sections of a family of tellurite glasses are compared as a function of compositions. As in Table2,wefind that for each specified transition,the absorption cross-section is dependent upon the composition of Na2O,confirming the small but observable differences in the cross-section withTable1A comparison of peak absorption cross-sections(r ab)in pm2,centre wavelengths(P),transition widths(D k),nm from600nm to 1100nm for Er3+-doped silicatefibres[9].Ratio Al:Ge650nm800nm980nmP D k(r ab)P D k(r ab)P D k(r ab) Al only651170.44795200.067978190.24 1:10652160.49794210.086978170.29 1:3365318.50.4795200.089979120.38 Ge only653200.27802200.073980100.36Table2A comparison of Er3+-ion absorption cross-sections(r ab)in pm2for various oxide andfluoride glasses at different wavelengths.Peak intensity ratio(±0.01) Glass composition(mol%)Absorption cross-sections(r ab)atk(nm±0.005pm2)153214959808001495/1532980/1532800/1532 80TeO2–9Na2O–10ZnO–1Er2O30.840.600.350.140.710.410.17 50GeO2–14Ga2O3–20PbO–15Bi2O30.740.390.230.0970.520.310.13 61SiO2–11Na2O–3Al2O3–10LaF3–10PbF2–1ErF30.760.370.210.0890.490.280.12 50ZrF4–20BaF2–20NaF–5AlF3–4LaF3–1ErF30.510.430.230.650.860.460.11composition.The intensity of optical transitions strongly depends on the total dipole strength contrib-uting to the transition.From the reciprocity of absorption and emission cross-sections,described by the Einstein equation and Ladenberg-Fuctbauer relation [4,17,18],the larger magnitude of the absorp-tion coefficient implies a large emission cross-section,which we discuss below by analysing the dipole strength and radiative transition probabilities of each of the Er-ion transitions,for example.2.2.Radiative and non-radiative rate processesThe lasing transition in a rare-earth ion doped host depends strongly upon the energy level structure of the dissolved ions and the resulting competition between the radiative andnon-radiative of the absorption cross-sections in Er 3+doped (NZT composition in mol%80TeO fluoride glass.The arrow shows the pump absorption wavelength used for populating 4567894I 13/24 x=5 x=10 x=15 x=20s -s e c t i o n *10-21 c m 2transitions.The radiative transitions are responsible for spontaneous and stimulated emissions,whereas most of the non-radiative processes are highly dissipative and deplete the energy of pump photons for population inversion.Another important parameter in the amplification of a fibre ampli-fier is the lifetime.The lifetime of inverted states decays exponentially with a time constant,which is characterised experimentally.When there are several pathways for the population to decay,the total probability is the sum of individual probabilities for each pathway.The two main paths for decay are radiative and non-radiative and hence we can write:1s ¼1s r þ1s nr ð6Þwhere s is the total lifetime,s r is the radiative lifetime,and s nr is the non-radiative lifetime.The radiative lifetime arises from the fluorescence from the excited level to all the levels below it.Non-radiative lifetimes depend largely on the glass composition and the vibration coupling between host ions and the rare-earth ions.At high concentrations of rare-earth ions,an effect known as the concen-tration quenching may take place which reduces the lifetimes of excited states.Concentration quench-ing becomes dominant if the lasing transition is in the vicinity of extrinsic impurity absorption bands;e.g.the presence of OH Àion intensifies the influence of like-ion pair induced concentration quenching for the Er 3+:4I 13/2?4I15/2(1500–1600nm),Tm 3+:3H 4?3F 4(1400–1530nm),and Pr 3+:1G 4?3H 5(1300–1350nm)transitions.Below,we briefly discuss the radiative and non-radiative processes using examples of rare-earth ion doped tellurite and germanate glasses.2.2.1.An introductory summary of radiative and non-radiative