the limit shape of the leaky abelian sandpile modelmain results let s(x) = n (0;0)(x) and topple...
TRANSCRIPT
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The Limit Shape of the Leaky AbelianSandpile Model
Ian M. Alevy
Department of MathematicsUniversity of Rochester
Joint work with Sevak Mkrtchyan
December 2, 2020
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The Abelian Sandpile Model (ASM) is a cellular automatondefined on a graph G = (V ,E).
An initial sandpile distribution s : V → NIf s(x) > deg(x) then x is unstable and topples distributingsand to its neighbors:{
s(x) 7→ s(x)− deg(x)s(y) 7→ s(y) + 1 if y ∼ x .
The sandpile evolves through toppling unstable sites.
In this talk G = Z2 but we will consider different toppling rules:
1D ASM+1 −2 //oo +1
Directed ASM+1
−2
OO
// +1
Uniform ASM+1
+1 −4
OO
//
��
oo +1
+1
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
-
The Abelian Sandpile Model (ASM) is a cellular automatondefined on a graph G = (V ,E).
An initial sandpile distribution s : V → NIf s(x) > deg(x) then x is unstable and topples distributingsand to its neighbors:{
s(x) 7→ s(x)− deg(x)s(y) 7→ s(y) + 1 if y ∼ x .
The sandpile evolves through toppling unstable sites.
In this talk G = Z2 but we will consider different toppling rules:
1D ASM+1 −2 //oo +1
Directed ASM+1
−2
OO
// +1
Uniform ASM+1
+1 −4
OO
//
��
oo +1
+1
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
-
The Abelian Sandpile Model (ASM) is a cellular automatondefined on a graph G = (V ,E).
An initial sandpile distribution s : V → NIf s(x) > deg(x) then x is unstable and topples distributingsand to its neighbors:{
s(x) 7→ s(x)− deg(x)s(y) 7→ s(y) + 1 if y ∼ x .
The sandpile evolves through toppling unstable sites.
In this talk G = Z2 but we will consider different toppling rules:
1D ASM+1 −2 //oo +1
Directed ASM+1
−2
OO
// +1
Uniform ASM+1
+1 −4
OO
//
��
oo +1
+1
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
-
The Abelian Sandpile Model (ASM) is a cellular automatondefined on a graph G = (V ,E).
An initial sandpile distribution s : V → NIf s(x) > deg(x) then x is unstable and topples distributingsand to its neighbors:{
s(x) 7→ s(x)− deg(x)s(y) 7→ s(y) + 1 if y ∼ x .
The sandpile evolves through toppling unstable sites.
In this talk G = Z2 but we will consider different toppling rules:
1D ASM+1 −2 //oo +1
Directed ASM+1
−2
OO
// +1
Uniform ASM+1
+1 −4
OO
//
��
oo +1
+1
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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1-Dimensional ASM
Start with initial sandpile s(x) = nδ(0,0)(x) topple untilreaching a stable sandpile s∞.
QuestionWhat is the stable sandpile?
Toppling rule
+1 −2 //oo +1
0 0 0 0 7 0 0 0 0Figure: Initial sandpile with n = 7.
0 0 0 1 5 1 0 0 0Figure: Result after toppling at the origin.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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1-Dimensional ASM
Start with initial sandpile s(x) = nδ(0,0)(x) topple untilreaching a stable sandpile s∞.
QuestionWhat is the stable sandpile?
Toppling rule
+1 −2 //oo +1
0 0 0 0 7 0 0 0 0Figure: Initial sandpile with n = 7.
0 0 0 1 5 1 0 0 0Figure: Result after toppling at the origin.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Sequence of topplings
0 0 0 2 3 2 0 0 0Figure: Origin toppled again.
0 0 1 1 3 1 1 0 0Figure: All unstable sites topple once more.
some more topples....
0 1 1 0 3 0 1 1 0and the stable sandpile:
0 1 1 1 1 1 1 1 0Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Limit Shape of 1D ASM
Let x = (x1, x2).
