Helium-3 surface spin echo

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Helium-3 surface spin echo (HeSE) is an inelastic scattering technique in surface science that has been used to measure microscopic dynamics at well-defined surfaces in ultra-high vacuum. The information available from HeSE complements and extends that available from other inelastic scattering techniques such as neutron spin echo and traditional helium-4 atom scattering (HAS).

Principles

The experimental principles of the HeSE experiment are analogous to those of neutron spin echo, differing in details such as the nature of the probe/sample interactions that give rise to scattering. In outline, a polarized 3He beam is created by a supersonic expansion followed by a spin-filtering stage (polariser). The helium scatters from the experimental sample and is detected at the end of the beamline after another spin-filtering stage (analyser). Before and after the scattering process, the beam passes through magnetic fields that precess the probe spins in the usual sense of a spin echo experiment. The raw data of the experiment are the spin-resolved scattered helium intensities as a function of the incoming magnetic field integral, outgoing field integral and any other variable parameters relevant to specific experiments, such as surface orientation and temperature. In the most general kind of scattering-with-precession experiment, the data can be used to construct the 2D 'wavelength intensity matrix' [1] for the surface scattering process, i.e. the probability that a helium atom of a certain incoming wavelength scatters into a state with a certain outgoing wavelength.

Conventional 'spin echo' measurements are a common special case of the more general scattering-with-precession measurements, in which the incoming and outgoing magnetic field integrals are constrained to be equal. The polarization of the outgoing beam is measured as a function of the precession field integral by measuring the intensity of the outgoing beam resolved into different spin states. The spin echo case is referred to as a type of 'tilted projection measurement'.[2] Spin echo measurements are an appropriate tilted projection for quasi-elastic measurements of surface dynamics because the raw data are closely related to the intermediate scattering function (ISF), which in many cases can be interpreted in terms of standard dynamical signatures.[3]

Applications

The surface processes that HeSE can measure can be broadly divided into elastic, quasielastic and inelastic processes. Measurements in which the predominant signal is elastically scattered include standard helium diffraction and the measurement of selective adsorption resonances. Quasielastic measurements generally correspond to measurements of microscopic surface diffusion in which the Doppler-like energy gain and loss of the helium atoms is small compared to the beam energy. More strongly inelastic measurements can provide information about energy loss channels on the surface such as surface phonons.

Microscopic diffusion

HeSE has been used to study the diffusion rates and mechanisms of atoms and molecules ('adsorbates') at surfaces. A non-exhaustive list of the research themes associated with HeSE diffusion measurements include: nuclear quantum effects in the surface diffusion of atomic hydrogen;[4][5] benchmarking the adsorbate/surface free energy landscape;[6] energy exchange ('friction') between adsorbates and the surface;[7] pairwise [8] and many-body [9] inter-adsorbate interactions.

Selective adsorption resonances

HeSE has been used to construct empirical helium-surface scattering potentials through the measurement of selective adsorption resonances (bound state resonances) on the clean LiF(001) surface [10] and the hydrogenated Si(111) surface.[11]

