In this paper, we study the Banach ∗-probability space (A⊗CLS, 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 A⊗CLS, 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
[1] | Ilwoo Cho . Certain $*$-homomorphisms acting on unital $C^{*}$-probability spaces and semicircular elements induced by $p$-adic number fields over primes $p$. Electronic Research Archive, 2020, 28(2): 739-776. doi: 10.3934/era.2020038 |
[2] | Yifan Luo, Kaisheng Lei, Qingzhong Ji . On the sumsets of units in a ring of matrices over $ \mathbb{Z}/m\mathbb{Z} $. Electronic Research Archive, 2025, 33(3): 1323-1332. doi: 10.3934/era.2025059 |
[3] | Kingshook Biswas, Rudra P. Sarkar . Dynamics of $ L^p $ multipliers on harmonic manifolds. Electronic Research Archive, 2022, 30(8): 3042-3057. doi: 10.3934/era.2022154 |
[4] | Francisco Javier García-Pacheco, María de los Ángeles Moreno-Frías, Marina Murillo-Arcila . On absolutely invertibles. Electronic Research Archive, 2024, 32(12): 6578-6592. doi: 10.3934/era.2024307 |
[5] | Yang Gao, Qingzhong Ji . On the inverse stability of $ z^n+c $. Electronic Research Archive, 2025, 33(3): 1414-1428. doi: 10.3934/era.2025066 |
[6] | Xintao Li, Rongrui Lin, Lianbing She . Periodic measures for a neural field lattice model with state dependent superlinear noise. Electronic Research Archive, 2024, 32(6): 4011-4024. doi: 10.3934/era.2024180 |
[7] | Hai-Liang Wu, Zhi-Wei Sun . Some universal quadratic sums over the integers. Electronic Research Archive, 2019, 27(0): 69-87. doi: 10.3934/era.2019010 |
[8] |
Jorge Garcia Villeda .
A computable formula for the class number of the imaginary quadratic field |
[9] | Yining Yang, Yang Liu, Cao Wen, Hong Li, Jinfeng Wang . Efficient time second-order SCQ formula combined with a mixed element method for a nonlinear time fractional wave model. Electronic Research Archive, 2022, 30(2): 440-458. doi: 10.3934/era.2022023 |
[10] | Jiangtao Zhai, Zihao Wang, Kun Duan, Tao Wang . A novel method for mobile application recognition in encrypted channels. Electronic Research Archive, 2024, 32(1): 193-223. doi: 10.3934/era.2024010 |
In this paper, we study the Banach ∗-probability space (A⊗CLS, 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 A⊗CLS, 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
(A⊗CLS, φA⊗τ0) |
for an arbitrarily fixed unital
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
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
In [8] and [12], we studied weighted-semicircular elements, and
corresponding semicircular elements induced by measurable functions on
In this paper, we are interested in how the (weighted-)semicircular law(s)
on
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
Notation and Assumption. As in the "traditional" free probability
theory, the pairs
For more about
For any fixed
Also, such a Banach field
Qp = (Qp, σ(Qp), μp), |
equipped with the left-and-right additive invariant Haar measure
μp(Zp) = 1, |
where
Zp def= {x ∈ Qp : |x|p ≤ 1} in Qp, |
consisting of all
As a topological space, the
Uk=pkZp={pkx∈Qp:x∈Zp}, | (1) |
for all
By understanding
Mp = C[{χS:S∈σ(Qp)}] |
consisting of
f=∑S∈σ(Qp)tSχS (tS∈C), |
where the sum
On
φp(f)=∫Qpfdμp,∀f∈Mp. | (2) |
Define now subsets
∂k=Uk∖Uk+1,forallk∈Z. | (3) |
We call these
Qp=⊔k∈Z∂k, | (4) |
where
μp(∂k)=μp(Uk)−μp(Uk+1)=1pk−1pk+1, | (5) |
for all
Note that, by (4), if
ΛS={j∈Z:S∩∂j≠∅}. | (6) |
Thus, by (6), one obtains the following proposition.
Proposition 2.1. Let
0≤rj≤1inR, for all j∈ΛS,and φp(χS)=∫QpχS dμp=∑j∈ΛSrj(1pj−1pj+1), | (7) |
where
Proof. The computation (7) is shown by (5). See [8], [9], [10], [11] and [12] for details.
Throughout this section, fix a prime
Let
∂k=Uk∖Uk+1,forallk∈Z. | (8) |
Define a linear functional
φp(f)=∫Qpfdμp,forallf∈Mp. | (9) |
Definition 3.1. The pairs
Then, by (7) and (9), one obtains that
φp(χUj) = 1pj, and φp(χ∂j) = 1pj−1pj+1, |
since
ΛUj = {k ∈ Z : k ≥ j}, and Λ∂j = {j}, |
for all
Proposition 3.1. Let
ΛS1,...,SN = N∩l=1ΛSl in Z, |
where
0≤rj≤1inR,∀j∈ΛS1,...,SN,andφp(NΠl=1χSl)=∑j∈ΛS1,...,SNrj(1pj−1pj+1). | (10) |
Proof. The formula (10) is proven by (7), since
NΠl=1χSl = χN∩l=1Sl in Mp. |
See [8] through [12], for details.
