Lattice Statistics on Kagome-Type Lattices
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Transcript of Lattice Statistics on Kagome-Type Lattices
Lattice Statistics on Kagome-Type Lattices
F. Y. Wu
Northeastern University
Kagome-type lattices
Syozi
Physics Today, 56 (Feb) 12 (2003).
(a) (b) (c)
Kagome Triangular kagomeKagome lattice with an internal structure
Kagome lattice 3-12 lattice
Kagome lattice with 3-site interactions 3-12 lattice with 3-site interactions
There has been a surge of recent interest in considering the “triangular kagome” lattice such as
Closed-packed dimers on the triangular kagome latticeY. L. Loh, D.-X. Yao, C. L. Carlson, PRB 78, 224410 (2008)
Bond percolation on the triangular kagome latticeA. Haji-Ankabari and R. M. Ziff, PRE 79 021118 (2009)
Close-packed dimers on the kagome lattice(and the triangular kagome lattice)
6/)(constant NxyzZ
The constant can be determined by a simple mapping
6/4constant N
F. Y. Wu and F. Wang, Physica A 387 (2008) 4148
Dimer-dimer correlation vanishes identically at distances greater than 2 lattice spacing
F. Wang and F. Y. Wu, Physica A 387 (2008) 4157
Potts model on the kagome lattice
Triangular lattice with 3-site interactions
),(),(),(),(,,,
kjKrkkji
jKrjiKrjji
iKr MK
Exact duality relation: Baxter, Temperley and Ashley (1978) using algebraic analysis Wu and Lin (1979) using graphical method
kjiijk
jiij MK
,,,
1 Kev 1* * Kev,
233 KMK eey 23* ***3 KMK eey,
The duality relation reads
qvyv *2* qyy ,
The self-dual point is v=v*, y = y* = q, or
qee KMK 233
Using a continuity argument, Wu and Zia (1981) established that this is indeed the critical point of the ferromagnetic triangular Potts model.
Exact duality relation
Define
123312312
123312312
)(1
])1(1)[1)(1)(1(
yv
evvv M
Generally, for
123312312 )( CBA
qAC
the critical point is C/A=q, or
for the lattice
1 Kevthe critical point is y=q.
Generalization
Example 1: 2x2 subnet
=
)1)(1)(1(
)1)(1)(1)(1)(1)(1(
465645
35342624166,5,4
15
vvv
vvvvvv
123312312 )( CBA
1 Kev
)]61518(3)[3(
)72230()5(2
)32150()433(9
3254
324322
23223
vvvvqvvC
vvvvvqvvqB
vvvvqvvqqA
Bond percolation:
0124572453931 98765432 pppppppp
C=qA gives
cp 0.471 628 788 268… (exact)
Kep 1q=1,
In agreement withHaji-Akbari and Ziff (Phys. Rev. E 79 020102(R) (2009))who obtained the result using a different consideration
q=2,Ising2KK eeu
C=qA gives
and the Ising critical point
5IsingKe 2.236 067 977 500…
Ising model:
0)1)(5( 2223 uuu
For the q=3 Potts model, C=qA gives
Ke 2.493 123 120 701 …
Example 2: The martini lattice (Wu. PRL 96 (2006) 090602)
=
0)3()316()15(6 532224 vvvqvvvqvqq
In agreement with Ziff and Scullard, JPA 39 (2006) 15083
For bond percolation with q=1, v=p/(1-p), this gives
12)(2 65432 ppppp
qee KMK 233
Triangular lattice with alternate 3-site interactions M and 0:
Conjecture (Wu, 1979)
Triangular lattice with alternate 3-site interactions M and N:
qee KNMK 233MMM
M
N
M
N N N
M
Exact expression
qee KMK 2323
Triangular lattice with 3-site interactions M in every face:
M M MM M M M
Star-triangle transformation: Diced lattice
T
Duality transformation:
Diced lattice kagome lattice
This gives the kagome critical threshold
0692126 6543223 vvvqvqvvqq
1 cKev
(Wu, 1979)
N’
N
L’L
K
M’ K
K
M’M’ M’
M’M
M
M M
M
N’
N
K’
Duality relation for Potts model with multi-site interactions(Essam, 1979; Wu, 1982)
22' )1)(1( ,)1)(1( ,)1)(1(''
qeeqeeqee NMNMKK
Kagome lattice with 2- and 3-site interactions K and M
3-12 lattice with 2- and 3-site interactions K* and M*
=
Using the exact duality relation
2*
*
)1)(1(
)1)(1(
qee
qeeMM
KK
General formulation for the kagome-type lattices:
dualityM
MM
M*
M*
K
K*K
K*
K*
=K* .L L
123312312 )( CBA =L
LLM*
)1(
)1(
)]1)(3()[(
*3
*2
*3
M
M
M
eFvC
eFvB
evqvqFA
1 Lev
Solve F, , , hence , in terms of A, B, C Le *Me Ke Me
qee KMK 2323
The conjectured threshold
2222 )2()(3)3( CqCqBCqBAq
gives the threshold for the general problem in terms of A, B. C
=
=
123312312 )( CBA
qee KNMK 233
More generally, the conjectured threshold
')2()'')((3)''3')(3( 22 CCqCqBCqBCqBAqCqBAq
gives the threshold for the general A, B. C, A’, B’, C’ problem
=
=
123312312 )( CBA
123312312 ')('' CBA
The 3-12 lattice
For the 3-12 lattice with uniform interactions K, the threshold is:
23 ,1 vvrev K
632422233 )2())((3)]()[()( rvqrqvqrvqrvqrqvq
For bond percolation, q=1, v=p/(1-p), this gives
For the Ising model, q=2, this gives
08862 234 vvvv
]13[]3341[ cv = 4.073 446 135 … (Soyzi, 1972)
... 317 423 0.740 cp
0471 5432 ppppp
(Scullard and Ziff (PRE 73 (2006) 045102)
1 Kev
For the lattice with uniform interactions K:
)]61518(3)[3(
)72230()5(2
)32150()433(9
3254
324322
23223
vvvvqvvC
vvvvvqvvqB
vvvvqvvqqA
For percolation, q=1 and v=p/(1-p), this gives
0737863708994816359162368232
12617852642733039183118171615141312
1110967654
ppppppp
pppppppp
cp
cp
= 0.600 870 248 238 …
This is compared to the Ziff-Gu (2009) numerical result
= 0.600 862 4
For Ising model, q=2 and v=p/(1-p), this gives the exact result
0863283 8642 uuuu
3.024 382 957 092 ,,,, Ising2Keu
The End