Listed here are short descriptions of the experiments which have taken data at FTBF, and are expected to return to continue taking data.
Experiments are listed below in no particular order. To see current dates of installation or beam time requests for each experiment see the
FTBF Schedule.
To become a test beam user contact the FTBF Coordinator. Experiments which are not expected to return are listed in Past Experiments.
Name of Experiment:Belle II iTOP counter prototype evaluation Number:T-1019 Location: MTest 6.2C Started Taking Data: December 19, 2011 Description:
T-1019 is an experiment to verify the performance of the primary particle identification detector, the imaging time-of-propagation detector (iTOP), for the Belle II experiment. The operating principle of the iTOP is a modified version of a technique known as detection of internally detected Cherenkov light, or DIRC. In a DIRC detector, charged particles pass through a bar of radiator material, usually synthetic fused silica. Since these particles travel faster than the speed of light within the bar, they produce a cone of light known as Cherenkov radiation. Particles of the same momentum but different mass will have Cherenkov cones of slightly different opening angle. The bar is precisely machined and highly polished, and much of the light that is produced undergoes total internal reflection to the end of the bar for detection, all while preserving information about the production angles of the Cherenkov light that was produced, and hence the identity of the particle can be determined. In the original DIRC design of the BaBar experiment, the end of the bar couples to a large imaging area, and Cherenkov light is visible as a ring. Since space in Belle II is extremely constrained, the iTOP uses a much smaller imaging plane. Instead of producing ring images in two spatial dimensions, much of the ring image must be resolved from precise timing measurements. To obtain such precision timing, the iTOP uses very fast micro-channel plate photomultiplier tubes, read out by custom waveform digitizing electronics. Although previous tests of the time-of-propagation concept have been performed at KEK and CERN, these tests utilized a radiator bar of roughly half of the final planned size for Belle-II, preliminary version of the photodetectors, and commercial rack-mount electronics for readout. T-1019 is the first test of a full-size radiator, with four times more densely pixelated photodetectors, all read out by prototypes of the custom electronics.
A Class 1 (635nm), 400mW peak pulsed, solid state, laser is being used for alignment purposes. This laser would not cause retina damage to the naked eye.
The detector is a large structure on a remotely controlled, moving table.
Name of Experiment:COUPP Iodine Recoil Threshold Experiment (CIRTE) Number:T-1017 Location: MTest 6.1B Started Taking Data: September 21, 2011 Description:
CIRTE(T-1017) is a calibration experiment for COUPP(E961) - the Dark
Matter search using a heavy liquid bubble chamber as a detector. COUPP
works by observing a single bubble produced when a dark matter particle
scatters hard enough off a nucleus to cause a bubble to form. The bubble
is formed by the energy given to the recoiling nucleus. CIRTE does the
same experiment with charged pions from the test beam in place of the dark
matter particles. Since we can measure how much the pions scatter - a
trick we can't pull with dark matter - we can measure the nuclear recoil
energy to get the threshold and efficiency of the bubble chamber for
these scatters. This calibrates COUPP's sensitivity for an assumed flux
and spectrum of dark matter. The measurement is made with a very small
(1 cm diameter) version of the COUPP bubble chamber in a -12 GeV/c
pion beam. The pions are measured before and after the chamber with a
Silicon pixel detector telescope. CIRTE is a repeat of the FNAL-E69
experiment to measure hadron-Nucleus elastic scattering run, in the same
beamline (then M6, now MTest), 35 years ago.
Name of Experiment:Dual Readout Calorimetry with Glasses Number:T-1015 Location: MTest 6.2B Started Taking Data: June 29, 2011 Description:
This particular experiment has two halves, the first dealing with relatively old technology, using lead glasses which act as a totally active absorbing material for the Čerenkov light and the scintillation light generated by the beam particles.
The second half employs a new, optical glass called ADRIANO, with a high refractive index, where the scintillating light is not generated in the glass, but in the fibers coming out of the glass, thus separating the Čerenkov signal from the scintillation signal.
The ultimate objective of the research being done by this experiment is to test the potential of Dual Readout hadron calorimetry when applied to calorimeters with totally active absorbing media. This program focuses on the use of glasses, and, because a supply of potentially suitable scintillating glasses is already present at the laboratory, it could be possible to perform a “proof of principle” test of Total Absorption Dual Readout calorimetry in a relatively short time and at reduced cost. New scintillating glasses, are also being developed and could eventually be substituted for the currently available ones.
