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

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

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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.