Supplementary Information

Similar documents
LIST of SUPPLEMENTARY MATERIALS

Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods

Anti-Bunching from a Quantum Dot

Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup

Manipulating and Probing Enzymatic Conformational Fluctuations and Enzyme-Substrate Interactions by Single-Molecule FRET- Magnetic Tweezers Microscopy

Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching

Supporting Information

Supplemental Materials and Methods

Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry

Lab 3 and 4: Single Photon Source

Nature Protocols: doi: /nprot Supplementary Figure 1

Supplementary Figures

Supplemental Material: Experimental and Theoretical Investigations of the Electronic Band Structure of Metal-Organic Framework of HKUST-1 Type

l* = 109 nm Glycerol Clean Water Glycerol l = 108 nm Wavelength (nm)

Electronic Supplementary Information

Optical Properties of CdSe Colloidal Quantum Dots and NV-Nanodiamonds

File Name: Supplementary Information Description: Supplementary Figures and Supplementary Note. File Name: Peer Review File Description:

Quantum Optics and Quantum Information Laboratory

Time-resolved Molecule Counting by Photon Statistics Across the Visible Spectrum

Using Alba with the FemtoFiber laser by Toptica for 2-photon quantitative imaging

Supplementary Information: Three-dimensional quantum photonic elements based on single nitrogen vacancy-centres in laser-written microstructures

BMB Class 17, November 30, Single Molecule Biophysics (II)

Supplementary figure 1 Application of tmfret in LeuT. (a) To assess the feasibility of using tmfret for distance-dependent measurements in LeuT, a

Confocal Microscope Imaging of Single emitter fluorescence and Observing Photon Antibunching Using Hanbury Brown and Twiss setup. Lab.

Supplemental material for Bound electron nonlinearity beyond the ionization threshold

Science Lab I Properties of Light

Confocal Microscope Imaging of Single-Emitter Fluorescence and Photon Antibunching

LAB 3: Confocal Microscope Imaging of single-emitter fluorescence. LAB 4: Hanbury Brown and Twiss setup. Photon antibunching. Roshita Ramkhalawon

SUPPLEMENTARY INFORMATION

Spatial Coherence Properties of Organic Molecules Coupled to Plasmonic Surface Lattice Resonances in the Weak and Strong Coupling Regimes

Near-field imaging and spectroscopy of electronic states in single-walled carbon nanotubes

16. More About Polarization

Solution set for EXAM IN TFY4265/FY8906 Biophysical microtechniques

Supporting Information

Single Photon Sources

Lab 3-4 : Confocal Microscope Imaging of Single-Emitter Fluorescence and Hanbury-Brown and Twiss Set Up, Photon Antibunching

Laser induced fluorescence

Supporting information for: Fast quantitative. single-molecule detection at ultralow concentrations. - Supporting Information -

Quantum and Nano Optics Laboratory. Jacob Begis Lab partners: Josh Rose, Edward Pei

Dual-Wavelength Lasing from Organic Dye Encapsulated Metal-Organic Framework Microcrystals

Supporting information

FROM LOCALIZATION TO INTERACTION

Abstract... I. Acknowledgements... III. Table of Content... V. List of Tables... VIII. List of Figures... IX

SUPPLEMENTARY INFORMATION

Controlled Assembly of Organic Whispering Gallery Mode Microlasers as Highly Sensitive Chemical Sensors

Lab3-4: Single Photon Source

A rule of seven in Watson-Crick base-pairing of mismatched sequences

Supplementary Figure 1: Determination of the ratio between laser photons and photons from an ensemble of SiV - centres under Resonance Fluorescence.

Supplementary Information. The Solution Structural Ensembles of RNA Kink-turn Motifs and Their Protein Complexes

Lipid Regulated Intramolecular Conformational Dynamics of SNARE-Protein Ykt6

SUPPLEMENTARY INFORMATION

Supporting Information: Ultrafast Excited State Transport and Decay Dynamics in Cesium Lead Mixed-Halide Perovskites

Digital Holographic Measurement of Nanometric Optical Excitation on Soft Matter by Optical Pressure and Photothermal Interactions

High Resolution Laser Microscopy: a fascinating method to explore the molecular world

Take that, Bell s Inequality!

