Difference between revisions of "Detector Description"
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=GEM Detector Design and Structure= | =GEM Detector Design and Structure= | ||
| − | The GEM preamplifier described in | + | |
| + | The GEM preamplifier described in section XXXX was used to increase the signal amplitude of the ionization chamber. Primary electrons are liberated by an ionizing particle intersecting an ionization chamber that has a 90/10 Ar/CO2 gas; the cathode's electric field accelerates the electrons towards the GEM preamplifier. As described in section XXX, a single GEM preamplifier can increase the number of liberated electron by three orders of magnitude via secondary ionization.<ref = "chechik"> R. Chechik, A. Breskin, G. P. Guedes, D. Mörmann, J. M. Maia, V. Dangendorf, D. Vartsky, J. M. F. Dos Santos, and J. F. C. A. Veloso, Recent Investigations of Cascaded GEM and MHSP detectors, IEEE Trans. Nucl. Sci. 2004 </ref> Using three pre-amplifiers will increase the signal amplitude making it measurable. A high voltage divider circuit is used to establish the electric fields for each preamplifier using a single power supply channel, and secondary electrons are guided towards a segmented charge collector. | ||
==Detector Structure== | ==Detector Structure== | ||
| + | The triple GEM detector is composed of three GEM preamplifiers, a cathode and an anode. A GEM preamplifier is a 50 micron thick kapton foil clad on both sides with 5 microns of copper. A staggered pattern of 50 micron diameter holes, equally spaced by distances comparable to the hole diameter, is chemically etched into the copper clad foil of a 140 um pitch distance over an area of 10x10cm. <ref name = "Souli"> F. Sauli, et al, NIM A 386, 531 (1997) </ref> The detector contains three GEM preamplifiers mounted on square plastic frames separated by a vertical distance of 2.8 mm and placed parallel to the cathode as shown in the figure below. | ||
| + | |||
| + | [[File:GEM_Detector_original.png | thumb |alt=Example alt text|Fig.1 shows the original GEM detector design.| center | 200px]] | ||
| − | + | The cathode is a square copper plate that is 10x10cm and is 3.5 mm away from the top of the first GEM card. This cathode design is capable of being set to be at a potential voltage of 5 kV (in the air) without any discharge. The charge collector (readout anode) is constructed of 50-80 micron wide strips that are insulated to determine the location of the collected electrons, and are arranged to allow equal charge sharing on the upper (x coordinate) and lower (y coordinate) charge collector layers <ref name= readout>Physik Department E18, Technische University Munchen, 2D readout Plane, 21 of Jun.2012. http://www.e18.ph.tum.de/research/compass/gempixelgem-tracking-detectors </ref>. | |
| − | + | [[File:Charge_collector.jpg | thumb |alt=Example alt text|Fig. shows the charge collector dimensions and arrangement <ref name = readout/>.| center| 200px]] | |
| − | + | All the above components exist in a sealed chamber that consists of two ertalyte plastic sheets; they are bolted together by a number of M3 plastic screws located around the detector window to form a well enclosed cavity. Also, the chamber has a 13x13cm kapton window to reduce the energy loss of incident particles entering the chamber. The figures below show top, bottom, and side views of the detector's chamber design. | |
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| − | |||
| − | [[File: | + | [[File:GEM_top.png | 200px]] [[File:GEM_bottom.png | 200px]] [[File:GEM_sides.png | 200px]] |
| − | + | =Modifying the GEM detector as neutron sensitive detector= | |
| + | The GEM’s original design was modified to convert it to a neutron-sensitive detector. As mentioned previously in Section YYY, fissionable material, inserted inside the chamber, may be used to indirectly detect neutrons by detecting the ionization caused by fission fragments released into the chamber if a neutron induced fission event occurs. The cathode design has a 3 cm diameter coating of U-233 with a 30-40 um thickness. The kapton window height was increased 2.5 mm to accommodate an increase in the distance of the cathode to 8 mm from the top of the first of GEM card (instead of 3.5 mm in the original design). An FR4 shutter which had enough area to cover the fissionable material was attached in the space between the cathode and the first GEM card. The shutter could be opened or closed from outside the chamber. When the shutter is closed, it covers the U-233 coating and stops the emitted fission fragments ionizing the gas beyond the shutter. When the shutter is open, the ionization due to fission fragments produces a signal. | ||