decay processesThe oscillator strengths (U )of absorption from a given ground state {L ,S ,J }i to a higher {L ,S ,J }j mul-tiplet,from where the optical transition occurs,depend upon the corresponding integrated absorption (r ab )and stimulated emission (r st )cross-sections over the frequency spectrum (R m d m )and are shown below [20]:u ab¼½4p e o mc p Z r ab ðm Þd m ð7a Þu em ¼½4p e o mc p 2Z r st ðm Þd m ð7b ÞHere [4pe o ]designates the permittivity in electrostatic unit,m and e are the mass and charge of an electron,respectively.For a stimulated emission from j multiplet to the ground state i ,the U ab and U em are related and determine the radiative rate (W R )[20–24]as shown in the following equations:u em ¼g i g j u ab ð8ÞW R ¼8ðp en Þ2p e o j !i Þ2Ág i j !u ab ð9Þk j ?I is the emission wavelength and in the case of stimulated emission,it represents the lasing wave-length.From Eq.(9)we can establish that the radiative rate is proportional to U ab ,gi j :the degeneracy ratio,and the materials refractive index,n .The refractive indices of the tellurite and germanate fam-ilies of glasses vary between 1.93and 2.30and 1.7and 2.3,respectively.The values of indices of refrac-tion are much larger than those for silicates,which range between 1.44and 1.55.From this comparison of refractive indices,we may find from Eq.(9)that a tellurite glass is expected to have1.5–2.5times larger radiative rates for a given transition compared to a silicate glass.The oscillator strength,U ab is directly proportional to the radiative rate,W R ,however,the total di-pole strength,U ab can be represented using the susceptibility or refractive index and the electric (U ed )and magnetic (U md )dipoles [20–24].In the context of defining the magnitudes of electric and mag-netic dipoles,Judd–Ofelt (J–O)analysis,discussed in [23],is especially important by characterising the host specific X i (X 2,X 4,X 6)parameters,the magnitudes of which explain the dipole structure1434 A.Jha et al./Progress in Materials Science 57(2012)1426–1491and spectroscopic processes.The magnitude of X 2determines the dominance of covalent character in dipoles,whereas the X 6may reflect on the probability for excited state absorption.The expressions for electric and magnetic dipoles and the total dipole strength in terms of refractive index and the frequency of optical transition,population inversion factor,g i are shown below in the following equa-tions [20,24]:v u ab ¼ðn 2þ2Þ2u ed þn u md ð10a ÞU ab ¼8p 2m v ab 3hg a ðn 2þ2Þ29n u ed þn u md "#ð10b Þwhere m ab is the mean frequency of transition a ?b .m ab ¼R m a ðm Þd m R a ðm Þd m.Using the J–O analysis,the individual and total radiative transition probabilities can be calculated and these vary for a given rare-earth ion in different hosts.In this context two of the most important parameters are the total radiative rate (W r )and the branching ratio,(b ij )of an optical transition,shown in the following equations:s r ¼1P i j W r ð11a Þb ij ¼W ij P i k W ik ¼W ij Ás rð11b ÞThe overall rate,as explained in Eq.(5),is also dependent on the non-radiative components,such as the multiphonon decay rate and the non-radiative energy transfer.Electronic states are excited from the ground state,i ,and populate the higher energy manifold,j ,separated by D E energy gap.The relax-ation process to the ground state may not be entirely radiative.A part of the total energy of the pump photon used for excitation,will be lost non-radiatively which shortens the lifetime of the occupied j states.When the non-radiative process is dominated by multiphonon decay,the occupied dopant ion electronic states may mediate the energy non-radiatively by bridging the D E gap with several overlap-ping vicinal phonons.The strength of overlapping electronic states with vicinal phonons represents the electron–phonon coupling.The coupling constant,a ep ,and the vicinal phonon energy, h x ,deter-mine the rate of multiphonon decay,as explained in Eq.