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horiba confocal raman microscope  (HORIBA Ltd)


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    Structured Review

    HORIBA Ltd horiba confocal raman microscope
    a TEM image of NGDY. b , c HR-TEM images of NGDY. d SAED pattern of NGDY. e HR-TEM image of stacked crystalline NGDY nanosheets. f The magnified HR-TEM image. g AFM image of NGDY nanosheet. h AFM image of stacked NGDY nanosheets. i HR-TEM image of NGDY showing interlayer spacing. j The cross-sectional analysis along the line in ( g )–( i ). k Top view and l side view of the crystal structure of NGDY with 9-layers stacking structure. m Simulated SAED pattern using the 9-layers stacking structure mode. n <t>Raman</t> spectrum of NGDY. o XPS C 1 s spectrum of NGDY. p XPS N 1 s spectrum of NGDY. Source data are provided as a Source Data file.
    Horiba Confocal Raman Microscope, supplied by HORIBA Ltd, used in various techniques. Bioz Stars score: 96/100, based on 390 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/product/raman+microscope/Modular+Raman+Microscope/pmc13392032-328-1-1
    Average 96 stars, based on 390 article reviews
    horiba confocal raman microscope - by Bioz Stars, 2026-11
    96/100 stars

    Images

    1) Product Images from "Direct solar energy charging of metal||air batteries enabled by photo-coupled electrodes"

    Article Title: Direct solar energy charging of metal||air batteries enabled by photo-coupled electrodes

    Journal: Nature Communications

    doi: 10.1038/s41467-026-73926-z

    a TEM image of NGDY. b , c HR-TEM images of NGDY. d SAED pattern of NGDY. e HR-TEM image of stacked crystalline NGDY nanosheets. f The magnified HR-TEM image. g AFM image of NGDY nanosheet. h AFM image of stacked NGDY nanosheets. i HR-TEM image of NGDY showing interlayer spacing. j The cross-sectional analysis along the line in ( g )–( i ). k Top view and l side view of the crystal structure of NGDY with 9-layers stacking structure. m Simulated SAED pattern using the 9-layers stacking structure mode. n Raman spectrum of NGDY. o XPS C 1 s spectrum of NGDY. p XPS N 1 s spectrum of NGDY. Source data are provided as a Source Data file.
    Figure Legend Snippet: a TEM image of NGDY. b , c HR-TEM images of NGDY. d SAED pattern of NGDY. e HR-TEM image of stacked crystalline NGDY nanosheets. f The magnified HR-TEM image. g AFM image of NGDY nanosheet. h AFM image of stacked NGDY nanosheets. i HR-TEM image of NGDY showing interlayer spacing. j The cross-sectional analysis along the line in ( g )–( i ). k Top view and l side view of the crystal structure of NGDY with 9-layers stacking structure. m Simulated SAED pattern using the 9-layers stacking structure mode. n Raman spectrum of NGDY. o XPS C 1 s spectrum of NGDY. p XPS N 1 s spectrum of NGDY. Source data are provided as a Source Data file.

    Techniques Used:

    a XPS N 1 s spectra of NGDY in the dark and under light irradiation. b XPS C 1 s spectra of NGDY in the dark and under light irradiation. c The ratio changes of sp -C/ sp 2 -C under light irradiation. d Raman spectra of NGDY in the dark and under light irradiation. e The 2D color-filled contour plot of the Raman spectra magnified in the dashed box in ( d ). f Schematic illustration of the photo-generated electron-hole pairs separation process in NGDY. g The transition map of electrons and holes in NGDY under the light excitation. h SPV image of NGDY. i Line profiles of the SPV of NGDY. j Schematic illustration of a conventional photoelectrode and our proposed light-induced dynamic reconfiguration of sp -C. Source data are provided as a Source Data file.
    Figure Legend Snippet: a XPS N 1 s spectra of NGDY in the dark and under light irradiation. b XPS C 1 s spectra of NGDY in the dark and under light irradiation. c The ratio changes of sp -C/ sp 2 -C under light irradiation. d Raman spectra of NGDY in the dark and under light irradiation. e The 2D color-filled contour plot of the Raman spectra magnified in the dashed box in ( d ). f Schematic illustration of the photo-generated electron-hole pairs separation process in NGDY. g The transition map of electrons and holes in NGDY under the light excitation. h SPV image of NGDY. i Line profiles of the SPV of NGDY. j Schematic illustration of a conventional photoelectrode and our proposed light-induced dynamic reconfiguration of sp -C. Source data are provided as a Source Data file.

