small changes

diff --git a/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.pdf b/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.pdf
index 15d40bfa4b19fbaa792e18d0c4de9f55454a0261..f541514612f598a357bfaf265e9714e9c20c2ccf 100644 (file)
Binary files a/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.pdf and b/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.pdf differ

diff --git a/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.ps b/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.ps
index 3f99091d5bab7462448ebfce32ec21734e26e03c..092748ee023e98306d9f21d3a0a47d871b15f2f4 100644 (file)
--- a/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.ps
+++ b/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.ps
@@ -1,7 +1,7 @@
 %!PS-Adobe-2.0
 %%Creator: dvips(k) 5.993 Copyright 2013 Radical Eye Software
 %%Title: F:/Eigene Dateien/Downloads/Dropbox/Promotion/Jahresbericht2014/reports/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.dvi
-%%CreationDate: Tue Feb 10 17:33:35 2015
+%%CreationDate: Fri Feb 13 10:52:02 2015
 %%Pages: 1
 %%PageOrder: Ascend
 %%BoundingBox: 0 0 595 842
@@ -15,7 +15,7 @@
 %+ pdf
 %+ "F:/Eigene Dateien/Downloads/Dropbox/Promotion/Jahresbericht2014/reports/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.dvi"
 %DVIPSParameters: dpi=8000
-%DVIPSSource:  TeX output 2015.02.10:1733
+%DVIPSSource:  TeX output 2015.02.13:1052
 %%BeginProcSet: tex.pro 0 0
 %!
 /TeXDict 300 dict def TeXDict begin/N{def}def/B{bind def}N/S{exch}N/X{S
@@ -2847,12 +2847,12 @@ TeXDict begin 39139632 55387786 1000 8000 8000
  TeXBase1Encoding ReEncodeFont }5 996.264 /Times-Italic
 rf /Fb 233[615 22[{}1 996.264 /EURM10 rf /Fc 197[284
 58[{}1 996.264 /CMMI9 rf /Fd 146[853 52[512 6[512 512
-48[{}4 996.264 /CMR9 rf /Fe 133[442 498 498 719 1[498
+48[{}4 996.264 /CMR9 rf /Fe 133[442 498 498 719 498 498
 277 388 332 1[498 498 498 775 277 498 1[277 498 498 332
 442 498 442 1[442 3[332 1[332 3[940 2[609 554 665 1[554
 719 719 886 609 2[332 2[554 609 719 665 1[719 6[277 498
 2[498 498 498 498 498 498 498 1[249 332 249 2[332 332
-1[775 38[{ TeXBase1Encoding ReEncodeFont }54 996.264
+1[775 38[{ TeXBase1Encoding ReEncodeFont }55 996.264
 /Times-Roman rf /Ff 140[517 590 3[739 7[442 590 1[590
 16[959 82[{ TeXBase1Encoding ReEncodeFont }7 1328.35
 /Times-Bold rf /Fg 252[424 3[{}1 664.176 /CMSY6 rf /Fh
@@ -2919,18 +2919,18 @@ b(T)-89 b(o)419 b(match)-1701 20606 y(those)444 b(requirements,)485
 b(we)443 b(intend)h(to)f(use)g(CMOS)g(Monolithic)-1701
 21934 y(Acti)-28 b(v)-17 b(e)300 b(Pix)-17 b(el)298 b(Sensors,)303
 b(which)c(are)f(de)-28 b(v)-17 b(eloped)302 b(by)d(the)f(PICSEL)-1701
-23263 y(group)322 b(of)f(IPHC)g(Strasbour)-20 b(g)322
-b(and)g(tested)f(at)g(the)g(IKF)g(Frankfurt)-1701 24591
-y(within)277 b(an)h(common)h(R&D)f(project.)-1701 25919
-y(A)441 b(\002rst)f(fully)g(inte)-17 b(grated)443 b(sensor)-44
-b(,)481 b(MIMOSA-28,)i(w)-11 b(as)440 b(de)-28 b(v)-17
-b(el-)-1701 27248 y(oped)385 b(in)d(the)i(AMS)f Fm(0)p
