De Broglie–Bohm theory
The de Broglie–Bohm theory, also known as the pilot wave theory, Bohmian mechanics, Bohm's interpretation, and the causal interpretation, is an interpretation of quantum mechanics. In addition to a wavefunction on the space of all possible configurations, it also postulates an actual configuration that exists even when unobserved. The evolution over time of the configuration (that is, the positions of all particles or the configuration of all fields) is defined by the wave function by a guiding equation. The evolution of the wave function over time is given by the Schrödinger equation. The theory is named after Louis de Broglie (1892–1987) and David Bohm (1917–1992).
The theory is deterministic^{[1]} and explicitly nonlocal: the velocity of any one particle depends on the value of the guiding equation, which depends on the configuration of the system given by its wavefunction; the latter depends on the boundary conditions of the system, which, in principle, may be the entire universe.
The theory results in a measurement formalism, analogous to thermodynamics for classical mechanics, that yields the standard quantum formalism generally associated with the Copenhagen interpretation. The theory's explicit nonlocality resolves the "measurement problem", which is conventionally delegated to the topic of interpretations of quantum mechanics in the Copenhagen interpretation. The Born rule in Broglie–Bohm theory is not a basic law. Rather, in this theory, the link between the probability density and the wave function has the status of a hypothesis, called the quantum equilibrium hypothesis, which is additional to the basic principles governing the wave function.
The theory was historically developed in the 1920s by de Broglie, who, in 1927, was persuaded to abandon it in favour of the thenmainstream Copenhagen interpretation. David Bohm, dissatisfied with the prevailing orthodoxy, rediscovered de Broglie's pilotwave theory in 1952. Bohm's suggestions were not then widely received, partly due to reasons unrelated to their content, but instead were connected to Bohm's youthful communist affiliations.^{[2]} De Broglie–Bohm theory was widely deemed unacceptable by mainstream theorists, mostly because of its explicit nonlocality. Bell's theorem (1964) was inspired by Bell's discovery of the work of David Bohm and his subsequent wondering whether the obvious nonlocality of the theory could be eliminated. Since the 1990s, there has been renewed interest in formulating extensions to de Broglie–Bohm theory, attempting to reconcile it with special relativity and quantum field theory, besides other features such as spin or curved spatial geometries.^{[3]}
The Stanford Encyclopedia of Philosophy article on Quantum decoherence (Guido Bacciagaluppi, 2012) groups "approaches to quantum mechanics" into five groups, of which "pilotwave theories" are one (the others being the Copenhagen interpretation, objective collapse theories, manyworld interpretations and modal interpretations).
There are several equivalent mathematical formulations of the theory, and it is known by a number of different names. The de Broglie wave has a macroscopic analogy termed Faraday wave.^{[4]}
Overview
De Broglie–Bohm theory is based on the following postulates:
 There is a configuration of the universe, described by coordinates , which is an element of the configuration space . The configuration space is different for different versions of pilotwave theory. For example, this may be the space of positions of particles, or, in case of field theory, the space of field configurations . The configuration evolves (for spin=0) according to the guiding equation
 where
is the probability current or probability flux, and
is the momentum operator. Here,
is the standard complexvalued wavefunction known from quantum theory, which evolves according to Schrödinger's equation
 This already completes the specification of the theory for any quantum theory with Hamilton operator of type .
 The configuration is distributed according to at some moment of time , and this consequently holds for all times. Such a state is named quantum equilibrium. With quantum equilibrium, this theory agrees with the results of standard quantum mechanics.
Notably, even though this latter relation is frequently presented as an axiom of the theory, in Bohm's original papers of 1952 it was presented as derivable from statisticalmechanical arguments. This argument was further supported by the work of Bohm in 1953 and was substantiated by Vigier and Bohm's paper of 1954, in which they introduced stochastic fluid fluctuations that drive a process of asymptotic relaxation from quantum nonequilibrium to quantum equilibrium (ρ → ψ^{2}).^{[5]}
Doubleslit experiment
The doubleslit experiment is an illustration of waveparticle duality. In it, a beam of particles (such as electrons) travels through a barrier that has two slits. If one puts a detector screen on the side beyond the barrier, the pattern of detected particles shows interference fringes characteristic of waves arriving at the screen from two sources (the two slits); however, the interference pattern is made up of individual dots corresponding to particles that had arrived on the screen. The system seems to exhibit the behaviour of both waves (interference patterns) and particles (dots on the screen).
If we modify this experiment so that one slit is closed, no interference pattern is observed. Thus, the state of both slits affects the final results. We can also arrange to have a minimally invasive detector at one of the slits to detect which slit the particle went through. When we do that, the interference pattern disappears.
The Copenhagen interpretation states that the particles are not localised in space until they are detected, so that, if there is no detector on the slits, there is no information about which slit the particle has passed through. If one slit has a detector on it, then the wavefunction collapses due to that detection.
In de Broglie–Bohm theory, the wavefunction is defined at both slits, but each particle has a welldefined trajectory that passes through exactly one of the slits. The final position of the particle on the detector screen and the slit through which the particle passes is determined by the initial position of the particle. Such initial position is not knowable or controllable by the experimenter, so there is an appearance of randomness in the pattern of detection. In Bohm's 1952 papers he used the wavefunction to construct a quantum potential that, when included in Newton's equations, gave the trajectories of the particles streaming through the two slits. In effect the wavefunction interferes with itself and guides the particles by the quantum potential in such a way that the particles avoid the regions in which the interference is destructive and are attracted to the regions in which the interference is constructive, resulting in the interference pattern on the detector screen.
To explain the behavior when the particle is detected to go through one slit, one needs to appreciate the role of the conditional wavefunction and how it results in the collapse of the wavefunction; this is explained below. The basic idea is that the environment registering the detection effectively separates the two wave packets in configuration space.
An experiment has been conducted in 2016 which demonstrates the potential validity of the deBroglieBohm theory via use of silicone oil droplets. In this experiment a drop of silicone oil is placed into a vibrating fluid bath, it then bounces across the bath propelled by waves produced by its own collisions, mimicking an electrons’ statistical behavior with remarkable accuracy.^{[7]}^{[8]}
The theory
The ontology
The ontology of de Broglie–Bohm theory consists of a configuration of the universe and a pilot wave . The configuration space can be chosen differently, as in classical mechanics and standard quantum mechanics.
Thus, the ontology of pilotwave theory contains as the trajectory we know from classical mechanics, as the wavefunction of quantum theory. So, at every moment of time there exists not only a wavefunction, but also a welldefined configuration of the whole universe (i.e., the system as defined by the boundary conditions used in solving the Schrödinger equation). The correspondence to our experiences is made by the identification of the configuration of our brain with some part of the configuration of the whole universe , as in classical mechanics.
While the ontology of classical mechanics is part of the ontology of de Broglie–Bohm theory, the dynamics are very different. In classical mechanics, the accelerations of the particles are imparted directly by forces, which exist in physical threedimensional space. In de Broglie–Bohm theory, the velocities of the particles are given by the wavefunction, which exists in a 3Ndimensional configuration space, where N corresponds to the number of particles in the system;^{[9]} Bohm hypothesized that each particle has a "complex and subtle inner structure" that provides the capacity to react to the information provided by the wavefunction by the quantum potential.^{[10]} Also, unlike in classical mechanics, physical properties (e.g., mass, charge) are spread out over the wavefunction in de Broglie–Bohm theory, not localized at the position of the particle.^{[11]}^{[12]}
The wavefunction itself, and not the particles, determines the dynamical evolution of the system: the particles do not act back onto the wave function. As Bohm and Hiley worded it, "the Schrödinger equation for the quantum field does not have sources, nor does it have any other way by which the field could be directly affected by the condition of the particles [...] the quantum theory can be understood completely in terms of the assumption that the quantum field has no sources or other forms of dependence on the particles".^{[13]} P. Holland considers this lack of reciprocal action of particles and wave function to be one "[a]mong the many nonclassical properties exhibited by this theory".^{[14]} It should be noted, however, that Holland has later called this a merely apparent lack of back reaction, due to the incompleteness of the description.^{[15]}
In what follows below, we will give the setup for one particle moving in followed by the setup for N particles moving in 3 dimensions. In the first instance, configuration space and real space are the same, while in the second, real space is still , but configuration space becomes . While the particle positions themselves are in real space, the velocity field and wavefunction are on configuration space, which is how particles are entangled with each other in this theory.
Extensions to this theory include spin and more complicated configuration spaces.
We use variations of for particle positions, while represents the complexvalued wavefunction on configuration space.
Guiding equation
For a spinless single particle moving in , the particle's velocity is given by
For many particles, we label them as for the th particle, and their velocities are given by
The main fact to notice is that this velocity field depends on the actual positions of all of the particles in the universe. As explained below, in most experimental situations, the influence of all of those particles can be encapsulated into an effective wavefunction for a subsystem of the universe.
Schrödinger's equation
The oneparticle Schrödinger equation governs the time evolution of a complexvalued wavefunction on . The equation represents a quantized version of the total energy of a classical system evolving under a realvalued potential function on :
For many particles, the equation is the same except that and are now on configuration space, :
This is the same wavefunction as in conventional quantum mechanics.
Relation to the Born rule
In Bohm's original papers [Bohm 1952], he discusses how de Broglie–Bohm theory results in the usual measurement results of quantum mechanics. The main idea is that this is true if the positions of the particles satisfy the statistical distribution given by . And that distribution is guaranteed to be true for all time by the guiding equation if the initial distribution of the particles satisfies .
For a given experiment, we can postulate this as being true and verify experimentally that it does indeed hold true, as it does. But, as argued in Dürr et al.,^{[16]} one needs to argue that this distribution for subsystems is typical. They argue that by virtue of its equivariance under the dynamical evolution of the system, is the appropriate measure of typicality for initial conditions of the positions of the particles. They then prove that the vast majority of possible initial configurations will give rise to statistics obeying the Born rule (i.e., ) for measurement outcomes. In summary, in a universe governed by the de Broglie–Bohm dynamics, Born rule behavior is typical.
