An improved design of R-MSGC

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Presentation transcript:

An improved design of R-MSGC R. Oliveira,1 V. Peskov,1,2 Pietropaolo,3 P.Picchi4 1CERN, Geneva, Switzerland 2UNAM, Mexico 3INFN Padova, Padova, Italy 4INFN Frascati, Frascati, Italy

“All futiure MPGDs will have resistive electrodes” R “All futiure MPGDs will have resistive electrodes” R.. Oliveira, CERN, 2010 The aim of ongoing work in our Lab is to demonstrate that all types of MPGD can be made spark-proved if they have resistive electrodes

We already proofed this in the case of TGEM/GEM and MICROMEGAS and of course other groups (see for example: F.Hartjes, Report at the MPGD Conf in Crete, R. Akimoto et al, presentation at MPGDs conference in Crete , V. Razin et al., arXiv:0911.4807, T. Alexopoulos et al., RD-51 Internal report #2010–006) also successfully working in this direction

At this time we focus on microstrip gas counters (MSGCs) Let me remind you that MSGCs were the first micropattern gaseous detectors invented a long time ago by A. Oed; however due to the sparking problems and due to the inventions of GEM and MICROMEGAS this type of micropattern detector is nowadays abandoned

However, if one makes the MSGC spark-protected, may be it will be not a so bad detector?

In the previous RD-51 meeting (a mini-week at CERN) we show some first preliminary results obtained with R-MSGCs (prototypes #1 and 2)

R-MSGC #1 Fiber glass plates (FR-4) Cu strips 50 μm wide were created on the top of the fiber glass plate by the photolithographic method Then in contact with the side surfaces of each Cu strip dielectric layers (Pyralux PC1025 Photoimageable coverlay by DuPont) were manufactured; Finally the detector surface was coated with resistive paste and polished so that the anode and the cathode resistive strips become separated by the Coverlay dielectric layer.

Results obtained with R-MSGC #1

R-MSGC #2 As a next step the middle part of the Cu strips were coated with 50 μm width layer of photoresist (Fig. d) and the rest of the area of the Cu strip were etched (Fig e); in such a way metallic anode strips 50 μm in width were created. Finally the gaps between Cu anode strip and the cathode resistive strips were filled with glue FR-4 and after it hardening the entire surface was mechanically polished. First by photolithographic technology Cu strip 200 μm in width were created on the top of the FR-4 plate (Figs a and b). Then the gaps between the strips were filled with the resistive paste (Fig. c).

Results obtained with R-MSGC#2 in Ne+5%CH4

After learning the problems we produced now much better R-MSGC allowing gas gains as high as with the best MSGCs manufactured on a glass substrate to be achieve

R-MSGC prototype #3

An improved and simplified technology of R-MSGC production: PCB with 5μm thick Cu layer Milled grooved 100 μm deep and 0.6 μm wide, pitch 1mm. 0.6mm The grooves were then filled with resistive paste 1mm 20μm By a photolithographic technology Cu 20 μm wide strips were created between the grooves

Covarlay protection layer 60mm Covarlay protection layer

Features: Printed circuit bard (not the glass!) Thin metallic anodes Resistive cathodes Coverlay (65 μm, laminated ) protection of edges

Coverlay layer reliably protects the edges region against the sparks

Electrodes edges arrangement in “classical” MSGC

Some results

Measurements in Ar/CO2 were done in order to compare with resistive MICROMEGAS

Resistive MICROMEGAS T. Alexopoulos et al., RD-51 Internal report #2010–006

Advantages of R-MSGC: ● Max. achievable gain is comparable to res Advantages of R-MSGC: ● Max. achievable gain is comparable to res. MICROMEGAS ● However, R-MSGC is easier to manufacture than MICROMEGAS ● Easier to clean form dust particles ● Less parts in the detector assembly (no cathode mesh) ● Can be assembled from patches practically without dead spaces/zones

MSGCs offer quite good position resolution

High granularity 2D R-MSGCs are under the development now in Rui Lab

competitive in some applications Conclusions: ●Our progress in development R-MSGCs is summarized in the table R-MSGC -type Max. achievable gain with 6keV photons 1 ~10 2 ~500 3 10000 ●Features of the new design (#3): Printed circuit substrate Thinner anode Resistive cathodes Coverlay protection of the edges regions ●The max. achievable gas gains are equal to the best glass MSGC and approaching R-MICROMEGAS ●The advantages: simple technology (less price), less elemenets, easier to clean We hope our works will renew the interest to MSCG detectors which can be competitive in some applications