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1
High Voltage Radiography with a Microtron.
1976-01-01

A brief introduction of the microtron, a newcomer among high-energy X-ray units, and a comparison of the radiographic features of a microtron and a linear accelerator are reported. (Atomindex citation 08:310875)

National Technical Information Service (NTIS)

2
INVESTIGATION OF THE ENERGY SPECTRA OF ...
1962-06-21

... Title : INVESTIGATION OF THE ENERGY SPECTRA OF ELECTRONS ACCELERATED BY THE ELECTRIC FIELD OF A MICROTRON ...

DTIC Science & Technology

3
Beam breakup in a microtron.
1997-01-01

In a microtron, the path length change from pass to pass is a fixed multiple of the RF wavelength, and the accelerating system can be reasonably well approximated as a single cavity. Under such circumstances it is possible to derive an analytical formula ...

National Technical Information Service (NTIS)

4
Phase Stability of a Microtron Driving a Terahertz FEL.
2008-01-01

The phase stability of bunches accelerated by a magnetron-driven microtron-injector of a terahertz Free Electron Laser (FEL) has been studied to optimize the microtron regimes providing good operation of the FEL. The study is based on a simulation of the ...

National Technical Information Service (NTIS)

5
Recirculating electron accelerators
1984-01-01

A comprehensive account of developments in the field of recirculating electron accelerators is presented. Chapters are included in the role of recirculation in electron acceleration, the conventional microtron, linear accelerators and recirculation, race-track microtrons, representative ...

Energy Citations Database

6
Integrated superconducting microtron
1988-12-01

By this modified version the RF generator and the accelerating cavity can be integrated and put, with the magnets and extractor, into an evacuated vessel cooled to superconductivity.

Energy Citations Database

7
Phase stability of a microtron driving a terahertz FEL
2008-08-01

The phase stability of bunches accelerated by a magnetron-driven microtron-injector of a terahertz Free Electron Laser (FEL) has been studied to optimize the microtron regimes providing good operation of the FEL. The study is based on a simulation of the beam dynamics in the microtron considering 2-D motion of the ...

Energy Citations Database

8
Superconducting microtron: losses, refrigeration energy, and orbit current
1973-03-01

Superconducting cavities allow one to consider the c.w. operation of a microtron-type accelerator. Some of the theoretical results obtained are discussed. These results deal with the losses, the refrigeration energy, and the orbit current. (auth)

Energy Citations Database

9
ENEA racetrack microtron: Design criteria and status.
1989-01-01

A variable energy (20-100 MeV) racetrack microtron (RTM) is under construction at ENEA (Italian Commission for Alternative Energy Sources) Accelerator Laboratories, Frascati, Italy. This machine, designed to serve as a driver for a free electron laser (FE...

National Technical Information Service (NTIS)

10
Racetrack microtron: its potential in radiation therapy
1974-01-01

A discussion of the desirable characteristics of an electron accelerator for radiotherapy is given, based on personal interviews with a number of radiotherapists and radiological physicists in the United States. It is quite possible that the racetrack microtron, in its fully-developed form, will meet these requirements at a price that is not ...

Energy Citations Database

11
Microtrons for electron and photon radiotherapy
1981-04-01

For radiation therapy at medium and high energies the circular and the racetract microtron are ideally suited electron accelerators. The fine energy definition of the electron beam from a microtron allows the use of beam transport from one accelerator to several treatment units. This possibility makes an ...

Energy Citations Database

12
Prototype Sector Magnets for the GeV Electron Microtron (GEM).
1983-01-01

Three prototypes of the sector magnets for GeV Electon Microtron accelerators have been designed. One has been built and two are being constructed. The first is a full scale, 168 ton prototype for one-half of a 2 GeV Double Sided Microtron (DSM) sector ma...

National Technical Information Service (NTIS)

13
Microtron. A new accelerator for high voltage radiography
1974-01-01

A now method of generating high-energy x-rays using a microtron is described. The performance of a prototype machine for industrial radiography, which has an energy of 8 MeV with a radiation output of 1,500 rad/min at 1 meter from a 2 mm diameter focus is described. The microtron has special advantages of compactness and simplicity. (auth)

Energy Citations Database

14
Conceptual design of a 4-GeV hexagonal microtron
1982-01-01

This paper describes a higher-order variant of the microtron which offers an attractive option for furnishing cw electron beams at 4 GeV. The accelerator is a six-sided microtron consisting of three dispersive straight sections and three dispersion-free straight sections of constant length where three linacs are located.

DOE Information Bridge

15
Conceptual Design of a 4-GeV Hexagonal Microtron.
1982-01-01

This paper describes a higher-order variant of the microtron which offers an attractive option for furnishing cw electron beams at 4 GeV. The accelerator is a six-sided microtron consisting of three dispersive straight sections and three dispersion-free s...

National Technical Information Service (NTIS)

16
Longitudinal phase-space matching between microtrons at 185 MeV
1983-01-01

Electrons are accelerated to 185 MeV by a microtron. Then, they are injected into another microtron to boost the net energy up to a few GeV. Between the two microtrons both longitudinal and transverse phase-space matching are required. In this paper, we consider a longitudinal phase-ellipse matching which utilizes ...

DOE Information Bridge

17
Electron depth absorbed dose distribution for a 10 MeV clinical microtron.
1975-01-01

Central axis depth absorbed dose distributions of the electron beam from a medical microtron accelerator have been measured. The measured distributions differ from those of existing betatrons and linear accelerators. A larger absorbed dose build-up and a sharper dose fall-off are obtained in close agreement with theoretical calcuations ...

PubMed

18
Microtron Modelling and Control
2010-01-05

The article describes the design of the mathematical model and automatic control system of the microtron (high frequency cyclic electron accelerator). This type of accelerator was controlled manually till now. The critical values have been set up empirically on the basis of the previous operational experiences. The designed automatic ...

Energy Citations Database

19
Microtron Modelling and Control
2010-01-01

The article describes the design of the mathematical model and automatic control system of the microtron (high frequency cyclic electron accelerator). This type of accelerator was controlled manually till now. The critical values have been set up empirically on the basis of the previous operational experiences. The designed automatic ...

NASA Astrophysics Data System (ADS)

20
Design objectives for a GeV C. W. electron accelerator
1980-01-01

Design objectives are proposed for a continuous beam 2 GeV electron accelerator. Various accelerator concepts are examined in light of these requirements. A double-sided microtron shows promise for yielding major savings in capital cost and excellent beam characteristics.

DOE Information Bridge

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21
Brazing Techniques for Side-Coupled Electron Accelerator Structures.
1986-01-01

The collaboration between the Los Alamos National Laboratory and the National Bureau of Standards (NBS), started in 1979, has led to the development of an advanced c-w microtron accelerator design. The four 2380-MHz NBS accelerating structures, containing...

National Technical Information Service (NTIS)

22
Bunching properties of a classical microtron-injector for a far infrared free electron laser
2001-12-01

Longitudinal bunching properties of a classical microtron have been investigated by the numerical simulation of the longitudinal motion of accelerated electrons. The simulations were performed for the 12-turn microtron that has been used as an injector for the KAERI far infrared free electron laser. Based on the bunching properties of ...

NASA Astrophysics Data System (ADS)

23
Accelerator Technology Program. Status report, April-September 1985
1986-09-01

This report presents highlights of major projects in the Accelerator Technology (AT) Division of the Los Alamos National Laboratory. Radio-frequency and microwave technology are dealt with. The p-bar gravity experiment, accelerator theory and simulation activities, the Proton Storage Ring, and the Fusion Materials Irradiation Test ...

DOE Information Bridge

24
Beam breakup in a microtron
1997-06-01

In a microtron, the path length change from pass to pass is a fixed multiple of the RF wavelength, and the accelerating system can be reasonably well approximated as a single cavity. Under such circumstances it is possible to derive an analytical formula for the multipass beam breakup threshold current. The threshold current determined by numerical ...

DOE Information Bridge

25
A 100-MeV injector race-track microtron for the max storage-ring/pulse-stretcher
1983-08-01

A 100 MeV pulsed race-track microtron (RTM) has been in operation at the University of Lund since 1979/sup 1/. The RTM will now be used as an injector for a storage-ring/pulse-stretcher currently being built. The RTM with its injection, acceleration and extraction systems are described and the beam characteristics are discussed.

