A033155
Configurations of linear chains for a square lattice.
Original entry on oeis.org
0, 0, 8, 32, 88, 256, 736, 2032, 5376, 14224, 36976, 95504, 243536, 619168, 1559168, 3916960, 9769072, 24321552, 60199464, 148803824, 366051864, 899559584, 2201636848, 5384254000, 13121348672, 31957730688, 77595810512
Offset: 1
- D. Bennett-Wood, I. G. Enting, D. S. Gaunt, A. J. Guttmann, J. L. Leask, A. L. Owczarek, and S. G. Whittington, Exact enumeration study of free energies of interacting polygons and walks in two dimensions, J. Phys. A: Math. Gen. 31 (1998), 4725-4741.
- M. E. Fisher and B. J. Hiley, Configuration and free energy of a polymer molecule with solvent interaction, J. Chem. Phys., 34 (1961), 1253-1267.
- Sean A. Irvine, Java program (github)
- A. M. Nemirovsky, K. F. Freed, T. Ishinabe, and J. F. Douglas, Marriage of exact enumeration and 1/d expansion methods: lattice model of dilute polymers, J. Statist. Phys., 67 (1992), 1083-1108; see Eq. 5 (p. 1090) and Eq. 7b (p. 1093).
A047057
Number of configurations of linear chains in a cubic lattice.
Original entry on oeis.org
0, 0, 24, 192, 1032, 5376, 26688, 128880, 605664, 2802576, 12755136, 57525552, 256574352, 1137418464, 5001796944, 21899428128, 95296531680, 413331190896
Offset: 1
A038749
Coefficients arising in the enumeration of configurations of linear chains.
Original entry on oeis.org
0, 0, 0, 2, 16, 96, 510, 2558, 12282, 57498, 263421, 1192480, 5330078, 23657520, 104106655, 455993276, 1984733843, 8609546380, 37164674383
Offset: 1
The first three 0's in the sequence were added by
Petros Hadjicostas, Jan 04 2019 to make it agree with Table II (p. 1093) and Eq. (5) (p. 1090) in the paper by Nemirovsky et al. (1992).
A336492
Total number of neighbor contacts for n-step self-avoiding walks on a 2D square lattice.
Original entry on oeis.org
0, 0, 8, 32, 152, 512, 1880, 5920, 19464, 59168, 183776, 545392, 1638400, 4778000, 14043224, 40422544, 116977176, 333346928, 953538440, 2695689520, 7642091352, 21464794032, 60417010152, 168787016352, 472315518008, 1313548558528, 3657850909680, 10133559518800
Offset: 1
a(1) = a(2) = 0 as a 1 and 2 step walk cannot approach a previous step.
a(3) = 8. The single walk where one interaction occurs, which can be taken in eight ways on a 2D square lattice, is:
.
+---+
|
X---+
.
Therefore, the total number of interactions is 1*1*8 = 8.
a(4) = 32. The four walks where one interaction occurs, each of which can be taken in eight ways on a 2D square lattice, are:
.
+---+---+ + +---+ +---+
| | | | |
X---+ +---+ X---+---+ X---+ +
|
X---+
.
Therefore, the total number of interactions is 4*1*8 = 32.
a(5) = 152. Considering only walks which start with one or more steps to the right followed by an upward step there are thirty-five different walks. Eleven of these have one neighbor contact (hence A033155(5) = 11*8 = 88) while four have two contacts. These are:
.
+---+---+ +---+---+ +---+ +---+
| | | | | |
+ X---+ X---+---+ +---+ + +
| |
X---+ X---+
.
Therefore, the total number of contacts is (11*1 + 4*2)*8 = 152.
- D. Bennett-Wood, I. G. Enting, D. S. Gaunt, A. J. Guttmann, J. L. Leask, A. L. Owczarek, and S. G. Whittington, Exact enumeration study of free energies of interacting polygons and walks in two dimensions, J. Phys. A: Math. Gen. 31 (1998), 4725-4741.
- M. E. Fisher and B. J. Hiley, Configuration and free energy of a polymer molecule with solvent interaction, J. Chem. Phys., 34 (1961), 1253-1267.
- A. M. Nemirovsky, K. F. Freed, T. Ishinabe, and J. F. Douglas, Marriage of exact enumeration and 1/d expansion methods: lattice model of dilute polymers, J. Statist. Phys., 67 (1992), 1083-1108.
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