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000483405 0247_ $$2INSPIRETeX$$aChauhan:2022inm
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000483405 0247_ $$2arXiv$$aarXiv:2210.09810
000483405 0247_ $$2datacite_doi$$a10.3204/PUBDB-2022-05293
000483405 037__ $$aPUBDB-2022-05293
000483405 041__ $$aEnglish
000483405 082__ $$a530
000483405 088__ $$2arXiv$$aarXiv:2210.09810
000483405 1001_ $$aChauhan, Ankur$$b0
000483405 245__ $$aTowards a New Generation of Monolithic Active Pixel Sensors
000483405 260__ $$c2022
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000483405 500__ $$a3 pages, 2 figures, presented at 15th Pisa Meeting on Advanced Detectors
000483405 520__ $$aA new generation of Monolithic Active Pixel Sensors (MAPS), produced in a 65 nm CMOS imaging process, promises higher densities of on-chip circuits and, for a given pixel size, more sophisticated in-pixel logic compared to larger feature size processes. MAPS are a cost-effective alternative to hybrid pixel sensors since flip-chip bonding is not required. In addition, they allow for significant reductions of the material budget of detector systems, due to the smaller physical thicknesses of the active sensor and the absence of a separate readout chip. The TANGERINE project develops a sensor suitable for future Higgs factories as well as for a beam telescope to be used at beam-test facilities. The sensors will have small collection electrodes (order of $\mu$m) to maximize the signal-to-noise ratio, which makes it possible to minimize power dissipation in the circuitry. The first batch of test chips, featuring full front-end amplifiers with Krummenacher feedback, was produced and tested at the Mainzer Mikrotron (MAMI) at the end of 2021. MAMI provides an electron beam with currents up to 100 $\mu$A and an energy of 855 MeV. The analog output signal of the test chips was recorded with a high bandwidth oscilloscope and used to study the charge-sensitive amplifier of the chips in terms of waveform analysis. A beam telescope was used as a reference system to allow for track-based analysis of the recorded data.
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000483405 588__ $$aDataset connected to INSPIRE
000483405 650_7 $$2INSPIRE$$adetector, pixel
000483405 650_7 $$2INSPIRE$$asemiconductor detector, pixel
000483405 650_7 $$2INSPIRE$$amatter, geometry
000483405 650_7 $$2INSPIRE$$apixel, size
000483405 650_7 $$2INSPIRE$$aelectron, beam
000483405 650_7 $$2INSPIRE$$adensity, high
000483405 650_7 $$2INSPIRE$$aamplifier
000483405 650_7 $$2INSPIRE$$aMainz Linac
000483405 650_7 $$2INSPIRE$$afeedback
000483405 650_7 $$2INSPIRE$$ahybrid
000483405 650_7 $$2INSPIRE$$areadout
000483405 650_7 $$2INSPIRE$$aimaging
000483405 650_7 $$2INSPIRE$$alogic
000483405 650_7 $$2INSPIRE$$adissipation
000483405 650_7 $$2INSPIRE$$aelectrode
000483405 650_7 $$2INSPIRE$$aHiggs-factory
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000483405 7001_ $$0M.D.Viera.2$$aViera, Manuel Del Rio$$b1
000483405 7001_ $$aEckstein, Doris$$b2
000483405 7001_ $$0P:(DE-H253)PIP1019720$$aFeindt, Finn$$b3$$eCorresponding author$$udesy
000483405 7001_ $$0P:(DE-H253)PIP1004563$$aGregor, Ingrid-Maria$$b4
000483405 7001_ $$aHansen, Karsten$$b5
000483405 7001_ $$aHuth, Lennart$$b6
000483405 7001_ $$0L.Helena.Mendes.1$$aMendes, Larissa$$b7
000483405 7001_ $$aMulyanto, Budi$$b8
000483405 7001_ $$aRastorguev, Daniil$$b9
000483405 7001_ $$aReckleben, Christian$$b10
000483405 7001_ $$0S.R.Daza.1$$aDaza, Sara Ruiz$$b11
000483405 7001_ $$aSchütze, Paul$$b12
000483405 7001_ $$aSimancas, Adriana$$b13
000483405 7001_ $$0P:(DE-H253)PIP1018940$$aSpannagel, Simon$$b14
000483405 7001_ $$0P:(DE-H253)PIP1014417$$aStanitzki, Marcel$$b15
000483405 7001_ $$aVelyka, Anastasiia$$b16
000483405 7001_ $$aVignola, Gianpiero$$b17
000483405 7001_ $$aWennlöf, Håkan$$b18
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000483405 9131_ $$0G:(DE-HGF)POF4-611$$1G:(DE-HGF)POF4-610$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMatter and the Universe$$vFundamental Particles and Forces$$x0
000483405 9141_ $$y2022
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000483405 9201_ $$0I:(DE-H253)FTX-20210408$$kFTX$$lTechnol. zukünft. Teilchenph. Experim.$$x2
000483405 9201_ $$0I:(DE-H253)FEC-20120731$$kFEC$$lMikro- und Optoelektronik$$x3
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