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Your search keyword '"HABS, D."' showing total 7 results
Start Over Author "HABS, D." Journal review of scientific instruments
7 results on '"HABS, D."'

1. A novel high resolution ion wide angle spectrometer

Author

Jung, D., primary, Hörlein, R., additional, Gautier, D. C., additional, Letzring, S., additional, Kiefer, D., additional, Allinger, K., additional, Albright, B. J., additional, Shah, R., additional, Palaniyappan, S., additional, Yin, L., additional, Fernández, J. C., additional, Habs, D., additional, and Hegelich, B. M., additional

Published
2011
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2. Development of a high resolution and high dispersion Thomson parabola

Author

Jung, D., primary, Hörlein, R., additional, Kiefer, D., additional, Letzring, S., additional, Gautier, D. C., additional, Schramm, U., additional, Hübsch, C., additional, Öhm, R., additional, Albright, B. J., additional, Fernandez, J. C., additional, Habs, D., additional, and Hegelich, B. M., additional

Published
2011
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3. Performance of the MLL-IonCatcher

Author

Neumayr, J. B., primary, Thirolf, P. G., additional, Habs, D., additional, Heinz, S., additional, Kolhinen, V. S., additional, Sewtz, M., additional, and Szerypo, J., additional

Published
2006
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7. A high resolution, broad energy acceptance spectrometer for laser wakefield acceleration experiments.

Author

Sears CM, Cuevas SB, Schramm U, Schmid K, Buck A, Habs D, Krausz F, and Veisz L

Abstract

Laser wakefield experiments present a unique challenge in measuring the resulting electron energy properties due to the large energy range of interest, typically several 100 MeV, and the large electron beam divergence and pointing jitter >1 mrad. In many experiments the energy resolution and accuracy are limited by the convolved transverse spot size and pointing jitter of the beam. In this paper we present an electron energy spectrometer consisting of two magnets designed specifically for laser wakefield experiments. In the primary magnet the field is produced by permanent magnets. A second optional electromagnet can be used to obtain better resolution for electron energies above 75 MeV. The spectrometer has an acceptance of 2.5-400 MeV (E(max)/E(min)>100) with a resolution of better than 1% rms for electron energies above 25 MeV. This high resolution is achieved by refocusing electrons in the energy plane and without any postprocessing image deconvolution. Finally, the spectrometer employs two complimentary detection mechanisms: (1) absolutely calibrated scintillation screens imaged by cameras outside the vacuum chamber and (2) an array of scintillating fibers coupled to a low-noise charge-coupled device.

Published
2010
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