Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston,...

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Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts

Transcript of Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston,...

Page 1: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Positronium trapping at

material surfaces

Bernardo Barbiellini

Northeastern University

Boston, Massachusetts

Page 2: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Content

• Positron annihilation spectroscopy: new way to probe the surface of nanoparticles.

• New theories of positron states at surfaces.• Formation of matter-antimatter molecules at surfaces.

Page 3: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Some applications of positron annihilation

• Gamma-Ray Astrophysics• Positron Emission Tomography (PET)• Positron Annihilation Spectroscopy (PAS)

in Material Science

Page 4: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Positron annihilation (Compton) Feynman diagram

(space)

(time)

The positron is the electron’s antimatter partner, whichcan annihilates with an electron.

Essentially the same Feynman diagram describes the amplitude for positron annihilation and for Compton scattering.

Page 5: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Compton scattering

The Compton scattering has been used to study the quantum nature of the hydrogen bond in ice. E.D. Isaacs et al., PRL 82, 600 (1999).

Page 6: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Electron Momentum Density (EMD) and positron Lifetime

p) ~ ∑n | ∫ dr e -ip .r (r) n(r) √[( r)] | 2

-1 ≈ re2 c ∫ dr dr+ (r+) (r) [( r)] r - r+)

The emitted gamma photons carry detailed information on the electron momentum distribution.

The positron lifetime typically between ~100 ps and ~0.5 ns (in absence of positronium formation) depends sensitively on the local electron density at the annihilation site.

Page 7: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Properties of the positron

• Positrons are positively charged: high sensitivity to detect and identify atomic scale defects in matter.

• Positrons have a magnetic moment: easy and direct imaging of the electronic structure of magnetic materials.

Page 8: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

EMD for magnetic electrons in bilayer manganites : an example.

EMD projections: Occupation breaks & Wave-function effects are visible.

.

Calculations based on Density Functional Theory (DFT).See Li et al., Phys. Rev. Lett. 93, 207206

Page 9: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Positron wave function

This density distribution (log-scale) in bilayer manganite show that the positron selects particular regions of the sample.

Page 10: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Positron lifetime in bulk material

The GGA theory based onDFT [Barbiellini, M. J. Puska, T. Torsti and R. M. Nieminen,Phys. Rev. B 51, 7341 (1995)] gives excellent agreement with experiment.

GGA

LDA

Page 11: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

PAS can probe surfacesLow energy (~10ev) positron in.Implantation, thermalization, diffusion, encountering the surface

Positron trapped in surface state

Annihilation of surface state positron with an electron

10-12 - 10-11 sec

10-10 sec

Page 12: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Experiments reveal surface states

The theory for positron surface states is still in its infancy. We have recently solved the case for a quartz surface.

Page 13: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

PAS a new probe for Nanoparticles

CdSe nanoparticles [Eijt et al., Nat. Mat. 5, 23 (2006) ]

The PAS provides a powerful tool to determine the composition of the surface region of NPs.

Page 14: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

PAS has confirmed the Self-healing mechanism in CdSe QDs

Theory: optical gap properties explained by Se atoms outward relaxation.

Cd: BlueSe: Green

Puzder et al. ,Phys. Rev. Lett. 92, 217401 (2004).

Page 15: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Positronium formation at a surface of quartz

Positronium (Ps) is a strange sort of atom in which an electron and a positron orbit one another without a nucleus.

Positrons can pair up with electrons as Ps at a surface of quartz and Ps can stick to the surface.

Michael Schirber, Phys Rev. Focus 20, story 7

Page 16: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Ps-surface interaction potential

Repulsive van der Waals z

0

z0

Saniz, B. Barbiellini, P. M. Platzman, and A. J. Freeman, PRL 99, 096101, (2007); PRL 100, 019902, (2008).

vdW constant:

Where is Ps polarizability and is the bulk dielectric function.

zVW = z0

Surface position

Page 17: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Bulk dielectric function

First-principles DFT for band structure: Full-potential linearized augmented plane wave (FLAPW).

We deduce

C=8.43 eV bohr3

Page 18: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Charge density exponential decay at the surface

z0=0.95 a.u.1/l =2.06 a.u.kc= 1/l

The repulsive part of the potential is given by

Page 19: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Ps surface states

Ground state : -0.112 eVExcited state: -0.005 eV

Page 20: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Molecular Ps FormationPs + Ps Ps2

Gas phase reaction - inefficient

More efficient channel on surfaces

Once two positroniums are

trapped on a surface, they can

easily combine to form a

dipositronium molecule.

The mechanism is analogous

to H2 formation on dust grain

surfaces in space.

D.B. Cassidy and A.P. Mills Jr., Nature 449, 195 (2007).

Page 21: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Langmuir-Hishelwood reaction

•2 Ps atoms bound to a surface•Effective Lennard-Jones potential•Collision → surface assisted recombination•DesorptionEnergy balance:

Ps2 binding energy: Eb=-0.44 eV

2×EPs > Eb => Ps + Ps → Ps2 + EK

Page 22: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Conclusion• The PAS has recently provided a powerful

technique to determine the composition of the surface region of nanoparticles (solar cells).

• We are still exploring the fascinating theory of positrons and Ps states at surfaces.

• These results also help guide researchers who aim to assemble larger collections of Ps into quantum state called a condensate (this is an important step toward the gamma ray laser).

Page 23: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Ps formation before annihilation

Page 24: Positronium trapping at material surfaces Bernardo Barbiellini Northeastern University Boston, Massachusetts.

Gamma-ray laser

As a result, there is a huge interest in the technology from energy researchers who believe the lasers could be used to kick-start nuclear fusion in a reactor.

We could use the spontaneous annihilation of the BEC, and the subsequent outburst of gamma-rays, to make a powerful laser.