Lambda counting

Introduction

This paper addresses the following question. Having a (theoretical) programming language and a property, what is the probability that a random program satisfies the given property ? In particular, is it the case that almost every random program satisfies the desired property i.e. the probability is 1 ? We consider, in this introduction, that this notion of probability is, at least intuitively, sufficiently clear but, of course, this will have to be made precise.

This kind of question has some known results for Turing machines and cellular automata. Some of them will be given in section ??. We will concentrate here on functional programming languages and, more specifically, on the lambda calculus, the simplest such language. Various properties can be studied. Some concern the structure of a term, some concern its behaviour.

The first question for which it would be desirable to have an answer is the following: give a "simple" equivalent for the number of terms of size n. This question is, at present and as far as we know, unsolved and the usual technics of generating functions does not work. See section ??? for more details. We give here upper and lower bounds for this number. This estimation will be enough for our purpose but the gap between the lower and the upper bound is to big to hope to find an equivalent.

For other questions, some experiments have already been done (see for example ...) which clearly indicates the desired result. For example, they "show" that almost every closed lambda term begins with a $\lambda$ but, as far as we know, there was no "proved" result of this form.

This paper proves some non trivial results on the structural form of a lambda term. In particular we show that almost every closed lambda term begins with "many" $\lambda$ (the precise meaning of this is given in theorem ??), that they bound "many" occurrences of the corresponding variables (theorem ??) and that, given any fixed closed term, almost no $\lambda$-term has this term as a sub-term (theorem ??).

Our original motivation was to consider the property of being terminating. Is a random term strongly normalizable (SN for short) i.e. every sequence of reduction terminates ? This question is, at present, unsolved and the experiments we have done do not even give an idea of what the result should be. It is known that being SN is an undecidable question and it is thus not easy to count the number of SN terms of big size. It is clear that having $(\delta \ \delta )$ as a sub-term is a sufficient (but not necessary) condition for being non SN but as the experiments have shown (and as we have proved) almost no terms contains $(\delta \ \delta )$ and this is thus useless to have a result for non SN. On the opposite direction, it is known that, if a term t is not SN, then a pattern "looking like" $(\delta \ \delta )$ (the precise meaning will be given in section ??) must appear in t but the experiments seem to show that almost every term possesses this pattern (actually, we have not been able to count for big enough terms to have a clear idea of the probability of possessing the desired pattern). But, again, this experimental result would be of no use to guess the result.

Another question, which is also undecidable, and for which finding the probability seems to be even more difficult, is to get the probability of being weakly normalizable i.e. there is a sequence of reduction that terminates.

Combinatory logic is another programming language related to the lambda calculus. It is a way of coding lambda terms without using bound variables. The coding is fair for the questions we are concerned with, in the sense that there are translations in both directions which, for example, preserve the property of being SN. We have also studied this language and, surprisingly, the results are very different from those for the lambda calculus. For example we show that, for every fixed term t_0, almost every term possess t_0 as a sub-term and this of course implies that almost every term is non SN. Note that the increase of size in the translation from the lambda calculus to combinatory logic is not known (we only have a lower bound) and thus results for combinatory logic cannot be used to get results for the lambda calculus.

The organization of the paper is as follows. Section ?? briefly recalls known results for Turing machines and cellular automata. Section ?? shows that, in combinatory logic, every fixed term appears in almost every term. In section ?? we recall the basic definitions of the lambda calculus and we discuss the various possibilities for counting the size of a term and the probability measure we put on sets of terms. Section ?? gives the combinatorial results we will need in our proofs and, in particular, the lower and upper bounds for the number of terms of size n. It also introduces Catalan and Motzkin numbers and the so-called Lambert function. Our main results, i.e. theorems ??, ?? and ?? appear in section ?? Section ?? gives experimental results for questions for which we have no proof. Finally, section ??? gives open questions and future work. The detailed proofs are given in an appendix.

Known results for Turing machines and cellular automata

In this section I propose to comment on paper [1] and [2].

Guillaume says: I am very skeptical about paper 2 by D'Abramo. I suggest to replace it by the paper by Calude and Stay [3].

