Freeness and the Transpose ( Matrices Just Wanna be Free ) Jamie - - PowerPoint PPT Presentation

freeness and the transpose matrices just wanna be free
SMART_READER_LITE
LIVE PREVIEW

Freeness and the Transpose ( Matrices Just Wanna be Free ) Jamie - - PowerPoint PPT Presentation

Freeness and the Transpose ( Matrices Just Wanna be Free ) Jamie Mingo (Queens University) with Mihai Popa Recent Developments in Quantum Groups, Operator Algebras and Applications, February 6, 2015 1 / 20 random variables and their


slide-1
SLIDE 1

Freeness and the Transpose (Matrices Just Wanna be Free)

Jamie Mingo (Queen’s University)

with Mihai Popa

Recent Developments in Quantum Groups, Operator Algebras and Applications, February 6, 2015

1 / 20

slide-2
SLIDE 2

random variables and their distributions

◮ (A, ϕ) unital algebra with state; ◮ Cx1, . . . , xs is the unital algebra generated by the

non-commuting variables x1, . . . , xs

◮ the distribution of a1, . . . , as ∈ (A, ϕ) is the state

µ : Cx1, . . . , xs → C given by µ(p) = ϕ(p(a1, . . . , as))

◮ convergence in distribution of {a(N) 1

, . . . , a(N)

s

} ⊂ (AN, ϕN) to {a1, . . . , as} ⊂ (A, ϕ) means pointwise convergence of distributions: µN(p) → µ(p) for p ∈ Cx1, . . . , xs.

freeness

◮ A1, A2 ⊆ A unital subalgebras are free if given

◮ a1, · · · , an ∈ A with ϕ(ai) = 0 for all i, ◮ ai ∈ Aj1 with j1 · · · jn

we have ϕ(a1 · · · an) = 0,

◮ a1 and a2 are free if alg(1, a1) and alg(1, a2) are free,

2 / 20

slide-3
SLIDE 3

freeness and asymptotic freeness

◮ {a(N) 1

, . . . , a(N)

s

} ⊂ (AN, ϕN) are asymptotically free if µn → µ and x1, . . . , xs are free with respect to µ

◮ if a and b are free with respect to ϕ then

ϕ(abab) = ϕ(a2)ϕ(b)2 + ϕ(a)2ϕ(b2) − ϕ(a)2ϕ(b)2

◮ in general if a1, . . . , as are free then all mixed moments

ϕ(xi1 · · · xin) can be written as a polynomial in the moments

  • f individual moments {ϕ(ak

i )}i,k. ◮ a(N) 1

, . . . , a(N)

s

∈ (An, ϕN) are asymptotically free if whenever we have b(N)

i

∈ alg(1, a(N)

ji

) is such that ϕN(b(N)

i

) = 0 and j1 j2 · · · jm we have ϕN(b(N)

1

· · · b(N)

m ) → 0

3 / 20

slide-4
SLIDE 4

simple distributions: Wigner and Marchenko-Pastur

◮ let f(t) = 1 √ 2πe−t2/2 be the density of the Gauss law ◮ then log(ˆ

f(is)) = s2 2 =

  • n=1

kn sn n! with k2 = 1 and kn = 0 for n 2, so the Gauss law is characterized by having all cumulants except k2 equal to 0

◮ µ a probability measure on R, z ∈ C+,

G(z) =

  • (z − t)−1 dµ(t) is the Cauchy transform of µ and

R(z) = G−1(z) − 1

z = κ1 + κ2z + κ3z2 + · · · is the

R-transform of µ

◮ if dµ(t) = 1 2π

√ 4 − t2 dt is the semi-circle law we have κn = 0 except for κ2 = 1

◮ if 0 < c and a = (1 − √c)2 and b = (1 + √c)2 we let

dµ = √

(b−t)(t−a) 2πt

dt for c 1 and dµ = (1 − c)δ0 + √

(b−t)(t−a) 2πt

dt for 0 < c < 1, the Marchenko-Pastur distribution: κn = c for all n

4 / 20

slide-5
SLIDE 5

GUE random matrices and asymptotic freeness

◮ XN = X∗ N =

1 √ N (xij)ij a N × N self-adjoint random matrix with xij independent complex Gaussians with E(xij) = 0 and E(|xij|2) = 1 (modulo self-adjointness)

◮ λ1 λ2 · · · λN eigenvalues of XN,

µN = 1 N(δλ1 + · · · + δλN) is the spectral measure of XN,

  • tk dµN(t) = tr(Xk

N) ◮

XN is the N × N GUE with limiting eigenvalue distribution given by Wigner’s semi-circle law

