Strangeness production around threshold region and a possibility with the new beam line and NKS2

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Strangeness production Strangeness production around threshold region around threshold region and and a possibility with a possibility with the new beam line and NKS2 the new beam line and NKS2 Masashi KANETA for the NKS2 collaboration Department of Physics, Tohoku Univ. [email protected]

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Strangeness production around threshold region and a possibility with the new beam line and NKS2. Masashi KANETA for the NKS2 collaboration Department of Physics, Tohoku Univ. [email protected]. Outlook of this talk. Introduction of the experiment Motivation - PowerPoint PPT Presentation

Transcript of Strangeness production around threshold region and a possibility with the new beam line and NKS2

Page 1: Strangeness production around threshold region and a possibility with  the new beam line and NKS2

Strangeness productionStrangeness productionaround threshold regionaround threshold region

andanda possibility with a possibility with

the new beam line and NKS2the new beam line and NKS2

Masashi KANETAfor the NKS2 collaboration

Department of Physics, Tohoku Univ.

[email protected]

Page 2: Strangeness production around threshold region and a possibility with  the new beam line and NKS2

Masashi Kaneta, Tohoku Univ. 2

Outlook of this talkOutlook of this talk

• Introduction of the experiment– Motivation

– Collaboration list

– Fruits of our study

• Physics topics– strangeness production

– model and data

• Experiment with Neutral Kaon Spectrometer (NKS)– setup

– results

• New spectrometer (NKS2)

• A possibility with new beam line and NKS2

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Masashi Kaneta, Tohoku Univ. 3

IntroductionIntroduction

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Masashi Kaneta, Tohoku Univ. 4

NKS experimentNKS experiment

• Focusing on strangeness production by Electromagnetic interaction– by +p and +n reaction– using photon beam at Laboratory of Nuclear Science (LNS)-Tohoku

• 0.8-1.1 GeV (accuracy: 6MeV) beam from 1.2 GeV (2mA) electron

– information for• meson-baryon interaction• hadron structure

• What are our characteristics?– measurement of neutral kaon

• K+ photo-/electro-production existed on markets in 1990’s– Bonn-SAPHIR, Jlab-CLAS, SPring8-LEPS

• however no K0 data on the neutron target• Studied with +C and +d reaction

– now under constructing a new spectrometer (NKS2)

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Masashi Kaneta, Tohoku Univ. 5

Collaborators are:Collaborators are:

• Department of Physics, Tohoku University

– K. Tsukada, M. Ejima, Y. Fujii, O. Hashimoto, K. Hirose, K. Hutatsugawa, S. Kameoka, H. Kanda, M. Kaneta, D. Kawama, H. Katoh, S. Kinoshita, T. Kon, K. Maeda, N. Maruyama, A. Matsumura, Y. Miura, Y. Miyagi, H. Miyasei, S.N. Nakamura, H. Nomura, K. Nonaka, A. Ohtani, Y. Okayasu, M. Oyamada, K. Shirotori, T. Takahashi, H. Tamura, H. Tsubota, D. Uchida, M. Ukai, H. Yamauchi, K. Yawata, M. Wakamatsu, T. Watanabe

• Laboratory of Nuclear Science, Tohoku University

– T. Ishikawa, T. Kinoshita, H. Miyahara, T. Nakabayashi, H. Shimizu, T. Tamae, T. Terasawa, H. Yamazaki

• Department of Electrical and Electric Engineering, Akita University

– A. Sasaki

• Department of Electrical Engineering, Ichinoseki National College of Technology

– O. Konno

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Masashi Kaneta, Tohoku Univ. 6

Fruits of our studyFruits of our study

• Thesis– 2 of Dr. Sci. (T. Watanabe, K. Tsukada),

7 of M. Sci. and 4 of B. Sci. in 5 years

• Conference talk– PANIC02

• Photoproduction of Neutral Kaons on C in the Threshold Region– LEPS03

• K0 and double pion photoproduction experiments at LNS– SENDAI03

• Photoproduction of Neutral Kaons in the Threshold Region at LNS– HYP2003

• K0 photoproduction on 12C in the threshold region– Hirschegg 2004

• Photoproduction of neutral kaons on carbon and liquid deuterium targets in the threshold region

• JPS talk– 15 talks in 2001-2005

• Publication– now on going.....

