Apart from the charmful decay channels of Y(4260), the charmless decay channels of Y(4260) also provide us a good platform to study the nature and the decay mechanism of Y(4260). In this paper, we propose to probe the structure of Y(4260) through the charmless decays Y(4260)→VP via intermediate D1D+c.c. meson loops, where V and P stand for light vector and pseudoscalar mesons, respectively. Under the molecule ansatz of Y(4260), the predicted total branching ratio BRVP for all Y(4260) → VP processes are about(0.34+0.32-0.23)% to(0.75+0.72-0.52)% with the cutoff parameter α=2–3. Numerical results show that the intermediate D1D+c.c. meson loops may be a possible transition mechanism in the Y(4260) → VP decays. These predicted branching ratios are the same order to that of Y(4260)→Z+c(3900)π-, which may be an evidence of D1 D molecule and can be examined by the forthcoming BESdata in the near future.
Apart from the charmful decay channels of Y(4260), the charmless decay channels of Y(4260) also provide us a good platform to study the nature and the decay mechanism of Y(4260). In this paper, we propose to probe the structure of Y(4260) through the charmless decays Y(4260)→VP via intermediate D1D+c.c. meson loops, where V and P stand for light vector and pseudoscalar mesons, respectively. Under the molecule ansatz of Y(4260), the predicted total branching ratio BRVP for all Y(4260) → VP processes are about(0.34+0.32-0.23)% to(0.75+0.72-0.52)% with the cutoff parameter α=2–3. Numerical results show that the intermediate D1D+c.c. meson loops may be a possible transition mechanism in the Y(4260) → VP decays. These predicted branching ratios are the same order to that of Y(4260)→Z+c(3900)π-, which may be an evidence of D1 D molecule and can be examined by the forthcoming BESdata in the near future.