true or false.

The default for this option is true, and so the abbreviations $\mathrm{kd\_}$ for KroneckerDelta and $\mathrm{ep\_}$ for LeviCivita are set when you load the package. Therefore, $\mathrm{kd\_}$ and KroneckerDelta can be used to perform the same operation. When abbreviations is set to false, these two abbreviations are unset. Alternatively, for these two or other Maple commands, you can set a macro to achieve the same results.

An equation with a Commutator or AntiCommutator on the left-hand side and an algebraic expression representing the result for that operation on the right-hand side; or a set, list or Matrix of them.

The operands in the (Anti)Commutator on the left-hand side of the equations are expected to be names, functions, or indexed functions, in which case the indices and functionality will be taken as parameters of the operation and expected to appear when arguments are passed to perform the operation (see examples of this in Commutator). These are used by Commutator and AntiCommutator to return results accordingly.

Tip: When setting algebra rules, use the inert forms %Commutator and %AntiCommutator instead of the active forms Commutator, AntiCommutator; this may help to prevent a premature evaluation of the Commutator or AntiCommutator.

aqua, black, blue, fuchsia, gray, green, lime, maroon, navy, olive, purple, red, silver, teal, or yellow.

When mathematicalnotation is set to true, the anticommutativecolor setting causes the Maple Standard GUI to display anticommutative variables in the selected color.

Any valid sequence of characters.

Sets the prefix of characters entering the symbols representing anticommutative variables; that is, variables $\mathrm{\θ1}$ and $\mathrm{\θ2}$ for which $\mathrm{\θ1}$ $\mathrm{\θ2}$ = $-\mathrm{\θ2}$ $\mathrm{\θ1}$. A

Note: In the context of the Physics package, the multiplication operator, * is commutative, anticommutative, or noncommutative, depending on the corresponding commutation properties of its operands (see type/commutative). Also, as soon as you set anticommutative variables in this way, you may want to solve differential equations with them (i.e. including derivative with respect to anticommutative variables), so that anticommutative integration constants will appear in the output, expressed using $\mathrm{\_lambda1},\mathrm{\_lambda2},\mathrm{...}$. See the last examples in dsolve,details.

true or false.

The default for this option is true, so that, when Physics is loaded, the Maple assuming command uses Physics:-Assume to place temporary assumptions. This makes the assuming command fully compatible with the Physics, DifferentialGeometry, DifferentialAlgebra and VectorCalculus packages. It is recommended to not change this setting. If assumingusesAssume is set to false, temporary assumptions placed by assuming are placed using the assume command, which redefines the variables receiving assumptions, so that, depending on the computation, the commands of these packages mentioned will fail in recognizing them within expressions (for example: when placing assumptions on the coordinates and computing with the spacetime metric).

true or false.

The default for this option is false, and when set to true the output corresponding to every single input (not just related to Physics) gets automatically simplified in size before being returned to the screen. This is convenient for interactive work in most situations.

A name $A$.

$A$ represents a space of quantum states, and the corresponding vectors (labeled with the same name) will be used when calling the Bracket command with a single argument. For example, $\mathrm{Bracket}\left(H\right)$ will be computed as $\mathrm{Bracket}\left(A\,H\,A\right)=⟨A\left|H\right|A⟩$.

An equation with a Bracket on the left-hand side and an algebraic expression representing the result for that bracket (scalar product) on the right-hand side.

The bracket can be of the form $⟨A|B⟩$ or $⟨A\left|H\right|B⟩$ for some Bra and Ket $A$ and $B$, and the quantum operator $H$ should have all the quantum numbers of $A$ and $B$ represented by symbols. The right-hand side is an algebraic expression depending on these symbols (see examples in Bracket). It is also possible to pass a set of bracket rules at once, as a set (by enclosing them between { }), as in $\mathrm{bracketrules}=\{...\}$. As a shortcut, it is valid to pass the right-hand side directly, without using an equation with the keyword bracketrules. These bracket rules are saved internally as procedures having the quantum numbers as parameters, and are used by Bracket when computing brackets.

Tip: when setting bracket rules, use the inert form %Bracket instead of the active form Bracket; this may help to prevent a premature evaluation of the bracket.

true or false.

The default for this option is false. When set to true, combination of powers of the same base (in products of powers or of exponentials) happens automatically, including taking care of the cases where the exponents or the base are not commutative (for example, using Glauber's formula to combine exponentials).

Any of the keywords cartesian, cylindrical or spherical, or a capital letter, or a set of them.