At the same time, a new technique (ADRIANO) has been proposed which employs glasses designed to act as a totally active absorbing medium for the Cherenkov component, and as the passive (sampling) medium for the scintillation component of a Dual Readout calorimeter.
Name of Experiment:Muon g-2 Calorimetry Number:T-1005 Location: MTest 6.2B Started Taking Data: May 14, 2010 Description:Test beam calibration of Muon g-2 Calorimeter equipment.
The proposed design is a tungsten-scintillating fiber calorimeter with 35 segments, each read out by a separate PMT. Tungsten, which is significantly denser than lead, produces compact showers. This is necessary, in order to improve shower separation in analysis and to fully contain the showers within a calorimeter that satisfies the strict space constraints of the experiment. A single calorimeter segment (4 x 6 x 15 cm3) has been constructed in order establish the feasibility of the new design and study its properties. Initial tests of the detector segment at the Paul Scherrer Institute were conducted with a low energy < 400 MeV/c electron beam. A higher-energy test with electrons up to a few GeV/c was performed at the Test Beam Facility under the experimental number T-967. All data from that test have been analyzed and published, and the tungsten-scintillating fiber calorimeter still appears to be a viable candidate. For this test beam run, a larger calorimeter (15 x 15 x 11 cm3) has been constructed and an emphasis will be placed on understanding shower leakage and the ability to separate pileup events with a more granular readout.
The experimenters will measure the energy resolution, linearity, and shower size of the calorimeter segment. This will provide important information for finalizing decisions on the angle of the fibers relative to the incoming electrons and the optimal granularity of the readout.
Name of Experiment:TAUWER Test Number:T-1012 Location: MTest 6.2B Started Taking Data: March 3, 2011 Description:
TAUWER is a proposed astro-particle experiment to detect ultrahigh energy TAU neutrinos, using detector towers arrayed on a mountainside looking down into a valley. This test is to study the possibility of replacing Hamamatsu miniature PMT's with SiPM's for readout by determining the response of scintillation detectors with SiPM readout to low energy electrons, 2 GeV or lower, as the beam will provide. The detector itself is a compact package, previously used in a parasitic test beam run on December 15, 2010, to compare the relative timing of the signals from three counters for Minimized Ionized Particles.
The experiment will take some electron data with 1.5 cm of Pb in front of counter 2 or counter 3, and without the Pb for calibration purposes.
The three scintillators are 0.7, 1.4, and 0.7 cm thick, each 19 x 19 cm square. Each has a single SiPM readout, seen in the picture. The SiPM operating voltage is 34 volts. This is introduced by BNC cables from power supplies in the electronics area. The red and white wires adapt the BNC cable to separate power and ground leads for the center counter. The SiPM signals are taken on RG174 cables to a local waveform digitizer (DRS4) adjacent to the optical box. The DRS4 is controlled by a PC located in the beam enclosure, operated remotely from the control room.
Name of Experiment:Response and Uniformity Studies of Directly Coupled Tiles Number:T-1006 Location: MTest 6.1B Started Taking Data: May 27, 2010 Description:
A finely-segmented scintillator-based calorimeter which capitalizes on the marriage of proven detection techniques with novel solid-state photo-detector devices such as Multi-pixel Photon Counters (MPPCs) is an interesting calorimetric system from the point of view of future detector design. A calorimeter system consisting of millions of channels will require a high degree of integration. The first steps towards this integration have already been facilitated by the small size and magnetic field immunity of the MPPCs. The photo-conversion occurs right at the tile, thus obviating the need for routing of long clear fibers. Similar considerations apply to the presence of wave-length shifting (WLS) fibers inside the tiles which couple it to the photo-detectors. Significant simplification in construction and assembly ensue if the MPPCs can be coupled directly to the scintillator tiles. The total absence of fibers would offer greater flexibility in the choice of the transverse segmentation while enhancing the electro-mechanical integrity of the design.
The tests involve a set of small directly-coupled tile counters fabricated at NIU which will be placed in the beam to study their response and response uniformity as a function of the incident position of the particles passing through them. The results will be relevant to high granularity scintillator/crystal electromagnetic and hadronic calorimetry.
