Pub Date : 1990-11-01DOI: 10.1051/JPHYS:0199000510220254300
O. Abillon, E. Perez
Nous avons mesure les forces entre deux surfaces de mica immergees dans une phase lamellaire gonflee a l'eau (CTAB/hexanol/eau salee). Les bicouches s'orientent parallelement aux surfaces de mica. Les courbes force-distance presentent des domaines ou l'eau est continument ejectee d'entre les lamelles, et des domaines ou le systeme saute rapidement a une autre distance en ejectant des lamelles. Nous avons etudie l'effet sur les forces d'un deplacement dans le diagramme de phases a periode spatiale constante et egalement le long de la ligne de dilution
{"title":"Swollen lamellar phases between two solid walls : undulation forces and generation of defects","authors":"O. Abillon, E. Perez","doi":"10.1051/JPHYS:0199000510220254300","DOIUrl":"https://doi.org/10.1051/JPHYS:0199000510220254300","url":null,"abstract":"Nous avons mesure les forces entre deux surfaces de mica immergees dans une phase lamellaire gonflee a l'eau (CTAB/hexanol/eau salee). Les bicouches s'orientent parallelement aux surfaces de mica. Les courbes force-distance presentent des domaines ou l'eau est continument ejectee d'entre les lamelles, et des domaines ou le systeme saute rapidement a une autre distance en ejectant des lamelles. Nous avons etudie l'effet sur les forces d'un deplacement dans le diagramme de phases a periode spatiale constante et egalement le long de la ligne de dilution","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"476 ","pages":"2543-2556"},"PeriodicalIF":0.0,"publicationDate":"1990-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91520417","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-11-01DOI: 10.1051/JPHYS:0199000510220257100
D. Ausserré, D. Chatenay, G. Coulon, B. Collin
L'apparition de domaines circulaires en relief a la surface de films de copolymeres bisequences deposes sur un solide soumis a une trempe est due a la formation d'un ordre lamellaire dans le film qui s'accompagne d'une quantification de son epaisseur locale. En admettant que la structure des bords des domaines est une simple dislocation, les equations decrivant l'evolution temporelle de la distribution de taille des domaines sont etablies
{"title":"Growth of two dimensional domains in copolymer thin films","authors":"D. Ausserré, D. Chatenay, G. Coulon, B. Collin","doi":"10.1051/JPHYS:0199000510220257100","DOIUrl":"https://doi.org/10.1051/JPHYS:0199000510220257100","url":null,"abstract":"L'apparition de domaines circulaires en relief a la surface de films de copolymeres bisequences deposes sur un solide soumis a une trempe est due a la formation d'un ordre lamellaire dans le film qui s'accompagne d'une quantification de son epaisseur locale. En admettant que la structure des bords des domaines est une simple dislocation, les equations decrivant l'evolution temporelle de la distribution de taille des domaines sont etablies","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"41 1","pages":"2571-2580"},"PeriodicalIF":0.0,"publicationDate":"1990-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"80773371","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-11-01DOI: 10.1051/JPHYS:0199000510220258100
J. Bulthuis, L. Plomp
The model of rotational diffusion in the presence of an orienting potential has been adapted to the case of an asymmetric top molecule in an orienting potential that is defined by two ordering parameters. It has been used to describe the relaxation by the quadrupolar mechanism of the deuterons in toluene, dissolved in «Phase V». No set of diffusion constants could be found, which simultaneously reproduce all spectral densities that were derived from the measured relaxation rates. Only very approximate agreement could be obtained with sets of diffusion constants in which two constants are of the same order of magnitude and the diffusion about the axis in the plane of the benzene ring and perpendicular to the axis of the methylgroup, is slower by an order of magnitude. The anisotropy in the viscosity of the solution has not explicitly been taken into account, but it has been indicated how this might be done. At this stage, therefore, no definitive conclusions can be drawn, but clearly the application of the rotational diffusion model in liquid crystalline solutions should be considered with care
