Johnston_summary_SSP_Collections

Status report of Solid State Physics, Biophysics and
Collections at ISOLDE
Karl Johnston
Outline
• Summary of the materials/systems under study
• Overview of how the various techniques are sub-divided between
experiments.
• Main results from experiments: semiconductors; Materials; biophysics;
medicine; “miscellaneous”…
• Request for retaining shifts
• Brief addendum to IS486
• End
Variety!
Semiconductors
1.
2.
3.
4.
5.
6.
7.
8.
IS432/450
IS453
IS481
IS486
IS489
IS492
IS501
IS544
•
•
•
•
•
•
•
Si
Ge
CdTe
ZnO
AlN
InN
Ga2O3
Biophysics/chemistry
12. IS488
•
•
Model systems
Proteins: designed and
natural
Medicine
•
13. IS528
Innovative isotopes for
treatment/imaging: Tb
Multiferroic/nanomaterials/misc
9. IS487
10. IS514
11. IS515
•
•
•
•
RMNO3
Spinels CdCr2S4
Intermetallic compounds
Magnetic Nanoparticles
Collections (e.g. neutrino physics)
14. IS500
15. IS533
• Long-lived sources for
calibration of
experiment, 83Rb
Applying radioactivity to solid state physics
Nuclear probes
Radioactive
Nuclei
g, a, b
Muons
 ß+
Nuclear
Physics
Ions
Neutrons
Positrons
Methods
•
•
DLTS
•
Radioactive
Photoluminescence
decay
Using radioactive decay…
•
Tracer Diffusion
•
Interactions
Hyperfine
Hyperfine
Interaction
Interactions
Coulomb
Coulomb
Interaction
Interaction
Scattering
Scattering
Diffraction
Diffraction
Nuclear
Reaction
ß+-eInteraction
Mößbauer effect
e--g, g-g angular correlation
Emission Channeling
Ion Channeling
Backscattering
Elastic Recoil
Resonant Scattering
Neutron Scattering
Nuclear Reaction Analysis
IS432
IS450
IS489
IS492
IS528 (sort of)
•
•
•
•
•
•
•
•
Positron Annihilation
Positron Angular Distribution
Positron Energy Distribution
IS481
IS487
SOLID STATE
PHYSICS
IS488
RESEARCH
IS492
IS501
IS514
IS515
IS544
•
IS453
IS489
Influence of metal layers on diffusion…
Diffusion without layer at 500 K
111Ag
in CdTe
Diffusion with Cu layer at 500 K
without metal layer
with metal layer
DC = DCTe
Metal layers can initiate uphill diffusion
(H. Wolf et al., Appl. Phys. Lett. 100 (2012) 171915 )
IS489
On-line diffusion chamber at ISOLDE
2012
ISOLDE beam
Manipulator
Sputter gun
Tape station
Furnace
Ge detector
6
1011
56
Concentration (cm-3)
IS489
Commissioning of online diffusion
chamber…Diffusion of metals in CdTe
tdiff = 60 min
Mn in CdTe:Te
1010
Tdiff = 850 K
109
Tdiff = 800 K
108
0
400
800
1200
Depth (nm)
1600
2000
2400
Isoelectronic
IS492
Single
Donor
Group IV
impurity
Group V
impurity
Ag Cd In Sn Sb
Sb
4.64 t1/2
1.99 t1/2
0.98 t1/2
0.22 t1/2
4.64 t1/2
1.99 t1/2
3.345
3.350
Energy (eV)
3.355
3.360
3.365
3.370
0.98 t1/2
0.22 t1/2
3.375
Normalised Integrated
Intensity (arb.units.)
I10
10
Time (hours)
100
Energy (eV)
J Cullen et al Appl. Phys. Lett. 102 192110 (2013)
Radiotracer PL has allowed for the full classification of
the dominant impurities in ZnO
IS492
• Radio PL allows for the subtle chemical
identification of luminescence through
different decay chains.
• Has allowed for the identification of
neutral and ionised donors [1, 2],
complexed impurities [3], “double
donor” centres [2, 4], and
isoelectronic centres [5].
1.
2.
3.
4.
5.
K. Johnston et al Phys Rev B 73 165212 (2006).
K. Johnston et al Phys Rev B 83 125205 (2011).
J Cullen et al Appl. Phys. Lett. 102 192110 (2013)
J. Cullen et al Phys Rev B 87 165202 (2013)
J. Cullen et al J. Appl Phys (2013)
Defects and electronic effects in wide
bandgap semiconductors
IS481
0.05
0.00
-0.05
-0.10
473K
-0.15
0.00
-0.05
R(t)
-0.10
673K
-0.15
0.00
-0.05
-0.10
873K
-0.15
0.00
-0.05
-0.10
1073K
-0.15
0
50
100
150
t [ns]
200
- The role of In in GaN and AlN has been studied by
PAC:
→ A defect, probably VN,is stabilized at the 111In
probe and is released at high temperatures after the
250
decay to Cd.
