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CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI Recent developments at in-flight facilities In-flight separators world-wide Evolution towards multiple-stage and high-resolution systems Storage rings, stopping cells, hybrid systems Future directions and new experiments Christoph Scheidenberger and

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CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Recent developments at in-flight facilities

In-flight separators world-wide

Evolution towards multiple-stage and high-resolution systems

Storage rings, stopping cells, hybrid systems

Future directions and new experiments

Christoph Scheidenberger

and

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Exotic nuclei: ISOL, in-flight separation, and more...

p

HI

p

ISOL

In-FlightSeparation

IGISOL

Sep.

Sep.

Sep.

ISOLDE, TRIUMF, ALTO, ...

LISE, FRS, RIPS, A-1200, ...

IGISOL, LISOL,...

HIHybrid Sep.SLOW-RI, FRS-Ion-Catcher,

ANL-Gas-Catcher, Cyclotron

Stopper, .....

no beam??? Sep. CARIBU

Proceedings of ARIS-2014 conference

CSch, JPS Conf. Proc. 6, 010027 (2015)

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

World map of in-flight (radioactive) beam facilities

Dubna

Acculinna

Acculinna-2GSI FRS

FAIR Super-FRS

GANIL LISE3, S3

NSCL/MSU

A1900

FRIB ARISANL*

RIKEN RIPS

RIBF BigRIPS

Notre

Dame*

Texas A&M

MARS

CNS CRIB*

RCNP

Lanzhou

RIBLL

RIBLL2

Delhi*

KVI

LNL*

LNS Catania San

Paulo** Low-energy facilitiesMultiple-stage systems

HIMAC

Adapted from: T. Kubo

Florida

State*RISP

Including those

in construction

HIAF

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Outline of the talk

Energy-Loss Spectrometer (dispersion matched)

Fragment Separator (with achromatic, mono-energ. or homog. degrader)

Pre-Separator Main Separator

Spectrometer,storage ring,

Pre-Separator Main Separator hybrid system, ...

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

First-generation

in-flight separators

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Low-energy fragmentation facilities

LISE3

Large relative velocity spread δv/v induced by fragmentation reaction

� Bρ-∆E-Bρ method not sufficient:

� Isotopic separation needs additional velocity analysis/separation

RF deflectorsystem

� Wien filter (GANIL)� RF deflector (RIKEN, MSU, Dubna)

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Separation principle: Bρ-∆E-Bρ method

Magnetic rigid ity

B = v * A/Zr g

V ~ VFragment Projectile A/Z ~ const. Magnetic-rigidity analysis of energy loss yields single isotope !

Magnetic rigidity analysis:

Bρ = γv · A/Z

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Important asset for precision measurements: dispersion matching

Target

1500 MeV/u12C

1500 MeV/u12C

12C + Be � 8B

8B

8B + C � 7Be

7Be

Analyzer Spectrometer

Other examples: SPEG, Grand-RAIDEN, SHARAQ, S-800, ...

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Spectroscopy by knock-out reactions

Sudden process

Reaction: ∆t ≈ 10-22 s

Internal motion: ≈ 10-21 s

1,4 GeV/u 8B�C

W. Schwab et al., Z. Phys. A350 (1995) 283

900 MeV/u AC + C → A-1C + x

Shell closurein 24O

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Next-generation

in-flight separators

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Multiple-stage mass separation for fusion products

Courtesy: H. Savajols

� talk yesterday by J.Piot

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Kinematics of projectile fragmentation and fission

Courtesy: H. Geissel

α /

[mra

d]

60

40

20

0

-20

-40

-60

-0.1 -0.05 0 0.05 0.1

60

40

20

0

-20

-40

-60

∆p/p

α /

[mra

d]

600 800 1000 1200 1400

Energy, MeV/u

Fragmentation

Fission

600 800 1000 1200 1400

Energy, MeV/u

Fission

Fragmentation

400 MeV/u U + 0.1 mg/cm C Sn238 2 12 132

400 MeV/u Xe + 0.1 mg/cm C Sn124 2 12 100

Fragmentation

Fission

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

The new generation of in-flight separators

Pre-Separator Main-Separator

TA

Coupling of two achromatic systems

Examples:

HIAF: HFRS (25Tm, 180m)

FAIR: Super-FRS (20Tm, 176m) H.Geissel et al.,NIM B204, (2003), 71

RIKEN: BigRIPS (9 Tm, 78m) T.Kubo et al.,NIM B204, (2003), 97

MSU: ARIS (8 Tm, ~80m) M.Hausmann et al.,NIM B317, (2013), 349

� all major, next-generation in-flight facilities are based on a pre- plus main-separator

DEG DEG

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

The new generation of fragment separators

Production Target

DegraderWorking Modes

• Achromatic • Dispersive• Mono-energetic

Pre-Separator Main-SeparatorHIAF: HFRS

25Tm, 180m

FAIR: Super-FRS

20Tm, 176mH.Geissel et al.,NIM B204 (2003), 71

RIKEN: BigRIPS

9 Tm, 78mT.Kubo et al.,NIM B204 (2003), 97

MSU: ARIS

8 Tm, ~80mM.Hausmann et al.,NIM B317 (2013), 349

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Reaction studies with relativistic radioactive beams

• Kinematic focusing � high efficiency

• Thick targets � high luminosity

• “Simple” reaction mechanism

(sudden approximation) � “easy” theory

• Particle tracking � complete kinematics

• Broad range of techniques, such as – in-beam gamma ray spectroscopy

– direct reaction studies

– heavy-ion collisions

– invariant-mass spectroscopy

– time-of-flight mass spectroscopy

� Few ions/sec.

