SLSpectroLAB @ X10SA

Figure 1: The SLSpectroLAB facility (lower right), located at beamline PXII (top) at the SLS. The facility provides both on-line as well as off-line setups.
Figure 1: The SLSpectroLAB facility (lower right), located at beamline PXII (top) at the SLS. The facility provides both on-line as well as off-line setups.
Macromolecular crystallography is a powerful method to obtain structural information of large biomolecules and molecular assemblies down to atomic resolution. The electron density maps provided by this method, however, are often not sufficient to e.g. resolve structural ambiguities or to assign the chemical state of co-factors. By combining the X-ray diffraction experiment with optical spectroscopic techniques such as UV/Vis absorption, fluorescence and Raman and Resonance Raman spectroscopy one can obtain valuable complementary information that can not be inferred from the crystal structure alone.

The SLS SpectroLAB facility is focused on providing the possibility for single crystal microspectrophotometry in combination with X-ray diffraction. Microspectroscopic investigation of protein crystals yields additional information, such as the redox state of metal centers or S-S bonds, identity of bound ligands, or degrees of radiation damage. The SLSpectroLAB is a general user facility at beamline X10SA (PXII) of the SLS providing the possibility of on-line and off-line multi-mode microspectrophotometry to the user community. It is currently the only facility providing on-axis geometry for all modes and thus is able to provide spectroscopic data without artifacts from probing different sample volumes (for details see below).

User Operation

External users can apply for spectroscopy measurement time at beamline X10SA through a collaboration with PSI MX scientific staff

General Information

On-Axis Geometry

Currently the SLSpectroLAB is the only laboratory employing an on-axis geometry - co-axial alignment of imaging, spectroscopic axis and X-ray beam. In contrast to the common off-axis geometry this is an invaluable advantage when it comes to conciliating spectroscopically probed volumes of a protein crystal with the volume exposed to the synchrotron radiation (see Figure 6 below). Off-Axis configurations are extremely sensitive to probing unexposed sample volumes thus yielding compromised information. The on-axis approach required in-house construction of the imaging, excitation and collection optics.

Spectroscopic Modes

Raman Spectroscopy

Raman spectroscopy is particularly suited for the identification of ligands and chemical species, e.g. by assignment of specific vibrational bands by difference Raman spectroscopy. A typical use case is the determination of ligand - active site interactions in soaking experiments.

Resonance Raman Spectroscopy

Resonance Raman spectroscopy builds on the enhanced Raman transition probability when the excitation wavelength is approaching resonance or is in resonance with an optical transition. Apart from a general increase in signal strength, the different selectivity to the involved vibrational modes enables thr assignment of vibrational bands related to the chromophore and its direct environment.

UV/Vis Absorption Spectroscopy

UV/Vis absorption spectroscopy is the method of choice for the observation of colored co-factors, metalloproteins and photo-sensitive proteins. In the context of X-ray diffraction experiments, a central point is the detection of radiation-induced changes such as e.g. the radiolytic reduction of metal centers or specific radiation damage such as the breakage of disulfide bridges. Of particular use in the context of structural enzymology is the possibility to characterize and monitor trapped catalytic intermediates in enzymatic reactions, both in time-resolved and static measurements.

Fluorescence Spectroscopy

Fluorescence spectroscopy finally can indicate the presence of co-factors or substrates and yield information on the redox state of metal centers. It further opens the possibility to investigate the fluorescence properties of photochromic fluorescent proteins.
Figure 2: Example of Resonance Raman spectra before and after X-ray exposure. (413nm Laser)
Figure 2: Example of Resonance Raman spectra before and after X-ray exposure. (413nm Laser)
Figure 3: Example of UV/Vis absorption spectra before and after X-ray exposure.
Figure 3: Example of UV/Vis absorption spectra before and after X-ray exposure.

Facility

SLS Microspectrophotometer V2

A multi-mode in-situ micro-spectrophotometer (MS) has been developed by the MX group at the SLS to perform UV/Visible absorption, fluorescence and Raman spectroscopy on protein crystals. The on-axis geometry ensures an optimal overlap between the X-ray beam and the spectroscopic probes, e.g. for a better characterization of specific radiation damage and more generally photo-induced reactions due to X-ray exposure.

