Abstract
In this mainly expository paper we present a detailed proof of several results contained in a paper by M. Bertelson and M. Gromov on Dynamical Morse Entropy. This is an introduction to the ideas presented in that work. Suppose M is compact oriented connected \(C^\infty \) manifold of finite dimension. Assume that \(f_0 :M \rightarrow [0,1]\) is a surjective Morse function. For a given natural number n, consider the set \(M^n\) and for \(x=(x_0,x_1,\ldots ,x_{n-1}) \in M^n\), denote \( f_n (x) = \frac{1}{n} \, \sum _{j=0}^{n-1} f_0 (x_j).\) The Dynamical Morse Entropy describes for a fixed interval \(I\subset [0,1]\) the asymptotic growth of the number of critical points of \(f_n\) in I, when \(n \rightarrow \infty \). The part related to the Betti number entropy does not requires the differentiable structure. One can describe generic properties of potentials defined in the XY model of Statistical Mechanics with this machinery.
Instituto de Matematica—UFRGS—Brasil A. O . Lopes was partially supported by CNPq and INCT.
Access provided by Autonomous University of Puebla. Download conference paper PDF
Similar content being viewed by others
Keywords
- Bertelson-Gromov dynamical morse entropy
- Asymptotic growth of critical points
- Singular homology
- Betti number entropy
1 Introduction
We follow the main guidelines and notation of [1].
A Morse function is a smooth function such all critical points are not degenerate (see [2]).
Suppose M is compact oriented \(C^\infty \) manifold of dimension \(q \ge 1.\) Assume that \(f_0 :M \rightarrow [0,1]\) is a surjective Morse function and \(\varGamma \) is a free group with basis \(\gamma _1,\ldots ,\gamma _n\). We assume that \(f_0\) has p critical points (\(p\ge 2\)).
Suppose \(\varOmega \subset \varGamma \) is a finite non-empty set. If \(x \in M^\varOmega \) we denote \(x_\gamma \in M\), \(\gamma \in \varOmega \), the corresponding coordinate.
Then, we define \(f_\varOmega : M^\varOmega \rightarrow [0,1]\) by the expression
where \(|\varOmega |\) is the cardinality of \(\varOmega \). This function \(f_\varOmega \) is also a surjective Morse function.
2 The \(X\,Y\) Model
As a particular case we can consider \(\varGamma =\mathbb {Z}\), the set \(M^\mathbb {Z}\) and for \(x=(x_j)_{j \in \mathbb {Z}} \in M^\mathbb {Z}\), \(n>0\), \(f_0: M \rightarrow \mathbb {R}\), and
We mention this case because it is a more well known model in the literature and we want to trace a parallel to what will be done here.
The question about the minus sign in front of the sum is not important but if we want that \(f_0\) represents a kind of Hamiltonian (energy) we will keep the—(at least in this section).
In this model it is natural to consider that adjacent molecules in the lattice interact via a potential (an Hamiltonian) which is described by the smooth function of two variables \(f_0\). The mean energy up to position n is described by \(f_n\). The points \(x\in M^n\) where the mean n-energy is lower or higher are of special importance. We are interested here, among other things, in the growth of the number of critical values, when \(n \rightarrow \infty \). The critical points are called the stationary states (see [1]).
Denote by \(\text {Cri}_n (I)\) the number of critical points of \(f_n\) in a certain interval \(f^{-1}(I)\). Roughly speaking the purpose of [1] is to provide for a fixed value \(c\in [0,1]\) a topological lower bound for
in terms of a certain strictly positive concave function (a special kind of entropy). This is done by taking into account the homological behavior of the functions \(f_n\).
The so called classical XY model consider the case where \(M=S^1\) (see for instance [3,4,5,6,7,8,9] or [10]). A function \(A: (S^1)^\mathbb {Z} \rightarrow \mathbb {R}\) describes an interaction between sites on the lattice \(\mathbb {Z}\) where the spins are on \(S^1\). One is interested in equilibrium probabilities \(\hat{\mu }\) on \((S^1)^\mathbb {Z}\) which are invariant for the shift \(\hat{\sigma }:(S^1)^\mathbb {Z} \rightarrow (S^1)^\mathbb {Z}.\) A point x on \((S^1)^\mathbb {Z}\) is denoted by \(x=(\ldots ,x_{-2},x_{-1}\,|\,x_0,x_1,x_2,\ldots ).\)
In the case the potential A depend just on the first coordinate \(x_0\in S^1\), that is \(A(x)=f_0(x_0)\), then the setting described above applies.
In the case the potential A depend just on the two first coordinate \(x_0,x_1\in S^1\), that is \(A(x)=f_0(x_0,x_1)\), then, we claim that the setting described above in the introduction applies. This is the case when \(f_0: S^1 \times S^1 \rightarrow \mathbb {R}\). Indeed, in this case one can take \(M = S^1 \times S^1\) and consider that \(f_0\) acts on M. In this case we can say that \(f_0\) depends just in the first coordinate on \(M^\mathbb {Z}=(S^1 \times S^1)^\mathbb {Z}\) and adapt the general formalism we describe here.
Therefore, we will state all results for \(f_0 : M \rightarrow \mathbb {R}\), that is, the case the potential on \(M^\mathbb {Z}\) depends just on the first coordinate.
In the case \(\hat{\mu }\) is ergodic the sequence \(f_n\) describes Birkhoff means which are \(\hat{\mu }\) almost everywhere constant. We are here interested more in the topological and not in the measure theoretical point of view.
In the measure theoretical (or Statistical Mechanics) point of view, if one is interested in equilibrium states at positive temperature \(T=1/\beta \), then, is natural to consider expressions like \(\int \,e^{ \sum _{j=0}^{n-1} -\beta \, f_0 (x_j)}\, dx_0\,dx_1 \ldots d_{x_{n-1}}\) (or, when the set of spins is finite: \(\sum e^{ \sum _{j=0}^{n-1} - \beta \, f_0 (x_j)} \)) and its normalization (see [11,12,13]) which defines the partition function.
