D. A. Shirley
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View article: RESONANCE AND THRESHOLD EFFECTS IN PHOTOEMISSION UP TO 3500 eV
RESONANCE AND THRESHOLD EFFECTS IN PHOTOEMISSION UP TO 3500 eV Open
Beam lines at the Stanford Synchrotron Radiation Laboratory (SSRL) now provide photon beams throughout the entire energy range 5 to 5000 eV, with a pulse structure very well-suited to time-of-flight (TOF) photoelectron spectroscopy. We hav…
View article: Surface structure determination of Au(1 ML)/Fe(15 ML)/Au(100) using angle-resolved photoemission extended fine structure
Surface structure determination of Au(1 ML)/Fe(15 ML)/Au(100) using angle-resolved photoemission extended fine structure Open
We have determined the atomic surface structure of a thin film of Fe (15 ML) grown on the Au(100) surface, Au(1 ML)/Fe(15 ML)/Au(100), with angle-resolved photoemission extended fine structure (ARPEFS) using the Au ${4f}_{7/2}$ core level.…
View article: The surface structure of (1x1)O/W(110)x12 determined by angle-resolved photoemission extended fine structure
The surface structure of (1x1)O/W(110)x12 determined by angle-resolved photoemission extended fine structure Open
Oxygen adsorption on tungsten is one of the earliest and most studied model adsorption systems. Researchers have identified multiple coverage-dependent phases on the W(110) face. The three ordered phases are the (2x1) with a coverage of {t…
View article: The structural determination of Au(1ML)/Fe(15ML)/Au(100) using angle-resolved photoemission extended fine structure
The structural determination of Au(1ML)/Fe(15ML)/Au(100) using angle-resolved photoemission extended fine structure Open
A great amount of attention has been given to investigating thin magnetic films and magnetic multilayers, especially systems involving iron and the noble metals. In most of these studies the authors assume that the Fe layers will maintain …
View article: Adsorption site and structure determination of c(2 × 2) (100) using angle-resolved photoemission extended fine structure
Adsorption site and structure determination of c(2 × 2) (100) using angle-resolved photoemission extended fine structure Open
View article: Holographic atom imaging from experimental photoelectron angular distribution patterns
Holographic atom imaging from experimental photoelectron angular distribution patterns Open
One of the most challenging areas of materials research is the imaging of technologically relevant materials with microscopic and atomic-scale resolution. As part of the development of these methods, near-surface atoms in single crystals w…
View article: Workshop on Soft X-Ray Interferometry
Workshop on Soft X-Ray Interferometry Open
Author(s): Howells, M.; Hussein, Z.; Moler, E.J.; Moller, D.; Roesler, F.; Shirley, D.A.; Thorne, A.
View article: A Detailed Study of c(2x2)Cl/Cu(001) Adsorbate Geometry and Substrate Surface Relaxation Using Temperature Dependent Angle-Resolved Photoemission Extended Fine Structure
A Detailed Study of c(2x2)Cl/Cu(001) Adsorbate Geometry and Substrate Surface Relaxation Using Temperature Dependent Angle-Resolved Photoemission Extended Fine Structure Open
Author(s): Wang, L.-Q.; Wittenau, A.E. Schach von; Ji, Z.G.; Wang, L.S.; Huang, Z.Q.; Shirley, D.A.
