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mathematics, an adjoint bundle is a vector bundle naturally associated with any smooth principal bundle. The fibers of the adjoint bundle carry a Lie algebra
Adjoint_bundle
with any tensorial forms on P {\displaystyle P} of adjoint type. Maurer–Cartan form Adjoint bundle S. Kobayashi, K. Nomizu. Foundations of Differential
Lie algebra–valued differential form
Lie_algebra–valued_differential_form
Study of vector bundles, principal bundles, and fibre bundles
The Lie algebra adjoint bundle is usually denoted ad ( P ) {\displaystyle \operatorname {ad} (P)} , and the Lie group adjoint bundle by Ad ( P ) {\displaystyle
Gauge_theory_(mathematics)
Mathematical term
In mathematics, the adjoint representation (or adjoint action) of a Lie group G is a way of representing the elements of the group as linear transformations
Adjoint_representation
Concept in mathematics
section of the vertical bundle V of P. Hence it is basic and so is determined by a 1-form on M with values in the adjoint bundle g P := P × G g . {\displaystyle
Connection_(principal_bundle)
Partial differential equations whose solutions are instantons
bundle. This connection has a curvature form F A {\displaystyle F_{A}} , which is a two-form on X {\displaystyle X} with values in the adjoint bundle
Yang–Mills_equations
Topics referred to by the same term
(mathematics), a connection over a principal bundle G with a section (the Higgs field) of the associated adjoint bundle Monopole, the first term in a multipole
Monopole
Defines a notion of parallel transport on a bundle
capital A adjoint bundle Ad ( F ( E ) ) {\displaystyle \operatorname {Ad} ({\mathcal {F}}(E))} of the frame bundle of the vector bundle E {\displaystyle
Connection_(vector_bundle)
Typically linear operator defined in terms of differentiation of functions
self-adjoint operator is an operator equal to its own (formal) adjoint. If Ω is a domain in Rn, and P a differential operator on Ω, then the adjoint of
Differential_operator
Second-rank tensor in quantum chromodynamics
field on the spacetime with values in the adjoint bundle of the chromodynamical SU(3) gauge group (see vector bundle for necessary definitions). Throughout
Gluon_field_strength_tensor
Yang–Mills coupled to a Higgs field
connection, and a Higgs field, given by a section of a vector bundle (specifically, the adjoint bundle). These equations are D A ∗ F A + ∗ [ Φ , D A Φ ] = 0
Yang–Mills–Higgs_equations
Equations describing magnetic monopoles
{\displaystyle G} -bundle over a 3-manifold M {\displaystyle M} , Φ {\displaystyle \Phi } is a section of the corresponding adjoint bundle, d A {\displaystyle
Bogomolny_equations
{C} )} there is still a natural associated vector bundle to P {\displaystyle P} , the adjoint bundle ad P {\displaystyle \operatorname {ad} P} , with
Stable_principal_bundle
Relationship between two functors abstracting many common constructions
this relationship are known as adjoint functors, one being the left adjoint and the other the right adjoint. Pairs of adjoint functors are ubiquitous in mathematics
Adjoint_functors
mathematics, a monopole is a connection over a principal bundle G with a section of the associated adjoint bundle. Physically, such a monopole can be interpreted
Monopole_(mathematics)
Structure group sub-bundle on a tangent frame bundle
difference of two adapted connections is a 1-form on M with values in the adjoint bundle AdQ. That is to say, the space AQ of adapted connections is an affine
G-structure_on_a_manifold
Special type of principal bundle
Unlike the associated vector bundle, a complex plane bundle, the adjoint vector bundle is a orientable real vector bundle of third rank. Also since SU
Principal_SU(2)-bundle
Concept in topology (mathematics)
Lie group bundle over the same base space whose Lie algebra bundle is isomorphic to the given Lie algebra bundle. Algebra bundle Adjoint bundle A. Weinstein
Lie_algebra_bundle
Euclidean space without distance and angles
1-forms, where ad ( P ) {\displaystyle {\text{ad}}(P)} is the associated adjoint bundle. For any non-empty subset X of an affine space A, there is a smallest
