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Princeton Instruments electron multiplying intensified ccd emiccd camera
(a) Custom‐built Raman microscopy measurement setup using a CW laser emitting at λ = 532 nm. The setup includes the gas chamber containing grating structures and gas flow at ∼1.95 atm pressure. A spectrometer coupled to an <t>emICCD</t> camera is used to measure the spectra of the gratings in air and in both gases. The two insets show a camera image of a grating fluorescing in N 2 , and a HIM image of a grating structure post‐fabrication. (b) Initial SERS spectrum of the carbonaceous seed layer on the grating collected in air, and evolution of SERS spectra emanating from two gratings under 1.95 atm CO 2 and N 2 gases respectively. The structures are pumped at λ = 532 nm in all cases.
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Oxford Instruments ixon ultra897 electron multiplying ccd emccd camera
(a) Custom‐built Raman microscopy measurement setup using a CW laser emitting at λ = 532 nm. The setup includes the gas chamber containing grating structures and gas flow at ∼1.95 atm pressure. A spectrometer coupled to an <t>emICCD</t> camera is used to measure the spectra of the gratings in air and in both gases. The two insets show a camera image of a grating fluorescing in N 2 , and a HIM image of a grating structure post‐fabrication. (b) Initial SERS spectrum of the carbonaceous seed layer on the grating collected in air, and evolution of SERS spectra emanating from two gratings under 1.95 atm CO 2 and N 2 gases respectively. The structures are pumped at λ = 532 nm in all cases.
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Princeton Instruments electron multiplied ccd camera
(a) Custom‐built Raman microscopy measurement setup using a CW laser emitting at λ = 532 nm. The setup includes the gas chamber containing grating structures and gas flow at ∼1.95 atm pressure. A spectrometer coupled to an <t>emICCD</t> camera is used to measure the spectra of the gratings in air and in both gases. The two insets show a camera image of a grating fluorescing in N 2 , and a HIM image of a grating structure post‐fabrication. (b) Initial SERS spectrum of the carbonaceous seed layer on the grating collected in air, and evolution of SERS spectra emanating from two gratings under 1.95 atm CO 2 and N 2 gases respectively. The structures are pumped at λ = 532 nm in all cases.
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Oxford Instruments spectrograph kymera 328i c
(a) Custom‐built Raman microscopy measurement setup using a CW laser emitting at λ = 532 nm. The setup includes the gas chamber containing grating structures and gas flow at ∼1.95 atm pressure. A spectrometer coupled to an <t>emICCD</t> camera is used to measure the spectra of the gratings in air and in both gases. The two insets show a camera image of a grating fluorescing in N 2 , and a HIM image of a grating structure post‐fabrication. (b) Initial SERS spectrum of the carbonaceous seed layer on the grating collected in air, and evolution of SERS spectra emanating from two gratings under 1.95 atm CO 2 and N 2 gases respectively. The structures are pumped at λ = 532 nm in all cases.
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Princeton Instruments electron multiplying ccd emccd camera
(a) Custom‐built Raman microscopy measurement setup using a CW laser emitting at λ = 532 nm. The setup includes the gas chamber containing grating structures and gas flow at ∼1.95 atm pressure. A spectrometer coupled to an <t>emICCD</t> camera is used to measure the spectra of the gratings in air and in both gases. The two insets show a camera image of a grating fluorescing in N 2 , and a HIM image of a grating structure post‐fabrication. (b) Initial SERS spectrum of the carbonaceous seed layer on the grating collected in air, and evolution of SERS spectra emanating from two gratings under 1.95 atm CO 2 and N 2 gases respectively. The structures are pumped at λ = 532 nm in all cases.
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(a) Custom‐built Raman microscopy measurement setup using a CW laser emitting at λ = 532 nm. The setup includes the gas chamber containing grating structures and gas flow at ∼1.95 atm pressure. A spectrometer coupled to an emICCD camera is used to measure the spectra of the gratings in air and in both gases. The two insets show a camera image of a grating fluorescing in N 2 , and a HIM image of a grating structure post‐fabrication. (b) Initial SERS spectrum of the carbonaceous seed layer on the grating collected in air, and evolution of SERS spectra emanating from two gratings under 1.95 atm CO 2 and N 2 gases respectively. The structures are pumped at λ = 532 nm in all cases.

Journal: Advanced Science

Article Title: Surface Plasmon Enhanced Photoluminescence of Carbon Dots Formed In Situ on Silver Gratings

doi: 10.1002/advs.202523200

Figure Lengend Snippet: (a) Custom‐built Raman microscopy measurement setup using a CW laser emitting at λ = 532 nm. The setup includes the gas chamber containing grating structures and gas flow at ∼1.95 atm pressure. A spectrometer coupled to an emICCD camera is used to measure the spectra of the gratings in air and in both gases. The two insets show a camera image of a grating fluorescing in N 2 , and a HIM image of a grating structure post‐fabrication. (b) Initial SERS spectrum of the carbonaceous seed layer on the grating collected in air, and evolution of SERS spectra emanating from two gratings under 1.95 atm CO 2 and N 2 gases respectively. The structures are pumped at λ = 532 nm in all cases.

Article Snippet: The emission was then focused into a multimode fiber using another objective and redirected to an electron‐multiplying intensified CCD (emICCD) camera connected to a spectrometer (Princeton Instruments).

Techniques: Microscopy