2007
DOI: 10.1063/1.2722413
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Experimental setup for low-energy laser-based angle resolved photoemission spectroscopy

Abstract: A laser-based angle resolved photoemission (ARPES) system utilizing 6 eV photons from the fourth harmonic of a mode-locked Ti:sapphire oscillator is described. This light source greatly increases the momentum resolution and photoelectron count rate, while reducing extrinsic background and surface sensitivity relative to higher energy light sources. In this review, the optical system is described, and special experimental considerations for low-energy ARPES are discussed. The calibration of the hemispherical el… Show more

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Cited by 74 publications
(70 citation statements)
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“…The TSS of Bi 2 Se 3 extends several layers deep into the bulk (about 2-3 nm) and therefore appears in the spectroscopy for a wide range of probing depths. Indeed, enhanced bulk sensitivity at 6-eV photon energy is provided by an order-of-magnitude larger probing depth than at 50-70 eV [27], and similarly at photon energies in the x-ray range. Specifically, our detailed analysis of the initial state identifies the low binding-energy states in Bi 2 Se 3 as mainly arising from different p orbitals of Bi (6p 3 ) and Se (4p 4 ).…”
Section: Discussionmentioning
confidence: 99%
“…The TSS of Bi 2 Se 3 extends several layers deep into the bulk (about 2-3 nm) and therefore appears in the spectroscopy for a wide range of probing depths. Indeed, enhanced bulk sensitivity at 6-eV photon energy is provided by an order-of-magnitude larger probing depth than at 50-70 eV [27], and similarly at photon energies in the x-ray range. Specifically, our detailed analysis of the initial state identifies the low binding-energy states in Bi 2 Se 3 as mainly arising from different p orbitals of Bi (6p 3 ) and Se (4p 4 ).…”
Section: Discussionmentioning
confidence: 99%
“…These finite widths represent the small chance that electrons interacting with the medium, primarily through electron-hole pair creation and plasmonic interaction, will have energy within the final-state gap. Typically, this final-state effect in ARPES is not used to measure unoccupied states, which are instead mapped by inverse photoemission[8] or very-low-energy electron diffraction [5,[9][10][11][12].Here we show that laser-based ARPES [13][14][15], under certain conditions, can be used to map final-state gaps in the electronic states of a material. This method provides the following advantages with respect to standard synchrotron-based ARPES: (a) improved momentum resolution and greater bulk sensitivity, due to the lower photon energy range available in laser-ARPES (6-7 eV)[13], * alanzara@lbl.gov and (b) access to unoccupied electron states closer to the Fermi level.…”
mentioning
confidence: 99%
“…Here we show that laser-based ARPES [13][14][15], under certain conditions, can be used to map final-state gaps in the electronic states of a material. This method provides the following advantages with respect to standard synchrotron-based ARPES: (a) improved momentum resolution and greater bulk sensitivity, due to the lower photon energy range available in laser-ARPES (6-7 eV) [13], * alanzara@lbl.gov and (b) access to unoccupied electron states closer to the Fermi level.…”
mentioning
confidence: 99%
“…[4] these lower orders can serve as an ideal pump pulse for many small molecules of intense theoretical interest with their first absorption band in the VUV. They also can serve as a compact table top source for angle resolved photoemission spectroscopy (ARPES) [5]. Here we demonstrate that by inserting a fluoride window into the path of an HHG beamline, the low orders of an HHG comb can be temporally separated and be used for femtosecond pump probe experiments.…”
mentioning
confidence: 99%
“…The spectrum of odd harmonics produced by intense femtosecond lasers in gas targets is typically divided into a "plateau" regime, where the harmonic yield is comparable from one harmonic to the next, and a "cutoff" regime, where the harmonic yield falls off rapidly with photon energy. Neglected in this description are the first few orders (3,5,7) which are usually much more intense than the plateau harmonics. As demonstrated by Kosma et.…”
mentioning
confidence: 99%