Sharper low power STED nanoscopy by time gating

Nature Methods: doi: /nmeth Supplementary Figure 1

1. Transition dipole moment

Increasing your confidence Proving that data is single molecule. Chem 184 Lecture David Altman 5/27/08

Correlation Spectroscopy in Polymer Physics Methodenseminar im Wahlpflichtfach Basics diffusion and brownian motion correlations functions

SUPPLEMENTARY INFORMATION

PHOTOLUMINESCENCE SPECTRA AND QUANTUM YIELDS OF GOLD NANOSPHERE MONOMERS AND DIMERS IN AQUEOUS SUSPENSION

Complex RNA Folding Kinetics Revealed by Single-Molecule FRET and Hidden Markov Models

Aluminum for nonlinear plasmonics: Methods Section

Optical Spectroscopy. Steady State and Time Dependent Fluorescence Measurements. Kai Wen Teng. October 8 th PHYS 403 Fall 2013

P = χ (1) E + χ (2) E 2 +

Supplementary Fig. 1 Experimental setup and additional sample characterization. (a) Schematics of the two-color confocal microscope.

Supporting Information

Third-harmonic generation

SUPPLEMENTARY INFORMATION

Figure 1: Left: Apparent radial velocities of Capella measured with the Chandra/HETGS. The dotted line shows the calculated apparent radial motion of

vapour deposition. Raman peaks of the monolayer sample grown by chemical vapour

Single-Molecule Methods I - in vitro

Structure Report for J. Reibenspies

Table S1. Overview of used PDZK1 constructs and their binding affinities to peptides. Related to figure 1.

SUPPLEMENTARY INFORMATION

Dielectric metasurfaces for complete control of phase and polarization with subwavelength spatial resolution and high transmission

Supplementary Material

Report on the new EFOSC2 VPH grisms

Solution structure and dynamics of biopolymers

Measurement of liquid surface properties by laser-induced surface deformation spectroscopy

PC Laboratory Raman Spectroscopy

SUPPLEMENTARY INFORMATION

Supplementary for Disorder Dependent Valley Properties in Monolayer WSe 2

Shot-Noise Limited Single-Molecule FRET Histograms: Comparison between Theory and Experiments

Simultaneous intracellular chloride and ph measurements using a GFPbased

Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca

SUPPLEMENTARY INFORMATION

Single Photon Generation & Application

Advanced Spectroscopy Laboratory

Wavelength-Dependent Photochemistry of Oxime. Ester Photoinitiators

OPSE FINAL EXAM Fall 2015 YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT.

Supporting Information - Inducing high ionic conductivity in the lithium superionic argyrodites Li 6+x P 1-x Ge x S 5 I for allsolid-state

Enhancement of Exciton Transport in Porphyrin. Aggregate Nanostructures by Controlling. Hierarchical Self-Assembly

D \ Basis for Detection. Rapid DNA SequencinglSingle-Molecule Spectroscopy. Steven A. Soper, Lloyd A.!?.Davis, and E. Brooks Shera

Supplementary Figure S1. AFM characterizations and topographical defects of h- BN films on silica substrates. (a) (c) show the AFM height

Modular scanning FCS quantifies receptor-ligand interactions in living multicellular organisms

Set-up for ultrafast time-resolved x-ray diffraction using a femtosecond laser-plasma kev x-ray-source

Electron Energy and Light

Transcription:

Supplementary Information Single molecule FRET reveals the energy landscape of the full length SAM I riboswitch Christoph Manz, 1,2 Andrei Yu. Kobitski, 1 Ayan Samanta, 3 Bettina G. Keller 4, Andres Jäschke, 2,3 and G. Ulrich Nienhaus 1,2,5,6,*. 1 Institute of Applied Physics, Karlsruhe Institute of Technology, Wolfgang Gaede Str. 1, 76131 Karlsruhe, Germany 2 HEiKA Heidelberg Karlsruhe Research Partnership, Karlsruhe Institute of Technology, Hermannvon Helmholtz Platz 1, 76344 Eggenstein Leopoldshafen, Germany 3 Institute of Pharmacy and Molecular Biotechnology, Heidelberg University, Im Neuenheimer Feld 364, 69120 Heidelberg, Germany 4 Freie Universität Berlin, Institute of Chemistry and Biochemistry, Takustr. 3, 14195 Berlin, Germany 5 Institute of Nanotechnology and Institute of Toxicology and Genetics, Karlsruhe Institute of Technology, Hermann von Helmholtz Platz 1, 76344 Eggenstein Leopoldshafen, Germany 6 Department of Physics, University of Illinois at Urbana Champaign, Urbana, Illinois 61801, USA *Corresponding author e mail: uli@uiuc.edu 1