Kessler et al. HFI 197 (2010) 187; pss c 9 (2012) 1032
Electronic effects in Ga2O3
IS481
→ Future work:
Studying electronic effects in Ga2O3 nanostructures and bluk crystals using g-g and e-g PAC
Motivation …..
Dietl et al, Science 287 (2000) 1019
Also motivation for IS432, IS450 and IS453
IS501
Fe: ZnO a ferromagnetic
semiconductor?
(no!)
IS501
ZnO C axis
6 fold spectrum: characteristic of magnetic
structure (at room temperature!!!).
B
Results in an external magnetic field show
that the spectrum shown to be a
slowly relaxing paramagnetic system .
Gunnlaugsson et al (APL 97 142501 2010)
After high-dose implantations, precipitates of
Fe-III are formed. These form clusters yielding
misleading information about the nature of
magnetism in ZnO (as reported by many groups
over the last number of years).
Gunnlaugsson et al APL 100 042109 (2012)
B
13
2012
Be
Mg
IS453
2012
WISH LIST
B
2009
2011
2008
Mn
Co
Ni
C
N
O
Si
P
S
first ever done bEC patterns
using 11Be(14 s)
in GaN
Ge
Source <-> detector : 60 cm
1
11Be
b-
-1
0
24Na
b-
-2
-1
0
1
2
3
1.812
1.725
1.638
1.550
1.463
1.375
1.288
1.200
0
-1
-1
-1
-3
1
0
-3
---------
1.900
1.812
1.725
1.638
1.550
1.463
1.375
1.288
0
-2
-1
0
1
2
3
-3
-2
-1
0
1
2
3
3
3
3
3
3
3
2
2
2
2
2
2
1
1
1
1
1
1
0
0
0
0
0
0
-1
-1
-1
-1
-1
-1
-2
-2
-2
-2
-2
-2
-3
-3
-3
-3
-3
-3
-2
-1
0
1
2
3
-3
-2
Source <-> detector : 30 cm
-1
0
1
2
3
-3
-3
-2
-1
0
1
2
14
3
1.812
1.725
1.638
1.550
1.463
1.375
1.288
1.200
---------
1.900
1.812
1.725
1.638
1.550
1.463
1.375
1.288
Emission channeling studies on a challenging case of impurity lattice location: cation versus anion
substitution in transition-metal doped GaN and ZnO
L.M.C. Pereira, U. Wahl, J.G. Correia, L.M. Amorim, D.J. Silva, S. Decoster, M.R. da Silva, K. Temst, and A. Vantomme
Lattice sites of implanted Mg in the group-III nitrides
L. M. Amorim, U. Wahl, S. Decoster, L.M.C. Pereira, J.G. Correia,
D.J. Silva, K. Temst and A. Vantomme
Influence of the doping on the lattice sites of Fe in Si
D.J. Silva, U. Wahl, J.G. Correia, and J.P. Araújo
Gauging Structural Aspects of ZnO nano-Crystal Growth Through X-ray Diffraction
Studies and PAC
Use of 111mCd on ZnO nano size crystals , studying structural aspects
IS 544
Future projection : Growing ZnO nano-grains on folic acid template : biological
applications , targeted drug delivery , use of 111m Cd +2 again for the PAC studies.
Growing GaO(OH) nano grains OR GaO2O3 grains and doping with Tl+3 or Ru+3 Or
In+3 ions for PAC analysis.
IS487
Study of Local Correlations of Magnetic and Multiferroic Compounds
Local PROBING of EFG and HMF in strongly correlated electron systems:
spin, charge, orbital and lattice degrees of freedom
EFG and the electric polarization correlations . Multiferroic
EFG/HMF relations
Confined and strained conditions (films&nanoP).
LuMn0.96O3±
magnetic frustration reduction by local
deformations in spin-ice systems DCr2O4,
(D=Mg, Cd, Zn, Hg)
LuMn1.08O3
hexagonal manganites:
single crystal (YMnO3), magnetically frustrated LuMnxO3.
