• Aucun résultat trouvé

Two-photon 3d optical data storage via aggregate switching of excimer-forming dyes

N/A
N/A
Protected

Academic year: 2022

Partager "Two-photon 3d optical data storage via aggregate switching of excimer-forming dyes"

Copied!
3
0
0

Texte intégral

(1)

1

Supporting Information for Two-Photon 3D Optical Data Storage via Aggregate Switching of Excimer-Forming Dyes

By Joseph Lott±, Christopher Ryan±, Brent Valle±, Jack R. Johnson III, David A. Schiraldi, Jie Shan, Kenneth D. Singer*and Christoph Weder*

± These authors contributed equally to the present work.

Joseph Lott, Jack R. Johnson III, Prof. David A. Schiraldi, Prof. Christoph Weder,

Department of Macromolecular Science and Engineering, Case Western Reserve University Cleveland, OH, 44106-7202, USA

Christopher Ryan, Brent Valle, Prof. Jie Shan, Prof. Kenneth D. Singer, Department of Physics, Case Western Reserve University

Cleveland, Ohio 44106 USA E-mail: kenneth.singer@case.edu Prof. Dr. Christoph Weder

Adolphe Merkle Institute, Polymer Chemistry and Materials, University of Fribourg Rte de l'Ancienne Papeterie, CH-1723 Marly 1, Switzerland

E-mail: christoph.weder@unifr.ch

Keywords: Photonics, Nonlinear Optics, Luminescence, Polymeric Materials

(2)

2

-10 -5 0 5 10

0.96 0.97 0.98 0.99 1.00 1.01 1.02

Normalized Transmittance

Z (mm)

Figure S1. Normalized transmittance established in the Z-scan measurement of a C18-RG solution (0.025M in toluene) measured at 650 nm with a peak incident irradiance of 60 GW/cm2. The solid line is a fit to an inverted Lorentzian model[32], which follows the on-axis irradiance of a focused Gaussian beam.

(3)

3

Figure S2. Intensity profiles of cross-sections taken along a straight line through the spots in

the top row of Figure 5. a) Raw fluorescence between 650 and 800 nm (Figure 5a). b) Raw fluorescence between 500 and 525 nm (Figure 5b). c) Composite image from the ratio of the intensities of the two images (Figure 5c). d) Composite image with a low pass filter applied.

Ă

ď

Đ

Ě

Références

Documents relatifs

Experimental setup for the excitation of the 1S-3S transition and the optical frequency measurement (Laser TiSa: titanium sapphire laser, FP: Fabry-Perot cavity, DL/Rb: laser

4 are the following distributions that would be expected to show dierences due to the presence of additional partons in the nal state: the visible invariant mass of the event (W vis

Measurement of the hadronic photon structure function F _2 γ (x, Q 2 ) in two-photon collisions at LEP.. A. Martin,

Monte Carlo simulation of four-pion events (open histogram) and the background estimated from the data (hatched histogram) are also shown in b). The arrows indicate the

Figures 5 a) − d) show the distributions of x f it , y f it , Q 2 and W γγ,f it , together with Monte Carlo background estimations, for the selected single-tag events, in

We present the mechanisms of a remanent alignment of polarizable molecules dispersed in a solid silica gel matrix, when submitted to powerful, femtosecond, linearly polarized,

The three ATLAS instruments' solar spectral irradiance measurements are first compared to one another and then the average of the ATLAS data is compared to simultaneous data

The OPAL Collaboration used the unlike- charge reference sample in their analysis of two-jet events, obtaining the ratio of radii. =R k