By analyzing 2.93 fb$^{−1}$ of $e^+e^−$ annihilation data taken at the center-of-mass energy $\sqrt s$= 3.773 GeV with the BESIII detector, we determine the branching fractions of the inclusive decays $D^+\to\phi X$ and $D^0\to\phi X$ to be (1.135 ± 0.034 ± 0.031)% and (1.091 ± 0.027 ± 0.035)% , respectively, where $X$ denotes any possible particle combination. The first uncertainties are statistical, and the second are systematic. We also determine the branching fractions of the decays $D\to\phi X$ and their charge conjugate modes $\bar{D}\to\phi \bar{X}$ separately for the first time, and no significant CP asymmetry is observed
By analyzing an $e^+e^-$ annihilation data sample with an integrated luminosity of $2.93\ \rm fb^{-1...
By analyzing 2.93 fb$^{-1}$ of data collected at $\sqrt s=3.773$ GeV with the BESIII detector, we me...
By analyzing 2.93 fb$$^{-1}$$ of data collected at $$\sqrt{s}=3.773$$ GeV with the BESIII detector, ...
By analyzing 2.93 fb(-1) of e(+)e(-) annihilation data taken at the center-of-mass energy root s = 3...
By analyzing 2.93 fb(-1) of e(+)e(-) annihilation data taken at the center-of-mass energy root s = 3...
By analyzing 2.93 fb(-1) of e(+)e(-) annihilation data taken at the center-of-mass energy root s = 3...
Using e+e- annihilation data corresponding to an integrated luminosity of 2.93 fb-1 taken at a cente...
Using e+e- annihilation data corresponding to an integrated luminosity of 2.93 fb-1 taken at a cente...
The four decay modes $D^{0}\to\phi\pi^{0}$, $D^{0}\to\phi\eta$, $D^{+}\to\phi\pi^{+}$, and $D^{+}\to...
By analyzing 2.93 fb$^{-1}$ data collected at the center-of-mass energy $\sqrt s=3.773$ GeV with the...
Using e+e- collision data corresponding to an integrated luminosity of 2.93 fb-1 taken at a center-o...
By analyzing 2.93 fb-1 of e+e- collision data taken at the center-of-mass energy of 3.773 GeV with t...
By analyzing 2.93 fb-1 of e+e- collision data taken at the center-of-mass energy of 3.773 GeV with t...
Using $e^+e^−$ collision data corresponding to an integrated luminosity of 2.93 fb$^{−1}$ taken at a...
By analyzing an $e^+e^-$ annihilation data sample with an integrated luminosity of $2.93\ \rm fb^{-1...
By analyzing an $e^+e^-$ annihilation data sample with an integrated luminosity of $2.93\ \rm fb^{-1...
By analyzing 2.93 fb$^{-1}$ of data collected at $\sqrt s=3.773$ GeV with the BESIII detector, we me...
By analyzing 2.93 fb$$^{-1}$$ of data collected at $$\sqrt{s}=3.773$$ GeV with the BESIII detector, ...
By analyzing 2.93 fb(-1) of e(+)e(-) annihilation data taken at the center-of-mass energy root s = 3...
By analyzing 2.93 fb(-1) of e(+)e(-) annihilation data taken at the center-of-mass energy root s = 3...
By analyzing 2.93 fb(-1) of e(+)e(-) annihilation data taken at the center-of-mass energy root s = 3...
Using e+e- annihilation data corresponding to an integrated luminosity of 2.93 fb-1 taken at a cente...
Using e+e- annihilation data corresponding to an integrated luminosity of 2.93 fb-1 taken at a cente...
The four decay modes $D^{0}\to\phi\pi^{0}$, $D^{0}\to\phi\eta$, $D^{+}\to\phi\pi^{+}$, and $D^{+}\to...
By analyzing 2.93 fb$^{-1}$ data collected at the center-of-mass energy $\sqrt s=3.773$ GeV with the...
Using e+e- collision data corresponding to an integrated luminosity of 2.93 fb-1 taken at a center-o...
By analyzing 2.93 fb-1 of e+e- collision data taken at the center-of-mass energy of 3.773 GeV with t...
By analyzing 2.93 fb-1 of e+e- collision data taken at the center-of-mass energy of 3.773 GeV with t...
Using $e^+e^−$ collision data corresponding to an integrated luminosity of 2.93 fb$^{−1}$ taken at a...
By analyzing an $e^+e^-$ annihilation data sample with an integrated luminosity of $2.93\ \rm fb^{-1...
By analyzing an $e^+e^-$ annihilation data sample with an integrated luminosity of $2.93\ \rm fb^{-1...
By analyzing 2.93 fb$^{-1}$ of data collected at $\sqrt s=3.773$ GeV with the BESIII detector, we me...
By analyzing 2.93 fb$$^{-1}$$ of data collected at $$\sqrt{s}=3.773$$ GeV with the BESIII detector, ...