Proposition
If s(x1, x2) = nδ(0,0)(x1, x2) then the stable sandpile for the 1DASM is
s∞(x1,0) =
1 if x1 = 0 and n is odd,0 if x1 = 0 and n is even,1 if 0 < |x1| ≤ bn2c,0 if bn2c < |x2|.
s∞(x1, x2) = 0 if x2 > 0.
When d ≥ 2 the limit shape exhibits self-organization.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Limit Shape of 1D ASM
Let x = (x1, x2).
Proposition
If s(x1, x2) = nδ(0,0)(x1, x2) then the stable sandpile for the 1DASM is
s∞(x1,0) =
1 if x1 = 0 and n is odd,0 if x1 = 0 and n is even,1 if 0 < |x1| ≤ bn2c,0 if bn2c < |x2|.
s∞(x1, x2) = 0 if x2 > 0.
When d ≥ 2 the limit shape exhibits self-organization.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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2D ASMLet s(x1, x2) = nδ(0,0)(x1, x2) and topple until stable usingthe uniform toppling rule.The stable sandpile has a limit shape (Pegden-Smart2013).
Toppling rule
+1
+1 −4
OO
//
��
oo +1
+1
Theorem (Levine-Peres 2008)The limit shape is boundedbetween circles of radii c1
√n
and c2√
n with c2/c1 =√
3√2.
Figure: Stable sandpile with n = 107.Colors correspond to heights of sandpile.
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2D ASMLet s(x1, x2) = nδ(0,0)(x1, x2) and topple until stable usingthe uniform toppling rule.The stable sandpile has a limit shape (Pegden-Smart2013).
Toppling rule
+1
+1 −4
OO
//
��
oo +1
+1
Theorem (Levine-Peres 2008)The limit shape is boundedbetween circles of radii c1
√n
and c2√
n with c2/c1 =√
3√2. Figure: Stable sandpile with n = 107.
Colors correspond to heights of sandpile.
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What is the limit shape of the ASM?The boundary of the limit shape is a Lipschitz graph(Aleksanyan-Shahgholian 2019)
Figure: Stable sandpile with n = 107. Colors correspond to heights ofsandpile.
Is the limit shape convex? Is it a circle, a polygon, or neither?
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Directed ASM
The toppling rule determines the limit shape:
Figure: Stable sandpile with n = 105. Black sites haveone grain of sand.
Toppling rule
+1
−2
OO
// +1
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Leaky Abelian Sandpile Model (Leaky-ASM)
We compute the limit shape in the presence of dissipation.
An initial sandpile distribution s : V → R≥0Dissipation d > 1
If s(x) > d · deg(x) then x isunstable and topplesdistributing sand to itsneighbors:{
s(x) 7→ s(x)− d · deg(x)s(y) 7→ s(y) + 1 if y ∼ x .
Uniform ASM withdissipation
+1
+1 −4d
OO
//
��
oo +1
+1
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Leaky Abelian Sandpile Model (Leaky-ASM)
We compute the limit shape in the presence of dissipation.
An initial sandpile distribution s : V → R≥0Dissipation d > 1
If s(x) > d · deg(x) then x isunstable and topplesdistributing sand to itsneighbors:{
s(x) 7→ s(x)− d · deg(x)s(y) 7→ s(y) + 1 if y ∼ x .
Uniform ASM withdissipation
+1
+1 −4d
OO
//
��
oo +1
+1
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Main ResultsLet s(x) = nδ(0,0)(x) and topple until stable using theuniform toppling rule.Dn,d is the set of sites which have toppled.
Theorem (A.- Mkrtchyan 2020)
Let d > 1 and r = log n − 12 log log n. The boundary of r−1Dn,d
converges to the dual of the boundary of the gaseous phase inthe amoeba of the spectral curve for the toppling rule.
Theorem (A.- Mkrtchyan 2020)Let dn = 1 + tn.
If tn � 1log(n) then the boundary of√
tnlog(n)
Dn,d converges to
a circle.If tn � 1n1−α with 0 < α < 1, then the boundary of√
tnlog(n)
Dn,d is between circles of radii c1 and c2 withc1c2→α.
