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* The [[proton mass]] ''m''<sub>p</sub> is composed primarily of [[gluon]]s, and of the [[quark]]s (the [[up quark]] and [[down quark]]) making up the proton. Hence ''m''<sub>p</sub>, and therefore the ratio ''μ'', are easily measurable consequences of the [[strong force]]. In fact, in the [[chiral]] limit, ''m''<sub>p</sub> is proportional to the [[Quantum chromodynamics|QCD]] energy scale, Λ<sub>QCD</sub>. At a given energy scale, the [[strong force|strong]] [[coupling constant]] ''α''<sub>s</sub> is related to the QCD scale (and thus ''μ'') as
* The [[proton mass]] ''m''<sub>p</sub> is composed primarily of [[gluon]]s, and of the [[quark]]s (the [[up quark]] and [[down quark]]) making up the proton. Hence ''m''<sub>p</sub>, and therefore the ratio ''μ'', are easily measurable consequences of the [[strong force]]. In fact, in the [[chiral]] limit, ''m''<sub>p</sub> is proportional to the [[Quantum chromodynamics|QCD]] energy scale, Λ<sub>QCD</sub>. At a given energy scale, the [[strong force|strong]] [[coupling constant]] ''α''<sub>s</sub> is related to the QCD scale (and thus ''μ'') as
::<math>\alpha_s=-\frac{2\pi}{\beta_0 \ln(E/\Lambda_{\rm QCD})}</math>
::<math>\alpha_s=-\frac{2\pi}{\beta_0 \ln(E/\Lambda_{\rm QCD})}</math>
:where ''β''<sub>0</sub> = −11 + 2''n''/3, with ''n'' being the number of [[flavor (particle physics)|flavors]] of [[quark]]s.
:where ''β''<sub>0</sub> = −11 + 2''n''/3, with ''n'' being the number of [[flavor (particle physics)|flavors]] of [[quark]]s.ratio of mass of proton and electron is 1:1857


==Variation of ''μ'' over time==
==Variation of ''μ'' over time==

Revision as of 15:35, 31 July 2019

In physics, the proton-to-electron mass ratio, μ or β, is simply the rest mass of the proton (a baryon found in atoms) divided by that of the electron (a lepton found in atoms). Because this is a ratio of like-dimensioned physical quantities, it is a dimensionless quantity, a function of the dimensionless physical constants, and has numerical value independent of the system of units, namely:

μ =  = .

The number enclosed in parentheses is the measurement uncertainty on the last two digits. The value of μ is known to about 0.1 parts per billion.


Discussion

μ is an important fundamental physical constant because:

where β0 = −11 + 2n/3, with n being the number of flavors of quarks.ratio of mass of proton and electron is 1:1857

Variation of μ over time

Astrophysicists have tried to find evidence that μ has changed over the history of the universe. (The same question has also been asked of the fine structure constant.) One interesting cause of such change would be change over time in the strength of the strong force.

Astronomical searches for time-varying μ have typically examined the Lyman series and Werner transitions of molecular hydrogen which, given a sufficiently large redshift, occur in the optical region and so can be observed with ground-based spectrographs.

If μ were to change, then the change in the wavelength λi of each rest frame wavelength can be parameterised as:

where Δμ/μ is the proportional change in μ and Ki is a constant which must be calculated within a theoretical (or semi-empirical) framework.

Reinhold et al. (2006) reported a potential 4 standard deviation variation in μ by analysing the molecular hydrogen absorption spectra of quasars Q0405-443 and Q0347-373. They found that Δμ/μ = (2.4 ± 0.6)×10−5. King et al. (2008) reanalysed the spectral data of Reinhold et al. and collected new data on another quasar, Q0528-250. They estimated that Δμ/μ = (2.6 ± 3.0)×10−6, different from the estimates of Reinhold et al. (2006).

Murphy et al. (2008) used the inversion transition of ammonia to conclude that |Δμ/μ| < 1.8×10−6 at redshift z = 0.68.

Bagdonaite et al. (2013) used methanol transitions in the spiral lens galaxy PKS 1830-211 to find μ/μ = (0.0 ± 1.0) × 10−7 at z = 0.89, a stringent limit at this redshift.[1][2]

Note that any comparison between values of Δμ/μ at substantially different redshifts will need a particular model to govern the evolution of Δμ/μ. That is, results consistent with zero change at lower redshifts do not rule out significant change at higher redshifts.

See also

Footnotes

  1. ^ Bagdonaite, Julija; Jansen, Paul; Henkel, Christian; Bethlem, Hendrick L.; Menten, Karl M.; Ubachs, Wim (December 13, 2012). "A Stringent Limit on a Drifting Proton-to-Electron Mass Ratio from Alcohol in the Early Universe". Science. 339 (6115): 46–48. Bibcode:2013Sci...339...46B. doi:10.1126/science.1224898. PMID 23239626.
  2. ^ Moskowitz, Clara (December 13, 2012). "Phew! Universe's Constant Has Stayed Constant". Space.com. Retrieved December 14, 2012.

References