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Physics topicsPhysics topics

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Strangeness photo-productionStrangeness photo-production

stealing from Kyo TSUKADA’s defense talk with respect

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Strangeness photo-productionStrangeness photo-production

stealing from Kyo TSUKADA’s defense talk with respect

Solid lines:theoreticalcalculationby Kaon-

MAID

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Strangeness photo-productionStrangeness photo-production

stealing from Kyo TSUKADA’s defense talk with respect

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Strangeness photo-productionStrangeness photo-production

stealing from Kyo TSUKADA’s defense talk with respect

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Masashi Kaneta, Tohoku Univ. 12

Strangeness photo-productionStrangeness photo-production

stealing from Kyo TSUKADA’s defense talk with respect

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Masashi Kaneta, Tohoku Univ. 13

Strangeness photo-productionStrangeness photo-production

stealing from Kyo TSUKADA’s defense talk with respect

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Strangeness photo-productionStrangeness photo-production

stealing from Kyo TSUKADA’s defense talk with respect

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Masashi Kaneta, Tohoku Univ. 15

ExperimentalExperimentalsetup of NKSsetup of NKS

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LNS STB ring and NKSLNS STB ring and NKS

• Conditions at this experiment– E : 0.81.1 GeV (Eth=0.91)

– Duty factor : ~ 60 %– Beam current : ~ 2 mA

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The spectrometerThe spectrometer

•TAGX magnet– Dipole magnet with 0.5 T

•Inner Hodoscope (IH) and Outer Hodoscope (OH)

– Trigger counter– Time of flight measurement

•CDC (cylindrical drift chamber) andSDC (straw drift chamber)

– Tracking – Momentum

•EV (electron veto counter)– e+e- background suppression

K0S

B.R. ~ 68.6 % ct ~ 2.67 cm

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Results from Results from NKS NKS

experimentexperiment+C(n) K0+X()

+d(n) K0+X()

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Results of NKS experimentResults of NKS experiment +C(n) K0+X()

K0: NKS (0.800 < cos< 1.000)K+: H.Yamazaki et al. (0.766 < cos< 0.985) Phys. Rev. C51 (1995) R1074

K0 cross section is close to K+ one

Integrated region: almost sameacceptance effect

K0: uncorrected (<5%)K+: corrected

( , 0)

( , )

1.1 0.1C K

C K

fromTakaomi Watanabe’s Dr. Thesis

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Results of NKS experimentResults of NKS experiment +C(n) K0+X()

– K0 Cross section as a function of momentum, cos (= pZ/p), and E

from Takaomi Watanabe’s Dr. Thesis

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Results of NKS experimentResults of NKS experiment

stealing from Takaomi Watanabe’s defense talk with respect

• The model has:– same order of

magnitude for cross section

– underestimate in low E and p region

• need a correction of the model for K0 channel

+C(n) K0+X()

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Results of NKS experimentResults of NKS experiment

stealing from Takaomi Watanabe’s defense talk with respect

when Kaon-MAID value is used for rKK1,

SLA model do not represent the data

With rKK1= -1.4 -1.8

good agreement with the data

+C(n) K0+X()

rKK1 = g(K10 K0 ) /g(K1

+ K+ )

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Results of NKS Results of NKS experimentexperiment

stealing from Takaomi Watanabe’s defense talk with respect

+d(n) K0+X()

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Results of NKS Results of NKS experimentexperiment

stealing from Takaomi Watanabe’s defense talk with respect

}backgroundestimated

1: pair from out of target ( etc)

2: accidental coincidence of from K0 and from

+d(n) K0+X()

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Results of NKS Results of NKS experimentexperiment

stealing from Takaomi Watanabe’s defense talk with respect

+d(n) K0+X()