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Main ResultsLet s(x) = nδ(0,0)(x) and topple until stable using theuniform toppling rule.Dn,d is the set of sites which have toppled.
Theorem (A.- Mkrtchyan 2020)
Let d > 1 and r = log n − 12 log log n. The boundary of r−1Dn,d
converges to the dual of the boundary of the gaseous phase inthe amoeba of the spectral curve for the toppling rule.
Theorem (A.- Mkrtchyan 2020)Let dn = 1 + tn.
If tn � 1log(n) then the boundary of√
tnlog(n)
Dn,d converges to
a circle.If tn � 1n1−α with 0 < α < 1, then the boundary of√
tnlog(n)
Dn,d is between circles of radii c1 and c2 withc1c2→α.
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(a) d = 1.05 (b) d = 2 (c) d = 1000
Figure: Simulations of the Leaky-ASM with n ≈ 10500.
Figure: Limit shapes from theorem.
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Vanishing dissipation limit
(a) d − 1 = 2.5 · 10−4 (b) d − 1 = 2.5 · 10−5
(c) d − 1 = 2.5 · 10−6 (d) d − 1 = 2.5 · 10−7
Figure: Leaky-ASM simulations with n = 107.
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Limiting sandpile
Figure: Uniform ASM with background height −1 and n = 107.Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Vanishing dissipation limit converges to uniform ASM
Theorem (A.- Mkrtchyan (2020))As d → 1 the stable sandpile of the Leaky-ASM convergespointwise to the stable sandpile of the ASM with backgroundheight −1.
Sketch of proof:Couple the leaky-ASM to a modified ASM in which sites toppleif they have 5 or more grains of sand.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Background
ASM introduced by Bak-Tang-Wiesenfeld in 1987 as amodel for fractals and self-organized criticality.
At each time step a site is chosen randomly and one grainof sand is added. All unstable sites topple. The distributionof avalanches has a power law tail (Dhar 2006?).
Dissipative sandpiles introduced by Manna-Kiss-Kertész in1990 to model systems in which the average transfer ratiois a parameter or random quantity
Avalanches of thermal neutrons in a nuclear reactorcontrolled by cadmium rods are one example.
Dhar-Sadhu (2013) proposed using sandpiles to modelpattern formation and proportionate growth.
The odometer is piecewise quadratic (Ostojic 2003).A limit pattern exists (Pegden-Smart 2013).The internal fractal structure is connected to Apolloniancircle packings (Levine-Pegden-Smart 2016 andPegden-Smart 2020).
The ASM is a discrete model of a free boundary problem.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
-
Background
ASM introduced by Bak-Tang-Wiesenfeld in 1987 as amodel for fractals and self-organized criticality.
At each time step a site is chosen randomly and one grainof sand is added. All unstable sites topple. The distributionof avalanches has a power law tail (Dhar 2006?).
Dissipative sandpiles introduced by Manna-Kiss-Kertész in1990 to model systems in which the average transfer ratiois a parameter or random quantity
Avalanches of thermal neutrons in a nuclear reactorcontrolled by cadmium rods are one example.
Dhar-Sadhu (2013) proposed using sandpiles to modelpattern formation and proportionate growth.
The odometer is piecewise quadratic (Ostojic 2003).A limit pattern exists (Pegden-Smart 2013).The internal fractal structure is connected to Apolloniancircle packings (Levine-Pegden-Smart 2016 andPegden-Smart 2020).
The ASM is a discrete model of a free boundary problem.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
-
Background
ASM introduced by Bak-Tang-Wiesenfeld in 1987 as amodel for fractals and self-organized criticality.
At each time step a site is chosen randomly and one grainof sand is added. All unstable sites topple. The distributionof avalanches has a power law tail (Dhar 2006?).
Dissipative sandpiles introduced by Manna-Kiss-Kertész in1990 to model systems in which the average transfer ratiois a parameter or random quantity
Avalanches of thermal neutrons in a nuclear reactorcontrolled by cadmium rods are one example.
Dhar-Sadhu (2013) proposed using sandpiles to modelpattern formation and proportionate growth.
