This document discusses the historical context of the "Stage III" phenomenon observed in metals like niobium and molybdenum, where resistivity suddenly decreases upon heating around 100-120°C. Previous studies using techniques like positron annihilation and elastic recoil detection showed this is due to the recovery of lattice defects like vacancies. More recent work suggests the presence of hydrogen plays a key role by binding to vacancies up to 100-120°C, above which the vacancies dissociate from hydrogen. The document then describes an elastic recoil detection study of the near-surface hydrogen concentration in niobium samples subjected to different baking treatments.
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Romanenko - Elastic Recoil Detection and Positron Annihilation Studies of the Mild Baking Effect
1. Elas%c
Recoil
Detec%on
and
Positron
Annihila%on
Studies
of
the
Mild
Baking
Effect
A.
Romanenko
Fermilab
L.
Goncharova,
P.
Simpson
Univ.
of
Western
Ontario
D.
Gidley
UMich
2. Different
mild
baking
mechanisms
• Models
previously
considered
– Inters%%al
oxygen-‐based
models
– Natural
oxide
modifica%on
• Inters%%al
hydrogen
in
the
near-‐surface
region
• LaJce
defects
– Local
misorienta%on
(disloca%on
density)
reduc%on
with
baking
revealed
by
EBSD
studies
3. Historical
Prospec%ve
• “Stage
III
controversy”
• Origin
-‐
observa%ons
of
resis%vity
recovery
(strong
change)
in
different
group
V
metals
(tungsten,
molybdenum,
niobium)
aSer
either
deforma%on
or
irradia%on
in
1960-‐70s
• Controversy
essence
-‐
is
it
inters%%al
impuri%es
or
laJce
defects,
which
are
changing
in
Stage
III
• Stage
III
happens
in
niobium
around
-‐50C
without
any
hydrogen
and
at
around
120C
with
hydrogen
presence
• Near-‐surface
niobium
is
exactly
that
-‐
niobium
with
some
hydrogen
4. D.
E.
Peacock,
A.
A.
Johnson,
Philosophical
Magazine,
Volume
8,
Issue
88
April
1963
,
pages
563
-‐
577
A
clear
resis%vity
recovery
stage
in
neutron
irradiated
niobium
iden%fied
at
around
100-‐120C
•
Radia%on
damage
–
laJce
defects
–
mostly
vacancies
and
disloca%on
loops
•
Degree
of
recovery
depends
on
the
amount
of
damage
–
the
“recovering”
en%ty
is
laJce
defects
•
Similar
stage
found
in
Mo
5. L.
Stals
and
J.
Nihoul,
Phys.
Stat.
Sol.
8,
785,
1965
Same
resis%vity
recovery
stage
in
heavily
cold
worked
niobium
iden%fied
at
around
100-‐120C
•
Heavy
cold
work
–
laJce
defects
–
mostly
disloca%ons
and
vacancies
•
From
the
analysis
of
recovery
at
different
temperatures
–
driving
process
most
likely
bimolecular
process
–
vacancies
annihila%ng
with
self-‐
inters%%als
•
Abributed
to
the
recovery
of
point
defects
6. P.
Hautojarvi
et
al,
Phys.
Rev.
B,
Vol.
32,
Num.
7,
1985
Positron
annihila%on
–
studies
of
open
volume
defects
(vacancies)
•
Temperature
of
the
Stage
III
recovery
depends
on
the
hydrogen
presence
-‐
vacancies
are
bound
by
hydrogen
up
to
100-‐120C
•
Similar
effect
found
in
Ta
7. Physica
Scripta.
Vol.
20,683-‐684,
1979
Annealing
of
Defects
in
Irradiated
Niobium
0.
K.
Alekseeva
et
al.
Positron
annihila%on
–
studies
of
open
volume
defects
(vacancies)
•
Clear
decrease
in
open
volume
defects
(i.e.
vacancies)
starts
at
around
120C
8. Hydrogen-‐induced
defects
• Hydrogen
can
cause
laJce
defects
–
vacancies
and
disloca%ons
depending
on
the
concentra%on
–
equivalent
to
heavy
cold-‐
work
• Superabundant
Vacancies
(SAVs)
–
general
phenomenon
recently
uncovered
for
M-‐H
systems
–
emerges
when
surface
chemisorp%on
is
preferable
to
inters%%al
solu%on
For
review
–
A.
Pundt
and
R.
Kirchheim,
Annu.
Rev.
Mater.
Res.
2006.
36:555–608
29
orders
of
magnitude
higher
concentra%on
of
vacancies
in
the
presence
of
hydrogen
as
compared
to
thermal
equilibrium
9. Inves%ga%on
of
near-‐surface
hydrogen
• Mo%vated
by
the
possible
driving
mechanism
for
the
mild
baking
effect
–
Vac-‐H
complexes
dissocia%on
occuring
around
100-‐120C
• Leading
to
the
elimina%on
of
the
HFQS
by
– LaJce
defect
density
reduc%on
in
the
near-‐
surface
layer?
[A
Romanenko
and
H
Padamsee
2010
Supercond.
Sci.
Technol.
23
045008]
– Or
hydrogen
concentra%on
decrease?
-‐
inves%gated
by
Elas%c
Recoil
Detec%on
(ERD)
10. Elas%c
Recoil
Detec%on
Sample
He+
Incident
energy
=
1.6MeV
He+
Incident
angle
=
75o
Scabering
Angle
=
29o
H+
Dose:
normalized
to
1µC
Facility
at
the
Univ.
of
Western
Ontario
(Prof.
L.
