E. Hazen
Boston University
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Featured researches published by E. Hazen.
Physical Review D | 2000
H. N. Brown; G. Bunce; R. M. Carey; P. Cushman; G. T. Danby; P. T. Debevec; H Deng; Sk Dhawan; V. P. Druzhinin; L. Duong; W. Earle; E. Efstathiadis; G. V. Fedotovich; F. J. M. Farley; S. Giron; F. Gray; M. Grosse-Perdekamp; A. Grossmann; Ulrich Haeberlen; M. F. Hare; E. Hazen; David W. Hertzog; Vw Hughes; M. Iwasaki; Klaus-Peter Jungmann; D Kawall; M. Kawamura; B. I. Khazin; J. Kindem; F. Krienen
A new measurement of the positive muons anomalous magnetic moment has been made at the Brookhaven Alternating Gradient Synchrotron using the direct injection of polarized muons into the superferric storage ring. The angular frequency difference omega (a) between the angular spin precession frequency omega (s) and the angular orbital frequency omega (c) is measured as well as the free proton MMR frequency omega (p). These determine R = omega (a)/omega (p) = 3.707 201(19) x 10(-3). With mu (mu)/mu (p) = 3.183 345 39(10) this gives a(mu+) = 11 659 191(59) x 10-(10) (+/-5 ppm), in good agreement with the previous CERN and BNL measurements for mu (+) and mu (-), and with the standard model prediction.
Physics Letters B | 1990
S. Ahlen; M. Ambrosio; G. Auriemma; A. Baldini; G.C. Barbarino; B. Barish; G. Battistoni; R. Bellotti; C. Bemporad; P. Bernardini; H. Bilokon; V. Bisi; C. Bloise; C. Bower; F. Cafagna; M. Calicchio; P. Campana; S. Cecchini; V. Chiarella; P. Chrysicopoulou; S. Coutu; I.D' Antone; C. De Marzo; G. de Cataldo; M. De Vincenzi; O. Erriquez; C. Favuzzi; D. Ficenec; V. Flaminio; C. Forti
Abstract The MACRO detector, located in the underground Gran Sasso Laboratory, had its initial data run from February 27 to May 30, 1989, using the first supermodule (SΩ∼800 m 2 sr ) . Approximately 245 000 muon events were recorded. Here are reported the results of the analysis of penetrating muons which determine the measured vertical muon flux at depths greater than 3000 m.w.e. In addition the data have been used to search for large scale anisotropies.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2001
G. T. Danby; L. Addessi; Z. Armoza; J. Benante; H. N. Brown; G. Bunce; J. Cottingham; J. Cullen; J. Geller; H. Hseuh; J. W. Jackson; L. Jia; S. Kochis; D. Koniczny; R.C. Larsen; Y. Y. Lee; M. Mapes; R. E. Meier; W. Meng; W. M. Morse; M. O'Toole; C. Pai; I. Polk; R. Prigl; Yannis K. Semertzidis; R. Shutt; L. Snydstrup; A. Soukas; T. Tallerico; F. Toldo
Abstract The muon g-2 experiment at Brookhaven National Laboratory has the goal of determining the muon anomalous g-value a μ (=(g−2)/2) to the very high precision of 0.35 parts per million and thus requires a storage ring magnet with great stability and homogeniety. A superferric storage ring with a radius of 7.11 m and a magnetic field of 1.45 T has been constructed in which the field quality is largely determined by the iron, and the excitation is provided by superconducting coils operating at a current of 5200 A. The storage ring has been constructed with maximum attention to azimuthal symmetry and to tight mechanical tolerances and with many features to allow obtaining a homogenous magnetic field. The fabrication of the storage ring, its cryogenics and quench protection systems, and its initial testing and operation are described.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2003
E. Hazen; C Lawlor; J. Rohlf; Shouxiang Wu; A. Baumbaugh; J. E. Elias; J. Freeman; D. Green; D Lazic; S. Los; A. Ronzhin; S Sergueev; T. Shaw; R. Vidal; J. Whitmore; T. Zimmerman; M. Adams; K Burchesky; W Qian; A. Baden; R. Bard; H Breden; T Grassi; A. Skuja; Wade Cameron Fisher; J. Mans; C. Tully; V. Barnes; A. T. Laasanen; P. de Barbaro
Abstract Relative calibration of the scintillator tiles used in the hadronic calorimeter for the Compact Muon Solenoid detector at the CERN Large Hadron Collider is established and maintained using a radioactive source technique. A movable source can be positioned remotely to illuminate each scintillator tile individually, and the resulting photo-detector current is measured to provide the relative calibration. The unique measurement technique described here makes use of the normal high-speed data acquisition system required for signal digitization at the 40 MHz collider frequency. The data paths for collider measurements and source measurements are then identical, and systematic uncertainties associated with having different signal paths are avoided. In this high-speed mode, the source signal is observed as a Poisson photo-electron distribution with a mean that is smaller than the width of the electronics noise (pedestal) distribution. We report demonstration of the technique using prototype electronics for the complete readout chain and show the typical response observed with a 144 channel test beam system. The electronics noise has a root-mean-square of 1.6 least counts, and a 1 mCi source produces a shift of the mean value of 0.1 least counts. Because of the speed of the data acquisition system, this shift can be measured to a statistical precision better than a fraction of a percent on a millisecond time scale. The result is reproducible to better than 2% over a time scale of 1 month.
