Note on Solar Neutrino Experiments Takeshi K. Komatsubara (KEK-IPNS) 2003-June-12(Thu) There are three processes for detecting ^8B solar neutrinos (5 p + p + e^- This is EXCLUSIVELY from the nu_e flux. The electron would be scattered to the backward of the original nu_e direction. 2. Elastic Scattering (ES) of neutrino and electron [both SNO and SK]: nu_x + e^- --> nu_x + e^- x=el,mu,tau The cross sections of mu and tau neutrinos (Neutral Current with Z) are smaller (15% for each) than the cross section of el neutrino (Charged Current with W and Neutrino Current with Z). This is MOSTLY from nu_el flux. The electron would be scattered to the forward of the original nu_e direction. 3. Neutral Current (NC) reaction of neutrino and deuteron [SNO] nu_a + D --> nu_a + p + n a=el,mu,tau The cross sections of el, mu and tau neutrinos are almost equal. This is the TOTAL neutrino flux from the sun. The neutron interacts with a deuteron and a monochromatic gamma ray (6 MeV) would be emitted isotropically. The pages 26-28 of hep-ph/0204288 should be read like this ( '** **' : my corrections). "The Kamiokande and Super-Kamiokande experiments are water Cherenkov detector. Here ** the elastic scattering (RS) in fig.12 **, nu_x + e^- --> nu_x + e^- (107) is used to detect solar neutrinos. ... An important step towards the final resolution of the solar neutrino problem was made by the recent results of the Sudbury Neutrino Observatory (SNO). Like the SuperKamiokande, high-energy ^8B neutrinos are observed, this time in a 1000 t detector of heavy water D_2O. This allows the observation of the charged current (CC) reaction nu_el + D --> p + p + e^- (108) as well as the ** neutral current (NC) reaction nu_a + D --> nu_a + p + n (109). ** From the CC reaction (108) ... Alternatively, one may assume that electron-neutrinos have partially been converted into muon- and tau-neutrinos. In this case, the flux extractedfrom the ** NC reaction ** (109) should coincide with the flux of ^8B neutrinos. One finds ..." ---- End of this note.