The odometer is piecewise quadratic (Ostojic 2003).A limit pattern exists (Pegden-Smart 2013).The internal fractal structure is connected to Apolloniancircle packings (Levine-Pegden-Smart 2016 andPegden-Smart 2020).
The ASM is a discrete model of a free boundary problem.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
-
Background
ASM introduced by Bak-Tang-Wiesenfeld in 1987 as amodel for fractals and self-organized criticality.
At each time step a site is chosen randomly and one grainof sand is added. All unstable sites topple. The distributionof avalanches has a power law tail (Dhar 2006?).
Dissipative sandpiles introduced by Manna-Kiss-Kertész in1990 to model systems in which the average transfer ratiois a parameter or random quantity
Avalanches of thermal neutrons in a nuclear reactorcontrolled by cadmium rods are one example.
Dhar-Sadhu (2013) proposed using sandpiles to modelpattern formation and proportionate growth.
The odometer is piecewise quadratic (Ostojic 2003).A limit pattern exists (Pegden-Smart 2013).The internal fractal structure is connected to Apolloniancircle packings (Levine-Pegden-Smart 2016 andPegden-Smart 2020).
The ASM is a discrete model of a free boundary problem.Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Computing the limit shape of the Leaky-ASM
Outline of our proof:Relate the Leaky-ASM to a killed random walk.
Use the steepest descent method to compute theasymptotic death probability.
Level curves of4n
and4(d − 1)
nin the death probability
bound the Leaky-ASM with n chips started at the origin.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Computing the limit shape of the Leaky-ASM
Outline of our proof:Relate the Leaky-ASM to a killed random walk.Use the steepest descent method to compute theasymptotic death probability.
Level curves of4n
and4(d − 1)
nin the death probability
bound the Leaky-ASM with n chips started at the origin.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
-
Computing the limit shape of the Leaky-ASM
Outline of our proof:Relate the Leaky-ASM to a killed random walk.Use the steepest descent method to compute theasymptotic death probability.
Level curves of4n
and4(d − 1)
nin the death probability
bound the Leaky-ASM with n chips started at the origin.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Killed random walkLet X1,X2, . . . be i.i.d random variables with
P{Xj = (1,0)} =1
4d, P{Xj = (−1,0)} =
14d
,
P{Xj = (0,1)} =1
4d, P{Xj = (0,−1)} =
14d
,
P{Xj = (0,0)} = 1−4
4d= 1− 1
d.
The killed random walk (KRW) started at x ∈ Z2 is thesequence S1,S2, . . . where
Sn = x +n∑
i=1
KiXi
and
Ki =
{1 if the walker is alive at step i0 else.
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Connection to sandpiles
Let Gd (x) = P(walker dies at x) be the death probability.
DefinitionThe odometer function u(x) = total sand emitted from x .
Start with initial sandpile s(x) = nδ0,0(x) and topple untilreaching the stable sandpile s∞(x).
Proposition (A.-Mkrtchyan 2020)For the operator
T =1d
∆−(
d − 1d
)I
we have
T (u(x)−Gd (x)) =d − 1
dns∞(x).
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Connection to sandpiles
Let Gd (x) = P(walker dies at x) be the death probability.
DefinitionThe odometer function u(x) = total sand emitted from x .
Start with initial sandpile s(x) = nδ0,0(x) and topple untilreaching the stable sandpile s∞(x).
Proposition (A.-Mkrtchyan 2020)For the operator
T =1d
∆−(
d − 1d
)I
we have
T (u(x)−Gd (x)) =d − 1
dns∞(x).
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Connection to sandpiles
Let Gd (x) = P(walker dies at x) be the death probability.
DefinitionThe odometer function u(x) = total sand emitted from x .
Start with initial sandpile s(x) = nδ0,0(x) and topple untilreaching the stable sandpile s∞(x).
Proposition (A.-Mkrtchyan 2020)For the operator
T =1d
∆−(
d − 1d
)I
we have
T (u(x)−Gd (x)) =d − 1
dns∞(x).