References

  1. ↑ Kole, P.R.; Jardine, A.P.; Hedgeland, H.; Alexandrowicz, G. (2010). "Measuring surface phonons with a 3He spin echo spectrometer: a two-dimensional approach". J. Phys.: Condens. Matter 22 (304018): 304018. doi:10.1088/0953-8984/22/30/304018. PMID 21399350. 
  2. ↑ Alexandrowicz, G.; Jardine, A.P. (2007). "Helium spin echo spectroscopy: studying surface dynamics with ultra-high-energy resolution". J. Phys.: Condens. Matter 19 (305001): 305001. doi:10.1088/0953-8984/19/30/305001. 
  3. ↑ Jardine, A.P.; Hedgeland, H.; Alexandrowicz, G.; Allison, W.; Ellis, J. (2009). "Helium-3 spin-echo: Principles and application to dynamics at surfaces". Prog. Surf. Sci. 84 (11–12): 323–379. doi:10.1016/j.progsurf.2009.07.001. 
  4. ↑ Jardine, A.P.; Lee, E.Y.M.; Ward, D.J.; Alexandrowicz, G.; Hedgeland, H.; Allison, W.; Ellis, J.; Pollak, E. (24 September 2010). "Determination of the Quantum Contribution to the Activated Motion of Hydrogen on a Metal Surface: H/Pt(111)". Phys. Rev. Lett. 105 (136101): 136101. doi:10.1103/physrevlett.105.136101. PMID 21230789. 
  5. ↑ McIntosh, Eliza; Wikfeldt, K. Thor; Ellis, John; Michaelides, Angelos; Allison, William (April 19, 2013). "Quantum Effects in the Diffusion of Hydrogen on Ru(0001)". J. Phys. Chem. Lett. 4 (9): 1565–1569. doi:10.1021/jz400622v. PMID 24920996. 
  6. ↑ Lechner, B.A.J.; Kole, P.R.; Hedgeland, H.; Jardine, A.P.; Allison, W.; Hinch, B.J.; Ellis, J. (2014). "Ultra-high precision determination of site energy differences using a Bayesian method". Phys. Rev. B 89 (121405(R)). doi:10.1103/PhysRevB.89.121405. http://oro.open.ac.uk/46462/1/prb2014.pdf. 
  7. ↑ Hedgeland, H.; Kole, P.R.; Davies, H.R.; Jardine, A.P.; Alexandrowicz, G.; Allison, W.; Ellis, J.; Fratesi, G. et al. (2009). "Surface dynamics and friction of K/Cu(001) characterized by helium-3 spin-echo and density functional theory". Phys. Rev. B 80 (125426). doi:10.1103/PhysRevB.80.125426. https://air.unimi.it/bitstream/2434/442441/2/PRB_2009_v80_p125426_Hedgeland_dynamics_friction_K_Cu001_He3_spin-echo_DFT.pdf. 
  8. ↑ Alexandrowicz, G.; Jardine, A.P.; Hedgeland, H.; Allison, W.; Ellis, J. (10 October 2006). "Onset of 3D collective surface diffusion in the presence of lateral interactions: Na/Cu(001).". Phys. Rev. Lett. 97 (156103): 156103. doi:10.1103/PhysRevLett.97.156103. PMID 17155343. Bibcode: 2006PhRvL..97o6103A. 
  9. ↑ Alexandrowicz, Gil; Kole, Pepijn R.; Lee, Everett Y.M.; Hedgeland, Holly; Ferrando, Riccardo; Jardine, Andrew P.; Allison, William; Ellis, John (May 6, 2008). "Prev. Article Next Article Table of Contents Observation of Uncorrelated Microscopic Motion in a Strongly Interacting Adsorbate System". J. Am. Chem. Soc. 130 (21): 6789–6794. doi:10.1021/ja800118x. PMID 18457388. 
  10. ↑ Riley, D.; Jardine, A.P.; Dworski, S.; Alexandrowicz, G.; Fouquet, P.; Ellis, J.; Allison, W. (13 March 2007). "A refined He–LiF(001) potential from selective adsorption resonances measured with high-resolution helium spin-echo spectroscopy". J. Chem. Phys. 126 (104702): 104702. doi:10.1063/1.2464087. PMID 17362076. 
  11. ↑ Tuddenham, F.E.; Hedgeland, H.; Knowling, J.; Jardine, A.P.; Maclaren, D.A.; Alexandrowicz, G.; Ellis, J.; Allison, W. (11 June 2009). "Linewidths in bound state resonances for helium scattering from Si(111)–(1 × 1)H". J. Phys.: Condens. Matter 21 (26): 264004. doi:10.1088/0953-8984/21/26/264004. PMID 21828452. http://eprints.gla.ac.uk/6523/1/6523.pdf. 



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