Improving EinsteinPodolskyRosen Steering Inequalities with State Information
Abstract
We discuss the relationship between entropic EinsteinPodolskyRosen (EPR)steering inequalities and their underlying uncertainty relations along with the hypothesis that improved uncertainty relations lead to tighter EPRsteering inequalities. In particular, we discuss how the intrinsic uncertainty in a mixed quantum state is used to improve existing uncertainty relations and how this information affects one’s ability to witness EPRsteering. As an example, we consider the recent improvement (using a quantum memory) to the entropic uncertainty relation between pairs of discrete observables (Nat. Phys. 6, 659 (2010)) and show that a trivial substitution of the tighter bound in the steering inequality leads to contradictions, due in part to the fact that the improved bound depends explicitly on the state being measured. By considering the assumptions that enter into the development of a steering inequality, we derive correct steering inequalities from these improved uncertainty relations and find that they are identical to ones already developed (Phys. Rev. A, 87, 062103 (2013)). In addition, we consider how one can use information about the quantum state to improve our ability to witness EPRsteering, and develop a new continuous variable symmetric EPRsteering inequality as a result.
keywords:
EPR steering, entanglement, EPRparadox, uncertainty relations, entropy1 Introduction
Uncertainty relations are used not only to great effect in expressing fundamental limitations of precision measurements; they are also useful in witnessing entanglement through demonstrations of the EPR paradox (1) by the violation of EPRsteering inequalities
EPRsteering is a form of nonlocality intermediate between Bellnonlocality and nonseparability (2). A joint quantum system is said to exhibit EPRsteering (or be EPRsteerable) if its local measurement correlations are sufficiently strong to demonstrate the EPRparadox (1). As a consequence of EPRsteering, consider two parties, Alice and Bob, sharing quantum systems A and B, respectively. Bob can determine that he and Alice share entanglement even when he does not trust Alice’s measurements provided A and B are sufficiently entangled. Bob does this by ruling out the possibility that Alice is preparing and sending systems to Bob, and then using her knowledge of those systems to announce fabricated ”measurements” she expects to be correlated to Bob’s results. In this scenario, the measurement correlations across complementary observables (say, in both position and momentum, or in linear and circular polarizations of light) can only be so high. These models, in which Bob is receiving an unknown, but welldefined quantum state classically correlated to Alice’s results are known as models of local hidden states (LHS) for Bob. When the measurement correlations across complementary observables is sufficiently high, Bob can rule out all LHS models and verify that he and Alice must be sharing entanglement.
Ruling out LHS models for Bob is done by violating EPRsteering inequalities, i.e., inequalities derived from the necessary form that the joint measurement probabilities must have (11) in an LHS model (for Bob). Steering inequalities are useful not only because they witness entanglement without needing to perform complete state tomography; they also verify entanglement between two parties even when the measurements of one party are untrusted (2). For this reason, steering inequalities have been shown to be useful in entanglementbased quantum key distribution (4).
In some cases, improvements to uncertainty relations lead to better EPRsteering inequalities. For example, BiałynickiBirula and Mycielski’s entropic uncertainty relation (5) for position and momentum encompasses the variancebased Heisenberg uncertainty relation (6). Similarly, the resulting entropic EPRsteering inequality (7) encompasses the variancebased steering inequality (8), permitting EPRsteering to be witnessed in more diverse systems. In spite of this particular example, however, improving uncertainty relations does not necessarily improve steering inequalities, as we shall show.
Previously (9), we showed how a stateindependent entropic uncertainty relation relating a pair of dimensional discrete observables, say, and , gives rise to a formulation of a corresponding EPRsteering inequality between a pair of systems and . In particular, given the uncertainty relation
(1)  
(2) 
there is a corresponding EPRsteering inequality,
(3) 
where is as defined in equation (2), but for observables on system . Here, is the Shannon entropy of the measurement probabilities of observable , i.e.,
(4) 
where . Similarly, is the Shannon entropy of the joint measurement probabilities of observables and , i.e.,
(5) 
where . In addition, is the conditional Shannon entropy, where , and all logarithms are taken to be base 2.
