Self Assembly, Clustering, Structural arrestBiopolymer-Vescicle Interactions 85Polyelectrolyte-Liposome Complexes: Evidence of Equilibrium Multi-Compartment Aggregates 86Dielectric Properties of Polyelectrolyte Aqueous Solutions: the Scaling Approach 87Aging of aqueous Laponite suspensions stu<strong>di</strong>ed by 23 Na Triple-Quantum NMR spectroscopy 88Clustering and Cooperative Dynamics in Reactive Mixtures 89Role of metal ions in protein aggregation processes 90Role of water around biomolecules and surfactants 91Multi-Scale Simulations of Macromolecular Systems 92Investigation of the Relation Between Local Inherent Structures Properties and the Diffusivity 93Coil-Globule Transition of DNA Molecules Induced by Cationic Surfactants 94Multi-Scale Coarse-Graining of Diblock Copolymer Self-Assembly 95Bernal Spiral Clusters in Colloid-Polymer Mixtures 96Molecular Clustering by High Resolution NMR 97Non-invasive 1 H-NMR in porous materials of artistic interest 98Elastic and anelastic scattering of neutrons and X-raysIon Density Fluctuations in Liquid Gallium 99Femtosecond dynamics in Ferromagnetic Metals 100<strong>Soft</strong> Resonant X-ray Scattering 101Picosecond-Timescale Fluctuations of Proteins in Glassy Matrices: The Role of Viscosity 102Neutron inelastic scattering on liquid CD 4 : a probe of the dynamics in simple molecular liquids 103The Dynamics of Dilute H 2 Enabling New Calibration Methods in Neutron Spectroscopy 104Effect of Solvent and of Confinement on the Dynamics of Hydrated Proteins 105Dynamics in Model Membranes, Membrane-Protein and Membrane-DNA Interactions 106Dynamics of Hydrated Saccharides and Saccharide Gels 10749SOFT Scientific <strong>Report</strong> 2004-06
Scientific <strong>Report</strong> – Non Equilibrium Dynamics and ComplexityLight and ComplexityIn a nutshell, a random laser is a <strong>di</strong>sorderedamplifying optical cavity emitting coherent ra<strong>di</strong>ation.The system can be realized by artificial nanostructuredoptical devices, or can be a self-organized<strong>di</strong>spersion of particles in the multi-scattering regime.In both cases, optical gain can be obtained with thead<strong>di</strong>tion of some active materials, like dyes orquantum dots. Random laser emission is stronglyaffected by the structure and the history of thematerial, hence it is an original and multi<strong>di</strong>sciplinaryapproach for the investigation of soft-matter.Ad<strong>di</strong>tionally, this kind of lasers strikingly <strong>di</strong>splaysthose ingre<strong>di</strong>ents which are typical of the physics ofcomplexity: randomness and nonlinearity.In Refs. [1], it has been shown that theory ofrandom laser can be reformulated as mean field spinglass theory and a series of new physical processes,inclu<strong>di</strong>ng for example a “glassy behaviour of light,”have been pre<strong>di</strong>cted. Such an approach open newopportunities for testing the modern theory ofcomplexity, and conceiving new experiments on theglass transition which should enable to investigatenew previously un-accessible regimes, due to theintrinsically fast dynamics of a “photon glass.”Specifically, a random optical cavity is characterizedby N resonant modes with angular frequencies ω nand complex amplitudes a n, (n=1…N); such that theenergy stored into each mode is ω n|a n| 2 . Laser theorysays that the moduli of the a n are slowly varying withrespect to the phases ϕ n, hence the former can betaken as quenched variables while the latter are therelevant dynamic variables and take the role ofspherical spins. The Hamiltonian is:∑H = cos( ϕ + ϕ −ϕ−ϕ)J spqrspqwhere the random coupling constants J aredetermined by the spatial overlap of the resonantmodes. The replica method is applied for determiningthe energy landscape of the model and the existenceof a one-step replica symmetry breaking (1RSB), orglass-transition. The role of the inverse temperatureis played by the ratio between the squared averageenergy stored into each mode and the amount ofnoise due to spontaneous emission. There exist acritical value of this effective temperature for theexistence of an exponentially large number of metastablestates, each correspon<strong>di</strong>ng to a <strong>di</strong>fferentrFig. 2: Ab initio 3D+1 computation of specklepatterns at 532nm obtained when light propagatesin high concentration colloidal materials, whosestructure is determined by molecular dynamicsimulations. These numerical techniques providenew opportunities for the investigation of softmaterialproperties, as they may enrich theinformation that can be extracted by experiments inthe multiple-scattering regime.mode-locking process of the random laser. In thisway the complexity (i.e. the configurational entropy)of light in random lasers can be calculated, and thecritical temperature is expressed in term ofexperimentally accessible quantities.Complex dynamics of light is also found, theoreticallyand experimentally, when focused laser beamspropagated in soft-matter like liquid crystals. [2] Inthis case, <strong>di</strong>sorder and nonlinearity contribute to thegeneration of multiple light filaments whosedynamics can be described by the same para<strong>di</strong>gmsof the physics of soft-matter. Understan<strong>di</strong>ng theseprocesses is relevant for various applications, fromall optical <strong>di</strong>gital devices to laser surgery.Photonics in <strong>di</strong>sordered or structured systems,(“complex photonics”) is a very active andmulti<strong>di</strong>sciplinary research field, to which we are alsocontributing by developing new computationalapproaches (figure 1), and designing novel opticaldevices [3] (as e.g. “photonic crystals”) which can beinfiltrated by soft-materials, and provideopportunities for femtoliter substance analysis.References[1] L. Angelani, C. Conti, G. Ruocco, F. Zamponi,Phys. Rev. Lett. 96, 065702 (2006); Condmat/0511427;L. Angelani, C. Conti, G. Ruocco, F.Zamponi, cond-mat/0604242, submitted to Phys.Rev. B[2] C. Conti, Phys. Rev. 72, 066620 (2005); C.Conti, M. Peccianti, G. Assanto, Opt. Lett. (2006),submitted.[3] A. Di Falco, C. Conti, G. Assanto, Appl. Phys. B81, 415 (2005); A. Di Falco C. Conti, G. Assanto,Opt. Lett. 31, 250 (2006); A. Di Falco C. Conti, G.Assanto, Opt. Lett. (2006), submittedFig. 1: Relevant overlap of the spin glass theoryof random lasers and complexity Vs the effectivetemperature (from Ref. 1)AuthorsL. Angelani (a), C. Conti (b,c), G. Ruocco (c) , F.Zamponi (d), G. Assanto (e), M. Peccianti (e)(a) SMC INFM-CNR (b) Research Center EnricoFermi (c) SOFT INFM-CNR (d) Ecole NormalSuperiore (e) University Roma Tre.SOFT Scientific <strong>Report</strong> 2004-0650
- 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: Scientific ReportsScientific Report
- 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 and 60: Scientific Report - Non Equilibrium
- Page 61 and 62: 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