• 検索結果がありません。

Tilings of half a hexagon

N/A
N/A
Protected

Academic year: 2022

シェア "Tilings of half a hexagon"

Copied!
34
0
0

読み込み中.... (全文を見る)

全文

(1)

a hexagon Nordenstam

Novak half-hexagon Limit shape Correlation kernel

Tilings of half a hexagon

Eric Nordenstam

Joint work with Benjamin Young

Fakult¨at f¨ur Mathematik Universit¨at Wien

SLC 69, Strobl, Austria

(2)

Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

Aztec diamonds of orders 1, 2, 3 and 4.

(3)

Tilings of half a hexagon Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

The Aztec Diamond

Aztec diamonds of orders 1, 2, 3 and 4.

The diamond of ordern can be tiled in 2n(n+1)/2 ways.

Elkies, Kuperberg, Larsen & Propp 1992

(4)

Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

(5)

a hexagon Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

The number of tilings of an ordern Aztec diamond is 2(n+12 ).

Jonathan Novak observed that det

2i j

n i,j=1

= 2(n+12 ).

(6)

Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

3 2 5 1 3 6

(7)

Tilings of half a hexagon Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

Limit shape

(8)

Limit shape Correlation

kernel The shuffling algorithm

The Arctic Parabola Theorem.

(9)

a hexagon Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

(10)

Limit shape Correlation kernel

(11)

a hexagon Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

(12)

Limit shape Correlation kernel

(13)

a hexagon Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

Introduce a coordinate system: Xji(t) is the position of thejth particle on leveli at time t.

3 2 5 1 3 6 1 3 5 7

Note that

Xji(t)≤Xji−1(t)<Xji+1(t)

(14)

Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

X11(t) =X11(t−1) +β11(t) X1j(t) =X1j(t−1) +β1j(t)

−1{X1j(t−1) +β1j(t) =X1j−1(t) + 1} for j ≥2 Xjj(t) =Xjj(t−1) +βjj(t)

+1{Xjj(t−1) +βjj(t) =Xjj−1−1(t)} for j ≥2 Xij(t) =Xij(t−1) +βij(t)

+1{Xij(t−1) +βij(t) =Xi−1j−1(t)}

−1{Xij(t−1) +βij(t) =Xij−1(t) + 1} for j >i >1 where allβi(t) are independent coin flips.

(15)

Tilings of half a hexagon Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

Particle dynamics

Time shift: xij(t) =Xij(t−j)

(16)

Nordenstam

Novak half-hexagon

Limit shape Correlation kernel

(17)

Tilings of half a hexagon Nordenstam

Novak half-hexagon Limit shape Correlation kernel

The Arctic Parabola Theorem

Theorem

Consider uniform measure on tilings of the Novak half-hexagon.

The region in which the density of particles (i.e. vertical lozenges) is assymptotically non-zero is bounded by a parabola.

(18)

Limit shape Correlation kernel

Proposition (N & Y 2011)

The limit shape in the Half-Aztec diamond is the semi-circle.

Jockusch, Propp & Shor (1998)

(19)

Tilings of half a hexagon Nordenstam

Novak half-hexagon Limit shape Correlation kernel

The Arctic Parabola Theorem

(20)

Nordenstam

Novak half-hexagon Limit shape Correlation kernel

(21)

Tilings of half a hexagon Nordenstam

Novak half-hexagon Limit shape Correlation kernel

Correlations

Considern Bernoulli walkers started at 1, 2, . . . ,n, and conditioned to end up at positionsy1, . . . , yn, at time N conditioned never to intersect.

The number of such configurations is given by the Lindstr¨om-Gessel-Viennot Theorem as the determinant of

M = N

yj −i n

i,j=1

(22)

Nordenstam

Novak half-hexagon Limit shape Correlation kernel

Theorem (Eynard & Mehta (1998), Borodin & Rains (2005)) The probability that there is a walker at each of(x1,t1), . . . , (xk,tk) is

det[K(ti,xi;tj,xj)]ki,j=1 where

K(r,x;s,y) =−1{s >r}

s−r y−x

+

n

X N−r yi−x

[M−1]i,j s

y−j

(23)

a hexagon Nordenstam

Novak half-hexagon Limit shape Correlation kernel

det

N

yi−j−1{j ≥s} n−1

i,j=1

=

n−1

Y

i=1

N!

(yi −1)!(N−yi +n)!

!

×det[f(i,j,s)]n−1i,j=1 where

f(i,j,s) =

((yij+ 1)· · ·(yi1)(Nyi+j+ 1)· · ·(Nyi+n), j<s, (yij)· · ·(yi1)(Nyi+j+ 2)· · ·(Nyi+n), js.