Goncharova)
• Based
on
the
detec%on
of
recoiled
H
ions
• Sensi%vity
of
order
1
at.%
• Depth
resolu%on
achievable
~
1
nm
• Depth
profile
is
reconstructed
from
energy
spectrum
of
ions
11. Hydrogen Concentration profiles obtained from energy spectra
simulations
• Area under each peak corresponds to the concentration of the element in a 1nm slab
• Peak shapes and positions come from energy loss, energy straggling and instrumental
resolution.
• The sum of the contributions of the different layers describes the depth profile.
12. Samples
inves%gated
with
ERD
Sample
Origin
Treatment
HA-‐1
Single
grain
Nb
BCP
150
um
HA-‐2
Single
grain
Nb
BCP
150
um
+
800C
4
hrs
HA-‐3
Single
grain
Nb
BCP
150
um
+
800C
4
hrs
+
110C
74
hrs
HA-‐4
Single
grain
Nb
BCP
150
um
+
800C
4
hrs
+
110C
74
hrs
+
HF
rinse
10
min
HA-‐5
Single
grain
Nb
BCP
150
um
+
600C
10
hrs
HA-‐6
Single
grain
Nb
BCP
150
um
+
600C
10
hrs
+
110C
54
hrs
LE1-‐37
hot
spot
Large
grain
Nb
cavity
BCP
200
um
cutout
TE1AES004
cold
spot
Fine
grain
Nb
EP
cavity
EP
100
um
+
120C
48
hrs
cutout
13. Experimental
data
(Overview)
Incident
energy
=
1.6MeV
He+
Incident
angle
=
75o
He+
Scabering
Angle
=
29o
Dose:
normalized
to
1µC
H+
15. Different
posi%ons
at
the
surface
BCP+800C
2
hrs
BCP
ERD
results
for
different
posi%ons
on
the
surface
are
shown;
integrated
intensi%es
for
bulk
(ch.100-‐240)
and
surface
(ch.240-‐320)
hydrogen
yield
are
listed
below
• difference
between
different
spots
is
noted
in
the
table
Sample Spot Integrated Yield, ch 100-240 Integrated Yield, ch 240-310
HA-1 1 566 1038
2 513 925
HA-2 1 383 761
2 347 756
3 347 846
16. Different
posi%ons
at
the
surface
ERD
results
for
different
posi%ons
on
the
surface
are
shown;
integrated
intensi%es
for
bulk
(ch.100-‐240)
and
surface
(ch.240-‐320)
hydrogen
yield
are
listed
below
• difference
between
different
spots
is
noted
in
the
table
Sample Spot Integrated Yield, ch 100-240 Integrated Yield, ch 240-310
HA-3 1 355 860
2 365 882
3 354 918
HA-4 1 472 1041
2 521 1136
3 533 1102
17. Different
posi%ons
at
the
surface
ERD
results
for
different
posi%ons
on
the
surface
are
shown;
integrated
intensi%es
for
bulk
(ch.100-‐240)
and
surface
(ch.240-‐320)
hydrogen
yield
are
listed
below
• difference
between
different
spots
is
noted
in
the
table
Sample Spot Integrated Yield, ch 100-240 Integrated Yield, ch 240-310
HA-5 1 393 1220
2 417 1045
HA-6 1 375 855
2 347 696
19. Data
on
cutout
samples
• Used
samples,
which
were
cut
out
of
real
RF
cavi%es
characterized
with
thermometry
during
the
tests
• One
sample
from
the
“hotspot”
in
Cornell
high
field
Q-‐slope
limited
large
grain
BCP
cavity
• One
sample
from
FNAL
baked
fine
grain
EP
cavity
–
no
high
field
Q-‐slope,
cavity
limited
by
local
quench
at
around
150
mT
at
the
other
loca%on
21. Large
grain
BCP
hot
spot
Fine
grain
EP
baked
cutout
Sample Spot Integrated Yield, ch 100-240 Integrated Yield, ch 240-310
Large grain
BCP cutout 1 464 1666
2 528 1877
3 511 2075
4 506 2082
EP baked
cutout 1 579 1829
2 596 2292
3 558 2279
4 636 2121
22. Sample
2
from
baked
EP
cavity
–
no
high
field
Q-‐slope,
losses
negligible
Sample
1
–
Hot
Spot
in
the
high
field
Q-‐
slope
of
large
grain
BCP
cavity
–
strong
dissipa%on
detected
by
thermometry
But
–
hydrogen
profile
is
the
same!
Sample Surface Content Bulk Content
#
1 7.6 nm Nb0.78H0.22 Nb0.994H0.006
2 7.5 nm Nb0.77H0.23 Nb0.994H0.006
23. Positron
Annihila%on
Doppler
Broadening
Spectroscopy
•
Positron
life%me
depends
on
the
electron
density
–
lives
longer
at
open
volume
defects
(i.e.
vacancies)
•
Width
of
the
spectra
of
gamma
quants
produced
on
annihila%on
depends
on
the
local
electron
density
and
momenta
•
Characterized
by
S-‐
parameter
–
roughly
the
higher
S
the
larger
the
concentra%on
of
open
volume
defects
•
Varying
positron
energy
–
non-‐
destruc%ve
depth
profiling
24. Doppler
broadening
spectroscopy
–
preliminary
results
UMich/NCSU
data
UWO
data
Baking
120C
in
situ
Baked/unbaked
Decrease
in
the
density
of
vacancies
detected
Life%me
spectra
in
both
cases
25. Conclusions
• Hydrogen
seems
to
be
uncorrelated
with
the
mild
baking
improvement
in
the
HFQS
– Same
H
content
with/without
HFQS
• HF
rinsing
results
in
the
smearing
of
H-‐profile
• Preliminary
positron
annihila%on
data
–
decrease
in
near-‐surface
laJce
defects
during
mild
baking
• Same
samples
from
ERD
are
going
to
be
used
for
further
positron
annihila%on
studies