(12)[20,23–25]:W NR ¼W MP ðT Þ¼A 1exp ðÀa ep D E Þ½1þn pð12Þn ¼eh x j T B À1 !À1ð13Þand the a ep is expressed as follows using the Reisfeld–Jorgensen model [25]:a ep ¼ð h x ÞÀ1ln p q ðn þ1ÞÀ1 !¼Àð h x ÞÀ1Á‘n e ep ð14Þwhere W MP (T )is the multiphonon relaxation rate at a temperature T ,and p is the number of phononsrequired to bridge the D E gap,and is equal to p ¼D E x .This means that if the local phonon energy around a dopant is small,the number of phonons,p required will be large and therefore,from the com-bination of the Bose–Einstein Eqs.(10)and (11),the overall multiphonon rate will decrease exponen-tially.q is another constant.The physical meaning of a large value of p is explained with two examples.For bridging an energy gap,e.g.D E =6000cm À1,in a boron oxide glass host,four B–O phonons with energy 1500cm À1are simultaneously required to bridge the gap.By comparison in a tellurite glass,where the maximum phonon energy is of the order of $800cm À1,more than seven phonons will be required to bridge the gap of 6000cm À1.As the number of phonons required to bridge the gap in-creases,the non-radiative decay becomes probabilistically less likely and consequently the radiative transition rate increases.In Table 3,the multiphonon decay parameters are compared for several glass A.Jha et al./Progress in Materials Science 57(2012)1426–14911435。
高二英语物理科学前沿发展趋势单选题40道
高二英语物理科学前沿发展趋势单选题40道1. The latest research in quantum physics shows that particles can exist in multiple states _____.A. simultaneouslyB. sequentiallyC. independentlyD. separately答案:A。
本题考查副词的词义辨析。
simultaneously 表示“同时地”;sequentially 意为“相继地”;independently 指“独立地”;separately 是“分别地”。
在量子物理的最新研究中,粒子能够同时存在于多种状态,A 选项符合语境。
2. The discovery of new materials in the field of nanotechnology has ______ many potential applications.A. led toB. resulted fromC. brought aboutD. come up with答案:A。
led to 表示“导致”;resulted from 意思是“由……造成”,逻辑关系不符;brought about 也有“引起,导致”的意思;come up with 是“提出,想出”。
纳米技术领域新材料的发现导致了许多潜在的应用,A 选项和C 选项都有“导致”的意思,但led to 更常用,A 选项更合适。
3. The study of black holes ______ significant challenges to our understanding of the universe.A. posesB. raisesC. createsD. produces答案:A。
pose 有“造成,引起(威胁、问题等)”的意思;raise 主要指“举起,提高,筹集”;create 侧重于“创造,创建”;produce 意为“生产,制造”。
群的概念教学中几个有限生成群的例子
群的概念教学中几个有限生成群的例子霍丽君(重庆理工大学理学院重庆400054)摘要:群的概念是抽象代数中的最基本的概念之一,在抽象代数课程的教学环节中融入一些有趣的群例,借助于这些较为具体的群例来解释抽象的群理论,对于激发学生的学习兴趣以及锻炼学生的数学思维能力等方面都会起到一定的积极作用。
该文介绍了一种利用英文字母表在一定的规则下构造的有限生成自由群的例子,即该自由群的同音商,称为英语同音群。
此外,该文结合线性代数中的矩阵相关知识,给出了有限生成群SL2(Z )以及若于有限生成特殊射影线性群的例子。
关键词:有限生成群英语同音群一般线性群特殊射影线性群中图分类号:O151.2文献标识码:A文章编号:1672-3791(2022)03(b)-0165-04Several Examples of Finitely Generated Groups in the ConceptTeaching of GroupsHUO Lijun(School of Science,Chongqing University of Technology,Chongqing,400054China)Abstract:The concept of group is one of the most basic concepts in abstract algebra.Integrating some interesting group examples into the teaching of abstract algebra course and explaining the abstract group theory with the help of these more specific group examples will play a positive role in stimulating students'learning interest and training students'mathematical thinking ability.In this paper,we introduce an example of finitely generated free group by using the English alphabet under some certain rules,which is called homophonic quotients of free groups,or briefly called English homophonic group.In addition,combined with the theory of matrix in linear algebra,we give some examples of about finitely generated group SL_2(Z)and finitely generated special projective linear groups.Key Words:Group;Finitely generated group,English homophonic group;General linear group;Special projective linear group1引言及准备知识群是代数学中一个最基本的代数结构,群的概念已有悠久的历史,最早起源于19世纪初叶人们对代数方程的研究,它是阿贝尔、伽罗瓦等著名数学家对高次代数方程有无公式解问题进行探索的结果,有关群的理论被公认为是19世纪最杰出的数学成就之一[1-2]。
