homogeneity in nb3sn wires: a route towards high quality … · 2019-08-30 · sem-edx homogeneity...

1
T4 - standard barrier 1 (0.025 ± 0.004) at. %/µm core (0.015 ± 0.004) at. %/µm 2 barrier core T3 - clusters Homogeneity in Nb 3 Sn Wires: A Route towards High Quality Superconductors Alice Moros 1 , Mattia Ortino 2 , Stephan Pfeiffer 1 , Stefan Löffler 1 , Maxim Alekseev 3 , Anastasia Tsapleva 3 , Pavel Lukyanov 3 , Ildar M. Abdyukhanov 3 , Victor Pantsyrny 3 , Bernardo Bordini 4 , Amalia Ballarino 4 , Simon C. Hopkins 4 , Michael Stöger-Pollach 1 , Johannes Bernardi 1 , Michael Eisterer 2 1 TU Wien, USTEM, Vienna, Austria - 2 TU Wien, Atominstitut, Vienna, Austria - 3 A. A. Bochvar High-Technology Research Institute on Inorganic Materials, Moscow, Russia - 4 CERN, Geneva, Switzerland 1 2 3 2 Cu-Sn Nb Cu Nb 3 Sn Ta Sn gradient evaluation 1 2 3 4 T4 Standard T3 Cluster RRP PIT Introduction Within the CERN Future Circular Collider Study, Nb 3 Sn represents the best candidate for the construction of dipole magnets providing a J c of 1.5 kA/mm 2 at 16 T and 4.2 K. In that context, a new cluster layout (2) of prototype internal tin Nb 3 Sn wires, manufactured by the Bochvar Institute, was analyzed and compared first to a standard layout (1) produced with the same heat treatment by the same manufacturer, then to a standard rod restack processed (RRP) (3) and a powder in tube (PIT) (4) wire produced by other manufacturers. The main reason for dividing the sub-element into clusters is reducing the “effective” sub-element size (d eff ). Wire identification T4 (1) Standard T3(2) Cluster (3) RRP (4) PIT Wire Ø [mm] 0.7 0.7 0.8 1 Barrier Distrib. Nb Distrib. Nb + Ta Distr. Nb Distr. Nb Subelements 37 (Ø=80 μm) 37 (Ø=80 μm) 108 (Ø=40 μm) 192 (Ø=40 μm) Dopant Ti Ti Ti Ta Cu-non-Cu ratio 1.3 1.15 1.02 1.24 As the homogeneity in Sn concentration influences the wire superconducting properties, the effect of the cluster layout on the Sn concentration gradient all over the wire cross section was evaluated by employing energy dispersive X- ray (EDX) spectroscopy with scanning electron microscopy (SEM). Furthermore, scanning Hall probe microscopy (SHPM) measurements were performed in order to understand how the sub-elements with the cluster geometry influence the local currents flowing all over the wire cross section on a microscale level. SEM-EDX homogeneity analysis: Sn gradient For both wires (1) and (2), EDX line scans were performed over different sub- elements along the radial direction, from the Nb barrier to the Cu-Sn core. The obtained results were then compared to the Sn gradients obtained for standard RRP (3) and PIT (4) wires produced by other manufacturers. 1 BARRIER CORE Acknowledgements This work is part of the Marie Skłodowska-Curie Action EASITrain, funded by the European Union’s H2020 Framework Programme under grant agreement no. 764879. Conclusion and Outlook The new cluster layout shows the smallest Sn concentration gradient. The average local current value is in line with state-of-art RRP wires. Other possible cluster configurations can lead to further improvements towards reaching the FCC target. EUCAS 2019, Glasgow (Scotland), September 1 st -5 th In wires with cluster sub-elements, the Sn concentration gradient was evaluated along the tangential directions (cluster width) too, and found to be negligible. 3 (0.035 ± 0.004) at. %/µm barrier core RRP 4 (0.076 ± 0.004) at. %/µm barrier core PIT SHPM: remnant field map & local currents evaluation The sample was fully magnetized, then scanned in self-field. Remnant-field line scans show inter-filament coupling. By inverting the remnant field profile it is possible to evaluate the contribution of each sub-element to the local current flow over the cross section. The average local J c value is comparable with the ones found in literature for standard RRP wires at 10 K, self-field. Inter-filament coupling Remnant-field profile at 10 K, 0 T T3 - clusters Local J c evaluation (A/m 2 ) T3 - clusters Sn 1 2 3 Schematic of the cluster layout (2) before heat treatment The Sn concentration gradient is smaller in the cluster layout than in the other cases: the cluster sub-elements seem thus to have a great potential in terms of producing wires with higher homogeneity.

