鶴 剛(京大)
[email protected]
森浩二(宮崎大),幸村孝由(工学院),田中孝明(京大)
中島真也,松村英晃(京大),武田彩希,新井康夫(
KEK
)20131213_SOI新学術WS_B01_XRPIX_v0.key
計画研究 B01
宇宙最初期ブラックホールの探査 研究を実現する衛星搭載
X 線精密イメージングの開拓
1
Neal Jackson, STScI and NASA
電波
Chris Carilli and NRAO/AUI
X線A. Wilson & A. Young, P. Shopbell, CXC, NASA
白鳥座
A
50
万光年超巨大ブラックホール
(太陽の 100 万倍から 10 億倍)
銀河の中心のブラックホール
銀河とブラックホールの共進化
銀河 : 地球 BH : 砂粒
2
最も暗いのが初期
BH SOIPIX
CCD
ざらざらは全て 背景ノイズ
学術的背景 3
宇宙初期現在
宇宙最初期
BH =
中質量BH
第1世代の星恒星質量
BH
や 星の合体原始
BH
これを発見する
超巨大
BH
Trajectory of particles inside the CCD
Irradiation of 1-MeV electrons onto the CCD
Non X-ray background of Suzaku XIS (BI)
Due to high energy particles on orbit.
4
X線SOIPIX素子 (スタック) 視野
非X線バック グラウンド (宇宙線が作る
2次的放射線)
アクティブ シールド 硬X線 軟X線
衛星搭載のFPGA・計算機 ● イベント駆動読み出し
● 非同時計数 (非X線BGDの除去) ● X線エネルギー・位置・時刻計測
1分
SOIPIX :イベント駆動読み出し型
•
反同時計数背景ノイズ2桁下げる.
• X
線が到達した瞬間にトリガ出力.•
アクティブシールドが同時に信号出力 宇宙線だと判断し,捨てる.•
アクティブシールドが同時に信号無し X線だと判断し,アナログ信号処理•
他の性能:撮像,分光(読み出しノイズ),検出感度は
CCD
と同等(以上).5
XRPIX Series - Road Map - 6
XRPIX1 XRPIX1b 2.4 mm 2.4 mm
1.0mm 1.0mm
XRPIX2b 4.5mm
6.0 mm XRPIX2
6.0 mm 4.0mm
First Model Trigger Output
2.9 mm 2.9 mm XRPIX3 XRPIX3b
A-R-Tec PROPRIETARY/CONFIDENTIAL 2.4mm 5
2.4mm XRPIX
ΔΣ-type ADC
2.4 mm
Middle Size Buttable
Charge
Sensitive AMP
1.0mm 1.0mm
2010 2011 2012 2013 2014
10μsec
5年間の目標:衛星搭載品を直ちに製造開始 7
項目 目標 現状 テクノロジ
超低
BGD 5e-5 c/s/
keV/10mm
角不明 トリガ出力
: OK
アクティブシールド
:
未 広帯域0.3 - 40keV 1.5 ? - 40keV >300μm: OK
裏面不感層
0.1μm:
未 精密分光 要求<10e-
ゴール
< 3e-
64e- (rms) XRPIX2 SmallPix
True-CDS:
未 プリアンプ:
未Built in ADC:
未 裏面のCCE
暗電流<2pA/cm2 200pA/cm2
(-40℃)
回路からの(?)
リークを下げる精密撮像
30-60μm 30.6μm,
61.2μm
ピクセル内のCCE
広視野
20mm
角3.9mm
角 モザイク可能(XRPIX2b)
デッド領域は出来るだけ小さく.