Affine_space
System of partial differential equations used in Higgs field theory
{\displaystyle {\text{ad}}P^{\mathbb {C} }} is the complexification of the adjoint bundle of P {\displaystyle P} , with fibre given by the complexification g
Hitchin's_equations
Special type of principal bundle
Principal bundles also have an adjoint vector bundle, which is trivial for principal U ( 1 ) {\displaystyle \operatorname {U} (1)} -bundles. By definition
Principal_U(1)-bundle
Relates 2 second-order elliptic operators on a manifold with the same principal symbol
are implemented for G-invariant self-adjoint operators between vector bundles associated to some principal G-bundle, although the precise conditions under
Weitzenböck_identity
Mathematics concept
vertical bundle and the horizontal bundle are vector bundles associated to a smooth fiber bundle. More precisely, given a smooth fiber bundle π : E → B
Vertical and horizontal bundles
Vertical_and_horizontal_bundles
Group of gauge symmetries in Yang–Mills theory
Yang–Mills gauge theory of principal connections on a principal bundle. Given a principal bundle P → X {\displaystyle P\to X} with a structure Lie group G {\displaystyle
Gauge_group_(mathematics)
Infinitesimal version of Lie groupoid
on P {\displaystyle P} , its isotropy Lie algebra bundle is isomorphic to the adjoint vector bundle P × G g {\displaystyle P\times _{G}{\mathfrak {g}}}
Lie_algebroid
Gradient flow of the Yang–Mills–Higgs action functional
\operatorname {Ad} (E):=E\times _{G}{\mathfrak {g}}\twoheadrightarrow B} be its adjoint bundle. A = Ω Ad 1 ( E , g ) {\displaystyle {\mathcal {A}}=\Omega _{\operatorname
Yang–Mills–Higgs_flow
Matrix operation which flips a matrix over its diagonal
resulting in an isomorphism between the transpose and adjoint of u. The matrix of the adjoint of a map is the transposed matrix only if the bases are
Transpose
MR 1207013. Fujita, Takao (1987), "On polarized manifolds whose adjoint bundles are not semipositive", Algebraic geometry, Sendai, 1985, Adv. Stud
Fujita_conjecture
Gradient flow of the Yang–Mills action functional
\operatorname {Ad} (E):=E\times _{G}{\mathfrak {g}}\twoheadrightarrow B} be its adjoint bundle. A = Ω Ad 1 ( E , g ) {\displaystyle {\mathcal {A}}=\Omega _{\operatorname
Yang–Mills_flow
Formula for spinors
is the self-dual part of the curvature of A. The asterisks denote the adjoint of the quantity and the brackets ⟨ , ⟩ {\displaystyle \langle ,\rangle
Lichnerowicz_formula
Elliptic differential operators in geometry mathematics
sections of E, and T*M is the cotangent bundle of M. It is possible to take the L 2 {\displaystyle L^{2}} -adjoint of ∇ {\displaystyle \nabla } , giving
Laplace operators in differential geometry
Laplace_operators_in_differential_geometry
Concept in differential geometry
holonomy of connections in vector bundles, holonomy of Cartan connections, and holonomy of connections in principal bundles. In each of these cases, the holonomy
Holonomy
Process in mathematics
linear operator, and is known as the transpose or composition operator. Its adjoint is the push-forward, or, in the context of functional analysis, the transfer
Pullback
Gradient flow of the Seiberg–Witten action functional
_{\operatorname {U} (1)}\mathbb {C} } using the balanced product and with trivial adjoint bundle Ad Fr U ( L ) ≅ End _ ( L ) ≅ C _ {\displaystyle \operatorname {Ad}
Seiberg–Witten_flow
of adjoint type. The "difference" of two connection forms is a tensorial form. Given P and ρ as above one can construct the associated vector bundle E
Vector-valued differential form
Vector-valued_differential_form
Mathematical result in differential geometry
the operators of the elliptic complex and their adjoints, restricted to the sum of the even bundles. If the manifold is allowed to have boundary, then
Atiyah–Singer_index_theorem
Quotient of special unitary group by its center
of PU. The adjoint action of the infinite projective unitary group is useful in geometric definitions of twisted K-theory. Here the adjoint action of the
Projective_unitary_group
