From f4cf4c90d9c65b70e2c5836458d2c4f4d3114819 Mon Sep 17 00:00:00 2001
From: Benjamin Linnik <blinnik@jspc28.x-matter.uni-frankfurt.de>
Date: Tue, 10 Feb 2015 17:35:46 +0100
Subject: [PATCH] Commit after M. Deveaux' review

---
 ...bericht2014_Linnik-FSBB-GSIbericht2014.pdf |  Bin 83453 -> 82626 bytes
 ...sbericht2014_Linnik-FSBB-GSIbericht2014.ps | 1798 ++++++++---------
 ...bericht2014_Linnik-FSBB-GSIbericht2014.tex |   21 +-
 GSI_2015_Linnik/Lit.bib                       |    6 +
 4 files changed, 900 insertions(+), 925 deletions(-)

diff --git a/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.pdf b/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.pdf
index bf624441a3c4176f722806d7b38b31b09f84503e..15d40bfa4b19fbaa792e18d0c4de9f55454a0261 100644
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diff --git a/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.ps b/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.ps
index 36846f8..3f99091 100644
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+%%EndFont 
+%%BeginFont: MSAM10
+%!PS-AdobeFont-1.0: MSAM10 003.002
+%%Title: MSAM10
+%Version: 003.002
+%%CreationDate: Mon Jul 13 16:17:00 2009
+%%Creator: David M. Jones
+%Copyright: Copyright (c) 1997, 2009 American Mathematical Society
+%Copyright: (<http://www.ams.org>), with Reserved Font Name MSAM10.
+% This Font Software is licensed under the SIL Open Font License, Version 1.1.
+% This license is in the accompanying file OFL.txt, and is also
+% available with a FAQ at: http://scripts.sil.org/OFL.
+%%EndComments
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+/FontName /MSAM10 def
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+/UniqueID 5031981 def
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+/version (003.002) readonly def
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+/FullName (MSAM10) readonly def
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+end readonly def
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+{restore}if
+%%EndFont 
 %%BeginFont: CMR7
 %!PS-AdobeFont-1.0: CMR7 003.002
 %%Title: CMR7
@@ -1194,6 +1690,7 @@ end readonly def
 /Encoding 256 array
 0 1 255 {1 index exch /.notdef put} for
 dup 50 /two put
+dup 53 /five put
 readonly def
 currentdict end
 currentfile eexec
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@@ -1432,14 +1936,8 @@ end readonly def
 /Encoding 256 array
 0 1 255 {1 index exch /.notdef put} for
 dup 58 /period put
-dup 61 /slash put
-dup 70 /F put
-dup 78 /N put
-dup 80 /P put
-dup 84 /T put
-dup 99 /c put
-dup 107 /k put
-dup 109 /m put
+dup 59 /comma put
+dup 60 /less put
 readonly def
 currentdict end
 currentfile eexec
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@@ -1731,7 +2179,7 @@ FontDirectory/CMR10 known{/CMR10 findfont dup/UniqueID known{dup
 end readonly def
 /Encoding 256 array
 0 1 255 {1 index exch /.notdef put} for
-dup 10 /Omega put
+dup 37 /percent put
 dup 40 /parenleft put
 dup 41 /parenright put
 dup 48 /zero put
@@ -1745,9 +2193,11 @@ dup 55 /seven put
 dup 56 /eight put
 dup 57 /nine put
 dup 61 /equal put
-dup 77 /M put
+dup 70 /F put
+dup 78 /N put
+dup 80 /P put
+dup 84 /T put
 dup 86 /V put
-dup 98 /b put
 dup 109 /m put
 dup 115 /s put
 readonly def
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-%%CreationDate: Mon Jul 13 16:17:00 2009
-%%Creator: David M. Jones
-%Copyright: Copyright (c) 1997, 2009 American Mathematical Society
-%Copyright: (<http://www.ams.org>), with Reserved Font Name CMMI12.
-% This Font Software is licensed under the SIL Open Font License, Version 1.1.
-% This license is in the accompanying file OFL.txt, and is also
-% available with a FAQ at: http://scripts.sil.org/OFL.
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-%%Title: CMR12
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-%%CreationDate: Mon Jul 13 16:17:00 2009
-%%Creator: David M. Jones
-%Copyright: Copyright (c) 1997, 2009 American Mathematical Society
-%Copyright: (<http://www.ams.org>), with Reserved Font Name CMR12.
-% This Font Software is licensed under the SIL Open Font License, Version 1.1.
-% This license is in the accompanying file OFL.txt, and is also
-% available with a FAQ at: http://scripts.sil.org/OFL.
-%%EndComments
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-eop end
+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
 %%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 d0995de..c2f4737 100644
--- a/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.tex
+++ b/GSI_2015_Linnik/Jahresbericht2014_Linnik-FSBB-GSIbericht2014.tex
@@ -18,7 +18,7 @@
 %%
 %\setlength{\titleblockheight}{33mm}
 \begin{document}
-\title{Yield studies of full-integrated sensors, produced in a novel $0.18\mum$ process\thanks{This work has been supported by BMBF (05P12RFFC7), HIC for FAIR and GSI.}}
+\title{Yield studies on a fully integrated sensor for the CBM-MVD\thanks{This work has been supported by BMBF (05P12RFFC7), HIC for FAIR, HGS-HIRe and GSI.}}
 \author[1,2]{B. Linnik}
 \author[1]{D. Doering}
 \author[1]{M. Deveaux}
@@ -32,10 +32,9 @@
 %85747 Garching, Germany}
 \maketitle
 %\section{Introduction}
-The fixed-target CBM-experiment at the future research facility FAIR will study strongly interacting matter in heavy ion collisions. It will covers the high dense region of the phase diagram complementary to the collider experiments STAR and PHENIX experiments at RHIC and ALICE at LHC.\newline
