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Certain -homomorphisms acting on unital C-probability spaces and semicircular elements induced by p-adic number fields over primes p

  • Received: 01 February 2020 Revised: 01 March 2020 Published: 01 June 2020
  • 05E15, 11G15, 11R47, 11R56, 46L10, 46L54, 47L30, 47L55

  • In this paper, we study the Banach -probability space (ACLS, τ0A) generated by a fixed unital C-probability space (A, φA), and the semicircular elements Θp,j induced by p-adic number fields Qp, for all p P, j Z, where P is the set of all primes, and Z is the set of all integers. In particular, from the order-preserving shifts g×h± on P × Z, and -homomorphisms θ on A, we define the corresponding -homomorphisms σ1:θ(±,1) on ACLS, and consider free-distributional data affected by them.

    Citation: Ilwoo Cho. Certain -homomorphisms acting on unital C-probability spaces and semicircular elements induced by p-adic number fields over primes p[J]. Electronic Research Archive, 2020, 28(2): 739-776. doi: 10.3934/era.2020038

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  • In this paper, we study the Banach -probability space (ACLS, τ0A) generated by a fixed unital C-probability space (A, φA), and the semicircular elements Θp,j induced by p-adic number fields Qp, for all p P, j Z, where P is the set of all primes, and Z is the set of all integers. In particular, from the order-preserving shifts g×h± on P × Z, and -homomorphisms θ on A, we define the corresponding -homomorphisms σ1:θ(±,1) on ACLS, and consider free-distributional data affected by them.



    The main purposes of this paper are (ⅰ) to re-consider (weighted-)semicircular elements in a certain Banach -probability space induced by measurable functions on p-adic number fields Qp, for primes p, and to study free-probabilistic properties of the Banach -probability space LS = (LS, τ0) generated by those mutually-free, (weighted-)semicircular elements, (ⅱ) to extend the structure LS to the tensor product Banach -probability space,

    (ACLS, φAτ0)

    for an arbitrarily fixed unital C-probability space (A, φA), and investigate (weighted-)semicircular elements of this new Banach -probabilistic structure, (ⅲ) to consider certain -homomorphisms acting on ACLS induced by shifting processes on the Cartesian product set P×Z, and to investigate how such -homomorphisms affect the free probability on ACLS, and (ⅳ) by extending such -homomorphisms of (ⅲ) to certain -homomorphisms induced by -homomorphisms acting on A, to study how such generalized morphisms distort the free probability on ACLS.

    The main results of this paper are interesting not only in applied number theory, but also in free-probabilistic operator theory. From number-theoretic objects, primes and corresponding p-adic number fields, the free-probabilistic objects, (weighted-)semicircular elements, are well-constructed; and the operator-theoretic objects, -homomorphisms and corresponding Banach-space operators, are acting on such (weighted-)semicircular elements well; and the structures and properties of them are characterized and shown. Moreover, under tensor product, operator-algebraic properties of tensor product structures, and free-distributional information are studied operator-algebraically. So, our works provide new connections among number theory, free probability, operator theory, and operator algebra theory. i.e., the main results would be applicable to statistical quantum physics, studying analysis on certain physical structures over the non-Archimedean structures (having "very small" distances, or metrics).

    For more about number-theoretic motivations of our proceeding works, see e.g., [16], [17], [18], [19], [31] and [32]. And, for more about statistical analysis, see [1], [2], [3], [4], [5], [6], [15], [21], [22] and [25]. Also, for free probability theory, see e.g., [26], [27], [28], [29], [30], [24], [20], [33], [34] and [35].

    Relations between primes and operators have been studied in various different approaches. For instance, we studied how primes act on certain operator algebras and dynamical systems, as operators, with help of p - adic, and Adelic analysis (e.g., [9]).

    In [8] and [12], we studied weighted-semicircular elements, and corresponding semicircular elements induced by measurable functions on p -adic number fields Qp, for p P. The main results of these papers show that p-adic analysis allows us to have the (weighted-)semicircular law(s), statistically. As applications of [8] and [12], free stochastic calculus for our (weighted-)semicircular law(s) was considered in [11]. And we globalize the (weighted-)semicircularity of [8] and [11] to those induced by Adelic analysis in [10].

    In this paper, we are interested in how the (weighted-)semicircular law(s) on (ACLS, φAτ0) is (are) affected, or distorted by certain -homomorphisms acting on ACLS.

    In this section, we briefly mention about backgrounds of our proceeding works.

    Free probability is the noncommutative operator-algebraic version of classical measure theory and statistics. The classical independence is replaced by the freeness by replacing measures on sets to linear functionals on noncommutative algebras (e.g., [26], [29], [30], [33] and [35]). It has various applications not only in pure mathematics (e.g., [23], [25], [27], [28], [24] and [20]), but also in related fields (e.g., [3] through [12]). In particular, we here use combinatorial approach of Speicher (e.g., [29] and [30]).

    In the text, without introducing detailed definitions and combinatorial backgrounds, free moments and free cumulants of operators will be computed. Also, we deal free product -probability spaces, without detailed introduction.

    Notation and Assumption. As in the "traditional" free probability theory, the pairs (B, φB) of noncommutative algebras B, and fixed linear functionals φB on B are said to be (noncommutative) free probability spaces. However, for our purposes, even though a given algebra A is commutative, we will call a pair (A, ψ) of a commutative algebra A and a linear functional ψ on A, a free probability space, "non-traditionally" (e.g., see [8] through [12]). The freeness on such a non-traditional free probability space (A, ψ) is trivial by the commutativity of A, but (traditional) free probability theory well-covers functional-and-statistical analysis on A, for ψ. So, without loss of much generality, we call the pairs (B, φB) of (noncommutative, or commutative) algebras B, and linear functionals φB on B, free probability spaces, below.

    For more about p-adic analysis, see [31] and [32] (also, see [17] and [22]). Let Qp be the p-adic number fields for p P. Recall that Qp are the maximal p -norm-topology closures in the normed space (Q, |.|p) of all rational numbers, where |.|p are the non-Archimedean norms, called p-norms on Q, for all p P.

    For any fixed p P, the Banach space Qp forms a field algebraically under the p-adic addition and the p-adic multiplication in the sense of [32], i.e., Qp is a Banach field.

    Also, such a Banach field Qp is understood as a measure space

    Qp = (Qp, σ(Qp), μp),

    equipped with the left-and-right additive invariant Haar measure μp on the σ-algebra σ(Qp), satisfying that

    μp(Zp) = 1,

    where Zp is the unit disk of Qp,

    Zp def= {x Qp : |x|p 1} in Qp,

    consisting of all p-adic integers of Qp, for all p P (e.g., [31] and [32]).

    As a topological space, the p-adic number field Qp contains its basis elements,

    Uk=pkZp={pkxQp:xZp}, (1)

    for all k Z. (e.g., [32]).

    By understanding Qp as a measure space, one can establish a -algebra Mp over C as a - algebra,

    Mp = C[{χS:Sσ(Qp)}]

    consisting of μp-measurable functions f,

    f=Sσ(Qp)tSχS   (tSC),

    where the sum is the finite sum, and χS are the usual characteristic functions of S.

    On Mp, one can naturally define a linear functional φp by the p-adic integral, i.e.,

    φp(f)=Qpfdμp,fMp. (2)

    Define now subsets k of Qp by

    k=UkUk+1,forallkZ. (3)

    We call these μp-measurable subsets k of (3), the k-th boundaries (of the basis elements Uk of (1)), for all k Z. By the basis property of the subsets Uk of (1), one obtains that

    Qp=kZk, (4)

    where means the disjoint union. Also, by measure-theoretic data, one has

    μp(k)=μp(Uk)μp(Uk+1)=1pk1pk+1, (5)

    for all k Z.

    Note that, by (4), if S σ(Qp), then there exists a subset ΛS of Z, such that

    ΛS={jZ:Sj}. (6)

    Thus, by (6), one obtains the following proposition.

    Proposition 2.1. Let S σ(Qp), and let χS Mp. Then there exist rj R, such that

      0rj1inR,  for  all  jΛS,and  φp(χS)=QpχS  dμp=jΛSrj(1pj1pj+1), (7)

    where ΛS is in the sense of (6).

    Proof. The computation (7) is shown by (5). See [8], [9], [10], [11] and [12] for details.

    Throughout this section, fix a prime p P, and let Qp be the corresponding p-adic number field, and let Mp be the p-adic -algebra of Qp. In this section, let's establish a suitable (non-traditional) free-probabilistic model on Mp.

    Let Uk = pkZp be the basis elements (1), and k, their boundaries (3) of Qp, i.e.,

    k=UkUk+1,forallkZ. (8)

    Define a linear functional φp : Mp C by the p-adic integral (2),

    φp(f)=Qpfdμp,forallfMp. (9)

    Definition 3.1. The pairs (Mp, φp) are called p-adic (non-traditional free) -probability spaces, for all p P.

    Then, by (7) and (9), one obtains that

    φp(χUj) = 1pj,  and   φp(χj) = 1pj1pj+1,

    since

    ΛUj = {k Z : k j},  and   Λj = {j},

    for all j Z.

    Proposition 3.1. Let Sl σ(Qp), and let χSl (Mp, φp), for l = 1,..., N, for N N. Let

    ΛS1,...,SN = Nl=1ΛSl in Z,

    where ΛSl are in the sense of (7), for l = 1,..., N. Then there exist rj R, such that

     0rj1inR,jΛS1,...,SN,andφp(NΠl=1χSl)=jΛS1,...,SNrj(1pj1pj+1). (10)

    Proof. The formula (10) is proven by (7), since

    NΠl=1χSl = χNl=1Sl in Mp.

    See [8] through [12], for details.

    Fix a prime p P. Let (Mp,φp) be the p-adic -probability space. By understanding Qp as a measure space, construct the L2-space,

    Hpdef=L2(Qp, σ(Qp), μp)=L2(Qp), (11)

    over C, equipped with its inner product <,>2,

    f1, f22def=Qpf1f2dμp, (12)

    for all f1, f2 Hp, inducing the L2-norm,

    f2def=f,f2,  for  all  fHp, (12')

    where <,>2 is the inner product (12) on Hp.

    Definition 4.1. We call the Hilbert space Hp of (11), the p-adic Hilbert space.

    By the definition (11) of the p-adic Hilbert space Hp, our -algebra Mp acts on Hp, via an algebra-action αp,

    αp(f)(h)=fh,  for  all  hHp, (13)

    for all f Mp. i.e., by (13), for any f Mp, the image αp(f) is a well-defined multiplication operator on Hp with its symbol f, satisfying

    αp(f1f2)=αp(f1)αp(f2)onHp,f1,f2Mp,and(αp(f))=α(f)onHp,fMp. (14)

    Notation. Denote αp(f) by αpf, for all f Mp. Also, for convenience, denote αpχS simply by αpS, for all S σ(Qp).

