Time Resolved X-rays Scattering from Disordered SystemsThe tehnique on ID09B beamline at the ESRF.This technique allows to probe the X-rays scatteringintensity changes following a perturbation induced inthe sample by a laser pulse. The time resolution isgiven by the pulsed structure of SynchrotronRa<strong>di</strong>ation: the pulse duration is determined by theelectrons bunch length and at the present timecorresponds to 100 ps. So the technique looks likean optical pump and probe experiment the uniquething being the microscopic structural informationprovided by an X-rays pulse as probe signal. Theexperiment is performed locking the laser phase onthe electrons bunch frequency in the ring. Themaximum repetition rate of the laser is much slowerrespect to the X-rays emission then a rotativechopper allows to reject the pulses to match the1Khz laser emission (or slower if needed). The timedelay is finely tuned by means of a fast timing <strong>di</strong>odefrom the value imposed by the repetition rate up tothe 100ps X-pulse resolution. For a fixed time delaythousands of pulses are collected on a CCD giving ascattering image: this is usually subtracted from ano-laser one to get a <strong>di</strong>fference pattern which couldbetter give the microscopic structural information. Asthe detector has not time resolution the sample mustbe replaced at each pulse: a standard experiments isthen usually performed making the liquid flowing ina jet in order to recover the scattering volume eachmillisecond. The optic pump setup now consists of acryogenically cooled 13 passes Dragon amplifierwhich make available 100 femtosecond pulses at800 nm wavelength with an energy up to 2.5 mJ perpulse; a TOPAS system is also available to tune thepump in a wide range of wavelengths.Probing photochemical reactions in solutions.One of the most important application of thetechnique has been the observation of the laserinduced reactions in photoactive molecules. The<strong>di</strong>fferent steps of the excited molecule reactionproduce a structural information that can bedetected in the <strong>di</strong>fference pattern: ref [1] gives anexhaustive example of a typical application inphotochemistry. In this kind of the experiments theanalysis has to account for the global changes of thesolution due to the solvent rearrangement aroundthe solute and the heat released: numericalsimulations and laser heating [2] experiments onthe solvent play a crucial role to extract the soluteinformation. Once this information is achieved onecan develop a sort of molecular movie provi<strong>di</strong>ngunique information on the structures involved in thereactions pattern and their lifetime.Impulsive Infrared Heating in simple liquids.The exigency of extracting solute information inphotoreactions dynamics turned our attention on thedynamic following an impulsive heating in a simpleliquid. An infrared pulse can be used toinstantaneously release heat in the sample producingan initial temperature and pressure jump at constantvolume which first induce a pressure wave to relax tomechanical equilibrium and then equilibrate thetemperature on larger timescales. Thishydrodynamics can be observed from a microscopicpoint of view by this technique allowing toinvestigate how the hydrodynamic theory accountsfor the temporal evolution of the signal on smalllength-scales. Typical <strong>di</strong>fference patterns at <strong>di</strong>fferenttime delays are reported for methanol in the figurebelow: the increment of the signal around 10nsmarks the expansion dynamics. Moreover severalliquids cross a metastable negative pressure stateduring the expansion dynamics following the heating(correspon<strong>di</strong>ng to