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Proceedings ArticleDOI

Analog front-end electronics for beam position measurement on the beam halo measurement

01 Jun 2001-Vol. 2, pp 1378-1380
TL;DR: In this paper, a log-ratio analog front-end electronics based on the Analog Devices 8307 logarithmic amplifier as used on the LEDA accelerator is presented.
Abstract: Enhancements have been made to the log-ratio analog front-end electronics based on the Analog Devices 8307 logarithmic amplifier as used on the LEDA accelerator. The dynamic range of greater than 85 dB, has been extended to nearly the full capability of the AD8307 from the previous design of approximately 65 dB through the addition of a 350 MHz band-pass filter, careful use of ground and power plane placement, signal routing, and power supply bypassing. Additionally, selection of high-isolation RF switches (55dB) has been an integral part of a new calibration technique, which is fully described in another paper submitted to this conference. Provision has also been made for insertion of a first-stage low-noise amplifier for using the circuit under low-signal conditions.

Summary (2 min read)

Introduction

  • Front-end electronics based on the Analog Devices 8307 logarithmic amplifier as used on the LEDA accelerator.
  • The dynamic range of greater than 85 dB, has been extended to nearly the full capability of the AD8307 from the previous design of approximately 65 dB through the addition of a 350 MHz band-pass filter, careful use of ground and power plane placement, signal routing, and power supply bypassing.
  • Provision has also been made for insertion of a first-stage low-noise amplifier for using the circuit under low-signal conditions.

1 BACKGROUND

  • A BPM signal processor based on the AD8307 was previously used by us on the Low Energy Demonstration Accelerator (LEDA), part of the Accelerator Production of Tritium (APT) project at Los Alamos.
  • Experience with that system was reported at the 2000 Beam Instrumentation Workshop [2].
  • Several of the problems encountered with that system have been corrected, as well as new capabilities added, with the resultant system being presented here.
  • Referring to the block diagram in Figure 1, signals from the four electrodes of the beam position monitors are band-pass filtered and input to the AD8307 log amplifier through a transformer balun, which is required because of the differential inputs with an impedance of 1 kΩ shunted by 1.4 pf to common.

3 IMPROVMENTS

  • The improvements to the previous design include: Correction of overlapping digital and analog power and ground planes.
  • Signal line re-routing to eliminate crossing gaps in the planes and/or keeping the planesignal types coplanar.
  • Input filter change from low-pass to band-pass.
  • This resulted in the largest dynamic range gain.
  • Impedance matching all input RF traces and careful attention to shortness of trace length between components and their bypass capacitors.

3.1 Input Filter

  • The authors previous design used a low-pass filter at the RF input.
  • The authors found that most of the debilitating noise they were experiencing could be eliminated by using a bandpass filter custom made by TTE, Inc [3].

3.2 Circuit Layout

  • Attention was given to the routes return currents traveled in order to make sure that those currents did not induce signals in low-signal parts of the circuitry.
  • Because the authors were not absolutely certain about this, they provided jumper pads for tying the analog and digital ground planes together at various points.
  • Additionally, the recommended printed circuit layout for the Analog Devices AD9241 A/D converter was followed.
  • Large co-planar power and ground planes were used to provide low-impedance power and return paths, as well as to increase the capacitive coupling between them for shunting unwanted signals.
  • Care was taken to make sure signal lines were not routed between these planes.

3.3 Dynamic Range improvement

  • Figure 4. shows the improved range of the circuit used on the HALO measurement.
  • The Analog Devices AD8307 Logarithmic amplifier’s superior 92dB dynamic range and 500 MHz bandwidth makes an excellent beam signal detector as compared to other techniques, e.g.. synchronous detection, as long as careful attention is given to following good noise reduction techniques.
  • Since the logarithmic non-conformance of this type of signal processing can introduce deterministic errors of up to +/-0.5 dB, calibration is used to further enhance accuracy [9].
  • The authors experience with the BPM VXI processing electronics modules has shown them to be highly reliable.
  • The few failures the authors have experienced have been due to mis-soldered components, mother-board problems, and in two cases, defective VXI crates.

