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Adrien Adrien

Adrien - PowerPoint Presentation

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Adrien - PPT Presentation

Matta Natasha Timofeyuk TREX MINIBALL 18 N 7 protons 11 neutrons p 12 1 d 52 3 Lowlying states dominated by proton p 12 1 ID: 582398

beam target mev states target beam states mev angle rex shifts peaks energy resolution pps carbon neutron levels putt

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Slide1
Slide2

Adrien

Matta

Natasha

Timofeyuk

T-REX, MINIBALLSlide3

18

N –

7 protons

, 11 neutrons p1/21

d

5/23

Low-lying states dominated by: proton( p1/21 ) (d5/23 )J=5/2 or (d5/23 )J=3/2 or s1/21 of which the 1 and 2 from the middle configuration can’t be populated in (d,p)

 

these levels are confused, in the compilationsSlide4

Neutron-rich pathway through light nuclei in explosive

nucleosynthesis

nitrogen

and carbon isotopes

near the start, and accessibleSlide5

Neutron-rich pathway through light nuclei in explosive

nucleosynthesis

sensitive

important

not included

includedSlide6

PREVIOUS WORK

Canberra data, Putt et al.

(

7Li,7Be)7Be* at 0.48 MeV

This reaction removes a proton,

adds a neutron

Should populate 3 at 0.75 MeV plus two OTHER statesapart from g.s. and 0.12 MeV

The starred peaks are the ones that contain at least in part the excited 7Be channel.The missing two peaks are the 0 and 1 from s1/2 transfer.Putt et al. identify the states as being at 0.75 and at 0.58, but we say 1.23 also possible.In the proposal, we have taken Putt et al.’s suggestion (0.58 and 0.75 peaks).like (d,p)Slide7

Reminder: this is what was shown earlier – current EXPERIMENTAL situation, with MIRROR

MIRROR

(study the

symmetry)

these levels are confused, in the compilationsSlide8

Otsuka

2012

EXPERIMENT

THREE STRONG PEAKS

AS WELL AS THE

2

(THE 0 AND 1 ARE MISSINGEXCEPT IN THE ANU RESULTS)Compare current EXPERIMENTAL situation, with THEORYSlide9

HIE-ISOLDE beam of

17

N

Reaction 17N(d,p

)

18

N5.5 MeV/A104 pps on targetT-REX plus MINIBALLGamma-ray gatingMeasure Ex and SF’s, ANC’s

THE EXPERIMENTSlide10

EXCITATION ENERGY RESOLUTION arising from the charged particle measurement

Limitations

: beam spot, strip pitch, (target thickness 0.5 mg/cm

2

)

Intensities

: using predicted cross sections and spectroscopic factors

Includes hypothetical state at neutron thresholdDeduced from measured angle and energy of protonSlide11

HOW GAMMA-RAYS WILL ALLOW THE NEAR-DEGENERATE STATES TO BE RESOLVED

Allows for Doppler correction

using crystal segment dataSlide12

40

0

(

d,p

) centre of mass angle

(

d,d

)(p,p)WHAT WE SHOULD OBSERVE WHEN WE PLOT THE T-REX ENERGY AGAINST LAB ANGLESlide13
Slide14

PARTICLES

GAMMA-RAYS

THE TRIFOILSlide15

TRIFOIL DETECTOR

LPC Caen

THE TRIFOILSlide16

Angle bins: 2 degrees in

c.m

.SIMULATION OF THE DIFFERENTIAL CROSS SECTION FOR ONE OF THE NEW S-WAVE STATES

Actual predicted statistics for one week of running with 0.5 mg/cm2 targetSlide17

SUMMARY of REQUEST

We are requesting 27 shifts of

17N beam at 5.5 MeV/AWith this, we will perform (d,p) with the 17N beam, and study all populatedstates in

18N, using gamma-rays to select and identify the closely spaced levels.Of this, 21 shifts are required in order to perform the (d,p

) measurement

We believe that we can save time by not running on a carbon target

We would run on a carbon target (target contaminant) if time permitsWe have allowed 6 shifts for optimising the charge state to accelerate (to minimise contaminants) (extraction will use NO+ from nanoCaO+O2, + plasma)

and stripping methodology (what foils, and where) to eliminate 17OWe are requesting 3 shifts for setting up with a stable pilot beam, toensure that detectors and electronics are set up correctlyWe request 104 pps on the reaction target. The beam should be delivered at the T-REX + Miniball setup.We have allowed for a 5mm diameter beam spot on target (dominates the resolution)Slide18
Slide19

Klupp

/

Muecher

@ Munich

Matta @ Surrey (

approx

)Reconstructed excitation energy for lowest four known states, assuming isotropic productionSlide20

220

g/cm2 CD

2 target, 275 keV FWHM resolution, 104 pps

, HELIOS at Argonne

(

Calem Hoffman, Florence INPC 2013, unpublished)