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Within limitations, one is free to choose a standard for the \ 4-potential. For example, if one decides that the divergence of A should \ always be zero, this is called choosing the Coulomb gauge. Gauge \ transformations are a very powerful technique for solving practical problems. \ Gauge symmetry also has profound implications theoretically, particularly \ for quantum field theory. Spacetime-dependent gauge symmetry leads to the \ gauge fields that form the symmetry of the forces in the standard model, \ U(1)xSU(2)xSU(3). \ \>", "Text"], Cell[TextData[StyleBox[ "In this notebook, I will explore gauge transformations with quaternions. \ This work suggests two types of constraints on those transformations. The \ first is the continuity equation for the scalar field. The second is a \ \"continuity-like\" equation for the vector field. This second constraint is \ relevant only under relativistic conditions."]], "Text"] }, Open ]], Cell[CellGroupData[{ Cell[TextData[StyleBox[" A quaternion gauge transformation"]], "Subsection", CellMargins->{{0, Inherited}, {Inherited, Inherited}}], Cell["\<\ The E and B fields can be generated from the 4-potential phi and A \ with the following quaternion equation:\ \>", "Text"], Cell[BoxData[{ \(op[{q[dt, \[EmptyDownTriangle]\&\[RightVector]]}, q[\[Phi][t], A\&\[RightVector][t]]].{1, 0}\), \({\(-\[EmptyDownTriangle]\&\[RightVector]\)\[CenterDot]A\&\[RightVector][ t] + \[PartialD]\[Phi][t]\/\[PartialD]t, \(\[EmptyDownTriangle]\&\[RightVector]\) X A\&\[RightVector][t] + \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] \[Phi][t] + \[PartialD]A\&\[RightVector][t]\/\[PartialD]t}\)}], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell[BoxData[ \(\((\[PartialD]\/\[PartialD]t, \[EmptyDownTriangle]\&\[RightVector])\) \((\[Phi], A\&\[RightVector])\) = \((\(-\[EmptyDownTriangle]\&\[RightVector]\)\[CenterDot]A \&\[RightVector] + \[PartialD]\[Phi]\/\[PartialD]t, \[PartialD]A\&\[RightVector]\/\[PartialD]t + \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] \[Phi] + \ \(\[EmptyDownTriangle]\&\[RightVector]\) X A\&\[RightVector]) \)\)], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell["\<\ The vector term is B - E. The scalar term has the form of a gauge \ relation. The typical scalar field used in a gauge transformation involves \ the gradient and the time derivative of the scalar field. For a quaternion \ field, there is also a 3-vector component. Consider the analogous quaternion \ field L (small \"g\" is a scalar field, and big \"G\" is a 3-vector field).\ \ \>", "Text"], Cell[BoxData[ \(L = { \(g'\)[t] + \ \[EmptyDownTriangle]\&\[RightVector]\[CenterDot]G\&\[RightVector][ t], \(-\(( \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] g[t]) \)\) + \ \(G\&\[RightVector]'\)[t]}\)], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell[BoxData[ \(L = \((g' + \ \[EmptyDownTriangle]\&\[RightVector]\[CenterDot]G \&\[RightVector], \(-\[EmptyDownTriangle]\&\[RightVector]\)\[InvisibleComma] g + \ G\&\[RightVector]')\)\)], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell["\<\ The terms with the small g are the typical scalar field gauge transformation. \ The terms with the big G are my guess at a reasonable extension from a \ scalar to a quaternion field. Big G is handled in a manner that parallels \ small g, namely there is a time derivative and del operation that transforms \ vector big G into the scalar div G, just like scalar small g was transformed \ to vector Grad g. Transform the quaternion potential with L.