裏面
CCE: A01
班,二重活性層によるイベント駆動True-CDS: A02
班1分
チーム( cf. 申請書)
•
全員X線天文分野,X線CCD
の経験あり•
鶴 剛(京大):総括,X線素子開発•
森浩二(宮崎):硬X
線性能評価•
幸村孝由(工学院):軟X
線性能評価•
田中孝明(京大):イベントドリブン読み出し,バックグラウ ンド評価•
中嶋大(阪大:
連携):ADC
• FY2014
から,KEK
武田彩希さんをPD
として雇用(京大)
素子・回路等の設計・製作,性能評価
•
各大学での大学院生.修論1
本/
年(京大)を目指す.• B01
チームで,投稿論文2
本/
年を目指す.8
1分
難しいと思っている事
•
最大の難関:低ノイズ化.要求=10e-(rms)
,ゴール=3e- (rms)
•
逐次読み出しではなく,イベントドリブン読み出しで実現.•
トリガも低い閾値ではなければいけない.目標= 0.3keV
.•
裏面の不感層と電荷収集効率(CCE)
•
いくつか有望な方法を試す• 1keV
以下のX線の評価•
実験室で手軽に強く質の良い軟X
線を得る方法.•
まだ手を付けていない事への不安(暗電流,BGD
,大型化)9
XRPIX の紹介と現在
10
XRPIX1: Pixel Circuit
STORE
CDS C 100fF Sample C
100fF
Sensor
Trigger output Trigger
CDS
Comparator
CDS _VRST VTH VDD18
PD_VRST
COL_AMP OUT_BUF
SF1 SF2
VDD18
GND18
GND18
Sample /Store
Sensor C
Analog output Analog
Readout
G=1 G=1
TEST_ECA EOXX
11
ピクセル回路
XRPIX1b-CZ : Event Driven Readout
・
COL Hit Add. Resister
Ro w H it Ad d. R es is ter
COL Readout ADDR COL Amp
RO W R ea do ut AD D R
TRIG_O O R
TRIG_COL TRIG_ROW
A_OUT
①
① ②
X-ray !
F P G
A
ADC
Takeda et al., IEEE Accepted (2012)
③
④
④
⑤
12
イベント駆動
TRIG_OUT SCLK
CA[151-0]
RA[151-0]
Trigger !
Address of Triggered Pixel
Trigger Address Readout Clock
Row Column
4μsec
Takeda et al., IEEE (2013)
- Event-driven mode basically operates.
- Capacity of event rate >1kHz.
- The gain is different. There is offset.
- Due to interference between analog and digital circuits
XRPIX2b-CZ : Event-driven Readout Mode 13
Pulse Hight (ch)
X-ray Energy (keV) Event-Driven
5.4 μV/e-
Offset
Frame-Mode 7.0 μV/e-
Fe-55 (5.9keV)
Pulse Hight (ch)
Note: Pixel gain is not calibrated.
Preliminary
Preliminary 22keV X-ray detection
Cd-109
イベント駆動
XRPIX1b-FZ(2012)-FI (7kΩcm) : Depletion Depth
back_bias 200V
• Counting Rate of 22keV X-ray (Cd-109) as a function of VBB.
(Attenuation Length = 1200μm > Physical Thickness = 500μm.)
• The data follow the expected slope of depletion VBB^1/2.
• Full Depletion of 500μm is reached at VBB=200V.
20130502_matsumura.pdf
Depletion VBB^1/2
14
Preliminary
Physical Thickness 500μm (not 260μm)
Counting Rate of 22keV X-ray
200V
空乏層
QE of LBNL’s BI-SOIPIX / SOImager-2-CZ-BI
Deplation 73±2μm Dead Layer 0.6±0.2μm
Battaglia+12 NIM-A
※
これは我々の素子ではなく,同じウェハを使用した別の素子です.LBNL “Pizza Process” 15
裏面照射
XRPIX2-CZ-FI (Small Pixel) : Spectrum in the frame mode
Nakashima et al., 2012, NIM A submitted
0 2 4 6 8 10 12 14 16 18 20
0 20 40 60 80 100 120 140
0 10 20
0 150
50 100
X-ray Energy (keV)
P ulse H igh t (ch)
XRPIX2 Gain 6.5 µV/e-
XRPIX1 Gain 3.6 µV/e-
Observed Readout
Noise Fano
Noise Pixel-Pixel Gain
Dispersion 1% Sum Cu Kα 656 eV 548 eV (FWHM)
64 e-(rms)
139 eV 255 eV 620 eV
Mo Kα 800 eV
548 eV (FWHM)
64 e-(rms) 205 eV 553 eV 805 eV
PH [ADU]
40 60 80 100 120 140 160
PH [ADU]
40 60 80 100 120 140 160
0 200 400 600 800 1000 1200 1400 1600 1800
40 80 120 160
Pulse Hight (ch = 244 µV) 1000
500 1500
C u C oun t
100 200
0 0
M o C oun t
Cu Kα (8.0 keV) Mo Kα (17.4 keV)
Mo Kβ (19.6 keV) 656 eV
FWHM
800 eV FWHM
Readout Noise 100→64e-
16
エネルギー分解能
Charge Amp Feedback
Capacitance 1fF Sensor
Node
Reset SW
XRPIX3/3b : Pre Amp in Each Pixel 17
• A charge sensitive amp (CSA) in every pixel in order to increase the gain and improve energy resolution.
• CSA is basically the same that developed in another SOIPIX (PIXOR).
• Readout noise = 64e (rms) → ....
Protection Diode
エネルギー分解能
IEEE NSS/MIC2013
ソウル前日...
