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Poisson

Poisson is a French surname. It may also refer to places in France, concepts in mathematics and physics named after the mathematician , and other uses.

People

Siméon Denis Poisson

was a prominent and born on June 21, 1781, in , , to a family of modest means; his father, a former soldier, held a lowly administrative post locally. He received his early education at home and in local schools before entering the École Centrale in in 1796 and excelling in the entrance examination to the in in 1798, where he studied under influential figures such as and . Poisson graduated in 1800 and began his academic career as a at the , advancing to deputy professor in 1802 and full professor in 1806. He also held positions as an astronomer at the Bureau des Longitudes from 1808, chair of mechanics at the Faculté des Sciences from 1809, and was elected to the physics section of the Académie des Sciences in 1812. Poisson's scholarly output was prolific, with over 300 mathematical works spanning , , , and partial differential equations. In probability, his 1837 treatise Recherches sur la probabilité des jugements en matière criminelle et en matière civile extended earlier ideas on the and introduced concepts central to modern statistical distributions. His contributions to physics included advancements in the , magnetism, and electricity, often building on the analytical frameworks of his mentors. Poisson's rigorous approach to applying to physical phenomena solidified his reputation as a key figure in the development of during the early . Poisson's legacy endures through numerous scientific concepts bearing his name, such as in electrostatics and the in , reflecting his enduring influence on both fields. He received several honors, including election as a in 1818 and progression through the ranks of the Légion d'honneur, culminating in the title of Commandeur in 1837. Poisson died on April 25, 1840, in Sceaux near , leaving a profound on science and international .

Poisson (surname)

Poisson is a French surname derived from the Old French word poisson, meaning "fish," and typically served as an occupational name for a fisherman, fishmonger, or seller, or occasionally as a nickname for someone with fish-like features. The name originated in medieval France and remains prevalent in French-speaking regions, including Quebec and other parts of Canada due to historical migration. Among notable individuals bearing the surname, beyond the renowned mathematician , are several historical figures from politics, arts, and culture. Jeanne Antoinette Poisson (1721–1764), known as , was the influential chief mistress of King and a prominent patron of . Her brother, Abel-François Poisson (1727–1781), Marquis de Marigny, served as director of the Bâtiments du Roi, overseeing major artistic and architectural projects under . In the theater world, Paul Poisson (1658–1735) was a celebrated French actor with the , renowned for his comedic roles including the character Crispin. Later, Paul Poisson (1887–1983) became a Canadian politician, serving as the first mayor of , in 1921 and representing Essex North in provincial politics. The surname's global distribution shows it held by around 21,000 people, ranking as the 26,335th most common worldwide, with the highest incidence in (approximately 13,000 bearers) and significant presence in and the . Genealogical databases like record over 100,000 historical entries for Poisson, reflecting its enduring use in communities. Variations such as Poissonnier or Pousson occasionally appear, often denoting related occupations like preparation.

Places

Poisson, Saône-et-Loire

Poisson is a commune located in the department of the region in eastern . It lies on the border between the Charolais and Brionnais areas in southern , at coordinates approximately 46°23′N 4°08′E, and covers an area of 35.48 km². The commune features varied terrain including prairies, woods, and the meandering Arconce River, which supports local pisciculture activities. As of the 2022 census, Poisson has a of 559 inhabitants, reflecting a slight decline from 603 in 1968, with an average annual variation of -0.2% between 2016 and 2022. The stands at 15.8 inhabitants per km². Historically, the commune has been tied to in the Charolais region, with its landscape shaped by agricultural traditions dating back to medieval times, including its position along the route of Romanesque churches. The local economy centers on , which accounts for about 50% of the 16 establishments in , employing 8 as of 2023. It is particularly renowned for Charolais beef production, with supporting amenities like an artisan bakery and a restaurant specializing in local meats and fish. Notable features include marked walking trails for and the Church of the Baptist, a key historical site. is handled by a , with recent administrative updates including the of the for alerts. The commune is situated near , approximately 35 km to the east, facilitating regional connections.