| − | |||
| − | + | What about alpha and beta particles. | |
| + | The shutter has the ability to stop the fission fragments that are emitted from U-233 coating. Having the U-233 as a source for alpha particles, the QDC charge spectrum showed a difference in case the shutter was open and when it was close, such a test proved the ability of the FR4 shutter to stop (or partially stop) the emitted alpha particles from U-233 coating. The figure below shows the charge spectra in case of shutter open and closed as the detector's operating voltage is 2.6 kV and 2.9 kV for GEM and cathode successively. | ||
| + | |||
| + | {| | ||
| + | |- | ||
| + | | [[File:2.6_2.9kV_4.5.png | thumb |alt=Example alt text|charge collected as the voltage is 2.60 2.90 kV for GEM and cathode successively| 200px]] | ||
| + | |} | ||
| + | Since the fission fragments are heavier ions than the alpha particles, a closed shutter should stop them. Such an ability is important to distinguish the fission fragments' signal from the other particles' signals in a heavy radiation environment created in an operating accelerator or reactor. | ||
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|[[File:GEM_design.png | thumb |alt=Example alt text|Adding modifications to GEM design.| 100px]] ||[[File:modified_GEM_pic.png | thumb |alt=Example alt text|Modifying the cavity size by the increasing the height of kapton window. | 100px]] | |[[File:GEM_design.png | thumb |alt=Example alt text|Adding modifications to GEM design.| 100px]] ||[[File:modified_GEM_pic.png | thumb |alt=Example alt text|Modifying the cavity size by the increasing the height of kapton window. | 100px]] | ||
| − | | | + | || |
|[[File:GEM_shutter_open.png | thumb |alt=Example alt text|Detector's shutter is open.| 100px]]|| [[File:GEM_shutter_close.png | thumb |alt=Example alt text|Detector's shutter is close.| 100px]] | |[[File:GEM_shutter_open.png | thumb |alt=Example alt text|Detector's shutter is open.| 100px]]|| [[File:GEM_shutter_close.png | thumb |alt=Example alt text|Detector's shutter is close.| 100px]] | ||
|} | |} | ||
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=High voltage divider circuit= | =High voltage divider circuit= | ||
| − | The GEM preamplifiers are connected | + | A high voltage divider circuit is used to proportionally apply voltages on both faces of each GEM preamplifier as defined by the resistors used in the circuit. The first GEM preamplifier that an electron encounters as it traverses the detector is set to have the most negative voltage. |
| + | The GEM preamplifiers are connected to a high voltage divider circuit that specifies the electron multiplication and supports (manages) their transfer to the charge collector. As mentioned previously, The applied voltage on GEM cards determines all the detector's properties, such as the order of electron multiplication, and the electron collection by the readout plate. A high voltage divider circuit was designed for these purposes as shown in the figure below: <ref = "SergeHV"> Pinto, Serge . Gas Electron Multipliers Development of large area GEMS and spherical GEMS. Diss. Mathematisch-Naturwissenschaftliche Fakultät , 2011 </ref> | ||
| + | {| | ||
| + | |[[Image:GEM_HV_Dist_Net.jpg | thumb |alt=Example alt text| Figure shows the HV-divider circuit.| 100px]] | ||
| + | |} | ||
| − | + | The HV circuit also provides the cathode with a voltage up to 3.6 kV to produce an electric field to drift most of the electrons, which are primarily produced by ionization. It provides the GEM cards with voltage between the top and bottom of each one and allows the voltage to decrease gradually to reach the minimum value between the third GEM's sides. So, the main advantages of the circuit design are to provide a voltage for electron multiplication, and to guide most of the drift electrons to the charge collector. | |
