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1
Measurement of the Intensity of the Beam in the Abort Gap at the Tevatron Utilizing Synchrotron Light.
2005-01-01

This paper discusses the implementation of abort gap beam intensity monitoring at the Tevatron collider at Fermilab. There are two somewhat independent monitors which measure the intensity of the synchrotron light emitted by particles in the abort gaps. O...

National Technical Information Service (NTIS)

2
Expected Performance of the LHC Synchrotron-Light Telescope (BSRT) and Abort-Gap Monitor (BSRA)
2010-06-07

This Report presents calculations of the synchrotron light from proton and lead-ion beams in the LHC at all energies from 0.45 to 7 TeV. It computes the emission from three sources: the uniform-field region of the D3 dipole, the dipole's edge field, and the short undulator just upstream. Light emitted at or near visible wavelengths is assessed for making optical measurements of transverse ...

Energy Citations Database

3
Development of an Abort Gap Monitor for High-Energy Proton Rings.
2004-01-01

The fill pattern in proton synchrotrons usually features an empty gap, longer than the abort kicker raise time, for machine protection. This gap is referred to as the 'abort gap' and any particles, which may accumulate in it due to injection errors and di...

National Technical Information Service (NTIS)

4
Measurement of the intensity of the beam in the abort gap at the Tevatron utilizing synchrotron light
2005-05-01

This paper discusses the implementation of abort gap beam intensity monitoring at the Tevatron collider at Fermilab. There are two somewhat independent monitors which measure the intensity of the synchrotron light emitted by particles in the abort gaps. One system uses a ...

Energy Citations Database

5
Development of an Abort Gap Monitor for High-Energy Proton Rings
2004-11-01

The fill pattern in proton synchrotrons usually features an empty gap, longer than the abort kicker raise time, for machine protection. This gap is referred to as the ``abort gap,'' and any particles, which may accumulate in it due to injection errors and diffusion between RF buckets, would be lost inside the ring, rather than in the beam dump, during the ...

NASA Astrophysics Data System (ADS)

6
Development of an abort gap monitor for the large hadroncollider
2004-07-01

The Large Hadron Collider (LHC), presently under construction at CERN, requires monitoring the parasitic charge in the 3.3ms long gap in the machine fill structure. This gap, referred to as the abort gap, corresponds to the raise time of the abort kickers magnets. Any circulating particle present in the abort ...

DOE Information Bridge

7
Development of an abort gap monitor for high-energy proton rings
2004-05-03

The fill pattern in proton synchrotrons usually features an empty gap, longer than the abort kicker raise time, for machine protection. This gap is referred to as the ''abort gap'' and any particles, which may accumulate in it due to injection errors and diffusion between RF buckets, would be lost inside the ring, rather ...

DOE Information Bridge

8
Development of an Abort Gap Monitor for High-Energy Proton Rings
2004-11-10

The fill pattern in proton synchrotrons usually features an empty gap, longer than the abort kicker raise time, for machine protection. This gap is referred to as the 'abort gap', and any particles, which may accumulate in it due to injection errors and diffusion between RF buckets, would be lost inside the ring, rather than in the beam ...

Energy Citations Database

9
Proton synchrotron radiation at Fermilab
2006-05-01

While protons are not generally associated with synchrotron radiation, they do emit visible light at high enough energies. This paper presents an overview of the use of synchrotron radiation in the Tevatron to measure transverse emittances and to monitor the amount of beam in the abort gap. The latter is necessary to ensure a clean ...

DOE Information Bridge

10
Proton Synchrotron Radiation at Fermilab
2006-11-20

While protons are not generally associated with synchrotron radiation, they do emit visible light at high enough energies. This paper presents an overview of the use of synchrotron radiation in the Tevatron to measure transverse emittances and to monitor the amount of beam in the abort gap. The latter is necessary to ensure a clean ...

Energy Citations Database

11
Proton Synchrotron Radiation at Fermilab
2006-11-01

While protons are not generally associated with synchrotron radiation, they do emit visible light at high enough energies. This paper presents an overview of the use of synchrotron radiation in the Tevatron to measure transverse emittances and to monitor the amount of beam in the abort gap. The latter is necessary to ensure a clean ...

