The laser control of the muon g -2 experiment at Fermilab

Anastasi, A.; Anastasio, A.; Avino, S.; Basti, A.; Bedeschi, F.; Boiano, A.; Cantatore, G.; Cauz, D.; Ceravolo, S.; Corradi, G.; Dabagov, S.; Meo, P. Di; Driutti, A.; Sciascio, G. Di; Stefano, R. Di; Escalante, O.; Ferrari, C.; Fienberg, A. T.; Fioretti, A.; Gabbanini, C.; Gagliardi, G.; Gioiosa, A.; Hampai, D.; Hertzog, D. W.; Iacovacci, M.; Incagli, M.; Karuza, M.; Kaspar, J.; Lusiani, A.; Marignetti, F.; Mastroianni, S.; Moricciani, D.; Nath, A.; Pauletta, G.; Piacentino, G. M.; Raha, N.; Santi, L.; Smith, M. W.; Venanzoni, G.

doi:10.1088/1748-0221/13/02/T02009

Title: The laser control of the muon g -2 experiment at Fermilab

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Abstract

Here, we present that the Muon g-2 Experiment at Fermilab is expected to start data taking in 2017. It will measure the muon anomalous magnetic moment, a_μ = (g_μ-2)/2 to an unprecedented precision: the goal is 0.14 parts per million (ppm). The new experiment will require upgrades of detectors, electronics and data acquisition equipment to handle the much higher data volumes and slightly higher instantaneous rates. In particular, it will require a continuous monitoring and state-of-art calibration of the detectors, whose response may vary on both the millisecond and hour long timescale. The calibration system is composed of six laser sources and a light distribution system will provide short light pulses directly into each crystal (54) of the 24 calorimeters which measure energy and arrival time of the decay positrons. A Laser Control board will manage the interface between the experiment and the laser source, allowing the generation of light pulses according to specific needs including detector calibration, study of detector performance in running conditions, evaluation of DAQ performance. Here we present and discuss the main features of the Laser Control board.

Publication Date:: Thu Nov 09 00:00:00 EST 2017

Research Org.:: Fermi National Accelerator Lab. (FNAL), Batavia, IL (United States)

Sponsoring Org.:: USDOE Office of Science (SC), High Energy Physics (HEP)

Contributing Org.:: Muon g-2 Collaboration

OSTI Identifier:: 1409836

Report Number(s):: FERMILAB-PUB-17-502-E
Journal ID: ISSN 1748-0221; 1637523

Grant/Contract Number:: AC02-07CH11359

Resource Type:: Accepted Manuscript

Journal Name:: Journal of Instrumentation

Additional Journal Information:: Journal Volume: 13; Journal Issue: 02; Journal ID: ISSN 1748-0221

Publisher:: Institute of Physics (IOP)

Country of Publication:: United States

Language:: English

Subject:: 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; Laser Calibration; FPGA

Citation Formats


                    Anastasi, A., Anastasio, A., Avino, S., Basti, A., Bedeschi, F., Boiano, A., Cantatore, G., Cauz, D., Ceravolo, S., Corradi, G., Dabagov, S., Meo, P. Di, Driutti, A., Sciascio, G. Di, Stefano, R. Di, Escalante, O., Ferrari, C., Fienberg, A. T., Fioretti, A., Gabbanini, C., Gagliardi, G., Gioiosa, A., Hampai, D., Hertzog, D. W., Iacovacci, M., Incagli, M., Karuza, M., Kaspar, J., Lusiani, A., Marignetti, F., Mastroianni, S., Moricciani, D., Nath, A., Pauletta, G., Piacentino, G. M., Raha, N., Santi, L., Smith, M. W., and Venanzoni, G. The laser control of the muon g -2 experiment at Fermilab.  United States: N. p., 2017. 
Web.  doi:10.1088/1748-0221/13/02/T02009.