2024年高一英语学术研讨会交流语言单选题20题
2024年高一英语学术研讨会交流语言单选题20题1.The professor gave a fascinating ______ at the academic seminar.A.speechB.talkC.lectureD.address答案:C。
“speech”一般指正式的演讲;“talk”比较随意的谈话;“lecture”常指学术性的讲座,符合在学术研讨会的场景;“address”通常指正式的演说或致辞。
本题考查了名词的辨析及常用搭配。
2.The participants actively ______ in the discussion at the seminar.A.joinB.take partC.participateD.attend答案:C。
“join”一般后面跟组织、团体等;“take part”后面常加in,再加活动;“participate”也与“in”搭配,表示参与;“attend”侧重于出席,不一定积极参与讨论。
本题考查了动词的辨析及固定搭配。
3.During the seminar, many valuable ______ were put forward.A.opinionsB.suggestionsC.advicesD.thoughts答案:B。
“advice”是不可数名词,没有“advices”这种形式;“opinions”强调观点;“thoughts”侧重于想法;“suggestions”在学术研讨会场景下,提出的有价值的多是建议。
本题考查了名词的辨析及用法。
4.The seminar focused on various ______ of academic research.A.aspectsB.partsC.sectionsD.factors答案:A。
“parts”部分;“sections”章节;“factors”因素;“aspects”方面,学术研讨会聚焦学术研究的各个方面更符合语境。
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TSINGHUA SCIENCE AND TECHNOLOGY ISSN 1007-0214 18/21 pp472-474 Volume 9, Number 4, August 2004)be The Dynamics of Semigroups of TranscendentalMeromorphic FunctionsHUANG Zhigang (黄志刚)**Department of Mathematical Sciences, Tsinghua University, Beijing 100084, China;Department of Applied Mathematics, University of Science and Technology of Suzhou, Suzhou 215009, ChinaAbstract: This paper considers the dynamics associated with an arbitrary semigroup of transcendental meromorphic functions. Fatou-Julia theory was used to investigate the dynamics of these semigroups. Some results of the dynamics of a rational mapping on the Riemann sphere were extended to the case. Key words: semigroup; dynamics; transcendental entire functionIntroductionLet transcendental mero-morphic functions. We denote byˆ:(1,2,j f C Cj →=K G = [f 1, f 2,K ],the semigroup generated by the family { f j : j =1,2,K } with the semigroup operation being functional compo-sition. We define the Fatou set of the semigroup G byF (G ) = {z ∈C : G is defined and normal in some neighborhood of z }and the Julia set of G by . The semi-group generated by a single function f is denoted by [ f ]. We write F ( f ) for F ([ f ]) and J ( f ) for J ([ f ]). Then F ( f ) and J ( f ) are the Fatou set and Julia set, re-spectively, in the Fatou-Julia classical iteration theory. It is obvious that the dynamics of a semigroup is more complicated than that of the iteration of a single func-tion. Some properties in the classical case cannot be preserved for the semigroup case. For example, F (G ) and J (G ) may not be complete invariant and J (G ) maynot be when J (G ) has an interior point, see the ex-amples in Ref. [1]. We can also list some same proper-ties of the dynamics of a semigroup as that for iteration of a single function ˆ()\()J G CF G =ˆC[1,2].In the series of their papers, Hinkkanen and Martintried to extend the classical theory of the dynamics as-sociated to the iteration of a rational function of a complex variable to the more general setting of an arbi-trary semigroup of rational functions [1,2]. In this paper, we will extend some results of the classical theory to the semigroup of meromorphic functions.1 Some Properties and Exceptional Sets of a Semigroup Generated by a Family of Meromorphic FunctionsLet G be a semigroup generated by a family of mero-morphic functions. For ˆz C∈, we define the backward orbit O −(z ) of z byO −(z )={there exists a g ∈G such that g (w )=z } ˆ:w C∈and the exceptional set of G is defined byE (G )= {ˆz C∈: O −(z ) is finite}. Proposition 1 If z is not an element of E (G ), then ()O z −⊇ J (G ).Proof First of all, we prove ˆ(\())g CO z −⊆ ˆ\(CO z −)for any g ∈G . For ˆ\(),x C O z −∈we need to prove that ˆ()\().g