    Techniques Used: Irradiation, Generated

    a In-situ Raman spectra of NGDY-based PZAB during the charging process in the dark. b In-situ Raman spectra of NGDY-based PZAB during the charging process under light irradiation, and c the corresponding 2D color-filled contour plot of the in-situ Raman spectra (Left: in the dark. Right: under light irradiation. Recorded during a LSV scan of the battery charging voltage from 1.6 V to 2.4 V at a scan rate of 0.1 mV s −1 , with spectra acquired at every 0.1 V interval). d Schematic illustration of OER pathways on the NGDY in the dark and under light irradiation. e Free energy diagrams of different sites for OER. f In-situ Raman spectra of NGDY-based PLOB in the dark. g In-situ Raman spectra of NGDY-based PLOB under light irradiation. The spectra were collected over a full cycle: discharging from 2.8 V to 1.6 V and then charging from 3.0 V to 4.2 V at a scan rate of 0.1 mV s −1 , with spectra recorded at 0.2 V intervals. h The corresponding 2D color-filled contour plot of the in-situ Raman spectra of NGDY-based PLOB during the charging process (Left: in the dark. Right: under light irradiation). Free energy diagrams at zero, equilibrium, discharge and charge voltages of NGDY for PLOB at i ground state and j excited state. All in-situ measurements were performed at 25 ± 0.5 °C. Source data are provided as a Source Data file.
    Figure Legend Snippet: a In-situ Raman spectra of NGDY-based PZAB during the charging process in the dark. b In-situ Raman spectra of NGDY-based PZAB during the charging process under light irradiation, and c the corresponding 2D color-filled contour plot of the in-situ Raman spectra (Left: in the dark. Right: under light irradiation. Recorded during a LSV scan of the battery charging voltage from 1.6 V to 2.4 V at a scan rate of 0.1 mV s −1 , with spectra acquired at every 0.1 V interval). d Schematic illustration of OER pathways on the NGDY in the dark and under light irradiation. e Free energy diagrams of different sites for OER. f In-situ Raman spectra of NGDY-based PLOB in the dark. g In-situ Raman spectra of NGDY-based PLOB under light irradiation. The spectra were collected over a full cycle: discharging from 2.8 V to 1.6 V and then charging from 3.0 V to 4.2 V at a scan rate of 0.1 mV s −1 , with spectra recorded at 0.2 V intervals. h The corresponding 2D color-filled contour plot of the in-situ Raman spectra of NGDY-based PLOB during the charging process (Left: in the dark. Right: under light irradiation). Free energy diagrams at zero, equilibrium, discharge and charge voltages of NGDY for PLOB at i ground state and j excited state. All in-situ measurements were performed at 25 ± 0.5 °C. Source data are provided as a Source Data file.

    Techniques Used: In Situ, Irradiation, Battery

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    Article Snippet: X-ray photoelectron spectroscopy (XPS) was performed on a Thermo Scientific K-Alpha spectrometer (Thermo Fisher Scientific, Waltham, MA, USA) using a monochromatic Al Kα source, with the C 1s peak (284.6 eV) as a reference for charge correction. .. Raman spectra were collected by a Raman microscope (HORIBA LabRAM HR 800, HORIBA Jobin Yvon, Paris, France) equipped with a solid-state laser at 532 nm as the excitation source from 200 to 800 cm−1, recorded at a resolution of 1 cm−1. .. Electron paramagnetic resonance (EPR) was performed on a Bruker A300-10 (Bruker BioSpin GmbH, Ettlingen, Germany) under vacuum conditions at room temperature without light illumination.