-Fl(:)p Fm(35)h Fk(\026)p Fm(m)f Fn(CMOS)g(process)h(and)g(it)e(is)f
-(used)-1701 28576 y(for)419 b(data)g(taking)h(in)f(the)h(ST)-103
+23263 y(group)279 b(of)f(IPHC)h(Strasbour)-20 b(g)279
+b(and)g(e)-28 b(v)-17 b(eluated)281 b(at)d(the)g(IKF)g(Frank-)-1701
+24591 y(furt)e(within)h(an)h(common)h(R&D)f(project.)-1701
+25919 y(A)441 b(\002rst)f(fully)g(inte)-17 b(grated)443
+b(sensor)-44 b(,)481 b(MIMOSA-28,)i(w)-11 b(as)440 b(de)-28
+b(v)-17 b(el-)-1701 27248 y(oped)385 b(in)d(the)i(AMS)f
+Fm(0)p Fl(:)p Fm(35)h Fk(\026)p Fm(m)f Fn(CMOS)g(process)h(and)g(it)e
+(is)f(used)-1701 28576 y(for)419 b(data)g(taking)h(in)f(the)h(ST)-103
 b(AR-HFT)420 b(since)f(2014.)771 b(Ho)-28 b(we)g(v)-17
-b(er)-44 b(,)-1701 29904 y(this)448 b(sensor)g(does)h(not)f(match)i
-(the)e(requirements)i(of)e(CBM)g(in)-1701 31233 y(terms)304
-b(of)h(radiation)h(tolerance)h(and)f(readout)g(speed.)428
+b(er)-44 b(,)-1701 29904 y(this)407 b(sensor)g(does)h(not)g(match)h
+(the)e(requirements)i(of)e(CBM)h(re-)-1701 31233 y(g)-6
+b(arding)346 b(radiation)e(tolerance)i(and)f(readout)g(speed.)544
 b(Therefore,)-1701 32561 y(the)399 b(sensor)f(architecture)h(w)-11
 b(as)398 b(migrated)h(to)f(a)g(no)-17 b(v)g(el)401 b
 Fm(0)p Fl(:)p Fm(18)e Fk(\026)p Fm(m)-1701 33889 y Fn(process.)433
@@ -2957,45 +2957,47 @@ Fm(22)253 b Fr(\002)f Fm(33)285 b Fk(\026)p Fm(m)15293
 47173 y(out)336 b(within)f Fm(40)h Fk(\026)p Fm(s)e Fn(via)i(a)f(pair)g
 (of)g(discriminators)g(at)g(the)h(end)g(of)-1701 48501
 y(each)284 b(column.)361 b(Hereafter)-44 b(,)283 b(the)g(digital)f
-(data)h(is)f(zero-suppressed)-1701 49830 y(and)308 b(sent)f(out)h(via)f
-(tw)-11 b(o)307 b(320)h(Mbps)g(digital)f(links.)432 b(The)308
-b(sensiti)-28 b(v)-17 b(e)-1701 51158 y(surf)-11 b(ace)245
-b(of)f(the)h(FSBB)g(is)e Fm(13)p Fl(:)p Fm(7)125 b Fr(\002)g
-Fm(9)p Fl(:)p Fm(2)247 b(mm)15005 50756 y Fj(2)15503
-51158 y Fn(.)332 b(The)245 b(\002nal)g(sensor)f(of)-1701
-52486 y(the)388 b(CBM-MVD)f(will)f(presumably)j(consist)e(of)g(three)h
-(FSBBs.)-1701 53815 y(The)317 b(FSBB-M0)f(w)-11 b(as)316
-b(tested)f(at)g(the)h(CERN-SPS)h(and)g(pro)-17 b(vided)-1701
-55143 y(a)330 b(detection)h(ef)-28 b(\002cienc)-17 b(y)332
-b(of)d Fi(&)405 b Fm(99)p Fl(;)184 b Fm(5\045)p Fn(,)345
-b(a)329 b(dark)h(rate)g(of)f Fi(.)404 b Fm(10)23094 54741
-y Fh(\000)p Fj(5)-1701 56471 y Fn(and)288 b(a)g(spatial)f(resolution)g
-(of)g Fl(<)326 b Fm(5)287 b Fk(\026)p Fm(m)g Fn(in)g(both)h(dimensions)
-g([3],)-1701 57800 y(which)278 b(matches)h(the)e(requirements)h(of)f
-(CBM.)-1701 59128 y(T)-89 b(o)255 b(test)e(the)i(rob)-22
-b(ustness)254 b(of)g(the)g(design)h(and)g(to)f(estimate)g(the)g(pro-)
--1701 60456 y(duction)426 b(costs)d(for)g(the)h(CBM-MVD,)h(we)f
-(measured)h(the)f(pro-)-1701 61785 y(duction)305 b(yield)f(of)f(the)h
-(FSBB.)h(In)e(accordance)k(with)c(our)h(e)-17 b(xperi-)-1701
-63113 y(ence,)256 b(we)249 b(assumed)h(that)f(production)i(mistak)-11
-b(es)249 b(w)-11 b(ould)250 b(turn)f(into)-1701 64442
-y(a)378 b(signi\002cant)g(deterioration)h(of)e(the)h(noise)g(of)f(the)h