x CO z −∈Suppose that ()g x ∉ ˆ\(CO z −)∞, then there exists a sequence x n ∈O −(z ) such that and a sequence {g ()()n x g x n →→n } in GReceived: 2002-12-05; revised: 2003-11-11﹡﹡ E-mail: huang.z.g@; Tel: 86-512-66111539HUANG Zhigang (黄志刚):The Dynamics of Semigroups of Transcendental (473)satisfying g n {x n }=z . Thus, we have 11{()}n n x g x −=∈. It implies that ()x O z −∈. It is a contradiction.Since ()z E G ∉,()O z − have at least three points. Then ˆ\()(CO z F G −⊆), i.e., ()O z −()J G ⊇. Proposition 1 follows.Let G be generated by a family H of rational func-tions with the degree at least 2. If card(H )<∞, then E (G ) ⊂ F (G ). If card(H ) = ∞, we cannot assert E (G )⊂ F (G ). Example 1 Set f m = a m z n , m = 1,2,K , n ≥ 2 and |a |>1. LetG = [f 1, f 2,K ].Then E (G )={0, ∞}. It is easy to see that 0 is a limit point of 1(){||||m n m J f za −−==}, and hence 0∈J (G ).In the classical case, for any component U of F ( f ),U 1\ f (U ) contains at most one point, where U 1 is a component of F ( f ) with U 1⊃f (U ). However, this result cannot be preserved for a general semigroup.Example 2 F (G ) of the semigroup G = [z n , az n ] with n > 2 and |a |>1 contains||z Ω=<< and{|z |>1}. By a simple calculation, for ,n f az =we have f (Ω )⊂ {|z |>1}, and {|z |>1}\ f (Ω ) is an unbounded domain. Proposition 2 Let G be a semigroup generated by a family of meromorphic functions. Then J (G ) is per-fect and the closure of the repelling fixed points of G where z 0 is called a repelling fixed point of G if there is an element f in G such that f (z 0)=z 0 and 0|()|1f z ′>. And furthermore()()f G J G J f ∈=U (1) We can prove Proposition 2 by the similar argumentto those for the classical case of interaction of a singlefunction. Then Eq. (1) immediately follows from theformer result.2 Semigroups of TranscendentalEntire FunctionsWe say a set M is forward invariant if f (M ) ⊂ M for any f ∈G and M is backward invariant if 1()f M −= {:()}z f z M M ∈⊂ for any f ∈G . It is easy to deduce that F (G ) is forward invariant and J (G ) is backward invariant. Since F (G ) is forward invariant, for anycomponent U of F (G ) and any g ∈G ,()()g U F G ⊂, and g (U ) is contained in a component, denoted by (U , g ), of F (G ).Definition 1 A component U of F (G ) is called a wandering domain of G provided that the set {(U , g ): ∀g ∈G } is infinite; otherwise, U is non-wandering.Theorem 1 Let G be a semigroup generated by a family of transcendental entire functions. Then a mul-tiply-connected component of F (G ) must be wandering and bounded, in other words, a non-wandering compo-nent of F (G ) must be simply-connected.Proof Let U be a multiply-connected component of F (G ). We can draw a simple closed curve γ in U which is not null-holomotopic. Then from Proposition 2, there is g ∈G such that J (g ) intersects the bounded interior surrounded by γ. Since γ ⊂ U ⊂ F (g ), γ is not null-homotopic with respect to F (g ), otherwise ∞∈F (g ). This is impossible, and the component Uof F (g ) which contains U is multiply-connected. By Theorem3.1 of Baker %[3], the set {( is infi-nite, and hence U is a wandering domain of G .,):1,2,}n Ug n =%K We denote by Cri( f ) the set of critical values of f and by Asy( f ) the set of asymptotic values of f . Define the set of singularities of the inverse function of f bySing(1f −)Cri()Asy()f f =U .We denote by B the family of meromorphic func-tions with the bounded Sing(f −1). The method of proof of Theorem 2 in Ref. [4] was used, and the following theorem, which is the main result in this paper, can easily be proved. The idea of his method comes essen-tially from Eremenko and Lyubich [5] and Bergweiler [6], but Zheng [4] finished the proof of his Theorem 2 by combining the hyperbolic metric instead. Theorem 2 Let G be a semigroup generated by afamily of transcendental meromorphic functions12,,...,.n f f f If each f j (1≤j ≤n )∈B , then for all z ∈F (G ),h m (z ) does not tend to infinity, as m ∞, where →11()...