ieee nuclear science symposium | 2011
A. Baumbaugh; B. Bilki; J. M. Butler; T. Cundiff; L. Dal Monte; P. De Lurgio; G. Drake; K. Francis; W. Haberichter; E. Hazen; J. Hoff; Scott Holm; A. Kreps; J. Repond; J. L. Schlereth; J. Smith; D. Trojand; Sau Lan Wu; L. Xia; Q. Zhang
A new detector technology is being developed for future colliding beam experiments that is based on the use of fine-grained calorimetry, to optimize the use of Particle Flow Algorithms (PFAs) in measuring hadronic jets. Instead of traditional tower geometry and energy summation from many sampling layers, the new approach measures energy deposition in 1 cm2 cells on each sampling layer using discriminators. Jets are reconstructed using hit patterns from each layer, combined with information from inner tracking and the electromagnetic calorimeter. We have built a 480,000 channel prototype detector that is based on Resistive Plate Chambers (RPCs) to demonstrate this concept. The development is part of the CALICE Collaboration. The readout system uses a 64-channel custom integrated circuit called DCAL to record hits from each cell and apply a global timestamp. The chips mount directly on sophisticated front-end boards that are not only an integral part of the charge collection of the detector chambers, but also incorporate digital signal transmission, clock and control, and power and ground. The readout of data is serial, multiplexed into high-speed serial streams and sent to a “back-end” VME system for time-sorting and higher-level triggering. The system can be operated with an external trigger or be self-triggered, and can produce trigger signals from the front-end chips. The construction, installation, and commissioning of this prototype system is now complete. We have begun a measurement program using a test beam at Fermilab. An overview of the system is described. Experiences in building this large prototype system are reported. Results from the test beam are presented.
Journal of Instrumentation | 2016
C. Adams; A. Bambaugh; B. Bilki; J. M. Butler; F. Corriveau; Tim Cundiff; G. Drake; K. Francis; B. Furst; V. J. Guarino; B. Haberichter; E. Hazen; J. Hoff; Scott Holm; A. Kreps; P. DeLurgio; Z. Matijas; L. Dal Monte; N. Mucia; E. Norbeck; D. Northacker; Y. Onel; B. Pollack; J. Repond; J. L. Schlereth; F. Skrzecz; J. Smith; D. Trojand; D. G. Underwood; M. Velasco
A novel hadron calorimeter is being developed for future lepton colliding beam detectors. The calorimeter is optimized for the application of Particle Flow Algorithms (PFAs) to the measurement of hadronic jets and features a very finely segmented readout with 1 × 1 cm2 cells. The active media of the calorimeter are Resistive Plate Chambers (RPCs) with a digital, i.e. one-bit, readout. To first order the energy of incident particles in this calorimeter is reconstructed as being proportional to the number of pads with a signal over a given threshold. A large-scale prototype calorimeter with approximately 500,000 readout channels has been built and underwent extensive testing in the Fermilab and CERN test beams. This paper reports on the design, construction, and commissioning of this prototype calorimeter.
