MRTOF mass measurements at GARIS-II: Toward SHE identification via - - PowerPoint PPT Presentation
MRTOF mass measurements at GARIS-II: Toward SHE identification via - - PowerPoint PPT Presentation
MRTOF mass measurements at GARIS-II: Toward SHE identification via mass spectroscopy Purpose of SlowSHE 118 117 Alpha decay Lv Spontaneous Fission 115 Beta Decay / Electron Capture Fl Directly Synthesizable / T <5 ms 175 1/2 113
Purpose of SlowSHE
- Already start to see increase in SF
- Eventually longer T1/2 will become bottleneck, too
Rf Db Sg Bh Hs Mt Ds Rg Cn 113 Fl 115 Lv 117 118 175 170 165 160 N= 155 150 Lr No Md 145 Alpha decay Spontaneous Fission Beta Decay / Electron Capture Directly Synthesizable / T <5 ms
1/2Directly Synthesizable / T >5 ms
1/2L
- n
g e r h a l f
- l
i v e s 3
- b
- d
y d e c a y m
- r
e l i k e l y L
- w
r a t e s
P . Schury
- Nov. 9, 2015
JCNP2015
SlowSHE Facility
SlowSHE
LINAC
Flat Trap Pulsed Drift Tube
P . Schury
- Nov. 9, 2015
JCNP2015
Low-energy beam preparation
Very fine wire rf-carpet
P . Schury
- Nov. 9, 2015
JCNP2015
Low-energy beam preparation
205Fr
P . Schury
- Nov. 9, 2015
JCNP2015
Low-energy beam preparation
ns pulse ns pulse μs pulse Continuous ion beam
Multi-directional flat rf-trap
P . Schury
- Nov. 9, 2015
JCNP2015
Simplified MRTOF Methodology
Ion Trap
+
MCP
- Approx. Potential
0V
P . Schury
- Nov. 9, 2015
JCNP2015
Simplified MRTOF Methodology
- 1. Accumulate and cool Ions
in trap
Ion Trap
+
MCP
- Approx. Potential
0V
P . Schury
- Nov. 9, 2015
JCNP2015
Simplified MRTOF Methodology
- 1. Accumulate and cool Ions
in trap
- 2. Lower voltage on injection
mirror
Ion Trap
+
MCP
- Approx. Potential
0V
P . Schury
- Nov. 9, 2015
JCNP2015
Simplified MRTOF Methodology
- 1. Accumulate and cool Ions
in trap
- 2. Lower voltage on injection
mirror
- 3. Eject ions from trap
Ion Trap
+
MCP
- Approx. Potential
0V
P . Schury
- Nov. 9, 2015
JCNP2015
Simplified MRTOF Methodology
- 1. Accumulate and cool Ions
in trap
- 2. Lower voltage on injection
mirror
- 3. Eject ions from trap
- 4. Raise voltage on injection
mirror
Ion Trap
+
MCP
- Approx. Potential
0V
P . Schury
- Nov. 9, 2015
JCNP2015
Simplified MRTOF Methodology
- 1. Accumulate and cool Ions
in trap
- 2. Lower voltage on injection
mirror
- 3. Eject ions from trap
- 4. Raise voltage on injection
mirror
- 5. Wait for N reflections
Ion Trap
+
MCP
- Approx. Potential
0V
P . Schury
- Nov. 9, 2015
JCNP2015
Simplified MRTOF Methodology
- 1. Accumulate and cool Ions
in trap
- 2. Lower voltage on injection
mirror
- 3. Eject ions from trap
- 4. Raise voltage on injection
mirror
- 5. Wait for N reflections
- 6. Lower voltage on ejection
mirror
Ion Trap
+
MCP
- Approx. Potential
0V
P . Schury
- Nov. 9, 2015
JCNP2015
Simplified MRTOF Methodology
- 1. Accumulate and cool Ions
in trap
- 2. Lower voltage on injection
mirror
- 3. Eject ions from trap
- 4. Raise voltage on injection
mirror
- 5. Wait for N reflections
- 6. Lower voltage on ejection
mirror
- 7. Detect ions at MCP
Ion Trap
+
MCP
- Approx. Potential
0V
m = mref ✓ t − t0 tref − t0 ◆2
P . Schury
- Nov. 9, 2015
JCNP2015
Comparison to PTMS
Rm=150,000 N≳150 ⇒δm/m≲5x10-7 N≳10⇒δm/m≲2x10-6
δm m = a Rm √ N
Isochronous!
