By S. Flugge
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Non-mesonicdecay modes ofhypernuclei. ,A450, 1986. • [4]B. J. F. Gibson. Phys. , C30(1),1984. [5]D. P. Kisslinger. Phgs. ,C33(2),1986. [6]J. Cohen. Progressin Particleand NuclearPh_/sics, 25, 1990. [7] N. K. o and M. S. Swami.. Indian Acad. , 7lA, 1970. al. Nonleptonicweak decayof_He and _2C. ,C43(2),1991. D. Grace. Weak Decay ofP ShellLambda llgpernuclei. PhD thesis, CarnegieMellon University, 1986. B. Dover. Few Body Hypernudear Systems:Weak Decays. Few-Body Systems,1989. [11]John Szymanski. The Weak Decal/of Lambda ]lypernuclei.
The apparatus consisted of a rigid rail which held a moveable cart carrying three high-precision Hall probes oriented to measure the three field components. The stepping motor which moved the cart along the rail was controlled by a computer which also read out the • Hall probes via tesla-meters and stored the results. position) could be mapped under computer Thus, a series of points (of common X and Y control as the cart was moved in steps in the Z direction. The track could then be manually moved in discrete jumps in the X and Y directions.
FP was positioned • slightly upstream with their active area facing between the Forward Cerenkov counter (FC) and the second Forward Drift Chamber (FD2), which is immediately in front of the 48D48 magnet gap. Its active area covers the beam and extends downwards to include events of interest. Because of its proximity PMT's. to the magnet, heavy iron shielding was required around the Due to this weight, the detector was designed to retract from the 48D48 field clamp aperture by sliding the detector along mounting rails to allow access to FD2.
Elasticity and Plasticity / Elastizitat und Plastizitat. by S. Flugge
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