N. Phinney

Publication List Details

Period

1989 - 2009

Number

63

Co-Authors

I Workstation Consoles for SLC’ (2009)

J. Bogart, A. Hunter, S. Kleban, N. Phinney, N. Spencer

A workstation console based on the DEC VAXstation GPx has been developed for the SLC control system. The three video monitors (touchpanel, color graphics display and terminal screen) of the original...

Feedback Systems For Linear Colliders (2007)

Hendrickson Grossberg Himel, L. Hendrickson, P. Grossberg, T. Himel, M. Minty, ...

Feedback systems are essential for stable operation of a linear collider, providing a cost-effective method for relaxing tight tolerances. In the Stanford Linear Collider (SLC), feedback controls...

Luminosity Upgrades For The Slc (2007)

Raimondi Breidenbach Clendenin, M. Breidenbach, J. E. Clendenin, F. J. Decker, M. Minty, N. Phinney, ...

Recent performance improvements at the SLAC Linear Collider (SLC) have led to a proposal to further increase the luminosity up to a factor of four through a series of modest hardware upgrades. New...

Pulse To Pulse Stability Issues In The Slc (2007)

Adolphsen Assmann Decker, C. Adolphsen, R. Assmann, F. J. Decker, P. Emma, J. Frisch, ...

Although the SLC achieved record luminosity in 1994, a major hindrance to further increases is pulse-to-pulse stability of the machine, often referred to as jitter. Raising the intensity of the SLC...

Performance Of The 1994/95 Slc Final Focus System (2007)

Zimmermann Barklow Ecklund, F. Zimmermann, T. Barklow, S. Ecklund, P. Emma, D. Mccormick, ...

Amajor upgrade to the SLC final focus was installed in 1994 to eliminate the dominant third-order aberration of the system, and thereby to reduce the vertical beam size at the IP by a factor of two....

1 Abstract Luminosity Optimization Feedback in the SLC (2007)

L. Hendrickson, S. Bes, P. Grossberg, D. Mccormick, N. Phinney, P. Raimondi, ...

The luminosity optimization at the SLC has been limited by the precision with which one can measure the micron size beams at the Interaction Point. Ten independent tuning parameters must be adjusted....

Design of the beam delivery system for the International Linear Collider (2007)

Seryi, A., Amann, J., Arnold, R., Asiri, F., Bane, K., Bellomo, P., ...

The beam delivery system for the linear collider focuses beams to nanometer sizes at its interaction point, collimates the beam halo to provide acceptable background in the detector and has a...

Design of the beam delivery system for the International Linear Collider (2007)

Seryi, A., Amann, J., Arnold, R., Asiri, F., Bane, K., Bellomo, P., ...

The beam delivery system for the linear collider focuses beams to nanometer sizes at its interaction point, collimates the beam halo to provide acceptable background in the detector and has a...

Design of the beam delivery system for the International Linear Collider (2007)

Seryi, A., Amann, J., Arnold, R., Asiri, F., Bane, K., Bellomo, P., ...

The beam delivery system for the linear collider focuses beams to nanometer sizes at its interaction point, collimates the beam halo to provide acceptable background in the detector and has a...

A Test Facility for the International Linear Collider at SLAC End Station A, for Prototypes of Beam Delivery and IR Components (2005)

Woods, M., Erickson, R., Frisch, J., Hast, C., Jobe, R. K., Keller, L., ...

The SLAC Linac can deliver damped bunches with ILC parameters for bunch charge and bunch length to End Station A. A 10Hz beam at 28.5 GeV energy can be delivered there, parasitic with PEP-II...

Proposal of the Next Incarnation of Accelerator Test Facility at KEK for the International Linear Collider (2005)

Araki, S., Hayano, H., Higashi, Y., Honda, Y., Kanazawa, K., Kubo, K., ...

To reach design luminosity, the International Linear Collider (ILC) must be able to create and reliably maintain nanometer size beams. The ATF damping ring is the unique facility where ILC emittances...

Proposal of the Next Incarnation of Accelerator Test Facility at KEK for the International Linear Collider (2005)

Araki, S., Hayano, H., Higashi, Y., Honda, Y., Kanazawa, K., Kubo, K., ...

To reach design luminosity, the International Linear Collider (ILC) must be able to create and reliably maintain nanometer size beams. The ATF damping ring is the unique facility where ILC emittances...

Proposal of the Next Incarnation of Accelerator Test Facility at KEK for the International Linear Collider (2005)

Araki, S., Hayano, H., Higashi, Y., Honda, Y., Kanazawa, K., Kubo, K., ...

To reach design luminosity, the International Linear Collider (ILC) must be able to create and reliably maintain nanometer size beams. The ATF damping ring is the unique facility where ILC emittances...

How to Commission, Operate and Maintain a Large Future Accelerator Complex From Far Remote Sites (2002)

Czarapata, P C, Hartill, D L, Myers, S, Peggs, S, Phinney, N, Serio, M, ...