By the other hand if one is interested in the zero temperature case (see for instance [14]), then, expressions like \( -\sum _{j=0}^{n-1} f_0 (x_j)\) are the main focus. For instance, if \(f_0\) has a unique point of minimum \(x^{-} \in S^1\), then \(\delta _{(x^{-})^\infty }\) defines the ground state (maximizing probability). In the generic case the function \(f_0\) has indeed a unique point of minimum.
Given \(f_0: M \times M \rightarrow \mathbb {R}\) and n one can also consider periodic conditions. In this case we are interested in sums like
or
In the case we want to get Gibbs states via the Thermodynamic Limit (see for instance [11] or [13]), given a natural number n, we have to look for the probability \(\mu \) on \(M^n\) (absolutely continuous with respect to Lebesgue probability) which maximizes
or, at zero temperature the periodic probability \(\mu \) on \(M^n\) which maximizes
One can easily adapt the reasoning of [15] to show that for a generic \(f_0\) we get that \(\tilde{f}_n\) is a Morse function for all n.
When \(f_0\) is not generic several pathologies can occur (see for instance [3, 5, 10]).
Suppose the case when there is a unique point \(x^{-}\) of minimum for \(f_0\). For each \(\beta >0\) and n denote by \(\mu _{n,\beta }\) the absolutely continuous with respect to Lebesgue probability which maximizes
By the Laplace method (adapting Proposition 3 in [7] or Lemma 4 in [8]) we get that when \(\beta \rightarrow \infty \) and \(n \rightarrow \infty \) the probability \(\mu _{n,\beta }\) converges to the Dirac delta on \((x^{-})^\infty \). Therefore, in the generic case this last probability is the ground state (zero temperature limit).
3 The General Model—The Dynamical Morse Entropy
From now we forget the—sign in front of \(f_0\). For instance, \( f_n (x) = \frac{1}{n} \, \sum _{j=0}^{n-1} f_0 (x_j, x_{j+1}).\)
Given \(c \in [0,1]\) and \(\delta >0\), take \(N_\varOmega (c, \delta )\) the number of critical points of \(f_\varOmega \) in \(f^{-1}_\varOmega [c-\delta , c+ \delta ]\). Note that if \(f_0\) has p critical points then \(f_\varOmega \) has \(p^{| \varOmega |}\) critical points.
Consider the cylinder sets
where \(a_j\) are integers.
Denote \(N_i (c, \delta )= N_{\varOmega _i}(c, \delta )\). Then, of course, \(N_i(c, \delta )\) for c fixed decrease with \(\delta \).
For a fixed \(0\le c \le 1\), we denote the entropy by
The above limit exists and it is bounded by \(\log p\) but in principle could take the value \(-\infty \). We call \(\varepsilon (c)\) the dynamical Morse entropy on the value c.
In the case \(\varGamma =\mathbb {Z}\) as we mentioned before \( \varepsilon (c)\) is described by
Later we introduce a function b(c) (see Definition 3 and also Definition 2), which will be a topological invariant of \(f_0\). The function b(c) is defined in terms of rank of linear operators and Cohomology groups.
We will show later that
(1) \( 0 \le b(c) \le \varepsilon (c), \) \(\,0\le c \le 1\);
(2) b(c) is continuous and concave;
(3) b(c) is not constant equal to 0.
Finally, in the case \(M=S^1\) (the unitary circle) and \(f_0\) has just two critical points, we show in Sect. 7 that
b(c) is sometimes called the Betti entropy of \(f_0\).
Our definition of b(c) is different from the one in [1] but we will show later (see Sect. 8) that is indeed the same.
A key result in the understanding of the main reasoning of the paper is Lemma 6 which claims that for any Morse function f, given \(a,b\in \mathbb {R}\), \(a<b\), the number of critical points of f in \(f^{-1} [a,b]\) is bigger or equal to the dimension of the vector space
where \(H^*\) denotes the corresponding cohomology groups which will be defined in the following paragraphs (see also [16] for basic definitions and properties).
\( H^* (X,\mathbb {R})\) denotes the usual cohomology. Note that \(H^*\) will have another meaning (see Definition 1).
4 Cohomology
Suppose X is a metrizable, compact, oriented topological manifold \(C^\infty \) manifold. We will consider the singular homology. Suppose \(U \subset X\) is an open set and \(a \in H^* (X, \mathbb {R}).\) The meaning of the statement supp \(a\, \subset U\) is: there exist an open set \(V\subset X\), such that, \(X= U \cup V\), and \(a|_V =0.\)
Definition 1
\(H^*_X (U)= \{\,a\in H^* (X,\mathbb {R}) \,:\, \text {supp } \,\,a \subset U\},\) where U is an open subset of X. When X is fixed we denote \(H^*_X(U) = H^* (U)\).
Remember (see for instance [16]) that when \(U\subset X\) is open we get the exact cohomology sequence:
where \(H_c^* \) denotes the compact support cohomology.
Lemma 1
If U is an open set, then
Proof
The second equality follows from the fact that the above sequence is exact.
We will prove that
Let \(a\in \text {Im} (\,\,H^*_c (U,\mathbb {R}) \rightarrow H^* (X,\mathbb {R})\,\,)\). Then, a is represented by a cocycle \(\alpha \) with compact support \(K\subset U\). Therefore, \(a\,|(X-K)=0\).
Defining \(V=X-K\) we have that \(U \cup V=X\) and \(a\,|V=0\). Then, \( a \in H^* (U)\).
Let be \(\alpha \in H^* (U)\). Let \(V\subset X\) be an open set such that \(U \cup V=X\) and \(\alpha \,| V=0\).
Since \(X-U\subset V\), we have \(\alpha \,|(X-U)=0\).
Then, \(\alpha \in \) Ker \((\,H^* (X, \mathbb {R}) \rightarrow H^* (X-U, \mathbb {R}) \,).\) \(\square \)
Lemma 2
If U is an open set then \(H^* (U)\) is a graded ideal of the ring of cohomology of X.