Energy Citations Database

26
GEM: ANL 4-GeV CW electron microtron design
1983-01-01

A six-sided hexagonal microtron has been chosen as the accelerator to generate the beams required to pursue a national research program at a CW 4 GeV electron laboratory. This option has the advantage of superior beam quality, low capital and operating cost, and promise of furnishing beams of several electron energies simultaneously. Only moderate rf power ...

DOE Information Bridge

27
Racetrack microtron radio-frequency system
1981-01-01

The design and construction progress of a prototype rf system to drive the Los Alamos-NBS racetrack microtron (RTM) electron accelerator is described. The rf system requires 450-kW cw at 2380 MHz from a single klystron. The output from the klystron is split three ways to drive a capture section, a preaccelerator section, and the main ...

Energy Citations Database

28
Overview of accelerators in medicine
1993-06-01

Accelerators used for medicine include synchrotrons, cyclotrons, betatrons, microtrons, and electron, proton, and light ion linacs. Some accelerators which were formerly found only at physics laboratories are now being considered for use in hospital-based treatment and diagnostic facilities. This paper presents typical operating ...

DOE Information Bridge

29
Overview of Particle Production Facilities Available in the Czech Republic
2007-11-26

A brief overview of particle production facilities available in Czech Republic is given. In particular are described the facilities at the Nuclear Physics Institute in Rez near Prague, namely: an isochronous cyclotron, an electrostatic accelerator tandetron and a microtron. An outline of the main research projects carried out is included.

Energy Citations Database

30
Overview of Particle Production Facilities Available in the Czech Republic
2007-11-01

A brief overview of particle production facilities available in Czech Republic is given. In particular are described the facilities at the Nuclear Physics Institute in Rez near Prague, namely: an isochronous cyclotron, an electrostatic accelerator tandetron and a microtron. An outline of the main research projects carried out is included.

NASA Astrophysics Data System (ADS)

31
Microtron Injector for LEP.
1979-01-01

In the 15 to 100 GeV position electron Colliding Beam Machine (LEP) under study by the European Committee for Future Accelerators it is intended to use a 460 MeV accumulation ring (ACR) to collect a previously bunched beam of electrons or positrons before...

National Technical Information Service (NTIS)

32
GeV C. W. electron microtron design report
1982-05-01

Rising interest in the nuclear physics community in a GeV C.W. electron accelerator reflects the growing importance of high-resolution short-range nuclear physics to future advances in the field. In this report major current problems are reviewed and the details of prospective measurements which could be made with a GeV C.W. electron facility are discussed, together with their ...

DOE Information Bridge

33
Critical issues for high-power FEL based on microtron recuperator/electron out-coupling scheme
1997-03-01

The FELs based on the RF accelerator-recuperator and the electron outcoupling is promising for obtaining average output power of hundreds of kilowatts. We present basic considerations for the system stability and performance optimization for this scheme.

Energy Citations Database

34
Accelerator Technology Program. Status Report, October 1984-March 1985.
1986-01-01

Activities of the racetrack-microtron development programs are highlighted, one of which is being done in collaboration with the National Bureau of Standards and the other with the University of Illinois; the BEAR (Beam Experiment Aboard Rocket) project; ...

National Technical Information Service (NTIS)

35
COMPARISON OF THE EFFECT OF ELECTRON IRRADIATION ON THE OPTICAL ACTIVITY OF RACEMATES AND OPTICAL ANTIPODES
1962-09-01

In connection with the assertions repeatedly appearing in the literature that electrons emitted during BETA decay or even accelerated in a microtron exert different effects on mirror isomers (antipodes), a detailed experimental investigation of the effect of electron irradiation of solid racemates and separated forms of optical isomers on their ...

Energy Citations Database

36
Prototype sector magnets for the GeV electron microtron (GEM)
1983-08-01

Three prototypes of the sector magnets for GeV Electron Microtron accelerators have been designed. One has been built and two are under construction. The first is a full-scale 168-ton prototype for one-half of a 2 GeV Double Sided Microtron sector magnet. The successful fabrication and testing of the pole pieces for this prototype have ...

Energy Citations Database

37
Variable-energy microtron-injector for a compact wide-band FIR free electron laser
2003-07-01

A microtron-injector (Proceedings of the 2001 Particle Accelerator Conference, USA, 2001, 2739) for the KAERI compact far infrared free electron laser (FIR FEL) facility has been upgraded to provide tuning of the FEL wavelength from 100?m to more than 300?m. The wide-band tunability of the radiation has been achieved by changing the kinetic energy of the ...

NASA Astrophysics Data System (ADS)

38
Magnetron-driven microtron injector of a terahertz free electron laser
2009-04-01

A magnetron-driven microtron injector has been developed for a terahertz free electron laser (FEL). An internal injection system was chosen for the microtron to achieve a compact and inexpensive design. The system provides acceleration of electrons with low emittance and energy spread that is highly important for the FEL. However, the ...

NASA Astrophysics Data System (ADS)

39
Electron gun with off-axis beam injection for a race-track microtron
2010-12-01

A miniature 12 MeV race-track microtron for medical applications is under construction at the Technical University of Catalonia in collaboration with several Spanish centers and companies and the Skobeltsyn Institute of Nuclear Physics of the Moscow State University. As a source of electrons a compact 3D on-axis electron gun with an off-axis cathode has been designed to allow ...

NASA Astrophysics Data System (ADS)

40
Method and apparatus for compensation of effects of misalignment between deflecting magnetic fields and a linear accelerator in a race track microtron
1978-10-31

A method for compensating the effects of misalignment between deflecting magnetic fields and a linear accelerator in a race track microtron where properly injected and accelerated electrons travel along successive complete orbits numbered in sequence comprises the steps of generating on both sides of the linear ...

Energy Citations Database

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41
Accelerator Technology Program: Status report, October 1985--March 1986: Volume 1
1988-07-01

This report presents highlights of the major projects in the Accelerator Technology (AT) Division of the Los Alamos National Laboratory. The first section details progress associated with the accelerator test stand. Following sections cover achievements in accelerator theory and simulation, LAMPF II accomplishments, and updates on ...

Energy Citations Database

42
Prototype sector magnets for the GeV electron microtron (GEM)
1983-01-01

Three prototypes of the sector magnets for GeV Electon Microtron accelerators have been designed. One has been built and two are being constructed. The first is a full scale, 168 ton prototype for one-half of a 2 GeV Double Sided Microtron (DSM) sector magnet. The successful fabrication and testing of the pole pieces for this prototype ...

Energy Citations Database

43
Study of a national 2-GeV continuous beam electron accelerator
1980-08-01

Current trends in research in medium energy physics with electromagnetic probes are reviewed briefly and design objectives are proposed for a continuous beam 2 GeV electron accelerator. Various types of accelerator systems are discussed and exploratory designs developed for two concepts, the linac-stretcher ring and a double-sided ...

Energy Citations Database

44
Study of a national 2 GeV continuous beam electron accelerator
1979-10-01

Current trends in research in medium energy physics with electromagnetic probes are reviewed briefly and design objectives are proposed for a national continuous beam 2 GeV electron accelerator. Various types of accelerator systems are discussed and exploratory designs developed for two concepts, the linac-stretcher ring and a modified ...

DOE Information Bridge

45
High-intensity accelerators
1981-01-01

The design of high-intensity accelerators is described, using examples of machines being built at the Los Alamos National Laboratory. The major design problem with these accelerators is associated with control of beam loss when accelerator intensity is increased. Beam dynamics, beam loss, and the radio-frequency quadrupole structure ...

DOE Information Bridge

46
Brazing techniques for side-coupled electron accelerator structures
1986-01-01

The collaboration between the Los Alamos National Laboratory and the National Bureau of Standards (NBS), started in 1979, has led to the development of an advanced c-w microtron accelerator design. The four 2380-MHz NBS accelerating structures, containing a total of 184 accelerating cavities, have been fabricated ...

DOE Information Bridge

47
Injection system for microtron-based terehertz FEL
2005-09-01

A reliable injection system of the widely tunable microtron-based terahertz Free Electron Laser (FEL) has been developed and during last few years provides stable operation of the FEL for users. The system is based on the long-life thermionic cathode assembly using 2.5 mm-in diameter monocrystalline LaB{sub 6} emitter, heated by the tungsten cylindrical filament with the power ...