Fix a prime
Hpdef=L2(Qp, σ(Qp), μp)=L2(Qp), | (11) |
over
⟨f1, f2⟩2def=∫Qpf1f∗2dμp, | (12) |
for all
‖f‖2def=√⟨f,f⟩2, for all f∈Hp, | (12') |
where
Definition 4.1. We call the Hilbert space
By the definition (11) of the
αp(f)(h)=fh, for all h∈Hp, | (13) |
for all
αp(f1f2)=αp(f1)αp(f2)onHp,∀f1,f2∈Mp,and(αp(f))∗=α(f∗)onHp,∀f∈Mp. | (14) |
Notation. Denote
Proposition 4.1. The pair
Proof. The proof is done by (14) (e.g., see [8] and [12]).
Definition 4.2. Let
Mpdef=¯αp(Mp)‖.‖=¯C[αpf :f∈Mp]‖.‖ | (15) |
in
Throughout this section, let's fix a prime
φpj(a)def=⟨a(χ∂j), χ∂j⟩2,∀a∈Mp, | (16) |
for all
Definition 5.1. Let
Now, fix
φpj(αpS)=⟨αpS(χ∂j), χ∂j⟩2=μp(S∩∂j)=rS(1pj−1pj+1), | (17) |
by (3.8), for some
Proposition 5.1. Let
φpj((αp∂k)n)=δj,k(1pj−1pj+1), | (18) |
for all
Proof. By (17), one has that
φpj(αp∂k)=δj,k(1pj−1pj+1), for all k∈N. | (19) |
Since
(αp∂k)2 = αp∂k = (αp∂k)∗ in Mp, |
the formula (18) holds by (19), for all
Let
Pp,j=αp∂j∈Mp, | (20) |
induced by boundaries
Definition 6.1. Fix
Sp=C∗({Pp,j}j∈Z)=¯C[{Pp,j}j∈Z] of Mp, | (21) |
where
Every
Proposition 6.1. Let
Sp∗-iso=⊕j∈Z(C⋅Pp,j)∗-iso=C⊕Z, | (22) |
in
Proof. It suffices to show that the generating projections
Pp,j1Pp,j2 = αp(χ∂pj1∩∂pj2) = δj1,j2αp∂pj1 = δj1,j2Pp,j1, |
in
Let
φpj(Pp,k)=δj,k(1pj−1pj+1),∀j,k∈Z | (23) |
by (18).
Let
ϕ : N → C, |
defined by
ϕ(n)=|{k∈N:k≤n, gcd(n,k)=1}|, | (24) |
for all
ϕ(q)=q−1=q(1−1q),∀q∈P, | (25) |
by (24).
So, one can get that
φpj(Pp,j)=1pj(1−1p)=ppj+1(1−1p)=ϕ(p)pj+1, | (26) |
by (23) and (25), for
Motivated by (26), define the new linear functionals
τpj=1ϕ(p)φpjonSp, | (27) |
satisfying that:
τpj(Pp,k) = δj,kϕ(p) φpj(Pp,j) = δj,kpj+1, |
for all
Proposition 7.1. Let
τpj(Pnp,k)=δj,kpj+1,foralln∈N. | (28) |
Proof. The free-moment formula (28) is proven by (27).
Let
Definition 7.1. Let
φ(an)=ωncn2, for all n∈N, | (29) |
where
ωn = {1if n is even0if n is odd, |
for all
ck = 1k+1(2kk) = 1k+1(2k)!(k!)2 = (2k)!k!(k+1)!, |
for all
It is well-known that, if
kn(a, a, ......, a⏟n-times)={1if n=20otherwise, | (30) |
for all
Motivated by (30), one can define so-called the weighted-semicircular elements.
Definition 7.2. Let
kn(a, a, ...., a⏟n-times)={t0if n=20otherwise, | (31) |
for all
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
φ(an)=ωntn20cn2, | (32) |
where
Let
Define now bounded linear transformations
cp(Pp,j)=Pp,j+1, | (33) |
and
ap(Pp,j) = Pp,j−1, |
on
By (33), one can understand
Definition 7.3.
The Banach-space operators
lp=cp+ap on Sp. | (34) |
We call this operator
Let
Lp=¯C[lp] in B(Sp), | (35) |
equipped with the inherited operator-norm
‖T‖=sup{‖Tx‖Sp:x∈Sp s.t. ‖x‖Sp=1}, |
where
‖x‖Sp=sup{‖x(h)‖2:h∈Hp s.t. ‖h‖2=1}, |
is the
On the Banach algebra
∞∑k=0sklkp∈Lp⟼∞∑k=0¯sklkp∈Lp, | (36) |
where
Then the operation (36) is a well-defined adjoint on
Definition 7.4. Let
Let
LSp=Lp⊗CSp, | (37) |
where
Take now a generating element
l0p=1Sp,theidentityoperatorofSp, |
in
Define now a bounded linear morphism
Ep(lkp⊗Pp,j)=(pj+1)k+1[k2]+1lkp(Pp,j), | (38) |
for all
By the cyclicity (35) of the tensor factor
Now, consider how our
cpap(Pp,j) = Pp,j = apcp(Pp,j), |
for all
cpap=1Sp=apcp on Sp. | (39) |
Lemma 7.2. Let
cnpanp=(cpap)n=1Sp=(apcp)n=anpcnp, | (40) |
and
cn1pan2p=an2pcn1p, on Sp, |
for all
Proof. The formulas in (40) holds by (39).
