effect

spin orbit coupling

Coupling between electron spin and orbital motion in quantum materials.
59 related articles · 6 formulas

Description

Spin-orbit coupling is a fundamental interaction in quantum physics where an electron's intrinsic angular momentum (its 'spin') is coupled to its motion through space (its 'orbital' angular momentum). This coupling arises from relativistic effects: from the electron's perspective, the electric field of the atomic nucleus appears as a magnetic field, which interacts with the electron's magnetic moment associated with its spin. This interaction is crucial for understanding the fine structure of atomic spectra, the electronic properties of solids, and the behavior of materials used in quantum technologies. It is the key mechanism behind phenomena such as the anomalous Hall effect, topological insulators, and the manipulation of quantum states in diamond-based sensors.

History

The concept of spin-orbit coupling was introduced to explain the fine structure of atomic spectra in the 1920s, with key contributions from Gregory Breit, Llewellyn Thomas, and others. It was later incorporated into the Dirac equation, which naturally describes the interaction.

How it works

In an atom, an electron moving around the nucleus experiences a magnetic field due to its own orbital motion (in its rest frame). This magnetic field interacts with the electron's spin magnetic moment, creating an energy shift that depends on the relative orientation of the spin and the orbital angular momentum. The strength of this coupling scales with the atomic number (Z) to the fourth power, making it much stronger in heavy elements. In solid-state materials, spin-orbit coupling can lead to a mixing of spin and momentum states, allowing electric fields to control spin orientation—a principle used in spintronics. In diamond with nitrogen-vacancy (NV) centers, spin-orbit coupling influences the energy levels of the defect, enabling optical readout of the spin state, which is essential for quantum sensing.

In practice

Spin-orbit coupling is exploited in spintronic devices for data storage and processing, in topological insulators for dissipationless electronics, and in diamond quantum sensors for high-precision magnetometry and thermometry.

Fun fact

The strength of spin-orbit coupling in a material can be tuned by applying strain or electric fields, allowing researchers to switch a material between being a conventional conductor and a topological insulator.

Concept graph →

Formulas

$$\Omega = \frac{1}{2m^2c^2}$$
Berry curvature for a free electron in vacuum.
What is in the formula
\OmegavariableBerry curvature — berry curvature square metre
mvariableelectron mass — mass kilogram
cvariablespeed of light in vacuum — speed metre per second
ω=\frac{1}{2m^2c^2} · 2506.01292v2
$$ rac{m_1 oldsymbol{\chi}_1 oldsymbol{\cdot} oldsymbol{L} + m_2 oldsymbol{\chi}_2 oldsymbol{\cdot} oldsymbol{L}}{m_1 + m_2}$$
Weighted average of spin projections onto the orbital angular momentum.
What is in the formula
m_1variablemass of the first compact object — mass kilogram
m_2variablemass of the second compact object — mass kilogram
\boldsymbol{\chi}_1variabledimensionless spin vector of the first object — dimensionless spin
\boldsymbol{\chi}_2variabledimensionless spin vector of the second object — dimensionless spin
\boldsymbol{L}variableunit vector along orbital angular momentum — unit vector
\cdotoperatorcomputes the scalar projection of one vector onto another — dot product
χ_{\rmeff}=\frac{m_1χ_1\cosθ_1+m_2χ_2\cosθ_2}{m_1+m_2} · 2607.00565v1
χ_{\rmeff}\simeq\frac{m_{\rmbh}}{m_{\rmns}+m_{\rmbh}}χ_{\rmbh}\cosθ_{\rmbh} · 2607.16136v2
$$v_c = \sqrt{\frac{G M}{r}}$$
Orbital speed for circular motion around a central mass.
What is in the formula
v_cvariableCircular orbital speed — velocity metre per second
MvariableCentral mass — mass kilogram
rvariableOrbital radius (distance from center of mass) — radius metre
GconstantNewtonian gravitational constant — gravitational constant = 6.67430e-11 metre cubed per kilogram per second squared
v_c(r)=\sqrt{\frac{g_nm_{{tot}}}{r}} · 2607.14450
$$\hat{H}_{\text{ex}} = J (\hat{\sigma}_+ \hat{\sigma}_- + \hat{\sigma}_- \hat{\sigma}_+)$$
Exchange interaction couples spin raising and lowering operators.
What is in the formula
Jvariableexchange coupling constant — exchange coupling constant joule
σ₊variablespin raising operator — spin raising operator
σ₋variablespin lowering operator — spin lowering operator
\hat{h}_{{eff}}=\lambda_{{nt}}(\hat{σ}_{+}\hat{σ}_{t}^{-}+\hat{σ}_{t}^{+}\hat{σ}_{-}) · 2505.00266v1
$$S = \frac{1}{16\pi G} \int d^4x \sqrt{-g} \, R$$
The action for general relativity in curved spacetime.
What is in the formula
SvariableAction — action joule second
gvariableDeterminant of the metric tensor — metric determinant
RvariableRicci scalar curvature — ricci scalar reciprocal metre squared
d^4xvariableFour-dimensional spacetime volume element — spacetime volume element metre to the fourth
GconstantNewton's constant of universal gravitation — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
\intoperatorIntegration over spacetime — integral operator
s=\frac{1}{16π}\intd^4x\sqrt{-g}(r-2(\nabla\varphi)^2+2λ\varphir^2_{gb}) · 2605.04224v1
s=\intd^4xh[-\frac{t}{2\kappa}-\xi\phi^*\phit+\mathcal{l}_m] · 2607.02017v1
$$H(\mathbf{k}) = \sum_{\alpha} c_{\alpha}(\mathbf{k}) \Gamma_{\alpha}$$
Hamiltonian for electrons in periodic lattice.
What is in the formula
HvariableHamiltonian matrix in momentum space — hamiltonian joule
kvariableCrystal momentum vector — crystal momentum kilogram metre per second
c_αvariableCoefficient function for each Γ_α term joule
Γ_αvariableMatrix representing hopping and on-site terms
∑operatorSum over all relevant terms α — summation
h({k})=(m+t\sum_i\cosk_i)τ_zσ_0+λ\sum_i\sink_iτ_xσ_i+m(\cosk_x-\cosk_y)τ_yσ_0 · 2607.04358
h_{\rmeff}=-j\sum_{j}(|w_j\rangle\langlew_{j+1}|+h.c.)+\sum_jε_j|w_j\rangle\langlew_j| · 2607.07225

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