DOE Information Bridge

48
Magnetron-driven microton-injector of a terahertz free electron laser
2008-01-01

A magnetron-driven microtron injector has been developed for a terahertz free electron laser (FEL). An internal injection system was chosen for the microtron to achieve a compact and inexpensive design. The system provides acceleration of electrons with low emittance and energy spread that is highly important for the FEL. However, the ...

Energy Citations Database

49
The Sao Paulo Microtron: Equipment and Planned Experiments
2007-10-26

The Linear Accelerator Laboratory (LAL) of the Instituto de Fisica da Universidade de Sao Paulo (IFUSP) is building a two-stage racetrack microtron, which will generate continuous wave electron beams with energies up to 38 MeV. This paper describes the characteristics of the accelerator, and reports on the experimental equipment that ...

Energy Citations Database

50
Control system for the NBS microtron accelerator
1985-01-01

As various subsystems of the National Bureau of Standards/Los Alamos racetrack microtron accelerator are being brought on-line, we are gaining experience with some of the innovations implemented in the control system. Foremost among these are the joystick-based operator controls, the hierarchical distribution of control system intelligence, and the ...

Energy Citations Database

51
CW side-coupled linac for the Los Alamos/NBS racetrack microtron
1983-08-01

A 2.7-m side-coupled linac has been built as part of the 5-MeV injector for the cw room-temperature racetrack microtron (RTM) being constructed in collaboration with the National Bureau of Standards (NBS). The linac is designed to accelerate the electron beam from 1 to 5 MeV with an accelerating gradient of 1.5 MeV/m. Fabrication of ...

Energy Citations Database

52
C-w side-coupled linac for the Los Alamos-NBS racetrack microtron
1983-01-01

A 2.7-m side-coupled linac has been built as part of the 5-MeV injector for the cw room-temperature racetrack microtron (RTM) being constructed in collaboration with the National Bureau of Standards (NBS). The linac is designed to accelerate the electron beam from 1 to 5 MeV with an accelerating gradient of 1.5 MeV/m. Fabrication of ...

DOE Information Bridge

53
Fabrication and tuning techniques for side-coupled electron accelerator structures
1986-01-01

Beginning in 1979, Los Alamos entered into a collaboration with the National Bureau of Standards (NBS) to develop an advanced cw microtron accelerator. The accelerating structures (one 0.9-m-long, one 2.7-m-long, and two 4.0-m-long) containing a total of 184 accelerating cavities have been fabricated and tuned to ...

Energy Citations Database

54
Performance of the high power rf system for the NIST--Los Alamos racetrack microtron
1988-01-01

The high power RF system of the NIST-LANL RTM has been tested at nominal full power levels and has accelerated electron beams successfully. RF stability and calibration measurements have been made using the accelerated electron beam. These measurements have been used to calculate the effective shunt impedance of the side- coupled ...

Energy Citations Database

55
Accelerator technology program. Status report, October 1984-March 1985
1986-04-01

Activities of the racetrack-microtron development programs are highlighted, one of which is being done in collaboration with the National Bureau of Standards and the other with the University of Illinois; the BEAR (Beam Experiment Aboard Rocket) project; work in beam dynamics; the proposed LAMPF II accelerator; and the Proton Storage Ring. Discussed next ...

Energy Citations Database

56
Accelerator technology program
1984-05-01

Highlights in beam dynamics, accelerator inertial fusion, radio frequency structure development, the racetrack microtron, CERN high energy physics experiment NA-12, and high flux radiographic linac study are reported. Selected proton Storage Ring activities and an update on the free electron laser are discussed. The fusion materials irradiation test ...

NASA Astrophysics Data System (ADS)

57
Accelerator Technology Program. Status report, October 1983-March 1984
1985-01-01

This report covers major projects in the Accelerator Technology (AT) Division of the Los Alamos National Laboratory. The first sections highlight activities related to beam dynamics, inertial fusion, structure development, the racetrack microtron, and the CERN high-energy physics experiment NA-12. Discussed next is the Fusion Materials Irradiation Test ...

DOE Information Bridge

58
The search for dark matter gauge bosons with the Mainz Microtron
2011-04-01

A pilot experiment in the search for light gauge bosons at the spectrometer setup of the A1 collaboration at MAMI is presented. Light gauge bosons arise naturally in a wide range of theoretical approaches beyond the standard model and are in accordance with several pieces of experimental evidence not yet understood in the standard model. A first test measurement at MAMI showed that existing limits ...

NASA Astrophysics Data System (ADS)

59
Compact muon source with electron accelerator for a mobile Mu SR facility
2008-01-01

In order to increase accessibility to the {mu}SR spectroscopy for people in various fields of science and engineering, a conceptual design study was made to realize a compact and inexpensive muon source by using 300-MeV electron microtron and a large-acceptance muon-capture. Advanced radiography imaging with muon spin probes will become possible for bio-medical studies, ...

Energy Citations Database

60
Racetrack microtron rf system
1985-01-01

The rf system for the National Bureau of Standards (NBS)/Los Alamos cw racetrack microtron is described. The low-power portion consists of five 75-W amplifers that drive two input ports in each of two chopper deflection cavities and one port in the prebuncher cavity. A single 500-kW klystron drives four separate 2380-MHz cavity sections: the two main ...

Energy Citations Database

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61
High-power RF controls for the NBS-Los Alamos racetrack microtron
1985-10-01

The high-power rf system for the National Bureau of Standards (NBS)-Los Alamos racetrack microtron (RTM) uses waveguide power splitters and waveguide phase shifters to distribute rf power from a single 500-kw cw klystron to four side-coupled accelerating structures. The amplitude and phase of each structure is controlled by a feedback system that uses the ...

Energy Citations Database

62
A racetrack microtron RF system
1985-10-01

The rf system for the National Bureau of Standards (NBS)/Los Alamos cw racetrack microtron is described. The low-power portion consists of five 75-W amplifiers that drive two input ports in each of two chopper deflection cavities and one port in the prebuncher cavity. A single 500-kW klystron drives four separate 2380-MHz cavity sections: the two main ...

Energy Citations Database

63
NBS-LASL racetrack microtron
1980-01-01

The NBS-LASL racetrack microtron (RTM) is a joint project of the National Bureau of Standards (NBS) and the Los Alamos Scientific Laboratory (LASL). This is a new accelerator research project whose goal is to determine the feasibility of building a high-energy, high-current, cw electron accelerator using beam recirculation and ...

Energy Citations Database

64
Dribs II:. a Source of Radioactive Nuclei
2002-12-01

The facility for neutron-rich nuclei production, as a specific part of the project DRIBS - phase II, based on the use of photofission and the characteristics of microtron MT-25 as a source of bremsstrahlung photons are described. Target selection with regard to maximum yield production of strong neutron-rich fission products and with respect to its safety and availability is ...

NASA Astrophysics Data System (ADS)

65
High Power Electronics. Number 5, 1968,
1971-01-27

... a microtron with a nonuniform magnetic field; Measurement of the magnetic field nonuniformity in a microtron with 30 orbits; Phase oscillations in a ...

DTIC Science & Technology

66
ACCELERATORS WITH STABLE OVERLAPPING PARTICLE TRAJECTORIES
1958-03-01

The features of a new type accelerator with a magnetic system consisting of several sectors separated by weak intermedate fields are described. The magnetic system has two mutually perpendicular synmetric planes but does not possess either axial or central symmetry. All orbits of the particles cross at the same point in which is found the ...

Energy Citations Database

67
Intrapulse frequency stability of a magnetron frequency-locked through a wave reflected from an accelerating cavity
2011-08-01

A laboratory-size Free Electron Laser (FEL) driven by a classical S-band microtron fed by a 2.5 MW magnetron generates terahertz radiation tunable in a wide range. The FEL provides output pulse power of �50 W in the wavelength range of 100�300 ?m with a pulse duration of 2�4 ?s. The FEL parameters are available due to stabilization of the accelerated ...

NASA Astrophysics Data System (ADS)

68
Accelerator Technology Program
1984-07-01

Highlights of major projects in the Accelerator Technology Division of the Los Alamos National Laboratory are presented. The first section deals with the Fusion Materials Irradiation Test Facility's 2-MeV accelerator on which tests began in May, as scheduled. Then, activities are reported on beam dynamics, inertial fusion, structure development, the ...