By (40), one can have that
lnp = (cp+ap)n = n∑k=0(nk) ckpan−kp, |
with identity:
c0p = 1Sp = a0p, | (41) |
for all
(nk)=n!k!(n−k)!, for all k≤n∈N0. |
By (41), one obtains the following proposition.
Proposition 7.3.
Let
(42)
(43)
for all
Proof. The proofs of (42) and (43) are done by straightforward computations (41), with help of (40). See [8] for details.
Fix
Qp,j=lp⊗Pp,j∈LSp, | (44) |
for
Qnp,j=(lp⊗Pp,j)n=lnp⊗Pnp,j=lnp⊗Pp,j, | (45) |
for all
By (37) and (45), these operators
Ep(Qnp,j)=(pj+1)n+1[n2]+1lnp(Pp,j), | (46) |
by (38) and (45), for all
For any fixed
τ0p,j=τpj∘EponLSp, | (47) |
where
By the linearity of both
By (46) and (47), if
τ0p,j(Qnp,j)=(pj+1)n+1[n2]+1τpj(lnp(Pp,j)), | (48) |
for all
Theorem 7.4. Let
τ0p,j(Qnp,j)=ωn(p2(j+1))n2cn2, | (49) |
for all
k0,p,jn(Qp,j, ......, Qp,j⏟n-times)={(pj+1)2 if n=20 otherwise, | (50) |
for all
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(j)=(LSp, τ0p,j), | (51) |
for all
Let
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
By (51), we have the family
{LSp(j)=(LSp, τ0p,j):p∈P, j∈Z} |
of (non-traditional) Banach
From this family, one can define the (traditional) free product Banach
(LS, τ0)def=⋆p∈P, j∈ZLSp(j),=(⋆p∈P, j∈ZLSp, ⋆p∈P, j∈Zτ0p,j) | (53) |
in the sense of [29], [30], [33] and [35].
The structures
Definition 8.1. The Banach
Let
Q={Qp,j=lp⊗Pp,j∈LSp(j)}p∈P, j∈Z | (54) |
of
Remark here that, by the choice of
Theorem 8.1. Let
Θp,j=1pj+1Qp,j∈LS | (55) |
satisfy
τ0(Θnp,j)=ωncn2, | (56) |
and
k0n(Θp,j, Θp,j, ..., Θp,j⏟n-times) = {1if n=20 otherwise, |
for all
Proof. Let
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
=ωncn2, | (57) |
for all
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
X={Θp,j∈LSp(j)|p∈P, j∈Z}. | (58) |
Recall that a subset
Definition 8.2. Let
So, we obtain the following result.
Theorem 8.2. Let
(59) The family
(60) The family
Proof. The proofs of (59) and (60) are done by (52), (53), (54), (56) and (58). See [8] for details.
Let
LSdef=¯C[Q]⊂LS, | (61) |
where
By (61), we obtain the corresponding Banach
LSdenote=(LS, τ0), | (62) |
as a free-probabilistic sub-structure of the free Adelic filterization
Definition 8.3. Let
Let
Theorem 8.3. Let
LS∗-iso=⋆p∈P, j∈Z(¯C[{Θp,j}])∗-iso=¯C[⋆p∈P,j∈Z{Θp,j}], | (63) |
in
Proof. By the definition (62) of our semicircular Adelic filterization
LS∗-iso=⋆p∈P, j∈Z(¯C[{Θp,j}])∗-iso=¯C[⋆p∈P,j∈Z{Θp,j}], | (64) |
since
Note that, every
Qp,j=pj+1Θp,j, for all p∈P,j∈Z, |
and hence, the free blocks
¯C[{Qp,j}]=¯C[{pj+1Θp,j}]=¯C[{Θp,j}], | (64') |
for all
Therefore, by (64), the first
Also, by (64), all elements
⋆p∈P, j∈Z¯C[{Θp,j}]∗-iso=¯C[{free words in X}]=¯C[⋆p∈P, j∈Z{Θp,j}]. | (65) |
Therefore, by (64), (64)
In the middle of the proof of (63), one can get the set-equality,
LSdef=¯C[Q]=¯C[X], in LS | (66) |
Let
φA(1A) = 1, |
where
Define the tensor product Banach
LSAdef=A⊗CLS, | (67) |
where
On this new Banach
τA(a⊗T)=τ0(φA(a)T), | (68) |
for all
By the definition (68) of the linear functional
τA(a⊗T) = τ0(T)φA(a) = φA(a)τ0(T), |
for all
Then the Banach
LSAdenote=(LSA, τA) | (69) |
is well-defined, where
Definition 9.1. Let
On the semicircular
Proposition 9.1. Let
Tap,j=a⊗Qp,j, and Xap,j=a⊗Θp,j, | (70) |
in the semicircular
τA((Tap,j)n) = (ωnpn(j+1)cn2)φA(an), | (71) |
and
τA((Xap,j)n) = (ωncn2)φA(an), |
for all
Proof. The proof of the free-distributional data (71) are shown by the
weighted-semicircularity on the free weighted-semicircular family
τA((Tap,j)n) = τA(an⊗Qnp,j) = φA(an)τ0(Qnp,j), |
and
τA((Xap,j)n) = τA(an⊗Θnp,j) = φA(an)τ0(Θnp,j), |
for all
By the above proposition, we obtain the following free-probabilistic
information on the semicircular
Theorem 9.2. Let
φA(a2n)=(φA(a))2n,withφA(a2)∈C×, | (72) |
for all
Proof. Let
(Tap,j)∗ = a∗⊗Q∗p,j = Tap,j, |
and
(Xap,j)∗ = a∗⊗Θ∗p,j = Xap,j, |
in
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
Therefore, if a free random variable
The following corollary is a direct consequence of the above theorem.
