19
E. Norbeck U. I owa Fast Gas Detector APR 05 Tampa 1 Small Fast Gas Detector for High- Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

Embed Size (px)

Citation preview

Page 1: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 1

Small Fast Gas Detector for High-Energy Electrons

E. Norbeck, J.E. Olson, and Y. Onel

University of Iowa

Page 2: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 2

Example of low-pressure PPAC (Parallel Plate Avalanche Counter)

• Two flat plates

• Separated by 1 mm• Filled with 100 torr

hydrocarbon• 1000 V between plates

• Simple, low cost device

• Unaffected by heat, light

• Can be radiation hard

Page 3: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 3

For high speed, the RC time constant must be kept small.

Only PPACs of small area are fast, ~1 ns

R = 50 Ω (coax cable). C is the capacity between the plates

Speed vs Size

Page 4: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 4

Single Pixel PPAC

• Gap 0.6 mm 950 V across gap• Cathode 7X0 = 29 mm of tantalum• Area of anode is 1.0 cm2

• Guard ring to simulate neighboring pixels

Detail of gap and guard ring

Page 5: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 5

New Detector with less inductanceSame signal width of 1.5 ns for isobutane at 80 torr.

Page 6: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 6

Test at home with a 7 mCi 137Cs source

Get up to 20 mV signals directly into 50 coax

Page 7: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 7

Signal into coax with no amplifier

Signal observed directly with fast scope

C(out)

Page 8: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 8

The signal is divided between the detector capacitance and the output capacitance.

The sum of the two provides energy for damaging sparks.

For small detectors we use a ratio of 20.

For large detectors we make them equal.

Page 9: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 9

We did not have high-energy electrons so we made them in situ from protons interacting near the front end of our tantalum cylinder.

The showers had amplitudes as much as 40 mV

Page 10: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 10

Signal Shape from Shower

-30 mV

1.62 ns FWHM

One third of amplitude of fast signal is lost in 20 m of standard RG-58 coax.

Page 11: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 11

•The signal comes from moving charges.

•In an avalanche, most of the electrons and ions are formed near the anode.

•The electron signal is fast but with a total area small compared with the ion signal.

•The ion signal is flat while the ions are moving and stops when the ions are collected.

•In the next slide, when the ions are collected at the cathode they liberate electrons.

Page 12: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 12

20 torr ethane 550 V 0.6 mm gap

Page 13: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 13

Gases that have been used

• C4H10

• C2H6

• CH4

• Argon -CO2

Alkanes work well as avalanche gases

But only at 1 atm pressure

• CF4

• C3F8

• C4F8 cyclo

Additional benefit with perfluoro-analog

Page 14: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 14

Many advantages to operating at atmospheric pressure

CF4 gives nice signals at 2500 V

95% Ar + 5% CO2 operates at 1100 V, but with a slow, 5 ns, fast signal. It also has a smaller useful operating range than CF4

For 0.6 mm spacing

Page 15: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 15

Advantages of Perfluro gasses

Not toxicDoes not burnResists agingEasily recycled (A small chemical cartridge can be inserted in the gas line that will remove all impurities from the gas)High density (more primary electrons)Contains no chlorine so is allowed in national laboratoriesWe found good results with 0.6 mm spacing, but not so good with 2.5 mm.

More study on this is needed.

Page 16: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 16

One plate can be divided into pixels to provide position resolution.

Page 17: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 17

PPAC Readout

-

+ Summing amplifier can be used to add PPAC signals,

increasing the effective size of PPAC (without increasing the time width of the signals)

Page 18: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 18

Cautions

Simple scaling of plate spacing, pressure, voltage, etc. does not apply over a wide range of parameters.

Look at wave form to make sure the signal is clean.

Page 19: E. Norbeck U. IowaFast Gas Detector APR 05 Tampa1 Small Fast Gas Detector for High-Energy Electrons E. Norbeck, J.E. Olson, and Y. Onel University of Iowa

E. Norbeck U. Iowa Fast Gas Detector APR 05 Tampa 19

CONCLUSIONS

PPACs for a calorimeter

•Can be made radiation hard.

•Can provide position information.

•Have good energy resolution for high energy showers.

•Have sub nanosecond time resolution.

•Can connect PPACs directly into 50 coax

•Can test with source on side