\ \>", "Text"], Cell[BoxData[{ \(\((op[{q[dt, \[EmptyDownTriangle]\&\[RightVector]]}, q[\[Phi][t], A\&\[RightVector][t]]]\ + \n\ \ op[{q[dt, \[EmptyDownTriangle]\&\[RightVector]]}, q[\(g'\)[t], \(-\((\[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] g[t])\)\)]]\ + \n\ \ op[{q[dt, \[EmptyDownTriangle]\&\[RightVector]]}, q[\ \[EmptyDownTriangle]\&\[RightVector]\[CenterDot]G \&\[RightVector][t], \(G\&\[RightVector]'\)[t]]])\).{1, 0} \), \({\(-\[EmptyDownTriangle]\&\[RightVector]\)\[CenterDot]A\&\[RightVector][ t] + \[PartialD]\[Phi][t]\/\[PartialD]t + \ \[EmptyDownTriangle]\&\[RightVector]\[CenterDot]\(( \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] g[t])\) + \[PartialD]\^2 g[t]\/\[PartialD]t\^2, \n\t \(+\ \[EmptyDownTriangle]\&\[RightVector]\) X A\&\[RightVector][t] + \((\[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] \[Phi][t]) \) + \[PartialD]A\&\[RightVector][t]\/\[PartialD]t\n\ - \(\[EmptyDownTriangle]\&\[RightVector]\) X \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] g[t] + \(\[EmptyDownTriangle]\&\[RightVector]\) X \[PartialD]G\&\[RightVector][t]\/\[PartialD]t + \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] \((\[EmptyDownTriangle]\&\[RightVector]\[CenterDot]G\&\[RightVector][ t])\) + \[PartialD]\^2 G\&\[RightVector][t]\/\[PartialD]t\^2} \)}], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell[BoxData[ \(\((\[PartialD]\/\[PartialD]t, \[EmptyDownTriangle]\&\[RightVector])\) \((\((\[Phi], A\&\[RightVector])\)\ + \((g', \(-\[EmptyDownTriangle]\&\[RightVector]\)\[InvisibleComma] g)\)\ + \((\[EmptyDownTriangle]\&\[RightVector]\[CenterDot]G \&\[RightVector], G\&\[RightVector]')\))\)\n = \((\[PartialD]\[Phi]\/\[PartialD]t - \[EmptyDownTriangle]\&\[RightVector]\[CenterDot]A \&\[RightVector]\ + \[PartialD]\^2 g\/\[PartialD]t\^2 + \ \[EmptyDownTriangle]\&\[RightVector]\[CenterDot]\ \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] g, \n\t \[PartialD]A\&\[RightVector]\/\[PartialD]t + \ \(\[EmptyDownTriangle]\&\[RightVector]\) X A\&\[RightVector] + \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] \[Phi] + \[PartialD]\^2 G\&\[RightVector]\/\[PartialD]t\^2 + \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] \[EmptyDownTriangle]\&\[RightVector]\[CenterDot]G\&\[RightVector] + \(\[EmptyDownTriangle]\&\[RightVector]\) X \[PartialD]G\&\[RightVector]\/\[PartialD]t - \(\[EmptyDownTriangle]\&\[RightVector]\) X \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] g)\)\)], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell["\<\ An equation should not be altered by a gauge transformation, but \ that does not appear to be the case with the quaternion field L at first \ glance! There are 5 extra terms here (one of the extra terms, curl grad g, \ is always zero).\ \>", "Text"], Cell["\<\ The two extra scalar terms must always add up to zero. These terms \ involve the time derivative of a scalar and the divergence of a vector. That \ sounds like the continuity equation, so test out the following mapping: grad \ g -> J, dg/dt -> rho.\ \>", "Text"], Cell[BoxData[{ RowBox[{ \(0 == \[EmptyDownTriangle]\&\[RightVector]\[CenterDot]\(( \[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] g[t])\) + \[PartialD]\^2 g[t]\/\[PartialD]t\^2\), " ", "/.", "\n", "\t", RowBox[{"{", RowBox[{ \(\((\[EmptyDownTriangle]\&\[RightVector]\[InvisibleComma] g[t])\) -> \ J\), ",", StyleBox[\(\(Derivative[2]\)[g] -> \(Derivative[1]\)[\[Rho]]\), ShowStringCharacters->True]}], "}"}]}], \(0 == \[EmptyDownTriangle]\&\[RightVector]\[CenterDot]J + \[PartialD]\[Rho][t]\/\[PartialD]t\)}], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell[BoxData[{ \(\[EmptyDownTriangle]\&\[RightVector]\[CenterDot]\[EmptyDownTriangle]\&\ \[RightVector]\[InvisibleComma] g + \[PartialD]\^2 g\/\[PartialD]t\^2 = 0\), RowBox[{ \(if\t\[EmptyDownTriangle]\&\[RightVector]\), "\[InvisibleComma]", RowBox[{\(g -> \ J\), ",", StyleBox[\(\[PartialD]g\/\[PartialD]t -> \[Rho]\), ShowStringCharacters->True], StyleBox[",", ShowStringCharacters->True], StyleBox[" ", ShowStringCharacters->True], RowBox[{ RowBox[{ RowBox[{ StyleBox["then", ShowStringCharacters->True], " ", \(\[EmptyDownTriangle]\&\[RightVector]\[CenterDot]J\)}], "+", \(\[PartialD]\[Rho]\/\[PartialD]t\)}], " ", "=", " ", "0"}]}]}]}], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell["\<\ This is the continuity equation. It is noteworthy that the \ continuity equation arises naturally from an analysis of a quaternion gauge \ transformation. The J must be irrotational (Curl J = Curl Grad g = 0). This \ may be due to my choice for big G which lacked a curl, but I am uncertain on \ this point.\ \>", "Text"], Cell["\<\ What about the three vector terms? They reform the vector \ potential with the following mapping.\ \>", "Text"], Cell[BoxData[{ RowBox[{ \(0 == \(\[EmptyDownTriangle]\&\[RightVector]\) X \( G\&\[RightVector]'\)[t] + \(\[EmptyDownTriangle]\&\[RightVector]\) \((\[EmptyDownTriangle]\&\[RightVector]\[CenterDot]G \&\[RightVector][t])\) + \[PartialD]\^2 G\&\[RightVector][t]\/\[PartialD]t\^2\), " ", "/.", "\n", "\t\t", RowBox[{"{", RowBox[{ \(\((\[EmptyDownTriangle]\&\[RightVector]\[CenterDot]G \&\[RightVector][t])\) -> \[Phi][t]\), ",", " ", StyleBox[ RowBox[{\(\(Derivative[2]\)[G\&\[RightVector]]\), "->", RowBox[{\(Derivative[1]\), "[", OverscriptBox[ StyleBox["A", ShowStringCharacters->True], "\[RightVector]"], "]"}]}], ShowStringCharacters->True], StyleBox[",", ShowStringCharacters->True], "\n", "\t\t\t\t", StyleBox[ RowBox[{\(\(Derivative[1]\)[G\&\[RightVector]]\), "->", OverscriptBox[ StyleBox["A", ShowStringCharacters->True], "\[RightVector]"]}], ShowStringCharacters->True]}], StyleBox["}", ShowStringCharacters->True]}]}], \(0 == \(\[EmptyDownTriangle]\&\[RightVector]\) X A\&\[RightVector][t] + \[EmptyDownTriangle]\&\[RightVector]\ \[Phi][t] + \[PartialD]A\&\[RightVector][t]\/\[PartialD]t\)}], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell[BoxData[{ \(\(\[EmptyDownTriangle]\&\[RightVector]\) X \[PartialD]G\&\[RightVector]\/\[PartialD]t + \(\[EmptyDownTriangle]\&\[RightVector]\) \((\[EmptyDownTriangle]\&\[RightVector]\[CenterDot]G \&\[RightVector])\) + \[PartialD]\^2 G\&\[RightVector]\/\[PartialD]t\^2\ = 0\), RowBox[{ RowBox[{\(if\ \ \ \[PartialD]G\&\[RightVector]\/\[PartialD]t\), StyleBox["->", ShowStringCharacters->True], StyleBox[ OverscriptBox[ StyleBox["A", ShowStringCharacters->True], "\[RightVector]"], ShowStringCharacters->True]}], StyleBox[" ", ShowStringCharacters->True], StyleBox[",", ShowStringCharacters->True], RowBox[{ RowBox[{ \(\[EmptyDownTriangle]\&\[RightVector]\[CenterDot]G\&\[RightVector]\), "->", RowBox[{ RowBox[{"\[Phi]", StyleBox[" ", ShowStringCharacters->True], StyleBox["then", ShowStringCharacters->True], StyleBox[" ", ShowStringCharacters->True], \(\[EmptyDownTriangle]\&\[RightVector]\), "X", \(A\&\[RightVector]\)}], "+", \(\[EmptyDownTriangle]\&\[RightVector]\ \[Phi]\), "+", \(\[PartialD]A\&\[RightVector]\/\[PartialD]t\)}]}], "=", "0"}]}]}], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell["\<\ This mapping proposes that the a gauge transformation will be valid \ only if B - E = 0. In some sense, this is like a continuity equation for the \ vector field big G. The time rate of change of A must balance the gradient \ phi and the curl of A, which all can be expressed in terms of the same vector \ field big G. This is a new constraint, but it neatly parallels the scalar \ continuity equation, which applied only to the scalar field g with the \ mapping discussed here.