A new measurement of ∆σ L for longitudinally polarized neutrons transmitted through a polarized proton target at 16.2 MeV has been made. This complements our previous measurement of ∆σ T at the same energy and after a phaseshift analysis improves the precision of the previous value of 3 S 1 − 3 D 1 mixing parameter 1 . The measurement yields the value ∆σ L = (−55 ± 20 ± 7) mb. The result of a simple phase shift analysis for 1 is presented and compared with the theoretical potential model predictions and other experiments. 25.40.Dn; 24.70.+s; 13.75.Cs In the last decade a considerable progress has been achieved in studying low energy neutron-proton elastic scattering. Beside other problems attention has been paid to clarify the role of tensor force in NN interaction. This force is characterized by the 3 S 1 − 3 D 1 mixing parameter 1 which cannot be measured directly, so only measurements of spin observables sensitive to it can improve the 1 determination. Such observables are the spin-dependent total cross-section differences ∆σ T and ∆σ L , the spin correlation coefficient A 00nn (ϑ) at 90 deg c.m. angle and the spin transfer parameter K 0nn0 (ϑ). The A 00nn (ϑ) measurement at 90 deg c.m. is presented by Schöberl et al. for 13.7 MeV neutron energy (Erlangen 1988 [1]) and by Doll et al. for 19, 21 and 25 MeV (Karlsruhe 1989 [2]). The spin transfer parameter K 0nn0 (133 deg c.m.) was measured at 25.8 and 17.4 MeV by Ockenfels et al. (Bonn 1990 [3, 4]), while ∆σ T was measured in TUNL in the 3.65-11.60 MeV energy range (1993 [5]) and at 16.2 MeV in our laboratory (1993 [6]). Furthermore, ∆σ L has been measured at 66 MeV incident neutron energy at Villigen (1992 [7]).
PACS:Analyses of the results show apparent discrepancies, namely around 15 MeV, where two older measurements from Erlangen and Bonn indicate the existence of a local minimum in contrary to potential model and PSA predictions, while our ∆σ T measurement supports the predicted behaviourof 1 .However, our value 1 = (1.46 ± 1.32) deg had a relatively large error, so we studied how to determine this mixing parameter more precisely to find a more definite answer to the 1 problem.As it became infeasible to improve the 1 precision via measuring ∆σ T , we performed a new measurement with longitudinally polarized beam and target to obtain ∆σ L and furthermore ∆σ T − ∆σ L , which is the quantity sensitive namely to 1 , as shown in [5].The measurement of ∆σ L has been performed using the classical transmission method, i.e. the relative difference in attenuation of a polarized neutron beam passing through a polarized proton target has been measured.The experimental setup was similar to the one used for the ∆σ T measurement described in [6], so only brief description with more stress to the modifications will be presented here.In the present experiment a frozen spin polarized proton target with a dilution refrigerator has been used. Propanediol C 3 H 8 O 2 with a paramagnetic Cr(V) impurity was used as a target material. Typical proton polarization obtained was 9...