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• Neutral kaon production by +n K0+is studied via– +C K0+X( and +d K0+X( reaction

• First time measurement of K0 cross section in +d

• Comparison of data with two models– Kaon-MAID

• in +C – seems to underestimate in low momentum (backward direction)

• in both +d and +C– over estimate in p>0.7GeV/c and E=1.0 – 1.1 GeV

– SLA• with tuning of the free parameter rKK1

– rKK1=-1.4 to -1.8 for +C data– rKK1 -2.0 for +d data

• Need more statistics to conclude rKK1– additionally, need to consider a nucleus effect in C

• We expect more statistics with NKS2– 2 times of K0 and 10 times of compared with NKS

Summary of the NKS experimentSummary of the NKS experiment

~

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The new The new spectrometerspectrometer

NKS2NKS2

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The new spectrometer (NKS2)The new spectrometer (NKS2)• New magnet (so called 680 magnet)

– used for cyclotron in CYRIC-Tohoku– 0.42T (1000A, 110V)

• New cylindrical drift chamber– covered forward region

bea

m

680 magnet

view from upstream

view from downstream

beam

beam

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Comparison of new CDC with old Comparison of new CDC with old oneone

•New CDC– covered forward

region– 3D tracking by x,u,v

wire read-out– acceptance

•20–80 cm radius165 deg in zx plane

along the beam165cm height•1.127 Sr (28.18% of

total solid angle)

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Some pictures of NKS2Some pictures of NKS2

STB ring

680 magnet

Detectors will be installed from this autumn

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A possibility withA possibility withthe new beam line the new beam line

and NKS2and NKS2

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A possibility(-ies)A possibility(-ies)

• It is just rough idea which MK hit upon....– that is, might be “Picture of Rice cakes (= “Pie in the sky”)

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A possibility(-ies)A possibility(-ies)

• With large acceptance of 680 Magnet + CDC + – Strangeness production study

, *,.. (also polarization measurement)– many resonances will be backgrounds

• multi-strangeness baryons are interesting – need inner tracker (Mini TPC, Si detector, etc.)

• charmonium??– cross section/polarization measurement– with several E, if possible

– Sea quark (ss) contribution in spin structure of nucleons• an asymmetry of production with polarized beam

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SummarySummary

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SummarySummary

• Neutral kaon production by +nK0+is studied via– +C K0+ and +d K0+ reaction

• First time measurement of K0 cross section in +d

• Comparison of data with two models– SLA show better agreement than Kaon-MAID

• however, it is not perfect

• to fix a free parameter rKK1, need more statistics

• We expect more statistics with NKS2– 2 times of K0 and 10 times of compared with NKS

• Some rough ideas for new beam line with NKS2 are presented

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BackupBackup

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K0 momentum (GeV) K0 momentum (GeV)

K0 momentum (GeV) K0 momentum (GeV)

0.90 GeV < Eγ < 0.95 GeV 0.90 GeV < Eγ < 0.95 GeV

1.05 GeV < Eγ < 1.10 GeV 1.05 GeV < Eγ < 1.10 GeV

cosθ

lab

cosθ

lab

cosθ

lab

cosθ

lab

Color : Acceptance

Solid line :

Kaon-MAID

D2

K0 生成断面積

ほぼ全運動学的領域を覆っている。K0 で 2 倍、 Λ で 10 倍の収量が期待できる。

新旧スペクトロメータの比較新旧スペクトロメータの比較 アクセプタンアクセプタンスス

NKS 新スペクトロメータ

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新旧スペクトロメータの比較 新旧スペクトロメータの比較 電磁石電磁石

旧スペクトロメータ (NKS)TAGX magnet

新スペクトロメータ680 magnet

磁極半径 535 mm 800 mm

ギャップ 600 mm 680 mm

重量 30 t 120 t

電流 500 A 1000 A

最大平均磁場 0.5 T 0.4 T (TOSCA simulation)

0

0 .1

0.2

0.3

0.4

0.5

0 200 400 600 800 1000 1200R dir. ( mm )

By

( T

)

TAGX magnet680 magnet