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Neutron ToF Spectrometer NeuLAND

 

Responsible: GSI.

Work is performed within the NeuLAND Working Group.

Contact person: Konstanze Boretzky.

 

General Information   Milestones     Literature

General Information

NeuLAND (new Large-Area Neutron Detector) is the next-generation neutron detector designed for R3B which meets all requirements defined by the ambitious physics program proposed for the R3B facility. NeuLAND features a high detection efficiency, a high resolution, and a large multi-neutron-hit resolving power. This is achieved by a highly granular design of plastic scintillators, avoiding insensitive converter material. The detector will consist of 3000 individual submodules with a size of 5x5x250 cm3, arranged in 30 double planes with 100 submodules providing an active face size of 250x250 cm2 and a total depth of 3 m. NeuLAND can be divided into two detectors for special applications and will be placed at different distances from the target, in order to meet specific experimental demands. A momentum resolution of Δp/p of 10-3 similar to that for the charged particles is desired, resulting in resolution requirements for the time of flight of σ(t) < 150 ps and a position resolution of σ(x,y,z) ≈ 1.5 cm for given flight paths in the range from 10 to 35 m. For an experiment on a medium mass nucleus at about 500 MeV/nucleon, invariant-mass resolutions of about ΔE =20 keV at 200 keV above the neutron threshold (ΔE=30 keV at 1 MeV respectively) will be reached using the maximum flight path. Apart from the excellent energy resolution of NeuLAND, the enhanced multi-neutron recognition capability with an efficiency of up to ~50% for a reconstructed five-neutron event at 1 GeV (see tabels below) will constitute a major step forward.

Neutron separation matrices for multiplicities of 1 to 5 neutrons.
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Neutron separation matrices for multiplicities of 1 to 5 neutrons.
Neutron separation matrices for multiplicities of 1 to 5 neutrons.

 

The final design containing details of the technical realization including mechanics, readout electronics, submodules tests, calibrations, and the construction procedure and described in the NeuLAND Technical Report is the result of several years of R&D studies. Different design concepts have been followed, including converter-based solutions, e.g., a detector based on steel converter plus charged-particle detection with resistive-plate chambers (RPC). The RPC concept has been ruled out mainly because of its insufficient multi-neutron detection capability. A fully active detector with calorimetric properties has turned out to be the best solution. The NeuLAND Technical Design Report has been finalzed in 2011 and accepted by FAIR on January 18, 2013.

NeuLAND detector with frame arranged for moving double planes. Left: the front sides of both frames are put to minimum distance; Right: half of double planes have been moved to the second frame.
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NeuLAND detector with frame arranged for moving double planes. Left: the front sides of both frames are put to minimum distance; Right: half of double planes have been moved to the second frame.
NeuLAND detector with frame arranged for moving double planes. Left: the front sides of both frames are put to minimum distance; Right: half of double planes have been moved to the second frame.

In 2012, the prototype of the NeuLAND detector consisting of 150 bars has been tested at GSI resulting in time resolutions better than the required σ(t) ≤ 150 ps, even with inexpensive photomultipliers. In accordance with simulations, improved timing properties have been obtained with optimized light guides.

The construction of the detector has started in spring 2013. During Oct. 2014 the NeuLAND demonstrator ( 1/6 of the full size detector) was successfully tested in GSI beam times. The contious mounting of NeuLAND double-planes is carried out at GSI with a team from all contributing institutes guided by the R3B group in the RB project area. Necessary quality controls have been established. The construction scheme allows the production of one double-plane per month. Prior to the installation of NeuLAND at its final location in the R3B hall at the FAIR site, the detector can be commissioned and available for experiments at Cave C, starting in 2017.

 

 

NeuLAND Milestones

2016: Jan  Feb  March  April  May  June  July  Aug  Sept  Oct  Nov  Dec

2015: Jan Feb March April May June July Aug Sept Oct Nov Dec

2014: Jan Feb March April May June July Aug Sept Oct Nov Dec

2013: Jan Feb March April May June July Aug Sept Oct Nov Dec

2012Oct Nov Dec

Milestones older than January 2015 are to be found in NeuLAND Milestone archive

 

May 2016

  • The NeuLAND demonstrator was part of the Sπrit TPC experiment carried out at RIKEN. In contrast to earlier experiments, the NeuLAND demonstrator joined, here, the detector seeing both charged particles and neutrons stemming from central collisions of 108,112,124,132Sn on 112,124 Sn target.
    Figure 1 shows a particle ID plot from the 1st NeuLAND plane, displaying the time of flight over the energy deposited in the hit.  Protons, deuterons, tritons, 3He and 4He were identified.
    Figure 2 shows the same distribution, but including a condition that no VETO hit was registered in the event.
    The left-over distribution is originating from neutrons and (at small time of flights) gamma-rays.
    Besides the main goal, the derivation of neutron over charged particle ratios for the Sπrit TPC experiment, the data taken are of great value for detector response studies, having charged and neutral particles hitting the detector at the same time.
Figure 1: Particle ID plot from the 1st NeuLAND plane
Figure 2: Same as Figure 1 but including a condition that no VETO hit was registered in the event.
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Figure 1: Particle ID plot from the 1st NeuLAND plane
Figure 2: Same as Figure 1 but including a condition that no VETO hit was registered in the event.
Figure 1: Particle ID plot from the 1st NeuLAND plane
Figure 2: Same as Figure 1 but including a condition that no VETO hit was registered in the event.

