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IEEE Transactions on Nuclear Science | 1985

Progress Report on the NBS/LOS Alamos RTM

S. Penner; R. L. Ayres; R. I. Cutler; P. H. Debenham; E. R. Lindstrom; D. L. Mohr; J. E. Rose; M. P. Unterweger; Mark Wilson; R.S. Biddle; E. R. Martin; J. E. Stovall; Paul J. Tallerico; L. Wilkerson; L.M. Young

The NBS-Los Alamos 200 MeV Racetrack Microtron (RTM) is being built under a program aimed at developing the technology needed for high-current intermediateenergy CW electron accelerators. In this report we give an overview of the present status of the project. Recent progress includes: (1) completion of testing of the 100 keV chopper-buncher system demonstrating a normalized emittance well under the design goal of 2.6 ¿ mm mrad at currents exceeding the design goal of 600 ¿A; (2) operation of the rf structures comprising the 5 MeV injector linac at power levels up to 50 kW/m, resulting in an accelerating gradient at ß=1 of 2 MV/m (compared to a design goal of 1.5 MV/m). The measured shunt impedance is 82.5 Mn/m; (3) construction and installation of the 30 ton end magnets of the RTM. Field mapping of one magnet has been completed and its uniformity exceeds the design goal of ±2 parts in 104; (4) performance tests (with beam) of prototype rf beam monitors which measure current, relative phase, and beam position in both transverse planes. (5) Installation and initial operation of the primary control system.


IEEE Transactions on Nuclear Science | 1983

NBS-LANL RTM Injector Installation

Mark Wilson; R. I. Cutler; E. R. Lindstrom; S. Penner; N. R. Yoder; R. L. Ayres; D. L. Mohr; L. M. Young; E. R. Martin

The injector for the NBS-LANL CW racetrack microtron consists of a 100 KeV electron gun and beam transport line followed by a 5 MeV linac. The function of the gun and transport line, which have been installed at NBS, is to provide a chopped and bunched 100 KeV and up to 0.67 mA dc or pulsed beam of very low transverse emittance for matched insertion into the linac. In this paper the authors present both the design and construction details of the 100 KeV system and the results of preliminary beam tests. The tests conducted thus far show the gun and transport system to be performing well within design specifications.


IEEE Transactions on Nuclear Science | 1983

Progress on the NBS-LANL CW Microtron

P. H. Debenham; S. Penner; R. L. Ayres; R. I. Cutler; E. R. Lindstrom; D. L. Mohr; J. E. Rose; Mark Wilson; N. R. Yoder; L. M. Young; R. E. Martin; A. Mitra; J. M. Potter; Richard H. Stokes; Paul J. Tallerico; L. Wilkerson

The NBS-LANL racetrack microtron (RTM) currently under construction at the National Bureau of Standards is a demonstration accelerator to determine the feasibility of, and to develop the technology necessary for building high-energy, high-current, continuous beam (CW) electron accelerators using beam recirculation through room temperature rf accelerating structures. Parameters of the RTM are: injection energy - 5 MeV; energy gain per pass - 12 MeV; number of passes - 15 or 16; final beam energy - 185-197 MeV; maximum current - 550 ¿A; rf frequency - 2380 MHz. At present, the electron gun and 100 keV beam transport line are operational, and most other major subsystems are in the construction or installation phase. Exceptions are the rf structure (under development), the 5 MeV beam transport line (in engineering design), and the extraction beam line (in conceptual design). Our studies of the original candidate accelerating structure, the disk-and-washer, have led to the discovery of beam steering modes which render this structure unsuitable for the RTM without at least substantial further development beyond the scope of the project. The most promising alternate for meeting the design goal of CW operation at 1.5 MeV/m is the side-coupled structure. A shunt impedance of 80 M¿/m has been measured in a test section of side-coupled structure at 2380 MHz, adequate cooling has been designed, and a 2.7 m long section of this design is under construction. The electron optics of the RTM have been studied in detail.


IEEE Transactions on Nuclear Science | 1983

A High Resolution Wire Scanner Beam Profile Monitor with a Microprocessor Data Acquisition System

R. I. Cutler; D. L. Mohr; Julian K. Whittaker; N. R. Yoder

A beam profile monitor has been constructed for the NBS-LANL Racetrack Microtron. The monitor consists of two perpendicular 30 ¿m diameter carbon wires that are driven through an electron beam by a pneumatic actuator. A long-lifetime, electroformed nickel bellows is used for the linear-motion vacuum feedthrough. Secondary emission current from the wires and a signal from a transducer measuring the position of the wires are simultaneously digitized by a microprocessor to yield beam current density profiles in two dimensions. The wire scanner is designed for use with both pulsed and cw beams.


IEEE Transactions on Nuclear Science | 1985

Performance of the 100 keV Chopper/Buncher System of the NBS-Los Alamos RTM Injector

Mark Wilson; R. I. Cutler; D. L. Mohr; S. Penner; L.M. Young

The purpose of the chopper/buncher system for the RTM injector is to chop a 100 keV 5 mA dc electron beam into 60/sup 0/-long pulses at 2380 MHz and then bunch these beam pulses to 10/sup 0/ at insertion into the 5 MeV injector linac. These beam manipulations must contribute a minimum increase in the phase space of the beam such that, at the entrance to the injector linac, the transverse emittance is less than 5..pi.. mm-mrad. Phase-shift measurements on the chopped beam indicate that the bunching fields are sufficient to achieve the required longitudinal compression. Beam envelope measurements, using wire scanners on the chopped and bunched beam, show that the emittance remains within design goals.