(24)

Limit shape Correlation kernel

variables. Fors = 1, sage gave us

Pn,1(N,y) = ∆(y)

n−2

Y(N+i)n−1−i

!

n−1

Y(yj −1)

(25)

a hexagon Nordenstam

Novak half-hexagon Limit shape Correlation kernel

Let ∆ mean taking the Vandermonde determinant in the variables. Fors = 2, sage gave us

P3,2(N,y) =(N+ 1)∆(y)(−2e2(y) + (N+ 4)e1(y)−(3N+ 8)) P4,2(N,y) =(N+ 1)2(N+ 2)∆(y)(−3e3(y) + (N+ 6)e2(y)

−(3N+ 12)e1(y) + (7N+ 24))

P5,2(N,y) =(N+ 1)3(N+ 2)2(N+ 3)∆(y)(−4e4(y) + (N+ 8)e3(y)−(3N+ 16)e2(y) + (7N+ 32)e1(y)−(15N+ 64))

P6,2(N,y) =(N+ 1)4(N+ 2)3(N+ 3)2(N+ 4)∆(y)(−5e5(y) + (N+ 10)e4(y)−(3N+ 20)e3(y) + (7N+ 40)e2(y)

−(15N+ 80)e1(y) + (31N+ 160))

(26)

Limit shape Correlation kernel

Pn,s(N,y) = ∆(y)

r=1

(N+r)n−1−r×

×

n−1

X

l=0 s−1

X

k=0 s

X

j=1 j

X

i=0

(−1)n+s+l+jNkjlen−1−l(y)

i!(s−1)! s(s−1−j,k−i)×

× d

dn i

(n−1)· · ·(n−j)

! s −1

j

(1)

(27)

Tilings of half a hexagon Nordenstam

Novak half-hexagon Limit shape Correlation kernel

Matrix Inverse

Theorem Let

M = N

yi−j n

i,j=1

.

Then

[M−1]i,j =

j

X

k=1

N+n−1 k−1

N−1+j−k

j−k

N+n−1 yi−1

(−1)k+j

n

Y

l=1,l6=i

k−yl yi −yl.

(28)

Nordenstam

Novak half-hexagon Limit shape Correlation kernel

[MM−1]α,γ =

n

X

β=1

[M]α,β[M−1]β,γ

=

n

X

β=1 γ

X

k=1

(−1)k

N+n−1 yβ−1

−1

N+n−1 k−1

×

N−1 +γ−k γ−k

N yβ−α

n

Y k−yi yβ−yi

. (2)

(29)

Tilings of half a hexagon Nordenstam

Novak half-hexagon Limit shape Correlation kernel

Lagrange interpolation

Let (x1,y1), . . . , (xn,yn)∈R2 and let pk(x) =

n

Y

i=1,i6=k

x−xi

xk −xi

.

Then

f(x) =

n

X

k=1

ykpk(x)

has the property thatf(xi) =yi for i = 1, . . . ,n.

(30)

Nordenstam

Novak half-hexagon Limit shape Correlation kernel

[MM−1]α,γ

=

γ

X

k=1

(−1)β+j

N−1 +β−k β−k

N k−γ

= 0

α,γ (3)

(31)

a hexagon Nordenstam

Novak half-hexagon Limit shape Correlation kernel

The correlation functions for the Novak half-hexagon are determinental, with kernel given by

K(r,x;s,y) =−φr,s(x,y) +

n

X

i,j=1 n+1−r

2i−x

s

y−j

2n 2i−1

j

X

k=1

2n k−1

n+j −k j−k

×

× (−1)k+j+i+n

(i−1)!(n−i)!

n

Y

l=1,l6=i

(k−2l)

where for r≥s,φ≡0and for r <s, φr,s(x,y) =

s−r y−x

.

(32)

Limit shape Correlation kernel

(33)

Tilings of half a hexagon Nordenstam

Novak half-hexagon Limit shape Correlation kernel

Thank you four your attention

Nordenstam, Young, Domino shuffling on Novak half-hexagons and Aztec half-diamonds, Electron. J. of Combin. 18 (2011), no. 1.

Nordenstam, Young, Correlations for the Novak Process, FPSAC 2012 proceedings, arXiv:1201.4138.

(34)

Nordenstam

Novak half-hexagon Limit shape Correlation kernel

N=

"

A Bj −i

q

q(Bj2−i)

#n

i,j=1

,

has inverse

[N−1]i,j = qnBi(Bi2)

A+n−1

Bi−1

q

n

Y

k=1,k6=i

1 qBi −qBk

×

j−1

X

a=0 n−1

X

b=0

b j−1−a

q

n−b−1 a

q

q(j−12 )+(a+b)(a−j−1)−b−1+aA× (−1)be (qB1, . . . ,qB , . . . ,qBn).

参照

関連したドキュメント

Loosely speaking, Class I consists of those graphs whose quotient graph is a “double-edged” cycle, Class II consists of graphs whose quotient is a cycle with a loop at each

Since all vertex degrees in AP n are equal to 4, the eigenvalues of its negative Lapla- cian are obtained by adding 4 to the eigenvalues of the adjacency matrix of AD n , which in

In a preliminary section, we establish an analogue of the Minkowski–Weyl theo- rem (Theorem 2), showing that a tropical polyhedron can be equivalently described either as the sum of

1Y and Y represent, respectively, the bipartite half and antipodal quotient of a P-polynomial scheme

The information herein is provided “as−is” and onsemi makes no warranty, representation or guarantee regarding the accuracy of the information, product features,

The output is protected for high power conditions during Current Limit by thermal shutdown and the Overcurrent Detection shutdown

The present edition is a continuation of the edition of the vijñānādvaitavāda section of the Nyāyamañjarī published in Kataoka 2003, a revised version of which is available

For GaN FETs that do not include a dedicated source Kelvin pin, best practice PCB layout techniques should be used to isolate the gate drive return current from the power stage,