NASA Astrophysics Data System (ADS)

69
NIST--Los Alamos racetrack microtron status
1988-01-01

The NIST-Los Alamos Racetrack Microtron (RTM) is designed to deliver a low-emittance electron beam of up to 0.5 mA cw over an energy range of 17 MeV to 185 MeV. Fed by a 5 MeV injector, the RTM contains two 180/degree/ end magnets that recirculate the beam up to 15 times through a 12 MeV RF linac. The linac, which operates in a standing-wave mode at 2380 MHz, has been tested ...

Energy Citations Database

70
Longitudinal beam dynamics with phase slip in race-track microtrons
2008-11-01

Implementation of low-energy injection schemes in race-track microtron (RTM) designs requires a better understanding of the longitudinal beam dynamics. Unlike the high-energy case a low-energy beam slips in phase with respect to the accelerating field phase so that the standard notion of synchronous particle is not applicable. In the article, we generalize ...

NASA Astrophysics Data System (ADS)

71
Electron Accelerators for Research at the Frontiers of Nuclear Physics
1986-10-01

Electron accelerators for the frontiers of nuclear physics must provide high duty factor (gte 80) for coincidence measurements; few-hundred-MeV through few-GeV energy for work in the nucleonic, hadronic, and confinement regimes; energy resolution of ~ 10-4; and high current (gte 100 zA). To fulfill these requirements new machines and upgrades of existing ...

DOE Information Bridge

72
DAW structure for the NBS/Los Alamos racetrack microtron
1981-01-01

The results of a testing program on the disk-and-washer (DAW) structure with tee supports are presented. These results have led to the design of a 2.4-m DAW linac for use as the preaccelerator section of the National Bureau of Standards (NBS)/Los Alamos racetrack microtron (RTM). This structure uses two tee supports for each pair of washers, instead of four, and the structure ...

DOE Information Bridge

73
Mikrotron MT-25. Rabochee soveshchanie po ispol'zovaniyu mikrotronov v yadernoj fizike. (Microtron MT-25. Workshop on application of microtrons in nuclear physics).
1993-01-01

Problems of development of microtron equipment and construction of microtrons at scientific centers of JINR country-members are discussed. Results of experimental conducted in microtron beams are presented in the directions of photonuclear reactions, fiss...

National Technical Information Service (NTIS)

74
A 22 MeV microtron for radiation therapy.
1977-04-01

The first 22 MeV micron installation for radiation therapy is described with regard to the general design, the beam transport and the gantry. The first measurements of the electron depth dose curves indicate that the distributions obtained are superior to those of most betatrons and linear accelerators. For the same electron beam energy the depth of dose maximum and the 90 or ...

PubMed

75
Generation of Extremely Low Frequency Electromagnetic Radiation by Beams
2001-10-01

In this report the results of investigation of extremely low frequency(ELF) secondary electromagnetic radiation(SER) generated by beams of electrons of microtron MT-22S (E=13 MeV,average current I=1-10 mkA,t=2,5 mks, f=386 Hz) in residual gas in dielectric electronpipe(glass,diametr d=50mm,length 120m) have been expounded. Measurements ...

NASA Astrophysics Data System (ADS)

76
THE MICROTRON AS A HIGH-ENERGY, HIGH CURRENT PARTICLE ACCELERATOR
1958-06-01

It is proposed that the conventional electron microtron may be converted into a high-energy accelerator for protons or electrons in the Bev range, and capable of very high currents. It would require a high-energy injector, e.g., an FFAG cyclotron, capable of supplying protons of energy above 500 Mev in a beam of high intensity and high quality. ...

Energy Citations Database

77
Present state of the MAMI control system
1990-08-01

MAMI (Mainz Microtron) is an electron accelerator consisting of a cascade of three race-track microtrons, with an output electron beam of 855 MeV and 100 ?A cw [1]. The first two stages (output energy 180 MeV) were operative for nuclear-physics experiments from 1983 to 1987 and have since been transferred to a new building. They will ...

NASA Astrophysics Data System (ADS)

78
The NBS proposal for a one GeV CW racetrack microtron facility
1983-08-01

As part of a joint accelerator research project with the Los Alamos National Laboratory, NBS is now building a 200 MeV, high current, CW racetrack microtron (RTM). Upon its completion, scheduled for 1984, the authors propose to use this machine to provide CW electron beams to nuclear physics experimenters, and also as the injector for a second stage RTM to ...

Energy Citations Database

79
High-power rf controls for the NBS-Los Alamos racetrack microtron
1985-01-01

The high-power rf system for the National Bureau of Standards (NBS)-Los Alamos racetrack microtron (RTM) uses waveguide power splitters and waveguide phase shifters to distribute rf power from a single 500-kW cw klystron to four side-coupled accelerating structures. The amplitude and phase of each structure is controlled by a feedback system that uses the ...

Energy Citations Database

80
Effect of synchrotron radiation in the proposed 4 GeV Argonne microtron
1983-01-01

Synchrotron radiation in the sector magnets of the 4-GeV microtron designed at the Argonne National Laboratory produces a small but noticeable distortion of the closed orbits of the system and a very-significant growth of the horizontal and longitudinal phase-space emittances. Because of the small apertures in the three 25-meter linacs, it is important that the expected growth ...

DOE Information Bridge

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81
Accelerator developments since the ZGS by ZGS people
1994-12-31

The ZGS was a facility, as well as an organization, where people got together to pursue a common goal of doing exciting science of the day. In this note, the authors describe notable events related to accelerators and accelerator people since the closing of the ZGS program some 15 years ago. Many of the same ZGS people have been carrying out the ...

DOE Information Bridge

82
Accelerator Technology Program. Progress report, January-June 1980
1980-03-01

The activities of Los Alamos Scientific Laboratory's (LASL) Accelerator Technology (AT) Division during the first six months of calendar 1980 are discussed. This report is organized around major projects of the Division, reflecting a wide variety of applications and sponsors. The first section summarizes progress on the Proton Storage Ring to be located between LAMPF ...

DOE Information Bridge

83
Radiation parameters of 6 to 20 MeV scanning electron beams from the Saturne linear accelerator

Depth doses of the scanning electron beams from the Saturne Therac-20 linear accelerator at nominal energies of 6,9,13,17, and 20 MeV were measured in polystyrene using a thin window parallel plate ionization chamber. Central axis depth dose curves are derived and are analyzed according to the method of Brahme and Svensson. For each of the five electron energies, values are ...

Energy Citations Database

84
NBS-LASL cw microtron
1980-01-01

The NBS-LASL racetrack microtron (RIM) is a joint research project of the National Bureau of Standards and the Los Alamos Scientific Laboratory. The project goals are to determine the feasibility of, and develop the necessary technology for building high-energy, high-current, continuous-beam (cw) electron accelerators using beam recirculation and ...

Energy Citations Database

85
Statistical treatment of misalignments in particle accelerators
2011-03-01

To know how much misalignment is tolerable for a particle accelerator is an important input for the design of these machines. In particle accelerators the beam must be guided and focused using bending magnets and magnetic lenses, respectively. The alignment of the lenses along a transport line aims to ensure that the beam passes through their optical axes ...

NASA Astrophysics Data System (ADS)

86
Compendium of Scientific Linacs
2003-05-16

The International Committee supported the proposal of the Chairman of the XVIII International Linac Conference to issue a new Compendium of linear accelerators. The last one was published in 1976. The Local Organizing Committee of Linac96 decided to set up a sub-committee for this purpose. Contrary to the catalogues of the High Energy Accelerators which ...

DOE Information Bridge

87
Accelerator Technology Program. Status report, January-September 1983
1984-07-01

This report presents highlights of major projects in the Accelerator Technology Division of the Los Alamos National Laboratory. The first section deals with the Fusion Materials Irradiation Test Facility's 2-MeV accelerator on which tests began in May, as scheduled. Then, activities are reported on beam dynamics, inertial fusion, structure ...

DOE Information Bridge

88
Accelerator technology program. Status report, July-December 1982
1984-05-01

Major projects of the Los Alamos National Laboratory's Accelerator Technology Division are discussed, covering activities that occurred during the last six months of calendar 1982. The first sections report highlights in beam dynamics, accelerator inertial fusion, radio-frequency structure development, the racetrack microtron, ...