-(sensors.)643 b(T)-89 b(o)-1701 65770 y(spot)335 b(such)i
-(deteriorations,)350 b(a)335 b(total)g(of)h(25)g(sensors)e(w)-11
-b(as)336 b(bonded)-1701 67098 y(on)398 b(PCB)g(and)g(operated)h(with)e
-(a)h(suited)f(readout)i(system.)703 b(The)-1701 68427
-y(temporal)395 b(noise)f(\(TN\))g(of)g(the)g(indi)-28
-b(vidual)396 b(pix)-17 b(els)394 b(w)-11 b(as)394 b(deri)-28
-b(v)-17 b(ed)-1701 69755 y(by)302 b(means)f(of)f(a)h(threshold)h(scan.)
-414 b(Moreo)-17 b(v)g(er)-44 b(,)309 b(we)301 b(measured)h(the)-1701
-71083 y(\002x)-17 b(ed)303 b(pattern)e(noise)g(\(FPN\),)f(which)i(is)d
-(caused)j(by)f(the)g(of)-28 b(fset)300 b(of)-1701 72412
-y(the)278 b(dark)f(signal)h(of)e(the)i(pix)-17 b(els.)p
--1701 74335 10394 45 v -660 75047 a Fg(\003)-107 75359
-y Fp(This)339 b(w)-9 b(ork)338 b(has)h(been)f(supported)f(by)h(BMBF)g
-(\(05P12RFFC7\),)367 b(HIC)338 b(for)-1701 76411 y(F)-66
-b(AIR,)223 b(HGS-HIRe)f(and)f(GSI.)23706 34104 y @beginspecial
-0 @llx 0 @lly 814 @urx 572 @ury 2891 @rwi @setspecial
+(data)h(is)f(zero-suppressed)-1701 49830 y(and)412 b(sent)f(out)h(via)f
+(tw)-11 b(o)411 b(320)h(Mbps)f(digital)g(links.)745 b(The)412
+b(sensi-)-1701 51158 y(ti)-28 b(v)-17 b(e)427 b(surf)-11
+b(ace)427 b(of)f(the)h(FSBB)g(is)e Fm(13)p Fl(:)p Fm(7)359
+b Fr(\002)d Fm(9)p Fl(:)p Fm(2)428 b(mm)18603 50756 y
+Fj(2)19100 51158 y Fn(.)791 b(The)427 b(\002nal)-1701
+52486 y(sensor)297 b(of)g(the)g(CBM-MVD)g(will)f(presumably)j(consist)d
+(of)h(three)-1701 53815 y(FSBBs.)567 b(The)353 b(FSBB-M0)g(w)-11
+b(as)351 b(tested)h(at)f(the)h(CERN-SPS)h(and)-1701 55143
+y(pro)-17 b(vided)319 b(a)d(detection)i(ef)-28 b(\002cienc)-17
+b(y)319 b(for)c(minimum)i(ionizing)g(par)-22 b(-)-1701
+56471 y(ticles)278 b(of)g Fi(&)310 b Fm(99)p Fl(;)184
+b Fm(5\045)p Fn(,)280 b(a)f(dark)g(rate)f(of)g Fi(.)310
+b Fm(10)15343 56070 y Fh(\000)p Fj(5)16810 56471 y Fn(and)280
+b(a)e(spatial)g(res-)-1701 57800 y(olution)308 b(of)f
+Fl(<)363 b Fm(5)307 b Fk(\026)p Fm(m)g Fn(in)g(both)h(dimensions)g
+([3],)314 b(which)308 b(matches)-1701 59128 y(the)278
+b(requirements)g(of)f(CBM.)-1701 60456 y(T)-89 b(o)255
+b(test)e(the)i(rob)-22 b(ustness)254 b(of)g(the)g(design)h(and)g(to)f
+(estimate)g(the)g(pro-)-1701 61785 y(duction)426 b(costs)d(for)g(the)h
+(CBM-MVD,)h(we)f(measured)h(the)f(pro-)-1701 63113 y(duction)380
+b(yield)g(of)e(the)h(FSBB.)h(In)e(accordance)k(with)d(our)g(e)-17
+b(xpe-)-1701 64442 y(rience,)468 b(we)430 b(assumed)g(that)f
+(production)j(mistak)-11 b(es)429 b(w)-11 b(ould)430
+b(turn)-1701 65770 y(into)343 b(a)f(signi\002cant)i(deterioration)g(of)
+e(the)h(noise)g(of)f(the)h(sensors.)-1701 67098 y(T)-89
+b(o)391 b(spot)f(such)h(deteriorations,)419 b(a)390 b(total)g(of)f(25)i
+(\(17)f(FSBB-M0a)-1701 68427 y(and)330 b(8)f(FSBB-M0b\))i(sensors)d(w)
+-11 b(as)329 b(bonded)j(on)d(PCB)h(and)g(oper)-22 b(-)-1701
+69755 y(ated)230 b(with)f(a)h(suited)f(readout)i(system.)327
+b(The)230 b(temporal)g(noise)g(\(TN\))-1701 71083 y(of)321
+b(the)h(indi)-28 b(vidual)323 b(pix)-17 b(els)322 b(w)-11
