The generalized spin-orbit interaction: a microscopic origin of the Ørsted magnetic field
Sherif Abdulkader Tawfik
cond-mat.mes-hall cond-mat.mtrl-sci

	



sherif.tawfic@gmail.com
School of Science, RMIT University, GPO Box 2476, Melbourne, Victoria 3001, Australia







This work introduces a generalization of the form of the spin-orbit interaction, the generalized spin-orbit interaction (GSOI). It expresses the magnetic field induced by two charged particles moving with a non-zero relative velocity as a field defined at all points in space, and exists in the reference frames of both particles. This is in contrast to spin-orbit interaction theory, in which the generated magnetic field is defined at only one point in space, and exists in the reference frame of one of the two particles. At the macroscopic scale, it is shown that the GSOI theory implies the same form of the Ørsted magnetic field produced by a current-carrying wire. However, the theory is incompatible with the microscopic form of the Biot-Savart equation that implies that a charged particle induces a magnetic field by having a non-zero velocity. The implications of the GSOI theory on properties of the Ørsted magnetic field in current-carrying atomically thin two-dimensional materials, such as graphene, are discussed. The framework established in this paper aims at re-imagining classical physical concepts in light of an advanced microscopic understanding.


The generalized spin-orbit interaction: a microscopic origin of the Ørsted magnetic field
    Sherif Abdulkader Tawfik
    December 30, 2023
=========================================================================================



§ INTRODUCTION
  


The Ampere's circuital law (ACL) describes the phenomenon of the creation of the Ørsted magnetic field due to the flow of an electric current through a current carrying wire, and is described by the equation J=∇×B <cit.>. This law has been verified numerous times and has become deeply entwined in the fabric of fundamental and applied physics. It is an essential ingredient of our present understanding of the connection between the Ørsted magnetic field and the electric current. With Maxwell's addition of the displacement field term to the ACL equation, the resulting equation, Maxwell-Ampere equation, in addition to the Maxwell-Faraday equation, form a closed (yet over-determined) set of equations that constitute the classical theory of electromagnetism. ACL was even used for the definition of the ampere in terms of the induced magnetic force between two infinitely long, infinitely thin wires <cit.>. However, going back to the original equation, ACL, a question that have never been asked in the literature, to the best of my knowledge, is: given that ACL is validated for macroscopic objects, is it also validated for microscopic objects?

The first direct application of ACL to a microscopic conducting object was reported by Tetienne et al. <cit.> two years ago, where the object is a monolayer graphene nanoribbon. The induced magnetic field was measured by the nitrogen vacancy defect in diamond, and the current density was then reconstructed from the magnetic field by inverting the Biot-Savart equation, using the model developed by Roth et al. <cit.> for thin slab conductors. Tetienne et al. verified the calculated current density by integrating it, which reproduced the value of current that was initially injected into the graphene nanoribbons. However, according to the authors, the system of equations that was used to reconstruct the current density is over-determined, such that solving any two of the four equations yields results that are different from solving by other two of equations. This clearly means that the model does not accurately describe the relationship between the current and Ørsted magnetic field in such systems. Importantly, a recent work by Tetienne et al. <cit.> directly revealed an inconsistency between the Biot-Savart law and the experimental measurements. This calls for a revision of the fundamental equations describing the induction of the Ørsted magnetic field in microscopic conductors.



In fact, the application of ACL to macroscopic wire conductors has not been free from controversy. ACL was shown to suffer a logical deficiency, which is known as the Ampere tension <cit.>: for an electric current flowing through a solid conductor, the application of ACL to a conductor will divide the conductor into longitudinal current elements. Each such element induces the Ørsted magnetic field, and therefore applies a repulsive force on the neighboring elements. For any amount of current, this repulsion should lead to longitudinal forces between the current elements, or Ampere tension, that would cause the explosion of the solid conductor. This obviously defies observation. While Graneau <cit.> reasoned that this tension is the cause of explosion of solid conductors under very high current, and that the size of the smallest possible partitioning of the wire should be that of the crystal lattice unit cell, the existence of an Ampere tension necessitates the existence of lattice strain in the wire during the passage of electric current, no matter how small the current is. This, however, has never been reported experimentally. With the large supercurrent densities in superconductors, the Ampere tension would certainly entail the explosion of any superconductor.

