1. Introduction
In this work we apply nonstandard techniques à la Abraham Robinson to -algebras, -probability spaces (also known as noncommutative probability spaces) and noncommutative stochastic processes.
Our starting point is the nonstandard hull construction due to Luxemburg [
1]. For the sake of completeness, in 
Section 2 we briefly outline such a construction in the case of a 
-algebra. Functional analysts are probably more familiar with the ultraproduct construction (see [
2]), which is an important tool in the study of 
-algebras (see also [
3] or [
4]). Actually, every ordinary ultraproduct of 
-algebras can be realized as the nonstandard hull of some internal 
-algebra. Therefore, we loosely say that we deal with ultraproducts of 
-algebras.
Concerning the terminology that we adopt throughout this paper, we use the attribute “ordinary”, rather than “standard", when referring to some mathematical notion which is familiar to most mathematicians. The reason being that the term “standard” has a precise technical meaning in the framework of nonstandard techniques. We refer the reader to [
5] as a valuable reference for the relevant notions and for the construction of nonstandard universes. We also mention [
6] [§1] for a concise axiomatic introduction to the subject.
We stress that we may almost completely rewrite this paper in ultraproduct language or, gearing towards logic, within the framework of continuous logic (see [
7]). In our opinion we get slightly more generality by working with nonstandard hulls. Indeed, most of the results in this paper apply to the internal 
-algebras and not just to the standard ones (the latter being the nonstandard extensions of ordinary 
-algebras). Admittedly, our approach is motivated by our familiarity with the nonstandard techniques and by our belief that, in many cases, a nonstandard proof is simpler and more intuitive than a proof of the same result written in ultraproduct language.
As for the paper’s contents, we begin by saying that a significant amount of the material that we present in the first part stems from questions or problems posed in [
8]. Actually, we devote 
Section 3 to nonstandard proofs of three known results which are related to the content of [
8]. While not strictly pertinent to noncommutative probability, we present those proofs mostly to give insight on the use of nonstandard techniques in the nonstandard hull framework. In 
Section 3, we occasionally point out what seem to be inaccuracies or mistakes in [
8].
In 
Section 4 we provide results about weights that are defined on nonstandard hulls and we prove a weak property of normality for a class of those weights, thus extending a result obtained in [
8].
In 
Section 5 we deal with 
-probability spaces. After some preliminary results about states, we show that the property of freeness of a family of subalgebras is preserved by forming the nonstandard hull of a 
-probability space. We introduce the nonstandard notion of almost freeness and we show that it coincides with freeness on standard families of subalgebras of a standard 
-probability space, thus obtaining a nonstandard characterization of the ordinary freeness property.
In 
Section 5 we also obtain a nonstandard characterization of the noncommutative notion of convergence in distribution and we provide an elementary nonstandard proof that the property of *-freeness is preserved by convergence in *-distribution. In the last part of 
Section 5, we investigate the behaviour of the free product of 
-probability spaces with respect to the nonstandard hull construction.
In 
Section 6 we apply the results from the previous section. After recalling the notion of stochastic process over a 
-algebra given in [
9], we extend the nonstandard hull construction to an internal noncommutative stochastic process. In this setting we deal with the notion of equivalence. We provide nonstandard versions of the reconstruction theorem in [
9] and of other results therein. In this regard, we notice that, in light of the above-mentioned relationship between nonstandard hulls and ultraproducts, the nonstandard hull of an internal noncommutative stochastic process should be related to some sort of ultraproduct construction that applies to a family of ordinary noncommutative stochastic processes. We could not find any reference to such a construction in the literature. Eventually, we briefly discuss the adaptedness and the Markov properties in the framework of noncommutative stochastic processes, with special attention to the case of the nonstandard hull of an internal process.
In the mostly speculative 
Section 7, we try to make sense of the belief that a nonstandard universe does, or should have, physical significance on its own (see [
10], for instance). We translate nonstandardly a result on the approximation of a Fock space by means of a sequence of so-called toy Fock spaces and we give a presentation of the nonstandard hull of an internal Fock space.
Finally, we point out that the ultraproduct construction is extensively used in [
10]. In our opinion, the nonstandard techniques allow for simpler and more natural proofs of a large number of results given therein.
  2. Preliminaries
We refer mostly to [
11] for the basics of the theory of 
-algebras. All 
-algebras are assumed to be unital. We denote an algebra unit by 1. The term subalgebra always stands for 
-subalgebra. Similarly, the term homomorphism of 
-algebras always refers to a *-homomorphism.
As in [
11], we use the term inner product rather than hermitian product.
We assume that the reader is familiar with the notions and the basic techniques of nonstandard analysis as introduced, for instance, in [
5]. The reader who is interested in an axiomatic presentation of those techniques may refer to [
6] [§1].
Here we just recall that a nonstandard universe allows to properly extend each infinite mathematical object X under consideration of an object  in a way that X and  satisfy the same properties which are definable by means of bounded quantifier formulas in the first order language of set theory. This property is referred to as the Transfer Principle.
We warn the reader that the notation  for the nonstandard extension of an ordinary mathematical object  should not be confused with  denoting the adjoint of some element  whenever the latter makes sense.
Sets of type  are called standard. An element of some standard set is called an internal set. If  are internal sets, by  we denote the internal set of all internal B-valued functions defined on 
Relative to a nonstandard universe one can formulate the internal equivalents of all ordinary mathematical notions. Intuitively, to each property P which is bounded quantifier-definable (possibly with parameters) in the language of set theory there corresponds a property  and the Transfer Principle ensures that a set X satisfies P if and only if its nonstandard extension  satisfies  Therefore we can consider, for instance, continuity; compactness, etc. For simplicity, we will omit the initial “star” when it is clear that the property under consideration applies to some internal set.
A nonstandard universe also contains sets which are not standard. This is ensured by the so-called 
κ-saturation property: for some uncountable cardinal 
 which is sufficiently large for our purposes, we require that every family of cardinality smaller than 
 of internal sets with the finite intersection property has nonempty intersection. It can be proved that, for every 
 as above, there exists some 
-saturated nonstandard universe (see, for instance, [
12]).
In the following we will also make use of Keisler’s Internal Definition Principle: In every nonstandard universe, a bounded quantifier formula in the first order language of set theory with internal parameters defines an internal set.
The so-called Overspill Lemma is a straightforward consequence of -saturation. We formulate the former relative to : Any internal subset of  that contains arbitrarily large finite (in absolute value) hypercomplex numbers also contains some infinite hypercomplex (i.e., some infinite element in ).
We assume that some sufficiently saturated nonstandard universe has been fixed throughout this paper and we briefly recall the nonstandard hull construction (see [
1]). As we mentioned in the Introduction, the nonstandard hull is a slight generalization of the ultraproduct construction in functional analysis. In this paper we prefer the former construction because, assuming familiarity with the nonstandard techniques, it is much simpler than the ultraproduct.
Let A be an internal -algebra. The nonstandard hull of A is the ordinary -algebra  defined by letting:
- (1)
- (2)
- for  if  
- (3)
- for  
- (4)
We define operations on 
 as follows:
      and norm by 
, for all 
 and all 
.
It can be easily verified that the operations on  are well defined and that  is a -algebra. If  we let  In particular, if B is a subalgebra of A then  is a subalgebra of 
Let A be an ordinary -algebra. Under the assumption that the set of individuals of our nonstandard universe is a superset of  we have that  Furthermore, by identifying  with  we have that A is a -subalgebra of  As is customary, we write  for 
If 
 is a homomorphism of ordinary 
-algebras, we let
      
