Tevatron performance goals for the coming decade

Holmes, Stephen D.

doi:10.1109/pac.1999.795620

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The Luminosity1

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2001

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Cited by 4 publications

(1 citation statement)

References 8 publications

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“…An important physical quantity used in the accelerators is the luminosity, which is directly connected with the amount of collisions produced at the machine. The expression for the Tevatron's luminosity C is given by [55]:…”

Section: The Luminositymentioning

confidence: 99%

Search for First Generation Leptoquarks in the $e \nu j j$ and $e e j j$ Decay Channels in $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.8-TeV

Strumia

2001

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Section: The Luminositymentioning

confidence: 99%

Search for First Generation Leptoquarks in the $e \nu j j$ and $e e j j$ Decay Channels in $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.8-TeV

Strumia

2001

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Strength and shape of the magnetic field of the Fermilab Main Injector dipoles

Harding

Brown²,

DiMarco³

et al.

Proceedings of the 1999 Particle Accelerator Conference (Cat. No.99CH36366)

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MAGNET STRENGTHMeasurements of 230 6-meter and 136 4-meter dipoles constructed for the Fermilab Main Injector were carried out as part of the magnet production effort. An automated measurement system provided data on magnetic field strength and shape using several partially redundant systems. Results of these measurements are available for each individual magnet for use in accelerator modelling. In this report we will summarise the results on all of the magnets to characterise the properties which will govern accelerator operation.Groups 4 and 5 define our nominal magnet strength at each current.The mean strength, including me 4-m magnets weighted at 2/3 of the 6-m magnets, was calculated for each current. Deviations from that strength (for the 6-m magnets) or from 2/3 of that strength (for the 4-m magnets) are normalized to the nominal strength of the 6-m magnets.These deviations are quoted here in "units" of parts in 104.

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Upgrading RHIC for higher luminosity

MacKay

Ben‐Zvi²,

Brennan³

et al.

PACS2001. Proceedings of the 2001 Particle Accelerator Conference (Cat. No.01CH37268)

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While RHIC has only just started running for its heavy ion physics program, in the first run last summer, we achieved 10% of the design luminosity. In this paper we discuss plans for increasing the luminosity by a factor of 35 beyond the nominal design. A factor of 4 should be straightforward by doubling the number of bunches per ring and squeezing the β* from 2 to 1 m at selected interaction points. An additional factor of 8 to 10 could be possible by using electron cooling to counteract intrabeam scattering and reduce emittances of the beams.

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Tevatron performance goals for the coming decade

Cited by 4 publications

References 8 publications

Search for First Generation Leptoquarks in the $e \nu j j$ and $e e j j$ Decay Channels in $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.8-TeV

Search for First Generation Leptoquarks in the $e \nu j j$ and $e e j j$ Decay Channels in $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.8-TeV

Strength and shape of the magnetic field of the Fermilab Main Injector dipoles

Upgrading RHIC for higher luminosity

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