Here we report a type of dynamic effect that is at the core of the so called "counterfactual computation" and especially "counterfactual communication" quantum effects that have generated a lot of interest recently. The basic feature of these counterfactual setups is the fact that particles seem to be affected by actions that take place in locations where they never (more precisely, only with infinitesimally small probability) enter. Specifically, the communication/computation takes place without the quantum particles that are supposed to be the information carriers travelling through the communication channel or entering the logic gates of the computer. Here we show that something far more subtle is taking place: It is not necessary for the particle to enter the region where the controlling action takes place; it is enough for the controlled property of the particle, (i.e., the property that is being controlled by actions in the control region), to enter that region. The presence of the controlled property, without the particle itself, is possible via a quantum Cheshire Cat type effect in which a property can be disembodied from the particle that possesses it. At the same time, we generalize the quantum Cheshire Cat effect to dynamical settings, in which the property that is "disembodied" from the particle possessing it propagates in space, and leads to a flux of "disembodied" conserved quantities.
Here we report a type of dynamic effect that is at the core of the so called "counterfactual computation" and especially "counterfactual communication" quantum effects that have generated a lot of interest recently. The basic feature of these counterfactual setups is the fact that particles seem to be affected by actions that take place in locations where they never (more precisely, only with infinitesimally small probability) enter. Specifically, the communication/computation takes place without the quantum particles that are supposed to be the information carriers travelling through the communication channel or entering the logic gates of the computer. Here we show that something far more subtle is taking place: It is not necessary for the particle to enter the region where the controlling action takes place; it is enough for the controlled property of the particle, (i.e., the property that is being controlled by actions in the control region), to enter that region. The presence of the controlled property, without the particle itself, is possible via a quantum Cheshire Cat type effect in which a property can be disembodied from the particle that possesses it. At the same time, we generalize the quantum Cheshire Cat effect to dynamical settings, in which the property that is "disembodied" from the particle possessing it propagates in space, and leads to a flux of "disembodied" conserved quantities.
Abstract We explore how one might detect the dynamical quantum Cheshire cat proposed by Aharonov et al We show that, in practice, we need to bias the initial state by adding/subtracting a small probability amplitude (‘field’) of the orthogonal state, which travels with the disembodied property, to make the effect detectable (i.e. if our initial state is | ↑ z ⟩ , we need to bias this with some small amount δ of state | ↓ z ⟩ ). This biasing, which can be done either directly or via weakly entangling the state with a pointer, effectively provides a phase reference with which we can measure the evolution of the state. The outcome can then be measured as a small probability difference in detections in a mutually unbiased basis, proportional to this biasing δ. We show this is different from counterfactual communication, which provably does not require any probe field to travel between sender Bob and receiver Alice for communication. We further suggest an optical polarisation experiment where these phenomena might be demonstrated in a laboratory.
We explore how one might detect the dynamical quantum Cheshire cat proposed by Aharonov et al. We show that, in practice, we need to bias the initial state by adding/subtracting a small probability amplitude ('field') of the orthogonal state, which travels with the disembodied property, to make the effect detectable (i.e. if our initial state is |↑z〉, we need to bias this with some small amount δ of state |↓z〉). This biasing, which can be done either directly or via weakly entangling the state with a pointer, effectively provides a phase reference with which we can measure the evolution of the state. The outcome can then be measured as a small probability difference in detections in a mutually unbiased basis, proportional to this biasing δ. We show this is different from counterfactual communication, which provably does not require any probe field to travel between sender Bob and receiver Alice for communication. We further suggest an optical polarisation experiment where these phenomena might be demonstrated in a laboratory.
Abstract We analyse the quantum Cheshire cat using contextuality theory, to see if this can tell us anything about how best to interpret this paradox. We show that this scenario can be analysed using the relation between three different measurements, which seem to result in a logical contradiction. We discuss how this contextual behaviour links to weak values, and coherences between prohibited states. Rather than showing a property of the particle is disembodied, the quantum Cheshire cat instead demonstrates the effects of these coherences, which are typically found in pre- and post-selected systems.