Figure 4: The SLS Microspectrophotometer, Version 2 (MS2). On the left site the exitation arm with the fiber-holder is clearly visible. The signal is collected through the middle arm and coupled into a fiber connected to the spectrograph. The imaging branch with photo-optics and a regular CCD camera is on the right.
Figure 5: Scheme of the on-line configuration of the MS2: Sample observation with the on-axis microscope(blue); illumination for UV/Vis absorption measurements (yellow); excitation-branch for Raman- and fluorescence spectroscopy and signal collection-branch to the spectrograph (red); X-ray beam (green). All light to and from the spectrophotometer is coupled via light fibers.
Figure 6: Size and location of the various beamspots in on-axis, on-line configuration.

Off-Line Facility

Figure 7: The SLSpectroLAB facility showing both the Control Hutch (front) and the Experimental Hutch (back) with the goniometer, mircospectrophotometer and laser assembly.
Figure 7: The SLSpectroLAB facility showing both the Control Hutch (front) and the Experimental Hutch (back) with the goniometer, mircospectrophotometer and laser assembly.
The Off-line facility at the SLSpectroLAB provides the opportunity to perform preparatory measurements or whole experiments which do not require X-ray exposure. Off-line measurement time, not being tied to the beamline shifts, can therefore be made available to users independently of the X-ray beamtime scheduling.

The facility consists of two hutches. The first is housing the control room with the terminal PCs. From here one can access the actual experimental hutch which is interlocked during the experiment according to the laser safety regulations. The experimental hutch houses a full crystallographic goniometer setup similar to the one used at the PXII beamline to offer all possibilities of the on-line setup. Just as at the beamline , a Cryojet cryo-cooling device is available for cooling the samples during the experiment.

Equipment

LASER

Various single-wavelength diode laser are available as well as a Coherent Innova302C Kr$^+$ Ion Laser. This allows for a multitude of different systems to be measured at the SLSpectroLAB.
Available Laser at the SLSpectroLAB
Wavelength Laser Type Application Power Status
266nm SWD UV illumination xxx mW OK
405nm SWD RRaman 350 mW OK
413nm Kr RRaman 200 mW CUA
473nm SWD RRaman 150 mW OK
532nm SWD Raman/Photo-bleaching 200 mW OK
594nm SWD RRaman 250 mW OK
647nm Kr Raman, RRaman >300 mW CUA
785nm SWD Raman >500 mW OK
OK: Available ° CUA: Currently unavailable ° N/A: Not available

Other Lightsources

For UV/Vis absorption spectroscopy we utilize a ZEISS Xenon-Arc lamp with sufficient power to illuminate even larger crystals. For higher light intensity in the deep UV, a combined Deuterium/Halogen fiber-coupled light source is provided.

References

How to Cite SLSpectroLAB

If you publish results you gained at the SLSpectroLAB or otherwise want to acknowledge the SLSpectroLAB, please use the following reference(s):
  • Pompidor, G., F.S.N. Dworkowski, et al. (2013). "A new on-axis micro-spectrophotometer for combining Raman, fluorescence and UV/Vis absorption spectroscopy with macromolecular crystallography at the Swiss Light Source." Journal of Synchrotron Radiation 20(5): 765-776. DOI:10.1107/S0909049513016063

Selected Publications

2018

  • Horrell, S., D. Kekilli, et al. (2018). "Enzyme catalysis captured using multiple structures from one crystal at varying temperatures" IUCrJ 5(3): 283-292 DOI:10.1107/S205225251800386X [UVVis]

2017

  • Kekilli, D., T. Moreno-Chicano, et al. (2017). "Photoreduction and validation of haem–ligand intermediate states in protein crystals by in situ single-crystal spectroscopy and diffraction" IUCrJ 4(3): 263-270 DOI:10.1107/S2052252517002159 [RRAMAN/UVVis]
  • Kekilli, D., C.A. Petersen, et al. (2017). "Engineering proximal vs. distal heme–NO coordination via dinitrosyl dynamics: implications for NO sensor design." Chem. Sci. 8(3): 1986-1994 DOI:10.1039/C6SC04190F [RRAMAN]

2015

  • Ghafoor, D.D., D. Kekilli, et al. (2015). "Hydrogen bonding of the dissociated histidine ligand is not required for formation of a proximal NO adduct in cytochrome c’" JBIC Journal of Biological Inorganic Chemistry 20(6):949-956. DOI:10.1007/s00775-015-1278-y [RAMAN, UVVis]
  • Dworkowski, F.S.N, M. Hough, et al. (2015). "Challenges and solutions for the analysis of in situ, in crystallo microspectrophotometric data" Acta Crystallographica Section D 71(1): 27-35 DOI:10.1107/S1399004714015107 [REVIEW, SOFTWARE]