6 REFERENCES

  • [1] D. Barr, J. D. Gilpatrick, R. Shurter, “Upgrade to Initial BPM Electronics Module and Beamline Components for Calibration of the LEDA Beam Position Measurements,” published at this conference. [2].
  • Analog Devices, Inc., www.analogdevices.com AD9241 specification [5].
  • T. Van Doren, “Circuit Board Layout to Reduce Electro-magnetic Emission and Susceptibility, National Technological University live video course #MC00032802, March 28, 2000. [7].
  • D. Barr, J. D. Gilpatrick, R. Shurter, “Upgrade to Initial BPM Electronics Module and Beamline Components for Calibration of the LEDA Beam Position Measurements,” published at this conference.

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ANALOG FRONT-END ELECTRONICS FOR BEAM POSITION
MEASUREMENT ON THE BEAM HALO MEASUREMENT
*
R. B. Shurter, T. Cote, J. D. Gilpatrick, Los Alamos National Laboratory, Los Alamos, NM 87545,
USA
Abstract
Enhancements have been made to the log-ratio analog
front-end electronics based on the Analog Devices 8307
logarithmic amplifier as used on the LEDA accelerator.
The dynamic range of greater than 85 dB, has been
extended to nearly the full capability of the AD8307 from
the previous design of approximately 65 dB through the
addition of a 350 MHz band-pass filter, careful use of
ground and power plane placement, signal routing, and
power supply bypassing. Additionally, selection of high-
isolation RF switches (55dB) has been an integral part of
a new calibration technique, which is fully described in
another paper submitted to this conference [1]. Provision
has also been made for insertion of a first-stage low-noise
amplifier for using the circuit under low-signal
conditions.
1 BACKGROUND
A BPM signal processor based on the AD8307 was
previously used by us on the Low Energy Demonstration
Accelerator (LEDA), part of the Accelerator Production
of Tritium (APT) project at Los Alamos. Experience with
that system was reported at the 2000 Beam
Instrumentation Workshop [2]. Several of the problems
encountered with that system have been corrected, as well
as new capabilities added, with the resultant system being
presented here. Currently the LEDA accelerator is
configured to conduct a beam halo experiment.
Beam diagnostics include fifteen beam position
monitors in the 52-quadrupole magnet focusing-
defocusing (FODO) lattice, along with wire scanners,
beam-loss monitors and current monitors [7]. The nature
of the experiment places a requirement for additional
dynamic range on the BPM electronics. Beam de-
bunching, which occurs as the beam is transported
through the lattice, reduces the signal power by about 40
dB from the last BPM with respect to the first.
2 CIRCUIT DESCRIPTION
Referring to the block diagram in Figure 1, signals from
the four electrodes of the beam position monitors are
band-pass filtered and input to the AD8307 log amplifier
through a transformer balun, which is required because of
the differential inputs with an impedance of 1 k shunted
by 1.4 pf to common. The circuit layout can accommodate
a Minicircuits Lab fixed attenuator (PAT-X) and/or a
Cougar Components AC566 pre-amplifier [8] installed
between the filter and the transformer. This attenuator-
amplifier combination allows us to adjust the signal high-
end for the log amp’s maximum input of approximately
+17 dBm, thereby obtaining the greatest signal to noise
ratio and dynamic range (approximately 92 dB is
specified for the AD8307.)
The log amp output is then amplified, scaled and offset-
adjusted by an AD8041 amplifier stage for a 0 to
approximately 4.6 V range. The signal is then low-pass
___________________________________________
* Supported by US DOE, Office of Defense Programs, and the Office of
Nuclear Energy, Science and Technology.
Digital Processing
Circuitry
AD9241 A/D
Converter
Xformer/Balun
AD
8307
Log
Amp
AD8041
Op Amp
2MHz Low Pass
Filter
350 MHz
Bandpass Filter
AC566
Preamp
Selectable
Attenuator
Solid-state
Switch
Σ
Summing
Junction
BPM
Signal Sources
T
B
R
L
Calibrator
'Top'
Channel
(of Four Identical
Channels)
From
Bottom, Right and
Left Channel Analog
Circuitry
D/A
AD8041
Op Amp
B
R
L
T
To Bottom, Right and Left Channels
Front Panel
Intensity Monitor
Output
Front Panel
Channel Monitor
Outputs
Four-Way
Splitter
Σ
Figure 1: BPM Signal Processing Block Diagram.
0-7803-7191-7/01/$10.00 ©2001 IEEE. 1378
Proceedings of the 2001 Particle Accelerator Conference, Chicago

