muon spin rotation facility development in u.s.: a call for a sssc...

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1 Muon spin rotation facility development in U.S.: a call for a SSSC Study R. Heffner, JAEA, Tokai (past president, ISMS) Y. J. Uemura, Columbia University D. MacLaughlin, University of California, Riverside Washington, DC, April 6, 2006

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Page 1: Muon spin rotation facility development in U.S.: a call for a SSSC …sites.nationalacademies.org/.../webpage/bpa_049544.pdf · 2020-04-08 · nFor studies of muonium and muoniated

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Muon spin rotation facility development in U.S.: a call for a

SSSC Study

R. Heffner, JAEA, Tokai (past president, ISMS)Y. J. Uemura, Columbia University

D. MacLaughlin, University of California, Riverside

Washington, DC, April 6, 2006

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Muon spin rotation, relaxation, resonance (μSR)

n A well-established technique.n Conceptually (but not technically) similar to

NMR.n Has made important contributions:üSuperconductivityüMagnetismn Semiconductorsn Chemistryn Biophysics

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Need

n μSR is an important area of medium-sized science, with no U.S. facilities.n There is a need for a critical review of μSR

science and future developments.n Would lay groundwork for competitive U.S.

position.

n We urge the SSSC to undertake such a study.

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The µSR technique

Muons are producedat a “meson factory”by pion decay:

π+ → µ+ + νµ .

A spin-polarized muon is stopped in the sam-ple. A clock is started.

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Muon lifetime ~2.2 μs. Posi-tron direction is correlated with muon spin. Decay time and direction of positron are recorded.

µ+ → e+ + νe + νµ. _

The muon precesses in an applied field H. Muon β decay:

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n Obtain a time histogram of positron count rate;

n Asymmetry plot: time evolution of muon spin polarization.n Analogous to NMR free

induction signal.

n Typically 106–108 events recorded. 10 min–10hr.

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Advantages of µSR

n Can be used on any system.n No problems with neutron-absorbing or NMR-

unfavorable nuclei.

n A local probe —no need to search reciprocal space (but need scattering to obtain structure).

n Extremely high sensitivity — can easily detect magnetic moments ~10−3µB .

n Needs no applied field, unlike NMR.n Simple spin-1/2 probe.

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Time Windows

Complementary time scales

10–1410–1210–1010–8 10–6 10–4 10–2 100 102 sec

neutron scattering

μSR

NMR

Mössbauerac susceptibility

remanence

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n TRIUMF, Vancouver, Canada

Existing μSR Facilities

n About 400 μSR users worldwide.

n J-PARC, JAEA, Japan (under construction)

n Paul Scherrer Institute (PSI), Switzerland

n ISIS, Rutherford Apple-ton Lab., UK

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n TRIUMF and PSI are con-tinuous muon sources;

n ISIS and J-PARC are pulsed sources.

n Each has specific advan-tages and disadvantages(like reactor vs. spallationneutron sources).

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Applications

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Superconductivity: vortex-state magnetic field distribution

§ Detailed information on supercurrent distribution in vortex lattice.§ Gives penetration depth and coherence length.§ Temperature dependence ⇒ strong evidence

for d-wave superconductivity in YBCO.

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Time-reversal symmetry violation in superconducting state

n Uncommon form of unconven-tional superconductivity.

n μSR evidence: onset of sponta-neous magnetic field belowTc .n Increase of relaxation rate ⇒

n Unique capability of μSR. n TRS-violating fields very weak; not

easily seen by other techniques.

Sr2RuO4

magnitude of spontaneous field.

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Actinide superconductivity

n PuCoGa5: Tc = 18 K!n Intermediate between

heavy-fermion and high-Tc superconductivity?

n Temperature dependence of penetration depth:n clear evidence for broken

point-group symmetry (lines of energy gap nodes).