2014

  • Bolze, C. S., R.E. Helbling, et al. (2014). "Human Cellular Retinaldehyde-Binding Protein Has Secondary Thermal 9-cis-Retinal Isomerase Activity." JACS 136(1): 137-146. DOI:10.1021/ja411366w [RAMAN, UV/Vis]
  • Kekilli, D., F.S.N. Dworkowski, et al. (2014). "Fingerprinting redox and ligand states in haemprotein crystal structures using resonance Raman spectroscopy." Acta Crystallogr D Biol Crystallogr 70(Pt 5): 1289-1296. DOI:10.1107/S1399004714004039 [RRAMAN]

2013

  • Pompidor, G., F.S.N. Dworkowski, et al. (2013). "A new on-axis micro-spectrophotometer for combining Raman, fluorescence and UV/Vis absorption spectroscopy with macromolecular crystallography at the Swiss Light Source." Journal of Synchrotron Radiation 20(5): 765-776. DOI:10.1107/S0909049513016063 [LUMINESCENCE, INSTRUMENTATION]
  • Merlino, A., M. R. Fuchs, et al. (2013). "Selective X-ray-induced NO photodissociation in haemoglobin crystals: evidence from a Raman-assisted crystallographic study." Acta Crystallographica Section D-Biological Crystallography 69: 137-140. DOI: 10.1107/S0907444912042229 [RAMAN]

2012

  • He, C., M. R. Fuchs, et. al. (2012). "Guanidine-Ferroheme Coordination in the Mutant Protein Nitrophorin 4(L130R)." Angewandte Chemie International Edition 51(18): 4470-4473. DOI: 10.1002/anie.201108691 [UV/Vis]
  • Owen, R. L., B. A. Yorke, et al. (2012). "X-ray-excited optical luminescence of protein crystals: a new tool for studying radiation damage during diffraction data collection." Acta Crystallographica Section D 68(5): 505-510. DOI: 10.1107/s0907444912002946 [XEOL]

2011

  • Regis Faro, A., P. Carpentier, et al. (2011). "Low-Temperature Chromophore Isomerization Reveals the Photoswitching Mechanism of the Fluorescent Protein Padron." Journal of the American Chemical Society. 133(41): 16362–16365 DOI:0.1021/ja207001y [UV/Vis, LASER INDUCED CHEMISTRY]
  • Antonyuk, S. V., M. A. Hough (2011). "Monitoring and validating active site redox states in protein crystals." Biochimica et Biophysica Acta (BBA) - Proteins & Proteomics 1814(6): 778-784. DOI:10.1016/j.bbapap.2010.12.017 [UV/Vis]
  • Rajendran, C., F. S. Dworkowski, et al. (2011). "Radiation damage in room-temperature data acquisition with the PILATUS 6M pixel detector." J Synchrotron Radiat 18(Pt 3): 318-328. DOI:10.1107/S090904951100968X [UV/Vis]

2010

  • McGeehan, J. E., D. Bourgeois, et al. (2010). "Raman-assisted crystallography of biomolecules at the synchrotron: Instrumentation, methods and applications." Biochim Biophys Acta. DOI:10.1016/j.bbapap.2010.07.021 [REVIEW]
  • Hersleth, H. P. and K. K. Andersson (2010). "How different oxidation states of crystalline myoglobin are influenced by X-rays." Biochim Biophys Acta. DOI:10.1016/j.bbapap.2010.07.019 [UV/Vis]

2009

  • Owen, R. L., A. R. Pearson, et al. (2009). "A new on-axis multimode spectrometer for the macromolecular crystallography beamlines of the Swiss Light Source." J. Synchrotron Rad. 16(Pt 2): 173-182. DOI:10.1107/S0909049508040120 [INSTRUMENTATION]
  • Pearson, A. R. and R. L. Owen (2009). "Combining X-ray crystallography and single-crystal spectroscopy to probe enzyme mechanisms." Biochemical Society Transactions 037(2): 378-381. DOI:10.1042/bst0370378 [REVIEW, INSTRUMENTATION]
https://intranet.psi.ch/wiki/bin/edit/sls/pxii/SpectroLabEN# For more information about the SLSpectroLAB and how to request measurement time please contact Dr. Florian Dworkowski.