Aliases are set by using the alias command so that the capital letter represents the sequence of associated coordinates, such as the lowercase letters postfixed with a positive integer ranging from 1 to the dimension. For example, coordinatesystems = X sets the alias $X=\mathrm{x1},\mathrm{x2},\mathrm{x3},\mathrm{x4}$, and sets $\mathrm{x0}=\mathrm{x4}$. See also Coordinates

0 or any algebraic expression.

The default value for the cosmological constant is 0, so that the Einstein and EnergyMomentum tensors are proportional. You can set the value of this constant to any valid algebraic expression, in which case the relationship defining those two tensors includes an additional term with this constant as usual - try for instance entering Einstein[definition] or EnergyMomentum[definition].

standard, chiral, or Majorana.

Sets the representation to be used for the Dirac matrices.

Note: The representation depends on the dimension of spacetime, and for a dimension lower than 4, only the standard representation is implemented.

A list with two operands: the name of the differentialoperator and a list with the related differentiation variables, or a set or list of those two-element lists.

Sets names to be considered differential operators, i.e. operators that do not commute with the differentiation variables indicated in the second list. In this way you can use them within products entering algebraic expressions, and have them applied only to the objects appearing to their right in products by using Library:-ApplyProductsOfDifferentialOperators.

A capital letter, or a list of differentiation variables.

Sets the default differentiation variables for the d_, D_ and d'Alembertian differentiation commands. These variables are automatically set when you define the first system of coordinates. If the setting for differentiationvariables is cleared (options clear, differentiationvariables), you can still use these three differentiation commands, provided you explicitly indicate the differentiation variables as a second argument.

A positive integer greater than 1.

Sets the dimension of the spacetime manifold. When this parameter is set, all of the definitions sensitive to the dimension are reset, such as aliases set by Coordinates, the representation for the Dirac matrices, and all tensor definitions introduced by Define. The behavior of the spacetime manifold depends also on the signature, which is another of the parameters that can be set (see below). As a shortcut, you can specify both the dimension and signature in one equation, with a list on the right-hand side, as in $\mathrm{dimension}=\left[d\,s\right]$, where $d$ is the dimension and $s$ is one of `+`, `-`, representing the signature, associated with a Euclidean or Minkowski spacetime, respectively. For example, the default value when you load the Physics package is $\mathrm{dimension}=\left[4\,\mathrm{`-`}\right]$, representing a 3 + 1 Minkowski spacetime with signature (-,-,-,+).

Remark: the conventions for the dimension only affect the results of computations with objects defined by you using Define or known because they were defined automatically when Physics was loaded.

A set of Ket labels that act on one and the same Hilbert space, or a set of sets of them.

By default, all quantum operators, set as such using the keyword quantumoperators, act on the same Hilbert space, for example, position and momentum. The disjointedspaces is used to indicate sets of operators that act on disjointed Hilbert spaces. Operators acting on disjointed spaces automatically commute between themselves, and their respective basis of eigenkets can be used to construct tensor products of states. For example, hilbertspaces = {{A}, {B}} indicates that the operator A acts on one Hilbert space while B acts on another one. The Hilbert spaces thus have no particular name (as in 1, 2, 3 ...) and are instead identified by the operators that act on it. There can be one or more Hilbert spaces, and operators acting on one space can act on other spaces too, for instance as in hilbertspaces = {{A, C}, {B, C}}.

greek, lowercaselatin, lowercaselatin_ah, lowercaselatin_is, or uppercaselatin.

Sets the identifier for gauge indices in that every index found in a tensor object defined by the Define command that has the genericindices prefix as a root and is followed by a positive integer will be interpreted as a gauge index.

true or false.

The default for this option is false, and this value is automatically changed to true when the Vectors subpackage of Physics is loaded. When geometricdifferentiation is set to true, both the Physics[diff] and Physics[Vectors][diff] commands differentiate expressions taking into account the geometrical relations between curvilinear unit vectors and coordinates of different types. Note that when Physics and Physics[Vectors] are both loaded, Physics[diff] and Physics[Vectors][diff] are the same command.

A name, or a set of them.

Indicates that these names represent linear hermitian quantum operators, that is, they satisfy $U=\mathrm{Dagger}\left(U\right)$. This information is taken into account when computing, for example, the Dagger of the operator. When an operator is set to be Hermitian, it is also automatically set to be a noncommutative quantum operator (see quantumoperators below).

true or false.

The default for this option is false. When passing hideketlabel = true, the labels of Bras and Kets are automatically suppressed when displaying them. Note that the labels are not removed, only suppressed in the display. Even when this option is set to true, you can see the Ket labels of an expression by entering show (see the Examples section), which works the same way as it does in the context of CompactDisplay.

standard, arbitrary, or a list of two operands: first an algebraic expression or value representing the Lapse, then a list with three algebraic expressions representing the 3 contravariant spatial components of the Shift.

