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Scientific Report 2007-2009<br />
Particle physics<br />
P23. Dual readout calorimetry with crystals<br />
In recent years, dual-readout calorimetry has emerged<br />
as a promising new solution for the need to detect<br />
both leptons and hadrons with excellent accuracy in<br />
high-energy particle physics experiments [1]. The Dual<br />
Readout Method (DREAM) is based on a simultaneous<br />
measurement of different types of signals which provide<br />
complementary information about details of the shower<br />
development. It has been argued and experimentally<br />
demonstrated that a comparison of the signals produced<br />
by Čerenkov light and scintillation light makes it possible<br />
to measure the energy fraction carried by the electromagnetic<br />
shower component, f em , event by event. Since<br />
the event by event fluctuation in f em is the main limitation<br />
for the energy resolution in hadronic calorimeters,<br />
this may lead to an important improvement in the performance<br />
of hadron calorimeters. The first calorimeter<br />
of this type was based on a copper absorber structure,<br />
equipped with two types of active media. Scintillating<br />
fibers measured the total energy deposited by all the<br />
shower particles, while Čerenkov light, generated only by<br />
charged relativistic particles, was produced in undoped<br />
optical fibers.<br />
The signals from certain high-density crystals<br />
(PbWO 4 , BGO) can also be unraveled into Čerenkov<br />
and scintillation components; such crystals, when used in<br />
conjunction with the fiber calorimeter mentioned above,<br />
can offer in principle the same advantages for hadronic<br />
shower detection and, at the same time, provide accurate<br />
energy resolution for the electromagnetic component.<br />
Figure 1: The average time structure of the UV signals from<br />
200 GeV π + in BGO crystal. The long tail is due to the<br />
scintillation component,while the prompt peak represents the<br />
Cerenkov contribution(a). The ”contamination” of scintillation<br />
light in a narrow time window ∆t around the prompt<br />
peak (b).<br />
We have performed a series of measurements in the<br />
H4 beam line of the SPS at CERN [2] providing a beam<br />
of high energy electrons and pions. Our detector was<br />
a high-density Bi 4 Ge 3 O 12 (BGO) crystal with a length<br />
of 24 cm mounted on a rotating table. The light produced<br />
by particles traversing this crystal was read out<br />
by two photomultiplier tubes Hamamatsu R5900U, 10-<br />
stage, bialkali photocathode, borosilicate window, located<br />
at the opposite ends. The light generated in the<br />
crystal was UV filtered at one side before being read out<br />
to reduce the scintillation contribution.<br />
Figure 2: The Čerenkov/scintillation ratio in the UV signals<br />
from the BGO crystal, for a gate of 10 ns around the prompt<br />
peak, as a function of the orientation of the crystal with respect<br />
to the beam. Data for 50 GeV electrons and 200 GeV<br />
π + .<br />
The purpose of these tests was to split the crystal<br />
signals into their scintillation and Čerenkov components.<br />
We exploited the following differences between these<br />
components: 1) differences in time structure. Čerenkov<br />
light is prompt, while the scintillation mechanism is<br />
characterized by one or several time constants. 2) differences<br />
in directionality. Contrary to scintillation light,<br />
which is emitted isotropically, Čerenkov light is emitted<br />
at a characteristic angle by the relativistic (shower)<br />
particles that traverse the detector. We measured the<br />
signals for different orientations of the crystal with<br />
respect to the particle beam. In Figure 1 the prompt<br />
Čerenkov signal is superimposed to the slow scintillation<br />
component, allowing an easy separation of the two<br />
contributions. In Figure 2 the ratio between Čerenkov<br />
and scintillation light is plotted as function of the angle<br />
of the crystal with respect to the beam direction; the<br />
peak around the angle of Čerenkov emission is clearly<br />
visible. At present additional studies with a large BGO<br />
matrix [3] and with different type of crystals [4] are<br />
performed.<br />
References<br />
1. R. Wigmans, New Journal of Physics 10 (2008) 025003.<br />
2. N. Akchurin, et al., N.I.M. A595 (2008) 359.<br />
3. N. Akchurin, et al., N.I.M. A610 (2009) 488.<br />
4. N. Akchurin, et al., N.I.M. A604 (2009) 710.<br />
Authors<br />
G. Ciapetti, F. Lacava, D. Pinci 1 , C. Voena 1<br />
<strong>Sapienza</strong> Università di Roma 130 Dipartimento di Fisica