1 1 2 2 0.1 0.2 0.3

  • ◮ YN another GUE with entries independent from those of

XN

◮ for large N mixed moments of XN and YN are close to those

  • f freely independent semi-circular operators (thus

asymptotically free)

5 / 20

slide-6
SLIDE 6

Wishart Random Matrices

◮ Suppose G1, . . . , Gd1 are d2 × p random matrices where

Gi = (g(i)

jk )jk and g(i) jk are complex Gaussian random

variables with mean 0 and (complex) variance 1, i.e. E(|g(i)

jk |2) = 1. Moreover suppose that the random variables

{g(i)

jk }i,j,k are independent. ◮

W = 1 d1d2    G1 . . . Gd1   

  • G∗

1

· · · G∗

d1

  • =

1 d1d2 (GiG∗

j )ij

is a d1d2 × d1d2 Wishart

  • matrix. We write

W = d−1

1 (W(i, j))ij as d1 × d1

block matrix with each entry the d2 × d2 matrix d−1

2 GiG∗ j .

6 / 20

slide-7
SLIDE 7

Partial Transposes on Md1(C) ⊗ Md2(C)

· Gi a d2 × p matrix · W(i, j) = 1

d2 GiG∗ j , a d2 × d2 matrix,

· W = 1

d1 (W(i, j))ij is a d1 × d1 block matrix with entries W(i, j)

· WT = 1

d1 (W(j, i)T)ij is the “full” transpose

· W

Γ

= 1

d1 (W(j, i))ij is the “left” partial transpose

· WΓ = 1

d1 (W(i, j)T)ij is the “right” partial transpose

· we assume that p d1d2 → c, 0 < c < ∞ · eigenvalue distributions of W and WT converge to Marchenko-Pastur with parameter c · eigenvalues of W

Γ

and WΓ converge to a shifted semi-circular with mean c and variance c (Aubrun, 2012) · W and WT are asymptotically free (M. and Popa, 2014) · what about WΓ and W

Γ

?

7 / 20

slide-8
SLIDE 8

Semi-circle and Marchenko-Pastur Distributions

Suppose p d1d2 → c.

◮ limit eigenvalue distribution of W (Marchenko-Pastur)

lim E(tr(Wn)) = b

a

tn

  • (b − t)(t − a)

2πt dt =

  • σ∈NC(n)

c#(σ) #(σ) is the number of blocks of σ, a = (1 − √c)2, and b = (1 + √c)2

◮ limit eigenvalue distribution of WΓ (semi-circle)

lim E(tr((WΓ)n)) =

  • σ∈NC1,2(n)

c#(σ) =

  • π∈NC(n)

κπ NC1,2(n) is the set of non-crossing partitions with only blocks of size 1 and 2. (c.f. Fukuda and ´ Sniady (2013) and Banica and Nechita (2013))

8 / 20

slide-9
SLIDE 9

main theorem

◮ thm: The matrices {W, W

Γ

, WΓ, WT} form an asymptotically free family · let (ǫ, η) ∈ {−1, 1}2 = Z2

2.

· let W(ǫ,η) =        W if (ǫ, η) = (1, 1) W

Γ

if (ǫ, η) = (−1, 1) WΓ if (ǫ, η) = (1, −1) WT if (ǫ, η) = (−1, −1) · let (ǫ1, η1), . . . , (ǫn, ηn) ∈ Zn

2

E(Tr(W(ǫ1,η1) · · · W(ǫn,ηn))) =

  • σ∈Sn

p d1d2 #(σ) d fǫ(σ)+#(σ)−n

1

d fη(σ)+#(σ)−n

2

where fǫ(σ) = #(ǫδγ−1δγδǫ ∨ σδσ−1) ( “∨” means the sup of partitions and # means the number of blocks or cycles)

9 / 20

slide-10
SLIDE 10

Computing Moments via Permutations, Notation

◮ [d1] = {1, 2, . . . , d1}, ◮ given i1, . . . , in ∈ [d1] we think of this n-tuple as a function

i : [n] → [d1]

◮ ker(i) ∈ P(n) is the partition of [n] such that i is constant on

the blocks of ker(i) and assumes different values on different blocks

◮ if σ ∈ Sn we also think of the cycles of σ as a partition and

write σ ker(i) to mean that i is constant on the cycles of σ

◮ given σ ∈ Sn we extend σ to a permutation on

[±n] = {−n, . . . , −1, 1, . . . , n} by setting σ(−k) = −k for k > 0

◮ γ = (1, 2, . . . , n), δ(k) = −k ◮ given ǫ1, . . . , ǫn ∈ {−1, 1} let ǫ ∈ S±n be given by