IEEE Transactions on Nuclear Science | 1983

The NBS-LANL RTM End-Magnet Field Mapper

E. R. Lindstrom; P. H. Debenham; D. L. Mohr; N. R. Yoder

A computer-controlled magnetic field mapper is under construction at the National Bureau of Standards to map the end magnets of the NBS-LANL racetrack microtron (RTM). The mapper consists of a large, two-dimensional translation stage which simultaneously positions a nuclear magnetic resonance (NMR) magnetometer probe in the 55 cm × 135 cm uniform field region and a temperature-compensated Hall effect probe in the fringe field region. A computer-based control system automatically positions the probes at points on a selected grid and records the measured field values and positions in computer memory. In this paper we describe the field mapping requirements, the mapper, its operation, and the field measurements and analysis that are to be performed.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1990

The hybrid undulator for the NIST-NRL free-electron laser

Ronald G. Johnson; D. L. Mohr; Mark Wilson; S. Penner; Francis C. Younger; Brian Ng; Kenneth M. Thomas

Abstract The NIST-NRL FEL will use a 3.64 m hybrid undulator that is being constructed at Brobeck Division of Maxwell Laboratories. The undulator has a period of 2.8 cm, a variable gap with a 1.0 cm minimum, a peak magnetic field of 0.54 T, and 130 total periods. The magnetic design uses SmCo permanent magnets and vanadium permendur pole pieces. Provision has been made to operate the undulator at half its length to enhance lasing at longer wavelengths. Remote control of gap and taper will permit on-line tuning of the wavelength and extraction efficiency. Vacuum chambers for both full- and half-length configurations are available. The oval aperture of the vacuum chambers is 0.86 cm by 1.6 cm. A system to measure the magnetic field along the undulator is included in the structure. A full-scale, one-period model of the magnetic design has been tested and the results exceed specifications. The mechanical structure of the undulator is nearly complete as is the control system. Construction of the magnet assemblies is under way.


IEEE Transactions on Nuclear Science | 1985

End Magnets for the NBS-LOS Alamos Racetrack Microtron

P. H. Debenham; E. R. Lindstrom; D. L. Mohr

Two end magnets have been designed and constructed for the 185 MeV NBS-Los Alamos racetrack microtron. The field has been measured in the first magnet and is uniform over a 0.62 m2 area to within ±2×10-4 at 1 T. The magnet meets all performance specifications. Field measurements are underway on the second magnet. In this paper, design and construction details which play an important role in magnetic performance are described, and the measured fields are compared with calculations.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1990

An optical resonator for the NIST-NRL free electron laser

B. Carol Johnson; Ronald G. Johnson; D. L. Mohr; Marc S. Price

Abstract A 9 m linear optical cavity will be used in the National Institute of Standards and Technology-Naval Research Laboratory free electron laser (NIST-NRL FEL). This FEL, which is driven by a racetrack microtron, is designed to lase from 0.2 to 10 μm. The resonator must accomodate the large dynamic range in wavelength, low gain, high average power and coherent harmonic emission of the laser. The laser can be configured for maximum gain, as is necessary in the ultraviolet, or to minimize diffraction losses, as is necessary in the infrared. This is done by changing the length of the undulator and the radius of curvature of the cavity mirrors.


1989 Intl Congress on Optical Science and Engineering | 1989

The NIST/NRL Free-Electron Laser Facility

P. H. Debenham; R. L. Ayres; John B. Broberg; R. I. Cutler; B. Carol Johnson; Ronald G. Johnson; E. R. Lindstrom; D. L. Mohr; J. E. Rose; Julian K. Whittaker; Neil D. Wilkin; Mark Wilson; Cha-Mei Tang; P. Sprangle; S. Penner

A free-electron laser (FEL) user facility is being constructed at the National Institute of Standards and Technology (NIST) in collaboration with the Naval Research Laboratory. The FEL, which will be operated as an oscillator, will be driven by the electron beam of the racetrack microtron (RTM) that is nearing completion. Variation of the electron kinetic energy from 17 MeV to 185 MeV will permit the FEL wavelength to be tuned from 200 nm to 10 pm. Performance will be enhanced by the high brightness, low energy spread, and continuous-pulse nature of the RTM electron beam. We are designing a new injector to increase the peak current of the RTM. A 3.6-m undulator is under construction, and the 9-m optical cavity is under design. The FEL will emit a continuous train of 3-ps pulses at 66 MHz with an average power of 10-200 W, depending on the wavelength, and a peak power of up to several hundred kW. An experimental area is being prepared with up to five stations for research using the FEL beam. Initial operation is scheduled for 1991.

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E. R. Lindstrom

National Institute of Standards and Technology

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Mark Wilson

National Institute of Standards and Technology

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R. I. Cutler

National Institute of Standards and Technology

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S. Penner

National Institute of Standards and Technology

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P. H. Debenham

National Institute of Standards and Technology

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Ronald G. Johnson

National Institute of Standards and Technology

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R. L. Ayres

National Institute of Standards and Technology

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J. E. Rose

National Institute of Standards and Technology

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Julian K. Whittaker

National Institute of Standards and Technology

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N. R. Yoder

National Institute of Standards and Technology

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