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rectangular microchannel  (VitroCom Inc)

 
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    VitroCom Inc rectangular microchannel
    Rectangular Microchannel, supplied by VitroCom Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/result/rectangular microchannel/product/VitroCom Inc
    Average 90 stars, based on 1 article reviews
    rectangular microchannel - by Bioz Stars, 2026-05
    90/100 stars

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    a , Basic crystal structure of LLTO, consisting of alternating Li-rich and -poor layers and Ti and O octahedra. b , Calculated partial density of states (DOS) for LLTO and indicated transitions for the XUV-SHG probe. c , Overview of the experimental setup used for measurement of XUV-SHG data in reflection geometry. The inset shows the layered sample structure with repeating layers of LLTO and LCO. d , Schematic representation of an LCO–LLTO stack forming a prototypical battery, with the XUV-SHG process indicated on the top surface; note that LLTO is polycrystalline in the film measured despite the schematic representation. XFEL, X-ray free-electron laser. MCP, <t>microchannel</t> plate.
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    a , Basic crystal structure of LLTO, consisting of alternating Li-rich and -poor layers and Ti and O octahedra. b , Calculated partial density of states (DOS) for LLTO and indicated transitions for the XUV-SHG probe. c , Overview of the experimental setup used for measurement of XUV-SHG data in reflection geometry. The inset shows the layered sample structure with repeating layers of LLTO and LCO. d , Schematic representation of an LCO–LLTO stack forming a prototypical battery, with the XUV-SHG process indicated on the top surface; note that LLTO is polycrystalline in the film measured despite the schematic representation. XFEL, X-ray free-electron laser. MCP, <t>microchannel</t> plate.
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    a , Basic crystal structure of LLTO, consisting of alternating Li-rich and -poor layers and Ti and O octahedra. b , Calculated partial density of states (DOS) for LLTO and indicated transitions for the XUV-SHG probe. c , Overview of the experimental setup used for measurement of XUV-SHG data in reflection geometry. The inset shows the layered sample structure with repeating layers of LLTO and LCO. d , Schematic representation of an LCO–LLTO stack forming a prototypical battery, with the XUV-SHG process indicated on the top surface; note that LLTO is polycrystalline in the film measured despite the schematic representation. XFEL, X-ray free-electron laser. MCP, <t>microchannel</t> plate.
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    a , Basic crystal structure of LLTO, consisting of alternating Li-rich and -poor layers and Ti and O octahedra. b , Calculated partial density of states (DOS) for LLTO and indicated transitions for the XUV-SHG probe. c , Overview of the experimental setup used for measurement of XUV-SHG data in reflection geometry. The inset shows the layered sample structure with repeating layers of LLTO and LCO. d , Schematic representation of an LCO–LLTO stack forming a prototypical battery, with the XUV-SHG process indicated on the top surface; note that LLTO is polycrystalline in the film measured despite the schematic representation. XFEL, X-ray free-electron laser. MCP, <t>microchannel</t> plate.
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    a , Basic crystal structure of LLTO, consisting of alternating Li-rich and -poor layers and Ti and O octahedra. b , Calculated partial density of states (DOS) for LLTO and indicated transitions for the XUV-SHG probe. c , Overview of the experimental setup used for measurement of XUV-SHG data in reflection geometry. The inset shows the layered sample structure with repeating layers of LLTO and LCO. d , Schematic representation of an LCO–LLTO stack forming a prototypical battery, with the XUV-SHG process indicated on the top surface; note that LLTO is polycrystalline in the film measured despite the schematic representation. XFEL, X-ray free-electron laser. MCP, <t>microchannel</t> plate.
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    Image Search Results


    a , Basic crystal structure of LLTO, consisting of alternating Li-rich and -poor layers and Ti and O octahedra. b , Calculated partial density of states (DOS) for LLTO and indicated transitions for the XUV-SHG probe. c , Overview of the experimental setup used for measurement of XUV-SHG data in reflection geometry. The inset shows the layered sample structure with repeating layers of LLTO and LCO. d , Schematic representation of an LCO–LLTO stack forming a prototypical battery, with the XUV-SHG process indicated on the top surface; note that LLTO is polycrystalline in the film measured despite the schematic representation. XFEL, X-ray free-electron laser. MCP, microchannel plate.

    Journal: Nature Materials

    Article Title: Probing lithium mobility at a solid electrolyte surface

    doi: 10.1038/s41563-023-01535-y

    Figure Lengend Snippet: a , Basic crystal structure of LLTO, consisting of alternating Li-rich and -poor layers and Ti and O octahedra. b , Calculated partial density of states (DOS) for LLTO and indicated transitions for the XUV-SHG probe. c , Overview of the experimental setup used for measurement of XUV-SHG data in reflection geometry. The inset shows the layered sample structure with repeating layers of LLTO and LCO. d , Schematic representation of an LCO–LLTO stack forming a prototypical battery, with the XUV-SHG process indicated on the top surface; note that LLTO is polycrystalline in the film measured despite the schematic representation. XFEL, X-ray free-electron laser. MCP, microchannel plate.

    Article Snippet: The beam was dispersed using a diffraction grating with 1,200 grooves mm –1 before collection on a microchannel plate detector (Rectangular, Hamamatsu Photonics) coated with CsI.

    Techniques: Battery