\ \>", "Text"] }, Open ]], Cell[CellGroupData[{ Cell["Implications", "Subsection", CellMargins->{{0, Inherited}, {Inherited, Inherited}}], Cell["\<\ Every constraint has regions where is is applicable. Newtonian \ physics works until the speed of light is approached. Classical atomic \ physics works until the number of particles gets small. The vector gauge \ continuity constraint is not relevant for classical electrodynamics. The \ classical region of spacetime happens for intervals where\ \>", "Text"], Cell[BoxData[ \(\(|\[CapitalDelta]t | \)\ >>> \ |\[CapitalDelta]x, \ \[CapitalDelta]y, \ \[CapitalDelta]z | \ \ \( == \ classical\ physics\)\)], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell[BoxData[ \(\(|\[CapitalDelta]t | \)\ >>> \ |\[CapitalDelta]x, \ \[CapitalDelta]y, \ \[CapitalDelta]z | \ \ \( == \ classical\ physics\)\)], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell["An analogous region for a gauge transformation is", "Text"], Cell[BoxData[ RowBox[{"g", " ", ">>>", " ", StyleBox[\(G\&\[RightVector]\ \ == \ classical\ EM\), ShowStringCharacters->True]}]], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell[BoxData[ RowBox[{"g", " ", ">>>", " ", StyleBox[\(G\&\[RightVector]\ \ == \ classical\ EM\), ShowStringCharacters->True]}]], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell["In this region, the gauge transformation then simplifies to", "Text"], Cell[BoxData[{ \(\[Phi]\ -> \ \[Phi]'\ = \ \[Phi]\ - \ \[PartialD]g[t]\/\[PartialD]t\), \(A\ -> \ A'\ = \ A\ + \ \[EmptyDownTriangle]\&\[RightVector]\ g\)}], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell[BoxData[{ \(\[Phi]\ -> \ \[Phi]'\ = \ \[Phi]\ - \ \[PartialD]g\/\[PartialD]t\), \(A\ -> \ A'\ = \ A\ + \ \[EmptyDownTriangle]\&\[RightVector]\ g\)}], "Input", CellMargins->{{18, Inherited}, {Inherited, Inherited}}, FontSize->16], Cell["\<\ This is precisely the type of transformation that has been used so \ often before, and it is still part of the quaternion formulation of the \ Maxwell equations in the classical domain.\ \>", "Text"], Cell["\<\ The question now concerns the validity of gauge freedom of the \ Maxwell equations under relativistic conditions, a cornerstone of quantum \ field theory. I prefer to constrain the vector portion of gauge \ transformations under relativistic conditions with a continuity equation for \ the vector field that has symmetry with the scalar continuity equation. This \ may help avoid the difficulties of regularization and renomalization, but \ that issue needs more investigation.\ \>", "Text"] }, Open ]] }, Open ]] }, FrontEndVersion->"Microsoft Windows 3.0", ScreenRectangle->{{0, 640}, {0, 451}}, AutoGeneratedPackage->None, WindowToolbars->{"RulerBar", "EditBar"}, CellGrouping->Automatic, WindowSize->{594, 299}, WindowMargins->{{-5, Automatic}, {Automatic, 7}}, PrintingCopies->1, PrintingPageRange->{1, Automatic}, PageHeaders->{{Cell[ TextData[ { CounterBox[ "Page"]}], "PageNumber"], Inherited, Cell[ TextData[ { ValueBox[ "FileName"]}], "Header"]}, {Cell[ TextData[ { ValueBox[ "FileName"]}], "Header"], Inherited, Cell[ TextData[ { CounterBox[ "Page"]}], "PageNumber"]}}, PrintingOptions->{"PrintingMargins"->{{72, 57.5625}, {57.5625, 72}}, "PrintCellBrackets"->False, "PrintRegistrationMarks"->False, "PrintMultipleHorizontalPages"->False, "FirstPageHeader"->False}, PrivateNotebookOptions->{"ColorPalette"->{RGBColor, 128}}, ShowCellTags->False, RenderingOptions->{"ObjectDithering"->True, "RasterDithering"->False}, CharacterEncoding->"MacintoshAutomaticEncoding", StyleDefinitions -> Notebook[{ Cell[CellGroupData[{ Cell[TextData[StyleBox["Style Definitions"]], "Subtitle"], Cell[TextData[StyleBox[ "Modify the definitions below to change the default appearance of all cells \ in a given style. 