Mathematics and Statistics

Poisson distribution

The Poisson distribution is a discrete probability distribution that models the probability of a given number of events occurring in a fixed of time or , when these events happen independently with a known constant average rate and independently of the time since the last event. It is particularly useful for describing rare or random events, such as the number of defects in or arrivals at a facility. The probability mass function of the Poisson distribution is given by P(K = k) = \frac{\lambda^k e^{-\lambda}}{k!} for k = 0, 1, 2, \dots, where \lambda > 0 is the rate parameter representing the expected number of events in the interval, and e is the base of the natural logarithm. The mean and variance of a Poisson random variable K are both equal to \lambda, which highlights the distribution's equidispersion property. The Poisson distribution arises as the limiting case of the when the number of trials n approaches infinity and the success probability p approaches zero such that np = \lambda remains constant, making it suitable for approximating rare events in large populations. Common applications include modeling customer arrivals in , where the number of arrivals in a fixed period follows a Poisson distribution under assumptions of a constant arrival rate, and counting radioactive decay events, as the unpredictable nature of atomic disintegrations aligns with the distribution's properties. In the context of a Poisson process, the number of events occurring in a fixed also follows this distribution. The distribution is named after the , who derived it in his 1837 work Recherches sur la probabilité des jugements en matière criminelle et en matière civile, where he applied probabilistic methods to legal judgments.

Poisson process

The Poisson process is a fundamental model used to describe the occurrence of random events in continuous time, where events happen independently and at a constant average rate. Formally, it is defined as a counting process \{N(t), t \geq 0\} with N(0) = 0, where the increments N(t + s) - N(t) over disjoint time intervals are independent random variables, and the number of events in any interval of length t follows a with mean \lambda t for a fixed rate parameter \lambda > 0. This structure captures scenarios such as particle arrivals or customer queues, ensuring that the process has no simultaneous events and restarts identically after each occurrence due to the memoryless property of the underlying distribution. Key properties of the Poisson process include stationary increments, meaning the distribution of N(t + s) - N(t) depends only on s and not on t, and independent increments across non-overlapping intervals. The number of events up to time t, N(t), has the P(N(t) = n) = \frac{(\lambda t)^n e^{-\lambda t}}{n!}, \quad n = 0, 1, 2, \dots which establishes the direct link to the for event counts. Additionally, the interarrival times between successive events are independent and identically distributed as random variables with rate \lambda, implying an expected interarrival time of $1/\lambda. These features make the process suitable for modeling systems where events are rare and uncorrelated, such as or traffic incidents. There are two primary types of Poisson processes: the homogeneous Poisson process, characterized by a constant rate \lambda, and the non-homogeneous Poisson process, where the rate varies with time as \lambda(t), allowing the expected number of events in an interval (t, t + s] to be \int_t^{t+s} \lambda(u) \, du. The homogeneous case assumes uniformity over time, while the non-homogeneous variant accommodates varying intensities, such as seasonal fluctuations. In applications, the homogeneous Poisson process models steady-state arrivals in networks, like packet transmissions, and the non-homogeneous form is used in to track failure rates in repairable systems over time. The marginal distribution of the number of events in fixed intervals remains , providing a probabilistic foundation for count-based analyses.