Corollary 9.3.
Let
(74) The operator
(75) The operator
(76) If the linear functional
φA(a1a2) = φA(a1)φA(a2), ∀a1, a2 ∈ A, |
and if
Proof. Let
φA(1nA) = φA(1A) = 1 = 1n = (φA(1A))n, |
for all
Assume now that the linear functional
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
Theorem 9.4. Let
LSA∗-iso=⋆p∈P, j∈Z(A⊗C¯C[{Θp,j}])∗-iso=⋆p∈P, j∈Z¯A[{Θp,j}], | (77) |
where
Proof. By the definition (69) of the semicircular
LSAdef=A⊗CLS∗-iso=A⊗C(⋆p∈P, j∈Z¯C[{Θp,j}]) |
by (63) and (66)
∗-iso=⋆p∈P, j∈Z(A⊗C¯C[{Θp,j}])∗-iso=⋆p∈P, j∈Z¯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
(78) If
LSA∗-iso=⊕Ck∈Δ(⋆p∈P, j∈Z¯Ak[{Θp,j}])∗-iso=⋆p∈P, j∈Z(⊕Ck∈Δ¯Ak[{Θp,j}]), |
where
(79) If
LSA∗-iso=⊗Ck∈Δ(⋆p∈P, j∈Z¯Ak[{Θp,j}])∗-iso=⋆p∈P, j∈Z(⊗Ck∈Δ¯Ak[{Θp,j}]), |
where
(80) Let
LSA∗-iso=⋆k∈Δ, p∈P, j∈Z¯Ak[{Θp,j}]. |
Proof. The proofs of the statements (78), (79) and (80) are done by (77).
Indeed, one has that: if
¯A[{Θp,j}]∗-iso=¯(⊕k∈ΔAk)[{Θp,j}]∗-iso=¯⊕Ck∈Δ(Ak[{Θp,j}])= ⊕Ck∈Δ¯Ak[{Θp,j}], |
for all
Similarly, if
¯A[{Θp,j}] ∗-iso= ⊗Ck∈Δ¯Ak[{Θp,j}]; |
and if
¯A[{Θp,j}] ∗-iso= ⋆k∈Δ¯Ak[{Θp,j}], |
for all
Our results of this section illustrate that the
free probability on
Throughout this section, we fix a unital
Xap,j=a⊗Θp,j | (81) |
be free random variables (70), generating
Define a subset
XAdef={Xap,j∈LSA:Xap,j}isinthesenseof(81). | (82) |
Then, as we discussed above this subset
LSA=¯C[XA], | (83) |
set-theoretically, by (63), (66) and (67).
Suppose a given
A=¯C[B]A, |
where
XA = {Xap,j ∈ LSA : a ∈ B, Θp,j ∈ X}. |
However, now, we take a
In this section, we consider how our free-distributional data on
Let
P = {p1 ≤ p2 ≤ p3 ≤ p4 ≤ ⋅⋅⋅} | (84) |
with
p1=2,p2=3,p3=5,p4=7,p5=11,..., etc.. |
From below, the set
Define now an injective functional
g(pk)=pk+1, for all k∈N. | (85) |
For the injection
gn=g∘g∘g∘⋅⋅⋅∘g⏟n-times, | (86) |
with axiomatization:
g0=idP,theidentitymaponP, |
for all
By (86), clearly,
gn(pk)=pk+n in P, for all k∈N, |
for all
g(2)=3,g2(3)=7,g5(5)=19, etc.. |
Definition 10.1. Let
Let
GA(Xap,j)=Xag(p),j=a⊗Θg(p),j, | (87) |
for all
By the multiplicativity, the morphism
S = NΠl=1(Xalpl,jl)nl, |
in
GA(S)=GA(NΠl=1(Xalpl,jl)nl)=NΠl=1GA((Xalpl,jl)nl) |
by the multiplicativity of
=NΠl=1(GA(Xalpl,jl))nl |
by the multiplicativity of
=NΠl=1(Xalg(pl),jl)nl=NΠl=1(al⊗Θg(pl),jl)nl |
by (87)
=NΠl=1(anl⊗Θnlg(pl),jl), |
i.e.,
GA(S)=NΠl=1(Xalg(pl),jl)nl, | (88) |
in
Also, this morphism
GA(S∗)=GA(NΠl=1Xa∗N−l+1pN−l+1,jN−l+1) |
because
(Xap,j)∗=(a⊗Θp,j)∗=a∗⊗Θp,j=Xa∗p,j, | (89) |
in
=NΠl=1Xa∗N−l+1g(pN−l+1), jN−l+1=(NΠl=1Xalg(pl),jl)∗ |
by (88)
=(GA(S))∗, | (90) |
by (89).
