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Hypernuclear Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment 3. Hyperball-J – Readout and DAQ J-PARC DAQ WS Oct. 14, 2005

Hypernuclear Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

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Page 1: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Hypernuclear Spectroscopy Experimentsand

Waveform Readout of Germanium Detectors

H. TamuraTohoku Univ.

1. Present Status and Hyperball22. DAY-1 experiment3. Hyperball-J – Readout and DAQ

J-PARC DAQ WS Oct. 14, 2005

Page 2: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

1.1. Present StatusPresent Status and Hyperball2 and Hyperball2

Page 3: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

PLB 579 (2004) 258

Nucl.Phys.A 754 (2005) 155c

Nucl.Phys.A 754 (2005) 155c

PRC 65 (2002) 034607

PRL 93 (2004) 232501

We want to publish “Table of Hyper-Isotopes”

The bible for nuclear physics

Present status of hypernuclear spectroscopy

Page 4: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

1. YN, YY interactions -> Unified picture of B-B interactions, Understand short-range nuclear forcesN spin-dependent forces, force, …

    Understand high density nuclear matter (n-star)         2. Impurity effects in nuclear structure   Changes of size/shape, symmetry, cluster/shell structure,.. B(E2) -> shrinking effect

3. Medium effects of baryons probed by hyperons B(M1) -> in nucleus

Motivation of Hypernuclear Spectroscopy High-precision (E ~ a few keV) spectroscopy with Ge detectors

At a short distance

Page 5: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Hyperball (Tohoku/ Kyoto/ KEK, used in 1998-2002)

Side view

BNL E930 setup

Page 6: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Hyperball2

Single Ge (r.e.=60%)

+ BGO(6PMT) x14

Clover Ge (4ch) (r.e. >120%)

+(BGO(12PMT)) x6

Ge: 38 ch, BGO: 156 ch

Peak eff.

~ 2.5% -> 5% at 1 MeV

efficiency x 4

Used at CYRIC (Tohoku) for ordinary nuclear spectroscopy 2005.6--7

Being used at KEK for E566 ( spectroscopy of 12C / 11

B) 2005.9--10

Page 7: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Hyperball2 at KEK-PS K6 Line (E566)

SKSHyperball2

K6 Q10

Page 8: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

2. DAY-1 experiment2. DAY-1 experiment

Page 9: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Proposal for DAY1 “Hypernuclear Spectroscopy by (K-,-

)”

Light (survey study)

・ A=4 - ~30 all possible targets 4He, 13

C/ 14N, 20

Ne, 23Na, 27

Al / 28Si, …

(-> Table of hyper-isotopes, N interaction, ...)

Light (detailed study for some important hypernuclei )

・ coin, , polarization -> level scheme, spin-parity

・ DSAM -> B(E2), B(M1)

Hyperfragments ( K-, (-) ), 0.8 GeV/c

・ Light targets (9Be,10B, 11B, 12C) 7He, 8

Li, 8Be, 9

Li, 9B,... (CSB,..)

Medium and heavy p=0.8--1.8, large -> large q

・ E1(p->s) ~4 MeV 89Y, 139

La, 208Pb (p-wave N int.,..)

K1.1+ SPESII

pK= 1.1 and 0.8 GeV/c

12C (parity mixing states), 20

Ne (parity inversion),..9Be (B(E2)), 13

C (B(E2)), 11B (B(M1)), …

Total beam time to be estimated.

non-spin-flip spin-flip

K1.8 + SKS

pK= 1.1 and 1.8 GeV/c or

Page 10: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

K- 1.1 + 0.8 GeV/c

Beam and Setup (K1.1 case) Beamline: K1.1 1.2x107 K-/spill at 1.1 GeV/c K/ > 1

Spectrometer: SPESII p/p < 2 MeV (FWHM) ~ 20 msr Hyperball-J

~ 10% at 1 MeV

-

Page 11: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Expected transitions

12C (+,K+) 12C

SKS E~1.5 MeV(FWHM)

Simulation: K1.1, 10g/cm2, 120 hours

(1-b) Light hypernuclei --- example of 12

C

b

a

c

d

g

fe

h ijk

lm

no

p

cb

h

g

k

e j

if

a

l

d

Page 12: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

angular correlation

-> spin assignment

coincidence and angular co

rrelations

coincidence spectru

m

-> level scheme

coinc. with a (21- ->11

- )

coinc. with c (12- -> 21

- ) kh

fj

h k

c

12C: simulation

Page 13: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

3. Hyperball-J3. Hyperball-J--Readout and DAQ--Readout and DAQ

Page 14: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Hyperball-J●(Segmented) Super Clover (350%) x 14 (or normal x 32?) + old normal (60%) x8●Waveform readout●Fast suppression counters (BGO=>PWO)