Proof
This follows at once from Lemma 1. \(\square \)
Now we consider a continuous function \(f:X \rightarrow \mathbb {R}.\)
Definition 2
Given \(\delta >0\) and \(c \in \mathbb {R}\) we define
Proposition 1
Suppose X and Y are metrizable compact, oriented topological manifolds, moreover take \(f:X \rightarrow \mathbb {R}\), \(g:Y \rightarrow \mathbb {R}\) continuous functions. If we define \(f \oplus g: X \times Y \rightarrow \mathbb {R}\), by \((f \oplus g)(x,y) = f(x) + g(y)\), then, if \(c,c'\in \mathbb {R}\), \(\delta , \delta '>0\), we get
Before the proof of this important proposition we need two more lemmas.
As it is known (see [16]) the cup product \(\vee \) defines an isomorphism
Lemma 3
If \(U\subset X\) and \(V\subset Y\) are open sets, then
Proof
By Lemma 1 we get
Then,
From simple Linear Algebra arguments the claim follows from Lemma 1. \(\square \)
Lemma 4
If \(U \subset X\) and \(V \subset Y\) are open sets then
Proof
The \(\vee \) product defines a natural isomorphism
By Lemma 1 and the exact relative cohomology sequence we get:
and
From this the claims follows at once. \(\square \)
Now we will present the proof of Proposition 1.
Take \(h= f \oplus g\) and denote
and
Note that
Consider the commutative diagram
From this follows the linear transformation
By the other hand
The first equality above follows from Lemma 3; the second follows from Linear Algebra; namely, if \(E_2\subset E_1 \subset E\) and \(F_2\subset F_1 \subset F\), then
From the above it follows that
Therefore,
\(\square \)
5 Critical Points
In what follows X is a compact, oriented \(C^\infty \) manifold and \(f:X \rightarrow \mathbb {R}\) is a Morse function.
Lemma 5
Suppose X is a compact, oriented \(C^\infty \) manifold and \(U\subset X\) is an open set. If \(a \in H^* (X, \mathbb {R}),\) then, supp \(a\subset U\), if and only if, there exists a closed \(C^\infty \) differentiable form w such that supp \(w \subset U\), and a is the de Rham cohomological class of w.
Proof
If there exists \(w \in a\), such that supp \(w \subset U\), then
If there exists an open set \(V\subset X\) such that \(U \cup V=X \) and \(a|_V =0\), then, there exist a \(C^\infty \) form \(\eta \) on V such that \(d \eta = w|_V\) where \(w \in a\).
Let W be an open set such that \(\overline{W}\subset V\) and \(W\cup U=X\). Take a \(C^\infty \) function \(\varphi : X \rightarrow [0,1]\) such that \(\varphi |_{\overline{W}} =1\) and \(\varphi |_{X-K} =0\), where K is compact set such that \(\overline{W} \subset K \subset V\). Then, \(\varphi \, \eta \) has an extension to X and \((w- d \,(\varphi \, \eta ) \,)\in a\). But,
\(\square \)
Lemma 6
Given \(a,b\in \mathbb {R}\), \(a<b\), then, the number of critical points of f in \(f^{-1} [a,b]\) is bigger or equal that
Proof
Without lost of generality we can assume that a and b are regular values of f (decrease a and increase b a little bit).
Given \(c_1<c_2< \cdots <c_m\), the critical values of f in (a, b), take
By Proposition 3 and Lemma 8, the number of critical points in \(f^{-1} (c_i)\), \(i=1=,2,\ldots ,m\), is bigger or equal to
Finally consider the filtration
\(\square \)
Now we denote \(b_\varOmega '(c,\delta )=b_{c,\delta }'(f_\varOmega )\) and \(b_i '(c,\delta )=b_{\varOmega _i}'(c,\delta )\), \(0\le c \le 1,\) \(\delta >0\).
Corollary 1
\(b_i '(c,\delta )\le N_i(c, \delta )\) for all \(i=1,2,3,\ldots \) and \(0\le c\le 1\), \(\delta >0\).
Now we define the function b using Proposition 3(a)
Definition 3
We will show that in above definition we can change the \(\liminf \) by \(\lim \).
Lemma 7
Proof
The first inequality follows from Corollary 1. From the definition is easy to see that \(\varepsilon (c)\) is smaller than \(\log \) of the number of critical points of \(f_0.\) \(\square \)
We denote \(B(\varGamma )\) a family of finite subsets of \(\varGamma \) and \(B_N (\varGamma )\), \(N \in \mathbb {N}\), the family of sets \(\varOmega \in B(\varGamma )\) such that \(|\varOmega | >N.\)
Proposition 2
Suppose \(\varOmega ', \varOmega ''\in B(\varGamma )\) are disjoint not empty sets. Then,
where \(0 \le c_1,c_2\le 1\), \(\delta >0\) and \(\alpha = \frac{| \,\varOmega '\,|}{|\,\varOmega ' \,| + | \,\varOmega ''\,|}.\)
Proof
By definition
By Proposition 1, as \(\delta = \alpha \, \delta + (1- \alpha ) \delta ,\) then
\(\square \)
Lemma 8
Suppose the interval [a, b] does no contains critical values of f. Then,
Proof
This follows from Lemma 1 and the fact that \(f^{-1} [b,\,\infty )\,\) is a deformation retract of \(f^{-1} [a,\,\infty \,).\) \(\square \)
Definition 4
Given \(c \in \mathbb {R} \) we define
Proposition 3
For a fixed c we have
(a) \( b_{c,\delta } ' (f)\) decreases with \(\delta \) and \(b_{c,\delta } ' (f) = \tilde{b}_c (f) \) for all \(\delta \) small enough.
(b) \(\tilde{b}_c (f)=0 \) if c is not a critical value of f
(c) \(\tilde{b}_c (f) \) is smaller than the number of critical points of f in \(f^{-1}(c)\)
(d) \(\sum _c \, \tilde{b}_c (f)=\) Dim \(H^* (X).\)
Proof
(a) follows from the above definitions and Lemma 8.