{"title":"On the applicability of the rotational diffusion model in liquid crystalline solvents. A nuclear magnetic relaxation study of toluene","authors":"J. Bulthuis, L. Plomp","doi":"10.1051/JPHYS:0199000510220258100","DOIUrl":"https://doi.org/10.1051/JPHYS:0199000510220258100","url":null,"abstract":"The model of rotational diffusion in the presence of an orienting potential has been adapted to the case of an asymmetric top molecule in an orienting potential that is defined by two ordering parameters. It has been used to describe the relaxation by the quadrupolar mechanism of the deuterons in toluene, dissolved in «Phase V». No set of diffusion constants could be found, which simultaneously reproduce all spectral densities that were derived from the measured relaxation rates. Only very approximate agreement could be obtained with sets of diffusion constants in which two constants are of the same order of magnitude and the diffusion about the axis in the plane of the benzene ring and perpendicular to the axis of the methylgroup, is slower by an order of magnitude. The anisotropy in the viscosity of the solution has not explicitly been taken into account, but it has been indicated how this might be done. At this stage, therefore, no definitive conclusions can be drawn, but clearly the application of the rotational diffusion model in liquid crystalline solutions should be considered with care","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"1 1","pages":"2581-2593"},"PeriodicalIF":0.0,"publicationDate":"1990-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"76162226","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-11-01DOI: 10.1051/JPHYS:0199000510210243100
M. Kleman
The phase degrees of freedom of aperiodic crystals (quasicrystals) are far from being understood. In this paper we study in great detail the geometrical and topological properties of the «phase space» of quasicrystals, for usual quasicrystalline symmetries (icosahedral and pentagonal cases) and for the cases d=3, d ∥ =1 and d=4, d ∥ =2. It is shown that the universal covering of the phase space is a curved crystal of negative Gaussian curvature, whose group of automorphisms contains therefore the fundamental group of the phase space as a subgroup. This fundamental group is calculated in each case. The results do not depend in any way on the cho Les degres de liberte relatifs a la phase des cristaux aperiodiques sont loin d'etre compris. Dans cet article, nous etudions en grand detail les proprietes geometriques et topologiques de l'espace representatif de la phase pour des symetries quasicristallines usuelles (icosaedrique et pentagonale) et pour les cas d=3, d ∥ =1 et d=4, d∥=2. On montre que l'espace de la phase a pour revetement universel un cristal d'espace courbe de courbure gaussienne negative; le groupe fondamental de l'espace de la phase est un sous-groupe du groupe d'automorphismes de ce cristal courbe. Nous le calculons dans chaque cas envisage. Les resultats ne dependent en aucune maniere du choix et de la «surface atomique» (le motif) qui decore la cellule de base du cristal hypercubique d'ou le quasicristal est engendre. En consequence, ils ne dependent pas non plus du fait que les phasons sont continus ou discrets. Ces recherches constituent un premier pas necessaire dans l'etude de la nature geometrique et topologique des deformations du type «phason». On discute en outre de l'homomorphisme entre l'espace de la phase et le groupe qui classe les dislocations. Finalement nous indiquons sans entrer dans les details que le groupe fondamental de l'espace de la phase classe les defauts topologiques du type phason
非周期晶体(准晶体)的相自由度尚不清楚。在本文中，我们详细地研究了准晶体的“相空间”的几何和拓扑性质，对于通常的准晶体对称(二十面体和五边形的情况)，对于d=3, d∥=1和d=4, d∥=2的情况。证明了相空间的普遍覆盖是一个负高斯曲率的弯曲晶体，因此其自同构群包含相空间的基群作为子群。这个基本组是在每种情况下计算出来的。结果不以任何方式依赖于三个自由度的关系，一个阶段的非周期性特征，一个阶段的非周期性特征。在第二篇文章中，noous etututions en grand detail les proprietes geometriques et topologiques de l'空间表征de la phase pour des des systemes准晶uselles (icosaedrique et pentagonale) et pour les cas d=3, d∥= 1 et d=4, d∥=2。On montre que l'espace de la phase a pour reveement universsel uncristle d'espace courbe de courbure gaussienne negative;基本群是指相空间的基本群;自同构群是指晶体的自同构群。现在，我们的计算和我们的设想是一样的。这些结果依赖于“表面原子”、“表面原子”、“细胞”、“晶体基”、“超立方体”和“准晶体”。因此，我们需要依赖于非事实和非事实，而不是连续的离散相。他的研究主要是关于“相位”型变形的组成、几何和拓扑结构的性质和必要性。讨论了位错的同态中心、位错的空间、位错的群、位错的类。finfinement的用法和样例:finfinement的用法和样例:finfinement的用法和样例:finfinement的用法和样例:finfinement
