Update on the Neutral Particle Spectrometer The NPS project is supported by NSF MRI PHY-1530874 NPS Carlos Muñoz Camacho for the NPS Collaboration NPS Collaboration Meeting: 21 Jan 2016 Thanks to Tanja Horn, Marco Carmignotto, Frédéric Georges and Gabriel Charles for slides/plots… Hall C Users Meeting, Jan 21-22 (2016) 1 2 Tomography of the Nucleon Beyond one-dimensional spatial densities (form factors) and longitudinal momentum densities (parton distributions) Connection to orbital angular momentum – nucleon spin 5D 3D description: TMDs 3D – Confined motion in a nucleon (semi-inclusive DIS) GPDs – Transverse spatial imaging (exclusive DIS) Major new capability with JLab12 3 4 5 6 7 8 The Neutral-Particle Spectrometer NSF MRI PHY-1530874 (NPS) The NPS is a standalone 25 msr spectrometer allowing for precision (coincidence) cross section measurements of neutral particles Consists of a PbWO4-based calorimeter preceded by a sweeping magnet NPS cantelevered off SHMS platform NPS on SHMS platform Magnet Magnet Detector Detector NPS angle range: 5.5 – 30 degrees NPS angle range: 25 – 60 degrees Remotely rotatable with the SHMS carriage The NPS is is an efficient way to meet the experimental requirements of the approved science program taking maximum advantage of existing infrastructure 9 NPS General Design Concept a ~25 msr neutral particle detector consisting of up to 1116 PbWO4 crystals in a temperature-controlled frame including gain monitoring and curing systems HV distribution bases with built-in amplifiers for operation in a high-rate environment Essentially deadtime-less digitizing electronics to independently sample the entire pulse form for each crystal – JLab-developed Flash ADCs A new sweeping magnet allowing for small-angle operation at 0.3 Tm (for electro-production) and large angle operation at 0.6 TM (for photo-production). The magnet is compatible with existing JLab power supplies. Modified beam pipe: critical angle 13.5 mr Cantelevered platforms off the SHMS carriage to allow for remote rotation (in the small angle range), and platforms to be on the SHMS carriage (in the large angle range) – new A beam pipe with as large critical angle as possible to reduce beamline-associated backgrounds – further study showed only a small section needs modification (JLab/Hall C) 10 E12-13-010: Exclusive0 cross sections 0 Chiral-odd GPDs may contribute to the transverse xsec Unseparated data from 6 GeV Jlab Hall B [Bedlinskiy et al., PRL 109 (2012) 112001] [Goloskokov, Kroll, EPJA, 47:112 (2011)] [Ahmad, Goldstein, Liuti, PRD79 054014 (2009)] Recent pion cross section data suggest that transverse photons play an important role in pion electroproduction To confirm the estimates of the contribution of transverse photons and potential to access GPDs in meson production requires a full separation of the cross section red circle=T, blue triangle=L Preliminary results from Hall A at 6 GeV Jlab suggest 2 2 that at Q ~2GeV T dominates for large values of t, 2 2 but that L is non-zero at Q ~2GeV [M. Defurne, talk at DIS2015] E12-13-010 goals: [F. Sabatie, talk at CIPANP2015] Measure 0 cross sections over a larger kinematic range to confirm the dominance of T in 12 GeV kinematics 11 E12-13-007: Basic (e,e’) cross sections Linked to framework of Transverse Momentum Dependent Parton Distributions Basic cross sections are a fundamental test of understanding SIDIS in 12 GeV kinematics and essential for most future m experiments and their interpretation p Validation of factorization theorem TMD X Target-mass corrections and ln(1-z) re-summations require precision large-z data q TMD (x,kT) Transverse momentum widths of quarks with different flavor (and polarization) can be different Advantages of (e,e’o) beyond (e,e’+/‐) Experimental and theoretical advantages to validate understanding of SIDIS Can verify: o(x,z) = ½ (+(x,z) + ‐(x,z)) Confirms understanding of flavor decomposition/kT dependence 2 2 PT = pt + z kt + O(kt /Q ) E12-13-007 goal: Measure the basic SIDIS cross sections of o production off ( ) the proton, including a map of the PT dependence (PT ~ < 0.5 GeV), to validate * flavor decomposition and the kT dependence of (unpolarized) up and down quarks (*) Can only be done using spectrometer setup capable of %‐type measurements (an essential ingredient of the global SIDIS program!) 12 E12-14-003: exploring factorization in Wide-Angle Compton Scattering (WACS) WACS is a powerful probe of nucleon structure -several theoretical approaches developed in recent years. Developments within the Soft Collinear Effective Theory (SCET) demonstrated importance of future data for interpretation of a wide variety of hard exclusive reactions. JLab Hall A data suggest factorization into hard and soft-collinear parts (but limited in -t). E12-14-003 will use the Hall C HMS and the new Neutral Particle Spectrometer to measure the differential cross section up to s~20 GeV2! Two main goals of E12-14-003 Four fixed -t scans will allow for a rigorous test of factorization. The t-dependence of the Compton form factor will allow for gaining valuable insights into proton structure at high momentum transfer. 