Advances in Condensed Matter Physics

Volume 2018 (2018), Article ID 1618252, 7 pages

https://doi.org/10.1155/2018/1618252

## Gravitation at the Josephson Junction

Department of Condensed Matter Physics, Sofia University, 5 Boul. J. Bourchier, 1164 Sofia, Bulgaria

Correspondence should be addressed to Victor Atanasov; moc.liamg@osanatav

Received 3 November 2017; Accepted 21 December 2017; Published 1 February 2018

Academic Editor: Jörg Fink

Copyright © 2018 Victor Atanasov. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

#### Abstract

A geometric potential from the kinetic term of a constrained to a curved hyperplane of space-time quantum superconducting condensate is derived. An energy conservation relation involving the geometric field at every material point in the superconductor is demonstrated. At a Josephson junction the energy conservation relation implies the possibility of transforming electric energy into geometric field energy, that is, curvature of space-time. Experimental procedures to verify that the Josephson junction can act as a voltage-to-curvature converter are discussed.

#### 1. Introduction

The success of the Laser Interferometer Gravitational Wave Observatory (LIGO) and its sister collaboration, VIRGO [1, 2], in observing the geometric field’s ripples in space-time has, in addition to opening a new experimental method of astrophysical observation, proved a practical scheme for measuring the space-time metric; that is, LIGO had seen the death spiral of a pair of black holes, through the dislocation and the associated change in optical (and physical) path travelled by light beams in the arms of an interferometer as the gravitational perturbation travels between the reflection points. In theory, the geometry of space-time, that is, the components of the Riemann curvature tensor, can be reconstructed by taking measurements of the deviation of two adjacent light paths (geodesics) [3, 4].

Bearing in mind this spectacular success in experimental astrophysics, we pose the following questions:* (i) Are there other experimentally relevant strategies for detecting space-time geometry? (ii) Is there other extremely sensitive measurement technique besides two-light beam interference that can potentially sense the geometric field?* The present paper aims to answer both questions and is organised as follows. The first section discusses the appearance of a geometric potential term from the kinetic energy term in the Schrödinger equation. In order to improve on the detection possibilities we assume this constrained to a hyperplane quantum dynamics to concern a superconducting condensate. The second section focuses on the hydrodynamic interpretation of the governing quantum equation and reveals that the geometric field enters it on an equal footing with the “quantum potential” (in Bohm’s views), thus making its way as a real force moving the condensate superfluid. The third section contains the proof that the emergent geometric field enters an energy conservation relation valid at each point of the superconducting condensate. Based on this conservation relation applied to a Josephson junction, an experimentally verifiable voltage-to-curvature conversion effect is proposed in the fourth section. The fifth section discusses possible experimental methodologies to test the reality of the effect.

#### 2. The Geometric Field in the Schrödinger Equation

The general theory of relativity conveyed an understanding of phenomena such as the distortion of time-space by a gravitational or acceleration field [5]. However, the manner in which the curvature of space-time, that is, the Riemannian space, affects the electronic properties of condensed matters systems on a microscopic scale is largely unknown and due to its experimental accessibility is of great interest [6, 7].

Riemannian geometric effects in a quantum system, which can either be free or constrained, stem from the dependance of the kinetic term on the metric of the embedding space or the metric of the submanifold onto which the quantum system is constrained by a confining potential (rigid chemical bond; electrostatic attraction).

The problem of constraining particle motion to a curved submanifold embedded in a Euclidean space can be resolved in one of two alternative ways. (i) In the* intrinsic* quantization approach, the motion is constrained to the curved submanifold in the first place. A Hamiltonian is constructed from generalised coordinates and momenta intrinsic to the submanifold and the system is quantized canonically. As a result, the embedding space is inaccessible and the quantum system depends only on the geometry intrinsic to the submanifold/hyperplane [8–11]. (ii) In the* confining* potential approach, a free in the embedding space quantum particle is subjected by a normal force to the submanifold force that in effect confines the dynamics in it. The effective Hamiltonian depends on the intrinsic geometry and on the way this submanifold is immersed in the embedding space.

On one hand, the intrinsic quantization procedure is plagued with ordering ambiguities that allow for multiple consistent quantization procedures different by a term proportional to the curvature of the submanifold [10–14]. On the other hand, the confining potential procedure leads to a unique effective Hamiltonian that depends on the constraint. In real microscopic quantum systems, constrained motion is a result of a strong confining force (electrostatic, rigid chemical bonds, etc.). Therefore, confining potential formalism seems a physically more realistic approach to constraints [15–25].