The lapseandshift value determines the values of the components of all the ThreePlusOne tensors (e.g. ExtrinsicCurvature) and so of tensorial expressions involving them (e.g. the ADMEquations). Those components are always computed first in terms of the Lapse and Shift and the space part $g_{i,j}$ of the 4D metric, then in a second step, if lapseandshift = standard, the Lapse and the Shift are replaced by their expressions in terms of the $g_{0,\mathrm{\mu }}$ part of the 4D metric, according to ${\mathbf{\alpha }}^2={\left(-g_{}^{0,0}\right)}^{-1}$ and ${\mathbf{\beta }}_j=g_{0,j}$, or if lapseandshift is passed as a list, in terms of the values indicated in that list (these values are not used to set the $g_{0,\mathrm{\mu }}$ part of the 4D metric). When lapseandshift = arbitrary, the second step is not performed and the Lapse and Shift evaluate to themselves, representing an arbitrary value for them. In the three cases, standard, arbitrary, or a list of values, the components of the ThreePlusOne tensors are computed in terms of a metric with line element ${\mathrm{ds}}^2=-{\mathit{\alpha }}^2{\mathrm{dt}}^2+{\mathit{\gamma }}_{i,j}\left({\mathrm{dx}}^i+{\mathit{\beta }}_{\phantom{}\phantom{i}}^{\phantom{}i}\mathrm{dt}\right)\left({\mathrm{dx}}^j+{\mathit{\beta }}_{\phantom{}\phantom{j}}^{\phantom{}j}\mathrm{dt}\right)$, where $\mathbf{\alpha }$ and ${\mathbf{\beta }}_{}^i$ have the Lapse and Shift values mentioned, and ${\mathbf{\gamma }}_{i,j}=g_{i,j}$ is the ThreePlusOne:-gamma3_ metric of the 3D hypersurface. This design permits working with any 4D metric set and, without changing its value, experimenting with different values of the Lapse and Shift (different values of $g_{0,\mathrm{\mu }}$) for the 3+1 decomposition of Einstein's equations. See also LapseAndShiftConditions.

galilean or nongalilean

Indicates that the LeviCivita (pseudo)tensor represents either the galilean totally antisymmetric symbol $\mathrm{\epsilon }$, whose components are all equal to 0, 1 or -1, or its generalization to curvilinear coordinates $\mathrm{{\rm E}}$ (see definition in LeviCivita).

Any name or a set of them.

Sets the fields that are massless. This information is used by the FeynmanDiagrams command when computing the propagators of vector fields entering Feynman integrals in momentum representation. For examples see FeynmanDiagrams.

true or false.

Provides a noticeable improvement in the display of expressions by using traditional mathematical notation for Physics objects. For example, vectors are displayed with an arrow on top, the vectorial differential operators (such as Nabla and Laplacian) are displayed with an upside down triangle, anti and noncommutative variables, and so all the quantum operators, are displayed in different colors, mathematical functions are displayed using textbook notation, and more. The same enhancement in the display can be obtained by using the Options dialog (go to Tools -> Options, select the Display tab, and set the Typesetting level dropdown to Extended; see also interface). To change this mathematical notation to your preferred one, see anticommutativecolor, noncommutativecolor and vectordisplay.

<keyword, line_element, Matrix, set(nonzero components)>

Indicates the spacetime metric; instead of the word metric the left-hand side can also be the metric tensor itself, as in g_[mu, nu]. The right-hand side can be a keyword, for instance any of arbitrary, Euclidean, Minkowski, Schwarzschild, Tolman or related to any of the metrics of the book on "Exact Solutions of Einstein's Field Equations" - see references at the end. To indicate a metric of the book, pass a list with three numbers, identifying the chapter, equation number and the case as found in the book, for example as in metric = [12, 12, 1].

Note: a search on the database of solutions to Einstein's equation can be launched by passing also an incomplete keyword or misspelled, so that a searchtext is performed among the keywords and comments in the database and if a match is found the metric is set accordingly, or if many matches are found then corresponding information is displayed on the screen. This same search can be launched directly from the g_ command, see g_ for examples.

The right-hand side in metric = ... or g[mu, nu] = ... can also be a line element, quadratic in the differentials of the coordinates (you must set the Coordinates first), passed using either of d_ or %d_, e.g. as in d_(x), d_(y), or by concatenating d with the coordinate, e.g. as in dx, dy, ...