Journal of Instrumentation | 2010
M Dimitriyev; E. Hazen; S. Wu; J. Rohlf
We are developing a Micro TCA Carrier Hub card which provides timing, control and data acquisition functions in a Micro TCA crate for HL-LHC readout electronics. This module may be mounted in the primary or redundant MCH slot in a Micro TCA crate, and distributes low-jitter LHC RF clock and encoded fast timing signals to up to 12 AMC modules. In addition, it receives buffer status signals and DAQ data at up to 600 MBytes/sec from each AMC. The prototype module is built on a commercial MCH base board with a custom mezzanine board stack. The latest Xilinx® Virtex®-6 FPGA are used to provide a clear upgrade path. Prototype modules have been developed for a CMS HCAL test beam in summer 2010. We describe the specifications of the module, its application in a Micro TCA system beyond CMS HCAL, and our experience in commissioning the module for the test beam.
Journal of Instrumentation | 2010
E. Hazen; U. Heintz; M. Johnson; R. Lipton; M. Narain; S. Wu
The luminosity goal for the Super-LHC is 1035/cm2/s. At this luminosity the number of proton-proton interactions in each beam crossing will be in the hundreds. This will stress many components of the CMS detector. One system that has to be upgraded is the trigger system. To keep the rate at which the level 1 trigger fires manageable, information from the tracker has to be integrated into the level 1 trigger. Current design proposals foresee tracking detectors that perform on-detector filtering to reject hits from low-momentum particles. In order to build a trigger system, the filtered hit data from different layers and sectors of the tracker will have to be transmitted off the detector and brought together in a logic processor that generates trigger tracks within the time window allowed by the level 1 trigger latency. This paper describes a possible architecture for the off-detector logic that accomplishes this goal.
ieee nuclear science symposium | 2008
A. Heering; P. Bohn; A. Clough; E. Hazen; J. Rohlf; S. Los; J. Freeman; E. Cascio; Y. Musienko; C. Piemonte
A typical scintillating tile sampling calorimeter consists of multiple layers of scintillators coupled to wavelength shifting fibers viewed by a suitable photo-detector. Long clear fibers are used to connect the tiles to the readout modules. We have investigated the use of silicon photomultipliers (SiPMs) at the Super Lagre Hadron Collider (SLHC). Because radiation hardness is the main concern, two sets of radiation data were taken using a 212 MeV proton beam at Massachusetts General Hospital. In the first data set we radiated up to a dose of 3×1010 protons per cm2 using diodes from three different manufactures (i.e., FBK, CPTA and Hamamatsu). At a dose of 3x1010 protons per cm2 only small effects of PDE loss were detected due to very high dark count always occupying one or more cells in a multi-cell SiPM. A second set of data up to 1013 protons per cm2 using very high pixel density MAPDs with up to 40,000 cells per mm2. After each small radiation dose multiple scope traces were taken to look at the PDE and dark count of the devices. The increase in dark count due to the radiation was compared to the DC leakage current. Also a comparison was made between multi-cell and single-cell samples of the FBK-IRST diodes.
ATOMIC PHYSICS 17: XVII International Conference on Atomic Physics; ICAP 2000 | 2001
V. W. Hughes; H. N. Brown; G. Bunce; R. M. Carey; P. Cushman; G. T. Danby; P. T. Debevec; H. Deng; S. Dhawan; V. P. Druzhinin; L. Duong; W. Earle; E. Efstathiadis; G. V. Fedotovich; F.J.M. Farley; S. Giron; F. Gray; M. Grosse-Perdekamp; A. Grossmann; Ulrich Haeberlen; M. F. Hare; E. Hazen; David W. Hertzog; Vw Hughes; M. Iwasake; K. Jungmann; D. Kawall; M. Kawamura; B. I. Khazin; J. Kindem
The muon g-2 experiment at the Brookhaven National Laboratory is described, including its motivation, goal and present status. The latest result based on 1998 data is aμ+=g−2/2=11 659 191(59)×10−10 (5 ppm), where the error is primarily statistical. This value agrees with the present theoretical value. Data obtained thus far and now being analyzed should have a statistical error of about 0.5 ppm.