Since homomorphisms are norm-contracting, the map  is well-defined. Furthermore, it is straightforward to verify that it is a homomorphism.
All the above assumptions and notations are in force throughout this paper.
Similarly to the above, one defines the nonstandard hull  of an internal Hilbert space  It is a straightforward verification that  is an ordinary Hilbert space with respect to the standard part of the inner product of  Furthermore, let  be the internal -algebra of bounded linear operators on some internal Hilbert space H and let A be a subalgebra of  Each  can be regarded as an element of  by letting  for all  of finite norm. (Note that  is well defined since a is norm–finite.) Therefore we can regard  as a -subalgebra of 
  4. Noncommutative Loeb Theory
At first reading, the title of this section may sound somewhat obscure. To clarify it, we recall that a Loeb probability measure is an ordinary probability measure that is obtained from an internal finitely-additive probability measure. See [
5] or [
6]. We recall that a 
-probability space is a pair 
 where 
A is a 
-algebra and 
 is a state, namely a positive linear functional with the property that 
In short: States are the noncommutative counterparts of probability measures. In the following we deal with the problem of obtaining an ordinary weight from an internal one. Moreover, weights are closely related to states. Hence the title of this section.
We begin by recalling some notions and elementary facts relative to an ordinary -algebra 
A weight is an additive, positively homogeneous function  i.e.,  for all  and all  with the convention that  (so that ).
Let 
 be a weight. From the inequality 
 (see [
11] [II.3.1.8]), it follows that 
 Therefore condition 
 is equivalent to 
 A weight is 
finite if it satisfies one of those two equivalent properties.
A finite weight 
 extends uniquely to a positive linear functional on 
 usually denoted by the same name. This is because each 
 can be uniquely written as 
 for some positive 
 each of norm 
 (Recall that 
 and see, for instance, [
8] [Corollary 3.21].) Conversely, every positive linear functional on 
A yields a finite weight.
A weight 
 is 
normal if for any uniformly norm-bounded increasing net 
 such that 
 exists in 
 then
      
Let  be a cardinal. We say that a weight  is -normal if the previous property holds for any uniformly norm-bounded directed family  with 
For the rest of this section, if not otherwise stated, A is assumed to be an internal -algebra.
Following nonstandard terminology we say that an internal weight 
 is 
S-continuous if 
 for all 
 We recall the following (see [
8] [Lemma 4.4]):
Lemma 2. The following are equivalent for an internal weight :
- (1)
- ϕ is S-continuous; 
- (2)
- (3)
- for all  if  then  
 For benefit of the reader who wants to check the proof of Lemma 2 given in [
8], we point out that [
8] [Proposition 3.12] lacks the crucial assumption 
 (which is trivially satisfied if 
 are positive elements). Actually, as it stands, [
8] [Proposition 3.12] is wrong, even for commutative internal algebras: Let 
 be the internal 
-algebra of 
-valued functions on some compact space 
X an let 
 be such that 
 Let 
 be the constant functions 
 and 
 Then 
 but there is no 
 that satisfies 
 and 
Let 
 be an internal 
S-continuous weight. By Lemma 2, 
 takes values in 
 (we will say that it is a 
finite weight). As previously noticed, we can extend 
 to an internal positive linear functional defined on 
 that we still denote by 
 By transfer of [
16] [Theorem 4.3.2], we have 
 It follows from Lemma 2(2) that 
 Hence there is a one-to-one correspondence between the internal 
S-continuous weights and the internal positive linear functionals of (standard) finite norm.
By Lemma 2(3), from an internal 
S-continuous weight 
 we can define a map
      