Examination of (1) and (3) suggests that entropic EPRsteering inequalities may be obtained from entropic uncertainty relations by a trivial substitution of conditional entropies for marginal entropies. Indeed, as we shall show below, when the uncertainty bound is stateindependent, this strategy is appropriate
Recently, Berta et. al (10) developed an improved entropic uncertainty relation which raises the bound on the right hand side of (2) when the von Neumann entropy of Bob’s system described by density operator is known,
(6) 
This improved uncertainty relation is a consequence of Berta et. al.’s uncertainty principle in the presence of quantum memory (10)
This statedependent improved uncertainty relation (6) cannot be adapted into an EPRsteering inequality by the substitution of conditional entropies for marginal ones, as doing so would lead to a contradiction. That is,
(7) 
If and were mutually unbiased observables, such that , and the subsystems and were maximally mixed, so that , we would find that the substitution leads to the following inequality,
(8) 
which is an inequality that separable states can violate. As an example, consider the maximally correlated mixed twoqubit state, i.e., the separable state obtained from an even mixture of the separable joint spinz states and ;
(9) 
In this system, the alleged inequality (8) has the form
(10) 
because bit. Measurement in the Pauli basis, which is the same as the eigenbasis, gives , and . Since the measurement result of is completely correlated with the result of , the conditional entropy, is zero bits. Measurement in the Pauli basis, which is mutually unbiased with respect to the basis, results in a uniform distribution for the joint measurement probabilities, and gives a conditional entropy, , of bit. Since the total on the left hand side of (10) is one bit less than the bound of 2 bits, we would conclude that this classically correlated separable state is not only entangled, but EPRsteerable. This is a contradiction. To resolve this contradiction, we must examine the assumption of an LHS model that goes into the derivation of entropic EPRsteering inequalities.
2 The LHS model assumption with the improved uncertainty bound
Given a pair of quantum systems and , we say that the pair admits an LHS model for if has a welldefined quantum state only classically correlated with . Such a system can be considered to be “EPRlocal”, and admits the possibility that Alice is preparing and sending systems to Bob and using her knowledge of those systems to announce “measurements” correlated to what she believes Bob’s outcomes will be. As such, being able to rule out such an LHS model successfully witnesses entanglement between Alice and Bob even when Alice’s results are untrusted (2).
In (9), as well as in (7), the assumption of an LHS model for is enforced by requiring the joint measurement probabilities to take the following form,
(11) 
Though this form bears striking resemblance to local hidden variable models (3), there is the additional assumption that Bob’s measurements arise from a quantum probability distribution (denoted by subscript ), where , and is only dependent on the details of the hidden parameter (governing the possible state prepared by Alice). No such assumption is imposed on Alice’s measurements. In this situation, we assume both that Bob’s measurements are constrained by quantum uncertainty relations, and that his measurement outcomes are conditionally independent of Alice’s results. With these assumptions, we are led to the LHS criterion (7); (9),
(12) 
In (9), the derivation of the entropic EPRsteering inequalities is finished by substituting Maassen and Uffink’s bound (2) into the right hand side of (12), giving us the steering inequality (3).
To develop an improved EPRsteering inequality, with the improved entropic uncertainty relation (6), we argue that for each value of the hidden variable(s) governing the preparation of Bob’s system, the improved uncertainty relation holds,
(13) 
giving us the inequality,
(14) 
for each LHS model given by and . As it stands, (14) is an unsatisfactory steering inequality since the righthand side retains an explicit dependence on . Instead, we desire an inequality that does not depend on , and which, when violated, rules out all possible LHS models for Bob. In other words, we need to determine a minimal constant ,
(15) 
which, with , gives the smallest possible sum of conditional entropies that an LHS model for Bob can have,
(16) 
When violated, (16) successfully rules out all LHS models for Bob, demonstrating EPRsteering.
In the following arguments, we show that must be zero. From there, we see that this particular statedependent improvement to the uncertainty relation (6) has no effect on the associated steering inequality (3).
