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Development of a New Search for
Neutron/Anti-neutron Oscillation at the
European Spallation Source
Matthew Frost
UTK HEP Seminar – April 5, 2017
Why study NNbar?• Novel Observation: The spontaneous transmutation of a neutron to an
anti-neutron would be the first experimental observation of Baryon number
violation.
• SUSY and BSM Physics: Reveals new physics that would exist in
constructs beyond the Standard model, setting energy scales for these new
physical phenomena. -> Δ 𝐵 − 𝐿 ; Δ𝐵 = 2
• Astronomical Observations: Justification of observed matter/anti-matter
imbalance in the universe.
• Historical Vindication: Ettore Majorana proposed that charge-neutral
fermions were in fact their own anti-particle.
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Neutron Oscillation
• For a two-level system the probability of oscillation is
For free neutrons, 𝑉 ≪ 1, and 𝑡 ≪ 1 yielding
𝑃𝑛~𝑡
𝜏𝑛−𝑛
2
, where the oscillation time 𝜏𝑛−𝑛 =ℏ
𝛼
Additional details in Josh Barrow’s March 8 presentation:www.phys.utk.edu/research/hep/seminar-slides/2017-spring/barrow-march08.pdf
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Experimental Figure of Merit
• Used to optimize experiment design in simulation.
Figure of Merit = Φ 𝑡2
• Φ →Total neutrons on detector (scales with source intensity)
• 𝑡2 →Square of Mean Flight Time (scales with wavelength)
• Sensitivity units are in “ILL/year”
• Compared to last observation attempt at ILL in 1990.
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Baseline Experiment GeometryThe proposed NNbar experiment at the European Spallation Source (ESS) entails four main
components:
• A large view of ESS cold neutron moderator systems.
• An Ellipsoidal super-mirror reflector about 40 meters in length.
• An ultra-high vacuum tube with magnetic field shielding about 200 meters in length.
• A 2 meter diameter carbon foil annihilation target surrounded by a particle tracker detection
system.
CTUB
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Baseline Experiment GeometryThis optimization has shown performance gains ~100x beyond the ILL experiment with other simulated
cold neutron sources, and thus provides a good configuration to test with other cold source concepts.
• Super Mirror Reflectivity m=6
• Minor Axis b=2 m
• Major Axis c=100 m
• Start/Stop reflector position 10-50 m
• Acceptance Angle ±5°
• Detector Efficiency 50%
CTUB
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The European Spallation Source
• A pulsed source of cold (<25meV)
neutrons designed particularly for
neutron scattering instrumentation
used in studies of advanced materials.
(Condensed Matter, Engineering
materials, Biological structures)
• Proposed startup in 2019.
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ESS Experiment Features
5MW, 14Hz, 3.2ms pulse width
Competitive with other sources.
Time Averaged brightness
comparable to ILL cold source.
Long flight paths are already
planned for scattering
instrumentation.
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Simulation Sensitivity History
Moderator TDR 2013 LD2 Pancake H2
Baseline FOM/yr 250 550 200
Preliminary investigations of experiment sensitivity with various
proposed source designs proved useful in determining whether to
pursue development of the experiment at ESS.
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Neutron Beam Phase Space• Beam trajectory phase spaces have lower dimensionality and distinct correlations between
those dimensions, and thus are easy to represent via distributions that are developed from a statistically relevant set of MC data.
• Source design and conceptual development is performed using MCNP• MCNP output events are investigated via correlation and histograming
• Space and trajectory distributions are fit and weighted against the calculated correlation
• The result is a suitable subroutine that provides events describing the complete phase space
• In development for high intensity LD2 source to advance experimental sensitivity.
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𝜌(𝑥, 𝑦, 𝑣𝑥, 𝑣𝑦, 𝑣, 𝑡)
BF2 Moderator Concept• The ESS will move forward with
the “Butterfly” shaped hybrid
moderator design for Mark-I of the
source moderator/reflector
system.
• This design incorporates elements
of both thermal and cold
moderating sources of neutrons
for scattering instrumentation.