Clearly 
 is additive and positive homogeneous, hence a (finite) weight. It can be regarded as a noncommutative Loeb integral operator (see the discussion in [
8] [§4.4]).
Here is an example of an internal weight which is not the nonstandard extension of any ordinary weight: Let  and let  be the internal -algebra of  matrices on  Let  be the normalized trace defined by  By Lemma 2, tr is S-continuous. Notice that the non-normalized trace is not S-continuous.
Next we want to prove that every 
S-continuous internal weight in a 
-saturated nonstandard universe is 
-normal, thus strengthening [
8] [Theorem 4.5] (see [
8] [Question 11]). We point out that, in the following result, differently from [
8] [Theorem 4.5], the internal weight is not required to be normal and the internal 
-algebra is not necessarily commutative.
Let . We write  if  or 
Theorem 1. Let  be an internal S-continuous weight in a κ-saturated nonstandard universe. Then the weight  defined in (2) is κ-normal.  Proof.  By Transfer of the Gelfand–Naimark Theorem ([
11] [Corollary II.6.4.10]), we assume that 
A is a subalgebra of the internal 
-algebra 
 for some internal Hilbert space 
 As remarked at the end of 
Section 2, we regard 
 as a subalgebra of 
 where 
 is the nonstandard hull of 
We denote by 
 the unit ball centered at the origin of 
 By [
11] [I.2.6.7], the following are equivalent for 
:
- (1)
- (2)
- for all  
- (3)
- for all  and  
Let  be an infinite norm-bounded directed family with  Let L be a norm-bound for the elements of  Let  be formed by picking exactly one representative for each element in  so that 
Let  Since F is norm-bounded, R is finite.
We claim that there exists  such that  for all  and  To prove this, let  be the set of finite subsets of  Notice that  For each  and each  let  be the internal subset of A whose elements x satisfy the following properties:
- (a)
- (b)
- for all  and all  and  
- (c)
By directness of  the equivalence  above and the definition of  the  are nonempty. Moreover they have the finite intersection property, since 
By 
-saturation, we let 
 Then 
 satisfies the required conditions. It follows that 
 for all 
 Being 
 a 
-upper bound of 
 if 
 exists in 
 then
        
Therefore  is -normal.    □
 With reference to the previous theorem, it is straightforward to check that the weight  is -completely additive, namely if I is a set of cardinality  and  is a family of elements of  such that  is defined, then 
We briefly comment on [
8] [Question 11]. If an internal weight 
 is not 
S-continuous and 
 is such that 
, then there exists 
 such that 
 Hence only when 
 is the so-called degenerate weight (namely 
 satisfies 
 and 
 for 
), it is possible to define a weight 
 as in (
2). In such case, 
 itself is the degenerate weight.
  5. Nonstandard Noncommutative Probability
In this section we will be mostly concerned with an important part of noncommutative probability known as free probability. The latter was initiated by Voiculescu to attack a problem in the theory of von Neumann algebras. See  [
17].
In 
Section 4, we already recalled the definition of 
-probability space (briefly: 
ps). We recall the following definitions.
We notice that, by Lemma 2, the state 
 in an internal 
ps 
 is 
S-continuous. Therefore, by defining 
 as in (
2) above, we have that 
 is an ordinary 
ps. We will use this fact without further mention.
We say that an internal state 
 is 
S-faithful if
      
We have the following characterization of faithfulness:
Proposition 9. Let  be an ordinary state. The following are equivalent:
- (1)
- ϕ is faithful; 
- (2)
-  is S-faithful; 
- (3)
-  is faithful. 
 Proof.   We assume (1). Let  be such that  Then there exists some nonnegative infinitesimal  such that  Hence  From the equality  we get 
 We assume (2). Let 
 We get the following chain of implications:
          
 Since we can assume without loss of generality that A is a subalgebra of  and that  extends  the result is straightforward.    □
 We say that an internal state 
 is 
S-tracial if
          