category (while the fundamental groupoid is a left adjoint to the inclusion of Gprd, the core is a right adjoint) Brown, Ronald (2006). Topology and Groupoids
Fundamental_groupoid
Math/physics concept
right action on T(FGE) with the adjoint representation of G. Conversely, a principal G-connection ω in a principal G-bundle P→M gives rise to a collection
Connection_form
Concept in mathematical theory of categories
reflective in B when the inclusion functor from A to B has a left adjoint. This adjoint is sometimes called a reflector, or localization. Dually, A is said
Reflective_subcategory
Topics referred to by the same term
of digits Normal operator, an operator that commutes with its Hermitian adjoint Normal order of an arithmetic function, a type of asymptotic behavior useful
Normal
Moduli space of the Yang–Mills equations
{\displaystyle \operatorname {Ad} (P):=P\times _{G}{\mathfrak {g}}} be the adjoint bundle, then the Yang–Mills equations as well as the (anti) self-dual Yang–Mills
Yang–Mills_moduli_space
Topological quantum field theory
flat G-principal bundle P on M there exists a unique homomorphism, called the Chern–Weil homomorphism, from the algebra of G-adjoint invariant polynomials
Chern–Simons_theory
Functor type
representable if and only if it has a left adjoint. The categorical notions of universal morphisms and adjoint functors can both be expressed using representable
Representable_functor
Describes a periodicity in the homotopy groups of classical groups
{\displaystyle \Omega } is the loop space functor, right adjoint to suspension and left adjoint to the classifying space construction. Bott periodicity
Bott_periodicity_theorem
given magnitude Einstein–Hermitian vector bundle Deformed Hermitian Yang–Mills equation Hermitian adjoint Hermitian connection, the unique connection
List of things named after Charles Hermite
List_of_things_named_after_Charles_Hermite
\operatorname {Ad} (E):=E\times _{G}{\mathfrak {g}}\twoheadrightarrow B} be its adjoint bundle. Ω Ad 1 ( E , g ) ≅ Ω 1 ( B , Ad ( E ) ) {\displaystyle \Omega _{\operatorname
F-Yang–Mills_equations
Mapping between categories
be proved by realizing that it is the right-adjoint to the diagonal functor and invoking the Freyd adjoint functor theorem. This requires a suitable version
Functor
Generalization of a vector bundle
In algebraic geometry, a cone is a generalization of a vector bundle. Specifically, given a scheme X, the relative Spec C = Spec X R {\displaystyle C=\operatorname
Cone_(algebraic_geometry)
Differential geometry construct on fiber bundles
on any smooth fiber bundle. In particular, it does not rely on the possible vector bundle structure of the underlying fiber bundle, but nevertheless, linear
Ehresmann_connection
\operatorname {Ad} (E):=E\times _{G}{\mathfrak {g}}\twoheadrightarrow B} be its adjoint bundle. Ω Ad 1 ( E , g ) ≅ Ω 1 ( B , Ad ( E ) ) {\displaystyle \Omega _{\operatorname
Bi-Yang–Mills_equations
topology and homological algebra, tensor product and the Hom functor are adjoint; however, they might not always lift to an exact sequence. This leads to
Lift_(mathematics)
Concept in differential geometry
{\displaystyle \operatorname {Ad} (E):=E\times _{G}{\mathfrak {g}}} be its adjoint bundle. A = Ω Ad 1 ( E , g ) {\displaystyle {\mathcal {A}}=\Omega _{\operatorname
Stable_Yang–Mills–Higgs_pair
Universal construction in multilinear algebra
tensor product. It is the free algebra on V, in the sense of being left adjoint to the forgetful functor from algebras to vector spaces: it is the "most
Tensor_algebra
Theorem in algebraic geometry
varieties, proved by Jean-Pierre Serre. The basic version applies to vector bundles on a smooth projective variety, but Alexander Grothendieck found wide generalizations
Serre_duality
Operator generalizing the Laplacian in differential geometry
consequence, the Laplace–Beltrami operator is negative and formally self-adjoint, meaning that for compactly supported functions f {\displaystyle f} and
Laplace–Beltrami_operator
Concept in differential geometry
{\displaystyle \operatorname {Ad} (E):=E\times _{G}{\mathfrak {g}}} be its adjoint bundle. A = Ω Ad 1 ( E , g ) {\displaystyle {\mathcal {A}}=\Omega _{\operatorname
