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Prospects and progress: new experimental searches for neutron-antineutron oscillations and related probes for new physics INT-17-69W A. R. Young Neutron Oscillation: appearance NCSU disappearance and baryogensis Thanks to J. Barrow, M.


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Prospects and progress: new experimental searches for neutron-antineutron oscillations and related probes for new physics

  • A. R. Young

NCSU

Thanks to J. Barrow, M. Frost,

  • Y. Kamyshkov, G. Brooijmans, for slides

PPSN 2018 ILL, May 24, 2018

INT-17-69W

Neutron Oscillation: appearance disappearance and baryogensis

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SLIDE 2

Outline

  • Oscillations in Neutral Systems

and B Violation

  • Current Limits
  • A Next Generation Experiment at

the ESS

  • Our Focus Now
  • A. R. Young

PPNS 2018 2

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SLIDE 3

Central Questions for the Standard Model

Vincenzo Cirigliano’s talk on BSM physics and Josh’s talk on NNbar in DUNE

  • A. R. Young

PPNS 2018 3

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SLIDE 4

Central Questions for the Standard Model

Sources of Baryon Number Violation

  • A. R. Young

PPNS 2018 4

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SLIDE 5

Central Questions for the Standard Model

Sources of Baryon Number Violation The cosmological baryon asymmetry

  • A. R. Young

PPNS 2018 5

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SLIDE 6

Central Questions for the Standard Model

Sources of Baryon Number Violation The cosmological baryon asymmetry Pattern of charges and masses for the SM Fermions

  • A. R. Young

PPNS 2018 6

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SLIDE 7

Central Questions for the Standard Model

Sources of Baryon Number Violation The cosmological baryon asymmetry Pattern of charges and masses for the SM Fermions Origins of neutrino mass

  • A. R. Young

PPNS 2018 7

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SLIDE 8

Central Questions for the Standard Model

All Connected by

models at higher energy scales …

Observable N-N

  • scillations in a next

generation experiment!

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SLIDE 9
  • A. R. Young

Example: Baryogensis

  • Not enough CP violation in the

quark sector for baryogenesis

  • Baryon number violation required
  • Accidental symmetry in SM, so

possible in the SM through B-L conserving excitations (sphalerons)

  • Many models exploit:

→ electrowk scale (SUSY) & B-L? → leptogenesis and B-L?

Also fjnd B-violation in GUTS ΔB=1: p decay → Λ > 1013 T eV strong exptl limits… ΔB=2: not constrained by

p decay Provides viable path to observed BAU through, e.g. Post Sphaleron baryogenesis!

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SLIDE 10

Experimental Probes for Baryogenesis models

  • Direct particle production at LHC
  • LHC measurements already putting pressure on EW

scale models like MSUSY and RPV SUSY predictions

  • (It’s also true that high scale models provide new
  • bservables potentially discoverable at the LHC or

LHC-u like di-quarks and the scalars in PSB models)

  • EDMs probe CP violation
  • Neutrino oscillations probe CP-phases in PMNS matrix
  • A. R. Young

PPNS 2018 10

Important and unique process to probe B violation and baryogenesis mechanisms at relevant energy scales

N- N

  • scillations

Very limited selection! Cold Neutron Beams ofger a clean and powerful probe for this physics

B

Can add to this short list... with factor of 1000+ gain in sensitjvity possible!

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SLIDE 11

The Power of Oscillations

  • A. R. Young

PPNS 2018 11

  • Neutral particle oscillations have played a huge

role in particle physics

  • K0-K0 oscillations (ΔS = 2) central to

understanding CP-violation in SM

  • B meson oscillations (ΔB = 2)
  • Sensitive to CKM elements and CP-violation
  • Sensitive to top mass (mt

2/mW 2)

→ fjrst indication of top mass 1987

  • Neutrino oscillations provided breakthroughs in

understanding the neutrino sector

  • Initial indication of non-zero mass
  • Current suggestion of CP-violating phases

Somewhat natural to expect that N-N oscillations can provide extremely sensitive probe for new physics. In fact, current sensitivity to couplings of order 4x10-23 eV (comparable to EDM measurements)...

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SLIDE 12
  • A. R. Young

PPNS 2018 12

Process, Critical Parameters

Current limit on α ≈ 4×10-29 MeV, or τnn = ħ/α ≈ ~1×108 s (free neutron)

  • Potential V:
  • Nuclear potential ≈ 100 MeV
  • μn· Bearth ≈ 10-18 MeV
  • Strongly suppressed unless quasi-

free condition holds (Vt/ħ << 1)

  • Free neutron experiment requires

substantial cancellation of Bearth

  • Free neutron result can be

cross-checked with magnetic fjeld (“switch ofg” oscillations with Bearth)

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SLIDE 13

Baldo-Ceolin et al, Z.Phys. C63 (1994) 409-416

  • Nt2 = 1.5 109s2, P < 1.6 10-18 (run lasted ~1 year) and τ > 0.86 108s
  • Many subtle optjmizatjons to minimize losses and backgrounds
  • CN integrated beam fmux was 1.25×1011 n/s
  • Experiment was background-free
  • Bound neutron limits ~3 tjmes betuer
  • Many consideratjons make these measurements complementary to free

neutron oscillatjons

Current Limits

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SLIDE 14

Limits for Intranuclear Decays from Underground Experiments

  • A. R. Young

PPNS 2018 14

ROx = 5×1022 s-1

Free neutron beam search goal at European Spallatjon Source CNN DUNE analysis No background

Josh Barrow’s presentation!