The situation is thus analogous to the situation in classical statistical physics. A lowentropy initial condition will, with overwhelmingly high probability, evolve into a higherentropy state: behavior consistent with the second law of thermodynamics is typical. There are, of course, anomalous initial conditions that would give rise to violations of the second law. However, in the absence of some very detailed evidence supporting the actual realization of one of those special initial conditions, it would be quite unreasonable to expect anything but the actually observed uniform increase of entropy. Similarly, in the de Broglie–Bohm theory, there are anomalous initial conditions that would produce measurement statistics in violation of the Born rule (i.e., in conflict with the predictions of standard quantum theory). But the typicality theorem shows that, in the absence of some specific reason to believe that one of those special initial conditions was in fact realized, the Born rule behavior is what one should expect.
It is in that qualified sense that the Born rule is, for the de Broglie–Bohm theory, a theorem rather than (as in ordinary quantum theory) an additional postulate.
It can also be shown that a distribution of particles that is not distributed according to the Born rule (that is, a distribution "out of quantum equilibrium") and evolving under the de Broglie–Bohm dynamics is overwhelmingly likely to evolve dynamically into a state distributed as .^{[17]}
The conditional wavefunction of a subsystem
In the formulation of the de Broglie–Bohm theory, there is only a wavefunction for the entire universe (which always evolves by the Schrödinger equation). It should, however, be noted that the "universe" is simply the system limited by the same boundary conditions used to solve the Schrödinger equation. However, once the theory is formulated, it is convenient to introduce a notion of wavefunction also for subsystems of the universe. Let us write the wavefunction of the universe as , where denotes the configuration variables associated to some subsystem (I) of the universe, and denotes the remaining configuration variables. Denote respectively by and the actual configuration of subsystem (I) and of the rest of the universe. For simplicity, we consider here only the spinless case. The conditional wavefunction of subsystem (I) is defined by
It follows immediately from the fact that satisfies the guiding equation that also the configuration satisfies a guiding equation identical to the one presented in the formulation of the theory, with the universal wavefunction replaced with the conditional wavefunction . Also, the fact that is random with probability density given by the square modulus of implies that the conditional probability density of given is given by the square modulus of the (normalized) conditional wavefunction (in the terminology of Dürr et al.^{[18]} this fact is called the fundamental conditional probability formula).
Unlike the universal wavefunction, the conditional wavefunction of a subsystem does not always evolve by the Schrödinger equation, but in many situations it does. For instance, if the universal wavefunction factors as
then the conditional wavefunction of subsystem (I) is (up to an irrelevant scalar factor) equal to (this is what standard quantum theory would regard as the wavefunction of subsystem (I)). If, in addition, the Hamiltonian does not contain an interaction term between subsystems (I) and (II), then does satisfy a Schrödinger equation. More generally, assume that the universal wave function can be written in the form
where solves Schrödinger equation and, for all and . Then, again, the conditional wavefunction of subsystem (I) is (up to an irrelevant scalar factor) equal to , and if the Hamiltonian does not contain an interaction term between subsystems (I) and (II), then satisfies a Schrödinger equation.
The fact that the conditional wavefunction of a subsystem does not always evolve by the Schrödinger equation is related to the fact that the usual collapse rule of standard quantum theory emerges from the Bohmian formalism when one considers conditional wavefunctions of subsystems.
Extensions
Relativity
Pilotwave theory is explicitly nonlocal, which is in ostensible conflict with special relativity. Various extensions of "Bohmlike" mechanics exist that attempt to resolve this problem. Bohm himself in 1953 presented an extension of the theory satisfying the Dirac equation for a single particle. However, this was not extensible to the manyparticle case because it used an absolute time.^{[19]}
A renewed interest in constructing Lorentzinvariant extensions of Bohmian theory arose in the 1990s; see Bohm and Hiley: The Undivided Universe, and,^{[20]}^{[21]} and references therein. Another approach is given in the work of Dürr et al.,^{[22]} in which they use Bohm–Dirac models and a Lorentzinvariant foliation of spacetime.
Thus, Dürr et al. (1999) showed that it is possible to formally restore Lorentz invariance for the Bohm–Dirac theory by introducing additional structure. This approach still requires a foliation of spacetime. While this is in conflict with the standard interpretation of relativity, the preferred foliation, if unobservable, does not lead to any empirical conflicts with relativity. In 2013, Dürr et al. suggested that the required foliation could be covariantly determined by the wavefunction.^{[23]}
The relation between nonlocality and preferred foliation can be better understood as follows. In de Broglie–Bohm theory, nonlocality manifests as the fact that the velocity and acceleration of one particle depends on the instantaneous positions of all other particles. On the other hand, in the theory of relativity the concept of instantaneousness does not have an invariant meaning. Thus, to define particle trajectories, one needs an additional rule that defines which spacetime points should be considered instantaneous. The simplest way to achieve this is to introduce a preferred foliation of spacetime by hand, such that each hypersurface of the foliation defines a hypersurface of equal time.
Initially, it had been considered impossible to set out a description of photon trajectories in the de Broglie–Bohm theory in view of the difficulties of describing bosons relativistically.^{[24]} In 1996, Partha Ghose had presented a relativistic quantummechanical description of spin0 and spin1 bosons starting from the Duffin–Kemmer–Petiau equation, setting out Bohmian trajectories for massive bosons and for massless bosons (and therefore photons).^{[24]} In 2001, JeanPierre Vigier emphasized the importance of deriving a welldefined description of light in terms of particle trajectories in the framework of either the Bohmian mechanics or the Nelson stochastic mechanics.^{[25]} The same year, Ghose worked out Bohmian photon trajectories for specific cases.^{[26]} Subsequent weakmeasurement experiments yielded trajectories that coincide with the predicted trajectories.^{[27]}^{[28]}
Chris Dewdney and G. Horton have proposed a relativistically covariant, wavefunctional formulation of Bohm's quantum field theory^{[29]}^{[30]} and have extended it to a form that allows the inclusion of gravity.^{[31]}
Nikolić has proposed a Lorentzcovariant formulation of the Bohmian interpretation of manyparticle wavefunctions.^{[32]} He has developed a generalized relativisticinvariant probabilistic interpretation of quantum theory,^{[33]}^{[34]}^{[35]} in which is no longer a probability density in space, but a probability density in spacetime. He uses this generalized probabilistic interpretation to formulate a relativisticcovariant version of de Broglie–Bohm theory without introducing a preferred foliation of spacetime. His work also covers the extension of the Bohmian interpretation to a quantization of fields and strings.^{[36]}
Roderick I. Sutherland at the University in Sydney has a Lagrangian formalism for the pilot wave and its beables. It draws on Yakir Aharonov's retrocasual weak measurements to explain manyparticle entanglement in a special relativistic way without the need for configuration space. The basic idea was already published by Costa de Beauregard in the 1950s and is also used by John Cramer in his transactional interpretation except the beables that exist between the von Neumann strong projection operator measurements. Sutherland's Lagrangian includes twoway actionreaction between pilot wave and beables. Therefore, it is a postquantum nonstatistical theory with final boundary conditions that violate the nosignal theorems of quantum theory. Just as special relativity is a limiting case of general relativity when the spacetime curvature vanishes, so, too is statistical noentanglement signaling quantum theory with the Born rule a limiting case of the postquantum actionreaction Lagrangian when the reaction is set to zero and the final boundary condition is integrated out.^{[37]}
Spin
To incorporate spin, the wavefunction becomes complexvectorvalued. The value space is called spin space; for a spin½ particle, spin space can be taken to be . The guiding equation is modified by taking inner products in spin space to reduce the complex vectors to complex numbers. The Schrödinger equation is modified by adding a Pauli spin term:
where
 — the mass, charge and magnetic moment of the –th particle
 — the appropriate spin operator acting in the –th particle's spin space
 — spin quantum number of the –th particle ( for electron)
 is vector potential in
 is the magnetic field in
 is the covariant derivative, involving the vector potential, ascribed to the coordinates of –th particle (in SI units)

— the wavefunction defined on the multidimensional configuration space; e.g. a system consisting of two spin1/2 particles and one spin1 particle has a wavefunction of the form
 where is a tensor product, so this spin space is 12dimensional
 is the inner product in spin space :
Quantum field theory
In Dürr et al.,^{[38]}^{[39]} the authors describe an extension of de Broglie–Bohm theory for handling creation and annihilation operators, which they refer to as "Belltype quantum field theories". The basic idea is that configuration space becomes the (disjoint) space of all possible configurations of any number of particles. For part of the time, the system evolves deterministically under the guiding equation with a fixed number of particles. But under a stochastic process, particles may be created and annihilated. The distribution of creation events is dictated by the wavefunction. The wavefunction itself is evolving at all times over the full multiparticle configuration space.
Hrvoje Nikolić^{[33]} introduces a purely deterministic de Broglie–Bohm theory of particle creation and destruction, according to which particle trajectories are continuous, but particle detectors behave as if particles have been created or destroyed even when a true creation or destruction of particles does not take place.
Curved space
To extend de Broglie–Bohm theory to curved space (Riemannian manifolds in mathematical parlance), one simply notes that all of the elements of these equations make sense, such as gradients and Laplacians. Thus, we use equations that have the same form as above. Topological and boundary conditions may apply in supplementing the evolution of Schrödinger's equation.
For a de Broglie–Bohm theory on curved space with spin, the spin space becomes a vector bundle over configuration space, and the potential in Schrödinger's equation becomes a local selfadjoint operator acting on that space.^{[40]}
Exploiting nonlocality
The causal interpretation of quantum mechanics set up by de Broglie and Bohm was extended later by Bohm, Vigier, Hiley, Valentini and others to include stochastic properties. Bohm and other physicists, including Valentini, view the Born rule linking to the probability density function as representing not a basic law, but rather as constituting a result of a system having reached quantum equilibrium during the course of the time development under the Schrödinger equation. It can be shown that, once an equilibrium has been reached, the system remains in such equilibrium over the course of its further evolution: this follows from the continuity equation associated with the Schrödinger evolution of .^{[42]} However, it is less straightforward to demonstrate whether and how such an equilibrium is reached in the first place.
Antony Valentini^{[43]} has extended the de Broglie–Bohm theory to include signal nonlocality that would allow entanglement to be used as a standalone communication channel without a secondary classical "key" signal to "unlock" the message encoded in the entanglement. This violates orthodox quantum theory but has the virtue that it makes the parallel universes of the chaotic inflation theory observable in principle.