A study on future large accelerators [1] has considered a facility, which is designed, built and operated by a worldwide collaboration of equal partner institutions, and which is remote from most of...

How to Commission, Operate and Maintain a Large Future Accelerator Complex From Far Remote Sites (2002)

Czarapata, P., Hartill, D., Myers, S., Peggs, S., Phinney, N., Serio, M., ...

A study on future large accelerators [1] has considered a facility, which is designed, built and operated by a worldwide collaboration of equal partner institutions, and which is remote from most of...

How to Commission, Operate and Maintain a Large Future Accelerator Complex From Far Remote Sites (2002)

Czarapata, P C, Hartill, D L, Myers, S, Peggs, S, Phinney, N, Serio, M, ...

A study on future large accelerators [1] has considered a facility, which is designed, built and operated by a worldwide collaboration of equal partner institutions, and which is remote from most of...

Status Report of the Inter-Laboratory Task Force on Remote Operation (2002)

Czarapata, P C, Hartill, D L, Myers, S, Peggs, S, Phinney, N, Serio, M, ...

In February 2000, the International Committee for Future Accelerators initiated a study of a new model for international collaboration on a future large accelerator project, the Global Accelerator...

Status Report of the Inter-Laboratory Task Force on Remote Operation (2002)

Czarapata, P C, Hartill, D L, Myers, S, Peggs, S, Phinney, N, Serio, M, ...

In February 2000, the International Committee for Future Accelerators initiated a study of a new model for international collaboration on a future large accelerator project, the Global Accelerator...

How to Commission, Operate and Maintain a Large Future Accelerator Complex from Far Remote (2001)

Czarapata, P., Hartill, D., Myers, S., Peggs, S., Phinney, N., Serio, M., ...

A study on future large accelerators [1] has considered a facility, which is designed, built and operated by a worldwide collaboration of equal partner institutions, and which is remote from most of...

Feedback Systems for Linear Colliders (2001)

Hendrickson, L., Grossberg, P., Himel, T., Minty, M., Phinney, N., Raimondi, P., ...

Feedback systems are essential for stable operation of a linear collider, providing a cost-effective method for relaxing tight tolerances. In the Stanford Linear Collider (SLC), feedback controls...

Beam-based Feedback Simulations for the NLC Linac (2000)

Hendrickson, L., Phinney, N., Raimondi, P., Raubenheimer, T., Seryi, A., Tenenbaum, P.

Extensive beam-based feedback systems are planned as an integral part of the Next Linear Collider (NLC) control system. Wakefield effects are a significant influence on the feedback design, imposing...

Stability Considerations for Final Focus Systems of Future Linear Colliders (2000)

Assmann, R W, Jeanneret, J B, Verdier, A, Vos, L, Wildner, E, Zimmermann, Frank, ...

The final focus systems for the future linear colliders need to focus beams to nm-range spot sizes at the collision point. The design spot size varies from several nm for 500 GeV to the one nm range...

Physics and technology of the Next Linear Collider (2000)

Kuhlman, S, Adolphsen, C E, Aiello, R, Akemoto, M, Alley, R, Assmann, R W, ...

We present the current expectations for the design and physics program of an e+e- linear collider of center of mass energy 500 GeV -- 1 TeV. We review the experiments that would be carried out at...

An automated focal point positioning and emittance measurement procedure for the interaction point of the SLC (1990)

Phinney, N., Bambade, P., Kozanecki, W., Koska, Wayne A.

To achieve maximum luminosity at the SLC, both the electron and positron beams must reach their minimum transverse size within 1 mm of the longitudinal location where the two bunches collide. This...

Beam-beam deflection as a beam tuning tool at the SLAC linear collider (1990)

Koska, Wayne A., Bambade, P., Kozanecki, W., Phinney, N., Wagner, S. R.

To achieve maximum integrated luminosity at the SLAC Linear Collider, a method of noninvasive beam tuning is required. Traditional luminosity monitors based on Bhabha scattering are inadequate...

Initial measurements of Z-boson resonance parameters in e+e- annihilation (1989)

Abrams, G. S., Adolphsen, C. E., Aleksan, R., Alexander, J. P., Allen, M. A., Atwood, W. B., ...

We have measured the mass of the Z boson to be 91.11±0.23 GeV/c^2, and its width to be 1.61-0.43+0.60 GeV. If we constrain the visible width to its standard-model value, we find the partial width to...

Parameters of the SLAC Next Linear Collider

Raubenheimer Adolphsen Burke, T. Raubenheimer, C. Adolphsen, D. Burke, P. Chen, S. Ecklund, ...

In this paper, we present the parameters and layout of the Next Linear Collider (NLC). The NLC is the SLAC design of a future linear collider using X-band RF technology in the main linacs. The...