()m m m i i i h z f f f z −=o o o ,and furthermore if , in addition, each f j is entire, then12()...()m m i i i g z f f f z =o o odoes not tend to ∞ on F (G ), , . 1k i n ≤≤1k m ≤≤Theorem 2 is an extension of Theorem 2 of Zheng [4]. In the proof of Theorem 2, we need the following result.474 Tsinghua Science and Technology , August 2004, 9(4): 472–474()∞Lemma 1 Suppose f ∈B and . Thenthere exist a positive constant R and a curve Γ connect-ing 0 and ∞ such that 10s s f ∞−=∉U |()|f z R ≤on Γ and for allwhich are not poles of f ,\{0}z C ∈ |()||'()|4||f z f z z ≥log |()|f z R (2)This first part of Lemma 1 is obvious and Inequality(2) was proved in Zheng [8] using the hyperbolic metric and in Ref. [9] for “16π” in place of “4” using the logarithmic change of variable in a neighborhood of infinity.Proof of Theorem 2 We can assume without any loss of generality that Then there areR and curves connecting 0 and ∞ such that 110ns j j s f ∞−==∉U U ().∞(1)j j n Γ≤≤|()|j f z R ≤on and for all z ∈ C\{0} which are not poles of f (1)j j n Γ≤≤j , we have|()|'()|2||j j |f z f z z ≥πlog |()j |f z R , 1. j n ≤≤Suppose that there are a point z 0∈F (G ) and a set, such that12{,,...}i i 1k i n ≤≤100()()m m i i h z f f z =→∞oKo m →∞, as . Since {h m (z )} is normal at z 0, we can take a fixed positive number R 0 such that and for m ≥m 00(,)|,m B z R h →∞0≥0,where B (z 00((,))(){||},m h B z R F G z R ⊂>I 0, R 0) denotes the disk with center z 0 and radius R 0. We can assume m 0=1 without any loss of generality. Lemma 1 implies00:(,)\m q h B z R C Γ→, . 1m q i +=By the principle of hyperbolic metric [7], we have\0001[()]|()|,q C m m h z h z R Γλ′≤ where \()q C z Γλis the hyperbolic density on C \Γq . SinceC \Γq is simply connected, it is easy from the Koebe 14Theorem to prove that\1inf{()dist(,):\}4q q q C z z z C ΓλΓΓ∀∈≥,where dist(z , Γq ) is the Euclidean distance of z to Γ q . Therefore,000044|'()|dist((),)|()|m m q h z h z h z R R Γ≤≤0m (3)Put w p =h p (z 0),1,2,,p =K w 0=z 0. Since w p ∈F (G ), w p is not a pole of any element of G . Then by Formula (2), we have|()||'()|2||j p j p p f w f w w ≥πlog |()|j p f w R , and therefore,1111000|||'()||'()|2||k m m k m i k k k k w h z f w w +−−+===≥π∏∏log 1||k w R +=1000|()|1||2m m k h z z −=π∏log 1||k w R+. This inequality contradicts Formula (3) since 1012m k −=π∏log 1||k w R +()m →∞→∞.If each f j ∈B is entire, every component of F (G ) issimply connected.is contained in a sim-ply connected component of F (G ). We can deduce Formula (3) by the same method. 00((,))m h B z R Theorem 2 follows. References[1] Hinkkanen A, Martin G J. The dynamics of semigroups ofrational functions I. Proc . London Math . Soc ., 1996, 73(3): 358-384.[2] Hinkkanen A, Martin G J. Julia sets of rational semigroups.Math. Z , 1996, 222: 161-169.[3] Baker I N. Wandering domains in the iteration of entirefunctions. Proc. London Math. Soc., 1984, 49: 563-576. [4] Zheng J H. Singularities and wandering domain in itera-tions of meromorphic functions. Illinois Math. J., 2000, 44(3): 520-530.[5] Eremenko A E, Lyubich M Y. Dynamical properties ofsome classes of entire functions. Ann. Inst. Fourier , 1992, 42: 989-1020.[6] Bergweiler W. Iterations of meromorphic functions. Bull.Amer. Math. Soc. (N .S ), 1993, 29: 151-188.[7] Zheng J H. Uniformly perfect sets and distortion of holo-morphic functions. Nagoya. Math. J., 2001, 164: 17-33. [8] Zheng J H. On transcendental meromorphic functionswhich are geometrically finite. J . Austral. Math. Soc ., 2002, 72: 93-107.[9] Rippon P J, Stallard G M. Iteration of a class of hyperbolicmeromorphic functions. Proc. Amer. Math. Soc., 1999, 207: 3251-3258.。