NASA Astrophysics Data System (ADS)

12
Synchrotron radiation based beam diagnostics at the Fermilab Tevatron
2011-09-01

Synchrotron radiation has been used for many years as a beam diagnostic at electron accelerators. It is not normally associated with proton accelerators as the intensity of the radiation is too weak to make detection practical. However, if one utilizes the radiation originating near the edge of a bending magnet, or from a short magnet, the rapidly changing magnetic field serves to enhance the ...

NASA Astrophysics Data System (ADS)

13
Monitoring the stability of the CMS electromagnetic calorimeter
2011-04-01

The lead tungstate electromagnetic calorimeter of the CMS experiment has been proved to achieve an excellent energy resolution during the commissioning phase of the detector. The uniformity of the relative response of individual channels and the energy scale for electrons and photons are constrained by the several calibration procedures. The stability of the detector in time is constantly ...

NASA Astrophysics Data System (ADS)

14
International Space Station National Laboratory - NASA

BIOTECHNOLOGY SPACE RESEARCH ALLIANCE (BSRA). Michael Wiskerchen ... SPACE TELESCIENCE & BIOTECHNOLOGY RESEARCH. EDUCATION ...

NASA Website

15
LHC-PROJECT-REPORT-1160 05Sep2008

. Kramer EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH European Laboratory for Particle Physics ABORT GAP densities within the 3 s of the dump kicker rising edge. High beam population in this so-called 'abort gap which will be counter-acted by an active abort gap cleaning ...

E-print Network

16
Test of the LHC DIAMOND Beam Loss Monitors

Chemical Vapour Deposition(CVD) diamond detectors were installed in the collimation area of the CERN LHC to study their feasibility as Fast Beam Loss Monitors in a high-�radiation environment. Four detectors were configured with fast, radiation-�hard pre-amplifiers with a bandwidth of 2GHz. The readout was via an oscilloscope with a bandwidth of 1GHz and a sampling rate of ...

E-print Network

17
ABORT GAP CLEANING IN RHIC.
2002-06-03

During the RHIC Au-run in 2001 the 200 MHz storage cavity system was used for the first time. The rebucketing procedure caused significant beam debunching in addition to amplifying debunching due to other mechanisms. At the end of a four hour store, debunched beam could account for approximately 30%-40% of the total beam intensity. Some of it will be in the abort ...

DOE Information Bridge

18
Abort Gap Cleaning in RHIC.
2002-01-01

During the RHIC Au-run in 2001 the 200 MHz storage cavity system was used for the first time. The rebucketing procedure caused significant beam debunching in addition to amplifying debunching due to other mechanisms. At the end of a four hour store, debun...

National Technical Information Service (NTIS)

19
Development of a longitudinal density monitor for storage rings
2003-05-28

We report on development of a new storage ring operations tool for measurement of longitudinal beam density profile. The technique mixes synchrotron light with light from a mode locked solid-state laser oscillator in a non-linear crystal and detects the up-converted radiation with a photo-multiplier. The laser is phase locked to the storage ring RF system. The laser choices available for ...

Energy Citations Database

20
NUCLEAR POWER FOR SHIP PROPULSION
1960-10-01

A short appraisal is given of the present position regarding the possible application of nuclear power to merchant-ship propulsion. The type of ship under consideration for the first application of nuclear power is the large oil tanker, and types of slightly enriched uranium reactor wich are being studied are reviewed and economic factors are discussed. More detailed consideration is ...

Energy Citations Database

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First Page Previous Page 1 2 Next Page Last Page
 
21
Cavitation Induced Hull Pressures Measured in a Water Tunnel for Comparison with Ship Trials on a Single Screw Cargo Carrier.
1981-01-01

The reports produced as a result of the program 'Propeller Hull Interactive Vibration Excitation', (PHIVE), which was carried out jointly by NMI and BSRA from 1977 to 1980, included comparisons between experiments in the water tunnel and full-scale trials...

National Technical Information Service (NTIS)

22
The special applications of Tevatron electron lens
2003-08-11

Besides the Tevatron Electron Lens (TEL) runs as a R and D project for Tevatron Beam-Beam Compensation, it is used daily as a Beam Abort Gap Cleaner for collider operations. It can also be served as beam exciter for beam dynamics measurements and slow proton or antiproton bunch remover. This report describes all these applications and observations.

Energy Citations Database

23
Electron lenses for particle collimation in LHC
2007-12-01

Electron Lenses built and installed in Tevatron have proven themselves as safe and very reliable instruments which can be effectively used in hadron collider operation for a number of applications, including compensation of beam-beam effects [1], DC beam removal from abort gaps [2], as a diagnostic tool. In this presentation we - following original ...