    Proposition 4.1. The pair (Hp, αp) is a well-determined Hilbert-space representation of Mp.

    Proof. The proof is done by (14) (e.g., see [8] and [12]).

    Definition 4.2. Let

    Mpdef=¯αp(Mp).=¯C[αpf :fMp]. (15)

    in B(Hp), where ¯X. mean the operator-norm closures of subsets X of B(Hp). This C-algebra Mp of (15) is called the p-adic C-algebra of (Mp, φp).

    Throughout this section, let's fix a prime p P. Let (Mp, φp) be the corresponding p -adic -probability space, and Mp, the p-adic C-algebra of (15). Define a linear functional φpj : Mp C by a linear morphism,

    φpj(a)def=a(χj), χj2,aMp, (16)

    for all j Z, where <,>2 is the inner product (12) on the p-adic Hilbert space Hp of (11).

    Definition 5.1. Let j Z, and let φpj be the linear functional (16) on the p-adic C-algebra Mp. Then the pair (Mp, φpj) is said to be the j-th p -adic (non-traditional) C-probability space.

    Now, fix j Z, and take the j-th p-adic C -probability space (Mp, φpj). For S σ(Qp), and an element αpS Mp, one has that

    φpj(αpS)=αpS(χj), χj2=μp(Sj)=rS(1pj1pj+1), (17)

    by (3.8), for some 0rS1 in R.

    Proposition 5.1. Let k be the k-th boundaries (8) of Qp, for all k Z. Then

    φpj((αpk)n)=δj,k(1pj1pj+1), (18)

    for all n N, for k Z.

    Proof. By (17), one has that

    φpj(αpk)=δj,k(1pj1pj+1),  for  all  kN. (19)

    Since αpk are projections in Mp, in the sense that:

    (αpk)2 = αpk = (αpk) in Mp,

    the formula (18) holds by (19), for all k Z.

    Let Mp be the p-adic C-algebra for p P. Take projections

    Pp,j=αpjMp, (20)

    induced by boundaries j of Qp, for all j Z. We now restrict our interests to these projections Pp,j of Mp.

    Definition 6.1. Fix p P. Let Sp be the C-subalgebra

    Sp=C({Pp,j}jZ)=¯C[{Pp,j}jZ] of Mp, (21)

    where Pp,j are projections (20), for all j Z. We call this C-subalgebra Sp, the p-adic boundary (C -)subalgebra of Mp.

    Every p-adic boundary subalgebra Sp satisfies the following structure theorem.

    Proposition 6.1. Let Sp be the p-adic boundary subalgebra (21) of the p-adic C-algebra Mp. Then

    Sp-iso=jZ(CPp,j)-iso=CZ, (22)

    in Mp.

    Proof. It suffices to show that the generating projections {Pp,j}jZ of Sp are mutually orthogonal from each other. But, one can get that, for any j1, j2 Z,

    Pp,j1Pp,j2 = αp(χpj1pj2) = δj1,j2αppj1 = δj1,j2Pp,j1,

    in Sp. Therefore, the structure theorem (22) holds. See [8] for more details.

    Let Mp be the p-adic C-algebra, and let Sp be the boundary subalgebra (21) of Mp, satisfying the structure theorem (22). Throughout this section, let's fix a prime p. Recall that if {Pp,k}kZ are the generating projections (20) of Sp, then

    φpj(Pp,k)=δj,k(1pj1pj+1),j,kZ (23)

    by (18).

    Let ϕ be the Euler totient function, which is an arithmetic function

    ϕ : N C,

    defined by

    ϕ(n)=|{kN:kn, gcd(n,k)=1}|, (24)

    for all n N, where |X| mean the cardinalities of sets X, and gcd means the greatest common divisor. Then

    ϕ(q)=q1=q(11q),qP, (25)

    by (24).

    So, one can get that

    φpj(Pp,j)=1pj(11p)=ppj+1(11p)=ϕ(p)pj+1, (26)

    by (23) and (25), for j Z.

    Motivated by (26), define the new linear functionals τpj : Sp C, by linear morphisms,

    τpj=1ϕ(p)φpjonSp, (27)

    satisfying that:

    τpj(Pp,k) = δj,kϕ(p) φpj(Pp,j) = δj,kpj+1,

    for all j, k Z.

    Proposition 7.1. Let Sp(j) = (Sp, τpj) be a (non-traditional) C-probability space, and let Pp,k be the generating projections of Sp, for all k Z. Then

    τpj(Pnp,k)=δj,kpj+1,forallnN. (28)

    Proof. The free-moment formula (28) is proven by (27).

    Let (A, φ) be a (traditional, or non-traditional) topological -probability space (C-probability space, or W-probability space, or Banach -probability space, etc.) equipped with a (noncommutative, resp., commutative) topological -algebra A (C-algebra, resp., W-algebra, resp., Banach -algebra), and a (bounded, or unbounded) linear functional φ on A.

    Definition 7.1. Let a be a self-adjoint operator in (A, φ). This operator a is said to be semicircular in (A, φ), if

    φ(an)=ωncn2,   for   all   nN, (29)

    where

    ωn = {1if  n  is  even0if  n  is  odd,

    for all n N, where ck are the k-th Catalan number,

    ck = 1k+1(2kk) = 1k+1(2k)!(k!)2 = (2k)!k!(k+1)!,

    for all k N0 = N {0}.

    It is well-known that, if kn(...) is the free cumulant on A in terms of φ (in the sense of [29] and [30]), then a self-adjoint operator a is semicircular in (A, φ), if and only if

    kn(a, a, ......, an-times)={1if  n=20otherwise, (30)

    for all n N (e.g., see [12]). The above characterization (30) of the semicircularity (29) is obtained by the Möbius inversion of [29] and [30]. Thus, the semicircular operators a of (A, φ) can be re-defined by the self-adjoint operators satisfying the free-cumulant characterization (30).

    Motivated by (30), one can define so-called the weighted-semicircular elements.

    Definition 7.2. Let a (A, φ) be a self-adjoint operator. It is said to be weighted-semicircular in (A, φ) with its weight t0 (in short, t0-semicircular), if there exists t0 C× = C{0}, such that

    kn(a, a, ...., an-times)={t0if n=20otherwise, (31)

    for all n N, where kn(...) is the free cumulant on A in terms of φ.

    By the definition (31), and by the Möbius inversion of [29] and [30], we obtain the following free-moment characterization (32) of (31): A self-adjoint operator a in a -probability space (A, φ) is t0-semicircular, if and only if there exists t0 C×, such that

    φ(an)=ωntn20cn2, (32)

    where ωn are in the sense of (29), for all n N.

    Let Sp(k) = (Sp, τpk) be a (non-traditional) C-probability space for p P, k Z. Throughout this section, we fix p P, k Z, and the corresponding C -probability space Sp(k).

    Define now bounded linear transformations cp and ap "acting on the C-algebra Sp," by linear morphisms satisfying,

    cp(Pp,j)=Pp,j+1, (33)

    and

    ap(Pp,j) = Pp,j1,

    on Sp, for all j Z.

    By (33), one can understand cp and ap as bounded operators contained in the operator space B(Sp), consisting of all bounded linear operators on Sp, by regarding Sp as a Banach space (e.g., [15]). Under this sense, the operators cp and ap of (33) are understood as well-defined Banach-space operators on Sp.

    Definition 7.3. The Banach-space operators cp and ap on Sp in the sense of (33) are called the p-creation, respectively, the p-annihilation on Sp. Define a new Banach-space operator lp by

    lp=cp+ap  on  Sp. (34)

    We call this operator lp of (34), the p-radial operator on Sp.

    Let lp be the p-radial operator (34) in B(Sp). Construct a Banach algebra Lp by

    Lp=¯C[lp]  in   B(Sp), (35)

    equipped with the inherited operator-norm . of B(Sp), defined by

    T=sup{TxSp:xSp  s.t. xSp=1},

    where

    xSp=sup{x(h)2:hHp  s.t.  h2=1},

    is the C-norm on Sp, where .2 is the L2-norm on the p-adic Hilbert space Hp = L2(Qp).

    On the Banach algebra Lp of (35), define a unary operation () by

    k=0sklkpLpk=0¯sklkpLp, (36)

    where sk C, with their conjugates ¯sk C.

    Then the operation (36) is a well-defined adjoint on Lp (e.g., [8] and [12]). So, equipped with the adjoint (36), this Banach algebra Lp of (35) forms a Banach -algebra embedded in the topological vector space B(Sp).

    Definition 7.4. Let Lp be a Banach -algebra (35) for a fixed p P. We call Lp, the p-radial (Banach--)algebra on Sp.

    Let Lp be the p-radial algebra on the boundary subalgebra Sp. Construct now the tensor product -algebra LSp by

    LSp=LpCSp, (37)

    where C is the tensor product of Banach -algebras.

    Take now a generating element lnpPp,j, for some n N0, and j Z, where Pp,j are the generating projections (20) of Sp, with axiomatization:

    l0p=1Sp,theidentityoperatorofSp,

    in B(Sp), for all j Z.

    Define now a bounded linear morphism Ep : LSp Sp by a linear transformation satisfying that:

    Ep(lkpPp,j)=(pj+1)k+1[k2]+1lkp(Pp,j), (38)

    for all k N0, j Z, where [k2] is the minimal integer greater than or equal to k2, for all k N0.

    By the cyclicity (35) of the tensor factor Lp of LSp, and by the structure theorem (22) of Sp, the above morphism Ep of (38) is indeed a well-defined linear transformation.

    Now, consider how our p-radial operator lp=cp+ap acts on Sp. Observe first that

    cpap(Pp,j) = Pp,j = apcp(Pp,j),

    for all j Z, p P, implying that

    cpap=1Sp=apcp  on  Sp. (39)

    Lemma 7.2. Let cp, ap be the p-creation, respectively, the p-annihilation on Sp. Then

    cnpanp=(cpap)n=1Sp=(apcp)n=anpcnp, (40)

    and

    cn1pan2p=an2pcn1p,  on  Sp,

    for all n, n1, n2 N.

    Proof. The formulas in (40) holds by (39).

    By (40), one can have that

    lnp = (cp+ap)n = nk=0(nk) ckpankp,

    with identity:

    c0p = 1Sp = a0p, (41)

    for all n N, where

    (nk)=n!k!(nk)!,  for  all  knN0.

    By (41), one obtains the following proposition.

