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Year Type Titledown Conference Journal
2001PSI Annual reportThe MSCB bus PSI Annual Report 01
Attachment 1: mscb.ps
mscb.ps mscb.ps
Attachment 2: mscb.tex
\title{The MSCB bus - a field bus tailored to particle physics experiments}
\author{S.~Ritt$^{1}$, R.~Schmidt$^{1}$ }
% You can optionally add the proposal numer and institutes, e.g.
\collaboration{R-99-05}{PSI$^{1}$}
% \abstract{ put your abstract here, this is optional}

\begin{contribution}

Particle physics experiments require what is commonly referred to as "slow control". This includes the measurement and control of environment variables such as temperature, pressure and humidity as well as the control of high voltages for photomultipliers and wire chambers. While most experiment use an inhomogeneous mix of systems involving RS232, GPIB and PLCs, the MUEGAMMA experiment (R-99-05) will use a new slow control system developed at PSI, called MSCB (Midas Slow Control Bus). This system will be used for the 960 high voltage channels of the experiment, for the control of the liquid xenon calorimeter and for the superconducting solenoid. The integration of all these systems into the central data acquisition and control system is essential for the long-term stability of the experiment.

The MSCB system uses a field bus- like architecture, where a number of "nodes" are connected to a serial bus, which is controlled by a central PC. Each node contains ADCs, DACs and digital I/O for measurement and controlling tasks. For critical installations the control PC can be backed up by a secondary PC for redundancy. The PCs are connected to the Midas DAQ system~\cite{R99-05:midas}, which allows for remote operation through a Web interface, history display, automatic alarm notification and for logging of slow control variables to tape. 

The hardware of a MSCB node is designed around a new generation of microcontrollers, which contain a 8051- compatible microcontroller core, ADCs, DACs and digital I/O on a single chip. We currently use the ADuC812~\cite{R99-05:aduc} from Analog Devices and the C8051F000 from Cygnal~\cite{R99-05:cygnal}. The nodes are connected via an RS-485 bus running at 384 kBaud. A segment can contain 256 nodes, and with one layer of repeaters 65536 nodes can be connected and addressed on a single bus. Two versions of MSCB nodes have been developed. A stand-alone module (Fig.~\ref{R99-05:node}) which can be embedded directly on a sensor or on an electronics board is powered from the bus, which uses a 10-wire twisted pair flat ribbon cable for distances up to 500 m. The production cost of such a node is about 50 CHF. A development kit for the Cygnal controller which includes a C compiler costs 99 US\$.

\begin{figure}[htb]
   \centering
   \includegraphics[width=1.0\linewidth]{R99-05-fig1.eps}
   \caption{Stand-alone node with an RS-485 transceiver, eight channel 12-bit ADC, two channel 12-bit DAC, 16-bit digital I/O and a temperature sensor. The right connector is for the MSCB bus, the one at the back for an optional LCD display.}
\label{R99-05:node}
\end{figure}                                      

In addition to the stand-alone module, a 19" rack system which hosts cards containing a MSCB node and signal conditioning, has been designed. Cards were made for voltage, current and temperature measurements as well as to control 220V consumers such as heaters. The MSCB bus runs on the back plane of the crate.

Using the local intelligence of the node controller, regulation loops (PID) and interlock systems can be realized without intervention of the central control PC. The nodes run a simple framework for the communication with the host system, which guarantees real-time behaviour. User routines can be added to implement application- specific logic. The nodes can be reprogrammed over the RS-485 bus. 

The MSCB protocol was optimised for minimal overhead. A 16-bit value from a node can be read out by sending a request of three bytes and receiving an reply of four bytes, both including a code (CRC) to avoid data corruption. Depending on the number of nodes,  a MSCB system can either use 8-bit or 16-bit addressing. A node can contain up to 256 "channels" for reading and writing and up to 256 "configuration parameters", which are stored in the EEPROM of the node and can for example be used as constants for PID regulation. Each channel and parameter is described by a set of attributes such as name, physical units and status. These attributes are stored in each node and can be queried from the control PC, making the configuration of large networks very simple. A special repeat mode has been defined which allows the readout of a series of nodes in less than 300 $\mu s$ per node.

For the control PC a "C" library has been developed running under Windows and Linux. Based on this library, a LabView driver and a driver for the Midas DAQ system are available. Simple LabView applications such as a data logger with graphical display has been implemented.

A prototype of the MSCB rack system is currently used for the pressure and high voltage control of the new proportional chamber for the SINQ POLDI detector. 

The final system will be available from the PSI electronics pool in spring 2002 upon request. It can be concluded that the MSCB system is an attractive alternative to GPIB multimeters and to Programmable Logic Controllers with respect to cost and integration. For more information visit the MSCB home page at http://midas.psi.ch/mscb.

\begin{thebibliography}{9}
\bibitem {R99-05:midas} MIDAS home page http://midas.psi.ch
\bibitem {R99-05:aduc} http://products.analog.com/products/info.asp?product= AduC812
\bibitem {R99-05:cygnal} http://www.cygnal.com/products/C8051F000.htm
\end{thebibliography}

