Abstract

We review the status as regards the existence of three- and four-body bound states made of neutrons and ΛΛ hyperons. For interesting cases, the coupling to neutral baryonic systems made of charged particles of different strangeness has been addressed. There are strong arguments showing that the ΛnnΛnn system has no bound states. ΛΛnnΛΛnn strong stable states are not favored by our current knowledge of the strangeness −1-1 and −2-2 baryon-baryon interactions. However, a possible Ξ−tΞ^- t quasibound state decaying to ΛΛnnΛΛnn might exist in nature. Similarly, there is a broad agreement about the nonexistence of ΛΛnΛΛn bound states. However, the coupling to ΞNNΞNN states opens the door to a resonance above the ΛΛnΛΛn threshold.

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