Energy Citations Database

89
Accelerator technology program. Progress report, July-December 1980
1982-01-01

The activities of Los Alamos National Laboratory's Accelerator Technology Division are discussed. This report covers the last six months of calendar 1980 and is organized around the Division's major projects. These projects reflect a wide variety of applications and sponsors. The major technological innovations promoted by the Pion Generator for Medical ...

Energy Citations Database

90
Accelerator technology program. Progress report, January-December 1979
1980-11-01

The activities of Los Alamos Scientific Laboratory's (LASL) Accelerator Technology (AT) Division during the calendar year 1979 are highlighted, with references to more detailed reports. This report is organized around the major projects of the Division, reflecting a wide variety of applications and sponsors. The first section covers the Fusion Materials Irradiation ...

DOE Information Bridge

91
Tagging Efficiency Measurements at the A2 Glasgow Photon Tagging Facility at MAMI
2010-02-01

We present the analysis of experiment-specific measurements of the efficiency of the Glasgow Photon Tagging Spectrometer in the A2 Hall at the Mainz Microtron (MAMI C). The photon tagger is being used for Crystal Ball and TAPS experiments. MAMI C is a particle accelerator capable of producing energies of up to 1.604 GeV. Photons are produced from the MAMI ...

NASA Astrophysics Data System (ADS)

92
Sub-MeV tunably polarized X-ray production with laser Thomson backscattering.
2008-05-01

Reported in this article is the generation of unique polarized x-rays in the sub-MeV region by means of the Thomson backscattering of the Nd:YAG laser photon with a wavelength of 1064 nm on the 150 MeV electron from the microtron accelerator. The maximum energy of the x-ray photons is estimated to be about 400 keV. The total energy of the backscattered ...

PubMed

93
Sub-MeV tunably polarized X-ray production with laser Thomson backscattering
2008-05-15

Reported in this article is the generation of unique polarized x-rays in the sub-MeV region by means of the Thomson backscattering of the Nd:YAG laser photon with a wavelength of 1064 nm on the 150 MeV electron from the microtron accelerator. The maximum energy of the x-ray photons is estimated to be about 400 keV. The total energy of the backscattered ...

Energy Citations Database

94
Radiation dosimetry: Electron beams with energies between 1 and 50 MeV
1984-09-15

The use of high-energy electrons in radiation therapy has expanded and linear accelerators and microtrons have come into more frequent use beside the previously dominating betatrons. The properties of the clinical electron beams in present use are, therefore, greatly diversified and new characterizations are needed to describe the beam qualities for ...

Energy Citations Database

95
Determination of a Thorium Content in Soil Samples by Means of Gamma-Activation Analysis and X-Ray Spectrometry

A highly sensitive method based on the reaction ^{232}Th(\\gamma, n)^{231}Th (T_{1/2} = 25.5 h) is developed for determining thorium in soil and environmental samples with a thorium content at a level of 3x10^{-7} g/g. Samples were irradiated for 4 hours with a maximum photon energy of 24.5 MeV at a compact electron accelerator - the MT-25 microtron of ...

E-print Network

96
A Mott polarimeter operating at MeV electron beam energies.
2011-03-01

We have developed a Mott electron polarimeter for the Mainzer microtron (MAMI) accelerator in Mainz, Germany. At beam energies ranging between 1.0 and 3.5 MeV two double focusing magnet spectrometers collect elastically backscattered electrons from gold targets. In spite of the small spectrometer acceptance, a sufficient statistical efficiency is achieved ...

PubMed

97
A Mott polarimeter operating at MeV electron beam energies
2011-03-01

We have developed a Mott electron polarimeter for the Mainzer microtron (MAMI) accelerator in Mainz, Germany. At beam energies ranging between 1.0 and 3.5 MeV two double focusing magnet spectrometers collect elastically backscattered electrons from gold targets. In spite of the small spectrometer acceptance, a sufficient statistical efficiency is achieved ...

NASA Astrophysics Data System (ADS)

98
Application of the linac of the IREN facility for production some radionuclides and multielemental activation analysis
2009-03-31

The possibility to develop multielemental activation analysis and production of some radionuclides widely used for the nuclear medicine, radiobiology and ecology monitoring at the linear electron accelerator (E{sub e}- = 75 MeV) of the facility IREN (FLNP, JINR) are considered. Based on the experimental data obtained at low energy (E{sub e}-<30 MeV) electron ...

Energy Citations Database

99
Utilization of Microtron for Multi-Element Photon Activation Analysis.
1983-01-01

Utilization of a microtron for multielement photon activation analysis of ferruginous laterites, soil and geological standards, iron-manganese nodules, meteorites and samples from superdeep drilled holes (h >= 7 Kms) was investigated. Interferences, cause...

National Technical Information Service (NTIS)

100
NBS/LANL Racetrack Microtron Control System.
1985-01-01

The distributed intelligence control system for the NBS/LANL racetrack microtron (RTM) is now nearing completion with all major subsystems implemented and tested, thus providing some operating experience with most of the control system innovations. These ...

National Technical Information Service (NTIS)

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101
Investigation of Meteorite Chemical Composition by Activation Analysis with Microtron.
1983-01-01

Application of bremsstrahlung and photoneutrons from a microtron for determining the chemical composition of stone and iron meteorites was investigated. Nearly 20 elements have been determined mostly by instrumental photon activation analysis, but instrum...

National Technical Information Service (NTIS)

102
Design of the Argonne double-sided microtron
1981-01-01

The design study of a double-sided microtron is presented. The result of beam-optic calculations in several sector-magnet configurations is described. Current limitation by beam backup is discussed.

DOE Information Bridge

103
Application of a Photoneutron Microtron for Nondestructive Activation Determination of Uranium.
1980-01-01

The application of a photoneutron microtron for a nondestructive activation determination of uranium has been investigated in samples of the compound chemical composition. The resonance neutron flux density is 2x10 exp 7 n/cm exp -2 xs exp -1 in the activ...

National Technical Information Service (NTIS)

104
Application of Bremsstrahlung and Photoneutrons of a Microtron for Activation Analysis of Tektites.
1984-01-01

A possibility to determine nearly 30 rock-forming and rare earth elements in tektites-Australites, Philippinites, Moldavites and glasses from Zhamanshin crater and an some basic rock types using microtron gamma-quanta and photoneutrons with the 10 exp -6 ...

National Technical Information Service (NTIS)

105
Accelerator technology program. Progress report, January-June 1981
1982-05-01

This report covers the activities of Los Alamos National Laboratory's Accelerator Technology Division during the first 6 months of calendar 1981. We discuss the Division's major projects, which reflect a variety of applications and sponsors. The varied technologies concerned with the Proton Storage ring are concerned with the Proton Storage Ring are ...

DOE Information Bridge

106
THE MICROTRON
1962-03-16

Page 1. UNCLASSIFIED AD214 0+60 ARMED SERVICES TECHNICAL' INFORMIAION AGENCY ARLINGTON HALL STATION ...

DTIC Science & Technology

107
Proposal for FEL Experiments Driven by the National Bureau ...
1985-12-31

... Accession Number : ADA163227. Title : Proposal for FEL Experiments Driven by the National Bureau of Standards' CW Microtron. ...

DTIC Science & Technology

108
Evaluation of a racetrack microtron for high-energy radiography
1982-01-01

A series of tests was conducted on the 50-MeV-racetrack microtron at the Royal Institute of Technology in Stockholm, Sweden for the purpose of determining the quality of industrial radiographs generated by the bremsstrahlung beam of the machine. The results of the experiments indicate that radiographs with a spatial sensitivity better than those produced by more conventional ...

Energy Citations Database

109
APPLICATION OF MICROTRONS IN NONDESTRUCTIVE ...
1980-03-01

... MELEKHIN,VN ; SERGEEV,VA. Report Date : MAR 1980. Pagination or Media Count : 4. Abstract : THE ARTICLE DISCUSSES ...