The microscopic reduction of ACL is obtained by the Biot-Savart equation. This is derived by taking the current density J as representing the velocity of a single charged particle, qv, where q is the charge. For a non-magnetostatic systems, the Jefimenko equations <cit.> are obtained. These two equations were never verified for the case of an electron beam in vacuum. This is surprising, given that electron beams are fundamental to many devices. The Ampere tension applies to the electrons flowing in an electron beam: the Jefimenko magnetic field induced by each electron will repel the field induced by the neighboring electrons, which would imply that electrons in an electron beam will deflect sideways, which again defies observation.

This work attempts to establish a relationship between current and the Ørsted magnetic field from first principles, based on the spin-orbit interaction (SOI) theory. The SOI is a relativistic effect <cit.> in which a magnetic field couples to the spin of two charged particles when they move relative to each other. The application of SOI theory to a two-dimensional electron gas by Dresselhaus <cit.> and Rashba <cit.> has unraveled the implications of SOI on electronic transport in semiconductors, giving rise to the anomalous Hall effect (AHE) <cit.>, the spin Hall effect (SHE) <cit.> and current-induced spin polarization (CISP) <cit.>. SOI also gives rise to interesting transport properties in metals, such as the anisotropic magnetoresistance in ferromagnets <cit.> and the SHE in metals <cit.>. A critical ingredient in these technological advances has been the development of accurate theoretical models for describing the SOI in various systems, such as Rashba's phenomenological model and the incorporation of SOI into density-functional theory (DFT) implementations. Here, I present a generalization of the SOI, the generalized SOI (GSOI), which extends the applicability of the SOI theory beyond the field of spintronics. The GSOI theory can explain the induction of a magnetic field in conducting wires due to the passage of an electric current, and is applicable to the macroscopic as well as the microscopic scales.



§ THE SPIN-ORBIT AND THE SPIN-OTHER-ORBIT INTERACTION
  

For two charged particles, A and B, with different velocity vectors v_A and v_B, the SOI, as derived from the special theory of relativity, is the interaction between the velocity of A and the magnetic field that A experiences in its own rest frame. This induced magnetic field will couple with the spin of A, μ_A, according to the spin-orbit coupling energy,

    H_SOI=-μ_A·B_A.


The induced magnetic field in the rest frame of particle i (i=A,B), B_i, is given by 

    B_SOI,i   =   -1/c^2(v_i-v_j)×E
       =   -1/c^2(v_i-v_j)× q_jr_i-r_j/| r_i-r_j| ^3

where v_i is the velocity of particle i and c is the speed of light. For illustration, the schematic in Fig. <ref>(a) shows the direction of the field induced in the reference frame of an electron moving next to an atom, as well as the field induced in the reference frame of the atom due to the motion of the electron.
	
The magnitudes and directions of B_SOI,A and  B_SOI,B depend on the charges of the two particles, q_A and q_B. If q_A=q_B, then B_SOI,A=B_SOI,B, such as for the case of two electrons moving relative to each other. For an electron moving with respect to an ion and experiencing its effective nuclear charge, the two fields are opposite in direction, and the magnitude of the field acting at the position of the electron will be larger than that acting at the position of the ion.

The field B_SOI,A has has no source, and there are no field lines except the field vectors defined at the positions of particle A and B. The theory of the SOI only accounts for the effect of the transformed field at the position of the particles, but does not aim at establishing a vector field in the reference frames of the particles. 














The SOI coupling hamiltonian in Eq. <ref> can be derived from the solution of the Dirac equation up to 1/c^2 order. The Dirac hamiltonian was then extended by Breit <cit.> to account for the effect of retardation on two Dirac particles. Of interest to the present work is the spin-other-orbit interaction (SOOI) in the Breit hamiltonian H_SOOI for two particles A and B, which is given by <cit.>


    -e^2/m^2c^21/4πϵ_0μ_B· (r_A-r_B)×p_A+  μ_A· (r_B-r_A)×p_B/|r_A-r_B|^3


where p_i, is the particle's momentum vector, i=A,B, r_i is its position vector, and μ_i is its spin operator vector. This terms can be interpreted as the energy required to align the spin operator vector of each particle with the magnetic field induced by the other particle (that is why it is called spin-other-orbit interaction). 

This property makes H_SOOI fundamentally different from H_SOI in Eqs. <ref> and <ref>. In SOI, the induced magnetic field at the reference frame of particle A couples with the spin of particle A, μ_A but this field is not observable in the reference frame of particle B. In the case of H_SOOI in Eq. <ref>, the magnetic field induced in the reference frame of particle A couples with the spin of particle B, μ_B. This means that the Breit interaction theory implicitly makes the induced SOI magnetic field observable in the reference frames of both particles.