The module will be mounted on supports allowing for its manual translation and rotation. The supports will be anchored to the pixel telescope dark box. The experimenters would need to access it every 2.5 – 3 hours to manipulate its position.
Name of Experiment:SuperB Muon Detector Prototype Number:T-1008 Location: MTest 6.2B Started Taking Data: December 1, 2010 Description:
The test objective is to optimize the muon identification in an experiment at a Super B Factory. To accomplish this, experimenters will study the muon identification capability of a detector with different iron configurations at different beam energies.
The detector is a full scale prototype, composed of a stack of iron tiles. The segmentation of the iron allows the study of different configurations. Between the tiles, one or two extruded scintillator slabs can be inserted to test two different readout options; a Binary Readout and a Time Readout. In the Binary Readout option the two coordinates are given by the two orthogonal scintillator bars, and the spatial resolution is driven by the bar width. In the Time Readout option one coordinate is determined by the scintillator position and the other by the arrival time of the signal read with a TDC.
The experimenters will need at least 1000 mu/pi per spill for 4, and 5 and maybe 6 GeV momentum particles. The lower momentums would be appreciated, but not crucial to the completion of the experiment. This request is unique as the experimenters are asking for momentum tagged muons at low momentum, rather than just "straight-thrus". The bulk of this effort falls on the PPD FTBF Group to provide Cherenkov and TOF for particle identification. It is likely the beam tuning will require inserting lead in the beam to reduce electrons. A remote lead piece for this purpose exists, and all parties are agreeable on its use. It's also likely that if FTBF is successful in tagging, it will require Accelerator Division to push the intensity limits. A best effort to meet the above requirements will be made.
The Downstream Cherenkov Detector in MT6.1 will be filled with C4F8O gas to give muon/pion separation for particles with momentum starting from about 2.2 GeV.
An iron absorber block, 18 cm x 30 cm x 30 cm, will be placed in front of the detector, on the facility motion table, to act as an electron filter and simulate the set-up of the actual Super-B experiment.
The mechanical structure of the detector has an overall length of 1.5 m, a width of 1.0 m (1.6 m taking into account the scintillator plane boxes) and a height of 0.8 m. The total weight is 4.0 tons. It will be placed upon a movable die cart and raised to beam height, then secured in place.
Name of Experiment:Fast Timing Counters for PSEC Number:T-979 Location: MTest 6.2B Started Taking Data: Description:
The experimenters will test time-of-flight particle detectors with the ultimate goal of achieving 1 psec timing resolution.
Proposed applications are:
diffractive Higgs production background reduction at the LHC
measuring the momentum of muons before and after a 6D cooling setup as proposed by the MANX experiment
particle identification at a Super-B factory
LHC detector upgrades
possible third generation Tevatron Collider flavor experiments
precision kaon measurements
astro-particle experiments
In addition, the development and testing of the associated electronics and timing algorithms may be directly applicable to advances in medical imaging. Much more information can be found at the PSEC web site, at http://hep.uchicago.edu/psec/.
The detectors will consist of micro channel plate photo-multiplier tubes (MCP-PMTs) with quartz radiators at the face. Incident particles will pass through the radiators and the tubes. Resultant Cherenkov light will be sensed by the tubes and converted into electronic signals whose leading edges will mark the time of the beam’s passage. A variety of MCP-PMTs differing in number and size of anodes, pore size and acceleration gap spacing, will be tested to determine the time measurement accuracy of each. Various connection schemes tying different numbers of adjacent anodes together will also be explored, with the overall goal to determine the optimal MCP-PMT construction and integration of electronics for time resolutions on the order of 1 psec.
Initial tests with the MCP-PMTs will utilize a fast (40Gs/sec) Tektronix TDS6154C oscilloscope to measure the signals from up to four MCP-PMTs. As time and resources permit additional channels will be instrumented using NIM/CAMAC based electronics and possibly also custom waveform sampling electronics in an effort to further improve timing resolution and to gain experience in the type of electronics necessary to construct large systems of this type in future experiments.
Variation in the spacing between MCP-PMTs will allow systemic exploration of the accuracy of time measurements. Additionally, as the custom waveform sampling electronics is integrated the experimenters will also explore solutions for high precision clock distribution and readout. Larger spacing, up to the maximum available, will be used to measure particle separation performance using the known particle mix of the test beam.