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FontSize->14, FontWeight->"Plain"], Cell[StyleData["Input", "Condensed"], CellMargins->{{40, 10}, {2, 3}}, FontFamily->"Courier", FontSize->14, FontWeight->"Plain"], Cell[StyleData["Input", "Printout"], CellMargins->{{39, 0}, {4, 6}}, FontFamily->"Courier", FontSize->14, FontWeight->"Plain"] }, Closed]], Cell[StyleData["InputOnly"], Evaluatable->True, CellGroupingRules->"InputGrouping", CellHorizontalScrolling->True, DefaultFormatType->DefaultInputFormatType, AutoItalicWords->{}, FormatType->InputForm, ShowStringCharacters->True, NumberMarks->True, CounterIncrements->"Input", StyleMenuListing->None, FontFamily->"Courier", FontSize->14, FontWeight->"Plain", FontSlant->"Plain", FontTracking->"Plain", FontVariations->{"Underline"->False, "Outline"->False, "Shadow"->False}], Cell[CellGroupData[{ Cell[StyleData["Output"], PageWidth->Infinity, CellMargins->{{42, 10}, {7, 5}}, CellEditDuplicate->True, Evaluatable->False, CellGroupingRules->"OutputGrouping", CellHorizontalScrolling->True, PageBreakWithin->False, GroupPageBreakWithin->False, GeneratedCell->True, CellAutoOverwrite->True, CellLabelMargins->{{23, Inherited}, {Inherited, Inherited}}, DefaultFormatType->DefaultOutputFormatType, LineSpacing->{1, 0}, AutoItalicWords->{}, FormatType->InputForm, CounterIncrements->"Output", AspectRatioFixed->True, FontFamily->"Courier", FontSize->14, FontWeight->"Plain", FontSlant->"Plain", FontTracking->"Plain", FontVariations->{"Underline"->False, "Outline"->False, "Shadow"->False}], Cell[StyleData["Output", "Presentation"], CellMargins->{{72, Inherited}, {10, 8}}, LineSpacing->{1, 0}, FontFamily->"Courier", FontSize->14], Cell[StyleData["Output", "Condensed"], CellMargins->{{41, Inherited}, {3, 2}}, FontFamily->"Courier", FontSize->14], Cell[StyleData["Output", "Printout"], CellMargins->{{39, 0}, {6, 4}}, FontFamily->"Courier", FontSize->14] }, Closed]], Cell[CellGroupData[{ Cell[StyleData["Message"], PageWidth->Infinity, CellMargins->{{42, Inherited}, {Inherited, Inherited}}, Evaluatable->False, CellGroupingRules->"OutputGrouping", PageBreakWithin->False, GroupPageBreakWithin->False, GeneratedCell->True, CellAutoOverwrite->True, ShowCellLabel->False, CellLabelMargins->{{23, Inherited}, {Inherited, Inherited}}, DefaultFormatType->DefaultOutputFormatType, LineSpacing->{1, 0}, AutoItalicWords->{}, FormatType->InputForm, CounterIncrements->"Message", AspectRatioFixed->True, StyleMenuListing->None, FontFamily->"Courier", FontSize->14, FontWeight->"Plain", FontSlant->"Plain", FontTracking->"Plain", FontColor->RGBColor[0.500008, 0, 0], FontVariations->{"Underline"->False, "Outline"->False, "Shadow"->False}], Cell[StyleData["Message", "Presentation"], CellMargins->{{72, Inherited}, {Inherited, Inherited}}, LineSpacing->{1, 0}, FontFamily->"Courier", FontSize->14], Cell[StyleData["Message", "Condensed"], CellMargins->{{41, Inherited}, {Inherited, Inherited}}, FontFamily->"Courier", FontSize->14], Cell[StyleData["Message", "Printout"], CellMargins->{{39, Inherited}, {Inherited, Inherited}}, FontFamily->"Courier", FontSize->14, FontColor->GrayLevel[0]] }, Closed]], Cell[CellGroupData[{ Cell[StyleData["Print"], PageWidth->Infinity, CellMargins->{{42, Inherited}, {Inherited, Inherited}}, Evaluatable->False, CellGroupingRules->"OutputGrouping", CellHorizontalScrolling->True, PageBreakWithin->False, GroupPageBreakWithin->False, GeneratedCell->True, CellAutoOverwrite->True, ShowCellLabel->False, CellLabelMargins->{{23, Inherited}, {Inherited, Inherited}}, DefaultFormatType->DefaultOutputFormatType, LineSpacing->{1, 0}, AutoItalicWords->{}, FormatType->InputForm, CounterIncrements->"Print", AspectRatioFixed->True, StyleMenuListing->None, FontFamily->"Courier", FontSize->14, FontWeight->"Plain", FontSlant->"Plain", FontTracking->"Plain", FontVariations->{"Underline"->False, "Outline"->False, "Shadow"->False}], Cell[StyleData["Print", "Presentation"], CellMargins->{{72, Inherited}, {Inherited, Inherited}}, LineSpacing->{1, 