\end{contribution}
2010ArticleThe MEG tiiming counter calibration and performance Nuclear Instruments and Methods In Physics Research A
Attachment 1: TC_NIM.pdf
TC_NIM.pdf TC_NIM.pdf TC_NIM.pdf TC_NIM.pdf TC_NIM.pdf TC_NIM.pdf
2009Conference with proceedingsThe MEG spectrometer at PSIThe 1st international conference on Technology and Instrumentation in Particle PhysicsNuclear Instrumentations and Methods in Physics Research, Section A
Attachment 1: EDS_I_3_cattaneo.pdf
EDS_I_3_cattaneo.pdf EDS_I_3_cattaneo.pdf EDS_I_3_cattaneo.pdf
2006Conference with proceedingsThe MEG positron spectrometer10th Topical Seminar on Innovative Particle and Radiation DetectorsNuclear Physics B (Proc. Suppl.)
2007Conference with proceedingsThe MEG positron spectrometer11th International Vienna Conference on InstrumentationNucl. Instr. and Meth. A
2002Conference with proceedingsThe MEG experiment: status and prospects4th International Workshop on Neutrino Factories (NuFact02)J. Phys. G: Nucl. Part. Phys.
Attachment 1: gio_nufact02.ppt
2013Conference with proceedingsThe MEG experiment upgradePontecorvo 100: Symposium in honour of Bruno Pontecorvo for the centennial of the birthNuovo Cim. C
2005Conference with proceedingsThe MEG experiment at PSI: status and prospectsParticles and Nuclei International Conference (PANIC05)AIP Conf. Proc.
Attachment 1: Panic05.pdf
Panic05.pdf Panic05.pdf Panic05.pdf
Attachment 2: signorelli_panic05.pdf
signorelli_panic05.pdf signorelli_panic05.pdf signorelli_panic05.pdf signorelli_panic05.pdf signorelli_panic05.pdf signorelli_panic05.pdf signorelli_panic05.pdf signorelli_panic05.pdf
2008ConferenceThe MEG experiment at PSI: status and prospects18th International Conference on Particles and Nuclei (PANIC 08) 
Attachment 1: Signorelli_PANIC08.pdf
Signorelli_PANIC08.pdf Signorelli_PANIC08.pdf Signorelli_PANIC08.pdf Signorelli_PANIC08.pdf Signorelli_PANIC08.pdf Signorelli_PANIC08.pdf Signorelli_PANIC08.pdf Signorelli_PANIC08.pdf
2006ConferenceThe MEG experiment at PSI: search for the mu to e gamma decaySummer School and Conference on New Trends in High Energy Physics 
Attachment 1: signorelli_yalta.pdf
signorelli_yalta.pdf signorelli_yalta.pdf signorelli_yalta.pdf signorelli_yalta.pdf signorelli_yalta.pdf signorelli_yalta.pdf signorelli_yalta.pdf signorelli_yalta.pdf
2003Conference with proceedingsThe MEG experiment at PSI: a sensitive search for mu -> e gamma decay.15th Conference on High Energy Physics (IFAE 2003)Italian Phys. Soc. Proc.
Attachment 1: ifae2003.pdf
ifae2003.pdf ifae2003.pdf ifae2003.pdf ifae2003.pdf
Attachment 2: fc_lecce03.ppt
2004Conference with proceedingsThe MEG experiment at PSI: Status and prospect6th International Workshop on Neutrino Factories and Superbeams (NuFact 04)Nucl. Phys. B Proc. Suppl.
Attachment 1: 1-s2.0-S0920563205007395-main.pdf
1-s2.0-S0920563205007395-main.pdf 1-s2.0-S0920563205007395-main.pdf 1-s2.0-S0920563205007395-main.pdf
2008Conference with proceedingsThe MEG experiment at PSINeutrino Oscillation Workshop (NOW2008)Nucl. Phys. B Proc. Suppl.
Attachment 1: fc_now08.ppt
2013ArticleThe MEG detector for µ+→e+γ decay search Eur. Phys. J. C

http://arxiv.org/abs/1303.2348

Attachment 1: Adam_et_al._-_2013_-_The_MEG_detector_for_μ_→e_γ_decay_search(2).pdf
Adam_et_al._-_2013_-_The_MEG_detector_for_μ_→e_γ_decay_search(2).pdf Adam_et_al._-_2013_-_The_MEG_detector_for_μ_→e_γ_decay_search(2).pdf Adam_et_al._-_2013_-_The_MEG_detector_for_μ_→e_γ_decay_search(2).pdf Adam_et_al._-_2013_-_The_MEG_detector_for_μ_→e_γ_decay_search(2).pdf Adam_et_al._-_2013_-_The_MEG_detector_for_μ_→e_γ_decay_search(2).pdf Adam_et_al._-_2013_-_The_MEG_detector_for_μ_→e_γ_decay_search(2).pdf Adam_et_al._-_2013_-_The_MEG_detector_for_μ_→e_γ_decay_search(2).pdf Adam_et_al._-_2013_-_The_MEG_detector_for_μ_→e_γ_decay_search(2).pdf
2004Conference with proceedingsThe MEG Experiment Study of the Origin of Mν by Searching for Lepton Flavor Violation in Charged Leptons5th Workshop on Neutrino Oscillations and their Origin (NOON2004)World Scientific
2003PSI Annual reportThe MEG Experiment PSI Annual Report 03
Attachment 1: MEG03.pdf
MEG03.pdf
2006Conference with proceedingsThe Liquid Xenon Calorimeter of the MEG experiment18th Conference on High Energy Physics (IFAE 2006) 
Attachment 1: fc_pavia06.ppt
2014Conference with proceedingsThe LXe calorimeter and the pixelated timing counter in the MEG II experimentINSTR-14JINST
2009Conference with proceedingsThe Drift Chamber System of the MEG ExperimentThe 1st international conference on Technology and Instrumentation in Particle Physics 2009Nuclear Instruments and Methods in Physics Research, Section A
Attachment 1: GAS_IV_1_Hildebrandt.pdf
GAS_IV_1_Hildebrandt.pdf GAS_IV_1_Hildebrandt.pdf GAS_IV_1_Hildebrandt.pdf
2002ConferenceThe Detector for the New µ → eγ Experiment MEG31st International Conference on High Energy Physics (ICHEP02) 
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