Characterization of AGIPD1.0: The full scale chip.

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Title: Characterization of AGIPD1.0: The full scale chip.
Authors: Mezza, D.1 davide.mezza@psi.ch, Allahgholi, A.2, Arino-Estrada, G.2, Bianco, L.2, Delfs, A.2, Dinapoli, R.1, Goettlicher, P.2, Graafsma, H.2,3, Greiffenberg, D.1, Hirsemann, H.2, Jack, S.2, Klanner, R.4, Klyuev, A.2, Krueger, H.5, Marras, A.2, Mozzanica, A.1, Poehlsen, J.2, Schmitt, B.1, Schwandt, J.4, Sheviakov, I.2
Source: Nuclear Instruments & Methods in Physics Research Section A. Dec2016, Vol. 838, p39-46. 8p.
Subjects: Integrated circuits, Gain measurement, Single photon generation, Computer simulation, Switching power supplies
Abstract: The AGIPD (adaptive gain integrating pixel detector) detector is a high frame rate (4.5 MHz) and high dynamic range (up to 10 4 ·12.4 keV photons) detector with single photon resolution (down to 4 keV taking 5 σ as limit and lowest noise settings) developed for the European XFEL (XFEL.EU). This work is focused on the characterization of AGIPD1.0, which is the first full scale version of the chip. The chip is 64×64 pixels and each pixel has a size of 200×200 μm 2 . Each pixel can store up to 352 images at a rate of 4.5 MHz (corresponding to 220 ns). A detailed characterization of the AGIPD1.0 chip has been performed in order to assess the main performance of the ASIC in terms of gain, noise, speed and dynamic range. From the measurements presented in this paper a good uniformity of the gain, a noise around 320 e − (rms) in standard mode and around 240 e − (rms) in high gain mode has been measured. Furthermore a detailed discussion about the non-linear behavior after the gain switching is presented with both experimental results and simulations. [ABSTRACT FROM AUTHOR]
Copyright of Nuclear Instruments & Methods in Physics Research Section A is the property of Elsevier B.V. and its content may not be copied or emailed to multiple sites without the copyright holder's express written permission. Additionally, content may not be used with any artificial intelligence tools or machine learning technologies. However, users may print, download, or email articles for individual use. This abstract may be abridged. No warranty is given about the accuracy of the copy. Users should refer to the original published version of the material for the full abstract. (Copyright applies to all Abstracts.)
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  Data: Characterization of AGIPD1.0: The full scale chip.
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  Data: <searchLink fieldCode="AR" term="%22Mezza%2C+D%2E%22">Mezza, D.</searchLink><relatesTo>1</relatesTo><i> davide.mezza@psi.ch</i><br /><searchLink fieldCode="AR" term="%22Allahgholi%2C+A%2E%22">Allahgholi, A.</searchLink><relatesTo>2</relatesTo><br /><searchLink fieldCode="AR" term="%22Arino-Estrada%2C+G%2E%22">Arino-Estrada, G.</searchLink><relatesTo>2</relatesTo><br /><searchLink fieldCode="AR" term="%22Bianco%2C+L%2E%22">Bianco, L.</searchLink><relatesTo>2</relatesTo><br /><searchLink fieldCode="AR" term="%22Delfs%2C+A%2E%22">Delfs, A.</searchLink><relatesTo>2</relatesTo><br /><searchLink fieldCode="AR" term="%22Dinapoli%2C+R%2E%22">Dinapoli, R.</searchLink><relatesTo>1</relatesTo><br /><searchLink fieldCode="AR" term="%22Goettlicher%2C+P%2E%22">Goettlicher, P.</searchLink><relatesTo>2</relatesTo><br /><searchLink fieldCode="AR" term="%22Graafsma%2C+H%2E%22">Graafsma, H.</searchLink><relatesTo>2,3</relatesTo><br /><searchLink fieldCode="AR" term="%22Greiffenberg%2C+D%2E%22">Greiffenberg, D.</searchLink><relatesTo>1</relatesTo><br /><searchLink fieldCode="AR" term="%22Hirsemann%2C+H%2E%22">Hirsemann, H.</searchLink><relatesTo>2</relatesTo><br /><searchLink fieldCode="AR" term="%22Jack%2C+S%2E%22">Jack, S.</searchLink><relatesTo>2</relatesTo><br /><searchLink fieldCode="AR" term="%22Klanner%2C+R%2E%22">Klanner, R.</searchLink><relatesTo>4</relatesTo><br /><searchLink fieldCode="AR" term="%22Klyuev%2C+A%2E%22">Klyuev, A.