Inequivalent positions for ions, in contrast to perovskite structure
and clustering effects
11,5 Shifts isotopes: 111mCd, 111Ag, 117Ag, 77Br, 73Br+73Se, 199mHg
IS515
Radioactive probe studies of coordination modes of heavy metal ions from
natural waters to functionalized magnetic nanoparticles
Local PROBING of EFG of local environment
0,1
of ionic species (Hg2+, Cd2+)
(g) DNPA4 - 100nm, T=‫؛‬20C,+DTC,R2
R(t)
(g) DNPA4 - 100nm, T=‫؛‬20C,+DTC,R2
0,1 main
Two
electric field gradients in functionalized NP
0,1
(g) DNPA4 - 100nm, T=‫؛‬20C,+DTC,R2
0,0
R(t)R(t)
0,1
0
(h)
+DTC
(g) DNPA5
DNPA4 -- 100nm,
100nm, T=20‫؛‬C,
T=‫؛‬20C,+DTC,R2
FT
0,0R(t)
0,0
0,1
EFG
0,0
1
0
= 0.58 (0.02)

=
1230
(20) Mrad/s
EFG2
FT EFG
= 20,16
(0,09)

629(47)
(47)Mrad/s
Mrad/s

==629
0 0 = 0.58 (0.02)
EFG
= 0,58 (0,02)
(i) DNPB5
T=20‫؛‬C
(h)
DNPA5 -- 50nm,
100nm,
T=20‫؛‬C, +DTC
0,0 0,0
(i) DNPB5
- 50nm,
T=20‫؛‬C
(i) DNPB5
- 50nm,
T=20‫؛‬C
0,1 0,1
2
0,0
0,1 0 (i) DNPB5 - 550nm, T=20‫؛‬C
10
0,0
15
time (ns)
0,0
0 0,0
= 1230 (20) Mrad/s
= 0,16 (0,09)
1 1
0 0 EFG

=
(20)
EFG
=1230
1230
(20)Mrad/s
Mrad/s
2

=
0,16
(0,09)
=
0,16
(0,09)
= 629 (47) Mrad/s
EFG
(h)
- 100nm,
T=20‫؛‬C,
+DTC
(h) DNPA5
- 100nm,
T=20‫؛‬C,
+DTC
0,1DNPA5
0,1
EFG1
0
5
5
10
10
time (ns)
2000 4000
 (Mrad/s)
15
2000 40000
15 2000
4000
0 = 629 (47) Mrad/s
= 0.58 (0.02)
Results in NP different from the pure Hg-DTC
compound, where Hg is coordinated to 4 sulphurs
instead of the expected 2 on the nanoparticle
surface.
Limited number of experiments
not yet significant statistics and systematic of
results for control variables needed
0
 (Mrad/s)
time
(ns)
 (Mrad/s) 0
complete
the
planned measurements
To 0
program
2000 4000
5
10
15
timeon
(ns)
-improvements
ion uptaking (Mrad/s)
brought by different morphology/sizes, coverage and pH of the
solutions, which determines the chemical speciation in the sample solution.
-study temperature dependence (0-30ºC), for signal quality/molecular motion in adsorbed
water remaining
-Modelling studies of the obtained EFG
9 Shifts isotopes: 111mCd, 199mHg
111mCd
in RIn3 (diffusion aspects
using PAC)
IS514
• Hope: observe defects bound to Cd impurity at room
temperature
• Result:LA045 LaIn , Cd impl, 30 keV
RN141_1 LuIn ,
Cd impl, 30 keV
111m
111m
3
LaIn
LuIn
3
TA = 880 °C, TM = RT
3
0.10
0.10
0.05
0.05
R(t)
R(t)
TA = 970 °C, TM = 3
RT
0.00
-0.05
0.00
0
100
200
300
-0.05
0
100
200
t (ns)
300
t (ns)
3
 =
85.5(3)
 = 0.16
Same signals
observed
using 111In PAC
noMHz,bound
 =as
72.3(1)
MHz,  = 0
 = 16.5(9) MHz,  = 0
polycrystal
defects observed,  binding energy toopolycrystal
low(?)
4
Q
Q
r amplitude
r amplitude
8
Q
2
111mCd
IS514
PAC in Pd3Ga7
• Goal: measure quadrupole relaxation at elevated temperature
to complement earlier 111In measurements
• Result of room temperature test measurements:
RN122 Pd3Ga7 (?), 111mCd impl, 30 keV
RN116 Pd3Ga7, 111mCd impl, 30 keV
premelt 870 °C, TA = 970 °C, TM = RT
Pd-poor
Pd-rich
premelted at 870 °C, TA = 910 °C
0.10
R(t)
R(t)
0.10
0.05
0.05
0.00
0.00
0
100
200
300
-0.05
0
100
200
300
t (ns)
t (ns)
4
3
mplitude
mplitude
Signals differ from 111In PAC results  improper sample
preparation
prior to implantation at ISOLDE  try again!
