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Wire Chamber
Heritage collection CERN-OBJ-CERN-OBJ-DE-041 · Unidad documental simple
Parte de Heritage Collection Test

Magnetoscriptive readout wire chamber. Multi-wire detectors contain layers of positively and negatively charged wires enclosed in a chamber full of gas. A charged particle passing through the chamber knocks negatively charged electrons out of atoms in the gas, leaving behind positive ions. The electrons are pulled towards the positively charged wires. They collide with other atoms on the way, producing an avalanche of electrons and ions. The movement of these electrons and ions induces an electric pulse in the wires which is collected by fast electronics. The size of the pulse is proportional to the energy loss of the original particle.

Heritage collection CERN-OBJ-CERN-OBJ-DE-042 · Unidad documental simple
Parte de Heritage Collection Test

Instrument used to test the wires of small chambers before closing them. The chambers were 50cm long, 0.45cm wide and 0.06cm thick. They were meant to be used in a calorimeter for a PS experiment.

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double counter
Heritage collection CERN-OBJ-CERN-OBJ-DE-044 · Unidad documental simple · 1970
Parte de Heritage Collection Test

A double counter made of a scintillation counter with 8 photomultiplier tubes and a cherenkov counter. Was used to identify particles.The dimensions include the support.

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DELPHI Silicon Tracker
Heritage collection CERN-OBJ-CERN-OBJ-DE-052 · Unidad documental simple
Parte de Heritage Collection Test

DELPHI was one of the four experiments installed at the LEP particle accelerator from 1989 - 2000. The silicon tracking detector was nearest to the collision point in the centre of the detector. It was used to pinpoint the collision and catch short-lived particles.

Heritage collection CERN-OBJ-CERN-OBJ-DE-056 · Unidad documental simple
Parte de Heritage Collection Test

OPAL was one of the four experiments installed at the LEP particle accelerator from 1989 - 2000. OPAL's central tracking system consists of (in order of increasing radius) a silicon microvertex detector, a vertex detector, a jet chamber, and z-chambers. All the tracking detectors work by observing the ionization of atoms by charged particles passing by: when the atoms are ionized, electrons are knocked out of their atomic orbitals, and are then able to move freely in the detector. These ionization electrons are detected in the different parts of the tracking system. (This piece includes the vertex, jet and Z chambers) In the picture above, the central detector is the piece being removed to the right.

Niobium LEP 2 accelerating cavities
Heritage collection CERN-OBJ-CERN-OBJ-AC-032 · Unidad documental simple
Parte de Heritage Collection Test

An accelerating cavity from LEP. This could be cut open to show the layer of niobium on the inside. Operating at 4.2 degrees above absolute zero, the niobium is superconducting and carries an accelerating field of 6 million volts per metre with negligible losses. Each cavity has a surface of 6 m2. The niobium layer is only 1.2 microns thick, ten times thinner than a hair. Such a large area had never been coated to such a high accuracy. A speck of dust could ruin the performance of the whole cavity so the work had to be done in an extremely clean environment. These challenging requirements pushed European industry to new achievements. 256 of these cavities were used in an upgrade of the LEP accelerator to double the energy of the particle beams.

LEP Radio Frequency Copper Cavity
Heritage collection CERN-OBJ-CERN-OBJ-AC-036 · Unidad documental simple
Parte de Heritage Collection Test

The pulse of a particle accelerator. 128 of these radio frequency cavities were positioned around CERN's 27-kilometre LEP ring to accelerate electrons and positrons. The acceleration was produced by microwave electric oscillations at 352 MHz. The electrons and positrons were grouped into bunches, like beads on a string, and the copper sphere at the top stored the microwave energy between the passage of individual bunches. This made for valuable energy savings as it reduced the heat generated in the cavity.

CMS Tracker Model
Heritage collection CERN-OBJ-CERN-OBJ-DE-068 · Unidad documental simple
Parte de Heritage Collection Test

Model of the tracking detector for the CMS experiment at the LHC. This object is a mock-up of an early design of the CMS Tracker mechanics. It is a segment of a “Wheel” to support Micro-Strip Gas Chamber (MSGC) detector modules on the outer layers and silicon-strip detector modules in the innermost layers. The particularity of that design is that modules are organised in spirals, along which power and optical cables and cooling pipes were planned to be routed. Some of such spirals are illustrated in the mock-up by the colors of the modules. With the detector development it became, however, evident that the silicon detectors would need to be operated in LHC experiments in cold temperatures, while the MSGC could stay in normal room-temperature. That split in two temperatures lead to separating those two detector types by a thermal barrier and therefore jeopardizing the idea of using common, vertical Wheels with services arranged along spirals.

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