banner image
No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Probing of molecular adsorbates on Au surfaces with large-amplitude temperature jumps
Rent this article for
View: Figures


Image of FIG. 1.
FIG. 1.

(a) Experimental arrangement for vibrational SFG spectroscopy of SAMs adsorbed on Au films. In the depiction, SFG probes CH-stretch transitions of the terminal methyl groups (circled) of an ODT SAM. BBIR and NBVIS are broadband IR and narrowband visible pulses. The Cr adhesion layer keeps Au from debonding during solution deposition of SAMs. (b) Lissajous pattern scanning of the substrate minimized accumulated optical damage by reducing multishot exposure.

Image of FIG. 2.
FIG. 2.

Reflectance changes of Au substrates heated to indicated temperatures. Although 530 nm has the largest reflectance change, the 600 nm portion of the white-light continuum was used for transient temperature determinations due to its greater intensity.

Image of FIG. 3.
FIG. 3.

Transient reflectance changes from Au films flash-heated from ambient temperature by 200 fs 400 nm (blue) pulses. The longer-time (>20 ps) reflectance change at 600 nm gives ΔT = 175 K. Note the nonlinear time axis.

Image of FIG. 4.
FIG. 4.

Reflectance transients at 600 nm from flash-heated Au films. ΔT was determined from ΔR/R in the plateau region using the calibration Eq. (1) . (a) A smaller-amplitude T-jump where ΔT = 35 K was produced by either 800 nm or 400 nm flash-heating pulses. The electron-phonon equilibration time constant was 1.25 ps with 400 nm and 1.65 ps with 800 nm pulses. Adsorbed SAMs had no effect. (b) A T-jump transient with ΔT = 175 K produced with 400 nm pulses. The time constant for electron-phonon equilibration increased to 3.45 ps.

Image of FIG. 5.
FIG. 5.

Results of flash-heating experiments where SFG probed ν(NO) of NBT SAMs on Au substrates flash-heated by either 800 nm or 400 nm pulses. When the same ΔT = 35 K was produced, the NBT transients were identical within experimental error.

Image of FIG. 6.
FIG. 6.

Results of flash-heating experiments with ΔT = 175 K where SFG probed ν(NO) of NBT SAM on Au. (a) SFG spectra at indicated delay times. (b) Zeroth spectral moment , representing the intensity (integrated peak area) loss induced by flash-heating. (c) First moment representing lineshape redshift. (d) Square-root of the second moment representing linewidth.

Image of FIG. 7.
FIG. 7.

(a) Time-dependent SFG spectra of ODT SAM on Au at indicated delay times after flash-heating by 400 nm pulses with ΔT = 175 K. The three main SFG transitions arise from ODT terminal methyl groups (see Fig. 1 ). (b) SFG spectrum of ODT after ∼1 h of signal averaging with the substrate moving in a Lissajous pattern. The effects of more than 1 × 10 laser pulses were negligible. (c) Changes in ODT SFG spectrum after a stationary sample was exposed to 10 flash-heating pulses with ΔT = 115 K. Exposure caused SFG signal loss. When the two spectra were normalized to facilitate comparisons, new transitions indicated by the arrows appeared. The new transitions are indicative of alkyl chains developing defects. The defects were created by the cumulative effects of many large-amplitude T-jumps.

Image of FIG. 8.
FIG. 8.

(a) VRF for ODT flash-heated by 400 nm pulses that produced ΔT = 175 K was characterized by an onset delay and a biexponential decay with time constants τ and τ. (b) Time dependent changes in the SFG intensity ratio ν(CH)/ν(CH) induced by smaller and larger T-jumps. (c)Definition of the methyl tilt angle . (d) Relative amplitudes of ν(CH) and ν(CH) as a function of ensemble-averaged methyl tilt angle , based on Hirose

Image of FIG. 9.
FIG. 9.

(a) Schematic of the NBT SAM ordered structure. Arrows indicate conformational degrees of freedom leading to nitro group disorder. (b) Vibrational excitations of NBT resulting from optical pumping of the Au layer. Hot electrons produced initially can excite higher-frequency vibrations including the probed ν(NO) and other vibrations not probed. As hot electrons decay and the Au lattice temperature rises from to , lower-energy NBT SAM lattice modes and NBT vibrations become excited by multiphonon up-pumping. (c) Schematic of SFG process for a vibration initially in  = 0, with coherent IR excitation followed by coherent anti-Stokes Raman scattering. When the probed vibration is excited into  = 1 by hot electrons, the SFG signal decreases due to ground-state depletion. (d) Schematic of vibrational energy exchange mechanism used to explain thermally induced redshifting and broadening. The notation |> indicates quanta in the probed mode and quanta in the other mode. When ν(NO) is probed and another anharmonically coupled vibration becomes excited, the new probed transition is redshifted by δν. The lifetime of the coupled vibration is and the extent of broadening is determined by the product δντ.


Article metrics loading...


Full text loading...

This is a required field
Please enter a valid email address
752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Probing of molecular adsorbates on Au surfaces with large-amplitude temperature jumps