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                    Anastasi, A., Anastasio, A., Avino, S., Basti, A., Bedeschi, F., Boiano, A., Cantatore, G., Cauz, D., Ceravolo, S., Corradi, G., Dabagov, S., Meo, P. Di, Driutti, A., Sciascio, G. Di, Stefano, R. Di, Escalante, O., Ferrari, C., Fienberg, A. T., Fioretti, A., Gabbanini, C., Gagliardi, G., Gioiosa, A., Hampai, D., Hertzog, D. W., Iacovacci, M., Incagli, M., Karuza, M., Kaspar, J., Lusiani, A., Marignetti, F., Mastroianni, S., Moricciani, D., Nath, A., Pauletta, G., Piacentino, G. M., Raha, N., Santi, L., Smith, M. W., & Venanzoni, G. The laser control of the muon g -2 experiment at Fermilab.  United States.  https://doi.org/10.1088/1748-0221/13/02/T02009

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                    Anastasi, A., Anastasio, A., Avino, S., Basti, A., Bedeschi, F., Boiano, A., Cantatore, G., Cauz, D., Ceravolo, S., Corradi, G., Dabagov, S., Meo, P. Di, Driutti, A., Sciascio, G. Di, Stefano, R. Di, Escalante, O., Ferrari, C., Fienberg, A. T., Fioretti, A., Gabbanini, C., Gagliardi, G., Gioiosa, A., Hampai, D., Hertzog, D. W., Iacovacci, M., Incagli, M., Karuza, M., Kaspar, J., Lusiani, A., Marignetti, F., Mastroianni, S., Moricciani, D., Nath, A., Pauletta, G., Piacentino, G. M., Raha, N., Santi, L., Smith, M. W., and Venanzoni, G. Thu .  
"The laser control of the muon g -2 experiment at Fermilab".  United States.  https://doi.org/10.1088/1748-0221/13/02/T02009.  https://www.osti.gov/servlets/purl/1409836.

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@article{osti_1409836,

  title        = {The laser control of the muon g -2 experiment at Fermilab},

  author       = {Anastasi, A. and Anastasio, A. and Avino, S. and Basti, A. and Bedeschi, F. and Boiano, A. and Cantatore, G. and Cauz, D. and Ceravolo, S. and Corradi, G. and Dabagov, S. and Meo, P. Di and Driutti, A. and Sciascio, G. Di and Stefano, R. Di and Escalante, O. and Ferrari, C. and Fienberg, A. T. and Fioretti, A. and Gabbanini, C. and Gagliardi, G. and Gioiosa, A. and Hampai, D. and Hertzog, D. W. and Iacovacci, M. and Incagli, M. and Karuza, M. and Kaspar, J. and Lusiani, A. and Marignetti, F. and Mastroianni, S. and Moricciani, D. and Nath, A. and Pauletta, G. and Piacentino, G. M. and Raha, N. and Santi, L. and Smith, M. W. and Venanzoni, G.},

  abstractNote = {Here, we present that the Muon g-2 Experiment at Fermilab is expected to start data taking in 2017. It will measure the muon anomalous magnetic moment, aμ = (gμ-2)/2 to an unprecedented precision: the goal is 0.14 parts per million (ppm). The new experiment will require upgrades of detectors, electronics and data acquisition equipment to handle the much higher data volumes and slightly higher instantaneous rates. In particular, it will require a continuous monitoring and state-of-art calibration of the detectors, whose response may vary on both the millisecond and hour long timescale. The calibration system is composed of six laser sources and a light distribution system will provide short light pulses directly into each crystal (54) of the 24 calorimeters which measure energy and arrival time of the decay positrons. A Laser Control board will manage the interface between the experiment and the laser source, allowing the generation of light pulses according to specific needs including detector calibration, study of detector performance in running conditions, evaluation of DAQ performance. Here we present and discuss the main features of the Laser Control board.},

  doi          = {10.1088/1748-0221/13/02/T02009},

  journal      = {Journal of Instrumentation},

  number       = 02,

  volume       = 13,

  place        = {United States},

  year         = {Thu Nov 09 00:00:00 EST 2017},

  month        = {Thu Nov 09 00:00:00 EST 2017}

}

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