We leave the straightforward proof of the following to the reader.
Proposition 10. Let  be an ordinary state. The following are equivalent:
- (1)
- ϕ is a tracial state; 
- (2)
-  is S-tracial; 
- (3)
-  is a tracial state. 
 To help the reader’s intuition, we stress that, in a ps  the elements of A play the roles of random variables, whose expectation is given by 
Next we formulate the property of free independence (for short: freeness). See [
17] [Proposition 3.5] for insights about such notion.
Definition 2. Let  be an ordinary ps. A family  of -subalgebras of A is free if for all  all  and all  such that  and  it holds that 
 We stress that freeness depends on the state  Therefore, in the previous definition, it would be more appropriate to say that the family  is free with respect to  Usually it is the context that prevents any ambiguity.
Notice that Definition 2 makes sense also for a family of unital *-subalgebras of 
Notational convention. A family  of -algebras is actually a function B defined on  Therefore we denote its nonstandard extension  which is a function defined on  by  For notational simplicity we write  for  Without loss of generality, we can further assume that 
The above notation and assumption are in force throughout this section.
The chain of equivalences in the following result provides a nonstandard characterization of freeness and proves that the latter is preserved and reflected by the nonstandard hull construction.
Proposition 11. Let  be an ordinary ps and let  be a family of -subalgebras of  The following are equivalent:
- (1)
-  is free; 
- (2)
- there exists some  for which the following holds: For all  all internal  and all internal  such that  if  then  
- (3)
-  is free with respect to  
 Proof.   is a consequence of Transfer.
Regarding  we fix N as in  Let  and  be such that  and  Then  for all  Let  Therefore  and  for all  It follows by assumption that  Since  we get  Therefore 
The proof of  is straightforward from  for all     □
 The proof of the previous proposition naturally leads to formulating a nonstandard variant of the notion of freeness.
Definition 3. Let  be an internal ps. A family  (not necessarily internal) of internal -subalgebras of A is almost free if, for all  all  and all  whenever  and  then 
 Proposition 12. Let  be an ordinary ps and let  be a family of subalgebras of  The following are equivalent:
- (1)
-  is free. 
- (2)
-  is almost free. 
 Proof.   Let  and  be such that  and  Since  for all  then  We notice that  where S is a standard finite sum of terms each having infinitesimal norm. Therefore  as required.
 The following chain of implications holds:  is almost free  is free  is free  is free. The leftmost implication is straightforward and the middle one holds by Proposition 11. The rightmost implication holds by Transfer.    □
 Corollary 2. Let  be as in Proposition 12. Then  is free if and only if  is almost free.
 Let  be an internal ps and let  be an internal free family of subalgebras of  Notice that the same proof as  in Proposition 12 shows that  is almost free.
Noncommutative probability has its own notion of convergence in distribution (see [
17]):
Definition 4. Let  and  be ordinary ps. For each  let  be a sequence in  and let  be a sequence in  We say that
- (1)
-  converges in distribution to a if, for all  and all  
- (2)
-  converges in *-distribution to a if for all  all  and all  
 We stress that, in the previous definition, the “*” refers to the adjoint operator.
With the notation of Definition 4 in force, let 
 for some 
 and let 
 be the extension of 
 defined by 
 for all 
 Similarly, let 
 be the extension of 
a obtained by letting 
 We make the trivial observation that 
 converges in *-distribution to 
a if and only if 
 converges in *-distribution to 
 From now on we assume that 
 and 
a satisfy the following property:
          
Let  be the nonstandard extension of  Without loss of generality we assume  We give the following nonstandard characterization of convergence in distribution. A similar characterization applies to convergence in *-distribution.
Proposition 13. With the notation of Definition 4 in force, and under the subsequent assumptions, the following are equivalent:
- (1)
-  converges in distribution to  
- (2)
- there exists  such that the following holds for all internal N-tuples  in : 
 Proof.  For  we denote by  the internal set formed by all internal tuples in 
 From (1) we get by Transfer and Overspill that the internal set
            
            properly contains 
 Any 
 witnessing the proper inclusion satisfies the required property.
 Let 
 be positive natural numbers. From (2), recalling 
, we get that 
Hence, by Transfer and by arbitrariness of , we get (1).    □
 Definition 5. Let  be an ordinary ps and let  be a family of subsets of A and let  be the unital -algebra generated by  for  We say that  is *-free if  is free.
A sequence  is *-free if so is 
 We have already noticed that the notion of freeness can be formulated with reference to a family of *-subalgebras of a given -algebra A in a ps  Actually the following holds:
Proposition 14. Let  be an ordinary ps. Let  be a family of unital *-algebras of A and, for each  let  be the -algebra generated by  Then  is free if and only if so is 
 Proof.  In order to establish the nontrivial implication we apply Corollary 2. Let  and  be the nonstandard extensions of the two families with the same names. Let  and  be such that  and  Since  is in the internal closure of  there exists some  such that  Hence  for each  By almost freeness of  we get that  Since  we finally get  Having established that  is almost free, we are done by Corollary 2.    □
 We apply the latter proposition and previous results to give an elementary nonstandard proof of the following known fact:
Proposition 15. Let  and  be ps. For each  let  be a *-free sequence in  If  converges in *-distribution to  then a is *-free.
 Proof.  For notational simplicity let us consider the case when  For  let  and 
Let  and let  and  be elements in the unital *-algebras generated by  and  respectively. Let us assume that  and  We claim that  Once more for the sake of simplicity, let us assume  and let  (The argument below immediately extends to any positive )
Recalling how the *-algebra generated by  is obtained, we associate to u a sequence  where  belongs to the *-algebra generated by  and  is defined from  in the same way as u is defined from  By assumption we have  We do the same with 
Let us denote by  and  the nonstandard extensions of  and  respectively.
Next we use the nonstandard characterization of convergence of a sequence. Let  and  be the nonstandard extensions of  and  respectively. For all  we have  and  By Corollary 2 we get that  for all  Hence     □
 Next we investigate the behaviour of the free product of 
-probability spaces with respect to the nonstandard hull construction. We begin by recalling the definition of free product (see [
18] [Definition 7.10]):
Definition 6. Let  be a family of ordinary ps such that the functionals  are faithful traces. A ps  with ϕ a faithful trace, is called a free product of the family  if there exists a family  of norm-preserving unital homomorphisms with the following properties:
- (1)
- for all  
- (2)
- the -subalgebras  form a free family in  
- (3)
-  generates the -algebra A. 
 It can be shown that a free product of the family 
 as in Definition 6 does exist. The assumption of faithfulness is just a technical simplification. Furthermore, 
 and the family 
 are unique up to isomorphism. See [
18] [Theorem 7.9].
Theorem 2. Let  be an ordinary family of ps such that the functionals  are faithful traces. Let  be the free product of the family with norm-preserving unital homomorphisms  as in Definition 6. If the -algebra  is generated by  then  is the free product of the family  with norm-preserving unital homomorphisms 
 Proof.  At the beginning of 
Section 5 we have already observed that if 
 is an ordinary 
ps then so is 
 Moreover, if 
 is faithful so is 
 by Proposition 9. Furthermore, if 
 is tracial so is 
: let 
 Then 
 where the middle equality holds by Transfer. Hence 
 We leave it to the reader to verify that if 
 is norm-preserving so is 
In light of the previous considerations and of the assumption that  is generated by  we are left to show that (1) and (2) of Definition 6 are satisfied by  and  Condition  holds for all  by Transfer and by definition of 
Eventually, the family  is free with respect to  by Proposition 11.    □
 With reference to the proof of the previous theorem, we point out that we do not use the explicit construction of the free product outlined in [
18] [Lecture 7]. We just make use of the universal property of that construction.
Regarding the assumption in the statement of Theorem 2 that the -algebra  is generated by  we notice that the other assumptions only ensure that the -algebra generated by  is a subalgebra of  Actually, if  is an internal family of -subalgebras of the internal -algebra A such that  generates  it might be that  generates a proper -subalgebra of  as the following shows.
Example.  Let 
 and let 
 Let us denote by 
 the internal 
-algebra of internal functions 
 equipped with the supremum norm and with componentwise addition, multiplication and conjugation. Let 
 be the unit of 
 and, for 
 let 
 be the function in 
 that takes value 1 on 
i and 0 elsewhere. Clearly, 
 is internally generated by 
 where 
 is the 
-algebra generated by 
 for 
 Let 
 be defined as follows:
          