(b) follows from Lemma 8
For the proof of (c) consider the exact diagram
where \(r_1\) and \(r_2\) are the restriction homomorphisms.
By Lemma 1
From this follows that
because the above sequence is exact.
In order to finish the proof we apply Morse Theory (see [2]) with \(\delta \) small enough.
For the proof of (d) suppose \(c_1<c_2< \cdots <c_m\) are the critical values of f. Now, consider
Now, from (a) and Lemma 8 we have
Finally, note that
\(\square \)
Lemma 9
Given \(\delta >0\), there exists an integer N such that: \(b_\varOmega ' (c, \delta )\ge 1\) for all \(c \in [0,1]\) and all \(\varOmega \in B_N (\varGamma )\). Therefore, \(b(c)\ge 0\), for all \(0\le c\le 1\).
Before the Proof of Lemma 9 we need two more lemmas.
Lemma 10
Suppose X is a compact oriented \(C^\infty \) manifold and \(f:X \rightarrow \mathbb {R}\) is a Morse function. Then, for all \(\delta >0\)
where \(a_1\) and \(a_2\) are respectively the maximum and minimum of f.
Proof
If \(\delta \) is small enough, \(f^{-1} (-\infty , a_2 + \delta )\) is the disjoint union of a finite number of open discs and \(f^{-1} (-\infty , a_2 -\delta )= \emptyset \).
If n is the dimension of X, then, it follows from Lemma 1 that
and
Then, \(b_{a_2, \delta } ' (f) \ge 1\), if \(\delta >0\) is small enough. Therefore, this claim is also true for any \(\delta >0\) by Proposition 3(a).
In a similar way we have that for small \(\delta >0\)
and
From this the final claim is proved. \(\square \)
Lemma 11
Consider \(\varOmega \in B (\varGamma )\) where \(|\varOmega |=m\ge 1\), then, \( b_\varOmega ' (k/m, \,\delta ) \ge 1,\) for all \(\delta > 0\) and \(k=0,1,2,\ldots ,m\).
Proof
If \(k=0\), or m, the claim follows from Lemma 10 with \(X=M^\varOmega \), \(f=f_\varOmega \).
Given 0, k, m, \(0<k<m\), take \(\varOmega = \varOmega ' \cup \varOmega ''\), where \(\varOmega ', \varOmega '' \) are disjoints and \(k=|\varOmega '|\).
By Proposition 2 with \(c_1=1\) and \(c_2=0\) we get
Yet from last lemma. \(\square \)
Now we will prove Lemma 9.
Proof
Take \(N> \frac{2}{\delta }\), \(\varOmega \in B_N (\varGamma ) , |\varOmega |=m >N\) and k such that \(\frac{k}{m} \le c < \frac{k+1}{m},\)
By definition,
since \(c-\delta <k/m-\delta /2\) and \(c+\delta >k/m + \delta /2\).
Therefore, \(b_\varOmega ' (c, \delta ) \ge b_\varOmega ' (k/m,\,\delta /2)\ge 1\) by Lemma 11. \(\square \)
Proposition 4
Proof
This follows from Lemmas 7 and 9\(\square \)
Lemma 12
Given \(c\in [0,1]\) and \(\delta >0\), consider a non-empty set \(\varOmega \in B(\varGamma )\) and \(\gamma \in \varGamma \). Then,
In the case \(\varGamma =\mathbb {Z}\) we have that for any \(\varOmega =\{1,2,\ldots ,k\}\)
where \(\hat{\sigma }\) is the shift acting on \(M^\mathbb {Z}\).
Proof
For fixed \(\gamma \) consider the transformation \( x\in M^\varOmega \rightarrow y\in M^{\varOmega + \gamma }\), such that \(y_w =x_{w-\gamma }\), which is a diffeomorphism which commutes \(f_{\varOmega + \gamma }\) with \(f_\varOmega \).
The result it follows from this fact. \(\square \)
We will show now that indeed one can change \(\liminf \) by \(\inf \) in Definition 3. In order to do that we need the following proposition which describes a kind of subadditivity.
Proposition 5
Given an integer number \(N>0\) take \(h: B_N (\varGamma ) \rightarrow \mathbb {R}\), \(h\ge 0\), which is invariant by \(\varGamma \) and such that
if \(\varOmega ', \,\varOmega ''\,\in B_N (\varGamma ),\) are disjoint. Then, the limiit
From this follows:
Corollary 2
For \(c\in [0,1]\) and \(\delta >0\),
(a) there exist the limit
(b) \(0 \le b ' (c,\delta ) \le \log \) (number of critical points of \(f_0\)),
(c) \(b(c)= \lim _{\delta \rightarrow 0} b' (c,\delta ) \)
Proof
The claim (a) follows from last proposition applied to \(h(\varOmega ) = \log b_\varOmega ' (c, \delta )\), by Lemma 9, Proposition 2 taking \(c_1=c_2=c\) and also by Lemma 12.
Item (b) follows from Lemma 2 and Corollary 1.
Item (c) follows from item (a) and the definition of b(c). \(\square \)
Before the proof of Proposition 5 we need two lemmas.
Lemma 13
Given an integer positive number k, then for each \(i > (3\, k\,+1)\) there exists \(\varOmega _{k,i} \in B(\varGamma )\) such that: (a) \(\varOmega _{k,i} \subset \varOmega _i\); (b) \(\varOmega _{k,i} \) is a disjoint union of a finite number of translates of \(\,\varOmega _k\) ; (c) \(\lim _{i \rightarrow \infty } \frac{|\,\varOmega _{k,i}|\, }{|\,\varOmega _i\,|} =1\); (d) \(|\varOmega _i| - |\varOmega _{k,i}|\ge (2k+1)^n\), where n is the number of generators of \(\varGamma \).