View article: The LBL 55-meter spherical grating monochromator at SSRL (Stanford Synchrotron Radiation Laboratory)
The LBL 55-meter spherical grating monochromator at SSRL (Stanford Synchrotron Radiation Laboratory) Open
The Lawrence Berkeley Laboratory 55-m spherical grating monochromator (SGM) beamline is located as a branch line of the 54-pole wiggler/undulator at the Stanford Synchrotron Radiation Laboratory (SSRL). It was designed and constructed by L…
View article: Threshold photoelectron spectrum of the Argon 3s satellites
Threshold photoelectron spectrum of the Argon 3s satellites Open
Lately a variety of techniques have studied the electron correlation satellites with binding energies between the Argon 3s binding energy (29.24 eV) and the 2p/sup /minus/2/ ionization potential (43.38 eV). One of these techniques, Thresho…
View article: REPLY TO THE COMMENT ON ""GEOMETRY OF (2X2)S/CU(001) DETERMINED WITH USE OF ANGLE-RESOLVED PHOTOEMISSION EXTENDED FINE STRUCTURE""
REPLY TO THE COMMENT ON ""GEOMETRY OF (2X2)S/CU(001) DETERMINED WITH USE OF ANGLE-RESOLVED PHOTOEMISSION EXTENDED FINE STRUCTURE"" Open
View article: Orbital-collapse effects in photoemission from atomic Eu
Orbital-collapse effects in photoemission from atomic Eu Open
Resonant photoelectron spectra of atomic Eu have been measured in the photon-energy ranges of the ``4d\ensuremath{\rightarrow}4f '' (110--170 eV) and 3d\ensuremath{\rightarrow}4f (1120--1165 eV) excitations. For the ``4d\ensuremath{\righta…
View article: Increasing quantum yield of sodium salicylate above 80 eV photon energy: Implications for photoemission cross sections
Increasing quantum yield of sodium salicylate above 80 eV photon energy: Implications for photoemission cross sections Open
The quantum yield of the visible scintillator sodium salicylate is found to increase in the incident photon-energy range 80--270 eV. Because of its use as a photon-flux monitor in recent gas-phase photoelectron spectroscopy measurements, p…
View article: Experimental and theoretical investigations of Cr(001) surface electronic structure
Experimental and theoretical investigations of Cr(001) surface electronic structure Open
The surface electronic structure of Cr(001) is characterized by angle-resolved photoelectron spectroscopy. The spectral properties of surface-related photoemission features are found to be consistent with results from a comprehensive spin-…
View article: Valence photoelectron satellites of neon
Valence photoelectron satellites of neon Open
Synchrotron radiation was directed at neon gas, creating ${\mathrm{Ne}}^{+}$ ions in ``satellite'' states characterized by the configurations 1${s}^{2}$2${s}^{2}$2${p}^{4}$nl, in addition to the main-line final states: 2${s}^{\mathrm{\ensu…
View article: Angle-resolved photoemission extended fine structure
Angle-resolved photoemission extended fine structure Open
Measurements of the Angle-Resolved Photoemission Extended Fine Structure (ARPEFS) from the S(1s) core level of a c(2 x 2)S/Ni(001) are analyzed to determine the spacing between the S overlayer and the first and second Ni layers. ARPEFS is …
View article: <title>Gas-Phase Photoemission With Soft X-Rays: Cross Sections And Angular Distributions</title>
Gas-Phase Photoemission With Soft X-Rays: Cross Sections And Angular Distributions Open
A summary is presented of typical gas-phase photoemission studies based on synchrotron radiation in the 50-5000 eV range, using beam lines at the Stanford Synchrotron Radiation Laboratory. Three topics are addressed: atomic inner-shell pho…
View article: Auger decay mechanism in photon-stimulated desorption from sodium fluoride
Auger decay mechanism in photon-stimulated desorption from sodium fluoride Open
Photon-stimulated desorption experiments were performed on the (001) face of LiF for photon energies near the F(2s) and Li(ls) edges (from 37 to 72 eV). There are structures in the F{sup +} yield above the F(2s) edge which are absent in th…
View article: Direct determination of surface structures from photoelectron diffraction
Direct determination of surface structures from photoelectron diffraction Open