 We observe that the ordinary -algebra generated by  is just the -algebra generated by  and we show that  does not belong to the latter.
First of all, we introduce a convenient presentation of 
 We associate to each 
f in 
 the map
          
Notice that 
 is well-defined because 
 for all 
 The set
          
          is closed under componentwise addition, multiplication and conjugation. It can be easily verified that, equipped with the supremum norm, 
A becomes a 
-subalgebra of the ordinary 
-algebra 
 of complex valued functions defined on the discrete space 
 A little bit of work is only required to prove that 
A is closed. We sketch the relative proof to highlight the use of a fairly routine nonstandard argument.
Let  be a Cauchy sequence in  Let  be such that  for all  Let  be a strictly increasing sequence of natural numbers with the following properties:
- (a)
- for all  
- (b)
- for all  it holds that  
For each positive natural number  we let  be the internal set of (internal) sequences  of elements of  with the following properties:
- (1)
- for all  
- (2)
- for all  
- (3)
- for all  
Each  is internal, by the Internal Definition Principle. It is easily seen that the family  has the finite intersection property. By saturation, there exists  Let  By definition of  for all  and all  Then  converges to 
Having established that 
A is a 
-algebra, it is straightforward to verify that the map
          
          is an isometric isomorphism. From now on we deal with 
 We regard the maps 
 and the 
’s, 
 as elements of 
 Finally, we prove that 
v does not belong to the 
-algebra generated by 
 First of all we notice that every element in the ordinary *-algebra 
B generated by 
 is a constant function on all but finitely many points. For the sake of contradiction, let 
 be such that 
 Let 
 and 
 be such that 
 From 
 we get a contradiction. Hence 
v does not belong to the norm-closure of 
Let  be a directed partially ordered set. If for all  there exists  such that  and  then the extra assumption in Theorem 2 is satisfied, as a consequence of the following:
Proposition 16. Let  be an internal directed set. Let  be an internal family of subalgebras of an internal -algebra B with the property that for all  there exists  such that  and 
If B is generated by  then  is generated by  Actually,  Proof.  Notice that  is an internal *-algebra. From the assumption that B is generated by  it follows that for each  there exist  and  such that  Hence  and so  The converse inclusion is trivial.    □
   6. Nonstandard Noncommutative Stochastics
We begin with the definition of stochastic process over a 
-algebra given in [
9]:
Definition 7. Let B be a -algebra and let T be a set. An ordinary noncommutative stochastic process (briefly: nsp) over B indexed by T is a triple  where
- (a)
-  is a ps; 
- (b)
- for each  is a -algebra homomorphism with the property that  
The stochastic process  is full if the -algebra A is generated by 
 Notice that, in [
9], all nsp’s are assumed to be full. Fullness is needed in the proof of [
9] [Proposition 1.1].
Let us recall some notation and terminology from [
9]: Let 
 be an ordinary nsp and, for all 
 let 
 We define the map 
 by letting 
 The 
-correlation kernel is the function
            
It is straightforward to verify that  is conjugate linear in each of the ’s components and linear in each of the ’s components. (This is the usual convention in Physics.)
We endow 
 with the supremum norm and we denote by 
 its unit ball. As is usual with sesquilinear forms, we define the norm of 
 for 
 as follows:
            