    Proposition 7.3. Let lp Lp be the p-radial operator on Sp. Then

    (42)    l2m1p does not contain 1Sp-term, and

    (43)    l2mp contains its 1Sp-term, (2mm)1Sp,

    for all m N.

    Proof. The proofs of (42) and (43) are done by straightforward computations (41), with help of (40). See [8] for details.

    Fix p P, and let LSp be the tensor product Banach -algebra (37), and let Ep : LSp Sp be the linear transformation (38). Throughout this section, let

    Qp,j=lpPp,jLSp, (44)

    for j Z, where Pp,j are projections (20) generating Sp. Observe that

    Qnp,j=(lpPp,j)n=lnpPnp,j=lnpPp,j, (45)

    for all n N, for all j Z.

    By (37) and (45), these operators Qp,j of (44) generate LSp, for all j Z. Consider now that, if Qp,j LSp is in the sense of (44) for j Z, then

    Ep(Qnp,j)=(pj+1)n+1[n2]+1lnp(Pp,j), (46)

    by (38) and (45), for all n N.

    For any fixed j Z, define a linear functional τ0p,j on LSp by

    τ0p,j=τpjEponLSp, (47)

    where τpj is a linear functional (27) on Sp.

    By the linearity of both τpj and Ep, the morphism τ0p,j of (47) is a well-defined linear functional on LSp. So, the pair (LSp, τ0p,j) forms a (non-traditional) Banach -probability space.

    By (46) and (47), if Qp,j is in the sense of (44), then

    τ0p,j(Qnp,j)=(pj+1)n+1[n2]+1τpj(lnp(Pp,j)), (48)

    for all n N.

    Theorem 7.4. Let Qp,j = lp Pp,j (LSp,τ0p,j), for a fixed j Z. Then Qp,j is p2(j+1)-semicircular in (LSp, τ0p,j). More precisely, one obtains that

    τ0p,j(Qnp,j)=ωn(p2(j+1))n2cn2, (49)

    for all n N, where ωn are in the sense of (7.1.5). Equivalently, if k0,p,jn(...) is the free cumulant on LSp in terms of the linear functional τ0p,j of (48), then

    k0,p,jn(Qp,j, ......, Qp,jn-times)={(pj+1)2  if  n=20  otherwise,   (50)

    for all n N.

    Proof. The formula (49) is proven by the straightforward computations from (48) with help of (28), (42) and (43). Also, the formula (50) is obtained by the Möbius inversion of [12] from (49). See [8] and [12] for more details.

    Let LSp and τ0p,j be in the sense of (37), respectively, (47). Then, one has the corresponding non-traditional Banach -probability spaces,

    LSp(j)=(LSp, τ0p,j), (51)

    for all p P, j Z.

    Let Qp,k = lpPp,k be the generating elements (44) of the Banach -probability space LSp(j) of (51), for p P, k Z. Then the "j-th" generating element Qp,j satisfies the p2(j+1)-semicircularity:

    k0,p,jn(Qp,j, ..., Qp,j) = {p2(j+1)if n=20otherwise, (52)

    and

    τ0p,j(Qnp,j) = ωn (p2(j+1))n2cn2,

    for all p P, j Z, for all n N, by (49) and (50).

    By (51), we have the family

    {LSp(j)=(LSp, τ0p,j):pP, jZ}

    of (non-traditional) Banach -probability spaces.

    From this family, one can define the (traditional) free product Banach -probability space,

    (LS, τ0)def=pP, jZLSp(j),=(pP, jZLSp, pP, jZτ0p,j) (53)

    in the sense of [29], [30], [33] and [35].

    The structures LSp(j) of (51) are the free blocks of this free product -probability space (LS, τ0) of (53). Note that the structure (53) is a well-determined (traditional) noncommutative Banach -probability space.

    Definition 8.1. The Banach -probability space LS denote= (LS, τ0) of (53) is called the free Adelic filterization.

    Let LS be the free Adelic filterization. Then, we obtain a subset

    Q={Qp,j=lpPp,jLSp(j)}pP, jZ (54)

    of LS, consisting of p2(j+1)-semicircular elements Qp,j in the free blocks LSp(j) of LS, for all p P, j Z.

    Remark here that, by the choice of Qp,j in the family Q of (54), all entries Qp,j are taken from the mutually-distinct free blocks LSp(j) of LS, for all p P, j Z. It means that all elements Qp,j of Q are mutually free from each other in the free Adelic filterization LS.

    Theorem 8.1. Let Qp,j Q in the free Adelic filterization LS of (53), where Q is the family (54), for p P, j Z. Then the operators

    Θp,j=1pj+1Qp,jLS (55)

    satisfy

    τ0(Θnp,j)=ωncn2, (56)

    and

    k0n(Θp,j, Θp,j, ..., Θp,jn-times) = {1if  n=20  otherwise,

    for all n N, where k0n(...) is the free cumulant on LS in terms of τ0. Equivalently, the operators Θp,j of (55) are semicircular in LS, for all p P, j Z.

    Proof. Let Θp,j = 1pj+1Qp,j be in the sense of (55), where Qp,j Q, for all p P, j Z, in the free Adelic filterization LS, where Q is the family (54). Since Qp,j are contained in the mutually distinct free blocks LSp(j) of LS, the operators Θnp,j are contained in LSp(j) in LS, for all n N, as free reduced words with their length-1. Thus, one has that

    τ0(Θnp,j)=τ0p,j(Θnp,j)=τ0p,j(1pn(j+1)Qnp,j)=(1pj+1)nτ0p,j(Qnp,j)=(1pj+1)n(ωnpn(j+1)cn2)

    by the p2(j+1)-semicircularity of Qp,j Q in LSp(j)

    =ωncn2, (57)

    for all n N. Therefore, by (29) and (30), the operators Θp,j are semicircular in LS, for all p P, j Z.

    Also, by (31) and (57), one obtains the free cumulant formula in (56) by the Möbius inversion of [29] and [30].

    The above theorem shows that, from the family Q of (54) consisting of p2(j+1)-semicircular elements Qp,j LSp(j), one can construct the corresponding semicircular elements Θp,j of (55) in the free Adelic filterization LS, for all p P, j Z, by (57). Let

    X={Θp,jLSp(j)|pP, jZ}. (58)

    Recall that a subset S = {at}tΔ of an arbitrary -probability space (B, φB) is said to be a free family, if all elements at S are free from each other in (B, φB) (e.g., [33] and [35]).

    Definition 8.2. Let S = {at}tΔ be a free family in a -probability space (B, φB). This family S is said to be a free semicircular family, if every element at of S is semicircular, for all t Δ. Similarly, the family S is called a free weighted-semicircular family, if all elements at of S are weighted-semicircular, for all t Δ.

    So, we obtain the following result.

    Theorem 8.2. Let LS be the free Adelic filterization (53).

    (59)    The family Q of (54) is a free weighted-semicircular family in LS.

    (60)    The family X of (58) is a free semicircular family in LS.

    Proof. The proofs of (59) and (60) are done by (52), (53), (54), (56) and (58). See [8] for details.

    Let LS be the free Adelic filterization (53), and let Q be the free weighted-semicircular family (59), and X, the free semicircular family (60) in LS. We now focus on the Banach -subalgebra LS of LS generated by the free family Q,

    LSdef=¯C[Q]LS, (61)

    where ¯X are the Banach-topology closures of subsets X of LS.

    By (61), we obtain the corresponding Banach -probability space,

    LSdenote=(LS, τ0), (62)

    as a free-probabilistic sub-structure of the free Adelic filterization LS, where τ0 is the restricted linear functional τ0LS on LS.

    Definition 8.3. Let LS = (LS, τ0) be the Banach -probability space (62) in the free Adelic filterization LS of (53). Then it is called the (free-)semicircular Adelic filterization (of LS, generated by the free semicircular family X of (59)).

    Let LS be the semicircular Adelic filterization (62). Then it satisfies the following structure theorem.

    Theorem 8.3. Let LS be the semicircular Adelic filterization (62) of the free Adelic filterization LS. Then the Banach -algebra LS satisfies that

    LS-iso=pP, jZ(¯C[{Θp,j}])-iso=¯C[pP,jZ{Θp,j}], (63)

    in LS, where the free product () in the first isomorphic relation of (63) means the free-probability-theoretic free product of [12] and [14] (with respect to the linear functional τ0 of (62)), and the free product () in the second isomorphic relation of (63) means the pure-algebraic free product inducing "finite" noncommutative free words in the free semicircular family Θ.

    Proof. By the definition (62) of our semicircular Adelic filterization LS, we have

    LS-iso=pP, jZ(¯C[{Θp,j}])-iso=¯C[pP,jZ{Θp,j}], (64)

    since X is a free family in LS, equivalently, since Qp,j are contained in the mutually distinct free blocks LSp(j) of LS, for all p P, j Z.

    Note that, every p2(j+1)-semicircular element Qp,j X of LS is identified with

    Qp,j=pj+1Θp,j,  for  all  pP,jZ,

    and hence, the free blocks ¯C[{Qp,j}] of (64) generating the semicircular Adelic filterization LS are identical to

    ¯C[{Qp,j}]=¯C[{pj+1Θp,j}]=¯C[{Θp,j}], (64')

    for all p P, j Z.

    Therefore, by (64), the first -isomorphic relation of (63) holds.

    Also, by (64), all elements T of LS are the limits of linear combinations of noncommutative free reduced words in X, under Banach-topology for LS. Since all noncommutative free words in X have their unique free-reduced-word forms in LS (as operators under operator-multiplication on LS), one obtains that

    pP, jZ¯C[{Θp,j}]-iso=¯C[{free words in X}]=¯C[pP, jZ{Θp,j}]. (65)

    Therefore, by (64), (64) and (65), the second -isomorphic relation of (63) holds true, too.

    In the middle of the proof of (63), one can get the set-equality,

    LSdef=¯C[Q]=¯C[X],  in  LS (66)

    Let LS = (LS, τ0) be the semicircular Adelic filterization generated by the free semicircular family X of (60). Let (A, φA) be an arbitrary (traditional) unital C-probability space satisfying

    φA(1A) = 1,

    where 1A is the unit (or the multiplication-identity) of the C -algebra A.

    Define the tensor product Banach -algebra LSA by

    LSAdef=ACLS, (67)

    where C is the tensor product of Banach -algebras.

    On this new Banach -algebra LSA of (67), define a linear functional τA by a linear morphism satisfying that

    τA(aT)=τ0(φA(a)T), (68)

    for all a (A, φA), and T LS (under linearity).

    By the definition (68) of the linear functional τA,

    τA(aT) = τ0(T)φA(a) = φA(a)τ0(T),

    for all a (A, φA), T LS.

