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CRC Press eBooks

Of Cats and Pointers

Bernard d’Espagnat

Published Mar 5, 2018• 0 citations
Publisher

Abstract

Up to now, the initial state of the instrument has been ascribed a state vector. This convention can be criticized, however, either by observing that the instrument is a complicated system which is therefore imperfectly known, or, more adequately still (this is again the difference between proper and improper mixtures), by noting that the instrument has interacted with many other systems before the time when it is used for measuring L , and that consequently it can be associated, not with any definite state vector, but only with a density matrix (in other words, an ensemble of such instruments identically prepared would be an improper mixture). We may wonder whether this remark offers a clue for solving the difficulty encountered at the end of Chapter 14 . There it was shown that, if the ensemble E of instruments is initially a pure case, it is in general impossible to consider that every instrument coordinate has some definite eigenvalue after the interaction with the system has taken place. Let us investigate whether or not this is still the case when ensemble E is a mixture.

DOI
10.1201/9780429501449-21

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Most of the predictions of quantum mechanics are of a statistical nature and therefore make sense only for ensembles. The axiomatics based on the quantum calculus of propositions might open the way toward a general definition of the quantum state of an individual system. It was soon recognized that this leads to separability and thereby to violation of some of the quantum-mechanical predictions. In contemporary literature, the concept of state is not wholly unambiguous. Some authors associate it with the notion of an individual system and say, for instance that a given system is in a given state. Others associate it exclusively with ensembles. The situation is complicated by the fact that for some theorists the concept of state refers only to ensembles that can be described by some state vector. For other authors it refers just as well to ensembles that cannot be associated with any state vector and for which only a density matrix description is therefore acceptable.

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Meaning of the Density Matrix

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Protective measurement, which was proposed as a method of observing the wavefunction of a single system, is extended to the observation of the density matrix of a single system. d'Espagnat's definition of `proper mixture' is shown to be improper because it does not allow for appropriate fluctuations. His claim that there could be different mixtures corresponding to the same density matrix is critically examined. These results provide a new meaning to the density matrix, which gives it the same ontological status as the wavefunction describing a pure state. This also enables quantum entropy to be associated with a single system.

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So far we have only considered states in Postulate 25.1(PS) which correspond to a maximal amount of information of the system. These are pure states φ s describable by unit vectors φ → https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6289.tif"/> . Often we may only have a partial knowledge of a system. As an example, consider a less than ideal state preparation process which is unable to prepare the system in a desired pure state φ s . Instead the state preparation process can only determine the system to within a set of possible pure states φ l s https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6290.tif"/> , ℓ = 1, 2,…, namely the system may end up to be in a pure state φ 1 s https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6291.tif"/> , or φ 2 s https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6292.tif"/> and so on. Suppose the state preparation process can also tell us the probabilities w ℓ of the system ending up in these pure states. In other words, we do not know for certain which pure state the system is actually in. We only know that the system has a probability w ℓ to be in pure state φ l s https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6293.tif"/> . The system is then said to be in a classical mixture of states . In more abstract terms, the concept can be stated as A classical mixture of states is a characterisation of a given quantum system in terms of a set of possible pure states φ → l https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6294.tif"/> together with a corresponding set of probabilities w ℓ of their occurrence .

•Jul 9, 2019•0 citations

Reply to Aharonov and Anandan's "Meaning of the Density Matrix"

Bernard d’Espagnat

Aharonov and Anandan's claim that the notion of ``proper mixture'' is improper is shown to be unjustified. The point is made that if a purely operationalist standpoint is taken the three difficulties these authors describe relatively to the conventional interpretation of density matrices in fact vanish. It is noted that nevertheless it is very difficult for us to do without any form of realism, in particular when the quantum measurement problem is considered, and it is stressed that the proper mixture notion comes in precisely at this level. The more general question of the real bearing of Aharonov and Anandan's ideas on the interpretation of quantum mechanics problem is considered.

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In Chap. 2 we solved for the probability amplitudes Ca and C.b explicitly. The results of our discussion, such as the probability of a transition or the value of the induced dipole moment, were invariably expressed in terms of bilinear combinations of the amplitudes, such as CaCa* and CaCi>*. In fact, the expectation value of any observable involves bilinear combinations. Hence an alternative formulation of quantum mechanics consists of dealing with the bilinear quantities directly. The method involves organizing the quantities in a matrix form called the density matrix. There are two principal advantages in doing so. First, the resulting mathematics is often simpler. Sec­ ond, when the wave function for an ensemble of systems is not known but the probabilities for having various different wave functions are known, the en­ semble can be described by a weighted sum of individual density matrices. In particular, the amplitudes cannot themselves describe simply certain com­ mon statistical phenomena, such as the effects of elastic collisions on the in­ duced dipole moments of atoms.

CRC Press eBooks•Mar 5, 2018•0 citations

The Density Matrix Formalism

Bernard d’Espagnat

Along with an elementary description of the well-known density matrix formalism and of its application to the description of quantum-statistical ensembles, this chapter includes the proofs of a few propositions that are especially useful for understanding most of the developments. In the new formulation, ensembles are directly described by density matrices, observables are still described by Hermitean operators, and the rules giving the statistical distribution and the mean values of the predicted measurement results are, respectively, expressions. When stated in this manner, the rules of quantum mechanics apply directly not only to pure states but also to mixtures. This is a distinct advantage. In the case of mixtures defined by their density matrices, the new formulation also has another merit. If two proper mixtures are described by the same density matrix, any state vector representing a subensemble of one of these mixtures can be expressed as a linear combination of the state vectors representing the subensembles of the other mixture.