We recall the following definition from [
9]:
Definition 8. Let  be ordinary nsp’s and let  be the GNS triples associated to  for  (see [11] [II.6.4]). The processes  and  are equivalent if there exists a unitary operator  such that  The following is a characterization of equivalence between full nsp’s (see [
9] [Proposition 1.1]).
Proposition 17. For  let  be ordinary full stochastic processes. The two processes are equivalent if and only if, for all  all  and all  it holds that  We make use of Proposition 17 to give a nonstandard characterization of equivalence.
Theorem 3. For  let  be ordinary full nsp’s. Let  be the nonstandard extension of  The following are equivalent:
 Proof.   is a straightforward consequence of Proposition 17 and of Transfer.
Concerning the converse implication, let 
N be as in (2). We fix 
 Let 
. We extend them to internal sequences of length 
N by letting, for instance, 
 Then
              
Being n arbitrary, by Proposition 17 we get that  and  are equivalent.    □
 The content of Theorem 3 is that a full nsp  is determined, up to equivalence, by the internal family of correlation kernels  of the process  for some infinite hyperatural 
The reader who is familiar with the notion of stochastic process, as introduced for instance in [
19], is invited to read the commentary on [
9] [
Section 1] to make sense of Definition 7. In short, let 
 be an ordinary stochastic process, where the 
’s are measurable functions defined on a probability space 
 with values in some measurable space 
 Let 
 be defined by 
 for all 
It can be shown that the triple
            
            where 
 for all 
 and all 
 forms a nsp in the sense of Definition 7. Furthermore, under additional assumptions on a nsp, one can associate to the latter an ordinary stochastic process.
Let 
 be an internal nsp. For all 
 the map 
 defined by 
 is well-defined because 
-algebra homomorphisms are norm contracting. It is straightforward to verify that the nonstandard hull 
 of 
 is an ordinary nsp. We point out that the 
-algebra generated by 
 is a subalgebra of 
 but, in general, fullness of 
 is not inherited by 
 In this regard, see the Example in 
Section 5 and the discussion preceding it. The following is a sufficient condition for preservation of fullness.
Proposition 18. Let  be an internal linearly ordered set and let  be an internal full nsp with the property that, for all  in  is a subalgebra of  Then  is an ordinary full nsp.
 Proof.  An immediate consequence of Proposition 16.    □
 Next we provide a nonstandard characterization of equivalence between nsp’s of the form 
We make a preliminary remark. Let 
 be an internal 
ps and let 
 be the associated internal GNS triple, where 
 is the cyclic vector of the representation. As we already remarked at the end of 
Section 2, we can identify 
 with a 
-subalgebra of 
 It can be easily verified that
            
            is a *-homomorphism and that, for all 
 where 
 denotes the inner product on 
In order to conclude the verification that  is a GNS triple for  we prove the following result, which is actually stronger than what we need:
Proposition 19. Let  be as above. Then 
Consequently,  is a GNS triple for 
 Proof.  Following [
11] [II.6.4], let 
 By the GNS construction, we have that 
 is the image of the unit of 
A in 
 and that 
 is the left multiplication operator by 
a on 
 Moreover 
 is an inner product space with respect to 
 defined by
              
Furthermore, 
H is the Hilbert space completion of 
 and the set
              
              is dense in 
Let 
 Then there exists 
 such that 
 and, by definition of norm on a quotient space, there exists also 
 such that 
 It follows that 
 is finite. Furthermore
              
Therefore there exists some  such that  For such a b it holds that     □
 Theorem 4. Let  be internal nsp’s over the -algebra B such that  and  are full. Let  be the internal GNS triples associated to  for  The following are equivalent:
- (1)
- the processes  and  are equivalent according to Definition 8; 
- (2)
- there exists an infinite hypernatural N such that, for all  the -correlation kernels  relative to  respectively satisfy the property  (namely, . 
 Proof.  (1)⇒(2) For 
 let 
 be the set
                
By the Internal Definition Principle, each 
 is internal. It follows from [
9] [Proposition 1.1] that the family 
 has the finite intersection property. By saturation, 
 Any 
N in the common intersection is an infinite hypernatural with the property that, for all 
 and all 
 Recalling that the supremum of an internal set of infinitesimals is itself an infinitesimal, we get that, for all 
 as required.
(2)⇒(1) Let 
N be as in (2) and let 
 be arbitrarily chosen. By [
9] [Proposition 1.1] and by linearity it suffices to prove that
                
Let  and let  We extend them to internal sequences of length N by letting 
From  we get immediately that     □
 The content of Theorem 4 is that the nonstandard hull  of an internal, full nsp  is determined, up to equivalence, by the internal family of correlation kernels  of  for some infinite hypernatural 
When  is an ordinary nsp we write  for  (The context will prevent any ambiguity.) Notice that if  is indexed by set  then  is indexed by 
We prove that, under the additional assumption of fullness, equivalence of nsp’s is preserved and reflected by the nonstandard hull construction.
Proposition 20. Let  be ordinary full nsp’s such that their nonstandard hulls are also full. Then  and  are equivalent if and only if  and  are equivalent.
 Proof.  Let us assume that  and  are equivalent. Notice that if u is an internal unitary operator then  is well-defined and unitary. Moreover equalities are preserved by the nonstandard hull construction. By Transfer of Definition 8 it is thus straightforward to prove that  and  are equivalent. Notice that we do not need the fullness property for this implication.
Regarding the converse implication, for all 
 and all 
 let us write 
 for 
 Let us assume that 
 and 
 are full. By Proposition 17, we have that 
 Then, for all 
Eventually, by applying Proposition 17 again, we get that  and  are equivalent.    □
 Next we provide a nonstandard version of the Reconstruction Theorem ([
9] [Theorem 1.3]). Let 
B be an internal 
-algebra and 
T an internal set. We let 
 If 
 we let 
 be the sequence obtained by removing the 
K-th component from the tuple 
 Same meaning for 
 when 
 and 
 Furthermore, we let 
 If 
 we let 
 be the time sequence obtained by inserting the component 
 between 
 and 
 We denote by 
 the length of the sequence 
 and by 
 the element 
 in 
 for some 
 (the context will prevent any ambiguity).
Let 
 Inspired by the notion of 
-correlation kernel previously introduced (see also [
9] [Proposition 1.2]), we say that an internal family 
 of maps is an 
N-system of correlation kernels over 
B if it satisfies the following properties (when not specified, quantifications refer to internal objects):
- CK0N
- for all  and all  it holds that
                     - –
-  and 
- –
- if  and  then  
 
