CMOS low noise monolithic frontends for Si strip detector readout

Aspell, P.; Boulter, R.; Czermak, A.; Jałocha, P.; Jarron, P.; Kjensmo, A.; Lange, W.; Nygård, E.; Rudge, A.; Toker, O.; Turała, M.; Lippe, H. von der; Walz, U.; Weilhammer, P.; Yoshioka, K.

doi:10.1016/0168-9002(92)90740-u

Cited by 31 publications

(6 citation statements)

References 2 publications

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“…The ver tex detector comprises amplifying multichannel inte grated circuits of two types: -Gassiplex chips [39] (16 channels, 10 MHz), which amplify the signals from the sensors of beam telescope MS 1 -MS 6 and vertex telescope MS 12 -MS 17 (Fig. 8, on the left); and -Viking chips [40] (128 channels, 10 MHz), which amplify the signals from sensors MS 18 -MS 21 of the tracking system (Fig. 8, on the right).…”

Section: A Vertex Microstrip Detectormentioning

confidence: 99%

Spectrometer with a vertex detector for experiments at the IHEP accelerator

et al. 2013

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The stages of development and the current status of the versatile "Spectrometer with a Vertex Detector" setup designed for physics experiments at the U 70 accelerator of the Institute for High Energy Physics (Protvino) is described. The main detectors of the setup are the vertex detector based on silicon microstrip detectors, the wide aperture magnetic spectrometer based on multiwire proportional chambers, and the lead glass hodoscope γ detector. In the setup, there is a fast two level trigger system for selecting required particle interactions. The key characteristics of the setup systems are presented, and the physical results obtained on it are briefly listed. * To study the dependence of the cross sections on the atomic number of the nucleus, a passive target-a lead foil 220 µm thick-is located at a point with Z coordinate of +8 mm, and the passive target-a carbon plate 500 µm thick-is located at a point with Z coordinate of +16 mm.

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Section: A Vertex Microstrip Detectormentioning

confidence: 99%

Spectrometer with a vertex detector for experiments at the IHEP accelerator

et al. 2013

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“…For example the original microstrip work (Borchelt [34]) made use of the 'Viking' multichannel amplifier and shaper integrated circuit, as previously mentioned. This device is described in Aspell [77]. It is a CMOS chip with 128 channels each containing a charge amplifier, a CR-RC charge shaper, and a sample-and-hold circuit.…”

Section: Electronics For Diamondmentioning

confidence: 99%

Diamond detectors in particle physics

Tapper

2000

Rep. Prog. Phys.

102

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Particle detectors made from artificial diamond have great promise for future experiments in particle physics because they are far less vulnerable to radiation damage than any other detector type. We review the history of diamond detectors and describe their current state of development. We also discuss the evidence which proves the resistance of these detectors to damage by various forms of incident radiation.

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“…Section 2 describes the basic structure of the KW01 and details the circuit schematics. The ASIC employs a newly designed high-impedance circuit instead of an FET used as a transfer gate for a feedback component, as is often used in several low-noise ASICs [12][13][14][15][16][17][18]. Section 3 presents the setup of the performance measurements.…”

Section: Introductionmentioning

confidence: 99%

Development of a low-noise analog front-end ASIC for CdTe detectors

Kishishita

Ikeda

Kiyuna³

et al. 2007

Nuclear Instruments and Methods in Physics Research Section A:

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This paper describes the recent development of a low-noise analog front-end ASIC for CdTe detectors. The ASIC is designed on the basis of the Open-IP LSI project led by JAXA and implemented using TSMC 0.35-mm CMOS technology. The ASIC contains eight identical channels, each of which includes a charge-sensitive amplifier, band-pass filters, and a sample-and-hold circuit. Preliminary testing of the ASIC achieved noise performance of 188e À þ 7:5e À =pF. In order to verify the low-noise characteristics, the ASIC was connected to a guard-ring-equipped CdTe diode detector with dimensions of 2:4 Â 2:4 mm and having a thickness of 0.5 mm. As a result, the gamma-ray spectra of radioactive sources were obtained with good energy resolutions of 2.51 and 2.35 keV (FWHM) for gamma rays of 59.5 and 122 keV, respectively, at room temperature. r

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CMOS low noise monolithic frontends for Si strip detector readout

Cited by 31 publications

References 2 publications

Spectrometer with a vertex detector for experiments at the IHEP accelerator

Spectrometer with a vertex detector for experiments at the IHEP accelerator

Diamond detectors in particle physics

Development of a low-noise analog front-end ASIC for CdTe detectors

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