English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Plus annual

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Plus monthly

Global: Zendy Tools annual

Global: Zendy Tools monthly

Global: Zendy Free Plan

The magnetic dipole moments of the doubly-heavy baryons include significantdata on their inner structure and geometric shape. Moreover, understanding theelectromagnetic properties of doubly-heavy baryons is the key to confinementand heavy flavor effects. Inspired by this, we extract the magnetic dipolemoments of the spin-$\frac{1}{2}$ bottom-charm baryons utilizing the QCDlight-cone sum rule with considering the distribution amplitudes of thephoton.The magnetic dipole moments are obtained as $\mu_{\Xi_{bc}^{+}} =-0.50^{+0.14}_{-0.12}~\mu_{N}$, $\mu_{\Xi_{bc}^{0}} =0.39^{+0.06}_{-0.05}~\mu_{N}$ and $\mu_{\Omega_{bc}^{0}} = 0.38^{+0.05}_{-0.04}~\mu_{N}$, $\mu_{\Xi_{bc}^{\prime +}} = 0.57^{+0.13}_{-0.12}~\mu_{N}$,$\mu_{\Xi_{bc}^{\prime 0}} =-0.29^{+0.07}_{-0.06}~\mu_{N}$ and$\mu_{\Omega_{bc}^{\prime 0}} = -0.26^{+0.06}_{-0.05}~\mu_{N}$. Comparing theresults obtained on the magnetic dipole moments of the$\Omega^{(\prime)0}_{bc}$ baryon with those of the $\Xi^{(\prime)0}_{bc}$baryon, the $U$-symmetry is minimally broken. We have compared our results withother theoretical predictions that could be a useful complementary tool for theinterpretation of the doubly-heavy baryon sector, and we observe that they arenot in mutual agreement with each other.

Magnetic dipole moments of bottom-charm baryons in light-cone QCD