 Currently limited by atmospheric neutrino backgrounds  Decay products signifjcantly “processed” by heavy nuclei – background rejectjon challenging!

Model dependent input → R “suppression factor”

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SLIDE 15

Limits for Intranuclear Decays from Underground Experiments

  • A. R. Young

PPNS 2018 15

ROx = 5×1022 s-1

Free neutron beam search goal at European Spallatjon Source CNN DUNE analysis 0 background

Josh Barrow’s presentatjon! Model dependent input → R “suppression factor” → Other exotjc decay modes have very similar signatures → Nuclear Environment can result in suppression or enhancement in some models Intranuclear decay measurements complementary to CN beams!

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SLIDE 16

Next Generation Free Neutron Experiment

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SLIDE 17

Next Generation Free Neutron Experiment

 Increase number of neutrons  Increase tjme of fmight  Keep (or increase) detectjon effjciency (50%)  Keep background at zero (need improved dets!)  Betuer BEarth suppression

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SLIDE 18

Next Generation Free Neutron Experiment

  • Increase number of neutrons
  • Moderator brightness
  • Longer run
  • Moderator area
  • Angular acceptance
  • Increase tjme-of-fmight
  • Longer beamline
  • Colder neutrons
  • Keep (or even increase) detectjon effjciency

(~50%), keep background at ~0

  • Exploit current, established hardware and sofuware

technologies

  • Betuer BEarth suppression
  • Improved passive (+ actjve) shield

Optjmizatjon requires remarkable facility...

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SLIDE 19

European Spallation Source

19

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SLIDE 20

20

2.0 GeV superconducting linac, 14 Hz, 5 MW

Preparations to test accelerator systems at end of summer are under way and the slab for the accelerator-to-monolith structure was just poured…

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Unprecedented

  • pportunity:

 Lower moderator volume available

for optimized (LD2?) source for N-Nbar

 Large beam port allows, in

principle, roughtly 2 orders of magnitude more integrated fmux in beam!

Commissioning:

 Very bright, “pancake moderator”

in top position

protons

and space for 200m beam-line...

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SLIDE 22

ESS Timeline

  • 2014: ESS construction start

Current plan:

  • 2019-2022: Initial phase: commissioning, intensity ramp,

experiments by friendly users

  • 2023-2025: Initial user program operations: reliable operations

with public users; establish basis for future cost sharing – full instrument set is 22 instruments – 15 instruments are under construction – 8 instruments are part of “hot commissioning” in 2022

22

N-Nbar@ESS

2018–2025: – R&D as a part of joint ANNI/HI-BEAM instrument proposal – develop full proposal compatible with as-built ESS

2025+: Mount experiment!

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SLIDE 23

Gustaaf Brooijmans Neutron-Anti-Neutron Oscillation Search

Beam-line and Detectors

2 3

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SLIDE 24

Next Generation Free Neutron Experiment

  • Increase number of neutrons
  • Moderator brightness
  • Longer run
  • Moderator area
  • Angular acceptance
  • Increase tjme-of-fmight
  • Longer beamline
  • Colder neutrons
  • Keep (or even increase) detectjon effjciency

(~50%), keep background at ~0

  • Exploit current, established hardware and sofuware

technologies

  • Betuer BEarth suppression
  • Improved passive (+ actjve) shield
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SLIDE 25

25

Conceptual Design

  • High-m super-mirror
  • Residual B fjeld < 5 nT
  • Good vacuum < 10-5 Pa

See e.g. NNbarX (Babu et al.), htup://arxiv.org/abs/arXiv:1310.8593

MC optjmizatjon of parameters ongoing!