 

April 2016

  • The NeuLAND demonstrator, currently located at RIKEN , Japan, was moved within the SAMURAI Area to 30 degrees with respect to the target, see photo below. At this new position, NeuLAND together with a VETO wall in front will take data in an upcoming experiment, studying central collision in several combinations of Sn isotopes beams and Sn isotope targets.

  •  

On the left side the NeuLAND demonstrator VETO Wall is visible, NeuLAND is standing right behind it. The right hand side shows Nebula and its VETO wall, still located at 0 degrees.
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On the left side the NeuLAND demonstrator VETO Wall is visible, NeuLAND is standing right behind it. The right hand side shows Nebula and its VETO wall, still located at 0 degrees.
On the left side the NeuLAND demonstrator VETO Wall is visible, NeuLAND is standing right behind it. The right hand side shows Nebula and its VETO wall, still located at 0 degrees.

 

March 2016

  • The status of the analysis of the 7Li(p,n) calibration experiment of the NeuLAND Demonstrator at RIKEN (see NeuLAND news Nov. 2015) is summarized in an RIKEN progress report. The figure below shows the preliminary experimental velocity spectrum of NeuLAND for ~ 110MeV neutrons with veto condition cut, and an energy cut E > 5MeVee. The background was evaluated with an empty-target run. The integral under the red curve indicates the neutron events, which will be used to derive the efficiency.
Preliminary experimental velocity spectrum of
fileadmin/Kernreaktionen/neuLAND_march2016.bmp
Preliminary experimental velocity spectrum of
Preliminary experimental velocity spectrum of ~ 110MeV neutrons measured with NeuLAND demonstrator at RIKEN.
  • On March 1st the NeuLAND Working Group Meeting took place with about 30 participants at GSI. In the first session the status and the preparations needed for NeuLAND up to the experimental campaign to be started in the beginning of 2018 was summarized. The progress of detector construction was discussed as well as the HV supplying system and the readout electronics. Measures to be taken concerning the data acquisition and slow control, simulations, analysis and calibrations were specified. In the second session the status of the analysis of data from the last experiments and the ongoing progress in simulations were presented and discussed.

 

December 2015

  • The first of the two NeuLAND frames has been built, see photograph. It allows to hold up to 20 double planes. Its design allows the junction with a second frame to support all foreseen 30 NeuLAND double-planes, but also allows the splitting of the detector in two independent components and placing at different distances and angles to the target, depending on the specific experimental demands. The service platform, visible in the technical drawing on the right side is currently under construction.

One part of the NeuLAND main frame.
Design figure of the same part of the NeuLAND main frame.
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One part of the NeuLAND main frame.
Design figure of the same part of the NeuLAND main frame.
One part of the NeuLAND main frame.
Design figure of the same part of the NeuLAND main frame.
  • Preliminary online analysis of NeuLAND data measured at RIKEN are very promising: An efficiency of  (31.5±1.1)% for one-neutron events  is extracted from the preliminary analysis for the 250 MeV neutron run for the NeuLAND configuration at RIKEN (4 double-planes, 40 cm of detector depth); this result is in good accordance with simulation (29%).
  • The figure below shows the paddle multiplicity summed over all NeuLAND and Nebula modules for two different incoming ions at 250 AMeV. For the (p,3p) reaction of 29Ne, three neutrons are emitted in forward direction, for the (p,2p) reaction of 29F four neutrons impinge on the neutron detectors. A clear increase in paddle multiplicity was observed online, indicating the higher number of neutrons detected. The unambigious identification of the number of neutrons and their momentum reconstruction requires a more complex offline analysis.  
Preliminary results: paddle multiplicity summed over all NeuLAND and Nebula modules for two different incoming ions at 250 AMeV.
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Preliminary results: paddle multiplicity summed over all NeuLAND and Nebula modules for two different incoming ions at 250 AMeV.
Preliminary results: paddle multiplicity summed over all NeuLAND and Nebula modules for two different incoming ions at 250 AMeV.

 

November 2015

  • Part of the NeuLAND detector is presently in operation as one major components in an experimental campaign performed with the SAMURAI setup at RIKEN, studying several exotic neutron-rich nuclei including the double-magic nucleus 28O. The experiments are complemented by a calibration experiment for the combination of  NeuLAND and NEBULA (the neutron detector at the SAMURAI setup),  determining the efficiency at neutron energies of 110 and 250 MeV.

 

June 2015

  • On June 1st the status of the NeuLAND subproject was presented  during the R3B collaboration meeting. An update on the status was given for the production of double-planes at GSI, the planned in-kind contributions from PNPI and the design of the NeuLAND electronics. The planned experimental campaign at RIKEN was discussed and very first simulations on a VETO concept for NeuLAND were presented. The session closed with a presentation on the latest findings from the SiPM study for a possible use at later stages of the NeuLAND project.