Based on the above, I propose a generalization for the form of the magnetic field induced by the SOI, the generalized spin-orbit interaction (GSOI) theory. 





§ THE GENERALIZED SPIN-ORBIT INTERACTION THEORY


In the GSOI theory, the magnetic field vector induced by the motion of a charged particle relative to another charged particle, B_SOI,ij (Eq. <ref>), is a magnetic field that exists in the reference frame of each of the two particles. That is, the field B_SOI,ij in the reference frame of one particle, A, is observable in the reference frame of the other particle, B. The form of the field B^0_GSOI,ij is mathematically similar to that of B_SOI:


    B_GSOI,ij(r)   =   B_SOI,ij  B_d,ijB_r(| r_i-r|)   , 
    
    B_d,ij   =   e^-k| r_i-r_j|  ,  
    
    B_rad(| r_i-r|)    =   κ/| r| +κ



where q_j is the charge of particle j, B_SOI,ij is given by Eq. <ref>, B_d,ij is the exponential decay of the electric field inside a conductor due to charge screening, B_rad(r) represents the radiation of the SOI magnetic field line, and κ is a decay constant in units of 1/Å.

The form of B_GSOI,ij(r) satisfies the following two conditions:


	
  * At the positions r_A and r_B of two charged particles A and B moving with non-zero relative velocity, B_GSOI(r)_i takes the form of Eq. <ref> by substituting r=r_i. That is, the GSOI field reduces to the SOI field at the positions of the two particles inducing the field.
	
  * For positions in space other than r_A and r_B,  B_GSOI(r)_i ∼ 1/r, where r=|r|.


The GSOI field B_GSOI,ij(r) complements the theory of SOI by defining a magnetic radiation field. The radiation source is the particle that is experiencing a point B_SOI,ij magnetic field.



Equation <ref> is illustrated by the schematic diagram in Figs. <ref>(b), showing electrons moving due to the application of an electric potential along the conductor's axis. The motion of the various electrons, labeled as e_1, e_2 and e_3, generates the GSOI field. The e_1 electron moves in the charge cloud surrounding the surface of the conductor, e_2 moves right below the surface while e_3 moves close to the center of the current-carrying wire. The e_1 electron experiences an interaction with the ions on the surface of the current-carrying wire, thus generating the GSOI field. The e_3 electron, on the other hand, does not contribute to the GSOI field because the generated field due to interactions with ions above it cancels out the GSOI field generated due to its interaction with ions below it. This cancellation becomes weaker as we approach the surface of the conductor, such as the case of e_2. Therefore the motion of the e_2 electron generates a non-negligible GSOI field. Thus, the closer an electron is to the surface of the conductor, the larger is the B_GSOI field it creates; the closer it is to the center, the weaker is the B_GSOI field it creates. 

























§ APPLICATION TO NANOMATERIALS




For the case reported in Ref. <cit.>, in which a conducting strip had a width of 10 μ m and thickness of 100 nm, the application of the Biot-Savart law deviated from the experimental measurement. For a conducting strip axis along the x-axis and with the z-axis normal to its plane, the experimentally measured  B_z field at the strip edge is smaller than the  B_BS,z calculated by the Biot-Savart law. 

In an attempt to use the GSOI theory to explain the form of the B_z field for the conducting strip, Fig. <ref>(e) compares the B_GSOI,z field against the Biot-Savart field  given by B_BS,z(x)=μ_0 I/4π w ln| x+w/2| /| x-w/2|, where I is the current flowing along the y-axis, and w is the width. The B_GSOI,z field at the strip edge is smaller than the B_BS,z, which is similar to the experimental measurement in Ref. <cit.>. While the plot in Fig. <ref>(e) is for a strip that is 120 nm, which is much smaller than the strip in Ref. <cit.> that is 10 μm wide, the behavior of B_GSOI,z and B_BS,z at the strip edge will be similar because of the asymptotic behavior of B_BS,z at the edge.


For the case of graphene, Fig. <ref>(e) displays the slab structure of a graphene nanoribbon. In a graphene nanoribbon that is suspended in vacuum, there are two conducting systems:

	
  * The two infinitely-thin conducting slabs, which are the π bond networks above and below the hexagonal carbon atoms and both are two-dimensional: These two networks are filled by electrons occupying the p_z orbital of the carbon atoms, and therefore a p_z electron is equally likely to occupy either π bond network, the top or the bottom. Only the p_z orbitals of graphene are the ones that contribute to the calculation of the SOI in graphene <cit.>. Therefore, only the π bond networks will contribute to the GSOI field generation.
	