~ 10% at 1 MeV (x4 of Hyperball) Rate limit ~2x107 particles /s (x5 of Hyperball) => Yield: x20 for single x80 for

PWO

Page 15: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Readout electronics at presentLow-Gain Transistor Reset Preamplifier Reset level ~150 MeV, 6V (gain~40mV/MeV) Fast reset time (~5 s) Resolution

2.2 -> 2.6 keV at 1.33 MeV

Ultra-High-rate Amp Pile up time = integration time (3 s) << normally: shaping time (3-6 s) x10 Fast recovery from reset (~15 s) Resolution 2.2 -> 2.6 keV at 1.33 MeV

pileup resetDead time = 6 s x 50 kHz + 20 s x 10 kHz 30% + 20% = 50%Trigger Rate ~ 500/spill(1 sec) x 2 k words in total

Page 16: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Example of Ge signals at a high rate

Shaper (0.5s) out

Gatedintegrator(GI) out

Preamp inhibit

pile up

reset

beam penetration

baselineshiftshaper

overload

GI dead GI dead

K6 (E566), 3M/1.5s, 15cm from beam

GI bad

Page 17: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Waveform readout method    Pileup decomposition and baseline correction by software Goals: single rate:100->500kHz, energy rate 0.5->2.5TeV/s beam limit: K6: 3x106/sec -> K1.1: 1.5x107/sec

Usual waveform method (Digital Signal Processor)

waveform digitizer ~14bit

~40MHz

Preamp. gain 40mV/MeV , Dynamic range 150 MeV-6V Required resolution < 1 keV = 0.04mV -> Digitizer resolution 150,000= 18bit -- impossible

Shaping, PZC, PH-ADC, time stampProcessing speed 200k ev/s

eg. XIA DGF

(We may use this waveform digitizer butwe should make software by ourselves.)

Page 18: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Waveform readout method – our case 

Hardware: technically OK, cheaper

Simulation(slow signal) 4s

2s

1s

High energy bg.~50 MeV

Nuclear -ray bg. ~1 MeV

We will take sample data in E566 with existing hardware -> software development -> optimize digitizer parameter

-> Design hardware

slowwaveform digitizer

slow amp

~1s

TFA ~0.1s

>12bit ~40MHz

Multi-hit TDClow-gain

transistor-resetpreamp

CFD

CFD out

Page 19: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Trigger rate and Data rate

Trigger rate (very rough estimate) AGS D6(E930): 200k K-/spill, (K-,-) tirg= 900 trig/spill, x 0.3 by Ge-hit OR

-> J-PARC (K1.1): 9M K-/spill, Hyperball-J x 0.3 -> 0.7 28000 trig/spill (At K1.8, K- intensity at 1.1 GeV/c is one order lower.)

Sever beam-through veto, sever Cerenkov cut to remove K decay x 1/2 PWO suppression in the trigger level x 1/3 PWO total-energy/multiplicity cut (remove 0) x 1/5 ? + Energy deposit tag (enhance hypernuclear events) if necessary Trigger rate < 1000 trig/spill

Data rate Waveform: [13bit x 20MHz x 20s ] x ( 5--20 Ge’s) x 1000 trig/spill ~ 2--8 kw/ev x 1000ev/spill = 4--16MB/spill Others: < 1kw/ev : negligible

Channels Ge: 134 -- 64 ch, waveform (13bit,20MHz) + multihitTDC PWO: 200--300ch, TDC + ADC

1st level 2nd level

2nd level

1st level

2nd level

1st level

Transfer data for Ge without PWO hit

Page 20: Hypernuclear  Spectroscopy Experiments and Waveform Readout of Germanium Detectors H. Tamura Tohoku Univ. 1. Present Status and Hyperball2 2. DAY-1 experiment

Things to be done Development of waveform analysis software -> How much improvement in high rate performance? -> Optimize digitizer parameters (resolution, sampling)

Shaper + Digitizer module Data transfer should be controlled using PWO info.

Data transfer scheme, Memory modules

“TFA with good BLR (equiv. ORTEC 579) + CFD” module or another digitizer (8bit,~100MHz) for timing info.? Trigger PWO discri. + FPGA module (TUL) ? PWO multiplicity: OK, PWO energy sum: + Linear F/I

Control / diagnostics module (HV control, alarm, Co pulsers,..)