Abstract
The time evolution of the baryon asymmetry of the universe due to superheavy Higgs bosons is obtained by integrating the Boltzmann equations. The interactions included are decays, inverse decays, and annihilations of the Higgs bosons. The minimal SU(5) model is used to calculate the interactions, although our results are more generally applicable. Decays and inverse decays of these bosons damp preexisting asymmetries by $\mathrm{exp}(\ensuremath{-}0.3K)$ to $\mathrm{exp}(\ensuremath{-}2.0K)$ where $K=2.9\ifmmode\times\else\texttimes\fi{}{10}^{17}{\ensuremath{\alpha}}_{H}\frac{\mathrm{GeV}}{{M}_{H}}$ (${\ensuremath{\alpha}}_{H}$ and ${M}_{H}$ are the coupling strength and mass of the Higgs boson). If both $C$ and $\mathrm{CP}$ are violated, then in an initially symmetrical universe a baryon asymmetry evolves and its value depends upon $K$ and $\frac{{\ensuremath{\alpha}}^{2}}{{\ensuremath{\alpha}}_{H}}$ ($\ensuremath{\alpha}$ is the gauge coupling strength). For $K\ensuremath{\ll}\frac{{\ensuremath{\alpha}}_{H}}{{\ensuremath{\alpha}}^{2}}$ the asymmetry produced is $\frac{k{n}_{B}}{s}\ensuremath{\simeq}2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}3}\ensuremath{\epsilon}$, and for $K\ensuremath{\gg}1$ it is $\frac{k{n}_{B}}{s}\ensuremath{\simeq}2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}3}\ensuremath{\epsilon}{(3K)}^{\ensuremath{-}1.2}$ ($\frac{\ensuremath{\epsilon}}{2}$=the baryon excess produced by the decay of a pair of $H$, $\overline{H}$ bosons). In SU(5) for ${M}_{H}\ensuremath{\gtrsim}3\ifmmode\times\else\texttimes\fi{}{10}^{13}$ GeV preexisting asymmetries are not damped and the observed asymmetry $\frac{k{n}_{B}}{s}={10}^{\ensuremath{-}9.8\ifmmode\pm\else\textpm\fi{}1.6}$ can be produced if $\ensuremath{\epsilon}\ensuremath{\simeq}{10}^{\ensuremath{-}7}$. In a companion paper the role of gauge bosons is considered.
Keywords
Affiliated Institutions
Related Publications
Precision Measurement of Half-Lives and Specific Activities of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">U</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>235</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">U</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>238</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>
New determinations of the half-lives of $^{235}\mathrm{U}$ and $^{238}\mathrm{U}$ have been made. Improved techniques have allowed the half-life values to be measured with great...
Domain Structure of Rochelle Salt and K<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">H</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>P<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
It has been verified by means of the polarization microscope that rochelle salt in the ferroelectric state consists of many domains. The domain structure in an annealed crystal ...
Lattice Vibrations in Pyrolitic Graphite
The dispersion relation for the longitudinal acoustic lattice waves propagating in the direction of the hexad axis in (pyrolitic) graphite, at room temperature, has been determi...
First-Principles Determination of the Soft Mode in Cubic<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>ZrO</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
A direct approach to calculate the phonon dispersion using an ab initio force constant method is introduced. The phonon dispersion and structural instability of cubic ${\mathrm{...
Energy of Lattice Distortion in Cold Worked Permalloy
The lattice distortion produced by severe cold working of permalloy of 70 percent Ni content has been studied by measuring the broadenin of the reflection of the Fe $K\ensuremat...
Publication Info
- Year
- 1980
- Type
- article
- Volume
- 22
- Issue
- 12
- Pages
- 2977-2988
- Citations
- 47
- Access
- Closed
External Links
Social Impact
Social media, news, blog, policy document mentions
Citation Metrics
Cite This
Identifiers
- DOI
- 10.1103/physrevd.22.2977