Lambert function, Catalan and Motzkin numbers

Catalan numbers

• $C(n)$ : Catalan numbers

Usual equivalent: $C(n)\sim {\frac {4^{n}}{n^{3/2}{\sqrt {\pi }}}}$ which is obtained using Strirling formula. However, using stirling series: $n!={\sqrt {2\pi n}}\left({n \over e}\right)^{n}\left(1+{1 \over 12n}+{1 \over 288n^{2}}-{139 \over 51840n^{3}}-{571 \over 2488320n^{4}}+\cdots \right)$, we get that for $n\geq 1$ we have ${\sqrt {2\pi n}}\left({n \over e}\right)^{n}\leq n!\leq {\frac {7}{6}}{\sqrt {2\pi n}}\left({n \over e}\right)^{n}$

Thus, using this and $\left({\frac {n}{n+1}}\right)^{n}>e^{-1}$, we have:

$C(n)={\frac {(2n)!}{(n+1)!n!}}\geq {\frac {36}{49{\sqrt {\pi }}}}{\frac {4^{n}}{(n+1)^{\frac {3}{2}}}}$ for all $n\geq 1$ but also for $n=0$.

Motzkin numbers

Let us define $M(n,k)$ the number of unary-binary trees with $n$ inner nodes and $k$ leafs. We get

$M(n,k)={\frac {(n+k-1)!}{(n-k+1)!(k-1)!k!}}$

Then, by summing we define $M(n)$ the number of unary-binary trees with $n$ inner nodes and give an equivalent:

$M(n)=\sum _{k=0}^{n}M(n,k)\sim \left({\frac {1}{3-2{\sqrt {2}}}}\right)^{n}{\frac {1}{n^{\frac {3}{2}}}}$

Lambert W function

The Lambert function $W(x)$ is defined by the equation $x=W(x)e^{W(x)}$ which has a unique solution in $\mathbb {R}$.

For $x\geq e$, we have $\ln(x)-\ln(\ln(x))\leq W(x)\leq \ln(x)$ which implies that $W(x)\sim \ln(x)$ near $+\infty$. To prove this, it is enough to remark that

$(\ln(x)-\ln(\ln(x))e^{\ln(x)-\ln(\ln(x))}=x\left(1-{\frac {\ln(\ln(x))}{\ln(x)}}\right)\leq x\leq x\ln(x)=\ln(x)e^{\ln(x)}$

This is not precise enough for our purpose. Using one step of the Newton method from $\ln(x)-\ln(\ln(x))$, we can find a better upper bound for $W(x)$ because $y\mapsto ye^{y}$ is increasing and convex. This gives:

$\ln(x)-\ln(\ln(x))\leq W(x)\leq \ln(x)-\ln(\ln(x))+{\frac {\ln(\ln(x))}{\ln(x)-\ln(\ln(x))+1}}$

Indeed, if we define $f(y)=ye^{y}$, we have $f'(y)=(1+y)e^{y}$ and therefore, newton's method from $A=\ln(x)-\ln(\ln(x))$ gives a point at position:

$A-{\frac {f(A)-x}{f'(A)}}=A+{\frac {x\ln(\ln(x))}{\ln(x)}}{\frac {\ln(x)}{x(\ln(x)-\ln(\ln(x))+1)}}=A+{\frac {\ln(\ln(x))}{\ln(x)-\ln(\ln(x))+1}}$

Finally, we show that for $x\geq e$, we have:

$\ln(x)-\ln(\ln(x))\leq W(x)\leq \ln(x)-\ln(\ln(x))+1$

Indeed, for $x>1$, we have $e^{\sqrt {ex}}\geq 1+{\sqrt {ex}}+{\frac {ex}{2}}\geq x$, which implies $ex\geq \ln ^{2}(x)$ and therefore $\ln(x)-\ln \ln(x)+1\geq \ln \ln(x)$.

combinatory logic

Basically the paper already written by Marek

tex file : [4]

pdf file :[5]

+ the following

As we will see in section ??, theorem ?? does not holds for the Lambda calculus. This may be surprising since there are translations between these systems which respect many properties (for exemple the one of being terminating). However these translations do not preserve the size.

The translation $T$ from combinatory logic to lambda calculus is linear, i.e. there is a constant $k$ such that, for all terms, $size(T(t))\leq k*size(t)$ but the translation $S$ in the other direction is not linear. As far as we know, there is no known bound on the size of $S(t)$ but it is not difficult to find exemples where $size(S(t))$ is of order $size(t)^{3}$.

The point is that $S$ has to code the binding in some way and this takes place. It will be interesting to compare the size of $S(t)$ with the one of $t$ using other notion of size than the usual one. See section ?? for some complement.

Generality on lambda calculus

definition

The set $\Lambda$ of lambda terms (or, simply, terms) is defined by the following grammar

$t,u:=Var\ \mid \ \lambda x.t\ \mid \ (t\ u)$

To be able to define the notion of a random term we have to define a distribution law on $\Lambda$. There are many possibilities for that. We choose here the simplest one. Note that this is the one for which, at least at present, we are able to prove some results. It is based on densities. For that we first have to define the size of a term.