- CK1N
- for all  - , all  -  all norm-finite  -  such that  -  and  -  it holds that
                     
- CK2N
- for all  -  all  -  and all internal sequences  -  and  -  it holds that
                     
- CK3N
- CK4N
- for all  such that  and all  it holds that
                     - –
- for all  -  all norm-finite  -  such that  -  and  -  the map
                         - 
                        is approximately conjugate linear, namely: For all  -  and all  
- –
- for all  -  all norm-finite  -  such that  -  and  -  the map
                         - 
                        is approximately linear (see above); 
 
- CK5N
- for all  and all norm-finite  the map  defined by  approximately factors through the map  namely: There exists some internal map  such that, for all  
- CK6N
- for all  -  all  -  all  -  and all  -  if  -  then
                     
A 1-system of correlation kernels is a family  of maps that satisfies CK0 and CK2–CK5
Notice that the definition of a system of correlation kernels given in [
9], strict equalities are required. We do not impose that condition because we claim that an 
N-system, for some 
 suffices to reconstruct an unique ordinary nsp. We prove that after a preliminary construction.
Let 
 and let 
 be an internal 
-system of correlation kernels over an internal 
-algebra 
 We define an 
N-system 
 as follows: we fix 
 and, for each 
 we let
                
By CK1, a different choice of  amounts to an infinitesimal perturbation in the value of 
The verification that  satisfies properties CK0– CK6 is straightforward. Thus we can repeat the construction and, by internal induction, we get a family  of K-systems of correlation kernels, one for each  Let 
We notice that, for all 
 holds. By CK0
, 
 the map
                
                is well-defined for all 
 We let 
The following holds:
Theorem 5. Let N be an infinite hypernatural, T an internal set and let  be an internal -system of correlation kernels over some internal -algebra  There exists an ordinary nsp  whose family of correlation kernels is the family  defined above. Moreover such  is unique up to equivalence.
 Proof.  We verify that the family 
 is a projective system of correlation kernels over 
 indexed by 
 according to [
9]. Equalities up to an infinitesimal turn into equalities when taking the nonstandard part. First of all we notice that 
 satisfies property CK1 as a consequence of the validity of CK1
 Concerning CK2, it suffices to keep in mind that the standard part of the sum of finitely many finite addends is the sum of their standard parts.
The only property whose verification requires a little bit of work is CK5. We fix  and  We notice that the map  is well-defined by CK0 We prove that it factors through the map  Let  be as in CK5 relative to  From  and from CK0 we get  and  whenever  Hence  is well-defined.
Let 
 We have:
                  
				  By arbitrariness of 
 we get 
The remaining properties are easily verified.
Finally, we get the existence of an ordinary nsp 
 with the required properties from [
9] [Theorem 1.3]. Notice also that the proof of the latter theorem ensures that 
 is full.    □
 Let N be an infinite hypernatural. As already anticipated, the content of Theorem 5 is that an N-system of correlation kernels contains enough information to uniquely reconstruct, up to equivalence, an ordinary nsp whose family of correlation kernels is determined by the N-system.
Let  be the nonstandard hull of some internal nsp  Admittedly, it is a limitation that the time set T of  is an internal set. This rules out many familiar sets. To overcome such restriction, we may suitably choose 
One possibility is to fix some infinite hypernatural M and to let  Then, for all  we let  and we define  as follows: . In this way, the time set of  is the real unit interval. We may also make the additional assumption that the internal process  is S-continuous, namely that, for all  implies  Under S-continuity, it follows that, for all  and all  if  and  then 
Another possibility is to fix the factorial M of some infinite hypernatural number and to define T as above. Thus the set  contains all the rationals in the unit interval. Under the assumption of S-continuity, the map  defined by  is a well-defined -algebra homomorphism (see above). Therefore we get an ordinary nsp  whose time set forms a dense subset of the real unit interval.
Alternatively, we may let  for some infinite hypernatural M or  and consider the ordinary nsp 
Next we discuss the Markov property relative to a nsp and we formulate sufficient conditions for recovering an ordinary Markov nsp from an internal one.
We begin by recalling the definition of conditional expectation in the noncommutative framework. Let A be an ordinary -algebra and let  be a -subalgebra of  A mapping  is called a conditional expectation if
- (1)
- E is a linear idempotent map onto  
- (2)
It is straightforward to check that 
 holds for a conditional expectation 
 Moreover, the following hold (see [
20]):
- (a)
-  for all  and all  
- (b)
-  for all  
- (c)
- E is positive. 
Let T be a linearly ordered set. We say that a nsp  is adapted if, for all  in  is a -subalgebra of  By adopting this terminology, the content of Proposition 18 is that fullness of an adapted nsp is preserved by the nonstandard hull construction.
Definition 9. Let T be a linearly ordered set. The adapted process  is a Markov process with conditional expectations if there exists a family  of conditional expectations such that, for all  the following hold:
- E2 
 