Stable_Yang–Mills_connection
First-order differential linear operator on spinor bundle, whose square is the Laplacian
space of smooth, square-integrable functions. It can be extended to a self-adjoint operator on that domain. The square, in this case, is not the Laplacian
Dirac_operator
G} , its quotient by the diagonal G {\displaystyle G} action is the adjoint bundle P × G g {\displaystyle P\times _{G}{\mathfrak {g}}} . In conclusion
Atiyah_algebroid
Most general completion of a commutative square given two morphisms with same codomain
maps) X ×B E is a fiber bundle over X called the pullback bundle. The associated commutative diagram is a morphism of fiber bundles. A special case is the
Pullback_(category_theory)
Branch of mathematics
K-theory is, roughly speaking, the study of a ring generated by vector bundles over a topological space or scheme. In algebraic topology, it is a cohomology
K-theory
Group of unitary complex matrices with determinant of 1
Tr(T_{a}T_{b})={\frac {1}{2}}\delta _{ab}.} In the (n2 − 1)-dimensional adjoint representation, the generators are represented by (n2 − 1) × (n2 − 1) matrices
Special_unitary_group
Operation that pairs a left and a right R-module into an abelian group
_{S}P=M\otimes _{R}(N\otimes _{S}P)} as abelian group. The general form of adjoint relation of tensor products says: if R is not necessarily commutative,
Tensor_product_of_modules
Relativistic quantum mechanical wave equation
}^{a}} , formally the connection on the principal bundle, which necessarily transforms in the adjoint representation of the gauge group. The covariant
Dirac_equation
Type of integrable system
system is a partial compactification of the cotangent bundle to the moduli space of stable G-bundles for some reductive group G, on some compact algebraic
Hitchin_system
Operation on fibered manifolds
acts on by the adjoint representation. There is the canonical imbedding of C to the quotient bundle TP/G which also is called the bundle of principal connections
Connection_(fibred_manifold)
Superconductivity theory
{Re} \langle D\psi ,\psi \rangle } where D ∗ {\displaystyle D^{*}} is the adjoint of D {\displaystyle D} , analogous to the codifferential δ = d ∗ {\displaystyle
Ginzburg–Landau_theory
Branch of mathematics
product X ∧ Y {\displaystyle X\wedge Y} which is characterized by the adjoint relation Map ( X ∧ Y , Z ) = Map ( X , Map ( Y , Z ) ) {\displaystyle
Homotopy_theory
Cohomology theory for Lie algebras
here. When M = g {\displaystyle M={\mathfrak {g}}} , the action is the adjoint action, x ⋅ y = [ x , y ] = ad ( x ) y {\displaystyle x\cdot y=[x,y]={\text{ad}}(x)y}
Lie_algebra_cohomology
Mathematical theory
points in C [ g ] {\displaystyle \mathbb {C} [{\mathfrak {g}}]} under the adjoint action of G; that is, the subalgebra consisting of all polynomials f such
Chern–Weil_homomorphism
symmetric bilinear form. Compatibility means that it is invariant under the adjoint representation. Examples of such are semisimple Lie algebras, such as su(n)
Quadratic_Lie_algebra
Universal construction of a complex Lie group from a real Lie group
iX, where u is a unitary operator in the compact group and X is a skew-adjoint operator in its Lie algebra. In this case the complexification is a complex
Complexification_(Lie_group)
Intrinsic geometric structures in mathematics
trivial bundle, in particular to a section of the original sub-bundle, although the resulting section might no longer be a section of the sub-bundle. This
Riemannian connection on a surface
Riemannian_connection_on_a_surface
involves a Hilbert space, an algebra of operators on it and an unbounded self-adjoint operator, endowed with supplemental structures. It was conceived by Alain
Spectral_triple
Concept in category theory
objects such as vector bundles can be defined. As an example, for each topological space there is the category of vector bundles on the space, and for
Fibred_category
Correspondence between topics in Lie theory
category of finite-dimensional (real) Lie-algebras. This functor has a left adjoint functor Γ {\displaystyle \Gamma } from (finite dimensional) Lie algebras
