金立gn5005后壳充电宝有DEsⅰgnedby

Journal list menu
Log in to Wiley Online Library
Email or Customer ID
Change Password
Old Password
New Password
Very Strong
Your password has been changed
Create a new account
Email or Customer ID
Forgot your password?
Enter your email address below. If your address has been previously registered, you will
receive an email with instructions on how to reset your password. If you don't receive an email,
you should register as a new user
Email or Customer ID
Please check your email for your password reset instructions.
Request Username
Can't sign in? Forgot your username?
Enter your email address below and we will send you your username
Email or Customer ID
If the address matches an existing account you will receive an email with instructions to retrieve your usernameAnthropogenic inputs of several heavy metals to nearshore basins off Los Angeles - ScienceDirect
ExportJavaScript is disabled on your browser. Please enable JavaScript to use all the features on this page., 1992, Pages 335-351Author links open overlay panelShow moreAbstractBudgets of anthropogenically-derived Cr, Zn and Pb in the Santa Monica-San Pedro Basin and the Palos Verdes Shelf are estimated from profiles of these metals in a large number of sediment cores. Comparisons of inventories in the deep basin with combined emissions from the responsible sewage outfalls indicate that no more than 7% of the Cr, 2% of the Zn and 5% of the Pb derived from the sewage source are buried in the nearshore basin. A similar comparison of metal accumulation on the Palos Verdes Shelf with discharges from the nearby JWPCP outfall indicates that 12% of the Zn and 20% of the Cr and Pb are deposited locally. The annual percentages of sewage-derived Pb retained should be significantly lower, because surface runoff and atmospheric fallout are also important input pathways for anthropogenic Pb. Offshore variations in sediment metal composition suggest that Cr is most strongly attached to sewage particles while Zn and Pb are more labile. We conclude that the majority of anthropogenic metals are exported offshore beyond the inner basin.Choose an option to locate/access this article:Check if you have access through your login credentials or your institution.orRecommended articlesCiting articles (0)Mean-field critical behaviour for percolation in high dimensions | SpringerLink
This service is more advanced with JavaScript available, learn more at http://activatejavascript.org
Advertisement
Mean-field critical behaviour for percolation in high dimensionsTakashi HaraGordon SladeArticleThe triangle condition for percolation states that\(\sum\limits_{x,y} {\tau (0,x)\tau (0,y) \cdot \tau (y,0)} \) is finite at the critical point, where τ(x, y) is the probability that the sitesx andy are connected. We use an expansion related to the lace expansion for a self-avoiding walk to prove that the triangle condition is satisfied in two situations: (i) for nearest-neighbour independent bond percolation on thed-dimensional hypercubic lattice, ifd is sufficiently large, and (ii) in more than six dimensions for a class of “spread-out” models of independent bond percolation which are believed to be in the same universality class as the nearest-neighbour model. The class of models in (ii) includes the case where the bond occupation probability is constant for bonds of length less than some large number, and is zero otherwise. In the course of the proof an infrared bound is obtained. The triangle condition is known to imply that various critical exponents take their mean-field (Bethe lattice) values\((\gamma
= 1,\delta
= \Delta _t
= 2, t\underset{\raise0.3em\hbox{$\smash{\scriptscriptstyle-}$}}{ \geqslant } 2)\) and that the percolation density is continuous at the critical point. We also prove thatv2 in (i) and (ii), wherev2 is the critical exponent for the correlation length.Neural Network Statistical Physic Complex System Nonlinear Dynamics High Dimension
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
This is a preview of subscription content,