PTMS ~ 304 T
ttof = L r m 2K ∂ttof ∂K ≈ 0
, , Slow
P . Schury
- Nov. 9, 2015
JCNP2015
Simultaneous Measurements
Counts / 6.4 ns Counts / 6.4 ns Counts / 3.2 ns
- 165Ho(40Ar, 4n)201At
- 169Tm(40Ar, 4n)205Fr
- 169Tm(40Ar, 3n)206Fr
- Decays or ypxn-channels?
P . Schury
27pSH-6
Results: Weighted average mass deviation
133Cs+ Species Δm [keV] Δm [keV] N [ions]
201At
- 342(45)(3)
522
201gPo
- 16(74)(3)
108
201Bi
- 35(385)(3)
6
205Fr
- 80(36)(60)
- 467
205Rn
212(320) 48
205At
73(420) 11
205Po
- 1059(2050)
2
206mFr
- 98(118)(1)
210
206Rn
551(600)(1) 3
206At
- 69(2150)(1)
3
Reference:
205Fr+
P . Schury
- Nov. 9, 2015
JCNP2015
Mass measurements from first run
- 3000
- 2500
- 2000
- 1500
- 1000
- 500
500 1000 1500 2000
201Bi 201gPo 201At 205Fr 205Rn 205At 205Po 206mFr 206Rn 206At
m - mAME’12 [keV]
P . Schury
- Nov. 9, 2015
JCNP2015
Next Step: TransFermium nuclei
Mass measurements of trans-Fermium isotopes will provide important data for nuclear shell models used to predict location and properties of the “Island of Stability”
Fm
252Rf
261Rf
259 252 2.3 m 251 4.2 m 250 52 s 256 6 2.9 s 3.5 m 255 0.8 s 1254 keV 2.54 s 252 2 51 s 1295 keV 265 ms 254 4 257 7 24.5 s 1.56 m 253 251 0.8 s 160 keV 1.0 s 254 17.1 s 31 s 40 keV 2.5 s 255 5 22 s 256 6 253 0.6 s 30# keV 1.3 sRf
256 6.6 msRf
257 4.8 s 73 keV 4.3 sDb
258 4.5 s 60# keV 1.9 sDb
257 2.3 s 140# keV 0.67 sSg
260 4.95 msSg
261 183 msCr
54Ti
50 500 pnACa
48 1 pμANe
22 3 pμAProjectile Beams
Lr
257 6.0 sLr
258 4.1 sLr
259 6.2 sLr
260 3.0 mN
15 1 pμAAr
40 1 pμAFm
244 3.5 msFm
245 4.2 sRf
255Rf
258Sg
259Db
259Db
260Db
262Sg
263Sg
262Bh
261Bh
264Bh
266Hs
264Hs
265Hs
267Mt
268Ds
269Mt
270Ds
271Rg
272Rg
274Cn
277Md
253D
VR
VM F
N=152Md
254Md
256Md
255Md
249Fm
247Fm
248Fm
249Fm
250Fm
251Sg
265Hs
269Ds
273113
278Deeper into the future...
- Already start to see increase in SF
- Eventually longer T1/2 will become bottleneck, too
Rf Db Sg Bh Hs Mt Ds Rg Cn 113 Fl 115 Lv 117 118 175 170 165 160 N= 155 150 Lr No Md 145 Alpha decay Spontaneous Fission Beta Decay / Electron Capture Directly Synthesizable / T <5 ms
1/2Directly Synthesizable / T >5 ms
1/2L
- n
g e r h a l f
- l
i v e s 3
- b
- d
y d e c a y m
- r
e l i k e l y L
- w
r a t e s
P . Schury
- Nov. 9, 2015
JCNP2015
Conclusion
- Simultaneous mass measurement
- Short-lived nuclei
- Heavy nuclei
- Identify nuclei with few counts
Using MRTOF-MS we can:
SlowSHE Facility
- 1. He Gas Cell Stopping
- 2. Ext. via RF-Carpet: 0-5 ms
- 3. OPIG Transport: < 1ms
- 4. Ion Cooling: ≈2 ms
- 5. MRTOF ToF-MS: 2~10 ms
≈60% ≈50% ≈100% >5% ≈100% Process Efficiency
Total ⪆1% ≈5~20 ms