filtered to a 200-KHz bandwidth and digitized by an
AD9241 14-bit analog to digital converter. Only 12 bits of
the A/D is used, giving a resolution of 5V/4096 = 1.2
mV/count. The result of one channel’s raw (calibrator
errors not corrected) calibration response, as seen on a
LabVIEW PC display, is given in figure 2.
4000
0
500
1000
1500
2000
2500
3000
3500
90
0
5
10
15
20
25
30
35
40
45
50
55
60
65
70
75
80
85
Counts
Relative input power (dB)
Figure 2. Calibration display
3 IMPROVMENTS
The improvements to the previous design include:
Correction of overlapping digital and analog power
and ground planes. Signal line re-routing to eliminate
crossing gaps in the planes and/or keeping the plane-
signal types coplanar.
Addition of an RF shield around the RF components.
Input filter change from low-pass to band-pass. This
resulted in the largest dynamic range gain.
Impedance matching all input RF traces and careful
attention to shortness of trace length between
components and their bypass capacitors.
Elimination of one baseband gain stage.
3.1 Input Filter
Our previous design used a low-pass filter at the RF
input. We found that most of the debilitating noise we
were experiencing could be eliminated by using a band-
pass filter custom made by TTE, Inc [3].
3.2 Circuit Layout
Attention was given to the routes return currents
traveled in order to make sure that those currents did not
induce signals in low-signal parts of the circuitry. Because
we were not absolutely certain about this, we provided
jumper pads for tying the analog and digital ground planes
together at various points. Additionally, the recommended
printed circuit layout for the Analog Devices AD9241
A/D converter was followed. The AD9241 product
specifications define how the analog and digital ground
planes are separated under and around the part [4][5].
Large co-planar power and ground planes were used to
provide low-impedance power and return paths, as well as
to increase the capacitive coupling between them for
shunting unwanted signals. Care was taken to make sure
signal lines were not routed between these planes.
Signal traces were never allowed to cross gaps in
ground planes, as this would create current loops, thereby
inducing currents in nearby components [6].
3.3 Dynamic Range improvement
Figure 3. shows a graph of the dynamic range of the
AFE circuit as previously used on the LEDA accelerator.
Figure 4. shows the improved range of the circuit used on
the HALO measurement.
-5.0
-4.0
-3.0
-2.0
-1.0
0.0
1.0
0204060
Relative Power (dB)
Figure 3. LEDA BPM AFE Linearity
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
2.0
-100-80-60-40-200
Power (dBm)
Figure 4. HALO BPM AFE Linearity
4 CONCLUSION
The Analog Devices AD8307 Logarithmic amplifier’s
superior 92dB dynamic range and 500 MHz bandwidth
makes an excellent beam signal detector as compared to
other techniques, e.g.. synchronous detection, as long as
careful attention is given to following good noise
reduction techniques.
Since the logarithmic non-conformance of this type of
signal processing can introduce deterministic errors of up
to +/-0.5 dB, calibration is used to further enhance
accuracy [9].
Our experience with the BPM VXI processing
electronics modules has shown them to be highly reliable.
The few failures we have experienced have been due to
mis-soldered components, mother-board problems, and in
two cases, defective VXI crates.
1379
Proceedings of the 2001 Particle Accelerator Conference, Chicago