    Article Title: Modification of Single-Walled Carbon Nanotubes with Halogen-Substituted Metal Phthalocyanines for Chemiresistive Ammonia Detection
    Article Snippet: .. The spectra were measured in backscattering collection geometry with a Raman microscope (Horiba Ltd., Kyoto, Japan). ..

    Article Title: The hydrogen puzzle in rock-enhanced biochar: Pyrogenic coating, mineral redox and pore accessibility
    Article Snippet: .. Raman spectroscopy was conducted under a LabRAM HR 800 Raman microscope (HORIBA Europe GmbH, Oberursel, Germany), which was coupled to an BX41 light microscope (Olympus Corporation, Tokyo, Japan). .. Raman spectroscopy was conducted under a LabRAM HR 800 Raman microscope (HORIBA Europe GmbH, Oberursel, Germany), which was coupled to an BX41 light microscope (Olympus Corporation, Tokyo, Japan).

    Article Title: Suspension plasma sprayed yttria-stabilized zirconia coatings from a non-flammable solvent: A story of thermal cycling, erosion, and calcium-magnesium-alumino-silicate
    Article Snippet: .. Raman spectroscopic investigations of the CMAS-exposed coatings were performed on polished cross-sections using a HORIBA LabRAM HR Raman microscope (Horiba Jobin YVON, Japan) equipped with a Synapse detector and a motorized XYZ translation stage (Marzhauser, Germany). ..

    Article Title: Cation–Carbonate Ion Pairing Suppresses Electrochemical Nitrate Reduction
    Article Snippet: .. In situ Raman measurements were carried out with a Raman microscope (LabRam, Horiba HR Evolution) and a customized in situ cell based on Li et al. A water-immersible objective (60× magnification, W.D. ..

    Article Title: Laser induced graphene interdigitated electrode sensor for direct detection of over-humidification in polymer electrolyte fuel cells
    Article Snippet: .. Raman spectroscopy is performed using a confocal Raman microscope (Horiba Jobin Yvon) equipped with a 633 nm excitation laser and an 1800 grooves mm− 1 grating, providing a spectral resolution of 0.35 cm− 1. ..

    Article Title: Cooperative Solvent‐Thermal Interactions Enable Multi‐Material Nanotransfer Printing for Multi‐Dimensional Molecular Profiling
    Article Snippet: .. Raman scattering signals were collected using a dispersive Raman microscope (ARAMIS, Horiba) system including excitation lasers with wavelengths of λ = 514, 633, and 785 nm. ..

    Article Title: Modularly integrated synergistic SERS strategy for ultra-trace detection of imidacloprid in fresh fruit and vegetable juices
    Article Snippet: .. Raman spectra were acquired using a Raman microscope (LabRAM HR, Horiba France SAS, Palaiseau, France). .. IMI recovery was determined using an HPLC system equipped with a 2998 PDA (Acquity Arc, Waters Co., Milford, USA).

    Raman Spectroscopy:

    Article Title: The hydrogen puzzle in rock-enhanced biochar: Pyrogenic coating, mineral redox and pore accessibility
    Article Snippet: .. Raman spectroscopy was conducted under a LabRAM HR 800 Raman microscope (HORIBA Europe GmbH, Oberursel, Germany), which was coupled to an BX41 light microscope (Olympus Corporation, Tokyo, Japan). .. Raman spectroscopy was conducted under a LabRAM HR 800 Raman microscope (HORIBA Europe GmbH, Oberursel, Germany), which was coupled to an BX41 light microscope (Olympus Corporation, Tokyo, Japan).