Finally, the right-hand side in metric = ... can also be a 2 x 2 symmetric Matrix, in which case Setup extracts from it the nonzero elements using ArrayElems and sets the metric with that information; or it can also be the set returned by ArrayElems itself.

aqua, black, blue, fuchsia, gray, green, lime, maroon, navy, olive, purple, red, silver, teal, or yellow.

When mathematicalnotation is set to true, the noncommutativecolor setting causes the Maple Standard GUI to display noncommutative variables in the selected color.

Any valid sequence of characters; the same as anticommutativeprefix.

Sets the identifier for noncommutative variables, that is, variables that are neither commutative nor anticommutative.

true or false.

The default for this option is false so that the Vectors[Norm] command computes the Euclidean norm of a vector, say $A$, that is $\sqrt{A·A}$. If, however, $A$ is not commutative, or the value for normusesconjugate is set to true, then Vectors[Norm] computes the norm on complex space, as $\sqrt{{\left(A·\stackrel{\&conjugate0;}{A}\right)}^{}}$.

An equation with a Ket-label on the left-hand side and a positive integer, an algebraic expression representing it, or a range (of the form $a..b$ where $a$ and $b$ can also be half-integers) on the right-hand side; or a set of such equations.

It is valid to state different dimensions for different quantum numbers of Kets of a single basis. For that purpose, if the label of the basis is A, you can set the dimension of each quantum number entering $\mathrm{quantumbasisdimension}=\left\{A_1=N\&comma;A_2=M\right\}$, where $N$ and $M$ are positive integers, algebraic expressions representing them, or ranges of the form $a..b$. This dimension of a quantum basis is used to construct projectors when you call the Projector command.

A name, or a set of them.

Bras and Kets labeled with this name will be considered state vectors of a continuous space of quantum states. This information is taken into account when computing Brackets and Projectors.

A name, or a set of them; equivalent to quantumcontinuousbasis.

Indicates that Bras and Kets labeled with the given names belong to a discrete space of quantum states. However, unlike the quantumcontinuousbasis case, when the label (first argument) in a Bra or a Ket has not been set to represent a continuous or discrete space of states, it is assumed that it represents a discrete space.

A name, or a set of them.

Indicates that these names represent linear quantum operators. This information is taken into account when computing Brackets and scalar products between these quantum operators and Bras or Kets.

A name or a function, or set of them.

To set and unset (when used together with the keyword clear) mathematical variables and functions as real, so that the is command, and through it the rest of the Maple library, take this property into account. The same, as well as more elaborated assumptions, can be placed directly with the Assume command.

true or false.

The default for this option is false. When set to true, the sum command is automatically redefined so that: a) it can perform multi-index summation (see the Add command of Physics Library), and b) it has not premature evaluation problems.

Any of `+`, `-`, or `---+`, `+---`, `+++-`, `-+++`,

This parameter is associated with the signature of spacetime, that is, it indicates the positive and negative values of the elements of the metric after reduction to a diagonal form at a given point. The four possible values `---+`, `+---`, `+++-`, `-+++`, represent the most frequently used settings for a Minkowski spacetime. The value `+` indicates an Euclidean spacetime and is equivalent to using ++++. The value `-` is a shortcut to indicate a Minkowski spacetime with signature `---+`, the default value of signature when Physics is loaded. These conventions apply as well to a spacetime of dimension different than 4. For example in a 2+1 spacetime, you can use for instance `++-`, etc. See dimension above for details.

greek, lowercaselatin, lowercaselatin_ah, lowercaselatin_is, or uppercaselatin; the same as genericindices.

Sets the identifier for spacetime indices in that every index found in a tensor object defined by the Define command that has the spacetimeindices prefix as a root and is followed by a positive integer will be interpreted as a spacetime index.

The same values as spacetimeindices.

Sets the identifier for space indices.

The same values as spacetimeindices.

Sets the identifier for spinor indices.

The same values as spacetimeindices.

Sets the identifier for SU2 indices, that run from 1 to 3, the dimension of the SU2 group.

The same values as spacetimeindices.

Sets the identifier for SU2 matrix indices, that run from 1 to 2, the dimension of the 2x2 matrices of the SU2 group in the fundamental representation.

The same values as spacetimeindices.

Sets the identifier for SU3 indices, that run from 1 to 8, the dimension of the SU3 group.

The same values as spacetimeindices.

Sets the identifier for SU3 matrix indices, that run from 1 to 3, the dimension of the 3x3 matrices of the SU3 group in the fundamental representation.

true or false.