Lie group–Lie algebra correspondence
Lie_group–Lie_algebra_correspondence
Exterior algebraic map taking tensors from p forms to n-p forms
cotangent bundle of a pseudo-Riemannian manifold, and hence to differential k-forms. This allows the definition of the codifferential as the Hodge adjoint of
Hodge_star_operator
Mathematical concept
pullback of forms along the right-translation in the group and Ad(h) is the adjoint action on the Lie algebra. If X is a left-invariant vector field on G,
Maurer–Cartan_form
Manifold with Riemannian, complex and symplectic structure
Lefschetz operator L := ω ∧ − {\displaystyle L:=\omega \wedge -} and its adjoint, the contraction operator Λ = L ∗ {\displaystyle \Lambda =L^{*}} . The
Kähler_manifold
(X)\colon {\mathfrak {g}}\to {\mathfrak {g}},X\in {\mathfrak {g}}} in its adjoint representation is hyperbolic, i.e., it has only real eigenvalues. Let G
Solvmanifold
operators on a Kähler manifold relating the Dolbeault operators and their adjoints, contraction and wedge operators of the Kähler form, and the Laplacians
Kähler_identities
Branch of mathematics
Hilbert space H {\displaystyle H} , together with a usually unbounded self-adjoint operator D {\displaystyle D} , such that ( 1 + D 2 ) − 1 / 2 {\displaystyle
Noncommutative_geometry
entanglement spinor, spinor group, spinor bundle Dirac sea Spin foam Poincaré group gamma matrices Dirac adjoint Wigner's classification anyon Copenhagen
List of mathematical topics in quantum theory
List_of_mathematical_topics_in_quantum_theory
Mathematical objects that generalise the notion of Hilbert spaces
a C*-algebra A {\displaystyle A} is said to be positive if it is self-adjoint with non-negative spectrum.) An analogue to the Cauchy–Schwarz inequality
Hilbert_C*-module
Local ring in commutative algebra
simply a line bundle (viewed as a complex in degree −dim(X)); this line bundle is called the canonical bundle of X. Using the canonical bundle, Serre duality
Gorenstein_ring
Group of real 2×2 matrices with unit determinant
PSL(2, R) can be described as the unit tangent bundle of the hyperbolic plane. It is a circle bundle, and has a natural contact structure induced by
SL2(R)
Generalisation of a sheaf; a fibered category that admits effective descent
situations where isomorphic, compatible geometrical objects (such as vector bundles on topological spaces) can be "glued together" within a restriction of
Stack_(mathematics)
Mathematical operation on vector spaces
(U,\mathrm {Hom} (V,W)).} This is an example of adjoint functors: the tensor product is "left adjoint" to Hom. The tensor product of two modules A and
Tensor_product
Combination of higher category theory with Chern–Weil theory
\colon \mathbf {H} \rightarrow \infty \operatorname {Grpd} } has a right adjoint Disc : ∞ Grpd → H {\displaystyle \operatorname {Disc} \colon \infty \operatorname
∞-Chern–Weil_theory
Real square matrix whose columns and rows are orthogonal unit vectors
(with inverse Q−1 = QT), unitary (Q−1 = Q∗), where Q∗ is the Hermitian adjoint (conjugate transpose) of Q, and therefore normal (Q∗Q = QQ∗) over the real
Orthogonal_matrix
{\displaystyle G} by left multiplication, right multiplication or conjugation; the adjoint action of G {\displaystyle G} on its Lie algebra g {\displaystyle {\mathfrak
Lie_group_action
Description of how spaces intersect in mathematics
[{\mathfrak {g}},e]} is the tangent space at e {\displaystyle e} to the adjoint orbit A d ( G ) e {\displaystyle {\rm {{Ad}(G)e}}} and so the affine space
Transversality
Generalisations of Serre duality in mathematics
'local' theory. The historical roots of the theory lie in the idea of the adjoint linear system of a linear system of divisors in classical algebraic geometry
Coherent_duality
Expression that may be integrated over a region
\Omega ^{k}(M)\rightarrow \Omega ^{k-1}(M)} , which has degree −1 and is adjoint to the exterior differential d. On a pseudo-Riemannian manifold, 1-forms
Differential_form
Application of Lagrangian mechanics to field theories
