The modification of the Doppler effect due to the coupling of the helicity of the radiation with the rotation of the source/receiver is considered in the case of the Pioneer 10/11 spacecraft. We explain why the Pioneer anomaly is not influenced by the helicity-rotation coupling.PACS: 03.30.+p ; 04.20.Cv Keywords: Pioneer anomaly; helicity-rotation coupling 1 The Pioneer 10/11 Missions were launched about three decades ago and have been the first to explore the outer solar system. The analysis of radio tracking data since about two decades ago -when the effective acceleration away from the Sun due to the solar radiation pressure on the spacecraft decreased below 5 × 10 −8 cm/sec 2 -has persistently indicated the existence of an anomaly in the Doppler navigational data [1,2,3]. This Pioneer anomaly is a Doppler drift that may be interpreted as being due to a small constant acceleration a P = (8.74 ± 1.33) × 10 −8 cm/sec 2 of the spacecraft toward the Sun. The source of the anomaly is suspected to be a systematic effect associated with the spacecraft; however, no definitive answer is known as yet [1,2,3].In a recent paper [4], the modification of the Doppler effect due to the coupling of photon spin with the rotation of the emitter/receiver has been elucidated. This result is of interest for the Doppler tracking of spacecraft, since circularly polarized radiation is routinely employed to communicate with spacecraft and, moreover, the Earth as well as the spacecraft rotate. The question then naturally arises whether the helicity-rotation coupling contributes to the Pioneer anomaly. It is the purpose of this Letter to explain why there is no such contribution, since the main effect has already been phenomenologically incorporated in the analysis of Doppler data.Let ω and k be the frequency and wave vector of a photon according to inertial observers at rest in a global inertial frame. The photon is received by a noninertial observer with velocity v and rotation frequency Ω such that Ω << ω. According to this rotating observer, the frequency of the photon iswhere ω = ck, γ = (1 − v 2 /c 2 ) −1/2 is the Lorentz factor andĤ = ±ck/ω is the unit helicity vector of the photon. The upper (lower) sign refers to a positive (negative) helicity photon [4,5]. The photon helicity is related to its intrinsic spin S by S =hĤ. A beam of positive (negative) helicity electromagnetic radiation is such that inertial observers at rest along the beam looking down at the approaching wave will see the electric and magnetic fields both rotate counterclockwise (clockwise) with frequency ω about the direction of propagation. Equation (1) expresses the standard relativistic Doppler effect together with an extra term due to the helicity-rotation coupling (−γĤ · Ω) that may be neglected for Ω/ω → 0; otherwise, for a small but nonzero Ω/ω << 1, ignoring helicity-rotation coupling would lead to a systematic Doppler shift of magnitude ∆v = cΩ/ω along the beam. It is possible to illustrate the contribution of helicity-rotation coupling to the ...