{"title":"Topology of the phase in aperiodic crystals","authors":"M. Kleman","doi":"10.1051/JPHYS:0199000510210243100","DOIUrl":"https://doi.org/10.1051/JPHYS:0199000510210243100","url":null,"abstract":"The phase degrees of freedom of aperiodic crystals (quasicrystals) are far from being understood. In this paper we study in great detail the geometrical and topological properties of the «phase space» of quasicrystals, for usual quasicrystalline symmetries (icosahedral and pentagonal cases) and for the cases d=3, d ∥ =1 and d=4, d ∥ =2. It is shown that the universal covering of the phase space is a curved crystal of negative Gaussian curvature, whose group of automorphisms contains therefore the fundamental group of the phase space as a subgroup. This fundamental group is calculated in each case. The results do not depend in any way on the cho Les degres de liberte relatifs a la phase des cristaux aperiodiques sont loin d'etre compris. Dans cet article, nous etudions en grand detail les proprietes geometriques et topologiques de l'espace representatif de la phase pour des symetries quasicristallines usuelles (icosaedrique et pentagonale) et pour les cas d=3, d ∥ =1 et d=4, d∥=2. On montre que l'espace de la phase a pour revetement universel un cristal d'espace courbe de courbure gaussienne negative; le groupe fondamental de l'espace de la phase est un sous-groupe du groupe d'automorphismes de ce cristal courbe. Nous le calculons dans chaque cas envisage. Les resultats ne dependent en aucune maniere du choix et de la «surface atomique» (le motif) qui decore la cellule de base du cristal hypercubique d'ou le quasicristal est engendre. En consequence, ils ne dependent pas non plus du fait que les phasons sont continus ou discrets. Ces recherches constituent un premier pas necessaire dans l'etude de la nature geometrique et topologique des deformations du type «phason». On discute en outre de l'homomorphisme entre l'espace de la phase et le groupe qui classe les dislocations. Finalement nous indiquons sans entrer dans les details que le groupe fondamental de l'espace de la phase classe les defauts topologiques du type phason","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"3 1","pages":"2431-2447"},"PeriodicalIF":0.0,"publicationDate":"1990-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"74930706","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-11-01DOI: 10.1051/JPHYS:0199000510210242100
J. Fontanari
The performance of a Hopfield network in learning an extensive number of concepts having access only to a finite supply of typical data which exemplify the concepts is studied. The minimal number of examples which must be taught to the network in order it starts to create representations for the concepts is calculated analitically. It is shown that the mixture states play a crucial role in the creation of these representations
{"title":"Generalization in a Hopfield network","authors":"J. Fontanari","doi":"10.1051/JPHYS:0199000510210242100","DOIUrl":"https://doi.org/10.1051/JPHYS:0199000510210242100","url":null,"abstract":"The performance of a Hopfield network in learning an extensive number of concepts having access only to a finite supply of typical data which exemplify the concepts is studied. The minimal number of examples which must be taught to the network in order it starts to create representations for the concepts is calculated analitically. It is shown that the mixture states play a crucial role in the creation of these representations","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"13 1","pages":"2421-2430"},"PeriodicalIF":0.0,"publicationDate":"1990-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"87560584","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-11-01DOI: 10.1051/JPHYS:0199000510220252100
S. Avrillier, E. Tinet, E. Delettre
An accurate Monte Carlo (MC) computer model is used to calculate the reflectances (R) and transmittances (T) of isotropic scattering media for the case of collimated beam illumination and for a wide range of absorption and scattering coefficients κ and σ per unit length. The MC results are presented by means of sets of curves with distance scaling in order to give an overall understanding of the subject. A simple diagram is constructed with accurate MC results and can be used for direct graphical determination of κ and σ from R and T measurements. The effects of reflections at the boundaries are described in the last section
{"title":"Monte Carlo simulation of collimated beam transmission through turbid media","authors":"S. Avrillier, E. Tinet, E. Delettre","doi":"10.1051/JPHYS:0199000510220252100","DOIUrl":"https://doi.org/10.1051/JPHYS:0199000510220252100","url":null,"abstract":"An accurate Monte Carlo (MC) computer model is used to calculate the reflectances (R) and transmittances (T) of isotropic scattering media for the case of collimated beam illumination and for a wide range of absorption and scattering coefficients κ and σ per unit length. The MC results are presented by means of sets of curves with distance scaling in order to give an overall understanding of the subject. A simple diagram is constructed with accurate MC results and can be used for direct graphical determination of κ and σ from R and T measurements. The effects of reflections at the boundaries are described in the last section","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"106 1","pages":"2521-2542"},"PeriodicalIF":0.0,"publicationDate":"1990-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78969087","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-11-01DOI: 10.1051/JPHYS:0199000510210239900