DTIC Science & Technology

110
Design Elements and State of Advance of a Microtron Model (2.5-5 Mev); ELEMENTI DI PROGETTO E STATO DI AVANZAMENTO DI UN MODELLO DI MICROTRONE (2.5-5 Mev)
1963-11-28

The principal characteristics of a microtron or electron cyclotron are briefly reviewed. The construction of the magnet, vacuum chamber, and the radiofrequency installation is described. (J.S.R.)

Energy Citations Database

111
Development of a sub-MeV X-ray source via Compton backscattering
2011-05-01

At the Kansai Photon Science Institute of the Japan Atomic Energy Agency, we have developed a Compton backscattered X-ray source in the energy region of a few hundred keV. The X-ray source consists of a 150-MeV electron beam, with a pulse duration of 10 ps (rms), accelerated by a Microtron accelerator and an Nd:YAG laser, with a pulse ...

NASA Astrophysics Data System (ADS)

112
Accelerator technology program. Progress report, July-December 1981
1982-08-01

We report on the major projects of the Los Alamos National Laboratory's Accelerator Technology Division during the last 6 months of calendar year 1981. We have continued work on the radio-frequency quadrupole linear accelerator; we are doing studies of octupole focusing. We have completed the design study on an unusual electron-linear radiographic ...

DOE Information Bridge

113
rf beam-current, -phase, and -position monitors
1984-12-12

A prototype rf beam monitor has been tested on the Racetrack Microtron's (RTM) 100 kV injector beam line at the National Bureau of Standards (NBS). This beam monitor is capable of measuring the current, the relative phase, and the position of the beam. The beam is bunched at 2380 MHz for acceleration by the linac in the injector beam line. This ...

Energy Citations Database

114
Transverse beam containment in the ANL 4-GeV microtron
1983-01-01

Optical systems have been designed to contain the electrons during the acceleration from 0.185 to 4.0 GeV. These systems are located in the dispersive straight sections and maintain a matched dispersion-free beam with ..beta..* = 15.0 m in the linac centers, and transverse beam waists in the centers of the dispersive straight sections. A thin-lens code has been developed to ...

DOE Information Bridge

115
The isomeric ratios in some photonuclear reactions (?, n), (?, p), (?, 2 n), and (?, np) induced by bremsstrahlungs with end-point energies in the Giant Dipole Resonance region
2009-03-01

We have determined the isomeric ratios in photonuclear reactions 116Cd(?, n)115 m, g Cd, 138Ce(?, n)137 m, g Ce, 153Eu(?, n)152 m, g Eu, 96Mo(?, p)95 m, g Nb, 118Sn(?, p)117 m, g In, 89Y(?, 2 n)87 m, g Y, 106Cd(?, np)104 m, g Ag, and 112Sn(?, np)110 m, g In induced by bremsstrahlungs with end-point energies in the Giant Dipole Resonance (GDR) region. The targets were irradiated at electron ...

NASA Astrophysics Data System (ADS)

116
Real Photon Physics at MAMI
2007-10-01

The scientific program at the Mainz Microtron (MAMI) is based on polarized electron and photon beams from the MAMI A-B-C accelerator complex with energies up to 1500 MeV. In order to deal with the energy increase, the photon tagger system has been extended and refurbished by the Glasgow University Nuclear Physics Group. It is now available for real photon ...

NASA Astrophysics Data System (ADS)

117
Polarization transfer in the ^4He( e,e' p)^3H reaction
2001-04-01

Polarization transfer in quasi-elastic nucleon knockout is sensitive to dynamical relativistic effects and to possible modification of the nucleon electromagnetic form factors in the nuclear medium. Although proper interpretation of the results requires accounting for effects such as final state interactions and meson exchange currents, their effect on polarization transfer is expected to be ...

NASA Astrophysics Data System (ADS)

118
Investigation of 6He yield in 7Li(?, p) reaction with 22 MeV electron beam
2010-03-01

The possibility of producing exotic 6He nuclei in the 7Li(?, p) reaction with 22 MeV electron beam at the MT-25 microtron in the Flerov Laboratory of Nuclear Reactions, Joint Institute for Nuclear Research (FLNR JINR), is studied. The 6He yield from the Li2CO3 target made up 6 � 105 s?1 per 1 ?A of the electron beam current. The obtained result is quite promising, taking ...

NASA Astrophysics Data System (ADS)

119
Independent Yields of Kr and Xe Fragments in the Photofission of {sup 237}Np and {sup 243}Am Odd Nuclei
2005-09-01

Results are presented that were obtained by measuring the independent yields of Kr (A = 89 - 93) and Xe (A = 135 - 142) appearing as fragments in the photofission of {sup 237}Np and {sup 243}Am odd nuclei. The respective experiments were performed in a beam of bremsstrahlung photons from electrons accelerated to an energy of 25 MeV at the microtron of the ...

Energy Citations Database

120
High energy electron irradiation effects on polystyrene films
2009-01-01

The effect of an 8 MeV electron-beam on the structural, optical and dielectric properties of polystyrene films has been investigated respectively by means of Fourier transform infrared (FTIR) spectroscopy, ultraviolet-visible (UV-VIS) spectroscopy and electrical impedance (LCR) analysis over a radiation dose in the range of 50-250 kGy using a Microtron ...

NASA Astrophysics Data System (ADS)

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121
3D field calculation of the GEM prototype magnet and comparison with measurements
1983-10-28

The proposed 4 GeV Electron Microtron (GEM) is designed to fill the existing buildings left vacant by the demise of the Zero Gradient Synchrotron (ZGS) accelerator. One of the six large dipole magnets is shown as well as the first 10 electron orbits. A 3-orbit prototype magnet has been built. The stepped edge of the magnet is to keep the beam exiting ...

Energy Citations Database

122
Status of radiographic study, development, and new applications in the LASL Nondestructive Testing Group
1979-10-01

Topics discussed include replacement of betatron with a racetrack microtron, development of tomography, cineradiography, and flash x ray, and new applications of flash x ray.

Energy Citations Database

123
Free-Electron Laser Driven by the NBS (National Bureau of ...
1988-03-31

... Accession Number : ADA201170. Title : Free-Electron Laser Driven by the NBS (National Bureau of Standards) CW Microtron. ...

DTIC Science & Technology

124
Fabrication and excitation of the disk and washer linac structure
1979-01-01

A scaled version of a typical disk loaded structure is compared with a proposed version of the disk and washer strucutre for the CW race track microtron application. (GHT)

Energy Citations Database

125
A 200 SUPERCONDUCTING RACETRACK MICROTRON,
1965-09-01

... current and cancelled), Joint Staff and other US Military (ie, Army, Navy, Air ... sections, a beam current of 100 microamps at unity duty cycle is feasible ...

DTIC Science & Technology

126
[Neutron pollution in roentgen beams from electron accelerators].
1983-11-01

The neutron dose was measured in X-ray beams with a limiting energy of 8 to 45 MeV and in 42 MeV electrons (10 X 10 cm2) from several electron accelerators (betatrons, linear accelerators, microtron). The measurements were taken with activation probes and nuclear films of polycarbonate coated with 0,5 mm Cd. On a 42 MeV betatron, the ...

PubMed

127
Future Plans for the Mainz Real Photon Facility
2003-06-01

In the last year an upgrade of the Mainz electron accelerator MAMI has been started to reach a beam energy of 1.5GeV. Therefore a fourth stage (MAMI C), a harmonic double sided microtron (HDSM) with four normal conducting dipole magnets and two antiparallel linear accelerators is under construction. The A2-Glasgow-Mainz tagger can ...

NASA Astrophysics Data System (ADS)

128
Medium energy nuclear physics research. Progress report, July 1, 1987--September 30, 1988
1988-09-01

The UMass group has concentrated on using electromagnetic probes, particularly the electron in high-energy scattering experiments at the Stanford Liner Accelerator Center (SLAC). Plans are also being made for high energy work at the Continuous Beam Accelerator Facility (CEBAF). The properties of this accelerator should permit a whole ...

Energy Citations Database

129
Medium energy nuclear physics research
1988-09-01

The UMass group has concentrated on using electromagnetic probes, particularly the electron in high-energy scattering experiments at the Stanford Liner Accelerator Center (SLAC). Plans are also being made for high energy work at the Continuous Beam Accelerator Facility (CEBAF). The properties of this accelerator should permit a whole ...

