Does QED have any real-world applications?

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SUMMARY

Quantum Electrodynamics (QED) has several real-world applications, particularly in atomic spectroscopy and laser-based chemistry. The Lamb shift, while a notable QED effect, is not the only consequence of QED; it is essential for high-accuracy spectral calculations and understanding phenomena like the color of gold and the liquid state of mercury at room temperature. Additionally, the cavity-QED regime is significant in the semiconductor laser industry, enhancing spontaneous emission rates. Overall, QED plays a crucial role in accurately describing interactions at the quantum level, particularly in complex systems.

PREREQUISITES
  • Understanding of Quantum Electrodynamics (QED)
  • Familiarity with atomic spectroscopy principles
  • Knowledge of laser-based chemistry
  • Basic concepts of quantum mechanics and relativistic effects
NEXT STEPS
  • Research the role of QED in atomic spectroscopy for high-accuracy measurements
  • Explore the applications of cavity-QED in semiconductor laser technology
  • Investigate the implications of the Lamb shift in quantum systems
  • Study the interaction of lasers with molecules through QED frameworks
USEFUL FOR

Physicists, chemists, and engineers involved in quantum mechanics, atomic spectroscopy, and laser technology will benefit from this discussion, particularly those interested in the practical applications of QED in modern science and technology.

petergreat
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I'm trying to think of real-world applications of the standard model of particle physics, but can't come up with anything.
Are there any technological applications in which neither non-relativistic quantum mechanics nor Dirac's relativistic wave mechanics is insufficient, and QED must be used? QED doesn't seem to be used in the electronics industry, but I'll be glad to be corrected.
And how about QCD? I thought of nuclear power, but the fact that nuclear weapons were tested in 1945, decades before QCD, makes me suspect that QCD doesn't have any unambiguous applications in nuclear engineering, either.
So I guess it's safe to say that the standard model doesn't have real-world applications, even though the seemingly more esoteric general relativity does have applications (GPS)?
 
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I guess you don't accept the LHC as an application ;-)
 
I also tried to come up with something related to atomic spectroscopy. I can even find applications of hyperfine energy levels, in nuclear engineering (uranium isotope separation), astronomy (hydrogen 21cm line), and quantum computing (hyperfine levels as qubits). But when it comes to the real hallmark of QED, the Lamb shift, I again found nothing...
 
I have some clues again. Are there technological applications that rely on the fact that the electron Lande g-factor is slightly greater than 2? This is certainly a QED effect. Maybe some instruments that measure magnetic fields accurately need to take this into account?
 
Gell-Mann used to tell us that his funding would be much greater if he claimed to be working on a quark bomb.
 
Hmm, I am not sure whether that is what you are after, but in the semiconductor laser industry, the so-called cavity-QED regime is pretty attractive for low threshold lasers. Very often tailored quantum dot microcavity or photonic crystal lasers make use of tailored cavities and use the Purcell effect to create an enhanced spontaneous emission rate into the lasing mode.
 
petergreat said:
I also tried to come up with something related to atomic spectroscopy. I can even find applications of hyperfine energy levels, in nuclear engineering (uranium isotope separation), astronomy (hydrogen 21cm line), and quantum computing (hyperfine levels as qubits). But when it comes to the real hallmark of QED, the Lamb shift, I again found nothing...

The Lamb shift is only one of a huge number of verifiable consequences of QED, and has no special status.
(It is famous only because it was the first calculation that made quantum field theory respectable. It is not even the most accurate prediction - this honor belongs to the anomalous magnetic moment.)

Atomic spectroscopy is a consequence of QED, though it can be applied to the standard N-particle Coulomb Hamiltonian (which is the nonrelativistic limit of QED, and thus may be considered not to require QED). But QED is needed if you want to get high accuracy spectra. For heavier elements, it is even needed to get the right order of magnitude. For example, it requires QED to get the color of gold (a spectroscopic property) right. Calculations from the N-particle Coulomb Hamiltonian get the color completely wrong, since important correction terms derived from QED are missing.