function on a fiber bundle, wherein the Euler–Lagrange equations can be interpreted as specifying the geodesics on the fiber bundle, leading to topics
Lagrangian_(field_theory)
Generalization of affine connections
concept of a principal connection, in which the geometry of the principal bundle is tied to the geometry of the base manifold using a solder form. Cartan
Cartan_connection
Recipe for constructing a quantum analog of a classical physical theory
an attempt is made to associate a quantum-mechanical observable (a self-adjoint operator on a Hilbert space) with a real-valued function on classical phase
Geometric_quantization
Concept in mathematics
from the direct sum of the two modules g(A) and ν(A) and should be called adjoint representation. Note however that in the more general case where ρ does
Representation_up_to_homotopy
Smooth manifold with an inner product on each tangent space
left-invariant Riemannian metric can be computed explicitly in terms of ge, the adjoint representation of G, and the Lie algebra associated to G. These formulas
Riemannian_manifold
Projective analogue of the spectrum of a ring
This situation is to be contrasted with the fact that the Spec functor is adjoint to the global sections functor in the category of locally ringed spaces
Proj_construction
ADJOINT BUNDLE
ADJOINT BUNDLE
Surname or Lastname
English
English : from Middle English pa(c)k ‘pack’, ‘bundle’ + the Anglo-Norman French pejorative suffix -ard, hence a derogatory occupational name for a peddler.English : pejorative derivative of the Middle English personal name Pack.English : from a Norman personal name, Pachard, Baghard, composed of the Germanic elements pac, bag ‘fight’ + hard ‘hardy’, ‘brave’, ‘strong’.Probably an Americanized spelling of German Packert, Päckert, from Germanic personal names formed with a word meaning ‘battle’ or ‘to fight’; or a variant of Packer 2 (with excrescent -t).
Boy/Male
Arabic, Australian, Muslim, Sindhi
Skillful; Adroit
Female
Irish
Variant spelling of Irish Éadan, ÉADAOIN means "face" or perhaps "against" or "opposite."
Surname or Lastname
English (southwest)
English (southwest) : occupational name for a digger of ditches or a builder of dikes, or a topographic name for someone who lived by a ditch or dike, from an agent derivative of Middle English diche, dike (see Dyke).English : regional name from an area of East Sussex, near Hellingly, called ‘the Dicker’ (hence also the hamlets of Upper and Lower Dicker), from Middle English dyker unit of ten (Latin decuria, from decem ‘ten’); the reason for the place being so named is not clear. It has been suggested that the reference is to a bundle of iron rods, in which sense dicras appears in Domesday Book. Such a bundle could have been the rent for property in this iron-working area. Surname forms such as atte dicker occur in the surrounding region in the 13th and 14th centuries.German and Jewish (Ashkenazic) : variant of Dick 2, from an inflected form.North German : variant of Low German Dieker, a topographic or an occupational name for someone who lived or worked at a dike (see Dieck).Americanized spelling of French Decaire.
Girl/Female
British, English, Latin
Dyer; Skillful; Dexterous; Adroit; Right-handed
Male
English
Anglicized form of Irish Gaelic Comhghall, COWAL means "joint pledge."
Surname or Lastname
English
English : from Old French balon ‘bundle’, ‘roll’, ‘pack’, hence a nickname for a small, rotund man or possibly a metonymic occupational name for a carrier of goods and merchandise.French (Bâlon) : generally regarded as a habitational name from Baalons in the Ardennes, it may however simply be from balon ‘ball’, ‘roll’ (see 1) or a derivative of Bal.
Girl/Female
Latin
Adroit; skillful.
Boy/Male
Muslim/Islamic
Skillful Adroit
Surname or Lastname
English
English : presumably from Old French joint ‘united’, ‘joined’. The application as a surname is unclear.
Girl/Female
Arabic, Muslim
Connection; Joint
Male
Irish
Contracted form of Irish Gaelic Comhghall, COMGAL means "joint pledge."
Girl/Female
Indian, Telugu
Love; To Joint
Boy/Male
Muslim
Skillful, Adroit (1)
Girl/Female
Biblical
To call, to anoint.