Angle‐resolved photoemission extended fine structure (ARPEFS) is induced by interference between primary and elastically scattered photoelectron waves originating from an adsorbate core level on an ordered surface. Analysis by procedures a…
View article: A new wiggler beam line for SSRL
A new wiggler beam line for SSRL Open
View article: Photoelectron and Auger electron asymmetries: Alignment of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">Xe</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo><mml:mn>2</mml:mn><mml:mn/></mml:mrow></mml:msup></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mfrac><mml:mrow><mml:mn>5</mml:mn></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mfrac></mml:mrow></mml:msub></mml:mrow></mml:math>by photoionization
Photoelectron and Auger electron asymmetries: Alignment ofby photoionization Open
We measured angular distributions of photoelectrons from the Xe 4d subshell, and N4,5OO Auger electrons using synchrotron radiation. The 4d asymmetry parameter exhibits strong oscillations with energy, in agreement with several …
View article: Substrate-Dependent<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">C</mml:mi><mml:mn/><mml:mo>(</mml:mo><mml:mn>1</mml:mn><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:mn/></mml:math>Shape Resonance in CO Overlayers on Ni(111) and Ni(001)
Substrate-DependentShape Resonance in CO Overlayers on Ni(111) and Ni(001) Open
A large resonance was observed in the C(1s) angle-resolved photoemission cross-section of CO overlayers on Ni(111) and Ni(001), using synchrotron radiation at SSRL, while none was observed for O(1s). Energy-, angular-, and polarization-dep…
View article: Photoemission from solids: The transition from solid-state to atomic physics
Photoemission from solids: The transition from solid-state to atomic physics Open
As the photon energy is increased, photoemission from solids undergoes a slow transition from solid-state to atomic behavior. However, throughout the energy range h..nu.. = 10 to 1000 eV or higher both types of phenomena are present. Thus …
View article: Angle-resolved photoemission measurements of band discontinuities in the GaAs-Ge heterojunction
Angle-resolved photoemission measurements of band discontinuities in the GaAs-Ge heterojunction Open
The conduction- and valence-band discontinuities for the (110) GaAs-Ge heterojunction have been measured as ΔEc=0.50 eV and ΔEv=0.25 eV by the angle-resolved ultraviolet photoemission (ARUPS) technique. These values are in good agreement w…
View article: Identification of a Surface State on the (111) Terraces of Stepped Cu(211).
Identification of a Surface State on the (111) Terraces of Stepped Cu(211). Open
The surface electronic structure of a stepped Cu(211) crystal was elucidated by angle-resolved photoemission spectroscopy. A surface state was found on the three-atom terraces, indicating that the terrace surface potential resembles that o…
View article: D-ORBITAL DIRECTED PHOTOEMISSION FROM MANGANESE FLUORIDE SINGLE CRYSTALS USING A1Kalpha RADIATION
D-ORBITAL DIRECTED PHOTOEMISSION FROM MANGANESE FLUORIDE SINGLE CRYSTALS USING A1Kalpha RADIATION Open
Angle-resolved photoemission energy distributions (PED's) were obtained from valence bands of MnF{sub 2} single crystals using AlK{alpha} radiation. A pronounced variation in the PED's was observed as the electron take-off angle was varied…
View article: Electron-correlation satellites in electron spectroscopy
Electron-correlation satellites in electron spectroscopy Open
View article: NUCLEAR ORIENTATION OP 2.3-d GOLD-198m
NUCLEAR ORIENTATION OP 2.3-d GOLD-198m Open
View article: Electronic density of states and bonding in chalcopyrite-type semiconductors
Electronic density of states and bonding in chalcopyrite-type semiconductors Open
Measured x-ray-photoemission spectra for ZnGe${\mathrm{P}}_{2}$ and CdSn${\mathrm{As}}_{2}$ are presented along with density-of-states $N(E)$ and charge-density calculations for ZnGe${\mathrm{P}}_{2}$. Analysis of the density-of-states spe…
View article: Summary of the international conference on hyperfine interactions studied by nuclear reactions and decay
Summary of the international conference on hyperfine interactions studied by nuclear reactions and decay Open