The fact that quicksilver is liquid at room temperature is also a genuine QED effect, as applying the usual statistical mechanics calculations to the N-particle Coulomb Hamiltonian gets the freezing point quite wrong.

One also needs QED in laser-based chemistry, as the interaction between a laser and a molecule cannot be described without QED.
 
For example, it requires QED to get the color of gold (a spectroscopic property) right. Calculations from the N-particle Coulomb Hamiltonian get the color completely wrong, since important correction terms derived from QED are missing.
I don't agree. The reflection spectrum of gold can be calculated correctly using a relativistic Hartree-Fock approximation. Requiring relativity is not the same as requiring QED!
The fact that quicksilver is liquid at room temperature is also a genuine QED effect, as applying the usual statistical mechanics calculations to the N-particle Coulomb Hamiltonian gets the freezing point quite wrong.
According to this article, the unusual melting point of Mercury is due to a contraction of the 6s orbital, again a result of relativity.
One also needs QED in laser-based chemistry, as the interaction between a laser and a molecule cannot be described without QED.
This does not even require relativity, just Bose statistics.
 
Bill_K said:
I don't agree. The reflection spectrum of gold can be calculated correctly using a relativistic Hartree-Fock approximation. Requiring relativity is not the same as requiring QED!
How do you get the relativistic Hartree-Fock approximation? Of course from QED. Otherwise you don't
have a guidance how to choose the terms in the Hamiltonian, and need to resort to extra experimental information beyond the mass and charge of a gold atom. Whereas from QED you get it with minimal input.
Bill_K said:
According to this article, the unusual melting point of Mercury is due to a contraction of the 6s orbital, again a result of relativity.
And again, the Hamiltonian used for the relativistic orbital calculations comes from QED.
Bill_K said:
[... Laser chemistry...]
This does not even require relativity, just Bose statistics.

One needs the concept of a photon and the form of its interactions with the electrons, both borrowed from QED.
 
  • #10
How do you get the relativistic Hartree-Fock approximation?
You write down and solve the Dirac Equation. Which was done in 1928, about 20 years before the development of QED. Contrast this with the other effects mentioned previously: the Lamb shift and the anomalous magnetic moment, which DO depend on QED.
One needs the concept of a photon and the form of its interactions with the electrons, both borrowed from QED.
Einstein and Planck, who developed these concepts, would be surprised to hear that you are crediting them with the discovery of QED.
 
  • #11
Bill_K said:
You write down and solve the Dirac Equation. Which was done in 1928, about 20 years before the development of QED.
The Dirac equation is a single particle equation. It doesn't tell how different charged particles interact.
Traditional Poincare invariant generalization to multiple particles suffer from inconsistencies involving the Dirac sea.

One needs QED to specify relativistic interactions consistently from an ab initio perspective (i.e., with only masses and charges of the particles given).
Bill_K said:
One needs the concept of a photon and the form of its interactions with the electrons, both borrowed from QED.
Einstein and Planck, who developed these concepts, would be surprised to hear that you are crediting them with the discovery of QED.
Where did Einstein or Planck specify the form of the interaction of a photon with an electron?
I'd be too curious to know.
 
  • #12
A. Neumaier said:
The Dirac equation is a single particle equation. It doesn't tell how different charged particles interact.
Traditional Poincare invariant generalization to multiple particles suffer from inconsistencies involving the Dirac sea.
One needs QED to specify relativistic interactions consistently from an ab initio perspective (i.e., with only masses and charges of the particles given).

I don't consider consistency in this context to be an important issue. For example, I don't consider nuclear beta decay, at least to the first approximation, to be an application of nonabelian SU(2)*U(1) gauge theory, because the old Fermi's 4-point interaction is already sufficient, even though it's manifestly inconsistent (nonunitary at high energy).

Another example. The lifetime of hydrogen 2p state can't really be calculated consistently without QED, because in non-relativistic QM it's formally an exact eigenstate so shouldn't decay. But by Einstein's A-B coefficient argument, this can be calculated. Again this was done decades before QED. So QED doesn't have anything groundbreaking to say here.
 

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