A High-Power Test of an X-Band Molybdenum-Iris Structure (2004)
Wuensch, Walter, Döbert, Steffen, Grudiev, A, Heikkinen, Samuli Tapio, Syratchev, I V, Taborelli, M, ...
In order to achieve accelerating gradients above 150 MV/m, alternative materials to copper are being investigated by the CLIC study. The potential of refractory metals has already been demonstrated...
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...
An Asset Test of the CLIC Accelerating Structure (2000)
Achard, Claude, Adolphsen, C E, Dehler, M, Jensen, E, Luong, M, McCormick, D, ...
Beam Current Monitors in the Nlcta (2000)
The current profile along the 126 ns, multi-bunch beam pulse in the Next Linear Collider Test Accelerator (NLCTA) is monitored with fast toroids (rise time ~1 ns). Inserted at several positions along...
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...
Beam loading compensation in the NLCTA (1997)
Adolphsen, C E, Lavine, T, Nantista, C D, Ruth, Ronald D, Wang, J
RF systems for the NLCTA (1997)
Wang, J W, Adolphsen, C E, Atkinson, R, Baumgartner, W H, Eichner, J, Fuller, R W, ...
NLCTA injector experimental results (1997)
Yeremian, A D, Adolphsen, C E, Miller, R H, Nantista, C D, Wang, J W
The computer program LIAR for the simulation and modeling of high performance linacs (1997)
Assmann, R W, Adolphsen, C E, Bane, Karl Leopold Freitag, Emma, P, Raubenheimer, T O, Siemann, R, ...
Beam profile monitors in the NLCTA (1997)
Nantista, C D, Adolphsen, C E, Brown, R L, Fuller, R, Rifkin, J
Performance issues, downtime recovery and tuning in the Next Linear Collider (NLC) (1997)
Zimmermann, Frank, Adolphsen, C E, Assmann, R W, Bane, Karl Leopold Freitag, Burke, D, Decker, Franz Josef, ...
Analysis and application of manifold radiation in DDS 1: first experiences (1997)
Jones, R M, Kroll, N M, Seidel, M, Adolphsen, C E, Bane, Karl Leopold Freitag, Fowkes, W R, ...
Recent results and plans for the future on SLAC damped detuned structures (DDS) (1997)
Kroll, N M, Jones, R M, Adolphsen, C E, Bane, Karl Leopold Freitag, Fowkes, W R, Ko, K, ...
A damped detuned structure for the next linear collider (1997)
Miller, R H, Adolphsen, C E, Bane, Karl Leopold Freitag, Fowkes, W R, Gluckstern, R L, Hanna, S M, ...
Higher order beam jitter in the SLC linac (1997)
Decker, Franz Josef, Adolphsen, C E, Podobedov, B V, Raimondi, Pantaleo
Vibration studies of the Stanford Linear Accelerator (1995)
Turner, J L, Adolphsen, C E, Bowden, G B, Decker, Franz Josef, Hartman, S C, Matsumoto, S, ...
Emittance and energy control in the NLC main linacs (1995)
Adolphsen, C E, Bane, Karl Leopold Freitag, Kubo, K, Raubenheimer, T O, Ruth, Ronald D, Thompson, K A, ...
Alignment tolerance of accelerating structures and corrections for future linear colliders (1995)
Kubo, K, Adolphsen, C E, Bane, Karl Leopold Freitag, Raubenheimer, T O, Thompson, K A
Feedback performance at the Stanford Linear Collider (1995)
Minty, Michiko G, Adolphsen, C E, Hendrickson, L J, Sass, R, Slaton, T, Woodley, M
Parameters of the SLAC Next Linear Collider (1995)
Raubenheimer, T O, Adolphsen, C E, Burke, D, Chen, P, Ecklund, S D, Irwin, J, ...
Measurement of the effect of collimator generated wakefields on the beams in the SLC (1995)
Bane, Karl Leopold Freitag, Adolphsen, C E, Decker, Franz Josef, Emma, P, Krejcik, P, Zimmermann, Frank
Fast feedback for linear colliders (1995)
Hendrickson, L, Adolphsen, C E, Allison, S, Gromme, T E, Grossberg, P, Himel, Thomas M, ...
Measurement of wakefield suppression in a detuned x-band accelerator structure (1995)
Adolphsen, C E, Bane, Karl Leopold Freitag, Higo, T, Kubo, K, Miller, R, Ruth, Ronald D, ...
Issues in multi-bunch emittance preservation in the NLC (1994)
Bane, Karl Leopold Freitag, Adolphsen, C E, Kubo, K, Thompson, K A
A reanalysis of B0-B0 mixing in e+e- annihilation at 29 GeV (1990)
Weir, A. J., Abrams, G., Adolphsen, C. E., Alexander, J. P., Alvarez, M., Amidei, D., ...
Data taken by the Mark II detector at the PEP storage ring was used to measure the rate of dilepton production in multihadronic events produced by e+e- annihilation at [radical sign]s=29 GeV. We...
Measurements of Z-boson resonance parameters in e+e- annihilation (1989)
Abrams, G. S., Adolphsen, C. E., Averill, D., Ballam, J., Barish, B. C., Barklow, T., ...
We have measured the mass of the Z boson to be 91.14±0.12 GeV/c^2, and its width to be 2.42-0.35+0.45 GeV. If we constrain the visible width to its standard-model value, we find the partial width to...
First measurements of hadronic decays of the Z boson (1989)
Abrams, G. S., Adolphsen, C. E., Aleksan, R., Alexander, J. P., Averill, D., Ballam, J., ...
We have observed hadronic final states produced in the decays of Z bosons. In order to study the parton structure of these events, we compare the distributions in sphericity, thurst, aplanarity, and...
Search for B-decay to Higgs bosons for Higgs boson masses between 50 and 210 MeV/c2 (1989)
Snyder, A., Murray, W. N., Abrams, G., Adolphsen, C. E., Akerlof, Carl W., Alexander, J. P., ...
We use data from the Mark II experiment at PEP to search for the process B-->h0X for mh0 between 50 and 210 MeV/c2. No evidence for the Higgs boson is seen in this mass range. The limit obtained...
Studies of jet production rates in e + e − annihilation at E cm =29 GeV (1989)
Schwarz, A. S., White, S. L., Koska, Wayne A., Fordham, C., Schmidke, W. B., Field, R. C., ...
Production rates of multijet hadronic final states are studied in e + e − annihilation at 29 GeV center of mass energy. QCD shower model calculations with exact first order matrix element weighting...
The Mark II detector for the SLC (1989)
Abrams, G., Adolphsen, C. E., Akerlof, Carl W., Alexander, J. P., Alvarez, M., Averill, Damon R., ...
The Mark II detector has been upgraded in preparation for its role as the first detector to take data at the Stanford Linear Collider. The new detector components include the central drift chamber,...
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...