DOE Information Bridge

24
CONTINUOUS ABORT GAP CLEANING AT RHIC.
2004-07-05

Since the RHIC Au-Au run in the year 2001 the 200 MHz cavity system was used at storage and a 28 MHz system during injection and acceleration. The rebucketing procedure potentially causes a higher debunching rate of heavy ion beams in addition to amplifying debunching due to other mechanisms. At the end of a four hour store, debunched beam can easily account for more than 50% of the total beam ...

DOE Information Bridge

25
Luminosity Increase at the Incoherent Beam-Beam Limit with Six Superbunches in RHIC
2003-12-01

By colliding bunches of greater length under a larger angle, the tune spread caused by the beam-beam interaction can be reduced. Assuming a constant limit for the beam-beam tune shift, the bunch intensity can then be raised. In this way, a luminosity increase is possible. We review this strategy for proton beams in RHIC, with two collisions and consider six long bunches. Barrier cavities are used ...

NASA Astrophysics Data System (ADS)

26
LUMINOSITY INCREASE AT THE INCOHERENT BEAM BEAM LIMIT WITH SIX SUPERBUNCHES IN RHIC.
2003-05-19

By colliding bunches of greater length under a larger angle, the tune spread caused by the beam-beam interaction can be reduced. Assuming a constant limit for the beam-beam tune shift, the bunch intensity can then be raised. In this way, a luminosity increase is possible. We review this strategy for proton beams in RHIC, with two collisions and consider six long bunches. Barrier cavities are used ...

Energy Citations Database

27
LHC particle collimation with hollow electron beams
2008-06-01

Electron lenses built and installed in the Tevatron have proven themselves as safe and very reliable instruments which can be effectively used in hadron collider operation for a number of applications, including compensation of beam-beam effects [1], a DC beam removal from abort gaps [2], and as a versatile diagnostic tool. In this article, we--following ...

DOE Information Bridge

28
Generation and diagnostics of uncaptured beam in the Fermilab Tevatron and its control by electron lenses
2008-05-01

In the collider run II, the Tevatron operates with 36 high intensity bunches of 980 GeV protons and antiprotons. Particles not captured by the Tevatron rf system pose a threat since they can quench the superconducting magnets during acceleration or at beam abort. We describe the main mechanisms for the origination of this uncaptured beam, and present measurements of its main parameters by means of ...

NASA Astrophysics Data System (ADS)

29
Transient beam loading and rf power distribution in the SSC (Superconducting Super Collider)
1986-01-01

Transient beam loading will occur in the SSC at injection as the fifteen individual batches from the High Energy Booster are loaded box-car fashion into the main rings. Periodic transient beam loading will be present also at injection due to the gaps between the successive batches as well as the gap that remains to be filled. Even after the rings have been ...

DOE Information Bridge

30
KEKB beam collision stability at the picosecond timing and micron position resolution as observed with the Belle detector
2010-03-01

Using the Belle detector we study the characteristics of beam collisions at the KEKB 3.5 GeV e+ on 8 GeV e- asymmetric energy collider. We investigate the collision timing tIP and its z-coordinate along the beam axis zIP as a function of the position of the colliding bunch in a beam train. The various tIP and zIP behaviors observed by Belle are attributed to beam loading effects in the radio ...

NASA Astrophysics Data System (ADS)

31
Characteristics of beam collision timing and position at the KEK B-factory
2010-11-01

Using the Belle detector we study the characteristics of beam collisions at the KEKB 3.5 GeV e+ and 8 GeV e- asymmetric energy collider. We investigate the collision timing tIP and its z-coordinate along the beam axis zIP as a function of the position of the colliding bunch in a beam train. The various tIP and zIP behaviors observed by Belle are attributed to beam loading effects in the radio ...

NASA Astrophysics Data System (ADS)

32
UP-GRADED RHIC INJECTION SYSTEM.
2003-05-12

The design of the RHIC injection systems anticipated the possibility of filling and operating the rings with a 120 bunch pattern, corresponding to 110 bunches after allowing for the abort gap. Beam measurements during the 2002 run confirmed the possibility, although at the expense of severe transverse emittance growth and thus not on an operational basis. ...

Energy Citations Database

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