+b(as)322 b(deri)-28 b(v)-17 b(ed)323 b(by)f(means)h(of)e(a)g(thresh-)
+-1701 72412 y(old)374 b(scan.)633 b(Moreo)-17 b(v)g(er)-44
+b(,)399 b(we)374 b(measured)h(the)f(\002x)-17 b(ed)376
+b(pattern)e(noise)p -1701 74335 10394 45 v -660 75047
+a Fg(\003)-107 75359 y Fp(This)339 b(w)-9 b(ork)338 b(has)h(been)f
+(supported)f(by)h(BMBF)g(\(05P12RFFC7\),)367 b(HIC)338
+b(for)-1701 76411 y(F)-66 b(AIR,)223 b(HGS-HIRe)f(and)f(GSI.)23706
+34104 y @beginspecial 0 @llx 0 @lly 814 @urx 572 @ury
+2891 @rwi @setspecial
 %%BeginDocument: TN-FPN.eps
 %!PS-Adobe-3.0 EPSF-3.0
 %%BoundingBox: 0 0 814 572
@@ -26351,48 +26353,51 @@ showpage
 %%EOF
 
 %%EndDocument
- @endspecial 25858 35506 a Fn(Figure)237 b(1:)323 b(TN)236
-b(and)h(FPN)g(measurement)h(of)e(a)g(subset)g(of)g(17)h(chips)25858
-39066 y(The)287 b(results)d(of)h(the)g(study)h(on)g(the)g(FSBB-M0a)h
-(is)d(sho)-28 b(wn)287 b(in)e(\002g-)25858 40395 y(ure)398
-b(1.)704 b(W)-89 b(e)398 b(found)g(all)f(sensors)g(tested)h(to)f(be)h
-(operational)h(and)25858 41723 y(the)-17 b(y)426 b(pro)-17
+ @endspecial 25858 35506 a Fn(Figure)292 b(1:)372 b(T)-77
+b(emporal)292 b(noise)f(and)h(\002x)-17 b(ed)293 b(pattern)f(noise)g
+(measure-)25858 36834 y(ment)278 b(of)f(a)g(subset)g(of)g(17)h(similar)
+d(chips.)25858 40395 y(\(FPN\),)339 b(which)h(is)e(caused)i(by)g(the)f
+(of)-28 b(fset)338 b(of)h(the)g(dark)g(signal)g(of)25858
+41723 y(the)278 b(pix)-17 b(els.)25858 43051 y(The)287
+b(results)d(of)h(the)g(study)h(on)g(the)g(FSBB-M0a)h(is)d(sho)-28
+b(wn)287 b(in)e(\002g-)25858 44380 y(ure)398 b(1.)704
+b(W)-89 b(e)398 b(found)g(all)f(sensors)g(tested)h(to)f(be)h
+(operational)h(and)25858 45708 y(the)-17 b(y)426 b(pro)-17
 b(vided)428 b(a)d Fm(TN)582 b(=)f(\(0)p Fl(:)p Fm(70)358
 b Fr(\006)d Fm(0)p Fl(:)p Fm(05\))427 b(mV)441 b Fn(and)426
-b Fm(FPN)582 b(=)25858 43051 y(\(0)p Fl(:)p Fm(73)263
+b Fm(FPN)582 b(=)25858 47036 y(\(0)p Fl(:)p Fm(73)263
 b Fr(\006)e Fm(0)p Fl(:)p Fm(14\))299 b(mV)15 b Fn(.)403
 b(Only)297 b(one)h(of)f(the)g(tested)g(sensors)f(sho)-28
-b(wed)25858 44380 y(a)214 b(higher)g(FPN)g(of)f Fr(\030)307
+b(wed)25858 48365 y(a)214 b(higher)g(FPN)g(of)f Fr(\030)307
 b Fm(1)p Fl(:)p Fm(2)214 b(mV)15 b Fn(,)227 b(which)214
-b(might)f(still)f(be)h(acceptable.)25858 45708 y(Similarly)253
+b(might)f(still)f(be)h(acceptable.)25858 49693 y(Similarly)253
 b(good)h(results)d(were)i(observ)-17 b(ed)255 b(with)d(the)h(eight)g
-(FSBB-)25858 47036 y(M0b)278 b(tested,)f(which)h(all)f(found)h
-(operational)h(\(not)e(sho)-28 b(wn\).)25858 48365 y(W)-89
-b(e)389 b(conclude)i(that)d(a)g(\002rst)f(full)h(size)g(sensor)g
-(matching)h(the)g(re-)25858 49693 y(quirements)536 b(of)f(CBM)g(in)g
-(terms)f(of)h(surf)-11 b(ace,)599 b(data)536 b(rate)f(and)25858
-51022 y(spatial)395 b(resolution)g(is)f(a)-22 b(v)-28
-b(ailable)396 b(no)-28 b(w)-72 b(.)698 b(Moreo)-17 b(v)g(er)-44
-b(,)425 b(the)395 b(design)25858 52350 y(mostly)286 b(reaches)g(out)g
-(speci\002cation)i(in)d(terms)g(of)g(readout)i(speed.)25858
-53678 y(Measurements)492 b(demonstrated)h(the)e(sensor)g(to)g(pro)-17