Unlike de Broglie–Bohm theory, Valentini's theory has the wavefunction evolution also depending on the ontological variables. This introduces an instability, a feedback loop that pushes the hidden variables out of "subquantal heat death". The resulting theory becomes nonlinear and nonunitary. Valentin argues that the laws of quantum mechanics are emergent and form a "quantum equilibrium" that has an analogous status to that of thermal equilibrium in classical dynamics. In principle therefore, other "quantum nonequilibrium" distributions may be potentially observed and exploited, for which the statistical predictions of quantum theory are violated. It is controversially argued that quantum theory is merely a special case of a much wider nonlinear physics, a physics in which nonlocal (superluminal) signalling is possible, and in which the uncertainty principle can be violated.^{[44]}^{[45]}
Results
Below are some highlights of the results that arise out of an analysis of de Broglie–Bohm theory. Experimental results agree with all of the standard predictions of quantum mechanics in so far as the latter has predictions. However, while standard quantum mechanics is limited to discussing the results of "measurements", de Broglie–Bohm theory is a theory that governs the dynamics of a system without the intervention of outside observers (p. 117 in Bell^{[46]}).
The basis for agreement with standard quantum mechanics is that the particles are distributed according to . This is a statement of observer ignorance, but it can be proven^{[16]} that for a universe governed by this theory, this will typically be the case. There is apparent collapse of the wave function governing subsystems of the universe, but there is no collapse of the universal wavefunction.
Measuring spin and polarization
According to ordinary quantum theory, it is not possible to measure the spin or polarization of a particle directly; instead, the component in one direction is measured; the outcome from a single particle may be 1, meaning that the particle is aligned with the measuring apparatus, or −1, meaning that it is aligned the opposite way. For an ensemble of particles, if we expect the particles to be aligned, the results are all 1. If we expect them to be aligned oppositely, the results are all −1. For other alignments, we expect some results to be 1 and some to be −1 with a probability that depends on the expected alignment. For a full explanation of this, see the Stern–Gerlach experiment.
In de Broglie–Bohm theory, the results of a spin experiment cannot be analyzed without some knowledge of the experimental setup. It is possible^{[47]} to modify the setup so that the trajectory of the particle is unaffected, but that the particle with one setup registers as spinup, while in the other setup it registers as spindown. Thus, for the de Broglie–Bohm theory, the particle's spin is not an intrinsic property of the particle; instead spin is, so to speak, in the wavefunction of the particle in relation to the particular device being used to measure the spin. This is an illustration of what is sometimes referred to as contextuality and is related to naive realism about operators.^{[48]} Interpretationally, measurement results are a deterministic property of the system and its environment, which includes information about the experimental setup including the context of comeasured observables; in no sense does the system itself possess the property being measured, as would have been the case in classical physics.
Measurements, the quantum formalism, and observer independence
De Broglie–Bohm theory gives the same results as quantum mechanics. It treats the wavefunction as a fundamental object in the theory, as the wavefunction describes how the particles move. This means that no experiment can distinguish between the two theories. This section outlines the ideas as to how the standard quantum formalism arises out of quantum mechanics. References include Bohm's original 1952 paper and Dürr et al.^{[16]}
Collapse of the wavefunction
De Broglie–Bohm theory is a theory that applies primarily to the whole universe. That is, there is a single wavefunction governing the motion of all of the particles in the universe according to the guiding equation. Theoretically, the motion of one particle depends on the positions of all of the other particles in the universe. In some situations, such as in experimental systems, we can represent the system itself in terms of a de Broglie–Bohm theory in which the wavefunction of the system is obtained by conditioning on the environment of the system. Thus, the system can be analyzed with Schrödinger's equation and the guiding equation, with an initial distribution for the particles in the system (see the section on the conditional wavefunction of a subsystem for details).
It requires a special setup for the conditional wavefunction of a system to obey a quantum evolution. When a system interacts with its environment, such as through a measurement, the conditional wavefunction of the system evolves in a different way. The evolution of the universal wavefunction can become such that the wavefunction of the system appears to be in a superposition of distinct states. But if the environment has recorded the results of the experiment, then using the actual Bohmian configuration of the environment to condition on, the conditional wavefunction collapses to just one alternative, the one corresponding with the measurement results.
Collapse of the universal wavefunction never occurs in de Broglie–Bohm theory. Its entire evolution is governed by Schrödinger's equation, and the particles' evolutions are governed by the guiding equation. Collapse only occurs in a phenomenological way for systems that seem to follow their own Schrödinger's equation. As this is an effective description of the system, it is a matter of choice as to what to define the experimental system to include, and this will affect when "collapse" occurs.
Operators as observables
In the standard quantum formalism, measuring observables is generally thought of as measuring operators on the Hilbert space. For example, measuring position is considered to be a measurement of the position operator. This relationship between physical measurements and Hilbert space operators is, for standard quantum mechanics, an additional axiom of the theory. The de Broglie–Bohm theory, by contrast, requires no such measurement axioms (and measurement as such is not a dynamically distinct or special subcategory of physical processes in the theory). In particular, the usual operatorsasobservables formalism is, for de Broglie–Bohm theory, a theorem.^{[49]} A major point of the analysis is that many of the measurements of the observables do not correspond to properties of the particles; they are (as in the case of spin discussed above) measurements of the wavefunction.
In the history of de Broglie–Bohm theory, the proponents have often had to deal with claims that this theory is impossible. Such arguments are generally based on inappropriate analysis of operators as observables. If one believes that spin measurements are indeed measuring the spin of a particle that existed prior to the measurement, then one does reach contradictions. De Broglie–Bohm theory deals with this by noting that spin is not a feature of the particle, but rather that of the wavefunction. As such, it only has a definite outcome once the experimental apparatus is chosen. Once that is taken into account, the impossibility theorems become irrelevant.
There have also been claims that experiments reject the Bohm trajectories ^{[50]} in favor of the standard QM lines. But as shown in other work,^{[51]}^{[52]} such experiments cited above only disprove a misinterpretation of the de Broglie–Bohm theory, not the theory itself.
There are also objections to this theory based on what it says about particular situations usually involving eigenstates of an operator. For example, the ground state of hydrogen is a real wavefunction. According to the guiding equation, this means that the electron is at rest when in this state. Nevertheless, it is distributed according to , and no contradiction to experimental results is possible to detect.
Operators as observables leads many to believe that many operators are equivalent. De Broglie–Bohm theory, from this perspective, chooses the position observable as a favored observable rather than, say, the momentum observable. Again, the link to the position observable is a consequence of the dynamics. The motivation for de Broglie–Bohm theory is to describe a system of particles. This implies that the goal of the theory is to describe the positions of those particles at all times. Other observables do not have this compelling ontological status. Having definite positions explains having definite results such as flashes on a detector screen. Other observables would not lead to that conclusion, but there need not be any problem in defining a mathematical theory for other observables; see Hyman et al.^{[53]} for an exploration of the fact that a probability density and probability current can be defined for any set of commuting operators.
Hidden variables
De Broglie–Bohm theory is often referred to as a "hiddenvariable" theory. Bohm used this description in his original papers on the subject, writing: "From the point of view of the usual interpretation, these additional elements or parameters [permitting a detailed causal and continuous description of all processes] could be called 'hidden' variables." Bohm and Hiley later stated that they found Bohm's choice of the term "hidden variables" to be too restrictive. In particular, they argued that a particle is not actually hidden but rather "is what is most directly manifested in an observation [though] its properties cannot be observed with arbitrary precision (within the limits set by uncertainty principle)".^{[54]} However, others nevertheless treat the term "hidden variable" as a suitable description.^{[55]}
Generalized particle trajectories can be extrapolated from numerous weak measurements on an ensemble of equally prepared systems, and such trajectories coincide with the de Broglie–Bohm trajectories. In particular, an experiment with two entangled photons, in which a set of Bohmian trajectories for one of the photons was determined using weak measurements and postselection, can be understood in terms of a nonlocal connection between that photon's trajectory and the other photon's polarization.^{[56]}^{[57]} However, not only the De Broglie–Bohm interpretation, but also many other interpretations of quantum mechanics that do not include such trajectories are consistent with such experimental evidence.
Heisenberg's uncertainty principle
The Heisenberg's uncertainty principle states that when two complementary measurements are made, there is a limit to the product of their accuracy. As an example, if one measures the position with an accuracy of and the momentum with an accuracy of , then If we make further measurements in order to get more information, we disturb the system and change the trajectory into a new one depending on the measurement setup; therefore, the measurement results are still subject to Heisenberg's uncertainty relation.
In de Broglie–Bohm theory, there is always a matter of fact about the position and momentum of a particle. Each particle has a welldefined trajectory, as well as a wavefunction. Observers have limited knowledge as to what this trajectory is (and thus of the position and momentum). It is the lack of knowledge of the particle's trajectory that accounts for the uncertainty relation. What one can know about a particle at any given time is described by the wavefunction. Since the uncertainty relation can be derived from the wavefunction in other interpretations of quantum mechanics, it can be likewise derived (in the epistemic sense mentioned above) on the de Broglie–Bohm theory.
To put the statement differently, the particles' positions are only known statistically. As in classical mechanics, successive observations of the particles' positions refine the experimenter's knowledge of the particles' initial conditions. Thus, with succeeding observations, the initial conditions become more and more restricted. This formalism is consistent with the normal use of the Schrödinger equation.
For the derivation of the uncertainty relation, see Heisenberg uncertainty principle, noting that this article describes the principle from the viewpoint of the Copenhagen interpretation.
Quantum entanglement, Einstein–Podolsky–Rosen paradox, Bell's theorem, and nonlocality
De Broglie–Bohm theory highlighted the issue of nonlocality: it inspired John Stewart Bell to prove his nowfamous theorem,^{[58]} which in turn led to the Bell test experiments.
In the Einstein–Podolsky–Rosen paradox, the authors describe a thought experiment that one could perform on a pair of particles that have interacted, the results of which they interpreted as indicating that quantum mechanics is an incomplete theory.^{[59]}
Decades later John Bell proved Bell's theorem (see p. 14 in Bell^{[46]}), in which he showed that, if they are to agree with the empirical predictions of quantum mechanics, all such "hiddenvariable" completions of quantum mechanics must either be nonlocal (as the Bohm interpretation is) or give up the assumption that experiments produce unique results (see counterfactual definiteness and manyworlds interpretation). In particular, Bell proved that any local theory with unique results must make empirical predictions satisfying a statistical constraint called "Bell's inequality".