  * The nanoribbon edge which is one-dimensional: as discussed above, the edge supports a persisting edge state that sustains the nanoribbon conduction current.


For a graphene sheet to which the z-axis is normal and through which a current flows along the +x direction, the two π-bond layers each induce a B_GSOI,t/b (where t stands for top, b for bottom) that is strictly in the direction of the +y-axis. The superposition of the top and bottom B_GSOI results in the total induced B_GSOI,y component of the field that is less than the B_GSOI,y component induced by each π-bond network alone. The B_GSOI,z component of the field, however, is enhanced by the superposition of the GSOI field across the width of the nanoribbon, as is displayed in Fig. <ref>(h). B_GSOI,z is also enhanced by the larger linear current density flowing through the edge of the nanoribbon.



























§ A MICROSCOPIC ORIGIN OF AMPERE'S CIRCUITAL LAW



A discussion of a possible microscopic origin for the Ørsted magnetic field actually took place in the years following Ampere's publication of the Ampere force law (AFL) <cit.>. AFL proposes an empirical action-at-a-distance formula between the electric current passing through two wires, the distance between the wires and the force induced by each wire on the other. In spite of its simplicity and experimental validation, its interpretation was problematic ever since it was published. While Ampere believed that his equation describes a fundamental law of the nature of the electric current, which he generalized to state that magnetism in magnetic materials arises due to the presence of microscopic currents, Biot and Savart proposed an alternative interpretation, the wire magnetization hypothesis (WMH) <cit.>. According to the WMH, the magnetic field in the current-carrying conductor arises because the wire itself becomes magnetized. Thus, the magnetic field does not arise from a moving charge, but instead arises from the lining up of microscopic magnetic particles around the circumference of the wire. This interpretation was criticized by Ampere <cit.>, and was not endorsed by the physics community. If that interpretation was true, however, the idea that a moving charge induces a magnetic field would have to be dropped, since that induction is only a result of the response of the material in the current-carrying conductor to the passing electric current. For the originators of WMH, this conclusion would actually contradict with the application of their own equation (the Biot-Savart equation) to the case of a moving charged point particle.

The WMH that is solely based on the alignment of microscopic magnetic dipoles through the current-carrying conductor is in fact problematic because the resulting force between two current-carrying conductors would scale as r^-4, which is the force between two dipoles separated by distance r, whereas the observed magnetic force between two current-carrying conductors scales as r^-2.

The GSOI theory proposed in this work derives the Ørsted magnetic field from a first principles theory. GSOI therefore re-introduces the WMH in terms of modern theoretical foundations. The GSOI theory proposes that the Ørsted magnetic field is a material, rather than a field property; the field only emerges when an electric current passes through a conducting medium, not solely due to the motion of charge. 

Would the GSOI theory affect the theory of field-particle interaction? This is not the case, because the field-matter interaction term, qp·A, where q is the particle's charge, p is the particle momentum and A is the vector potential, is fully derivable by constructing the wave-particle Lagrangian based on three ingredients, the Maxwell-Faraday equation, the relationship B=∇×A and the Lorentz force equation. None of these ingredients depend on the Maxwell-Ampere equation.

	


§ CONCLUSION 
 

The generalized spin-orbit interaction (GSOI) theory is proposed. It expresses the magnetic field induced by two charged particles moving with a non-zero relative velocity as a field defined at all points in space. This is in contrast to spin-orbit interaction theory, in which the generated magnetic field is defined at only one point in space, and is observable in the reference frame of only one of the two particles. When applied to a current-carrying wire, the GSOI theory can reproduce the Biot-Savart form of the Ørsted magnetic field. Hence, GSOI can potentially replace the Maxwellian conception of Ørsted magnetic induction, in which a single moving point charge induces a magnetic field. 