Supplementary Results Supplementary Table 1. Total number of molecules analyzed for compilation of the FRET histograms in Figs. 2 and 4 and Supplementary Figs. 1 and 2. [Mg 2+ ]/ mm RS AA RS EA RS EA @ [Mg 2+ ] = 20 mm No. of molecules [Mg 2+ ]/ mm No. of molecules [SAM]/ µm No. of molecules 0.1 8905 0 4613 0 3441 0.5 7923 0.4 8637 0.01 3790 0.75 7506 0.8 2958 0.1 2482 1 8284 1.6 3598 1 2449 2 8548 3.125 4370 10 5053 3 6414 6.25 4663 5 11862 12.5 5049 7.5 17192 25 1989 10 15121 50 5041 25 5741 100 2710 50 11499 100 14262 2

Supplementary Table 2. Peak positions of subpopulations determined by global fits of FRET histograms, and the resulting inter dye distances for riboswitch constructs RS EA and RS AA at <0.1 mm and >20 mm Mg 2+ concentration (na, not available; nd, not determined). Conformation [Mg 2+ ] < 0.1 mm [Mg 2+ ] > 20 mm E r( E ) / Å E r( E ) / Å RS EA AT 1 0.73 45 0.80 42 AT 2 0.50 53 0.57 51 T 1 0.24 64 0.40 57 T 2 0.13 73 0.18 68 RS EA /SAM SAM AT 1 na na 0.87 39 SAM AT 2 na na 0.67 47 SAM T 1 na na 0.45 55 SAM T 2 na na 0.28 62 RS AA AT 1 0.24 64 0.44 55 AT 2 nd nd 0.07 81 T 1 0.31 61 0.61 49 T 2 0.09 78 nd nd 3

Supplementary Figure 1. Mg 2+ and SAM dependent smfret histograms of SAM I riboswitch construct RS EA. The data were acquired by burst analysis of intensity time traces taken with freely diffusing molecules on the confocal microscope. (a) Histograms for selected Mg 2+ ion concentrations between 0 and 100 mm (grey bars). Colored lines represent best fit results with four states modelled by Gaussian distributions; the dashed black lines show the sum. The entire data set was fitted globally by using the following constraints: (i) For the data at 12.5 mm, peak positions were fixed to the values obtained from the HMM analysis; (ii) fractions of the T 1 state (green) for data with [Mg 2+ ] < 2 mm were restricted (within the error) to the values obtained from individual two state model fits of FRET efficiency histograms of construct RS AA at the corresponding Mg 2+ concentrations; (iii) the full width at half maximum (FWHM) values of the four subpopulations were set to be Mg 2+ independent; the fit yielded the values of 0.16, 0.2, 0.2 and 0.22 for the T 1 (green), T 2 (blue), AT 1 (violet) and AT 2 (orange) states, respectively. (b) smfret histograms at various SAM ligand concentrations between 0 and 10 µm in the presence of 20 mm Mg 2+. FRET efficiency histogram at 10 µm of SAM concentration was fitted with four Gaussian model distributions, introducing constraints on the peak positions according to the HMM result; the dashed black line shows the sum. 4

Supplementary Figure 2. Mg 2+ dependent smfret histograms of SAM I riboswitch construct RS AA. The data were taken on immobilized molecules at various concentrations of Mg 2+ by collecting ptirfm images with 1 s exposure time. Lines represent global fits of all histograms with a three state model using the following constraints: (i) fractions of the T 1 (green) and AT 1 (red) states were restricted (within the error) to the values from the global fit of FRET efficiency histograms of the construct RS EA with a four state model; (ii) full widths at half maximum (FWHM) were set to be Mg 2+ independent; the fit yielded values of 0.21, 0.21, and 0.28 for T 2 + AT 2 (cyan), T 1 (green), and AT 1 (violet), respectively. 5

