@article{Paschalis2013,
abstract = {The Gamma-Ray Energy Tracking In-beam Nuclear Array (GRETINA) is a new generation high-resolution $\gamma$-ray spectrometer consisting of electrically segmented high-purity germanium crystals. GRETINA is capable of reconstructing the energy and position of each $\gamma$-ray interaction point inside the crystal with high resolution. This enables $\gamma$-ray energy tracking which in turn provides an array with large photopeak efficiency, high resolution and good peak-to-total ratio. GRETINA is used for nuclear structure studies with demanding $\gamma$-ray detection requirements and it is suitable for experiments with radioactive-ion beams with high recoil velocities. The GRETINA array has a 1$\pi$ solid angle coverage and constitutes the first stage towards the full 4$\pi$ array GRETA. We present in this paper the main parts and the performance of the GRETINA system. {\textcopyright} 2013 Elsevier B.V. All rights reserved.},
author = {Paschalis, S. and Lee, I. Y. and MacChiavelli, A. O. and Campbell, C. M. and Cromaz, M. and Gros, S. and Pavan, J. and Qian, J. and Clark, R. M. and Crawford, H. L. and Doering, D. and Fallon, P. and Lionberger, C. and Loew, T. and Petri, M. and Stezelberger, T. and Zimmermann, S. and Radford, D. C. and Lagergren, K. and Weisshaar, D. and Winkler, R. and Glasmacher, T. and Anderson, J. T. and Beausang, C. W.},
doi = {10.1016/j.nima.2013.01.009},
issn = {01689002},
journal = {Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment},
keywords = {Ge $\gamma$-ray energy tracking arrays,HPGe detectors,Segmented Ge crystals,$\gamma$-ray tracking},
pages = {44--55},
title = {{The performance of the Gamma-Ray Energy Tracking In-beam Nuclear Array GRETINA}},
volume = {709},
year = {2013}
}

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This enables $\\gamma$-ray energy tracking which in turn provides an array with large photopeak efficiency, high resolution and good peak-to-total ratio. GRETINA is used for nuclear structure studies with demanding $\\gamma$-ray detection requirements and it is suitable for experiments with radioactive-ion beams with high recoil velocities. The GRETINA array has a 1$\\pi$ solid angle coverage and constitutes the first stage towards the full 4$\\pi$ array GRETA. We present in this paper the main parts and the performance of the GRETINA system. \\textcopyright 2013 Elsevier B.V. All rights reserved.","author":[{"propositions":[],"lastnames":["Paschalis"],"firstnames":["S."],"suffixes":[]},{"propositions":[],"lastnames":["Lee"],"firstnames":["I.","Y."],"suffixes":[]},{"propositions":[],"lastnames":["MacChiavelli"],"firstnames":["A.","O."],"suffixes":[]},{"propositions":[],"lastnames":["Campbell"],"firstnames":["C.","M."],"suffixes":[]},{"propositions":[],"lastnames":["Cromaz"],"firstnames":["M."],"suffixes":[]},{"propositions":[],"lastnames":["Gros"],"firstnames":["S."],"suffixes":[]},{"propositions":[],"lastnames":["Pavan"],"firstnames":["J."],"suffixes":[]},{"propositions":[],"lastnames":["Qian"],"firstnames":["J."],"suffixes":[]},{"propositions":[],"lastnames":["Clark"],"firstnames":["R.","M."],"suffixes":[]},{"propositions":[],"lastnames":["Crawford"],"firstnames":["H.","L."],"suffixes":[]},{"propositions":[],"lastnames":["Doering"],"firstnames":["D."],"suffixes":[]},{"propositions":[],"lastnames":["Fallon"],"firstnames":["P."],"suffixes":[]},{"propositions":[],"lastnames":["Lionberger"],"firstnames":["C."],"suffixes":[]},{"propositions":[],"lastnames":["Loew"],"firstnames":["T."],"suffixes":[]},{"propositions":[],"lastnames":["Petri"],"firstnames":["M."],"suffixes":[]},{"propositions":[],"lastnames":["Stezelberger"],"firstnames":["T."],"suffixes":[]},{"propositions":[],"lastnames":["Zimmermann"],"firstnames":["S."],"suffixes":[]},{"propositions":[],"lastnames":["Radford"],"firstnames":["D.","C."],"suffixes":[]},{"propositions":[],"lastnames":["Lagergren"],"firstnames":["K."],"suffixes":[]},{"propositions":[],"lastnames":["Weisshaar"],"firstnames":["D."],"suffixes":[]},{"propositions":[],"lastnames":["Winkler"],"firstnames":["R."],"suffixes":[]},{"propositions":[],"lastnames":["Glasmacher"],"firstnames":["T."],"suffixes":[]},{"propositions":[],"lastnames":["Anderson"],"firstnames":["J.","T."],"suffixes":[]},{"propositions":[],"lastnames":["Beausang"],"firstnames":["C.","W."],"suffixes":[]}],"doi":"10.1016/j.nima.2013.01.009","issn":"01689002","journal":"Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment","keywords":"Ge $\\gamma$-ray energy tracking arrays,HPGe detectors,Segmented Ge crystals,$\\gamma$-ray tracking","pages":"44–55","title":"The performance of the Gamma-Ray Energy Tracking In-beam Nuclear Array GRETINA","volume":"709","year":"2013","bibtex":"@article{Paschalis2013,\nabstract = {The Gamma-Ray Energy Tracking In-beam Nuclear Array (GRETINA) is a new generation high-resolution $\\gamma$-ray spectrometer consisting of electrically segmented high-purity germanium crystals. GRETINA is capable of reconstructing the energy and position of each $\\gamma$-ray interaction point inside the crystal with high resolution. This enables $\\gamma$-ray energy tracking which in turn provides an array with large photopeak efficiency, high resolution and good peak-to-total ratio. GRETINA is used for nuclear structure studies with demanding $\\gamma$-ray detection requirements and it is suitable for experiments with radioactive-ion beams with high recoil velocities. The GRETINA array has a 1$\\pi$ solid angle coverage and constitutes the first stage towards the full 4$\\pi$ array GRETA. We present in this paper the main parts and the performance of the GRETINA system. {\\textcopyright} 2013 Elsevier B.V. All rights reserved.},\nauthor = {Paschalis, S. and Lee, I. Y. and MacChiavelli, A. O. and Campbell, C. M. and Cromaz, M. and Gros, S. and Pavan, J. and Qian, J. and Clark, R. M. and Crawford, H. 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