the peak region in the figure): thisstate together with cavitations effects can bestu<strong>di</strong>ed in his structural and dynamical features.Impulsive infrared heating in glassformers. Onthe way of using this technique as a sort of thermalstimulated scattering with a microscopic probe andtaking advantage of the extremely large timescaleswindow available our attention is now moving to thestudy of complex liquids and glasses: in this class ofsystems the presence of the slow structuralrelaxations dynamics allows to observe the structuralchanges before the thermodynamic equilibrium isreached. This project is still work in progress:developments of the sample environment have beennecessary to extend the technique to not flowingsystems and to implement a thermal control to heatand cryogenically cool the sample. A rotative cellsystem has been tested and is now available toreplace the scattering volume at the repetition rateneeded. The application of this technique to glassesmight offer a new tool for the study of the slowdynamics in this class of complex systems from amicroscopic point of view. Further developments inpotentially interesting <strong>di</strong>rections for the SOFTcommunity might include polymers stu<strong>di</strong>es andcolloidal systems also considering that time resolvedsmall angle experiments have already beensuccessfully performed [3].References[1]H.Ihee et al., Science 309, 1223 (2005).[2] M.Cammarata et al., JCP 124, 124504 (2006).[3] A.Plech et al. CPL 401, 565 (2005).Authors:M. Cammarata(a), M. Lorusso(a), Q. Kong(a), E.Pontecorvo(b), G. Ruocco(b), F.Sette(a), M.Wulff (a).(a) ESRF, Grenoble, France.(b) <strong>Dipartimento</strong> <strong>di</strong> <strong>Fisica</strong>, Universita' <strong>di</strong> Roma 'La<strong>Sapienza</strong>' and CRS SOFT-INFM-CNR, Roma, Italy.59SOFT Scientific <strong>Report</strong> 2004-06
Scientific <strong>Report</strong> – Non Equilibrium Dynamics and ComplexityGlass Transition in Photosensitive PolymersOptical pumping of the isomerization transition inpolymeric systems containing the azobenzene moietyhas received much attention in recent years, mainlybecause of applications to optical writing, potentiallydown to the nanoscale [1]. To this end, however,much fundamental study is still necessary, due tothe complexity of the systems, which feature a richphenomenology of relevance to phase transitions inliquid crystals, the glass transition, dewettingphenomena[2], the anomalous <strong>di</strong>ffusional andvibrational dynamics in spatially heterogeneoussystems, and to the well known anomalies in the lowfrequency vibrational density of states (VDOS)ofglass formers. A link is generally found between thedynamical fragility m, and the Boson Peak, which inturn seems in many cases to be related to the localstructure of the glass. However it is still not clearwhat is the cause of the vibrational anomalies, oreven if there is only one general cause. It is hopedthat the study of photosensitive polymers could helpin solving this problem, in particular due to thepossibility of inducing or mo<strong>di</strong>fying morphology downto the nanoscale.As part of this general program, we have describedseveral effects on the macroscopic scale: changes inrheological properties probed by opticalmeasurements [3] and by <strong>di</strong>rect measurements onLangmuir monolayers [4] and in bulk [5], lea<strong>di</strong>ng tothe possibility of fast optical quenching of thematerial; relaxation times are sensitive to theapproach of the glass transition [6]. In spite of theextent of experimental work and modeling, it is stillnot clear what the actual connection is between themicroscopic phenomena related to