27.04.2015 Views

download report - Sapienza

download report - Sapienza

download report - Sapienza

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

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

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!