ǫ(k) = ǫ|k| · k

◮ δγ−1δγδ = (1, −n)(2, −1) · · · (n, −(n − 1))

10 / 20

slide-11
SLIDE 11

Computing Moments via Permutations, II

◮ δγ−1δγδ = (1, −n)(2, −1) · · · (n, −(n − 1)) ◮ if Ak = (a(k) ij )ij, a N × N matrix, then

Tr(A1 · · · An) =

N

  • i1,...,in=1

a(1)

i1i2a(2) i2i3 · · · a(n) ini1 =

  • i±1,...,i±n

δγ−1δγδker(i)

a(1)

i1i−1a(2) i2i−2 · · · a(n) ini−n

Tr

  • W(ǫ1,η1) · · · W(ǫn,ηn)

= d−n

1

  • i1,...,in

Tr

  • W(ǫ1,η1)

i1i2 · · ·

  • W(ǫn,ηn))ini1
  • =

d−n

1

  • i±1,...,i±n

Tr

  • W(ǫ1,η1)

i1i−1 · · ·

  • W(ǫn,ηn))ini−n
  • =

d−n

1

  • j±1,...,j±n

Tr

  • W(j1, j−1)(η1) · · · W(jn, j−n)(ηn)

where δγ−1δγδ ker(i), ǫδγ−1δγδǫ ker(j) and j = i ◦ ǫ

11 / 20

slide-12
SLIDE 12

Example of Twisting

n = 5, ǫ = (1, 1, −1, −1, 1) δγ−1δγ = (1, −5)(2, −1)(3, −2)(4, −3)(5, −4)

j1 j−1 j2 j−2 j3 j−3 j4 j−4 j5 j−5

ǫδγ−1δγǫ = (1, −5)(2, −1)(3, −4)(−3, −2)(4, 5)

j1 j−1 j2 j−2 j3 j−3 j4 j−4 j5 j−5

12 / 20

slide-13
SLIDE 13

Computing Moments via Permutations, III

Tr

  • W(ǫ1,η1) · · · W(ǫn,ηn)

= d−n

1

  • j±1,...,j±n

Tr

  • W(j1, j−1)(η1) · · · W(jn, j−n)(ηn)

with ǫδγ−1δγδǫ ker(j). Let s = r ◦ η then for δγ−1δγδ ker(r) Tr

  • W(j1, j−1)(η1) · · · W(jn, j−n)(ηn)

=

  • r±1,...,r±n
  • W(j1, j−1)(η1))r1r−1 · · ·
  • W(jn, j−n)(ηn)

rnr−n

=

  • s±1,...,s±n
  • W(j1, j−1)
  • s1s−1 · · ·
  • W(jn, j−n)
  • sns−n

= d−n

2

  • s±1,...,s±n
  • Gj1G∗

j−1

  • s1s−1 · · ·
  • GjnG∗

j−n

  • sns−n

= d−n

2

  • s±1,...,s±n
  • t1,...,tn

g(j1)

s1t1g(j−1) s−1t1 · · · g(jn) sntng(j−n) s−ntn

13 / 20

slide-14
SLIDE 14

Gaussian entries

E(Tr(W(ǫ1,η1) · · · W(ǫ1,η1))) = (d1d2)−n

  • j±1,...,j±n
  • s±1,...,s±n
  • t1,...,tn

E(g(j1)

s1t1g(j−1) s−1t1 · · · g(jn) sntng(j−n) s−ntn)

= (d1d2)−n

  • j±1,...,j±n
  • s±1,...,s±n
  • t1,...,tn

E(g(j1)

s1t1 · · · g(jn) sntn g(j−1) s−1t1 · · · g(j−n) s−ntn)

[subject to the condition that ǫδγ−1δγδǫ ker(j) and ηδγ−1δγδη ker(s)] = (d1d2)−n

  • j±1,...,j±n
  • s±1,...,s±n
  • t1,...,tn

E(gα(1) · · · gα(n)gβ(1) · · · gβ(n)) where gα(k) = g(jk)

sktk and gβ(k) = g(j−k) s−ktk . Using

E(gα(1) · · · gα(n)gβ(1) · · · gβ(n)) = |{σ ∈ Sn | β = α ◦ σ}|

14 / 20

slide-15
SLIDE 15

Thus E(Tr(W(ǫ1,η1) · · · W(ǫ1,η1))) = (d1d2)−n

  • j±1,...,j±n
  • s±1,...,s±n
  • t1,...,tn

|{σ ∈ Sn | “various conditions”}| where “various conditions” means

◮ ǫδγ−1δγδǫ ker(j) ◮ ηδγ−1δγδη ker(s) ◮ j−k = jσ(k) which is equivalent to σδσ−1 ker(j) ◮ s−k = sσ(k) which is equivalent to σδσ−1 ker(s) ◮ tk = tσ(k) which is equivalent to σ ker(t)