-b(vide)493 b(good)25858 55007 y(performances)257 b(for)e(Minimum)h
-(Ionizing)g(P)-17 b(article)256 b(detection)h(and)25858
-56335 y(the)278 b(production)h(yield)e(w)-11 b(as)277
-b(found)i(to)e(e)-17 b(xceed)280 b(95\045.)35765 59279
-y Ff(Refer)-24 b(ences)25858 61244 y Fe([1])553 b(D.)313
-b(Doering)f(et)h(al.)560 b(Noise)312 b(performance)i(and)e(ionizing)h
-(radiation)27573 62462 y(tolerance)346 b(of)f(CMOS)f(MAPS)h(using)g
-(the)g Fd(0)p Fc(:)p Fd(18)g Fb(\026)p Fd(m)h Fe(CMOS)e(pro-)27573
-63680 y(cess.)359 b Fa(J)-25 b(.)249 b(of)h(I.)p Fe(,)f(9\(05\):C0551,)
-g(2014.)25858 65340 y([2])553 b(F)-80 b(.)378 b(Morel)e(et)i(al.)768
+(FSBB-)25858 51022 y(M0b)278 b(tested,)f(which)h(all)f(found)h
+(operational)h(\(not)e(sho)-28 b(wn\).)25858 52350 y(W)-89
+b(e)315 b(conclude)i(that)e(a)f(\002rst)g(full)f(size)i(sensor)f(meets)
+g(the)h(require-)25858 53678 y(ments)292 b(of)f(CBM)h(re)-17
+b(g)-6 b(arding)294 b(surf)-11 b(ace,)295 b(data)e(rate)e(and)i
+(spatial)e(res-)25858 55007 y(olution.)788 b(Moreo)-17
+b(v)g(er)-44 b(,)464 b(the)425 b(design)h(mostly)f(reaches)i(out)e
+(speci-)25858 56335 y(\002cation)330 b(in)f(terms)e(of)i(readout)g
+(speed.)499 b(Measurements)330 b(demon-)25858 57663 y(strated)236
+b(the)h(sensor)f(pro)-17 b(vide)239 b(good)f(performances)g(for)e
+(minimum)25858 58992 y(ionizing)474 b(particle)f(detection)i(and)e(the)
+g(production)i(yield)e(w)-11 b(as)25858 60320 y(found)279
+b(to)d(e)-17 b(xceed)281 b(95\045.)35765 63264 y Ff(Refer)-24
+b(ences)25858 65229 y Fe([1])553 b(D.)313 b(Doering)f(et)h(al.)560
+b(Noise)312 b(performance)i(and)e(ionizing)h(radiation)27573
+66447 y(tolerance)346 b(of)f(CMOS)f(MAPS)h(using)g(the)g
+Fd(0)p Fc(:)p Fd(18)g Fb(\026)p Fd(m)h Fe(CMOS)e(pro-)27573
+67665 y(cess.)359 b Fa(J)-25 b(.)249 b(of)h(I.)p Fe(,)f(9\(05\):C0551,)
+g(2014.)25858 69325 y([2])553 b(F)-80 b(.)378 b(Morel)e(et)i(al.)768
 b(MISTRAL)375 b(&)i(ASTRAL:)g(tw)-10 b(o)377 b(CMOS)f(Pix)-15
-b(el)27573 66558 y(Sensor)334 b(architectures)g(suited)f(to)h(the)g
-(Inner)f(T)-35 b(racking)334 b(System)g(of)27573 67775
+b(el)27573 70543 y(Sensor)334 b(architectures)g(suited)f(to)h(the)g
+(Inner)f(T)-35 b(racking)334 b(System)g(of)27573 71760
 y(the)250 b(ALICE)e(e)-15 b(xperiment.)360 b Fa(J)-25
 b(.)249 b(of)h(I.)p Fe(,)e(9\(01\):C01026,)i(2014.)25858
-69436 y([3])553 b(Marc)250 b(W)-40 b(inter)-55 b(.)359
-b(Personal)249 b(communication.)p eop end
+73421 y([3])553 b(Marc)250 b(W)-40 b(inter)-55 b(.)359
+b(Pri)-25 b(v)g(ate)250 b(communication.)p eop end
 %%Trailer
 
 userdict /end-hook known{end-hook}if

diff --git a/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.tex b/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.tex
index c2f4737db5134b19f15a16dfeb67794976406e6e..4a3c78a70524de5ea9500b348f8d0002dbc6bffa 100644 (file)
--- a/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.tex
+++ b/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.tex
@@ -32,21 +32,21 @@
 %85747 Garching, Germany}