Proof
For the purpose of the proof we can assume that \(\varGamma = \underbrace{\mathbb {Z} \oplus \mathbb {Z}\oplus \cdots \oplus \mathbb {Z}}_n\) and take \(\gamma _1,\gamma _2, \ldots ,\gamma _n\) the canonical basis.
Take \(m \ge 1\) an integer such that
and
It is easy to see that the sets \( \varOmega _{k,i} \) satisfy all the above claims. \(\square \)
Lemma 14
Given real numbers \(x_i\ge 0\) \(i=1,2,3,\ldots \), suppose that for each k and each \(\varepsilon >0\) there exist \(N_{k,\varepsilon }\) such that
Then, the \(\lim _{i \rightarrow \infty } x_i\) exists (can finite or \(+\infty \)).
Proof
Take \(L= \limsup _{i \rightarrow \infty } x_i\) and \(a\in \mathbb {R}\), \(a<L\). Then, there exists \(x_k>a\). Therefore, \(x_i \ge a\), if i is very large. Then, \( \liminf _{i \rightarrow \infty } x_i \ge a\). From this follows the claim. \(\square \)
Now we will prove Proposition 5.
Proof
Suppose k is such that \((2 k +1)^n>N\). Take \(i> 3 \, k +1\), then, \(|\,\varOmega _{k,i}\,| \ge (2 k + 1)^n>\,N\) and \(|\varOmega _i - \varOmega _{k,i}| \ge (2 k +1)^n >N\).
Then, \(h(\varOmega _i) = h ( \,\varOmega _{k,i} \,\cup \, (\,\varOmega _i - \varOmega _{k,i} )\,) \ge h(\varOmega _{k,i}).\)
Moreover, each translate of \(\varOmega _k\) has cardinality \((2k+1)^n\). Therefore,
From this follows that
and the claim is a consequence of Lemmas 13 and 14. \(\square \)
The next lemma will be used later
Lemma 15
Under the hypothesis of Proposition 5 consider
Then,
Proof
If \(i >N\), then \(|\varOmega _i|>N\). Therefore,
From this follows
Therefore,
We assume that \(\varGamma = \underbrace{\mathbb {Z} \oplus \mathbb {Z}\oplus ... \oplus \mathbb {Z}}_n\) and \(\gamma _1,\gamma _2,..,\gamma _n\) is the canonical basis.
Take k such that \((2 k +1)^n >N\). For \(i> 5 \,k + 2\), take \(m>1\) such that \(k + m\, (2 k +1) \le i \le k + (m+1)\, (2\, k +1).\)
Consider
Then, \( \varOmega _{k,i}' \subset \varOmega _i\), and \( \varOmega _{k,i} '\) is a finite union of disjoints translates of \(\varOmega _k '\). Moreover \(\lim _{i \rightarrow \infty } \frac{|\varOmega _{k,i} '|}{|\varOmega _i|}=1\),
From this follows that
By the other hand, all translate of \(\varOmega _k '\) has cardinality bigger than N.
Therefore,
Then,
Now, for a fixed k, taking \(i \rightarrow \infty \) in the above inequality we get
From this follows that
\(\square \)
6 Properties of b(c)
Lemma 16
There exists \(c\in [0,1]\) such that
Proof
Note that dim \( (\,H^* (M)\,)\ge 2\) because dim \(M\ge 1\). Let q be the number of connected components of M.
If \(|\varOmega _i|=m_i\), take \(0=t_0<t_1< \cdots <t_{m_i} =1\), a partition of [0, 1] in \(m_i\) intervals of the same size. By Lemma 1
Denote \(A_{ij}\) a supplement of \(H^* ( f_{\varOmega _i}^{-1} (-\infty , t_{j-1}))\) in \(H^* ( f_{\varOmega _i}^{-1} (-\infty , t_{j}))\), \(1\le j\le m_{i}\). Then,
Therefore, there exists a certain \(A_{i \, j_i}=A_i\), such that,
Denote \(s_i\) the middle point of \((t_{j_i -1}, t_{j_i}]\) and \(\delta _i = \frac{1}{2\, m_i}.\)
Then, by definition of \( b_i ' (s_i,\delta _i) = \) dim \( A_i\).
There exists a subsequence \(s_{i_k}\rightarrow c\in [0,1]\), when \(k \rightarrow \infty \).
Given \(\delta >0\), there exists a \(K>0\) such that \( \delta _{i_k} < \delta /2\) and \(|s_{i_k} - c| < \delta /2\), if \(k>K\).
This means \(c-\delta < s_{i_k} - \delta _{i_k} \) and \(s_{i_k} + \delta _{i_k} < c + \delta .\)
From this follows that \( b_{i_k} ' (c,\delta )\ge b_{i_k} ' (s_{i_k},\delta _{i_k})=\) dim \( A_{i_k}\).
Finally, we get
Now, taking limit in \(k \rightarrow \infty \) in the above expression we get
\(\square \)
Lemma 17
The function b(c) is upper semicontinuous.
Proof
Suppose \(c_k\), \(k \in \mathbb {N}\) is a sequence of points in [0, 1] such that, \(c_k \rightarrow c\).
Given \(\varepsilon >0\), take \(\delta >0\), such that, \(b ' (c,\delta ) < b(c) + \varepsilon \). There exists a \(N>0\) such that \(|c-c_k|< \delta /2\), if \(k \ge N.\) Then, \( c- \delta < c_k - \delta /2\) and \(c_k + \delta /2< c + \delta \), if \(k \ge N.\)
Then, \( b_i ' (c, \delta ) \ge b_i ' (c_k, \delta /2)\), if \(k\ge N\), for all \(i=1,2,3,\ldots \)
From this follows that \(b' (c, \delta ) \ge b ' (c_k, \delta /2)\). Therefore,
Therefore
for any \(\varepsilon >0\). From this it follows the claim. \(\square \)
Lemma 18
The function b(c) is concave.
Proof
Consider \(0\le c_1< c_2\le 1\) and \(0\le t\le 1\), we will show that
First we will show the claim for \(t=1/2\). Denote \(\tilde{\varOmega }_i = \varOmega _i + (2\, i +1) \gamma _1\) and \(\varOmega _i ' = \varOmega _i \cup \tilde{\varOmega }_i\).