Name of Experiment:Tests of radiation-hard sensors for the SLHC Number:T-992 Location: MTest 6.1 Started Taking Data: Description:
At the SLHC, after 2500 pb-1 of data, the expected maximum fluencies for the pixel region (20 cm) will be 2.5 x 1016 cm-2. To cope with this unprecedented radiation environment a variety of solutions have been pursued for vertex and tracking detectors at the SLHC. These include diamond sensors, 3D sensors, MCZ planar silicon detectors made from MCZ wafers, epitaxial, p-type silicon wafers and thin silicon detectors.
The experimenters wish to compare the performance of this wide variety of detectors in a test beam before and after irradiation. To do so, the experimenters plan to use the CMS pixel-based telescope currently being commissioned and constructed for the MTest beamline. In particular, the experimenters are planning to study the charge collection efficiency of the irradiated and un irradiated devices and the spatial resolution as a function of the track incident angle. The experimenters will change the incident angle of the beam by moving the sensors, to investigate how the resolution varies with angle.
Name of Experiment:MINERvA Experiment Number:T-977 Location: MTest 6.2 Description: Test beam calibration of MINERvA detector components
The MINERvA test beam detector is a small version of the full detector.
The experimenter's primary need is to calibrate the MINERvA scintillator response (visible energy) to protons, pions, and electrons, to measure the resolution of that response, and to estimate and ultimately reduce the bias on the calorimetric shower energy reconstruction for these particles.
This experiment required the design and construction of a tertiary beamline that will bend particles to the right of the nominal secondary beam. The beam instrumentation and the detector will be placed in this area.
Name of Experiment:Muon Detector / Tail Catcher R&D Number:T-995 Location: MTest 6.2C Started Taking Data: February 8, 2010 Description: This R&D program continues the T-956 studies using particle beams to test long strip counters, up to 6m, and new prototype TB4 electronics developed at Fermilab.
The muon counter tests will focus on:
Setup and testing of Fermilab-based TB4 front-end (FE) electronics designed to sample the input signals at 5ns intervals.
Measurement of the number of photo-electrons (p.e.) for short (1m) and long (6m) strips equipped with 1.2mm dia. wave-length
shifting fiber (KurarayY-11 double clad) with several different varieties of PPDs (HPK, FBK-IRST, SensL, Zecotek)
with various pixel sizes, fill-factors, and planar shapes. The scintillating strips will be equipped with PPDs at either one or
both ends of the strips for comparison of single and dual readout.
Evaluation of the position of the impact point along the strip from the timing difference between signals read out from both ends or
between direct and reflected (from the mirrored end) signals read out from the same end.
Optimization of pulse shaping and charge integration for charge resolution so as to be able to identify single
photoelectron peaks for self calibration
Optimization of optical couplings between WLS fibres and PPDs
Measurement of signal attenuation as a function of position of the beam along the length of the strips and the inefficiency
across the strips due to the ~1mm thick coating of white TiO2 that ensures good light pulse reflection along the scintillating
strip. This measurement will require upstream tracking to project the charged particle to the scintillator.
One of the test objectives is the optimization of extrusion type , e.g. measurement of photo-electron yield for scintillator
with an extruded hole instead of a groove for holding the WLS fiber. A variation on this theme is to test two fibers in two extruded holes.
One important application of the pulse – shape digitization is that it will allow evaluation of the relative contributions of
WLS and scintillator relaxation times to the overall time distribution of the signals. The relaxation time of the WLS is reported to be 12ns.
Name of Experiment:Total Absorption Dual Readout Calorimetry R&D Number:T-1004 Location: MTest 6.2B Started Taking Data: April 1, 2010 Description:The tests objective is to continue the development of elements and techniques related to total absorption dual readout calorimetry
The initial studies will involve single (or, at most, a few) crystal or glass samples as a continuation and acceleration of on-going work using cosmic-ray muons. The purpose of these studies is to evaluate the performance of the different crystal and glass samples in combination with different light collection and readout alternatives to optimize simultaneous collection of Cherenkov and scintillation light components for application of the Dual Readout technique to total absorption calorimetry. To determine the correlation of the light collection efficiency with the parent particle trajectory a tracking system will be required to determine the path of particles through the crystal/glass sample. Crystals will be equipped with various optical filters to study the separation of Cherenkov and scintillation light capability via the wavelength separation. Several photo-detectors will be placed in different positions on the crystal sides to investigate the angular and position dependence of the collected light
The experiment plans to investigate several possible photo-detectors. The optical couplers are designed to allow an arbitrary choice of the photo-detectors and any mix of them.