CRC Press eBooks•Mar 5, 2018•1 citation
Up to now, the initial state of the instrument has been ascribed a state vector. This convention can be criticized, however, either by observing that the instrument is a complicated system which is therefore imperfectly known, or, more adequately still (this is again the difference between proper and improper mixtures), by noting that the instrument has interacted with many other systems before the time when it is used for measuring L , and that consequently it can be associated, not with any definite state vector, but only with a density matrix (in other words, an ensemble of such instruments identically prepared would be an improper mixture). We may wonder whether this remark offers a clue for solving the difficulty encountered at the end of Chapter 14 . There it was shown that, if the ensemble E of instruments is initially a pure case, it is in general impossible to consider that every instrument coordinate has some definite eigenvalue after the interaction with the system has taken place. Let us investigate whether or not this is still the case when ensemble E is a mixture.
Most of the predictions of quantum mechanics are of a statistical nature and therefore make sense only for ensembles. The axiomatics based on the quantum calculus of propositions might open the way toward a general definition of the quantum state of an individual system. It was soon recognized that this leads to separability and thereby to violation of some of the quantum-mechanical predictions. In contemporary literature, the concept of state is not wholly unambiguous. Some authors associate it with the notion of an individual system and say, for instance that a given system is in a given state. Others associate it exclusively with ensembles. The situation is complicated by the fact that for some theorists the concept of state refers only to ensembles that can be described by some state vector. For other authors it refers just as well to ensembles that cannot be associated with any state vector and for which only a density matrix description is therefore acceptable.
Protective measurement, which was proposed as a method of observing the wavefunction of a single system, is extended to the observation of the density matrix of a single system. d'Espagnat's definition of `proper mixture' is shown to be improper because it does not allow for appropriate fluctuations. His claim that there could be different mixtures corresponding to the same density matrix is critically examined. These results provide a new meaning to the density matrix, which gives it the same ontological status as the wavefunction describing a pure state. This also enables quantum entropy to be associated with a single system.
So far we have only considered states in Postulate 25.1(PS) which correspond to a maximal amount of information of the system. These are pure states φ s describable by unit vectors φ → https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6289.tif"/> . Often we may only have a partial knowledge of a system. As an example, consider a less than ideal state preparation process which is unable to prepare the system in a desired pure state φ s . Instead the state preparation process can only determine the system to within a set of possible pure states φ l s https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6290.tif"/> , ℓ = 1, 2,…, namely the system may end up to be in a pure state φ 1 s https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6291.tif"/> , or φ 2 s https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6292.tif"/> and so on. Suppose the state preparation process can also tell us the probabilities w ℓ of the system ending up in these pure states. In other words, we do not know for certain which pure state the system is actually in. We only know that the system has a probability w ℓ to be in pure state φ l s https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6293.tif"/> . The system is then said to be in a classical mixture of states . In more abstract terms, the concept can be stated as A classical mixture of states is a characterisation of a given quantum system in terms of a set of possible pure states φ → l https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203702413/2f242b9b-104e-4a03-b478-d3f6577cf44e/content/eq6294.tif"/> together with a corresponding set of probabilities w ℓ of their occurrence .
Aharonov and Anandan's claim that the notion of ``proper mixture'' is improper is shown to be unjustified. The point is made that if a purely operationalist standpoint is taken the three difficulties these authors describe relatively to the conventional interpretation of density matrices in fact vanish. It is noted that nevertheless it is very difficult for us to do without any form of realism, in particular when the quantum measurement problem is considered, and it is stressed that the proper mixture notion comes in precisely at this level. The more general question of the real bearing of Aharonov and Anandan's ideas on the interpretation of quantum mechanics problem is considered.
In Chap. 2 we solved for the probability amplitudes Ca and C.b explicitly. The results of our discussion, such as the probability of a transition or the value of the induced dipole moment, were invariably expressed in terms of bilinear combinations of the amplitudes, such as CaCa* and CaCi>*. In fact, the expectation value of any observable involves bilinear combinations. Hence an alternative formulation of quantum mechanics consists of dealing with the bilinear quantities directly. The method involves organizing the quantities in a matrix form called the density matrix. There are two principal advantages in doing so. First, the resulting mathematics is often simpler. Sec­ ond, when the wave function for an ensemble of systems is not known but the probabilities for having various different wave functions are known, the en­ semble can be described by a weighted sum of individual density matrices. In particular, the amplitudes cannot themselves describe simply certain com­ mon statistical phenomena, such as the effects of elastic collisions on the in­ duced dipole moments of atoms.
Along with an elementary description of the well-known density matrix formalism and of its application to the description of quantum-statistical ensembles, this chapter includes the proofs of a few propositions that are especially useful for understanding most of the developments. In the new formulation, ensembles are directly described by density matrices, observables are still described by Hermitean operators, and the rules giving the statistical distribution and the mean values of the predicted measurement results are, respectively, expressions. When stated in this manner, the rules of quantum mechanics apply directly not only to pure states but also to mixtures. This is a distinct advantage. In the case of mixtures defined by their density matrices, the new formulation also has another merit. If two proper mixtures are described by the same density matrix, any state vector representing a subensemble of one of these mixtures can be expressed as a linear combination of the state vectors representing the subensembles of the other mixture.