By Proposition 2 and Lemma 12 we get:
for all \(\delta >0\).
Now, applying Lemma 15 to \(h(\varOmega ) = \log b_{\varOmega } ' ( 1/2\, c_1 + 1/2\, c_2, \delta )\), we get \(b ' ( 1/2\, c_1 + 1/2\, c_2, \delta )\ge 1/2\, b ' (\, c_1, \delta )\, +\,1/2\,b ' ( \, c_2, \delta )\).
Now, taking \(\delta \rightarrow 0\), we get \(b ( 1/2\, c_1 + 1/2\, c_2)\ge 1/2 b (\, c_1)\,+\, 1/2\, b ( \, c_2)\).
The inequality we have to prove is true for a dense set of values of t in [0, 1]. Then, by Lemma 17 is true for all \(t\in [0,1]\). \(\square \)
Corollary 3
The function b(c) is continuous for \(c \in [0,]\).
Proof
This follows from Lemmas 17 and 18. \(\square \)
We summarize the above results in the following theorem.
Theorem 1
(a) \( 0 \le b(c) \le \varepsilon (c) \le \log (\) number of critical points of \(f_0\)), for all \(0 \le c \le 1\).
(b) b(c) is continuous on [0, 1]
(c) b(c) is concave, that is, its graph is always above the cord
(d) b(c) is not constant equal zero. Moreover, there exists a point c where \(b(c)\ge \log \) ( dim \(H^* (M,\mathbb {R})\,)>0\).
7 An Example
The next example shows that the item (d) in the above theorem can not be improved.
Take \(M=S^n\), \(n \ge 1\), and a Morse function \(f_0: M \rightarrow [0,1]\) which is surjective with only two critical points. Suppose \(x_{-}\) is the minimum and \(x_{+}\) the maximum of \(f_0\). We will compute b(c) and \(\varepsilon (c)\).
Take \(\varOmega \in B(\varGamma )\) with \(|\varOmega |=m\ge 1\). For each \(\varOmega ' \subset \varOmega \) consider the canonical projection \(p_{\varOmega '}: M^\varOmega \rightarrow M^{\varOmega '}.\) Now, take
where \([\,\,\,]\) represents fundamental class. Then,
is a \(\mathbb {R}\)-homogeneous basis of \( H^* (M^{\varOmega },\mathbb {R}). \)
For \(0\le d\le 1\) denote
For \(x \in M^\varOmega \) we denote by \(x_\gamma \) the corresponding coordinate, where \(\gamma \in \varGamma \).
Lemma 19
If \(0\le d\le 1\), where d is not rational, then
is a basis of \(H^* (L_d)\).
Proof
Take \( K_d = M^\varOmega - L_d\). By Lemma 1
The claim follows from
(1) \(H^k (M^\varOmega ,\mathbb {R}) \rightarrow H^k (K_d,\mathbb {R}) \) is zero if \(k> m \,(1-d)\, n\), and
(2) \(H^k (M^\varOmega ,\mathbb {R}) \rightarrow H^k (K_d,\mathbb {R}) \) is injective if \(k< m \,(1-d)\, n\).
Now we prove (1) and (2).
(1) Suppose \(\varOmega ' \subset \varOmega \) is such that \(\mu ^{\varOmega '} \in H^k (M^\varOmega )\) where \(k> m\, (1-d)\, n\). Then, \(|\varOmega '| > m\, (1-d)\). Suppose
If \(x \in F_{\varOmega '}\), then \(f_\varOmega (x) \le \frac{1}{m}\, (m- | \varOmega '|)< d\). Then, \(F_{\varOmega '} \cap K_d=\emptyset .\) This means that: if \(x \in K_d\, \rightarrow \, x_\gamma \ne x_{-}\) for some \(\gamma \in \varOmega '.\) Then, \(K_d \subset p^{-1}_{\varOmega '} (M^{\varOmega '} -\,\{z\})\) where \(z_\gamma =x_{-}\) for all \(\gamma \in \varOmega '\).
From this follows
(2) Denote \(T=\{x \in M^\varOmega \,:\, \text {cardinality} (\, \{\gamma \,:\, x_\gamma = x^{+} \,\})\,>\, m\, d\,\}.\) The set T is closed.
If \(x \in T\), then \(f_\varOmega (x) > \frac{1}{m}\, m\, d =d\). Then, \(T\subset K_d\).
We have to show that
As we had seen before \(H^k (M^\varOmega ,\mathbb {R})=0\) if k is not multiple of n. Then, we can assume that \(k=q\, n\), if \(q=0,1,2,\ldots \). The claim follows from the next lemma, taking s the integer part of \(m\, d\), by the exact sequence of homology, given that \(U= U_s (\varOmega ).\)
Lemma 20
Suppose \(s=0,1,2,..,m\). Suppose
then, \(H^k_c ( U_s ( \varOmega ),\mathbb {R}) =0\), if \(k <(m-s)\,n\).
Proof
The claim is trivial for \(s=0\) or \(s=m\) (\(U_0(\varOmega )\) is homeomorphic to \((\,\mathbb {R}^n\,)^m\)).
The proof is by induction in m. The claim for \(m=1\) is trivial. Suppose is true for \(m-1\ge 1\). Take \(0<s<m\). Fix \(w\in \varOmega \) and take \(\varOmega ' = \varOmega -\{w\}\).
Consider \(\varphi : M^{\varOmega '} \rightarrow M^\varOmega \) and \(\psi : M^{\varOmega '} \times (M-\{\,x^{+}\,\}) \, \rightarrow \, M^\varOmega \), where for a given x we define \(\varphi (x)\) by \( x_\omega = x^{+}\) if \( x \in M^{\varOmega ' },\) and \(\psi (x,u)\) is defined by \(x_w =u\) if \(x \in M^{\varOmega '}\) and \(u \in M,\) \(u \ne x^{+}.\)
\(\psi \) identifies \(U_s (\varOmega ') \times (\,M - \{x^{+}\}\,)\) with an open set A contained in \(U_s (\varOmega )\).