By (88) and (90), one can verify that, for all
GA(T∗)=GA(T)∗,inLSA. | (91) |
Proposition 10.1. Let
Proof. The proof is done by (91). i.e., this multiplicative linear
transformation
For the
G0A=1LSA,theidentityoperatoronLSA, |
satisfying
G0A(Xap,j) = Xag0(p), j = Xap,j = 1LS(Xap,j), |
for all
Then it is not difficult to check that
GnA(Xap,j)=Xagn(p), jinLS,∀n∈N0, | (92) |
for all
Definition 10.2. The
Based on our
Theorem 10.2. Let
τA((GnA(Xap,j))k)=(ωkck2)φA(ak)=τA((Xap,j)k), | (93) |
for all
Proof. Let
GnA(Xap,j) = Xagn(p),j = a⊗Θgn(p),j ∈ LSA, |
for any
(GnA(Xap,j))k=(a⊗Θgn(p),j)k=ak⊗Θkgn(p),j, | (94) |
for all
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
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
Proof. Let
(Xap,j)∗ = a∗⊗Θ∗p,j = Xap,j in LSA. |
Note now that, since
(GnA(XAp,j))∗ = a∗⊗Θ∗gn(p),j = Xagn(p),j = GnA(XAp,j), |
in
Recall that the free distributions of self-adjoint operators are
characterized by the free-moment sequence. So, the free distribution of
(τA((Xap,j)k))∞k=1 = (ωkck2φA(ak))∞k=1, |
by (71).
Also, the free distributions of
(τA((GnA(Xap,j))k))∞k=1 = (τA((Xap,j)k))∞k=1, |
by the self-adjointness of them, and by (93), for all
It shows that the free distributions of
(0, c1φA(a2), 0, c2φA(a4), 0, c3φA(a6), ....), |
for all
Let's generalize the above corollary. In fact, the
free-distributional formula (93) guarantees that the free distributions
of the generators
τA((GnA(Xap,j))k) = τA((Xap,j)k), | (96) |
and
τA(((GnA(Xap,j))∗)k)=τA((GnA(Xa∗p,j))k)=τA((Xa∗p,j)k)=τA(((Xap,j)∗)k), |
for all
(Xap,j)∗ = a∗⊗Θp,j = Xa∗p,j in XA, |
in
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
Therefore, one obtains the following theorem.
Theorem 10.4.
Let
(98) the free distribution of
in
Proof. Let
Assume now that
(Xap,j)∗ = Xa∗p,j ≠ Xap,j in LSA. |
It also shows that
GnA(Xp,j)∗ = (Xagn(p),j)∗ = Xa∗gn(p),j ≠ Xagn(p),j = GnA(Xp,j), |
in
So, the free distribution of
{τA(Xr1Xr2...Xrk)|(r1,...,rk)∈{1,∗}k,for all k∈N}, |
and similarly, the free distributions of
{τA(Xr1(n)Xt2(n)...Xrk(n))|(r1,...,rk)∈{1,∗}k,for all k∈N}, |
since
However, by (96) and (97), one has that
τA(Xr1(n)Xr2(n)...Xrk(n)) = τA(Xr1Xr2...Xrk), |
for all
Therefore, the free distributions of
The above theorem shows that the
Corollary 10.5. The
Proof. Note that all elements
GnA(free words in XA) |
are identical to those for free words in
It guarantees that free distribution of every element
In this section, motivated by the main results (93) and (98)
of Section 10.2, we consider free-homomorphic relations on our semicircular
Definition 10.3. Let
φ2(Φ(b))=φ1(b), for all b∈B1. | (99) |
Then the topological
If
By the above free-homomorphic relation (99), one can get the following result.
Theorem 10.6. Let
(100) the
Proof. For any arbitrarily fixed
Throughout this section, fix a unital
In this section, we consider certain shifting processes
Let
h+(j)=j+1,andh−(j)=j−1, | (101) |
for all
h+∘h−=idZ=h−∘h+, | (102) |
where
Definition 11.1. Let
Let
hn±=h±∘h±∘⋅⋅⋅∘ h±⏟n-times, | (103) |
for all
h0± = idZ on Z, |
satisfying
h0+(j)=j=h0−(j), for all j∈Z. |
Definition 11.2.
