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fine-structure constant

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fine-structure constant
Namefine-structure constant
Valuealpha
Unitsdimensionless quantity
Uncertaintyalpha

fine-structure constant is a fundamental dimensionless physical constant that characterizes the strength of the electromagnetic interaction between elementary charged particles. It is a crucial quantity in quantum electrodynamics and appears in formulas describing phenomena such as the fine structure of the hydrogen atom. The constant's value, approximately 1/137, has intrigued physicists for over a century due to its role in shaping the universe's structure.

Definition and value

The constant is defined as α = e²/(4πε₀ħc), where e is the elementary charge, ε₀ is the vacuum permittivity, ħ is the reduced Planck constant, and c is the speed of light in vacuum. This combination yields a dimensionless number, currently measured with high precision by institutions like the National Institute of Standards and Technology. Its recommended value in the CODATA international adjustment is approximately 0.0072973525693, with the inverse α⁻¹ being about 137.035999084. The constancy of α across time and space is a key postulate in the standard model of particle physics.

Physical significance

In atomic physics, α governs the splitting of spectral lines in atoms, known as fine structure, first observed in the hydrogen spectrum by Albert A. Michelson. It sets the scale for the strength of interactions between light and matter, influencing the energy levels of electrons bound in atoms like helium. The value of α determines the probability of events such as photon emission in quantum electrodynamics calculations performed at CERN. Furthermore, it plays a role in the Lamb shift and the anomalous magnetic dipole moment of the electron.

Measurement and precision

High-precision determinations of α employ various independent methods, creating a critical test for the consistency of physical theory. One method uses the quantum Hall effect measured in devices at the Laboratoire national de métrologie et d'essais, relating it to the von Klitzing constant. Another technique involves measuring the anomalous magnetic moment of the electron in Penning trap experiments, famously conducted at Harvard University. Atom recoil measurements from photon momentum in rubidium or cesium atoms, as done at the University of California, Berkeley, provide another route. The most precise value comes from comparing these results in the CODATA adjustment.

Theoretical interpretations

The numerical value of α, particularly why it is near 1/137, lacks a complete derivation from first principles within the standard model. Some attempts to explain it arise from grand unified theory frameworks that seek to merge the electromagnetic interaction with the weak interaction and strong interaction. The Dirac large numbers hypothesis and later work by Arthur Eddington offered speculative numerical associations. In string theory, α may relate to the vacuum expectation value of a dilaton field. The concept of a varying fine-structure constant has been explored in relation to dark energy and models like the Brans–Dicke theory.

History and development

The constant emerged from Arnold Sommerfeld's 1916 extension of the Bohr model to explain the fine structure of hydrogen; he introduced α as a dimensionless ratio. Its fundamental nature was later cemented within the development of quantum electrodynamics by figures like Richard Feynman, Julian Schwinger, and Sin-Itiro Tomonaga. The quest to measure α precisely motivated innovations such as the Josephson effect and the development of the quantum Hall effect, recognized by Nobel Prizes for Klaus von Klitzing and Brian Josephson. Debates about its constancy over cosmological time were spurred by analyses of quasar absorption lines by John K. Webb.

Role in fundamental physics

As a coupling constant, α is pivotal in defining the architecture of the observable universe. Its value influences nuclear synthesis in stars, determining the rates of processes in the proton–proton chain and the triple-alpha process inside stellar cores like that of the Sun. In particle physics, the strength of the electromagnetic interaction relative to the weak interaction is set by α and the Weinberg angle. If α were significantly different, the stability of atoms and the formation of complex structures, as studied in cosmology, would be profoundly altered, affecting the potential for life in the cosmos.

Category:Dimensionless numbers Category:Physical constants Category:Quantum electrodynamics