Many counterfactual predictions are made by quantum theory, such as quantum tunneling and violations of Bell’s inequalities. Experimental verifications of these predictions demonstrate that quantum theory is reliable for the microscopic world. Despite its widespread application, consistent theoretical interpretations of quantum theory remain a challenge. Recently, Aharonov et al. proposed several new and intriguing counterfactuals based on quantum weak measurement and interaction-free measurement, such as the quantum violation of the pigeonhole principle and the departure of physical properties from particles, also known as the quantum Cheshire cat effect. These counterfactuals garnered considerable interest. Although no common consensus has been reached, many pioneering experiments have already been conducted in light of these theoretical proposals. Furthermore, these counterfactuals and the key concepts underlying them, weak measurement and interaction-free measurement, open up a whole new way of thinking about and understanding the strange quantum theory. Herein, our aim is to provide a unified perspective on these counterfactuals. The theoretical ideas, particularly the fundamental quantum concepts underlying these counterfactuals, are the focus of our attention. First, we present concise and insightful introductions to weak measurement and interaction-free measurement, which are the two key fundamental constructions for discussing all of the following quantum counterfactuals. Next, we discuss the quantum violation of the pigeonhole principle in depth, explicitly demonstrating that the key idea leading to the violation is destructive quantum interference between the possible paths of two particles traveling along the same path. Then, two key proposals of the quantum Cheshire cat effect are examined based on weak values of certain physical properties. Both proposals are built around interaction-free measurement, and the departure of physical properties from their bodies is realized based on the quantum Zeno effect. After introducing the weak measurement and weak value, the non-locality in the quantum Cheshire cat effect can be dismissed, and the physical properties leave the body continuously with infinitesimal quantum amplitudes. Meanwhile, during the departure, the total property in the entire space remains invariant. Finally, we present our conclusion on quantum counterfactuals, arguing that when coherent processes are endowed with concrete physical properties, counterfactuals are unavoidable. Throughout our discussions, we try to elaborate on the key roles played by the quantum concepts, quantum amplitudes, and quantum coherence in these counterfactuals. The idea behind weak measurement and weak value is that information about a coherent process can be obtained with sufficiently weak coupling. In other words, a quantum coherent process becomes observable with a weak measurement and even acquires a specific property quantified by a weak value. When compared to our conventional understanding of quantum coherent processes, this is a mind-boggling viewpoint. The idea behind interaction-free measurement is that weak amplitudes can cause large system evolution even if they cannot transport the body of the system, which is also astonishing! This demonstrates the enormous power of infinitesimal quantum amplitudes in quantum communication and computation. Therefore, all quantum counterfactuals provide new perspectives to further investigate these fundamental quantum concepts.
Abstract One of the common conceptions of nature, typically derived from the experiences with classical systems, is that attributes of the matter coexist with the substance. In the quantum regime, however, the quantum particle itself and its physical property may be in spatial separation, known as the quantum Cheshire cat effect. While there have been several reports to date on the observation of the quantum Cheshire cat effect, all such experiments are based on first-order interferometry and destructive projection measurement, thus allowing simple interpretation due to measurement-induced disturbance and also subject to trivial interpretation based on classical waves. In this work, we report an experimental observation of the quantum Cheshire cat effect with noninvasive weak quantum measurement as originally proposed. The use of the weak-measurement probe has allowed us to identify the location of the single photon and that of the disembodied polarization state in a quantum interferometer. The weak-measurement probe based on two-photon interference makes our observation unable to be explained by classical physics. We furthermore elucidate the quantum Cheshire cat effect as quantum interference of the transition amplitudes for the photon and the polarization state which are directly obtained from the measurement outcomes or the weak values. Our work not only reveals the true quantum nature of Cheshire cat effect but also sheds light on a comprehensive understanding for the counter-intuitive quantum phenomena.
Even the subtle and apparently strange quantum effects can sometimes survive otherwise lethal influence of an omnipresent decoherence. We show that an archetypal quantum Cheshire Cat, a paradox of a separation between a position of a quantum particle, a photon, and its internal property, the polarization, in a two-path Mach–Zehnder setting, is robust to decoherence caused by a bosonic infinite bath locally coupled to the polarization of a photon. Decoherence affects either the cat or its grin depending on which of the two paths is noisy. For a pure decoherence, in an absence of photon–environment energy exchange, we provide exact results for weak values of the photon position and polarization indicating that the information loss affects the quantum Cheshire Cat only qualitatively and the paradox survives. We show that it is also the case beyond the pure decoherence for a small rate of dissipation.