    Then the Banach -probability space

    LSAdenote=(LSA, τA) (69)

    is well-defined, where LSA and τA are in the sense of (67), respectively, (68).

    Definition 9.1. Let LSA = (LSA, τA) be the Banach -probability space (69) induced by a fixed unital C-probability space (A, φA) and the semicircular Adelic filterization LS. Then we call LSA, the semicircular A-tensor(-Adelic) filterization (of (A, φA)).

    On the semicircular A-tensor filterization LSA, we obtain the following free distributional data.

    Proposition 9.1. Let Qp,j Q, and Θp,j X in LS, and a (A, φA), inducing

    Tap,j=aQp,j,  and  Xap,j=aΘp,j, (70)

    in the semicircular A-tensor filterization LSA of (69). Then

    τA((Tap,j)n) = (ωnpn(j+1)cn2)φA(an), (71)

    and

    τA((Xap,j)n) = (ωncn2)φA(an),

    for all n N.

    Proof. The proof of the free-distributional data (71) are shown by the weighted-semicircularity on the free weighted-semicircular family Q, and the semicircularity on the free semicircular family X in LS. Indeed, if Tap,j and Xap,j are in the sense of (70), then

    τA((Tap,j)n) = τA(anQnp,j) = φA(an)τ0(Qnp,j),

    and

    τA((Xap,j)n) = τA(anΘnp,j) = φA(an)τ0(Θnp,j),

    for all n N, by (68).

    By the above proposition, we obtain the following free-probabilistic information on the semicircular A-tensor filterization LSA.

    Theorem 9.2. Let LSA = (LSA, τA) be the semicircular A -tensor filterization, and let Tap,j and Xap,j be free random variables (70) in LSA. Suppose a is a self-adjoint operator of (A, φA), satisfying

    φA(a2n)=(φA(a))2n,withφA(a2)C×, (72)

    for all n N. Then Tap,j is (p(j+1)φA(a))2-semicircular, and Xap,j is φA(a)2 -semicircular in LSA.

    Proof. Let a (A, φA) be a self-adjoint free random variable satisfying (72). Then, by the self-adjointness, the operators Tap,j and Xap,j of (70) are self-adjoint in LSA, too. Indeed, one has that

    (Tap,j) = aQp,j = Tap,j,

    and

    (Xap,j) = aΘp,j = Xap,j,

    in LSA.

    Also, we have that

    τA((Tap,j)n)=(ωnpn(j+1)cn2)φA(an)=ωnpn(j+1)φA(a)ncn2=ωn(p2(j+1)φA(a)2)n2cn2, (73)

    and

    τA((Xap,j)n)=(ωncn2)φA(an)=ωnφA(a)ncn2=ωn(φA(a)2)n2cn2,

    for all n N, by (71) and (72).

    Therefore, if a free random variable a (A, φA) satisfies the additional condition (72), then Tap,j is (pj+1φA(a))2-semicircular, and Xap,j is φA(a)2-semicircular in the semicircular A-tensor filterization LSA, by (73).

    The following corollary is a direct consequence of the above theorem.

    Corollary 9.3. Let LSA be the semicircular A-tensor filterization (69) of (A, φA).

    (74)    The operator T1Ap,j in the sense of (70) is p2(j+1) -semicircular in LSA.

    (75)    The operator X1Ap,j in the sense of (70) is semicircular in LSA.

    (76)    If the linear functional φA : A C is a state in the sense that

    φA(a1a2) = φA(a1)φA(a2), a1, a2 A,

    and if a (A, φA) is a self-adjoint free random variable with φA(a) C×, then the operator Tap,j of (70) is (pj+1φA(a))2-semicircular, and the operator Xap,j of (70) is φA(a)2-semicircular in LSA.

    Proof. Let 1A be the unit of (A, φA). Since our fixed C-probability space (A, φA) is unital in the sense that φA(1A) = 1, one has

    φA(1nA) = φA(1A) = 1 = 1n = (φA(1A))n,

    for all n N. Therefore, this self-adjoint free random variable 1A satisfies the condition (72). Thus, by (73), the operator T1Ap,j is p2(j+1)-semicircular, and the operator X1Ap,j is semicircular in LSA. It proves the statements (74) and (75), respectively.

    Assume now that the linear functional φA is a state on A, equivalently, assume φA is a multiplicative linear functional on A. Then, for any self-adjoint free random variable a (A, φA) with φA(a) C×,

    φA(an) = φA(a)n, for all n N.

    So, it satisfies the condition (72). Therefore, the statement (76) holds by (73).

    In the above theorem and corollary, we considered the free-distributional information of the generating operators, on the semicircular A-tensor filterization LSA.

    Theorem 9.4. Let LSA be the semicircular A-tensor filterization (69) of a unital C-probability space (A, φA). Then

    LSA-iso=pP, jZ(AC¯C[{Θp,j}])-iso=pP, jZ¯A[{Θp,j}], (77)

    where ¯Z in the first -isomorphic relation of (77) are the Banach-topology closures of subsets Z of the semicircular Adelic filterization LS, and ¯Y in the second -isomorphic relation of (77) are the Banach-topology closures of subsets Y of LSA, where A[Y] mean the polynomial rings (and hence, algebras, in this case) generated by the subsets Y over A in LSA.

    Proof. By the definition (69) of the semicircular A-tensor filterization LSA,

    LSAdef=ACLS-iso=AC(pP, jZ¯C[{Θp,j}])

    by (63) and (66)

    -iso=pP, jZ(AC¯C[{Θp,j}])-iso=pP, jZ¯A[{Θp,j}]

    (e.g., see [29], [30], [33] and [35]). Therefore, the free-structure theorem (77) holds.

    As corollary, one obtains the following structure theorems.

    Corollary 9.5. Let LSA be the semicircular A-tensor filterization of (A, φA).

    (78)    If A is a direct product C-algebra kΔAk of its C-subalgebras {Ak}kΔ, where is the direct product of C-algebras, and Δ is a countable (finite, or infinite) index set, then

    LSA-iso=CkΔ(pP, jZ¯Ak[{Θp,j}])-iso=pP, jZ(CkΔ¯Ak[{Θp,j}]),

    where C is the direct product of Banach -algebras.

    (79)    If A is a tensor product C-algebra kΔAk of its C-subalgebras {Ak}kΔ, where is the tensor product of C-algebras, then

    LSA-iso=CkΔ(pP, jZ¯Ak[{Θp,j}])-iso=pP, jZ(CkΔ¯Ak[{Θp,j}]),

    where C is the tensor product of Banach -algebras.

    (80)    Let (A, φA) be the fixed unital C-probability space. For the linear functional φA, assume that the C -algebra A is a free product C-algebra of its C-subalgebras {Ak}kΔ. Then

    LSA-iso=kΔ, pP, jZ¯Ak[{Θp,j}].

    Proof. The proofs of the statements (78), (79) and (80) are done by (77). Indeed, one has that: if A = kΔAk, then

    ¯A[{Θp,j}]-iso=¯(kΔAk)[{Θp,j}]-iso=¯CkΔ(Ak[{Θp,j}])= CkΔ¯Ak[{Θp,j}],

    for all p P, j Z.

    Similarly, if A = kΔAk, then

    ¯A[{Θp,j}] -iso= CkΔ¯Ak[{Θp,j}];

    and if A = kΔAk, then

    ¯A[{Θp,j}] -iso= kΔ¯Ak[{Θp,j}],

    for all p P, j Z.

    Our results of this section illustrate that the free probability on LSA is characterized by the both free probability on (A, φA), and that on the semicircular Adelic filterization LS. In particular, such a characterization is analyzed by the formula (71), and the structure theorem (77).

    Throughout this section, we fix a unital C-probability space (A, φA), and the corresponding semicircular A-tensor filterization LSA = (LSA, τA) of (A, φA). Also, let

    Xap,j=aΘp,j (81)

    be free random variables (70), generating LSA, for all a (A, φA), and Θp,j X LS, where LS is the semicircular Adelic filterization and X is the free semicircular family (60). Indeed, all operators Xap,j formed by (81) generate LSA, by (63) and (66).

    Define a subset XA of LSA by

    XAdef={Xap,jLSA:Xap,j}isinthesenseof(81). (82)

    Then, as we discussed above this subset XA of (82) generates LSA, i.e.,

    LSA=¯C[XA], (83)

    set-theoretically, by (63), (66) and (67).

    Suppose a given C-algebra A is generated by a subset B of A, i.e., by (83), if

    A=¯C[B]A,

    where ¯YA mean the C-topology closures of subsets Y of A, then one can re-define the generator set XA of (82) by

    XA = {Xap,j LSA : a B, Θp,j X}.

    However, now, we take a C-algebra A arbitrarily. So, in the following text, we understand the generator set XA of LSA as in the general sense of (82).

    In this section, we consider how our free-distributional data on LSA are affected (or distorted) by certain shift processes on the set P of all primes.

    Let P be the set of all primes in N. Note that the set P is a totally ordered set (or, in short, TOset) under the usual inequality (). So, one can index P orderly by

    P = {p1 p2 p3 p4 } (84)

    with

    p1=2,p2=3,p3=5,p4=7,p5=11,...,  etc..

    From below, the set P is understood as the TOset (84).

    Define now an injective functional g : P P by

    g(pk)=pk+1,  for  all  kN. (85)

    For the injection g of (85), we define gn : P P by

    gn=ggggn-times, (86)

    with axiomatization:

    g0=idP,theidentitymaponP,

    for all n N0, where () is the usual functional composition.

    By (86), clearly, g1 = g, in the sense of (85), and

    gn(pk)=pk+n  in  P,  for  all  kN,

    for all n N0. For example,

    g(2)=3,g2(3)=7,g5(5)=19, etc..

    Definition 10.1. Let gn be in the sense of (86) for all n N0. Then these functions gn on P are said to be n-shifts on P, for all n N0. In particular, the 1-shift g = g1 of (85) is simply called the shift on P.

    Let LSA be our semicircular A-tensor filterization, and let g be the shift (85) on the TOset P of (84), inducing the n-shifts gn of (86) on P. Define a - homomorphism GA on LSA by a bounded "multiplicative" linear transformation satisfying

    GA(Xap,j)=Xag(p),j=aΘg(p),j, (87)

    for all Xap,j XA, where XA is the generator set (82) of LSA, where g = g1 is the shift (85) on P.