</searchLink><relatesTo>2</relatesTo><br /><searchLink fieldCode="AR" term="%22Krueger%2C+H%2E%22">Krueger, H.</searchLink><relatesTo>5</relatesTo><br /><searchLink fieldCode="AR" term="%22Marras%2C+A%2E%22">Marras, A.</searchLink><relatesTo>2</relatesTo><br /><searchLink fieldCode="AR" term="%22Mozzanica%2C+A%2E%22">Mozzanica, A.</searchLink><relatesTo>1</relatesTo><br /><searchLink fieldCode="AR" term="%22Poehlsen%2C+J%2E%22">Poehlsen, J.</searchLink><relatesTo>2</relatesTo><br /><searchLink fieldCode="AR" term="%22Schmitt%2C+B%2E%22">Schmitt, B.</searchLink><relatesTo>1</relatesTo><br /><searchLink fieldCode="AR" term="%22Schwandt%2C+J%2E%22">Schwandt, J.</searchLink><relatesTo>4</relatesTo><br /><searchLink fieldCode="AR" term="%22Sheviakov%2C+I%2E%22">Sheviakov, I.</searchLink><relatesTo>2</relatesTo>
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  Data: <searchLink fieldCode="JN" term="%22Nuclear+Instruments+%26+Methods+in+Physics+Research+Section+A%22">Nuclear Instruments & Methods in Physics Research Section A</searchLink>. Dec2016, Vol. 838, p39-46. 8p.
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  Data: <searchLink fieldCode="DE" term="%22Integrated+circuits%22">Integrated circuits</searchLink><br /><searchLink fieldCode="DE" term="%22Gain+measurement%22">Gain measurement</searchLink><br /><searchLink fieldCode="DE" term="%22Single+photon+generation%22">Single photon generation</searchLink><br /><searchLink fieldCode="DE" term="%22Computer+simulation%22">Computer simulation</searchLink><br /><searchLink fieldCode="DE" term="%22Switching+power+supplies%22">Switching power supplies</searchLink>
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  Label: Abstract
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  Data: The AGIPD (adaptive gain integrating pixel detector) detector is a high frame rate (4.5 MHz) and high dynamic range (up to 10 4 ·12.4 keV photons) detector with single photon resolution (down to 4 keV taking 5 σ as limit and lowest noise settings) developed for the European XFEL (XFEL.EU). This work is focused on the characterization of AGIPD1.0, which is the first full scale version of the chip. The chip is 64×64 pixels and each pixel has a size of 200×200 μm 2 . Each pixel can store up to 352 images at a rate of 4.5 MHz (corresponding to 220 ns). A detailed characterization of the AGIPD1.0 chip has been performed in order to assess the main performance of the ASIC in terms of gain, noise, speed and dynamic range. From the measurements presented in this paper a good uniformity of the gain, a noise around 320 e − (rms) in standard mode and around 240 e − (rms) in high gain mode has been measured. Furthermore a detailed discussion about the non-linear behavior after the gain switching is presented with both experimental results and simulations. [ABSTRACT FROM AUTHOR]
– Name: AbstractSuppliedCopyright
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  Data: <i>Copyright of Nuclear Instruments & Methods in Physics Research Section A is the property of Elsevier B.V. and its content may not be copied or emailed to multiple sites without the copyright holder's express written permission. Additionally, content may not be used with any artificial intelligence tools or machine learning technologies. However, users may print, download, or email articles for individual use. This abstract may be abridged. No warranty is given about the accuracy of the copy. Users should refer to the original published version of the material for the full abstract.</i> (Copyright applies to all Abstracts.)
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        Value: 10.1016/j.nima.2016.09.007
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        Text: English
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      – SubjectFull: Single photon generation
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      – SubjectFull: Computer simulation
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      – SubjectFull: Switching power supplies
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