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Key lemma
“Invert”
T =1d
∆−(
d − 1d
)I
and use inequality0 ≤ s∞(x) < 4d
to obtain the key lemma:
Lemma (A.-Mkrtchyan 2020)
1 If Gd (x) <4(d − 1)
n, then u(x) = 0, i.e. x 6∈ Dn,d .
2 If Gd (x) ≥4dn
, then u(x) ≥ 4d, i.e. x ∈ Dn,d .
Dn,d is the set of sites which topple.
Consequence
Asymptotics of Gd (x) give the boundary of the limit shape.
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Key lemma
“Invert”
T =1d
∆−(
d − 1d
)I
and use inequality0 ≤ s∞(x) < 4d
to obtain the key lemma:
Lemma (A.-Mkrtchyan 2020)
1 If Gd (x) <4(d − 1)
n, then u(x) = 0, i.e. x 6∈ Dn,d .
2 If Gd (x) ≥4dn
, then u(x) ≥ 4d, i.e. x ∈ Dn,d .
Dn,d is the set of sites which topple.
Consequence
Asymptotics of Gd (x) give the boundary of the limit shape.
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Massive Laplacian
The spectral curve of the massive Laplacian can be used tocompute asymptotics of Gd (x).
Definition
The massive Laplacian ∆m : CV → CV is defined by
(∆mf )(x) =∑y∼x
P(x → y)(f (y)− f (x))− P(dies)f (x)
=∑y∼x
P(x → y)f (y)− f (x)
where P(x → y) is the probability that the KRW moves fromvertex x to y and P(dies) is the probability it is killed.
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Spectral curve of KRW
When the probabilities are periodic the spectral curve is
P(z,w) = det ∆m(z,w).
Probabilities are modified by z or w when crossing afundamental domain.
For the KRW the fundamental domain has size 1× 1 and
(∆mf )(x) =∑y∼x
14d
f (y)− f (x).
∆m is a 1× 1 matrix with spectral curve
P(z,w) = 4d −(
z + z−1 + w + w−1).
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Spectral curve of KRW
When the probabilities are periodic the spectral curve is
P(z,w) = det ∆m(z,w).
Probabilities are modified by z or w when crossing afundamental domain.For the KRW the fundamental domain has size 1× 1 and
(∆mf )(x) =∑y∼x
14d
f (y)− f (x).
∆m is a 1× 1 matrix with spectral curve
P(z,w) = 4d −(
z + z−1 + w + w−1).
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Asymptotic death probability
Expand the normalized spectral curve in a power seriesconvergent near (1,1) to compute probabilities:
4(d − 1)P(z,w)
=4(d − 1)
4d − (z + z−1 + w + w−1)
=d − 1
d
∞∑k=0
(z + z−1 + w + w−1
4d
)k=∑
k ,l∈ZGd (k , l)zkw l ,
where Gd (k , l) is the probability the KRW dies at (k , l).
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Contour integration gives the coefficients in the directionva = (1,a) for 0 < a < 1:
Gd (rva) =1
(2πi)2
∮Cw
∮Cz
4(d − 1)P(z,w)
dzzr+1
dwwar+1
=4(d − 1)
2πi
∮C
f (w)erS(w)dw
where
f (w) =1
w√
(4d − w − 1/w)2 − 4
S(w) = log
4d − w − 1w −√(
4d − w − 1w)2 − 4
2wa
.
Use the steepest descent method to compute the asymptotics.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Contour integration gives the coefficients in the directionva = (1,a) for 0 < a < 1:
Gd (rva) =1
(2πi)2
∮Cw
∮Cz
4(d − 1)P(z,w)
dzzr+1
dwwar+1
=4(d − 1)
2πi
∮C
f (w)erS(w)dw
where
f (w) =1
w√
(4d − w − 1/w)2 − 4
S(w) = log
4d − w − 1w −√(
4d − w − 1w)2 − 4
2wa
.Use the steepest descent method to compute the asymptotics.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Steepest descent methodLet w+ be the real critical point of S(w) with w+ > 1Deform the contour of integration to pass through thecritical point and make the change of variablew = w+ + i y√r :
Gd (rva) =4(d − 1)
2πi
∮C
f (w)erS(w)dw
=4(d − 1)
2π√
rf (w+)erS(w+)
∫ ∞−∞
e−S′′(w+)y2
2 (1 + o(1))dy .