Moreover, \(\varphi \) identifies \(U_{s-1} (\varOmega ')\) with the complement of this open set A in \(U_s (\varOmega )\).
As \(M - \{x^{+}\}\) is homeomorphic to \(\mathbb {R}^n\) and by recurrence we get that
if \(k< (m -1 -s)\, n +n = (m-s)\, n\) and, moreover, \(H^k_c (\,U_{s-1} (\varOmega ',\mathbb {R})\,)=0\), if \( k< (\, (m-1) - (s-1)\,) \, n= (m-s)\, n\).
Now, using the exact sequence of homology we finish the proof. \(\square \)
Now we fix irrationals \(d_1,d_2\), \(0< d_1<d_2<1\). Denote \( a_m = m\, (1-d_1)\), \( b_m = m (1-d_2),\) and, \( c_m =\) dim \( (\, H^* (L_{d_2})/ H^* (L_ {d_1})\,)\).
By Lemma 19 we get
Assume m is much bigger than \((d_2-d_1)\).
Take an integer \(j_m\), such that \(b_m<j_m<a_m\),
Then,
By Stirling formula:
Therefore,
when \(m \sim \infty \).
As \(1- d_2< \frac{j_m}{m}< 1- d_1\), then (changing x by \((1-x)\)) we get
and
From this follows
and
Proposition 6
Proof
Given \( 0<c<1\), there exists small \(\delta >0\) such that
From the above for \(d_1= c -\delta \) and \(d_2= c + \delta \) we get
Now, taking \(\delta \rightarrow 0\), we get
For \(c=0\) or \(c=1\) the result follows from continuity.
Now we will estimate \(\varepsilon (c).\)
The critical values of \(f_\varOmega \) are \(0,\frac{1}{m},\frac{2}{m},\ldots , 1\).
To the critical values \(\frac{j}{m}\) (\(j=0,1,2, \ldots ,m\)) corresponds \(\left( \begin{array}{cc} m\\ j \end{array} \right) \,\) critical points.
Therefore, given \(d_1,d_2 \in \mathbb {R}\) \(d_1<d_2\), the number \(c_m '\) of critical points of \(f_\varOmega \) in \( f^{-1}_\varOmega (d_1,d_2)\) is
The computation of \(\varepsilon (c)\) is analogous to the one for b(c). This also follows from the last Theorem and the fact that \(H^* (M)\) = number critical points of \(f_0\) in the present case. \(\square \)
8 About the Definition of b(c)
We will show that the definition of b(c) presented here coincides with the one in [1].
Suppose X is a compact connected oriented \(C^\infty \) manifold.
Lemma 21
Given an open set V in X consider \(\alpha \in H^* (X,\mathbb {R})\) such that \(\alpha |_V \ne 0.\) Then, there exists \(\beta \in H^* (V)\) such that \(\alpha \wedge \beta \ne 0.\)
Proof
Take \(w \in \alpha \). As \(\alpha |_V \ne 0\), then there exists a cycle z on V such that \(\int _z w \ne 0.\)
Suppose \(w'\) is a closed form with compact support on V such that its cohomology class in \(H^*_c (V,\mathbb {R})\) is the Poincare dual of the homology class of z in \(H_* (V,\mathbb {R}).\)
\(w'\) can be extended to a closed form on X (putting 0 where needed) and by Poincare duality:
Therefore, \(w \wedge w'\) is not exact on X.
Denote \(\beta \in H^* (X,\mathbb {R})\) the cohomology class of \(w'\). By Lemma 1 we have that \(\beta \in H^*(V)\). As \(w \wedge w'\) is not exact we get that \(\alpha \wedge \beta \ne 0.\) \(\square \)
Notation: if \(S \subset X\), then \(\mathscr {H}^* (S)=\cap \,\{ H^* (W) \, : W \subset X\) is an open set and \( S \subset W \}\).
Lemma 22
Suppose \(U,V \subset X\) are open sets and \(X=U \cup V\). Take \(K=U-V\) and \(\alpha \in H^* (U).\) Then, \(\alpha \wedge \beta =0\) for all \(\beta \in H^* (V)\), if and only if, \(\alpha \in \mathscr {H}^* (K).\)
Proof
Suppose \(\alpha \in \mathscr {H}^* (K)\) and take \(\beta \in H^* (V) \). By Lemma 5 there exists \(w \in \beta \) such that supp \(w \subset V\).
Take \(W= X-\) supp w (which contains K). By definition we get that \(\alpha \in H^* (W).\) Then, by Lemma 5, there exists \(w ' \in \alpha \) such that supp \(w' \subset W\). Therefore, \(w \wedge w'=0,\) and finally it follows that \(\alpha \wedge \beta =0.\)
Reciprocally, suppose that \(\alpha \wedge \beta =0\) for all \(\beta \in H^*(V)\). By Lemma 21 we have that \(\alpha \,|V =0\). Take \(W \supset K\), then \(V \cup W=X\). Therefore, by definition \(\alpha \in H^* (W).\) \(\square \)
Lemma 23
Take \(K \subset X\) a compact submanifold with boundary such that \(K- \delta K\) is an open subset of X.
Then,
WE leave the rest of the proof for the reader.
Proof
Take W an open set by adding a necklace to K. Then, \(X-K\) can be retracted by deformation over \(X-W\).
Then, if \(\alpha \in H^* (X,\mathbb {R})\), we get that \(\alpha |_{X-K} =0\) is equivalent to \(\alpha |_{X-W}=0.\)
Now, the claim follows from Lemma 1 and by the definition of \(\mathscr {H}(K).\) \(\square \)
Corollary 4
Under the same hypothesis of last lemma it also follows that \( \mathscr {H} (K) = H^* ( \) int \( (K)\,)\).
