joining n tof: why and how?€¦ · between 880 kev to 3.5 mev. 4 • accelerator based neutron...

10
Paula Salvador-Castiñeira Michael Bunce Giuseppe Lorusso Joining n_ToF: why and how?

Upload: others

Post on 28-Oct-2020

8 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Joining n ToF: why and how?€¦ · between 880 keV to 3.5 MeV. 4 • Accelerator based neutron sources. 5 Monoenergetic Thermal Neutron irradiation capabilities Beam Energy (MeV)*

Paula Salvador-Castiñeira

Michael Bunce

Giuseppe Lorusso

Joining n_ToF: why and how?

Page 2: Joining n ToF: why and how?€¦ · between 880 keV to 3.5 MeV. 4 • Accelerator based neutron sources. 5 Monoenergetic Thermal Neutron irradiation capabilities Beam Energy (MeV)*

2

Recent (n, f) measurement at NPL(Paula Salvador-Castiñeira et al., )

Page 3: Joining n ToF: why and how?€¦ · between 880 keV to 3.5 MeV. 4 • Accelerator based neutron sources. 5 Monoenergetic Thermal Neutron irradiation capabilities Beam Energy (MeV)*

3

HOW can me make a positive strong

contribution to n_TOF?

• Geography

• Common list of measurement priority for the UK

• Very cool new detector development

Page 4: Joining n ToF: why and how?€¦ · between 880 keV to 3.5 MeV. 4 • Accelerator based neutron sources. 5 Monoenergetic Thermal Neutron irradiation capabilities Beam Energy (MeV)*

Neutron irradiation capabilities

The NPL Nuclear Metrology Group (NMG) has a 3.5 MV Van de Graaff

accelerator. It can accelerate protons and deuterons to energies

between 880 keV to 3.5 MeV.

4

• Accelerator based neutron sources

Page 5: Joining n ToF: why and how?€¦ · between 880 keV to 3.5 MeV. 4 • Accelerator based neutron sources. 5 Monoenergetic Thermal Neutron irradiation capabilities Beam Energy (MeV)*

5

Monoenergetic

Thermal

Neutron irradiation capabilities

Beam Energy (MeV)* Neutron Energy range

(MeV)Reaction

Max fluence at 1 m

(cm-2 s-1)

2.905-2.945 0.001 0.05 45Sc(p,n)45Ti ~ 8

1.925-2.355 0.05 0.63 7Li(p,n)7Be 500 2000**

1.450-2.985 0.63 2.2 T(p,n)3He 1200 2100**

0.880-2.740 4 6 D(d,n)3He ~ 850

0.880-2.550 13 19 T(d,n)4He ~ 620

Page 6: Joining n ToF: why and how?€¦ · between 880 keV to 3.5 MeV. 4 • Accelerator based neutron sources. 5 Monoenergetic Thermal Neutron irradiation capabilities Beam Energy (MeV)*

6

Coaxial design

High Current > 1 mA

Accelerator upgrade

T-shaped design

Current max = 200 µA

2MV TVdG

↑ Ibeam= ↑ fluence

↓ Ebeam= 14 MeV

↑ Reliable = ↑ uptime

Pulsed

Page 7: Joining n ToF: why and how?€¦ · between 880 keV to 3.5 MeV. 4 • Accelerator based neutron sources. 5 Monoenergetic Thermal Neutron irradiation capabilities Beam Energy (MeV)*

Thermal

pile

Proposed layout

Page 8: Joining n ToF: why and how?€¦ · between 880 keV to 3.5 MeV. 4 • Accelerator based neutron sources. 5 Monoenergetic Thermal Neutron irradiation capabilities Beam Energy (MeV)*

Case for expansion

Nuclear Metrology is working in the growth area of

radiopharmaceutical standardisation looking to expand

Seize this opportunity to explore the options of co-locating

another accelerator

This would accelerate the already planned expansion into

this work

Other areas: Radiation biology, nuclear structure

Page 9: Joining n ToF: why and how?€¦ · between 880 keV to 3.5 MeV. 4 • Accelerator based neutron sources. 5 Monoenergetic Thermal Neutron irradiation capabilities Beam Energy (MeV)*

9

Conclusions

• Scale up NPL cross section measurement program

• Collaboration with Manchester U. strengthen the UK

position in n_TOF

• Positive contribution to n_TOF

Page 10: Joining n ToF: why and how?€¦ · between 880 keV to 3.5 MeV. 4 • Accelerator based neutron sources. 5 Monoenergetic Thermal Neutron irradiation capabilities Beam Energy (MeV)*

10

High intensity facility

Plans for a facility are being developed based on 9Be(d,n)10B reaction

MCNP6 used to model potential shielding solutions

Theoretical fluence for radiation hardness testing for electronic devices

1 MeV-equivalent fluence rate in Si = 1.45x106 neutrons cm-2 s-1

(3 MeV Ds, 20 uA beam current, d = 1 m)

Theoretical dose rates for overload testing radiation protection devices

H*(10) rate = 1.7 Sv h-1 (3 MeV Ds, 20 uA beam current, d = 1 m)