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Cyclotron Instrumentation for Nuclear Spectroscopy at Medium Resolution in Energy

dc.contributor.authorBach, David Rudolphen_US
dc.contributor.authorChilds, W. J.en_US
dc.contributor.authorHockney, R. W.en_US
dc.contributor.authorHough, Paul V. C.en_US
dc.contributor.authorParkinson, William Charlesen_US
dc.date.accessioned2010-05-06T23:25:31Z
dc.date.available2010-05-06T23:25:31Z
dc.date.issued1956-07en_US
dc.identifier.citationBach, D. R.; Childs, W. J.; Hockney, R. W.; Hough, P. V. C.; Parkinson, W. C. (1956). "Cyclotron Instrumentation for Nuclear Spectroscopy at Medium Resolution in Energy." Review of Scientific Instruments 27(7): 516-526. <http://hdl.handle.net/2027.42/71238>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/71238
dc.description.abstractThe instrumentation for the magnetic focusing and analysis of the external beam of the Michigan cyclotron is described. It provides to a scattering chamber in an adjacent room a beam of deuterons of a few tenths microampere monoenergetic to within 15 kev at a mean energy of 7.8 Mev. A double‐focusing analyzer magnet of mean radius one meter, focuses reaction products of magnetic rigidity less than or equal to that of a 20‐Mev proton. At the optimum energy resolution of the system, proton groups from (d,p) reactions differing in Q by about 20 kev can be resolved. Particles can be observed over a continuum of angles from −7° to +112° relative to the incident beam. The determination of reaction energies and the measurement of relative differential cross sections are discussed.en_US
dc.format.extent3102 bytes
dc.format.extent1193969 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleCyclotron Instrumentation for Nuclear Spectroscopy at Medium Resolution in Energyen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumHarrison M. Randall Laboratory of Physics, The University of Michigan, Ann Arbor, Michiganen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/71238/2/RSINAK-27-7-516-1.pdf
dc.identifier.doi10.1063/1.1715622en_US
dc.identifier.sourceReview of Scientific Instrumentsen_US
dc.identifier.citedreferenceParkinson, Beach, and King, Phys. Rev. 87, 387(L) (1952).en_US
dc.identifier.citedreferenceVan Patter, Endt, Sperduto, and Buechner, Phys. Rev. 86, 502 (1952).en_US
dc.identifier.citedreferenceBeach, Childs, Hough, King, and Parkinson, Phys. Rev. 86, 582(A) (1952).en_US
dc.identifier.citedreferenceP. V. C. Hough, Rev. Sci. Instr. 24, 42 (1953).en_US
dc.identifier.citedreferenceR. Grismore and W. C. Parkinson (to be published).en_US
dc.identifier.citedreferenceObtained from Consolidated Water Power and Paper Company, Wisconsin Rapids, Wisconsin.en_US
dc.identifier.citedreferenceJ. L. Lawson and A. W. Tyler, Rev. Sci. Instr. 10, 304 (1939).en_US
dc.identifier.citedreferenceD. Judd, Rev. Sci. Instr. 21, 213 (1950).en_US
dc.identifier.citedreferenceE. S. Rosenblum, Rev. Sci. Instr. 21, 586 (1950).en_US
dc.identifier.citedreferenceFor reaction protons of energy greater than 1 Mev, single scattering is most important. See E. Segre, Experimental Nuclear Physics (John Wiley and Sons, Inc., New York, 1953), p. 249 ff.en_US
dc.identifier.citedreferenceParkinson, Grover, and Crane, Rev. Sci. Instr. 18, 734 (1947).en_US
dc.identifier.citedreferenceK. Siegbahn and Svartholm, Arkiv. Mat. Astron. Fysik 33A, No. 21 (1946).en_US
dc.identifier.citedreferenceModel V‐4400, Varian Associates, Palo Alto, California.en_US
dc.identifier.citedreferenceModel 524A, Hewlett‐Packard, Palo Alto, California.en_US
dc.identifier.citedreferenceP. M. Endt and J. C. Kluyver, Revs. Modern Phys. 26, 95 (1954), and references therein.en_US
dc.identifier.citedreferenceF. B. Shull and D. M. Dennison, Phys. Rev. 71, 681 (1947), and 72, 256 (1947).en_US
dc.identifier.citedreferenceM. S. Livingston and H. A. Bethe, Revs. Modern Phys. 9, 245 (1937).en_US
dc.identifier.citedreferenceG. H. Briggs, Revs. Modern Phys. 26, 1 (1954).en_US
dc.identifier.citedreferenceThe method was proposed by Bach and Hockney, and has been demonstrated experimentally by Bach.en_US
dc.identifier.citedreferenceBrown, Snyder, Fowler, and Lauritsen, Phys. Rev. 82, 159 (1951), Appendices A, B, and C.en_US
dc.identifier.citedreferencePeterson, Fowler, and Lauritsen, Phys. Rev. 96, 1250 (1954), the un‐numbered formula, p. 1257.en_US
dc.identifier.citedreferenceEnge, Buechner, and Sperduto, Phys. Rev. 88, 963 (1952).en_US
dc.identifier.citedreferenceS. T. Butler, Proc. Roy. Soc. (London) A208, 559 (1951).en_US
dc.identifier.citedreferenceFor this and for other references see the review article by S. K. Allison and S. D. Warshaw, Revs. Modern Phys. 25, 779 (1953).en_US
dc.owningcollnamePhysics, Department of


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