Proof
This follows from the fact that \(H^* ( X - \) int \((K)\,,\mathbb {R}) \rightarrow H^* (X-K,\mathbb {R})\) is an isomorphism. \(\square \)
Proposition 7
Suppose U, V are open sets such that \(X= U\cup V\) and moreover that \(\overline{U},\overline{V}\) are submanifolds with boundary of X.
Consider the linear transformation L such that
where, \(a \rightarrow \,(\, b \rightarrow a \wedge b\,).\)
Then, the rank of L is dim \( ( \,H^*(U)/ H^* (M - \overline{V})\,).\)
Proof
By Lemma 22 we get that Ker \(L= H^* (X-V)\). Finally, by the last corollary \(H^* (X-V)= H^* (M-\overline{V}).\) \(\square \)
Consider now a Morse function \(f:X \rightarrow \mathbb {R}\) and \(c\in \mathbb {R}\), \(\delta >0.\)
Definition 5
\(b_{c,\delta } (f)\) is the rank of the linear transformation
where \(a \rightarrow (b\, \rightarrow a \wedge b).\)
Note that \(b_{c,\delta } (f)\) decreases with \(\delta \).
Lemma 24
If \(c-\delta \) and \(c+ \delta \) are regular values of f, then
Proof
Just apply Proposition 7 to \(U= f^{-1} (-\infty , c + \delta )\) and \(V= f^{-1} (\, c - \delta , \infty \,).\) \(\square \)
Note that \(b_\varOmega (c,\delta )= b_{c, \delta } ( f_\varOmega )\), where \(\varOmega \in B(\varGamma )\) and \(\varOmega \ne \emptyset \), and moreover that \(b_i (c,\delta ) = b_{\varOmega _i} (c, \delta ).\) The next limit exists (see [1]).
Definition 6
The set \(S\subset [0,1]\) of all critical values of all \(f_\varOmega \) is countable. By Lemma 24 we get that \(b_i ' (c, \delta )=b_i (c, \delta )\) if \(c-\delta \notin S\) and \(c+\delta \notin S\). Therefore, \(b'(c,\delta ) = b(c,\delta )\) if \(c-\delta \notin S\) and \(c+\delta \notin S\).
Finally,
because both limits exist.
Therefore the function b(c) we define coincides with the one presented in [1].
References
Bertelson, M., Gromov, M.: Dynamical Morse Entropy, Modern Dynamical Systems and Applications, pp. 27–44. Cambridge University Press, Cambridge (2004)
Milnor, J.: Morse Theory. Princeton University Press, Princeton (1963)
Baraviera, A.T., Cioletti, L., Lopes, A.O., Mohr, J., Souza, R.R.: On the general one-dimensional XY model: positive and zero temperature, selection and non-selection. Rev. Math. Phys. 23(10), 1063–1113, 82Bxx (2011)
Chou, W., Griffiths, R.: Ground states of one-dimensional systems using effective potentials. Phys. Rev. B 34(9), 6219–6234 (1986)
Coronel, D., Rivera-Letelier, J.: Sensitive dependence of Gibbs measures. J. Stat. Phys. 160, 1658–1683 (2015)
Fukui, Y., Horiguchi, M.: One-dimensional chiral \(XY\) model at finite temperature. Interdiscip. Inf. Sci. 1(2), 133–149 (1995)
Lopes, A.O., Mohr, J., Souza, R.R., Thieullen, P.: Negative Entropy, Zero temperature and stationary Markov chains on the interval. Bull. Soc. Bras. Math. 40(1), 1–52 (2009)
Lopes, A.O., Mengue, J.K., Mohr, J., Souza, R.R.: Entropy and variational Principle for one-dimensional lattice systems with a general a-priori probability: positive and zero temperature. Ergod. Theory Dyn. Syst. 35(6), 1925–1961 (2015)
Thompson, C.: Infinite-spin ising model in one dimension. J. Math. Phys. 9(2), 241–245 (1968)
van Enter, A.C.D., Ruszel, W.M.: Chaotic temperature dependence at zero temperature. J. Stat. Phys. 127(3), 567–573 (2007)
Cioletti, L., Lopes, A.: Interactions, Specifications, DLR probabilities and the Ruelle operator in the one-dimensional lattice. Discret. Contin. Dyn. Syst.-Ser. A 37(12), 6139–6152 (2017)
Cioletti, L., Lopes, A.: Phase Transitions in one-dimensional translation invariant systems: a Ruelle operator approach. J. Stat. Phys. 159(6), 1424–1455 (2015)
Sarig, O.: Lecture notes on thermodynamic formalism for topological Markov shifts. Penn State (2009)
Baraviera, A., Leplaideur, R., Lopes, A.O.: Ergodic Optimization, Zero temperature limits and the Max-Plus Algebra, mini-course in XXIX Colóquio Brasileiro de Matemática - IMPA - Rio de Janeiro (2013)
Asaoka, M., Fukaya, T., Mitsui, K., Tsukamoto, M.: Growth of critical points in one-dimensional lattice systems. J. d’Anal. Math. 127, 47–68 (2015)
Massey, W.: Homology and Cohomology, M. Dekker (1978)
Author information
Authors and Affiliations
Editor information
Editors and Affiliations
Rights and permissions
Copyright information
© 2021 Springer Nature Switzerland AG
About this paper
Cite this paper
Lopes, A.O., Sebastiani, M. (2021). On Bertelson-Gromov Dynamical Morse Entropy. In: Pinto, A., Zilberman, D. (eds) Modeling, Dynamics, Optimization and Bioeconomics IV. ICABR DGS 2017 2018. Springer Proceedings in Mathematics & Statistics, vol 365. Springer, Cham. https://doi.org/10.1007/978-3-030-78163-7_13
Download citation
DOI: https://doi.org/10.1007/978-3-030-78163-7_13
Published:
Publisher Name: Springer, Cham
Print ISBN: 978-3-030-78162-0
Online ISBN: 978-3-030-78163-7
eBook Packages: Mathematics and StatisticsMathematics and Statistics (R0)