 \maketitle
 %\section{Introduction}
-The CBM-experiment will study the phase diagram of hadronic matter in the region of highest baryon densities by means of rare probes like open charm particles. Reconstructing those particles calls for a vertex detector providing a unique combination of excellent spatial resolution, light material budget and high rate capability. To match those requirements, we intend to use CMOS Monolithic Active Pixel Sensors, which are developed by the PICSEL group of IPHC Strasbourg and tested at the IKF Frankfurt within an common R\&D project. \newline
-A first fully integrated sensor, MIMOSA-28, was developed in the AMS $0.35\ \upmu \rm m$ CMOS process and it is used for data taking in the STAR-HFT since 2014. However, this sensor does not match the requirements of CBM in terms of radiation tolerance and readout speed. Therefore, the sensor architecture was migrated to a novel $0.18\mum$ process. This process was found to provide a higher tolerance to ionizing radiation \cite{IWORID2013}. Moreover, its higher packing density allows for reading two lines in parallel, which accelerates the readout by a factor of two with respect to the elder design. \newline
+The CBM-experiment will study the phase diagram of hadronic matter in the region of highest baryon densities by means of rare probes like open charm particles. Reconstructing those particles calls for a vertex detector providing a unique combination of excellent spatial resolution, light material budget and high rate capability. To match those requirements, we intend to use CMOS Monolithic Active Pixel Sensors, which are developed by the PICSEL group of IPHC Strasbourg and eveluated at the IKF Frankfurt within an common R\&D project. \newline
+A first fully integrated sensor, MIMOSA-28, was developed in the AMS $0.35\ \upmu \rm m$ CMOS process and it is used for data taking in the STAR-HFT since 2014. However, this sensor does not match the requirements of CBM regarding radiation tolerance and readout speed. Therefore, the sensor architecture was migrated to a novel $0.18\mum$ process. This process was found to provide a higher tolerance to ionizing radiation \cite{IWORID2013}. Moreover, its higher packing density allows for reading two lines in parallel, which accelerates the readout by a factor of two with respect to the elder design. \newline
 In 2014, a first fully integrated prototype sensor (FSBB-M0) was realized in the new process \cite{StrasbourgPaper2014Mistral}. The sensor was realized in two flavors (FSBB-M0a and FSBB-M0b), which differ slightly in the dimensions of some transistors. It features $416 \times 416$ pixels of $22 \times 33 \mum^2$ pitch and it is read out within $40 \mus$ via a pair of discriminators at the end of each column. Hereafter, the digital data is zero-suppressed and sent out via two 320 Mbps digital links. The sensitive surface of the FSBB is  $13.7\times9.2 ~\rm mm^2$. The final sensor of the CBM-MVD will presumably consist of three FSBBs.