The default for this option is true, and so the the tensor product operator $\otimes$ is displayed when a product involves operators acting in different Hilbert spaces. In computations with paper and pencil, however, the display of that operator is frequently omitted. For that purpose, use $\mathrm{Setup}\left(\mathrm{tensorproductnotation}=\mathrm{false}\right)$.

Any procedure to be automatically applied when tensor components are computed (e.g. for the general relativity tensors)

The default tensor simplifier, automatically applied when computing the components of the predefined general relativity tensors, and also of any user-defined tensor, is Physics:-TensorSimplifier, a general simplifier with emphasis in handling radicals. Depending on the problem, however, other kinds of simplification may be more convenient. When the tensor components involve large algebraic expressions, for speed reasons, one may also prefer to only apply a (fast) normalization - for this purpose use tensorsimplifier = normal (see normal). One can also set tensorsimplifier = none in which case no simplification is applied but for some unavoidable zero recognitions performed in a few intermediate steps (e.g. when you set a spacetime metric, to verify that its determinant is different from zero). To restore the tensor simplifier to its default value use tensorsimplifier = default or Setup(redo, tensorsimplifier).

<keyword, Matrix, set(nonzero components)>

Indicates the tetrad (vierbein), relating spacetime tensor components to their components in a tetrad (local) system of references. Instead of the word tetrad the left-hand side can also be the tetrad tensor $\mathrm{\&efr;\_\_a,\&mu;}$ itself, as in e_[a, mu]. The right-hand side can be one of the keywords null (Newman-Penrose formalism), or orthonormal (related to a tetrad metric of Minkowski kind). For details, see e_.

The right-hand side in tetrad = ... or e_[mu, nu] = ... can also be a 2 x 2 symmetric Matrix, in which case Setup extracts from it the nonzero elements using ArrayElems and sets the tetrad with that information. Finally, the tetrad can be set directly by passing, on the right-hand side of tetrad = ... the set of elements returned by ArrayElems itself.

The same values as spacetimeindices.

Sets the identifier for 2 tetrad indices.

<keyword, Matrix, set(nonzero components)>

Indicates the tetrad metric. Instead of the word tetradmetric the left-hand side can also be the tetradmetric tensor ${\mathrm{eta}}_{a\&comma;b}$ itself, as in eta_[a, b]. The right-hand side can be one of the keywords null (Newman-Penrose formalism), or orthonormal (of Minkowski kind). For details, see eta_.

The right-hand side in tetradmetric = ... or eta_[mu, nu] = ... can also be a 2 x 2 symmetric Matrix, in which case Setup extracts from it the nonzero elements using ArrayElems and sets the tetradmetric with that information. Finally, the tetrad metric can be set directly by passing, on the right-hand side of tetradmetric = ... the set of elements returned by ArrayElems itself.

true or false.

The default value for this option is true, so that Trace considers scalars everything but the algebraic representation for Dirac (Dgamma) and Pauli (Psigma) matrices as tensors of one index, or objects explicitly of type matrix or Matrix (Array). The Maple 16 behavior, where everything but constants were considered traceable objects can be restored with the new Setup option traceonlymatrices = false (its default value is true). This permits using Trace more naturally in the typical case, which is the computation of traces of expressions involving Dirac matrices where the coefficients are not just constants.

A name, or a set of them.

Indicates that these names represent unitary quantum operators, that is, they satisfy $U\mathrm{Dagger}\left(U\right)=1$. This information is taken into account when simplifying products of operators using the Simplify command. When an operator is set to be unitary, it is also automatically set to be a noncommutative quantum operator (see quantumoperators).

true or false.

The default for this option is false. When set to true, you can use the coordinates themselves as tensor indices (they will represent a number, i.e. their position in the list of coordinates of the coordinates system), approximating more the notation to what we do with paper and pencil changing this setting to false.

true or false.

The default for this option is true, and so each pair of contracted tensor indices in a tensorial expression is automatically rewritten as one covariant and one contravariant. If you are handling tensorial expressions of thousands of terms and experience a slowdown in performance you can try changing this setting to false.

true or false.

The default for this option is false. When set to true, the differentiation rule of the six complex components abs, argument, conjugate, Im, Re, and signum are redefined taking complex variables and their conjugates as independent and in equal footing.

none, arrow, bold, or halfarrow.

When mathematicalnotation is set to true, the vectordisplay setting causes the Maple Standard GUI to display non-projected vectors with an arrow or halfarrow on top, or in bold, as specified.

Any valid sequence of characters.

Sets the identifier for non-projected 3-D vectors of the Physics[Vectors] subpackage.