Let
By (101) and (103), the
hn+(j)=j+n, for all j∈Z, | (104) |
and
hn−(j)=j−n, for all j∈Z, |
for all
hn+∘hn−=idZ=hn−∘hn+,∀n∈N0. | (105) |
Let
βn+(Xap,j)=Xap,hn+(j)=Xap,j+n, | (106) |
and
βn−(Xap,j) = Xap,hn−(j) = Xap,j−n, |
with
β0±(Xap,j) = Xap,h0±(j) = Xap,j = 1LSA(Xap,j), |
for all
By the multiplicativity of the morphisms
T = NΠl=1(Xalpl,jl)nl ∈ LSA, for n1, ..., nN ∈ N, |
is a free reduced word with its length-
βn±(T)=βn±(NΠl=1(Xalpl,jl)nl)=NΠl=1βn±((Xalpl,jl)nl)=NΠl=1(βn±(Xalpl,jl))nl |
by the multiplicativity of
=NΠl=1(Xalpl,hn±(jl))nl=NΠl=1(Xalpl,jl±n)nl, | (107) |
in
βn±((Xap,j)∗)=βn±(Xa∗p,j)=Xa∗p,j±n=(Xap,j±n)∗=(βn±(Xap,j))∗, | (108) |
for all
So, by (107) and (108), if
βn±(W∗) = (βn±(W))∗, |
implying that
βn±(T∗)=(βn±(T))∗,forallT∈LSA, | (109) |
for all
Proposition 11.1. Let
Proof. Note that the
Definition 11.3. We call the
The above proposition shows a difference between our prime-shifts, and the
integer-shifts on
Remark 11.1. Note that our
Now, consider how our
Theorem 11.2. Let
τA((βn±(Xap,j))k)=ωkck2φA(ak)=τA((Xap,j)k), | (110) |
for all
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
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
(111)
Proof. By (110), the
In this section, we consider both prime shifts, and integer shifts,
which are well-defined free-homomorphisms on the semicircular
Now, we consider certain
N±0 denote= {±} × N0. |
Now, consider the Cartesian product set
Pdef=P×Z. | (112) |
Let
g0=idP,and h0±=idZ. |
Define now shifts on the set
sn1(e,n2)def=gn1×hn2edenote=(gn1,hn2e), | (113) |
for all
sn1(e,n2)(p,j) = (gn1(p), hn2e(j)) = (gn1(p), jen2) |
in
jen2 = {j+n2if e=+j−n2if e=−. |
For example,
s2(−,5)(3, −1) = (g2(3), h5−(−1)) = (7, −6) |
in
Definition 12.1. Let
s0(e,0) = idP×idZ = idP, |
where
idP(p,j)=(p, j) in P, for all (p,j)∈P. |
Then these injections
Let
σn1(e,n2)=Gn1Aβn2e on LSA, | (114) |
for all
Notation and Assumption. From below, for convenience, we simply
write our
Since
Proposition 12.1.
Let
σn1(e,n2)def=Gn1βn2e=βn2eGn1onLSA, | (115) |
for all
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
Since all elements of
σn1(e,n2) def= Gn1βn2e = βn2eGn1 on LSA, |
for all
Let
σ(LSA)={σn1(e,n2):n1∈N0,(e,n2)∈N±0}, | (116) |
where
Definition 12.2.
We call the
Now, let's consider the following structure theorem of the system
Theorem 12.2.
Let
(117)
Proof. Let
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(j) = {+if j≥0−if j<0, |
for all
The formula (118) shows that the product (or composition), inherited from
that on
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
(Gn1Gn2)Gn3=Gn1+n2Gn3=Gn1+n2+n3=Gn1Gn2+n3=Gn1(Gn2Gn3), | (120) |
on
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
Thus, the operation (
Definitely, one can take an element
σ0(e,0)=G0β0e=1LSA⋅1LSA=1LSA∈σ(LSA), | (122) |
satisfying that
σn(e,k)⋅1LSA = σn(e,k) = 1LSA ⋅ σn(e,k) in σ(LSA), |
for all
So, the semigroup
Finally, consider that
Gn1Gn2=Gn1+n2=Gn2+n1=Gn2Gn1, | (123) |
and
βk1e1βk2e2 = β|e1k1e2k2|sgn(e1k1e2k2) = β|e2k2e1k1|sgn(e2k2e1k1) = βk2e2βk1e1, |
on
Therefore,
σn1(e1,k1)σn2(e2,k2)=σn1+n2(sgn(e1k1e2k2),|e1k1e2k2|)=σn2(e2,k2)σn1(e1,k1), | (124) |
on
So, the monoid
The above structure theorem (117) characterizes the algebraic
structure of
Definition 12.3. Let
Let
Recall-and-note that the prime-shifts
Lemma 12.3.
Let
σ denote= σn(e,k) ∈ σ(LSA), for n ∈ N0, (e,k) ∈ N±0, |
be a pi-shift on
τA((σ(Xap,j))l)=ωlcl2φA(al)=τA((Xap,j)l), | (125) |
for all
Proof. Let
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
Therefore, the free-distributional data (125) holds.
By the above lemma, we obtain the following result.
Theorem 12.4.
Let
Proof. By the similar arguments of the proofs for (100) and (111), all
pi-shifts of the pi-shift monoid
Remark that, by the definition (114), a pi-shift
Theorem 12.5.
Let
(126)
Proof. (
σn(e,k) = σ0(e,k) = G0βke = 1LSAβke = βke, |
and
(
Therefore, the characterization (126) holds.
The above theorem characterizes the free-isomorphic property in the
pi-shift monoid
By the above two theorems, a pi shift
Let
Let
σn:θ(e,k)(Xap,j)=σn:θ(e,k)(a⊗Θp,j)def=σn(e,k)(θ(a)⊗Θp,j)=σn(e,k)(Xθ(a)p,j)=Xθ(a)gn(p),jek, | (127) |
for all
Let
σn:θ(e,k)(Xa1p1,j1Xa2p2,j2)=σn:θ(e,k)(a1a2⊗Θp1,j1Θp2,j2)={σn:θ(e,k)(a1a2⊗Θp1,j1Θp2,j2)if (p1,j1)≠(p2,j2) in Pσn:θ(a1a2⊗Θ2p1,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(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
Also, we have, for any
σn:θ(e,k)((Xap,j)∗)=σn:θ(e,k)(Xa∗p,j)=Xθ(a∗)gn(p),jek |
by (127)
=Xθ(a)∗gn(p),jek=(Xθ(a)gn(p),jek)∗ |
since
=(σn:θ(e,k)(Xap,j))∗, |
implying that
σn:θ(e,k)(T∗)=(σn:θ(e,k)(T))∗, | (129) |
for all
Therefore, the morphism
Define now a subset
σA(LSA)={σn:θ(e,k)|σn:θ(e,k) are in the sense of (127),for all θ∈Hom(A), andσn(e,k)∈σ(LSA)}. | (130) |
Then one can get the following structure theorem.
