Materials for EM calorimeters


The energy resolution of a calorimeter RMS(E)/E is typically parametrized with a term depending on the energy (called sometimes a stochastic term) a/Eb and a constant term, added in quadratures. The power b is close to 1/2 for sampling calorimeters, lead glass calorimeters etc. For materials with a very high yield, like NaI, b is close to 1/4. In the table only the factor a is shown. The constant term depends on the number of channels, calibration etc, and for large calorimeters is about 1-2%.

Properties of the materials used for electro-magnetic calorimeters.
Material Rad. length (cm) Nucl. length (cm) Molière R (cm) Ecrit, (MeV) Refrac. index Density (g/cm3) Decay const (ns) Peak emiss. (nm) Rel. light yield E resol GeV½ Rad. hardn.
TF1 glass 2.74 ? 4.70 15 1.647 3.86 Cher. Cher. 0.001 ? 0.06 2 krad
NaI(Tl) 2.59 41.4 4.50 ? 1.85 3.67 250 410 . 1.0 0.02 low
PbWO4 0.89 22.4 2.20 ? 2.30 8.28 5-15 420-440 0.01 0.034 high
PbF2 0.93 ? 2.22 ? 1.82 7.77 Cher. Cher. 0.001 0.06 high

Properties of several lead glasses
Material Rad. length (cm) Nucl. coll. length (cm) Moliere R (cm) Ecrit, (MeV) Refrac. index Density (g/cm3) Pb weight % Rad. hardn.
TF1 2.74 56.6* 4.70 15 1.647 3.86 ? low
F-2 3.06 22.7 ? ? 18.4 1.620 3.60 45 ?
F8-00 3.1 22.5 ? ? 1.620 3.60 ? ?
SF-2 2.76 21.8 ? ? 17.5 1.648 3.86 51 ?
SF-5 2.54 21.4 ? ? 15.8 1.673 4.08 55 ?
DF6c/SF6 1.70 17.8 ? ? 13.8 1.805 5.20 71 ?
SF57 1.546 ? 2.61 12.4 1.89 5.51 70? ?
* - Nuclear interaction length (not the collision length)
Table 2.

The chemical structure of lead-glass

F8-00TF1-000TF101
PbO45.0%51.2%51.2%
SiO242.8%41.3%41.5%
K2O10.4%7.0%7.0%
Na2O1.8%
As2O30.5%
CeO20.2%
Refractive index, ne1.621.651.65

E-Mail : gen@jlab.org
Last updated: Wed, 19 July 2001