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Page 1: Homogeneity in Nb3Sn Wires: A Route towards High Quality … · 2019-08-30 · SEM-EDX homogeneity analysis: Sn gradient For both wires (1) and (2), EDX line scans were performed

T4 - standardbarrier1

𝑮𝒓𝒂𝒅𝒊𝒆𝒏𝒕(0.025 ± 0.004) at. %/µm

core

𝑮𝒓𝒂𝒅𝒊𝒆𝒏𝒕(0.015 ± 0.004) at. %/µm

2 barrier coreT3 - clusters

Homogeneity in Nb3Sn Wires:A Route towards High Quality Superconductors

Alice Moros1, Mattia Ortino2, Stephan Pfeiffer1, Stefan Löffler1, Maxim Alekseev3, Anastasia Tsapleva3, Pavel Lukyanov3, Ildar M. Abdyukhanov3, Victor Pantsyrny3, Bernardo Bordini4, Amalia Ballarino4, Simon C. Hopkins4, Michael Stöger-Pollach1, Johannes Bernardi1, Michael Eisterer2

1 TU Wien, USTEM, Vienna, Austria - 2 TU Wien, Atominstitut, Vienna, Austria - 3 A. A. Bochvar High-Technology Research Institute on Inorganic Materials, Moscow, Russia -4 CERN, Geneva, Switzerland

1

2

3

2

Cu-SnNb CuNb3Sn Ta

Sn gradient evaluation

1 2

3 4

T4Standard

T3Cluster

RRP PIT

IntroductionWithin the CERN Future Circular Collider Study, Nb3Sn represents the bestcandidate for the construction of dipole magnets providing a Jc of 1.5 kA/mm2

at 16 T and 4.2 K. In that context, a new cluster layout (2) of prototypeinternal tin Nb3Sn wires, manufactured by the Bochvar Institute, wasanalyzed and compared first to a standard layout (1) produced with the sameheat treatment by the same manufacturer, then to a standard rod restackprocessed (RRP) (3) and a powder in tube (PIT) (4) wire produced by othermanufacturers. The main reason for dividing the sub-element into clusters isreducing the “effective” sub-element size (deff).

Wire

identification

T4 (1)

Standard

T3(2)

Cluster

(3)

RRP

(4)

PITWire Ø [mm] 0.7 0.7 0.8 1

Barrier Distrib. NbDistrib.

Nb + TaDistr. Nb Distr. Nb

Subelements 37 (Ø=80 µm) 37 (Ø=80 µm) 108 (Ø=40 µm) 192 (Ø=40 µm)

Dopant Ti Ti Ti Ta

Cu-non-Cu

ratio1.3 1.15 1.02 1.24

As the homogeneity in Sn concentration influences the wire superconductingproperties, the effect of the cluster layout on the Sn concentration gradient allover the wire cross section was evaluated by employing energy dispersive X-ray (EDX) spectroscopy with scanning electron microscopy (SEM).Furthermore, scanning Hall probe microscopy (SHPM) measurements wereperformed in order to understand how the sub-elements with the clustergeometry influence the local currents flowing all over the wire cross sectionon a microscale level.

SEM-EDX homogeneity analysis: Sn gradientFor both wires (1) and (2), EDX line scans were performed over different sub-elements along the radial direction, from the Nb barrier to the Cu-Sn core.The obtained results were then compared to the Sn gradients obtained forstandard RRP (3) and PIT (4) wires produced by other manufacturers.

1BARRIER

CORE

AcknowledgementsThis work is part of the Marie Skłodowska-Curie Action EASITrain,funded by the European Union’s H2020 Framework Programme undergrant agreement no. 764879.

Conclusion and Outlook➢ The new cluster layout shows the smallest Sn concentration gradient.➢ The average local current value is in line with state-of-art RRP wires.➢ Other possible cluster configurations can lead to further

improvements towards reaching the FCC target.

EUCAS 2019, Glasgow (Scotland), September 1st - 5th

In wires with cluster sub-elements, the Sn concentrationgradient was evaluated along the tangential directions(cluster width) too, and found to be negligible.

3

𝑮𝒓𝒂𝒅𝒊𝒆𝒏𝒕(0.035 ± 0.004) at. %/µm

barrier core

RRP

4

𝑮𝒓𝒂𝒅𝒊𝒆𝒏𝒕(0.076 ± 0.004) at. %/µm

barrier core

PIT

SHPM: remnant field map & local currents evaluation

The sample was fully magnetized, thenscanned in self-field. Remnant-field linescans show inter-filament coupling.By inverting the remnant field profile itis possible to evaluate the contributionof each sub-element to the local currentflow over the cross section. The averagelocal Jc value is comparable with theones found in literature for standardRRP wires at 10 K, self-field.

Inter-filament couplingRemnant-field profile at 10 K, 0 TT3 - clusters

Local Jc evaluation (A/m2)

T3 - clusters

Sn1

2

3Schematic of the clusterlayout (2) before heattreatment

The Sn concentration gradient is smaller in the cluster layout than in theother cases: the cluster sub-elements seem thus to have a greatpotential in terms of producing wires with higher homogeneity.