Poisson regression

Poisson regression is a type of (GLM) designed for analyzing count data, where the response variable represents the number of events occurring in a fixed interval of time or space and is assumed to follow a . Introduced as part of the GLM framework, it allows the expected count μ_i for the i-th observation to be modeled as a function of predictor variables through a log-link , ensuring that predicted means are positive. The model assumes equidispersion, meaning the of the response equals its conditional mean, which aligns with the properties of the . The core model equation is given by \log(\mu_i) = \mathbf{X}_i \boldsymbol{\beta}, where μ_i is the expected count for the i-th observation, \mathbf{X}_i is the vector of predictors (including an intercept), and \boldsymbol{\beta} is the vector of regression coefficients. This formulation implies that the expected count is μ_i = \exp(\mathbf{X}_i \boldsymbol{\beta}), and under the equidispersion assumption, the variance is also μ_i. Parameters are estimated via maximum likelihood, which maximizes the log-likelihood function \ell(\boldsymbol{\beta}) = \sum_{i=1}^n \left[ y_i \log(\lambda_i) - \lambda_i - \log(y_i!) \right], with λ_i = \exp(\mathbf{X}_i \boldsymbol{\beta}); however, no closed-form solution exists, so iterative methods like iteratively reweighted least squares are employed. In practice, real-world count data often exhibit overdispersion, where the variance exceeds the mean, violating the equidispersion assumption and leading to underestimated standard errors in standard Poisson models. To address this, quasi-Poisson regression incorporates a dispersion parameter φ > 1 to scale the variance as φ μ_i, while maintaining the same mean structure and using quasi-likelihood estimation. Alternatively, negative binomial regression models the variance as μ_i + α μ_i^2 (with dispersion parameter α > 0), providing a more flexible distribution for overdispersed counts and enabling full likelihood-based inference. The choice between quasi-Poisson and negative binomial depends on the variance-mean relationship: quasi-Poisson assumes a linear scaling, suitable for moderate overdispersion, whereas negative binomial captures quadratic variance, often preferred for highly clustered data. Poisson regression finds wide application in fields requiring count modeling, such as for estimating disease incidence rates and relative risks across covariate strata, as seen in analyses of cancer data where it accounts for interactions and nonlinear effects. In , it is used to model rates, predicting the frequency of events like traffic incidents based on factors such as road conditions or driver characteristics. Model diagnostics include goodness-of-fit tests, particularly the deviance test, which assesses whether the fitted model adequately captures the data by comparing the deviance statistic D = -2 \ell(\hat{\boldsymbol{\beta}}) to a distribution with n - p , where n is the sample size and p the number of parameters. A non-significant (e.g., p > 0.05) indicates good fit, while can be detected if the deviance exceeds expectations.

Physics and Mechanics

Poisson's ratio

Poisson's ratio, denoted by \nu, is a fundamental measure of a material's elastic behavior, defined as the negative ratio of transverse strain to axial strain under uniaxial stress: \nu = -\frac{\epsilon_{\text{transverse}}}{\epsilon_{\text{axial}}}, where the negative sign accounts for the typical contraction in the transverse direction when the material is extended axially. This property was introduced by the mathematician and physicist in his 1829 memoir on the elasticity of solids, where he derived it theoretically from molecular interaction hypotheses, predicting a value of \nu = 1/4 for isotropic materials based on contemporary experiments with wires. For most stable, isotropic, linear elastic materials, thermodynamic constraints limit \nu to the range -1 < \nu < 0.5, with typical values falling between 0.2 and 0.5; metals such as and aluminum exhibit \nu \approx 0.3, while rubber approaches \nu \approx 0.5 due to near-incompressibility. Certain engineered auxetic materials, however, display negative values, such as \nu = -0.7 in re-entrant polymer foams, causing lateral expansion under axial tension and enhancing properties like . In elasticity theory and engineering design, informs the prediction of deformation in structures like beams and components, where it influences anticlastic and concentrations; it relates to other elastic moduli via \nu = \frac{3K - 2G}{6K + 2G}, with K as the and G as the , highlighting trade-offs in incompressibility and resistance. In , it connects to the formulation of for displacement fields in elastic media.

Poisson bracket

In and , the is a fundamental defined on the space of smooth functions over the of a . It was introduced by the French mathematician in 1809 during his investigations into the variation of arbitrary constants in problems of dynamics, particularly in the context of . This operation plays a central role in by encoding the symplectic structure of and facilitating the description of and symmetries. For two smooth functions f and g on the with (q_1, \dots, q_n, p_1, \dots, p_n), where q_i are generalized positions and p_i are conjugate momenta, the is defined as \{f, g\} = \sum_{i=1}^n \left( \frac{\partial f}{\partial q_i} \frac{\partial g}{\partial p_i} - \frac{\partial f}{\partial p_i} \frac{\partial g}{\partial q_i} \right). This expression arises naturally from the symplectic form on and is under transformations, preserving the underlying geometric structure. The Poisson bracket exhibits several key algebraic properties that make it a Lie bracket on the algebra of functions: it is bilinear, meaning \{\alpha f + \beta g, h\} = \alpha \{f, h\} + \beta \{g, h\} and similarly for the second argument; it is antisymmetric, with \{f, g\} = -\{g, f\}; and it satisfies the Jacobi identity, \{f, \{g, h\}\} + \{g, \{h, f\}\} + \{h, \{f, g\}\} = 0. Additionally, it obeys the Leibniz rule, \{f, gh\} = g \{f, h\} + h \{f, g\}, reflecting its derivation-like behavior. These properties ensure that the Poisson bracket defines a Lie algebra structure, essential for analyzing integrability and symmetries in mechanical systems. In Hamiltonian mechanics, the Poisson bracket generates the time evolution of any function f via Hamilton's equations: \frac{df}{dt} = \{f, H\} + \frac{\partial f}{\partial t}, where H is the Hamiltonian function. If \frac{\partial f}{\partial t} = 0 and \{f, H\} = 0, then f is a constant of the motion. This framework extends to broader applications in symplectic geometry, where the Poisson bracket defines the Poisson manifold structure underlying Hamiltonian systems. It also serves as a classical precursor to quantum mechanics, where the commutator [ \hat{f}, \hat{g} ] / i \hbar replaces the Poisson bracket \{f, g\} in the quantization process, establishing a direct correspondence between classical and quantum observables.