The nonrelativistic quantum mechanics in a three-dimensional hyperplane of the four-dimensional curved space-time can be treated in a well established manner [14]. In this case the embedding space-time is non-Euclidean but equipped with a metric. This four-dimensional metric is related to the matter distribution by the Einstein equation. Suppose the four-dimensional space-time is topologically the product , where represents a space-like three-dimensional hyperplane. We can then foliate by a one-parameter family of embeddings given by the map such that , which means that is the image of the map in for a fixed “time” We assume that the leaves are space-like with respect to the metric in As a result, there exists in a time-like field normal to the leaves , and therefore there is a notion of future and past. This time evolution vector field, , satisfies , so that local coordinates (satisfying , for ) can be introduced. In effect, the space-time is splittable into 3 + 1 dimensions and the induced Riemannian metric onto the three-dimensional can be used to write the Laplace-Beltrami operator , which is the kinetic energy term in the Schrödinger equation for the subjected to the geometric field quantum particle or quantum condensate:

The emergence of the geometric field from the kinetic term can be made clearer in the vicinity of the origin where the following Taylor expansion of the induced metric in normal coordinates applies: (in fact, Riemann used the expansion of a metric in normal coordinates to originally define the curvature tensor; in normal coordinates there is no necessity to distinguish between co- and contravariant indices; see [26, 27]), and expanding the square root of the determinant of the metric yields Using a standard renormalisation of the wave-function and keeping the lowest order terms (the only relevant for the quantum dynamics) in the Taylor expansion we get for the kinetic term in the Schrödinger equation Here is the Laplacian on flat space. Adding an additional potential that may act in the system we convey the complete symbolic equation with which we will further work: Here where is the three-dimensional Ricci scalar curvature and is a numeric coefficient. The emergence of a geometric potential from the kinetic term is obvious. Such a term is a standard coupling term between curvature and a quantum field in quantum field theory in curved space-time.

Note that the particular form of the geometric potential may vary and in the case of a constraining potential approach it takes the expressions: (i) , where is the principle curvature of a space curve embedded in [17, 18, 20, 21]; (ii) , where , for , are the principle curvatures of a surface embedded in [15–18]; (iii) , where , for , are the principle curvatures of a three-dimensional manifold embedded in [23–25].

When electric field (defined with the potential ) and magnetic field, defined through the vector potential , are present the Schrödinger equation takes the following form:

#### 3. Hydrodynamic Interpretation of the Condensate Wave-Function

Suppose that we deal with a Cooper pair condensate inside a superconductor. The Schrödinger equation for the Cooper pair will be (6) with , that is, twice the charge of the electron. This equation will describe the state of the entire condensate. Therefore, we may write , where is the charge density of the condensate and is its phase. Upon substitution of this form of the wave-function into (6) we can separate the real and imaginary part of the equation to arrive at slightly modified standard result: Here is the current density, which in the case of a superconducting condensate stands also for the probability current. The generalised momentum is contained in the expression for , and therefore the current density is just the velocity of the superconducting current times the charge density.

Taking the gradient of the whole equation (8) and expressing from (7) (akin to [28]) we obtain the modified version of the hydrodynamic interpretation of the quantum condensate dynamics: where is the Lorentz force acting on the charged Cooper pairs. These two equations are the equations of motion of the superconducting Cooper pair fluid in the presence of an induced curvature (from the embedding space-time), which in this paper is referred to as geometric field. Note that the geometric field enters the gradient of the mystical quantum mechanical potential, recognised by Bohm as a unique interaction with the field itself [29, 30]. As a result, the geometric field and the field (in view of Bohmian quantum mechanics) have similar and competing action.

Next we recall the London equations for the quantum superconducting current density [31] where (see eq. in [28]). For brevity we will call the introduced quantity , which can be either of scalar or tensorial character, the polarisation operator. A correct microscopic theory of superconductivity can produce an expression for it in terms of the energy gap and critical temperature [32, 33].

Note that an important issue needs to be addressed, namely, to what extent the London equations hold in curved space-time. The above London equation is implicitly contained in the Schrödinger equation within the form of the canonical momentum. However, in the curved space case, the canonical momentum (7) coincides with the flat space case (see [28]); therefore we will not seek any generalisation of (11). An additional reinforcement of this choice comes from the original London brothers’ derivation; namely, the supercurrent is being accelerated under the influence of external electromagnetic fields as if made up of free charged particles. Therefore in curved space-time , where is the electromagnetic tensor [34]. Reducing the above to the space part and using (2) within the zero-th order in the vicinity of the origin (the same approximation as the one used in the derivation of (6)) we obtain , which coincides with the flat space case; therefore the second London equation (produced by taking a curl from this one) should also coincide with the flat space one, that is, (11). London equations are grounded in the electrodynamics of the superconductor and more specifically the phenomenological description of its ideal diamagnetism. We do not have any indication that this material property is rendered invalid in curved space-time.

In addition, the London theory can be viewed as a limit (the London limit) of the phenomenological Ginzburg-Landau theory, which in the case of curved space-time is extended with an extra term encoding the interaction with the geometric field, besides the standard extension of the covariant derivatives, to include the Christoffel symbols [35, 36]. The supercurrent operator emerging from this approach coincides with (7) (see eq. from [35, 36]); therefore the above conclusion on the validity of the London theory in curved space-time is preserved. London theory remains valid also in the case of the gravitoelectromagnetic approximation to the Einstein field equations [37, 38].