Alain Aspect performed a series of Bell test experiments that test Bell's inequality using an EPRtype setup. Aspect's results show experimentally that Bell's inequality is in fact violated, meaning that the relevant quantummechanical predictions are correct. In these Bell test experiments, entangled pairs of particles are created; the particles are separated, traveling to remote measuring apparatus. The orientation of the measuring apparatus can be changed while the particles are in flight, demonstrating the apparent nonlocality of the effect.
The de Broglie–Bohm theory makes the same (empirically correct) predictions for the Bell test experiments as ordinary quantum mechanics. It is able to do this because it is manifestly nonlocal. It is often criticized or rejected based on this; Bell's attitude was: "It is a merit of the de Broglie–Bohm version to bring this [nonlocality] out so explicitly that it cannot be ignored."^{[60]}
The de Broglie–Bohm theory describes the physics in the Bell test experiments as follows: to understand the evolution of the particles, we need to set up a wave equation for both particles; the orientation of the apparatus affects the wavefunction. The particles in the experiment follow the guidance of the wavefunction. It is the wavefunction that carries the fasterthanlight effect of changing the orientation of the apparatus. An analysis of exactly what kind of nonlocality is present and how it is compatible with relativity can be found in Maudlin.^{[61]} Note that in Bell's work, and in more detail in Maudlin's work, it is shown that the nonlocality does not allow signaling at speeds faster than light.
Classical limit
Bohm's formulation of de Broglie–Bohm theory in terms of a classically looking version has the merits that the emergence of classical behavior seems to follow immediately for any situation in which the quantum potential is negligible, as noted by Bohm in 1952. Modern methods of decoherence are relevant to an analysis of this limit. See Allori et al.^{[62]} for steps towards a rigorous analysis.
Quantum trajectory method
Work by Robert E. Wyatt in the early 2000s attempted to use the Bohm "particles" as an adaptive mesh that follows the actual trajectory of a quantum state in time and space. In the "quantum trajectory" method, one samples the quantum wavefunction with a mesh of quadrature points. One then evolves the quadrature points in time according to the Bohm equations of motion. At each time step, one then resynthesizes the wavefunction from the points, recomputes the quantum forces, and continues the calculation. (QuickTime movies of this for H + H_{2} reactive scattering can be found on the Wyatt group website at UT Austin.) This approach has been adapted, extended, and used by a number of researchers in the chemical physics community as a way to compute semiclassical and quasiclassical molecular dynamics. A recent (2007) issue of the Journal of Physical Chemistry A was dedicated to Prof. Wyatt and his work on "computational Bohmian dynamics".
Eric R. Bittner's group at the University of Houston has advanced a statistical variant of this approach that uses Bayesian sampling technique to sample the quantum density and compute the quantum potential on a structureless mesh of points. This technique was recently used to estimate quantum effects in the heat capacity of small clusters Ne_{n} for n ≈ 100.
There remain difficulties using the Bohmian approach, mostly associated with the formation of singularities in the quantum potential due to nodes in the quantum wavefunction. In general, nodes forming due to interference effects lead to the case where This results in an infinite force on the sample particles forcing them to move away from the node and often crossing the path of other sample points (which violates singlevaluedness). Various schemes have been developed to overcome this; however, no general solution has yet emerged.
These methods, as does Bohm's Hamilton–Jacobi formulation, do not apply to situations in which the full dynamics of spin need to be taken into account.
Similarities with the manyworlds interpretation
Kim Joris Boström has proposed a nonrelativistic quantum mechanical theory that combines elements of the de BroglieBohm mechanics and that of Everett’s many‘worlds’. In particular, the unreal MW interpretation of Hawking and Weinberg is similar to the Bohmian concept of unreal empty branch ‘worlds’:
The second issue with Bohmian mechanics may at first sight appear rather harmless, but which on a closer look develops considerable destructive power: the issue of empty branches. These are the components of the postmeasurement state that do not guide any particles because they do not have the actual configuration q in their support. At first sight, the empty branches do not appear problematic but on the contrary very helpful as they enable the theory to explain unique outcomes of measurements. Also, they seem to explain why there is an effective “collapse of the wavefunction”, as in ordinary quantum mechanics. On a closer view, though, one must admit that these empty branches do not actually disappear. As the wavefunction is taken to describe a really existing field, all their branches really exist and will evolve forever by the Schrödinger dynamics, no matter how many of them will become empty in the course of the evolution. Every branch of the global wavefunction potentially describes a complete world which is, according to Bohm’s ontology, only a possible world that would be the actual world if only it were filled with particles, and which is in every respect identical to a corresponding world in Everett’s theory. Only one branch at a time is occupied by particles, thereby representing the actual world, while all other branches, though really existing as part of a really existing wavefunction, are empty and thus contain some sort of “zombie worlds” with planets, oceans, trees, cities, cars and people who talk like us and behave like us, but who do not actually exist. Now, if the Everettian theory may be accused of ontological extravagance, then Bohmian mechanics could be accused of ontological wastefulness. On top of the ontology of empty branches comes the additional ontology of particle positions that are, on account of the quantum equilibrium hypothesis, forever unknown to the observer. Yet, the actual configuration is never needed for the calculation of the statistical predictions in experimental reality, for these can be obtained by mere wavefunction algebra. From this perspective, Bohmian mechanics may appear as a wasteful and redundant theory. I think it is considerations like these that are the biggest obstacle in the way of a general acceptance of Bohmian mechanics.^{[63]}
Many authors have expressed critical views of the de Broglie–Bohm theory by comparing it to Everett's manyworlds approach. Many (but not all) proponents of the de Broglie–Bohm theory (such as Bohm and Bell) interpret the universal wavefunction as physically real. According to some supporters of Everett's theory, if the (never collapsing) wavefunction is taken to be physically real, then it is natural to interpret the theory as having the same many worlds as Everett's theory. In the Everettian view the role of the Bohmian particle is to act as a "pointer", tagging, or selecting, just one branch of the universal wavefunction (the assumption that this branch indicates which wave packet determines the observed result of a given experiment is called the "result assumption"^{[64]}); the other branches are designated "empty" and implicitly assumed by Bohm to be devoid of conscious observers.^{[64]} H. Dieter Zeh comments on these "empty" branches:^{[65]}
“  It is usually overlooked that Bohm's theory contains the same "many worlds" of dynamically separate branches as the Everett interpretation (now regarded as "empty" wave components), since it is based on precisely the same ... global wave function ...  ” 
David Deutsch has expressed the same point more "acerbically":^{[64]}^{[66]}
“  pilotwave theories are paralleluniverse theories in a state of chronic denial.  ” 
Occam'srazor criticism
Both Hugh Everett III and Bohm treated the wavefunction as a physically real field. Everett's manyworlds interpretation is an attempt to demonstrate that the wavefunction alone is sufficient to account for all our observations. When we see the particle detectors flash or hear the click of a Geiger counter, then Everett's theory interprets this as our wavefunction responding to changes in the detector's wavefunction, which is responding in turn to the passage of another wavefunction (which we think of as a "particle", but is actually just another wave packet).^{[64]} No particle (in the Bohm sense of having a defined position and velocity) exists, according to that theory. For this reason Everett sometimes referred to his own manyworlds approach as the "pure wave theory". Talking of Bohm's 1952 approach, Everett says:^{[67]}
“  Our main criticism of this view is on the grounds of simplicity – if one desires to hold the view that is a real field, then the associated particle is superfluous, since, as we have endeavored to illustrate, the pure wave theory is itself satisfactory.  ” 
In the Everettian view, then, the Bohm particles are superfluous entities, similar to, and equally as unnecessary as, for example, the luminiferous ether, which was found to be unnecessary in special relativity. This argument of Everett is sometimes called the "redundancy argument", since the superfluous particles are redundant in the sense of Occam's razor.^{[68]}
According to Brown & Wallace,^{[64]} the de Broglie–Bohm particles play no role in the solution of the measurement problem. These authors claim^{[64]} that the "result assumption" (see above) is inconsistent with the view that there is no measurement problem in the predictable outcome (i.e. singleoutcome) case. These authors also claim^{[64]} that a standard tacit assumption of the de Broglie–Bohm theory (that an observer becomes aware of configurations of particles of ordinary objects by means of correlations between such configurations and the configuration of the particles in the observer's brain) is unreasonable. This conclusion has been challenged by Valentini,^{[69]} who argues that the entirety of such objections arises from a failure to interpret de Broglie–Bohm theory on its own terms.
According to Peter R. Holland, in a wider Hamiltonian framework, theories can be formulated in which particles do act back on the wave function.^{[70]}
Derivations
De Broglie–Bohm theory has been derived many times and in many ways. Below are six derivations, all of which are very different and lead to different ways of understanding and extending this theory.
 Schrödinger's equation can be derived by using Einstein's light quanta hypothesis: and de Broglie's hypothesis: .
 The guiding equation can be derived in a similar fashion. We assume a plane wave: . Notice that . Assuming that for the particle's actual velocity, we have that . Thus, we have the guiding equation.
 Notice that this derivation does not use Schrödinger's equation.
 Preserving the density under the time evolution is another method of derivation. This is the method that Bell cites. It is this method that generalizes to many possible alternative theories. The starting point is the continuity equation for the density . This equation describes a probability flow along a current. We take the velocity field associated with this current as the velocity field whose integral curves yield the motion of the particle.
 A method applicable for particles without spin is to do a polar decomposition of the wavefunction and transform Schrödinger's equation into two coupled equations: the continuity equation from above and the Hamilton–Jacobi equation. This is the method used by Bohm in 1952. The decomposition and equations are as follows:
 Decomposition: Note that corresponds to the probability density .
 Continuity equation: .
 Hamilton–Jacobi equation:
 The Hamilton–Jacobi equation is the equation derived from a Newtonian system with potential and velocity field The potential is the classical potential that appears in Schrödinger's equation, and the other term involving is the quantum potential, terminology introduced by Bohm.
 This leads to viewing the quantum theory as particles moving under the classical force modified by a quantum force. However, unlike standard Newtonian mechanics, the initial velocity field is already specified by , which is a symptom of this being a firstorder theory, not a secondorder theory.
 A fourth derivation was given by Dürr et al.^{[16]} In their derivation, they derive the velocity field by demanding the appropriate transformation properties given by the various symmetries that Schrödinger's equation satisfies, once the wavefunction is suitably transformed. The guiding equation is what emerges from that analysis.
