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Daniel Rees

Researcher at Los Alamos National Laboratory

Publications -  54
Citations -  254

Daniel Rees is an academic researcher from Los Alamos National Laboratory. The author has contributed to research in topics: Klystron & RF power amplifier. The author has an hindex of 9, co-authored 54 publications receiving 251 citations.

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Journal ArticleDOI

Kinetics of the Microwave-Heated CO Oxidation Reaction over Alumina-Supported Pd and Pt Catalysts

TL;DR: In this paper, the reaction kinetics of the CO oxidation reaction on Pt/Al 2 O 3 and Pd/Al O 3 were measured in a packed bed reactor heated by microwave energy.
Proceedings Article

Commissioning of the low-energy demonstration accelerator (leda) radio-frequency quadrupole (rfq)*

TL;DR: In this article, the initial commissioning of a 6.7-MeV 100-mA RFQ is reported, which is part of the H + injector for the Accelerator Production of Tritium (APT) project.
ReportDOI

Results and lessons learned from conditioning 1 MW CW 350 MHz coaxial vacuum windows

TL;DR: The high-power RF testing of the 16 EEV coaxial windows of Chelmsford, England are described and the successes and failures in the conditioning, manufacturing and testing techniques of the windows are presented.
Proceedings ArticleDOI

The RF system design for the Spallation Neutron Source

Abstract: Spallation Neutron Source (SNS) accelerator includes a nominally 1000 MeV, 2 mA average current linac consisting of a radio frequency quadrupole (RFQ), drift tube linac (DTL), coupled cavity linac (CCL), a medium and high beta superconducting (SC) linac, and two buncher cavities for beam transport to the ring. Los Alamos is responsible for the RF systems for all sections of the linac. The SNS linac is a pulsed proton linac and the RF system must support a 1 msec beam pulse at up to a 60 Hz repetition rate. The RFQ and DTL utilize seven, 2.5 MW klystrons and operate at 402.5 MHz. The CCL, SC, and buncher cavities operate at 805 MHz. Six, 5 MW klystrons are utilized for the CCL and buncher cavities while eighty-one 550 kW klystrons are used for the SC cavities. All of the RF hardware for the SNS linac is currently in production. This paper will present details of the RF system-level design as well as specific details of the SNS RF equipment. The design parameters will be discussed. One of the design challenges has been achieving a reasonable cost with the very large number of high-power klystrons. The approaches we used to reduce cost and the resulting design compromises will be discussed.