E(tr(W(ǫ1,η1) · · · W(ǫn,ηn))) =

  • σ∈Sn

p d1d2 #(σ) d fǫ(σ)+#(σ)−(n+1)

1

d fη(σ)+#(σ)−(n+1)

2

. where fǫ(σ) = #(ǫδγ−1δγδǫ ∨ σδσ−1) ( “∨” means the sup of partitions)

15 / 20

slide-16
SLIDE 16

finding the highest order terms

◮ general fact: if p and q are pairings then #(p ∨ q) = 1 2#(pq).

In fact we can write the permutation pq as a product of cycles c1c′

1 · · · ckc′ k where c′ i = qc−1 i

q and the blocks of p ∨ q are ci ∪ c′

i ◮ #(ǫδγ−1δγδǫ ∨ σδσ−1) = 1 2#(δγ−1δγ · ǫδσδσ−1ǫ) ◮ if π, σ ∈ Sn and π, σ (the subgroup generated by π and σ)

has only one orbit then there is an integer g (the “genus”) such that #(π) + #(π−1σ) + #(σ) = n + 2(1 − g) and g = 0 only when π is planar or non-crossing with respect to σ.

◮ δγ−1δγ has two cycles so δγ−1δγ, ǫδσδσ−1ǫ can have

either 1 or 2 orbits

◮ if δγ−1δγ, ǫδσδσ−1ǫ has one orbit then

#(ǫδγ−1δγδǫ ∨ σδσ−1) + #(σ) n

16 / 20

slide-17
SLIDE 17

genus of a pairing

1 2 3 4 5 6

17 / 20

slide-18
SLIDE 18

E(tr(W(ǫ1,η1) · · · W(ǫn,ηn))) =

  • σ∈Sn

p d1d2 #(σ) d fǫ(σ)+#(σ)−(n+1)

1

d fη(σ)+#(σ)−(n+1)

2

.

◮ σ will not contribute to the limit unless

δγ−1δγ, ǫδσδσ−1ǫ has two orbits, i.e. ǫ is constant on the cycles of σ (write ǫδσδσ−1ǫ = δǫσǫδ(ǫσǫ)−1)

◮ if ǫ is constant on the cycles of σ there is σǫ ∈ Sn such that

ǫδσδσ−1ǫ = δσǫδσ−1

ǫ

(if σ = c1c2 · · · ck then σǫ = cλ1

1 · · · cλk k

where λi is the sign of ǫ on ci)

◮ then 1 2#(δγ−1δγ · ǫδσδσ−1ǫ) = #(γσ−1 ǫ ) ◮ #(σ) + fǫ(σ) = #(σǫ) + #(γσ−1 ǫ ) n + 1 with equality only

if σǫ is non-crossing

◮ #(σ) + fη(σ) = #(ση) + #(γσ−1 η ) n + 1 with equality only

if ση is non-crossing

18 / 20

slide-19
SLIDE 19

E(tr(W(ǫ1,η1) · · · W(ǫn,ηn))) =

  • σ

p d1d2 #(σ) + O 1 d1d2

  • .

where the sum runs over σ ∈ Sn such that

◮ ǫ and η are constant on the cycles of σ and ◮ both σǫ and ση are both non-crossing. ◮ if ǫ η on a cycle of σ then this cycle must be either a fixed

point or a pair; σǫ = ση and so fǫ(σ) = fη(σ)

◮ σ can only connect W(1,1) to another W(1,1), a W(−1,1) to

another W(−1,1), a W(1,−1) to another W(1,−1), and a W(−1,−1) to another W(−1,−1)

19 / 20

slide-20
SLIDE 20

σ and σ−1

σ = (1, 3, 4)(2)(5)

1 2 3 4 5 1 2 3 4 5 −1 −2 −3 −4 −5

σ = (1, 4, 3)(2)(5)

1 2 3 4 5 1 2 3 4 5 −1 −2 −3 −4 −5

20 / 20