2013/10/26 13:38
1 2 3 4 5 6 7 8
0 50 100 150 200 250 300 350 400 450 500
Energy (keV)
Co un ts
55
Fe Spectrum
5.9 keV
FWHM : 8 % (470 eV) FWHM : 14 % (830 eV)
6.4 keV
CSA Pixel
Normal Pixel
(solid) : fitting line (dot) : data
.
Development of New Circuit for X-ray Astronomical SOI Pixel Detector
Ayaki Takeda (SOKENDAI / KEK) Y.Arai (KEK / IPNS)
T.G.Tsuru, T.Tanaka, S.Nakashima, and H.Matsumura (Kyoto Univ.) For X-ray Astronomy
SOI Pixel Detector (SOIPIX)
Design Specification of XRPIX3
2013 IEEE NSS @ COEX, Seoul, Korea - 2013.10.30 WED -
Summary
- We have been developing SOIPIX for future X-ray astronomical satellite mission.
- A new device, “XRPIX3” was designed in order to improve energy resolution.
- By CSA pixel circuit, we succeeded in the improvement of energy resolution.
Normal -> 14 % (FWHM) , CSA -> 8 % (FWHM) @ 5.9 keV (
55Fe) - We will optimize CSA circuit for the next design.
Please contact us if you are interested. -> http://rd.kek.jp/project/soi/
mail: yasuo.arai @ kek.jp (Yasuo Arai (PL)), atakeda @ post.kek.jp (Ayaki Takeda)
X-rays
New Circuit
First prototype of XRPIX CSA circuit.
Comparison of Normal and CSA pixel.
(Fabricated Jun, 2013) Components
- Chip Size : 2.9 mm sq.
(Effective Area : 1.0 mm sq. ) - Pixel Size : 30 µ m sq.
- # of Pixel : 32 x 32 (= 1,024)
- Thickness of Sensor Layer : 260 µm - Sensor Wafer : 700 Ω cm
-> Czochralski (CZ) The performance required of a future X-ray astronomical satellite
is the following ...
- FWHM ≤ 140 eV @ 6 keV (Readout Noise ≤ 10 e-) - ≤ 100 µ m pitch pixel
- ~10 µ s per event readout
- Wide energy range : 0.3 - 40 keV
In order to achieve these requirement, we have been developing the SOIPIX
with a trigger information output function.
(Event-Driven Readout mode) -> XRPIX Series
We aim at realization with a spectroscopy system as shown in the right figure.
- A monolithic pixel detector with silicon-on-insulator (SOI) Technology -> 0.2 µ m fully-depleted (FD)-SOI pixel process
Processed by LAPIS Semi. Co. Ltd.
NP02-124
SOIPIX Advantages
- No mechanical bump bonding
-> High density, Low parasitic capacitance, High sensitivity
- Standard CMOS circuits can be built
- Based on industrial standard technology
Basic Components
-> Tr Si Layer : 40 nm, BOX : 200 nm, Sensor Layer : 100 ~ 725 µ m
Column Amp. (COL_AMP) Column Address Decoder
Row Address Decoder
0
31 Column Shift Register (32 bit)
Row Shift Register (32 bit) TRIG_OUT
OR
31
ANALOG OUT
TRIG_ROW
TRIG_COL
32 x 32 Pixel Array 1Pixel = 30 µm x 30 µm
Normal Charge Sensitive
Amp.
0 5 10 15 20 25 30
0 50 100 150 200 250 300 350 400 450 500
Energy (keV)
Pu ls e H ei gh t ( ADU )
Normal Pixel 5.3 µV/e-
CSA Pixel 18.2 µV/e-
Energy Calibration
Our Works with XRPIX
First Results of XRPIX with CSA
The difference between Normal and CSA pixel is a circuit configuration of preceding stage.
- Normal : Source Follower (SF) by Common-Drain of a PMOS transistor
- CSA : CSA by Common-Source of a NMOS transistor and a feedback capacitance (1 fF)
The signal charge can overcome the circuit noise of following stage electronics by CSA.
Then, the readout noise decreases.
We have been developing 4 devices and shown some basic performances.
- X-ray responsivity of XRPIX (SOIPIX) -> XRPIX1/1b [1], [2]
- Difference in pixel size or structure -> XRPIX2 [3]
- Event-Driven readout mode -> XRPIX1b [4]
The basic function of XRPIX is realized by our previous works.
Next step is improvement in spectroscopy performance.
x 3.4 Note : Pixel gain was not calibrated.
ANALOG OUT
VTH TRIG OUT
ROW_READ COL_READ
COL_AMP OUT_BUF SF
CDS_RST
CDS Cap.