Male
Japanese
(1-å·§, 2-åŒ , 3-å·¥) Japanese name TAKUMI means 1) "adroit," 2) "artisan," or 3) "skilful."
Surname or Lastname
English (Kent)
English (Kent) : from Middle English shefe ‘sheaf’, ‘bundle’ (Old English scēaf), hence possibly a metonymic occupational name for a harvest worker, or for someone who paid or collected tithes, from the same term in the sense ‘tenth’ (or other proportion of produce paid as a tithe).Jacob Sheafe (d. 1658) was one of the founds of Boston MA. He is buried in the King’s Chapel Burying Ground there.
Biblical
to call; to anoint
Surname or Lastname
English
English : occupational nickname for a peddler, from Old French trousse ‘bundle’, ‘pack’.Ukrainian : nickname from trus ‘rabbit’, typically applied to someone thought to be a coward.
Surname or Lastname
English
English : from a pet form of Fulcher.German (also Füge) : nickname for a skillful, adroit person, from Middle High German vüege ‘skillful’, ‘fitting’ (see Fiegel).
ADJOINT BUNDLE
ADJOINT BUNDLE
Boy/Male
Gujarati, Hindu, Indian, Kannada, Malayalam, Marathi, Punjabi, Sikh
Emerald
Girl/Female
English
Divine.
Boy/Male
Hindu, Indian
King Cobra
Girl/Female
Hindu
Daughter of jambavan
Girl/Female
American, Australian, Chinese, Dutch, Finnish, French, German, Greek, Latin, Swedish
The Holy One; Black Beauty; Dark One; Very Holy Woman; Similar to Ariadne; Utterly Pure
Boy/Male
Tamil
Parnabha | பரà¯à®¨à®¾à®ªà®¾Â
Boy/Male
Tamil
To keep in mind. to point at something
Girl/Female
Biblical
The end, a pause.
Female
English
Variant spelling of English Eileen, ILEEN means "beauty, radiance."Â
Girl/Female
Tamil
th place in the Raga scale- sa re ga ma pa dha
ADJOINT BUNDLE
ADJOINT BUNDLE
ADJOINT BUNDLE
ADJOINT BUNDLE
ADJOINT BUNDLE
v. i.
To lie or be next, or in contact; to be contiguous; as, the houses adjoin.
v. t.
To provide with a joint or joints; to articulate.
a.
Joined; united; combined; concerted; as joint action.
a.
United, joined, or sharing with another or with others; not solitary in interest or action; holding in common with an associate, or with associates; acting together; as, joint heir; joint creditor; joint debtor, etc.
n.
A joining of two things or parts so as to admit of motion; an articulation, whether movable or not; a hinge; as, the knee joint; a node or joint of a stem; a ball and socket joint. See Articulation.
a.
Shared by, or affecting two or more; held in common; as, joint property; a joint bond.
v. t.
To reunite the joints of; to joint anew.
a.
Dexterous in the use of the hands or in the exercise of the mental faculties; exhibiting skill and readiness in avoiding danger or escaping difficulty; ready in invention or execution; -- applied to persons and to acts; as, an adroit mechanic, an adroit reply.
v. t.
To separate the joints; of; to divide at the joint or joints; to disjoint; to cut up into joints, as meat.
n.
The part or space included between two joints, knots, nodes, or articulations; as, a joint of cane or of a grass stem; a joint of the leg.
imp. & p. p.
of Adjoin
p. pr. & vb. n.
of Adjoin
n.
The space between the adjacent surfaces of two bodies joined and held together, as by means of cement, mortar, etc.; as, a thin joint.
n.
An adjunct; a helper.
v. i.
To join one's self.
v. i.
To fit as if by joints; to coalesce as joints do; as, the stones joint, neatly.
n.
The place or part where two things or parts are joined or united; the union of two or more smooth or even surfaces admitting of a close-fitting or junction; junction as, a joint between two pieces of timber; a joint in a pipe.
v. t.
To unite by a joint or joints; to fit together; to prepare so as to fit together; as, to joint boards.
v. t.
To join or unite to; to lie contiguous to; to be in contact with; to attach; to append.