- E3 
 
 Definition 9 is a restatement in the current setting of the definition of Markov nsp with conditional expectations in [
9] [§2.2]. By property (a) above it follows immediately that property E1 in [
9] [§2.2] holds and that, for all 
For all  let  be the -algebra generated by  It is straightforward to check that the Markov property
Let  be as in Definition 9. By letting  for  in  we get a family  of conditional expectations satisfying
- (1)
-  for all  
- (2)
-  for all  in T - as well as the Markov property M in [ 9- ]. It follows that the statement of [ 9- ] [Theorem 2.1] (with the exception of the normality property) and subsequent results do hold for  -  and  -  In particular the quantum regression theorem [ 9- ] [Corollary 2.2.1] does hold. 
So far for the ordinary setting. Next we fix the factorial N of some infinite hypernatural number and we let  Let  be an internal S-continuous adapted Markov process with an internal family  of conditional expectations.
We have previously remarked that the ordinary nsp  is well-defined and that  Furthermore,  holds for all  and the map  given by  is a well-defined conditional expectation. Under the assumption that the family  is S-continuous, namely  whenever  it follows that the map  defined by  is well-defined. Moreover, the family  satisfies E2 and E3 of Definition 9 and the Markov property M Hence  is an ordinary adapted noncommutative Markov process with conditional expectations. It seems that the adaptedness property of the internal process  is needed in order to get the above conclusion, due to the already mentioned fact that the nonstandard hull construction, in general, does not behave well with respect to the operation of forming the -algebra generated by family of subalgebras of a given algebra.
  7. Nonstandard Fock Spaces
In most cases nonstandard universes are used to derive results about the standard universe. Some authors go beyond that. For instance, in [
10], the author contends that “a nonstandard universe has physical significance in its own right" and, more specifically, “the states and observables of the nonstandard Fock space have physical significance”. Admittedly, the author does not elaborate much on his statements in quotations.
In this short section we derive from standard results that each element of the nonstandard extension of the free Fock space is infinitely close to some “simple” element of a nonstandard free toy Fock space, in a sense that we make precise in the following.
Let 
H be a complex Hilbert space. We let
                  
                  where, for 
 is the 
n-fold tensor product of 
H and 
 is a one-dimensional space which is often denoted by 
 Here 
 is a distinguished unit vector, called the vacuum vector. Recall that the elements of 
 are of the form 
 with 
 for all 
 and 
 where 
 is the norm on 
 The space 
 is equipped with the norm 
 defined by
                  
In the following by the free Fock space we mean the space  We denote the latter by  Regarding the physical import of  we just say that it describes the quantum states of a number of identical particles from the single particle Hilbert space 
We write an element  as  where  is the vacuum vector and, for all 
Next we introduce the 
free toy Fock space. For each 
 let 
 be an isomorphic copy of 
 and let 
 be the standard basis of 
 (Here and in the following we write vectors as column vectors.) The free toy Fock space 
 is defined as
                  
                  where 
 is the identification of the vacuum vectors 
 As pointed out in [
21], there is a one-to-one correspondence between the orthonormal basis of 
 which is naturally associated to the construction of the latter and the set of all finite sequences 
 and 
It can be shown quite easily that 
 can be embedded into 
 (see [
21] [§5]). More interestingly for us, in [
21] [§6] the authors construct a sequence of toy Fock spaces that approximate 
 We recast the authors’ main result in the framework of a nonstandard universe. First of all we notice that, by transfer, the nonstandard extension 
 of 
 is the internal norm closure of the internal direct sum of the Hilbert spaces 
Let 
 and let 
 be an internal partition of 
 such that, for all 
 For each 
 let 
 be the normalized characteristic function of the interval 
 namely the function
                  
We form the internal toy Fock space
                  
                  where the innermost direct sum is intended to range over all internal 
N-tuples 
 of hypernaturals such that 
Let 
 be the internal orthogonal projection onto 
 We apply [
21] [Theorem 1(1)] to the sequence of partitions 
 where 
 has constant step 
 By Transfer and by the nonstandard characterization of convergence of a sequence we get that 
 for all 
 It follows that, up to an infinitesimal displacement, we can regard each 
 as a hyperfinite (hence: A formally finite) sum of pairwise orthogonal elements, each belonging to some of the direct summands that occur in the definition of 
 Moreover, since the supremum of an internal set of infinitesimals is itself an infinitesimal, we also get 
 Hence, by passing to nonstandard hulls and by writing 
 for 
 as is usual, the map 
 defined by 
 for 
 is just 
 As a consequence we get that 
 Notice that the latter equality provides an equivalent definition of 
 In particular, every element of 
 can be lifted to some hyperfinite sum of the form described above.
By similar arguments, and in light of [
21] [Theorem 1(2)], we can approximate up to an infinitesimal displacement the creation and the annihilation operator on 
 by means of hyperfinite sums involving the discrete counterparts of those operators defined on 
 See [
21] for details.