The usual definition is the following.

definition

The size (denoted as $size_{1}(t)$) of a term $t$ is defined by the following rules.

- $size_{1}(t)=1$ if $t$ is a variable.

- $size_{1}(\lambda x.t)=size_{1}(t)+1$

- $size_{1}((t\ u))=size_{1}(t)+size_{1}(u)+1$

In the rest of the paper we will use another definition (denoted as $size_{0}(t)$) which is similar but gives simpler computations. We believe (but we have not yet checked the details) that, with $size_{1}$ we would have similar results. The computation, with $size_{1}$, of the upper and lower bounds of the number of terms of size $n$ will be done in section ??

definition

The size (denoted as $size_{0}(t)$ or, more simply $size(t)$) of a term $t$ is defined by the following rules.

- $size_{0}(t)=1$ if $t$ is a variable.

- $size_{0}(\lambda x.t)=size_{0}(t)+1$

- $size_{0}((t\ u))=size_{0}(t)+size_{0}(u)+1$

These definitions of the size are, for the implementation point of view, not realistic because, in case a term has a lot of distinct variables, it is not realistic to use a single bit to code them. The usual way to implement this coding is to replace the names of variables by their so called de Bruijn indices: a variable is replaced by the number of $\lambda$ that occur, on the path from the variable to the root, between the variable and the $lambda$ that binds it. Note that, in this case, different occurrences of the same variable may be represented by different indices.

Choosing the way we code these de Bruijn indices gives different other ways of defining the size of a term. This can be done in the following ways

- Use unary notation, i.e. the size of the index $n$ simply is $n$ itself

- Use optimal binary notation, i.e. the size of the index $n$ is $log_{2}(n)$ i.e. the logarithm of $n$ in base 2.

- Use uniform binary notation, i.e. the size of an index is the logarithm, in base 2, of the number of leaves of the term.

Remark

See section ?? for a discusion about these different size.

definition

Let $n$ be an integer. We denote by $\Lambda _{n}$ the set of $\lambda$ terms of size n.

definition

Let A be a set of $\lambda$ terms.

1) We denote by $\#(A)$ the cardinality of A.

2) We denote by $d(A)$ the limit, for n going to $\infty$, of ${\frac {\#(A\cap \Lambda _{n})}{\#(\Lambda _{n})}}$.

Remark

Note that d is not exactly a measure since $d(A)$ is undefined if the previous limit does not exist

definition

Let P be a property of terms. We will say that almost every term satisfies P (this will be also stated as P holds a.e.) if $d(\{t\ |\ P(t)holds\})=1$

generating functions

this does not work (by now) because radius of convergence 0

no known results for the number of terms of size n (denoted $L_{n}$)

our results

(the proof of result of section k needs the result of section (k-1))

Upper and lower bounds for $L_{n}$

For the lower bound, we will first count the number $LB(n,k)$ of lambda-terms of size $n$ starting with $k$ lambdas and having no other lambda below. This means that the lower part of the term is a binary tree of size $n-k$ with $k$ possibility for each leaf. Therefore we have:

$LB(n,k)=C(n-k)k^{n-k+1}$

And therefore, for $n>k$, using our lower bound for $C(n)$ and $n+1\geq n-k+1$, we get:

$LB(n,k)\geq K{\frac {(4k)^{n-k+1}}{(n+1)^{\frac {3}{2}}}}$ with $K={\frac {36}{49{\sqrt {\pi }}}}$

Now, for $n$ fixed, we define $f(\alpha )=\left(4n\alpha \right)^{n(1-\alpha )+1}$ (so $LB(n,k)\geq {\frac {K}{(n+1)^{\frac {3}{2}}}}f\left({\frac {k}{n}}\right)$) and look for the maximum of this function. We have $f'(\alpha )=f(\alpha )\left(-n\ln(4n\alpha )+{\frac {n(1-\alpha )+1}{\alpha }}\right)$. Thus, $f'(\alpha )\geq 0$ is equivalent to ${\frac {n+1}{n\alpha }}e^{\frac {n+1}{n\alpha }}\geq 4e(n+1)$. The Lambert function begin increasing this means that $f'(\alpha )\geq 0$ is equivalent to $\alpha \leq {\frac {n+1}{nW(4e(n+1))}}$. Therefore, $f(\alpha )$ reaches a maximum for $\alpha ={\frac {n+1}{nW(4e(n+1))}}$.