Figure 5. HALO BPM AFE Circuit Board
Figure 6. HALO BPM VXI Module withAFE on
Motherboard
5 ACKNOWLEDGMENT
The authors wish to thank John Power for his initial
work on this measurement design, as well as his
continued help.
6 REFERENCES
[1] D. Barr, J. D. Gilpatrick, R. Shurter, “Upgrade to
Initial BPM Electronics Module and Beamline
Components for Calibration of the LEDA Beam
Position Measurements,” published at this conference.
[2] R.B. Shurter, J. D. Gilpatrick, J. Power, “BPM Analog
Front-End Electronics Based on the AD8307 Log
Amplifier,” 9
th
Beam Instrumentation Workshop,
Cambridge, MA, May 8-11, 2000.
[3] TTE, Inc., http://www.tte.com/
. Filter specifications-
Model number: K4034-350M-20M-50-484, 3-pole
chebyshev, F
0
: 350 MHz, Insertion loss @ F
0
: 5dB
max., Rejection (typical): -40 dB @ 270MHz and
360MHz, Impedance: 50 ohms.
[4] Analog Devices, Inc., www.analogdevices.com
AD9241 specification
[5] Analog Devices, Inc., AN-404 Application note.
[6] T. Van Doren, Circuit Board Layout to Reduce
Electro-magnetic Emission and Susceptibility,
National Technological University live video course
#MC00032802, March 28, 2000.
[7] J. D. Gilpatrick, et al., "Experience with the Low
Energy Demonstration Accelerator (LEDA) Halo
Experiment Beam Instrumentation,” published at this
conference.
[8] Cougar Components, Inc.,
http://www.cougarcorp.com/
[9] D. Barr, J. D. Gilpatrick, R. Shurter, “Upgrade to
Initial BPM Electronics Module and Beamline
Components for Calibration of the LEDA Beam
Position Measurements,” published at this conference.
1380
Proceedings of the 2001 Particle Accelerator Conference, Chicago
Citations
More filters
Proceedings ArticleDOI
01 Jan 2001
TL;DR: A 52 quadrupole-magnet FODO lattice has been assembled and operated at the Los Alamos National Laboratory as mentioned in this paper, which provides a platform to measure the resulting beam halo as the first four magnets of the lattice produce various mismatch conditions.
Abstract: A 52 quadrupole-magnet FODO lattice has been assembled and operated at the Los Alamos National Laboratory. The purpose of this lattice is to provide a platform to measure the resulting beam halo as the first four magnets of the lattice produce various mismatch conditions. These data are then compared with particle simulations so that halo formation mechanisms may be better understood. The lattice is appended to the LEDA 6.7-MeV radiofrequency quadrupole (RFQ) and is followed by a short high-energy beam transport (HEBT) that safely dumps the beam into a 670-kW beam stop. Beam diagnostic instruments are interspersed within the lattice and HEBT. The primary instruments for measuring the beam halo are nine interceptive devices that acquire the beam's horizontal and vertical projected particle density distributions out to an approximate 10/sup 5/:1 dynamic range. These distributions are acquired using both traditional wire scanners and water-cooled graphite scraping devices. The lattice and HEBT instrumentation set also includes position, bunched-beam current, pulsed current, and beam loss measurements. This paper briefly describes and details the operation of each instrument compares measured data from the different types of instruments, and refers to other detailed papers.

17 citations


Cites background or methods from "Analog front-end electronics for be..."

  • ...4 shows the quality of the position and bunched beam current measurements presently installed in the 10 latticeBPM locations....

    [...]

  • ...Bunched beam current measurements are acquired at each BPM location....

    [...]

  • ...Even though neighboring bunches overlap, there is sufficient 350-MHz current modulation to use devices such as BPMs to detect beam position, current, and possibly other beam parameters....

    [...]

  • ...The beam position measurement consists of a traditional micro-stripline type of beam position monitor (BPM), a cable plant, a 200-kHz log-ratio electronics processor [10], and an interface from LabVIEW to EPICS that provides the linearization and calibration algorithms....

    [...]

  • ...An error assessment was performed of all known absolute errors, such as mechanical displacement errors of the BPM, cable mismatch errors, errors shown in Fig....

    [...]

