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PEP-II Status and Future Plans

PEP-II Status and Future Plans
Author:
Publisher:
Total Pages: 4
Release: 2002
Genre:
ISBN:

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The PEP-II B-Factory at SLAC has reached a luminosity of 4.6 x 1033/cm2/s and has delivered 94 fb−1 of data to the BaBar physics detector by the end of May 2002. PEP-II has delivered over 309 pb−1 in 24 hours and over 6.35 fb−1 in one month. The accelerator physics issues for these performance levels include electron cloud, beam-beam effects, parasitic beam-beam collisions, and RF beam loading. Upgrades to PEP-II are underway to increase the luminosity to 2 to 4 x 1034/cm2/s by FY2007. The accelerator physics effects that must be dealt with during these upgrades include RF loading, multi-bunch feedback, IR beta function, bunch length reduction, and interaction region vacuum chamber upgrades.


Status and Future Plans of the PEP-II B-Factory

Status and Future Plans of the PEP-II B-Factory
Author:
Publisher:
Total Pages: 3
Release: 2002
Genre:
ISBN:

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The PEP-II e+e- collider [1,2,3,4] has been operating for two years with the BaBar detector at the energy of the Upsilon 4S resonance. The peak luminosity has reached 3.3 x 1033/cm2/s with 693 bunches with a positron current of 1.5 A and an electron current of 0.8 A. PEP-II has delivered in excess of 38 fb−1 of data to BaBar. The beam-beam tune shift limits are approaching 0.05-0.07 horizontally and 0.03-0.05 vertically [5]. The electron cloud instability ECI enlarges the positron beam size at high currents but is reduced by a solenoidal field on the vacuum chambers [6]. The beam currents in PEP-II are being raised to increase the number of bunches and the luminosity. Over the next few years the luminosity goal for PEP-II is 1034/cm2/s.


PEP-II Status and Outlook

PEP-II Status and Outlook
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Total Pages: 5
Release: 2012
Genre:
ISBN:

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PEP-II/BABAR are presently in their second physics run. With machine and detector performance and reliability at an all-time high, almost 51 fb−1 have been integrated by BABAR up to mid-October 2001. PEP-II luminosity has reached 4.4 x 1033 cm−2 s−1 and our highest monthly delivered luminosity has been above 6 pb−1, exceeding the performance parameters given in the PEP-II CDR by almost 50%. The increase compared to the first run in 2000 has been achieved by a combination of beam-current increase and beam-size decrease. In this paper we will summarize the PEP-II performance and the present limitations as well as our plans to further increase machine performance.


PEP-II Status Report

PEP-II Status Report
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Total Pages: 6
Release: 1998
Genre:
ISBN:

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The main design features of the PEP-II asymmetric two-ring electron-positron B Factory collider, built at the Stanford Linear Accelerator Center, are described. This facility will complete construction in June 1998. The high energy ring, completed in May 1997, has had 3 months of commissioning and successfully stored 0.75 A of electrons. The success of the high energy ring testing validates not only its ring components, but also the injection system, the RF system and the control system all of which are common to the two rings.


Energy Research Abstracts

Energy Research Abstracts
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Publisher:
Total Pages: 544
Release: 1994-06
Genre: Power resources
ISBN:

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IR Up Grade Plans for the PEP-II B-Factory

IR Up Grade Plans for the PEP-II B-Factory
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Release: 2004
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PEP-II, the SLAC, LBNL, LLNL B-factory has achieved a peak luminosity of over 9 x 10[sup 33] cm[sup -2]s[sup -1], more than 3 times the design luminosity, and plans to obtain a luminosity of over 1 x 10[sup 34] cm[sup -2] sec[sup -1] in the next year. In order to push the luminosity performance of PEP-II to even higher levels an upgrade to the interaction region (IR) is being designed. In the present design, the interaction point (IP) is a head-on collision with two strong horizontal dipole magnets located between 21-70 cm from the IP that bring the beams together and separate the beams after the collision. The first parasitic crossing (PC) is 63 cm from the IP in the present by2 bunch spacing. Future improvements to PEP-II performance include lowering the [beta]*[sub y] values of both rings. This will increase the [beta][sub y] value at the PCs which increases the beam-beam effect at these non-colliding crossings. Introducing a horizontal crossing angle at the IP quickly increases the beam separation at the PCs but recent beam-beam studies indicate that a significant luminosity reduction occurs when a crossing angle is introduced at the IP. We discuss these issues and describe the present interaction region upgrade design.