May 2015

  • Seventh double-plane of the NeuLAND detector has been built.

April 2015

  •  The four NeuLAND double-planes located at the SAMURAI setup at RIKEN  have been successfully taken into operation and the calibration using cosmic rays has been performed. Next steps are the combined data taking with the NEBULA Veto Wall and with the NEBULA Detector itself.

March 2015

  • In connection with the NUSTAR week a NeuLAND working group meeting on March 3 at GSI discussed the future analysis framework for R3B, status of NeuLAND@RIKEN and future experiments there. Presentations on the status of the the analysis of S406 and S438a-c as well as on needed simulations were given. The performance of SiPMTs, which might become in the future an alternative for conventional PMTs, was presented.

 

February 2015

  • NeuLAND has been incorporated into experimental set-up in the SAMURAI cave. In the photo below, one can see four double planes of the NeuLAND detector positioned between SAMURAI exit window (left) and NEBULA detector (right).
NeuLAND prototype in the SAMURAI cave.
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NeuLAND prototype in the SAMURAI cave.
NeuLAND prototype in the SAMURAI cave.
  • On February 15th the four double-planes of the NeuLAND detector have been integrated into SAMURAI setup.

 

January 2015

  • At GSI the double plane 6 has been assembled in its final configuration.
  • On January 12th, the box containing the four NeuLAND double-planes has left GSI (see picture below, left) and has arrived on January 27th at RIKEN. On January 31st the box has been transported down to the SAMURAI cave, see photo below right.
Four double planes of the NeuLAND detector leave GSI.
NeuLAND panes are transporting to the SAMURAI cave.
fileadmin/Kernreaktionen/NeuLAND_IMG_20150112_171451.jpg
fileadmin/Kernreaktionen/NeuLAND_IMG-20150131-WA0002.jpg
Four double planes of the NeuLAND detector leave GSI.
NeuLAND panes are transporting to the SAMURAI cave.
Four double planes of the NeuLAND detector leave GSI.
NeuLAND panes are transporting to the SAMURAI cave.

 

Older news can be found here.

NeuLAND Literature
  • The NeuLAND Technical Design Report, available here.
  • "NeuLAND - from double-planes to the demonstrator", K. Boretzky et al, Scientific Report 2014 GSI Report 2015-1,  200-202 p. (2015) [10.15120/GR-2015-1-MU-NUSTAR-NR-12] 
  • "NeuLAND test-beam data analysis with R3BRoot framework", D. Kresan et al, Scientific Report 2014 GSI Report 2015-1,  378-379 p. (2015) [10.15120/GR-2015-1-INFRASTRUCTURE-IT-10]
  • "A compact readout system for the R3B High-Resolution Neutron Time-of-Flight Spectrometer (NeuLAND)", C. Ugur et al, Scientific Report 2014 GSI Report 2015-1,  204-205 p. (2015) [10.15120/GR-2015-1-MU-NUSTAR-NR-14]
  • "Multi-Neutron detection in R3B at FAIR with alternative detector model", V. Wagner et al, Scientific Report 2014 GSI Report 2015-1,  203 p. (2015) [10.15120/GR-2015-1-MU-NUSTAR-NR-13]
  • "NeuLAND - from prototypes to double-planes", K. Boretzky et al, Scientific Report 2013 GSI Report 2014-1,  346-350 p. (2014) [10.15120/GR-2014-1-FG-S-FRS-11]
  • "Tests of timing silicon photomultipliers for NeuLAND", S. Gohl et al, Scientific Report 2013 GSI Report 2014-1,  150 p. (2014) [10.15120/GR-2014-1-NUSTAR-KR-11]
  • "Construction and Test of a Large NeuLAND Prototype Array", K. Boretzky et al, GSI Scientific Report 2012, PHN-ENNA-EXP-60
  • "Recent Developments in NeuLAND Simulations", D. Kresan et al, GSI Scientific Report 2012, PHN-ENNA-EXP-64
  • "NeuLAND@R3B: A Fully-Active Detector for Time-of-Flight and Calorimetry of Fast Neutrons", K. Boretzky et al, GSI Sci. Rep. 2011, PHN-NUSTAR-NR-02, p. 174.
  • "Recent Developments in NEULAND Simulations", D. Kresan et al, GSI Sci. Rep. 2011, PHN-NUSTAR-NR-03, p. 175.
  • "Implementation and Performance of Neutron Tracking Algorithm for NEULAND", D. Kresan et al, GSI Sci. Rep. 2011, PHN-IS-IT-13, GSI Sci. Rep. 2011, p. 272.
  • "NeuLAND - Concepts for the Detection of Fast Neutrons", T. Aumann et al, GSI Sci. Rep. 2010, PHN-NUSTAR-NR-18, p. 180.
  • "NeuLAND: Simulations for the Scintillator Concept ", M. Heil et al, GSI Sci. Rep. 2010, PHN-NUSTAR-NR-19, p. 181.