Theorem 13.1.
Let
(131)
Moreover,
Proof. Let
σldenote=σnl:θl(el,kl)∈σA(LSA), for l=1,2. |
Observe that, for any generating operator
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
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
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
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
Let
σ0:1A(e,0)=1LSA,theidentitymaponLSA, | (136) |
which is a
σ⋅1LSA = σ = 1LSA⋅σ, ∀σ ∈ σA(LSA). |
Therefore, by (136), the semigroup
Definitely, by (126), an element
Remark that, homomorphism semigroups are not commutative in general. Since
our
However, by (134) and by the commutativity of our pi-shift monoid
The above theorem characterizes the algebraic property of the subset
Definition 13.1.
Let
In Section 12, we showed that all pi-shifts in the pi-shift monoid
First of all, one can immediately obtain the following corollary of (125) and (126).
Corollary 13.2. Let
Proof. Let
σ(Xap,j) = X1A(a)gn(p),jek = Xagn(p),jek = σn(e,k)(Xap,j), |
for all generating operators
σ=σn:1A(e,k)=σn(e,k)onLSA. | (137) |
Therefore, by (125),
By the above corollary, we have the following result.
Corollary 13.3.
Let
(138)
Proof. The proof of (138) is done by (137).
The above corollaries shows that "some" elements of the
Lemma 13.4. Let
τA((σθ(Xap,j))l)=(ωlcl2)φA(θ(al))=τA((Xθ(a)p,j)l), | (139) |
for all
Proof. Let
(σθ(Xap,j))l=(Xθ(a)gn(p),jek)l=θ(a)l⊗Θlgn(p),jek=θ(al)⊗Θlgn(p),jek, |
in
Thus, one obtains that
τA((σθ(Xap,j))l) = (ωlcl2)φA(θ(al)), |
for all
Also, one has that
τA((Xθ(a)p,j)l) = (ωlcl2)φA(θ(al)), |
for all
Therefore, the free-distributional data (139) holds.
More general to (137) and (138), we obtain the following result.
Theorem 13.5. Let
fHom(A)def={θ∈Hom(A)|θ is afree-homomorphismon A}, | (140) |
Define a subset
σfA(LSA)def={σn:θ(e,k)∈σA(LSA)|θ∈fHom(A)}. | (141) |
(142)
(143) All elements of
(144)
n=0, and θ is bijective on A. |
Proof. Let
σl = σnl:θl(el,kl) ∈ σfA(LSA), for l = 1, 2, |
we have
σ1σ2=σn1+n2:θ1θ2(sgn(e1k1e2k2), |e1k1e2k2|)let=σ, | (145) |
in
Remark that if
φA(θ1θ2(x)) = φA(θ1(θ2(x))) = φA(θ2(x)) = φA(x), |
since
It shows that if
Now, let
τA((σθ(Xap,j))l)=(ωlcl2)φA(θ(al)) |
by (139)
=(ωlcl2)φA(al)=τA((Xap,j)l), | (146) |
since
Therefore, every element of the sub-monoid
Let
n≠0inN0,orθisnotbijectiveonA, |
then
If
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
Therefore, the characterization (144) holds true.
The above theorem generalizes the free-homomorphic properties
(137) and (138) in the
Definitely, if one takes an element
[1] |
Albeverio S., Jorgensen P. E. T., Paolucci A. M. (2012) On fractional Brownian motion and wavelets. Compl. Anal. Oper. Theo. 6: 33-63. ![]() |
[2] |
S. Albeverio, P. E. T. Jorgensen and A. M. Paolucci, Multiresolution wavelet analysis of integer scale Bessel functions, J. Math. Phy., 48 (2007), 073516, 24 pp.
10.1063/1.2750291 MR2337697 |
[3] |
Alpay D., Jorgensen P. E. T., Levanony D. (2017) On the equivalence of probability spaces. J. Theo. Prob. 30: 813-841. ![]() |
[4] |
D. Alpay, P. E. T. Jorgensen and D. P. Kimsey, Moment problems in an infinite number of variables, Infin. Dimens. Anal. Quantum Probab. Relat. Top., 18 (2015), 1550024, 14 pp.