In addition to single crystal studies the experiment plans an exposure of several electromagnetic crystal calorimeters to investigate the issues associated with larger systems, to establish and check the calibration procedures and to evaluate various potential crystal samples.
Studies of the single crystals will require beams of hadrons, electrons, and muons over the available energy range. No particular requirements regarding momentum resolution are necessary.
Investigations of the electromagnetic calorimeters modules will be carried out with electrons or positrons at a few different energies over the available range. The beam energy and its spread should be kept as low as possible.
Beam Requirements:
Particles: see above
Energy: all
Intensity Needed: 4000 - 40000 counts per spill
A small spot size of the order of few cm2 is preferred
Name of Experiment:JASMIN Number:T-994 Location: MTest 6.2 Started Taking Data: February 10, 2010 Description: The purpose of these measurements is to obtain basic nuclear data and to develop instrumental techniques for characterization of particle fields of protons, neutrons, muons, etc.
This experiment has two programs:
Activation: a target will be placed at the M01 area because of the availability of an intense proton beam. The target is a stack of foils with different materials. An irradiation of dozens of minutes by primary beam is performed in each of several days. After the irradiation, the target is moved to HIL(High Intensity Lab) for gamma spectrometry as soon as possible.
Counting Secondary Particles: starts after removal of the target. A charged particle beam of 120 GeV, 3E5 proton/spill (or greater, if possible) hits a cylindrical target (60cm long copper). Secondary particles from the target are measured by counters placed at several angles with respect to the beam axis. To determine particle energy, TOF and an unfolding method are used.
Name of Experiment:Diamond Detector Research Number:T-932 Location: MTest 6.2B Started Taking Data: March 15, 2010 Description:
This beam time request is to test Chemical Vapor Deposition (CVD) diamond pixel detectors. Research in this area began nearly a
decade ago when it was realized CVD diamond is a promising, radiation-hard alternative to silicon.
Name of Experiment:Čerenkov Light Test Number:T-953 Location: MTest 6.2 Started Taking Data: Description:
The University of Iowa has pioneered in application of Čerenkov radiation for high-energy detectors. One of the results of this effort is the huge forward calorimeter for CMS (at the LHC) with a half million quartz fibers in iron. The laboratory plans to use this expertise to develop a variety of detectors making use of Čerenkov light and photo tubes as the active elements in calorimeters for high-energy particles. There are three immediate applications related to forward angle calorimeters in CMS; ZDC, CASTOR, and the HE upgrade.
The University of Iowa will make the detailed design for the Zero Degree Calorimeter. The proposed design uses tungsten plates interleaved with sheets of quartz fibers. In the EM part the plates are perpendicular to the beam, in the rear hadronic part they are at an angle of 45o. Because of the limited cross sectional area of the plates, there will be considerable leakage of shower particles out of the four sides. We plan to measure this leakage and compare the results with simulations. The leakage will be measured by placing a polished aluminum tank, 4 in wide, 20 in long and 8 in deep on top of absorber material made of blocks of tantalum and copper. The fluid in the tank, that generates the Čerenkov light, could be water; but ethylene glycol (antifreeze, but without the added color) would be better. Being non-polar, it is not corrosive like water, and it has a higher index of refraction, l.42 vs. 1.33. The larger index of refraction would result in more Čerenkov light and better coupling to the PMT.
The University of Iowa has been asked to design the light guides for CASTOR that take the light from the quartz plates, in which the light is produced, and carry it to the PMTs. These plates, interleaved with tungsten plates, are oriented at 45o.
The University of Iowa has been asked to consider methods for replacing the scintillators in the HE hadronic calorimeter with quartz plates, which will not be harmed by the high radiation levels expected with the proposed LHC upgrade in luminosity. The success of this project depends on finding an extremely effective way to couple the Čerenkov light into wave-length shifting fibers.
For all of the tests, the setup will be small, at most only a few cubic feet. There will be no gas supply or complicated mechanical devices. The active devices will be a few PMTs
The overall project will consist of a number of short, simple experiments, each lasting from one to three days