=4(d − 1)√2πS′′(w+)r
f (w+)erS(w+)(1 + o(1)).
Solving
Gd (rova) =4(d − 1)
nand Gd (riva) =
4dn.
gives the boundaries for the limit shape.
-
Steepest descent methodLet w+ be the real critical point of S(w) with w+ > 1Deform the contour of integration to pass through thecritical point and make the change of variablew = w+ + i y√r :
Gd (rva) =4(d − 1)
2πi
∮C
f (w)erS(w)dw
=4(d − 1)
2π√
rf (w+)erS(w+)
∫ ∞−∞
e−S′′(w+)y2
2 (1 + o(1))dy .
=4(d − 1)√2πS′′(w+)r
f (w+)erS(w+)(1 + o(1)).
Solving
Gd (rova) =4(d − 1)
nand Gd (riva) =
4dn.
gives the boundaries for the limit shape.
-
The limit shape for initial sandpile s0 = nδ(0,0) is parametrizedby
− log(n)(
1S(w+)
,a
S(w+)
)for 0 ≤ a ≤ 1,
and its reflections with respect to the coordinate axes and theline y = x .
Figure: Limit shapes with d = 1.05,2, and 1000.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Limit Shapes and AmoebaeThe amoeba of a polynomial P(z,w) is the image of{(z,w) ∈ C2 : P(z,w) = 0} under the map
(z,w) 7→ (log |z|, log |w |).
Figure: The boundary of the amoeba ofP(z,w) = 4d −
(z + z−1 + w + w−1
)and its dual curve. The red
curve bounds the gaseous phase.
DefinitionThe bounded complementary component of an amoeba is thegaseous phase.
-
Theorem (A.-Mkrtchyan 2020)The limit shape of the Leaky-ASM is (up to scale) the dual ofthe boundary of the gaseous phase in the amoeba.
For P(z,w) = 4d −(z + z−1 + w + w−1
)the boundary of
the gaseous phase is given by the implicit equation
4d = ex + e−x + ey + e−y with x , y ∈ R.
The boundary of the gaseous phase is z,w ∈ R with zw > 0.
The other boundary components correspond to zw < 0.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Theorem (A.-Mkrtchyan 2020)The limit shape of the Leaky-ASM is (up to scale) the dual ofthe boundary of the gaseous phase in the amoeba.
For P(z,w) = 4d −(z + z−1 + w + w−1
)the boundary of
the gaseous phase is given by the implicit equation
4d = ex + e−x + ey + e−y with x , y ∈ R.
The boundary of the gaseous phase is z,w ∈ R with zw > 0.
The other boundary components correspond to zw < 0.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Theorem (A.-Mkrtchyan 2020)The limit shape of the Leaky-ASM is (up to scale) the dual ofthe boundary of the gaseous phase in the amoeba.
For P(z,w) = 4d −(z + z−1 + w + w−1
)the boundary of
the gaseous phase is given by the implicit equation
4d = ex + e−x + ey + e−y with x , y ∈ R.
The boundary of the gaseous phase is z,w ∈ R with zw > 0.
The other boundary components correspond to zw < 0.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Why do amoebae appear?
Asymptotic level curves of
Gd (rva) =4(d − 1)
2πi
∮C
f (w)erS(w)dw
correspond to the limit shape.If the model has a spectral curve P(z,w) andS(w) = − ln(zwa) for (z,w) satisfying P(z,w) = 0 then theasymptotic level curves of Pd (rva) are given by theboundary of the gaseous phase in the amoeba.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model
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Thank you!I. Alevy and S. Mkrtchyan, The Limit Shape of the LeakyAbelian Sandpile Model,arXiv e-prints , arXiv:2010.01946 (October 2020),2010.01946.
Ian M. Alevy The Limit Shape of the Leaky Abelian Sandpile Model