    By the multiplicativity, the morphism GA of (87) satisfies that: if

    S = NΠl=1(Xalpl,jl)nl,

    in LSA, for n1,..., nN N, as a free reduced words with its length-N (in the sense of (77)) for N N, then

    GA(S)=GA(NΠl=1(Xalpl,jl)nl)=NΠl=1GA((Xalpl,jl)nl)

    by the multiplicativity of GA

    =NΠl=1(GA(Xalpl,jl))nl

    by the multiplicativity of GA

    =NΠl=1(Xalg(pl),jl)nl=NΠl=1(alΘg(pl),jl)nl

    by (87)

    =NΠl=1(anlΘnlg(pl),jl),

    i.e.,

    GA(S)=NΠl=1(Xalg(pl),jl)nl, (88)

    in LSA.

    Also, this morphism GA of (87) satisfies that

    GA(S)=GA(NΠl=1XaNl+1pNl+1,jNl+1)

    because

    (Xap,j)=(aΘp,j)=aΘp,j=Xap,j, (89)

    in LSA, for all Xap,j XA, and hence, the above formula goes to

    =NΠl=1XaNl+1g(pNl+1), jNl+1=(NΠl=1Xalg(pl),jl)

    by (88)

    =(GA(S)), (90)

    by (89).

    By (88) and (90), one can verify that, for all T LSA,

    GA(T)=GA(T),inLSA. (91)

    Proposition 10.1. Let GA be the multiplicative linear transformation (87) on LSA. Then it is a -homomorphism on LSA.

    Proof. The proof is done by (91). i.e., this multiplicative linear transformation GA preserves adjoints in the sense of (91). Thus, it is a well-defined -homomorphism on LSA.

    For the -homomorphism GA of (87), one can have the iterated products (or compositions) GnA of (n-copies of) GA, as -homomorphisms on LSA, with G1A = GA, for all n N0, with axiomatization:

    G0A=1LSA,theidentityoperatoronLSA,

    satisfying

    G0A(Xap,j) = Xag0(p), j = Xap,j = 1LS(Xap,j),

    for all Xap,j XA in LSA, where XA is the generator set (82) of LSA.

    Then it is not difficult to check that GnA satisfy

    GnA(Xap,j)=Xagn(p), jinLS,nN0, (92)

    for all Xap,j XA LSA.

    Definition 10.2. The -homomorphism GA of (87) on the semicircular A-tensor filterization LSA is called the prime-shift (-homomorphism) on LSA. Also, the n-th powers GnA of (92) are called the n-prime-shift(--homomorphism)s on LSA, for all n N0.

    Based on our n-prime-shifts (92), we obtain the following free-distributional data.

    Theorem 10.2. Let Xap,j XA be a generating operator of LSA, and let GnA be the n-prime-shift on LSA, for n N0. Then

    τA((GnA(Xap,j))k)=(ωkck2)φA(ak)=τA((Xap,j)k), (93)

    for all k N.

    Proof. Let Xap,j XA in LSA, for a (A, φA), p P, and j Z. Then

    GnA(Xap,j) = Xagn(p),j = aΘgn(p),j LSA,

    for any n N0. Thus,

    (GnA(Xap,j))k=(aΘgn(p),j)k=akΘkgn(p),j, (94)

    for all k N.

    So, one has that

    τA((GnA(Xap,j))k)=τA((Xagn(p),j)k)

    by (94)

    =φA(ak)τ0(Θkgn(p),j)=φA(ak)(ωkck2), (95)

    by (71), for all k N.

    Therefore, the first equality of (93) holds by (95), and the second equality of (93) holds by (71).

    By the above theorem, one can get the following result.

    Corollary 10.3. Let a (A, φA) be a self-adjoint free random variable, and let Xap,j XA be a generating operator (81) of LSA. Let GnA be the n-prime shifts (92) on LSA, for n N0. Then the free distribution of Xap,j and the free distributions of GnA(Xap,j) are identical in LSA, for all n N0.

    Proof. Let a (A, φA) be given as above. Then, by the self-adjointness of a, the corresponding generating operator Xap,j is self-adjoint in LSA, too. Indeed,

    (Xap,j) = aΘp,j = Xap,j in LSA.

    Note now that, since GnA(Xap,j) = Xagn(p),j,

    (GnA(XAp,j)) = aΘgn(p),j = Xagn(p),j = GnA(XAp,j),

    in LSA, for all n N0. Therefore, the images GnA(Xap,j) of our n-prime shifts GnA preserve the self-adjointness of Xap,j in LSA, for all n N0.

    Recall that the free distributions of self-adjoint operators are characterized by the free-moment sequence. So, the free distribution of Xap,j is characterized by

    (τA((Xap,j)k))k=1 = (ωkck2φA(ak))k=1,

    by (71).

    Also, the free distributions of GnA(Xap,j) are characterized by

    (τA((GnA(Xap,j))k))k=1 = (τA((Xap,j)k))k=1,

    by the self-adjointness of them, and by (93), for all n N0.

    It shows that the free distributions of GnA(Xap,j) are all identically characterized by the free-moment sequence,

    (0, c1φA(a2), 0, c2φA(a4), 0, c3φA(a6), ....),

    for all n N0.

    Let's generalize the above corollary. In fact, the free-distributional formula (93) guarantees that the free distributions of the generators Xap,j XA are preserved by the n-prime shifts GnA on LSA, for all n N0, since, even though a is not self-adjoint in A, one can have

    τA((GnA(Xap,j))k) = τA((Xap,j)k), (96)

    and

    τA(((GnA(Xap,j)))k)=τA((GnA(Xap,j))k)=τA((Xap,j)k)=τA(((Xap,j))k),

    for all k N, because

    (Xap,j) = aΘp,j = Xap,j in XA,

    in LSA.

    Therefore, one can verify that

    τA((GnA(Xar1p,j))(GnA(Xar2p,j))...(GnA(Xarkp,j)))=τA((Xar1gn(p),j)(Xar2gn(p),j)...(Xarkgn(p),j))=τA((ar1ar2...ark)Θkgn(p),j)=φA(ar1ar2...ark)τ0(Θkgn(p),j)=(ωkck2)φA(ar1ar2...ark)

    by (71)

    =φA(ar1ar2...ark)τ0(Θkp,j)=τA(Xar1p,jXar2p,j...Xarkp,j), (97)

    by (71), for all (r1,..., rk) {1, }k, for all k N.

    Therefore, one obtains the following theorem.

    Theorem 10.4. Let Xap,j XA be a generating operator of the semicircular A-tensor filterization LSA, where a (A, φA) is arbitrarily given, and let GnA be the n-prime shifts on LSA, for all n N0. Then the free distribution of Xap,j and the free distributions of GnA(Xap,j) are identically same in LSA, for all n N0. i.e.,

    (98)    the free distribution of GnA(Xap,j) = the free distribution of Xap,j,

    in LSA, for all n N0.

    Proof. Let a (A, φA) be self-adjoint, and hence, Xap,j XA, a self-adjoint generating operator of LSA. Then, by the above corollary, the free distribution of Xap,j and those of GnA(Xap,j) are identical in LSA, for all n N0.

    Assume now that a is not self-adjoint in A. Then the corresponding operator Xap,j is not self-adjoint too, since

    (Xap,j) = Xap,j Xap,j in LSA.

    It also shows that

    GnA(Xp,j) = (Xagn(p),j) = Xagn(p),j Xagn(p),j = GnA(Xp,j),

    in LSA, for all n N0.

    So, the free distribution of X denote= Xap,j is characterized by the "joint" free moments,

    {τA(Xr1Xr2...Xrk)|(r1,...,rk){1,}k,for all kN},

    and similarly, the free distributions of X(n) denote= GnA(Xap,j) are characterized by the joint free moments,

    {τA(Xr1(n)Xt2(n)...Xrk(n))|(r1,...,rk){1,}k,for all kN},

    since X(n) are not self-adjoint in LSA, for all n N0.

    However, by (96) and (97), one has that

    τA(Xr1(n)Xr2(n)...Xrk(n)) = τA(Xr1Xr2...Xrk),

    for all (r1,..., rk) {1, }, for all k N, for any n N0.

    Therefore, the free distributions of X(n) are identically same with the free distribution of X in LSA, for all n N0.

    The above theorem shows that the n-prime shifts GnA preserve the free probability on the semicircular A-tensor filterization LSA, for all n N0.

    Corollary 10.5. The -homomorphisms, the n-prime shifts, GnA preserve the free probability on LSA, for all n N0.

    Proof. Note that all elements T of LSA are the limits of linear combinations of free reduced words in the generator set XA of LSA, by (77). And, by (98), the free distributions for GnA(XA) are identical to those for XA in LSA, for all n N0. Therefore, the free distributions for

    GnA(free words in XA)

    are identical to those for free words in XA, by (88) and (90), in LSA, for all n N0.

    It guarantees that free distribution of every element T is identical to the free distribution of GnA(T), for all T LSA, for all n N0. Equivalently, the free probability on LSA is preserved by the actions of n-prime shifts {GnA}nN0.

    In this section, motivated by the main results (93) and (98) of Section 10.2, we consider free-homomorphic relations on our semicircular A-tensor filterization LSA under n-prime shifts GnA, for n N0.

    Definition 10.3. Let (B1, φ1), and (B2, φ2) be topological -probability spaces. Suppose there exists a bounded -homomorphism Φ : B1 B2, and assume that

    φ2(Φ(b))=φ1(b),   for   all   bB1. (99)

    Then the topological -probability space (B1, φ1) is said to be free-homomorphic to (B2, φ2). In particular, a -homomorphism Φ is called a free-(-)homomorphism from (B1, φ1) to (B2, φ2).

    If Φ is a -isomorphism satisfying (99), then (B1, φ1) is said to be free-isomorphic to (B2, φ2). In such a case, this -isomorphism Φ is called a free-(-)isomorphism.

    By the above free-homomorphic relation (99), one can get the following result.

    Theorem 10.6. Let LSA be the semicircular A-tensor filterization of (A, φA). Then

    (100)    the n-prime shifts GnA are free-homomorphisms on LSA, n N0.

    Proof. For any arbitrarily fixed n N0, take the n -prime shift GnA on LSA. Then, by (93) and (98), for any free reduced words W of LSA in the generator set XA, the free distributions of GnA(W) are identical to the free distribution of W in LSA. Thus, the -homomorphisms GnA preserve the free probability on LSA, for all n N0, i.e., the statement (100) holds true.

    Throughout this section, fix a unital C-probability space (A, φA), and the corresponding semicircular A-tensor filterization LSA = (LSA, τA) of (A, φA). In Section 10, we defined the n-prime shifts GnA of (92), which are the -homomorphism on LSA, and showed that they are free-homomorphisms on LSA, for all n N0, by (100).

    In this section, we consider certain shifting processes h± on Z, and the corresponding -homomorphisms β± on LSA.

    Let Z be the set of all integers as usual. Define functions h+ and h on Z by the bijections on Z,

    h+(j)=j+1,andh(j)=j1, (101)

    for all j Z. By the definition (101), one can have

    h+h=idZ=hh+, (102)

    where idZ is the identity map on Z.