V. Dmitriev, Yu. M. Gufan, S. Rochal, R. Toledano
A theoretical model is proposed for the formation of quasicrystalline alloys. The icosahedral phase is known to result from a reconstructive transition of the displacive type from a parent crystalline structure. Two order parameters are involved in the transition mechanism: a displacement field which transforms a number of sublattices into icosahedral clusters, and an icosahedral density wave which breaks incommensurately the initial translational order. The main features of the model are introduced through the illustrative example of AlMnSi Un modele theorique est propose pour expliquer la formation des alliages quasicristallins. La phase icosaedrique resulte dans ce modele, d'une transition reconstructive de type displacif a partir d'une phase mere cristalline. Le mecanisme de la transition met en jeu deux parametres d'ordre distincts: un champ de deplacements qui transforme certains sous-reseaux cristallins en assemblages icosaedriques, et une onde de densite qui brise de facon incommensurable l'ordre translationnel de la phase mere. Les principaux aspects de la theorie sont introduits a travers l'exemple de AlMnSi
{"title":"Theory of the formation of quasicrystals","authors":"V. Dmitriev, Yu. M. Gufan, S. Rochal, R. Toledano","doi":"10.1051/JPHYS:0199000510210239900","DOIUrl":"https://doi.org/10.1051/JPHYS:0199000510210239900","url":null,"abstract":"A theoretical model is proposed for the formation of quasicrystalline alloys. The icosahedral phase is known to result from a reconstructive transition of the displacive type from a parent crystalline structure. Two order parameters are involved in the transition mechanism: a displacement field which transforms a number of sublattices into icosahedral clusters, and an icosahedral density wave which breaks incommensurately the initial translational order. The main features of the model are introduced through the illustrative example of AlMnSi Un modele theorique est propose pour expliquer la formation des alliages quasicristallins. La phase icosaedrique resulte dans ce modele, d'une transition reconstructive de type displacif a partir d'une phase mere cristalline. Le mecanisme de la transition met en jeu deux parametres d'ordre distincts: un champ de deplacements qui transforme certains sous-reseaux cristallins en assemblages icosaedriques, et une onde de densite qui brise de facon incommensurable l'ordre translationnel de la phase mere. Les principaux aspects de la theorie sont introduits a travers l'exemple de AlMnSi","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"31 1","pages":"2399-2405"},"PeriodicalIF":0.0,"publicationDate":"1990-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"79443288","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-11-01DOI: 10.1051/JPHYS:0199000510220260500
I. Barnes, P. Dérian, S. Hyde, B. Ninham, T. Zemb
et leurs predictions confrontees aux resultats experimentaux. Abstract. 2014 The « anomalous » fluid isotropic phase in the DDAB/tetradecane/water system differs in important ways from microemulsion phases in related systems, and is thus a useful test for models. On the basis of absolute scaled neutron and X-ray scattering data we show here that the microstructure is best characterised as a randomly folded reverse bilayer. All previously reported examples of this structure are restricted to a narrow range of composition and temperature. In this case of a stiff bilayer with low spontaneous interfacial curvature it extends over a large region of the ternary phase diagram at room temperature, the boundaries of which are explained in terms of simple geometric constraints. Other possible microstructures are
{"title":"A disordered lamellar structure in the isotropic phase of a ternary double-chain surfactant system","authors":"I. Barnes, P. Dérian, S. Hyde, B. Ninham, T. Zemb","doi":"10.1051/JPHYS:0199000510220260500","DOIUrl":"https://doi.org/10.1051/JPHYS:0199000510220260500","url":null,"abstract":"et leurs predictions confrontees aux resultats experimentaux. Abstract. 2014 The « anomalous » fluid isotropic phase in the DDAB/tetradecane/water system differs in important ways from microemulsion phases in related systems, and is thus a useful test for models. On the basis of absolute scaled neutron and X-ray scattering data we show here that the microstructure is best characterised as a randomly folded reverse bilayer. All previously reported examples of this structure are restricted to a narrow range of composition and temperature. In this case of a stiff bilayer with low spontaneous interfacial curvature it extends over a large region of the ternary phase diagram at room temperature, the boundaries of which are explained in terms of simple geometric constraints. Other possible microstructures are","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"6 1","pages":"2605-2628"},"PeriodicalIF":0.0,"publicationDate":"1990-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"76448808","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-11-01DOI: 10.1051/JPHYS:0199000510210240700