Energy Citations Database

130
Uranium Analysis by Activation with Bremsstrahlung of Microtron.
1980-01-01

Uranium analysis has been investigated by activation with 16 MeV bremsstrahlung from a microtron in samples of compound chemical composition (geological objects). The sensitivity of uranium determination is 1x10 exp -7 g/g in (30-60) min measurements by a...

National Technical Information Service (NTIS)

131
Sposoby instrumental'nogo opredeleniya soderzhaniya urana i toriya s ispol'zovaniem mikrotrona. (Instrumental methods for Uranium and Thorium determination using a microtron).
1990-01-01

Methods for a gamma-ray spectroscopy determination of natural radioactive elements and U and Th instrumental determination using bremstrahlung and photoneutrons generated at a microtron are described. The limit of the detection for U and Th is obtained to...

National Technical Information Service (NTIS)

132
Performance of an RF Beam Monitor on the NBS-Los Alamos Racetrack Microtron.
1985-01-01

A prototype rf beam-position, current, and phase monitor has been used on the 100-keV injector beamline of the racetrack microtron (RTM) where performance was measured with the chopped and bunched beam. This monitor works with both a pulsed beam and a cw ...

National Technical Information Service (NTIS)

133
NIST (National Institute of Standards and Technology) - Los Alamos Racetrack Microtron Status.
1988-01-01

The NIST-Los Alamos Racetrack Microtron (RTM) is designed to deliver a low-emittance electron beam of up to 0.5 mA cw over an energy range of 17 MeV to 185 MeV. Fed by a 5 MeV injector, the RTM contains two 180 degree end magnets that recirculate the beam...

National Technical Information Service (NTIS)

134
Mnogoehlementnyj gamma-aktivatsionnyj analiz medno-molibdenovykh rud i produktov ikh pererabotki na mikrotrone. (Multielemental gamma activation analysis of copper-molybdenum ores and its production of processing using microtron).
1991-01-01

A method of multielemental instrumental gamma activation analysis (IGAA) of copper-molybdenum ores and its production of processing using microtron bremsstrahlung is described. Activities of irradiated samples were measured by means of Ge(Li) and HP Ge-de...

National Technical Information Service (NTIS)

135
Instrumental gamma-Activation Analysis of Products of the Current Chemical Source Production Using the Microtrons.
1982-01-01

An instrumental gamma-activation analysis of products of the current chemical source production was carried out on microtrons (Esub( gamma sub(max))=13.6 MeV) of the Saratov State University and Kiev Institute for Nuclear Research. An anode and cathode ma...

National Technical Information Service (NTIS)

136
INFORMATION ON A 2.5 Mev MICROTRON
1957-09-01

An electron microtron of the a = 3, b = l model has been built and its essential parts are described. Ten orbits have been obtained and the final energy of the particles is 2.5 Mev. The machine is at present without an extractor and therefore only gamma rays are available. The average intensity on the last orbits is some 10/sup -7/ A. (auth)

Energy Citations Database

137
Status of The Indian SRS Indus-2
2009-07-07

Raja Ramanna Centre for Advanced Technology (RRCAT, formerly called Centre for Advanced Technology) is a prime R and D laboratory of Indian Department of Atomic Energy devoted to developing technologies related to accelerators and lasers as well as their applications. RRCAT is home to 2 synchrotron radiation sources (SRS): Indus-1 (a 100 mA, 450 MeV storage ring) and Indus-2 ...

Energy Citations Database

138
Status of The Indian SRS Indus-2
2009-07-01

Raja Ramanna Centre for Advanced Technology (RRCAT, formerly called Centre for Advanced Technology) is a prime R&D laboratory of Indian Department of Atomic Energy devoted to developing technologies related to accelerators and lasers as well as their applications. RRCAT is home to 2 synchrotron radiation sources (SRS): Indus-1 (a 100 mA, 450 MeV storage ring) & Indus-2 ...

NASA Astrophysics Data System (ADS)

139
Pulse Compression of Nd:YAG Laser with Stimulated Brillouin Scattering for Compton Backscattered X-ray Source
2009-07-01

Compton backscattered x-ray source is developed in the energy region of a few hundred keV at Kansai Photon Science Institute of Japan Atomic Energy Agency (KPSI-JAEA). A remarkable feature of the Compton backscattered x-ray source is that the generated x-ray beam is a well-collimated and has a definite polarization property. The Compton backscattered x-ray source at KPSI-JAEA consists of the ...

NASA Astrophysics Data System (ADS)

140
Photon Activation Analysis-An Analytical Application Of High-Energy Electron Accelerators
2009-03-01

Photon activation analysis (PAA) was introduced about contemporarily with the other activation analysis methods (neutron, NAA, and charged particle activation, CPAA). Nonetheless, for different reasons, PAA has been applied less frequently than the other techniques mentioned. The incident photon energy should exceed about 12 MeV (except in some special rare applications) so as to obtain ...

NASA Astrophysics Data System (ADS)

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141
Photon Activation Analysis--An Analytical Application Of High-Energy Electron Accelerators
2009-03-10

Photon activation analysis (PAA) was introduced about contemporarily with the other activation analysis methods (neutron, NAA, and charged particle activation, CPAA). Nonetheless, for different reasons, PAA has been applied less frequently than the other techniques mentioned. The incident photon energy should exceed about 12 MeV (except in some special rare applications) so as to obtain ...

Energy Citations Database

142
Developing an Efficient Read-Out System for the A2 Pair Spectrometer at Mainz
2008-10-01

The scientific program at the Mainz Microton (MAMI) is based on polarized electron and photon beams from the MAMI A-B-C accelerator complex. The scientific program at the Mainz Microtron (MAMI) is based on polarized electron and photon beams from the MAMI A-B-C accelerator complex with energies up to 1.5GeV. In order to deal with the ...

NASA Astrophysics Data System (ADS)

143
The FEL-microtron activity at the C.N.E.N. Frascati Center Progress and perspectives
1982-01-01

Since the conduction of the pioneering experiments concerning the free electron laser (FEL), new and more efficient FEL devices have been proposed, taking into consideration the relation between laser beam characteristics and electron beam sources. Electron beam sources can be divided into two categories, including single pass machines and devices in which the beam is recirculated. The design of a ...

NASA Astrophysics Data System (ADS)

144
Fringe field calculations for the inhomogeneous Twente Eindhoven microtron magnets
1992-05-01

The Twente Eindhoven microtron, a 25 MeV electron source for a 10 ?m free electron laser has inhomogeneous magnetic fields to improve the focusing properties of the microtron. In order to design the shape of the magnets, the fringe field properties like the effective field boundary and the defocusing force in the vertical plane, have been determined. In ...

NASA Astrophysics Data System (ADS)

145
185-MeV injector design for the ANL 4-GeV microtron project
1983-01-01

The injector starts with a 5 MeV preinjector followed by an 18 MeV S-band linac. The 23 MeV electrons are transported and injected into a Racetrack Microtron via a 10/sup 0/ achromatic bend system. Twenty-seven turns are used to boost the energy to 185 MeV. Reverse-field stripes on the 180/sup 0/ end magnets and quadrupole focussing on the return paths maintain a ...

DOE Information Bridge

146
The Cerenkov free-electron laser
1988-11-01

In the Cerenkov free-electron laser experiments, dielectric-loaded quasi-optic resonators were used to couple the electron beam to the electromagnetic field. Three types of electron beam generators were employed: a pulse-transformer-based modulator (which operates in the 50 to 250 KV range), a Marx generator (which operated in the 500 kv to 1.1 MV range), and a circular RF ...

NASA Astrophysics Data System (ADS)

147
Measurement of angular distribution of soft X-ray radiation from thin targets in the tabletop storage ring MIRRORCLE-20SX.
2011-07-16

The only available tabletop electron storage rings are the machines from the MIRRORCLE series. The electrons are accelerated in a microtron and injected into the storage ring. During its circulation, each electron passes through a tiny target many times, emitting a photon beam. Both the spectrum and the angular distribution of the radiation depend on the ...

PubMed

148
FEASIBILITY AND CONCEPTUAL DESIGN OF A C.W. POSITRON SOURCE AT CEBAF
2010-08-31

A feasibility study of a CW positron source for the 12 GeV upgrade at Jefferson Lab (JLAB) is provided. The proposed � 100 nA Continuous Wave (CW) positron source at JLAB has several unique and challenging characteristics: high current incident electron beam at 126 MeV with a high beam power (up to a MW); CW e� beam and CW e+ production. The multiple scattering is a dominant process when ...