10.1142/S0219025715500241 MR3447225 |
[5] | Alpay D., Jorgensen P. E. T. (2015) Spectral theory for Gaussian processes: Reproducing kernels. Random Functions and Operator Theory 83: 211-229. |
[6] |
Alpay D., Jorgensen P. (2015) Spectral theory for Gaussian processes: Reproducing kernels, boundaries, & L2 -wavelet generators with fractional scales. Numb. Funct. Anal, Optim. 36: 1239-1285. ![]() |
[7] |
Alpay D., Jorgensen P., Salomon G. (2014) On free stochastic processes and their derivatives. Stochastic Process. Appl. 124: 3392-3411. ![]() |
[8] |
Cho I. (2017) Free semicircular families in free product Banach ∗-algebras induced by p-adic number fields over primes p. Compl. Anal. Oper. Theo. 11: 507-565. ![]() |
[9] |
Cho I. (2017) Adelic analysis and functional analysis on the finite adele ring. Opuscula Math. 38: 139-185. ![]() |
[10] |
Cho I. (2019) Semicircular-like and semicircular laws on Banach ∗-probability spaces induced by dynamical systems of the finite adele ring. Adv. Oper. Theo. 4: 24-70. ![]() |
[11] | Cho I. (2016) p-adic free stochastic integrals for p-adic weighted-semicircular motions determined by primes p. Libertas Math. (New S.) 36: 65-110. |
[12] |
Cho I., Jorgensen P. E. T. (2017) Semicircular elements induced by p-adic number fields. Opuscula Math. 37: 665-703. ![]() |
[13] | Connes A. (1994) Noncommutative Geometry. Inc., San Diego, CA: Academic Press. |
[14] |
Bost J.-B., Connes A. (1995) Hecke algebras, type III-factors, and phase transitions with spontaneous symmetry breaking in number theory. Selecta Math. (N.S.) 1: 411-457. ![]() |
[15] | A. Connes, Trace formula in noncommutative Geometry and the zeroes of the Riemann zeta functions, Available at: http://www.alainconnes.org/en/download.php. |
[16] |
Dragovich B., Radyno Ya., Khennikov A. (2007) Distributions on adéles. J. Math. Sci. 142: 2105-2112. ![]() |
[17] |
Dragovich B., Khennikov A., Mihajiović D. (2007) Linear fractional p-adic and adelic dynamical systems. Rep. Math. Phy. 60: 55-68. ![]() |
[18] |
T. L. Gillespie, Superposition of Zeroes of Automorphic L-Functions and Functoriality, Thesis (Ph.D.)–The University of Iowa, 2011, 75 pp.
MR2942141 |
[19] |
Gillespie T., Ji G. H. (2011) Prime number theorems for Rankin-Selberg L-functions over number fields. Sci. China Math. 54: 35-46. ![]() |
[20] |
Haagerup U., Larsen F. (2000) Brown's spectrial distribution measure for R-diagonal elements in finite von Neumann algebras. J. Funct. Anal. 176: 331-367. ![]() |
[21] |
Jorgensen P. E. T., Paolucci A. M. (2012) Markov measures and extended zeta functions. J. Appl. Math. Comput. 38: 305-323. ![]() |
[22] |
Jorgensen P. E. T., Paolucci A. M. (2011) States on the Cuntz algebras and p-adic random walks. J. Aust. Math. Soc. 90: 197-211. ![]() |
[23] |
Kaygorodov I., Shestakov I., Umirbaev U. (2018) Free generic Poisson fields and algebras. Comm. Alg. 46: 1799-1812. ![]() |
[24] |
Kemp T., Speicher R. (2007) Strong Haagerup inequalities for free R-diagonal elements. J. Funct. Anal. 251: 141-173. ![]() |
[25] |
Makar-Limanov L., Shestakov I. (2012) Polynomials and Poisson dependence in free Poisson algebras and free Poisson fields. J. Alg. 349: 372-379. ![]() |
[26] |
A. Nica and R. Speicher, Lectures on the Combinatorics of Free Probability, London Mathematical Society Lecture Note Series, 335. Cambridge University Press, Cambridge, 2006.
10.1017/CBO9780511735127 MR2266879 |
[27] |
Rǎdulescu F. (1994) Random matrices, amalgamated free products and subfactors of the von Neumann algebra of a free group of nonsingular index. Invent. Math. 115: 347-389. ![]() |
[28] | Radulescu F. (2014) Free group factors and Hecke operators. The Varied Landscape of Operator Theory, Theta Ser. Adv. Math., Theta, Bucharest 17: 241-257. |
[29] |
R. Speicher, Combinatorial theory of the free product with amalgamation and operator-valued free probability theory, Mem. Amer. Math. Soc., 132 (1998).
10.1090/memo/0627 MR1407898 |
[30] |
Speicher R. (2000) A conceptual proof of a basic result in the combinatorial approach to freeness. Infinit. Dimention. Anal. Quant. Prob. Relat. Topics 3: 213-222. ![]() |
[31] |
Vladimirov V. S., Volovich I. V. (1989) p-adic quantum mechanics. Comm. Math. Phy. 123: 659-676. ![]() |
[32] |
V. S. Vladimirov, I. V. Volovich and E. I. Zelenov, p-Adic Analysis and Mathematical Physics, Series on Soviet and East European Mathematics, 1. World Scientific Publishing Co., Inc., River Edge, NJ, 1994.
10.1142/1581 MR1288093 |
[33] |
Voiculescu D.-V. (2008) Aspects of free analysis. Jpn. J. Math. 3: 163-183. ![]() |
[34] |
Voiculescu D. (2005) Free probability and the von Neumann algebras of free groups. Rep. Math. Phy. 55: 127-133. ![]() |
[35] |
D. V. Voiculescu, K. J. Dykemma and A. Nica, Free Random Variables: A Noncommutative Probability Approach to Free Products with Applications to Random Matrices, Operator Algebras and Harmonic Analysis on Free Groups, CRM Monograph Series, 1. American Mathematical Society, Providence, RI, 1992.
MR1217253 |