| − | + | The circuit provides a trigger signal through a high pass filter connected to the third GEM electrode. One of the ways to get the detector signal is by a high pass filter that is in contact with the bottom side of the third GEM card; a positive signal is detected by the oscilloscope, since all the electrons are leaving the last GEM electrode toward the charge collector. The job of the high pass filter is to block all the low signal frequencies to provide a signal that can clearly be detected by a 50 ohm terminated oscilloscope. | |
| − | The | + | |
| + | The table shows the measurements of voltage between the sides of the GEM electrodes, and voltage between each side and the ground that are provided by the HV-voltage divider circuit shown above. | ||
{| border="1" cellpadding="4" | {| border="1" cellpadding="4" | ||
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|} | |} | ||
| + | =Construction environment= | ||
| + | |||
| + | Detectors are very sensitive devices, its components are connected to high voltage power supplies in a relatively thin chamber with Ar/CO2 90/10 gas mixture. As a result, the method of construction and maintaining demands a laminar flow hood that accommodates a clean environment from any source of dust in the atmosphere or any surrounding objects, Also the gloves are used to avoid any particle transfer to the detector's components through the steps of its construction or testing. | ||
Latest revision as of 02:56, 27 March 2014
GEM Detector Design and Structure
The GEM preamplifier described in section XXXX was used to increase the signal amplitude of the ionization chamber. Primary electrons are liberated by an ionizing particle intersecting an ionization chamber that has a 90/10 Ar/CO2 gas; the cathode's electric field accelerates the electrons towards the GEM preamplifier. As described in section XXX, a single GEM preamplifier can increase the number of liberated electron by three orders of magnitude via secondary ionization.<ref = "chechik"> R. Chechik, A. Breskin, G. P. Guedes, D. Mörmann, J. M. Maia, V. Dangendorf, D. Vartsky, J. M. F. Dos Santos, and J. F. C. A. Veloso, Recent Investigations of Cascaded GEM and MHSP detectors, IEEE Trans. Nucl. Sci. 2004 </ref> Using three pre-amplifiers will increase the signal amplitude making it measurable. A high voltage divider circuit is used to establish the electric fields for each preamplifier using a single power supply channel, and secondary electrons are guided towards a segmented charge collector.
Detector Structure
The triple GEM detector is composed of three GEM preamplifiers, a cathode and an anode. A GEM preamplifier is a 50 micron thick kapton foil clad on both sides with 5 microns of copper. A staggered pattern of 50 micron diameter holes, equally spaced by distances comparable to the hole diameter, is chemically etched into the copper clad foil of a 140 um pitch distance over an area of 10x10cm. <ref name = "Souli"> F. Sauli, et al, NIM A 386, 531 (1997) </ref> The detector contains three GEM preamplifiers mounted on square plastic frames separated by a vertical distance of 2.8 mm and placed parallel to the cathode as shown in the figure below.
The cathode is a square copper plate that is 10x10cm and is 3.5 mm away from the top of the first GEM card. This cathode design is capable of being set to be at a potential voltage of 5 kV (in the air) without any discharge. The charge collector (readout anode) is constructed of 50-80 micron wide strips that are insulated to determine the location of the collected electrons, and are arranged to allow equal charge sharing on the upper (x coordinate) and lower (y coordinate) charge collector layers <ref name= readout>Physik Department E18, Technische University Munchen, 2D readout Plane, 21 of Jun.2012. http://www.e18.ph.tum.de/research/compass/gempixelgem-tracking-detectors </ref>.
All the above components exist in a sealed chamber that consists of two ertalyte plastic sheets; they are bolted together by a number of M3 plastic screws located around the detector window to form a well enclosed cavity. Also, the chamber has a 13x13cm kapton window to reduce the energy loss of incident particles entering the chamber. The figures below show top, bottom, and side views of the detector's chamber design.
