Difference between revisions of "Simulation in the aTAM"
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==Informal Description of Simulation== | ==Informal Description of Simulation== | ||
− | For TAS's $\mathcal{T}$ and $\mathcal{S}$, simulation of $\mathcal{T}$ by $\mathcal{S}$ can be done according to a simple "block substitution scheme" where equal-size square blocks of tiles in assemblies produced by $\mathcal{S}$ represent tiles in assemblies produced by $\mathcal{T}$. Furthermore, since we wish to simulate the entire process of self-assembly, and not only the final result, it is critical that the simulation be such that the "local transition rules" involving intermediate producible (and nonterminal) assemblies of $\mathcal{T}$ be faithfully represented in the simulation. | + | For TAS's $\mathcal{T}$ and $\mathcal{S}$, simulation of $\mathcal{T}$ by $\mathcal{S}$ can be done according to a simple "block substitution scheme" where equal-size square blocks of tiles in assemblies produced by $\mathcal{S}$ represent tiles in assemblies produced by $\mathcal{T}$. Furthermore, since we wish to simulate the entire process of self-assembly, and not only the final result, it is critical that the simulation be such that the "local transition rules" involving intermediate producible (and nonterminal) assemblies of $\mathcal{T}$ be faithfully represented in the simulation. Simulation has been studied in the context of [[Intrinsic universality of the aTAM | intrinsic universality]]<ref name=USA /><ref name=IUSA />. |
===Example=== | ===Example=== | ||
− | A single tile that assembles a line can be simulation in such a way that each tile of the simulated line is represented by $2\times 2$ blocks. | + | A single tile that assembles a line can be simulation in such a way that each tile of the simulated line is represented by $2\times 2$ blocks. This basic example is meant to capture the idea of simulation using block representation. In practice, simulation is achieved using block sizes much larger than $2\times 2$<ref name=IUSA />. |
{{multiple image | {{multiple image | ||
| align = center | | align = center | ||
− | + | | footer = A TAS with the tile set in the middle can simulate a TAS with tile set consisting of the single tile on the left. Simulation is depicted in the figure on the right. | |
− | | footer = A TAS with the tile set | ||
| image1 = Line_tile.png | | image1 = Line_tile.png | ||
| alt1 = A single tile that assembles a line | | alt1 = A single tile that assembles a line | ||
Line 14: | Line 13: | ||
| image2 = 2block_line_tiles.png | | image2 = 2block_line_tiles.png | ||
| alt2 = A tile set that simulates single tile line assembly | | alt2 = A tile set that simulates single tile line assembly | ||
− | | caption2 = | + | | caption2 = Seeded with a single $2\times 2$ block representing the single tile $L$, this tile set will simulate the assembly of the line with $2$-block super-tiles. |
| image3 = Simulation_line.png | | image3 = Simulation_line.png | ||
| width3 = 360 | | width3 = 360 | ||
Line 23: | Line 22: | ||
==Formal Definition== | ==Formal Definition== | ||
− | === | + | Since the notion of simulation is intended to capture not only what is being assembled by a TAS but also how assembly takes place, the definition has been split into two parts: ''equivalent production'' and ''equivalent dynamics''. The definition of both of these uses the idea of block representation. |
+ | |||
+ | ===Block Representation=== | ||
From this point on, let $T$ be a $d$-dimensional tile set, and let | From this point on, let $T$ be a $d$-dimensional tile set, and let | ||
$m\in\mathbb{Z}^+$. | $m\in\mathbb{Z}^+$. | ||
Line 63: | Line 64: | ||
==References== | ==References== | ||
<references> | <references> | ||
+ | |||
+ | <ref name =USA><bibtex> | ||
+ | @inproceedings{USA, | ||
+ | author = "David Doty and Jack H. Lutz and Matthew J. Patitz and Scott M. Summers and Damien Woods", | ||
+ | title = "Intrinsic Universality in Self-Assembly", | ||
+ | booktitle = "Proceedings of the 27th International Symposium on Theoretical Aspects of Computer Science", | ||
+ | year = 2009, | ||
+ | pages = "275--286" | ||
+ | } | ||
+ | </bibtex></ref> | ||
+ | |||
+ | <ref name =IUSA><bibtex> | ||
+ | @inproceedings{IUSA, | ||
+ | author = {David Doty and | ||
+ | Jack H. Lutz and | ||
+ | Matthew J. Patitz and | ||
+ | Robert T. Schweller and | ||
+ | Scott M. Summers and | ||
+ | Damien Woods}, | ||
+ | title = {The tile assembly model is intrinsically universal}, | ||
+ | booktitle = {Proceedings of the 53rd Annual IEEE Symposium on Foundations of Computer Science}, | ||
+ | series = {FOCS 2012}, | ||
+ | year = {2012}, | ||
+ | location = {New Brunswick, New Jersey}, | ||
+ | } | ||
+ | </bibtex></ref> | ||
</references> | </references> | ||
[[Category: Simulation in Self-assembly]] | [[Category: Simulation in Self-assembly]] |
Latest revision as of 16:45, 12 July 2013
Contents
Informal Description of Simulation
For TAS's \(\mathcal{T}\) and \(\mathcal{S}\), simulation of \(\mathcal{T}\) by \(\mathcal{S}\) can be done according to a simple "block substitution scheme" where equal-size square blocks of tiles in assemblies produced by \(\mathcal{S}\) represent tiles in assemblies produced by \(\mathcal{T}\). Furthermore, since we wish to simulate the entire process of self-assembly, and not only the final result, it is critical that the simulation be such that the "local transition rules" involving intermediate producible (and nonterminal) assemblies of \(\mathcal{T}\) be faithfully represented in the simulation. Simulation has been studied in the context of intrinsic universality[1][2].
