Evidence of a structure in $$\bar{K}^{0} \Lambda _{c}^{+}$$ <math><mrow><msup><mrow><mover><mrow><mi>K</mi></mrow><mrow><mo>¯</mo></mrow></mover></mrow><mn>0</mn></msup><msubsup><mi>Λ</mi><mrow><mi>c</mi></mrow><mo>+</mo></msubsup></mrow></math> consistent with a charged $$\Xi _c(2930)^{+}$$ <math><mrow><msub><mi>Ξ</mi><mi>c</mi></msub><msup><mrow><mo>(</mo><mn>2930</mn><mo>)</mo></mrow><mo>+</mo></msup></mrow></math> , and updated measurement of $$\bar{B}^{0} \rightarrow \bar{K}^{0} \Lambda _{c}^{+} \bar{\Lambda }_{c}^{-}$$ <math><mrow><msup><mrow><mover><mrow><mi>B</mi></mrow><mrow><mo>¯</mo></mrow></mover></mrow><mn>0</mn></msup><mo>→</mo><msup><mrow><mover><mrow><mi>K</mi></mrow><mrow><mo>¯</mo></mrow></mover></mrow><mn>0</mn></msup><msubsup><mi>Λ</mi><mrow><mi>c</mi></mrow><mo>+</mo></msubsup><msubsup><mover><mrow><mi>Λ</mi></mrow><mrow><mo>¯</mo></mrow></mover><mrow><mi>c</mi></mrow><mo>-</mo></msubsup></mrow></math> at Belle

We report evidence for the charged charmed-strange baryon $$\Xi _{c}(2930)^+$$ Ξc(2930)+ with a signal significance of 3.9$$\sigma $$ σ with systematic errors included. The charged $$\Xi _{c}(2930)^+$$ Ξc(2930)+ is found in its decay to $$K_{S}^{0} \Lambda _{c}^+$$ KS0Λc+ in the substructure of $$\bar{B}^{0} \rightarrow K^{0}_{S} \Lambda _{c}^{+} \bar{\Lambda }_{c}^{-}$$ B&#175;0→KS0Λc+Λ&#175;c- decays. The measured mass and width are $$[2942.3 \pm 4.4 ({\mathrm{stat.}}) \pm {1.5}({\mathrm{syst.}})]$$ [2942.3&#177;4.4(stat.)&#177;1.5(syst.)] MeV/$$c^{2}$$ c2 and $$[14.8 \pm 8.8({\mathrm{stat.}}) \pm {2.5}({\mathrm{syst.}})]$$ [14.8&#177;8.8(stat.)&#177;2.5(syst.)] MeV, respectively, and the product branching fraction is $$\mathcal{B}(\bar{B}^{0} \rightarrow \Xi _c(2930)^{+} \bar{\Lambda }_{c}^{-}) \mathcal{B}(\Xi _c(2930)^{+}\rightarrow \bar{K}^{0} \Lambda _{c}^{+})=[2.37 \pm 0.51 ({\mathrm{stat.}})\pm 0.31({\mathrm{syst.}})]\times 10^{-4}$$ B(B&#175;0→Ξc(2930)+Λ&#175;c-)B(Ξc(2930)+→K&#175;0Λc+)=[2.37&#177;0.51(stat.)&#177;0.31(syst.)]&#215;10-4 . We also measure $$\mathcal{B}(\bar{B}^{0} \rightarrow \bar{K}^{0} \Lambda _{c}^{+} \bar{\Lambda }_{c}^{-}) = [3.99 \pm 0.76({\mathrm{stat.}}) \pm 0.51({\mathrm{syst.}})] \times 10^{-4}$$ B(B&#175;0→K&#175;0Λc+Λ&#175;c-)=[3.99&#177;0.76(stat.)&#177;0.51(syst.)]&#215;10-4 with greater precision than previous experiments, and present the results of a search for the charmonium-like state Y(4660) and its spin partner, $$Y_{\eta }$$ Yη , in the $$\Lambda _{c}^{+}\bar{\Lambda }_{c}^{-}$$ Λc+Λ&#175;c- invariant mass spectrum. No clear signals of the Y(4660) or $$Y_{\eta }$$ Yη are observed and the 90% credibility level (C.L.) upper limits on their production rates are determined. These measurements are obtained from a sample of $$(772\pm 11)\times 10^{6} B\bar{B}$$ (772&#177;11)&#215;106BB&#175; pairs collected at the $$\Upsilon (4S)$$ Υ(4S) resonance by the Belle detector at the KEKB asymmetric energy electron-positron collider.