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== History and Development ==
[[File:Koinzidenzdetector.png|thumb|right|Coincidence measurement in simplified depiction.]]
PAC goes back to a theoretical work by Donald R. Hamilton <ref>Donald R. Hamilton: On Directional Correlation of Successive Quanta. In: Physical Review. Band 58, Nr. 2, 15. Juli 1940, S. 122–131, doi:10.1103/PhysRev.58.122</ref> from 1940. The first successful experiment was carried out by Brady and Deutsch <ref>Edward L. Brady, Martin Deutsch: Angular Correlation of Successive Gamma-Ray Quanta. In: Physical Review. Band 72, Nr. 9, 1. November 1947, S. 870–871, doi:10.1103/PhysRev.72.870</ref> in 1947. Essentially spin and parity of nuclear spins were investigated in these first PAC experiments. However, it was recognized early on that electric and magnetic fields interact with the nuclear moment,<ref>H. Aeppli, A.S. Bishop, H. Frauenfelder, M. Walter, W. Zünti, Phys. Rev. 82 (1951) 550.</ref>
Step by step the theory was developed.<ref>J.W. Gardner, Proc. Phys. Soc. (London) A62 (1949) 763.</ref><ref>D.S. Ling, D.L. Falkoff, Phys, Rev. 76 (1949) 1639.</ref><ref>M. Fierz, Helv. Phys. Acta 22 (1949) 489.</ref><ref>J.A. Spiers, Nat. Res. Council Canada, Publ. No. 1925 (1950) Phys. Rev. 80 (1950) 491.</ref><ref>D.L. Falkoff, G.E. Uhlenboeck, Phys. Rev. 79 (1950) 232.</ref><ref>G. Racah, Phys. Rev. 84 (1951) 910.</ref><ref>U. Fano, Nat'l. Bureau of Standards Report 1214; Phys. Rev. 90 (1953)577.</ref><ref>S.P. Lloyd, Phys. Rev. 85 (1952) 904.</ref><ref>K. Adler, Helv. Phys. Acta 25 (1952) 235.</ref><ref>S.R. de Groot, Physica 18 (1952) 1201.</ref><ref>F. Coester, J.M. Jauch, Helv. Phys. Acta 26 (1953) 3.</ref><ref>L.C. Biedenharn, M.E. Rose, Rev. Mod. Phys. 25 (1953) 729.</ref>
After Abragam and Pound <ref>A. Abragam, R. V. Pound: Influence of Electric and Magnetic Fields on Angular Correlations. In: Physical Review. Band 92, Nr. 4, 15. November 1953, S. 943–962, doi:10.1103/PhysRev.92.943</ref> published their work on the theory of PAC in 1953
While until about 2008 PAC instruments used conventional high-frequency electronics of the 1970s, in 2008 Christian Herden and Jens Röder et al. developed the first fully-digitized PAC instrument that enables extensive data analysis and parallel use of multiple probes.<ref>C. Herden, J. Röder, J. A. Gardner, K. D. Becker: Fully digital time differential perturbed angular correlation (TDPAC) spectrometer. In: Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. Band 594, Nr. 2, 1. September 2008, S. 155–161, doi:10.1016/j.nima.2008.05.001</ref> Replicas and further developments followed.<ref>Matthias Nagl, Ulrich Vetter, Michael Uhrmacher, Hans Hofsäss: A new all-digital time differential γ-γ angular correlation spectrometer. In: Review of Scientific Instruments. Band 81, Nr. 7, 1. Juli 2010, S. 073501, doi:10.1063/1.3455186</ref><ref>M. Jäger, K. Iwig, T. Butz: A user-friendly fully digital TDPAC-spectrometer. In: Hyperfine Interactions. Band 198, Nr. 1, 1. Juni 2010, S. 167–172, doi:10.1007/s10751-010-0201-8</ref>
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== Laboratories ==
The currently largest PAC laboratory in the world is located at [[ISOLDE]] in [[CERN]] with about 10 PAC instruments, that receives its major funding form [[BMBF]]. Radioactive ion beams are produced at the ISOLDE by bombarding protons from the booster onto target materials (uranium carbide, liquid tin, etc.) and evaporating the spallation products at high temperatures (up to 2000 °C), then ionizing them and then accelerating them. With the subsequent mass separation usually very pure isotope beams can be produced, which can be implanted in PAC samples. Of particular interest to the PAC are short-lived isomeric probes such as: <sup>111m</sup>Cd, <sup>199m</sup>Hg, <sup>204m</sup>Pb, and various rare earth probes.
== Theory ==
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{{Reflist}}
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[[Category:Nuclear physics]]
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