Yes, the proton structure includes electrons and positrons, but their contribution is negligible because electromagnetism is so much weaker than the strong interaction that produces the proton's quark-gluon sea. The contribution from photons is, however, a hundred times greater than the $e^+e^-$ contribution and is – according to "How Bright is the Proton? A Precise Determination of the Photon Parton Distribution Function" – too large to be ignored in current parameterizations of the proton's Parton Distribution Functions (PDF).
According to Figure 20 of "The photon content of the proton", the fraction of a proton's momentum carried by photons increases logarithmically with the energy scale being probed, from about $0.3\%$ at $10$ GeV to $0.6\%$ at $10$ TeV.
These values are consistent with naive expectations based on the lowest order processes involved.
For momenta high enough for the parton masses to be negligible, we roughly expect the contributions of different particles to the proton's structure to be:
- gluons: $\sim \alpha_S \sim 1$
- quark-antiquark pairs: $\sim (\alpha_S)^2 \sim 1$
- photons: $\sim \alpha_{QED} \approx 1/137 \sim 10^{-2}$
- electron-positron pairs: $\sim (\alpha_{QED})^2 \sim 10^{-4}$
I am not aware of any attempt to precisely determine the electron-positron content of the proton, but the analogous electron-positron content of the electron is more tractable and has been calculated. If my quick and dirty numerical integrations of the PDFs in Figure 5 (below) of "The partonic structure of the electron at the next-to-leading logarithmic accuracy in QED" are correct, at an energy scale of $100$ GeV, photons carry a few percent of an electron's momentum and positrons carry about $0.02\%$.