Poisson's equation

is a fundamental in , describing the relationship between a and its source distribution in various physical fields. It was derived by the mathematician and physicist in 1812, building on the work of Laplace and Lagrange in scalar potential formulations for gravitational and electrostatic problems. In , takes the form \nabla^2 \phi = -\frac{\rho}{\varepsilon_0}, where \phi is the , \rho is the , \varepsilon_0 is the , and \nabla^2 is the Laplacian . This equation arises from combining with the definition of the as the negative of the potential. In Newtonian , the analogous form is \nabla^2 \phi = 4\pi G \rho, where \phi is now the , \rho is the mass density, and G is the ; this follows from the form of Newton's law of gravitation. When the source term vanishes (\rho = 0), the equation reduces to , \nabla^2 \phi = 0, which governs source-free regions. Solutions to can be obtained using the approach, which transforms the into an . The G(\mathbf{r}, \mathbf{r}') satisfies \nabla^2 G = -\delta(\mathbf{r} - \mathbf{r}') with appropriate boundary conditions, such as vanishing at in unbounded space. For in three dimensions, the fundamental solution is G(\mathbf{r}, \mathbf{r}') = \frac{1}{4\pi |\mathbf{r} - \mathbf{r}'|}, leading to the integral form \phi(\mathbf{r}) = \frac{1}{4\pi \varepsilon_0} \int \frac{\rho(\mathbf{r}')}{|\mathbf{r} - \mathbf{r}'|} \, dV'. This integral represents the superposition of contributions from all source points, generalizing for continuous charge distributions. For a point charge q at the origin, it recovers \phi(\mathbf{r}) = \frac{q}{4\pi \varepsilon_0 r}, the Coulomb potential. The gravitational case follows similarly, with G = -1 replaced by the appropriate constant. Poisson's equation finds broad applications across physics. In electrodynamics, it determines the electrostatic potential in charge distributions, forming the basis for solving boundary-value problems in dielectrics and conductors. In , a pressure Poisson equation emerges in the incompressible Navier-Stokes equations, obtained by taking the of the momentum equation and applying mass conservation, which enforces the divergence-free velocity field. In , it appears in the Hartree-Fock method for approximating the many-electron , where the self-consistent potential satisfies a Poisson equation sourced by the .

Other Uses

Poisson (crater)

Poisson is a lunar located on the in the southern highlands, centered at 30.34° S and 10.56° E . It has a of 41.4 and lies to the east of the crater Aliacensis and to the northwest of Gemma Frisius. The crater's rim is eroded and irregular, with overlaps from adjacent formations along its western and southern sides, and satellite craters such as Poisson Z attached to the northwest rim and Poisson A to the south. The interior floor of Poisson is relatively flat and covered by darker material, indicative of resurfacing by basaltic lava flows during the period. Low ridges cross the floor, likely resulting from tectonic compression or volcanic processes, while possible remnants of additional lava flows contribute to its smooth appearance. The crater's blanket extends outward, overlapping the western portion of the nearby Aliacensis crater. Due to its position on the Moon's near side, Poisson is visible from , particularly under conditions of favorable . It has been cataloged in comprehensive global lunar crater databases as part of efforts to map impact features larger than 1–2 km in diameter.) The crater was named by the in 1935 after (1781–1840), the French mathematician renowned for contributions to , , and . This naming honors his scientific legacy, as part of a broader tradition of commemorating notable scientists through lunar features. The designation appears in the authoritative compilation Named Lunar Formations by Mary A. Blagg and Karl Müller. High-resolution imagery of Poisson and its surroundings has been captured by NASA's (LRO) since 2009, enabling detailed analysis of its morphology, composition, and geological through the Lunar Reconnaissance Orbiter Camera (LROC). While no Apollo missions landed in this region, orbital from Apollo flights provided early views, supplemented by modern that reveal the crater's basaltic and structural details.

