The performance of a total absorption spectrometer up to energies of 60 GeV

Böhmer, Volker; Engler, J.; Flauger, W.; Keim, H.; Mönnig, F.; Pack, K.; Schopper, H.; Babaev, A.; Brachman, E.; Eliseev, G.P.; Ermilov, A.; Galaktionov, Yu.; Gorodkov, Yu.; Kamishkov, Yu.; Leikin, E.M.; Lubimov, V.; Shevchenko, V.; Zeldovich, O.

doi:10.1016/0029-554x(74)90494-7

Cited by 25 publications

(1 citation statement)

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“…The different response of hadron calorimeters to electromagnetic and hadronic showers, observed for the first generation of hadron calorimeters [1,2,3], are a source of non-linearities, deviations of the relative resolution from the statistically expected 1/ √ E -behaviour and the origin of the non-gaussian shape of the response function [4,5]. Two different methods have been proposed to avoid these disadvantages.…”

Section: Introductionmentioning

confidence: 99%

An improved weighting algorithm to achieve software compensation in a fine grained LAr calorimeter

İşsever

Borras

Wegener

2005

Nuclear Instruments and Methods in Physics Research Section A:

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An improved weighting algorithm applied to hadron showers has been developed for a fine grained LAr calorimeter. The new method uses tabulated weights which depend on the density of energy deposited in individual cells and in a surrounding cone whose symmetry axis connects the interaction vertex with the highest energy cluster in the shower induced by a hadron. The weighting of the visible energy and the correction for losses due to noise cuts are applied in separate steps. In contrast to standard weighting procedures the new algorithm allows to reconstruct the total energy as well as the spatial energy deposition on the level of individual calorimeter cells.The linearity and the energy resolution of the pion signal in the momentum interval 2 GeV /c ≤ p ≤ 20 GeV /c studied in this analysis are considerably improved in comparison to the standard weighting algorithm as practiced presently by the H1 collaboration. Moreover the energy spectra reconstructed with the new method follow in a broad interval a Gaussian distribution and have less pronounced tails.

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