Modifying the GEM detector as neutron sensitive detector
The GEM’s original design was modified to convert it to a neutron-sensitive detector. As mentioned previously in Section YYY, fissionable material, inserted inside the chamber, may be used to indirectly detect neutrons by detecting the ionization caused by fission fragments released into the chamber if a neutron induced fission event occurs. The cathode design has a 3 cm diameter coating of U-233 with a 30-40 um thickness. The kapton window height was increased 2.5 mm to accommodate an increase in the distance of the cathode to 8 mm from the top of the first of GEM card (instead of 3.5 mm in the original design). An FR4 shutter which had enough area to cover the fissionable material was attached in the space between the cathode and the first GEM card. The shutter could be opened or closed from outside the chamber. When the shutter is closed, it covers the U-233 coating and stops the emitted fission fragments ionizing the gas beyond the shutter. When the shutter is open, the ionization due to fission fragments produces a signal.
What about alpha and beta particles.
The shutter has the ability to stop the fission fragments that are emitted from U-233 coating. Having the U-233 as a source for alpha particles, the QDC charge spectrum showed a difference in case the shutter was open and when it was close, such a test proved the ability of the FR4 shutter to stop (or partially stop) the emitted alpha particles from U-233 coating. The figure below shows the charge spectra in case of shutter open and closed as the detector's operating voltage is 2.6 kV and 2.9 kV for GEM and cathode successively.
Since the fission fragments are heavier ions than the alpha particles, a closed shutter should stop them. Such an ability is important to distinguish the fission fragments' signal from the other particles' signals in a heavy radiation environment created in an operating accelerator or reactor.
The figures below show the modified components of the detector.
High voltage divider circuit
A high voltage divider circuit is used to proportionally apply voltages on both faces of each GEM preamplifier as defined by the resistors used in the circuit. The first GEM preamplifier that an electron encounters as it traverses the detector is set to have the most negative voltage. The GEM preamplifiers are connected to a high voltage divider circuit that specifies the electron multiplication and supports (manages) their transfer to the charge collector. As mentioned previously, The applied voltage on GEM cards determines all the detector's properties, such as the order of electron multiplication, and the electron collection by the readout plate. A high voltage divider circuit was designed for these purposes as shown in the figure below: <ref = "SergeHV"> Pinto, Serge . Gas Electron Multipliers Development of large area GEMS and spherical GEMS. Diss. Mathematisch-Naturwissenschaftliche Fakultät , 2011 </ref>
The HV circuit also provides the cathode with a voltage up to 3.6 kV to produce an electric field to drift most of the electrons, which are primarily produced by ionization. It provides the GEM cards with voltage between the top and bottom of each one and allows the voltage to decrease gradually to reach the minimum value between the third GEM's sides. So, the main advantages of the circuit design are to provide a voltage for electron multiplication, and to guide most of the drift electrons to the charge collector.
The circuit provides a trigger signal through a high pass filter connected to the third GEM electrode. One of the ways to get the detector signal is by a high pass filter that is in contact with the bottom side of the third GEM card; a positive signal is detected by the oscilloscope, since all the electrons are leaving the last GEM electrode toward the charge collector. The job of the high pass filter is to block all the low signal frequencies to provide a signal that can clearly be detected by a 50 ohm terminated oscilloscope.
The table shows the measurements of voltage between the sides of the GEM electrodes, and voltage between each side and the ground that are provided by the HV-voltage divider circuit shown above.
| 2550 | 2579 | 2259 | 304 | 1671 | 1394 | 279 | 818 | 570 | 245 |
| 2600 | 2630 | 2303 | 310 | 1704 | 1421 | 285 | 834 | 581 | 250 |
| 2650 | 2680 | 2348 | 316 | 1737 | 1449 | 290 | 850 | 592 | 255 |
| 2700 | 2731 | 2393 | 322 | 1770 | 1476 | 296 | 866 | 603 | 260 |
| 2750 | 2781 | 2373 | 328 | 1803 | 1503 | 302 | 882 | 614 | 264 |
| 2800 | 2832 | 2482 | 332 | 1836 | 1530 | 307 | 898 | 625 | 269 |
Construction environment
Detectors are very sensitive devices, its components are connected to high voltage power supplies in a relatively thin chamber with Ar/CO2 90/10 gas mixture. As a result, the method of construction and maintaining demands a laminar flow hood that accommodates a clean environment from any source of dust in the atmosphere or any surrounding objects, Also the gloves are used to avoid any particle transfer to the detector's components through the steps of its construction or testing.
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