 A fifth derivation, given by Dürr et al.^{[38]} is appropriate for generalization to quantum field theory and the Dirac equation. The idea is that a velocity field can also be understood as a firstorder differential operator acting on functions. Thus, if we know how it acts on functions, we know what it is. Then given the Hamiltonian operator , the equation to satisfy for all functions (with associated multiplication operator ) is , where is the local Hermitian inner product on the value space of the wavefunction.
 This formulation allows for stochastic theories such as the creation and annihilation of particles.
 A further derivation has been given by Peter R. Holland, on which he bases the entire work presented in his quantumphysics textbook The Quantum Theory of Motion,^{[71]} a main reference book on the de Broglie–Bohm theory. It is based on three basic postulates and an additional fourth postulate that links the wavefunction to measurement probabilities:
 1. A physical system consists in a spatiotemporally propagating wave and a point particle guided by it.
 2. The wave is described mathematically by a solution to Schrödinger's wave equation.
 3. The particle motion is described by a solution to in dependence on initial condition , with the phase of .
 The fourth postulate is subsidiary yet consistent with the first three:
 4. The probability to find the particle in the differential volume at time t equals .
History
De Broglie–Bohm theory has a history of different formulations and names. In this section, each stage is given a name and a main reference.
Pilotwave theory
Louis de Broglie presented his pilot wave theory at the 1927 Solvay Conference,^{[72]} after close collaboration with Schrödinger, who developed his wave equation for de Broglie's theory. At the end of the presentation, Wolfgang Pauli pointed out that it was not compatible with a semiclassical technique Fermi had previously adopted in the case of inelastic scattering. Contrary to a popular legend, de Broglie actually gave the correct rebuttal that the particular technique could not be generalized for Pauli's purpose, although the audience might have been lost in the technical details and de Broglie's mild manner left the impression that Pauli's objection was valid. He was eventually persuaded to abandon this theory nonetheless because he was "discouraged by criticisms which [it] roused".^{[73]} De Broglie's theory already applies to multiple spinless particles, but lacks an adequate theory of measurement as no one understood quantum decoherence at the time. An analysis of de Broglie's presentation is given in Bacciagaluppi et al.^{[74]}^{[75]} Also, in 1932 John von Neumann published a paper,^{[76]} that was widely (and erroneously, as shown by Jeffrey Bub^{[77]}) believed to prove that all hiddenvariable theories are impossible. This sealed the fate of de Broglie's theory for the next two decades.
In 1926, Erwin Madelung had developed a hydrodynamic version of Schrödinger's equation, which is incorrectly considered as a basis for the density current derivation of the de Broglie–Bohm theory.^{[78]} The Madelung equations, being quantum Euler equations (fluid dynamics), differ philosophically from the de Broglie–Bohm mechanics^{[79]} and are the basis of the stochastic interpretation of quantum mechanics.
Peter R. Holland has pointed out that, earlier in 1927, Einstein had actually submitted a preprint with a similar proposal but, not convinced, had withdrawn it before publication.^{[80]} According to Holland, failure to appreciate key points of the de Broglie–Bohm theory has led to confusion, the key point being "that the trajectories of a manybody quantum system are correlated not because the particles exert a direct force on one another (à la Coulomb) but because all are acted upon by an entity – mathematically described by the wavefunction or functions of it – that lies beyond them".^{[81]} This entity is the quantum potential.
After publishing a popular textbook on Quantum Mechanics that adhered entirely to the Copenhagen orthodoxy, Bohm was persuaded by Einstein to take a critical look at von Neumann's theorem. The result was 'A Suggested Interpretation of the Quantum Theory in Terms of "Hidden Variables" I and II' [Bohm 1952]. It was an independent origination of the pilot wave theory, and extended it to incorporate a consistent theory of measurement, and to address a criticism of Pauli that de Broglie did not properly respond to; it is taken to be deterministic (though Bohm hinted in the original papers that there should be disturbances to this, in the way Brownian motion disturbs Newtonian mechanics). This stage is known as the de Broglie–Bohm Theory in Bell's work [Bell 1987] and is the basis for 'The Quantum Theory of Motion' [Holland 1993].
This stage applies to multiple particles, and is deterministic.
The de Broglie–Bohm theory is an example of a hiddenvariables theory. Bohm originally hoped that hidden variables could provide a local, causal, objective description that would resolve or eliminate many of the paradoxes of quantum mechanics, such as Schrödinger's cat, the measurement problem and the collapse of the wavefunction. However, Bell's theorem complicates this hope, as it demonstrates that there can be no local hiddenvariable theory that is compatible with the predictions of quantum mechanics. The Bohmian interpretation is causal but not local.
Bohm's paper was largely ignored or panned by other physicists. Albert Einstein, who had suggested that Bohm search for a realist alternative to the prevailing Copenhagen approach, did not consider Bohm's interpretation to be a satisfactory answer to the quantum nonlocality question, calling it "too cheap",^{[82]} while Werner Heisenberg considered it a "superfluous 'ideological superstructure' ".^{[83]} Wolfgang Pauli, who had been unconvinced by de Broglie in 1927, conceded to Bohm as follows:
I just received your long letter of 20th November, and I also have studied more thoroughly the details of your paper. I do not see any longer the possibility of any logical contradiction as long as your results agree completely with those of the usual wave mechanics and as long as no means is given to measure the values of your hidden parameters both in the measuring apparatus and in the observe [sic] system. As far as the whole matter stands now, your ‘extra wavemechanical predictions’ are still a check, which cannot be cashed.^{[84]}
He subsequently described Bohm's theory as "artificial metaphysics".^{[85]}
According to physicist Max Dresden, when Bohm's theory was presented at the Institute for Advanced Study in Princeton, many of the objections were ad hominem, focusing on Bohm's sympathy with communists as exemplified by his refusal to give testimony to the House UnAmerican Activities Committee.^{[86]}
In 1979, Chris Philippidis, Chris Dewdney and Basil Hiley were the first to perform numeric computations on the basis of the quantum potential to deduce ensembles of particle trajectories.^{[87]}^{[88]} Their work renewed the interests of physicists in the Bohm interpretation of quantum physics.^{[89]}
Eventually John Bell began to defend the theory. In "Speakable and Unspeakable in Quantum Mechanics" [Bell 1987], several of the papers refer to hiddenvariables theories (which include Bohm's).
The trajectories of the Bohm model that would result for particular experimental arrangements were termed "surreal" by some.^{[90]}^{[91]} Still in 2016, mathematical physicist Sheldon Goldstein said about Bohm's theory: "There was a time when you couldn’t even talk about it because it was heretical. It probably still is the kiss of death for a physics career to be actually working on Bohm, but maybe that’s changing."^{[57]}
Bohmian mechanics
Bohmian mechanics is the same theory, but with an emphasis on the notion of current flow, which is determined on the basis of the quantum equilibrium hypothesis that the probability follows the Born rule. The term "Bohmian mechanics" is also often used to include most of the further extensions past the spinless version of Bohm. While de Broglie–Bohm theory has Lagrangians and HamiltonJacobi equations as a primary focus and backdrop, with the icon of the quantum potential, Bohmian mechanics considers the continuity equation as primary and has the guiding equation as its icon. They are mathematically equivalent in so far as the HamiltonJacobi formulation applies, i.e., spinless particles. The papers of Dürr et al. popularized the term.
All of nonrelativistic quantum mechanics can be fully accounted for in this theory.
Causal interpretation and ontological interpretation
Bohm developed his original ideas, calling them the Causal Interpretation. Later he felt that causal sounded too much like deterministic and preferred to call his theory the Ontological Interpretation. The main reference is "The Undivided Universe" [Bohm, Hiley 1993].
This stage covers work by Bohm and in collaboration with JeanPierre Vigier and Basil Hiley. Bohm is clear that this theory is nondeterministic (the work with Hiley includes a stochastic theory). As such, this theory is not, strictly speaking, a formulation of the de Broglie–Bohm theory. However, it deserves mention here because the term "Bohm Interpretation" is ambiguous between this theory and the de Broglie–Bohm theory.
An indepth analysis of possible interpretations of Bohm's model of 1952 was given in 1996 by philosopher of science Arthur Fine.^{[92]}
Hydrodynamic quantum analogs
Pioneering experiments on hydrodynamical analogs of quantum mechanics beginning with the work of Couder and Fort (2006)^{[93]}^{[94]} have shown that macroscopic classical pilotwaves can exhibit characteristics previously thought to be restricted to the quantum realm. Hydrodynamic pilotwave analogs have been able to duplicate the double slit experiment, tunneling, quantized orbits, and numerous other quantum phenomena which have led to a resurgence in interest in pilot wave theories.^{[95]}^{[96]}^{[97]} Coulder and Fort note in their 2006 paper that pilotwaves are nonlinear dissipative systems sustained by external forces. A dissipative system is characterized by the spontaneous appearance of symmetry breaking (anisotropy) and the formation of complex, sometimes chaotic or emergent, dynamics where interacting fields can exhibit long range correlations. Stochastic electrodynamics (SED) an extension of the de Broglie–Bohm interpretation of quantum mechanics, with the electromagnetic zeropoint field (ZPF) playing a central role as the guiding pilotwave. Modern approaches to SED consider wave and particlelike quantum effects as wellcoordinated emergent systems that are the result of speculated subquantum interactions with the zeropoint field^{[98]}^{[99]}^{[100]}
Hydrodynamic walkers  de Broglie  SED pilot wave  

Driving  bath vibration  internal clock  vacuum fluctuations 
Spectrum  monochromatic  monochromatic  broad 
Trigger  bouncing  zitterbewegung  zitterbewegung 
Trigger frequency  
Energetics  GPE wave  EM  
Resonance  dropletwave  harmony of phases  unspecified 
Dispersion  
Carrier  
Statistical 
Experiments
Researchers performed the ESSW experiment.^{[107]} They found that the photon trajectories aren’t surrealistic after all but more precisely, that the paths may seem surrealistic, but only if one fails to take into account the nonlocality inherent in Bohm’s theory.^{[108]}^{[109]}^{[110]}
See also
 David Bohm
 Faraday wave
 Interpretation of quantum mechanics
 Madelung equations
 Local hiddenvariable theory
 Quantum mechanics
 Pilot wave
 Superfluid vacuum theory
 Fluid analogs in quantum mechanics
 Probability current
Notes
 ↑ Bohm, David (1952). "A Suggested Interpretation of the Quantum Theory in Terms of 'Hidden Variables' I". Physical Review. 85 (2): 166–179. Bibcode:1952PhRv...85..166B. doi:10.1103/PhysRev.85.166. ("In contrast to the usual interpretation, this alternative interpretation permits us to conceive of each individual system as being in a precisely definable state, whose changes with time are determined by definite laws, analogous to (but not identical with) the classical equations of motion. Quantummechanical probabilities are regarded (like their counterparts in classical statistical mechanics) as only a practical necessity and not as an inherent lack of complete determination in the properties of matter at the quantum level.")
