(* Content-type: application/mathematica *) (*** Wolfram Notebook File ***) (* http://www.wolfram.com/nb *) (* CreatedBy='Mathematica 7.0' *) (*CacheID: 234*) (* Internal cache information: NotebookFileLineBreakTest NotebookFileLineBreakTest NotebookDataPosition[ 145, 7] NotebookDataLength[ 707152, 13737] NotebookOptionsPosition[ 693722, 13327] NotebookOutlinePosition[ 694267, 13348] CellTagsIndexPosition[ 694224, 13345] WindowFrame->Normal*) (* Beginning of Notebook Content *) Notebook[{ Cell[CellGroupData[{ Cell["Quantum Particle in a Box ", "Title", CellChangeTimes->{{3.472162146123662*^9, 3.4721621604241257`*^9}, { 3.4726734841923733`*^9, 3.472673484539587*^9}, 3.5710918705215187`*^9}], Cell[TextData[{ StyleBox["A little paradox, traced to a failure of hermiticity", "Subsubtitle", FontSlant->"Italic"], StyleBox["\n", "Subsubtitle"] }], "Text", CellChangeTimes->{{3.571092411435142*^9, 3.5710924286491623`*^9}, { 3.5710924873416653`*^9, 3.571092514320097*^9}, 3.571092548198052*^9}], Cell["\<\ Nicholas Wheeler 10 January 2010 Revised 16 January, in response to some observations by David Griffiths, \ Darrell Schroeder & Joel Franklin \ \>", "Text", CellChangeTimes->{{3.472162166187393*^9, 3.47216218171863*^9}, { 3.472673378816163*^9, 3.472673379712291*^9}, {3.472673495184366*^9, 3.472673505903164*^9}, {3.4726735434288073`*^9, 3.472673605777493*^9}, { 3.571092584215043*^9, 3.571092604091201*^9}}, FontSize->10], Cell[BoxData["\[IndentingNewLine]"], "Input", CellChangeTimes->{3.472162185185794*^9}], Cell[CellGroupData[{ Cell["Introduction", "Subsection", CellChangeTimes->{{3.4721622161640253`*^9, 3.472162220058502*^9}}], Cell[TextData[{ "A quantum particle of mass ", StyleBox["m", FontSlant->"Italic"], " moves on the interval 0 < ", StyleBox["x", FontSlant->"Italic"], " < ", StyleBox["a", FontSlant->"Italic"], ". 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led thus to define expansion coefficients", "Text", CellChangeTimes->{{3.472165522820037*^9, 3.472165525666668*^9}, { 3.472260794422271*^9, 3.4722608064821653`*^9}}], Cell[BoxData[ RowBox[{ RowBox[{"c", "[", "k_", "]"}], ":=", RowBox[{ FractionBox["1", SuperscriptBox[ RowBox[{"(", RowBox[{ RowBox[{"2", "k"}], "+", "1"}], ")"}], "3"]], FractionBox[ RowBox[{"8", " ", SqrtBox["15"]}], SuperscriptBox["\[Pi]", "3"]]}]}]], "Input", CellChangeTimes->{{3.472186137626004*^9, 3.472186179318109*^9}}], Cell["which are found to satisfy the normalization condition", "Text", CellChangeTimes->{{3.472260821807363*^9, 3.472260825638348*^9}, { 3.472675265973579*^9, 3.472675267403462*^9}, {3.472675538464785*^9, 3.472675575299849*^9}}], Cell[CellGroupData[{ Cell[BoxData[ RowBox[{ UnderoverscriptBox["\[Sum]", RowBox[{"k", "=", "0"}], "\[Infinity]"], SuperscriptBox[ RowBox[{"c", "[", "k", "]"}], "2"]}]], "Input"], Cell[BoxData["1"], "Output", CellChangeTimes->{3.472675556564424*^9, 3.472999320647811*^9, 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SuperscriptBox["\[ScriptCapitalH]", "2"]}]}]], "Output", CellChangeTimes->{3.473013702475313*^9, 3.571083274506514*^9}] }, Open ]], Cell[TextData[{ "Our Hamiltonian has revcaled itself to be ", StyleBox["non-Hermitian", FontWeight->"Bold"], "." }], "Text", CellChangeTimes->{{3.473013959740284*^9, 3.473013994024534*^9}}], Cell[BoxData["\[IndentingNewLine]"], "Input", CellChangeTimes->{3.5710907567024727`*^9}], Cell[TextData[{ StyleBox["MEMORANDA", "Subsection"], "\n" }], "Text", CellChangeTimes->{{3.571090774364999*^9, 3.571090812756093*^9}}], Cell["\<\ I had stewed about this problem for a couple of days when, on January 7th, I \ brought the problem to the attention of David Griffiths, who promptly \ responded as follows:\ \>", "Text", CellChangeTimes->{{3.4723191863449173`*^9, 3.472319220032589*^9}, { 3.472319357890669*^9, 3.472319359142972*^9}, {3.571090941102159*^9, 3.571090991393228*^9}}], Cell["\<\ Nick, Here's my first guess as to your error: H^2 is not a valid operator (or \ rather, your second wave function is not in the space of functions for which \ it is well-defined/Hermitian). Both your wave functions have kinks at each \ end, which means that the first derivative is discontinuous and the second \ carries a delta function. You get away with ignoring this when you calculate \ for the \"accidental\" reason reason that it is multiplied by a function \ that is zero at the ends, so the delta function does not contribute. But \ when you go to H^2 you need two more derivatives (hence the second derivative \ of the delta function). Integration by parts transfers them over to the \ other function, which means you now have the product of two deltas. For some \ reason that works in the case of the ground state, but not in the case of the \ the quadratic. Is this even vaguely relevant to your problem? David\ \>", "Text", CellChangeTimes->{3.472319224109828*^9}, FontColor->RGBColor[0, 0, 1]], Cell["\<\ When (on January 11th\[LongDash]yesterday) I mentioned the problem with \ Darrell Schroeter he made an essentially similar remark: he suggested that my \ wave function might better be written\ \>", "Text", CellChangeTimes->{{3.472319297786707*^9, 3.472319383200652*^9}, { 3.472319414171632*^9, 3.47231944751904*^9}, 3.472327826798554*^9}], Cell[BoxData[ RowBox[{ RowBox[{"\[CapitalPsi]", "[", RowBox[{"x", ",", "a"}], "]"}], "=", RowBox[{ RowBox[{"\[Psi]", "[", RowBox[{"x", ",", "a"}], "]"}], RowBox[{"S", "[", RowBox[{"x", ",", "a"}], "]"}]}]}]], "Output", CellChangeTimes->{{3.4723194629959507`*^9, 3.472319533304762*^9}}], Cell[TextData[{ "where ", StyleBox["S[x, a]", "Output"], " has unit value inside the box and vanishes outside the box. Those \ remarks/suggestions have motivated the preceeding discussion. \n\nI end with \ record of some commands that figured in earlier versions of this notebook, \ which I preserve for whatever they may someday prove to be worth:" }], "Text", CellChangeTimes->{{3.472319810337818*^9, 3.472319870976997*^9}, { 3.472328007549898*^9, 3.472328056233128*^9}, {3.571091017805304*^9, 3.5710910597706747`*^9}, {3.571091391402347*^9, 3.571091428646913*^9}}], Cell[CellGroupData[{ Cell[BoxData[ RowBox[{"CoeffList", "=", RowBox[{"Table", "[", RowBox[{ RowBox[{ SubsuperscriptBox["\[Integral]", "0", "1"], RowBox[{"x", " ", RowBox[{"e", "[", RowBox[{"x", ",", "n"}], "]"}], RowBox[{"\[DifferentialD]", "x"}]}]}], ",", RowBox[{"{", RowBox[{"n", ",", "1", ",", "20"}], "}"}]}], "]"}]}]], "Input", CellChangeTimes->{{3.4730926432585087`*^9, 3.473092666565897*^9}, { 3.473092796395226*^9, 3.47309279659888*^9}}], Cell[BoxData[ RowBox[{"{", RowBox[{ FractionBox[ SqrtBox["2"], "\[Pi]"], ",", RowBox[{"-", 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