Space flight experience with the AMS infrared tracker alignment system (TAS)

Physics

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Scientific paper

The large acceptance Antimatter Spectrometer (AMS) experiment (Becker, 1999) has been flown successfully on the STS91 (02-June-98 12-June-98) shuttle flight. AMS-01 particle tracking is based on 6 planes of double sided Si detectors in a permanent magnetic field. The position stability of the tracking elements has been con-trolled using infrared laser generated and cosmic straight tracks. Over the whole flight -including lift-off and landingall tracking elements were found at their expected positions within ±15 µm. 1 Intoduction AMS-01 high accuracy momentum measurement is based on 6 (2+1)D high precision position determinations of charged particle tracks through a 1m3 magnetic field (|B| ≈ 1.2kG) volume. A particle track of 10 GeV has a 0.5 mm sagitta. 2D particle position information is derived from double sided Silicon strip detectors arranged in "ladders" of up to 65cm of length (fig. 1) tiling the 6 detector planes. The main component of the magnetic field runs parallel to the "y-strips" on the junction side of the Si detectors. From the electrical signals on the implantations (pitch ˜y/˜x 27.5/52 µm) the sagitta can be measured to about 25 µm precision (Alcaraz et al. 1999). The third dimension is derived from metrology during the assembly of the tracker plates (˜z ≈ 50 µm). Taking multiple scattering into account the AMS-01 tracker has about 10% momentum resolution at 10 GeV allowing for a maximum detectable momentum (MDM) of 500 GeV. It is evident that a precise momentum measurement is only possible if the detector positions perpendicular to the magnetic field vector (y-axis) are known at all times with an accuracy of better than a small fraction of the to be measured sagitta. 2 Tracker alignment Straight tracks measured with the Si sensors themselves are most appropriate for an alignment check of these sensors on the 6 detector planes. In the following a subset of AMS-01 Si ladders are aligned using both artificial straight tracks produced by laser (λ = 1082 nm) beams (fig. 1) and quasi straight tracks of high rigidity (p > 4 GV) particles (fig. 2). J. Vandenhirtz1, W. Wallraff1, M. Weisgerber1 1RWTH-Aachen, 1.Physikalisches Institut

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