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  2. Single-molecule mid-infrared spectroscopy and detection through…

    https://www.np.phy.cam.ac.uk/files/natphot23_mirval.pdf
    29 Aug 2023: c. 100. 200. 0. MIR transduced signal(on-o)/o. Without MIRWith MIR at 1,623 cm–1. ... 850750 8007006500. 200. 400 λpump. Fig. 2 | Transduced MIR in vibrationally assisted luminescence.
  3. Metal to insulator transition for conducting polymers in plasmonic…

    https://www.np.phy.cam.ac.uk/files/lsa24_enpom_pedot.pdf
    3 Jan 2024: Scale bar: 20 nm. d Dark-field scattering spectra for Au@PEDOT with d = 3 nm in air (N = 200), with histogram of coupled plasmon modeλc positions. ... A 633 nmlaser illuminates individual NPoMs for over 200 s per timescans at optical powers 6 μW to
  4. Kinetics of Light‐Responsive CNT / PNIPAM Hydrogel Microactuators

    https://www.np.phy.cam.ac.uk/files/small23_cntpnipnactuators.pdf
    23 Oct 2023: actuated here by illuminating with a 532 nm laserover a range of powers (40–200 mW, resulting in irradiance10–55 W cm2) so that the CNTs absorb light and heat the ... www.advancedsciencenews.com www.small-journal.com. Figure 2. Deswelling of a
  5. Video‐Rate Switching of High‐Reflectivity Hybrid Cavities Spanning…

    https://www.np.phy.cam.ac.uk/files/advmat23_nanocaves.pdf
    28 Jun 2023: 1.5 V at 200 mV s1 rel-ative to the reference electrode (Ag/AgCl). ... For each full switch (fromred to green, >95% intensity change), the charge transfer is Q = Idt 200 μC in 30 ms.
  6. Solar-driven liquid multi-carbon fuel production using a standalone…

    https://www.np.phy.cam.ac.uk/files/natenergy23_bivo4leaf.pdf
    28 Jun 2023: Pd 3d5/2. g. Pd(0). Pd(0). e. Cu-rich phasePd-rich phaseCu2OCarbon. a. 2 nm0.206 nmCuPd(200). ... 0.18 nm Cu (200). d. Cu. Fig. 1 | Artificial leaf overview and physical characterization of the bimetallic catalyst.
  7. Accelerated molecular vibrational decay and suppressed electronic…

    https://www.np.phy.cam.ac.uk/files/prb24_cars_npom.pdf
    2 May 2024: Therefore, we reduce the pulsedlaser intensity Il by 20-fold to 200 nW µm2 per beam (forpump, Stokes, and probe lasers; pulse energy 2.5 fJ), corre-. ... Laser intensity 200 nW µm2 per beam (pulse energy 2.5 fJ).Error bars represent standard deviation
  8. Extensive photochemical restructuring of molecule-metal surfaces…

    https://www.np.phy.cam.ac.uk/files/natcomm24_bpdroomlight.pdf
    4 Mar 2024: 0.06040200. 600. 400. 200. 06040200. 0.2. 0.1. 0.0. 0. 0. 0.
  9. In situ electrochemical regeneration of nanogap hotspots for…

    https://www.np.phy.cam.ac.uk/files/natcomm24_resers.pdf
    6 Mar 2024: Magnification ranged from 80,000–200,000x. SERS enhancement factor calculationThe SERS enhancement factor of MLagg-CB[5] was calculated based onthe SERS and Raman signal of CB[5] (Supplementary Fig. ... The Raman spectrum of a 2 mM CB[5]solution in
  10. Photoluminescence upconversion in monolayer WSe2 activated by…

    https://www.np.phy.cam.ac.uk/files/natcomm23_wse2darknpom.pdf
    15 Sep 2023: 1 μm. XB XD1L WSe2 Au. 200 μm. 5 μm. 633 nm. ... The variation in anti-Stokes PLenhancement is even larger, ranging from EFaS = 1 to >200, with anaverage EFaS. =
  11. Controlling Atomic-Scale Restructuring and Cleaning of Gold Nanogap…

    https://www.np.phy.cam.ac.uk/files/acssensors23_mlagg_plasmaclean.pdf
    7 Jul 2023: SERSspectra are taken with a 200 μm grid size (1020 rows and columns,depending on film diameter) exposing the sample for 1 s perspectrum. ... All spectra are referenced to a white light scatteringtarget (Labsphere). Grid size is consistent with SERS

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