 \begin{figure}[htb]
 %\centering
 \hspace*{-0.75cm}
 \includegraphics[width=0.6\textwidth]{TN-FPN}
 \vspace*{-0.75cm}
-\caption{TN and FPN measurement of a subset of 17 chips}
+\caption{Temporal noise and fixed pattern noise measurement of a subset of 17 similar chips.}
 \label{fig:figure1}
 \end{figure}
-The FSBB-M0 was tested at the CERN-SPS and provided a detection efficiency of $\gtrsim 99,5\%$, a dark rate of $\lesssim 10^{-5}$ and a spatial resolution of $<5 \mum$ in both dimensions \cite{MarcPersonalCommunication}, which matches the requirements of CBM. \newline
-To test the robustness of the design and to estimate the production costs for the CBM-MVD, we measured the production yield of the FSBB. In accordance with our experience, we assumed that production mistakes would turn into a significant deterioration of the noise of the sensors. To spot such deteriorations, a total of 25 sensors was bonded on PCB and operated with a suited readout system. The temporal noise (TN) of the individual pixels was derived by means of a threshold scan. Moreover, we measured the fixed pattern noise (FPN), which is caused by the offset of the dark signal of the pixels. \newline
+The FSBB-M0 was tested at the CERN-SPS and provided a detection efficiency for minimum ionizing particles of $\gtrsim 99,5\%$, a dark rate of $\lesssim 10^{-5}$ and a spatial resolution of $<5 \mum$ in both dimensions \cite{MarcPersonalCommunication}, which matches the requirements of CBM. \newline
+To test the robustness of the design and to estimate the production costs for the CBM-MVD, we measured the production yield of the FSBB. In accordance with our experience, we assumed that production mistakes would turn into a significant deterioration of the noise of the sensors. To spot such deteriorations, a total of 25 (17 FSBB-M0a and 8 FSBB-M0b) sensors was bonded on PCB and operated with a suited readout system. The temporal noise (TN) of the individual pixels was derived by means of a threshold scan. Moreover, we measured the fixed pattern noise (FPN), which is caused by the offset of the dark signal of the pixels. \newline
 The results of the study on the FSBB-M0a is shown in figure~\ref{fig:figure1}. We found all sensors tested to be operational and they provided a $\rm TN=(0.70\pm 0.05) ~\rm mV$ and $\rm FPN=(0.73\pm 0.14) ~\rm mV$. Only one of the tested sensors showed a higher FPN of $\sim 1.2~\rm mV$, which might still be acceptable. Similarly good results were observed with the eight FSBB-M0b tested, which all found operational (not shown).\newline
-We conclude that a first full size sensor matching the requirements of CBM in terms of surface, data rate and spatial resolution is available now. Moreover, the design mostly reaches out specification in terms of readout speed. Measurements demonstrated the sensor to provide good performances for Minimum Ionizing Particle detection and the production yield was found to exceed 95\%.
+We conclude that a first full size sensor meets the requirements of CBM regarding surface, data rate and spatial resolution. Moreover, the design mostly reaches out specification in terms of readout speed. Measurements demonstrated the sensor provide good performances for minimum ionizing particle detection and the production yield was found to exceed 95\%.
 
  
 \bibliographystyle{plain}