13 14 15 Magnet-Dump as a Compact Photon Source Distance to target ~200 cm Uses a magnet as dump for the photon beam diameter on target ~2.0 mm electron beam producing a 2mm hole narrow intense untagged photon 1.2µA e- γ beam 8.8 GeV B ~ 1.5T - e 3cm NH3 Beam Dump In the magnet PR12-15-003: worked out the concept in more detail for WACS-ALL measurements with NPS extending the range in s with wide kinematic coverage 2 s: 8.0 – 16.0 GeV 2 -t: 3.0 – 7.0 GeV 2 -u: 3.0 – 7.0 GeV θCM: 80° – 100° Compact Photon Source would optimize science using photon beam accessible with NPS 16 17 NPS Sweeping Magnet Construction Horizontal field design satisfies the requirements of all approved NPS experiments Small angle operation at 0.3 Tm (for electroproduction) and large angle operation at 0.6 TM (photo-production) Field clamp and bucking coil in front of the magnet minimize stray fields Compatible with existing power supplies 30 cm 2 deg. 157 cm Magnet Features: . the beam side is free of coils . the beam opening is +/- 1 degree Design drawings are underway . open aperture to detector above 2 degrees! Interferences with Hall equipment . vertical aperture is 60 cm; horizontal is 30 cm being worked out 18 Studies of PbWO4 NPS CalorimeterCrystal Quality: Prototype synergy with EIC R&D Two PbWO4 manufacturers: SICCAS/China and CRYTUR/Czech Republic – the company that produced crystals for CMS is out of business Our studies show significant crystal-to-crystal variations for crystals manufactured at SICCAS after 2012 – consistent with findings at PANDA Evaluation of this variation and possibly determining the origin of it is one of the main goals of this R&D project Example of radiation hardness studies from PANDA. Only 3 out of 10 crystals would pass the specifications JLab BNL Caltech PbWO4 crystal #7 80 There are differences in crystal 60 lengthwise characterization results at different institutions lengthwise' 40 transverse @ 3.2cm transverse @ 5cm % transmission transverse @ 7cm transverse @ 9cm transverse @ 11cm transverse @ 12cm transverse @ 13cm 20 transverse @ 15cm transverse @ 16.8cm Transmittance (%) Understanding the effect of this is important 0 200 300 400 500 600 700 800 wavelength (nm) Wavelength (nm) for interpretation of crystal quality and Systematic differences between setups setting up specifications for EIC 19 Crystal Testing NPS Facility Calorimeter Setup Prototype at CUA Close proximity to JLab (synergy with the PbWO4-based NPS project) and The Vitreous State Laboratory (state-of-the-art crystal testing instrumentation and expertise) Optical Transmittance (LT/TT) Perkin-Elmer Lambda 750 spectrometer Setup was commissioned for LT and TT with reproducibility ~0.2% Crystal light yield and timing Na-22 source and 2-inch PMT (XP2262) Temperature control with accuracy and stability better than 1 °C Anode signals digitized with charge sensitive ADC (LeCroy 2249W) Radiation hardness and recovery X-ray irradiation system and radioactive sources Chemical analysis (XRF, SEM, TEM, Raman, etc.) 20 Light yield results JLab sample of SICCA's crystals Temperature dependence Comparison with Gissen measurement: High variability within the same lot of crystals LY @ 18 oC CUA: 19.4 +/- 0.7 pe/MeV Gissen: 19.2 pe/MeV (work in progress to measure more crystals) Important: PMTs quantum efficiencies are similar, but probably different. Other activities Light annealing (LED) Thermal annealing (oven) Joining forces with VSL at CUA to characterize PbWO4 crystals! Crystal Testing NPS Facility Calorimeter Setup Prototype at IPN-Orsay Close proximity to Giessen University (cross calibration of setup and expertise) Optical Transmittance (L/T) Varian Cary 5000 spectrometer Setup was commissioned with BTCP crystals on loan from Giessen To accommodate crystals of lengths greater than 15 cm a more versatile configuration with a fiber-based spectrometer is being built 90 80 70 Longitudinal 60 Co (3000 Cu) 60 Large end Crystal light yield and timing 50 Centre Transmittance [%] Transmittance 40 Small end A setup is currently being tested 30 with cosmic rays 20 10 0 300 350 400 450 500 550 600 650 λ [nm] Radiation Hardness Panoramic irradiation facility available (60Co sources): • 5000 Gy/h at 10 cm • 300 Gy/h at 35 cm At ~1m 30 Gy in ~30 min 23 Laboratoire de Chimie Physique (Orsay) • 6 Gy/h at 260 cm Light yield measurements in Orsay Vertical cosmics through a PWO crystal Cosmic setup to measure light yield at room temperature Results so far on a old BTCP crystal Mean value at 182 ADC ch with a pedestal at 72. This yields 117 photons per MeV at room temperature, very close to values measured for these crystals by other groups.