Sample Cap.
STORE SF
PD_RST
CDS_RSTV PD_RSTV
Protection Diode
VDD18 VB_SF
PD
Sense-node
GND
Pixel Circuit
Column Readout
CDS + Trigger Circuit
TRIG_COL (SR)
TRIG_ROW (SR) TRIG_OUT (OR) Trigger Info. Output
Comparator
GND
&
Normal Pixel
ANALOG OUT
CDS_RSTV TRIGGER
H/L OUT
ROW_READ COL_READ
COL_AMP OUT_BUF SF
CDS_RST
CDS Cap.
Sample Cap.
STORE
AMP.
PD_RSTProtection Diode
VDD18 VB_SF
PD
Sense-node
GND
Pixel Circuit
Column Readout
# AMP. # + CDS + Trigger Circuit
TRIG_COL (SR)
TRIG_ROW (SR) TRIG_OUT (OR) Trigger Info. Output
GND
&
Feedback Cap.
VTH
Comparator
CSA
CSA Pixel Circuit
CSA Pixel Layout
MIM Cap. (comp. 1) MIM Cap. (comp. 2)
MIM Cap. (sample) MIM Cap. (CDS)
1 pixel area
trigger circuit
trigger circuit trigger circuit
14 μm
30 µ m
PD BPW
Feedback Cap. (1 fF) analog signal circuit
Charge sensitive amplifier (CSA) in each pixel in order to increase the gain and improve energy resolution.
Energy Calibration 55 Fe Spectrum
(1 ADU = 244 µ V)
Reference
[1] S.G.Ryu et. al., IEEE TNS., Vol.58, Issue:5, pp.2528-2536, 2011.
[2] S.G.Ryu et. al., IEEE TNS., Vol.60, Issue:1 , pp.465-469, 2013.
[3] S.Nakashima et. al., Phys. Procedia, Vol.37C, pp.1392-1399, 2013.
[4] A.Takeda et. al., IEEE TNS., Vol.60, Issue:2, pp.586-591, 2013.
Our New Device -> “XRPIX3”
- The pixel circuit with CSA works good. (3.4 times higher gain)
Gain (from left fig.) : Normal -> 5.3 µ V/e- , CSA -> 18.2 µ V/e- - The CSA Pixel succeeded in improvement of energy resolution.
Comparison of
55Fe energy spectrum at Normal and CSA (right fig.) @ 5.9 keV : Normal -> 14 % (FWHM) , CSA -> 8 % (FWHM)
- However, the experimental value of a gain differs from a design value.
Gain : Design value -> 50 µV/e- , Experimental value -> 18.2 µV/e- It has influence of parasitic capacitance.
(-50
oC)
These results are reflected on the next design.
X-ray
hard soft cosmic ray (non-X-ray BG) field of view
active shield
onboard processor
・anti-coincidence (NXB rejection)
・hit-pattern selection (NXB rejection)
・direct pixel access (X-ray readout) XRPIX
エネルギー分解能
18
IEEE NSS/MIC2013
ソウル前日...
2013/10/27 05:30
1 2 3 4 5 6 7
0 20 40 60 80 100 120 140 160 180
1 2 3 4 5 6 7
0 20 40 60 80 100 120 140 160 180
1 2 3 4 5 6 7
0 20 40 60 80 100 120 140 160 180
1 2 3 4 5 6 7
0 20 40 60 80 100 120 140 160 180
1 2 3 4 5 6 7
0 20 40 60 80 100 120 140 160 180
遂に時は来た!
33e (rms), 300eV (FWHM)
エネルギー分解能
19
さらなる展開
図4:製作するカメラの模式図.PINダイオード で構成するアンチカウンタの中にSOIPIXを入 れる.高エネルギー粒子PINとSOIPIXの両方 に同時に信号を作るので,非X線として除去 可能(非同時計数).
2次元符号化マスク 入射X線
SOIPIX
PINダイオード
PINダイオード PINダイオード
非 X 線 バ ッ ク グ ラ ウンド(高 エ ネ ル ギ ー電子等)
5cm
大立体角X線監視観測
宇宙の爆発現象を捉え,即時通報する
暗黒物質探査実験
XRPIX 1kg
シンチレーター
1-10GeV
の低質量:
探査不十分 神戸大 身内さんと共同研究20
まとめ
SOI Pixel Project : General View
Feb. 28, 2011 SOI International
Review Meeting Yasuo Arai, KEK [email protected]
http://rd.kek.jp/project/soi/
/TEG
URL: http://www.a-r-tec.jp Email: [email protected]
A-R-Tec
Analog and RF Technologies