azobenzeneisomerization and the changes in the macroscopicproperties of the system. We have stu<strong>di</strong>ed the lowfrequency dynamics on the same material by acombination of neutron scattering techniques,showing that while at low energy, low momentum,we had a standard picture for a polymer but nophotoinduced effect, in the interme<strong>di</strong>ate region ofEnergy (meV)1412108642Fig. 1.Hg OFFHg ON00 5 10 15Exchange momentum, Q (nm -1 )the BP a reduction of the v-DOS was observed uponUV illumination [7]. Therefore basic purpose of ourmost recent activity is to connect the nanoscalesingle molecule optically induced conformationalchanges of the azobenzene side chain to the above<strong>di</strong>scussed macroscopic effects of flui<strong>di</strong>fication andspatial homogenization, through the study of theeventual photoinduced changes in the low frequencyvibrational dynamics as probed by <strong>di</strong>fferenttechniques.As an example in the following we <strong>di</strong>scuss the resultsrecently obtained by Inelastic X-Ray scattering onthe beamline ID16 of ESRF in dark and under UVillumination, with the incoming X-ray beam focuseddown to 30X100 µm 2 . The measured Q rangecovered up to the first sharp maximum in the staticstructure factor S(Q). IXS data were analyzed with astandard Damped Harmonic Oscillator model plus apurely elastic component. In the figure we show the<strong>di</strong>spersion curves as measured at T=200K in darkand under UV photoperturbation.The photoperturbation mostly affects the <strong>di</strong>spersioncurve in the high Q region, while the low Q, longrange structure of the polymer remains unaltered.The photoinduced <strong>di</strong>fference becomes maximumaround 15 nm -1 , which corresponds to the first sharpmaximum in the static structure factor. This suggeststhat photoisomerization, a process that is located onthe scale of the single molecule, affects macroscopicproperties such as viscosity, via the softening of aborder zone mode which is likely to have at leastsome transverse (or localized) character. These ideashave received preliminary confirmation from lowfrequency Raman data, and a preliminary report hasbeen submitted for pubblication [8].References[1] P. Camorani, M. Labar<strong>di</strong>, M. Allegrini - Mol. Cryst.Liq. Cryst. 372, 365-372 (2001).[2] L. Cristofolini, S. Arisi, M. P. Fontana - Phys.Rev. Letters 85, 4912 (2000). L. Cristofolini, M.P.Fontana T. Berzina, P. Camorani - Mol. Cryst. Liq.Cryst. 398, 11 (2003).[3] Sanchez,-C.; Alcala,-R.; Hvilsted,-S.;Ramanujam,-P.-S. Appl.Phys.Lett. 77, 1440 (2000)P. Camorani, PhD Thesis, Univ. of Parma (2004).[4] L. Cristofolini, M.P. Fontana - PhilosophicalMagazine B 84, 1537, (2004).[5] P. Camorani, L. Cristofolini, G. Galli, M. P.Fontana - Mol. Cryst. Liq. Cryst. 375, 175 (2002).[6] L. Cristofolini, P. Cicuta, M.P. Fontana- J.Physics: Condensed Matter, 15, S1031 (2003).[7] L. Cristofolini, M.P. Fontana, M. Laus B. Frick -Phys. Rev. E, 64, 061803 (2001)[8] L. Cristofolini et al. Submitted for pubblicationAuthorsP.Camorani, L.Cristofolini, M.P.Fontana, E.PontecorvoUniversity of Parma CRS SOFT CNR-INFM.SOFT Scientific <strong>Report</strong> 2004-0660
- Page 4 and 5:
Istituto Nazionale per la Fisica de
- Page 6 and 7:
ContentsIntroduction 7Scientific Mi
- Page 8 and 9:
IntroductionSOFT is a CRS (Centro d
- Page 10 and 11: Scientific MissionThe scientific wo
- Page 13 and 14: Missioncolloids and soft colloidal
- Page 15 and 16: PersonnelManagement, Personnel and
- Page 17 and 18: FacilitiesSOFT Scientific Report 20
- Page 19 and 20: FacilitiesX-ray Diffraction Laborat
- Page 21 and 22: FacilitiesThin Film Laboratory - Ud
- Page 23 and 24: FacilitiesBrillouin Light Scatterin