 ↑ F. David Peat, Infinite Potential: The Life and Times of David Bohm (1997), p. 133. James T. Cushing, Quantum Mechanics: Historical Contingency and the Copenhagen Hegemony (1994) discusses "the hegemony of the Copenhagen interpretation of quantum mechanics" over theories like Bohmian mechanics as an example of how the acceptance of scientific theories may be guided by social aspects.
 ↑ David Bohm and Basil J. Hiley, The Undivided Universe – An Ontological Interpretation of Quantum Theory appreared after Bohm's death, in 1993; reviewed by Sheldon Goldstein in Physics Today (1994). J. Cushing, A. Fine, S. Goldstein (eds.), Bohmian Mechanics and Quantum Theory – An Appraisal (1996).
 ↑ John W. M. Bush: "Quantum mechanics writ large".
 ↑ Publications of D. Bohm in 1952 and 1953 and of J.P. Vigier in 1954 as cited in Antony Valentini; Hans Westman (2005). "Dynamical origin of quantum probabilities". Proc. R. Soc. A. 461 (2053): 253–272. arXiv:quantph/0403034. Bibcode:2005RSPSA.461..253V. CiteSeerX 10.1.1.252.849. doi:10.1098/rspa.2004.1394. p. 254.
 ↑ "Observing the Average Trajectories of Single Photons in a TwoSlit Interferometer"
 ↑ MacIsaac, Dan (January 2017). "Bouncing droplets, pilot waves, the doubleslit experiment, and deBroglieBohm theory". The Physics Teacher. 55 (1): 62. Bibcode:2017PhTea..55S..62.. doi:10.1119/1.4972510. ISSN 0031921X.
 ↑ "When fluid dynamics mimic quantum mechanics". MIT News. Retrieved 20180719.
 ↑ David Bohm (1957). Causality and Chance in Modern Physics. Routledge & Kegan Paul and D. Van Nostrand. ISBN 9780812210026. , p. 117.
 ↑ D. Bohm and B. Hiley: The undivided universe: An ontological interpretation of quantum theory, p. 37.
 ↑ H. R. Brown, C. Dewdney and G. Horton: "Bohm particles and their detection in the light of neutron interferometry", Foundations of Physics, 1995, Volume 25, Number 2, pp. 329–347.
 ↑ J. Anandan, "The Quantum Measurement Problem and the Possible Role of the Gravitational Field", Foundations of Physics, March 1999, Volume 29, Issue 3, pp. 333–348.
 ↑ D. Bohm and B. Hiley: The undivided universe: An ontological interpretation of quantum theory, p. 24.
 ↑ Peter R. Holland: The Quantum Theory of Motion: An Account of the De Broglie–Bohm Causal Interpretation of Quantum Mechanics, Cambridge University Press, Cambridge (first published 25 June 1993), ISBN 0521354048 hardback, ISBN 0521485436 paperback, transferred to digital printing 2004, Chapter I. section (7) "There is no reciprocal action of the particle on the wave", p. 26.
 ↑ P. Holland: "Hamiltonian theory of wave and particle in quantum mechanics II: HamiltonJacobi theory and particle backreaction", Nuovo Cimento B 116, 2001, pp. 1143–1172, full text preprint p. 31).
 1 2 3 4 Dürr, D.; Goldstein, S.; Zanghì, N. (1992). "Quantum Equilibrium and the Origin of Absolute Uncertainty". Journal of Statistical Physics. 67 (5–6): 843–907. arXiv:quantph/0308039. Bibcode:1992JSP....67..843D. doi:10.1007/BF01049004.
 ↑ Towler, M. D.; Russell, N. J.; Valentini, A. (2011). "Timescales for dynamical relaxation to the Born rule". Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences. 468 (2140): 990. arXiv:1103.1589. Bibcode:2012RSPSA.468..990T. doi:10.1098/rspa.2011.0598. . A video of the electron density in a 2D box evolving under this process is available here.
 ↑ Dürr, Detlef; Goldstein, Sheldon; Zanghí, Nino (2003). "Quantum Equilibrium and the Origin of Absolute Uncertainty". Journal of Statistical Physics. 67 (5–6): 843–907. arXiv:quantph/0308039. Bibcode:1992JSP....67..843D. doi:10.1007/BF01049004.
 ↑ Passon, Oliver (2006). "What you always wanted to know about Bohmian mechanics but were afraid to ask". Physics and Philosophy. 3 (2006). arXiv:quantph/0611032. Bibcode:2006quant.ph.11032P. doi:10.17877/DE290R14213. hdl:2003/23108.
 ↑ Nikolic, H. (2004). "Bohmian particle trajectories in relativistic bosonic quantum field theory". Foundations of Physics Letters. 17 (4): 363–380. arXiv:quantph/0208185. Bibcode:2004FoPhL..17..363N. CiteSeerX 10.1.1.253.838. doi:10.1023/B:FOPL.0000035670.31755.0a.
 ↑ Nikolic, H. (2005). "Bohmian particle trajectories in relativistic fermionic quantum field theory". Foundations of Physics Letters. 18 (2): 123–138. arXiv:quantph/0302152. Bibcode:2005FoPhL..18..123N. doi:10.1007/s1070200539573.
 ↑ Dürr, D.; Goldstein, S.; MünchBerndl, K.; Zanghì, N. (1999). "Hypersurface Bohm–Dirac Models". Physical Review A. 60 (4): 2729–2736. arXiv:quantph/9801070. Bibcode:1999PhRvA..60.2729D. doi:10.1103/physreva.60.2729.
 ↑ Dürr, Detlef; Goldstein, Sheldon; Norsen, Travis; Struyve, Ward; Zanghì, Nino (2013). "Can Bohmian mechanics be made relativistic?". Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences. 470 (2162): 20130699. arXiv:1307.1714. Bibcode:2013RSPSA.47030699D. doi:10.1098/rspa.2013.0699. PMC 3896068. PMID 24511259.
 1 2 Ghose, Partha (1996). "Relativistic quantum mechanics of spin0 and spin1 bosons" (PDF). Foundations of Physics. 26 (11): 1441–1455. Bibcode:1996FoPh...26.1441G. doi:10.1007/BF02272366.
 ↑ Cufaro Petroni, Nicola; Vigier, JeanPierre (2001). "Remarks on Observed Superluminal Light Propagation". Foundations of Physics Letters. 14 (4): 395–400. doi:10.1023/A:1012321402475. , therein: section 3. Conclusions, page 399.
 ↑ Ghose, Partha; Majumdar, A. S.; Guhab, S.; Sau, J. (2001). "Bohmian trajectories for photons" (PDF). Physics Letters A. 290 (5–6): 205–213. arXiv:quantph/0102071. Bibcode:2001PhLA..290..205G. doi:10.1016/s03759601(01)006776.
 ↑ Sacha Kocsis, Sylvain Ravets, Boris Braverman, Krister Shalm, Aephraim M. Steinberg: "Observing the trajectories of a single photon using weak measurement" Archived 26 June 2011 at the Wayback Machine. 19th Australian Institute of Physics (AIP) Congress, 2010.
 ↑ Kocsis, Sacha; Braverman, Boris; Ravets, Sylvain; Stevens, Martin J.; Mirin, Richard P.; Shalm, L. Krister; Steinberg, Aephraim M. (2011). "Observing the Average Trajectories of Single Photons in a TwoSlit Interferometer". Science. 332 (6034): 1170–1173. Bibcode:2011Sci...332.1170K. doi:10.1126/science.1202218. PMID 21636767.
 ↑ Dewdney, Chris; Horton, George (2002). "Relativistically invariant extension of the de Broglie Bohm theory of quantum mechanics". Journal of Physics A: Mathematical and General. 35 (47): 10117–10127. arXiv:quantph/0202104. Bibcode:2002JPhA...3510117D. doi:10.1088/03054470/35/47/311.
 ↑ Dewdney, Chris; Horton, George (2004). "A relativistically covariant version of Bohm's quantum field theory for the scalar field". Journal of Physics A: Mathematical and General. 37 (49): 11935–11943. arXiv:quantph/0407089. Bibcode:2004JPhA...3711935H. doi:10.1088/03054470/37/49/011.
 ↑ Dewdney, Chris; Horton, George (2010). "A relativistic hiddenvariable interpretation for the massive vector field based on energymomentum flows". Foundations of Physics. 40 (6): 658–678. Bibcode:2010FoPh...40..658H. doi:10.1007/s1070101094569.
 ↑ Nikolić, Hrvoje (2005). "Relativistic Quantum Mechanics and the Bohmian Interpretation". Foundations of Physics Letters. 18 (6): 549–561. arXiv:quantph/0406173. Bibcode:2005FoPhL..18..549N. CiteSeerX 10.1.1.252.6803. doi:10.1007/s1070200511281.
 1 2 Nikolic, H (2010). "QFT as pilotwave theory of particle creation and destruction". International Journal of Modern Physics. 25 (7): 1477–1505. arXiv:0904.2287. Bibcode:2010IJMPA..25.1477N. doi:10.1142/s0217751x10047889.
 ↑ Nikolic, H. (2009). "Time in relativistic and nonrelativistic quantum mechanics". Int.J.Quant.Inf. 7 (3): 595–602. arXiv:0811.1905. Bibcode:2008arXiv0811.1905N. doi:10.1142/s021974990900516x.
 ↑ Nikolic, H. (2010). "Making nonlocal reality compatible with relativity". Int. J. Quantum Inf. 9 (2011): 367–377. arXiv:1002.3226. Bibcode:2010arXiv1002.3226N.
 ↑ Hrvoje Nikolić: "Bohmian mechanics in relativistic quantum mechanics, quantum field theory and string theory", 2007 Journal of Physics: Conf. Ser. 67 012035.