Example
A single tile that assembles a line can be simulation in such a way that each tile of the simulated line is represented by \(2\times 2\) blocks. This basic example is meant to capture the idea of simulation using block representation. In practice, simulation is achieved using block sizes much larger than \(2\times 2\)[2].
Formal Definition
Since the notion of simulation is intended to capture not only what is being assembled by a TAS but also how assembly takes place, the definition has been split into two parts: equivalent production and equivalent dynamics. The definition of both of these uses the idea of block representation.
Block Representation
From this point on, let \(T\) be a \(d\)-dimensional tile set, and let \(m\in\mathbb{Z}^+\). An \(m\)-block supertile over \(T\) is a partial function \(\alpha:\mathbb{Z}_m^d \dashrightarrow T\), where \(\mathbb{Z}_m = \{0,1,\ldots,m-1\}\). Note that the dimension of the \(m\)-block is implicitly defined by the dimension of \(T\). Let \(B^T_m\) be the set of all \(m\)-block supertiles over \(T\). The \(m\)-block with no domain is said to be empty. For a general assembly \(\alpha:\mathbb{Z}^d \dashrightarrow T\) and \((x_0,\ldots x_{d-1})\in\mathbb{Z}^d\), define \(\alpha^m_{x_0,\ldots x_{d-1}}\) to be the \(m\)-block supertile defined by \(\alpha^m_{x_0,\ldots, x_{d-1}}(i_0,\ldots, i_{d-1}) = \alpha(mx_0+i_0,\ldots, mx_{d-1}+i_{d-1})\) for \(0 \leq i_0, \ldots, i_{d-1}< m.\) For some tile set \(S\) of dimension \(d' \geq d\), a partial function \(R: B^{S}_m \dashrightarrow T\) is said to be a valid \(m\)-block supertile representation from \(S\) to \(T\) if for any \(\alpha,\beta \in B^{S}_m\) such that \(\alpha \sqsubseteq \beta\) and \(\alpha \in \dom R\), then \(R(\alpha) = R(\beta)\).
Let \(d' \in \{ 2,3 \}\) and \(d \in \{ d' -1, d' \} \). Let \(f: \mathbb{Z}^{d'} \rightarrow \mathbb{Z}^{d}\), where \(f(x_0,\ldots,x_{d'-1}) = (x_0,\ldots,x_{d'-1})\) if \(d'=d\) and \(f(x_0,\ldots,x_{d'-1}) = (x_0,\ldots,x_{d-1},0)\) if \(d = d' -1\), and undefined otherwise. For a given valid \(m\)-block supertile representation function \(R\) from tile set \(S\) to tile set \(T\), define the assembly representation function \(R^*: \mathcal{A}^{S} \rightarrow \mathcal{A}^T\) such that \(R^*(\alpha') = \alpha\) if and only if \(\alpha(x_0,\ldots, x_{d-1}) = R\left(\alpha'^m_{x_0,\ldots, x_{d'-1}}\right)\) for all \((x_0,\ldots x_{d'-1}) \in \Z^{d'-1}\). Note that \(R^*\) is a total function since every assembly of \(S\) represents some assembly of \(T\); the functions \(R\) and \(\alpha\) are partial to allow undefined points to represent empty space. For an assembly \(\alpha' \in \mathcal{A}^{S}\) such that \(R(\alpha') = \alpha\), \(\alpha'\) is said to map cleanly to \(\alpha \in \mathcal{A}^T\) under \(R^*\) if for all non empty blocks \(\alpha'^m_{x_0,\ldots, x_{d'-1}},\) \((f(x_0,\ldots,x_{d'-1})+f(u_0,\ldots,u_{d'-1})) \in \dom \alpha\) for some \(u_0,\ldots, u_{d'-1} \in \{-1,0,1\}\) such that \(u_0^2 + \cdots + u_{d'-1}^2 \leq 1\), or if \(\alpha'\) has at most one non-empty \(m\)-block \(\alpha^m_{0, \ldots, 0}\). In other words, \(\alpha'\) may have tiles on supertile blocks representing empty space in \(\alpha\), but only if that position is adjacent to a tile in \(\alpha\). We call such growth "around the edges" of \(\alpha'\) fuzz and thus restrict it to be adjacent to only valid supertiles, but not diagonally adjacent (i.e. we do not permit diagonal fuzz).