-One interesting probe among others are heavy-flavor hadrons. In order to study them close to their production threshold precise vertex reconstruction and high rates are required. None available sensor technology was able to fulfill these requirements. CMOS Monolithic Active Pixel Sensors (MAPS) feature excellent spatial resolution and ultra-light material budget compromising with moderate radiation hardness and read-out speed. Intense R\&D is being carried out within a joint research program of the PICSEL group of the IPHC Strasbourg and the IKF Frankfurt in order to improve their radiation hardness and read-out speed to the needs for the application in the vertex detector of CBM. Synergies with the vertex detector of STAR and ALICE are used to share the R\&D. \newline
-Using the AMS-0.35-technology, a first vertex detector based on CMOS sensors is taking data in the heavy-ion experiment STAR since 2014. Achieving the required non-ionizing radiation hardness, the ionizing radiation hardness and read-out speed of sensors in the AMS-0.35-process was not sufficient for the application in the vertex detectors of ALICE and CBM. Therefore, a novel $0.18\mum$ process was exploited and found to provide a higher tolerance to ionizing radiation \cite{IWORID2013}. Moreover, the smaller feature size allows for the integration of a more complex logic into the pixel providing a faster read-out.\newline
-In 2014, the first full-integrated prototype sensor FSBB-M0 was designed and tested. Three of such sensor units will compose one full sensor to be used in the vertex detector. The $9{.}2 \times 16.9~\rm mm^2$ large FSBB-M0 sensors are made in the novel $0{.}18 \mum$ process, based on a high resistivity ($~1 k\Omega cm$) epitaxial layer of $18 \mum$ thickness. The chip consists of $416 \times 416$, $22 \times 33 \mum^2$ sized pixels connected to 208 end-of-column discriminator pairs. Therefore two rows are read simultaneously in rolling shutter mode (200 ns per 2 rows). The read-out provides a normal operation mode with zero-suppression and a data output of $640~\rm Mb/s$. The chip provides also different test modes for the analog and digital part to characterize the pixels and the discriminators.\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 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
+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}
@@ -44,12 +43,12 @@ In 2014, the first full-integrated prototype sensor FSBB-M0 was designed and tes
 \caption{TN and FPN measurement of a subset of 17 chips}
 \label{fig:figure1}
 \end{figure}
-The FSBB-M0 sensor has two matrices (FSBB-M0a and FSBB-M0b) and each is divided in two submatrices. They differ in diode size or have different input transistor dimensions of the in-pixel pre-amplifier \cite{StrasbourgPaper2014Mistral}.\newline
-Extensive yield studies were performed measuring the s-curves to compare the temporal noise (TN) and the fixed-pattern-noise (FPN) of the sensors. A total set of 25 FSBB-M0 chips have been characterized. A subset of 17 sensors are shown in figure~\ref{fig:figure1}. They provide a remarkably similar performance of a $TN=(0.70\pm 0.05) ~\rm mV$ and $FPN=(0.73\pm 0.14) ~\rm mV$. The exception is one outlier chip number 12. However its FPN of $1.2~\rm mV$ might also be still acceptable. In conclusion, the new architecture based on the $0{.}18 \mum$ process has an excellent yield and a reliable behavior. \newline
-% The benefit of the in-pixel in comparison to the column-wise discrimination is the lower power consumption ($~14 \muA$ instead of $~120 \muA$ per pixel -- the analog buffer doesn't have to drive the long distance along the column) and the faster readout times ($15 \mus$ read-out time in comparison to $30 \mus$ -- the A-D conversion can be halved due to the small local parasitic). On the other hand, the in-pixel discrimination is an innovative architecture which has to be tested and validated more, while the column wise discrimination is a mature technology, which was already successfully implemented and used in previous MIMOSA chips.
-%For the discrimination in the columns, . 
-%A sample transfer function study is shown in \ref{fig:figure1}.  Each curve discribes the fire behavior of one pixel averaged over time as a function of the reference voltage. The distribution of the slopes is called temporal noise and is shown in \ref{fig:figure2}. %The two discrimination modes, as well as different transitor sizes were tested: 
-%For the discrimination in the pixel one observes a distribution with two peaks, it seems that there are two main types of pixel behavior. To investigate the fixed pattern noise, the behavior of the pixels for different threshold voltages 
+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 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\%.
+
+ 
 \bibliographystyle{plain}
 \bibliography{Lit}
 \end{document}
diff --git a/GSI_2015_Linnik/Lit.bib b/GSI_2015_Linnik/Lit.bib
index bd98587..cfb7360 100644
--- a/GSI_2015_Linnik/Lit.bib
+++ b/GSI_2015_Linnik/Lit.bib
@@ -16,6 +16,12 @@ pages = "432 - 436",
 year = "2010",
 
 }
+
+@misc{MarcPersonalCommunication,
+  author = "Winter, Marc",
+  howpublished = "Personal communication."
+}
+
 @MASTERSTHESIS{PaulMaster,
 mylabel="Scha13",
   author  = {{Scharrer}, P.},
-- 
2.43.0