Proceedings ArticleDOI
01 Jun 2001
TL;DR: In this paper, the authors present the calibration algorithms and switching system interactions for the Low-Energy Demonstration Accelerator (LEDA) beam-halo formation at the Los Alamos National Laboratory.
Abstract: The Low-Energy Demonstration Accelerator (LEDA), designed and built at the Los Alamos National Laboratory, is part of the Accelerator Production of Tritium (APT) program and provides a platform for measuring high-power proton beam-halo formation. Beam Position Monitors (BPMs) are placed along the FODO lattice and the HEBT. The BPM systems employing log-ratio processor electronics have recently been upgraded for all fifteen BPMs along the accelerator. Two types of calibration are now used. The first corrects for errors within the electronics module and the log-amp transfer function non-conformity. The second is a single-point routine used to correct for cable plant attenuation differences. This paper also covers the new switching systems used for various system calibration modes as well as various results from LEDA beam runs. New switching algorithms were implemented in order to remove sensitive electronic switches from within the beam tunnel radiation environment. Attention will be paid to the calibration algorithms and switching system interactions, and how well they work in practice.

6 citations


Cites background from "Analog front-end electronics for be..."

  • ...For details of the AFE and AD8307 log-amplifier see [3,4]....

    [...]

Journal ArticleDOI
TL;DR: In this paper, a beam position monitor (BPM) system is developed in order to monitor the beam position and meet all the requirements of the future ESS-Bilbao Linac.
Abstract: A versatile and configurable system has been developed in order to monitorize the beam position and to meet all the requirements of the future ESS-Bilbao Linac. At the same time the design has been conceived to be open and configurable so that it could eventually be used in different kinds of accelerators, independent of the charged particle, with minimal change. The design of the Beam Position Monitors (BPMs) system includes a test bench both for button-type pick-ups (PU) and striplines (SL), the electronic units and the control system. The electronic units consist of two main parts. The first part is an Analog Front-End (AFE) unit where the RF signals are filtered, conditioned and converted to base-band. The second part is a Digital Front-End (DFE) unit which is based on an FPGA board where the base-band signals are sampled in order to calculate the beam position, the amplitude and the phase. To manage the system a Multipurpose Controller (MC) developed at ESSB has been used. It includes the FPGA management, the EPICS integration and Archiver Instances. A description of the system and a comparison between the performance of both PU and SL BPM designs measured with this electronics system are fully described and discussed.

5 citations


Cites methods from "Analog front-end electronics for be..."

  • ...[10] a different logarithmic amplifier board has also been selected because its dynamic range and bandwidth make an excellent beam signal detector as compared to other techniques....

    [...]

Proceedings ArticleDOI
12 May 2003
TL;DR: In this article, the beam position instrumentation for both of these beam lines uses a microstripline beam position monitor (BPM) with a 50-mm or 75-mm radius.
Abstract: The Los Alamos Neutron Science Center (LANSCE) is installing two beam lines to both improve operational tuning and provide new capabilities. The Isotope Production Facility (IFF) will provide isotopes for medical purposes by using the H/sup +/ beam spur at 100 MeV and the Switchyard Kicker Upgrade (SYK) will allow the LANSCE 800-MeV H/sup -/ beam to be rapidly switched between various beam lines within the facility. The beam position instrumentation for both of these beam lines uses a microstripline beam position monitor (BPM) with a 50-mm or 75-mm radius. The cable plant is unique in that it unambiguously verifies the operation of the complete position instrumentation. The processing electronics use a log ratio technique with error correction such that it has a dynamic range of -12 dBm to -85 dBm with errors less than 0.15 dB within this range. This paper will describe the primary components of these measurement systems and provide initial data of their operation.