In the following definitions, let \(\mathcal{T} = \left(T,\sigma_T,\tau_T\right)\) be a \(d\)-TAS for \(d \in \{2,3\}\), let \(\mathcal{S} = \left(S,\sigma_S,\tau_S\right)\) be a \(d'\)-TAS for \(d' \geq d\), and let \(R\) be an \(m\)-block representation function \(R:B^S_m \rightarrow T\).
Equivalent production
We say that \(\mathcal{S}\) and \(\mathcal{T}\) have equivalent productions (under \(R\)), and we write \(\mathcal{S} \Leftrightarrow \mathcal{T}\) if the following conditions hold:
- \(\left\{R^*(\alpha') | \alpha' \in \prodasm{\mathcal{S}}\right\} = \prodasm{\mathcal{T}}\).
- \(\left\{R^*(\alpha') | \alpha' \in \termasm{\mathcal{S}}\right\} = \termasm{\mathcal{T}}\).
- For all \(\alpha'\in \prodasm{\mathcal{S}}\), \(\alpha'\) maps cleanly to \(R^*(\alpha')\).
Equivalent dynamics
Follows
We say that \(\mathcal{T}\) follows \(\mathcal{S}\) (under \(R\)), and we write \(\mathcal{T} \dashv_R \mathcal{S}\) if \(\alpha' \rightarrow^\mathcal{S} \beta'\), for some \(\alpha',\beta' \in \mathcal{A}[\mathcal{S}]\), implies that \(R^*(\alpha') \to^\mathcal{T} R^*(\beta')\).
Models
We say that \(\mathcal{S}\) models \(\mathcal{T}\) (under \(R\)), and we write \(\mathcal{S} \models_R \mathcal{T}\), if for every \(\alpha \in \mathcal{A}[\mathcal{T}]\), there exists \(\Pi \subset \mathcal{A}[\mathcal{S}]\) where \(R^*(\alpha') = \alpha\) for all \(\alpha' \in \Pi\), such that, for every \(\beta \in \mathcal{A}[\mathcal{T}]\) where \(\alpha \rightarrow^\mathcal{T} \beta\), (1) for every \(\alpha' \in \Pi\) there exists \(\beta' \in \mathcal{A}[\mathcal{S}]\) where \(R^*(\beta') = \beta\) and \(\alpha' \rightarrow^\mathcal{S} \beta'\), and (2) for every \(\alpha'' \in \mathcal{A}[\mathcal{S}]\) where \(\alpha'' \rightarrow^\mathcal{S} \beta'\), \(\beta' \in \mathcal{A}[\mathcal{S}]\), \(R^*(\alpha'') = \alpha\), and \(R^*(\beta') = \beta\), there exists \(\alpha' \in \Pi\) such that \(\alpha' \rightarrow^\mathcal{S} \alpha''\).
The previous definition essentially specifies that every time \(\mathcal{S}\) simulates an assembly \(\alpha \in \mathcal{A}[\mathcal{T}]\), there must be at least one valid growth path in \(\mathcal{S}\) for each of the possible next steps that \(\mathcal{T}\) could make from \(\alpha\) which results in an assembly in \(\mathcal{S}\) that maps to that next step.
Simulation
We say that \(\mathcal{S}\) simulates \(\mathcal{T}\) (under \(R\)) if \(\mathcal{S} \Leftrightarrow_R \mathcal{T}\) (equivalent productions), \(\mathcal{T} \dashv_R \mathcal{S}\) and \(\mathcal{S} \models_R \mathcal{T}\) (equivalent dynamics).
References
- ↑
David Doty, Jack H. Lutz, Matthew J. Patitz, Scott M. Summers, Damien Woods - Intrinsic Universality in Self-Assembly
- Proceedings of the 27th International Symposium on Theoretical Aspects of Computer Science pp. 275--286,2009
- BibtexAuthor : David Doty, Jack H. Lutz, Matthew J. Patitz, Scott M. Summers, Damien Woods
Title : Intrinsic Universality in Self-Assembly
In : Proceedings of the 27th International Symposium on Theoretical Aspects of Computer Science -
Address :
Date : 2009
- ↑ 2.0 2.1
David Doty, Jack H. Lutz, Matthew J. Patitz, Robert T. Schweller, Scott M. Summers, Damien Woods - The tile assembly model is intrinsically universal
- Proceedings of the 53rd Annual IEEE Symposium on Foundations of Computer Science ,2012
- BibtexAuthor : David Doty, Jack H. Lutz, Matthew J. Patitz, Robert T. Schweller, Scott M. Summers, Damien Woods
Title : The tile assembly model is intrinsically universal
In : Proceedings of the 53rd Annual IEEE Symposium on Foundations of Computer Science -
Address :
Date : 2012