    Definition 11.1. Let h± be the bijections (101) satisfying (102). Then we call h±, the (±)-shifts on Z.

    Let h± be the (±)-shifts (101) on Z. Define the functions hn± on Z by

    hn±=h±h± h±n-times, (103)

    for all n N0, with axiomatization:

    h0± = idZ on Z,

    satisfying

    h0+(j)=j=h0(j),  for  all  jZ.

    Definition 11.2. Let hn± be in the sense of (103), for all n N0, where h± are the (±)-shifts (102) on Z. Then they are called the n-(±)-shifts on Z, for all n N0.

    By (101) and (103), the n-(±)-shifts hn± satisfy

    hn+(j)=j+n,  for  all  jZ, (104)

    and

    hn(j)=jn,  for  all  jZ,

    for all n N0. Also, by (102), one has

    hn+hn=idZ=hnhn+,nN0. (105)

    Let hn± be the n-(±)-shifts (103) on Z, satisfying (104) and (105), for n N0. We now define "multiplicative" linear transformations βn+ and βn on the semicircular A-tensor filterization LSA by the morphisms satisfying

    βn+(Xap,j)=Xap,hn+(j)=Xap,j+n, (106)

    and

    βn(Xap,j) = Xap,hn(j) = Xap,jn,

    with

    β0±(Xap,j) = Xap,h0±(j) = Xap,j = 1LSA(Xap,j),

    for all Xap,j XA, for all n N0, where XA is the generator set (82) of LSA (by (77)).

    By the multiplicativity of the morphisms βn± of (106) on LSA, if

    T = NΠl=1(Xalpl,jl)nl LSA, for n1, ..., nN N,

    is a free reduced word with its length-N (in the sense of (77)), for Xalpl,jl XA, for l = 1,..., N, for N N, then

    βn±(T)=βn±(NΠl=1(Xalpl,jl)nl)=NΠl=1βn±((Xalpl,jl)nl)=NΠl=1(βn±(Xalpl,jl))nl

    by the multiplicativity of βn±

    =NΠl=1(Xalpl,hn±(jl))nl=NΠl=1(Xalpl,jl±n)nl, (107)

    in LSA, for all n N0. Also, the morphisms βn± satisfy

    βn±((Xap,j))=βn±(Xap,j)=Xap,j±n=(Xap,j±n)=(βn±(Xap,j)), (108)

    for all Xap,j XA, in LSA, for all n N0.

    So, by (107) and (108), if W is a free reduced word of LSA in XA, then

    βn±(W) = (βn±(W)),

    implying that

    βn±(T)=(βn±(T)),forallTLSA, (109)

    for all n N0.

    Proposition 11.1. Let βn± be the n-(±)-integer shifts on LSA, for n N0. Then they are -isomorphisms on LSA.

    Proof. Note that the n-(±)-shifts hn± are bijections on Z, for n N0. So, the restrictions βn±XA of our n-(±)-integer shifts (106) are bijections on the generator set XA, for n N0. Therefore, these morphisms βn± of (106) are bijective on LSA, because of the generator-preserving property, for all n N0. Moreover, by (107) and (109), these multiplicative linear transformations βn± are -homomorphisms on LSA, and hence, they are -isomorphisms on LSA, for all n N0.

    Definition 11.3. We call the -homomorphisms βn± of (106), the n-(±)-integer-shifts on LSA, for all n N0. If n = 1 in N0, we simply call β± = β1±, the (±)-integer-shifts on LS.

    The above proposition shows a difference between our prime-shifts, and the integer-shifts on LSA.

    Remark 11.1. Note that our n-prime shifts GnA are injective -homomorphisms, but not -isomorphisms in general. In particular, if n 0 in N0, then they are not -isomorphisms on LSA. It is easily verified because the n-shifts gn of (86) are injective but not bijective on the TOset P of (84), whenever n 0 in N0. It also shows that GnA are free-homomorphisms, but not free-isomorphisms on LSA, in (100), for all n 0 in N0.

    Now, consider how our n-(±)-integer shifts βn± affect the free probability on LSA, for n N0.

    Theorem 11.2. Let n N0, and βn±, the corresponding n -(±)-integer shifts on the semicircular A-tensor filterization LSA. Then, for any Xap,j XA, we have

    τA((βn±(Xap,j))k)=ωkck2φA(ak)=τA((Xap,j)k), (110)

    for all k N.

    Proof. Under hypothesis, consider that

    τA((βn±(Xap,j))k)=τA((Xap,j±n)k)

    by (107)

    =φA(ak)τ0(Θkp,j±n)=ωkck2φA(ak)

    by (71)

    =φA(ak)τ0(Θkp,j)=τA((Xap,j)k),

    for all k N, for all n N0.

    Therefore, the free-distributional data (110) is obtained.

    Similar to the proof of (98) and that of (100), we obtain the following theorem by (110).

    Theorem 11.3. Let LSA be the semicircular A-tensor filterization, and let βn± be the n-(±)-integer shifts on LSA, for all n N0. Then

    (111)    βn± are free-isomorphisms on LSA.

    Proof. By (110), the -isomorphisms βn± preserves free distributions of generating operators of LSA, contained in XA. Therefore, by the similar arguments of the proofs of (98) and (100), the free probability on LSA is preserved by the action of βn±, for all n N0.

    In this section, we consider both prime shifts, and integer shifts, which are well-defined free-homomorphisms on the semicircular A-tensor filterization LSA of a fixed unital C-probability space (A, φA). In particular, we showed that the prime shifts are injective free-homomorphisms, and the integer shifts are free-isomorphisms on LSA, by (100), respectively, by (111).

    Now, we consider certain -homomorphisms on LSA induced by both prime shifts and integer shifts. From below, for convenience, we let

    N±0 denote= {±} × N0.

    Now, consider the Cartesian product set P,

    Pdef=P×Z. (112)

    Let gn be the n-shifts on P, and let hke be the k-(e)-shifts on Z, for n N0, and (e,k) N±0, with axiomatization,

    g0=idP,and h0±=idZ.

    Define now shifts on the set P of (112) by

    sn1(e,n2)def=gn1×hn2edenote=(gn1,hn2e), (113)

    for all n1 N0, and (e,n2) N±0. i.e., for any (p, j) P,

    sn1(e,n2)(p,j) = (gn1(p), hn2e(j)) = (gn1(p), jen2)

    in P, where

    jen2 = {j+n2if e=+jn2if e=.

    For example,

    s2(,5)(3, 1) = (g2(3), h5(1)) = (7, 6)

    in P.

    Definition 12.1. Let sn1(e,n2) be injections (113) on the set P of (112), for n1 N0, and (e,n2) N±0, with identity,

    s0(e,0) = idP×idZ = idP,

    where idP is the identity map on P, satisfying

    idP(p,j)=(p, j)  in  P,  for  all  (p,j)P.

    Then these injections sn1(e,n2) are called the shift(-function)s on P.

    Let P be the Cartesian product set (112), and let sn1(e,n2) be shifts (113) on P. Then, for such a shift sn1(e,n2), one can construct the corresponding -homomorphism σn1(e,n2) on the semicircular A-tensor filterization LSA, defined by the bounded multiplicative linear transformation on LSA,

    σn1(e,n2)=Gn1Aβn2e on  LSA, (114)

    for all n1 N0, and (e,n2) N±0, where Gn1 are the n1-prime shifts, and βn2e are n2-(e)-integer shifts on LSA.

    Notation and Assumption. From below, for convenience, we simply write our n-prime shifts GnA simply by Gn, for all n N0.

    Since Gn1 are -homomorphisms, and βn2e are -isomorphisms on LSA, the morphism σn1(e,n2) of (114) are indeed well-defined -homomorphisms on LSA.

    Proposition 12.1. Let σn1(e,n2) be a -homomorphism (114) on LSA. Then

    σn1(e,n2)def=Gn1βn2e=βn2eGn1onLSA, (115)

    for all n1 N0, (e,n2) N±0.

    Proof. By the very definition (114),

    σn1(e,n2)(Xap,j)=Gn1(βn2e(Xap,j))=Gn1(Xap,jen2)=Xagn1(p), jen2=βn2e(Xagn1(p),j)=βn2e(Gn1(Xap,j))=βn2eGn1(Xap,j),

    for all generating operators Xap,j XA.

    Since all elements of LSA are the limits of linear combinations of free reduced words in XA by (77), we have

    σn1(e,n2) def= Gn1βn2e = βn2eGn1 on LSA,

    for all n1 N0, (e, n2) N±0.

    Let Hom(LSA) be the (-) homomorphism semigroup acting on the semicircular A-tensor filterization LSA, consisting of all -homomorphisms on LSA. Define now the subset σ(LSA) of Hom(LSA) by

    σ(LSA)={σn1(e,n2):n1N0,(e,n2)N±0}, (116)

    where σn1(e,n2) are the -homomorphisms (114) on LSA.

    Definition 12.2. We call the -homomorphisms σn1(e,n2) of (114), the prime-integer shift(--homomorphism)s (in short, pi-shifts) on LSA.

    Now, let's consider the following structure theorem of the system σ(LSA) of (116) in the homomorphism semigroup Hom(LSA).

    Theorem 12.2. Let σ(LSA) be the system (116) in Hom(LSA). Then

    (117)     σ(LSA) is a commutative sub-monoid of Hom(LSA).

    Proof. Let σ(LSA) be the subset (116) of Hom(LSA). Then one can obtain that

    σn1(e,n2)σk1(r,k2)=(Gn1βn2e)(Gk1βk2r)

    by (114)

    =(Gn1Gk1)(βn2eβk2r)

    by (115)

    =Gn1+k1β|en2+rk2|sgn(en2+rk2)=σn1+k1sgn(en2+rk2), (118)

    where sgn is the sign map on Z, satisfying

    sgn(j) = {+if j0if j<0,

    for all j Z, and |.| means the absolute value on Z, for all n1,k1,n2,k2 N0, and e, r {±}.

    The formula (118) shows that the product (or composition), inherited from that on Hom(LSA), is closed on the set σ(LSA). Thus, one can consider σ(LSA) as an algebraic sub-structure (σ(LSA), ) in Hom(LSA).

    Observe now that

    (βn1e1βn2e2)βn3e3=β|e1n1+e2n2|sgn(e1n1+e2n2)βn3e3=β||e1n1+e2n2|+e3n3|sgn(e1n1+e2n2+e3n3)=β|e1n1+|e2n2+e3n3||sgn(e1n1+e2n2+e3n3)=βn1e1β|e2n2+e3n3|sgn(e2n2+e3n3)=βn1e1(βn2e2βn3e3), (119)

    on LSA, for (el,nl) N±0, for all l = 1, 2, 3; also, one has

    (Gn1Gn2)Gn3=Gn1+n2Gn3=Gn1+n2+n3=Gn1Gn2+n3=Gn1(Gn2Gn3), (120)

    on LSA, for all n1, n2, n3 N0.

