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Photon source

No commercial instruments specifically for UPS usually an add-on to XPS (incremental cost " 30,000) or done using a synchrotron facility as the photon source... [Pg.23]

Soft X-ray absorption measurements are done at low-energy synchrotron X-ray facilities such as the UV ring at NSLS or the Advanced Photon Source (APS) at Lawrence Berkeley National Laboratory (LBNL). The beam size is typically 1 mm in diameter. The electron yield data are usually obtained in the total electron yield (EY) mode, measuring the current from a channel electron multiplier (Channeltron). Sometimes a voltage bias is applied to increase surface sensitivity. This is referred to as the partial electron yield (PEY) mode. Huorescence yield (EY) data are recorded using a windowless energy dispersive Si (Li) detector. The experiments are conducted in vacuum at a pressure of 2 X 10 torr. [Pg.515]

However, a nonzero background in the experiment always produces a small contribution from the detection events that fall in the central Nq peak. For example, a signal-to-background ratio of 7 leads to an Nc/Nl ratio of about 0.2. In the present case, an Nc/Nl ratio of 0.06 was determined. Hence, the Nc/Nl value also indicates that the present nanocrystal behaves as a single-photon source. [Pg.220]

In this section, we have demonstrated that a single organic dye nanocrystal comprised of many chromophores shows photon antibunching when the size is sufficiently small. The present results indicate that molecular assemblies can also be considered as candidates for new single-photon sources. [Pg.221]

I., Beljonne, D., Champagne, B., Mullen, K., Sauer, M., Hofkens, J. andDe Schryver, F. C. (2004) Multichromophoric dendrimers as single-photon sources a single-molecule study. J. Phys. Chem. B., 108, 16686-16696. [Pg.224]

The PID is nondestructive, relatively inexpensive, of rugged construction and easy to operate. With the 10.2 eV photon source Bost molecules are ionized the exceptions are the penument... [Pg.655]

Fig. 5. Electron escape depth as a function of electron energy. The energies of several photon sources are shown. Fig. 5. Electron escape depth as a function of electron energy. The energies of several photon sources are shown.
It should be mentioned that another synchrotron source, the Advanced Photon Source (APS) will be built at the Argonne National Laboratory and should be operational in the mid-1990s.]... [Pg.287]

A photonic realization of qubit can be obtained through the polarization state of a photon or usingthe continuous phase and amplitude of a many-photon laser beam [5,48]. At first, the difficulty in achieving significant photon-photon interactions necessary for multi-qubit operations can be seen as a drawback of this proposal. However, it was demonstrated that scalable QC is possible using only linear optical circuits and single-photon sources and detectors [16]. The method (known as the KLM scheme for Knill, Laflamme and Milburn) [49] uses quantum interference with auxiliary photons at a beam splitter as the source of interactions, and has... [Pg.191]

In situ CO-TPR XAFS studies were performed at the Materials Research Collaborative Access Team (MR-CAT) beam line at the Advanced Photon Source,... [Pg.122]

Figure 11.11. Integration of nanowire photonics with silicon electronics. Schematic illustrating fabrication of hybrid structures. A silicon-on-insulator (SOI) substrate is patterned by standard electron-beam or photolithography followed by reactive ion etching. Emissive NWs are then aligned onto the patterned SOI substrate to form photonic sources. [Reprinted with permission from Ref. 59. Copyright 2005 Wiley-VCH Verlag.]... Figure 11.11. Integration of nanowire photonics with silicon electronics. Schematic illustrating fabrication of hybrid structures. A silicon-on-insulator (SOI) substrate is patterned by standard electron-beam or photolithography followed by reactive ion etching. Emissive NWs are then aligned onto the patterned SOI substrate to form photonic sources. [Reprinted with permission from Ref. 59. Copyright 2005 Wiley-VCH Verlag.]...
Bulk and micro-XAFS analyses were performed at the PNC-CAT s bending magnet (20-BM) and undulator (20-ID) beamlines of the Advanced Photon Source (APS), Argonne, IL, USA. Other microanalytical and mineralogical characterization studies were conducted at CANMET. Details of the methodology can be found in Paktunc (2008) and other publications by the author. [Pg.359]

The XAFS experiments were carried out at the Pacific Northwest Consortium -Collaborative Access Team s (PNC/XOR) beamline at the Advanced Photon Source... [Pg.361]

Figure 1.4 The electromagnetic spectrum, along with common photon sources and a number of characterization techniques based on photons. Figure 1.4 The electromagnetic spectrum, along with common photon sources and a number of characterization techniques based on photons.
Advanced Photon Source (APS), 26 412 Advanced Photo System (APS), 19 266 Advanced power reactors, 17 594—595 Advanced SclairTech dual-reactor system, 20 197... [Pg.20]


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See also in sourсe #XX -- [ Pg.7 ]




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