4 citations

Dissertation
06 May 2014
TL;DR: In this paper, a modelo generico that representa the respuesta dinamica de la cavidad bajo the influencia del haz de particulas is presented.
Abstract: En esta tesis se describen diversas soluciones analogicas y digitales para realizar sistemas de control LLRF (Radio Frecuencia de Bajo Nivel) para cavidades resonantes de radiofrecuencia de aceleradores de particulas. Para analizar dichas cavidades, se desarrolla un modelo generico que representa la respuesta dinamica de la cavidad bajo la influencia del haz de particulas. Despues, se usa este modelo para desarrollar y analizar un sistema analogico de LLRF para el booster' del sincrotron ALBA, asi como un sistema LLRF digital para el linac de la futura Fuente Europea de Protones y Neutrones de Bilbao (ESS-Bilbao). A continuacion, se presentan los detalles del diseno e implementacion de los dos sistemas LLRF aludidos, asi como los resultados experimentales obtenidos en distintas cavidades de radiofrecuencia, asi verificando la validez de los dos disenos propuestos. Tambien, se presenta el diseno basico de la electronica de RF de un sistema de Monitorizacion de la Posicion del Haz de Particulas (BPM) y los resultados preliminares obtenidos con un haz simulado en un banco de ensayos desarrollado al efecto. Hay dos consideraciones importantes a la hora de desarrollar un modelo electrico de cavidades radiofrecuencia util para analizar el sistema o disenar un lazo de LLRF: la respuesta transitoria y los desajustes de impedancia. Sin embargo, en la literatura raramente se consideran estas cuestiones de manera conjunta, y una suele prevalecer sobre la otra, dependiendo de si la cavidad de radiofrecuencia se mira desde una perspectiva de alta potencia o de LLRF. En esta tesis, en primer lugar, se desarrolla un modelo para representar los aspectos mas importantes de la cavidad, incluyendo desajustes de impedancia, potencia reflejada y la respuesta transitoria, por ejemplo en el arranque del sistema o en los instantes de llegada del haz de particulas que carga la cavidad. Como un caso especial, se aplica el modelo a las cavidades RF del anillo de almacenamiento (storage ring) de ALBA, estudiando asi los efectos de carga del haz (beam loading), el arranque del sistema y los retardos en la respuesta de los lazos de regulacion. Para simular estos lazos, se emplea una tecnica matematica para hacer corresponder la frecuencia resonante de la cavidad a banda base, obteniendo de esta manera un modelo equivalente en banda base de la cavidad, con una respuesta aproximadamente igual al modelo convencional RF, pero con una velocidad de simulacion mucho mayor. A continuacion, se presenta el diseno y la implementacion del sistema de LLRF analogico del booster' de ALBA, basado en lazos de realimentacion de las senales IQ del sistema. Se miden los parametros importantes del LLRF operando la cavidad tanto a baja como a alta potencia de RF, verificando asi el diseno propuesto. Finalmente, se presenta el diseno, implementacion y diversos resultados experimentales del sistema LLRF digital pulsado que hemos desarrollado para el Cuadrupolo de Radio Frecuencia (RFQ) del Rutherford Appleton Laboratory - Front End Test Stand (Oxfordshire, Inglaterra) y para el futuro linac de ESS-Bilbao. En lugar de emplear un front-end' analogico estandar que convierta las senales medidas en la cavidad a una Frecuencia Intermedia (IF) para a continuacion submuestrear este senal, en este diseno usamos un demodulador IQ analogico, que transforma directamente las senales RF medidas en sus componentes En-fase (I) y Cuadratura (Q) en banda base. La ventaja principal de usar este metodo es eliminar la necesidad para un sistema preciso y complejo de sincronizacion y timing', lo cual da lugar a un sistema LLRF simple y versatil que puede servir para un rango grande de frecuencias y virtualmente para cualquier aplicacion LLRF, sean pulsadas, en rampa o de onda continua (CW). Los errores asociados al uso de demoduladores de IQ analogicos han sido identificados y corregidos mediante algoritmos implementados en la FPGA y por medio del ajuste apropiado de los parametros del lazo de control. Ademas, se ha desarrollado un modelo equivalente en banda base del RFQ en MATLAB-Simulink para estudiar su respuesta transitoria en condiciones de carga del haz y en presencia de errores de fase y retardos. Los resultados experimentales obtenidos con una cavidad de prueba y un modelo en cobre del RFQ verifican que en lazo cerrado pueden obtenerse campos acelerantes con niveles de estabilidad de amplitud y fase superiores al 1 por ciento y un grado respectivamente, ademas de un margen de fase mayor de +/- 50 grados que confiere robustez al sistema, conservando al mismo tiempo la linealidad y el ancho de banda de los lazos de regulacion, y cumpliendo por tanto sobradamente las especificaciones requeridas para el acelerador.