Poisson (software)

PoissonRecon is an open-source C++ software library designed for from oriented point clouds by solving a using adaptive finite element methods. It formulates the reconstruction problem as an (PDE), specifically a Poisson system, to generate watertight meshes that faithfully represent the input geometry while handling noise and incompleteness in the data. Developed primarily for and scientific visualization, the library employs multigrid solvers to efficiently handle the resulting linear systems, making it suitable for high-resolution tasks. Key features include support for 3D point clouds with oriented normals, adaptive octree-based meshing for efficient discretization in 2D and 3D domains, and configurable parameters such as degree (default linear) and boundary conditions ( by default). The library enables for large datasets and outputs formats like PLY for meshes, for grids, and OFF for octrees, facilitating integration into visualization pipelines. Applications span in and rendering, as well as extensions to image processing, such as seamless blending in panoramas via screened Poisson solving. For instance, it has been used to reconstruct models like the eagle statue from scans, achieving smooth surfaces with minimal artifacts. Originally released in the mid-2000s by researchers at and , PoissonRecon stems from foundational work on Poisson-based published in 2006, with significant updates through the 2010s incorporating screened variants and envelope constraints. It has been integrated into broader toolkits like the Point Cloud Library (PCL) and Open3D for enhanced functionality in processing workflows. Usage examples include academic research in and industrial applications in 3D printing preparation, where it outperforms greedy projection methods in handling sparse or noisy inputs. While effective for linear elliptic problems like the , the library is primarily tuned for tasks and may require extensions from other frameworks, such as deal.II or FEniCS, for nonlinear PDE variants or custom material properties in simulations like . It assumes oriented input data, potentially limiting direct applicability to unoriented point sets without preprocessing.

French word for fish

In , "poisson" is a masculine denoting a , typically referring to aquatic vertebrates with gills and fins, such as or . The word's traces back to "peis" or "pois," derived directly from the Latin "piscis," meaning "fish," with early attestations around 980 AD in forms like "pescion." The plural form is "poissons," used for multiple , as in "les poissons rouges" for . The term features prominently in , where dishes emphasize fresh, seasonal preparations; examples include "poisson à la bordelaise," a of white with shallots, white , and breadcrumbs, or "poisson meunière," pan-fried in with and . In , the zodiac sign is translated as "les Poissons," symbolizing and adaptability for those born between February 19 and March 20. Idioms like "ni chair ni poisson" describe something or someone indecisive or indefinable, literally meaning "neither flesh nor ," originating from medieval dietary distinctions between meat and during religious fasts. Culturally, fish hold symbolic value in French literature and art, often representing abundance, transformation, or tranquility; for instance, Henri Matisse's 1912 painting Goldfish uses the motif to evoke serene mindfulness amid life's chaos. In heraldry, fish appear in coats of arms to signify fishing heritage or virtues like temperance, as seen in the arms of coastal towns like Cassis, where paired fish highlight maritime importance. As of 2021, France's annual per capita fish consumption is approximately 33.6 kilograms, reflecting a strong culinary tradition; in 2022, over 8 billion euros were spent yearly on seafood. Linguistically, "poissonnier" refers to a fishmonger or the fish preparation station in a professional kitchen, while "poissonnerie" denotes a fish shop. The word has near-homophones like "poison" (poison), distinguished by pronunciation—"poisson" as /pwa.sɔ̃/ with a clear 's' sound, versus /pwa.zɔ̃/ for the toxin—leading to common learner mix-ups but no true homophones in standard French. Surnames like Poisson often originate from occupational ties to fishing or fish selling.

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