 ↑ Sutherland, Roderick (2015). "Lagrangian Description for Particle Interpretations of Quantum Mechanics  Entangled ManyParticle Case". Foundations of Physics. 47 (2): 174–207. arXiv:1509.02442. Bibcode:2017FoPh...47..174S. doi:10.1007/s1070101600436.
 1 2 Duerr, Detlef; Goldstein, Sheldon; Tumulka, Roderich; Zanghi, Nino (2003). "Bohmian Mechanics and Quantum Field Theory". Physical Review Letters. 93 (9): 090402. arXiv:quantph/0303156. Bibcode:2004PhRvL..93i0402D. CiteSeerX 10.1.1.8.8444. doi:10.1103/PhysRevLett.93.090402. PMID 15447078.
 ↑ Duerr, Detlef; Goldstein, Sheldon; Tumulka, Roderich; Zanghi, Nino (2005). "BellType Quantum Field Theories". Journal of Physics A: Mathematical and General. 38 (4): R1. arXiv:quantph/0407116. Bibcode:2005JPhA...38R...1D. doi:10.1088/03054470/38/4/R01.
 ↑ Dürr, D.; Goldstein, S.; Taylor, J.; Tumulka, R.; Zanghì, N. (2007). "Quantum Mechanics in MultiplyConnected Spaces". J. Phys. A. 40 (12): 2997–3031. arXiv:quantph/0506173. Bibcode:2007JPhA...40.2997D. doi:10.1088/17518113/40/12/s08.
 ↑ Valentini, Antony (2013). "Hidden Variables in Modern Cosmology". youtube.com. Philosophy of Cosmology. Retrieved 23 December 2016.
 ↑ See for ex. Detlef Dürr, Sheldon Goldstein, Nino Zanghí: Bohmian mechanics and quantum equilibrium, Stochastic Processes, Physics and Geometry II. World Scientific, 1995 page 5
 ↑ Valentini, A (1991). "SignalLocality, Uncertainty and the Subquantum HTheorem. II". Physics Letters A. 158 (1–2): 1–8. Bibcode:1991PhLA..158....1V. doi:10.1016/03759601(91)90330b.
 ↑ Valentini, Antony (2009). "Beyond the quantum". Physics World. 22 (11): 32–37. arXiv:1001.2758. Bibcode:2009PhyW...22k..32V. doi:10.1088/20587058/22/11/36. ISSN 09538585.
 ↑ Musser, George (18 November 2013). "Cosmological Data Hint at a Level of Physics Underlying Quantum Mechanics". blogs.scientificamerican.com. Scientific American. Retrieved 5 December 2016.
 1 2 Bell, John S. (1987). Speakable and Unspeakable in Quantum Mechanics. Cambridge University Press. ISBN 9780521334952.
 ↑ Albert, D. Z., 1992, Quantum Mechanics and Experience, Cambridge, MA: Harvard University Press.
 ↑ Daumer, M.; Dürr, D.; Goldstein, S.; Zanghì, N. (1997). "Naive Realism About Operators". Erkenntnis. 45: 379–397. arXiv:quantph/9601013. Bibcode:1996quant.ph..1013D.
 ↑ Dürr, Detlef; Goldstein, Sheldon; Zanghì, Nino (2003). "Quantum Equilibrium and the Role of Operators as Observables in Quantum Theory". Journal of Statistical Physics. 116 (1–4): 959. arXiv:quantph/0308038. Bibcode:2004JSP...116..959D. CiteSeerX 10.1.1.252.1653. doi:10.1023/B:JOSS.0000037234.80916.d0.
 ↑ Brida, G.; Cagliero, E.; Falzetta, G.; Genovese, M.; Gramegna, M.; Novero, C. (2002). "A first experimental test of de BroglieBohm theory against standard quantum mechanics". Journal of Physics B: Atomic, Molecular and Optical Physics. 35 (22): 4751. arXiv:quantph/0206196. Bibcode:2002JPhB...35.4751B. doi:10.1088/09534075/35/22/316.
 ↑ Struyve, W.; De Baere, W. (2001). "Comments on some recently proposed experiments that should distinguish Bohmian mechanics from quantum mechanics". Quantum Theory: Reconsideration of Foundations. Vaxjo: Vaxjo University Press. p. 355. arXiv:quantph/0108038. Bibcode:2001quant.ph..8038S.
 ↑ Nikolic, H. (2003). "On compatibility of Bohmian mechanics with standard quantum mechanics". arXiv:quantph/0305131.
 ↑ Hyman, Ross; Caldwell, Shane A; Dalton, Edward (2004). "Bohmian mechanics with discrete operators". Journal of Physics A: Mathematical and General. 37 (44): L547. arXiv:quantph/0401008. Bibcode:2004JPhA...37L.547H. doi:10.1088/03054470/37/44/L02.
 ↑ David Bohm, Basil Hiley: The Undivided Universe: An Ontological Interpretation of Quantum Theory, edition published in the Taylor & Francis elibrary 2009 (first edition Routledge, 1993), ISBN 0203980387, p. 2.
 ↑ "While the testable predictions of Bohmian mechanics are isomorphic to standard Copenhagen quantum mechanics, its underlying hidden variables have to be, in principle, unobservable. If one could observe them, one would be able to take advantage of that and signal faster than light, which – according to the special theory of relativity – leads to physical temporal paradoxes." J. Kofler and A. Zeiliinger, "Quantum Information and Randomness", European Review (2010), Vol. 18, No. 4, 469–480.
 ↑ Dylan H. Mahler, Lee Rozema, Kent Fisher, Lydia Vermeyden, Kevin J. Resch, Howard M. Wiseman, and Aephraim Steinberg: Experimental nonlocal and surreal Bohmian trajectories, Science Advances 19 February 2016, Vol. 2, no. 2, e1501466, doi:10.1126/science.1501466
 1 2 Anil Ananthaswamy: Quantum weirdness may hide an orderly reality after all, newscientist.com, 19 February 2016.
 ↑ Bell J. S. (1964). "On the Einstein Podolsky Rosen Paradox" (PDF). Physics. 1: 195.
 ↑ Einstein; Podolsky; Rosen (1935). "Can Quantum Mechanical Description of Physical Reality Be Considered Complete?" (Submitted manuscript). Phys. Rev. 47 (10): 777–780. Bibcode:1935PhRv...47..777E. doi:10.1103/PhysRev.47.777.
 ↑ Bell, page 115.
 ↑ Maudlin, T. (1994). Quantum NonLocality and Relativity: Metaphysical Intimations of Modern Physics. Cambridge, Mass.: Blackwell. ISBN 9780631186090.
 ↑ Allori, V.; Dürr, D.; Goldstein, S.; Zanghì, N. (2002). "Seven Steps Towards the Classical World". Journal of Optics B. 4 (4): 482–488. arXiv:quantph/0112005. Bibcode:2002JOptB...4S.482A. doi:10.1088/14644266/4/4/344.
 ↑ Valentini, Antony; Westman, Hans (2012). "Combining Bohm and Everett: Axiomatics for a Standalone Quantum Mechanics". arXiv:1208.5632 [quantph].
 1 2 3 4 5 6 7 Brown, Harvey R.; Wallace, David (2005). "Solving the measurement problem: de Broglie–Bohm loses out to Everett" (PDF). Foundations of Physics. 35 (4): 517–540. arXiv:quantph/0403094. Bibcode:2005FoPh...35..517B. doi:10.1007/s1070100420093. Abstract: "The quantum theory of de Broglie and Bohm solves the measurement problem, but the hypothetical corpuscles play no role in the argument. The solution finds a more natural home in the Everett interpretation."
 ↑ Daniel Dennett (2000). With a little help from my friends. In D. Ross, A. Brook, and D. Thompson (Eds.), Dennett's Philosophy: a comprehensive assessment. MIT Press/Bradford, ISBN 026268117X.
 ↑ David Deutsch, Comment on Lockwood. British Journal for the Philosophy of Science 47, 222228, 1996.
 ↑ See section VI of Everett's dissertation Theory of the Universal Wavefunction, pp. 3–140 of Bryce Seligman DeWitt, R. Neill Graham, eds, The ManyWorlds Interpretation of Quantum Mechanics, Princeton Series in Physics, Princeton University Press (1973), ISBN 069108131X.
 ↑ Craig Callender: "The Redundancy Argument Against Bohmian Mechanics".
 ↑ Valentini, Antony (2010). "De BroglieBohm PilotWave Theory: Many Worlds in Denial?". 'Many Worlds? Everett, Quantum Theory, and Reality', Eds. S. Saunders et Al. (Oxford University Press, ), Pp. 509. 2010 (476). arXiv:0811.0810. Bibcode:2008arXiv0811.0810V.
 ↑ P. Holland, "Hamiltonian Theory of Wave and Particle in Quantum Mechanics I, II", Nuovo Cimento B 116, 1043, 1143 (2001) online.
 ↑ Peter R. Holland: The quantum theory of motion, Cambridge University Press, 1993 (reprinted 2000, transferred to digital printing 2004), ISBN 0521485436, p. 66 ff.
 ↑ Solvay Conference, 1928, Electrons et Photons: Rapports et Descussions du Cinquieme Conseil de Physique tenu a Bruxelles du 24 au 29 October 1927 sous les auspices de l'Institut International Physique Solvay
 ↑ Louis be Broglie, in the foreword to David Bohm's Causality and Chance in Modern Physics (1957). p. x.
 ↑ Bacciagaluppi, G., and Valentini, A., "Quantum Theory at the Crossroads": Reconsidering the 1927 Solvay Conference
 ↑ See the brief summary by Towler, M., "Pilot wave theory, Bohmian metaphysics, and the foundations of quantum mechanics"
 ↑ von Neumann, J. 1932 Mathematische Grundlagen der Quantenmechanik
 ↑ Bub, Jeffrey (2010). "Von Neumann's 'No Hidden Variables' Proof: A ReAppraisal". Foundations of Physics. 40 (9–10): 1333–1340. arXiv:1006.0499. Bibcode:2010FoPh...40.1333B. doi:10.1007/s1070101094809.
 ↑ Madelung, E. (1927). "Quantentheorie in hydrodynamischer Form". Z. Phys. 40 (3–4): 322–326. Bibcode:1927ZPhy...40..322M. doi:10.1007/BF01400372.