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SLIDE 26

26

Supermirror Reflector

  • Crucial in acceptance gain
  • 2D, so acceptance scales quadratjcally
  • Modern multj-layer supermirrors have good refmectjvity at

increasingly large momentum transfers

Ni refmectjvity → 0 defjnes m=1

(Swiss Neutronics) Actjve R&D at Nagoya University, with devices used at JPARC

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SLIDE 27

Next Generation Free Neutron Experiment

  • Increase number of neutrons
  • Moderator brightness
  • Longer run
  • Moderator area
  • Angular acceptance
  • Increase tjme-of-fmight
  • Longer beamline
  • Colder neutrons
  • Keep (or even increase) detectjon effjciency

(~50%), keep background at ~0

  • Exploit current, established hardware and sofuware

technologies

  • Betuer BEarth suppression
  • Improved passive (+ actjve) shield

Current work characterizing magnetjc noise Current work characterizing magnetjc noise

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SLIDE 28

28

Detector

  • Antj-neutron annihilatjon target
  • High annihilatjon probability, low Z, high transparency to

neutrons

  • ILL experiment used a carbon foil, 130 μm thick
  • Annihilatjon produces pions, <n> ~ 5
  • Background suppression:
  • Precise annihilatjon vertex identjfjcatjon of multjtrack events
  • Good mass and positjon resolutjon
  • Beam tjme structure? (Mainly for background control samples)
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SLIDE 29

Gustaaf Brooijmans Neutron-Anti-Neutron Oscillation Search

Detector

2 9

cosmic veto cosmic veto

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SLIDE 30

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Early Simulations: Detector

G4-based

Identjfy Target Improvements over ILL

acceptance ~90% (x1.8) X3 red. in tjming window (50 ns)

Recent developments in Detector Development!

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SLIDE 31

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Expected Sensitivity

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SLIDE 32

32

Potential Gains wrt ILL

x 1000 in probability, reach τ ~ 2-3 x 109 s

Brightness ≥ 1 Moderator area Needs large aperture 2 Angular Acceptance Quadratic sensitivity 40 length Scale with t2, so L2 5 Run Time ILL run was 1 year 3 Total ≥ 1000

Many sources of gain not taken, but fjnal geometry of lower moderator and port not established

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SLIDE 33

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Early Simulations: Sensitivity

  • Neutron spectrum fjles from ESS
  • 50% detectjon effjciency (as for ILL)

Assumptjons:

 Lower moderator: LD2 optjmized for

integrated fmux

 No obstructjons in large beam port

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SLIDE 34

Gustaaf Brooijmans Neutron-Anti-Neutron Oscillation Search

Collaboration

  • Regular collaboratjon

meetjngs

  • ESS very supportjve
  • Explored impact of the

current moderator and monolith through many iteratjons...

3 4

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SLIDE 35
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SLIDE 36

An Overview of the

Institute for Nuclear Theory’s Workshop

  • n

Neutron Oscillations:

Appearance, Disappearance, and Baryogenesis

By Joshua Barrow jbarrow3@vols.utk.edu For HEP/Astro Seminar January 17th, 2018

During 5 days of workshop 36 partjcipants delivered 40 presentatjons!

  • D. Milstead: NORDITA workshop being scheduled for December, 2018
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SLIDE 37

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Our Focus Now

At ESS: initjatjng coordinated approach to partjcle physics R&D at ESS, including a joint HIBEAM and ANNI proposal for fundamental neutron physics at ESS In Partjcle Physics Community: Contribute partjcle physics roadmaps and a encourage a culture-shifu in the expectatjons for medium scale partjcle physics experiments to include the possibility of sitjng experiments at traditjonally scatuering laboratories (we already do this...) Refocus R&D on productjve experiments: We have several, potentjally high impact experiments that can mounted on current cold neutron or ultracold neutron facilitjes N-Nbar: Ballistjc and collision-compensated geometries possible (Nesvizhevsky)! Strong cold neutron beams available at several facilitjes Very strong UCN sources (PNPI Super Source) essentjally ready for commissioning! N-N’ resonant and transitjon magnetjc moment searches Proposal in preparatjon at ORNL

Berezhiani and Kamyshkov, Possibly relevant to lifetjme, Limits exprimentally feasible

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SLIDE 38

Ongoing R&D

P07: Takuyu Hosobata 9m elliptjcal optjc being tested at J-PARC Optjcs: (Shimizu-group, Hino-group, RIKEN,...) Detectors (proto-type system for evaluatjon identjfjed) (Stockholm and Lund group) Event generators (Golubeva et al.), new signatures and couplings to new physics, as well as a cornucopia of new ideas... (Kamyshkov group) characterizing impact of magnetjc fjeld fmuctuatjons, etc..

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SLIDE 39

39

  • Search for n-n oscillatjon strongly motjvated:
  • ΔB=2 baryon number violatjon appears in many models
  • Probe scales from 105 - 1012 GeV
  • Connectjon with baryogenesis, neutrino masses, …
  • Experiment well within current capabilitjes
  • Very low technical risk – plenty of opportunitjes to optjmize the approach

and improve the project!

  • Substantjal community exists
  • Bridges partjcle and nuclear physics communitjes
  • Synergies with ESS neutron scatuering community
  • Complementary to planned science at LHC (observable partjcle productjon…)

and the Underground Physics program

  • Exploratjon of test beam program and physics measurements by collaboratjon

is underway Opportunitjes to gain a factor 1000 in sensitjvity to processes at core of our existence and understanding of universe are rare

Should not be squandered

htup://www.nnbar-at-ess.org

Conclusion