This means that $(4k)^{n-k}$ reaches its maximum for $n$ fixed when $k$ is near to ${\frac {n+1}{W(4e(n+1))}}$ which is likely not to be an integer. However, there are at least $\left\lfloor {\frac {n(\ln(\ln(4en))-1)}{\ln ^{2}(4en)}}\right\rfloor$ integer between ${\frac {n+1}{W(4e(n+1))}}$ and ${\frac {n+1}{\ln(4e(n+1))}}$. Indeed, using our inequalities on Lambert W function, we have:

${\frac {n+1}{W(4e(n+1))}}-{\frac {n+1}{\ln(4e(n+1))}}={\frac {(n+1)(\ln(4e(n+1))-W(4e(n+1)))}{W(4e(n+1))\ln(4e(n+1))}}\geq {\frac {(n+1)(\ln(\ln(4e(n+1)))-1)}{\ln ^{2}(4e(n+1))}}$

Thus, we get the following lowerbound for $L_{n}$:

$\#(L_{n})\geq \sum _{k=1}^{n}LB(n,k)\geq \sum _{k=\lceil {\frac {n+1}{\ln(4e(n+1))}}\rceil }^{\lfloor {\frac {n+1}{W(4e(n+1))}}\rfloor }K{\frac {(4k)^{n-k+1}}{(n+1)^{\frac {3}{2}}}}\geq K\left\lfloor {\frac {(n+1)(\ln(\ln(4e(n+1)))-1)}{\ln ^{2}(4e(n+1))}}\right\rfloor {\frac {\left({\frac {4(n+1)}{\ln(4e(n+1))}}\right)^{n-{\frac {n+1}{\ln(4e(n+1))}}+1}}{(n+1)^{\frac {3}{2}}}}$

To simplify, using the fact that $\lim _{n\to +\infty }\left({\frac {\ln(n)}{\ln(4en)}}\right)^{n}=0$ and taking $n$ large enough, we have the following lowerbound:

$\#(L_{n})\geq {\frac {\sqrt {n}}{\ln ^{3}(n)}}\left({\frac {4n}{\ln(n)}}\right)^{n-{\frac {n}{\ln(n)}}}$

We now compute an upper bound $UB(n,k)$ for the number of lambda-terms of size $n$ with exactly $k$ lambdas (that is with $n-k+1$ leaves using the Motzkin numbers and allowing any lambda to bind any variable (regardless of the real scope):

$UB(n,k)=M(n,n-k+1)k^{n-k+1}$

If we sum this for all possible $k$ and get an upper bound of $k^{n-k+1}$ using Lambert function as for the lower bound, we get the following upper bound for $L_{n}$:

$\#(L_{n})\leq M(n)\left({\frac {n+1}{W(e(n+1))}}\right)^{n-{\frac {n+1}{W(e(n+1))}}+1}$

The ration between our upper bound and lower bound is equivalent to (NEEDS FURTHER CHECKING):

$\left({\frac {1}{4(3-2{\sqrt {2}})}}\right)^{n}{\frac {\ln ^{3}(n)}{n^{2}}}\simeq 1.46^{n}{\frac {\ln ^{3}(n)}{n^{2}}}$

upper and lower bounds for number of lambdas in a term of size n

Let Ls be defined as follows: lambda term of size n belongs to Ls iff it contains more than ${\frac {3n}{ln(n)}}$ lambdas.

Claim 1. Density of Ls equals 0.

Proof: straighforward using lower and upper bounds.

$Ls_{n}$ denote the number of elements of Ls of size n. It is clearly smaller then $M(n)\cdot ({\frac {3n}{ln(n)}})^{n-{\frac {3n}{ln(n)}}}.$ Dividing by the lower bound $LB(n,{\frac {n}{ln(n)}})$, we get ${\frac {M(n)}{C(n-{\frac {n}{ln(n)}})}}{\frac {({\frac {3n}{ln(n)}})^{n-{\frac {3n}{ln(n)}}}}{({\frac {n}{ln(n)}})^{n-{\frac {n}{ln(n)}}}}}$ which tends to 0 when $n\rightarrow \infty .$

Corollary. Random lambda term of size n contains no more then ${\frac {3n}{ln(n)}}$ lambdas.

Once we know this we can improve the upper bound.