0}, FontFamily->"Courier", FontSize->14], Cell[StyleData["Print", "Condensed"], CellMargins->{{41, Inherited}, {Inherited, Inherited}}, FontFamily->"Courier", FontSize->14], Cell[StyleData["Print", "Printout"], CellMargins->{{39, Inherited}, {Inherited, Inherited}}, FontFamily->"Courier", FontSize->14] }, Closed]], Cell[CellGroupData[{ Cell[StyleData["Graphics"], PageWidth->Infinity, CellMargins->{{7, Inherited}, {Inherited, Inherited}}, Evaluatable->False, CellGroupingRules->"GraphicsGrouping", CellHorizontalScrolling->True, PageBreakWithin->False, GroupPageBreakWithin->False, GeneratedCell->True, CellAutoOverwrite->True, ShowCellLabel->False, DefaultFormatType->DefaultOutputFormatType, FormatType->InputForm, CounterIncrements->"Graphics", AspectRatioFixed->True, ImageSize->{387, 393}, ImageMargins->{{34, Inherited}, {Inherited, 0}}, StyleMenuListing->None, FontFamily->"Courier", FontSize->14, FontWeight->"Plain", FontSlant->"Plain", FontTracking->"Plain", FontVariations->{"Underline"->False, "Outline"->False, "Shadow"->False}], Cell[StyleData["Graphics", "Presentation"], ImageMargins->{{62, Inherited}, {Inherited, 0}}, FontFamily->"Courier", FontSize->14], Cell[StyleData["Graphics", "Condensed"], ImageSize->{175, 175}, ImageMargins->{{38, Inherited}, {Inherited, 0}}, FontFamily->"Courier", FontSize->14], Cell[StyleData["Graphics", "Printout"], ImageSize->{250, 250}, ImageMargins->{{30, Inherited}, {Inherited, 0}}, FontFamily->"Courier", FontSize->14] }, Closed]], Cell[CellGroupData[{ Cell[StyleData["CellLabel"], StyleMenuListing->None, FontFamily->"Courier", FontSize->14, FontWeight->"Plain", FontSlant->"Plain", FontTracking->"Plain", FontColor->RGBColor[0, 0, 1], FontVariations->{"Underline"->False, "Outline"->False, "Shadow"->False}], Cell[StyleData["CellLabel", "Presentation"], FontFamily->"Courier", FontSize->14], Cell[StyleData["CellLabel", "Condensed"], FontFamily->"Courier", FontSize->14], Cell[StyleData["CellLabel", "Printout"], FontFamily->"Courier", FontSize->14, FontColor->GrayLevel[0]] }, Closed]] }, Closed]], Cell[CellGroupData[{ Cell[TextData[StyleBox["Formulas and Programming"]], "Section"], Cell[CellGroupData[{ Cell[StyleData["InlineFormula"], CellMargins->{{10, 4}, {0, 8}}, CellHorizontalScrolling->True, ScriptLevel->1, SingleLetterItalics->True], Cell[StyleData["InlineFormula", "Presentation"], CellMargins->{{24, 10}, {10, 10}}, LineSpacing->{1, 5}], Cell[StyleData["InlineFormula", "Condensed"], CellMargins->{{8, 10}, {6, 6}}, LineSpacing->{1, 1}], Cell[StyleData["InlineFormula", "Printout"], CellMargins->{{2, 0}, {6, 6}}] }, Closed]], Cell[CellGroupData[{ Cell[StyleData["DisplayFormula"], CellMargins->{{42, Inherited}, {Inherited, Inherited}}, CellHorizontalScrolling->True, DefaultFormatType->DefaultInputFormatType, ScriptLevel->0, SingleLetterItalics->True, UnderoverscriptBoxOptions->{LimitsPositioning->True}], Cell[StyleData["DisplayFormula", "Presentation"], LineSpacing->{1, 5}], Cell[StyleData["DisplayFormula", "Condensed"], LineSpacing->{1, 1}], Cell[StyleData["DisplayFormula", "Printout"]] }, Closed]] }, Closed]], Cell[CellGroupData[{ Cell[TextData[StyleBox["Styles for Headers and Footers"]], "Section"], Cell[StyleData["Header"], CellMargins->{{7, 0}, {4, 1}}, Evaluatable->False, PageBreakWithin->Automatic, AspectRatioFixed->True, StyleMenuListing->None, FontFamily->"Times", FontSize->12, FontSlant->"Italic"], Cell[StyleData["Footer"], CellMargins->{{7, 0}, {0, 4}}, Evaluatable->False, PageBreakWithin->Automatic, TextAlignment->Center, AspectRatioFixed->True, StyleMenuListing->None, FontFamily->"Times", FontSize->12, FontSlant->"Italic"], Cell[StyleData["PageNumber"], CellMargins->{{0, 0}, {4, 1}}, StyleMenuListing->None, FontFamily->"Times", FontSize->10] }, Closed]], Cell[CellGroupData[{ Cell[TextData[StyleBox["Palette Styles"]], "Section"], Cell[TextData[StyleBox[ "The cells below define styles that define standard ButtonFunctions, for \ use in palette buttons."]], "Text"], Cell[StyleData["Paste"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`NotebookApply[ FrontEnd`InputNotebook[ ], #, After]}]&)}], Cell[StyleData["Evaluate"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`NotebookApply[ FrontEnd`InputNotebook[ ], #, All], SelectionEvaluate[ FrontEnd`InputNotebook[ ], All]}]&)}], Cell[StyleData["EvaluateCell"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`NotebookApply[ FrontEnd`InputNotebook[ ], #, All], FrontEnd`SelectionMove[ FrontEnd`InputNotebook[ ], All, Cell, 1], FrontEnd`SelectionEvaluateCreateCell[ FrontEnd`InputNotebook[ ], All]}]&)}], Cell[StyleData["CopyEvaluate"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`SelectionCreateCell[ FrontEnd`InputNotebook[ ], All], FrontEnd`NotebookApply[ FrontEnd`InputNotebook[ ], #, All], FrontEnd`SelectionEvaluate[ FrontEnd`InputNotebook[ ], All]}]&)}], Cell[StyleData["CopyEvaluateCell"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`SelectionCreateCell[ FrontEnd`InputNotebook[ ], All], FrontEnd`NotebookApply[ FrontEnd`InputNotebook[ ], #, All], FrontEnd`SelectionEvaluateCreateCell[ FrontEnd`InputNotebook[ ], All]}]&)}] }, Closed]], Cell[CellGroupData[{ Cell[TextData[StyleBox["Hyperlink Styles"]], "Section"], Cell[TextData[StyleBox[ "The cells below define styles useful for making hypertext ButtonBoxes. \ The \"Hyperlink\" style is for links within the same Notebook, or between \ Notebooks."]], "Text"], Cell[CellGroupData[{ Cell[StyleData["Hyperlink"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, FontColor->RGBColor[0, 0, 1], FontVariations->{"Underline"->True}, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`NotebookLocate[ #2]}]&), Active->True, ButtonNote->ButtonData}], Cell[StyleData["Hyperlink", "Presentation"]], Cell[StyleData["Hyperlink", "Condensed"]], Cell[StyleData["Hyperlink", "Printout"], FontColor->GrayLevel[0], FontVariations->{"Underline"->False}] }, Closed]], Cell[TextData[StyleBox[ "The following styles are for linking automatically to the on-line help \ system."]], "Text"], Cell[CellGroupData[{ Cell[StyleData["MainBookLink"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, FontColor->RGBColor[0, 0, 1], FontVariations->{"Underline"->True}, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`HelpBrowserLookup[ "MainBook", #]}]&), Active->True, ButtonFrame->"None"}], Cell[StyleData["MainBookLink", "Presentation"]], Cell[StyleData["MainBookLink", "Condensed"]], Cell[StyleData["MainBookLink", "Printout"], FontColor->GrayLevel[0], FontVariations->{"Underline"->False}] }, Closed]], Cell[CellGroupData[{ Cell[StyleData["AddOnsLink"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, FontFamily->"Courier", FontColor->RGBColor[0, 0, 1], FontVariations->{"Underline"->True}, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`HelpBrowserLookup[ "AddOns", #]}]&), Active->True, ButtonFrame->"None"}], Cell[StyleData["AddOnsLink", "Presentation"]], Cell[StyleData["AddOnsLink", "Condensed"]], Cell[StyleData["AddOnLink", "Printout"], FontColor->GrayLevel[0], FontVariations->{"Underline"->False}] }, Closed]], Cell[CellGroupData[{ Cell[StyleData["RefGuideLink"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, FontFamily->"Courier", FontColor->RGBColor[0, 0, 1], FontVariations->{"Underline"->True}, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`HelpBrowserLookup[ "RefGuideLink", #]}]&), Active->True, ButtonFrame->"None"}], Cell[StyleData["RefGuideLink", "Presentation"]], Cell[StyleData["RefGuideLink", "Condensed"]], Cell[StyleData["RefGuideLink", "Printout"], FontColor->GrayLevel[0], FontVariations->{"Underline"->False}] }, Closed]], Cell[CellGroupData[{ Cell[StyleData["GettingStartedLink"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, FontColor->RGBColor[0, 0, 1], FontVariations->{"Underline"->True}, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`HelpBrowserLookup[ "GettingStarted", #]}]&), Active->True, ButtonFrame->"None"}], Cell[StyleData["GettingStartedLink", "Presentation"]], Cell[StyleData["GettingStartedLink", "Condensed"]], Cell[StyleData["GettingStartedLink", "Printout"], FontColor->GrayLevel[0], FontVariations->{"Underline"->False}] }, Closed]], Cell[CellGroupData[{ Cell[StyleData["OtherInformationLink"], StyleMenuListing->None, ButtonStyleMenuListing->Automatic, FontColor->RGBColor[0, 0, 1], FontVariations->{"Underline"->True}, ButtonBoxOptions->{ButtonFunction:>(FrontEndExecute[ { FrontEnd`HelpBrowserLookup[ "OtherInformation", #]}]&), Active->True, ButtonFrame->"None"}], Cell[StyleData["OtherInformationLink", "Presentation"]], Cell[StyleData["OtherInformationLink", "Condensed"]], Cell[StyleData["OtherInformationLink", "Printout"], FontColor->GrayLevel[0], FontVariations->{"Underline"->False}] }, Closed]] }, Closed]], Cell[CellGroupData[{ Cell[TextData[StyleBox["Placeholder Styles"]], "Section"], Cell[TextData[StyleBox[ "The cells below define styles useful for making placeholder objects in \ palette templates."]], "Text"], Cell[CellGroupData[{ Cell[StyleData["Placeholder"], Editable->False, Selectable->False, StyleBoxAutoDelete->True, Placeholder->True, StyleMenuListing->None], Cell[StyleData["Placeholder", "Presentation"]], Cell[StyleData["Placeholder", "Condensed"]], Cell[StyleData["Placeholder", "Printout"]] }, Closed]], Cell[CellGroupData[{ Cell[StyleData["SelectionPlaceholder"], Editable->False, Selectable->False, StyleBoxAutoDelete->True, Placeholder->Primary, StyleMenuListing->None, DrawHighlighted->True], Cell[StyleData["SelectionPlaceholder", "Presentation"]], Cell[StyleData["SelectionPlaceholder", "Condensed"]], Cell[StyleData["SelectionPlaceholder", "Printout"]] }, Closed]] }, Closed]], Cell[CellGroupData[{ Cell[TextData[StyleBox["FormatType Styles"]], "Section"], Cell[TextData[StyleBox[ "The cells below define styles that are mixed in with the styles of most \ cells. If a cell's FormatType matches the name of one of the styles defined \ below, then that style is applied between the cell's style and its own \ options."]], "Text"], Cell[StyleData["CellExpression"], PageWidth->Infinity, CellMargins->{{6, Inherited}, {Inherited, Inherited}}, ShowCellLabel->False, ShowSpecialCharacters->False, AllowInlineCells->False, AutoItalicWords->{}, StyleMenuListing->None, FontFamily->"Courier", Background->GrayLevel[1]], Cell[StyleData["InputForm"], AllowInlineCells->False, StyleMenuListing->None, FontFamily->"Courier"], Cell[StyleData["OutputForm"], PageWidth->Infinity, TextAlignment->Left, LineSpacing->{1, -5}, StyleMenuListing->None, FontFamily->"Courier"], Cell[StyleData["StandardForm"], LineSpacing->{1.25, 0}, StyleMenuListing->None, FontFamily->"Courier"], Cell[StyleData["TraditionalForm"], LineSpacing->{1.25, 0}, SingleLetterItalics->True, TraditionalFunctionNotation->True, DelimiterMatching->None, StyleMenuListing->None], Cell[TextData[StyleBox[ "The style defined below is mixed in to any cell that is in an inline cell \ within another."]], "Text"], Cell[StyleData["InlineCell"], TextAlignment->Left, ScriptLevel->1, StyleMenuListing->None], Cell[StyleData["InlineCellEditing"], StyleMenuListing->None, Background->RGBColor[1, 0.749996, 0.8]] }, Closed]] }, Open ]] }] ] (*********************************************************************** Cached data follows. 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