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Magnetism–highlights

n A probe of static and dynamic internal fields.n Yields temperature dependence and magnitude of

static magnetic moment (ordered or disordered).n Examples:

n Weak-moment magnetism in heavy-fermion metals.

n Disorder and inhomogeneous magnetism in spin glasses, CMR materials and non-Fermi liquids.n Disordered spin freezing;n Interplay of lattice, charge, and spin degrees of

freedom.

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n Dynamic (spin-lattice) muon relaxation. Probes χ′′(ω). n Muon depolarization function

exhibits time-field scaling:P (t,H ) = P (T/H x).

Example: Singular spin dynamics in f-electron non-Fermi liquids

n ⇒ χ′′(ω) divergent at extremely low frequencies. Novel spin dynamics.

n Interplay between disorder and quantum criticality.

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Other areas

n Magnetism in reduced dimensions; geometrical frustration;

n Magnetism and superconductivity in organic con-ductors, magnetic polymers, other novel materials;

n Muonium atom (µ+−e−) as a light hydrogen isotope in semiconductors & insulators;

n Muonic and muoniated radical chemistry in liquids and gases;

n . . .

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Slow muons—a new development

n Very low energy muons (eV–keV) for study of films, surfaces, & interfaces.n Tunable implantation depths over

range <1 nm–1000 nm.n Available at PSI; under develop-

ment at ISIS/RIKEN and J-PARC.

n PSI facility was immediately over-subscribed when it came on line!

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n Field distribution in Fe-Ag-Fe trilayers:

PbYBCO

First applications of slow muons

n Direct measurement of Meissner-state field penetration:n Non-local corrections

to London relation.

n RKKY-like oscillations in nonmagnetic Ag layer.

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n International society for μSR spectroscopy (ISMS):

ISMS

n founded four years ago to promote technique and facility development.

n First president (elected by membership) was Bob Heffner (Los Alamos, JAEA).

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Recent μSR prizewinners

n Don Fleming—2004 ACS SeaborgPrize for Nuclear Chemistry

n Tomo Uemura—2005 ISMS Yamazaki Prize for μSR Science

n For studies of muonium and muoniated free radical chemistry.

n For studies of magnetism and superconductivity using μSR.

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n Lack of suitable U.S. muon sources ⇒ small (but productive) U.S. user community.

n A U.S. μSR facility will ensure future growth:n Large body of specialists in related fields (neutron

scattering, NMR);n In host countries most growth from users with

other primary specialties.

n μSR is certain to produce important new physics.

No μSR facilities in U.S.

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Current situation; cost

n Design study in progress at LANSCE/LANL:n High-acceptance channel, laser ionization technique

for low energy muon production.n Depends on refurbishing the LANSCE accelerator at

Los Alamos.

n Relatively modest cost:n Beam line + general-purpose μSR instrument:

comparable to cost of a modern neutron scattering spectrometer.

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Call for SSSC study

n We propose a study committee of experts in μSR and related areas.n Review of the science.n Study of resources:

n Existing proton accelerators (LANL, BNL)?

n Proposed Rare Isotope Accelerator?n Completely new accelerator (FFAG)?

n Recommendations for new facilities.

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BCS superconductivity in Rb3C60

n Relaxation rate 1/T1 of muon in endohedralmuonium.

n “Hebel-Slichter peak”just below Tc.

n Conventional supercon-ductivity!

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n Development of long-time tails in spin correla-tions below (and above) spin-glass transition temperature.

Spin glasses

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Electron transfer in macromolecules

n Muon-injected electronic state

n Conducting polymers:n Polyacetylene

n Biological macromolecules:n Cytochrome cn DNA

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Medicine

n μSR in human blood.n Field dependence of

asymmetry different for oxygenated and deoxy-genated blood.

n Potential as a diagnostic tool.

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n Most current μSR re-search is in magnetism.

n Then superconductivity, then semiconductors, chemistry, …

n TRIUMF data; similar usage at other facilities.

Facility usage

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n New μSR facilities being built at TRIUMF, ISIS, PSI, J-PARC .

New facilities

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J-PARC, Tokai

n Integrated with spallationneutron & synchrotron radiation facilities.

n Will be brightest source of short-pulse muons in the world.