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 Tools annual

Global: Zendy Free Plan

Global: Zendy Tools monthly

Global: Zendy Plus monthly

We use the non-perturbative Q\bar Q potential at finite temperatures derivedin the Field Correlator Method to obtain binding energies for the lowesteigenstates in the Q\bar Q and QQQ systems (Q=c,b). The three--quark problem issolved by the hyperspherical method. The solution provides an estimate of themelting temperature and the radii for the different diquark and triquark boundstates. In particular we find that J/\psi and $ccc$ ground states survive up toT \sim 1.3 T_c, where T_c is the critical temperature, while the correspondingbottomonium states survive even up to higher temperature, T \sim 2.2 T_c.

Diquark and triquark correlations in the deconfined phase of QCD