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NASA Scientific and Technical Aerospace Reports

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needs to underst<strong>and</strong> the relationship between pH <strong>and</strong> resistivity of the diluted BCP mix. This report is an attempt to address<br />

these issues.<br />

NTIS<br />

Polishing; Ph; Electrical Resistivity<br />

20040120853 Fermi National Accelerator Lab., Batavia, IL, USA<br />

E781 Hyperon Spectrometer Constants<br />

Lach, J.; May 04, 2004; 16 pp.; In English<br />

Report No.(s): DE2004-823428; FERMILAB-TM-2128; No Copyright; Avail: Department of Energy Information Bridge<br />

This is a discussion of the physical measurements, sizes, distances <strong>and</strong> magnetic fields of the Hyperon Spectrometer<br />

Magnet <strong>and</strong> its components. Some we get from construction drawings (like the target dimensions) <strong>and</strong> others from<br />

measurements in differing coordinate systems. Included also are the properties of the hyperon productions targets used in<br />

E781.<br />

NTIS<br />

Spectrometers; Dimensional Measurement<br />

20040120854 California Univ., Lawrence Berkeley National Lab., Berkeley, CA, USA, California Univ., Berkeley, CA,<br />

USA<br />

Evaluation of Si(Li) Detectors for Use in Compton Telescopes<br />

Tindall, C.; Hau, I. D.; Luke, P. N.; May 2002; In English<br />

Report No.(s): DE2004-823269; LBNL-50234; No Copyright; Avail: National <strong>Technical</strong> Information Service (NTIS)<br />

Si(Li) detectors are currently being developed for use in large Compton telescopes. A major advantage of silicon when<br />

compared with germanium is its ability to operate at significantly higher temperature. To determine the feasibility of using<br />

Si(Li) detectors in a Compton telescope, their performance as a function of temperature has been studied. We present leakage<br />

current, noise data <strong>and</strong> gamma-ray spectral performance at various temperatures for single 6-mm thick planar devices. It has<br />

been determined that for detectors without a guard ring, the noise began to rise significantly around 210K. Adding a guard<br />

ring improved the leakage current by about an order of magnitude <strong>and</strong> reduced the total noise (detector plus electronics) by<br />

about 25 percent. The noise of the detectors with(approx)130 mm2 area <strong>and</strong> a guard ring did not exceed our performance goal<br />

of 2 keV FWHM until the temperature was approximately 240K. For 122 keV gamma rays, no evidence of ballistic deficit<br />

was seen at 8 ms peaking time <strong>and</strong> bias voltages corresponding to an internal electric field of(approx)1150 V/cm. Some<br />

evidence of ballistic deficit was seen for 662 keV gamma rays at temperatures above 220K.<br />

NTIS<br />

Telescopes; Silicon; Lithium<br />

20040120855 California Univ., Lawrence Berkeley National Lab., Berkeley, CA, USA<br />

Jets as a Probe of Dense Matter at RHIC<br />

Filimonov, K.; 2004; In English<br />

Report No.(s): DE2004-822980; No Copyright; Avail: National <strong>Technical</strong> Information Service (NTIS)<br />

Jet quenching in the matter created in high energy nucleus-nucleus collisions provides a tomographic tool to probe the<br />

medium properties. Recent experimental results on jet production at the Relativistic Heavy-Ion Collider (RHIC) are reviewed.<br />

Jet properties in p+p <strong>and</strong> d+Au collisions have been measured, establishing the baseline for studying jet modification in<br />

heavy-ion collisions. Current progress on detailed studies of high transverse momentum production in Au+Au collisions is<br />

discussed, with an emphasis on dihadron correlation measurements.<br />

NTIS<br />

Nuclear Interactions; Tomography<br />

20040120856 Fermi National Accelerator Lab., Batavia, IL, USA<br />

Indicators of the Energy Error in the Linac to Booster Transfer<br />

Yang, X.; MacLachlan, J.; Apr. 2004; 20 pp.; In English<br />

Report No.(s): DE2004-822915; FERMILAB-TM-2240; No Copyright; Avail: Department of Energy Information Bridge<br />

The match between the Linac beam energy <strong>and</strong> the energy determined by the bending field of the Booster magnets is<br />

crucial for rf capture, beam quality, <strong>and</strong> the transmission efficiency in a Booster cycle. The observation of the injection energy<br />

match is important for injection tuning. Several signals, such as phase shift drive (PSD), radial position error (RPOS),<br />

282

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