to check access.Unable to display preview.&1.Aizenman, M.: Geometric analysis of φ4 fields and Ising models, Parts I and II. Commun. Math. Phys.86, 1–48 (1982)2.Aizenman, M., Barsky, D.J.: Sharpness of the phase transition in percolation models. Commun. Math. Phys.108, 489–526 (1987)3.Aizenman, M., Fernández, R.: On the critical behaviour of the magnetization in high dimensional Ising models. J. Stat. Phys.44, 393–454 (1986)4.Aizenman, M., Graham, R.: On the renormalized coupling constant and the susceptibility in λφd4 field theory and the Ising model in four dimensions. Nucl. Phys. B225 [FS9], 261–288 (1983)5.Aizenman, M., Kesten, H., Newman, C.M.: Uniqueness of the infinite cluster and continuity of connectivity functions for short and long range percolation. Commun. Math. Phys.111, 505–531 (1987)6.Aizenman, M., Newman, C.M.: Tree graph inequalities and critical behaviour in percolation models. J. Stat. Phys.36, 107–143 (1984)7.Aizenman, M., Simon, B.: Local Ward identities and the decay of correlations in ferromagnets. Commun. Math. Phys.77, 137–143 (1980)8.Barsky, D.J., Aizenman, M.: Percolation critical exponents under the triangle condition. Preprint (1988)9.van den Berg, J., Kesten, H.: Inequalities with applications to percolation and reliability, J. Appl. Prob.22, 556–569 (1985)10.Broadbent, S.R., Hammersley, J.M.: Percolation processes. I. Crystals and mazes. Proc. Camb. Phil. Soc.53, 629–641 (1957)11.Brydges, D.C., Fr?hlich, J., Sokal, A.D.: A new proof of the existence and nontriviality of the continuum φ24 and φ34 quantum field theories. Commun. Math. Phys.91, 141–186 (1983)12.Brydges, D.C., Spencer, T.: Self-avoiding walk in 5 or more dimensions. Commun. Math. Phys.97, 125–148 (1985)13.Chayes, J.T., Chayes, L.: On the upper critical dimension of Bernoulli percolation. Commun. Math. Phys.113, 27–48 (1987)14.Essam, J.W.: Percolation Theory. Rep. Prog. Phys.43, 833–912 (1980)15.Fr?hlich, J.: On the triviality of φd4 theories and the approach to the critical point in\(d\mathop
& \limits_{( = )} 4\) dimensions. Nucl. Phys. B200 [FS4], 281–296 (1982)16.Fr?hlich, J., Simon, B., Spencer, T.: Infrared bounds, phase transitions, and continuous symmetry breaking. Commun. Math. Phys.50, 79–95 (1976)17.Grimmett, G.: Percolation, Berlin Heidelberg New York: Springer 198918.Hammersley, J.M.: Percolation processes. Lower bounds for the critical probability. Ann. Math. Statist.28, 790–795 (1957)19.Hammersley, J.M.: Bornes supérieures de la probabilité critique dans un processus de filtration. In: Le Calcul des Probabilités et ses Applications 17–37 CNRS Paris (1959)20.Hara, T.: Mean field critical behaviour of correlation length for percolation in high dimensions. Preprint (1989)21.Hara, T., Slade, G.: On the upper critical dimension of lattice trees and lattice animals. Submitted to J. Stat. Phys.22.Hara, T., Slade, G.: Unpublished23.Kac, M., Uhlenbeck, G.E., Hemmer, P.C.: On the van der Waals theory of the vapor-liquid equilibrium. I. Discussion of a one-dimensional model. J. Math. Phys.4, 216–288 (1963)24.Kesten, H.: Percolation theory and first passage percolation. Ann. Probab.15,
(1987)25.Lawler, G.: The infinite self-avoiding walk in high dimensions. To appear in Ann. Probab. (1989)26.Lebowitz, J.L., Penrose, O.: Rigorous treatment of the van der Waals-Maxwell theory of the liquid-vapor transition. J. Math. Phys.7, 98–113 (1966)27.Menshikov, M.V., Molchanov, S.A., Sidorenko, A.F.: Percolation theory and some applications, Itogi Nauki i Tekhniki (Series of Probability Theory, Mathematical Statistics, Theoretical Cybernetics)24, 53–110 (1986). English translation. J. Soviet Math.42,
(1988)28.Nguyen, B.G.: Gap exponents for percolation processes with triangle condition. J. Stat. Phys.49, 235–243 (1987)29.Park, Y.M.: Direct estimates on intersection probabilities of random walks. To appear in J. Stat. Phys.30.Russo, L.: On the critical percolation probabilities. Z. Wahrsch. Verw. Gebiete.56, 229–237 (1981)31.Slade, G.: The diffusion of self-avoiding random walk in high dimensions. Commun. Math. Phys.110, 661–683 (1987)32.Slade, G.: The scaling limit of self-avoiding random walk in high dimensions. Ann. Probab.17, 91–107 (1989)33.Slade, G.: Convergence of self-avoiding random walk to Brownian motion in high dimensions. J. Phys. A: Math. Gen.21, L417-L420 (1988)34.Slade, G.: The lace expansion and the upper critical dimension for percolation, Lectures notes from the A.M.S. Summer Seminar, Blacksburg, June 198935.Sokal, A.D.: A rigorous inequality for the specific heat of an Ising or φ4 ferromagnet. Phys. Lett.71A, 451–453 (1979)36.Sokal, A.D., Thomas, L.E.: Exponential convergence to equilibrium for a class of random walk models. J. Stat. Phys.54, 797–828 (1989)37.Stauffer, D.: Introduction to percolation theory. Taylor and Francis, London Philadelphia (1985)38.Tasaki, H.: Hyperscaling inequalities for percolation. Commun. Math. Phys.113, 49–65 (1987)39.Tasaki, H.: Private communication40.Yang, W., Klein, D.: A note on the critical dimension for weakly self avoiding walks. Prob. Th. Rel. Fields79, 99–114 (1988)41.Ziff, R.M., Stell, G.: Critical behaviour in three-dimensional percolation: Is the percolation threshold a Lifshitz point? Preprint (1988)Takashi Hara1Gordon Slade21.Courant Institute of Mathematical SciencesN.Y.U.New YorkUSA2.Department of Mathematics and StatisticsMcMaster UniversityHamiltonCanada

我要回帖

更多关于 金立gn800手机壳 的文章

 

随机推荐