 ↑ Tsekov, Roumen (2012). "Bohmian Mechanics versus Madelung Quantum Hydrodynamics". Annuaire de l'Université de Sofia: 112–119. arXiv:0904.0723. doi:10.13140/RG.2.1.3663.8245.
 ↑ Holland, Peter (2004). "What's wrong with Einstein's 1927 hiddenvariable interpretation of quantum mechanics?". Foundations of Physics. 35 (2): 177–196. arXiv:quantph/0401017. Bibcode:2005FoPh...35..177H. doi:10.1007/s1070100419407.
 ↑ Holland, Peter (2004). "What's wrong with Einstein's 1927 hiddenvariable interpretation of quantum mechanics?". Foundations of Physics. 35 (2): 177–196. arXiv:quantph/0401017. Bibcode:2005FoPh...35..177H. doi:10.1007/s1070100419407.
 ↑ (Letter of 12 May 1952 from Einstein to Max Born, in The Born–Einstein Letters, Macmillan, 1971, p. 192.
 ↑ Werner Heisenberg, Physics and Philosophy (1958), p. 133.
 ↑ Pauli to Bohm, 3 December 1951, in Wolfgang Pauli, Scientific Correspondence, Vol IV – Part I, [ed. by Karl von Meyenn], (Berlin, 1996), pp. 436–441.
 ↑ Pauli, W. (1953). "Remarques sur le probleme des parametres caches dans la mecanique quantique et sur la theorie de l'onde pilote". In A. George (Ed.), Louis de Broglie—physicien et penseur (pp. 33–42). Paris: Editions Albin Michel.
 ↑ F. David Peat, Infinite Potential: The Life and Times of David Bohm (1997), p. 133.
 ↑ Statement on that they were in fact the first in: B. J. Hiley: Nonlocality in microsystems, in: Joseph S. King, Karl H. Pribram (eds.): Scale in Conscious Experience: Is the Brain Too Important to be Left to Specialists to Study?, Psychology Press, 1995, pp. 318 ff., p. 319, which takes reference to: Philippidis, C.; Dewdney, C.; Hiley, B. J. (2007). "Quantum interference and the quantum potential". Il Nuovo Cimento B. 52 (1): 15. Bibcode:1979NCimB..52...15P. doi:10.1007/BF02743566.
 ↑ Olival Freire, Jr.: Continuity and change: charting David Bohm's evolving ideas on quantum mechanics, In: Décio Krause, Antonio Videira (eds.): Brazilian Studies in the Philosophy and History of Science, Boston Studies in the Philosophy of Science, Springer, ISBN 9789048194216, pp.291–300, therein p. 296–297
 ↑ Olival Freire jr.: A story without an ending: the quantum physics controversy 1950–1970, Science & Education, vol. 12, pp. 573–586, 2003, p. 576
 ↑ BG. Englert, M. O. Scully, G. Sussman and H. Walther, 1992, Surrealistic Bohm Trajectories, Z. Naturforsch. 47a, 1175–1186.
 ↑ Hiley, B. J.; E Callaghan, R.; Maroney, O. (2000). "Quantum trajectories, real, surreal or an approximation to a deeper process?". arXiv:quantph/0010020.
 ↑ A. Fine: "On the interpretation of Bohmian mechanics", in: J. T. Cushing, A. Fine, S. Goldstein (Eds.): Bohmian mechanics and quantum theory: an appraisal, Springer, 1996, pp. 231−250.
 ↑ Couder, Yves; Fort, Emmanuel (2006). "SingleParticle Diffraction and Interference at a Macroscopic Scale" (PDF). Phys. Rev. Lett. 97 (15): 154101. Bibcode:2006PhRvL..97o4101C. doi:10.1103/PhysRevLett.97.154101. PMID 17155330.
 ↑ Hardesty, Larry (12 September 2014). "Fluid mechanics suggests alternative to quantum orthodoxy". news.mit.edu. Retrieved 7 December 2016.
 ↑ Bush, John W. M. (2015). "The new wave of pilotwave theory" (PDF). Physics Today. 68 (8): 47. Bibcode:2015PhT....68h..47B. doi:10.1063/PT.3.2882. hdl:1721.1/110524.
 ↑ Bush, John W. M. (2015). "PilotWave Hydrodynamics". Annual Review of Fluid Mechanics. 47 (1): 269–292. Bibcode:2015AnRFM..47..269B. doi:10.1146/annurevfluid010814014506. hdl:1721.1/89790.
 ↑ Wolchover, Natalie (24 June 2014). "Fluid Tests Hint at Concrete Quantum Reality". Quanta Magazine. Retrieved 28 November 2016.
 ↑ Pena, Luis de la; Cetto, Ana Maria; ValdesHernandez, Andrea (2014). The Emerging Quantum: The Physics Behind Quantum Mechanics. p. 95. doi:10.1007/9783319078939. ISBN 9783319078939.
 ↑ Grössing, G.; Fussy, S.; Mesa Pascasio, J.; Schwabl, H. (2012). "An explanation of interference effects in the double slit experiment: Classical trajectories plus ballistic diffusion caused by zeropoint fluctuations". Annals of Physics. 327 (2): 421–437. arXiv:1106.5994. Bibcode:2012AnPhy.327..421G. doi:10.1016/j.aop.2011.11.010.
 ↑ Grössing, G.; Fussy, S.; Mesa Pascasio, J.; Schwabl, H. (2012). "The Quantum as an Emergent System". Journal of Physics: Conference Series. 361 (1): 012008. arXiv:1205.3393. Bibcode:2012JPhCS.361a2008G. doi:10.1088/17426596/361/1/012008.
 ↑ Bush, John W.M. (2015). "PilotWave Hydrodynamics" (PDF). Annual Review of Fluid Mechanics. 47: 269–292. Bibcode:2015AnRFM..47..269B. doi:10.1146/annurevfluid010814014506. hdl:1721.1/89790.
 ↑ De Broglie, Louis (1956). "Une tentative d'interprétation causale et non linéaire de la mécanique ondulatoire: (la théorie de la double solution)". GauthierVillars.
 ↑ de Broglie, Louis (1987). "Interpretation of quantum mechanics by the double solution theory" (PDF). Annales de la Fondation. 12 (4): 399–421. ISSN 01824295.
 ↑ Kracklauer, A. F. (1992). "An Intuitive Paradigm For Quantum Mechanics" (Submitted manuscript). Physics Essays. 5 (2): 226–234. arXiv:quantph/0008121. Bibcode:1992PhyEs...5..226K. doi:10.4006/1.3028975.
 ↑ de la Peña, Luis; Cetto, A.M. (1996). The Quantum Dice: An Introduction to Stochastic Electrodynamics. Springer. doi:10.1007/9789401587235. ISBN 9789048146468.
 ↑ Haisch, Bernard; Rueda, Alfonso (2000). "On the relation between a zeropointfieldinduced inertial effect and the Einsteinde Broglie formula". Physics Letters A. 268 (4–6): 224–227. arXiv:grqc/9906084. Bibcode:2000PhLA..268..224H. CiteSeerX 10.1.1.339.2104. doi:10.1016/S03759601(00)001869.
 ↑ Englert, BertholdGeorg; Scully, Marian O.; Süssmann, Georg; Walther, Herbert (1992). "Surrealistic Bohm Trajectories". Zeitschrift für Naturforschung A. 47 (12): 1175. Bibcode:1992ZNatA..47.1175E. doi:10.1515/zna19921201.
 ↑ Mahler, D. H; Rozema, L; Fisher, K; Vermeyden, L; Resch, K. J; Wiseman, H. M; Steinberg, A (2016). "Experimental nonlocal and surreal Bohmian trajectories". Science Advances. 2 (2): e1501466. Bibcode:2016SciA....2E1466M. doi:10.1126/sciadv.1501466.
 ↑ Mahler, D. H.; Rozema, L.; Fisher, K.; Vermeyden, L.; Resch, K. J.; Wiseman, H. M.; Steinberg, A. (2016). "Experimental nonlocal and surreal Bohmian trajectories". Science Advances. 2 (2): e1501466. Bibcode:2016SciA....2E1466M. doi:10.1126/science.1501466. PMC 4788483. PMID 26989784.
 ↑ https://www.wired.com/2016/05/newsupportalternativequantumview/
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 Holland, Peter R. (1993). The Quantum Theory of Motion : An Account of the de Broglie–Bohm Causal Interpretation of Quantum Mechanics. Cambridge: Cambridge University Press. ISBN 9780521485432.
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 Bohmian mechanics on arxiv.org
Further reading
 John S. Bell: Speakable and Unspeakable in Quantum Mechanics: Collected Papers on Quantum Philosophy, Cambridge University Press, 2004, ISBN 0521818621
 David Bohm, Basil Hiley: The Undivided Universe: An Ontological Interpretation of Quantum Theory, Routledge Chapman & Hall, 1993, ISBN 0415065887
 Detlef Dürr, Sheldon Goldstein, Nino Zanghì: Quantum Physics Without Quantum Philosophy, Springer, 2012, ISBN 9783642306907
 Detlef Dürr, Stefan Teufel: Bohmian Mechanics: The Physics and Mathematics of Quantum Theory, Springer, 2009, ISBN 9783540893431
 Peter R. Holland: The quantum theory of motion, Cambridge University Press, 1993 (reprinted 2000, transferred to digital printing 2004), ISBN 0521485436
External links
Wikiversity has learning resources about Making sense of quantum mechanics 
 "PilotWave Hydrodynamics" Bush, J. W. M., Annual Review of Fluid Mechanics, 2015
 "Bohmian Mechanics" (Stanford Encyclopedia of Philosophy)
 Videos answering frequently asked questions about Bohmian Mechanics
 "BohmianMechanics.net", the homepage of the international research network on Bohmian Mechanics that was started by D. Dürr, S. Goldstein and N. Zanghì.
 Workgroup Bohmian Mechanics at LMU Munich (D. Dürr)
 Bohmian Mechanics Group at University of Innsbruck (G. Grübl)
 "Pilot waves, Bohmian metaphysics, and the foundations of quantum mechanics", lecture course on de BroglieBohm theory by Mike Towler, Cambridge University.
 "21stcentury directions in de BroglieBohm theory and beyond", August 2010 international conference on de BroglieBohm theory. Site contains slides for all the talks – the latest cuttingedge deBB research.
 "Observing the Trajectories of a Single Photon Using Weak Measurement"
 "Bohmian trajectories are no longer 'hidden variables'"
 The David Bohm Society