Next, we divide both sides of (11) by the current density and then differentiate with respect to time only to equate the r.h.s. of (9) with the r.h.s. of (12):

#### 4. The Geometric Effect

In the case when the superconducting state is robust, we may assume that the current density in the superconductor is approximately constant as well as the polarisation operator (no internal changes in the microscopic mechanism). The ideal diamagnetism of the superconducting state reduces the Lorentz force to its electrostatic part, which is nonvanishing only in the case when a Josephson junction is present (two separated conducting domains at different electrostatic potentials). Finally, the above simplifications yield which is simply an expression for the conservation of energy.

Let us take a line integral of the above along an open path from point to point : Next we introduce the geometric field energy Recall that , which means that is the electromotive potential difference between the two points and Finally (16) can be rewritten using (7) as Now, suppose the Cooper pair charge velocity is constant at the two adjacent points; then the last integral quantity measures the difference in the interaction energy between the Cooper pairs and the vector potential at the two points: Introducing the electrostatic energy we can put (16) in its final form As a result of introducing the scalar polarisation operator from (11) and [39], the following conserved quantity at each material point of the superconductor emerges: Here is the electrical energy of the Cooper pairs.

#### 5. Direct and Reversed Effect

In the previous section we have seen that the geometric field is equivalent to an electric field in the superconductor (15) the statement of which is analogous to the law of conservation of energy (25). Therefore, provided the superconducting element is homogeneous, we can expect and as a result of the perfect conductor aspect of the superconducting state, we can also expect a redistribution of the shift by the geometric field charges inside the superconductor in order to maintain the superconductor at a constant potential.

A completely different behaviour can be expected at the Josephson junction. We will discuss two cases of the junction, one between superconducting sides made from the same superconductor (symmetric) and one between two different superconductors (asymmetric).

Clearly, in the symmetric junction, the interaction energy will be the same on both sides. However the electrostatic potential on the two sides can be different and the voltage drop can be equated to the geometric potential, that is, the curvature scalar itself. In effect, the difference in the geometric field between the two sides can produce a voltage drop at the junction (direct effect) or the voltage drop across the junction can produce curvature difference (reversed effect): In this case, we may regard the Josephson junction as a curvature-to-voltage converter with the following ratio ( is the free electron mass): Note, the only difference the asymmetric junction can introduce is the difference in the interaction energy between the supercurrent and the electromagnetic field at the two sides of the junction. Suppose the supercurrent flows in the junction at vanishing potential difference ; then the interaction energy gradient can produce rippling in the geometric field according to The interaction energy (20) is a function of the supercurrent drift velocity and one may view the asymmetric effect as produced by a sharp change in momentum, which converts into rippling of the geometric field. We may expect a backreaction on the entire junction as well. The kinetic energy of the bulk material can certainly be included in (25). The backreaction will increase with the increase in the difference between the interaction energy of the supercurrent with the electromagnetic field on both sides.

#### 6. Proposed Experimental Verification

An argument that the Josephson junction can act as a reversible curvature-to-voltage converter was presented in the previous section. In effect, the argument is prone to experimental testing and now we will discuss how and to what extent. Note that the conversion factor (25) points to the impossibility to observe the travelling ripples in space-time, that is, gravitational waves, with a Josephson junction. Along the span of the junction (few angstrom [Å]) the expected difference in the induced scalar curvature is very small []; therefore according to (25) we may not hope for potential difference greater than [V] which is unmeasurable. We are in a position to answer the questions from the introduction. We are unable to sense the geometric field produced by a gravitational wave at the Josephson junction.

However, since we expect that the effect is reversible, we may attempt to create a geometric field at the junction by an electric discharge between its sides. The greater the potential difference that can be created between the sides, the greater the geometric field that could be created. We are unaware of the dynamics of the created geometric field and do not have any governing equations at the present stage of discussion on its propagation. Nevertheless, we can propose two detection methods which in theory can confirm the proposed effect.

The first approach stems from the reversibility argument; see Figure 1(a). Suppose we have two junctions in close proximity. We have no firm reason to choose a particular set-up but choose to discuss the idea of the experiment with the two junctions placed along a line in such a way that the plane of the junctions (the insulating layer) is normal to the imaginary line connecting them. Both junctions should be magnetically and electrically shielded from each other and the surrounding environment. One of them will serve as an emitter and the other as detector. A high-voltage discharge should be conducted in the emitter and an induced voltage drop should be recorded at the detector. Provided such an electric potential difference is recorded via proper coincidence scheme (an additional detector junction involved), we may confirm that the geometric effect at the Josephson junction is a physical reality.