E. Guitter
We analyze by field theoretical methods the large scale behavior of a stack of tethered or polymerized membranes. We show that, in the decoupled phase where there is no resistance to the shear between successive membranes, anharmonic terms dictated by rotational symmetry in the bulk have to be taken into account. They renormalize the elastic coefficients and lead to a large distance anomalous elasticity, as in the case of a single tethered membrane Nous analysons par des techniques de theorie des champs le comportement a grande echelle d'un empilement de membranes reticulees ou polymerisees. Nous montrons que, dans la phase decouplee ou il n'y a pas de resistance au cisaillement entre membranes successives, la symetrie de rotation dans l'espace ambiant oblige a tenir compte de certains termes anharmoniques. Ces termes additionnels renormalisent les coefficients elastiques et conduisent a une elasticite anormale a grandes distances, de la meme maniere que pour une membrane reticulee isolee
我们用场理论方法分析了一堆系绳或聚合膜的大尺度行为。我们表明，在解耦阶段，连续膜之间没有剪切阻力，必须考虑由体中旋转对称性决定的非调和项。它们使弹性系数重新规范化，并导致大距离异常弹性，就像在单个系绳膜的情况下，Nous分析par des techniques de theorie des champs le comcomement a grande echelle d'un empement de membrane reticulees或polymerises一样。“Nous montrons que”，“dans la phase decpleplee”，“Nous montrons que”，“dans la phase decplee”，“Nous montrons que”，“Nous montrons que”，“Nous montrons que”，“Nous montrons que”。这两项是附加的正态化系数，弹性系数和传导系数，弹性系数和传导系数，在大的距离上，de la meme maniere que pour 1膜网状隔离
{"title":"Anharmonic theory of a stack of tethered membranes","authors":"E. Guitter","doi":"10.1051/JPHYS:0199000510210240700","DOIUrl":"https://doi.org/10.1051/JPHYS:0199000510210240700","url":null,"abstract":"We analyze by field theoretical methods the large scale behavior of a stack of tethered or polymerized membranes. We show that, in the decoupled phase where there is no resistance to the shear between successive membranes, anharmonic terms dictated by rotational symmetry in the bulk have to be taken into account. They renormalize the elastic coefficients and lead to a large distance anomalous elasticity, as in the case of a single tethered membrane Nous analysons par des techniques de theorie des champs le comportement a grande echelle d'un empilement de membranes reticulees ou polymerisees. Nous montrons que, dans la phase decouplee ou il n'y a pas de resistance au cisaillement entre membranes successives, la symetrie de rotation dans l'espace ambiant oblige a tenir compte de certains termes anharmoniques. Ces termes additionnels renormalisent les coefficients elastiques et conduisent a une elasticite anormale a grandes distances, de la meme maniere que pour une membrane reticulee isolee","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"31 6","pages":"2407-2420"},"PeriodicalIF":0.0,"publicationDate":"1990-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91495803","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-11-01DOI: 10.1051/JPHYS:0199000510210239500
S. Komura, A. Baumgärtner
The spectral dimension d s of polymerized and fluid self-avoiding vesicles are investigated by Monte Carlo methods. For both cases we obtained d s =2, which indicates that these surfaces belong to the same class of «microcanonical» surfaces
用蒙特卡罗方法研究了聚合和流体自避囊泡的光谱维数。对于这两种情况，我们得到了d s =2，这表明这些曲面属于同一类“微正则”曲面
{"title":"Spectral dimension of fluid membranes","authors":"S. Komura, A. Baumgärtner","doi":"10.1051/JPHYS:0199000510210239500","DOIUrl":"https://doi.org/10.1051/JPHYS:0199000510210239500","url":null,"abstract":"The spectral dimension d s of polymerized and fluid self-avoiding vesicles are investigated by Monte Carlo methods. For both cases we obtained d s =2, which indicates that these surfaces belong to the same class of «microcanonical» surfaces","PeriodicalId":14747,"journal":{"name":"Journal De Physique","volume":"33 1","pages":"2395-2398"},"PeriodicalIF":0.0,"publicationDate":"1990-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"87999073","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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