    So, one obtains that

    (σn1(e1,k1)σn2(e2,k2))σn3(e3,k3)=σn1+n2(sgn(e1k1+e2k2),|e1k1+e2k2|)σn3(e3,k3)

    by (118)

    =σ(n1+n2)+n3(sgn(e1k1+e2k2+e3k3), ||e1k1+e2k2|+e3k3|)=σn1+(n2+n3)(sgn(e1k1+e2k2+e3k3),|e1k1+|e2k2+e3k3||)=σn1(e1,k1)σn2+n3(sgn(e2k2+e3k3),|e2k2+e3k3|)=σn1(e1,k1)(σn2(e2,k2) σn3(e3,k3)), (121)

    by (119) and (120), for nl N0, (el, kl) N±0, for all l = 1, 2, 3.

    Thus, the operation () on σ(LSA) is associative by (121), and hence, the algebraic pair (σ(LSA), ) forms a semigroup.

    Definitely, one can take an element

    σ0(e,0)=G0β0e=1LSA1LSA=1LSAσ(LSA), (122)

    satisfying that

    σn(e,k)1LSA = σn(e,k) = 1LSA σn(e,k) in σ(LSA),

    for all n N0, and (e,k) N±0.

    So, the semigroup (σ(LSA), ) contains its ()-identity 1LSA = σ0(e,0) of (122), and hence, it is a well-defined monoid in Hom(LSA).

    Finally, consider that

    Gn1Gn2=Gn1+n2=Gn2+n1=Gn2Gn1, (123)

    and

    βk1e1βk2e2 = β|e1k1e2k2|sgn(e1k1e2k2) = β|e2k2e1k1|sgn(e2k2e1k1) = βk2e2βk1e1,

    on LSA, for all n1, n2 N0, and (e1,k1), (e2,k2) N±0.

    Therefore,

    σn1(e1,k1)σn2(e2,k2)=σn1+n2(sgn(e1k1e2k2),|e1k1e2k2|)=σn2(e2,k2)σn1(e1,k1), (124)

    on LSA, for all n1, n2 N0, and (e1,k1), (e2,k2) N±0, by (115) and (123).

    So, the monoid (σ(LSA), ) is commutative by (124). Therefore, the system σ(LSA) of (116) is a commutative sub-monoid of the homomorphism semigroup Hom(LSA).

    The above structure theorem (117) characterizes the algebraic structure of σ(LSA) as a commutative monoid embedded in Hom(LS).

    Definition 12.3. Let σ(LSA) be a commutative sub-monoid (116) embedded in the homomorphism semigroup Hom(LSA). Then this monoid σ(LSA) is called the prime-integer-shift monoid (in short, the pi-shift monoid) on LSA.

    Let LSA be the fixed semicircular A-tensor filterization of (A, φA), and let σ(LSA) be the pi-shift monoid (116) on LSA, which is a commutative sub-monoid of the homomorphism semigroup Hom(LSA) by (117). In this section, we consider how pi-shift monoid σ(LSA) affects the free-distributional data on LSA.

    Recall-and-note that the prime-shifts Gn are injective free-homomorphisms on LSA, and hence, they preserves the free probability on LSA by (100), for all n N0; and the integer-shifts βne are free-isomorphisms on LSA, and hence, they preserves the free probability on LSA, by (111), for all (e,n) N±0. So, it is not difficult to verify that every pi-shift σn(e,k) σ(LSA) preserves the free probability on LSA, for all n N0 and (e,k) N±0.

    Lemma 12.3. Let σ(LSA) be the pi-shift monoid (116) on the semicircular A-tensor filterization LSA, and let

    σ denote= σn(e,k) σ(LSA), for n N0, (e,k) N±0,

    be a pi-shift on LSA. Then

    τA((σ(Xap,j))l)=ωlcl2φA(al)=τA((Xap,j)l), (125)

    for all l N.

    Proof. Let σ = σn(e,k) σ(LSA) be a pi-shift, for n N0, (e,k) N±0. Then, for any generating operator Xap,j XA of LSA, one has

    σ(Xap,j)l = (Xagn(p),jek)l,

    and hence,

    τA((σ(Xap,j))l)=τA((Xagn(p),jek)l)=φA(al)τ0(Θlgn(p),jek)=ωlcl2φA(al)=φA(al)τ0(Θlp,j)=τA((Xap,j)l),

    for all l N.

    Therefore, the free-distributional data (125) holds.

    By the above lemma, we obtain the following result.

    Theorem 12.4. Let σ(LSA) be the pi-shift monoid on the semicircular A -tensor filterization LSA. Then every pi-shift σ σ(LSA) is a free-homomorphism on LSA.

    Proof. By the similar arguments of the proofs for (100) and (111), all pi-shifts of the pi-shift monoid σ(LSA) are free-homomorphisms on LSA by (125).

    Remark that, by the definition (114), a pi-shift σn(e,k) is not a free-isomorphism on LSA, in general. In particular, if n 0 in N0, then σn(e,k) = Gnβke is not bijective, since Gn is not bijective on LSA, and hence, it cannot be a free-isomorphism.

    Theorem 12.5. Let σn(e,k) σ(LSA) be a pi-shift. Then

    (126)   σn(e,k) is a free-isomorphism, if and only if n = 0 in N0.

    Proof. () Suppose n = 0 in N0. Then

    σn(e,k) = σ0(e,k) = G0βke = 1LSAβke = βke,

    and βke is a free-isomorphism by (111), in σ(LSA).

    () Assume that n 0 in N0. Then, as we discussed in the very above paragraph, σn(e,k) is not a free-isomorphism on LSA.

    Therefore, the characterization (126) holds.

    The above theorem characterizes the free-isomorphic property in the pi-shift monoid σ(LSA).

    By the above two theorems, a pi shift σn(e,k) σ(LSA) is either a free-homomorphism (if n 0), or a free-isomorphism (if n = 0) on the semicircular A-tensor filterization LSA, i.e., it preserves the free probability on LSA.

    Let (A, φA) be a fixed unital C-probability space, and LSA = (LSA, τA), the semicircular A-tensor filterization of (A, φA), and let σ(LSA) be the pi-shift monoid on LSA. By the main results of Section 12, all elements of σ(LSA) are free-homomorphisms in the homomorphism semigroup Hom(LSA). In this section, we generalize the pi-shift monoid σ(LSA) by acting the homomorphism semigroup Hom(A) of the C-algebra A, and construct a new subset σA(LSA) of Hom(LSA). We study how such a subset σA(LSA) acts on (the free probability on) LSA.

    Let Hom(A) be the homomorphism semigroup of A, consisting of all -homomorphisms on the C-algebra A, where (A, φA) is our fixed unital C-probability space. Let θ Hom(A), and σn(e,k) σ(LSA), for n N0, (e,k) N±0. Define a -homomorphism σn:θ(e,k) on LSA by the morphism satisfying

    σn:θ(e,k)(Xap,j)=σn:θ(e,k)(aΘp,j)def=σn(e,k)(θ(a)Θp,j)=σn(e,k)(Xθ(a)p,j)=Xθ(a)gn(p),jek, (127)

    for all Xap,j XA in LSA, where XA is the generator set (82) of LSA.

    Let Xalpl,jl XA in LSA, for l = 1, 2. Then, for the morphism σn:θ(e,k) of (127), one obtains that

    σn:θ(e,k)(Xa1p1,j1Xa2p2,j2)=σn:θ(e,k)(a1a2Θp1,j1Θp2,j2)={σn:θ(e,k)(a1a2Θp1,j1Θp2,j2)if (p1,j1)(p2,j2) in Pσn:θ(a1a2Θ2p1,j1)if (p1,j1)=(p2,j2) in P={θ(a1a2)Θgn(p1),j1ekΘgn(p2),j2ekif (p1,j1)(p2,j2)θ(a1a2)Θ2gn(p1),j1ekif (p1,j1)=(p2,j2)

    by (127)

    ={θ(a1)θ(a2)Θgn(p1),j1ekΘgn(p2),j2ekresp.,θ(a1)θ(a2)Θgn(p1),j1ekΘgn(p1),j1ek

    since θ Hom(A)

    =(θ(a1)Θgn(p1),j1ek)(θ(a2)Θgn(p2),j2ek)=(Xθ(a1)gn(p1),j1ek)(Xθ(a2)gn(p2),j2ek)=(σn:θ(e,k)(Xap1,j1))(σn:θ(e,k)(Xap2,j2)),

    implying that

    σn:θ(e,k)(T1T2)=(σn:θ(e,k)(T1))(σn:θ(e,k)(T2)) (128)

    in LSA, for all T1, T2 LSA.

    Also, we have, for any Xap,j XA,

    σn:θ(e,k)((Xap,j))=σn:θ(e,k)(Xap,j)=Xθ(a)gn(p),jek

    by (127)

    =Xθ(a)gn(p),jek=(Xθ(a)gn(p),jek)

    since a Hom(A)

    =(σn:θ(e,k)(Xap,j)),

    implying that

    σn:θ(e,k)(T)=(σn:θ(e,k)(T)), (129)

    for all T LSA.

    Therefore, the morphism σn:θ(e,k) of (127) is indeed a well-defined -homomorphism on LSA, by (128) and (129), for any θ Hom(A), and σn(e,k) σ(LSA).

    Define now a subset σA(LSA) of the homomorphism semigroup Hom(LSA) of LSA by

    σA(LSA)={σn:θ(e,k)|σn:θ(e,k) are in the sense of (127),for all θHom(A), andσn(e,k)σ(LSA)}. (130)

    Then one can get the following structure theorem.

    Theorem 13.1. Let σA(LSA) be the subset (130) of Hom(LSA). Then

    (131)     σA(LSA) is a noncommutative monoid, in general.

    Moreover, σA(LSA) becomes a commutative sub-monoid of Hom(LSA), if and only if the C-algebra A is commutative.

    Proof. Let σA(LSA) be the subset (130) of Hom(LSA). Take

    σldenote=σnl:θl(el,kl)σA(LSA), for  l=1,2.