� Unbound systems

� Studies beyond the driplines

• Nuclear structure

• Nuclear astrophysics,

• Applications (space, medicine, energy)

High Rigidity Spectrometer (HRS) at FRIB

Other facilities for RRR beams:

• RIKEN: Zero-Degree Spectrometer

• SHARAQ

• Super-FRS: LEB E-Buncher/Spectrometer

• R3B+High-Resolution Spectrometer

Courtesy: R. Zegers

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

High-resolution spectrometers coupled with in-flight separators

Dispersion matched Energy-Loss Spectrometer

Standard operation mode of LEB

Pre-Separator Dispersion-matched Main-Separator

Ta-1

Energy-Buncher

Analyzer

Ta-1 Ta-2

Spectrometer

Pre-Separator

Super-FRS + LEB operated as dispersion matched spectrometer

The tiny momentum change δp = 0.1%, induced in TA-2, can be resolved!

Nuclear reactions in TA-1 lead to

a momentum spread e.g. δp0 = 1%

Courtesy: H. Geissel

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Storage and

cooler rings

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Storage and cooler rings coupled to in-flight separators

GSI: FRS+ESR RIKEN: BigRIPS+RI-Ring IMP-Lanzhou: RIBLL+CSRe

Discovery potential:

• Mass measurements

• New decay modes of HCI

• Nuclear reactions

• Astrophys. reaction ratesOdd Z

Even Z

Isomer discoveriesand studies Bound beta decays

Dripline and shells

(In-)elastic scattering

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Hybrid systems

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Hybrid systems (I): reaccelerated beams at MSU with ReA facility

ReA builds on various ion-stopping and manipulation techniques• gas-filled ion catcher

• cyclotron stopper

• solid beam catchers

EBIT/S charge breeder and linac

Recent result with ReA3: 3 MeV/u

~1% overall

efficiency

First successful rare isotope beam

experiment with ReA3 in September 2015

ISLA (ISochronous Large-Aperture spectrometer), based on former TOFI

SECAR (SEparator for CApture Reactions)

AT-TPC: 46Ar, 40Ar (α,α’), 32S, 38SJENSA: 34Ar, 34m+gCl, 40Ar, 39K, (α,α’), (α,p)General Purpose Line:

46K, 39K Fusion-Fission47K, ANASEN75Ga, 85Rb, NERO, (α,n)47K, 39K, Fusion77Br, 82,84Kr, 85Rb, SuN (p,γ)

Courtesy: D. Morrissey

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Hybrid systems (II): SHE identification and mass measurements

with high-resolution MR-TOF-MS at GARIS-II

GARIS-II

Ion

trap Ion mirrorTOF de-

tectorIon mirror

254No++

Y. Ito et al, submitted arXive: 1709.06468

10 SHE masses measured

80 masses in 4 weeks 30 masses for first time

Shortest T1/2 ≈ 10 msPrecision δm/m ≈ 2·10-7

Courtesy: M. Wada

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Hybrid systems (III): laser spectroscopy of superheavy elements

M. Laatiaoui et al., Nature 538 (2016) 495M. Laatiaoui et al., Eur. Phys. J. D 68 (2014) 71H. Backe et al., Eur. Phys. J. D 45, 99 (2007)

254No

253No

252No

Recent laser spectroscopy results:

• Study of Rydberg states

• Determination of first ionization potential (254No)

• Hyperfine spectroscopy (253No)

• Atomic structure

• Isotope shifts (252...254No)

• Charge radii

SHIP + optical cell

� talk yesterday by M.Laathiaoui

Courtesy: M. Block

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Hybrid systems (IV): isomeric beams

-> Production-> Separation In-Flight-> Energy-Bunching-> Slowing-Down-> Buffer-Gas-Cooling-> High-Resolution

Separation+Meas-urements

First spatial separation of ground state and isomeric state with an MR-TOF-MS

5474 5553 5632 5712 5791

0.0

0.1

0.2

0.3

0.0

0.2

0.4

0.6

0.8

Counts

/ s

Counts

/ s

α-Energy / keV

211mPo

211mPo

BNG on

BNG off

211gPo

Gate off

Gate on

T. Dickel et al., Phys. Lett. B 744 (2015) 137

Courtesy: W.R.Plass

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Complex focal-

plane equipment

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

(Particle-)detector arrays coupled to high-res.spectrometer stages

Exotic hypernucleiExotic atoms (eta‘)Nucleon resonances

� New opportunities at the boarder line of nuclear and hadron physics with (Super-)FRS

FRS

Courtesy: T. Saito

WASA

CdG-2017, Amboise (France), October 16-20, 2017 Christoph Scheidenberger - GSI

Summary

1. Special ion optical systems (energy-loss spectrometer, isochronoussystems)

2. Phase-sp. reduction by beam cooling(stochastic, electron or laser cooling instorage rings, buffer-gas cooling)

3. Multiple-stage separators(coupling of various sections for momentum and energy(-loss) analysis)

4. Coincidence measurements (in front and behind the reaction target,

event-by-event tracking)

B) Solutions for precision measurements

with RIBs with large emittance

A) The elements of a modern

in-flight facility