Consider that the sum being minimized in is a weighted sum of von Neumann entropies, , of the states Bob is receiving from Alice. These entropies, like all von Neumann entropes must take values between zero and . Since Alice is free to send any distribution of states to Bob, the weighted sum of entropies can also take any value between zero and , the lower limit being when Alice is sending to Bob a distribution of pure states (with zero von Neumann entropies). Thus in order to have a bound which when violated, rules out all possible LHS models for Bob, must be zero. Knowing this, remains the lower bound for witnessing EPRsteering through (3), even when the state can be determined through the use of a quantum memory.
3 Using state information to improve steering inequalities
Though the previous statedependent improved entropic uncertainty relation (6) did not yield an improved EPRsteering inequality, it is straightforward to show that one can use information about the state of a quantum system to improve one’s ability to witness EPRsteering. To explore this, we note that uncertainty relations can be defined as any physically imposed constraint on measurement probability distributions. Most uncertainty relations are lower bounds on measurement uncertainties, but it is also possible to bound measurement uncertainties from above (11). As explored in (9); (12), upper bounds on measurement uncertainties are used to develop symmetric steering inequalities
(17) 
and for continuous observables as:
(18) 
Note that for continuous observables, the entropies , , and are differential entropies (13), where
(19) 
and is the probability density of continuous random variable .
In ((9)), we used the fact that the discrete entropy of an dimensional system is no larger than to develop symmetric EPRsteering inequalities using the discrete mutual information. From the conditional steering inequality (3), we developed the symmetric steering inequality,
(20) 
For continuous observables, however, there is no known stateindependent upper limit to the entropy. We can attempt to derive a symmetric EPRsteering inequality in the same fashion for continuous variables bu subtracting Walborn et. al’s (7) conditonal entropic steering inequality,
(21) 
from the sum of marginal entropies , but since this sum of marginal entropies is unbounded for continuous variables, the resulting sum of mutual informations, , is also unbounded. However, by using additional information about the state of the system, we can form an upper bound.
To find an upper bound for the sum of mutual informations, we use the fact that knowledge of measurement statistics allows one to further constrain the measurement probability distributions. In particular, we can bound from above the differential entropy if we know the variance , (5); (13), so that
(22) 
giving us the relation,
(23) 
Subtracting this inequality from (21) and symmetrizing gives us the inequality
(24) 
which we make symmetric by taking the largest bound between Alice and Bob’s measurements.
Incidentally, this leads directly to an experimentally tenable symmetric steering inequality using discrete approximations to the continuous mutual informations similar to the one in ((12)) by noting that the mutual information between the discrete approximations of two continuous variables, (), is never more than the mutual information between the continuous variables themselves () (14).
(25) 
4 Conclusion
We have shown that even substantially improved uncertainty relations do not necessarily lead to improved EPRsteering inequalities when these improvements are statedependent
We gratefully acknowledge support from DARPA DSO under grant numbers W911NR1010404 and W31P4Q1210015. CJB acknowledges support from ARO W911NF0910385 and NSF PHY1203931.
Footnotes
 journal: Physics Letters A
 EPRsteering inequalities are relations illustrating that, if the effect of measurement indeed cannot travel faster than light, then the measurement uncertainties of one party, whether or not they are conditioned on the outcomes of another party, have the same lower bound.
 This point was made in a previous publication in which only stateindependent uncertainty relations were considered (9).
 The improved uncertainty relation (6) has the appealing intuition that if the minimum uncertainty limit when measuring a pure state is given by , then the minimum uncertainty limit when measuring a mixture of pure states is larger by the intrinsic uncertainty of the mixture.
 Symmetric steering inequalities are steering inequalities that are symmetric between parties. As such, the violation of a symmetric steering inequality rules out models of local hidden states for both Alice and Bob, allowing both of them to verify entanglement even when neither of them trusts each other’s measurements (though they trust their own).
 We note that there are stateindependent improvements to Maassen and Uffink’s uncertainty relation when the observables are not fully unbiased, but that Maassen and Uffink’s relation remains tight for mutually unbiased observables (15); (16); (17); (18).
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