Be Reflector Enclosure
Be Reflector Enclosure
Spallation Target
Upper BF2
Lower BF2
To Nnbar/HIBEAM Experiment
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Large Beam Port• A Large Beam Port was designed
to accommodate high-intensity
experiments like NNbar.
• Equivalent to three traditional
beam ports in horizontal.
• Allows a view of both the top and
bottom moderator systems.
• Enables placement of optical
devices closer to the source.
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• Once the BF2 configuration was finalized, further optimization of the position of super-mirror reflector was pursued.
• Due to the spatial distribution of the cold neutron emitting surfaces of the BF2, the baseline experiment ellipsoid will not be the most effective means by which to transport the cold intensity.
Reflector Geometry for BF2
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Baseline ellipsoid
centered on lower cold spot 313
Baseline ellipsoid
centered on middle of
lower BF2
188
Baseline ellipsoid centered
on middle of both BF2 201
• Using a more complex
parameterized lobed reflector
model, an optimized geometry
specifically tailored to BF2 can be
determined
• “Clover” reflector
• z0, zend, m(z)
• btop, bbottom, ytop, ybottom, xoffset
Quadruple Focusing (Lobed) Ellipse
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btop
bbottom
ybottom
ytop
xoffset
Cross Section of Clover Reflector
Segmentation of Reflectors• Initial simulations are performed
using an ideal ellipsoid, but this ultimately will prove to be impractical.
• A method will be developed to most economically segment the reflector, while minimally impacting the overall sensitivity contribution.
• Current super-mirror guide geometries are constructed of many surfaces approximately 50cm in length, and 5-10cm wide
• Initial results suggest that angular segmentation near focal points and around beam trajectory has much greater impact on transport as compared to along the axis
• With modern super-mirror substrate technologies, a hybrid design can be conceived.
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Segmentation of Reflectors
0
50
100
150
200
250
300
0 0.05 0.1 0.15 0.2 0.25 0.3
Inverse Number of Segments
Sen
siti
vity Ideal Ellipse (No Segmentation)
• Initial results suggest that angular segmentation near focal points and around beam trajectory has much greater impact on transport as compared to along the axis
• With modern super-mirror substrate technologies, a hybrid design can be conceived.
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Reflectivity Optimization• Cold neutron intensity could be
enhanced with high reflectivity
super-mirrors
• Higher reflectivity increases
cost, and may provide little
benefit closer to reflector
entrance.
• Benefit strongly depends on
reflector geometry, and is
included in optimization
parameter space.
Target
Reflector
Source
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• Significant decrease in length, with little
compromise on reflector illumination,
yielding a higher overall FOM.
• Resources can be saved with a smaller
reflector area, however the system is
further complicated by suspension of optics
and smaller, more complex segmentation
• First order calculations show a possible
30% increase in sensitivity with nested
optics
Nested Ellipse Geometry
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R. Cubitt et al. / Nuclear Instruments and Methods inPhysics Research A 622 (2010) 182–185
Multi-SANS for Neutron Reflection
Model Dependencies:• Particle Radius Distribution
• Scattering amplitudes
• Absorption probability
• Bulk Density and Depth• Macroscopic determination of free-path lengths
• Incident Particle Velocity
• Nano-particle temperature• Down/Up inelastic scattering
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Multi-SANS for Neutron Reflection
• Increase in experiment sensitivity due to• Divergence redirection More neutrons on specular reflector
• In-elastic down-scattering Longer Free Flight Time• If particles are actively cooled
Sub-Thermal Neutron Phase Space Map at R = 2755 mm to be used for further analysis.
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Preliminary Hardware R&D
• The ESS will startup at low power and slowly ramp to full power as planned over a 2-3 year period.
• One moderator will be used in the first generation reflector/moderator system
• HIBEAM provides an opportunity to test experiment concepts applicable to a final NNbar experiment.• Novel Optics• Annihilation Detector Systems
• Magnetic Shielding
• Background investigations• Radiological Shielding
• Other Fundamental Neutron Physics endeavors can be pursed as well.
High Intensity Baryon Extraction And Measurement
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Questions?
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