4 citations

References
More filters
Proceedings ArticleDOI
01 Jan 2001
TL;DR: A 52 quadrupole-magnet FODO lattice has been assembled and operated at the Los Alamos National Laboratory as mentioned in this paper, which provides a platform to measure the resulting beam halo as the first four magnets of the lattice produce various mismatch conditions.
Abstract: A 52 quadrupole-magnet FODO lattice has been assembled and operated at the Los Alamos National Laboratory. The purpose of this lattice is to provide a platform to measure the resulting beam halo as the first four magnets of the lattice produce various mismatch conditions. These data are then compared with particle simulations so that halo formation mechanisms may be better understood. The lattice is appended to the LEDA 6.7-MeV radiofrequency quadrupole (RFQ) and is followed by a short high-energy beam transport (HEBT) that safely dumps the beam into a 670-kW beam stop. Beam diagnostic instruments are interspersed within the lattice and HEBT. The primary instruments for measuring the beam halo are nine interceptive devices that acquire the beam's horizontal and vertical projected particle density distributions out to an approximate 10/sup 5/:1 dynamic range. These distributions are acquired using both traditional wire scanners and water-cooled graphite scraping devices. The lattice and HEBT instrumentation set also includes position, bunched-beam current, pulsed current, and beam loss measurements. This paper briefly describes and details the operation of each instrument compares measured data from the different types of instruments, and refers to other detailed papers.

17 citations


"Analog front-end electronics for be..." refers methods in this paper

  • ...Beam diagnostics include fifteen beam position monitors in the 52-quadrupole magnet focusingdefocusing (FODO) lattice, along with wire scanners, beam-loss monitors and current monitors [ 7 ]....

    [...]

Proceedings ArticleDOI
27 Mar 2001
TL;DR: In this paper, the Analog Devices AD8307 logarithmic amplifier was used for beam position monitor (BPM) signal processing at the Low Energy Demonstration Accelerator (LEDA), part of the Accelerator Production of Tritium (APT) project.
Abstract: Beam position monitor (BPM) signal-processing electronics utilizing the Analog Devices AD8307 logarithmic amplifier has been developed for the Low Energy Demonstration Accelerator (LEDA), part of the Accelerator Production of Tritium (APT) project at Los Alamos. The low-pass filtered 350 MHz fundamental signal from each of the four microstrip electrodes in a BPM is “detected” by an AD8307 log amp, amplified and scaled to accommodate the 0 to +5 V input of an analog-to-digital (A/D) converter. The resultant four digitized signals represent a linear power relationship to the electrode signals, which are in turn related to beam current and position. As the AD8307 has a potential dynamic range of approximately 92 dB, much attention must be given to noise reduction, sources of which can be digital signals on the same board, power supplies, inter-channel coupling, stray RF and others. This paper will describe the operational experience of this particular analog front-end electronic circuit design.

9 citations

Proceedings ArticleDOI
01 Jun 2001
TL;DR: In this paper, the authors present the calibration algorithms and switching system interactions for the Low-Energy Demonstration Accelerator (LEDA) beam-halo formation at the Los Alamos National Laboratory.
Abstract: The Low-Energy Demonstration Accelerator (LEDA), designed and built at the Los Alamos National Laboratory, is part of the Accelerator Production of Tritium (APT) program and provides a platform for measuring high-power proton beam-halo formation. Beam Position Monitors (BPMs) are placed along the FODO lattice and the HEBT. The BPM systems employing log-ratio processor electronics have recently been upgraded for all fifteen BPMs along the accelerator. Two types of calibration are now used. The first corrects for errors within the electronics module and the log-amp transfer function non-conformity. The second is a single-point routine used to correct for cable plant attenuation differences. This paper also covers the new switching systems used for various system calibration modes as well as various results from LEDA beam runs. New switching algorithms were implemented in order to remove sensitive electronic switches from within the beam tunnel radiation environment. Attention will be paid to the calibration algorithms and switching system interactions, and how well they work in practice.

6 citations