Let Ll be $\Lambda \setminus Ls$. In a term from Ll the proportion between unary and binary nodes is smaller then ${\frac {3}{ln(n)}}$ which is far from typical proportion in unary-binary trees which tends to some nonzero constant. Rough estimation gives

$Ll_{n}\leq C(n){n \choose {\frac {3}{ln(n)}}}((1+\epsilon ){\frac {n}{ln(n)}})^{n}$

where C(n) corresponds to the binary structure, ${n \choose {\frac {3}{ln(n)}}}$ to the possible distribtions of lambdas in binary structure and $((1+\epsilon ){\frac {n}{ln(n)}})^{n}$ to the possibilities of bindings (one can optimal number of unary nodes involving Lambert's function to get rid of epsilon here). The crucial observation now is that ${n \choose {\frac {3}{ln(n)}}}$ is subexponential.

Comparing this upper bound with $LB(n,{\frac {n}{ln(n)}})$ we would obtain that the asymptotic ratio between upper and lower bound is subexponential.

I think it has some serious consequences. In particular it seems that in a random lambda term almost all lambdas lie on one path.

at least $o({\sqrt {n/\ln(n)}})$ lambdas in head position and number of lambdas in one path

Remark: (may be 4) can be done directly without 3))

every fixed closed term (including the identity !) does not appear in a random term (in fact we have much more than that)

Let $\Lambda ^{t_{0}}$ denote the set of lambda terms which have $t_{0}$ as a subterm and let $T_{k}$ be the set of those lambda trees in which the number of unbounded leaves (occurrences of free variables) is equal to $k$.

Theorem

For any integers $k$ and $k'\geq k+1$ and for any term $t_{0}\in T_{k}$ of length $k'$ the following holds:

$\lim _{n\to \infty }{\frac {\#(\Lambda _{n}\cap \Lambda ^{t_{0}})}{\#\Lambda _{n}}}=0.$

Proof

Fix $k$ and $k'\geq k+1$. Let $t_{0}$ be a lambda tree of size $k'$ with exactly $k$ occurrences of free variables, denoted $x_{1},\ldots ,x_{k}$ (not necessarily distinct). Since there are at most $k'-k+1$ occurrences of lambdas and at most $k'+1$ leaves in $t_{0}$, there are at most

$K=M(k')(k'+1)^{k'+1}$

such trees and we can enumerate them in a fixed way. Let $m$ be the number of $t_{0}$. The tree $t_{0}$ contains at least one occurrence of lambda, otherwise it would either contain more free variables or would be of a bigger size.

Let $n$ be an integer satisfying ${\sqrt {\frac {n}{\ln(n)}}}\geq K$.

We will construct an injective function $f\colon \Lambda _{n}\cap \Lambda ^{t_{0}}\to \Lambda _{n}$ such that its image is of density 0 in $\Lambda _{n}$.

Let $t$ be a term of size $n$ with $t_{0}$ as its subterm. Let us consider the tree $T$ which is built from the tree $t$ by adding an additional unary node (labelled with $\lambda x$) at depth $m$. Next, let $T'$ be the tree obtained by replacing the subtree $t_{0}$ in $T$ by the tree $t_{1}=UB$, where $U$ is a binary tree of size $k'-k-1$ such that $U=x(x(\ldots (xx)\ldots ))$ and $B=x_{1}(x_{2}(\ldots (x_{k-1}x_{k})\ldots ))$, so the size of $B$ is equal to $k-1$. Thus, the size of $T'$ is equal to $n$. The variable $x$ is bound by the $m$-th lambda in the tree $T'$. Let us take $f(t)=T'$. Since $m$ is the number of the tree $t_{0}$, the function $f$ is injective.

By Theorem \ref{?}, each of $K$ head lambdas in a random tree of size $n$ binds more than $k'$ variables. Trees from the image $f(\Lambda _{n}\cap \Lambda ^{t_{0}})$ do not have this property, since the $m$-th lmabda binds only $k'$ variables. Thus, those trees are negligible among all trees of size $n$.

Corollary

Let $t_{0}$ be a closed lambda term. Then the density of $\Lambda ^{t_{0}}$ is equal to $0$.

Corollary

Let $t_{0}$ be a lambda term in which there are at least two occurrences of lambdas. Then the density of $\Lambda ^{t_{0}}$ is equal to $0$.

comment : so different situation in combinatory logic and lambda calculus ; the coding uses a big size so need to count variables in a different way

Experiments

results of the experiments we have done

some experiments that have to be done : e.g. density of terms having $\lambda x.y$ or big Omega pattern ...

to be done

Upper and lower bounds for $L_{n}$ with other size for variables especially one, binary with fixed size

Open questions and Future work

.....