- Page 25 and 26: Facilitieslaserf 2BSf 1FOBSSoftware
- Page 27 and 28: FacilitiesStatic Light Scattering L
- Page 29 and 30: FacilitiesSpectroscopy Laboratory -
- Page 31 and 32: LSFSOFT Scientific Report 2004-0630
- Page 33 and 34: LSFFig. 1 - BRISP layoutBackground
- Page 35 and 36: LSFBRISP first spectraLeft panel: e
- Page 37 and 38: LSFNeutron guideMonochromator cryst
- Page 39 and 40: LSFAXES: Advanced X-ray Emission Sp
- Page 41 and 42: LSFID16: Inelastic X-ray Scattering
- Page 43 and 44: LSFExperiments at LSFYear 2004Elett
- Page 45 and 46: LSFYear 2005Elettra - IUVS• High
- Page 47 and 48: LSFYear 2006Elettra - IUVS• Study
- Page 49 and 50: Scientific ReportsScientific Report
- Page 51 and 52: Scientific Report - Non Equilibrium
- Page 53 and 54: Scientific Report - Non Equilibrium
- Page 55 and 56: Scientific Report - Non Equilibrium
- Page 57 and 58: Scientific Report - Non Equilibrium
- Page 59: Scientific Report - Non Equilibrium
- Page 63 and 64: Scientific Report - Non Equilibrium
- Page 65 and 66: Scientific Report - Non Equilibrium
- Page 67 and 68: Scientific Report - Non Equilibrium
- Page 69 and 70: Scientific Report - Non Equilibrium
- Page 71 and 72: Scientific Report - Non Equilibrium
- Page 73 and 74: Scientific Report - Non Equilibrium
- Page 75 and 76: Scientific Report - Non Equilibrium
- Page 77 and 78: Scientific Report - Non Equilibrium
- Page 79 and 80: Scientific Report - Non Equilibrium
- Page 81 and 82: Scientific Report - Non Equilibrium
- Page 83 and 84: Scientific Report - Non Equilibrium
- Page 85 and 86: Scientific Report - Non Equilibrium
- Page 87 and 88: Scientific Report - Self Assembly,
- Page 89 and 90: Scientific Report - Self Assembly,
- Page 91 and 92: Scientific Report - Self Assembly,
- Page 93 and 94: Scientific Report - Self Assembly,
- Page 95 and 96: Scientific Report - Self Assembly,
- Page 97 and 98: Scientific Report - Self Assembly,
- Page 99 and 100: Scientific Report - Self Assembly,
- Page 101 and 102: Scientific Report - Elastic and ine
- Page 103 and 104: Scientific Report - Elastic and ine
- Page 105 and 106: Scientific Report - Elastic and ine
- Page 107 and 108: Scientific Report - Elastic and ine
- Page 109 and 110: Projects and CollaborationsSOFT Sci
- Page 111 and 112:
Projects and CollaborationsPAIS 200
- Page 113 and 114:
Projects and CollaborationsCollabor
- Page 115 and 116:
DisseminationSOFT Scientific Report
- Page 117 and 118:
DisseminationWe also point out the
- Page 119 and 120:
DisseminationF. A. Gorelli, V. M. G
- Page 121 and 122:
DisseminationL. Angelani, G. Foffi,
- Page 123 and 124:
DisseminationC. Casieri, F. De Luca
- Page 125 and 126:
DisseminationM. Finazzi, M. Portalu
- Page 127 and 128:
DisseminationS. Magazu, F. Migliard
- Page 129 and 130:
DisseminationB. Rossi, G. Viliani,
- Page 131 and 132:
DisseminationE. Zaccarelli, C. Maye
- Page 133 and 134:
DisseminationV. Bortolotti, M. Cama
- Page 135 and 136:
DisseminationC. De Michele, A. Scal
- Page 137 and 138:
DisseminationJ. Gutierrez, F. J. Be
- Page 139 and 140:
DisseminationA. Monaco, A. I. Chuma
- Page 141 and 142:
DisseminationM. Reale, M. A. De Lut
- Page 143 and 144:
DisseminationF. Bordi, C. Cametti,
- Page 145 and 146:
DisseminationSOFT Scientific Report
- Page 147 and 148:
DisseminationXII Liquid and Amorpho
- Page 149 and 150:
DisseminationConference on "new pro
- Page 151 and 152:
DisseminationX International worksh
- Page 153 and 154:
DisseminationXAFS13, 13 th Internat
- Page 155 and 156:
DisseminationOrganization of School
- Page 157 and 158:
DisseminationSoft Annual WorkshopsE
- Page 159 and 160:
DisseminationSoft WebSiteThe Web Si
- Page 161 and 162:
DisseminationContactsINFM-CNR Resar