Supplementary Figure 3. Validation of hidden Markov models. (a) Time window dependent FRET efficiency histograms with 10, 50 and 250 ms bin widths of the experimentally determined data set (black line) and its 95% confidence interval (region between the grey lines) and the HMM prediction (red line). (b) Residence time distributions of the individual states calculated from the maximumlikelihood paths. The different states are colored as in Figure 3. 6

Supplementary Figure 4. Mg 2+ dependence of fractional areas and peak positions of the Gaussian distributions resulting from global fits of smfret histograms. Legends assigning the data to specific states are given in the insets. Lines through the data points are fits of either fractional subpopulations or peak positions, X, with a Hill equation X([Mg 2+ ]) = X(0) + ΔX/(1+[Mg 2+ ] 0.5 /[Mg 2+ ]), where [Mg 2+ ] 0.5 is the transition midpoint concentration. (a) RS EA construct; the fractional populations show exchanges between T 2 and AT 2 with [Mg 2+ ] 0.5 = (1.5 ± 0.6) mm and between T 1 and AT 1 with [Mg 2+ ] 0.5 = (7.5 ± 0.5) mm. The peak positions of all subpopulations shift to higher FRET efficiencies with [Mg 2+ ] 0.5 = (8 ± 1) mm, although to a different extent. (b) RS AA construct; dashed lines depict the fractional populations of RS EA ; the solid cyan line represents the sum of the orange and blue dashed lines. The peak positions of the T 1 and AT 1 states shift markedly ([Mg 2+ ] 0.5 = (8 ± 1) and (15 ± 2) mm, respectively). Also shown are the average peak positions of 0.09 and 0.07 FRET efficiency at low (< 1.5 mm, blue) and high (> 1.5 mm, orange) Mg 2+ concentration for the sum of the T 2 and AT 2 states. Error bars represent uncertainties given by the non linear least squares fitting software (OriginPro 2015). 7

Supplementary Figure 5. Alternative secondary structure model of the B. subtilis yitj SAM I riboswitch (169 nt fragment) in the anti terminator (AT) conformation. Base pairing in the putative P1 and P1 regions is indicated by dots. Donor (Cy3) and acceptor (Cy5) dye labeling sites of the two labeled constructs (RS AA and RS EA ) are shown as green and red stars, respectively. Biotin is represented by a black diamond at the 3 end. 8

Supplementary Figure 6. Schematic diagram of the confocal microscope with single molecule sensitivity. Abbreviations: AOTF acousto optical tunable filter, APD avalanche photodiode, DM dichroic mirror, F optical filter, L lens, M mirror, P pinhole, PC personal computer, T telescope lens. Details are described in Methods. 9

Supplementary Figure 7. Schematic depiction of the AOTF based programmable beam splitter of the confocal microscope. It consists of four acousto optical tunable filters (AOTF, Model #97 01776 01, Crystal Technology, Palo Alto, CA) and allows us to excite the sample with one of four wavelengths in a computer controlled fashion by using a multi function data acquisition card (PCI 6713, National Instruments, Austin, TX). AOTF1 deflects the incoming laser beam into the first order diffraction maximum emitted along the optical axis of the objective. The other three AOTFs are required to compensate for dispersion and birefringence effects introduced by AOTF1. Shown are the excitation and emission light paths through the four AOTFs. Arrows mark the common usage direction for coupling into the zeroth order. Circles with crosses mark the top and empty circles the bottom of the AOTF crystals. 10

Supplementary Figure 8. Schematic diagram of the ptirf microscope setup. Abbreviations: AOTF acousto optical tunable filter, BS beam splitter, DM dichroic mirror, F optical filter, L lens, M mirror. The close up schematic shows RNA molecules immobilized by using BSAbiotin/streptavidin/biotin RNA. For details, see Methods. 11