Energy Citations Database

149
FEASIBILITY AND CONCEPTUAL DESIGN OF A C.W. POSITRON SOURCE AT CEBAF
2010-08-31

A feasibility study of a CW positron source for the 12 GeV upgrade at Jefferson Lab (JLAB) is provided. The proposed ? 100 nA Continuous Wave (CW) positron source at JLAB has several unique and challenging characteristics: high current incident electron beam at 126 MeV with a high beam power (up to a MW); CW e? beam and CW e+ production. The multiple scattering is a dominant process when ...

DOE Information Bridge

150
Dose rate effect of pulsed electron beam on micronucleus frequency in human peripheral blood lymphocytes.
2010-03-01

The micronucleus assay in human peripheral blood lymphocytes is a sensitive indicator of radiation damage and could serve as a biological dosimeter in evaluating suspected overexposure to ionising radiation. Micronucleus (MN) frequency as a measure of chromosomal damage has also extensively been employed to quantify the effects of radiation dose rate on biological systems. Here we studied the ...

PubMed

151
Direct imaging of explosives.

Any technique that can detect nitrogen concentrations can screen for concealed explosives. However, such a technique would have to be insensitive to metal, both encasing and incidental. If images of the nitrogen concentrations could be captured, then, since form follows function, a robust screening technology could be developed. However these images would have to be sensitive to the surface ...

PubMed

152
Cyclotrons: From Science to Human Health
2011-04-01

Lawrence's invention of the cyclotron, whose 80th anniversary we have just celebrated, not only revolutionized nuclear physics, but proved the starting point for a whole variety of recirculating accelerators, from the smallest microtron to the largest synchrotron, that have had an enormous impact in almost every branch of science and in several areas of ...

NASA Astrophysics Data System (ADS)

153
An electron fixed target experiment to search for a new vector boson A' decaying to e + e -
2011-02-01

We describe an experiment to search for a new vector boson A' with weak coupling ?' ? 6 � 10-8 ? to electrons ( ? = e 2/4 ?) in the mass range 65 MeV < m A' < 550 MeV. New vector bosons with such small couplings arise naturally from a small kinetic mixing of the "dark photon" A' with the photon � one of the very few ways in which new forces can couple to the Standard Model � and have ...

NASA Astrophysics Data System (ADS)

154
Twenty years of physics at MAMI --What did it mean?
2006-06-01

The development over the last twenty years of the physics program and the experimental facilities at the Mainz Microtron MAMI will be reviewed. Ground-breaking contributions have been made to the development of experimental techniques and to our understanding of the structure of nucleons and nuclei.

DOE Information Bridge

155
Three-Dimensional Field Program.
1983-01-01

The high-energy microtrons studied at Argonne National Laboratory (ANL) require complicated magnetic field shapes. A three-dimensional infinite-permeability magnetic field program was written to show that poles and coils can be devised to produce these fi...

National Technical Information Service (NTIS)

156
The RF power system for the chopper/buncher system on the NBS-Los Alamos RTM
1985-10-01

The rf power system and its closed-loop feedback control for the racetrack microtron (RTM) chopper/ buncher system are described. Measurements made on the response of the feedback system to external perturbations are also reported.

Energy Citations Database

157
THE IASA RACETRACK MICROTRON FACILITY: A PROGRESS REPORT

& Applications, P.O. Box 17214, 10024 Athens, Greece H. Herminghaus, MAMI, Mainz, Germany A. Zolfaghari, MIT, attached in a "L" pattern to small ceramic standoffs on a metal frame [5]. Current from the wires (due

E-print Network

158
Rf power system for the chopper/buncher system on the NBS-Los Alamos RTM
1985-01-01

The rf power system and its closed-loop feedback control for the racetrack microtron (RTM) chopper/buncher system are described. Measurements made on the response of the feedback system to external perturbations will also be reported.

DOE Information Bridge

159
Rf Beam-Current, -Phase, and -Position Monitors.
1984-01-01

A prototype rf beam monitor has been tested on the Racetrack Microtron's (RTM) 100 kV injector beam line at the National Bureau of Standards (NBS). This beam monitor is capable of measuring the current, the relative phase, and the position of the beam. Th...

National Technical Information Service (NTIS)

160
Research Opportunities Below 300 nm at the NBS Free-Electron Laser Facility,
1987-01-01

A free-electron laser (FEL) which will be driven by the cw racetrack microtron (RTM), will be operated as an oscillator with the fundamental wavelength variable from approximately 200 nm to 10 micrometers. The presence of harmonics should allow for operat...

National Technical Information Service (NTIS)

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161
Project of high free electron laser using race-track microtron-recuperator.
1993-01-01

The high power electron alaser (FEL) is under construction in the Novosibirst. The goal of this project is to provide the user facility for photochemical researches. 15 refs. (Atomindex citation 25:055675)

National Technical Information Service (NTIS)

162
Meson photoproduction on light Nuclei
2005-05-01

The photoproduction of mesons on light nuclei was studied intensively with the calorimeter TAPS at the tagged photon facility of the Mainzer Microtron MAMI. Threshold enhancements for ? production on light nuclei are summarized. Furthermore, the evidence of ?-mesic 3He is discussed.

NASA Astrophysics Data System (ADS)

163
Erratum: Experimental study of the ?p??p reaction with the Crystal Ball detector at the Mainz Microtron (MAMI-C) [Phys. Rev. C 82, 035208 (2010)
2011-08-01

Here we correct a factor of 2 missed in one of figures and the corresponding sentence in the text. It does not change any conclusions.

NASA Astrophysics Data System (ADS)

164
Calculation of Distribution of Thermal Neutron Flux from the Microtron Converter inside a Graphite Moderator with a Water Reflector.
1977-01-01

The question of the use of a reflector (water) in addition to a graphite moderator for the increase of the thermal neutron flux is considered. The diffusion method with four energy groups is used for the solution of the problem. The distribution of therma...

National Technical Information Service (NTIS)

165
Application of gamma-Activation Analysis to the Investigation of the Earth Ancient Crystalline Rocks.
1984-01-01

Application of bremsstrahlung and photoneutrons from a microtron for multielement activation analysis of samples of the Earth ancient crystallized rocks was investigated. Nearly 30 elements have been determined mostly by the instrumental photon activation...

National Technical Information Service (NTIS)

166
Status report on the normal conducting CW racetrack microtron cascade ''MAMI''
1983-08-01

At present, the first two stages (175 MeV) of the three-stage c.w. microtron cascade MAMI have been completed. The report concentrates on the design of the 2nd stage, which had been completed by the end of 1982 and which, so far, has not yet been described in detail elsewhere. First beam had been obtained by Feb. 1983, best beam transmission obtained so far is in excess of ...

Energy Citations Database

167
Performance of an rf beam monitor on the NBS-Los Alamos racetrack microtron
1985-01-01

A prototype rf beam-position, current, and phase monitor has been used on the 100-keV injector beamline of the racetrack microtron (RTM) where performance was measured with the chopped and bunched beam. This monitor works with both a pulsed beam and a cw beam. The pulsed beam consists of beam pulses with a FWHM of 40 ns. The rf beam monitor was tested with beam currents from ...

DOE Information Bridge

168
Investigation of the chemical composition of meteorites by an activation method using a microtron
1984-01-01

The feasibility of using bremsstrahlung and photoneutrons from a microtron to measure the chemical composition of stony and iron meteorites is demonstrated. Conditions are established for the activation determination of approximately 20 elements in meteorite samples without their destruction. The optimal geometry and mode of irradiation are established; the contribution of ...

NASA Astrophysics Data System (ADS)

169
End magnets for the NBS-Los Alamos racetrack microtron
1985-10-01

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 m/sup 2/ area to within + or - 2 X 10/sup -4/ at 1 T. The magnet meets all performance specifications. Field measurements are underway on the second magnet. In this paper, design and construction ...

Energy Citations Database

170
Observations of Collective Ion Acceleration.

... Descriptors : *Linear accelerators, *Ion accelerators, *Particle accelerator components, *Electron accelerators, *Proton accelerators, Electron beams ...

DTIC Science & Technology

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