    Article Title: Laser induced graphene interdigitated electrode sensor for direct detection of over-humidification in polymer electrolyte fuel cells
    Article Snippet: .. Raman spectroscopy is performed using a confocal Raman microscope (Horiba Jobin Yvon) equipped with a 633 nm excitation laser and an 1800 grooves mm− 1 grating, providing a spectral resolution of 0.35 cm− 1. ..

    Light Microscopy:

    Article Title: The hydrogen puzzle in rock-enhanced biochar: Pyrogenic coating, mineral redox and pore accessibility
    Article Snippet: .. Raman spectroscopy was conducted under a LabRAM HR 800 Raman microscope (HORIBA Europe GmbH, Oberursel, Germany), which was coupled to an BX41 light microscope (Olympus Corporation, Tokyo, Japan). .. Raman spectroscopy was conducted under a LabRAM HR 800 Raman microscope (HORIBA Europe GmbH, Oberursel, Germany), which was coupled to an BX41 light microscope (Olympus Corporation, Tokyo, Japan).

    In Situ:

    Article Title: Cation–Carbonate Ion Pairing Suppresses Electrochemical Nitrate Reduction
    Article Snippet: .. In situ Raman measurements were carried out with a Raman microscope (LabRam, Horiba HR Evolution) and a customized in situ cell based on Li et al. A water-immersible objective (60× magnification, W.D. ..



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    Image Search Results


    Crystal structures from single-crystal X-ray diffraction showing the low- and high-temperature phases of (a) BA 2 SnI 4 at 125 K (structural data from ref ) and 296 K and of (b) DABSnI 4 at 100 and 296 K, determined in this work. Evolution of structural parameters determined from single-crystal XRD structures: (c) interplanar distances between inorganic layers (measured as the distance between iodides in the apical position), (d) in-plan tilt angle (D in ), the out-of-plane tilt angle (D out ), octahedral tilting (D tilt ), and (e) quadratic elongation. See Table S3 for additional details. The structural parameters for BA 2 SnI 4 at 125 K are calculated from the crystal structures reported in ref . Temperature-dependent low-energy Raman spectra of (f) BA 2 SnI 4 measured with a 785 nm laser, with a cutoff filter at 50 cm –1 (after 230 cm –1 , the wavenumbers are multiplied by a factor of 5 for clarity), and (g) DABSnI 4 , measured with 647.1 nm laser excitation. The main spectral changes occurring at the phase transitions are highlighted in the insets.

    Journal: Journal of the American Chemical Society

    Article Title: Structural Rigidity Enables Amplified Spontaneous Emission in 2D Alkylammonium Tin Perovskites

    doi: 10.1021/jacs.6c14883

    Figure Lengend Snippet: Crystal structures from single-crystal X-ray diffraction showing the low- and high-temperature phases of (a) BA 2 SnI 4 at 125 K (structural data from ref ) and 296 K and of (b) DABSnI 4 at 100 and 296 K, determined in this work. Evolution of structural parameters determined from single-crystal XRD structures: (c) interplanar distances between inorganic layers (measured as the distance between iodides in the apical position), (d) in-plan tilt angle (D in ), the out-of-plane tilt angle (D out ), octahedral tilting (D tilt ), and (e) quadratic elongation. See Table S3 for additional details. The structural parameters for BA 2 SnI 4 at 125 K are calculated from the crystal structures reported in ref . Temperature-dependent low-energy Raman spectra of (f) BA 2 SnI 4 measured with a 785 nm laser, with a cutoff filter at 50 cm –1 (after 230 cm –1 , the wavenumbers are multiplied by a factor of 5 for clarity), and (g) DABSnI 4 , measured with 647.1 nm laser excitation. The main spectral changes occurring at the phase transitions are highlighted in the insets.

    Article Snippet: The Raman spectra of BA 2 SnI 4 were acquired with a confocal Raman microscope (Horiba Xplora Plus, Horiba) equipped with edge filters enabling measurements as close as 50 cm –1 to the Rayleigh line.

    Techniques: Phase Transitions