99
	
Jackson  John David Jackson, Classical Electrodynamics (3rd ed.). New York: Wiley (1999).
Maxwell1  James Clerk Maxwell, Phil. Tran. Royal Soc. Lond. 155, 459-512, (1865).
SI NIST Special Publication 330, 2008 Edition, Barry N. Taylor and Ambler Thompson, Editors.
NV Jean-Philippe Tetienne, Nikolai Dontschuk, David A. Broadway, Alastair Stacey, David A. Simpson, Lloyd C. L. Hollenberg, Quantum imaging of current flow in graphene, Sci. Adv. 3, e1602429 (2017).
2DCurrent Bradley J. Roth, Nestor G. Sepulveda, and John P. Wikswo, Jr., Using a magnetometer to image a two-dimensional current distribution, J. Appl. Phys., 65, 361 (1989).
NV_Problem J.-P. Tetienne, N. Dontschuk, D. A. Broadway, S. E. Lillie, T. Teraji, D. A. Simpson, A. Stacey, and L. C. L. Hollenberg, Apparent delocalization of the current density in metallic wires observed with diamond nitrogen-vacancy magnetometry, Phys. Rev. B 99, 014436 (2019).

Tension Peter Graneau, First indication of Ampere tension in solid electric conductors, Phys. Lett. 97A, 6 (1983).
Tension2 A. E. Robson and J. D. Sethian, Railgun recoil, ampere tension, and the laws of electrodynamics, Amer. J. Phys. 60, 1111 (1992).
Tension3 Peter Graneau, Ampere Tension in Electric Conductors, IEEE Trans. Mag. Mag-20, 2 (1984).
Jefimenko Oleg D. Jefimenko, Direct calculation of the electric and magnetic fields of an electric point charge moving with constant velocity, American Journal of Physics 62, 79 (1994).

Dresselhaus G. Dresselhaus, Spin-Orbit Coupling Effects in Zinc Blende Structures, Phys. Rev. 100, 580–586 (1955).
Rashba Y. A. Bychkov,  and E.I. Rasbha, Properties of a 2D electron gas with lifted spectral degeneracy, P. Zh. Eksp. Teor. Fiz. 39, 66–69 (1984).
AHE Crepieux, A.  and P. Bruno, Theory of the anomalous Hall effect from the Kubo formula and the Dirac equation. Phys. Rev. B 64, 014416. (2001).

SHE1 Y. K. Kato, R. C. Myers, A. C. Gossard, D. D. Awschalom, Observation of the Spin Hall Effect in Semiconductors, Science 306, 1911 (2004).
SHE2 M. I. Dyakonov, and V. I. Perel, Possibility of orienting electron spins with curent, ZhETF Pis. Red. 13, 657-660 (1971).
CISP3  Y. K. Kato, R. C. Myers, A. C. Gossard, and D. D. Awschalom, Current-Induced Spin Polarization in Strained Semiconductors, Phys. Rev. Lett. 93, 176601 (2004).
AMR T. McGuire and R. Potter, Anisotropic magnetoresistance in ferromagnetic 3d alloys, IEEE Trans. Magnet. 11, 1018-1038 (1975).
SHE3  A. Hoffmann, Spin Hall Effects in Metals, IEEE Trans. Magn. 49, 5172-5193 (2013).

Breit G. Breit, Dirac's Equation and the Spin-Spin Interactions of Two Electrons, Phys. Rev. 39, 616 (1932).
Breit2 M. D. Stiles, S. V. Halilov, R. A. Hyman, and A. Zangwill, Spin-other-orbit interaction and magnetocrystalline anisotropy, Phys. Rev. B, 64, 104430 (2001).



RashbaGraphene Hongki Min, J. E. Hill, N. A. Sinitsyn, B. R. Sahu, Leonard Kleinman, and A. H. MacDonald, Intrinsic and Rashba spin-orbit interactions in graphene sheets, Phys. Rev. B 74, 165310 (2006).







Assis Andre Koch Torres Assis and J. P. M. C. Chaib. Ampère's Electrodynamics: Analysis of the Meaning and Evolution of Ampere's Force Between Current Elements, Together with a Complete Translation of His Masterpiece: Theory of Electrodynamic Phenomena, Uniquely Deduced from Experience, C. Roy Keys Incorporated, 2015.


BiotSavart1 J. B. Biot  and F. Savart, Note sur le magnetisme de la pile de Volta, Annales de Chimie et de Physique, 15,222-223 (1820).
BiotSavart2 J. B. Biot, Precis elementaire de Physique experimentale, volume II. Deterville, Paris (1821).
BiotSavart3 J. B. Biot, Sur l Aimantation imprimee aux metaux par lelectricite en mouvement: lu a la seance publique de l Academie des sciences, J. des Savants, 221-235 (1821).