2
2
IS488
Metal ion transfer between proteins:
199mHg
The Cu(I) binding protein HAH1
PAC
pH 7.5
8.5
9.4
pH 7.5
199Hg
NMR
pH 9.4
Luczkowski et al.,
Chem. Eur. J., 2013, 19, 9042
IS528
Significant improvement for shipping short-lived samples…
Spécificités : transports vie courte ISOLDE
Objectif 1 : Faire les transports Type A le plus rapidement possible
Valeurs A2 avec
U. Koester et K. Johnston
Procédure spéciale
En collaboration avec M. Magistris
Slide thanks to Abderrahim Errahhaoui
22
Terbium-149: alpha-Emitter
Folate Receptor Targeted a-Radionuclide Therapy
a-Therapy
Ce Pr Nd Pm
Group A: control
Group B: 149Tb-folate 2.2 MBq
Group C: 149Tb-folate 3.0 MBq
Müller et al. 2012, J Nucl Med 53:1951.
Müller et al. 2013, Pharmaceuticals, submitted
Dy Ho Er Tm Yb
IS528
IS500
• For monitoring of KATRIN conversion electrons needed from decay of 83mKr
T_1/2 = 1.8 h)
• 83mKr is generated by decay of 83Rb (T1/2 = 86 d), which is implanted into a
solid platinum substrate (Ø 12 mm)
• ISOLDE produced 11 sources of 83Rb
• Bonn can now produce more reliable sources.
(IS533 similar principle)
Isotope
yield (/uC) target – ion source
Shifts
(8h)
IS432/IS450
52Mn
56Co
5.107
106
Nb foil
RILIS
YO/ZrO (VADIS)
2
3
IS432/450
IS481
111mCd
108
115Ag/115Cd 108
/115In
117Ag/117Cd
108
/117In
111mCd
108
199mHg
108
77Br,
108
Molten Sn / plasma
UC2, Ag RILIS with Nb or Ta ion
source cavity to decrease In
contamination
UC2, Ag RILIS with Nb or Ta ion
source cavity to decrease In
contamination
IS487
Molten Sn / plasma
Pb / Plasma, run it at LOW temp,
avoiding Tl
ZrO / plasma
4
0.5
IS481
3.5
7
1
IS487
1
73Br+73Se
204mPb
199mHg
1e8
1e8
29Al
108
108
108
IS488
UCx – RILIS
Pb – VADIS
IS489
UC2 – W surface
UC2 – W surface
UC2 - LIS
108
108
IS492
ZrO2–HP
UC2 - LIS
38Cl
111Ag
2
2
1
1
1
111Ag
117Ag/117Cd
1
2
Further work on Ga2O3. g-g, e-g
and b-g studies … allows for
unique information.
Continue work on magnetic
frustration, links between EFG
and polarisation , investigate
multiferroic ACrO3 compounds…
IS488
Pb preferred,: challenging. Test
with synthetic protein.
IS489
Further
commissioning
of
online chamber. Role of metallic
contacts.
117Ag/117Cd
77Br
No recent results due to various
technical problems : still
relevant physics; RILIS Co
scheme available…
IS492
Further studies on Br in ZnO.
Examine in more detail recently
discovered Sn feature.
83Rb-83
57Mn
119In
57Co
111mCd
IS500
500pA/ Uc-Ta
1.6μA
IS501
(2UCx, Mn RILIS
3)×108
(2UCx, In RILIS
3)×108
9×107
ZrO2/YtO2,
V/R(?)
IS514
2×108
Sn – HP
(VADIS)
111mCd
108
199mHg
108
83Rb
111mCd 5e8 µC
IS515
Molten Sn /
plasma
Pb / Plasma,
IS533
UC-W / UC-Ta
IS544
Molten Sn /
plasma
1
IS500
Contingency shift
problems at Bonn.
in
case
2
1
IS501
1
8
2
IS514
IS515
7
6
2
Co available with RILIS….
Complete
programme
on
oxides, location of In in oxides.
Previous results failed due to
problems
with
sample
preparation. Now resolved,
experiments to be repeated.
Understanding Hg-coordination,
temperature dependence.
IS533
No previous shifts taken due to
problems at ISOLDE. Still
relevant
IS544
Further investigations on folic
acid and cyclo
IS486: Addendum
• Request for extra
shifts
for
commissioning the
new
general
implantation
chamber
(due
Summer 2014)
• Also: 2 shifts for
development
of
online PAC using
19O
isotope yield
(/uC)
172-Lu 5e7
149-Gd 5e7
19-O
1e6
target – ion source
Ta or other (RILIS if possible)
Ta or other (RILIS if possible)
UCx VADIS
Shifts
(8h)
1
1
2
Summary
• 65 shifts to be kept for 13 experiments (of which 1 is for contingency
only)
• 4 Shifts requested for IS486 to help complete their programme and
commission the new GLM 2.0 chamber.
Publications & Theses
• 89 Publications published or accepted.
• 32 Theses (PhD, Masters either completed or about to be…)
Many thanks to collaborators for the slides