    Observe that, for any generating operator Xap,j XA of LSA,

    σ1σ2(Xap,j)=σ1(Xθ2(a)gn2(p),je2k2)=Xθ1(θ2(a))gn1(gn2(p)),je2k2e1k1=Xθ1θ2(a)gn1+n2(p), j(sgn(je1k1e2k2)+)|e1k1e2k2| (132)

    by (132). Indeed, note that if βklel are the kl-(el)-integer shifts (106) on LSA, for (el,kl) N±0, for l = 1, 2, then

    βk1e1βk2e2=β|e1k1e2k2|sgn(e1k1e2k2)=βk2e2βk1e1 on  LSA,

    because

    βk1e1βk2e2(Xap,j)=βk1e1(Xap,je2k2)=Xap,je2k2e1k1=β|e2k2e1k1|sgn(e2k2e1k1)(Xap,j)=β|e1k1e2k2|sgn(e1k1e2k2)(Xap,j)=βk2e2βk1e1(Xap,j), (133)

    for all Xap,j XA, in LSA.

    So, the formula (132) holds by (133). It shows that

    σ1σ2=σ(n1+n2):θ1θ2(sgn(e1k1e2k2), |e1k1e2k2|)σA(LSA), (134)

    too.

    Therefore, under the inherited product, the algebraic pair (σA(LSA), ) is a well-determined algebraic sub-structure of Hom(LSA). Now, let σ1 and σ2 be given as above in σA(LSA), and let

    σ3 = σn3:θ3(e3,k3) σA(LSA).

    Then

    (σ1σ2)σ3=(σ(n1+n2):θ1θ2(sgn(e1k1e2k2), |e1k1e2k2|))σ3

    by (134)

    =σ(n1+n2)+n3:(θ1θ2)θ3(sgn((e1k1e2k2)e3k3),|(e1k1e2k2)e3k3|)

    by (134)

    =σn1+(n2+n3):θ1(θ2θ3)(sgn(e1k1(e2k2e3k3)), |e1k1(e2k2e3k3)|)=σ1(σ(n2+n3):θ2θ3(sgn(e2k2e3k3), |e2k2e3k3|))=σ1(σ2σ3). (135)

    By (135), the algebraic pair (σA(LS), ) forms a semigroup in Hom(LSA).

    Let 1A Hom(A) be the identity map on A, which is a -isomorphism on A. Take σ0:1A(e,0) in σA(LSA). Then

    σ0:1A(e,0)=1LSA,theidentitymaponLSA, (136)

    which is a -isomorphism in Hom(LSA), satisfying that

    σ1LSA = σ = 1LSAσ, σ σA(LSA).

    Therefore, by (136), the semigroup (σA(LSA), ) contains the ()-identity, 1LSA = σ0:1A(e,0), and hence, it is a sub-monoid in Hom(LSA). i.e., the statement (131) holds.

    Definitely, by (126), an element σn:1A(e,k) is not bijective on LSA, whenever n 0 in N0. So, the monoid σA(LSA) cannot be a group in Hom(LSA).

    Remark that, homomorphism semigroups are not commutative in general. Since our C-algebra A is arbitrarily chosen, it is natural to understand the corresponding homomorphism semigroup Hom(A) is not commutative, in general. Under this sense, even though the pi-shift monoid σ(LSA) is commutative, the monoid σA(LSA) is not commutative, in general.

    However, by (134) and by the commutativity of our pi-shift monoid σ(LSA), this monoid σA(LSA) can be commutative, if and only if the homomorphism semigroup Hom(A) of A is commutative, if and only if A is a commutative C-algebra.

    The above theorem characterizes the algebraic property of the subset σA(LSA) of (130), as a noncommutative sub-monoid of Hom(LSA) (in general).

    Definition 13.1. Let σA(LSA) be the sub-monoid (130) of Hom(LSA). We call it the A-tensor-pi-shift monoid (acting) on LSA.

    In Section 12, we showed that all pi-shifts in the pi-shift monoid σ(LSA) are free-homomorphisms on LSA, preserving the free probability on the semicircular A-tensor filterization LSA of a fixed unital C-probability space (A, φA). In Section 13.1, we extended the pi-shift monoid σ(LSA) to the A -tensor pi-shift monoid σA(LSA) in the sense of (130); and we showed there that, in general, the algebraic property of σA(LSA) is different from that of σ(LSA) in the homomorphism semigroup Hom(LSA). So, it is natural to consider how the free-distributional data on LSA is affected by the action of σA(LSA).

    First of all, one can immediately obtain the following corollary of (125) and (126).

    Corollary 13.2. Let σ = σn:1A(e,k) σA(LSA), where 1A is the identity -isomorphism in Hom(A). Then σ is a free-homomorphism on LSA. Moreover, σ is a free-isomorphism, if and only if n = 0 in N0.

    Proof. Let σ be given as above in the A-tensor pi-shift monoid σA(LSA). Then, by definition,

    σ(Xap,j) = X1A(a)gn(p),jek = Xagn(p),jek = σn(e,k)(Xap,j),

    for all generating operators Xap,j XA of LSA, where σn(e,k) is the pi-shift contained in the pi-shift monoid σ(LSA) in Hom(LSA). Therefore, we have that

    σ=σn:1A(e,k)=σn(e,k)onLSA. (137)

    Therefore, by (125), σ is a free-homomorphism on LSA; and, by (126), it is a free-isomorphism, if and only if n = 0 in N0.

    By the above corollary, we have the following result.

    Corollary 13.3. Let σ(LSA) be the pi-shift monoid, and let σA(LSA) be the A-tensor pi-shift monoid in the homomorphism semigroup Hom(LSA). Then

    (138)    σ(LSA) is a commutative sub-monoid of σA(LSA), in Hom(LSA).

    Proof. The proof of (138) is done by (137).

    The above corollaries shows that "some" elements of the A-tensor pi-shift monoid σA(LSA) preserve the free probability on LSA, by (137) and (138).

    Lemma 13.4. Let σθ = σn:θ(e,k) σA(LSA), for θ Hom(A). Then

    τA((σθ(Xap,j))l)=(ωlcl2)φA(θ(al))=τA((Xθ(a)p,j)l), (139)

    for all l N.

    Proof. Let σθ be given as above in the A-tensor pi-shift monoid σA(LSA). Then, for any generating operator Xap,j XA of LSA,

    (σθ(Xap,j))l=(Xθ(a)gn(p),jek)l=θ(a)lΘlgn(p),jek=θ(al)Θlgn(p),jek,

    in LSA, for all l N, since θ Hom(A).

    Thus, one obtains that

    τA((σθ(Xap,j))l) = (ωlcl2)φA(θ(al)),

    for all l N, by (125).

    Also, one has that

    τA((Xθ(a)p,j)l) = (ωlcl2)φA(θ(al)),

    for all l N, too.

    Therefore, the free-distributional data (139) holds.

    More general to (137) and (138), we obtain the following result.

    Theorem 13.5. Let fHom(A) be the sub-semigroup of the homomorphism semigroup Hom(A) of the fixed C-algebra A, defined by

    fHom(A)def={θHom(A)|θ is afree-homomorphismon A}, (140)

    Define a subset σfA(LSA) of the A-tensor pi-shift monoid σA(LSA) by

    σfA(LSA)def={σn:θ(e,k)σA(LSA)|θfHom(A)}. (141)

    (142)    σfA(LSA) is a sub-monoid of σA(LSA).

    (143)    All elements of σfA(LSA) are free-homomorphisms on LSA.

    (144)    σn:θ(e,k) σfA(LSA) is a free-isomorphism, if and only if

    n=0,  and  θ  is  bijective  on  A.

    Proof. Let σfA(LSA) be a subset (141) of σA(LSA). Then, for any

    σl = σnl:θl(el,kl) σfA(LSA), for l = 1, 2,

    we have

    σ1σ2=σn1+n2:θ1θ2(sgn(e1k1e2k2), |e1k1e2k2|)let=σ, (145)

    in σA(LSA), by (134).

    Remark that if θ1 and θ2 are free-homomorphisms on A, then

    φA(θ1θ2(x)) = φA(θ1(θ2(x))) = φA(θ2(x)) = φA(x),

    since θ1, θ2 fHom(A), for x (A, φA).

    It shows that if θ1, θ2 fHom(A), then θ1θ2 fHom(A), where fHom(A) is the subset (140) of Hom(A). Therefore, the -homomorphism σ of (145) is also contained in σfA(LSA), too. i.e., σfA(LSA) is a sub-semigroup of the A-tensor pi-shift monoid σA(LSA). It is clear that the identity -isomorphism 1A is contained in fHom(A), and hence, the identity σ0:1A(e,0) = 1LSA is contained in σfA(LSA), too. Thus, σfA(LSA) forms a sub-monoid of σA(LSA). Equivalently, the statement (142) holds.

    Now, let σθ = σn:θ(e,k) σfA(LSA), with θ fHom(A). Then

    τA((σθ(Xap,j))l)=(ωlcl2)φA(θ(al))

    by (139)

    =(ωlcl2)φA(al)=τA((Xap,j)l), (146)

    since θ fHom(A), for all l N, for all Xap,j XA LSA.

    Therefore, every element of the sub-monoid σfA(LSA) preserves the free probability on LSA, i.e., it is a free-homomorphism on LSA, by (146). So, the statement (143) is proven.

    Let σθ be given as above in the sub-monoid σfA(LSA) of the A-tensor pi-shift monoid σA(LSA). If either

    n0inN0,orθisnotbijectiveonA,

    then σθ cannot be a -isomorphism. i.e., it is a free-homomorphism, but not a free-isomorphism on LSA.

    If n = 0, and θ is bijective on A, then θ is a free-isomorphism on A, and hence, σθ is bijective on LSA; and since

    σθ(Xap,j) = σ0:θ(e,k)(Xap,j) = Xθ(a)p,jek,

    we have

    τA((σθ(Xap,j))l)=(ωlcl2)φA(θ(al))=(ωlcl2)φA(al)=τA((Xap,j)l),

    for all l N, for all Xap,j XA LSA, and hence, it is a free-homomorphism on LSA. i.e., if n = 0 in N0, and θ fHom(A) is bijective on A, then σθ is a bijective free-homomorphism, a free-isomorphism, on LSA.

    Therefore, the characterization (144) holds true.

    The above theorem generalizes the free-homomorphic properties (137) and (138) in the A-tensor pi-shift monoid σA(LSA). i.e., there exists the maximal sub-monoid σfA(LSA) of σA(LSA), consisting of free-homomorphisms on LSA (containing the pi-shift monoid σ(LSA)), by (142) and (143). Moreover, we characterize free-isomorphic property of σfA(LSA) by (144).

    Definitely, if one takes an element σ in σA(LSA) σfA(LSA), then it is a -homomorphism in Hom(LSA), but not a free-homomorphism on the semicircular A-tensor filterization LSA. In other words, such a -homomorphism σ distorts the free probability on LSA.



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